Sample records for ice pack test

  1. Ice Pack Heat Sink Subsystem - Phase I. [astronaut liquid cooling garment design and testing

    NASA Technical Reports Server (NTRS)

    Roebelen, G. J., Jr.

    1973-01-01

    This paper describes the design and test at one-g of a functional laboratory model (non-flight) Ice Pack Heat Sink Subsystem to be used eventually for astronaut cooling during manned space missions. In normal use, excess heat in the liquid cooling garment (LCG) coolant is transferred to a reusable/regenerable ice pack heat sink. For emergency operation, or for extension of extravehicular activity mission time after all the ice has melted, water from the ice pack is boiled to vacuum, thereby continuing to remove heat from the LCG coolant. This subsystem incorporates a quick connect/disconnect thermal interface between the ice pack heat sink and the subsystem heat exchanger.

  2. Effect of local cooling on excitation-contraction coupling in myasthenic muscle: Another mechanism of ice-pack test in myasthenia gravis.

    PubMed

    Yamamoto, Daisuke; Imai, Tomihiro; Tsuda, Emiko; Hozuki, Takayoshi; Yamauchi, Rika; Hisahara, Shin; Kawamata, Jun; Shimohama, Shun

    2017-11-01

    The ice-pack test is a convenient diagnostic testing procedure for myasthenia gravis (MG). We investigated the underlying mechanism of the ice-pack test performed on bilateral masseters. We performed trigeminal repetitive nerve stimulation (RNS), excitation-contraction (E-C) coupling assessment (Imai's method) and bite force measurement before and after cooling of the masseters in MG patients and normal controls. After placing the ice-pack on the masseters for 3min, serial recordings of the three tests were performed at various time intervals during 10min after cooling. The bite force increased significantly after cooling in ice-pack-positive MG patients. The acceleration and acceleration ratio (acceleration at a given time to baseline acceleration) of jaw movement increased significantly after cooling of the masseters in ice-pack-positive MG patients compared to ice-pack-negative patients and normal controls. The prolonged effect of cooling continued until the end of recording even though decremental response to RNS had returned to baseline value. Cooling of myasthenic muscle may induce two effects. One is relatively short effect on electrical synaptic transmission at the endplate, and another is prolonged effect on E-C coupling in the muscle. The ice-pack test induces a prolonged effect of ameliorating impaired E-C coupling in MG. Copyright © 2017 International Federation of Clinical Neurophysiology. Published by Elsevier B.V. All rights reserved.

  3. Ice pack heat sink subsystem - Phase 1, Volume 1

    NASA Technical Reports Server (NTRS)

    Roebelen, G. J., Jr.

    1973-01-01

    The design, development, fabrication, and test at one-g of a functional laboratory model (non-flight) ice pack heat sink subsystem to be used eventually for astronaut cooling during manned space missions are discussed. In normal use, excess heat in the liquid cooling garment (LCG) coolant is transferred to a reusable/regenerable ice pack heat sink. For emergency operation, or for extension of extravehicular activity mission time after all the ice has melted, water from the ice pack is boiled to vacuum, thereby continuing to remove heat from the LCG coolant. This subsystem incorporates a quick connect/disconnect thermal interface between the ice pack heat sink and the subsystem heat exchanger.

  4. STS-48 ESC Earth observation of ice pack, Antarctic Ice Shelf

    NASA Technical Reports Server (NTRS)

    1991-01-01

    STS-48 Earth observation taken aboard Discovery, Orbiter Vehicle (OV) 103, is of the breakup of pack ice along the periphery of the Antarctic Ice Shelf. Strong offshore winds, probably associated with katabatic downdrafts from the interior of the continent, are seen peeling off the edges of the ice shelf into long filaments of sea ice, icebergs, bergy bits, and growlers to flow northward into the South Atlantic Ocean. These photos are used to study ocean wind, tide and current patterns. Similar views photographed during previous missions, when analyzed with these recent views may yield information about regional ice drift and breakup of ice packs. The image was captured using an electronic still camera (ESC), was stored on a removable hard disk or small optical disk, and was converted to a format suitable for downlink transmission. The ESC documentation was part of Development Test Objective (DTO) 648, Electronic Still Photography.

  5. SPH Modelling of Sea-ice Pack Dynamics

    NASA Astrophysics Data System (ADS)

    Staroszczyk, Ryszard

    2017-12-01

    The paper is concerned with the problem of sea-ice pack motion and deformation under the action of wind and water currents. Differential equations describing the dynamics of ice, with its very distinct mateFfigrial responses in converging and diverging flows, express the mass and linear momentum balances on the horizontal plane (the free surface of the ocean). These equations are solved by the fully Lagrangian method of smoothed particle hydrodynamics (SPH). Assuming that the ice behaviour can be approximated by a non-linearly viscous rheology, the proposed SPH model has been used to simulate the evolution of a sea-ice pack driven by wind drag stresses. The results of numerical simulations illustrate the evolution of an ice pack, including variations in ice thickness and ice area fraction in space and time. The effects of different initial ice pack configurations and of different conditions assumed at the coast-ice interface are examined. In particular, the SPH model is applied to a pack flow driven by a vortex wind to demonstrate how well the Lagrangian formulation can capture large deformations and displacements of sea ice.

  6. Breakup of Pack Ice, Antarctic Ice Shelf

    NASA Technical Reports Server (NTRS)

    1991-01-01

    Breakup of Pack Ice along the periphery of the Antarctic Ice Shelf (53.5S, 3.0E) produced this mosaic of ice floes off the Antarctic Ice Shelf. Strong offshore winds, probably associated with strong katabatic downdrafts from the interior of the continent, are seen peeling off the edges of the ice shelf into long filamets of sea ice, icebergs, bergy bits and growlers to flow northward into the South Atlantic Ocean. 53.5S, 3.0E

  7. Ice pack heat sink subsystem, phase 2. [astronaut life support cooling system

    NASA Technical Reports Server (NTRS)

    Roebelen, G. J., Jr.; Kellner, J. D.

    1975-01-01

    The report describes the design, development, fabrication, and test at one gravity of a prototype ice pack heat sink subsystem to be used eventually for astronaut cooling during manned space missions; the investigation of thermal storage material with the objective of uncovering materials with heats of fusion and/or solution in the range of 300 Btu/lb (700 kilojoules/kilogram); and the planned procedure for implementing an ice pack heat sink subsystem flight experiment. In normal use, excess heat in the liquid cooling garment (LCG) coolant is transferred to a reusable/regenerable ice pack heat sink. For emergency operation, or for extension of extravehicular activity mission time after all the ice has melted, water from the ice pack is boiled to vacuum, thereby continuing to remove heat from the LCG coolant. This subsystem incorporates a quick disconnect thermal interface between the ice pack heat sink and the subsystem heat exchanger.

  8. Length of perineal pain relief after ice pack application: A quasi-experimental study.

    PubMed

    de Souza Bosco Paiva, Caroline; Junqueira Vasconcellos de Oliveira, Sonia Maria; Amorim Francisco, Adriana; da Silva, Renata Luana; de Paula Batista Mendes, Edilaine; Steen, Mary

    2016-04-01

    Ice pack is effective for alleviating postpartum perineal pain in primiparous women while multiparous women's levels of perineal pain appear to be poorly explored. Ice pack is a low-cost non-invasive localised treatment that can be used with no impact on breastfeeding. However, how long perineal analgesia persists after applying an ice pack is still unknown. To evaluate if perineal analgesia is maintained up to 2h after applying an ice pack to the perineum for 20min. A quasi-experimental study, using a pre and post-test design, was undertaken with a sample size of 50 multiparous women in Brazil. Data was collected by structured interview. The intervention involved a single application of an ice pack applied for 20min to the perineal area of women who reported perineal pain ≥3 by use of a numeric rating scale (0-10), with intact perineum, 1st or 2nd degree lacerations or episiotomy, between 6 and 24h after spontaneous vaginal birth. Perineal pain was evaluated at three points of time: before, immediately after and 2h after applying an ice pack. Immediately after applying an ice pack to the perineal area, there was a significant reduction in the severity of perineal pain reported (5.4 vs. 1.0, p<0.0005), which continued for 1h 35min up to 2h after the local application. Ice pack application for 20min is effective for alleviating postpartum perineal pain and continues to be effective between 1h 35min for up to 2h. Copyright © 2015 Australian College of Midwives. Published by Elsevier Ltd. All rights reserved.

  9. Ice pack heat sink subsystem - phase 1, volume 2

    NASA Technical Reports Server (NTRS)

    Roebelen, G. J., Jr.

    1973-01-01

    The design, development, and test of a functional laboratory model ice pack heat sink subsystem are discussed. Operating instructions to include mechanical and electrical schematics, maintenance instructions, and equipment specifications are presented.

  10. Experimental Investigation of the Resistance Performance and Heave and Pitch Motions of Ice-Going Container Ship Under Pack Ice Conditions

    NASA Astrophysics Data System (ADS)

    Guo, Chun-yu; Xie, Chang; Zhang, Jin-zhao; Wang, Shuai; Zhao, Da-gang

    2018-04-01

    In order to analyze the ice-going ship's performance under the pack ice conditions, synthetic ice was introduced into a towing tank. A barrier using floating cylinder in the towing tank was designed to carry out the resistance experiment. The test results indicated that the encountering frequency between the ship model and the pack ice shifts towards a high-velocity point as the concentration of the pack ice increases, and this encountering frequency creates an unstable region of the resistance, and the unstable region shifts to the higher speed with the increasing concentration. The results also showed that for the same speed points, the ratio of the pack ice resistance to the open water resistance increases with the increasing concentration, and for the same concentrations, this ratio decreases as the speed increases. Motion characteristics showed that the mean value of the heave motion increases as the speed increases, and the pitch motion tends to increase with the increasing speed. In addition, the total resistance of the fullscale was predicted.

  11. Method to estimate drag coefficient at the air/ice interface over drifting open pack ice from remotely sensed data

    NASA Technical Reports Server (NTRS)

    Feldman, U.

    1984-01-01

    A knowledge in near real time, of the surface drag coefficient for drifting pack ice is vital for predicting its motions. And since this is not routinely available from measurements it must be replaced by estimates. Hence, a method for estimating this variable, as well as the drag coefficient at the water/ice interface and the ice thickness, for drifting open pack ice was developed. These estimates were derived from three-day sequences of LANDSAT-1 MSS images and surface weather charts and from the observed minima and maxima of these variables. The method was tested with four data sets in the southeastern Beaufort sea. Acceptable results were obtained for three data sets. Routine application of the method depends on the availability of data from an all-weather air or spaceborne remote sensing system, producing images with high geometric fidelity and high resolution.

  12. Simple Cloud Chambers Using Gel Ice Packs

    ERIC Educational Resources Information Center

    Kamata, Masahiro; Kubota, Miki

    2012-01-01

    Although cloud chambers are highly regarded as teaching aids for radiation education, school teachers have difficulty in using cloud chambers because they have to prepare dry ice or liquid nitrogen before the experiment. We developed a very simple and inexpensive cloud chamber that uses the contents of gel ice packs which can substitute for dry…

  13. Mapping and Assessing Variability in the Antarctic Marginal Ice Zone, the Pack Ice and Coastal Polynyas

    NASA Astrophysics Data System (ADS)

    Stroeve, Julienne; Jenouvrier, Stephanie

    2016-04-01

    Sea ice variability within the marginal ice zone (MIZ) and polynyas plays an important role for phytoplankton productivity and krill abundance. Therefore mapping their spatial extent, seasonal and interannual variability is essential for understanding how current and future changes in these biological active regions may impact the Antarctic marine ecosystem. Knowledge of the distribution of different ice types to the total Antarctic sea ice cover may also help to shed light on the factors contributing towards recent expansion of the Antarctic ice cover in some regions and contraction in others. The long-term passive microwave satellite data record provides the longest and most consistent data record for assessing different ice types. However, estimates of the amount of MIZ, consolidated pack ice and polynyas depends strongly on what sea ice algorithm is used. This study uses two popular passive microwave sea ice algorithms, the NASA Team and Bootstrap to evaluate the distribution and variability in the MIZ, the consolidated pack ice and coastal polynyas. Results reveal the NASA Team algorithm has on average twice the MIZ and half the consolidated pack ice area as the Bootstrap algorithm. Polynya area is also larger in the NASA Team algorithm, and the timing of maximum polynya area may differ by as much as 5 months between algorithms. These differences lead to different relationships between sea ice characteristics and biological processes, as illustrated here with the breeding success of an Antarctic seabird.

  14. SAR imagery of the Grand Banks (Newfoundland) pack ice pack and its relationship to surface features

    NASA Technical Reports Server (NTRS)

    Argus, S. D.; Carsey, F. D.

    1988-01-01

    Synthetic Aperture Radar (SAR) data and aerial photographs were obtained over pack ice off the East Coast of Canada in March 1987 as part of the Labrador Ice Margin Experiment (LIMEX) pilot project. Examination of this data shows that although the pack ice off the Canadian East Coast appears essentially homogeneous to visible light imagery, two clearly defined zones of ice are apparent on C-band SAR imagery. To identify factors that create the zones seen on the radar image, aerial photographs were compared to the SAR imagery. Floe size data from the aerial photographs was compared to digital number values taken from SAR imagery of the same ice. The SAR data of the inner zone acquired three days apart over the melt period was also examined. The studies indicate that the radar response is governed by floe size and meltwater distribution.

  15. Sea ice motions in the Central Arctic pack ice as inferred from AVHRR imagery

    NASA Technical Reports Server (NTRS)

    Emery, William; Maslanik, James; Fowler, Charles

    1995-01-01

    Synoptic observations of ice motion in the Arctic Basin are currently limited to those acquired by drifting buoys and, more recently, radar data from ERS-1. Buoys are not uniformly distributed throughout the Arctic, and SAR coverage is currently limited regionally and temporally due to the data volume, swath width, processing requirements, and power needs of the SAR. Additional ice-motion observations that can map ice responses simultaneously over large portions of the Arctic on daily to weekly time intervals are thus needed to augment the SAR and buoys data and to provide an intermediate-scale measure of ice drift suitable for climatological analyses and ice modeling. Principal objectives of this project were to: (1) demonstrate whether sufficient ice features and ice motion existed within the consolidated ice pack to permit motion tracking using AVHRR imagery; (2) determine the limits imposed on AVHRR mapping by cloud cover; and (3) test the applicability of AVHRR-derived motions in studies of ice-atmosphere interactions. Each of these main objectives was addressed. We conclude that AVHRR data, particularly when blended with other available observations, provide a valuable data set for studying sea ice processes. In a follow-on project, we are now extending this work to cover larger areas and to address science questions in more detail.

  16. Ecology of southern ocean pack ice.

    PubMed

    Brierley, Andrew S; Thomas, David N

    2002-01-01

    Around Antarctica the annual five-fold growth and decay of sea ice is the most prominent physical process and has a profound impact on marine life there. In winter the pack ice canopy extends to cover almost 20 million square kilometres--some 8% of the southern hemisphere and an area larger than the Antarctic continent itself (13.2 million square kilometres)--and is one of the largest, most dynamic ecosystems on earth. Biological activity is associated with all physical components of the sea-ice system: the sea-ice surface; the internal sea-ice matrix and brine channel system; the underside of sea ice and the waters in the vicinity of sea ice that are modified by the presence of sea ice. Microbial and microalgal communities proliferate on and within sea ice and are grazed by a wide range of proto- and macrozooplankton that inhabit the sea ice in large concentrations. Grazing organisms also exploit biogenic material released from the sea ice at ice break-up or melt. Although rates of primary production in the underlying water column are often low because of shading by sea-ice cover, sea ice itself forms a substratum that provides standing stocks of bacteria, algae and grazers significantly higher than those in ice-free areas. Decay of sea ice in summer releases particulate and dissolved organic matter to the water column, playing a major role in biogeochemical cycling as well as seeding water column phytoplankton blooms. Numerous zooplankton species graze sea-ice algae, benefiting additionally because the overlying sea-ice ceiling provides a refuge from surface predators. Sea ice is an important nursery habitat for Antarctic krill, the pivotal species in the Southern Ocean marine ecosystem. Some deep-water fish migrate to shallow depths beneath sea ice to exploit the elevated concentrations of some zooplankton there. The increased secondary production associated with pack ice and the sea-ice edge is exploited by many higher predators, with seals, seabirds and whales

  17. Mapping and assessing variability in the Antarctic marginal ice zone, pack ice and coastal polynyas in two sea ice algorithms with implications on breeding success of snow petrels

    NASA Astrophysics Data System (ADS)

    Stroeve, Julienne C.; Jenouvrier, Stephanie; Campbell, G. Garrett; Barbraud, Christophe; Delord, Karine

    2016-08-01

    Sea ice variability within the marginal ice zone (MIZ) and polynyas plays an important role for phytoplankton productivity and krill abundance. Therefore, mapping their spatial extent as well as seasonal and interannual variability is essential for understanding how current and future changes in these biologically active regions may impact the Antarctic marine ecosystem. Knowledge of the distribution of MIZ, consolidated pack ice and coastal polynyas in the total Antarctic sea ice cover may also help to shed light on the factors contributing towards recent expansion of the Antarctic ice cover in some regions and contraction in others. The long-term passive microwave satellite data record provides the longest and most consistent record for assessing the proportion of the sea ice cover that is covered by each of these ice categories. However, estimates of the amount of MIZ, consolidated pack ice and polynyas depend strongly on which sea ice algorithm is used. This study uses two popular passive microwave sea ice algorithms, the NASA Team and Bootstrap, and applies the same thresholds to the sea ice concentrations to evaluate the distribution and variability in the MIZ, the consolidated pack ice and coastal polynyas. Results reveal that the seasonal cycle in the MIZ and pack ice is generally similar between both algorithms, yet the NASA Team algorithm has on average twice the MIZ and half the consolidated pack ice area as the Bootstrap algorithm. Trends also differ, with the Bootstrap algorithm suggesting statistically significant trends towards increased pack ice area and no statistically significant trends in the MIZ. The NASA Team algorithm on the other hand indicates statistically significant positive trends in the MIZ during spring. Potential coastal polynya area and amount of broken ice within the consolidated ice pack are also larger in the NASA Team algorithm. The timing of maximum polynya area may differ by as much as 5 months between algorithms. These

  18. Pack ice along the Kamchatka Peninsula, Russia as seen from STS-60

    NASA Technical Reports Server (NTRS)

    1994-01-01

    Pack ice is documented in this photograph along the coast of the Kamchatka Peninsula of Russia in Zaliv Ozernoj. Detailed photographs of the ice provide information to scientists in both Russia and the United States about the location and fluctuation of ice edges, and how this new sea ice interacts with ocean and littoral currents.

  19. Is it worth packing the head with ice in patients undergoing deep hypothermic circulatory arrest?

    PubMed

    O'Neill, Bridie; Bilal, Haris; Mahmood, Sarah; Waterworth, Paul

    2012-10-01

    A best evidence topic in cardiac surgery was written according to a structured protocol. The question addressed was: Is it worth packing the head with ice in patients undergoing deep hypothermic circulatory arrest (DHCA)? Altogether more than 34 papers were found using the reported search, of which 7 represented the best evidence to answer the clinical question, 5 of which were animal studies, 1 was a theoretical laboratory study and 1 study looked at the ability to cool using circulating water 'jackets' in humans. There were no available human studies looking at the neurological outcome with or without topical head cooling with ice without further adjunct methods of cerebral protection. The authors, journal, date and country of publication, patient group studied, study type, relevant outcomes and results of these papers are tabulated. Four papers studied animals undergoing DHCA for 45 min-2 h depending on the study design, with or without packing the head with ice. The studies all demonstrated improved cerebral cooling when the head was packed with ice during DHCA. They also illustrated an improved neurological outcome, with better behavioural scores (P < 0.05), and in some, survival, when compared with animals whose heads were not packed in ice. One study examined selective head cooling with the use of packing the head with ice during rewarming after DHCA. However, they demonstrated worse neurological outcomes in these animals, possibly due to the loss of cerebral vasoregulation and cerebral oedema. One study involved a laboratory experiment showing improved cooling using circulating cool water in cryotherapy braces than by using packed ice. They extrapolated that newer devices to cool the head may improve cerebral cooling during DHCA. The final study discussed here demonstrated the use of circulating water to the head in humans undergoing pulmonary endarterectomy. They found that tympanic membrane temperatures could be maintained significantly lower than bladder

  20. Year-Round Pack Ice in the Weddell Sea, Antarctica: Response and Sensitivity to Atmospheric and Oceanic Forcing

    NASA Technical Reports Server (NTRS)

    Geiger, Cathleen A.; Ackley, Stephen F.; Hibler, William D., III

    1997-01-01

    Using a dynamic-thermodynamic numerical sea-ice model, external oceanic and atmospheric forcings on sea ice in the Weddell Sea are examined to identify physical processes associated with the seasonal cycle of pack ice, and to identify further the parameters that coupled models need to consider in predicting the response of the pack ice to climate and ocean-circulation changes. In agreement with earlier studies, the primary influence on the winter ice-edge maximum extent is air temperature. Ocean heat flux has more impact on the minimum-ice-edge extent and in reducing pack-ice thickness, especially in the eastern-Weddell Sea. Low relative humidity enhances ice growth in thin ice and open-water regions, producing a more realistic ice edge along the coastal areas of the western-Weddell Sea where dry continental air has an impact. The modeled extent of the Weddell summer pack is equally sensitive to ocean heat flux and atmospheric relative humidity variations with the more dynamic responses being from the atmosphere. Since the atmospheric regime in the eastern Weddell is dominated by marine intrusions from lower latitudes, with high humidity already, it is unlikely that either the moisture trans- port could be further raised or that it could be significantly lowered because of its distance from the continent (the lower humidity source). Ocean heat-transport variability is shown to lead to overall ice thinning in the model response and is a known feature of the actual system, as evidenced by the occurrence of the Weddell Polynya in the mid 1970s.

  1. Leads in Arctic pack ice enable early phytoplankton blooms below snow-covered sea ice

    PubMed Central

    Assmy, Philipp; Fernández-Méndez, Mar; Duarte, Pedro; Meyer, Amelie; Randelhoff, Achim; Mundy, Christopher J.; Olsen, Lasse M.; Kauko, Hanna M.; Bailey, Allison; Chierici, Melissa; Cohen, Lana; Doulgeris, Anthony P.; Ehn, Jens K.; Fransson, Agneta; Gerland, Sebastian; Hop, Haakon; Hudson, Stephen R.; Hughes, Nick; Itkin, Polona; Johnsen, Geir; King, Jennifer A.; Koch, Boris P.; Koenig, Zoe; Kwasniewski, Slawomir; Laney, Samuel R.; Nicolaus, Marcel; Pavlov, Alexey K.; Polashenski, Christopher M.; Provost, Christine; Rösel, Anja; Sandbu, Marthe; Spreen, Gunnar; Smedsrud, Lars H.; Sundfjord, Arild; Taskjelle, Torbjørn; Tatarek, Agnieszka; Wiktor, Jozef; Wagner, Penelope M.; Wold, Anette; Steen, Harald; Granskog, Mats A.

    2017-01-01

    The Arctic icescape is rapidly transforming from a thicker multiyear ice cover to a thinner and largely seasonal first-year ice cover with significant consequences for Arctic primary production. One critical challenge is to understand how productivity will change within the next decades. Recent studies have reported extensive phytoplankton blooms beneath ponded sea ice during summer, indicating that satellite-based Arctic annual primary production estimates may be significantly underestimated. Here we present a unique time-series of a phytoplankton spring bloom observed beneath snow-covered Arctic pack ice. The bloom, dominated by the haptophyte algae Phaeocystis pouchetii, caused near depletion of the surface nitrate inventory and a decline in dissolved inorganic carbon by 16 ± 6 g C m−2. Ocean circulation characteristics in the area indicated that the bloom developed in situ despite the snow-covered sea ice. Leads in the dynamic ice cover provided added sunlight necessary to initiate and sustain the bloom. Phytoplankton blooms beneath snow-covered ice might become more common and widespread in the future Arctic Ocean with frequent lead formation due to thinner and more dynamic sea ice despite projected increases in high-Arctic snowfall. This could alter productivity, marine food webs and carbon sequestration in the Arctic Ocean. PMID:28102329

  2. Fifteen-second skin icing using a frozen gel pack is effective for reducing goserelin injection pain.

    PubMed

    Naya, Yoshio; Hagiwara, Nobuhisa; Takeuchi, Ichiro; Mori, Masaru; Inagaki, Akinori; Nakanouchi, Tsuneyuki; Mikami, Kazuya

    2014-01-01

    The efficacy of skin icing to reduce the pain of goserelin injection has been reported. We investigated the optimal icing time with a frozen gel pack and its effectiveness. Abdominal skin temperatures of 49 healthy volunteers were measured after application of the frozen gel pack for 10, 15 and 30 s, and it was decided that a 15-second icing was adequate. For 55 consecutive patients who received goserelin (10.8 mg) injection, pain was evaluated employing a visual analog scale (VAS). The first injection was administered routinely. A second injection was administered after skin icing in 27 of 55 patients who wanted to try icing. At the time of the third injection, all patient decided whether they were to receive icing or the routine method. After icing, VAS scores decreased in 20 of 27 patients. At the third injection, 18 patients requested icing. When a patient complains of injection pain, the icing method should be considered for pain reduction. 2014 S. Karger AG, Basel.

  3. Comparisons of ice packs, hot water immersion, and analgesia injection for the treatment of centipede envenomations in Taiwan.

    PubMed

    Chaou, Chung-Hsien; Chen, Chian-Kuang; Chen, Jih-Chang; Chiu, Te-Fa; Lin, Chih-Chuan

    2009-08-01

    To compare the effectiveness of ice packs and hot water immersion for the treatment of centipede envenomations. Sixty patients envenomated by centipedes were randomized into three groups and were treated with ice packs, hot water immersion, or analgesia injection. The visual analog score (VAS) for pain was measured before the treatment and 15 min afterward. Demographic data and data on local and systemic effects after centipede bites were collected. The VAS scores and the pain decrease (DeltaVAS) were compared between the three groups. All patients suffered from pain at the affected sites; other local effects included redness (n = 49, 81.7%), swelling (n = 32, 53.3%), heat (n = 14, 23.3%), itchiness (n = 5, 8.3), and bullae formation (n = 3, 5.0%). Rare systemic effects were reported. All three groups had similar VAS scores before and after treatment. They also had similar effectiveness in reducing pain caused by centipedes bites (DeltaVAS = 2.55 +/- 1.88, 2.33 +/- 1.78, and 1.55 +/- 1.68, with ice packs, analgesia, and hot water immersion, respectively, p = 0.165). Ice packs, hot water immersion, and analgesics all improved the pain from centipede envenomation. Ice pack treatment is a safe, inexpensive, and non-invasive method for pre-hospital management in patients with centipede envenomation.

  4. Effects of lead structure in Bering Sea pack ice on the flight costs of wintering spectacled eiders

    NASA Astrophysics Data System (ADS)

    Bump, Joseph K.; Lovvorn, James R.

    2004-10-01

    In polar regions, sea ice is critical habitat for many marine birds and mammals. The quality of pack ice habitat depends on the duration and spacing of leads (openings in the ice), which determine access to water and air for diving endotherms, and how often and how far they must move as leads open and close. Recent warming trends have caused major changes in the extent and nature of sea ice at large scales used in climate models. However, no studies have analyzed lead structure in terms of habitat for ice-dependent endotherms, or effects of climate on ice habitat at scales relevant to their daily movements. Based on observations from an icebreaker and synthetic aperture radar (SAR) images, we developed methods to describe the dynamics and thermodynamics of lead structure relative to use by spectacled eiders ( Somateria fischeri) wintering in pack ice of the Bering Sea. By correlating lead structure with weather variables, we then used these methods to estimate changes in lead dynamics from 1945 to 2002, and effects of such changes on flight costs of the eiders. For 1991-1992, when images were available about every 3 days throughout winter, SAR images were divided among five weather regimes defined by wind speed, wind direction, and air temperature. Based on 12.5-m pixels, lead shape, compass orientation, and fetch across leads did not differ among the weather regimes. However, the five regimes differed in total area of open water, leads per unit area, and distance between leads. Lead duration was modeled based on air temperature, wind, and fetch. Estimates of mean daily flight time for eiders, based on lead duration and distance between neighboring leads, differed among regimes by 0 to 15 min. Resulting flight costs varied from 0 to 158 kJ day -1, or from 0% to 11% of estimated field metabolic rate. Over 57 winters (1945-2002), variation among years in mean daily flight time was most influenced by the north-south wind component, which determined pack divergence

  5. Oral health-related quality of life following third molar surgery with or without application of ice pack therapy.

    PubMed

    Ibikunle, Adebayo A; Adeyemo, Wasiu L

    2016-09-01

    To evaluate the effect of ice pack therapy on oral health-related quality of life (OHRQoL) following third molar surgery. All consecutive subjects who required surgical extraction of lower third molars and satisfied the inclusion criteria were randomly allocated into two groups. Subjects in group A were instructed to apply ice packs directly over the masseteric region on the operated side intermittently after third molar surgery. This first application was supervised in the clinic and was repeated at the 24-h postoperative review. Subjects in group A were further instructed to apply the ice pack when at home every one and a half hours on postoperative days 0 and 1 while he/she was awake as described. Group B subjects did not apply ice pack therapy. Facial swelling, pain, trismus, and quality of life (using Oral Health Impact Profile-14 (OHIP-14) instrument) were evaluated both preoperatively and postoperatively. Postoperative scores in both groups were compared. A significant increase in the mean total and subscale scores of OHIP-14 was found in both groups postoperatively when compared with preoperative value. Subjects who received ice pack therapy had a better quality of life than those who did not. Subjects whose postoperative QoL were affected were statistically significantly higher in group B than in group A at all postoperative evaluation points (P < 0.05). Statistically significant differences were also observed between the groups in the various subscales analyzed, with better quality of life seen among subjects in group A. Quality of life after third molar surgery was significantly better in subjects who had cryotherapy after third molar than those who did not have cryotherapy. Cryotherapy is a viable alternative or adjunct to other established modes of improving the quality of life of patients following surgical extraction of third molars.

  6. The zooplankton food web under East Antarctic pack ice - A stable isotope study

    NASA Astrophysics Data System (ADS)

    Jia, Zhongnan; Swadling, Kerrie M.; Meiners, Klaus M.; Kawaguchi, So; Virtue, Patti

    2016-09-01

    Understanding how sea ice serves zooplankton species during the food-limited season is crucial information to evaluate the potential responses of pelagic food webs to changes in sea-ice conditions in the Southern Ocean. Stable isotope analyses (13C/12C and 15N/14N) were used to compare the dietary preferences and trophic relationships of major zooplankton species under pack ice during two winter-spring transitions (2007 and 2012). During sampling, furcilia of Euphausia superba demonstrated dietary plasticity between years, herbivory when feeding on sea-ice biota, and with a more heterotrophic diet when feeding from both the sea ice and the water column. Carbon isotope signatures suggested that the pteropod Limacina helicina, small copepods Oithona spp., ostracods and amphipods relied heavily on sea-ice biota. Post larval E. superba and omnivorous krill Thysanoessa macrura consumed both water column and ice biota, but further investigations are needed to estimate the contribution from each source. Large copepods and chaetognaths overwintered on a water column-based diet. Our study suggests that warm and permeable sea ice is more likely to provide food for zooplankton species under the ice than the colder ice.

  7. Pack ice along the Kamchatka Peninsula, Russia as seen from STS-60

    NASA Image and Video Library

    1994-02-09

    STS060-73-038 (3-11 Feb 1994) --- Pack ice is documented in this photograph along the coast of the Kamchatka Peninsula of Russia in Zaliv Ozernoj. Newly formed ice continually breaks away from the land and takes the form imposed by coastal currents. Detailed photographs of the ice provide information to scientists in both Russia and the united States about the location and fluctuation of ice edges, and how this new sea ice interacts with ocean and littoral currents. This information results in better ice warnings to shipping traffic and provides data points for long-range climate change research for both the Mission-To-Planet Earth and the Russian Priroda ("Nature") monitoring and assessment programs that are respectively coordinated by NASA and the Russian Academy of Sciences. This photography of ice development in the North Pacific, North Atlantic, the Southern Ocean, the Baltic and North Seas, and the Great Lakes is of great interest to the international scientific community. NASA scientists feel high-resolution analog and digital photography from the Space Shuttle and future craft can be a particularly important component in satisfying their data needs on both an operational and a long-term research basis.

  8. Comparisons of Cubed Ice, Crushed Ice, and Wetted Ice on Intramuscular and Surface Temperature Changes

    PubMed Central

    Dykstra, Joseph H; Hill, Holly M; Miller, Michael G; Cheatham, Christopher C; Michael, Timothy J; Baker, Robert J

    2009-01-01

    Context: Many researchers have investigated the effectiveness of different types of cold application, including cold whirlpools, ice packs, and chemical packs. However, few have investigated the effectiveness of different types of ice used in ice packs, even though ice is one of the most common forms of cold application. Objective: To evaluate and compare the cooling effectiveness of ice packs made with cubed, crushed, and wetted ice on intramuscular and skin surface temperatures. Design: Repeated-measures counterbalanced design. Setting: Human performance research laboratory. Patients or Other Participants: Twelve healthy participants (6 men, 6 women) with no history of musculoskeletal disease and no known preexisting inflammatory conditions or recent orthopaedic injuries to the lower extremities. Intervention(s): Ice packs made with cubed, crushed, or wetted ice were applied to a standardized area on the posterior aspect of the right gastrocnemius for 20 minutes. Each participant was given separate ice pack treatments, with at least 4 days between treatment sessions. Main Outcome Measure(s): Cutaneous and intramuscular (2 cm plus one-half skinfold measurement) temperatures of the right gastrocnemius were measured every 30 seconds during a 20-minute baseline period, a 20-minute treatment period, and a 120-minute recovery period. Results: Differences were observed among all treatments. Compared with the crushed-ice treatment, the cubed-ice and wetted-ice treatments produced lower surface and intramuscular temperatures. Wetted ice produced the greatest overall temperature change during treatment and recovery, and crushed ice produced the smallest change. Conclusions: As administered in our protocol, wetted ice was superior to cubed or crushed ice at reducing surface temperatures, whereas both cubed ice and wetted ice were superior to crushed ice at reducing intramuscular temperatures. PMID:19295957

  9. CO2 flux over young and snow-covered Arctic pack ice in winter and spring

    NASA Astrophysics Data System (ADS)

    Nomura, Daiki; Granskog, Mats A.; Fransson, Agneta; Chierici, Melissa; Silyakova, Anna; Ohshima, Kay I.; Cohen, Lana; Delille, Bruno; Hudson, Stephen R.; Dieckmann, Gerhard S.

    2018-06-01

    Rare CO2 flux measurements from Arctic pack ice show that two types of ice contribute to the release of CO2 from the ice to the atmosphere during winter and spring: young, thin ice with a thin layer of snow and older (several weeks), thicker ice with thick snow cover. Young, thin sea ice is characterized by high salinity and high porosity, and snow-covered thick ice remains relatively warm ( > -7.5 °C) due to the insulating snow cover despite air temperatures as low as -40 °C. Therefore, brine volume fractions of these two ice types are high enough to provide favorable conditions for gas exchange between sea ice and the atmosphere even in mid-winter. Although the potential CO2 flux from sea ice decreased due to the presence of the snow, the snow surface is still a CO2 source to the atmosphere for low snow density and thin snow conditions. We found that young sea ice that is formed in leads without snow cover produces CO2 fluxes an order of magnitude higher than those in snow-covered older ice (+1.0 ± 0.6 mmol C m-2 day-1 for young ice and +0.2 ± 0.2 mmol C m-2 day-1 for older ice).

  10. Breakup of Pack Ice, Antarctic Ice Shelf

    NASA Image and Video Library

    1991-09-18

    STS048-152-007 (12-18 Sept 1991) --- The periphery of the Antarctic ice shelf and the Antarctic Peninsula were photographed by the STS 48 crew members. Strong offshore winds, probably associated with katabatic winds from the interior of the continent, are peeling off the edges of the ice shelf into ribbons of sea ice, icebergs, bergy bits and growlers into the cold waters of the circum-Antarctic southern ocean.

  11. The winter pack-ice zone provides a sheltered but food-poor habitat for larval Antarctic krill.

    PubMed

    Meyer, Bettina; Freier, Ulrich; Grimm, Volker; Groeneveld, Jürgen; Hunt, Brian P V; Kerwath, Sven; King, Rob; Klaas, Christine; Pakhomov, Evgeny; Meiners, Klaus M; Melbourne-Thomas, Jessica; Murphy, Eugene J; Thorpe, Sally E; Stammerjohn, Sharon; Wolf-Gladrow, Dieter; Auerswald, Lutz; Götz, Albrecht; Halbach, Laura; Jarman, Simon; Kawaguchi, So; Krumpen, Thomas; Nehrke, Gernot; Ricker, Robert; Sumner, Michael; Teschke, Mathias; Trebilco, Rowan; Yilmaz, Noyan I

    2017-12-01

    A dominant Antarctic ecological paradigm suggests that winter sea ice is generally the main feeding ground for krill larvae. Observations from our winter cruise to the southwest Atlantic sector of the Southern Ocean contradict this view and present the first evidence that the pack-ice zone is a food-poor habitat for larval development. In contrast, the more open marginal ice zone provides a more favourable food environment for high larval krill growth rates. We found that complex under-ice habitats are, however, vital for larval krill when water column productivity is limited by light, by providing structures that offer protection from predators and to collect organic material released from the ice. The larvae feed on this sparse ice-associated food during the day. After sunset, they migrate into the water below the ice (upper 20 m) and drift away from the ice areas where they have previously fed. Model analyses indicate that this behaviour increases both food uptake in a patchy food environment and the likelihood of overwinter transport to areas where feeding conditions are more favourable in spring.

  12. There goes the sea ice: following Arctic sea ice parcels and their properties.

    NASA Astrophysics Data System (ADS)

    Tschudi, M. A.; Tooth, M.; Meier, W.; Stewart, S.

    2017-12-01

    Arctic sea ice distribution has changed considerably over the last couple of decades. Sea ice extent record minimums have been observed in recent years, the distribution of ice age now heavily favors younger ice, and sea ice is likely thinning. This new state of the Arctic sea ice cover has several impacts, including effects on marine life, feedback on the warming of the ocean and atmosphere, and on the future evolution of the ice pack. The shift in the state of the ice cover, from a pack dominated by older ice, to the current state of a pack with mostly young ice, impacts specific properties of the ice pack, and consequently the pack's response to the changing Arctic climate. For example, younger ice typically contains more numerous melt ponds during the melt season, resulting in a lower albedo. First-year ice is typically thinner and more fragile than multi-year ice, making it more susceptible to dynamic and thermodynamic forcing. To investigate the response of the ice pack to climate forcing during summertime melt, we have developed a database that tracks individual Arctic sea ice parcels along with associated properties as these parcels advect during the summer. Our database tracks parcels in the Beaufort Sea, from 1985 - present, along with variables such as ice surface temperature, albedo, ice concentration, and convergence. We are using this database to deduce how these thousands of tracked parcels fare during summer melt, i.e. what fraction of the parcels advect through the Beaufort, and what fraction melts out? The tracked variables describe the thermodynamic and dynamic forcing on these parcels during their journey. This database will also be made available to all interested investigators, after it is published in the near future. The attached image shows the ice surface temperature of all parcels (right) that advected through the Beaufort Sea region (left) in 2014.

  13. Design, development, and fabrication of a prototype ice pack heat sink subsystem. Flight experiment physical phenomena experiment chest

    NASA Technical Reports Server (NTRS)

    Roebelen, G. J., Jr.; Dean, W. C., II

    1975-01-01

    The concept of a flight experiment physical phenomena experiment chest, to be used eventually for investigating and demonstrating ice pack heat sink subsystem physical phenomena during a zero gravity flight experiment, is described.

  14. Acoustic effects of oil-production activities on bowhead and white whales visible during spring migration near Pt. Barrow, Alaska-1990 phase: sound propagation and whale responses to playbacks of continuous drilling noise from an ice platform, as studied in pack ice conditions. Final report

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Richardson, W.J.; Greene, C.R.; Koski, W.R.

    1991-10-01

    The report concerns the effects of underwater noise from simulated oil production operations on the movements and behavior of bowhead and white whales migrating around northern Alaska in spring. An underwater sound projector suspended from pack ice was used to introduce recorded drilling noise and other test sounds into leads through the pack ice. These sounds were received and measured at various distances to determine the rate of sound attenuation with distance and frequency. The movements and behavior of bowhead and white whales approaching the operating projector were studied by aircraft- and ice-based observers. Some individuals of both species weremore » observed to approach well within the ensonified area. However, behavioral changes and avoidance reactions were evident when the received sound level became sufficiently high. Reactions to aircraft are also discussed.« less

  15. Ice interaction with offshore structures

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Cammaert, A.B.; Muggeridge, D.B.

    1988-01-01

    Oil platforms and other offshore structures being built in the arctic regions must be able to withstand icebergs, ice islands, and pack ice. This reference explain the effect ice has on offshore structures and demonstrates design and construction methods that allow such structures to survive in harsh, ice-ridden environments. It analyzes the characteristics of sea ice as well as dynamic ice forces on structures. Techniques for ice modeling and field testing facilitate the design and construction of sturdy, offshore constructions. Computer programs included.

  16. Heated Debates: Hot-Water Immersion or Ice Packs as First Aid for Cnidarian Envenomations?

    PubMed Central

    Wilcox, Christie L.; Yanagihara, Angel A.

    2016-01-01

    Cnidarian envenomations are an important public health problem, responsible for more deaths than shark attacks annually. For this reason, optimization of first-aid care is essential. According to the published literature, cnidarian venoms and toxins are heat labile at temperatures safe for human application, which supports the use of hot-water immersion of the sting area(s). However, ice packs are often recommended and used by emergency personnel. After conducting a systematic review of the evidence for the use of heat or ice in the treatment of cnidarian envenomations, we conclude that the majority of studies to date support the use of hot-water immersion for pain relief and improved health outcomes. PMID:27043628

  17. Heated Debates: Hot-Water Immersion or Ice Packs as First Aid for Cnidarian Envenomations?

    PubMed

    Wilcox, Christie L; Yanagihara, Angel A

    2016-04-01

    Cnidarian envenomations are an important public health problem, responsible for more deaths than shark attacks annually. For this reason, optimization of first-aid care is essential. According to the published literature, cnidarian venoms and toxins are heat labile at temperatures safe for human application, which supports the use of hot-water immersion of the sting area(s). However, ice packs are often recommended and used by emergency personnel. After conducting a systematic review of the evidence for the use of heat or ice in the treatment of cnidarian envenomations, we conclude that the majority of studies to date support the use of hot-water immersion for pain relief and improved health outcomes.

  18. Analysis of sea ice dynamics

    NASA Technical Reports Server (NTRS)

    Zwally, J.

    1988-01-01

    The ongoing work has established the basis for using multiyear sea ice concentrations from SMMR passive microwave for studies of largescale advection and convergence/divergence of the Arctic sea ice pack. Comparisons were made with numerical model simulations and buoy data showing qualitative agreement on daily to interannual time scales. Analysis of the 7-year SMMR data set shows significant interannual variations in the total area of multiyear ice. The scientific objective is to investigate the dynamics, mass balance, and interannual variability of the Arctic sea ice pack. The research emphasizes the direct application of sea ice parameters derived from passive microwave data (SMMR and SSMI) and collaborative studies using a sea ice dynamics model. The possible causes of observed interannual variations in the multiyear ice area are being examined. The relative effects of variations in the large scale advection and convergence/divergence within the ice pack on a regional and seasonal basis are investigated. The effects of anomolous atmospheric forcings are being examined, including the long-lived effects of synoptic events and monthly variations in the mean geostrophic winds. Estimates to be made will include the amount of new ice production within the ice pack during winter and the amount of ice exported from the pack.

  19. Biogeochemical Impact of Snow Cover and Cyclonic Intrusions on the Winter Weddell Sea Ice Pack

    NASA Astrophysics Data System (ADS)

    Tison, J.-L.; Schwegmann, S.; Dieckmann, G.; Rintala, J.-M.; Meyer, H.; Moreau, S.; Vancoppenolle, M.; Nomura, D.; Engberg, S.; Blomster, L. J.; Hendrickx, S.; Uhlig, C.; Luhtanen, A.-M.; de Jong, J.; Janssens, J.; Carnat, G.; Zhou, J.; Delille, B.

    2017-12-01

    Sea ice is a dynamic biogeochemical reactor and a double interface actively interacting with both the atmosphere and the ocean. However, proper understanding of its annual impact on exchanges, and therefore potentially on the climate, notably suffer from the paucity of autumnal and winter data sets. Here we present the results of physical and biogeochemical investigations on winter Antarctic pack ice in the Weddell Sea (R. V. Polarstern AWECS cruise, June-August 2013) which are compared with those from two similar studies conducted in the area in 1986 and 1992. The winter 2013 was characterized by a warm sea ice cover due to the combined effects of deep snow and frequent warm cyclones events penetrating southward from the open Southern Ocean. These conditions were favorable to high ice permeability and cyclic events of brine movements within the sea ice cover (brine tubes), favoring relatively high chlorophyll-a (Chl-a) concentrations. We discuss the timing of this algal activity showing that arguments can be presented in favor of continued activity during the winter due to the specific physical conditions. Large-scale sea ice model simulations also suggest a context of increasingly deep snow, warm ice, and large brine fractions across the three observational years, despite the fact that the model is forced with a snowfall climatology. This lends support to the claim that more severe Antarctic sea ice conditions, characterized by a longer ice season, thicker, and more concentrated ice are sufficient to increase the snow depth and, somehow counterintuitively, to warm the ice.

  20. Formation processes of sea ice floe size distribution in the interior pack and its relationship to the marginal ice zone off East Antarctica

    NASA Astrophysics Data System (ADS)

    Toyota, Takenobu; Kohout, Alison; Fraser, Alexander D.

    2016-09-01

    To understand the behavior of the Seasonal Ice Zone (SIZ), which is composed of sea-ice floes of various sizes, knowledge of the floe size distribution (FSD) is important. In particular, FSD in the Marginal Ice Zone (MIZ), controlled by wave-ice interaction, plays an important role in determining the retreating rates of sea-ice extent on a global scale because the cumulative perimeter of floes enhances melting. To improve the understanding of wave-ice interaction and subsequent effects on FSD in the MIZ, FSD measurements were conducted off East Antarctica during the second Sea Ice Physics and Ecosystems eXperiment (SIPEX-2) in late winter 2012. Since logistical reasons limited helicopter operations to two interior ice regions, FSD in the interior ice region was determined using a combination of heli-photos and MODIS satellite visible images. The possible effect of wave-ice interaction in the MIZ was examined by comparison with past results obtained in the same MIZ, with our analysis showing: (1) FSD in the interior ice region is basically scale invariant for both small- (<100 m) and large- (>1 km) scale regimes; (2) although fractal dimensions are quite different between these two regimes, they are both rather close to that in the MIZ; and (3) for floes <100 m in diameter, a regime shift which appeared at 20-40 m in the MIZ is absent. These results indicate that one role of wave-ice interaction is to modulate the FSD that already exists in the interior ice region, rather than directly determine it. The possibilities of floe-floe collisions and storm-induced lead formation are considered as possible formation processes of FSD in the interior pack.

  1. Pain Intensity after an Ice Pack Application Prior to Venipuncture among School-Age Children: An Experimental Study

    ERIC Educational Resources Information Center

    Alalo, Fadeelah Mansour Ahmed; Ahmad, Awatef El Sayed; El Sayed, Hoda Mohamed Nafee

    2016-01-01

    Venipuncture and other invasive procedures as blood draws, intramuscular injections or heel pricks are the most commonly performed painful procedures in children. These can be a terrifying and painful experience for children and their families. The present study aimed to identify Pain intensity after an ice pack application prior to venipuncture…

  2. Consequences of long-distance swimming and travel over deep-water pack ice for a female polar bear during a year of extreme sea ice retreat

    USGS Publications Warehouse

    Durner, George M.; Whiteman, J.P.; Harlow, H.J.; Amstrup, Steven C.; Regehr, E.V.; Ben-David, M.

    2011-01-01

    Polar bears (Ursus maritimus) prefer to live on Arctic sea ice but may swim between ice floes or between sea ice and land. Although anecdotal observations suggest that polar bears are capable of swimming long distances, no data have been available to describe in detail long distance swimming events or the physiological and reproductive consequences of such behavior. Between an initial capture in late August and a recapture in late October 2008, a radio-collared adult female polar bear in the Beaufort Sea made a continuous swim of 687 km over 9 days and then intermittently swam and walked on the sea ice surface an additional 1,800 km. Measures of movement rate, hourly activity, and subcutaneous and external temperature revealed distinct profiles of swimming and walking. Between captures, this polar bear lost 22% of her body mass and her yearling cub. The extraordinary long distance swimming ability of polar bears, which we confirm here, may help them cope with reduced Arctic sea ice. Our observation, however, indicates that long distance swimming in Arctic waters, and travel over deep water pack ice, may result in high energetic costs and compromise reproductive fitness.

  3. Occurrence of nonspecific reactions among stool specimens tested by the Abbott TestPack rotavirus enzyme immunoassay.

    PubMed Central

    Lipson, S M; Leonardi, G P; Salo, R J; Schutzbank, T E; Kaplan, M H

    1990-01-01

    Sixty-five stool specimens obtained from children suffering from gastroenteritis were tested for the presence of antigen to rotavirus by the Abbott TestPack Rotavirus (TestPack) enzyme immunoassay kit. The Kallestad Pathfinder enzyme immunoassay, polyacrylamide gel electrophoresis, immune electron microscopy, and virus isolation were utilized as reference assays. Fifty-four specimens were in accord by TestPack and Kallestad Pathfinder. Among 11 discordant specimens positive with TestPack but negative by Kallestad Pathfinder, rotavirus was not identified by polyacrylamide gel electrophoresis, immune electron microscopy, or isolation in primary African green monkey kidney cell cultures. TestPack displayed a performance specificity of 83%. The inordinately high number of stool specimens reported as false-positive by TestPack precludes the incorporation of this antigen detection kit into our routine regimen of diagnostic virologic testing. Images PMID:2166074

  4. Parameterization and scaling of arctic ice conditions in the context of ice-atmospheric processes

    NASA Technical Reports Server (NTRS)

    Barry, R. G.; Steffen, K.; Heinrichs, J. F.; Key, J. R.; Maslanik, J. A.; Serreze, M. C.; Weaver, R. L.

    1995-01-01

    The goals of this project are to observe how the open water/thin ice fraction in a high-concentration ice pack responds to different short-period atmospheric forcings, and how this response is represented in different scales of observation. The objectives can be summarized as follows: determine the feasibility and accuracy of ice concentration and ice typing by ERS-1 SAR backscatter data, and whether SAR data might be used to calibrate concentration estimates from optical and massive-microwave sensors; investigate methods to integrate SAR data with other satellite data for turbulent heat flux parameterization at the ocean/atmosphere interface; determine how the development and evolution of open water/thin ice areas within the interior ice pack vary under different atmospheric synoptic regimes; compare how open-water/thin ice fractions estimated from large-area divergence measurements differ from fractions determined by summing localized openings in the pack; relate these questions of scale and process to methods of observation, modeling, and averaging over time and space.

  5. Methods for Scaling Icing Test Conditions

    NASA Technical Reports Server (NTRS)

    Anderson, David N.

    1995-01-01

    This report presents the results of tests at NASA Lewis to evaluate several methods to establish suitable alternative test conditions when the test facility limits the model size or operating conditions. The first method was proposed by Olsen. It can be applied when full-size models are tested and all the desired test conditions except liquid-water content can be obtained in the facility. The other two methods discussed are: a modification of the French scaling law and the AEDC scaling method. Icing tests were made with cylinders at both reference and scaled conditions representing mixed and glaze ice in the NASA Lewis Icing Research Tunnel. Reference and scale ice shapes were compared to evaluate each method. The Olsen method was tested with liquid-water content varying from 1.3 to .8 g/m(exp3). Over this range, ice shapes produced using the Olsen method were unchanged. The modified French and AEDC methods produced scaled ice shapes which approximated the reference shapes when model size was reduced to half the reference size for the glaze-ice cases tested.

  6. Polyurethane Foam Pack Outdoor Storage Test

    DTIC Science & Technology

    1987-10-01

    formed between the polyurthane foam and the plywood. No nails "re used to secure the top. It was impossible to tell If the pack was completely filled...Ulm. rILE: toury AD-A 187 729 - N T. ;I[ POLYURIET!AN FOAM PACK OUTDOOR STORAGE TEST I OCTOBU 1987 DTIC &%ELECTEi NOV 3 0197 * 1’• Thomas M...U.S. ARMY TANK-AUTOMOTIVE COMMANDRESEARCH, DEVELOPMENT & ENGINEERING CENTERWarren, Michigan 48397-5000 REPRODUCTION QUALITY NOTICE This document is the

  7. Advanced ice protection systems test in the NASA Lewis icing research tunnel

    NASA Technical Reports Server (NTRS)

    Bond, Thomas H.; Shin, Jaiwon; Mesander, Geert A.

    1991-01-01

    Tests of eight different deicing systems based on variations of three different technologies were conducted in the NASA Lewis Research Center Icing Research Tunnel (IRT) in June and July 1990. The systems used pneumatic, eddy current repulsive, and electro-expulsive means to shed ice. The tests were conducted on a 1.83 m span, 0.53 m chord NACA 0012 airfoil operated at a 4 degree angle of attack. The models were tested at two temperatures: a glaze condition at minus 3.9 C and a rime condition at minus 17.2 C. The systems were tested through a range of icing spray times and cycling rates. Characterization of the deicers was accomplished by monitoring power consumption, ice shed particle size, and residual ice. High speed video motion analysis was performed to quantify ice particle size.

  8. Coupling of Waves, Turbulence and Thermodynamics Across the Marginal Ice Zone

    DTIC Science & Technology

    2013-09-30

    ice . The albedo of sea ice is large compared to open water, and most of the incoming solar radiation...ocean and the ice pack where the seasonal retreat of the main ice pack takes place. It is a highly variable sea ice environment, usually comprised of...many individual floes of variable shape and size and made of mixed ice types, from young forming ice to fragmented multiyear ice . The presence of sea

  9. Preliminary Results From a Heavily Instrumented Engine Ice Crystal Icing Test in a Ground Based Altitude Test Facility

    NASA Technical Reports Server (NTRS)

    Flegel, Ashlie B.; Oliver, Michael J.

    2016-01-01

    Preliminary results from the heavily instrumented ALF502R-5 engine test conducted in the NASA Glenn Research Center Propulsion Systems Laboratory are discussed. The effects of ice crystal icing on a full scale engine is examined and documented. This same model engine, serial number LF01, was used during the inaugural icing test in the Propulsion Systems Laboratory facility. The uncommanded reduction of thrust (rollback) events experienced by this engine in flight were simulated in the facility. Limited instrumentation was used to detect icing on the LF01 engine. Metal temperatures on the exit guide vanes and outer shroud and the load measurement were the only indicators of ice formation. The current study features a similar engine, serial number LF11, which is instrumented to characterize the cloud entering the engine, detect/ characterize ice accretion, and visualize the ice accretion in the region of interest. Data were acquired at key LF01 test points and additional points that explored: icing threshold regions, low altitude, high altitude, spinner heat effects, and the influence of varying the facility and engine parameters. For each condition of interest, data were obtained from some selected variations of ice particle median volumetric diameter, total water content, fan speed, and ambient temperature. For several cases the NASA in-house engine icing risk assessment code was used to find conditions that would lead to a rollback event. This study further helped NASA develop necessary icing diagnostic instrumentation, expand the capabilities of the Propulsion Systems Laboratory, and generate a dataset that will be used to develop and validate in-house icing prediction and risk mitigation computational tools. The ice accretion on the outer shroud region was acquired by internal video cameras. The heavily instrumented engine showed good repeatability of icing responses when compared to the key LF01 test points and during day-to-day operation. Other noticeable

  10. Preliminary Results From a Heavily Instrumented Engine Ice Crystal Icing Test in a Ground Based Altitude Test Facility

    NASA Technical Reports Server (NTRS)

    Flegel, Ashlie B.; Oliver, Michael J.

    2016-01-01

    Preliminary results from the heavily instrumented ALF502R-5 engine test conducted in the NASA Glenn Research Center Propulsion Systems Laboratory are discussed. The effects of ice crystal icing on a full scale engine is examined and documented. This same model engine, serial number LF01, was used during the inaugural icing test in the Propulsion Systems Laboratory facility. The uncommanded reduction of thrust (rollback) events experienced by this engine in flight were simulated in the facility. Limited instrumentation was used to detect icing on the LF01 engine. Metal temperatures on the exit guide vanes and outer shroud and the load measurement were the only indicators of ice formation. The current study features a similar engine, serial number LF11, which is instrumented to characterize the cloud entering the engine, detect/characterize ice accretion, and visualize the ice accretion in the region of interest. Data were acquired at key LF01 test points and additional points that explored: icing threshold regions, low altitude, high altitude, spinner heat effects, and the influence of varying the facility and engine parameters. For each condition of interest, data were obtained from some selected variations of ice particle median volumetric diameter, total water content, fan speed, and ambient temperature. For several cases the NASA in-house engine icing risk assessment code was used to find conditions that would lead to a rollback event. This study further helped NASA develop necessary icing diagnostic instrumentation, expand the capabilities of the Propulsion Systems Laboratory, and generate a dataset that will be used to develop and validate in-house icing prediction and risk mitigation computational tools. The ice accretion on the outer shroud region was acquired by internal video cameras. The heavily instrumented engine showed good repeatability of icing responses when compared to the key LF01 test points and during day-to-day operation. Other noticeable

  11. Validation Ice Crystal Icing Engine Test in the Propulsion Systems Laboratory at NASA Glenn Research Center

    NASA Technical Reports Server (NTRS)

    Oliver, Michael J.

    2014-01-01

    The Propulsion Systems Laboratory (PSL) is an existing altitude simulation jet engine test facility located at NASA Glenn Research Center in Cleveland, OH. It was modified in 2012 with the integration of an ice crystal cloud generation system. This paper documents the inaugural ice crystal cloud test in PSL--the first ever full scale, high altitude ice crystal cloud turbofan engine test to be conducted in a ground based facility. The test article was a Lycoming ALF502-R5 high bypass turbofan engine, serial number LF01. The objectives of the test were to validate the PSL ice crystal cloud calibration and engine testing methodologies by demonstrating the capability to calibrate and duplicate known flight test events that occurred on the same LF01 engine and to generate engine data to support fundamental and computational research to investigate and better understand the physics of ice crystal icing in a turbofan engine environment while duplicating known revenue service events and conducting test points while varying facility and engine parameters. During PSL calibration testing it was discovered than heated probes installed through tunnel sidewalls experienced ice buildup aft of their location due to ice crystals impinging upon them, melting and running back. Filtered city water was used in the cloud generation nozzle system to provide ice crystal nucleation sites. This resulted in mineralization forming on flow path hardware that led to a chronic degradation of performance during the month long test. Lacking internal flow path cameras, the response of thermocouples along the flow path was interpreted as ice building up. Using this interpretation, a strong correlation between total water content (TWC) and a weaker correlation between median volumetric diameter (MVD) of the ice crystal cloud and the rate of ice buildup along the instrumented flow path was identified. For this test article the engine anti-ice system was required to be turned on before ice crystal

  12. Validation Ice Crystal Icing Engine Test in the Propulsion Systems Laboratory at NASA Glenn Research Center

    NASA Technical Reports Server (NTRS)

    Oliver, Michael J.

    2014-01-01

    The Propulsion Systems Laboratory (PSL) is an existing altitude simulation jet engine test facility located at NASA Glenn Research Center in Clevleand, OH. It was modified in 2012 with the integration of an ice crystal cloud generation system. This paper documents the inaugural ice crystal cloud test in PSLthe first ever full scale, high altitude ice crystal cloud turbofan engine test to be conducted in a ground based facility. The test article was a Lycoming ALF502-R5 high bypass turbofan engine, serial number LF01. The objectives of the test were to validate the PSL ice crystal cloud calibration and engine testing methodologies by demonstrating the capability to calibrate and duplicate known flight test events that occurred on the same LF01 engine and to generate engine data to support fundamental and computational research to investigate and better understand the physics of ice crystal icing in a turbofan engine environment while duplicating known revenue service events and conducting test points while varying facility and engine parameters. During PSL calibration testing it was discovered than heated probes installed through tunnel sidewalls experienced ice buildup aft of their location due to ice crystals impinging upon them, melting and running back. Filtered city water was used in the cloud generation nozzle system to provide ice crystal nucleation sites. This resulted in mineralization forming on flow path hardware that led to a chronic degradation of performance during the month long test. Lacking internal flow path cameras, the response of thermocouples along the flow path was interpreted as ice building up. Using this interpretation, a strong correlation between total water content (TWC) and a weaker correlation between median volumetric diameter (MVD) of the ice crystal cloud and the rate of ice buildup along the instrumented flow path was identified. For this test article the engine anti-ice system was required to be turned on before ice crystal icing

  13. Preliminary Results From a Heavily Instrumented Engine Ice Crystal Icing Test in a Ground Based Altitude Test Facility

    NASA Technical Reports Server (NTRS)

    Flegel, Ashlie B.; Oliver, Michael J.

    2016-01-01

    Preliminary results from the Heavily Instrumented ALF503R-5 Engine test conducted in the NASA Glenn Research Center Propulsion Systems Laboratory will be discussed. The effects of ice crystal icing on a full scale engine is examined and documented. This model engine, serial number LF01, was used during the inaugural icing test in the PSL facility. The reduction of thrust (rollback) events experienced by this engine in flight were replicated in the facility. Limited instrumentation was used to detect icing. Metal temperature on the exit guide vanes and outer shroud and the load measurement were the only indicators of ice formation. The current study features a similar engine, serial number LF11, which is instrumented to characterize the cloud entering the engine, detect characterize ice accretion, and visualize the ice accretion in the region of interest.

  14. Ice shelf breaking and increase velocity of glacier: the view from analogue experiment

    NASA Astrophysics Data System (ADS)

    Corti, Giacomo; Iandelli, Irene

    2013-04-01

    Collapse of the Larsen II platform during the late 90s has generated an increase in velocity if ice sheet discharge, highlighting that these processes may strongly destabilize large ice masses speeding up the plateau discharge toward the sea. Parameters such as ice thickness, valley width and slope, ice pack dimensions may contribute to modulate the effect of increase in ice flow velocity following the removal of ice. We analyze this process through scale analogue models, aimed at reproducing the flow of ice from a plateau into the sea through a narrow valley. The ice is reproduced with a transparent silicone (Polydimethisiloxane), flowing at velocities of a few centimeters per hour and simulating natural velocities in the range of a few meters per year. Having almost the same density of the ice, PDMS floats on water and simulate the ice-shelf formation. Results of preliminary experimental series support that this methodology is able to reasonably reproduce the process and support a significant increase in velocity discharge following the removal of ice pack. Additional tests are designed to verify the influence of the above-mentioned parameters on the increase in ice velocity.

  15. Early Testing in the Icing Research Tunnel

    NASA Image and Video Library

    1944-09-21

    National Advisory Committee for Aeronautics (NACA) design engineers added the Icing Research Tunnel to the new Aircraft Engine Research Laboratory’s original layout to take advantage of the massive refrigeration system being constructed for the Altitude Wind Tunnel. The Icing Research Tunnel was built to study the formation of ice on aircraft surfaces and methods of preventing or eradicating that ice. Ice buildup adds extra weight, effects aerodynamics, and sometimes blocks airflow through engines. The Icing Research Tunnel is a closed-loop atmospheric wind tunnel with a 6- by 9-foot test section. The tunnel can produce speeds up to 300 miles per hour and temperatures from about 30 to –45⁰ F. Initially the tunnel used a spray bar system to introduce moisture into the airstream. NACA engineers struggled for nearly 10 years to perfect the spray system. The Icing Research Tunnel began testing in June of 1944. Initial testing, seen in this photograph, studied ice accumulation on propellers of a military aircraft. NACA reserach also produced a protected air scoop for the C–46 transport aircraft. A large number of C–46 aircraft were lost due to icing while flying supply runs over the Himalayas during World War II.

  16. Facility for testing ice drills

    NASA Astrophysics Data System (ADS)

    Nielson, Dennis L.; Delahunty, Chris; Goodge, John W.; Severinghaus, Jeffery P.

    2017-05-01

    The Rapid Access Ice Drill (RAID) is designed for subsurface scientific investigations in Antarctica. Its objectives are to drill rapidly through ice, to core samples of the transition zone and bedrock, and to leave behind a borehole observatory. These objectives required the engineering and fabrication of an entirely new drilling system that included a modified mining-style coring rig, a unique fluid circulation system, a rod skid, a power unit, and a workshop with areas for the storage of supplies and consumables. An important milestone in fabrication of the RAID was the construction of a North American Test (NAT) facility where we were able to test drilling and fluid processing functions in an environment that is as close as possible to that expected in Antarctica. Our criteria for site selection was that the area should be cold during the winter months, be located in an area of low heat flow, and be at relatively high elevation. We selected a site for the facility near Bear Lake, Utah, USA. The general design of the NAT well (NAT-1) started with a 27.3 cm (10.75 in.) outer casing cemented in a 152 m deep hole. Within that casing, we hung a 14 cm (5.5 in.) casing string, and, within that casing, a column of ice was formed. The annulus between the 14 and 27.3 cm casings provided the path for circulation of a refrigerant. After in-depth study, we chose to use liquid CO2 to cool the hole. In order to minimize the likelihood of the casing splitting due to the volume increase associated with freezing water, the hole was first cooled and then ice was formed in increments from the bottom upward. First, ice cubes were placed in the inner liner and then water was added. Using this method, a column of ice was incrementally prepared for drilling tests. The drilling tests successfully demonstrated the functioning of the RAID system. Reproducing such a facility for testing of other ice drilling systems could be advantageous to other research programs in the future.

  17. Parameterization and scaling of Arctic ice conditions in the context of ice-atmosphere processes

    NASA Technical Reports Server (NTRS)

    Barry, R. G.; Heinrichs, J.; Steffen, K.; Maslanik, J. A.; Key, J.; Serreze, M. C.; Weaver, R. W.

    1994-01-01

    This report summarizes achievements during year three of our project to investigate the use of ERS-1 SAR data to study Arctic ice and ice/atmosphere processes. The project was granted a one year extension, and goals for the final year are outlined. The specific objects of the project are to determine how the development and evolution of open water/thin ice areas within the interior ice pack vary under different atmospheric synoptic regimes; compare how open water/thin ice fractions estimated from large-area divergence measurements differ from fractions determined by summing localized openings in the pack; relate these questions of scale and process to methods of observation, modeling, and averaging over time and space; determine whether SAR data might be used to calibrate ice concentration estimates from medium and low-rate bit sensors (AVHRR and DMSP-OLS) and the special sensor microwave imager (SSM/I); and investigate methods to integrate SAR data for turbulent heat flux parametrization at the atmosphere interface with other satellite data.

  18. UNC ice vest testing

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Bartley, P.L.

    1986-09-04

    The Barrir Wear Ice Vest (Barrier Vest) was tested at UNC from June 6, 1986 to June 24, 1986. The test was very successful with 27 of the 29 test responses indicating a safer work environment and a desire to wear the vest again.

  19. Measured Black Carbon Deposition on the Sierra Nevada Snow Pack and Implication for Snow Pack Retreat

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Hadley, O.L.; Corrigan, C.E.; Kirchstetter, T.W.

    2010-01-12

    Modeling studies show that the darkening of snow and ice by black carbon deposition is a major factor for the rapid disappearance of arctic sea ice, mountain glaciers and snow packs. This study provides one of the first direct measurements for the efficient removal of black carbon from the atmosphere by snow and its subsequent deposition to the snow packs of California. The early melting of the snow packs in the Sierras is one of the contributing factors to the severe water problems in California. BC concentrations in falling snow were measured at two mountain locations and in rain atmore » a coastal site. All three stations reveal large BC concentrations in precipitation, ranging from 1.7 ng/g to 12.9 ng/g. The BC concentrations in the air after the snow fall were negligible suggesting an extremely efficient removal of BC by snow. The data suggest that below cloud scavenging, rather than ice nuclei, was the dominant source of BC in the snow. A five-year comparison of BC, dust, and total fine aerosol mass concentrations at multiple sites reveals that the measurements made at the sampling sites were representative of large scale deposition in the Sierra Nevada. The relative concentration of iron and calcium in the mountain aerosol indicates that one-quarter to one-third of the BC may have been transported from Asia.« less

  20. Winter snow conditions on Arctic sea ice north of Svalbard during the Norwegian young sea ICE (N-ICE2015) expedition

    NASA Astrophysics Data System (ADS)

    Merkouriadi, Ioanna; Gallet, Jean-Charles; Graham, Robert M.; Liston, Glen E.; Polashenski, Chris; Rösel, Anja; Gerland, Sebastian

    2017-10-01

    Snow is a crucial component of the Arctic sea ice system. Its thickness and thermal properties control heat conduction and radiative fluxes across the ocean, ice, and atmosphere interfaces. Hence, observations of the evolution of snow depth, density, thermal conductivity, and stratigraphy are crucial for the development of detailed snow numerical models predicting energy transfer through the snow pack. Snow depth is also a major uncertainty in predicting ice thickness using remote sensing algorithms. Here we examine the winter spatial and temporal evolution of snow physical properties on first-year (FYI) and second-year ice (SYI) in the Atlantic sector of the Arctic Ocean, during the Norwegian young sea ICE (N-ICE2015) expedition (January to March 2015). During N-ICE2015, the snow pack consisted of faceted grains (47%), depth hoar (28%), and wind slab (13%), indicating very different snow stratigraphy compared to what was observed in the Pacific sector of the Arctic Ocean during the SHEBA campaign (1997-1998). Average snow bulk density was 345 kg m-3 and it varied with ice type. Snow depth was 41 ± 19 cm in January and 56 ± 17 cm in February, which is significantly greater than earlier suggestions for this region. The snow water equivalent was 14.5 ± 5.3 cm over first-year ice and 19 ± 5.4 cm over second-year ice.

  1. Icing Simulation Research Supporting the Ice-Accretion Testing of Large-Scale Swept-Wing Models

    NASA Technical Reports Server (NTRS)

    Yadlin, Yoram; Monnig, Jaime T.; Malone, Adam M.; Paul, Bernard P.

    2018-01-01

    The work summarized in this report is a continuation of NASA's Large-Scale, Swept-Wing Test Articles Fabrication; Research and Test Support for NASA IRT contract (NNC10BA05 -NNC14TA36T) performed by Boeing under the NASA Research and Technology for Aerospace Propulsion Systems (RTAPS) contract. In the study conducted under RTAPS, a series of icing tests in the Icing Research Tunnel (IRT) have been conducted to characterize ice formations on large-scale swept wings representative of modern commercial transport airplanes. The outcome of that campaign was a large database of ice-accretion geometries that can be used for subsequent aerodynamic evaluation in other experimental facilities and for validation of ice-accretion prediction codes.

  2. High-Strain-Rate Compression Testing of Ice

    NASA Technical Reports Server (NTRS)

    Shazly, Mostafa; Prakash, Vikas; Lerch, Bradley A.

    2006-01-01

    In the present study a modified split Hopkinson pressure bar (SHPB) was employed to study the effect of strain rate on the dynamic material response of ice. Disk-shaped ice specimens with flat, parallel end faces were either provided by Dartmouth College (Hanover, NH) or grown at Case Western Reserve University (Cleveland, OH). The SHPB was adapted to perform tests at high strain rates in the range 60 to 1400/s at test temperatures of -10 and -30 C. Experimental results showed that the strength of ice increases with increasing strain rates and this occurs over a change in strain rate of five orders of magnitude. Under these strain rate conditions the ice microstructure has a slight influence on the strength, but it is much less than the influence it has under quasi-static loading conditions. End constraint and frictional effects do not influence the compression tests like they do at slower strain rates, and therefore the diameter/thickness ratio of the samples is not as critical. The strength of ice at high strain rates was found to increase with decreasing test temperatures. Ice has been identified as a potential source of debris to impact the shuttle; data presented in this report can be used to validate and/or develop material models for ice impact analyses for shuttle Return to Flight efforts.

  3. Ice Crystal Icing Engine Testing in the NASA Glenn Research Center's Propulsion Systems Laboratory: Altitude Investigation

    NASA Technical Reports Server (NTRS)

    Oliver, Michael J.

    2014-01-01

    The National Aeronautics and Space Administration (NASA) conducted a full scale ice crystal icing turbofan engine test using an obsolete Allied Signal ALF502-R5 engine in the Propulsion Systems Laboratory (PSL) at NASA Glenn Research Center. The test article used was the exact engine that experienced a loss of power event after the ingestion of ice crystals while operating at high altitude during a 1997 Honeywell flight test campaign investigating the turbofan engine ice crystal icing phenomena. The test plan included test points conducted at the known flight test campaign field event pressure altitude and at various pressure altitudes ranging from low to high throughout the engine operating envelope. The test article experienced a loss of power event at each of the altitudes tested. For each pressure altitude test point conducted the ambient static temperature was predicted using a NASA engine icing risk computer model for the given ambient static pressure while maintaining the engine speed.

  4. Time-dependence of sea-ice concentration and multiyear ice fraction in the Arctic Basin

    USGS Publications Warehouse

    Gloersen, P.; Zwally, H.J.; Chang, A.T.C.; Hall, D.K.; Campbell, W.J.; Ramseier, R.O.

    1978-01-01

    The time variation of the sea-ice concentration and multiyear ice fraction within the pack ice in the Arctic Basin is examined, using microwave images of sea ice recently acquired by the Nimbus-5 spacecraft and the NASA CV-990 airborne laboratory. The images used for these studies were constructed from data acquired from the Electrically Scanned Microwave Radiometer (ESMR) which records radiation from earth and its atmosphere at a wavelength of 1.55 cm. Data are analyzed for four seasons during 1973-1975 to illustrate some basic differences in the properties of the sea ice during those times. Spacecraft data are compared with corresponding NASA CV-990 airborne laboratory data obtained over wide areas in the Arctic Basin during the Main Arctic Ice Dynamics Joint Experiment (1975) to illustrate the applicability of passive-microwave remote sensing for monitoring the time dependence of sea-ice concentration (divergence). These observations indicate significant variations in the sea-ice concentration in the spring, late fall and early winter. In addition, deep in the interior of the Arctic polar sea-ice pack, heretofore unobserved large areas, several hundred kilometers in extent, of sea-ice concentrations as low as 50% are indicated. ?? 1978 D. Reidel Publishing Company.

  5. Setup in the Icing Research Tunnel Test Section

    NASA Image and Video Library

    1969-02-21

    Technicians set up test hardware inside the test section of the Icing Research Tunnel at the National Aeronautics and Space Administration (NASA) Lewis Research Center. The Icing Research Tunnel was built in the early 1940s to study the formation of ice on aircraft surfaces and develop methods of preventing or eradicating that ice. Ice buildup is dangerous because it adds extra weight, effects aerodynamics, and sometimes blocks air flow through engines. The Icing Research Tunnel is a closed-loop atmospheric wind tunnel with a 6- by 9-foot test section. The tunnel can produce speeds up to 300 miles per hour and temperatures from 30 to -45 °F. NACA engineers struggled initially to perfect a spray bar system to introduce moisture into the airstream. The tunnel was shut down in the late 1950s as the center focused its energy exclusively on space. Industrial customers began using the tunnel sporadically, then steadily, in the 1960s. Boeing, Aerojet, Lockheed, Sikorsky, Beech and others ran tests during the 1960s. Boeing analyzed engine inlets for the CH-47 Chinook, CH-46 (Sea Knight) and CH-113. This photograph was taken during a series of 100 ice-phobic coatings for the Federal Aviation Administration. They found that many of the coatings reduced ice adhesion to the test sample, but they could not be used for aircraft applications.

  6. The phase diagram of high-pressure superionic ice

    DOE PAGES

    Sun, Jiming; Clark, Bryan K.; Torquato, Salvatore; ...

    2015-08-28

    Superionic ice is a special group of ice phases at high temperature and pressure, which may exist in ice-rich planets and exoplanets. In superionic ice liquid hydrogen coexists with a crystalline oxygen sublattice. At high pressures, the properties of superionic ice are largely unknown. Here we report evidence that from 280 GPa to 1.3 TPa, there are several competing phases within the close-packed oxygen sublattice. At even higher pressure, the close-packed structure of the oxygen sublattice becomes unstable to a new unusual superionic phase in which the oxygen sublattice takes the P2 1/c symmetry. We also discover that higher pressuremore » phases have lower transition temperatures. The diffusive hydrogen in the P2 1/c superionic phase shows strong anisotropic behaviour and forms a quasi-two-dimensional liquid. The ionic conductivity changes abruptly in the solid to close-packed superionic phase transition, but continuously in the solid to P2 1/c superionic phase transition.« less

  7. Establishing the Test-Retest Reliability & Concurrent Validity for the Repeat Ice Skating Test (RIST) in Adolescent Male Ice Hockey Players

    ERIC Educational Resources Information Center

    Power, Allan; Faught, Brent E.; Przysucha, Eryk; McPherson, Moira; Montelpare, William

    2012-01-01

    In this study the authors examine the test-retest reliability and concurrent validity of the Repeat Ice Skating Test (RIST). This was an on-ice field anaerobic test that measured average peak power and was validated with 3 anaerobic lab tests: (a) vertical jump, (b) the Margaria-Kalamen stair test, and (c) the Wingate Anaerobic Test. The…

  8. Laboratory test for ice adhesion strength using commercial instrumentation.

    PubMed

    Wang, Chenyu; Zhang, Wei; Siva, Adarsh; Tiea, Daniel; Wynne, Kenneth J

    2014-01-21

    A laboratory test method for evaluating ice adhesion has been developed employing a commercially available instrument normally used for dynamic mechanical analysis (TA RSA-III). This is the first laboratory ice adhesion test that does not require a custom-built apparatus. The upper grip range of ∼10 mm is an enabling feature that is essential for the test. The method involves removal of an ice cylinder from a polymer coating with a probe and the determination of peak removal force (Ps). To validate the test method, the strength of ice adhesion was determined for a prototypical glassy polymer, poly(methyl methacrylate). The distance of the probe from the PMMA surface has been identified as a critical variable for Ps. The new test provides a readily available platform for investigating fundamental surface characteristics affecting ice adhesion. In addition to the ice release test, PMMA coatings were characterized using DSC, DCA, and TM-AFM.

  9. Tests of the Performance of Coatings for Low Ice Adhesion

    NASA Technical Reports Server (NTRS)

    Anderson, David N.; Reich, Allen D.

    1997-01-01

    This paper reports studies of the performance of low-ice-adhesion coatings by NASA Lewis and BFGoodrich. Studies used impact ice accreted both in the NASA Lewis Icing Research Tunnel (IRT) and in the BFGoodrich Icing Wind Tunnel (IWT) and static ice in a BFGoodrich bench-top parallel-plate shear rig. Early tests at NASA Lewis involved simple qualitative evaluations of the ease of removing impact ice from a surface. Coated surfaces were compared with uncoated ones. Some of the coatings were tested again with static ice at BFGoodrich to obtain quantitative measurements. Later, methods to establish the adhesion force on surfaces subjected to impact ice were explored at Lewis. This paper describes the various test programs and the results of testing some of the coatings looked at over the past 5 years. None of the coatings were found to be truly ice-phobic; however, the most effective coatings were found to reduce the adhesion of ice to about 1/2 that of an uncoated aluminum sample.

  10. Electro-impulse de-icing testing analysis and design

    NASA Technical Reports Server (NTRS)

    Zumwalt, G. W.; Schrag, R. L.; Bernhart, W. D.; Friedberg, R. A.

    1988-01-01

    Electro-Impulse De-Icing (EIDI) is a method of ice removal by sharp blows delivered by a transient electromagnetic field. Detailed results are given for studies of the electrodynamic phenomena. Structural dynamic tests and computations are described. Also reported are ten sets of tests at NASA's Icing Research Tunnel and flight tests by NASA and Cessna Aircraft Company. Fabrication of system components are described and illustrated. Fatigue and electromagnetic interference tests are reported. Here, the necessary information for the design of an EIDI system for aircraft is provided.

  11. Ice-Accretion Test Results for Three Large-Scale Swept-Wing Models in the NASA Icing Research Tunnel

    NASA Technical Reports Server (NTRS)

    Broeren, Andy P.; Potapczuk, Mark G.; Lee, Sam; Malone, Adam M.; Paul, Benard P., Jr.; Woodard, Brian S.

    2016-01-01

    Icing simulation tools and computational fluid dynamics codes are reaching levels of maturity such that they are being proposed by manufacturers for use in certification of aircraft for flight in icing conditions with increasingly less reliance on natural-icing flight testing and icing-wind-tunnel testing. Sufficient high-quality data to evaluate the performance of these tools is not currently available. The objective of this work was to generate a database of ice-accretion geometry that can be used for development and validation of icing simulation tools as well as for aerodynamic testing. Three large-scale swept wing models were built and tested at the NASA Glenn Icing Research Tunnel (IRT). The models represented the Inboard (20% semispan), Midspan (64% semispan) and Outboard stations (83% semispan) of a wing based upon a 65% scale version of the Common Research Model (CRM). The IRT models utilized a hybrid design that maintained the full-scale leading-edge geometry with a truncated afterbody and flap. The models were instrumented with surface pressure taps in order to acquire sufficient aerodynamic data to verify the hybrid model design capability to simulate the full-scale wing section. A series of ice-accretion tests were conducted over a range of total temperatures from -23.8 deg C to -1.4 deg C with all other conditions held constant. The results showed the changing ice-accretion morphology from rime ice at the colder temperatures to highly 3-D scallop ice in the range of -11.2 deg C to -6.3 deg C. Warmer temperatures generated highly 3-D ice accretion with glaze ice characteristics. The results indicated that the general scallop ice morphology was similar for all three models. Icing results were documented for limited parametric variations in angle of attack, drop size and cloud liquid-water content (LWC). The effect of velocity on ice accretion was documented for the Midspan and Outboard models for a limited number of test cases. The data suggest that

  12. Ice-Accretion Test Results for Three Large-Scale Swept-Wing Models in the NASA Icing Research Tunnel

    NASA Technical Reports Server (NTRS)

    Broeren, Andy P.; Potapczuk, Mark G.; Lee, Sam; Malone, Adam M.; Paul, Bernard P., Jr.; Woodard, Brian S.

    2016-01-01

    Icing simulation tools and computational fluid dynamics codes are reaching levels of maturity such that they are being proposed by manufacturers for use in certification of aircraft for flight in icing conditions with increasingly less reliance on natural-icing flight testing and icing-wind-tunnel testing. Sufficient high-quality data to evaluate the performance of these tools is not currently available. The objective of this work was to generate a database of ice-accretion geometry that can be used for development and validation of icing simulation tools as well as for aerodynamic testing. Three large-scale swept wing models were built and tested at the NASA Glenn Icing Research Tunnel (IRT). The models represented the Inboard (20 percent semispan), Midspan (64 percent semispan) and Outboard stations (83 percent semispan) of a wing based upon a 65 percent scale version of the Common Research Model (CRM). The IRT models utilized a hybrid design that maintained the full-scale leading-edge geometry with a truncated afterbody and flap. The models were instrumented with surface pressure taps in order to acquire sufficient aerodynamic data to verify the hybrid model design capability to simulate the full-scale wing section. A series of ice-accretion tests were conducted over a range of total temperatures from -23.8 to -1.4 C with all other conditions held constant. The results showed the changing ice-accretion morphology from rime ice at the colder temperatures to highly 3-D scallop ice in the range of -11.2 to -6.3 C. Warmer temperatures generated highly 3-D ice accretion with glaze ice characteristics. The results indicated that the general scallop ice morphology was similar for all three models. Icing results were documented for limited parametric variations in angle of attack, drop size and cloud liquid-water content (LWC). The effect of velocity on ice accretion was documented for the Midspan and Outboard models for a limited number of test cases. The data suggest

  13. The Preservation and Recycling of Snow Pack Nitrate at the West Antarctic Ice Sheet (WAIS) Divide Ice Core Site from the Present Day to the Last Glacial Period.

    NASA Astrophysics Data System (ADS)

    Robinson, J. W.; Buffen, A.; Hastings, M. G.; Schauer, A. J.; Moore, L.; Isaacs, A.; Geng, L.; Savarino, J. P.; Alexander, B.

    2017-12-01

    We use observations of the nitrogen isotopic composition of nitrate (δ15N(NO3-)) from snow and ice collected at the West Antarctic ice sheet (WAIS) divide ice core site to quantify the preservation and recycling of snow nitrate. Ice-core samples cover a continuous section from 36 to 52 thousand years ago and discrete samples from the Holocene, the last glacial maximum (LGM), and the glacial-Holocene transition. Higher δ15N of nitrate is consistently associated with lower temperatures with δ15N(NO3-) varying from 26 to 45 ‰ during the last glacial period and from 1 to 45 ‰ between the Holocene and glacial periods, respectively. We attribute the higher δ15N in colder periods to lower snow accumulation rates which lead to greater loss of snow nitrate via photolysis before burial beneath the snow photic zone. Modeling of nitrate preservation in snow pack was performed for modern and LGM conditions. The model is used in conjunction with observations to estimate the fraction of snow nitrate that is photolyzed, re-oxidized, and re-deposited over WAIS divide versus the fraction of primary nitrate that is deposited via long range transport. We used these estimates of fractional loss of snow nitrate in different time periods to determine the variation in the deposition flux of primary nitrate at WAIS divide with climate. Our findings have implications for the climate sensitivity of the oxidizing capacity of the polar atmosphere and the interpretation of ice-core records of nitrate in terms of past atmospheric composition.

  14. Windows in Arctic sea ice: Light transmission and ice algae in a refrozen lead

    NASA Astrophysics Data System (ADS)

    Kauko, Hanna M.; Taskjelle, Torbjørn; Assmy, Philipp; Pavlov, Alexey K.; Mundy, C. J.; Duarte, Pedro; Fernández-Méndez, Mar; Olsen, Lasse M.; Hudson, Stephen R.; Johnsen, Geir; Elliott, Ashley; Wang, Feiyue; Granskog, Mats A.

    2017-06-01

    The Arctic Ocean is rapidly changing from thicker multiyear to thinner first-year ice cover, with significant consequences for radiative transfer through the ice pack and light availability for algal growth. A thinner, more dynamic ice cover will possibly result in more frequent leads, covered by newly formed ice with little snow cover. We studied a refrozen lead (≤0.27 m ice) in drifting pack ice north of Svalbard (80.5-81.8°N) in May-June 2015 during the Norwegian young sea ICE expedition (N-ICE2015). We measured downwelling incident and ice-transmitted spectral irradiance, and colored dissolved organic matter (CDOM), particle absorption, ultraviolet (UV)-protecting mycosporine-like amino acids (MAAs), and chlorophyll a (Chl a) in melted sea ice samples. We found occasionally very high MAA concentrations (up to 39 mg m-3, mean 4.5 ± 7.8 mg m-3) and MAA to Chl a ratios (up to 6.3, mean 1.2 ± 1.3). Disagreement in modeled and observed transmittance in the UV range let us conclude that MAA signatures in CDOM absorption spectra may be artifacts due to osmotic shock during ice melting. Although observed PAR (photosynthetically active radiation) transmittance through the thin ice was significantly higher than that of the adjacent thicker ice with deep snow cover, ice algal standing stocks were low (≤2.31 mg Chl a m-2) and similar to the adjacent ice. Ice algal accumulation in the lead was possibly delayed by the low inoculum and the time needed for photoacclimation to the high-light environment. However, leads are important for phytoplankton growth by acting like windows into the water column.

  15. Ice Growth Measurements from Image Data to Support Ice Crystal and Mixed-Phase Accretion Testing

    NASA Technical Reports Server (NTRS)

    Struk, Peter M.; Lynch, Christopher J.

    2012-01-01

    This paper describes the imaging techniques as well as the analysis methods used to measure the ice thickness and growth rate in support of ice-crystal icing tests performed at the National Research Council of Canada (NRC) Research Altitude Test Facility (RATFac). A detailed description of the camera setup, which involves both still and video cameras, as well as the analysis methods using the NASA Spotlight software, are presented. Two cases, one from two different test entries, showing significant ice growth are analyzed in detail describing the ice thickness and growth rate which is generally linear. Estimates of the bias uncertainty are presented for all measurements. Finally some of the challenges related to the imaging and analysis methods are discussed as well as methods used to overcome them.

  16. Ice Growth Measurements from Image Data to Support Ice-Crystal and Mixed-Phase Accretion Testing

    NASA Technical Reports Server (NTRS)

    Struk, Peter, M; Lynch, Christopher, J.

    2012-01-01

    This paper describes the imaging techniques as well as the analysis methods used to measure the ice thickness and growth rate in support of ice-crystal icing tests performed at the National Research Council of Canada (NRC) Research Altitude Test Facility (RATFac). A detailed description of the camera setup, which involves both still and video cameras, as well as the analysis methods using the NASA Spotlight software, are presented. Two cases, one from two different test entries, showing significant ice growth are analyzed in detail describing the ice thickness and growth rate which is generally linear. Estimates of the bias uncertainty are presented for all measurements. Finally some of the challenges related to the imaging and analysis methods are discussed as well as methods used to overcome them.

  17. Radar image interpretation techniques applied to sea ice geophysical problems

    NASA Technical Reports Server (NTRS)

    Carsey, F. D.

    1983-01-01

    The geophysical science problems in the sea ice area which at present concern understanding the ice budget, where ice is formed, how thick it grows and where it melts, and the processes which control the interaction of air-sea and ice at the ice margins is discussed. The science problems relate to basic questions of sea ice: how much is there, thickness, drift rate, production rate, determination of the morphology of the ice margin, storms feeling for the ice, storms and influence at the margin to alter the pack, and ocean response to a storm at the margin. Some of these questions are descriptive and some require complex modeling of interactions between the ice, the ocean, the atmosphere and the radiation fields. All involve measurements of the character of the ice pack, and SAR plays a significant role in the measurements.

  18. Mobility of icy sand packs, with application to Martian permafrost

    USGS Publications Warehouse

    Durham, W.B.; Pathare, A.V.; Stern, L.A.; Lenferink, H.J.

    2009-01-01

    [1] The physical state of water on Mars has fundamental ramifications for both climatology and astrobiology. The widespread presence of "softened" Martian landforms (such as impact craters) can be attributed to viscous creep of subsurface ground ice. We present laboratory experiments designed to determine the minimum amount of ice necessary to mobilize topography within Martian permafrost. Our results show that the jammed-to-mobile transition of icy sand packs neither occurs at fixed ice content nor is dependent on temperature or stress, but instead correlates strongly with the maximum dry packing density of the sand component. Viscosity also changes rapidly near the mobility transition. The results suggest a potentially lower minimum volatile inventory for the impact-pulverized megaregolith of Mars. Furthermore, the long-term preservation of partially relaxed craters implies that the ice content of Martian permafrost has remained close to that at the mobility transition throughout Martian history. Copyright 2009 by the American Geophysical Union.

  19. Observing Radiative Properties of a Thinner, Seasonal Arctic Ice Pack

    NASA Astrophysics Data System (ADS)

    Hudson, S. R.; Nicolaus, M.; Granskog, M.; Gerland, S.; Wang, C.

    2011-12-01

    The Arctic is coming to be dominated by young ice, much of it seasonal. Many of our observations of the radiative properties of sea ice come from drifting stations on thick, multi-year ice. To better understand the Arctic climate system in a warmer world, we need more data about the radiative properties and their seasonal and spatial variability on thinner, younger ice. Since this younger ice is not always thick enough to support lengthy drifting stations, there is a need for new technologies to help us get optical measurements on seasonal ice. One challenge is obtaining seasonal data on ice that is too weak to support even a ship-based camp, and especially to have these observations extend well into the melt season. For these situations, we have developed a spectral radiation monitoring buoy that can be deployed during a one-day ice station, and that can then autonomously observe the spectral albedo and transmittance of the sea ice, transmitting all data in near real time by satellite, until the buoy melts out. Similar installations at manned or regularly visited sites have provided good data, with surprisingly few data-quality problems due to frost, precipitation, or tilting. The buoys consist of 3 spectral radiometers, covering wavelengths 350 to 800 nm, and a datalogger with an Irridium modem. The datalogger and necessary batteries are inside a sealed housing which is frozen into a hole drilled in the ice. Arms extend from both the top and bottom of the housing, holding sensors that measure incident, reflected, and transmitted spectra. The under-ice radiometer is equipped with a bioshutter to avoid algal growth on the sensor. They will be deployed alongside ice mass balance buoys, providing data about the physical development of the ice and snow, as well as position. While the buoys provide an excellent record of diurnal, synoptic, and seasonal variability, they are fixed to one location in the ice, so other methods are still needed for measuring the spatial

  20. Variational Ridging in Sea Ice Models

    NASA Astrophysics Data System (ADS)

    Roberts, A.; Hunke, E. C.; Lipscomb, W. H.; Maslowski, W.; Kamal, S.

    2017-12-01

    This work presents the results of a new development to make basin-scale sea ice models aware of the shape, porosity and extent of individual ridges within the pack. We have derived an analytic solution for the Euler-Lagrange equation of individual ridges that accounts for non-conservative forces, and therefore the compressive strength of individual ridges. Because a region of the pack is simply a collection of paths of individual ridges, we are able to solve the Euler-Lagrange equation for a large-scale sea ice field also, and therefore the compressive strength of a region of the pack that explicitly accounts for the macro-porosity of ridged debris. We make a number of assumptions that have simplified the problem, such as treating sea ice as a granular material in ridges, and assuming that bending moments associated with ridging are perturbations around an isostatic state. Regardless of these simplifications, the ridge model is remarkably predictive of macro-porosity and ridge shape, and, because our equations are analytic, they do not require costly computations to solve the Euler-Lagrange equation of ridges on the large scale. The new ridge model is therefore applicable to large-scale sea ice models. We present results from this theoretical development, as well as plans to apply it to the Regional Arctic System Model and a community sea ice code. Most importantly, the new ridging model is particularly useful for pinpointing gaps in our observational record of sea ice ridges, and points to the need for improved measurements of the evolution of porosity of deformed ice in the Arctic and Antarctic. Such knowledge is not only useful for improving models, but also for improving estimates of sea ice volume derived from altimetric measurements of sea ice freeboard.

  1. Ice Crystal Icing Engine Testing in the NASA Glenn Research Center's Propulsion Systems Laboratory (PSL): Altitude Investigation

    NASA Technical Reports Server (NTRS)

    Oliver, Michael J.

    2015-01-01

    The National Aeronautics and Space Administration conducted a full scale ice crystal icing turbofan engine test in the NASA Glenn Research Centers Propulsion Systems Laboratory (PSL) Facility in February 2013. Honeywell Engines supplied the test article, an obsolete, unmodified Lycoming ALF502-R5 turbofan engine serial number LF01 that experienced an un-commanded loss of thrust event while operating at certain high altitude ice crystal icing conditions. These known conditions were duplicated in the PSL for this testing.

  2. Collar temperature sensor data reveal long-term patterns in southern Beaufort Sea polar bear den distribution on pack ice and land

    USGS Publications Warehouse

    Olson, Jay W; Rode, Karyn D.; Eggett, Dennis L.; Smith, T.S.; Wilson, R. R.; Durner, George M.; Fischbach, Anthony S.; Atwood, Todd C.; Douglas, David C.

    2017-01-01

    In response to a changing climate, many species alter habitat use. Polar bears Ursus maritimus in the southern Beaufort Sea have increasingly used land for maternal denning. To aid in detecting denning behavior, we developed an objective method to identify polar bear denning events using temperature sensor data collected by satellite-linked transmitters deployed on adult females between 1985 and 2013. We then applied this method to determine whether southern Beaufort Sea polar bears have continued to increase land denning with recent sea-ice loss and examined whether sea-ice conditions affect the distribution of dens between pack-ice and coastal substrates. Because land use in summer and autumn has also increased, we examined potential associations between summering substrate and denning substrate. Statistical process control methods applied to temperature-sensor data identified denning events with 94.5% accuracy in comparison to direct observations (n = 73) and 95.7% accuracy relative to subjective classifications based on temperature, location, and activity sensor data (n = 116). We found an increase in land-based denning during the study period. The frequency of land denning was directly related to the distance that sea ice retreated from the coast. Among females that denned, all 14 that summered on land subsequently denned there, whereas 29% of the 69 bears summering on ice denned on land. These results suggest that denning on land may continue to increase with further loss of sea ice. While the effects that den substrate have on nutrition, energetics, and reproduction are unclear, more polar bears denning onshore will likely increase human-bear interactions.

  3. Arctic Ice Dynamics Joint Experiment (AIDJEX) assumptions revisited and found inadequate

    NASA Astrophysics Data System (ADS)

    Coon, Max; Kwok, Ron; Levy, Gad; Pruis, Matthew; Schreyer, Howard; Sulsky, Deborah

    2007-11-01

    This paper revisits the Arctic Ice Dynamics Joint Experiment (AIDJEX) assumptions about pack ice behavior with an eye to modeling sea ice dynamics. The AIDJEX assumptions were that (1) enough leads were present in a 100 km by 100 km region to make the ice isotropic on that scale; (2) the ice had no tensile strength; and (3) the ice behavior could be approximated by an isotropic yield surface. These assumptions were made during the development of the AIDJEX model in the 1970s, and are now found inadequate. The assumptions were made in part because of insufficient large-scale (10 km) deformation and stress data, and in part because of computer capability limitations. Upon reviewing deformation and stress data, it is clear that a model including deformation on discontinuities and an anisotropic failure surface with tension would better describe the behavior of pack ice. A model based on these assumptions is needed to represent the deformation and stress in pack ice on scales from 10 to 100 km, and would need to explicitly resolve discontinuities. Such a model would require a different class of metrics to validate discontinuities against observations.

  4. Evaluation of constant-Weber-number scaling for icing tests

    NASA Technical Reports Server (NTRS)

    Anderson, David N.

    1996-01-01

    Previous studies showed that for conditions simulating an aircraft encountering super-cooled water droplets the droplets may splash before freezing. Other surface effects dependent on the water surface tension may also influence the ice accretion process. Consequently, the Weber number appears to be important in accurately scaling ice accretion. A scaling method which uses a constant-Weber-number approach has been described previously; this study provides an evaluation of this scaling method. Tests are reported on cylinders of 2.5 to 15-cm diameter and NACA 0012 airfoils with chords of 18 to 53 cm in the NASA Lewis Icing Research Tunnel (IRT). The larger models were used to establish reference ice shapes, the scaling method was applied to determine appropriate scaled test conditions using the smaller models, and the ice shapes were compared. Icing conditions included warm glaze, horn glaze and mixed. The smallest size scaling attempted was 1/3, and scale and reference ice shapes for both cylinders and airfoils indicated that the constant-Weber-number scaling method was effective for the conditions tested.

  5. Multiscale Models of Melting Arctic Sea Ice

    DTIC Science & Technology

    2013-09-30

    September 29, 2013 LONG-TERM GOALS Sea ice reflectance or albedo , a key parameter in climate modeling, is primarily determined by melt pond...and ice floe configurations. Ice - albedo feedback has played a major role in the recent declines of the summer Arctic sea ice pack. However...understanding the evolution of melt ponds and sea ice albedo remains a significant challenge to improving climate models. Our research is focused on

  6. Implications of fractured Arctic perennial ice cover on thermodynamic and dynamic sea ice processes

    NASA Astrophysics Data System (ADS)

    Asplin, Matthew G.; Scharien, Randall; Else, Brent; Howell, Stephen; Barber, David G.; Papakyriakou, Tim; Prinsenberg, Simon

    2014-04-01

    Decline of the Arctic summer minimum sea ice extent is characterized by large expanses of open water in the Siberian, Laptev, Chukchi, and Beaufort Seas, and introduces large fetch distances in the Arctic Ocean. Long waves can propagate deep into the pack ice, thereby causing flexural swell and failure of the sea ice. This process shifts the floe size diameter distribution smaller, increases floe surface area, and thereby affects sea ice dynamic and thermodynamic processes. The results of Radarsat-2 imagery analysis show that a flexural fracture event which occurred in the Beaufort Sea region on 6 September 2009 affected ˜40,000 km2. Open water fractional area in the area affected initially decreased from 3.7% to 2.7%, but later increased to ˜20% following wind-forced divergence of the ice pack. Energy available for lateral melting was assessed by estimating the change in energy entrainment from longwave and shortwave radiation in the mixed-layer of the ocean following flexural fracture. 11.54 MJ m-2 of additional energy for lateral melting of ice floes was identified in affected areas. The impact of this process in future Arctic sea ice melt seasons was assessed using estimations of earlier occurrences of fracture during the melt season, and is discussed in context with ocean heat fluxes, atmospheric mixing of the ocean mixed layer, and declining sea ice cover. We conclude that this process is an important positive feedback to Arctic sea ice loss, and timing of initiation is critical in how it affects sea ice thermodynamic and dynamic processes.

  7. Sea ice and surface water circulation, Alaskan Continental Shelf

    NASA Technical Reports Server (NTRS)

    Wright, F. F. (Principal Investigator); Sharma, G. D.; Burn, J. J.

    1973-01-01

    The author has identified the following significant results. The boundaries of land-fast ice, distribution of pack ice, and major polynya were studied in the vicinity of the Bering Strait. Movement of pack ice during 24 hours was determined by plotting the distinctly identifiable ice floes on ERTS-1 imagery obtained from two consecutive passes. Considerably large shallow area along the western Seward Peninsula just north of the Bering Strait is covered by land fast ice. This ice hinders the movement of ice formed in eastern Chukchi Sea southward through the Bering Strait. The movement of ice along the Russian coast is relatively faster. Plotting of some of the ice floes indicated movement of ice in excess of 30 km in and south of the Bering Strait between 6 and 7 March, 1973. North of the Bering Strait the movement approached 18 km. The movement of ice observed during March 6 and 7 considerably altered the distribution and extent of polynya. These features when continually plotted should be of considerable aid in navigation of ice breakers. The movement of ice will also help delineate the migration and distribution of sea mammals.

  8. Atmospheric forcing of sea ice leads in the Beaufort Sea

    NASA Astrophysics Data System (ADS)

    Lewis, B. J.; Hutchings, J.; Mahoney, A. R.; Shapiro, L. H.

    2016-12-01

    Leads in sea ice play an important role in the polar marine environment where they allow heat and moisture transfer between the oceans and atmosphere and act as travel pathways for both marine mammals and ships. Examining AVHRR thermal imagery of the Beaufort Sea, collected between 1994 and 2010, sea ice leads appear in repeating patterns and locations (Eicken et al 2005). The leads, resolved by AVHRR, are at least 250m wide (Mahoney et al 2012), thus the patterns described are for lead systems that extend up to hundreds of kilometers across the Beaufort Sea. We describe how these patterns are associated with the location of weather systems relative to the coastline. Mean sea level pressure and 10m wind fields from ECMWF ERA-Interim reanalysis are used to identify if particular lead patterns can be uniquely forecast based on the location of weather systems. Ice drift data from the NSIDC's Polar Pathfinder Daily 25km EASE-Grid Sea Ice Motion Vectors indicates the role shear along leads has on the motion of ice in the Beaufort Gyre. Lead formation is driven by 4 main factors: (i) coastal features such as promontories and islands influence the origin of leads by concentrating stresses within the ice pack; (ii) direction of the wind forcing on the ice pack determines the type of fracture, (iii) the location of the anticyclone (or cyclone) center determines the length of the fracture for certain patterns; and (iv) duration of weather conditions affects the width of the ice fracture zones. Movement of the ice pack on the leeward side of leads originating at promontories and islands increases, creating shear zones that control ice transport along the Alaska coast in winter. . Understanding how atmospheric conditions influence the large-scale motion of the ice pack is needed to design models that predict variability of the gyre and export of multi-year ice to lower latitudes.

  9. Particulate matter in pack ice of the Beaufort Gyre

    USGS Publications Warehouse

    Reimnitz, E.; Barnes, P.W.; Weber, W.S.

    1993-01-01

    Fine sediment occurred in very small patches of turbid ice, as thin spotty surface layers, in mud pellets or in old snowdrifts. The latter were widespread south of 74??N, containing an estimated 22 tonnes of silt and clay km-2. Average particle concentration in sea ice (40 mg1-1) was much higher than in sea water (0.8 mg 1 -1) or in new snow. Assuming one-third of the load is released each year, the estimated deposition rate would equal the measured Holocene rate (~2cm 1000 year-1). Therefore, modern sea-ice rafting represents a substantial fraction of the total Arctic Ocean sediment budget. -from Authors

  10. Characterization of the mechanical behavior of sea ice as a frictional material

    NASA Astrophysics Data System (ADS)

    Lade, Poul V.

    2002-12-01

    The mechanical properties of sea ice are determined by the formation process, and the consequent material behavior at the element scale exhibits viscoelastic behavior at the early loading stages, followed by brittle fracture or ductile, irrecoverable deformation that may be captured by hardening/softening plasticity models with nonassociated flow. Failure of sea ice under different loading conditions follows a pattern that demonstrates its highly cross-anisotropic nature as well as its behavior as a frictional material. The interactions between the floes in the pack ice resemble those observed in granular materials. These materials are frictional in nature, they exhibit both contractive and dilative volume changes, the plastic flow is nonassociated, and their stiffnesses and strengths increase with confining pressure, but they do not have any strength when unconfined. The overall behavior of the pack ice may be close to isotropic. Constitutive modeling of this behavior may be achieved by models used in geotechnical engineering. Formation of leads and subsequent freezing of the water results in cementation between the ice floes, and the pack ice becomes stronger. The behavior of the pack ice may now be compared with that observed in cemented soils or concrete. For these materials, increasing amounts of cementation result in increasing rates of dilation when sheared, and this accounts for the largest contribution to the increase in shear strength.

  11. Ice tracking techniques, implementation, performance, and applications

    NASA Technical Reports Server (NTRS)

    Rothrock, D. A.; Carsey, F. D.; Curlander, J. C.; Holt, B.; Kwok, R.; Weeks, W. F.

    1992-01-01

    Present techniques of ice tracking make use both of cross-correlation and of edge tracking, the former being more successful in heavy pack ice, the latter being critical for the broken ice of the pack margins. Algorithms must assume some constraints on the spatial variations of displacements to eliminate fliers, but must avoid introducing any errors into the spatial statistics of the measured displacement field. We draw our illustrations from the implementation of an automated tracking system for kinematic analyses of ERS-1 and JERS-1 SAR imagery at the University of Alaska - the Alaska SAR Facility's Geophysical Processor System. Analyses of the ice kinematic data that might have some general interest to analysts of cloud-derived wind fields are the spatial structure of the fields, and the evaluation and variability of average deformation and its invariants: divergence, vorticity and shear. Many problems in sea ice dynamics and mechanics can be addressed with the kinematic data from SAR.

  12. Dissolved iron and iron(II) distributions beneath the pack ice in the East Antarctic (120°E) during the winter/spring transition

    NASA Astrophysics Data System (ADS)

    Schallenberg, Christina; van der Merwe, Pier; Chever, Fanny; Cullen, Jay T.; Lannuzel, Delphine; Bowie, Andrew R.

    2016-09-01

    Distributions of dissolved iron (dFe) and its reduced form, Fe(II), to a depth of 1000 m were investigated under the seasonal pack ice off East Antarctica during the Sea Ice Physics and Ecosystem experiment (SIPEX-2) sea-ice voyage in September-October 2012. Concentrations of dFe were elevated up to five-fold relative to Southern Ocean background concentrations and were spatially variable. The mean dFe concentration was 0.44±0.4 nM, with a range from 0.09 to 3.05 nM. Profiles of dFe were more variable within and among stations than were macronutrients, suggesting that coupling between these biologically-essential elements was weak at the time of the study. Brine rejection and drainage from sea ice are estimated to be the dominant contributors to elevated dFe concentrations in the mixed layer, but mass budget considerations indicate that estimated dFe fluxes from brine input alone are insufficient to account for all observed dFe. Melting icebergs and shelf sediments are suspected to provide the additional dFe. Fe(II) was mostly below the detection limit but elevated at depth near the continental shelf, implying that benthic processes are a source of reduced Fe in bottom waters. The data indicate that dFe builds up under the seasonal sea-ice cover during winter and that reduction of Fe may be hampered in early spring by several factors such as lack of electron donors, low biological productivity and inadequate light below the sea ice. The accumulated dFe pool in the mixed layer is expected to contribute to the formation of the spring bloom as the ice retreats.

  13. Survey of aircraft icing simulation test facilities in North America

    NASA Technical Reports Server (NTRS)

    Olsen, W.

    1981-01-01

    A survey was made of the aircraft icing simulation facilities in North America: there are 12 wind tunnels, 28 engine test facilities, 6 aircraft tankers and 14 low velocity facilities, that perform aircraft icing tests full or part time. The location and size of the facility, its speed and temperature range, icing cloud parameters, and the technical person to contact are surveyed. Results are presented in tabular form. The capabilities of each facility were estimated by its technical contact person. The adequacy of these facilities for various types of icing tests is discussed.

  14. Wind Tunnel Tests Conducted to Develop an Icing Flight Simulator

    NASA Technical Reports Server (NTRS)

    Ratvasky, Thomas P.

    2001-01-01

    As part of NASA's Aviation Safety Program goals to reduce aviation accidents due to icing, NASA Glenn Research Center is leading a flight simulator development activity to improve pilot training for the adverse flying characteristics due to icing. Developing flight simulators that incorporate the aerodynamic effects of icing will provide a critical element in pilot training programs by giving pilots a pre-exposure of icing-related hazards, such as ice-contaminated roll upset or tailplane stall. Integrating these effects into training flight simulators will provide an accurate representation of scenarios to develop pilot skills in unusual attitudes and loss-of-control events that may result from airframe icing. In order to achieve a high level of fidelity in the flight simulation, a series of wind tunnel tests have been conducted on a 6.5-percent-scale Twin Otter aircraft model. These wind tunnel tests were conducted at the Wichita State University 7- by 10-ft wind tunnel and Bihrle Applied Research's Large Amplitude Multiple Purpose Facility in Neuburg, Germany. The Twin Otter model was tested without ice (baseline), and with two ice configurations: 1) Ice on the horizontal tail only; 2) Ice on the wing, horizontal tail, and vertical tail. These wind tunnel tests resulted in data bases of aerodynamic forces and moments as functions of angle of attack; sideslip; control surface deflections; forced oscillations in the pitch, roll, and yaw axes; and various rotational speeds. A limited amount of wing and tail surface pressure data were also measured for comparison with data taken at Wichita State and with flight data. The data bases from these tests will be the foundation for a PC-based Icing Flight Simulator to be delivered to Glenn in fiscal year 2001.

  15. Variability of Antarctic Sea Ice 1979-1998

    NASA Technical Reports Server (NTRS)

    Zwally, H. Jay; Comiso, Josefino C.; Parkinson, Claire L.; Cavalieri, Donald J.; Gloersen, Per; Koblinsky, Chester J. (Technical Monitor)

    2001-01-01

    The principal characteristics of the variability of Antarctic sea ice cover as previously described from satellite passive-microwave observations are also evident in a systematically-calibrated and analyzed data set for 20.2 years (1979-1998). The total Antarctic sea ice extent (concentration > 15 %) increased by 13,440 +/- 4180 sq km/year (+1.18 +/- 0.37%/decade). The area of sea ice within the extent boundary increased by 16,960 +/- 3,840 sq km/year (+1.96 +/- 0.44%/decade). Regionally, the trends in extent are positive in the Weddell Sea (1.5 +/- 0.9%/decade), Pacific Ocean (2.4 +/- 1.4%/decade), and Ross (6.9 +/- 1.1 %/decade) sectors, slightly negative in the Indian Ocean (-1.5 +/- 1.8%/decade, and strongly negative in the Bellingshausen-Amundsen Seas sector (-9.5 +/- 1.5%/decade). For the entire ice pack, small ice increases occur in all seasons with the largest increase during autumn. On a regional basis, the trends differ season to season. During summer and fall, the trends are positive or near zero in all sectors except the Bellingshausen-Amundsen Seas sector. During winter and spring, the trends are negative or near zero in all sectors except the Ross Sea, which has positive trends in all seasons. Components of interannual variability with periods of about 3 to 5 years are regionally large, but tend to counterbalance each other in the total ice pack. The interannual variability of the annual mean sea-ice extent is only 1.6% overall, compared to 5% to 9% in each of five regional sectors. Analysis of the relation between regional sea ice extents and spatially-averaged surface temperatures over the ice pack gives an overall sensitivity between winter ice cover and temperature of -0.7% change in sea ice extent per K. For summer, some regional ice extents vary positively with temperature and others negatively. The observed increase in Antarctic sea ice cover is counter to the observed decreases in the Arctic. It is also qualitatively consistent with the

  16. Females roam while males patrol: divergence in breeding season movements of pack-ice polar bears (Ursus maritimus).

    PubMed

    Laidre, Kristin L; Born, Erik W; Gurarie, Eliezer; Wiig, Øystein; Dietz, Rune; Stern, Harry

    2013-02-07

    Intraspecific differences in movement behaviour reflect different tactics used by individuals or sexes to favour strategies that maximize fitness. We report movement data collected from n = 23 adult male polar bears with novel ear-attached transmitters in two separate pack ice subpopulations over five breeding seasons. We compared movements with n = 26 concurrently tagged adult females, and analysed velocities, movement tortuosity, range sizes and habitat selection with respect to sex, reproductive status and body mass. There were no differences in 4-day displacements or sea ice habitat selection for sex or population. By contrast, adult females in all years and both populations had significantly more linear movements and significantly larger breeding range sizes than males. We hypothesized that differences were related to encounter rates, and used observed movement metrics to parametrize a simulation model of male-male and male-female encounter. The simulation showed that the more tortuous movement of males leads to significantly longer times to male-male encounter, while having little impact on male-female encounter. By contrast, linear movements of females are consistent with a prioritized search for sparsely distributed prey. These results suggest a possible mechanism for explaining the smaller breeding range sizes of some solitary male carnivores compared to females.

  17. Overview of Sea-Ice Properties, Distribution and Temporal Variations, for Application to Ice-Atmosphere Chemical Processes.

    NASA Astrophysics Data System (ADS)

    Moritz, R. E.

    2005-12-01

    The properties, distribution and temporal variation of sea-ice are reviewed for application to problems of ice-atmosphere chemical processes. Typical vertical structure of sea-ice is presented for different ice types, including young ice, first-year ice and multi-year ice, emphasizing factors relevant to surface chemistry and gas exchange. Time average annual cycles of large scale variables are presented, including ice concentration, ice extent, ice thickness and ice age. Spatial and temporal variability of these large scale quantities is considered on time scales of 1-50 years, emphasizing recent and projected changes in the Arctic pack ice. The amount and time evolution of open water and thin ice are important factors that influence ocean-ice-atmosphere chemical processes. Observations and modeling of the sea-ice thickness distribution function are presented to characterize the range of variability in open water and thin ice.

  18. Study of Cold Heat Energy Release Characteristics of Flowing Ice Water Slurry in a Pipe

    NASA Astrophysics Data System (ADS)

    Inaba, Hideo; Horibe, Akihiko; Ozaki, Koichi; Yokota, Maki

    This paper has dealt with melting heat transfer characteristics of ice water slurry in an inside tube of horizontal double tube heat exchanger in which a hot water circulated in an annular gap between the inside and outside tubes. Two kinds of heat exchangers were used; one is made of acrylic resin tube for flow visualization and the other is made of stainless steel tube for melting heat transfer measurement. The result of flow visualization revealed that ice particles flowed along the top of inside tube in the ranges of small ice packing factor and low ice water slurry velocity, while ice particles diffused into the whole of tube and flowed like a plug built up by ice particles for large ice packing factor and high velocity. Moreover, it was found that the flowing ice plug was separated into numbers of small ice clusters by melting phenomenon. Experiments of melting heat transfer were carried out under some parameters of ice packing factor, ice water slurry flow rate and hot water temperature. Consequently, the correlation equation of melting heat transfer was derived as a function of those experimental parameters.

  19. Wave effects on ocean-ice interaction in the marginal ice zone

    NASA Technical Reports Server (NTRS)

    Liu, Antony K.; Hakkinen, Sirpa; Peng, Chih Y.

    1993-01-01

    The effects of wave train on ice-ocean interaction in the marginal ice zone are studied through numerical modeling. A coupled two-dimensional ice-ocean model has been developed to include wave effects and wind stress for the predictions of ice edge dynamics. The sea ice model is coupled to the reduced-gravity ocean model through interfacial stresses. The main dynamic balance in the ice momentum is between water-ice stress, wind stress, and wave radiation stresses. By considering the exchange of momentum between waves and ice pack through radiation stress for decaying waves, a parametric study of the effects of wave stress and wind stress on ice edge dynamics has been performed. The numerical results show significant effects from wave action. The ice edge is sharper, and ice edge meanders form in the marginal ice zone owing to forcing by wave action and refraction of swell system after a couple of days. Upwelling at the ice edge and eddy formation can be enhanced by the nonlinear effects of wave action; wave action sharpens the ice edge and can produce ice meandering, which enhances local Ekman pumping and pycnocline anomalies. The resulting ice concentration, pycnocline changes, and flow velocity field are shown to be consistent with previous observations.

  20. Satellite remote sensing over ice

    NASA Technical Reports Server (NTRS)

    Thomas, R. H.

    1984-01-01

    Satellite remote sensing provides unique opportunities for observing ice-covered terrain. Passive-microwave data give information on snow extent on land, sea-ice extent and type, and zones of summer melting on the polar ice sheets, with the potential for estimating snow-accumulation rates on these ice sheets. All weather, high-resolution imagery of sea ice is obtained using synthetic aperture radars, and ice-movement vectors can be deduced by comparing sequential images of the same region. Radar-altimetry data provide highly detailed information on ice-sheet topography, with the potential for deducing thickening/thinning rates from repeat surveys. The coastline of Antarctica can be mapped accurately using altimetry data, and the size and spatial distribution of icebergs can be monitored. Altimetry data also distinguish open ocean from pack ice and they give an indication of sea-ice characteristics.

  1. Satellite remote sensing over ice

    NASA Technical Reports Server (NTRS)

    Thomas, R. H.

    1986-01-01

    Satellite remote sensing provides unique opportunities for observing ice-covered terrain. Passive-microwave data give information on snow extent on land, sea-ice extent and type, and zones of summer melting on the polar ice sheets, with the potential for estimating snow-accumulation rates on these ice sheets. All weather, high-resolution imagery of sea ice is obtained using synthetic aperture radars, and ice-movement vectors can be deduced by comparing sequential images of the same region. Radar-altimetry data provide highly detailed information on ice-sheet topography, with the potential for deducing thickening/thinning rates from repeat surveys. The coastline of Antarctica can be mapped accurately using altimetry data, and the size and spatial distribution of icebergs can be monitored. Altimetry data also distinguish open ocean from pack ice and they give an indication of sea-ice characteristics.

  2. The Pack Method for Compressive Tests of Thin Specimens of Materials Used in Thin-Wall Structures

    NASA Technical Reports Server (NTRS)

    Aitchison, C S; Tuckerman, L B

    1939-01-01

    The strength of modern lightweight thin-wall structures is generally limited by the strength of the compression members. An adequate design of these members requires a knowledge of the compressive stress-strain graph of the thin-wall material. The "pack" method was developed at the National Bureau of Standards with the support of the National Advisory Committee for Aeronautics to make possible a determination of compressive stress-strain graphs for such material. In the pack test an odd number of specimens are assembled into a relatively stable pack, like a "pack of cards." Additional lateral stability is obtained from lateral supports between the external sheet faces of the pack and outside reactions. The tests seems adequate for many problems in structural research.

  3. Long-Term Observations of Atmospheric CO2, O3 and BrO over the Transitioning Arctic Ocean Pack-ice: The O-Buoy Chemical Network

    NASA Astrophysics Data System (ADS)

    Matrai, P.

    2016-02-01

    Autonomous, sea ice-tethered O-Buoys have been deployed (2009-2016) across the Arctic sea ice for long-term atmospheric measurements (http://www.o-buoy.org). O-Buoys (15) provide in-situ concentrations of three sentinel atmospheric chemicals, ozone, CO2 and BrO, as well as meteorological parameters and imagery, over the frozen ocean. O-Buoys were designed to transmit daily data over a period of 2 years while deployed in sea ice, as part of automated ice-drifting stations that include snow/ice measurement systems (e.g. Ice Mass Balance buoys) and oceanographic measurements (e.g. Ice Tethered Profilers). Seasonal changes in Arctic atmospheric chemistry are influenced by changes in the characteristics and presence of the sea ice vs. open water as well as air mass trajectories, especially during the winter-spring and summer-fall transitions when sea ice is melting and freezing, respectively. The O-Buoy Chemical Network provides the unique opportunity to observe these transition periods in real-time with high temporal resolution, and to compare them with those collected on land-based monitoring stations located. Due to the logistical challenges of measurements over the Arctic Ocean region, most long term, in-situ observations of atmospheric chemistry have been made at coastal or island sites around the periphery of the Arctic Ocean, leaving large spatial and temporal gaps that O-Buoys overcome. Advances in floatation, communications, power management, and sensor hardware have been made to overcome the challenges of diminished Arctic sea ice. O-Buoy data provide insights into enhanced seasonal, interannual and spatial variability in atmospheric composition, atmospheric boundary layer control on the amount of halogen activation, enhancement of the atmospheric CO2 signal over the more variable and porous pack ice, and to develop an integrated picture of the coupled ocean/ice/atmosphere system. As part of the Arctic Observing Network, we provide data to the community (www.aoncadis.org).

  4. Estimation of Antarctic Land-Fast Sea Ice Algal Biomass and Snow Thickness From Under-Ice Radiance Spectra in Two Contrasting Areas

    NASA Astrophysics Data System (ADS)

    Wongpan, P.; Meiners, K. M.; Langhorne, P. J.; Heil, P.; Smith, I. J.; Leonard, G. H.; Massom, R. A.; Clementson, L. A.; Haskell, T. G.

    2018-03-01

    Fast ice is an important component of Antarctic coastal marine ecosystems, providing a prolific habitat for ice algal communities. This work examines the relationships between normalized difference indices (NDI) calculated from under-ice radiance measurements and sea ice algal biomass and snow thickness for Antarctic fast ice. While this technique has been calibrated to assess biomass in Arctic fast ice and pack ice, as well as Antarctic pack ice, relationships are currently lacking for Antarctic fast ice characterized by bottom ice algae communities with high algal biomass. We analyze measurements along transects at two contrasting Antarctic fast ice sites in terms of platelet ice presence: near and distant from an ice shelf, i.e., in McMurdo Sound and off Davis Station, respectively. Snow and ice thickness, and ice salinity and temperature measurements support our paired in situ optical and biological measurements. Analyses show that NDI wavelength pairs near the first chlorophyll a (chl a) absorption peak (≈440 nm) explain up to 70% of the total variability in algal biomass. Eighty-eight percent of snow thickness variability is explained using an NDI with a wavelength pair of 648 and 567 nm. Accounting for pigment packaging effects by including the ratio of chl a-specific absorption coefficients improved the NDI-based algal biomass estimation only slightly. Our new observation-based algorithms can be used to estimate Antarctic fast ice algal biomass and snow thickness noninvasively, for example, by using moored sensors (time series) or mapping their spatial distributions using underwater vehicles.

  5. Floating ice-algal aggregates below melting arctic sea ice.

    PubMed

    Assmy, Philipp; Ehn, Jens K; Fernández-Méndez, Mar; Hop, Haakon; Katlein, Christian; Sundfjord, Arild; Bluhm, Katrin; Daase, Malin; Engel, Anja; Fransson, Agneta; Granskog, Mats A; Hudson, Stephen R; Kristiansen, Svein; Nicolaus, Marcel; Peeken, Ilka; Renner, Angelika H H; Spreen, Gunnar; Tatarek, Agnieszka; Wiktor, Jozef

    2013-01-01

    During two consecutive cruises to the Eastern Central Arctic in late summer 2012, we observed floating algal aggregates in the melt-water layer below and between melting ice floes of first-year pack ice. The macroscopic (1-15 cm in diameter) aggregates had a mucous consistency and were dominated by typical ice-associated pennate diatoms embedded within the mucous matrix. Aggregates maintained buoyancy and accumulated just above a strong pycnocline that separated meltwater and seawater layers. We were able, for the first time, to obtain quantitative abundance and biomass estimates of these aggregates. Although their biomass and production on a square metre basis was small compared to ice-algal blooms, the floating ice-algal aggregates supported high levels of biological activity on the scale of the individual aggregate. In addition they constituted a food source for the ice-associated fauna as revealed by pigments indicative of zooplankton grazing, high abundance of naked ciliates, and ice amphipods associated with them. During the Arctic melt season, these floating aggregates likely play an important ecological role in an otherwise impoverished near-surface sea ice environment. Our findings provide important observations and measurements of a unique aggregate-based habitat during the 2012 record sea ice minimum year.

  6. Floating Ice-Algal Aggregates below Melting Arctic Sea Ice

    PubMed Central

    Assmy, Philipp; Ehn, Jens K.; Fernández-Méndez, Mar; Hop, Haakon; Katlein, Christian; Sundfjord, Arild; Bluhm, Katrin; Daase, Malin; Engel, Anja; Fransson, Agneta; Granskog, Mats A.; Hudson, Stephen R.; Kristiansen, Svein; Nicolaus, Marcel; Peeken, Ilka; Renner, Angelika H. H.; Spreen, Gunnar; Tatarek, Agnieszka; Wiktor, Jozef

    2013-01-01

    During two consecutive cruises to the Eastern Central Arctic in late summer 2012, we observed floating algal aggregates in the melt-water layer below and between melting ice floes of first-year pack ice. The macroscopic (1-15 cm in diameter) aggregates had a mucous consistency and were dominated by typical ice-associated pennate diatoms embedded within the mucous matrix. Aggregates maintained buoyancy and accumulated just above a strong pycnocline that separated meltwater and seawater layers. We were able, for the first time, to obtain quantitative abundance and biomass estimates of these aggregates. Although their biomass and production on a square metre basis was small compared to ice-algal blooms, the floating ice-algal aggregates supported high levels of biological activity on the scale of the individual aggregate. In addition they constituted a food source for the ice-associated fauna as revealed by pigments indicative of zooplankton grazing, high abundance of naked ciliates, and ice amphipods associated with them. During the Arctic melt season, these floating aggregates likely play an important ecological role in an otherwise impoverished near-surface sea ice environment. Our findings provide important observations and measurements of a unique aggregate-based habitat during the 2012 record sea ice minimum year. PMID:24204642

  7. Ice Accretion Test Results for Three Large-Scale Swept-Wing Models in the NASA Icing Research Tunnel

    NASA Technical Reports Server (NTRS)

    Broeren, Andy; Potapczuk, Mark; Lee, Sam; Malone, Adam; Paul, Ben; Woodard, Brian

    2016-01-01

    The design and certification of modern transport airplanes for flight in icing conditions increasing relies on three-dimensional numerical simulation tools for ice accretion prediction. There is currently no publically available, high-quality, ice accretion database upon which to evaluate the performance of icing simulation tools for large-scale swept wings that are representative of modern commercial transport airplanes. The purpose of this presentation is to present the results of a series of icing wind tunnel test campaigns whose aim was to provide an ice accretion database for large-scale, swept wings.

  8. Relationship between Physiological Off-Ice Testing, On-Ice Skating, and Game Performance in Division I Women's Ice Hockey Players.

    PubMed

    Boland, Michelle; Miele, Emily M; Delude, Katie

    2017-10-07

    The purpose was to identify off-ice testing variables that correlate to skating and game performance in Division I collegiate women ice hockey players. Twenty female, forward and defensive players (19.95 ± 1.35 yr) were assessed for weight, height, percent fat mass (%FAT), bone mineral density, predicted one repetition maximum (RM) absolute and relative (REL%) bench press (BP) and hex bar deadlift (HDL), lower body explosive power, anaerobic power, countermovement vertical jump (CMJ), maximum inspiratory pressure (MIP), and on-ice repeated skate sprint (RSS) performance. The on-ice RSS test included 6 timed 85.6 m sprints with participants wearing full hockey equipment; fastest time (FT), average time (AT) and fatigue index (FI) for the first length skate (FLS; 10 m) and total length skate (TLS; 85.6 m) were used for analysis. Game performance was evaluated with game statistics: goals, assists, points, plus-minus, and shots on goal (SOG). Correlation coefficients were used to determine relationships. Percent fat mass was positively correlated (p < 0.05) with FLS-FI and TLS-AT; TLS-FT was negatively correlated with REL%HDL; BP-RM was negatively correlated with FLS-FT and FLS-AT; MIP positively correlated with assists, points, and SOG; FLS-AT negatively correlated with assists. Game performance in women ice hockey players may be enhanced by greater MIP, repeat acceleration ability, and mode-specific training. Faster skating times were associated with lower %FAT. Skating performance in women ice hockey players may be enhanced by improving body composition, anaerobic power, and both lower and upper body strength in off-ice training.

  9. On the 2012 Record Low Arctic Sea Ice Cover: Combined Impact of Preconditioning and an August Storm

    NASA Technical Reports Server (NTRS)

    Parkinson, Claire L.; Comiso, Josefino C.

    2013-01-01

    A new record low Arctic sea ice extent for the satellite era, 3.4 x 10(exp 6) square kilometers, was reached on 13 September 2012; and a new record low sea ice area, 3.01 x 10(exp 6) square kilometers was reached on the same date. Preconditioning through decades of overall ice reductions made the ice pack more vulnerable to a strong storm that entered the central Arctic in early August 2012. The storm caused the separation of an expanse of 0.4 x 10(exp 6) square kilometers of ice that melted in total, while its removal left the main pack more exposed to wind and waves, facilitating the main pack's further decay. Future summer storms could lead to a further acceleration of the decline in the Arctic sea ice cover and should be carefully monitored.

  10. Numerical model of ice melange expansion during abrupt ice-shelf collapse

    NASA Astrophysics Data System (ADS)

    Guttenberg, N.; Abbot, D. S.; Amundson, J. M.; Burton, J. C.; Cathles, L. M.; Macayeal, D. R.; Zhang, W.

    2010-12-01

    Satellite imagery of the February 2008 Wilkins Ice-Shelf Collapse event reveals that a large percentage of the involved ice shelf was converted to capsized icebergs and broken fragments of icebergs over a relatively short period of time, possibly less than 24 hours. The extreme violence and short time scale of the event, and the considerable reduction of gravitational potential energy between upright and capsized icebergs, suggests that iceberg capsize might be an important driving mechanism controlling both the rate and spatial extent of ice shelf collapse. To investigate this suggestion, we have constructed an idealized, 2-dimensional model of a disintegrating ice shelf composed of a large number (N~100 to >1000) of initially well-packed icebergs of rectangular cross section. The model geometry consists of a longitudinal cross section of the idealized ice shelf from grounding line (or the upstream extent of ice-shelf fragmentation) to seaward ice front, and includes the region beyond the initial ice front to cover the open, ice-free water into which the collapsing ice shelf expands. The seawater in which the icebergs float is treated as a hydrostatic fluid in the computation of iceberg orientation (e.g., the evaluation of buoyancy forces and torques), thereby eliminating the complexities of free-surface waves, but net horizontal drift of the icebergs is resisted by a linear drag law designed to energy dissipation by viscous forces and surface-gravity-wave radiation. Icebergs interact via both elastic and inelastic contacts (typically a corner of one iceberg will scrape along the face of its neighbor). Ice-shelf collapse in the model is embodied by the mass capsize of a large proportion of the initially packed icebergs and the consequent advancement of the ice front (leading edge). Model simulations are conducted to examine (a) the threshold of stability (e.g., what density of initially capsizable icebergs is needed to allow a small perturbation to the system

  11. Sea Ice, Climate and Fram Strait

    NASA Technical Reports Server (NTRS)

    Hunkins, K.

    1984-01-01

    When sea ice is formed the albedo of the ocean surface increases from its open water value of about 0.1 to a value as high as 0.8. This albedo change effects the radiation balance and thus has the potential to alter climate. Sea ice also partially seals off the ocean from the atmosphere, reducing the exchange of gases such as carbon dioxide. This is another possible mechanism by which climate might be affected. The Marginal Ice Zone Experiment (MIZEX 83 to 84) is an international, multidisciplinary study of processes controlling the edge of the ice pack in that area including the interactions between sea, air and ice.

  12. Spaceborne SAR and sea ice

    NASA Technical Reports Server (NTRS)

    Weeks, W. F.

    1983-01-01

    A number of remote sensing systems deployed in satellites to view the Earth which are successful in gathering data on the behavior of the world's snow and ice covers are described. Considering sea ice which covers over 10% of the world ocean, systems that have proven capable to collect useful data include those operating in the visible, near-infrared, infrared, and microwave frequency ranges. The microwave systems have the essential advantage in observing the ice under all weather and lighting conditions. Without this capability data are lost during the long polar night and during times of storm passage, periods when ice activity can be intense. The margins of the ice pack, a region of particular interest, is shrouded in cloud between 80 and 90% of the time.

  13. Landward and eastward shift of Alaskan polar bear denning associated with recent sea ice changes

    USGS Publications Warehouse

    Fischbach, Anthony S.; Amstrup, Steven C.; Douglas, David C.

    2007-01-01

    Polar bears (Ursus maritimus) in the northern Alaska region den in coastal areas and on offshore drifting ice. We evaluated changes in the distribution of polar bear maternal dens between 1985 and 2005, using satellite telemetry. We determined the distribution of maternal dens occupied by 89 satellite collared female polar bears between 137°W and 167°W longitude. The proportion of dens on pack ice declined from 62% in 1985–1994 to 37% in 1998–2004 (P = 0.044) and among pack ice dens fewer occurred in the western Beaufort Sea after 1998. We evaluated whether hunting, attraction to bowhead whale remains, or changes in sea ice could explain changes in den distribution. We concluded that denning distribution changed in response to reductions in stable old ice, increases in unconsolidated ice, and lengthening of the melt season. In consort, these changes have likely reduced the availability and quality of pack ice denning habitat. Further declines in sea ice availability are predicted. Therefore, we expect the proportion of polar bears denning in coastal areas will continue to increase, until such time as the autumn ice retreats far enough from shore that it precludes offshore pregnant females from reaching the Alaska coast in advance of denning.

  14. Diagnostic value of repeated ice tests in the evaluation of ptosis in myasthenia gravis.

    PubMed

    Park, Jun Young; Yang, Hee Kyung; Hwang, Jeong-Min

    2017-01-01

    Twenty-six patients with ptosis related to Myasthenia gravis (MG) and 38 controls with ptosis other than MG were included. All patients were tested with the ice test 2 times on separate days in the afternoon. The margin reflex distance (MRD) was measured before and immediately after 2-minute application of ice on the eyelids. The ice test was judged positive if there was an improvement of at least 2.0 mm of MRD after the ice test. Among the patients with negative test results, 'equivocal' was defined by improvement of MRD from at least 1.0 mm to less than 2.0 mm after the ice test. Repeated ice test results showed an agreement of 61.5% in MG, and 97.4% in nonmyasthenic ptosis. Repeated ice tests increased the sensitivity by 34.6% compared to a single test. Among the patients with repeatedly negative test results, 63.6% of those who showed equivocal results at least once turned out to be MG. Of those with repeated non-equivocal negative results, nobody turned out to be MG. There was no significant difference of the ice test results between ocular MG and generalized MG (p = 0.562).

  15. Diagnostic value of repeated ice tests in the evaluation of ptosis in myasthenia gravis

    PubMed Central

    2017-01-01

    Twenty-six patients with ptosis related to Myasthenia gravis (MG) and 38 controls with ptosis other than MG were included. All patients were tested with the ice test 2 times on separate days in the afternoon. The margin reflex distance (MRD) was measured before and immediately after 2-minute application of ice on the eyelids. The ice test was judged positive if there was an improvement of at least 2.0 mm of MRD after the ice test. Among the patients with negative test results, 'equivocal’ was defined by improvement of MRD from at least 1.0 mm to less than 2.0 mm after the ice test. Repeated ice test results showed an agreement of 61.5% in MG, and 97.4% in nonmyasthenic ptosis. Repeated ice tests increased the sensitivity by 34.6% compared to a single test. Among the patients with repeatedly negative test results, 63.6% of those who showed equivocal results at least once turned out to be MG. Of those with repeated non-equivocal negative results, nobody turned out to be MG. There was no significant difference of the ice test results between ocular MG and generalized MG (p = 0.562). PMID:28562609

  16. Future Interannual Variability of Arctic Sea Ice Area and its Implications for Marine Navigation

    NASA Astrophysics Data System (ADS)

    Vavrus, S. J.; Mioduszewski, J.; Holland, M. M.; Wang, M.; Landrum, L.

    2016-12-01

    As both a symbol and driver of ongoing climate change, the diminishing Arctic sea ice pack has been widely studied in a variety of contexts. Most research, however, has focused on time-mean changes in sea ice, rather than on short-term variations that also have important physical and societal consequences. In this study we test the hypothesis that interannual Arctic sea ice variability will increase in the future by utilizing a set of 40 independent simulations from the Community Earth System Model's Large Ensemble for the 1920-2100 period. The model projects that ice variability will indeed grow substantially in all months but with a strong seasonal dependence in magnitude and timing. The variability increases most during late autumn (November-December) and least during spring. This increase proceeds in a time-transgressive manner over the course of the year, peaking soonest (2020s) in late-summer months and latest (2090s) during late spring. The variability in every month is inversely correlated with the average melt rate, resulting in an eventual decline in both terms as the ice pack becomes seasonal by late century. These projected changes in sea ice variations will likely have significant consequences for marine navigation, which we assess with the empirical Ice Numeral (IN) metric. A function of ice concentration and thickness, the IN quantifies the difficulty in traversing a transect of sea ice-covered ocean as a function of vessel strength. Our results show that although increasingly open Arctic seas will mean generally more favorable conditions for navigation, the concurrent rise in the variability of ice cover poses a competing risk. In particular, future intervals featuring the most rapid declines in ice area that coincide with the highest interannual ice variations will offer more inviting shipping opportunities tempered by less predictable navigational conditions.

  17. Variability in Arctic sea ice topography and atmospheric form drag: Combining IceBridge laser altimetry with ASCAT radar backscatter.

    NASA Astrophysics Data System (ADS)

    Petty, A.; Tsamados, M.; Kurtz, N. T.

    2016-12-01

    Here we present atmospheric form drag estimates over Arctic sea ice using high resolution, three-dimensional surface elevation data from NASA's Operation IceBridge Airborne Topographic Mapper (ATM), and surface roughness estimates from the Advanced Scatterometer (ASCAT). Surface features of the ice pack (e.g. pressure ridges) are detected using IceBridge ATM elevation data and a novel surface feature-picking algorithm. We use simple form drag parameterizations to convert the observed height and spacing of surface features into an effective atmospheric form drag coefficient. The results demonstrate strong regional variability in the atmospheric form drag coefficient, linked to variability in both the height and spacing of surface features. This includes form drag estimates around 2-3 times higher over the multiyear ice north of Greenland, compared to the first-year ice of the Beaufort/Chukchi seas. We compare results from both scanning and linear profiling to ensure our results are consistent with previous studies investigating form drag over Arctic sea ice. A strong correlation between ASCAT surface roughness estimates (using radar backscatter) and the IceBridge form drag results enable us to extrapolate the IceBridge data collected over the western-Arctic across the entire Arctic Ocean. While our focus is on spring, due to the timing of the primary IceBridge campaigns since 2009, we also take advantage of the autumn data collected by IceBridge in 2015 to investigate seasonality in Arctic ice topography and the resulting form drag coefficient. Our results offer the first large-scale assessment of atmospheric form drag over Arctic sea ice due to variable ice topography (i.e. within the Arctic pack ice). The analysis is being extended to the Antarctic IceBridge sea ice data, and the results are being used to calibrate a sophisticated form drag parameterization scheme included in the sea ice model CICE, to improve the representation of form drag over Arctic and

  18. Upper Ocean Evolution Across the Beaufort Sea Marginal Ice Zone

    NASA Astrophysics Data System (ADS)

    Lee, C.; Rainville, L.; Gobat, J. I.; Perry, M. J.; Freitag, L. E.; Webster, S.

    2016-12-01

    The observed reduction of Arctic summertime sea ice extent and expansion of the marginal ice zone (MIZ) have profound impacts on the balance of processes controlling sea ice evolution, including the introduction of several positive feedback mechanisms that may act to accelerate melting. Examples of such feedbacks include increased upper ocean warming though absorption of solar radiation, elevated internal wave energy and mixing that may entrain heat stored in subsurface watermasses (e.g., the relatively warm Pacific Summer and Atlantic waters), and elevated surface wave energy that acts to deform and fracture sea ice. Spatial and temporal variability in ice properties and open water fraction impact these processes. To investigate how upper ocean structure varies with changing ice cover, how the balance of processes shift as a function of ice fraction and distance from open water, and how these processes impact sea ice evolution, a network of autonomous platforms sampled the atmosphere-ice-ocean system in the Beaufort, beginning in spring, well before the start of melt, and ending with the autumn freeze-up. Four long-endurance autonomous Seagliders occupied sections that extended from open water, through the marginal ice zone, deep into the pack during summer 2014 in the Beaufort Sea. Gliders penetrated up to 200 km into the ice pack, under complete ice cover for up to 10 consecutive days. Sections reveal strong fronts where cold, ice-covered waters meet waters that have been exposed to solar warming, and O(10 km) scale eddies near the ice edge. In the pack, Pacific Summer Water and a deep chlorophyll maximum form distinct layers at roughly 60 m and 80 m, respectively, which become increasingly diffuse late in the season as they progress through the MIZ and into open water. Stratification just above the Pacific Summer Water rapidly weakens near the ice edge and temperature variance increases, likely due to mixing or energetic vertical exchange associated with strong

  19. Under the sea ice: Exploring the relationship between sea ice and the foraging behaviour of southern elephant seals in East Antarctica

    NASA Astrophysics Data System (ADS)

    Labrousse, Sara; Sallée, Jean-Baptiste; Fraser, Alexander D.; Massom, Robert A.; Reid, Phillip; Sumner, Michael; Guinet, Christophe; Harcourt, Robert; McMahon, Clive; Bailleul, Frédéric; Hindell, Mark A.; Charrassin, Jean-Benoit

    2017-08-01

    Investigating ecological relationships between predators and their environment is essential to understand the response of marine ecosystems to climate variability and change. This is particularly true in polar regions, where sea ice (a sensitive climate variable) plays a crucial yet highly dynamic and variable role in how it influences the whole marine ecosystem, from phytoplankton to top predators. For mesopredators such as seals, sea ice both supports a rich (under-ice) food resource, access to which depends on local to regional coverage and conditions. Here, we investigate sex-specific relationships between the foraging strategies of southern elephant seals (Mirounga leonina) in winter and spatio-temporal variability in sea ice concentration (SIC) and coverage in East Antarctica. We satellite-tracked 46 individuals undertaking post-moult trips in winter from Kerguelen Islands to the peri-Antarctic shelf between 2004 and 2014. These data indicate distinct general patterns of sea ice usage: while females tended to follow the sea ice edge as it extended northward, the males remained on the continental shelf despite increasing sea ice. Seal hunting time, a proxy of foraging activity inferred from the diving behaviour, was longer for females in late autumn in the outer part of the pack ice, ∼150-370 km south of the ice edge. Within persistent regions of compact sea ice, females had a longer foraging activity (i) in the highest sea ice concentration at their position, but (ii) their foraging activity was longer when there were more patches of low concentration sea ice around their position (either in time or in space; 30 days & 50 km). The high spatio-temporal variability of sea ice around female positions is probably a key factor allowing them to exploit these concentrated patches. Despite lack of information on prey availability, females may exploit mesopelagic finfishes and squids that concentrate near the ice-water interface or within the water column (from

  20. An integrated approach to the remote sensing of floating ice

    NASA Technical Reports Server (NTRS)

    Campbell, W. J.; Ramseier, R. O.; Weeks, W. F.; Gloersen, P.

    1976-01-01

    Review article on remote sensing applications to glaciology. Ice parameters sensed include: ice cover vs open water, ice thickness, distribution and morphology of ice formations, vertical resolution of ice thickness, ice salinity (percolation and drainage of brine; flushing of ice body with fresh water), first-year ice and multiyear ice, ice growth rate and surface heat flux, divergence of ice packs, snow cover masking ice, behavior of ice shelves, icebergs, lake ice and river ice; time changes. Sensing techniques discussed include: satellite photographic surveys, thermal IR, passive and active microwave studies, microwave radiometry, microwave scatterometry, side-looking radar, and synthetic aperture radar. Remote sensing of large aquatic mammals and operational ice forecasting are also discussed.

  1. Evaluation of Methods to Select Scale Velocities in Icing Scaling Tests

    NASA Technical Reports Server (NTRS)

    Anderson, David N.; Ruff, Gary A.; Bond, Thomas H. (Technical Monitor)

    2003-01-01

    A series of tests were made in the NASA Glenn Icing Research Tunnel to determine how icing scaling results were affected by the choice of scale velocity. Reference tests were performed with a 53.3-cm-chord NACA 0012 airfoil model, while scale tests used a 27.7-cm-chord 0012 model. Tests were made with rime, mixed, and glaze ice. Reference test conditions included airspeeds of 67 and 89 m/s, an MVD of 40 microns, and LWCs of 0.5 and 0.6 g/cu m. Scale test conditions were established by the modified Ruff (AEDC) scaling method with the scale velocity determined in five ways. The resulting scale velocities ranged from 85 to 220 percent of the reference velocity. This paper presents the ice shapes that resulted from those scale tests and compares them to the reference shapes. It was concluded that for freezing fractions greater than 0.8 as well as for a freezing fraction of 0.3, the value of the scale velocity had no effect on how well the scale ice shape simulated the reference shape. For freezing fractions of 0.5 and 0.7, the simulation of the reference shape appeared to improve as the scale velocity increased.

  2. Geophysics of an Oceanic Ice Shell on Snowball Earth

    NASA Technical Reports Server (NTRS)

    Gaidos, E. J.

    2000-01-01

    Kirschvink proposed Precambrian low-latitude glaciation could result in an albedo-driven catastrophic runaway to a "Snowball Earth" state in which pack ice up to 1 km thick covered the world ocean. The geophysical state of an ice crust on a Snowball Earth is examined.

  3. Statistical Analyses of High-Resolution Aircraft and Satellite Observations of Sea Ice: Applications for Improving Model Simulations

    NASA Astrophysics Data System (ADS)

    Farrell, S. L.; Kurtz, N. T.; Richter-Menge, J.; Harbeck, J. P.; Onana, V.

    2012-12-01

    Satellite-derived estimates of ice thickness and observations of ice extent over the last decade point to a downward trend in the basin-scale ice volume of the Arctic Ocean. This loss has broad-ranging impacts on the regional climate and ecosystems, as well as implications for regional infrastructure, marine navigation, national security, and resource exploration. New observational datasets at small spatial and temporal scales are now required to improve our understanding of physical processes occurring within the ice pack and advance parameterizations in the next generation of numerical sea-ice models. High-resolution airborne and satellite observations of the sea ice are now available at meter-scale resolution or better that provide new details on the properties and morphology of the ice pack across basin scales. For example the NASA IceBridge airborne campaign routinely surveys the sea ice of the Arctic and Southern Oceans with an advanced sensor suite including laser and radar altimeters and digital cameras that together provide high-resolution measurements of sea ice freeboard, thickness, snow depth and lead distribution. Here we present statistical analyses of the ice pack primarily derived from the following IceBridge instruments: the Digital Mapping System (DMS), a nadir-looking, high-resolution digital camera; the Airborne Topographic Mapper, a scanning lidar; and the University of Kansas snow radar, a novel instrument designed to estimate snow depth on sea ice. Together these instruments provide data from which a wide range of sea ice properties may be derived. We provide statistics on lead distribution and spacing, lead width and area, floe size and distance between floes, as well as ridge height, frequency and distribution. The goals of this study are to (i) identify unique statistics that can be used to describe the characteristics of specific ice regions, for example first-year/multi-year ice, diffuse ice edge/consolidated ice pack, and convergent

  4. A Comparison of Sea Ice Type, Sea Ice Temperature, and Snow Thickness Distributions in the Arctic Seasonal Ice Zones with the DMSP SSM/I

    NASA Technical Reports Server (NTRS)

    St.Germain, Karen; Cavalieri, Donald J.; Markus, Thorsten

    1997-01-01

    Global climate studies have shown that sea ice is a critical component in the global climate system through its effect on the ocean and atmosphere, and on the earth's radiation balance. Polar energy studies have further shown that the distribution of thin ice and open water largely controls the distribution of surface heat exchange between the ocean and atmosphere within the winter Arctic ice pack. The thickness of the ice, the depth of snow on the ice, and the temperature profile of the snow/ice composite are all important parameters in calculating surface heat fluxes. In recent years, researchers have used various combinations of DMSP SSMI channels to independently estimate the thin ice type (which is related to ice thickness), the thin ice temperature, and the depth of snow on the ice. In each case validation efforts provided encouraging results, but taken individually each algorithm gives only one piece of the information necessary to compute the energy fluxes through the ice and snow. In this paper we present a comparison of the results from each of these algorithms to provide a more comprehensive picture of the seasonal ice zone using passive microwave observations.

  5. Modeling Wave-Ice Interactions in the Marginal Ice Zone

    NASA Astrophysics Data System (ADS)

    Orzech, Mark; Shi, Fengyan; Bateman, Sam; Veeramony, Jay; Calantoni, Joe

    2015-04-01

    The small-scale (O(m)) interactions between waves and ice floes in the marginal ice zone (MIZ) are investigated with a coupled model system. Waves are simulated with the non-hydrostatic finite-volume model NHWAVE (Ma et al., 2012) and ice floes are represented as bonded collections of smaller particles with the discrete element system LIGGGHTS (Kloss et al., 2012). The physics of fluid and ice are recreated as authentically as possible, to allow the coupled system to supplement and/or substitute for more costly and demanding field experiments. The presentation will first describe the development and validation of the coupled system, then discuss the results of a series of virtual experiments in which ice floe and wave characteristics are varied to examine their effects on energy dissipation, MIZ floe size distribution, and ice pack retreat rates. Although Wadhams et al. (1986) suggest that only a small portion (roughly 10%) of wave energy entering the MIZ is reflected, dissipation mechanisms for the remaining energy have yet to be delineated or measured. The virtual experiments are designed to focus on specific properties and processes - such as floe size and shape, collision and fracturing events, and variations in wave climate - and measure their relative roles the transfer of energy and momentum from waves to ice. Questions to be examined include: How is energy dissipated by ice floe collisions, fracturing, and drag, and how significant is the wave attenuation associated with each process? Do specific wave/floe length scale ratios cause greater wave attenuation? How does ice material strength affect the rate of wave energy loss? The coupled system will ultimately be used to test and improve upon wave-ice parameterizations for large-scale climate models. References: >Kloss, C., C. Goniva, A. Hager, S. Amberger, and S. Pirker (2012). Models, algorithms and validation for opensource DEM and CFD-DEM. Progress in Computational Fluid Dynamics 12(2/3), 140-152. >Ma, G

  6. Body and blubber relationships in antarctic pack ice seals: implications for blubber depth patterns.

    PubMed

    Castellini, M A; Trumble, S J; Mau, T L; Yochem, P K; Stewart, B S; Koski, M A

    2009-01-01

    Morphometrics and blubber depths from all four high Antarctic seals (Weddell, Ross, crabeater, and leopard) were obtained during a midsummer research cruise in the Ross Sea as the physiological ecology component of the U.S. Antarctic Pack Ice Seals project. These data are the only in vivo measurements of all four species from the same location and time of year and focused on variances in morphometrics and blubber depth related to species, sex, and age. By controlling for location and season, this cross-species design provided the means to differentiate how blubber mass might be influenced in these groups. We measured both absolute blubber depth and ratio of blubber depth to body core diameter. We found that adult and younger animals showed differences in blubber depth, but male versus female seals did not show differences within any given species. However, when compared across species, the ratio of blubber ring depth to body core diameter suggests that adult Weddell seals differ in their use of blubber compared with the other three species. We propose that this difference in blubber pattern is most likely related to Weddell nutritional requirements during the breeding season having a greater influence on blubber depth than thermal requirements when compared with the other three species.

  7. Influence of work clothing on physiological responses and performance during treadmill exercise and the Wildland Firefighter Pack Test.

    PubMed

    Phillips, Devin B; Ehnes, Cameron M; Welch, Bradley G; Lee, Lauren N; Simin, Irina; Petersen, Stewart R

    2018-04-01

    This study investigated physiological responses and performance during three separate exercise challenges (Parts I, II, and III) with wildland firefighting work clothing ensemble (boots and coveralls) and a 20.4 kg backpack in four conditions: U-EX (no pack, exercise clothing); L-EX (pack, exercise clothing); U-W (no pack, work clothing); and, L-W (pack and work clothing). Part I consisted of randomly-ordered graded exercise tests, on separate days, in U-EX, L-EX and L-W conditions. Part II consisted of randomly-ordered bouts of sub-maximal treadmill exercise in the four conditions. In Part III, subjects completed, in random-order on separate days, 4.83 km Pack Tests in L-EX or L-W conditions. In Part I, peak oxygen uptake was reduced (p < .05) in L-W. In Part II, mass-specific oxygen uptake was significantly higher in both work clothing conditions. In Part III, Pack Test time was slower (p < .05) in L-W. These results demonstrate the negative impact of work clothing and load carriage on physiological responses to exercise and performance. Copyright © 2017 Elsevier Ltd. All rights reserved.

  8. ICE stereocamera system - photogrammetric setup for retrieval and analysis of small scale sea ice topography

    NASA Astrophysics Data System (ADS)

    Divine, Dmitry; Pedersen, Christina; Karlsen, Tor Ivan; Aas, Harald; Granskog, Mats; Renner, Angelika; Spreen, Gunnar; Gerland, Sebastian

    2013-04-01

    A new thin-ice Arctic paradigm requires reconsideration of the set of parameterizations of mass and energy exchange within the ocean-sea-ice-atmosphere system used in modern CGCMs. Such a reassessment would require a comprehensive collection of measurements made specifically on first-year pack ice with a focus on summer melt season when the difference from typical conditions for the earlier multi-year Arctic sea ice cover becomes most pronounced. Previous in situ studies have demonstrated a crucial importance of smaller (i.e. less than 10 m) scale surface topography features for the seasonal evolution of pack ice. During 2011-2012 NPI developed a helicopter borne ICE stereocamera system intended for mapping the sea ice surface topography and aerial photography. The hardware component of the system comprises two Canon 5D Mark II cameras, combined GPS/INS unit by "Novatel" and a laser altimeter mounted in a single enclosure outside the helicopter. The unit is controlled by a PXI chassis mounted inside the helicopter cabin. The ICE stereocamera system was deployed for the first time during the 2012 summer field season. The hardware setup has proven to be highly reliable and was used in about 30 helicopter flights over Arctic sea-ice during July-September. Being highly automated it required a minimal human supervision during in-flight operation. The deployment of the camera system was mostly done in combination with the EM-bird, which measures sea-ice thickness, and this combination provides an integrated view of sea ice cover along the flight track. During the flight the cameras shot sequentially with a time interval of 1 second each to ensure sufficient overlap between subsequent images. Some 35000 images of sea ice/water surface captured per camera sums into 6 Tb of data collected during its first field season. The reconstruction of the digital elevation model of sea ice surface will be done using SOCET SET commercial software. Refraction at water/air interface can

  9. Remote sensing of the Fram Strait marginal ice zone

    USGS Publications Warehouse

    Shuchman, R.A.; Burns, B.A.; Johannessen, O.M.; Josberger, E.G.; Campbell, W.J.; Manley, T.O.; Lannelongue, N.

    1987-01-01

    Sequential remote sensing images of the Fram Strait marginal ice zone played a key role in elucidating the complex interactions of the atmosphere, ocean, and sea ice. Analysis of a subset of these images covering a 1-week period provided quantitative data on the mesoscale ice morphology, including ice edge positions, ice concentrations, floe size distribution, and ice kinematics. The analysis showed that, under light to moderate wind conditions, the morphology of the marginal ice zone reflects the underlying ocean circulation. High-resolution radar observations showed the location and size of ocean eddies near the ice edge. Ice kinematics from sequential radar images revealed an ocean eddy beneath the interior pack ice that was verified by in situ oceanographic measurements.

  10. Antarctic Sea ice--a habitat for extremophiles.

    PubMed

    Thomas, D N; Dieckmann, G S

    2002-01-25

    The pack ice of Earth's polar oceans appears to be frozen white desert, devoid of life. However, beneath the snow lies a unique habitat for a group of bacteria and microscopic plants and animals that are encased in an ice matrix at low temperatures and light levels, with the only liquid being pockets of concentrated brines. Survival in these conditions requires a complex suite of physiological and metabolic adaptations, but sea-ice organisms thrive in the ice, and their prolific growth ensures they play a fundamental role in polar ecosystems. Apart from their ecological importance, the bacterial and algae species found in sea ice have become the focus for novel biotechnology, as well as being considered proxies for possible life forms on ice-covered extraterrestrial bodies.

  11. Microbiological quality of cuttlefish (Sepia pharaonis) fillets stored in dry and wet ice.

    PubMed

    Jeyasekaran, G; Jeya Shakila, R; Sukumar, D

    2012-10-01

    Microbiological quality of cuttlefish (Sepia pharaonis) fillets stored in three different ice conditions was studied. Fillets stored in wet ice at a ratio of 1:1 (package III) were sensorially acceptable for only 18 h, while that stored in dry ice at 1:1 (package I) and combination of dry ice and wet ice at 1:0.2:0.5 (package II) were in acceptable condition up to 24 h without re-icing and thus there was an extension of shelf life by about 33%. Total bacterial load was 7 log₁₀ cfu/g at the end of the storage period. Total psychrophilic population increased from zero to 7 log₁₀ cfu/g while total lactic acid bacteria from zero to 5 log₁₀ cfu/g. H₂S producers were detected only at 18 h, with a count of 1 log₁₀ cfu/g. Sulphite-reducing Clostridia increased gradually from zero to 110 most probable number count/g. Fresh cuttlefish fillets carried a bacterial flora of Micrococcus, Planococcus, Streptococcus, Moraxella, Proteus and Aeromonas. Pseudomonas was dominant in wet ice pack, while Aeromonas was dominant in both the dry ice and combination pack. Immediately after packing, the temperatures recorded in packages I, II and III were 10.5, 1.2 and 3.0 °C, respectively, which drastically decreased in 1 h and then maintained and finally increased gradually. The results indicate that use of combination of dry ice and wet ice is economical and very much useful to seafood industries, as this package considerably reduced the cost of air freight, as well as improved the quality and shelf life of cuttlefish.

  12. NASA Engine Icing Research Overview: Aeronautics Evaluation and Test Capabilities (AETC) Project

    NASA Technical Reports Server (NTRS)

    Veres, Joseph P.

    2015-01-01

    The occurrence of ice accretion within commercial high bypass aircraft turbine engines has been reported by airlines under certain atmospheric conditions. Engine anomalies have taken place at high altitudes that have been attributed to ice crystal ingestion by the engine. The ice crystals can result in degraded engine performance, loss of thrust control, compressor surge or stall, and flameout of the combustor. The Aviation Safety Program at NASA has taken on the technical challenge of a turbofan engine icing caused by ice crystals which can exist in high altitude convective clouds. The NASA engine icing project consists of an integrated approach with four concurrent and ongoing research elements, each of which feeds critical information to the next element. The project objective is to gain understanding of high altitude ice crystals by developing knowledge bases and test facilities for testing full engines and engine components. The first element is to utilize a highly instrumented aircraft to characterize the high altitude convective cloud environment. The second element is the enhancement of the Propulsion Systems Laboratory altitude test facility for gas turbine engines to include the addition of an ice crystal cloud. The third element is basic research of the fundamental physics associated with ice crystal ice accretion. The fourth and final element is the development of computational tools with the goal of simulating the effects of ice crystal ingestion on compressor and gas turbine engine performance. The NASA goal is to provide knowledge to the engine and aircraft manufacturing communities to help mitigate, or eliminate turbofan engine interruptions, engine damage, and failures due to ice crystal ingestion.

  13. The minimal ice water caloric test compared with established vestibular caloric test procedures.

    PubMed

    Schmäl, Frank; Lübben, Björn; Weiberg, Kerstin; Stoll, Wolfgang

    2005-01-01

    Caloric testing of the vestibular labyrinth is usually performed by classical caloric test procedures (CCTP) using water warmed to 30 degrees C and 44 degrees C. Ice water irrigation (4 degrees C) is usually not performed, although it might be useful as a bedside test. To verify the validity of the Minimal Ice Water Caloric Test (MIWCT), comparative video-oculographic investigations were performed in 22 healthy subjects using ice water (0.5 ml, 1.0 ml, 2 ml), CCTP, and cold air (27 degrees C). Frequency, amplitude, slow phase velocity (SPV), the onset, and the duration of nystagmus were documented. After addition of three ice cubes, the temperature of conventional tap water (16 degrees C) fell within 13 min to 4 degrees C. In pessimum position the subjects demonstrated no nystagmus response. Compared to CCTP, MIWCT was associated with a significantly later onset of nystagmus and a significant prolongation of the nystagmus reaction. In contrast to air stimulation (27 degrees C), a significant Spearman's correlation was noted between MIWCT (1 and 2 ml) and established CCTP in respect of essential nystagmus parameters (frequency, amplitude and SPV). Furthermore, MIWCT (0.5 and 1 ml) showed a higher sensitivity and specificity with regard to the detection of canal paresis based on Jongkees' formula compared to stimulation with air 27 degrees C. Thus, MIWCT appears to be a suitable procedure for bedside investigation of vestibular function outside the vestibular laboratory, e.g. in a hospital ward, where bedridden patients with vertigo occasionally require vestibular testing.

  14. 1. DETAIL OF TUBE ICE MACHINE OUTLET AT SOUTHWEST CORNER ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    1. DETAIL OF TUBE ICE MACHINE OUTLET AT SOUTHWEST CORNER OF BUILDING 162; ICE MANUFACTURED INSIDE THE BUILDING WAS AUGURED THROUGH THE WALL AND DROPPED INTO COMPARTMENTS IN REFIGERATED RAIL CARS - Rath Packing Company, Cooler Building, Sycamore Street between Elm & Eighteenth Streets, Waterloo, Black Hawk County, IA

  15. Sea Ice Topography Profiling using Laser Altimetry from Small Unmanned Aircraft Systems

    NASA Astrophysics Data System (ADS)

    Crocker, Roger Ian

    Arctic sea ice is undergoing a dramatic transition from a perennial ice pack with a high prevalence of old multiyear ice, to a predominantly seasonal ice pack comprised primarily of young first-year and second-year ice. This transition has brought about changes in the sea ice thickness and topography characteristics, which will further affect the evolution and survivability of the ice pack. The varying ice conditions have substantial implications for commercial operations, international affairs, regional and global climate, our ability to model climate dynamics, and the livelihood of Arctic inhabitants. A number of satellite and airborne missions are dedicated to monitoring sea ice, but they are limited by their spatial and temporal resolution and coverage. Given the fast rate of sea ice change and its pervasive implications, enhanced observational capabilities are needed to augment the current strategies. The CU Laser Profilometer and Imaging System (CULPIS) is designed specifically for collecting fine-resolution elevation data and imagery from small unmanned aircraft systems (UAS), and has a great potential to compliment ongoing missions. This altimeter system has been integrated into four different UAS, and has been deployed during Arctic and Antarctic science campaigns. The CULPIS elevation measurement accuracy is shown to be 95±25 cm, and is limited primarily by GPS positioning error (<25 cm), aircraft attitude determination error (<20 cm), and sensor misalignment error (<20 cm). The relative error is considerably smaller over short flight distances, and the measurement precision is shown to be <10 cm over a distance of 200 m. Given its fine precision, the CULPIS is well suited for measuring sea ice topography, and observed ridge height and ridge separation distributions are found to agree with theoretical distributions to within 5%. Simulations demonstrate the inability of course-resolution measurements to accurately represent the theoretical distributions

  16. Generation of Fullspan Leading-Edge 3D Ice Shapes for Swept-Wing Aerodynamic Testing

    NASA Technical Reports Server (NTRS)

    Camello, Stephanie C.; Lee, Sam; Lum, Christopher; Bragg, Michael B.

    2016-01-01

    The deleterious effect of ice accretion on aircraft is often assessed through dry-air flight and wind tunnel testing with artificial ice shapes. This paper describes a method to create fullspan swept-wing artificial ice shapes from partial span ice segments acquired in the NASA Glenn Icing Reserch Tunnel for aerodynamic wind-tunnel testing. Full-scale ice accretion segments were laser scanned from the Inboard, Midspan, and Outboard wing station models of the 65% scale Common Research Model (CRM65) aircraft configuration. These were interpolated and extrapolated using a weighted averaging method to generate fullspan ice shapes from the root to the tip of the CRM65 wing. The results showed that this interpolation method was able to preserve many of the highly three dimensional features typically found on swept-wing ice accretions. The interpolated fullspan ice shapes were then scaled to fit the leading edge of a 8.9% scale version of the CRM65 wing for aerodynamic wind-tunnel testing. Reduced fidelity versions of the fullspan ice shapes were also created where most of the local three-dimensional features were removed. The fullspan artificial ice shapes and the reduced fidelity versions were manufactured using stereolithography.

  17. Potential use of battery packs from NCAP tested vehicles.

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Lamb, Joshua; Orendorff, Christopher J.

    2013-10-01

    Several large electric vehicle batteries available to the National Highway Traffic Safety Administration are candidates for use in future safety testing programs. The batteries, from vehicles subjected to NCAP crashworthiness testing, are considered potentially damaged due to the nature of testing their associated vehicles have been subjected to. Criteria for safe shipping to Sandia is discussed, as well as condition the batteries must be in to perform testing work. Also discussed are potential tests that could be performed under a variety of conditions. The ultimate value of potential testing performed on these cells will rest on the level of accessmore » available to the battery pack, i.e. external access only, access to the on board monitoring system/CAN port or internal electrical access to the battery. Greater access to the battery than external visual and temperature monitoring would likely require input from the battery manufacturer.« less

  18. Delicious ice cream, why does salt thaw ice?

    NASA Astrophysics Data System (ADS)

    Bagnoli, Franco

    2016-03-01

    Plain Awful is an imaginary valley on the Andes populated by a highly-imitative, cubical people for which the most criminal offence is to exhibit round objects. The duck family (Scrooge, Donald and nephews) are teaming against Scrooge's worst enemy, Flintheart Glomgold, trying to buy the famous Plain Awful square eggs. Inadvertently, Scrooge violates the taboo, showing his Number One Dime, and is imprisoned in the stone quarries. He can be released only after the presentation of an ice cream soda to the President of Plain Awful. Donald and his nephews fly with Flintheart to deliver it, but Scrooge's enemy, of course, betrays the previous agreement after getting the ice cream, forcing the ducks into making an emergence replacement on the spot. Using dried milk, sugar and chocolate from their ration packs, plus some snow and salt for cooling they are able make the ice cream, and after dressing it with the carbonated water from a fire extinguisher they finally manage to produce the desired dessert. This comic may serve as an introduction to the "mysterious" phenomenon that added salt melts the ice and, even more surprising, does it by lowering the temperature of the mixture.

  19. Bearing Capacity Tests on Ice Reinforced With Geogrid

    DTIC Science & Technology

    1992-12-01

    reinforce an ice bridge on rivers, lakes and oceans every winter in cold re- the Imjin River in Korea; Carnes (1964) reports that gions around the...increased the flexural aircraft in World War U. Although this "Pykrete," strength up to 31%. Creep tests on ice beams with as it was called, never was used...The Second World War , Clos- CONCLUSIONS ing the Ring, vol. 5. Boston: Houghton Mifflin, pp. 75-76. Thebearingcapacity testsconductedinCRREL’s

  20. Spatial scales of light transmission through Antarctic pack ice: Surface flooding vs. floe-size distribution

    NASA Astrophysics Data System (ADS)

    Arndt, S.; Meiners, K.; Krumpen, T.; Ricker, R.; Nicolaus, M.

    2016-12-01

    Snow on sea ice plays a crucial role for interactions between the ocean and atmosphere within the climate system of polar regions. Antarctic sea ice is covered with snow during most of the year. The snow contributes substantially to the sea-ice mass budget as the heavy snow loads can depress the ice below water level causing flooding. Refreezing of the snow and seawater mixture results in snow-ice formation on the ice surface. The snow cover determines also the amount of light being reflected, absorbed, and transmitted into the upper ocean, determining the surface energy budget of ice-covered oceans. The amount of light penetrating through sea ice into the upper ocean is of critical importance for the timing and amount of bottom sea-ice melt, biogeochemical processes and under-ice ecosystems. Here, we present results of several recent observations in the Weddell Sea measuring solar radiation under Antarctic sea ice with instrumented Remotely Operated Vehicles (ROV). The combination of under-ice optical measurements with simultaneous characterization of surface properties, such as sea-ice thickness and snow depth, allows the identification of key processes controlling the spatial distribution of the under-ice light. Thus, our results show how the distinction between flooded and non-flooded sea-ice regimes dominates the spatial scales of under-ice light variability for areas smaller than 100-by-100m. In contrast, the variability on larger scales seems to be controlled by the floe-size distribution and the associated lateral incidence of light. These results are related to recent studies on the spatial variability of Arctic under-ice light fields focusing on the distinctly differing dominant surface properties between the northern (e.g. summer melt ponds) and southern (e.g. year-round snow cover, surface flooding) hemisphere sea-ice cover.

  1. Top predators in relation to bathymetry, ice and krill during austral winter in Marguerite Bay, Antarctica

    USGS Publications Warehouse

    Ribic, C.A.; Chapman, E.; Fraser, William R.; Lawson, G.L.; Wiebe, P.H.

    2008-01-01

    A key hypothesis guiding the US Southern Ocean Global Ocean Ecosystems Dynamics (US SO GLOBEC) program is that deep across-shelf troughs facilitate the transport of warm and nutrient-rich waters onto the continental shelf of the Western Antarctic Peninsula, resulting in enhanced winter production and prey availability to top predators. We tested aspects of this hypothesis during austral winter by assessing the distribution of the resident pack-ice top predators in relation to these deep across-shelf troughs and by investigating associations between top predators and their prey. Surveys were conducted July-August 2001 and August-September 2002 in Marguerite Bay, Antarctica, with a focus on the main across-shelf trough in the bay, Marguerite Trough. The common pack-ice seabird species were snow petrel (Pagodroma nivea, 1.2 individuals km-2), Antarctic petrel (Thalassoica antarctica, 0.3 individuals km-2), and Ade??lie penguin (Pygoscelis adeliae, 0.5 individuals km-2). The most common pack-ice pinniped was crabeater seal (Lobodon carcinophagus). During both winters, snow and Antarctic petrels were associated with low sea-ice concentrations independent of Marguerite Trough, while Ade??lie penguins occurred in association with this trough. Krill concentrations, both shallow and deep, also were associated with Ade??lie penguin and snow petrel distributions. During both winters, crabeater seal occurrence was associated with deep krill concentrations and with regions of lower chlorophyll concentration. The area of lower chlorophyll concentrations occurred in an area with complex bathymetry close to land and heavy ice concentrations. Complex or unusual bathymetry via its influence on physical and biological processes appears to be one of the keys to understanding how top predators survive during the winter in this Antarctic region. ?? 2007 Elsevier Ltd. All rights reserved.

  2. Variations of mesoscale and large-scale sea ice morphology in the 1984 Marginal Ice Zone Experiment as observed by microwave remote sensing

    NASA Technical Reports Server (NTRS)

    Campbell, W. J.; Josberger, E. G.; Gloersen, P.; Johannessen, O. M.; Guest, P. S.

    1987-01-01

    The data acquired during the summer 1984 Marginal Ice Zone Experiment in the Fram Strait-Greenland Sea marginal ice zone, using airborne active and passive microwave sensors and the Nimbus 7 SMMR, were analyzed to compile a sequential description of the mesoscale and large-scale ice morphology variations during the period of June 6 - July 16, 1984. Throughout the experiment, the long ice edge between northwest Svalbard and central Greenland meandered; eddies were repeatedly formed, moved, and disappeared but the ice edge remained within a 100-km-wide zone. The ice pack behind this alternately diffuse and compact edge underwent rapid and pronounced variations in ice concentration over a 200-km-wide zone. The high-resolution ice concentration distributions obtained in the aircraft images agree well with the low-resolution distributions of SMMR images.

  3. The Seasonal Evolution of Sea Ice Floe Size Distribution

    DTIC Science & Technology

    2013-09-30

    the summer breakup of the ice cover . Large-scale, lower resolution imagery from MODIS and other platforms will also be analyzed to determine changes...control number. 1. REPORT DATE 30 SEP 2013 2. REPORT TYPE 3. DATES COVERED 00-00-2013 to 00-00-2013 4. TITLE AND SUBTITLE The Seasonal Evolution...appearance and morphology of the Arctic sea ice cover over and annual cycle. These photos were taken over the pack ice near SHEBA in May (left) and

  4. Relative influences of the metocean forcings on the drifting ice pack and estimation of internal ice stress gradients in the Labrador Sea

    NASA Astrophysics Data System (ADS)

    Turnbull, I. D.; Torbati, R. Z.; Taylor, R. S.

    2017-07-01

    Understanding the relative influences of the metocean forcings on the drift of sea ice floes is a crucial component to the overall characterization of an ice environment and to developing an understanding of the factors controlling the ice dynamics. In addition, estimating the magnitude of the internal stress gradients on drifting sea ice floes generated by surrounding ice cover is important for modeling operations, informing the design of offshore structures and vessels in ice environments, and for the proper calibration of Discrete Element Models (DEM) of fields of drifting ice floes. In the spring of 2015 and 2016, four sea ice floes offshore Makkovik, Labrador were tagged with satellite-linked ice tracking buoys along with one satellite-linked weather station on each floe to transmit wind speed and direction. Twenty satellite-linked Lagrangian surface ocean current tracking buoys were also deployed in the open water adjacent to the targeted ice floes. In this paper, the dynamics of the four ice floes are explored in terms of the relative proportions which were forced by the wind, current, sea surface topography, Coriolis, and internal stress gradients. The internal ice stress gradients are calculated as residuals between the observed accelerations of the floes as measured by the tracking buoys and the sums of the other metocean forcings. Results show that internal ice stress gradients accounted for up to 50% of the observed forcing on the floes, and may have reached up to around 0.19 kPa.

  5. Performance and durability tests of smart icephobic coatings to reduce ice adhesion

    NASA Astrophysics Data System (ADS)

    Janjua, Zaid A.; Turnbull, Barbara; Choy, Kwang-Leong; Pandis, Christos; Liu, Junpeng; Hou, Xianghui; Choi, Kwing-So

    2017-06-01

    The accretion of ice can cause damage in applications ranging from power lines and shipping decks, to wind turbines and rail infrastructure. In particular on aircraft, it can change aerodynamic characteristics, greatly affecting the flight safety. Commercial aircraft are therefore required to be equipped with de-icing devices, such as heating mats over the wings. The application of icephobic coatings near the leading edge of a wing can in theory reduce the high power requirements of heating mats, which melt ice that forms there. Such coatings are effective in preventing the accretion of runback ice, formed from airborne supercooled droplets, or the water that the heating mats generate as it is sheared back over the wing's upper surface. However, the durability and the practicality of applying them over a large wing surface have been prohibitive factors in deploying this technology so far. Here, we evaluated the ice adhesion strength of four non-conductive coatings and seven thermally conductive coatings by shearing ice samples from coated plates by spinning them in a centrifuge device. The durability of the coating performance was also assessed by repeating the tests, each time regrowing ice samples on the previously-used coatings. Contact angle parameters of each coating were tested for each test to determine influence on ice adhesion strength. The results indicate that contact angle hysteresis is a crucial parameter in determining icephobicity of a coating and hydrophobicity is not necessarily linked to icephobicity.

  6. Flight test report of the NASA icing research airplane: Performance, stability, and control after flight through natural icing conditions

    NASA Technical Reports Server (NTRS)

    Jordan, J. L.; Platz, S. J.; Schinstock, W. C.

    1986-01-01

    Flight test results are presented documenting the effect of airframe icing on performance and stability and control of a NASA DHC-6 icing research aircraft. Kohlman System Research, Inc., provided the data acquisition system and data analysis under contract to NASA. Performance modeling methods and MMLE techniques were used to determine the effects of natural ice on the aircraft. Results showed that ice had a significant effect on the drag coefficient of the aircraft and a modest effect on the MMLE derived longitudinal stability coefficients (code version MMLE). Data is also presented on asymmetric power sign slip maneuvers showing rudder floating characteristics with and without ice on the vertical stabilizer.

  7. Wind-Driven Formation of Ice Bridges in Straits.

    PubMed

    Rallabandi, Bhargav; Zheng, Zhong; Winton, Michael; Stone, Howard A

    2017-03-24

    Ice bridges are static structures composed of tightly packed sea ice that can form during the course of its flow through a narrow strait. Despite their important role in local ecology and climate, the formation and breakup of ice bridges is not well understood and has proved difficult to predict. Using long-wave approximations and a continuum description of sea ice dynamics, we develop a one-dimensional theory for the wind-driven formation of ice bridges in narrow straits, which is verified against direct numerical simulations. We show that for a given wind stress and minimum and maximum channel widths, a steady-state ice bridge can only form beyond a critical value of the thickness and the compactness of the ice field. The theory also makes quantitative predictions for ice fluxes, which are particularly useful to estimate the ice export associated with the breakup of ice bridges. We note that similar ideas are applicable to dense granular flows in confined geometries.

  8. Effects of an Arctic under-ice phytoplankton bloom on bio-optical properties of surface waters during the Norwegian Young Sea Ice Cruise (N-ICE2015)

    NASA Astrophysics Data System (ADS)

    Pavlov, A. K.; Granskog, M. A.; Hudson, S. R.; Taskjelle, T.; Kauko, H.; Hamre, B.; Assmy, P.; Mundy, C. J.; Nicolaus, M.; Kowalczuk, P.; Stedmon, C. A.; Fernandez Mendez, M.

    2016-02-01

    A thinner and younger Arctic sea-ice cover has led to an increase in solar light transmission into the surface ocean, especially during late spring and summer. A description of the seasonal evolution of polar surface water optical properties is essential, in order to understand how changes are affecting light availability for photosynthetic organisms and the surface ocean energy budget. The development of the bio-optical properties of Arctic surface waters under predominantly first-year sea ice in the southern Nansen Basin were studied from January to June 2015 during the Norwegian Young Sea Ice Cruise (N-ICE2015). Observations included inherent optical properties, absorption by colored dissolved organic matter and particles, as well as radiometric measurements. We documented a rapid transition from relatively clear and transparent waters in winter to turbid waters in late May and June. This transition was associated with a strong under-ice phytoplankton bloom detected first under the compact ice pack and then monitored during drift across the marginal ice zone. We discuss potential implications of underwater light availability for photosynthesis, heat redistribution in the upper ocean layer, and energy budget of the sea-ice - ocean system.

  9. Sea-Ice Conditions in the Norwegian, Barents, and White Seas

    DTIC Science & Technology

    1976-08-01

    pack, aided by relatively warm water from the Murman coast current, would reduce the maximum ice thickness predicted by the equation used for...THICKNESS With the aid of the ice growth model in the appendix, it is pos- sible to relate the maximum ice thickness attained during a winter season to a...inserted merely to aid the reader in discerning differences between individual winter seasons. As was the case for the 12-month mean temperatures

  10. Simple Cloud Chambers Using a Freezing Mixture of Ice and Cooking Salt

    ERIC Educational Resources Information Center

    Yoshinaga, Kyohei; Kubota, Miki; Kamata, Masahiro

    2015-01-01

    We have developed much simpler cloud chambers that use only ice and cooking salt instead of the dry ice or ice gel pack needed for the cloud chambers produced in our previous work. The observed alpha-ray particle tracks are as clear as those observed using our previous cloud chambers. The tracks can be observed continuously for about 20?min, and…

  11. Arctic multiyear ice classification and summer ice cover using passive microwave satellite data

    NASA Astrophysics Data System (ADS)

    Comiso, J. C.

    1990-08-01

    The ability to classify and monitor Arctic multiyear sea ice cover using multispectral passive microwave data is studied. Sea ice concentration maps during several summer minima have been analyzed to obtain estimates of ice surviving the summer. The results are compared with multiyear ice concentrations derived from data the following winter, using an algorithm that assumes a certain emissivity for multiyear ice. The multiyear ice cover inferred from the winter data is approximately 25 to 40% less than the summer ice cover minimum, suggesting that even during winter when the emissivity of sea ice is most stable, passive microwave data may account for only a fraction of the total multiyear ice cover. The difference of about 2×106 km2 is considerably more than estimates of advection through Fram Strait during the intervening period. It appears that as in the Antarctic, some multiyear ice floes in the Arctic, especially those near the summer marginal ice zone, have first-year ice or intermediate signatures in the subsequent winter. A likely mechanism for this is the intrusion of seawater into the snow-ice interface, which often occurs near the marginal ice zone or in areas where snow load is heavy. Spatial variations in melt and melt ponding effects also contribute to the complexity of the microwave emissivity of multiyear ice. Hence the multiyear ice data should be studied in conjunction with the previous summer ice data to obtain a more complete characterization of the state of the Arctic ice cover. The total extent and actual areas of the summertime Arctic pack ice were estimated to be 8.4×106 km2 and 6.2×106 km2, respectively, and exhibit small interannual variability during the years 1979 through 1985, suggesting a relatively stable ice cover.

  12. Analysis of an Artificial Tailplane Icing Flight Test of a High-Wing, Twin-Engine Aircraft

    NASA Astrophysics Data System (ADS)

    Shaikh, Shehzad M.

    The US Air Force Flight Test Center (AFFTC) conducted a civilian, Federal Aviation Administration (FAA) sponsored, evaluation of tailplane icing of a twin-turboprop business transport at Edwards Air Force Base. The flight test was conducted to evaluate ice shape growth and extent of ice on the tailplane for specific weather conditions of Liquid Water Content (LWC), droplet size, and ambient temperature. This work analyzes the flight test data comparing the drag for various tailplane icing conditions with respect to a flight test verified calibrated aircraft model. Although less than a third of the test aircraft was involved in the icing environment, the results of this analysis shows a significant increase in the aircraft drag with respect to the LWC, droplet size, and ambient temperature.

  13. Ice Accretions and Icing Effects for Modern Airfoils

    NASA Technical Reports Server (NTRS)

    Addy, Harold E., Jr.

    2000-01-01

    Icing tests were conducted to document ice shapes formed on three different two-dimensional airfoils and to study the effects of the accreted ice on aerodynamic performance. The models tested were representative of airfoil designs in current use for each of the commercial transport, business jet, and general aviation categories of aircraft. The models were subjected to a range of icing conditions in an icing wind tunnel. The conditions were selected primarily from the Federal Aviation Administration's Federal Aviation Regulations 25 Appendix C atmospheric icing conditions. A few large droplet icing conditions were included. To verify the aerodynamic performance measurements, molds were made of selected ice shapes formed in the icing tunnel. Castings of the ice were made from the molds and placed on a model in a dry, low-turbulence wind tunnel where precision aerodynamic performance measurements were made. Documentation of all the ice shapes and the aerodynamic performance measurements made during the icing tunnel tests is included in this report. Results from the dry, low-turbulence wind tunnel tests are also presented.

  14. The Seasonal Evolution of Sea Ice Floe Size Distribution

    DTIC Science & Technology

    2014-09-30

    summer breakup of the ice cover . Large-scale, lower resolution imagery from MODIS and other platforms will also be analyzed to determine changes in floe...number. 1. REPORT DATE 30 SEP 2014 2. REPORT TYPE 3. DATES COVERED 00-00-2014 to 00-00-2014 4. TITLE AND SUBTITLE The Seasonal Evolution of Sea...morphology of the Arctic sea ice cover over and annual cycle. These photos were taken over the pack ice near SHEBA in May (left) and August (right

  15. NASA/FAA Tailplane Icing Program: Flight Test Report

    NASA Technical Reports Server (NTRS)

    Ratvasky, Thomas P.; VanZante, Judith Foss; Sim, Alex

    2000-01-01

    This report presents results from research flights that explored the characteristics of an ice-contaminated tailplane using various simulated ice shapes attached to the leading edge of the horizontal tailplane. A clean leading edge provided the baseline case, then three ice shapes were flown in order of increasing severity. Flight tests included both steady state and dynamic maneuvers. The steady state points were 1G wings level and steady heading sideslips. The primary dynamic maneuvers were pushovers to various G-levels; elevator doublets; and thrust transitions. These maneuvers were conducted for a full range of flap positions and aircraft angle of attack where possible. The analysis of this data set has clearly demonstrated the detrimental effects of ice contamination on aircraft stability and controllability. Paths to tailplane stall were revealed through parameter isolation and transition studies. These paths are (1) increasing ice shape severity, (2) increasing flap deflection, (3) high or low speeds, depending on whether the aircraft is in a steady state (high speed) or pushover maneuver (low speed), and (4) increasing thrust. The flight research effort was very comprehensive, but did not examine effects of tailplane design and location, or other aircraft geometry configuration effects. However, this effort provided the role of some of the parameters in promoting tailplane stall. The lessons learned will provide guidance to regulatory agencies, aircraft manufacturers, and operators on ice-contaminated tailplane stall in the effort to increase aviation safety and reduce the fatal accident rate.

  16. Lewis icing research tunnel test of the aerodynamic effects of aircraft ground deicing/anti-icing fluids

    NASA Technical Reports Server (NTRS)

    Runyan, L. James; Zierten, Thomas A.; Hill, Eugene G.; Addy, Harold E., Jr.

    1992-01-01

    A wind tunnel investigation of the effect of aircraft ground deicing/anti-icing fluids on the aerodynamic characteristics of a Boeing 737-200ADV airplane was conducted. The test was carried out in the NASA Lewis Icing Research Tunnel. Fluids tested include a Newtonian deicing fluid, three non-Newtonian anti-icing fluids commercially available during or before 1988, and eight new experimental non-Newtonian fluids developed by four fluid manufacturers. The results show that fluids remain on the wind after liftoff and cause a measurable lift loss and drag increase. These effects are dependent on the high-lift configuration and on the temperature. For a configuration with a high-lift leading-edge device, the fluid effect is largest at the maximum lift condition. The fluid aerodynamic effects are related to the magnitude of the fluid surface roughness, particularly in the first 30 percent chord. The experimental fluids show a significant reduction in aerodynamic effects.

  17. Analysis of Droplet Size during the Ice Accumulation Phase Of Flight Testing

    NASA Technical Reports Server (NTRS)

    Miller, Eric James

    2004-01-01

    There are numerous hazards associated with air travel. One of the most serious dangers to the pilot and passengers safety is the result of flying into conditions which are conducive to the formation of ice on the surface of an aircraft. Being a pilot myself I am very aware of the dangers that Icing can pose and the effects it can have on an airplane. A couple of the missions of the Icing branch is to make flying safer with more research to increase our knowledge of how ice effects the aerodynamics of an airfoil, and to increase are knowledge of the weather for better forecasting. The Icing Branch uses three different tools to determine the aerodynamic affects that icing has on a wing. The Icing research tunnel is an efficient way to test various airfoils in a controlled setting. To make sure the data received from the wind tunnel is accurate the Icing branch conducts real flight tests with the DHC-6 Twin Otter. This makes sure that the methods used in the wind tunnel accurately model what happens on the actual aircraft. These two tools are also compared to the LEWICE code which is a program that models the ice shape that would be formed on an airfoil in the particular weather conditions that are input by the user. One benefit of LEWICE is that it is a lot cheaper to run than the wind tunnel or flight tests which make it a nice tool for engineers designing aircraft that don t have the money to spend on icing research. Using all three of these tools is a way to cross check the data received from one and check it against the other two. industries, but it is also looked at by weather analysts who are trying to improve forecasting methods. The best way to avoid the troubles of icing encounters is to not go into it in the first place. By looking over the flight data the analyst can determine which conditions will most likely lead to an icing encounter and then this information will aid forecasters when briefing the pilots on the weather conditions. am looking at the

  18. Physical processes contributing to an ice free Beaufort Sea during September 2012

    NASA Astrophysics Data System (ADS)

    Babb, D. G.; Galley, R. J.; Barber, D. G.; Rysgaard, S.

    2016-01-01

    During the record September 2012 sea ice minimum, the Beaufort Sea became ice free for the first time during the observational record. Increased dynamic activity during late winter enabled increased open water and seasonal ice coverage that contributed to negative sea ice anomalies and positive solar absorption anomalies which drove rapid bottom melt and sea ice loss. As had happened in the Beaufort Sea during previous years of exceptionally low September sea ice extent, anomalous solar absorption developed during May, increased during June, peaked during July, and persisted into October. However in situ observations from a single floe reveal less than 78% of the energy required for bottom melt during 2012 was available from solar absorption. We show that the 2012 sea ice minimum in the Beaufort was the result of anomalously large solar absorption that was compounded by an arctic cyclone and other sources of heat such as solar transmission, oceanic upwelling, and riverine inputs, but was ultimately made possible through years of preconditioning toward a younger, thinner ice pack. Significant negative trends in sea ice concentration between 1979 and 2012 from June to October, coupled with a tendency toward earlier sea ice reductions have fostered a significant trend of +12.9 MJ m-2 yr-1 in cumulative solar absorption, sufficient to melt an additional 4.3 cm m-2 yr-1. Overall through preconditioning toward a younger, thinner ice pack the Beaufort Sea has become increasingly susceptible to increased sea ice loss that may render it ice free more frequently in coming years.

  19. Physical Processes contributing to an ice free Beaufort Sea during September 2012

    NASA Astrophysics Data System (ADS)

    Babb, D.; Galley, R.; Barber, D. G.; Rysgaard, S.

    2016-12-01

    During the record September 2012 sea ice minimum the Beaufort Sea became ice free for the first time during the observational record. Increased dynamic activity during late winter enabled increased open water and seasonal ice coverage that contributed to negative sea ice anomalies and positive solar absorption anomalies which drove rapid bottom melt and sea ice loss. As had happened in the Beaufort Sea during previous years of exceptionally low September sea ice extent, anomalous solar absorption developed during May, increased during June, peaked during July and persisted into October. However in situ observations from a single floe reveal less than 78% of the energy required for bottom melt during 2012 was available from solar absorption. We show that the 2012 sea ice minimum in the Beaufort was the result of anomalously large solar absorption that was compounded by an arctic cyclone and other sources of heat such as solar transmission, oceanic upwelling and riverine inputs, but was ultimately made possible through years of preconditioning towards a younger, thinner ice pack. Significant negative trends in sea ice concentration between 1979 and 2012 from June to October, coupled with a tendency towards earlier sea ice reductions have fostered a significant trend of +12.9 MJ m-2 year-1 in cumulative solar absorption, sufficient to melt an additional 4.3 cm m-2 year-1. Overall through preconditioning towards a younger, thinner ice pack the Beaufort Sea has become increasingly susceptible to increased sea ice loss that may render it ice free more frequently in coming years.

  20. The usefulness and reliability of fitness testing protocols for ice hockey players: a literature review.

    PubMed

    Nightingale, Steven C; Miller, Stuart; Turner, Anthony

    2013-06-01

    Ice hockey, like most sports, uses fitness testing to assess athletes. This study reviews the current commonly used fitness testing protocols for ice hockey players, discussing their predictive values and reliability. It also discusses a range of less commonly used measures and limitations in current testing protocols. The article concludes with a proposed testing program suitable for ice hockey players.

  1. Antarctic Sea-Ice Freeboard and Estimated Thickness from NASA's ICESat and IceBridge Observations

    NASA Technical Reports Server (NTRS)

    Yi, Donghui; Kurtz, Nathan; Harbeck, Jeremy; Manizade, Serdar; Hofton, Michelle; Cornejo, Helen G.; Zwally, H. Jay; Robbins, John

    2016-01-01

    ICESat completed 18 observational campaigns during its lifetime from 2003 to 2009. Data from all of the 18 campaign periods are used in this study. Most of the operational periods were between 34 and 38 days long. Because of laser failure and orbit transition from 8-day to 91-day orbit, there were four periods lasting 57, 16, 23, and 12 days. IceBridge data from 2009, 2010, and 2011 are used in this study. Since 2009, there are 19 Airborne Topographic Mapper (ATM) campaigns, and eight Land, Vegetation, and Ice Sensor (LVIS) campaigns over the Antarctic sea ice. Freeboard heights are derived from ICESat, ATM and LVIS elevation and waveform data. With nominal densities of snow, water, and sea ice, combined with snow depth data from AMSR-E/AMSR2 passive microwave observation over the southern ocean, sea-ice thickness is derived from the freeboard. Combined with AMSR-E/AMSR2 ice concentration, sea-ice area and volume are also calculated. During the 2003-2009 period, sea-ice freeboard and thickness distributions show clear seasonal variations that reflect the yearly cycle of the growth and decay of the Antarctic pack ice. We found no significant trend of thickness or area for the Antarctic sea ice during the ICESat period. IceBridge sea ice freeboard and thickness data from 2009 to 2011 over the Weddell Sea and Amundsen and Bellingshausen Seas are compared with the ICESat results.

  2. 10 CFR 32.103 - Schedule D-prototype tests for ice detection devices containing strontium-90.

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... 10 Energy 1 2010-01-01 2010-01-01 false Schedule D-prototype tests for ice detection devices... § 32.103 Schedule D—prototype tests for ice detection devices containing strontium-90. An applicant for a license pursuant to § 32.61 shall conduct prototype tests on each of five prototype ice detection...

  3. 10 CFR 32.103 - Schedule D-prototype tests for ice detection devices containing strontium-90.

    Code of Federal Regulations, 2011 CFR

    2011-01-01

    ... 10 Energy 1 2011-01-01 2011-01-01 false Schedule D-prototype tests for ice detection devices... § 32.103 Schedule D—prototype tests for ice detection devices containing strontium-90. An applicant for a license pursuant to § 32.61 shall conduct prototype tests on each of five prototype ice detection...

  4. 10 CFR 32.103 - Schedule D-prototype tests for ice detection devices containing strontium-90.

    Code of Federal Regulations, 2012 CFR

    2012-01-01

    ... 10 Energy 1 2012-01-01 2012-01-01 false Schedule D-prototype tests for ice detection devices... § 32.103 Schedule D—prototype tests for ice detection devices containing strontium-90. An applicant for a license pursuant to § 32.61 shall conduct prototype tests on each of five prototype ice detection...

  5. Arctic continental shelf morphology related to sea-ice zonation, Beaufort Sea, Alaska

    USGS Publications Warehouse

    Reimnitz, E.; Toimil, L.; Barnes, P.

    1978-01-01

    Landsat-1 and NOAA satellite imagery for the winter 1972-1973, and a variety of ice and sea-floor data were used to study sea-ice zonation and dynamics and their relation to bottom morphology and geology on the Beaufort Sea continental shelf of arctic Alaska. In early winter the location of the boundary between undeformed fast ice and westward-drifting pack ice of the Pacific Gyre is controlled by major coastal promontories. Pronounced linear pressure- and shear-ridges, as well as hummock fields, form along this boundary and are stabilized by grounding, generally between the 10- and 20-m isobaths. Slippage along this boundary occurs intermittently at or seaward of the grounded ridges, forming new grounded ridges in a widening zone, the stamukhi zone, which by late winter extends out to the 40-m isobath. Between intermittent events along the stamukhi zone, pack-ice drift and slippage is continuous along the shelf edge, at average rates of 3-10 km/day. Whether slippage occurs along the stamukhi zone or along the shelf edge, it is restricted to a zone several hundred meters wide, and ice seaward of the slip face moves at uniform rates without discernible drag effects. A causal relationship is seen between the spatial distribution of major ice-ridge systems and offshore shoals downdrift of major coastal promontories. The shoals appear to have migrated shoreward under the influence of ice up to 400 m in the last 25 years. The sea floor seaward of these shoals within the stamukhi zone shows high ice-gouge density, large incision depths, and a high degree of disruption of internal sedimentary structures. The concentration of large ice ridges and our sea floor data in the stamukhi zone indicate that much of the available marine energy is expended here, while the inner shelf and coast, where the relatively undeformed fast ice grows, are sheltered. There is evidence that anomalies in the overall arctic shelf profile are related to sea-ice zonation, ice dynamics, and bottom

  6. The effect of cool water pack preparation on vaccine vial temperatures in refrigerators.

    PubMed

    Goldwood, Geneva; Diesburg, Steven

    2018-01-02

    Cool water packs are a useful alternative to ice packs for preventing unintentional freezing of vaccines during outreach in some situations. Current guidelines recommend the use of a separate refrigerator for cooling water packs from ambient temperatures to prevent possible heat degradation of adjacent vaccine vials. To investigate whether this additional equipment is necessary, we measured the temperatures that vaccine vials were exposed to when warm water packs were placed next to vials in a refrigerator. We then calculated the effect of repeated vial exposure to those temperatures on vaccine vial monitor status to estimate the impact to the vaccine. Vials were tested in a variety of configurations, varying the number and locations of vials and water packs in the refrigerator. The calculated average percentage life lost during a month of repeated warming ranged from 20.0% to 30.3% for a category 2 (least stable) vaccine vial monitor and from 3.8% to 6.0% for a category 7 (moderate stability) vaccine vial monitor, compared to 17.0% for category 2 vaccine vial monitors and 3.1% for category 7 vaccine vial monitors at a constant 5 °C. The number of vials, number of water packs, and locations of each impacted vial warming and therefore percentage life lost, but the vaccine vial monitor category had a higher impact on the average percentage life lost than any of the other parameters. The results suggest that damage to vaccines from repeated warming over the course of a month is not certain and that cooling water packs in a refrigerator where vaccines are being stored may be a useful practice if safe procedures are established. Copyright © 2017 The Author(s). Published by Elsevier Ltd.. All rights reserved.

  7. 2. DETAIL OF DISCHARGE CHUTES FROM VOGT AUTOMATIC TUBE ICE ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    2. DETAIL OF DISCHARGE CHUTES FROM VOGT AUTOMATIC TUBE ICE MACHINE IN SOUTHWEST CORNER OF LEVEL 5; ICE DROPPED INTO HOLDING BIN BEFORE BEING TRANSFERRED TO RAIL CARS OUTSIDE BUILDING (HENRY VOGT MACHINE COMPANY, LOUISVILLE, USA, PATENT NO. 2,200,424 - Rath Packing Company, Cooler Building, Sycamore Street between Elm & Eighteenth Streets, Waterloo, Black Hawk County, IA

  8. Advances in Airborne Altimetric Techniques for the Measurement of Snow on Arctic Sea Ice

    NASA Astrophysics Data System (ADS)

    Newman, T.; Farrell, S. L.; Richter-Menge, J.; Elder, B. C.; Ruth, J.; Connor, L. N.

    2014-12-01

    Current sea ice observations and models indicate a transition towards a more seasonal Arctic ice pack with a smaller, and geographically more variable, multiyear ice component. To gain a comprehensive understanding of the processes governing this transition it is important to include the impact of the snow cover, determining the mechanisms by which snow is both responding to and forcing changes to the sea ice pack. Data from NASA's Operation IceBridge (OIB) snow radar system, which has been making yearly surveys of the western Arctic since 2009, offers a key resource for investigating the snow cover. In this work, we characterize the OIB snow radar instrument response to ascertain the location of 'side-lobes', aiding the interpretation of snow radar data. We apply novel wavelet-based techniques to identify the primary reflecting interfaces within the snow pack from which snow depth estimates are derived. We apply these techniques to the range of available snow radar data collected over the last 6 years during the NASA OIB mission. Our results are validated through comparison with a range of in-situ data. We discuss the impact of sea ice surface morphology on snow radar returns (with respect to ice type) and the topographic conditions over which accurate snow-radar-derived snow depths may be obtained. Finally we present improvements to in situ survey design that will allow for both an improved sampling of the snow radar footprint and more accurate assessment of the uncertainties in radar-derived snow depths in the future.

  9. Numerical test of the Edwards conjecture shows that all packings are equally probable at jamming

    NASA Astrophysics Data System (ADS)

    Martiniani, Stefano; Schrenk, K. Julian; Ramola, Kabir; Chakraborty, Bulbul; Frenkel, Daan

    2017-09-01

    In the late 1980s, Sam Edwards proposed a possible statistical-mechanical framework to describe the properties of disordered granular materials. A key assumption underlying the theory was that all jammed packings are equally likely. In the intervening years it has never been possible to test this bold hypothesis directly. Here we present simulations that provide direct evidence that at the unjamming point, all packings of soft repulsive particles are equally likely, even though generically, jammed packings are not. Typically, jammed granular systems are observed precisely at the unjamming point since grains are not very compressible. Our results therefore support Edwards’ original conjecture. We also present evidence that at unjamming the configurational entropy of the system is maximal.

  10. Mixed ice accretion on aircraft wings

    NASA Astrophysics Data System (ADS)

    Janjua, Zaid A.; Turnbull, Barbara; Hibberd, Stephen; Choi, Kwing-So

    2018-02-01

    Ice accretion is a problematic natural phenomenon that affects a wide range of engineering applications including power cables, radio masts, and wind turbines. Accretion on aircraft wings occurs when supercooled water droplets freeze instantaneously on impact to form rime ice or runback as water along the wing to form glaze ice. Most models to date have ignored the accretion of mixed ice, which is a combination of rime and glaze. A parameter we term the "freezing fraction" is defined as the fraction of a supercooled droplet that freezes on impact with the top surface of the accretion ice to explore the concept of mixed ice accretion. Additionally we consider different "packing densities" of rime ice, mimicking the different bulk rime densities observed in nature. Ice accretion is considered in four stages: rime, primary mixed, secondary mixed, and glaze ice. Predictions match with existing models and experimental data in the limiting rime and glaze cases. The mixed ice formulation however provides additional insight into the composition of the overall ice structure, which ultimately influences adhesion and ice thickness, and shows that for similar atmospheric parameter ranges, this simple mixed ice description leads to very different accretion rates. A simple one-dimensional energy balance was solved to show how this freezing fraction parameter increases with decrease in atmospheric temperature, with lower freezing fraction promoting glaze ice accretion.

  11. The internal structure of the Brunt Ice Shelf, Antarctica from ice-penetrating radar

    NASA Astrophysics Data System (ADS)

    King, Edward; De Rydt, Jan; Gudmundsson, Hilmar

    2016-04-01

    The Brunt Ice Shelf is a small feature on the Coats Land Coast of the Weddell Sea, Antarctica. It is unusual among Antarctic ice shelves because the ice crossing the grounding line from the ice sheet retains no structural integrity, so the ice shelf comprises icebergs of continental ice cemented together by sea ice, with the whole blanketed by in-situ snowfall. The size and distribution of the icebergs is governed by the thickness profile along the grounding line. Where bedrock troughs discharge thick ice to the ice shelf, the icebergs are large and remain close together with little intervening sea ice. Where bedrock ridges mean the ice crossing the grounding line is thin, the icebergs are small and widely-scattered with large areas of sea ice between them. To better understand the internal structure of the Brunt Ice Shelf and how this might affect the flow dynamics we conducted ice-penetrating radar surveys during December 2015 and January 2016. Three different ground-based radar systems were used, operating at centre frequencies of 400, 50 and 10 MHz respectively. The 400 MHz system gave detailed firn structure and accumulation profiles as well as time-lapse profiles of the active propagation of a crevasse. The 50 MHz system provided intermediate-level detail of iceberg distribution and thickness as well as information on the degree of salt water infiltration into the accumulating snow pack. The 10 MHz system used a high-power transmitter in an attempt to measure ice thickness beneath salt-impregnated ice. In this poster we will present example data from each of the three radar systems which will demonstrate the variability of the internal structure of the ice shelf. We will also present preliminary correlations between the internal structure and the surface topography from satellite data.

  12. [The ice water test and bladder cooling reflex. Physiology, pathophysiology and clinical importance].

    PubMed

    Hüsch, T; Neuerburg, T; Reitz, A; Haferkamp, A

    2016-04-01

    Urodynamic studies are utilised for identification and follow-up of functional disorders of the lower urinary tract. Provocation tests are used to determine disorders which could not be revealed in standard cystometry. The ice water test is a simple test to identify neurogenic bladder dysfunction and to screen the integrity of the upper motor neuron in neurogenic bladder dysfunction. Development and significance of the ice water test is presented in this review against the background of physiology and pathophysiology of the lower urinary tract. A systematic review of PubMed and ScienceDirect databases was performed in April 2015. No language or time limitation was applied. The following key words and Medical Subject Heading terms were used to identify relevant studies: "ice water test", "bladder cooling reflex", "micturition" and "neuronal control". Review articles and bibliographies of other relevant studies identified were hand searched to find additional studies. The ice water test is performed by rapid instillation of 4-8 °C cold fluid into the urinary bladder. Hereby, afferent C fibers are activated by cold receptors in the bladder leading to the bladder cooling reflex. It is a spinal reflex which causes an involuntarily contraction of the urinary bladder. The test is normally positive in young infants during the first 4 years of life and become negative with maturation of the central nervous system afterwards by inhibition of the reflex. The damage of the upper motor neuron causes the recurrence of the reflex in the adulthood and indicates spinal and cerebral lesions. The ice water test is utilised to identify lesions of the upper motor neuron. However, in the case of detrusor acontractility the test will always be negative and can not be utilized to distinguish between neurogenic or muscular causes. Furthermore, the test is also positive in a small percentage of cases of non-neurogenic diseases, e.g. in prostate-related bladder outlet obstruction or

  13. Review of the Aerodynamic Acceptance Test and Application to Anti-Icing Fluids Testing in the NRC Propulsion and Icing Wind Tunnel

    NASA Technical Reports Server (NTRS)

    Broeren, Andy P.; Riley, James T.

    2012-01-01

    In recent years, the FAA has worked with Transport Canada, National Research Council of Canada (NRC) and APS Aviation, Inc. to develop allowance times for aircraft operations in ice-pellet precipitation. These allowance times are critical to ensure safety and efficient operation of commercial and cargo flights. Wind-tunnel testing with uncontaminated anti-icing fluids and fluids contaminated with simulated ice-pellets had been carried out at the NRC Propulsion and Icing Wind Tunnel (PIWT) to better understand the flowoff characteristics and resulting aerodynamic effects. The percent lift loss on the thin, high-performance wing model tested in the PIWT was determined at 8 angle of attack and used as one of the evaluation criteria in determining the allowance times. Because it was unclear as to how performance degradations measured on this model were relevant to an actual airplane configuration, some means of interpreting the wing model lift loss was deemed necessary. In this report, the lift loss was related to the loss in maximum lift of a Boeing 737-200ADV airplane through the Aerodynamic Acceptance Test (AAT) performed for fluids qualification. This report provides a review of the research basis of the AAT in order to understand how this correlation was applied. A loss in maximum lift coefficient of 5.24 percent on the B737-200ADV airplane (which was adopted as the threshold in the AAT) corresponds to a lift loss of 7.3 percent on the PIWT model at 8 degrees angle of attack. There is significant scatter in the data used to develop the correlation related to varying effects of the various antiicing fluids that were tested and other factors. A statistical analysis indicated the upper limit of lift loss on the PIWT model was 9.2 percent. Therefore, for cases resulting in PIWT model lift loss from 7.3 to 9.2 percent, extra scrutiny of the visual observations is required in evaluating fluid performance with contamination. Additional research may result in future

  14. Lower limb ice application alters ground reaction force during gait initiation

    PubMed Central

    Muniz, Thiago B.; Moraes, Renato; Guirro, Rinaldo R. J.

    2015-01-01

    BACKGROUND: Cryotherapy is a widely used technique in physical therapy clinics and sports. However, the effects of cryotherapy on dynamic neuromuscular control are incompletely explained. OBJECTIVES: To evaluate the effects of cryotherapy applied to the calf, ankle and sole of the foot in healthy young adults on ground reaction forces during gait initiation. METHOD: This study evaluated the gait initiation forces, maximum propulsion, braking forces and impulses of 21 women volunteers through a force platform, which provided maximum and minimum ground reaction force values. To assess the effects of cooling, the task - gait initiation - was performed before ice application, immediately after and 30 minutes after removal of the ice pack. Ice was randomly applied on separate days to the calf, ankle and sole of the foot of the participants. RESULTS: It was demonstrated that ice application for 30 minutes to the sole of the foot and calf resulted in significant changes in the vertical force variables, which returned to their pre-application values 30 minutes after the removal of the ice pack. Ice application to the ankle only reduced propulsion impulse. CONCLUSIONS: These results suggest that although caution is necessary when performing activities that require good gait control, the application of ice to the ankle, sole of the foot or calf in 30-minute intervals may be safe even preceding such activities. PMID:25993625

  15. Lower limb ice application alters ground reaction force during gait initiation.

    PubMed

    Muniz, Thiago B; Moraes, Renato; Guirro, Rinaldo R J

    2015-01-01

    Cryotherapy is a widely used technique in physical therapy clinics and sports. However, the effects of cryotherapy on dynamic neuromuscular control are incompletely explained. To evaluate the effects of cryotherapy applied to the calf, ankle and sole of the foot in healthy young adults on ground reaction forces during gait initiation. This study evaluated the gait initiation forces, maximum propulsion, braking forces and impulses of 21 women volunteers through a force platform, which provided maximum and minimum ground reaction force values. To assess the effects of cooling, the task--gait initiation--was performed before ice application, immediately after and 30 minutes after removal of the ice pack. Ice was randomly applied on separate days to the calf, ankle and sole of the foot of the participants. It was demonstrated that ice application for 30 minutes to the sole of the foot and calf resulted in significant changes in the vertical force variables, which returned to their pre-application values 30 minutes after the removal of the ice pack. Ice application to the ankle only reduced propulsion impulse. These results suggest that although caution is necessary when performing activities that require good gait control, the application of ice to the ankle, sole of the foot or calf in 30-minute intervals may be safe even preceding such activities.

  16. Flight Testing an Iced Business Jet for Flight Simulation Model Validation

    NASA Technical Reports Server (NTRS)

    Ratvasky, Thomas P.; Barnhart, Billy P.; Lee, Sam; Cooper, Jon

    2007-01-01

    A flight test of a business jet aircraft with various ice accretions was performed to obtain data to validate flight simulation models developed through wind tunnel tests. Three types of ice accretions were tested: pre-activation roughness, runback shapes that form downstream of the thermal wing ice protection system, and a wing ice protection system failure shape. The high fidelity flight simulation models of this business jet aircraft were validated using a software tool called "Overdrive." Through comparisons of flight-extracted aerodynamic forces and moments to simulation-predicted forces and moments, the simulation models were successfully validated. Only minor adjustments in the simulation database were required to obtain adequate match, signifying the process used to develop the simulation models was successful. The simulation models were implemented in the NASA Ice Contamination Effects Flight Training Device (ICEFTD) to enable company pilots to evaluate flight characteristics of the simulation models. By and large, the pilots confirmed good similarities in the flight characteristics when compared to the real airplane. However, pilots noted pitch up tendencies at stall with the flaps extended that were not representative of the airplane and identified some differences in pilot forces. The elevator hinge moment model and implementation of the control forces on the ICEFTD were identified as a driver in the pitch ups and control force issues, and will be an area for future work.

  17. [Ice application for reducing pain associated with goserelin acetate injection].

    PubMed

    Ishii, Kaname; Nagata, Chika; Koshizaki, Eiko; Nishiuchi, Satoko

    2013-10-01

    We investigated the effectiveness of using an ice pack for reducing the pain associated with goserelin acetate injection. In this study, 39 patients with prostate cancer and 1 patient with breast cancer receiving hormonal therapy with goserelin acetate were enrolled. All patients completed a questionnaire regarding the use of ice application. We used the numerical rating scale (NRS) to assess the pain associated with injection. The NRS scores indicated that the pain was significantly less with ice application than with the usual method (p < 0.001). Further, ice application could decrease the duration of pain sensation. Ice application at the injection site is safe and effective for reducing pain.

  18. Acquisition of Airborne Sea Ice Remote Sensing Data with CULPIS-X: an Instrument Mounted on a US Coast Guard C-130

    NASA Astrophysics Data System (ADS)

    Tschudi, M. A.; Tooth, M.; Barton-Grimley, R. A.

    2016-12-01

    To obtain high-resolution observations of sea ice, we developed the University of Colorado LIDAR Profiler Instrument Suite - Extended (CULPIS-X). CULPIS-X, originally funded by NASA and currently supported by ONR, is being deployed in the flare tube of a US Coast Guard (USCG) C-130 aircraft, during Arctic Domain Awareness (ADA) flights from Kodiak, AK to the Arctic, in cooperation with the Coast Guard and with the Seasonal Ice Zone Remote Sensing (SIZRS, J. Morrison, PI) program. CULPIS-X (Figure 1) contains a LIDAR, digital camera, thermal infrared and hyperspectral radiometers, along with a GPS for aircraft altitude and an Inertial Measurement Unit (IMU) for aircraft attitude, and a computer to process and write the instrument data to SD cards. The package is designed to fly over Arctic sea ice for the purposes of measuring sea ice roughness, estimating sea ice thickness, and measuring ice surface temperature and reflectance. CULPIS-X had its inaugural flight aboard a C-130 out of USCG Air Station Sacramento in April 2016. This flight tested the structure of CULPIS-X, along with instrument readiness. The inaugural Arctic flight of CULPIS-X took place on June 15, 2016. The C-130 took off from Kodiak and flew towards Deadhorse, where it turned on to the 150W longitude line and proceeded north to 76N. The C-130 descended to a lower altitude ( 500 feet) during several flight segments along the 150W line, from Deadhorse to 76N and back. The lower altitude is required to obtain ULS LIDAR return pulses as they reflect off the ocean and sea ice. A similar flight was also performed on July 13, 2016. LIDAR data will be utilized to determine the surface roughness of the overflown ice pack. Furthermore, we will pick locations where open water occurred near or within the ice pack, to establish the freeboard of the ice pack, which will be used to estimate the sea ice thickness. More flights are scheduled for this season, in mid-Aug, Sept, and Oct, and are designed to overfly

  19. Measuring the sea ice floe size distribution

    NASA Technical Reports Server (NTRS)

    Rothrock, D. A.; Thorndike, A. S.

    1984-01-01

    The sea ice covering the Arctic Ocean is broken into distinct pieces,called floes. In the summer, these floes, which have diameters ranging up to 100 km, are separated from each other by a region of open water. In the winter, floes still exist, but they are less easily identified. An understanding of the geometry of the ice pack is of interest for a number of practical applications associated with transportation in ice-covered seas and with the design of offshore structures intended to survive in the presence of ice. The present investigation has the objective to clarify ideas about floe sizes and to propose techniques for measuring them. Measurements are presented with the primary aim to illustrate points of technique or approach. A preliminary discussion of the floe size distribution of sea ice is devoted to questions of definition and of measurement.

  20. Airborne gravity measurement over sea-ice: The western Weddel Sea

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Brozena, J.; Peters, M.; LaBrecque, J.

    1990-10-01

    An airborne gravity study of the western Weddel Sea, east of the Antarctic Peninsula, has shown that floating pack-ice provides a useful radar altimetric reference surface for altitude and vertical acceleration corrections surface for alititude and vertical acceleration corrections to airborne gravimetry. Airborne gravimetry provides an important alternative to satellite altimetry for the sea-ice covered regions of the world since satellite alimeters are not designed or intended to provide accurate geoidal heights in areas where significant sea-ice is present within the radar footprint. Errors in radar corrected airborne gravimetry are primarily sensitive to the variations in the second derivative ofmore » the sea-ice reference surface in the frequency pass-band of interest. With the exception of imbedded icebergs the second derivative of the pack-ice surface closely approximates that of the mean sea-level surface at wavelengths > 10-20 km. With the airborne method the percentage of ice coverage, the mixture of first and multi-year ice and the existence of leads and pressure ridges prove to be unimportant in determining gravity anomalies at scales of geophysical and geodetic interest, provided that the ice is floating and not grounded. In the Weddell study an analysis of 85 crosstrack miss-ties distributed over 25 data tracks yields an rms error of 2.2 mGals. Significant structural anomalies including the continental shelf and offsets and lineations interpreted as fracture zones recording the early spreading directions within the Weddell Sea are observed in the gravity map.« less

  1. An investigation of the effect of rapid slurry chilling on blown pack spoilage of vacuum-packaged beef primals.

    PubMed

    Reid, R; Fanning, S; Whyte, P; Kerry, J; Bolton, D

    2017-02-01

    The aim of this study was to investigate if rapid slurry chilling would retard or prevent blown pack spoilage (BPS) of vacuum-packaged beef primals. Beef primals were inoculated with Clostridium estertheticum subspp. estertheticum (DSMZ 8809), C. estertheticum subspp. laramenise (DSMZ 14864) and C. gasigenes (DSMZ 12272), and vacuum-packaged with and without heat shrinkage (90°C for 3 s). These packs were then subjected to immediate chilling in an ice slurry or using conventional blast chilling systems and stored at 2°C for up to 100 days. The onset and progress of BPS was monitored using the following scale; 0-no gas bubbles in drip; 1-gas bubbles in drip; 2-loss of vacuum; 3-'blown'; 4-presence of sufficient gas inside the packs to produce pack distension and 5-tightly stretched, 'overblown' packs/packs leaking. Rapid slurry chilling (as compared to conventional chilling) did not significantly affect (P > 0.05) the time to the onset or progress of BPS. It was therefore concluded that rapid chilling of vacuum-packaged beef primals, using an ice slurry system, may not be used as a control intervention to prevent or retard blown pack spoilage. This study adds to our growing understanding of blown pack spoilage of vacuum-packaged beef primals and suggests that rapid chilling of vacuum-packaged beef primals is not a control option for the beef industry. The results suggest that neither eliminating the heat shrinkage step nor rapid chilling of vacuum-packaged beef retard the time to blown pack spoilage. © 2016 The Society for Applied Microbiology.

  2. AUV Commercialization - Who’s Leading the Pack?

    DTIC Science & Technology

    2000-09-01

    the Theseus and ARCS, is designing a deep water commercial site survey AUV for Fugro GeoServices Inc. Called the Explorer, the vehicle will conduct...ISE has the ARCS and the Theseus vehicles and Perry Technologies has the MUST. These vehicles have each performed some dramatic operations including the...deployment of fiber optic cables. In the case of Theseus , the fiber optic cable was deployed under the ice pack. Mid-size vehicles include those from

  3. A simple video-based timing system for on-ice team testing in ice hockey: a technical report.

    PubMed

    Larson, David P; Noonan, Benjamin C

    2014-09-01

    The purpose of this study was to describe and evaluate a newly developed on-ice timing system for team evaluation in the sport of ice hockey. We hypothesized that this new, simple, inexpensive, timing system would prove to be highly accurate and reliable. Six adult subjects (age 30.4 ± 6.2 years) performed on ice tests of acceleration and conditioning. The performance times of the subjects were recorded using a handheld stopwatch, photocell, and high-speed (240 frames per second) video. These results were then compared to allow for accuracy calculations of the stopwatch and video as compared with filtered photocell timing that was used as the "gold standard." Accuracy was evaluated using maximal differences, typical error/coefficient of variation (CV), and intraclass correlation coefficients (ICCs) between the timing methods. The reliability of the video method was evaluated using the same variables in a test-retest analysis both within and between evaluators. The video timing method proved to be both highly accurate (ICC: 0.96-0.99 and CV: 0.1-0.6% as compared with the photocell method) and reliable (ICC and CV within and between evaluators: 0.99 and 0.08%, respectively). This video-based timing method provides a very rapid means of collecting a high volume of very accurate and reliable on-ice measures of skating speed and conditioning, and can easily be adapted to other testing surfaces and parameters.

  4. Direct observations of atmosphere - sea ice - ocean interactions during Arctic winter and spring storms

    NASA Astrophysics Data System (ADS)

    Graham, R. M.; Itkin, P.; Granskog, M. A.; Assmy, P.; Cohen, L.; Duarte, P.; Doble, M. J.; Fransson, A.; Fer, I.; Fernandez Mendez, M.; Frey, M. M.; Gerland, S.; Haapala, J. J.; Hudson, S. R.; Liston, G. E.; Merkouriadi, I.; Meyer, A.; Muilwijk, M.; Peterson, A.; Provost, C.; Randelhoff, A.; Rösel, A.; Spreen, G.; Steen, H.; Smedsrud, L. H.; Sundfjord, A.

    2017-12-01

    To study the thinner and younger sea ice that now dominates the Arctic the Norwegian Young Sea ICE expedition (N-ICE2015) was launched in the ice-covered region north of Svalbard, from January to June 2015. During this time, eight local and remote storms affected the region and rare direct observations of the atmosphere, snow, ice and ocean were conducted. Six of these winter storms passed directly over the expedition and resulted in air temperatures rising from below -30oC to near 0oC, followed by abrupt cooling. Substantial snowfall prior to the campaign had already formed a snow pack of approximately 50 cm, to which the February storms contributed an additional 6 cm. The deep snow layer effectively isolated the ice cover and prevented bottom ice growth resulting in low brine fluxes. Peak wind speeds during winter storms exceeded 20 m/s, causing strong snow re-distribution, release of sea salt aerosol and sea ice deformation. The heavy snow load caused widespread negative freeboard; during sea ice deformation events, level ice floes were flooded by sea water, and at least 6-10 cm snow-ice layer was formed. Elevated deformation rates during the most powerful winter storms damaged the ice cover permanently such that the response to wind forcing increased by 60 %. As a result of a remote storm in April deformation processes opened about 4 % of the total area into leads with open water, while a similar amount of ice was deformed into pressure ridges. The strong winds also enhanced ocean mixing and increased ocean heat fluxes three-fold in the pycnocline from 4 to 12 W/m2. Ocean heat fluxes were extremely large (over 300 W/m2) during storms in regions where the warm Atlantic inflow is located close to surface over shallow topography. This resulted in very large (5-25 cm/day) bottom ice melt and in cases flooding due to heavy snow load. Storm events increased the carbon dioxide exchange between the atmosphere and ocean but also affected the pCO2 in surface waters

  5. Remarkable antiagglomeration effect of a yeast biosurfactant, diacylmannosylerythritol, on ice-water slurry for cold thermal storage.

    PubMed

    Kitamoto, D; Yanagishita, H; Endo, A; Nakaiwa, M; Nakane, T; Akiya, T

    2001-01-01

    Antiagglomeration effects of different surfactants on ice slurry formation were examined to improve the efficiency of an ice-water slurry system to be used for cold thermal storage. Among the chemical surfactants tested, a nonionic surfactant, poly(oxyethylene) sorbitan dioleate, was found to show a greater antiagglomeration effect on the slurry than anionic, cationic, or amphoteric surfactants. More interestingly, diacylmannosylerythritol, a glycolipid biosurfactant produced by a yeast strain of Candida antarctica, exhibited a remarkable effect on the slurry, attaining a high ice packing factor (35%) for 8 h at a biosurfactant concentration of 10 mg/L. These nonionic glycolipid surfactants are likely to effectively adsorb on the ice surface in a highly regulated manner to suppress the agglomeration or growth of the ice particles. This is the first report on the utilization of biosurfactant for thermal energy storage, which may significantly expand the commercial applications of the highly environmentally friendly slurry system.

  6. Refrigerated Wind Tunnel Tests on Surface Coatings for Preventing Ice Formation

    NASA Technical Reports Server (NTRS)

    Knight, Montgomery; Clay, William C

    1930-01-01

    This investigation was conducted to determine the effectiveness of various surface coatings as a means for preventing ice formations on aircraft in flight. The substances used as coatings for these tests are divided into two groups: compounds soluble in water, and those which are insoluble in water. It was found that certain soluble compounds were apparently effective in preventing the formation of ice on an airfoil model, while all insoluble compounds which were tested were found to be ineffective.

  7. Square ice in graphene nanocapillaries.

    PubMed

    Algara-Siller, G; Lehtinen, O; Wang, F C; Nair, R R; Kaiser, U; Wu, H A; Geim, A K; Grigorieva, I V

    2015-03-26

    Bulk water exists in many forms, including liquid, vapour and numerous crystalline and amorphous phases of ice, with hexagonal ice being responsible for the fascinating variety of snowflakes. Much less noticeable but equally ubiquitous is water adsorbed at interfaces and confined in microscopic pores. Such low-dimensional water determines aspects of various phenomena in materials science, geology, biology, tribology and nanotechnology. Theory suggests many possible phases for adsorbed and confined water, but it has proved challenging to assess its crystal structure experimentally. Here we report high-resolution electron microscopy imaging of water locked between two graphene sheets, an archetypal example of hydrophobic confinement. The observations show that the nanoconfined water at room temperature forms 'square ice'--a phase having symmetry qualitatively different from the conventional tetrahedral geometry of hydrogen bonding between water molecules. Square ice has a high packing density with a lattice constant of 2.83 Å and can assemble in bilayer and trilayer crystallites. Molecular dynamics simulations indicate that square ice should be present inside hydrophobic nanochannels independently of their exact atomic nature.

  8. Square ice in graphene nanocapillaries

    NASA Astrophysics Data System (ADS)

    Algara-Siller, G.; Lehtinen, O.; Wang, F. C.; Nair, R. R.; Kaiser, U.; Wu, H. A.; Geim, A. K.; Grigorieva, I. V.

    2015-03-01

    Bulk water exists in many forms, including liquid, vapour and numerous crystalline and amorphous phases of ice, with hexagonal ice being responsible for the fascinating variety of snowflakes. Much less noticeable but equally ubiquitous is water adsorbed at interfaces and confined in microscopic pores. Such low-dimensional water determines aspects of various phenomena in materials science, geology, biology, tribology and nanotechnology. Theory suggests many possible phases for adsorbed and confined water, but it has proved challenging to assess its crystal structure experimentally. Here we report high-resolution electron microscopy imaging of water locked between two graphene sheets, an archetypal example of hydrophobic confinement. The observations show that the nanoconfined water at room temperature forms `square ice'--a phase having symmetry qualitatively different from the conventional tetrahedral geometry of hydrogen bonding between water molecules. Square ice has a high packing density with a lattice constant of 2.83 Å and can assemble in bilayer and trilayer crystallites. Molecular dynamics simulations indicate that square ice should be present inside hydrophobic nanochannels independently of their exact atomic nature.

  9. A Method for Calculating the Heat Required for Windshield Thermal Ice Prevention Based on Extensive Flight Tests in Natural Icing Conditions

    NASA Technical Reports Server (NTRS)

    Jones, Alun R; Holdaway, George H; Steinmetz, Charles P

    1947-01-01

    An equation is presented for calculating the heat flow required from the surface of an internally heated windshield in order to prevent the formation of ice accretions during flight in specified icing conditions. To ascertain the validity of the equation, comparison is made between calculated values of the heat required and measured values obtained for test windshields in actual flights in icing conditions. The test windshields were internally heated and provided data applicable to two common types of windshield configurations; namely the V-type and the type installed flush with the fuselage contours. These windshields were installed on a twin-engine cargo airplane and the icing flights were conducted over a large area of the United States during the winters of 1945-46 and 1946-47. In addition to the internally heated windshield investigation, some test data were obtained for a windshield ice-prevention system in which heated air was discharged into the windshield boundary layer. The general conclusions resulting from this investigation are as follows: 1) The amount of heat required for the prevention of ice accretions on both flush- and V-type windshields during flight in specified icing conditions can be calculated with a degree of accuracy suitable for design purposes. 2) A heat flow of 2000 to 2500 Btu per hour per square foot is required for complete and continuous protection of a V-type windshield in fight at speeds up to 300 miles per hour in a moderate cumulus icing condition. For the same degree of protection and the same speed range, a value of 1000 Btu per hour per square foot suffices in a moderate stratus icing condition. 3) A heat supply of 1000 Btu per hour per square foot is adequate for a flush windshield located well aft of the fuselage stagnation region, at speeds up to 300 miles per hour, for flight in both stratus and moderate cumulus icing conditions. 4) The external air discharge system of windshield thermal ice prevention is thermally

  10. The Rapidly Diminishing Arctic ice Cover and its Potential Impact on Navy Operational Considerations

    NASA Astrophysics Data System (ADS)

    Muench, R. D.; Conlon, D.; Lamb, D.

    2001-12-01

    Observations made from U.S. Navy Fleet submarines during the 1990s have revealed a dramatic decrease in thickness, when compared to historical values, of the central Arctic Ocean pack ice cover. Estimates of this decrease have been as high as 40%. Remote sensing observations have shown a coincident decrease in the areal extent of the pack. The areal decrease has been especially apparent during winter. The overall loss of ice appears to have accelerated over the past decade, raising the possibility that the Northwest Passage and the Northern Sea Route may become seasonally navigable on a regular basis in the coming decade. The ice loss has been most evident in the peripheral seas and continental shelf areas. For example, during winter 2000-2001 the Bering Sea was effectively ice-free, with strong and immediate impacts on the surrounding indigenous populations. Lessening of the peripheral pack ice cover will presumably, lead to accelerated development of the resource-rich regions that surround the deep, central Arctic Ocean basin. This raises potential issues with respect to national security and commercial interests, and has implicit strategic concerns for the Navy. The timeline for a significantly navigable Arctic may extend decades into the future; however, operational requirements must be identified in the nearer term to ensure that the necessary capabilities exist when future Arctic missions do present themselves. A first step is to improve the understanding of the coupled atmosphere/ice/ocean system. Current environmental measurement and prediction, including Arctic weather and ice prediction, shallow water acoustic performance prediction, dynamic ocean environmental changes and data to support navigation is inadequate to support sustained naval operations in the Arctic. A new focus on data collection is required in order to measure, map, monitor and model Arctic weather, ice and oceanographic conditions.

  11. Oil and ice in the arctic ocean: possible large-scale interactions.

    PubMed

    Campbell, W J; Martin, S

    1973-07-06

    The diffusion and transport mechanisms generated by the pack ice dynamics of the Beaufort Sea, combined with the slow rate of biodegradation of oil under Arctic conditions, would combine to diffuse an oil spill over the sea and eventually deposit the oil on the ice surface, where it would lower the natural albedo over a large area.

  12. A Decade of Arctic Sea Ice Thickness Change from Airborne and Satellite Altimetry (Invited)

    NASA Astrophysics Data System (ADS)

    Farrell, S. L.; Richter-Menge, J.; Kurtz, N. T.; McAdoo, D. C.; Newman, T.; Zwally, H.; Ruth, J.

    2013-12-01

    Altimeters on both airborne and satellite platforms provide direct measurements of sea ice freeboard from which sea ice thickness may be calculated. Satellite altimetry observations of Arctic sea ice from ICESat and CryoSat-2 indicate a significant decline in ice thickness, and volume, over the last decade. During this time the ice pack has experienced a rapid change in its composition, transitioning from predominantly thick, multi-year ice to thinner, increasingly seasonal ice. We will discuss the regional trends in ice thickness derived from ICESat and IceBridge altimetry between 2003 and 2013, contrasting observations of the multi-year ice pack with seasonal ice zones. ICESat ceased operation in 2009, and the final, reprocessed data set became available recently. We extend our analysis to April 2013 using data from the IceBridge airborne mission, which commenced operations in 2009. We describe our current efforts to more accurately convert from freeboard to ice thickness, with a modified methodology that corrects for range errors, instrument biases, and includes an enhanced treatment of snow depth, with respect to ice type. With the planned launch by NASA of ICESat-2 in 2016 we can expect continuity of the sea ice thickness time series through the end of this decade. Data from the ICESat-2 mission, together with ongoing observations from CryoSat-2, will allow us to understand both the decadal trends and inter-annual variability in the Arctic sea ice thickness record. We briefly present the status of planned ICESat-2 sea ice data products, and demonstrate the utility of micro-pulse, photon-counting laser altimetry over sea ice.

  13. Testing and Failure Mechanisms of Ice Phase Change Material Heat Exchangers

    NASA Technical Reports Server (NTRS)

    Leimkuehler, Thomas O.; Stephan, Ryan A.; Hawkins-Reynolds, Ebony

    2010-01-01

    Phase change materials (PCM) may be useful for thermal control systems that involve cyclical heat loads or cyclical thermal environments such as Low Earth Orbit (LEO) and Low Lunar Orbit (LLO). Thermal energy can be stored in the PCM during peak heat loads or in adverse thermal environments. The stored thermal energy can then be released later during minimum heat loads or in more favorable thermal environments. One advantage that PCM s have over evaporators in this scenario is that they do not use a consumable. The use of water as a PCM rather than the more traditional paraffin wax has the potential for significant mass reduction since the latent heat of formation of water is approximately 70% greater than that of wax. One of the potential drawbacks of using ice as a PCM is its potential to rupture its container as water expands upon freezing. In order to develop a space qualified ice PCM heat exchanger, failure mechanisms must first be understood. Therefore, a methodical experimental investigation has been undertaken to demonstrate and document specific failure mechanisms due to ice expansion in the PCM. A number of ice PCM heat exchangers were fabricated and tested. Additionally, methods for controlling void location in order to reduce the risk of damage due to ice expansion were investigated. This paper presents the results of testing that occurred from March through September of 2010 and builds on testing that occurred during the previous year.

  14. Impacts of Organic Macromolecules, Chlorophyll and Soot on Arctic Sea Ice

    NASA Astrophysics Data System (ADS)

    Ogunro, O. O.; Wingenter, O. W.; Elliott, S.; Flanner, M.; Dubey, M. K.

    2014-12-01

    Recent intensification of Arctic amplification can be strongly connected to positive feedback relating black carbon deposition to sea ice surface albedo. In addition to soot deposition on the ice and snow pack, ice algal chlorophyll is likely to compete as an absorber and redistributor of energy. Hence, solar radiation absorption by chlorophyll and some components of organic macromolecules in/under the ice column is currently being examined to determine the level of influence on predicted rate of ice loss. High amounts of organic macromolecules and chlorophyll are produced in global sea ice by the bottom microbial community and also in vertically distributed layers where substantial biological activities take place. Brine channeling in columnar ice can allow for upward flow of nutrients which leads to greater primary production in the presence of moderate light. Modeling of the sea-ice processes in tandem with experiments and field observations promises rapid progress in enhancing Arctic ice predictions. We are designing and conducting global climate model experiments to determine the impact of organic macromolecules and chlorophyll on Arctic sea ice. Influences on brine network permeability and radiation/albedo will be considered in this exercise. Absorption by anthropogenic materials such as soot and black carbon will be compared with that of natural pigments. We will indicate areas of soot and biological absorption dominance in the sense of single scattering, then couple into a full radiation transfer scheme to attribute the various contributions to polar climate change amplification. The work prepares us to study more traditional issues such as chlorophyll warming of the pack periphery and chemical effects of the flow of organics from ice internal communities. The experiments started in the Arctic will broaden to include Antarctic sea ice and shelves. Results from the Arctic simulations will be presented.

  15. Bacterial activity in sea ice and open water of the Weddell Sea, Antarctica: A microautoradiographic study.

    PubMed

    Grossmann, S

    1994-07-01

    Metabolic activity of bacteria was investigated in open water, newly forming sea ice, and successive stages of pack ice in the Weddell Sea. Microautoradiography, using [(3)H]leucine as substrate, was compared with incorporation rates of [(3)H]leucine into proteins. Relation of [(3)H]leucine incorporation to the biomass of active bacteria provides information about changes of specific metabolic activity of cells. During a phytoplankton bloom in an ice-free, stratified water column, total numbers of bacteria in the euphotic zone averaged 2.3 × 10(5) ml(-1), but only about 13% showed activity via leucine uptake. Growth rate of the active bacteria was estimated as 0.3-0.4 days(-1). Total cell concentration of bacteria in 400 m depth was 6.6 × 10(4) ml(-1). Nearly 50% of these cells were active, although biomass production and specific growth rate were only about one-tenth that of the surface populations. When sea ice was forming in high concentrations of phytoplankton, bacterial biomass in the newly formed ice was 49.1 ng C ml(-1), exceeding that in open water by about one order of magnitude. Attachment of large bacteria to algal cells seems to cause their enrichment in the new ice, since specific bacterial activity was reduced during ice formation, and enrichment of bacteria was not observed when ice formed at low algal concentration. During growth of pack ice, biomass of bacteria increased within the brine channel system. Specific activity was still reduced at these later stages of ice development, and percentages of active cells were as low as 3-5%. In old, thick pack ice, bacterial activity was high and about 30% of cells were active. However, biomass-specific activity of bacteria remained significantly lower than that in open water. It is concluded that bacterial assemblages different to those of open water developed within the ice and were dominated by bacteria with lower average metabolic activity than those of ice-free water.

  16. Multiyear ice transport and small scale sea ice deformation near the Alaska coast measured by air-deployable Ice Trackers

    NASA Astrophysics Data System (ADS)

    Mahoney, A. R.; Kasper, J.; Winsor, P.

    2015-12-01

    Highly complex patterns of ice motion and deformation were captured by fifteen satellite-telemetered GPS buoys (known as Ice Trackers) deployed near Barrow, Alaska, in spring 2015. Two pentagonal clusters of buoys were deployed on pack ice by helicopter in the Beaufort Sea between 20 and 80 km offshore. During deployment, ice motion in the study region was effectively zero, but two days later the buoys captured a rapid transport event in which multiyear ice from the Beaufort Sea was flushed into the Chukchi Sea. During this event, westward ice motion began in the Chukchi Sea and propagated eastward. This created new openings in the ice and led to rapid elongation of the clusters as the westernmost buoys accelerated away from their neighbors to the east. The buoys tracked ice velocities of over 1.5 ms-1, with fastest motion occurring closest to the coast indicating strong current shear. Three days later, ice motion reversed and the two clusters became intermingled, rendering divergence calculations based on the area enclosed by clusters invalid. The data show no detectable difference in velocity between first year and multiyear ice floes, but Lagrangian timeseries of SAR imagery centered on each buoy show that first year ice underwent significant small-scale deformation during the event. The five remaining buoys were deployed by local residents on prominent ridges embedded in the landfast ice within 16 km of Barrow in order to track the fate of such features after they detached from the coast. Break-up of the landfast ice took place over a period of several days and, although the buoys each initially followed a similar eastward trajectory around Point Barrow into the Beaufort Sea, they rapidly dispersed over an area more than 50 km across. With rapid environmental and socio-economic change in the Arctic, understanding the complexity of nearshore ice motion is increasingly important for predict future changes in the ice and the tracking ice-related hazards

  17. 77 FR 1591 - Energy Conservation Program: Test Procedure for Automatic Commercial Ice Makers

    Federal Register 2010, 2011, 2012, 2013, 2014

    2012-01-11

    .... Establishment of a Metric for Potable Water Used to Produce Ice 6. Standardization of Water Hardness for Measurement of Potable Water Used in Making Ice 7. Testing of Batch Type Ice Makers at the Highest Purge..., AHRI Standard 810 with Addendum 1. This addendum revised the definition of ``potable water use rate...

  18. Modeling Sea Ice Trajectories for Oil Spill Tracking.

    DTIC Science & Technology

    1981-06-01

    is compared with sea ice motions observed during the AIDJEX main field experiment in the Beaufort Sea from April 1975 to February 1976. The average ...more recently grown on leads formed as the floes fracture and divide. The large-scale average thickness of the pack ice is roughly 3 m. As an...opposite extreme, during the summer when air temperatures rise above freezing, melting and offshore winds combine to form an approximately 300-km-wide swath

  19. Peopling of the high Arctic - induced by sea ice?

    NASA Astrophysics Data System (ADS)

    Funder, Svend

    2010-05-01

    'We travelled in the winter after the return of daylight and did not go into fixed camp until spring, when the ice broke up. There was good hunting on the way, seals, beluga, walrus, bear.' (From Old Merkrusârk's account of his childhood's trek from Baffin Island to Northwest Greenland, told to Knud Rasmussen on Saunders Island in 1904) Five thousand years ago people moving eastwards from Beringia spread over the barrens of the Canadian high Arctic. This was the first of three waves of prehistoric Arctic 'cultures', which eventually reached Greenland. The passage into Greenland has to go through the northernmost and most hostile part of the country with a 5 month Polar night, and to understand this extraordinary example of human behaviour and endurance, it has been customary to invoke a more favourable (warmer) climate. This presentation suggests that land-fast sea ice, i.e. stationary sea ice anchored to the coast, is among the most important environmental factors behind the spread of prehistoric polar cultures. The ice provides the road for travelling and social communion - and access to the most important source of food, the ocean. In the LongTerm Project (2006 and 2007) we attempted to establish a Holocene record for sea ice variations along oceanic coasts in northernmost Greenland. Presently the coasts north of 80° N are beleaguered by year-round sea ice - for ten months this is land-fast ice, and only for a period in the stormy autumn months are the coasts exposed to pack-ice. This presentation Land-fast ice - as opposed to pack-ice - is a product of local temperatures, but its duration over the year, and especially into the daylight season, is also conditioned by other factors, notably wind strength. In the geological record we recognize long lasting land-fast ice by two absences: absence of traces of wave action (no beach formation), which, however, can also be a result of pack-ice along the coast; - and absence of driftwood on the shore (land-fast ice

  20. Under the Sea Ice: Exploration of the Relationships Between Sea Ice Patterns and Foraging Movements of a Marine Predator in East Antarctica.

    NASA Astrophysics Data System (ADS)

    Labrousse, S.; Sallee, J. B.; Fraser, A. D.; Massom, R. A.; Reid, P.; Sumner, M.; Guinet, C.; Harcourt, R.; Bailleul, F.; Hindell, M.; Charrassin, J. B.

    2016-02-01

    Investigating ecological relationships between top predators and their environment is essential to understand the response of marine ecosystems to climate variability. Specifically, variability and changes in sea ice, which is known as an important habitat for marine ecosystems, presents complex patterns in East Antarctic. The impact for ecosystems of such changes of their habitat is however still unknown. Acting as an ecological double-edged sword, sea ice can impede access to marine resources while harboring a rich ecosystem during winter. Here, we investigated which type of sea ice habitat is used by male and female southern elephant seals during winter and examine if and how the spatio-temporal variability of sea ice concentration (SIC) influence their foraging strategies. We also examined over a 10 years time-series the impact of SIC and sea ice advance anomaly on foraging activity. To do this, we studied 46 individuals equipped with Satellite linked data recorders between 2004 and 2014, undertaking post-moult trips in winter from Kerguelen to the peri-Antarctic shelf. The general patterns of sea ice use by males and females are clearly distinct; while females tended to follow the sea ice edge as it extended northward, males remained on the continental shelf. Female foraging activity was higher in late autumn in the outer part of the pack ice in concentrated SIC and spatially stable. They remained in areas of variable SIC over time and low persistence. The seal hunting time, a proxy of foraging activity inferred from the diving behaviour, was much higher during earlier advance of sea ice over female time-series. The females were possibly taking advantage of the ice algal autumn bloom sustaining krill and an under ice ecosystem without being trapped in sea ice. Males foraging activity increased when they remained deep inside sea ice over the shelf using variable SIC in time and space, presumably in polynyas or flaw leads between fast and pack ice. This strategy

  1. Inferring Firn Permeability from Pneumatic Testing: A Case Study on the Greenland Ice Sheet

    NASA Astrophysics Data System (ADS)

    Sommers, Aleah N.; Rajaram, Harihar; Weber, Eliezer P.; MacFerrin, Michael J.; Colgan, William T.; Stevens, C. Max

    2017-03-01

    Across the accumulation zone of the Greenland ice sheet, summer temperatures can be sufficiently warm to cause widespread melting, as was the case in July 2012 when the entire ice sheet experienced a brief episode of enhanced surface ablation. The resulting meltwater percolates into the firn and refreezes, to create ice lenses and layers within the firn column. This is an important process to consider when estimating the surface mass balance of the ice sheet. The rate of meltwater percolation depends on the permeability of the firn, a property that is not well constrained in the presence of refrozen ice layers and lenses. We present a novel, inexpensive method for measuring in-situ firn permeability using pneumatic testing, a well-established technique used in environmental engineering and hydrology. To illustrate the capabilities of this method, we estimate both horizontal and vertical permeability from pilot tests at six sites on the Greenland ice sheet: KAN-U, DYE-2, EKT, NASA-SE, Saddle, and EastGRIP. These sites cover a range of conditions from mostly dry firn (EastGRIP), to firn with several ice layers and lenses from refrozen meltwater (Saddle, NASA-SE, EKT), to firn with extensive ice layers (DYE-2 and KAN-U). The estimated permeability in firn without refrozen ice layers at EastGRIP agrees well with the range previously reported using an air permeameter to measure permeability through firn core samples at Summit, Greenland. At sites with ice lenses or layers, we find high degrees of anisotropy, with vertical permeability much lower than horizontal permeability. Pneumatic testing is a promising and low-cost technique for measuring firn permeability, particularly as meltwater production increases in the accumulation zone and ice layers and lenses from refrozen melt layers become more prevalent. In these initial proof-of-concept tests, the estimated permeabilities represent effective permeability at the meter scale. With appropriately higher vacuum pressures

  2. Field Results for an Arctic AUV Designed for Characterizing Circulation and Ice Thickness

    NASA Astrophysics Data System (ADS)

    Bellingham, J. G.; Kirkwood, W. J.; Tervalon, N.; Cokelet, E.; Thomas, H.; Sibenac, M.; Gashler, D.; McEwen, R.; Henthorn, R.; Shane, F.; Osborn, D. J.; Johnson, K.; Overland, J.; Stein, P.; Bahlavouni, A.; Anderson, D.

    2002-12-01

    An Autonomous Underwater Vehicle designed for operation at high latitudes and under ice completed its first Arctic field tests from the USCGC Healy in fall of 2001. The ALTEX AUV has been under development since 1998, and is being created to provide: unprecedented endurance, ability to navigate at high latitudes, a depth rating of 1500 to 4500 meters depending on payload, and the capability to relay data through the ice to satellites via data buoys. The AUV's initial applications are focused on tracking the warm Atlantic Layer inflow - the primary source of seawater to the Arctic Ocean. Consequently the primary payloads are twin pumped CTD systems. Oxygen and nitrate sensors provide the ability to use NO as a tracer. An ice profiling sonar allows the AUV to estimate the ice thickness in real-time and is designed to generate high quality post-processed ice draft data comparable to that collected through the SCICEX program. The experiments in October aboard the USCGC Healy generated numerous water column and under-ice data sets. Traditional ship-based CTD operations were used to provide a comparison data set for AUV water column measurements. The post-processed ice draft results show reasonable ice profiles and have the potential, when combined with other science data collected, to shed some additional light on upper water column processes in ice-covered regions. Cruise results include: operating the AUV from the USCGC Healy in the ice pack, demonstrating inertial navigation system performance, obtaining oceanographic sections with the AUV, obtaining ice draft measurements with an AUV born sonar, and testing the data-buoy system. This work is supported by the National Science Foundation under grant NSF-OPP 9910290. The Packard Foundation and the Office of Naval Research have also provided support. The project was initiated under the National Ocean Partnership Program under contract N00014-98-1-0814.

  3. Results of a low power ice protection system test and a new method of imaging data analysis

    NASA Technical Reports Server (NTRS)

    Shin, Jaiwon; Bond, Thomas H.; Mesander, Geert A.

    1992-01-01

    Tests were conducted on a BF Goodrich De-Icing System's Pneumatic Impulse Ice Protection (PIIP) system in the NASA Lewis Icing Research Tunnel (IRT). Characterization studies were done on shed ice particle size by changing the input pressure and cycling time of the PIIP de-icer. The shed ice particle size was quantified using a newly developed image software package. The tests were conducted on a 1.83 m (6 ft) span, 0.53 m (221 in) chord NACA 0012 airfoil operated at a 4 degree angle of attack. The IRT test conditions were a -6.7 C (20 F) glaze ice, and a -20 C (-4 F) rime ice. The ice shedding events were recorded with a high speed video system. A detailed description of the image processing package and the results generated from this analytical tool are presented.

  4. Testing and Failure Mechanisms of Ice Phase Change Material Heat Exchangers

    NASA Technical Reports Server (NTRS)

    Leimkuehler, Thomas O.; Stephan, Ryan A.; Hawkins-Reynolds, Ebony

    2011-01-01

    Phase change materials (PCM) may be useful for thermal control systems that involve cyclical heat loads or cyclical thermal environments such as specific spacecraft orientations in Low Earth Orbit (LEO) and low beta angle Low Lunar Orbit (LLO). Thermal energy can be stored in the PCM during peak heat loads or in adverse thermal environments. The stored thermal energy can then be released later during minimum heat loads or in more favorable thermal environments. One advantage that PCM s have over evaporators in this scenario is that they do not use a consumable. The use of water as a PCM rather than the more traditional paraffin wax has the potential for significant mass reduction since the latent heat of formation of water is approximately 70% greater than that of wax. One of the potential drawbacks of using ice as a PCM is its potential to rupture its container as water expands upon freezing. In order to develop a space qualified ice PCM heat exchanger, failure mechanisms must first be understood. Therefore, a methodical experimental investigation has been undertaken to demonstrate and document specific failure mechanisms due to ice expansion in the PCM. A number of ice PCM heat exchangers were fabricated and tested. Additionally, methods for controlling void location in order to reduce the risk of damage due to ice expansion were investigated. This paper presents the results of testing that occurred from March through September of 2010 and builds on testing that occurred during the previous year.

  5. Snow depth evolution on sea ice from Snow Buoy measurement

    NASA Astrophysics Data System (ADS)

    Nicolaus, M.; Arndt, S.; Hendricks, S.; Hoppmann, M.; Katlein, C.; König-Langlo, G.; Nicolaus, A.; Rossmann, H. L.; Schiller, M.; Schwegmann, S.; Langevin, D.

    2016-12-01

    Snow cover is an Essential Climate Variable. On sea ice, snow dominates the energy and momentum exchanges across the atmosphere-ice-ocean interfaces, and actively contributes to sea ice mass balance. Yet, snow depth on sea ice is one of the least known and most difficult to observe parameters of the Arctic and Antarctic; mainly due to its exceptionally high spatial and temporal variability. In this study; we present a unique time series dataset of snow depth and air temperature evolution on Arctic and Antarctic sea ice recorded by autonomous instruments. Snow Buoys record snow depth with four independent ultrasonic sensors, increasing the reliability of the measurements and allowing for additional analyses. Auxiliary measurements include surface and air temperature, barometric pressure and GPS position. 39 deployments of such Snow Buoys were achieved over the last three years either on drifting pack ice, on landfast sea ice or on an ice shelf. Here we highlight results from two pairs of Snow Buoys installed on drifting pack ice in the Weddell Sea. The data reveals large regional differences in the annual cycle of snow depth. Almost no reduction in snow depth (snow melt) was observed in the inner and southern part of the Weddell Sea, allowing a net snow accumulation of 0.2 to 0.9 m per year. In contrast, summer snow melt close to the ice edge resulted in a decrease of about 0.5 m during the summer 2015/16. Another array of eight Snow Buoys was installed on central Arctic sea ice in September 2015. Their air temperature record revealed exceptionally high air temperatures in the subsequent winter, even exceeding the melting point but with almost no impact on snow depth at that time. Future applications of Snow Buoys on Arctic and Antarctic sea ice will allow additional inter-annual studies of snow depth and snow processes, e.g. to support the development of snow depth data products from airborne and satellite data or though assimilation in numerical models.

  6. Weddell-Scotia sea marginal ice zone observations from space, October 1984

    NASA Technical Reports Server (NTRS)

    Carsey, F. D.; Holt, B.; Martin, S.; Rothrock, D. A.; Mcnutt, L.

    1986-01-01

    Imagery from the Shuttle imaging radar-B experiment as well as other satellite and meteorological data are examined to learn more about the open sea ice margin of the Weddell-Scotia Seas region. At the ice edge, the ice forms into bandlike aggregates of small ice floes similar to those observed in the Bering Sea. The radar backscatter characteristics of these bands suggest that their upper surface is wet. Further into the pack, the radar imagery shows a transition to large floes. In the open sea, large icebergs and long surface gravity waves are discernable in the radar images.

  7. Icing Test Results on an Advanced Two-Dimensional High-Lift Multi-Element Airfoil

    NASA Technical Reports Server (NTRS)

    Shin, Jaiwon; Wilcox, Peter; Chin, Vincent; Sheldon, David

    1994-01-01

    An experimental study has been conducted to investigate ice accretions on a high-lift, multi-element airfoil in the Icing Research Tunnel at the NASA Lewis Research Center. The airfoil is representative of an advanced transport wing design. The experimental work was conducted as part of a cooperative program between McDonnell Douglas Aerospace and the NASA Lewis Research Center to improve current understanding of ice accretion characteristics on the multi-element airfoil. The experimental effort also provided ice shapes for future aerodynamic tests at flight Reynolds numbers to ascertain high-lift performance effects. Ice shapes documented for a landing configuration over a variety of icing conditions are presented along with analyses.

  8. Dynamic Wind-Tunnel Testing of a Sub-Scale Iced S-3B Viking

    NASA Technical Reports Server (NTRS)

    Lee, Sam; Barnhart, Billy; Ratvasky, Thomas P.

    2012-01-01

    The effect of ice accretion on a 1/12-scale complete aircraft model of S-3B Viking was studied in a rotary-balance wind tunnel. Two types of ice accretions were considered: ice protection system failure shape and runback shapes that form downstream of the thermal ice protection system. The results showed that the ice shapes altered the stall characteristics of the aircraft. The ice shapes also reduced the control surface effectiveness, but mostly near the stall angle of attack. There were some discrepancies with the data with the flaps deflected that were attributed to the low Reynolds number of the test. Rotational and forced-oscillation studies showed that the effects of ice were mostly in the longitudinal forces, and the effects on the lateral forces were relatively minor.

  9. CICE, The Los Alamos Sea Ice Model

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Hunke, Elizabeth; Lipscomb, William; Jones, Philip

    The Los Alamos sea ice model (CICE) is the result of an effort to develop a computationally efficient sea ice component for a fully coupled atmosphere–land–ocean–ice global climate model. It was originally designed to be compatible with the Parallel Ocean Program (POP), an ocean circulation model developed at Los Alamos National Laboratory for use on massively parallel computers. CICE has several interacting components: a vertical thermodynamic model that computes local growth rates of snow and ice due to vertical conductive, radiative and turbulent fluxes, along with snowfall; an elastic-viscous-plastic model of ice dynamics, which predicts the velocity field of themore » ice pack based on a model of the material strength of the ice; an incremental remapping transport model that describes horizontal advection of the areal concentration, ice and snow volume and other state variables; and a ridging parameterization that transfers ice among thickness categories based on energetic balances and rates of strain. It also includes a biogeochemical model that describes evolution of the ice ecosystem. The CICE sea ice model is used for climate research as one component of complex global earth system models that include atmosphere, land, ocean and biogeochemistry components. It is also used for operational sea ice forecasting in the polar regions and in numerical weather prediction models.« less

  10. Western Ross Sea and McMurdo Sound Ice Forecasting Guide.

    DTIC Science & Technology

    1975-06-01

    areal ice distribution and follow the sane historical proqression of pack disintergration . This technique assumes that environmental conditions...30-day) are based on historical ice data which cxnbine averaae disintergration rates as well as averace wind and current drift. Iong-range wind...original 2 to 3 okta area and its new cnfiguration remains the same, the products of ocnoentrations and widths at the verifying time must equal the

  11. Prediction of ice accretion on a swept NACA 0012 airfoil and comparisons to flight test results

    NASA Technical Reports Server (NTRS)

    Reehorst, Andrew L.

    1992-01-01

    In the winter of 1989-90, an icing research flight project was conducted to obtain swept wing ice accretion data. Utilizing the NASA Lewis Research Center's DHC-6 DeHavilland Twin Otter aircraft, research flights were made into known icing conditions in Northeastern Ohio. The icing cloud environment and aircraft flight data were measured and recorded by an onboard data acquisition system. Upon entry into the icing environment, a 24 inch span, 15 inch chord NACA 0012 airfoil was extended from the aircraft and set to the desired sweep angle. After the growth of a well defined ice shape, the airfoil was retracted into the aircraft cabin for ice shape documentation. The ice accretions were recorded by ice tracings and photographs. Ice accretions were mostly of the glaze type and exhibited scalloping. The ice was accreted at sweep angles of 0, 30, and 45 degrees. A 3-D ice accretion prediction code was used to predict ice profiles for five selected flight test runs, which include sweep angle of zero, 30, and 45 degrees. The code's roughness input parameter was adjusted for best agreement. A simple procedure was added to the code to account for 3-D ice scalloping effects. The predicted ice profiles are compared to their respective flight test counterparts. This is the first attempt to predict ice profiles on swept wings with significant scalloped ice formations.

  12. Observations and analyses of an intense waves-in-ice event in the Sea of Okhotsk

    NASA Astrophysics Data System (ADS)

    Marko, John R.

    2003-09-01

    Ice draft, ice velocity, ice concentration, and current profile data gathered at an array of eight continental shelf monitoring sites east of Sakhalin Island were analyzed in conjunction with regional meteorological data to document and explain intense wave occurrences several hundred kilometers inside the Sea of Okhotsk ice pack. The studied event was associated with the 19-21 March 1998 passage of an intense cyclone, which produced waves with amplitudes in excess of 1 m at the most offshore monitoring location. The relatively monochromatic character of the waves allowed extraction of wave intensity time series from ice draft time series data. Spatial and temporal variations in these data were used to establish directions and speeds of wave energy propagation for comparisons with an earlier interpretation [, 1988] of an Antarctic intense waves-in-ice event. It was concluded that although both events are compatible with a two-stage process in which initially slowly advancing wave activity increases subsequent ice cover wave transmissivity, the first stage of the Sea of Okhotsk event was not explicable in terms of the static stress-induced changes in the waves-in-ice dispersion relationship proposed by Liu and Mollo-Christensen. An alternative explanation is offered that eschews the linkage between wave group velocities and the observed slow rates of wave energy propagation and attributes the subsequent transition to more normal wave propagation behavior to ice pack divergence.

  13. Arctic landfast sea ice

    NASA Astrophysics Data System (ADS)

    Konig, Christof S.

    Landfast ice is sea ice which forms and remains fixed along a coast, where it is attached either to the shore, or held between shoals or grounded icebergs. Landfast ice fundamentally modifies the momentum exchange between atmosphere and ocean, as compared to pack ice. It thus affects the heat and freshwater exchange between air and ocean and impacts on the location of ocean upwelling and downwelling zones. Further, the landfast ice edge is essential for numerous Arctic mammals and Inupiat who depend on them for their subsistence. The current generation of sea ice models is not capable of reproducing certain aspects of landfast ice formation, maintenance, and disintegration even when the spatial resolution would be sufficient to resolve such features. In my work I develop a new ice model that permits the existence of landfast sea ice even in the presence of offshore winds, as is observed in mature. Based on viscous-plastic as well as elastic-viscous-plastic ice dynamics I add tensile strength to the ice rheology and re-derive the equations as well as numerical methods to solve them. Through numerical experiments on simplified domains, the effects of those changes are demonstrated. It is found that the modifications enable landfast ice modeling, as desired. The elastic-viscous-plastic rheology leads to initial velocity fluctuations within the landfast ice that weaken the ice sheet and break it up much faster than theoretically predicted. Solving the viscous-plastic rheology using an implicit numerical method avoids those waves and comes much closer to theoretical predictions. Improvements in landfast ice modeling can only verified in comparison to observed data. I have extracted landfast sea ice data of several decades from several sources to create a landfast sea ice climatology that can be used for that purpose. Statistical analysis of the data shows several factors that significantly influence landfast ice distribution: distance from the coastline, ocean depth, as

  14. Modern Airfoil Ice Accretions

    NASA Technical Reports Server (NTRS)

    Addy, Harold E., Jr.; Potapczuk, Mark G.; Sheldon, David W.

    1997-01-01

    This report presents results from the first icing tests performed in the Modem Airfoils program. Two airfoils have been subjected to icing tests in the NASA Lewis Icing Research Tunnel (IRT). Both airfoils were two dimensional airfoils; one was representative of a commercial transport airfoil while the other was representative of a business jet airfoil. The icing test conditions were selected from the FAR Appendix C envelopes. Effects on aerodynamic performance are presented including the effects of varying amounts of glaze ice as well as the effects of approximately the same amounts of glaze, mixed, and rime ice. Actual ice shapes obtained in these tests are also presented for these cases. In addition, comparisons are shown between ice shapes from the tests and ice shapes predicted by the computer code, LEWICE for similar conditions. Significant results from the tests are that relatively small amounts of ice can have nearly as much effect on airfoil lift coefficient as much greater amounts of ice and that glaze ice usually has a more detrimental effect than either rime or mixed ice. LEWICE predictions of ice shapes, in general, compared reasonably well with ice shapes obtained in the IRT, although differences in details of the ice shapes were observed.

  15. Europa Ice Rafts

    NASA Technical Reports Server (NTRS)

    1997-01-01

    This high resolution image shows the ice-rich crust of Europa, one of the moons of Jupiter. Seen here are crustal plates ranging up to 13 kilometers (8 miles) across, which have been broken apart and 'rafted' into new positions, superficially resembling the disruption of pack-ice on polar seas during spring thaws on Earth. The size and geometry of these features suggest that motion was enabled by ice-crusted water or soft ice close to the surface at the time of disruption.

    The area shown is about 34 kilometers by 42 kilometers (21 miles by 26 miles), centered at 9.4 degrees north latitude, 274 degrees west longitude, and the resolution is 54 meters (59 yards). This picture was taken by the Solid State Imaging system on board the Galileo spacecraft on February 20, 1997, from a distance of 5,340 kilometers (3,320 miles) during the spacecraft's close flyby of Europa.

    The Jet Propulsion Laboratory, Pasadena, CA, manages the mission for NASA's Office of Space Science, Washington D.C. This image and other images and data received from Galileo are posted on the World Wide Web Galileo mission home page at: http://galileo.jpl.nasa.gov.

  16. Sea-ice eukaryotes of the Gulf of Finland, Baltic Sea, and evidence for herbivory on weakly shade-adapted ice algae.

    PubMed

    Majaneva, Markus; Blomster, Jaanika; Müller, Susann; Autio, Riitta; Majaneva, Sanna; Hyytiäinen, Kirsi; Nagai, Satoshi; Rintala, Janne-Markus

    2017-02-01

    To determine community composition and physiological status of early spring sea-ice organisms, we collected sea-ice, slush and under-ice water samples from the Baltic Sea. We combined light microscopy, HPLC pigment analysis and pyrosequencing, and related the biomass and physiological status of sea-ice algae with the protistan community composition in a new way in the area. In terms of biomass, centric diatoms including a distinct Melosira arctica bloom in the upper intermediate section of the fast ice, dinoflagellates, euglenoids and the cyanobacterium Aphanizomenon sp. predominated in the sea-ice sections and unidentified flagellates in the slush. Based on pigment analyses, the ice-algal communities showed no adjusted photosynthetic pigment pools throughout the sea ice, and the bottom-ice communities were not shade-adapted. The sea ice included more characteristic phototrophic taxa (49%) than did slush (18%) and under-ice water (37%). Cercozoans and ciliates were the richest taxon groups, and the differences among the communities arose mainly from the various phagotrophic protistan taxa inhabiting the communities. The presence of pheophytin a coincided with an elevated ciliate biomass and read abundance in the drift ice and with a high Eurytemora affinis read abundance in the pack ice, indicating that ciliates and Eurytemora affinis were grazing on algae. Copyright © 2016 Elsevier GmbH. All rights reserved.

  17. Microalgal photophysiology and macronutrient distribution in summer sea ice in the Amundsen and Ross Seas, Antarctica

    PubMed Central

    Fransson, Agneta; Currie, Kim; Wulff, Angela; Chierici, Melissa

    2018-01-01

    Our study addresses how environmental variables, such as macronutrients concentrations, snow cover, carbonate chemistry and salinity affect the photophysiology and biomass of Antarctic sea-ice algae. We have measured vertical profiles of inorganic macronutrients (phosphate, nitrite + nitrate and silicic acid) in summer sea ice and photophysiology of ice algal assemblages in the poorly studied Amundsen and Ross Seas sectors of the Southern Ocean. Brine-scaled bacterial abundance, chl a and macronutrient concentrations were often high in the ice and positively correlated with each other. Analysis of photosystem II rapid light curves showed that microalgal cells in samples with high phosphate and nitrite + nitrate concentrations had reduced maximum relative electron transport rate and photosynthetic efficiency. We also observed strong couplings of PSII parameters to snow depth, ice thickness and brine salinity, which highlights a wide range of photoacclimation in Antarctic pack-ice algae. It is likely that the pack ice was in a post-bloom situation during the late sea-ice season, with low photosynthetic efficiency and a high degree of nutrient accumulation occurring in the ice. In order to predict how key biogeochemical processes are affected by future changes in sea ice cover, such as in situ photosynthesis and nutrient cycling, we need to understand how physicochemical properties of sea ice affect the microbial community. Our results support existing hypothesis about sea-ice algal photophysiology, and provide additional observations on high nutrient concentrations in sea ice that could influence the planktonic communities as the ice is retreating. PMID:29634756

  18. Quantification of Ice Accretions for Icing Scaling Evaluations

    NASA Technical Reports Server (NTRS)

    Ruff, Gary A.; Anderson, David N.

    2003-01-01

    The comparison of ice accretion characteristics is an integral part of aircraft icing research. It is often necessary to compare an ice accretion obtained from a flight test or numerical simulation to one produced in an icing wind tunnel or for validation of an icing scaling method. Traditionally, this has been accomplished by overlaying two-dimensional tracings of ice accretion shapes. This paper addresses the basic question of how to compare ice accretions using more quantitative methods. For simplicity, geometric characteristics of the ice accretions are used for the comparison. One method evaluated is a direct comparison of the percent differences of the geometric measurements. The second method inputs these measurements into a fuzzy inference system to obtain a single measure of the goodness of the comparison. The procedures are demonstrated by comparing ice shapes obtained in the Icing Research Tunnel at NASA Glenn Research Center during recent icing scaling tests. The results demonstrate that this type of analysis is useful in quantifying the similarity of ice accretion shapes and that the procedures should be further developed by expanding the analysis to additional icing data sets.

  19. Test results of Thermal Ice Cap prototype and final comments. Final report

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Burley, W.

    1982-01-01

    The design and testing of an insulating cover, Ice Cap, for an ice rink are described. The radio-controlled reel system which houses, deploys, and harvests the 17,000 square feet of insulating material is essential to the success of the cover. Photographs showing the use of the system are included. (MHR)

  20. Upper Ocean Evolution Across the Beaufort Sea Marginal Ice Zone from Autonomous Gliders

    NASA Astrophysics Data System (ADS)

    Lee, Craig; Rainville, Luc; Perry, Mary Jane

    2016-04-01

    The observed reduction of Arctic summertime sea ice extent and expansion of the marginal ice zone (MIZ) have profound impacts on the balance of processes controlling sea ice evolution, including the introduction of several positive feedback mechanisms that may act to accelerate melting. Examples of such feedbacks include increased upper ocean warming though absorption of solar radiation, elevated internal wave energy and mixing that may entrain heat stored in subsurface watermasses (e.g., the relatively warm Pacific Summer (PSW) and Atlantic (AW) waters), and elevated surface wave energy that acts to deform and fracture sea ice. Spatial and temporal variability in ice properties and open water fraction impact these processes. To investigate how upper ocean structure varies with changing ice cover, and how the balance of processes shift as a function of ice fraction and distance from open water, four long-endurance autonomous Seagliders occupied sections that extended from open water, through the marginal ice zone, deep into the pack during summer 2014 in the Beaufort Sea. Sections reveal strong fronts where cold, ice-covered waters meet waters that have been exposed to solar warming, and O(10 km) scale eddies near the ice edge. In the pack, Pacific Summer Water and a deep chlorophyll maximum form distinct layers at roughly 60 m and 80 m, respectively, which become increasingly diffuse as they progress through the MIZ and into open water. The isopynal layer between 1023 and 1024 kgm-3, just above the PSW, consistently thickens near the ice edge, likely due to mixing or energetic vertical exchange associated with strong lateral gradients in this region. This presentation will discuss the upper ocean variability, its relationship to sea ice extent, and evolution over the summer to the start of freeze up.

  1. Upper Ocean Evolution Across the Beaufort Sea Marginal Ice Zone from Autonomous Gliders

    NASA Astrophysics Data System (ADS)

    Lee, C.; Rainville, L.; Perry, M. J.

    2016-02-01

    The observed reduction of Arctic summertime sea ice extent and expansion of the marginal ice zone (MIZ) have profound impacts on the balance of processes controlling sea ice evolution, including the introduction of several positive feedback mechanisms that may act to accelerate melting. Examples of such feedbacks include increased upper ocean warming though absorption of solar radiation, elevated internal wave energy and mixing that may entrain heat stored in subsurface watermasses (e.g., the relatively warm Pacific Summer (PSW) and Atlantic (AW) waters), and elevated surface wave energy that acts to deform and fracture sea ice. Spatial and temporal variability in ice properties and open water fraction impact these processes. To investigate how upper ocean structure varies with changing ice cover, and how the balance of processes shift as a function of ice fraction and distance from open water, four long-endurance autonomous Seagliders occupied sections that extended from open water, through the marginal ice zone, deep into the pack during summer 2014 in the Beaufort Sea. Sections reveal strong fronts where cold, ice-covered waters meet waters that have been exposed to solar warming, and O(10 km) scale eddies near the ice edge. In the pack, Pacific Summer Water and a deep chlorophyll maximum form distinct layers at roughly 60 m and 80 m, respectively, which become increasingly diffuse as they progress through the MIZ and into open water. The isopynal layer between 1023 and 1024 kg m-3, just above the PSW, consistently thickens near the ice edge, likely due to mixing or energetic vertical exchange associated with strong lateral gradients in this region. This presentation will discuss the upper ocean variability, its relationship to sea ice extent, and evolution over the summer to the start of freeze up.

  2. Snow contribution to first-year and second-year Arctic sea ice mass balance north of Svalbard

    NASA Astrophysics Data System (ADS)

    Granskog, Mats A.; Rösel, Anja; Dodd, Paul A.; Divine, Dmitry; Gerland, Sebastian; Martma, Tõnu; Leng, Melanie J.

    2017-03-01

    The salinity and water oxygen isotope composition (δ18O) of 29 first-year (FYI) and second-year (SYI) Arctic sea ice cores (total length 32.0 m) from the drifting ice pack north of Svalbard were examined to quantify the contribution of snow to sea ice mass. Five cores (total length 6.4 m) were analyzed for their structural composition, showing variable contribution of 10-30% by granular ice. In these cores, snow had been entrained in 6-28% of the total ice thickness. We found evidence of snow contribution in about three quarters of the sea ice cores, when surface granular layers had very low δ18O values. Snow contributed 7.5-9.7% to sea ice mass balance on average (including also cores with no snow) based on δ18O mass balance calculations. In SYI cores, snow fraction by mass (12.7-16.3%) was much higher than in FYI cores (3.3-4.4%), while the bulk salinity of FYI (4.9) was distinctively higher than for SYI (2.7). We conclude that oxygen isotopes and salinity profiles can give information on the age of the ice and enables distinction between FYI and SYI (or older) ice in the area north of Svalbard.Plain Language SummaryThe role of snow in sea <span class="hlt">ice</span> mass balance is largely two fold. Firstly, it can slow down growth and melt due to its high insulation and high reflectance, but secondly it can actually contribute to sea <span class="hlt">ice</span> growth if the snow cover is turned into <span class="hlt">ice</span>. The latter is largely a consequence of high mass of snow on top of sea <span class="hlt">ice</span> that can push the surface of the sea <span class="hlt">ice</span> below sea level and seawater can flood the <span class="hlt">ice</span>. This mixture of seawater and snow can then freeze and add to the growth of sea <span class="hlt">ice</span>. This is very typical in the Antarctic but not believed to be so important in the Arctic. In this work we show, for the first time, that snow actually contributes significantly to the growth of Arctic sea <span class="hlt">ice</span>. This is likely a consequence of the thinning of the Arctic sea <span class="hlt">ice</span>. The conditions in the Arctic, with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140003875','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140003875"><span>Modeling Commercial Turbofan Engine <span class="hlt">Icing</span> Risk With <span class="hlt">Ice</span> Crystal Ingestion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jorgenson, Philip C. E.; Veres, Joseph P.</p> <p>2013-01-01</p> <p>The occurrence of <span class="hlt">ice</span> accretion within commercial high bypass aircraft turbine engines has been reported under certain atmospheric conditions. Engine anomalies have taken place at high altitudes that have been attributed to <span class="hlt">ice</span> crystal ingestion, partially melting, and <span class="hlt">ice</span> accretion on the compression system components. The result was degraded engine performance, and one or more of the following: loss of thrust control (roll back), compressor surge or stall, and flameout of the combustor. As <span class="hlt">ice</span> crystals are ingested into the fan and low pressure compression system, the increase in air temperature causes a portion of the <span class="hlt">ice</span> crystals to melt. It is hypothesized that this allows the <span class="hlt">ice</span>-water mixture to cover the metal surfaces of the compressor stationary components which leads to <span class="hlt">ice</span> accretion through evaporative cooling. <span class="hlt">Ice</span> accretion causes a blockage which subsequently results in the deterioration in performance of the compressor and engine. The focus of this research is to apply an engine <span class="hlt">icing</span> computational tool to simulate the flow through a turbofan engine and assess the risk of <span class="hlt">ice</span> accretion. The tool is comprised of an engine system thermodynamic cycle code, a compressor flow analysis code, and an <span class="hlt">ice</span> particle melt code that has the capability of determining the rate of sublimation, melting, and evaporation through the compressor flow path, without modeling the actual <span class="hlt">ice</span> accretion. A commercial turbofan engine which has previously experienced <span class="hlt">icing</span> events during operation in a high altitude <span class="hlt">ice</span> crystal environment has been <span class="hlt">tested</span> in the Propulsion Systems Laboratory (PSL) altitude <span class="hlt">test</span> facility at NASA Glenn Research Center. The PSL has the capability to produce a continuous <span class="hlt">ice</span> cloud which are ingested by the engine during operation over a range of altitude conditions. The PSL <span class="hlt">test</span> results confirmed that there was <span class="hlt">ice</span> accretion in the engine due to <span class="hlt">ice</span> crystal ingestion, at the same simulated altitude operating conditions as experienced previously in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840002650','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840002650"><span>Antartic sea <span class="hlt">ice</span>, 1973 - 1976: Satellite passive-microwave observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zwally, H. J.; Comiso, J. C.; Parkinson, C. L.; Campbell, W. J.; Carsey, F. D.; Gloersen, P.</p> <p>1983-01-01</p> <p>Data from the Electrically Scanning Microwave Radiometer (ESMR) on the Nimbus 5 satellite are used to determine the extent and distribution of Antarctic sea <span class="hlt">ice</span>. The characteristics of the southern ocean, the mathematical formulas used to obtain quantitative sea <span class="hlt">ice</span> concentrations, the general characteristics of the seasonal sea <span class="hlt">ice</span> growth/decay cycle and regional differences, and the observed seasonal growth/decay cycle for individual years and interannual variations of the <span class="hlt">ice</span> cover are discussed. The sea <span class="hlt">ice</span> data from the ESMR are presented in the form of color-coded maps of the Antarctic and the southern oceans. The maps show brightness temperatures and concentrations of <span class="hlt">pack</span> <span class="hlt">ice</span> averaged for each month, 4-year monthly averages, and month-to-month changes. Graphs summarizing the results, such as areas of sea <span class="hlt">ice</span> as a function of time in the various sectors of the southern ocean are included. The images demonstrate that satellite microwave data provide unique information on large-scale sea <span class="hlt">ice</span> conditions for determining climatic conditions in polar regions and possible global climatic changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCD.....6..505F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCD.....6..505F"><span>Quantification of ikaite in Antarctic sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, M.; Thomas, D. N.; Krell, A.; Nehrke, G.; Göttlicher, J.; Norman, L.; Riaux-Gobin, C.; Dieckmann, G. S.</p> <p>2012-02-01</p> <p>Calcium carbonate precipitation in sea <span class="hlt">ice</span> can increase pCO2 during precipitation in winter and decrease pCO2 during dissolution in spring. CaCO3 precipitation in sea <span class="hlt">ice</span> is thought to potentially drive significant CO2 uptake by the ocean. However, little is known about the quantitative spatial and temporal distribution of CaCO3 within sea <span class="hlt">ice</span>. This is the first quantitative study of hydrous calcium carbonate, as ikaite, in sea <span class="hlt">ice</span> and discusses its potential significance for the carbon cycle in polar oceans. <span class="hlt">Ice</span> cores and brine samples were collected from <span class="hlt">pack</span> and land fast sea <span class="hlt">ice</span> between September and December 2007 during an expedition in the East Antarctic and another off Terre Adélie, Antarctica. Samples were analysed for CaCO3, Salinity, DOC, DON, Phosphate, and total alkalinity. A relationship between the measured parameters and CaCO3 precipitation could not be observed. We found calcium carbonate, as ikaite, mostly in the top layer of sea <span class="hlt">ice</span> with values up to 126 mg ikaite per liter melted sea <span class="hlt">ice</span>. This potentially represents a contribution between 0.12 and 9 Tg C to the annual carbon flux in polar oceans. The horizontal distribution of ikaite in sea <span class="hlt">ice</span> was heterogenous. We also found the precipitate in the snow on top of the sea <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190395','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190395"><span>Polar bears and sea <span class="hlt">ice</span> habitat change</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Durner, George M.; Atwood, Todd C.; Butterworth, Andy</p> <p>2017-01-01</p> <p>The polar bear (Ursus maritimus) is an obligate apex predator of Arctic sea <span class="hlt">ice</span> and as such can be affected by climate warming-induced changes in the extent and composition of <span class="hlt">pack</span> <span class="hlt">ice</span> and its impacts on their seal prey. Sea <span class="hlt">ice</span> declines have negatively impacted some polar bear subpopulations through reduced energy input because of loss of hunting habitats, higher energy costs due to greater <span class="hlt">ice</span> drift, <span class="hlt">ice</span> fracturing and open water, and ultimately greater challenges to recruit young. Projections made from the output of global climate models suggest that polar bears in peripheral Arctic and sub-Arctic seas will be reduced in numbers or become extirpated by the end of the twenty-first century if the rate of climate warming continues on its present trajectory. The same projections also suggest that polar bears may persist in the high-latitude Arctic where heavy multiyear sea <span class="hlt">ice</span> that has been typical in that region is being replaced by thinner annual <span class="hlt">ice</span>. Underlying physical and biological oceanography provides clues as to why polar bear in some regions are negatively impacted, while bears in other regions have shown no apparent changes. However, continued declines in sea <span class="hlt">ice</span> will eventually challenge the survival of polar bears and efforts to conserve them in all regions of the Arctic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860017796','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860017796"><span>Analyses and <span class="hlt">tests</span> for design of an electro-impulse de-<span class="hlt">icing</span> system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zumwalt, G. W.; Schrag, R. L.; Bernhart, W. D.; Friedberg, R. A.</p> <p>1985-01-01</p> <p>De-<span class="hlt">icing</span> of aircraft by using the electro-magnetic impulse phenomenon was proposed and demonstrated in several European countries. However, it is not available as a developed system due to lack of research on the basic physical mechanisms and necessary design parameters. The de-<span class="hlt">icing</span> is accomplished by rapidly discharging high voltage capacitors into a wire coil rigidly supported just inside the aircraft skin. Induced eddy currents in the skin create a repulsive force resulting in a hammer-like force which cracks, de-bonds, and expels <span class="hlt">ice</span> on the skin surface. The promised advantages are very low energy, high reliability of de-<span class="hlt">icing</span>, and low maintenance. Three years of Electo-Impulse De-<span class="hlt">icing</span> (EIDI) research is summarized and the analytical studies and results of <span class="hlt">testing</span> done in the laboratory, in the NASA <span class="hlt">Icing</span> Research Tunnel, and in flight are presented. If properly designed, EIDI was demonstrated to be an effective and practical <span class="hlt">ice</span> protection system for small aircraft, turbojet engine inlets, elements of transport aircraft, and shows promise for use on helicopter rotor blades. Included are practical techniques of fabrication of impulse coils and their mountings. The use of EIDI with nonmetallic surface materials is also described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29089107','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29089107"><span>Column-to-column <span class="hlt">packing</span> variation of disposable pre-<span class="hlt">packed</span> columns for protein chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schweiger, Susanne; Hinterberger, Stephan; Jungbauer, Alois</p> <p>2017-12-08</p> <p>In the biopharmaceutical industry, pre-<span class="hlt">packed</span> columns are the standard for process development, but they must be qualified before use in experimental studies to confirm the required performance of the <span class="hlt">packed</span> bed. Column qualification is commonly done by pulse response experiments and depends highly on the experimental <span class="hlt">testing</span> conditions. Additionally, the peak analysis method, the variation in the 3D <span class="hlt">packing</span> structure of the bed, and the measurement precision of the workstation influence the outcome of qualification runs. While a full body of literature on these factors is available for HPLC columns, no comparable studies exist for preparative columns for protein chromatography. We quantified the influence of these parameters for commercially available pre-<span class="hlt">packed</span> and self-<span class="hlt">packed</span> columns of disposable and non-disposable design. Pulse response experiments were performed on 105 preparative chromatography columns with volumes of 0.2-20ml. The analyte acetone was studied at six different superficial velocities (30, 60, 100, 150, 250 and 500cm/h). The column-to-column <span class="hlt">packing</span> variation between disposable pre-<span class="hlt">packed</span> columns of different diameter-length combinations varied by 10-15%, which was acceptable for the intended use. The column-to-column variation cannot be explained by the <span class="hlt">packing</span> density, but is interpreted as a difference in particle arrangement in the column. Since it was possible to determine differences in the column-to-column performance, we concluded that the columns were well-<span class="hlt">packed</span>. The measurement precision of the chromatography workstation was independent of the column volume and was in a range of±0.01ml for the first peak moment and±0.007 ml 2 for the second moment. The measurement precision must be considered for small columns in the range of 2ml or less. The efficiency of disposable pre-<span class="hlt">packed</span> columns was equal or better than that of self-<span class="hlt">packed</span> columns. Copyright © 2017 The Author(s). Published by Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26808844','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26808844"><span>Off-<span class="hlt">Ice</span> Anaerobic Power Does Not Predict On-<span class="hlt">Ice</span> Repeated Shift Performance in Hockey.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Peterson, Ben J; Fitzgerald, John S; Dietz, Calvin C; Ziegler, Kevin S; Baker, Sarah E; Snyder, Eric M</p> <p>2016-09-01</p> <p>Peterson, BJ, Fitzgerald, JS, Dietz, CC, Ziegler, KS, Baker, SE, and Snyder, EM. Off-<span class="hlt">ice</span> anaerobic power does not predict on-<span class="hlt">ice</span> repeated shift performance in hockey. J Strength Cond Res 30(9): 2375-2381, 2016-Anaerobic power is a significant predictor of acceleration and top speed in team sport athletes. Historically, these findings have been applied to <span class="hlt">ice</span> hockey although recent research has brought their validity for this sport into question. As <span class="hlt">ice</span> hockey emphasizes the ability to repeatedly produce power, single bout anaerobic power <span class="hlt">tests</span> should be examined to determine their ability to predict on-<span class="hlt">ice</span> performance. We <span class="hlt">tested</span> whether conventional off-<span class="hlt">ice</span> anaerobic power <span class="hlt">tests</span> could predict on-<span class="hlt">ice</span> acceleration, top speed, and repeated shift performance. Forty-five hockey players, aged 18-24 years, completed anthropometric, off-<span class="hlt">ice</span>, and on-<span class="hlt">ice</span> <span class="hlt">tests</span>. Anthropometric and off-<span class="hlt">ice</span> <span class="hlt">testing</span> included height, weight, body composition, vertical jump, and Wingate <span class="hlt">tests</span>. On-<span class="hlt">ice</span> <span class="hlt">testing</span> consisted of acceleration, top speed, and repeated shift fatigue <span class="hlt">tests</span>. Vertical jump (VJ) (r = -0.42; r = -0.58), Wingate relative peak power (WRPP) (r = -0.32; r = -0.43), and relative mean power (WRMP) (r = -0.34; r = -0.48) were significantly correlated (p ≤ 0.05) to on-<span class="hlt">ice</span> acceleration and top speed, respectively. Conversely, none of the off-<span class="hlt">ice</span> <span class="hlt">tests</span> correlated with on-<span class="hlt">ice</span> repeated shift performance, as measured by first gate, second gate, or total course fatigue; VJ (r = 0.06; r = 0.13; r = 0.09), WRPP (r = 0.06; r = 0.14; r = 0.10), or WRMP (r = -0.10; r = -0.01; r = -0.01). Although conventional off-<span class="hlt">ice</span> anaerobic power <span class="hlt">tests</span> predict single bout on-<span class="hlt">ice</span> acceleration and top speed, they neither predict the repeated shift ability of the player, nor are good markers for performance in <span class="hlt">ice</span> hockey.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/638276-sea-ice-polar-climate-ncar-csm','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/638276-sea-ice-polar-climate-ncar-csm"><span>Sea <span class="hlt">ice</span> and polar climate in the NCAR CSM</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Weatherly, J.W.; Briegleb, B.P.; Large, W.G.</p> <p></p> <p>The Climate System Model (CSM) consists of atmosphere, ocean, land, and sea-<span class="hlt">ice</span> components linked by a flux coupler, which computes fluxes of energy and momentum between components. The sea-<span class="hlt">ice</span> component consists of a thermodynamic formulation for <span class="hlt">ice</span>, snow, and leads within the <span class="hlt">ice</span> <span class="hlt">pack</span>, and <span class="hlt">ice</span> dynamics using the cavitating-fluid <span class="hlt">ice</span> rheology, which allows for the compressive strength of <span class="hlt">ice</span> but ignores shear viscosity. The results of a 300-yr climate simulation are presented, with the focus on sea <span class="hlt">ice</span> and the atmospheric forcing over sea <span class="hlt">ice</span> in the polar regions. The atmospheric model results are compared to analyses from themore » European Centre for Medium-Range Weather Forecasts and other observational sources. The sea-<span class="hlt">ice</span> concentrations and velocities are compared to satellite observational data. The atmospheric sea level pressure (SLP) in CSM exhibits a high in the central Arctic displaced poleward from the observed Beaufort high. The Southern Hemisphere SLP over sea <span class="hlt">ice</span> is generally 5 mb lower than observed. Air temperatures over sea <span class="hlt">ice</span> in both hemispheres exhibit cold biases of 2--4 K. The precipitation-minus-evaporation fields in both hemispheres are greatly improved over those from earlier versions of the atmospheric GCM.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17999163','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17999163"><span>Effects of vial <span class="hlt">packing</span> density on drying rate during freeze-drying of carbohydrates or a model protein measured using a vial-weighing technique.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gieseler, Henning; Lee, Geoffrey</p> <p>2008-02-01</p> <p>To determine the effects of vial <span class="hlt">packing</span> density in a laboratory freeze dryer on drying rate profiles of crystalline and amorphous formulations. The Christ freeze-drying balance measured cumulative water loss, m(t), and instantaneous drying rate, m(t), of water, mannitol, sucrose and sucrose/BSA formulations in commercial vials. Crystalline mannitol shows drying rate behaviour indicative of a largely homogeneous dried-product layer. The drying rate behaviour of amorphous sucrose indicates structural heterogeneity, postulated to come from shrinkage or microcollapse. Trehalose dries more slowly than sucrose. Addition of BSA to either disaccharide decreases primary drying time. Higher vial <span class="hlt">packing</span> density greatly reduces drying rate because of effects of radiation heat transfer from chamber walls to <span class="hlt">test</span> vial. Plots of m(t) versus radical t and m(t) versus layer thickness (either <span class="hlt">ice</span> or dried-product) allow interpretation of changes in internal cake morphology during drying. Vial <span class="hlt">packing</span> density greatly influences these profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002337','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002337"><span>Possible Mechanisms for Turbofan Engine <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> at High Altitude</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsao, Jen-Ching; Struk, Peter M.; Oliver, Michael</p> <p>2014-01-01</p> <p>A thermodynamic model is presented to describe possible mechanisms of <span class="hlt">ice</span> formation on unheated surfaces inside a turbofan engine compression system from fully glaciated <span class="hlt">ice</span> crystal clouds often formed at high altitude near deep convective weather systems. It is shown from the analysis that generally there could be two distinct types of <span class="hlt">ice</span> formation: (1) when the "surface freezing fraction" is in the range of 0 to 1, dominated by the freezing of water melt from fully or partially melted <span class="hlt">ice</span> crystals, the <span class="hlt">ice</span> structure is formed from accretion with strong adhesion to the surface, and (2) when the "surface melting fraction" is the range of 0 to 1, dominated by the further melting of <span class="hlt">ice</span> crystals, the <span class="hlt">ice</span> structure is formed from accumulation of un-melted <span class="hlt">ice</span> crystals with relatively weak bonding to the surface. The model captures important qualitative trends of the fundamental <span class="hlt">ice</span>-crystal <span class="hlt">icing</span> phenomenon reported earlier1,2 from the research collaboration work by NASA and the National Research Council (NRC) of Canada. Further, preliminary analysis of <span class="hlt">test</span> data from the 2013 full scale turbofan engine <span class="hlt">ice</span> crystal <span class="hlt">icing</span> <span class="hlt">test</span>3 conducted in the NASA Glenn Propulsion Systems Laboratory (PSL) has also suggested that (1) both types of <span class="hlt">ice</span> formation occurred during the <span class="hlt">test</span>, and (2) the model has captured some important qualitative trend of turning on (or off) the <span class="hlt">ice</span> crystal <span class="hlt">ice</span> formation process in the <span class="hlt">tested</span> engine low pressure compressor (LPC) targeted area under different <span class="hlt">icing</span> conditions that ultimately would lead to (or suppress) an engine core roll back (RB) event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160011109','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160011109"><span>Possible Mechanisms for Turbofan Engine <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> at High Altitude</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsao, Jen-Ching; Struk, Peter M.; Oliver, Michael J.</p> <p>2016-01-01</p> <p>A thermodynamic model is presented to describe possible mechanisms of <span class="hlt">ice</span> formation on unheated surfaces inside a turbofan engine compression system from fully glaciated <span class="hlt">ice</span> crystal clouds often formed at high altitude near deep convective weather systems. It is shown from the analysis that generally there could be two distinct types of <span class="hlt">ice</span> formation: (1) when the "surface freezing fraction" is in the range of 0 to 1, dominated by the freezing of water melt from fully or partially melted <span class="hlt">ice</span> crystals, the <span class="hlt">ice</span> structure is formed from accretion with strong adhesion to the surface, and (2) when the "surface melting fraction" is the range of 0 to 1, dominated by the further melting of <span class="hlt">ice</span> crystals, the <span class="hlt">ice</span> structure is formed from accumulation of un-melted <span class="hlt">ice</span> crystals with relatively weak bonding to the surface. The model captures important qualitative trends of the fundamental <span class="hlt">ice</span>-crystal <span class="hlt">icing</span> phenomenon reported earlier (Refs. 1 and 2) from the research collaboration work by NASA and the National Research Council (NRC) of Canada. Further, preliminary analysis of <span class="hlt">test</span> data from the 2013 full scale turbofan engine <span class="hlt">ice</span> crystal <span class="hlt">icing</span> <span class="hlt">test</span> (Ref. 3) conducted in the NASA Glenn Propulsion Systems Laboratory (PSL) has also suggested that (1) both types of <span class="hlt">ice</span> formation occurred during the <span class="hlt">test</span>, and (2) the model has captured some important qualitative trend of turning on (or off) the <span class="hlt">ice</span> crystal <span class="hlt">ice</span> formation process in the <span class="hlt">tested</span> engine low pressure compressor (LPC) targeted area under different <span class="hlt">icing</span> conditions that ultimately would lead to (or suppress) an engine core roll back (RB) event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920052553&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmarginal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920052553&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmarginal"><span>Correlation studies of passive and active microwave data in the marginal <span class="hlt">ice</span> zone</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Comiso, J. C.</p> <p>1991-01-01</p> <p>The microwave radiative and backscatter characteristics of sea <span class="hlt">ice</span> in an Arctic marginal <span class="hlt">ice</span> zone have been studied using near-simultaneous passive and active synthetic aperture radar microwave data. Intermediate-resolution multichannel passive microwave data were registered and analyzed. Passive and active microwave data generally complement each other as the two sensors are especially sensitive to different physical properties of the sea <span class="hlt">ice</span>. In the inner <span class="hlt">pack</span>, undeformed first-year <span class="hlt">ice</span> is observed to have low backscatter values but high brightness temperatures while multiyear <span class="hlt">ice</span> has generally high backscatter values and low brightness temperatures. However, in the marginal <span class="hlt">ice</span> zone, the signature and backscatter for multiyear <span class="hlt">ice</span> are considerably different and closer to those of first-year <span class="hlt">ice</span>. Some floes identified by photography as snow-covered thick <span class="hlt">ice</span> have backscatter similar to that of new <span class="hlt">ice</span> or open water while brash <span class="hlt">ice</span> has backscatter similar to or higher than that of ridged <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020004347','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020004347"><span>Sea <span class="hlt">Ice</span> Remote Sensing Using Surface Reflected GPS Signals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Komjathy, Attila; Maslanik, James; Zavorotny, Valery U.; Axelrad, Penina; Katzberg, Stephen J.</p> <p>2000-01-01</p> <p>This paper describes a new research effort to extend the application of Global Positioning System (GPS) signal reflections, received by airborne instruments, to cryospheric remote sensing. Our experimental results indicate that reflected GPS signals have potential to provide information on the presence and condition of sea and freshwater <span class="hlt">ice</span> as well as the freeze/thaw state of frozen ground. In this paper we show results from aircraft experiments over the <span class="hlt">ice</span> <span class="hlt">pack</span> near Barrow, Alaska indicating correlation between forward-scattered GPS returns and RADARSAT backscattered measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1919531L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1919531L"><span>Ensemble sea <span class="hlt">ice</span> forecast for predicting compressive situations in the Baltic Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lehtiranta, Jonni; Lensu, Mikko; Kokkonen, Iiro; Haapala, Jari</p> <p>2017-04-01</p> <p>Forecasting of sea <span class="hlt">ice</span> hazards is important for winter shipping in the Baltic Sea. In current numerical models the <span class="hlt">ice</span> thickness distribution and drift are captured well, but compressive situations are often missing from forecast products. Its inclusion is requested by the shipping community, as compression poses a threat to ship operations. As compressing <span class="hlt">ice</span> is capable of stopping ships for days and even damaging them, its inclusion in <span class="hlt">ice</span> forecasts is vital. However, we have found that compression can not be predicted well in a deterministic forecast, since it can be a local and a quickly changing phenomenon. It is also very sensitive to small changes in the wind speed and direction, the prevailing <span class="hlt">ice</span> conditions, and the model parameters. Thus, a probabilistic ensemble simulation is needed to produce a meaningful compression forecast. An ensemble model setup was developed in the SafeWIN project for this purpose. It uses the HELMI multicategory <span class="hlt">ice</span> model, which was amended for making simulations in parallel. The ensemble was built by perturbing the atmospheric forcing and the physical parameters of the <span class="hlt">ice</span> <span class="hlt">pack</span>. The model setup will provide probabilistic forecasts for the compression in the Baltic sea <span class="hlt">ice</span>. Additionally the model setup provides insight into the uncertainties related to different model parameters and their impact on the model results. We have completed several hindcast simulations for the Baltic Sea for verification purposes. These results are shown to match compression reports gathered from ships. In addition, an ensemble forecast is in preoperational <span class="hlt">testing</span> phase and its first evaluation will be presented in this work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890024803&hterms=Phytoplankton&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DPhytoplankton','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890024803&hterms=Phytoplankton&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DPhytoplankton"><span>Phytoplankton standing crops within an Antarctic <span class="hlt">ice</span> edge assessed by satellite remote sensing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sullivan, C. W.; Mcclain, C. R.; Comiso, J. C.; Smith, W. O., Jr.</p> <p>1988-01-01</p> <p>The dynamic interactions between the <span class="hlt">pack-ice</span> recession and the occurrence of <span class="hlt">ice</span> blooms of phytoplankton in waters of the marginal <span class="hlt">ice</span> zone within an Antarctic <span class="hlt">ice</span> edge were investigated using CZCS and SMMR imageries from the Nimbus 7 satellite (September 16-December 17, 1983), together with in situ measurements of pigments and sea <span class="hlt">ice</span> concentration carried out from November 7 to December 2. A substantial amount of spatial variability in pigment concentration was observed to occur along the <span class="hlt">ice</span> edge in the Weddell Sea. The relationships among light, <span class="hlt">ice</span> distribution, and vertical stability and their effects on observed spatial variations in phytoplankton biomass are discussed. The results of this investigation suggest that the retreat of <span class="hlt">ice</span> provides an input of significant volumes of meltwater which creates vertical stability for a period necessary to permit growth and accumulation of phytoplankton.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150004436','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150004436"><span>Sea-<span class="hlt">Ice</span> Freeboard Retrieval Using Digital Photon-Counting Laser Altimetry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Farrell, Sinead L.; Brunt, Kelly M.; Ruth, Julia M.; Kuhn, John M.; Connor, Laurence N.; Walsh, Kaitlin M.</p> <p>2015-01-01</p> <p>Airborne and spaceborne altimeters provide measurements of sea-<span class="hlt">ice</span> elevation, from which sea-<span class="hlt">ice</span> freeboard and thickness may be derived. Observations of the Arctic <span class="hlt">ice</span> <span class="hlt">pack</span> by satellite altimeters indicate a significant decline in <span class="hlt">ice</span> thickness, and volume, over the last decade. NASA's <span class="hlt">Ice</span>, Cloud and land Elevation Satellite-2 (ICESat-2) is a next-generation laser altimeter designed to continue key sea-<span class="hlt">ice</span> observations through the end of this decade. An airborne simulator for ICESat-2, the Multiple Altimeter Beam Experimental Lidar (MABEL), has been deployed to gather pre-launch data for mission development. We present an analysis of MABEL data gathered over sea <span class="hlt">ice</span> in the Greenland Sea and assess the capabilities of photon-counting techniques for sea-<span class="hlt">ice</span> freeboard retrieval. We compare freeboard estimates in the marginal <span class="hlt">ice</span> zone derived from MABEL photon-counting data with coincident data collected by a conventional airborne laser altimeter. We find that freeboard estimates agree to within 0.03m in the areas where sea-<span class="hlt">ice</span> floes were interspersed with wide leads, and to within 0.07m elsewhere. MABEL data may also be used to infer sea-<span class="hlt">ice</span> thickness, and when compared with coincident but independent <span class="hlt">ice</span> thickness estimates, MABEL <span class="hlt">ice</span> thicknesses agreed to within 0.65m or better.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013718','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013718"><span>Propagation and Directional Scattering of Ocean Waves in the Marginal <span class="hlt">Ice</span> Zone and Neighboring Seas</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>expected to be the average of the kernel for 10 s and 12 s. This means that we should be able to calculate empirical formulas for 2 the scattering kernel...floe <span class="hlt">packing</span>. Thus, establish a way to incorporate what has been done by Squire and co-workers into the wave model paradigm (in which the phase of the...cases observed by Kohout et al. (2014) in Antarctica . vii. Validation: We are planning validation <span class="hlt">tests</span> for wave-<span class="hlt">ice</span> scattering / attenuation model by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25345526','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25345526"><span>Immersion freezing of supermicron mineral dust particles: freezing results, <span class="hlt">testing</span> different schemes for describing <span class="hlt">ice</span> nucleation, and <span class="hlt">ice</span> nucleation active site densities.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wheeler, M J; Mason, R H; Steunenberg, K; Wagstaff, M; Chou, C; Bertram, A K</p> <p>2015-05-14</p> <p><span class="hlt">Ice</span> nucleation on mineral dust particles is known to be an important process in the atmosphere. To accurately implement <span class="hlt">ice</span> nucleation on mineral dust particles in atmospheric simulations, a suitable theory or scheme is desirable to describe laboratory freezing data in atmospheric models. In the following, we investigated <span class="hlt">ice</span> nucleation by supermicron mineral dust particles [kaolinite and Arizona <span class="hlt">Test</span> Dust (ATD)] in the immersion mode. The median freezing temperature for ATD was measured to be approximately -30 °C compared with approximately -36 °C for kaolinite. The freezing results were then used to <span class="hlt">test</span> four different schemes previously used to describe <span class="hlt">ice</span> nucleation in atmospheric models. In terms of ability to fit the data (quantified by calculating the reduced chi-squared values), the following order was found for ATD (from best to worst): active site, pdf-α, deterministic, single-α. For kaolinite, the following order was found (from best to worst): active site, deterministic, pdf-α, single-α. The variation in the predicted median freezing temperature per decade change in the cooling rate for each of the schemes was also compared with experimental results from other studies. The deterministic model predicts the median freezing temperature to be independent of cooling rate, while experimental results show a weak dependence on cooling rate. The single-α, pdf-α, and active site schemes all agree with the experimental results within roughly a factor of 2. On the basis of our results and previous results where different schemes were <span class="hlt">tested</span>, the active site scheme is recommended for describing the freezing of ATD and kaolinite particles. We also used our <span class="hlt">ice</span> nucleation results to determine the <span class="hlt">ice</span> nucleation active site (INAS) density for the supermicron dust particles <span class="hlt">tested</span>. Using the data, we show that the INAS densities of supermicron kaolinite and ATD particles studied here are smaller than the INAS densities of submicron kaolinite and ATD particles</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28708127','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28708127"><span>An active bacterial community linked to high chl-a concentrations in Antarctic winter-<span class="hlt">pack</span> <span class="hlt">ice</span> and evidence for the development of an anaerobic sea-<span class="hlt">ice</span> bacterial community.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Eronen-Rasimus, Eeva; Luhtanen, Anne-Mari; Rintala, Janne-Markus; Delille, Bruno; Dieckmann, Gerhard; Karkman, Antti; Tison, Jean-Louis</p> <p>2017-10-01</p> <p>Antarctic sea-<span class="hlt">ice</span> bacterial community composition and dynamics in various developmental stages were investigated during the austral winter in 2013. Thick snow cover likely insulated the <span class="hlt">ice</span>, leading to high (<4 μg l -1 ) chlorophyll-a (chl-a) concentrations and consequent bacterial production. Typical sea-<span class="hlt">ice</span> bacterial genera, for example, Octadecabacter, Polaribacter and Glaciecola, often abundant in spring and summer during the sea-<span class="hlt">ice</span> algal bloom, predominated in the communities. The variability in bacterial community composition in the different <span class="hlt">ice</span> types was mainly explained by the chl-a concentrations, suggesting that as in spring and summer sea <span class="hlt">ice</span>, the sea-<span class="hlt">ice</span> bacteria and algae may also be coupled during the Antarctic winter. Coupling between the bacterial community and sea-<span class="hlt">ice</span> algae was further supported by significant correlations between bacterial abundance and production with chl-a. In addition, sulphate-reducing bacteria (for example, Desulforhopalus) together with odour of H 2 S were observed in thick, apparently anoxic <span class="hlt">ice</span>, suggesting that the development of the anaerobic bacterial community may occur in sea <span class="hlt">ice</span> under suitable conditions. In all, the results show that bacterial community in Antarctic sea <span class="hlt">ice</span> can stay active throughout the winter period and thus possible future warming of sea <span class="hlt">ice</span> and consequent increase in bacterial production may lead to changes in bacteria-mediated processes in the Antarctic sea-<span class="hlt">ice</span> zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870060026&hterms=British+Petroleum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DBritish%2BPetroleum','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870060026&hterms=British+Petroleum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DBritish%2BPetroleum"><span>Shuttle Imaging Radar B (SIR-B) Weddell Sea <span class="hlt">ice</span> observations - A comparison of SIR-B and scanning multichannel microwave radiometer <span class="hlt">ice</span> concentrations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Martin, Seelye; Holt, Benjamin; Cavalieri, Donald J.; Squire, Vernon</p> <p>1987-01-01</p> <p><span class="hlt">Ice</span> concentrations over the Weddell Sea were studied using SIR-B data obtained during the October 1984 mission, with special attention given to the effect of ocean waves on the radar return at the <span class="hlt">ice</span> edge. Sea <span class="hlt">ice</span> concentrations were derived from the SIR-B data using two image processing methods: the classification scheme at JPL and the manual classification method at Scott Polar Research Institute (SPRI), England. The SIR <span class="hlt">ice</span> concentrations were compared with coincident concentrations from the Nimbus-7 SMMR. For concentrations greater than 40 percent, which was the smallest concentration observed jointly by SIR-B and the SMMR, the mean difference between the two data sets for 12 points was 2 percent. A comparison between the JPL and the SPRI SIR-B algorithms showed that the algorithms agree to within 1 percent in the interior <span class="hlt">ice</span> <span class="hlt">pack</span>, but the JPL algorithm gives slightly greater concentrations at the <span class="hlt">ice</span> edge (due to the fact that the algorithm is affected by the wind waves in these areas).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16349347','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16349347"><span>Bacterial Standing Stock, Activity, and Carbon Production during Formation and Growth of Sea <span class="hlt">Ice</span> in the Weddell Sea, Antarctica.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grossmann, S; Dieckmann, G S</p> <p>1994-08-01</p> <p>Bacterial response to formation and growth of sea <span class="hlt">ice</span> was investigated during autumn in the northeastern Weddell Sea. Changes in standing stock, activity, and carbon production of bacteria were determined in successive stages of <span class="hlt">ice</span> development. During initial <span class="hlt">ice</span> formation, concentrations of bacterial cells, in the order of 1 x 10 to 3 x 10 liter, were not enhanced within the <span class="hlt">ice</span> matrix. This suggests that physical enrichment of bacteria by <span class="hlt">ice</span> crystals is not effective. Due to low concentrations of phytoplankton in the water column during freezing, incorporation of bacteria into newly formed <span class="hlt">ice</span> via attachment to algal cells or aggregates was not recorded in this study. As soon as the <span class="hlt">ice</span> had formed, the general metabolic activity of bacterial populations was strongly suppressed. Furthermore, the ratio of [H]leucine incorporation into proteins to [H]thymidine incorporation into DNA changed during <span class="hlt">ice</span> growth. In thick <span class="hlt">pack</span> <span class="hlt">ice</span>, bacterial activity recovered and growth rates up to 0.6 day indicated actively dividing populations. However, biomass-specific utilization of organic compounds remained lower than in open water. Bacterial concentrations of up to 2.8 x 10 cells liter along with considerably enlarged cell volumes accumulated within thick <span class="hlt">pack</span> <span class="hlt">ice</span>, suggesting reduced mortality rates of bacteria within the small brine pores. In the course of <span class="hlt">ice</span> development, bacterial carbon production increased from about 0.01 to 0.4 mug of C liter h. In thick <span class="hlt">ice</span>, bacterial secondary production exceeded primary production of microalgae.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996JPhA...29.2671Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996JPhA...29.2671Z"><span>Effect of <span class="hlt">packing</span> method on the randomness of disc <span class="hlt">packings</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Z. P.; Yu, A. B.; Oakeshott, R. B. S.</p> <p>1996-06-01</p> <p>The randomness of disc <span class="hlt">packings</span>, generated by random sequential adsorption (RSA), random <span class="hlt">packing</span> under gravity (RPG) and Mason <span class="hlt">packing</span> (MP) which gives a <span class="hlt">packing</span> density close to that of the RSA <span class="hlt">packing</span>, has been analysed, based on the Delaunay tessellation, and is evaluated at two levels, i.e. the randomness at individual subunit level which relates to the construction of a triangle from a given edge length distribution and the randomness at network level which relates to the connection between triangles from a given triangle frequency distribution. The Delaunay tessellation itself is also analysed and its almost perfect randomness at the two levels is demonstrated, which verifies the proposed approach and provides a random reference system for the present analysis. It is found that (i) the construction of a triangle subunit is not random for the RSA, MP and RPG <span class="hlt">packings</span>, with the degree of randomness decreasing from the RSA to MP and then to RPG <span class="hlt">packing</span>; (ii) the connection of triangular subunits in the network is almost perfectly random for the RSA <span class="hlt">packing</span>, acceptable for the MP <span class="hlt">packing</span> and not good for the RPG <span class="hlt">packing</span>. <span class="hlt">Packing</span> method is an important factor governing the randomness of disc <span class="hlt">packings</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170011211','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170011211"><span><span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Research at NASA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flegel, Ashlie B.</p> <p>2017-01-01</p> <p><span class="hlt">Ice</span> crystals found at high altitude near convective clouds are known to cause jet engine power-loss events. These events occur due to <span class="hlt">ice</span> crystals entering a propulsion system's core flowpath and accreting <span class="hlt">ice</span> resulting in events such as uncommanded loss of thrust (rollback), engine stall, surge, and damage due to <span class="hlt">ice</span> shedding. As part of a community with a growing need to understand the underlying physics of <span class="hlt">ice</span> crystal <span class="hlt">icing</span>, NASA has been performing experimental efforts aimed at providing datasets that can be used to generate models to predict the <span class="hlt">ice</span> accretion inside current and future engine designs. Fundamental <span class="hlt">icing</span> physics studies on particle impacts, accretion on a single airfoil, and <span class="hlt">ice</span> accretions observed during a rollback event inside a full-scale engine in the Propulsion Systems Laboratory are summarized. Low fidelity code development using the results from the engine <span class="hlt">tests</span> which identify key parameters for <span class="hlt">ice</span> accretion risk and the development of high fidelity codes are described. These activities have been conducted internal to NASA and through collaboration efforts with industry, academia, and other government agencies. The details of the research activities and progress made to date in addressing <span class="hlt">ice</span> crystal <span class="hlt">icing</span> research challenges are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170006539','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170006539"><span><span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Research at NASA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flegel, Ashlie B.</p> <p>2017-01-01</p> <p><span class="hlt">Ice</span> crystals found at high altitude near convective clouds are known to cause jet engine power-loss events. These events occur due to <span class="hlt">ice</span> crystals entering a propulsion systems core flowpath and accreting <span class="hlt">ice</span> resulting in events such as uncommanded loss of thrust (rollback), engine stall, surge, and damage due to <span class="hlt">ice</span> shedding. As part of a community with a growing need to understand the underlying physics of <span class="hlt">ice</span> crystal <span class="hlt">icing</span>, NASA has been performing experimental efforts aimed at providing datasets that can be used to generate models to predict the <span class="hlt">ice</span> accretion inside current and future engine designs. Fundamental <span class="hlt">icing</span> physics studies on particle impacts, accretion on a single airfoil, and <span class="hlt">ice</span> accretions observed during a rollback event inside a full-scale engine in the Propulsion Systems Laboratory are summarized. Low fidelity code development using the results from the engine <span class="hlt">tests</span> which identify key parameters for <span class="hlt">ice</span> accretion risk and the development of high fidelity codes are described. These activities have been conducted internal to NASA and through collaboration efforts with industry, academia, and other government agencies. The details of the research activities and progress made to date in addressing <span class="hlt">ice</span> crystal <span class="hlt">icing</span> research challenges are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005APS..MARA34005M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005APS..MARA34005M"><span>First Principles Simulations of <span class="hlt">Ice</span> Nucleation at Metal Surfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Michaelides, Angelos</p> <p>2005-03-01</p> <p><span class="hlt">Ice</span> nucleation at solid surfaces is of relevance to countless scientific and technological processes. In particular the nucleation of <span class="hlt">ice</span> nano-crystals on metal surfaces is often a key first step in cloud formation and corrosion [1]. Yet unfortunately this remains one of the most poorly understood natural phenomena; severely lacking in atomic level understanding. Here, we discuss detailed density functional theory studies aimed at putting our understanding of <span class="hlt">ice</span> nucleation at metals on a much firmer footing. Specifically the properties of H2O hexamers - the smallest `building blocks' of <span class="hlt">ice</span> - adsorbed on a number of close-<span class="hlt">packed</span> transition metal surfaces have been examined. We find that the competing influences of substrate reactivity and hexamer-substrate epitaxial mismatch conspire to yield a rich variety of (novel) hexameric <span class="hlt">ice</span> structures, some of which have been observed by recent scanning tunnelling microscopy experiments [2]. [1] H.R. Pruppacher and J.D. Klett, Microphysics of Clouds and Precipitation, (Kluwer, Dordrecht, 2003). [2] K. Morgenstern, et al., (To be published).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910044116&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmarginal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910044116&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmarginal"><span>Wave propagation in the marginal <span class="hlt">ice</span> zone - Model predictions and comparisons with buoy and synthetic aperture radar data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, Antony K.; Holt, Benjamin; Vachon, Paris W.</p> <p>1991-01-01</p> <p>Ocean wave dispersion relation and viscous attenuation by a sea <span class="hlt">ice</span> cover are studied for waves propagating into the marginal <span class="hlt">ice</span> zone (MIZ). The Labrador <span class="hlt">ice</span> margin experiment (LIMEX), conducted on the MIZ off the east coast of Newfoundland, Canada in March 1987, provided aircraft SAR imagery, <span class="hlt">ice</span> property and wave buoy data. Wave energy attenuation rates are estimated from SAR data and the <span class="hlt">ice</span> motion package data that were deployed at the <span class="hlt">ice</span> edge and into the <span class="hlt">ice</span> <span class="hlt">pack</span>, and compared with a model. It is shown that the model data comparisons are quite good for the <span class="hlt">ice</span> conditions observed during LIMEX 1987.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DPPP10145C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DPPP10145C"><span>Accretion growth of water-<span class="hlt">ice</span> grains in astrophysically-relevant dusty plasma experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chai, Kil-Byoung; Marshall, Ryan; Bellan, Paul</p> <p>2016-10-01</p> <p>The grain growth process in the Caltech water-<span class="hlt">ice</span> dusty plasma experiment has been studied using a high-speed camera equipped with a long-distance microscope lens. It is found that (i) the <span class="hlt">ice</span> grain number density decreases four-fold as the average grain length increases from 20 to 80 um, (ii) the <span class="hlt">ice</span> grain length has a log-normal distribution rather than a power-law dependence, and (iii) no collisions between <span class="hlt">ice</span> grains are apparent. The grains have a large negative charge so the agglomeration growth is prevented by their strong mutual repulsion. It is concluded that direct accretion of water molecules is in good agreement with the observed <span class="hlt">ice</span> grain growth. The volumetric <span class="hlt">packing</span> factor of the <span class="hlt">ice</span> grains must be less than 0.25 in order for the grain kinetic energy to be sufficiently small to prevent collisions between <span class="hlt">ice</span> grains; this conclusion is consistent with <span class="hlt">ice</span> grain images showing a fractal character.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12588561','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12588561"><span>PCR detection of psychrophilic Clostridium spp. causing 'blown <span class="hlt">pack</span>' spoilage of vacuum-<span class="hlt">packed</span> chilled meats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Broda, D M; Boerema, J A; Bell, R G</p> <p>2003-01-01</p> <p>To develop a practical molecular procedure that directly, without isolation, and specifically detects the presence of clostridia which cause 'blown <span class="hlt">pack</span>' spoilage of vacuum-<span class="hlt">packed</span> meat. Primer sets and PCR amplification procedures were developed that detect the presence of 16S rDNA gene and/or 16S-23S rDNA internal transcribed spacer fragments of 'blown <span class="hlt">pack</span>' causing clostridia in meat. The specificity of the developed procedures was evaluated with DNA obtained from close phylogenetic neighbours of 'blown <span class="hlt">pack</span>' causing clostridia, food clostridia and common meat spoilage microorganisms. The sensitivity of detection was assessed in non-enriched and low-temperature-enriched beef mince inoculated with serially diluted pure cultures of Clostridium estertheticum DSMZ 8809T and Cl. gasigenes DB1AT. The efficacy of detection procedures was evaluated for naturally contaminated vacuum-<span class="hlt">packed</span> meat samples. Three primer sets, 16SE, 16SDB and EISR, produced amplicons of the expected size with DNA templates from target clostridia, but failed to yield PCR products with DNAs from any other microorganisms <span class="hlt">tested</span>. With 16SE and 16SDB primers, minimum levels of detection were 104 CFU g(-1) for non-enriched, and 102 CFU g(-1) for enriched meat samples. Based on the established specificity of these primers, as well as DNA sequencing of amplicons, Cl. gasigenes was confirmed as the causative agent of 'blown <span class="hlt">pack</span>' spoilage in two <span class="hlt">packs</span>, and Cl. estertheticum as the causative agent in the third. The developed method can be used for rapid detection of 'blown <span class="hlt">pack</span>' causing clostridia in commercial blown <span class="hlt">packs</span>, or following low temperature enrichment, for detection of these microorganisms in meat containing as few as 100 clostridial cells per gram. The paper reports practical procedures that can be used for rapid confirmation of the causative agents of clostridial 'blown <span class="hlt">pack</span>' spoilage in commercial spoiled <span class="hlt">packs</span>, or for detection of psychrophilic clostridia in epidemiological trace back of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130011328','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130011328"><span><span class="hlt">Pack</span> Density Limitations of Hybrid Parachutes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zwicker, Matthew L.; Sinclair, Robert J.</p> <p>2013-01-01</p> <p>The development and <span class="hlt">testing</span> of the Orion crew capsule parachute system has provided a unique opportunity to study dense parachute <span class="hlt">packing</span> techniques and limits, in order to establish a new baseline for future programs. The density of parachute <span class="hlt">packs</span> has a significant influence on vibration loads, retention system stresses, and parachute mortar performance. Material compositions and <span class="hlt">pack</span> densities of existing designs for space capsule recovery were compared, using the <span class="hlt">pack</span> density of the Apollo main parachutes as the current baseline. The composition of parachutes has changed since Apollo, incorporating new materials such as Kevlar , Vectran , Teflon and Spectra . These materials have different specific densities than Nylon, so the densities of hybrid parachute <span class="hlt">packs</span> cannot be directly compared to Nylon parachutes for determination of feasibility or volume allocation. Six parachute <span class="hlt">packs</span> were evaluated in terms of weighted average solid density in order to achieve a non-dimensional comparison of <span class="hlt">packing</span> density. Means of mitigating damage due to <span class="hlt">packing</span> pressure and mortar firing were examined in light of the Capsule Parachute Assembly System (CPAS) and Apollo experience. Parachute design improvements including incorporation of modern materials and manufacturing processes serves to make CPAS the new knowledge base on which future spacecraft parachute systems will be built.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GMD....10.3105P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GMD....10.3105P"><span>Sea-<span class="hlt">ice</span> evaluation of NEMO-Nordic 1.0: a NEMO-LIM3.6-based ocean-sea-<span class="hlt">ice</span> model setup for the North Sea and Baltic Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pemberton, Per; Löptien, Ulrike; Hordoir, Robinson; Höglund, Anders; Schimanke, Semjon; Axell, Lars; Haapala, Jari</p> <p>2017-08-01</p> <p>The Baltic Sea is a seasonally <span class="hlt">ice</span>-covered marginal sea in northern Europe with intense wintertime ship traffic and a sensitive ecosystem. Understanding and modeling the evolution of the sea-<span class="hlt">ice</span> <span class="hlt">pack</span> is important for climate effect studies and forecasting purposes. Here we present and evaluate the sea-<span class="hlt">ice</span> component of a new NEMO-LIM3.6-based ocean-sea-<span class="hlt">ice</span> setup for the North Sea and Baltic Sea region (NEMO-Nordic). The setup includes a new depth-based fast-<span class="hlt">ice</span> parametrization for the Baltic Sea. The evaluation focuses on long-term statistics, from a 45-year long hindcast, although short-term daily performance is also briefly evaluated. We show that NEMO-Nordic is well suited for simulating the mean sea-<span class="hlt">ice</span> extent, concentration, and thickness as compared to the best available observational data set. The variability of the annual maximum Baltic Sea <span class="hlt">ice</span> extent is well in line with the observations, but the 1961-2006 trend is underestimated. Capturing the correct <span class="hlt">ice</span> thickness distribution is more challenging. Based on the simulated <span class="hlt">ice</span> thickness distribution we estimate the undeformed and deformed <span class="hlt">ice</span> thickness and concentration in the Baltic Sea, which compares reasonably well with observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820016728','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820016728"><span>SEASAT views oceans and sea <span class="hlt">ice</span> with synthetic aperture radar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fu, L. L.; Holt, B.</p> <p>1982-01-01</p> <p>Fifty-one SEASAT synthetic aperture radar (SAR) images of the oceans and sea <span class="hlt">ice</span> are presented. Surface and internal waves, the Gulf Stream system and its rings and eddies, the eastern North Pacific, coastal phenomena, bathymetric features, atmospheric phenomena, and ship wakes are represented. Images of arctic <span class="hlt">pack</span> and shore-fast <span class="hlt">ice</span> are presented. The characteristics of the SEASAT SAR system and its image are described. Maps showing the area covered, and tables of key orbital information, and listing digitally processed images are provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930005722','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930005722"><span>Results of low power deicer <span class="hlt">tests</span> on a swept inlet component in the NASA Lewis <span class="hlt">icing</span> research tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bond, Thomas H.; Shin, Jaiwon</p> <p>1993-01-01</p> <p><span class="hlt">Tests</span> were conducted under a USAF/NASA Low Power Deicer program on two expulsive technologies to examine system performance on hardware representative of a modern aircraft part. The BF Goodrich Electro-Expulsive Deicing System and Pneumatic Impulse <span class="hlt">Ice</span> Protection System were installed on a swept, compound curve, engine inlet component with varying leading edge radius, and <span class="hlt">tested</span> through a range of <span class="hlt">icing</span> and system operating conditions in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel. A description of the experimental procedure and results, including residual <span class="hlt">ice</span> thickness, shed <span class="hlt">ice</span> particle size, and changes in system energy/pressure characteristics are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930038554&hterms=Research+power&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DResearch%2Bpower','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930038554&hterms=Research+power&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DResearch%2Bpower"><span>Results of Low Power Deicer <span class="hlt">tests</span> on a swept inlet component in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bond, Thomas H.; Shin, Jaiwon</p> <p>1993-01-01</p> <p><span class="hlt">Tests</span> were conducted under a USAF/NASA Low Power Deicer program on two expulsive technologies to examine system performance on hardware representative of a modern aircraft part. The BF Goodrich Electro-Expulsive Deicing System and Pneumatic Impulse <span class="hlt">Ice</span> Protection system were installed on a swept, compound curve, engine inlet component with varying leading edge radius, and <span class="hlt">tested</span> through a range of <span class="hlt">icing</span> and system operating conditions in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel. A description of the experimental procedure and results, including residual <span class="hlt">ice</span> thickness, shed <span class="hlt">ice</span> particle size, and changes in system energy/pressure characteristics are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TRACE..17..529S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TRACE..17..529S"><span>Development of a Compact and Efficient <span class="hlt">Ice</span> Thermal Energy Storage Vessel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sasaguchi, Kengo; Ishikawa, Masatoshi; Muta, Kenji; Yoshino, Kiyotaka; Hayashi, Hiroko; Baba, Yoshiyuki</p> <p></p> <p>In the present study, the authors propose the use of a low concentration aqueous solution as phase change material for static-type <span class="hlt">ice</span>-storage-vessels, instead of pure water commonly used today. If an aqueous solution with low concentration is used, even when a large amount of solution (aqueous ethylene glycol in this study) is solidified and bridging of <span class="hlt">ice</span> developed around cold tubes occurs, the pressure increase could be prevented by the existence of a continuous liquid phase in the solid-liquid two-phase layer (mushy layer) which opens to an air gap at the top of a vessel. Therefore, one can continue to solidify an aqueous solution after bridging, achieving a high <span class="hlt">ice</span> <span class="hlt">packing</span> factor (IPF). First, experiments using small-scale <span class="hlt">test</span> cells have been conducted to confirm the present idea, and then we have performed experiments using a large vessel with an early practical size. It was seen that a large pressure increase is prevented for the initial concentration of the solution C0 of 1.0%, and IPF obtained using the solution is much greater than 0.65 using pure water for which the solidification must be stopped before the bridging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007702','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007702"><span>Particle Size Measurements From the First Fundamentals of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics <span class="hlt">Test</span> in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, Michael C.; Bachalo, William; Kurek, Andrzej</p> <p>2017-01-01</p> <p>This paper presents particle measurements by the Artium Technologies, Inc. Phase Doppler Interferometer and High Speed Imaging instruments from the first Fundamental <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics <span class="hlt">test</span> conducted in the NASA Propulsion Systems Laboratory. The work focuses on humidity sweeps at a larger and a smaller median volumetric diameter. The particle size distribution, number density, and water content measured by the Phase Doppler Interferometer and High Speed Imaging instruments from the sweeps are presented and compared. The current capability for these two instruments to measure and discriminate ICI conditions is examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170008109','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170008109"><span>Particle Size Measurements from the first Fundamentals of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics <span class="hlt">Test</span> in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, Michael C.; Bachalo, William; Kurek, Andrzej</p> <p>2017-01-01</p> <p>This presentation shows particle measurements by the Artium Technologies, Inc. Phase Doppler Interferometer and High Speed Imaging instruments from the first Fundamental <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics <span class="hlt">test</span> conducted in the NASA Propulsion Systems Laboratory. The work focuses on humidity sweeps at a larger and a smaller median volumetric diameter. The particle size distribution, number density, and water content measured by the Phase Doppler Interferometer and High Speed Imaging instruments from the sweeps are presented and compared. The current capability for these two instruments to measure and discriminate ICI conditions is examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050182000&hterms=asbestos&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dasbestos','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050182000&hterms=asbestos&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dasbestos"><span>NASA Lewis' <span class="hlt">Icing</span> Research Tunnel Works With Small Local Company to <span class="hlt">Test</span> Coatings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1998-01-01</p> <p>Dynamic Coatings, Inc., wanted to <span class="hlt">test</span> coating products that would enable the company to approach new markets. A Space Act Agreement with NASA Lewis Research Center afforded them this opportunity. They used Lewis' <span class="hlt">Icing</span> Research Tunnel to <span class="hlt">test</span> coating products for reduced <span class="hlt">ice</span> adhesion, industrial and aerospace lubrication applications, a tiremold release coating now used in the production of tires for the Boeing 777, and a product that solidifies asbestos fibers (which is being <span class="hlt">tested</span> as an insulator in a power plant in Iowa). Not only was the <span class="hlt">testing</span> a success, but during these activities, Dynamic Coatings met another coating company with whom they now have a joint venture offering a barnacle-repellent coating for marine applications, now on the market in Florida.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29846723','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29846723"><span>Presence of Counterfeit Marlboro Gold <span class="hlt">Packs</span> in Licensed Retail Stores in New York City: Evidence From <span class="hlt">Test</span> Purchases.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kurti, Marin; He, Yi; Silver, Diana; Giorgio, Margaret; von Lampe, Klaus; Macinko, James; Ye, Hua; Tan, Fidelis; Mei, Victoria</p> <p>2018-05-26</p> <p>There are no independent studies measuring the availability of premium brand counterfeit cigarettes in New York City from licensed retailers. We forensically analyzed the cigarette packaging of Marlboro Gold (n = 1021) purchased from licensed tobacco retailers in New York City, using ultraviolet irradiation and light microscopy to determine whether they were counterfeit. We find that while only 0.5% (n = 5) of our sample exhibits at least one characteristic synonymous with counterfeit packaging, none of our <span class="hlt">packs</span> can be conclusively classified as counterfeit. We do not find any counterfeit Marlboro Gold <span class="hlt">packs</span> purchased at full price from licensed cigarette retailers throughout New York City. Future research using <span class="hlt">test</span> purchases should include other venues (eg, street and online) and specifically ask for discounts to ascertain the overall presence of counterfeit cigarettes. This is the first study to independently measure the availability of counterfeit cigarette <span class="hlt">packs</span> purchased at full price from licensed retailers in New York City. We find that none of the Marlboro Gold <span class="hlt">packs</span> purchased from licensed cigarette retailers are counterfeit.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004DSRI...51.1601M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004DSRI...51.1601M"><span>Effects of summer <span class="hlt">ice</span> coverage on phytoplankton assemblages in the Ross Sea, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mangoni, O.; Modigh, M.; Conversano, F.; Carrada, G. C.; Saggiomo, V.</p> <p>2004-11-01</p> <p>An oceanographic cruise was conducted in the Ross Sea (Antarctica) during summer 2001 as part of the Italian National Program for Antarctic Research (PNRA). Extensive areas of <span class="hlt">pack</span> <span class="hlt">ice</span> occurred over the Ross Sea, atypical for summer when offshore waters are normally free of <span class="hlt">ice</span>. The present study focuses on the effects of increased <span class="hlt">ice</span> coverage on phytoplankton assemblages. Water samples collected at various depths at 72 hydrographical stations in offshore and coastal waters were used to determine size-fractionated phytoplankton biomass as chlorophyll a (chla) concentrations, and HPLC photosynthetic pigments. For the offshore waters, the average chla concentration was 57.8 mg m-2, approximately three times the values recorded under <span class="hlt">ice</span>-free conditions during summer 1996. In coastal waters, the average chla concentrations were 102 and 206 mg m-2 during January and February, respectively, i.e., up to 2.5 times those of 1996. Micro- and nano-phytoplankton size fractions made up about 90% of the phytoplankton biomass over the entire study area and were composed primarily of diatoms with a pico-phytoplankton fraction dominated by prymnesiophyceans. The broken <span class="hlt">pack</span> and melting <span class="hlt">ice</span> was strongly coloured by an extensive algal biomass suggesting that the phytoplankton was a result of seeding from <span class="hlt">ice</span> algal communities. The Ross Sea considered to be one of the most productive areas of the Southern Ocean, had primary production values about four-fold those of other areas. The lengthening of the <span class="hlt">ice</span> season observed in the Western Ross Sea, associated with a considerable increase in phytoplankton biomass as observed in summer 2001, would have a major impact on the trophic structure of the entire ecosystem, and presumably, also on carbon export.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29123023','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29123023"><span>Young adult smokers' perceptions of plain <span class="hlt">packs</span>, numbered <span class="hlt">packs</span> and <span class="hlt">pack</span> inserts in Turkey: a focus group study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mucan, Burcu; Moodie, Crawford</p> <p>2017-11-09</p> <p>The Turkish Government's 'National Tobacco Control Program 2015-2018' included plans to introduce plain packaging and also a ban on brand names on cigarette <span class="hlt">packs</span>, allowing only assigned numbers on <span class="hlt">packs</span>. We explored perceptions of these proposed measures, and also <span class="hlt">pack</span> inserts with cessation messages, another novel way of using the packaging to communicate with consumers. Eight focus groups were conducted with 47 young adult smokers in Manisa and Kutahya (Turkey) in December 2016. Participants were shown three straight-edged plain cigarette <span class="hlt">packs</span>, as required in Australia, and then three bevelled-edged plain <span class="hlt">packs</span>, as permitted in the UK. They were then shown plain <span class="hlt">packs</span> with numbers rather than brand names, and finally three <span class="hlt">pack</span> inserts with messages encouraging quitting or offering tips on how to do so. Participants were asked about their perceptions of each. Plain <span class="hlt">packs</span> were considered unappealing and off-putting, although the bevelled-edged <span class="hlt">packs</span> were viewed more favourably than the straight-edged <span class="hlt">packs</span>. Numbered <span class="hlt">packs</span> were thought by some to diminish the appeal created by the brand name and potentially decrease interest among never smokers and newer smokers. <span class="hlt">Pack</span> inserts were thought to have less of an impact than the on-<span class="hlt">pack</span> warnings, but could potentially help discourage initiation and encourage cessation. That bevelled-edged plain <span class="hlt">packs</span> were perceived more positively than straight-edged plain <span class="hlt">packs</span> is relevant to countries planning to introduce plain packaging. The study provides a first insight into smokers' perceptions of a ban on brand names, which was perceived to reduce appeal among young people. © Article author(s) (or their employer(s) unless otherwise stated in the text of the article) 2017. All rights reserved. No commercial use is permitted unless otherwise expressly granted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C33C1211G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C33C1211G"><span>Is snow-<span class="hlt">ice</span> now a major contributor to sea <span class="hlt">ice</span> mass balance in the western Transpolar Drift region?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Graham, R. M.; Merkouriadi, I.; Cheng, B.; Rösel, A.; Granskog, M. A.</p> <p>2017-12-01</p> <p>During the Norwegian young sea <span class="hlt">ICE</span> (N-<span class="hlt">ICE</span>2015) campaign, which took place in the first half of 2015 north of Svalbard, a deep winter snow <span class="hlt">pack</span> (50 cm) on sea <span class="hlt">ice</span> was observed, that was 50% thicker than earlier climatological studies suggested for this region. Moreover, a significant fraction of snow contributed to the total <span class="hlt">ice</span> mass in second-year <span class="hlt">ice</span> (SYI) (9% on average). Interestingly, very little snow (3% snow by mass) was present in first-year <span class="hlt">ice</span> (FYI). The combination of sea <span class="hlt">ice</span> thinning and increased precipitation north of Svalbard is expected to promote the formation of snow-<span class="hlt">ice</span>. Here we use the 1-D snow/<span class="hlt">ice</span> thermodynamic model HIGHTSI forced with reanalysis data, to show that for the case study of N-<span class="hlt">ICE</span>2015, snow-<span class="hlt">ice</span> would even form over SYI with an initial thickness of 2 m. In current conditions north of Svalbard, snow-<span class="hlt">ice</span> is ubiquitous and contributes to the thickness growth up to 30%. This contribution is important, especially in the absence of any bottom thermodynamic growth due to the thick insulating snow cover. Growth of FYI north of Svalbard is mainly controlled by the timing of growth onset relative to snow precipitation events and cold spells. These usually short-lived conditions are largely determined by the frequency of storms entering the Arctic from the Atlantic Ocean. In our case, a later freeze onset was favorable for FYI growth due to less snow accumulation in early autumn. This limited snow-<span class="hlt">ice</span> formation but promoted bottom thermodynamic growth. We surmise these findings are related to a regional phenomenon in the Atlantic sector of the Arctic, with frequent storm events which bring increasing amounts of precipitation in autumn and winter, and also affect the duration of cold temperatures required for <span class="hlt">ice</span> growth in winter. We discuss the implications for the importance of snow-<span class="hlt">ice</span> in the future Arctic, formerly believed to be non-existent in the central Arctic due to thick perennial <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.C43D0577F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.C43D0577F"><span>Sea <span class="hlt">Ice</span> and Hydrographic Variability in the Northwest North Atlantic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fenty, I. G.; Heimbach, P.; Wunsch, C. I.</p> <p>2010-12-01</p> <p>Sea <span class="hlt">ice</span> anomalies in the Northwest North Atlantic's Labrador Sea are of climatic interest because of known and hypothesized feedbacks with hydrographic anomalies, deep convection/mode water formation, and Northern Hemisphere atmospheric patterns. As greenhouse gas concentrations increase, hydrographic anomalies formed in the Arctic Ocean associated with warming will propagate into the Labrador Sea via the Fram Strait/West Greenland Current and the Canadian Archipelago/Baffin Island Current. Therefore, understanding the dynamical response of sea <span class="hlt">ice</span> in the basin to hydrographic anomalies is essential for the prediction and interpretation of future high-latitude climate change. Historically, efforts to quantify the link between the observed sea <span class="hlt">ice</span> and hydrographic variability in the region has been limited due to in situ observation paucity and technical challenges associated with synthesizing ocean and sea <span class="hlt">ice</span> observations with numerical models. To elaborate the relationship between sea <span class="hlt">ice</span> and ocean variability, we create three one-year (1992-1993, 1996-1997, 2003-2004) three-dimensional time-varying reconstructions of the ocean and sea <span class="hlt">ice</span> state in Labrador Sea and Baffin Bay. The reconstructions are syntheses of a regional coupled 32 km ocean-sea <span class="hlt">ice</span> model with a suite of contemporary in situ and satellite hydrographic and <span class="hlt">ice</span> data using the adjoint method. The model and data are made consistent, in a least-squares sense, by iteratively adjusting several model control variables (e.g., ocean initial and lateral boundary conditions and the atmospheric state) to minimize an uncertainty-weighted model-data misfit cost function. The reconstructions reveal that the <span class="hlt">ice</span> <span class="hlt">pack</span> attains a state of quasi-equilibrium in mid-March (the annual sea <span class="hlt">ice</span> maximum) in which the total <span class="hlt">ice</span>-covered area reaches a steady state -<span class="hlt">ice</span> production and dynamical divergence along the coasts balances dynamical convergence and melt along the pack’s seaward edge. Sea <span class="hlt">ice</span> advected to the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvL.115n8501T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvL.115n8501T"><span>Theory of the Sea <span class="hlt">Ice</span> Thickness Distribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Toppaladoddi, Srikanth; Wettlaufer, J. S.</p> <p>2015-10-01</p> <p>We use concepts from statistical physics to transform the original evolution equation for the sea <span class="hlt">ice</span> thickness distribution g (h ) from Thorndike et al. into a Fokker-Planck-like conservation law. The steady solution is g (h )=N (q )hqe-h /H, where q and H are expressible in terms of moments over the transition probabilities between thickness categories. The solution exhibits the functional form used in observational fits and shows that for h ≪1 , g (h ) is controlled by both thermodynamics and mechanics, whereas for h ≫1 only mechanics controls g (h ). Finally, we derive the underlying Langevin equation governing the dynamics of the <span class="hlt">ice</span> thickness h , from which we predict the observed g (h ). The genericity of our approach provides a framework for studying the geophysical-scale structure of the <span class="hlt">ice</span> <span class="hlt">pack</span> using methods of broad relevance in statistical mechanics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26551827','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26551827"><span>Theory of the Sea <span class="hlt">Ice</span> Thickness Distribution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Toppaladoddi, Srikanth; Wettlaufer, J S</p> <p>2015-10-02</p> <p>We use concepts from statistical physics to transform the original evolution equation for the sea <span class="hlt">ice</span> thickness distribution g(h) from Thorndike et al. into a Fokker-Planck-like conservation law. The steady solution is g(h)=N(q)h(q)e(-h/H), where q and H are expressible in terms of moments over the transition probabilities between thickness categories. The solution exhibits the functional form used in observational fits and shows that for h≪1, g(h) is controlled by both thermodynamics and mechanics, whereas for h≫1 only mechanics controls g(h). Finally, we derive the underlying Langevin equation governing the dynamics of the <span class="hlt">ice</span> thickness h, from which we predict the observed g(h). The genericity of our approach provides a framework for studying the geophysical-scale structure of the <span class="hlt">ice</span> <span class="hlt">pack</span> using methods of broad relevance in statistical mechanics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvE..91d2203J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvE..91d2203J"><span>Cluster and constraint analysis in tetrahedron <span class="hlt">packings</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jin, Weiwei; Lu, Peng; Liu, Lufeng; Li, Shuixiang</p> <p>2015-04-01</p> <p>The disordered <span class="hlt">packings</span> of tetrahedra often show no obvious macroscopic orientational or positional order for a wide range of <span class="hlt">packing</span> densities, and it has been found that the local order in particle clusters is the main order form of tetrahedron <span class="hlt">packings</span>. Therefore, a cluster analysis is carried out to investigate the local structures and properties of tetrahedron <span class="hlt">packings</span> in this work. We obtain a cluster distribution of differently sized clusters, and peaks are observed at two special clusters, i.e., dimer and wagon wheel. We then calculate the amounts of dimers and wagon wheels, which are observed to have linear or approximate linear correlations with <span class="hlt">packing</span> density. Following our previous work, the amount of particles participating in dimers is used as an order metric to evaluate the order degree of the hierarchical <span class="hlt">packing</span> structure of tetrahedra, and an order map is consequently depicted. Furthermore, a constraint analysis is performed to determine the isostatic or hyperstatic region in the order map. We employ a Monte Carlo algorithm to <span class="hlt">test</span> jamming and then suggest a new maximally random jammed <span class="hlt">packing</span> of hard tetrahedra from the order map with a <span class="hlt">packing</span> density of 0.6337.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.C53B0778M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.C53B0778M"><span>Impact of surface roughness on L-band emissivity of the sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miernecki, M.; Kaleschke, L.; Hendricks, S.; Søbjærg, S. S.</p> <p>2015-12-01</p> <p>In March 2014 a joint experiment IRO2/SMOSice was carried out in the Barents Sea. R/V Lance equipped with meteorological instruments, electromagnetic sea <span class="hlt">ice</span> thickness probe and engine monitoring instruments, was performing a series of <span class="hlt">tests</span> in different <span class="hlt">ice</span> conditions in order to validate the <span class="hlt">ice</span> route optimization (IRO) system, advising on his route through <span class="hlt">pack</span> <span class="hlt">ice</span>. In parallel cal/val activities for sea <span class="hlt">ice</span> thickness product obtained from SMOS (Soil Moisture and Ocean Salinity mission) L-band radiometer were carried out. Apart from helicopter towing the EMbird thickness probe, Polar 5 aircraft was serving the area during the experiment with L-band radiometer EMIRAD2 and Airborne Laser Scanner (ALS) as primary instruments. Sea <span class="hlt">ice</span> Thickness algorithm using SMOS brightness temperature developed at University of Hamburg, provides daily maps of thin sea <span class="hlt">ice</span> (up to 0.5-1 m) in polar regions with resolution of 35-50 km. So far the retrieval method was not taking into account surface roughness, assuming that sea <span class="hlt">ice</span> is a specular surface. Roughness is a stochastic process that can be characterized by standard deviation of surface height σ and by shape of the autocorrelation function R to estimate it's vertical and horizontal scales respectively. Interactions of electromagnetic radiation with the surface of the medium are dependent on R and σ and they scales with respect to the incident wavelength. During SMOSice the radiometer was observing sea <span class="hlt">ice</span> surface at two incidence angles 0 and 40 degrees and simultaneously the surface elevation was scanned with ALS with ground resolution of ~ 0.25 m. This configuration allowed us to calculate σ and R from power spectral densities of surface elevation profiles and quantify the effect of surface roughness on the emissivity of the sea <span class="hlt">ice</span>. First results indicate that Gaussian autocorrelation function is suitable for deformed <span class="hlt">ice</span>, for other <span class="hlt">ice</span> types exponential function is the best fit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007898','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007898"><span>Evaluation of Alternative Altitude Scaling Methods for Thermal <span class="hlt">Ice</span> Protection System in NASA <span class="hlt">Icing</span> Research Tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Sam; Addy, Harold E. Jr.; Broeren, Andy P.; Orchard, David M.</p> <p>2017-01-01</p> <p>A <span class="hlt">test</span> was conducted at NASA <span class="hlt">Icing</span> Research Tunnel to evaluate altitude scaling methods for thermal <span class="hlt">ice</span> protection system. Two new scaling methods based on Weber number were compared against a method based on Reynolds number. The results generally agreed with the previous set of <span class="hlt">tests</span> conducted in NRCC Altitude <span class="hlt">Icing</span> Wind Tunnel where the three methods of scaling were also <span class="hlt">tested</span> and compared along with reference (altitude) <span class="hlt">icing</span> conditions. In those <span class="hlt">tests</span>, the Weber number-based scaling methods yielded results much closer to those observed at the reference <span class="hlt">icing</span> conditions than the Reynolds number-based <span class="hlt">icing</span> conditions. The <span class="hlt">test</span> in the NASA IRT used a much larger, asymmetric airfoil with an <span class="hlt">ice</span> protection system that more closely resembled designs used in commercial aircraft. Following the trends observed during the AIWT <span class="hlt">tests</span>, the Weber number based scaling methods resulted in smaller runback <span class="hlt">ice</span> than the Reynolds number based scaling, and the <span class="hlt">ice</span> formed farther upstream. The results show that the new Weber number based scaling methods, particularly the Weber number with water loading scaling, continue to show promise for <span class="hlt">ice</span> protection system development and evaluation in atmospheric <span class="hlt">icing</span> tunnels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/419613-classification-baltic-sea-ice-types-airborne-multifrequency-microwave-radiometer','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/419613-classification-baltic-sea-ice-types-airborne-multifrequency-microwave-radiometer"><span>Classification of Baltic Sea <span class="hlt">ice</span> types by airborne multifrequency microwave radiometer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kurvonen, L.; Hallikainen, M.</p> <p></p> <p>An airborne multifrequency radiometer (24, 34, 48, and 94 GHz, vertical polarization) was used to investigate the behavior of the brightness temperature of different sea <span class="hlt">ice</span> types in the Gulf of Bothnia (Baltic Sea). The measurements and the main results of the analysis are presented. The measurements were made in dry and wet conditions (air temperature above and below 0 C). The angle of incidence was 45{degree} in all measurements. The following topics are evaluated: (a) frequency dependency of the brightness temperature of different <span class="hlt">ice</span> types, (b) the capability of the multifrequency radiometer to classify <span class="hlt">ice</span> types for winter navigationmore » purposes, and (c) the optimum measurement frequencies for mapping sea <span class="hlt">ice</span>. The weather conditions had a significant impact on the radiometric signatures of some <span class="hlt">ice</span> types (snow-covered compact <span class="hlt">pack</span> <span class="hlt">ice</span> and frost-covered new <span class="hlt">ice</span>); the impact was the highest at 94 GHz. In all cases the overall classification accuracy was around 90% (the kappa coefficient was from 0.86 to 0.96) when the optimum channel combination (24/34 GHz and 94 GHz) was used.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70020441','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70020441"><span>Greenland Sea Odden sea <span class="hlt">ice</span> feature: Intra-annual and interannual variability</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shuchman, R.A.; Josberger, E.G.; Russel, C.A.; Fischer, K.W.; Johannessen, O.M.; Johannessen, J.; Gloersen, P.</p> <p>1998-01-01</p> <p>The "Odden" is a large sea <span class="hlt">ice</span> feature that forms in the east Greenland Sea that may protrude eastward to 5??E from the main sea <span class="hlt">ice</span> <span class="hlt">pack</span> (at about 8??W) between 73?? and 77??N. It generally forms at the beginning of the winter season and can cover 300,000 km2. Throughout the winter the outer edge of the Odden may advance and retreat by several hundred kilometers on timescales of a few days to weeks. Satellite passive microwave observations from 1978 through 1995 provide a continuous record of the spatial and temporal variations of this extremely dynamic phenomenon. Aircraft synthetic aperture radar, satellite passive microwave, and ship observations in the Odden show that the Odden consists of new <span class="hlt">ice</span> types, rather than older <span class="hlt">ice</span> types advected eastward from the main <span class="hlt">pack</span>. The 17-year record shows both strong interannual and intra-annual variations in Odden extent and temporal behavior. For example, in 1983 the Odden was weak, in 1984 the Odden did not occur, and in 1985 the Odden returned late in the season. An analysis of the <span class="hlt">ice</span> area and extent time series derived from the satellite passive microwave observations along with meteorological data from the International Arctic Buoy Program (IABP) determined the meteorological forcing associated with Odden growth, maintenance, and decay. The key meteorological parameters that are related to the rapid <span class="hlt">ice</span> formation and decay associated with the Odden are, in order of importance, air temperature, wind speed, and wind direction. Oceanographic parameters must play an important role in controlling Odden formation, but it is not yet possible to quantify this role because of a lack of long-term oceanographic observations. Copyright 1998 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980237537','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980237537"><span>Spatial Distribution of Trends and Seasonality in the Hemispheric Sea <span class="hlt">Ice</span> Covers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gloersen, P.; Parkinson, C. L.; Cavalieri, D. J.; Cosmiso, J. C.; Zwally, H. J.</p> <p>1998-01-01</p> <p>We extend earlier analyses of a 9-year sea <span class="hlt">ice</span> data set that described the local seasonal and trend variations in each of the hemispheric sea <span class="hlt">ice</span> covers to the recently merged 18.2-year sea <span class="hlt">ice</span> record from four satellite instruments. The seasonal cycle characteristics remain essentially the same as for the shorter time series, but the local trends are markedly different, in some cases reversing sign. The sign reversal reflects the lack of a consistent long-term trend and could be the result of localized long-term oscillations in the hemispheric sea <span class="hlt">ice</span> covers. By combining the separate hemispheric sea <span class="hlt">ice</span> records into a global one, we have shown that there are statistically significant net decreases in the sea <span class="hlt">ice</span> coverage on a global scale. The change in the global sea <span class="hlt">ice</span> extent, is -0.01 +/- 0.003 x 10(exp 6) sq km per decade. The decrease in the areal coverage of the sea <span class="hlt">ice</span> is only slightly smaller, so that the difference in the two, the open water within the <span class="hlt">packs</span>, has no statistically significant change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005552','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005552"><span>ICESat Observations of Seasonal and Interannual Variations of Sea-<span class="hlt">Ice</span> Freeboard and Estimated Thickness in the Weddell Sea, Antarctica (2003-2009)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yi, Donghui; Robbins, John W.</p> <p>2010-01-01</p> <p>Sea-<span class="hlt">ice</span> freeboard heights for 17 ICESat campaign periods from 2003 to 2009 are derived from ICESat data. Freeboard is combined with snow depth from Advanced Microwave Scanning Radiometer for Earth Observing System (AMSR-E) data and nominal densities of snow, water and sea <span class="hlt">ice</span>, to estimate sea-<span class="hlt">ice</span> thickness. Sea-<span class="hlt">ice</span> freeboard and thickness distributions show clear seasonal variations that reflect the yearly cycle of growth and decay of the Weddell Sea (Antarctica) <span class="hlt">pack</span> <span class="hlt">ice</span>. During October-November, sea <span class="hlt">ice</span> grows to its seasonal maximum both in area and thickness; the mean freeboards are 0.33-0.41 m and the mean thicknesses are 2.10-2.59 m. During February-March, thinner sea <span class="hlt">ice</span> melts away and the sea-<span class="hlt">ice</span> <span class="hlt">pack</span> is mainly distributed in the west Weddell Sea; the mean freeboards are 0.35-0.46 m and the mean thicknesses are 1.48-1.94 m. During May-June, the mean freeboards and thicknesses are 0.26-0.29 m and 1.32-1.37 m, respectively. The 6 year trends in sea-<span class="hlt">ice</span> extent and volume are (0.023+/-0.051) x 10(exp 6)sq km/a (0.45%/a) and (0.007+/-1.0.092) x 10(exp 3)cu km/a (0.08%/a); however, the large standard deviations indicate that these positive trends are not statistically significant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950038689&hterms=glacier+melt&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dglacier%2Bmelt','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950038689&hterms=glacier+melt&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dglacier%2Bmelt"><span>Radar measurements of melt zones on the Greenland <span class="hlt">Ice</span> Sheet</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jezek, Kenneth C.; Gogineni, Prasad; Shanableh, M.</p> <p>1994-01-01</p> <p>Surface-based microwave radar measurements were performed at a location on the western flank of the Greenland <span class="hlt">Ice</span> Sheet. Here, firn metamorphasis is dominated by seasonal melt, which leads to marked contrasts in the vertical structure of winter and summer firn. This snow regime is also one of the brightest radar targets on Earth with an average backscatter coefficient of 0 dB at 5.3 GHz and an incidence angle of 25 deg. By combining detailed observations of firn physical properties with ranging radar measurements we find that the glaciological mechanism associated with this strong electromagnetic response is summer <span class="hlt">ice</span> lens formation within the previous winter's snow <span class="hlt">pack</span>. This observation has important implications for monitoring and understanding changes in <span class="hlt">ice</span> sheet volume using spaceborne microwave sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.C31A0435M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.C31A0435M"><span>Help, I don’t know which sea <span class="hlt">ice</span> algorithm to use?!: Developing an authoritative sea <span class="hlt">ice</span> climate data record</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meier, W.; Stroeve, J.; Duerr, R. E.; Fetterer, F. M.</p> <p>2009-12-01</p> <p>The declining Arctic sea <span class="hlt">ice</span> is one of the most dramatic indicators of climate change and is being recognized as a key factor in future climate impacts on biology, human activities, and global climate change. As such, the audience for sea <span class="hlt">ice</span> data is expanding well beyond the sea <span class="hlt">ice</span> community. The most comprehensive sea <span class="hlt">ice</span> data are from a series of satellite-borne passive microwave sensors. They provide a near-complete daily timeseries of sea <span class="hlt">ice</span> concentration and extent since late-1978. However, there are many complicating issues in using such data, particularly for novice users. First, there is not one single, definitive algorithm, but several. And even for a given algorithm, different processing and quality-control methods may be used, depending on the source. Second, for all algorithms, there are uncertainties in any retrieved value. In general, these limitations are well-known: low spatial-resolution results in an imprecise <span class="hlt">ice</span> edge determination and lack of small-scale detail (e.g., lead detection) within the <span class="hlt">ice</span> <span class="hlt">pack</span>; surface melt depresses concentration values during summer; thin <span class="hlt">ice</span> is underestimated in some algorithms; some algorithms are sensitive to physical surface temperature; other surface features (e.g., snow) can influence retrieved data. While general error estimates are available for concentration values, currently the products do not carry grid-cell level or even granule level data quality information. Finally, metadata and data provenance information are limited, both of which are essential for future reprocessing. Here we describe the progress to date toward development of sea <span class="hlt">ice</span> concentration products and outline the future steps needed to complete a sea <span class="hlt">ice</span> climate data record.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.7235C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.7235C"><span>Meteorological conditions in a thinner Arctic sea <span class="hlt">ice</span> regime from winter to summer during the Norwegian Young Sea <span class="hlt">Ice</span> expedition (N-<span class="hlt">ICE</span>2015)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cohen, Lana; Hudson, Stephen R.; Walden, Von P.; Graham, Robert M.; Granskog, Mats A.</p> <p>2017-07-01</p> <p>Atmospheric measurements were made over Arctic sea <span class="hlt">ice</span> north of Svalbard from winter to early summer (January-June) 2015 during the Norwegian Young Sea <span class="hlt">Ice</span> (N-<span class="hlt">ICE</span>2015) expedition. These measurements, which are available publicly, represent a comprehensive meteorological data set covering the seasonal transition in the Arctic Basin over the new, thinner sea <span class="hlt">ice</span> regime. Winter was characterized by a succession of storms that produced short-lived (less than 48 h) temperature increases of 20 to 30 K at the surface. These storms were driven by the hemispheric scale circulation pattern with a large meridional component of the polar jet stream steering North Atlantic storms into the high Arctic. Nonstorm periods during winter were characterized by strong surface temperature inversions due to strong radiative cooling ("radiatively clear state"). The strength and depth of these inversions were similar to those during the Surface Heat Budget of the Arctic Ocean (SHEBA) campaign. In contrast, atmospheric profiles during the "opaquely cloudy state" were different to those from SHEBA due to differences in the synoptic conditions and location within the <span class="hlt">ice</span> <span class="hlt">pack</span>. Storm events observed during spring/summer were the result of synoptic systems located in the Barents Sea and the Arctic Basin rather than passing directly over N-<span class="hlt">ICE</span>2015. These synoptic systems were driven by a large-scale circulation pattern typical of recent years, with an Arctic Dipole pattern developing during June. Surface temperatures became near-constant 0°C on 1 June marking the beginning of summer. Atmospheric profiles during the spring and early summer show persistent lifted temperature and moisture inversions that are indicative of clouds and cloud processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930013511','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930013511"><span>The influence of the hydrologic cycle on the extent of sea <span class="hlt">ice</span> with climatic implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dean, Kenneson G.; Stringer, William J.; Searcy, Craig</p> <p>1993-01-01</p> <p>Multi-temporal satellite images, field observations, and field measurements were used to investigate the mechanisms by which sea <span class="hlt">ice</span> melts offshore from the Mackenzie River delta. Advanced Very High Resolution Radiometer (AVHRR) satellite data recorded in 1986 were analyzed. The satellite data were geometrically corrected and radiometrically calibrated so that albedo and temperature values could be extracted. The investigation revealed that sea <span class="hlt">ice</span> melted approximately 2 weeks earlier offshore from the Mackenzie River delta than along coasts where river discharge is minimal or non-existent. There is significant intra-delta variability in the timing and patterns of <span class="hlt">ice</span> melt. An estimation of energy flux indicates that 30 percent more of the visible wavelength energy and 25 percent more of the near-infrared wavelength energy is absorbed by water offshore of the delta compared to coastal areas with minimal river discharge. The analysis also revealed that the removal of sea <span class="hlt">ice</span> involves the following: over-<span class="hlt">ice</span>-flooding along the coast offshore from river delta channels; under-<span class="hlt">ice</span> flow of 'warm' river water; melting and calving of the fast <span class="hlt">ice</span>; and, the formation of a bight in the <span class="hlt">pack</span> <span class="hlt">ice</span> edge. Two stages in the melting of sea <span class="hlt">ice</span> were identified: (1) an early stage where heat is supplied to overflows largely by solar radiation, and (2) a later stage where heat is supplied by river discharge in addition to solar radiation. A simple thermodynamic model of the thaw process in the fast <span class="hlt">ice</span> zone was developed and parameterized based on events recorded by the satellite images. The model treats river discharge as the source of sensible heat at the base of the <span class="hlt">ice</span> cover. The results of a series of sensitivity <span class="hlt">tests</span> to assess the influence of river discharge on the near shore <span class="hlt">ice</span> are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007926','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007926"><span>Preliminary Evaluation of Altitude Scaling for Turbofan Engine <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsao, Jen-Ching</p> <p>2017-01-01</p> <p>Preliminary evaluation of altitude scaling for turbofan engine <span class="hlt">ice</span> crystal <span class="hlt">icing</span> simulation was conducted during the 2015 LF11 engine <span class="hlt">icing</span> <span class="hlt">test</span> campaign in PSL.The results showed that a simplified approach for altitude scaling to simulate the key reference engine <span class="hlt">ice</span> growth feature and associated <span class="hlt">icing</span> effects to the engine is possible. But special considerations are needed to address the facility operation limitation for lower altitude engine <span class="hlt">icing</span> simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C43B0756M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C43B0756M"><span>Laboratory Studies of Sea-<span class="hlt">Ice</span>-Wave Interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monty, J.; Meylan, M. H.; Babanin, A. V.; Toffoli, A.; Bennetts, L.</p> <p>2016-12-01</p> <p>A world-first facility for studying the Marginal <span class="hlt">Ice</span> Zone has been constructed in the Michell Hydrodynamics Laboratory at the University of Melbourne. A 14m long wave tank (0.75m wide, 0.6m deep) resides in a freezer, where air temperature can be controlled down to -15C. This permits the freezing of the water surface. Large stainless steel <span class="hlt">ice</span>-making trays (up to 4 m long) are also available to create <span class="hlt">ice</span> of desired thickness and microstructure, which can be lowered onto the water surface. A computer controlled wave generator is capable of creating waves of any desired form. The temperature of the water in the tank can also be controlled between 2 and 30C. The tank frame is constructed of marine-treated wood and the entire tank is glass and acrylic, permitting the use of corrosive fluids, such as salt water. Here we present the first laboratory experiments of break-up of a controlled thickness, fresh water <span class="hlt">ice</span> sheet impacted by regular and JONSWAP spectrum surface waves. The geometry of the resultant <span class="hlt">ice</span>-floes is measured with high-resolution, time-resolved imaging, providing the crucial data of floe size distribution. Initial observations show that, in the case of high steepness waves, the primary mechanisms of <span class="hlt">ice</span> break-up at the <span class="hlt">ice</span> edge are overwash and rafting, both of which put weight on the <span class="hlt">ice</span> interior to the <span class="hlt">ice</span>-water interface. This additional weight (and impact in the case of rafting) breaks more <span class="hlt">ice</span>, which allows overwash and rafting deeper into the <span class="hlt">ice</span> sheet, breaking more <span class="hlt">ice</span> and so on. For lower steepness waves, overwash and rafting are still present but far less significant. Finally, results of vertical <span class="hlt">ice</span> movement using laser height gauges will be presented showing the attenuation of waves into an <span class="hlt">ice</span> sheet and through a <span class="hlt">pack</span> of <span class="hlt">ice</span> floes. These results are compared with field data and theory available (e.g. Squire & Moore, Nature, 1980 and Kohout et al., Nature, 2014).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150019656','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150019656"><span>Method to Generate Full-Span <span class="hlt">Ice</span> Shape on Swept Wing Using <span class="hlt">Icing</span> Tunnel Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Sam; Camello, Stephanie</p> <p>2015-01-01</p> <p>There is a collaborative research program by NASA, FAA, ONERA, and university partners to improve the fidelity of experimental and computational simulation methods for swept-wing <span class="hlt">ice</span> accretion formulations and resultant aerodynamic effects on large transport aircraft. This research utilizes a 65 scale Common Research Model as the baseline configuration. In order to generate the <span class="hlt">ice</span> shapes for the aerodynamic <span class="hlt">testing</span>, <span class="hlt">ice</span>-accretion <span class="hlt">testing</span> will be conducted in the NASA <span class="hlt">Icing</span> Research Tunnel utilizing hybrid model from the 20, 64, and 83 spanwise locations. The models will have full-scale leading edges with truncated chord in order to fit the IRT <span class="hlt">test</span> section. The <span class="hlt">ice</span> shapes from the IRT <span class="hlt">tests</span> will be digitized using a commercially available articulated-arm 3D laser scanning system. The methodology to acquire 3D <span class="hlt">ice</span> shapes using a laser scanner was developed and validated in a previous research effort. Each of these models will yield a 1.5ft span of <span class="hlt">ice</span> than can be used. However, a full-span <span class="hlt">ice</span> accretion will require 75 ft span of <span class="hlt">ice</span>. This means there will be large gaps between these spanwise <span class="hlt">ice</span> sections that must be filled, while maintaining all of the important aerodynamic features. A method was developed to generate a full-span <span class="hlt">ice</span> shape from the three 1.5 ft span <span class="hlt">ice</span> shapes from the three models.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910031156&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmarginal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910031156&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmarginal"><span>Wave evolution in the marginal <span class="hlt">ice</span> zone - Model predictions and comparisons with on-site and remote data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, A. K.; Holt, B.; Vachon, P. W.</p> <p>1989-01-01</p> <p>The ocean-wave dispersion relation and viscous attenuation by a sea <span class="hlt">ice</span> cover were studied for waves in the marginal <span class="hlt">ice</span> zone (MIZ). The Labrador <span class="hlt">ice</span> margin experiment (Limex), conducted off the east coast of Newfoundland, Canada in March 1987, provided aircraft SAR, wave buoy, and <span class="hlt">ice</span> property data. Based on the wave number spectrum from SAR data, the concurrent wave frequency spectrum from ocean buoy data, and accelerometer data on the <span class="hlt">ice</span> during Limex '87, the dispersion relation has been derived and compared with the model. Accelerometers were deployed at the <span class="hlt">ice</span> edge and into the <span class="hlt">ice</span> <span class="hlt">pack</span>. Data from the accelerometers were used to estimate wave energy attenuation rates and compared with the model. The model-data comparisons are reasonably good for the <span class="hlt">ice</span> conditions observed during Limex' 87.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140008692','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140008692"><span>PSL <span class="hlt">Icing</span> Facility Upgrade Overview</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Griffin, Thomas A.; Dicki, Dennis J.; Lizanich, Paul J.</p> <p>2014-01-01</p> <p>The NASA Glenn Research Center Propulsion Systems Lab (PSL) was recently upgraded to perform engine inlet <span class="hlt">ice</span> crystal <span class="hlt">testing</span> in an altitude environment. The system installed 10 spray bars in the inlet plenum for <span class="hlt">ice</span> crystal generation using 222 spray nozzles. As an altitude <span class="hlt">test</span> chamber, the PSL is capable of simulating <span class="hlt">icing</span> events at altitude in a groundtest facility. The system was designed to operate at altitudes from 4,000 to 40,000 ft at Mach numbers up to 0.8M and inlet total temperatures from -60 to +15 degF. This paper and presentation will be part of a series of presentations on PSL <span class="hlt">Icing</span> and will cover the development of the <span class="hlt">icing</span> capability through design, developmental <span class="hlt">testing</span>, installation, initial calibration, and validation engine <span class="hlt">testing</span>. Information will be presented on the design criteria and process, spray bar developmental <span class="hlt">testing</span> at Cox and Co., system capabilities, and initial calibration and engine validation <span class="hlt">test</span>. The PSL <span class="hlt">icing</span> system was designed to provide NASA and the <span class="hlt">icing</span> community with a facility that could be used for research studies of engine <span class="hlt">icing</span> by duplicating in-flight events in a controlled ground-<span class="hlt">test</span> facility. With the system and the altitude chamber we can produce flight conditions and cloud environments to simulate those encountered in flight. The <span class="hlt">icing</span> system can be controlled to set various cloud uniformities, droplet median volumetric diameter (MVD), and <span class="hlt">icing</span> water content (IWC) through a wide variety of conditions. The PSL chamber can set altitudes, Mach numbers, and temperatures of interest to the <span class="hlt">icing</span> community and also has the instrumentation capability of measuring engine performance during <span class="hlt">icing</span> <span class="hlt">testing</span>. PSL last year completed the calibration and initial engine validation of the facility utilizing a Honeywell ALF502-R5 engine and has duplicated in-flight roll back conditions experienced during flight <span class="hlt">testing</span>. This paper will summarize the modifications and buildup of the facility to accomplish these <span class="hlt">tests</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17781630','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17781630"><span>The surface of the <span class="hlt">ice</span>-age Earth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p></p> <p>1976-03-19</p> <p>In the Northern Hemisphere the 18,000 B.P. world differed strikingly from the present in the huge land-based <span class="hlt">ice</span> sheets, reaching approximately 3 km in thickness, and in a dramatic increase in the extent of <span class="hlt">pack</span> <span class="hlt">ice</span> and marine-based <span class="hlt">ice</span> sheets. In the Southern Hemisphere the most striking contrast was the greater extent of sea <span class="hlt">ice</span>. On land, grasslands, steppes, and deserts spread at the expense of forests. This change in vegetation, together with extensive areas of permanent <span class="hlt">ice</span> and sandy outwash plains, caused an increase in global surface albedo over modern values. Sea level was lower by at least 85 m. The 18,000 B.P. oceans were characterized by: (i) marked steepening of thermal gradients along polar frontal systems, particularly in the North Atlantic and Antarctic; (ii) an equatorward displacement of polar frontal systems; (iii) general cooling of most surface waters, with a global average of -2.3 degrees C; (iv) increased cooling and up-welling along equatorial divergences in the Pacific and Atlantic; (v) low temperatures extending equatorward along the western coast of Africa, Australia, and South America, indicating increased upwelling and advection of cool waters; and (vi) nearly stable positions and temperatures of the central gyres in the subtropical Atlantic, Pacific, and Indian oceans.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6293171-place-burning-crude-oil-broken-ice-testing-ohmsett-oil-hazardous-materials-simulated-environmental-test-tank','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6293171-place-burning-crude-oil-broken-ice-testing-ohmsett-oil-hazardous-materials-simulated-environmental-test-tank"><span>In-place burning of crude oil in broken <span class="hlt">ice</span>: 1985 <span class="hlt">testing</span> at OHMSETT (Oil and Hazardous Materials Simulated Environmental <span class="hlt">Test</span> Tank)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Smith, N.K.; Diaz, A.</p> <p>1985-08-01</p> <p>In January and March of 1985, in-place oil burning <span class="hlt">tests</span> were conducted at the U.S. Environmental Protection Agency's Oil and Hazardous Materials Simulated Environmental <span class="hlt">Test</span> Tank. (OHMSETT) facility in Leonardo, New Jersey. In-place combustion of Prudhoe Bay and Amauligak crude oil slicks was attempted in varying <span class="hlt">ice</span> coverages, oil conditions, and ambient conditions. An emulsion of Amauligak crude oil and water was also ignited three times and burned in 80% <span class="hlt">ice</span> cover, removing nearly 50% of the emulsion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910004108','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910004108"><span>A review of <span class="hlt">ice</span> accretion data from a model rotor <span class="hlt">icing</span> <span class="hlt">test</span> and comparison with theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Britton, Randall K.; Bond, Thomas H.</p> <p>1991-01-01</p> <p>An experiment was conducted by the Helicopter <span class="hlt">Icing</span> Consortium (HIC) in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel (IRT) in which a 1/6 scale fuselage model of a UH-60A Black Hawk helicopter with a generic rotor was subjected to a wide range of <span class="hlt">icing</span> conditions. The HIC consists of members from NASA, Bell Helicopter, Boeing Helicopter, McDonnell Douglas Helicopters, Sikorsky Aircraft, and Texas A&M University. Data was taken in the form of rotor torque, internal force balance measurements, blade strain gage loading, and two dimensional <span class="hlt">ice</span> shape tracings. A review of the <span class="hlt">ice</span> shape data is performed with special attention given to repeatability and correctness of trends in terms of radial variation, rotational speed, <span class="hlt">icing</span> time, temperature, liquid water content, and volumetric median droplet size. Moreover, an indepth comparison between the experimental data and the analysis of NASA's <span class="hlt">ice</span> accretion code LEWICE is given. Finally, conclusions are drawn as to the quality of the <span class="hlt">ice</span> accretion data and the predictability of the data base as a whole. Recommendations are also given for improving data taking technique as well as potential future work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24769440','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24769440"><span>Water promotes the sealing of nanoscale <span class="hlt">packing</span> defects in folding proteins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fernández, Ariel</p> <p>2014-05-21</p> <p>A net dipole moment is shown to arise from a non-Debye component of water polarization created by nanoscale <span class="hlt">packing</span> defects on the protein surface. Accordingly, the protein electrostatic field exerts a torque on the induced dipole, locally impeding the nucleation of <span class="hlt">ice</span> at the protein-water interface. We evaluate the solvent orientation steering (SOS) as the reversible work needed to align the induced dipoles with the Debye electrostatic field and computed the SOS for the variable interface of a folding protein. The minimization of the SOS is shown to drive protein folding as evidenced by the entrainment of the total free energy by the SOS energy along trajectories that approach a Debye limit state where no torque arises. This result suggests that the minimization of anomalous water polarization at the interface promotes the sealing of <span class="hlt">packing</span> defects, thereby maintaining structural integrity and committing the protein chain to fold.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950024430','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950024430"><span>A laser-based <span class="hlt">ice</span> shape profilometer for use in <span class="hlt">icing</span> wind tunnels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hovenac, Edward A.; Vargas, Mario</p> <p>1995-01-01</p> <p>A laser-based profilometer was developed to measure the thickness and shape of <span class="hlt">ice</span> accretions on the leading edge of airfoils and other models in <span class="hlt">icing</span> wind tunnels. The instrument is a hand held device that is connected to a desk top computer with a 10 meter cable. It projects a laser line onto an <span class="hlt">ice</span> shape and used solid state cameras to detect the light scattered by the <span class="hlt">ice</span>. The instrument corrects the image for camera angle distortions, displays an outline of the <span class="hlt">ice</span> shape on the computer screen, saves the data on a disk, and can print a full scale drawing of the <span class="hlt">ice</span> shape. The profilometer has undergone extensive <span class="hlt">testing</span> in the laboratory and in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel. Results of the <span class="hlt">tests</span> show very good agreement between profilometer measurements and known simulated <span class="hlt">ice</span> shapes and fair agreement between profilometer measurements and hand tracing techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25384192','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25384192"><span>The interaction of propionic and butyric acids with <span class="hlt">ice</span> and HNO₃-doped <span class="hlt">ice</span> surfaces at 195-212 K.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Romanias, Manolis N; Papadimitriou, Vassileios C; Papagiannakopoulos, Panos</p> <p>2014-12-04</p> <p>The interaction of propionic and butyric acids on <span class="hlt">ice</span> and HNO3-doped <span class="hlt">ice</span> were studied between 195 and 212 K and low concentrations, using a Knudsen flow reactor coupled with a quadrupole mass spectrometer. The initial uptake coefficients (γ0) of propionic and butyric acids on <span class="hlt">ice</span> as a function of temperature are given by the expressions: γ0(T) = (7.30 ± 1.0) × 10(-10) exp[(3216 ± 478)/T] and γ0(T) = (6.36 ± 0.76) × 10(-11) exp[(3810 ± 434)/T], respectively; the quoted error limits are at 95% level of confidence. Similarly, γ0 of propionic acid on 1.96 wt % (A) and 7.69 wt % (B) HNO3-doped <span class="hlt">ice</span> with temperature are given as γ(0,A)(T) = (2.89 ± 0.26) × 10(-8) exp[(2517 ± 266)/T] and γ(0,B)(T) = (2.77 ± 0.29) × 10(-7) exp[(2126 ± 206)/T], respectively. The results show that γ0 of C1 to C4 n-carboxylic acids on <span class="hlt">ice</span> increase with the alkyl-group length, due to lateral interactions between alkyl-groups that favor a more perpendicular orientation and well <span class="hlt">packing</span> of H-bonded monomers on <span class="hlt">ice</span>. The high uptakes (>10(15) molecules cm(-2)) and long recovery signals indicate efficient growth of random multilayers above the first monolayer driven by significant van der Waals interactions. The heterogeneous loss of both acids on <span class="hlt">ice</span> and HNO3-doped <span class="hlt">ice</span> particles in dense cirrus clouds is estimated to take a few minutes, signifying rapid local heterogeneous removal by dense cirrus clouds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA167187','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA167187"><span>An Evaluation of Foods Processed in Tray <span class="hlt">Pack</span> versus Two Standard Food Service Containers. Part 1. Sensory, Container and Bacteriological <span class="hlt">Tests</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1986-02-01</p> <p>precooked frozen <span class="hlt">packed</span> foods; (2) shelf life of Tray <span class="hlt">Pack</span> vs. the no. 10 can at ambient and stressful storage temperatures; (3) changes in nutrient...bacteriological <span class="hlt">tests</span> to certify safety for human consumption. Both Natick RD&E Center and Kraft products were subjected to 9 I...heat processed products that were storage temperature stressed at 380 C, QS data indicated that expected storage life of seven of the CC products was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150019752','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150019752"><span>Preliminary Findings of Inflight <span class="hlt">Icing</span> Field <span class="hlt">Test</span> to Support <span class="hlt">Icing</span> Remote Sensing Technology Assessment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, Michael; Reehorst, Andrew; Serke, Dave</p> <p>2015-01-01</p> <p>NASA and the National Center for Atmospheric Research have developed an <span class="hlt">icing</span> remote sensing technology that has demonstrated skill at detecting and classifying <span class="hlt">icing</span> hazards in a vertical column above an instrumented ground station. This technology has recently been extended to provide volumetric coverage surrounding an airport. Building on the existing vertical pointing system, the new method for providing volumetric coverage will utilize a vertical pointing cloud radar, a multifrequency microwave radiometer with azimuth and elevation pointing, and a NEXRAD radar. The new terminal area <span class="hlt">icing</span> remote sensing system processes the data streams from these instruments to derive temperature, liquid water content, and cloud droplet size for each examined point in space. These data are then combined to ultimately provide <span class="hlt">icing</span> hazard classification along defined approach paths into an airport.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080022412','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080022412"><span><span class="hlt">Ice</span>Val DatAssistant: An Interactive, Automated <span class="hlt">Icing</span> Data Management System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levinson, Laurie H.; Wright, William B.</p> <p>2008-01-01</p> <p>As with any scientific endeavor, the foundation of <span class="hlt">icing</span> research at the NASA Glenn Research Center (GRC) is the data acquired during experimental <span class="hlt">testing</span>. In the case of the GRC <span class="hlt">Icing</span> Branch, an important part of this data consists of <span class="hlt">ice</span> tracings taken following <span class="hlt">tests</span> carried out in the GRC <span class="hlt">Icing</span> Research Tunnel (IRT), as well as the associated operational and environmental conditions documented during these <span class="hlt">tests</span>. Over the years, the large number of experimental runs completed has served to emphasize the need for a consistent strategy for managing this data. To address the situation, the <span class="hlt">Icing</span> Branch has recently elected to implement the <span class="hlt">Ice</span>Val DatAssistant automated data management system. With the release of this system, all publicly available IRT-generated experimental <span class="hlt">ice</span> shapes with complete and verifiable conditions have now been compiled into one electronically-searchable database. Simulation software results for the equivalent conditions, generated using the latest version of the LEWICE <span class="hlt">ice</span> shape prediction code, are likewise included and are linked to the corresponding experimental runs. In addition to this comprehensive database, the <span class="hlt">Ice</span>Val system also includes a graphically-oriented database access utility, which provides reliable and easy access to all data contained in the database. In this paper, the issues surrounding historical <span class="hlt">icing</span> data management practices are discussed, as well as the anticipated benefits to be achieved as a result of migrating to the new system. A detailed description of the software system features and database content is also provided; and, finally, known issues and plans for future work are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070031804','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070031804"><span><span class="hlt">Ice</span>Val DatAssistant: An Interactive, Automated <span class="hlt">Icing</span> Data Management System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levinson, Laurie H.; Wright, William B.</p> <p>2008-01-01</p> <p>As with any scientific endeavor, the foundation of <span class="hlt">icing</span> research at the NASA Glenn Research Center (GRC) is the data acquired during experimental <span class="hlt">testing</span>. In the case of the GRC <span class="hlt">Icing</span> Branch, an important part of this data consists of <span class="hlt">ice</span> tracings taken following <span class="hlt">tests</span> carried out in the GRC <span class="hlt">Icing</span> Research Tunnel (IRT), as well as the associated operational and environmental conditions during those <span class="hlt">tests</span>. Over the years, the large number of experimental runs completed has served to emphasize the need for a consistent strategy to manage the resulting data. To address this situation, the <span class="hlt">Icing</span> Branch has recently elected to implement the <span class="hlt">Ice</span>Val DatAssistant automated data management system. With the release of this system, all publicly available IRT-generated experimental <span class="hlt">ice</span> shapes with complete and verifiable conditions have now been compiled into one electronically-searchable database; and simulation software results for the equivalent conditions, generated using the latest version of the LEWICE <span class="hlt">ice</span> shape prediction code, are likewise included and linked to the corresponding experimental runs. In addition to this comprehensive database, the <span class="hlt">Ice</span>Val system also includes a graphically-oriented database access utility, which provides reliable and easy access to all data contained in the database. In this paper, the issues surrounding historical <span class="hlt">icing</span> data management practices are discussed, as well as the anticipated benefits to be achieved as a result of migrating to the new system. A detailed description of the software system features and database content is also provided; and, finally, known issues and plans for future work are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170000246','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170000246"><span>Modeling of Highly Instrumented Honeywell Turbofan Engine <span class="hlt">Tested</span> with <span class="hlt">Ice</span> Crystal Ingestion in the NASA Propulsion System Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Veres, Joseph P.; Jorgenson, Philip C. E.; Jones, Scott M.</p> <p>2016-01-01</p> <p>The Propulsion Systems Laboratory (PSL), an altitude <span class="hlt">test</span> facility at NASA Glenn Research Center, has been used to <span class="hlt">test</span> a highly instrumented turbine engine at simulated altitude operating conditions. This is a continuation of the PSL <span class="hlt">testing</span> that successfully duplicated the <span class="hlt">icing</span> events that were experienced in a previous engine (serial LF01) during flight through <span class="hlt">ice</span> crystal clouds, which was the first turbofan engine <span class="hlt">tested</span> in PSL. This second model of the ALF502R-5A serial number LF11 is a highly instrumented version of the previous engine. The PSL facility provides a continuous cloud of <span class="hlt">ice</span> crystals with controlled characteristics of size and concentration, which are ingested by the engine during operation at simulated altitudes. Several of the previous operating points <span class="hlt">tested</span> in the LF01 engine were duplicated to confirm repeatability in LF11. The instrumentation included video cameras to visually illustrate the accretion of <span class="hlt">ice</span> in the low pressure compressor (LPC) exit guide vane region in order to confirm the <span class="hlt">ice</span> accretion, which was suspected during the <span class="hlt">testing</span> of the LF01. Traditional instrumentation included static pressure taps in the low pressure compressor inner and outer flow path walls, as well as total pressure and temperature rakes in the low pressure compressor region. The <span class="hlt">test</span> data was utilized to determine the losses and blockages due to accretion in the exit guide vane region of the LPC. Multiple data points were analyzed with the Honeywell Customer Deck. A full engine roll back point was modeled with the Numerical Propulsion System Simulation (NPSS) code. The mean line compressor flow analysis code with <span class="hlt">ice</span> crystal modeling was utilized to estimate the parameters that indicate the risk of accretion, as well as to estimate the degree of blockage and losses caused by accretion during a full engine roll back point. The analysis provided additional validation of the <span class="hlt">icing</span> risk parameters within the LPC, as well as the creation of models for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..108e2073Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..108e2073Y"><span>Wind Tunnel <span class="hlt">Tests</span> on Aerodynamic Characteristics of two types of <span class="hlt">Iced</span> Conductors with Elastic Support</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yi, You; Cheng, He; Xinxin, Wang</p> <p>2018-01-01</p> <p>The wind tunnel <span class="hlt">tests</span> were carried out to obtain the variation laws of static aerodynamic characteristics of crescent and D-shape <span class="hlt">iced</span> conductor with different wind velocities, wind attack angles and torsional elastic support stiffness. <span class="hlt">Test</span> results show that the variation of wind velocity has a relatively large influence on the aerodynamic coefficients of crescent conductor with torsional elastic support 1. However, the influence on that of D-shape conductor is not obvious. With the increase of the torsional elastic support stiffness, the lift and moment coefficient curves of the crescent <span class="hlt">iced</span> conductor form an obvious peak phenomenon in the range of 0 ° ∼30°. Meanwhile, the wind attack angle position corresponding to the maximum value of the lift and moment coefficients of the D-shape <span class="hlt">iced</span> conductor appear a backward moving phenomenon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040172041&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dbalance%2Bsheet','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040172041&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dbalance%2Bsheet"><span>Advances in Measuring Antarctic Sea-<span class="hlt">Ice</span> Thickness and <span class="hlt">Ice</span>-Sheet Elevations with ICESat Laser Altimetry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zwally, H. Jay</p> <p>2004-01-01</p> <p> elevation changes over select areas of the <span class="hlt">ice</span> sheet is demonstrated with using both crossover analysis and precise-repeat track analysis. Sea <span class="hlt">ice</span> freeboard-height distributions over the Antarctic sea <span class="hlt">pack</span> are derived over distances of 50 km and converted into maps of average freeboard thickness and sea-<span class="hlt">ice</span> thickness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810023062','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810023062"><span><span class="hlt">Ice</span> sheet altimetry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brooks, R. L.</p> <p>1981-01-01</p> <p>Generalized surface slopes were computed for the Antarctic and Greenland <span class="hlt">ice</span> sheets by differencing plotted contour levels and dividing them by the distance between the contours. It was observed that more than 90% of the <span class="hlt">ice</span> sheets have surface slopes less than 1%. Seasat <span class="hlt">test</span> mode-1 Seasat altimeter measurements over Greenland were analyzed by comparisons with collinear and intersecting normal mode Seasat altimeter passes. Over the <span class="hlt">ice</span> sheet, the computed surface elevations from <span class="hlt">test</span> mode-1 measurements were consistently lower by about 45 m and the AGC levels were down by approximately 6 dB. No <span class="hlt">test</span> mode-1 data were acquired over Antarctica. It is concluded that analysis of the existing altimeter data base over the two <span class="hlt">ice</span> sheets is crucial in designing a future improved altimeter tracking capability. It is recommended that additional waveform retracking be performed to characterize <span class="hlt">ice</span> sheet topography as a function of geographic area and elevation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008PhDT........96P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008PhDT........96P"><span>Design, fabrication, and <span class="hlt">testing</span> of an ultrasonic de-<span class="hlt">icing</span> system for helicopter rotor blades</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palacios, Jose Luis</p> <p></p> <p>A low-power, non-thermal ultrasonic de-<span class="hlt">icing</span> system is introduced as a possible substitute for current electro-thermal systems. The system generates delaminating ultrasonic transverse shear stresses at the interface of accreted <span class="hlt">ice</span>. A PZT-4 disk driven at 28.5 KHz (radial resonance of the disk) instantaneously de-bonds 2 mm thick freezer <span class="hlt">ice</span> layers. The <span class="hlt">ice</span> layers are accreted to a 0.7 mm thick, 30.4 cm x 30.4 cm steel plate at an environment temperature of -20°C. A power input of 50 Watts is applied to the actuator (50 V, 19.6 KV/m), which translates to a de-<span class="hlt">icing</span> power of 0.07 W/cm2. A finite element model of the actuator bonded to the isotropic plate is used to guide the design of the system, and predicts the transverse shear stresses at the <span class="hlt">ice</span> interface. Wind tunnel <span class="hlt">icing</span> <span class="hlt">tests</span> were conducted to demonstrate the potential use of the proposed system under impact <span class="hlt">icing</span> conditions. Both glaze <span class="hlt">ice</span> and rime <span class="hlt">ice</span> were generated on steel and composite plates by changing the cloud conditions of the wind tunnel. Continuous ultrasonic vibration prevented impact <span class="hlt">ice</span> formation around the actuator location at an input power not exceeding 0.18 W/cm 2 (1.2 W/in2). As <span class="hlt">ice</span> thickness reached a critical thickness of approximately 1.2 mm, shedding occurred on those locations where ultrasonic transverse shear stresses exceeded the shear adhesion strength of the <span class="hlt">ice</span>. Finite element transverse shear stress predictions correlate with observed experimental impact <span class="hlt">ice</span> de-bonding behavior. To increase the traveling distance of propagating ultrasonic waves, ultrasonic shear horizontal wave modes are studied. Wave modes providing large modal interface transverse shear stress concentration coefficients (ISCC) between the host structure (0.7 mm thick steel plate) and accreted <span class="hlt">ice</span> (2.5 mm thick <span class="hlt">ice</span> layer) are identified and investigated for a potential increase in the wave propagation distance. Ultrasonic actuators able to trigger these optimum wave modes are designed and fabricated. Despite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950012870','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950012870"><span><span class="hlt">Ice</span> Accretion with Varying Surface Tension</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bilanin, Alan J.; Anderson, David N.</p> <p>1995-01-01</p> <p>During an <span class="hlt">icing</span> encounter of an aircraft in flight, super-cooled water droplets impinging on an airfoil may splash before freezing. This paper reports <span class="hlt">tests</span> performed to determine if this effect is significant and uses the results to develop an improved scaling method for use in <span class="hlt">icing</span> <span class="hlt">test</span> facilities. Simple laboratory <span class="hlt">tests</span> showed that drops splash on impact at the Reynolds and Weber numbers typical of <span class="hlt">icing</span> encounters. Further confirmation of droplet splash came from <span class="hlt">icing</span> <span class="hlt">tests</span> performed in the NaSA Lewis <span class="hlt">Icing</span> Research Tunnel (IRT) with a surfactant added to the spray water to reduce the surface tension. The resulting <span class="hlt">ice</span> shapes were significantly different from those formed when no surfactant was added to the water. These results suggested that the droplet Weber number must be kept constant to properly scale <span class="hlt">icing</span> <span class="hlt">test</span> conditions. Finally, the paper presents a Weber-number-based scaling method and reports results from scaling <span class="hlt">tests</span> in the IRT in which model size was reduced up to a factor of 3. Scale and reference <span class="hlt">ice</span> shapes are shown which confirm the effectiveness of this new scaling method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030025277&hterms=statistics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dstatistics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030025277&hterms=statistics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dstatistics"><span>Space/Time Statistics of Polar <span class="hlt">Ice</span> Motion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Emery, William J.; Fowler, Charles; Maslanik, James A.</p> <p>2003-01-01</p> <p> <span class="hlt">ice</span> <span class="hlt">pack</span> and lead to an <span class="hlt">ice</span>-free Arctic Ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017TCry...11.2137T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017TCry...11.2137T"><span>Modelling radiative transfer through ponded first-year Arctic sea <span class="hlt">ice</span> with a plane-parallel model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taskjelle, Torbjørn; Hudson, Stephen R.; Granskog, Mats A.; Hamre, Børge</p> <p>2017-09-01</p> <p>Under-<span class="hlt">ice</span> irradiance measurements were done on ponded first-year <span class="hlt">pack</span> <span class="hlt">ice</span> along three transects during the <span class="hlt">ICE</span>12 expedition north of Svalbard. Bulk transmittances (400-900 nm) were found to be on average 0.15-0.20 under bare <span class="hlt">ice</span>, and 0.39-0.46 under ponded <span class="hlt">ice</span>. Radiative transfer modelling was done with a plane-parallel model. While simulated transmittances deviate significantly from measured transmittances close to the edge of ponds, spatially averaged bulk transmittances agree well. That is, transect-average bulk transmittances, calculated using typical simulated transmittances for ponded and bare <span class="hlt">ice</span> weighted by the fractional coverage of the two surface types, are in good agreement with the measured values. Radiative heating rates calculated from model output indicates that about 20 % of the incident solar energy is absorbed in bare <span class="hlt">ice</span>, and 50 % in ponded <span class="hlt">ice</span> (35 % in pond itself, 15 % in the underlying <span class="hlt">ice</span>). This large difference is due to the highly scattering surface scattering layer (SSL) increasing the albedo of the bare <span class="hlt">ice</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/229584-use-bauxite-packing-material-steam-injection-wells','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/229584-use-bauxite-packing-material-steam-injection-wells"><span>Use of bauxite as <span class="hlt">packing</span> material in steam injection wells</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Scoglio, J.; Joubert, G.; Gallardo, B.</p> <p>1995-12-31</p> <p>Cyclic steam injection, also known as steam soak, has proven to be the most efficient method for producing heavy crude oil and bitumen from unconsolidated sands. The application of steam injection may, however, generate sand production, causing, among other things, a decrease in production. The gravel <span class="hlt">pack</span> technique is the most efficient way to prevent fines production from cold producing wells. But, once they are steam stimulated, a dissolution of quartz containing gravel material takes place reducing greatly the <span class="hlt">packing</span> permeability and eventually sand production. Different types of <span class="hlt">packing</span> material have been used to avoid sand production after cyclic steammore » injection, such as gravel, ceramics, bauxite, coated resin, and American sand. This paper presents the results of field <span class="hlt">test</span>, using sinterized bauxite as a <span class="hlt">packing</span> material, carried out in Venezuela`s heavy oil operations as a part of a comprehensive program aimed at increasing the <span class="hlt">packing</span> durability and reducing sand production. This paper also verify the results of laboratory <span class="hlt">tests</span> in which Bauxite was found to be less soluble than other <span class="hlt">packing</span> material when steam injected.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130000320','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130000320"><span>Development of 3D <span class="hlt">Ice</span> Accretion Measurement Method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Sam; Broeren, Andy P.; Addy, Harold E., Jr.; Sills, Robert; Pifer, Ellen M.</p> <p>2012-01-01</p> <p><span class="hlt">Icing</span> wind tunnels are designed to simulate in-flight <span class="hlt">icing</span> environments. The chief product of such facilities is the <span class="hlt">ice</span> accretion that forms on various <span class="hlt">test</span> articles. Documentation of the resulting <span class="hlt">ice</span> accretion key piece of data in <span class="hlt">icing</span>-wind-tunnel <span class="hlt">tests</span>. Number of currently used options for documenting <span class="hlt">ice</span> accretion in <span class="hlt">icing</span>-wind-tunnel <span class="hlt">testing</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990026834','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990026834"><span>[Tail Plane <span class="hlt">Icing</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1997-01-01</p> <p>The Aviation Safety Program initiated by NASA in 1997 has put greater emphasis in safety related research activities. <span class="hlt">Ice</span>-contaminated-tailplane stall (ICTS) has been identified by the NASA Lewis <span class="hlt">Icing</span> Technology Branch as an important activity for aircraft safety related research. The ICTS phenomenon is characterized as a sudden, often uncontrollable aircraft nose- down pitching moment, which occurs due to increased angle-of-attack of the horizontal tailplane resulting in tailplane stall. Typically, this phenomenon occurs when lowering the flaps during final approach while operating in or recently departing from <span class="hlt">icing</span> conditions. <span class="hlt">Ice</span> formation on the tailplane leading edge can reduce tailplane angle-of-attack range and cause flow separation resulting in a significant reduction or complete loss of aircraft pitch control. In 1993, the Federal Aviation Authority (FAA) and NASA embarked upon a four-year research program to address the problem of tailplane stall and to quantify the effect of tailplane <span class="hlt">ice</span> accretion on aircraft performance and handling characteristics. The goals of this program, which was completed in March 1998, were to collect aerodynamic data for an aircraft tail with and without <span class="hlt">ice</span> contamination and to develop analytical methods for predicting the effects of tailplane <span class="hlt">ice</span> contamination. Extensive dry air and <span class="hlt">icing</span> tunnel <span class="hlt">tests</span> which resulted in a database of the aerodynamic effects associated with tailplane <span class="hlt">ice</span> contamination. Although the FAA/NASA tailplane <span class="hlt">icing</span> program generated some answers regarding <span class="hlt">ice</span>-contaminated-tailplane stall (ICTS) phenomena, NASA researchers have found many open questions that warrant further investigation into ICTS. In addition, several aircraft manufacturers have expressed interest in a second research program to expand the database to other tail configurations and to develop experimental and computational methodologies for evaluating the ICTS phenomenon. In 1998, the <span class="hlt">icing</span> branch at NASA Lewis initiated a second</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P31A2092B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P31A2092B"><span>Jamming of granular <span class="hlt">ice</span> mélange in tidewater glacial fjords</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burton, J. C.; Cassotto, R.; Amundson, J. M.; Kuo, C. C.; Dennin, M.</p> <p>2016-12-01</p> <p>In tidewater glacial fjords, the open water in front of the glacier terminus is often filled with a collection of calved iceberg fragments and sea <span class="hlt">ice</span>. For glaciers with large calving rates, this "mélange" of <span class="hlt">ice</span> can be jam-<span class="hlt">packed</span>, so that the flow is mostly determined by granular interactions, in addition to underlying fjord currents. As the glacier pushes the <span class="hlt">ice</span> mélange through the fjord, the mélange will become jammed and may potentially influence calving rates if the back-stress applied to the glacier terminus is large enough. However, the stress applied by a granular <span class="hlt">ice</span> mélange will depend on its rheology, i.e. iceberg-iceberg contact forces, geometry, friction, etc. Here we report 2D, discrete particle simulations to model the granular mechanics of <span class="hlt">ice</span> mélange. A polydisperse collection of particles is <span class="hlt">packed</span> into a long channel and pushed downfjord at a constant speed, the latter derived from terrestrial radar interferometry (TRI). Each individual particle experiences viscoelastic contact forces and tangential frictional forces upon collision with another particle or channel walls. We find the two most important factors that govern the total force applied to the glacier are the geometry of the channel, and the shape of the particles. In addition, our simulated velocity fields reveal shearing margins near the fjord walls with more uniform flow in the middle of the mélange, consistent with TRI observations. Finally, we find that the magnitude of the back-stress applied to the glacier terminus can influence calving, however, the maximum back-stress is limited by the buckling of icebergs into the fjord waters, so that the stress in the quasi-2D mélange is partially determined by the thickness of the mélange layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913097K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913097K"><span>Improved method for sea <span class="hlt">ice</span> age computation based on combination of sea <span class="hlt">ice</span> drift and concentration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Korosov, Anton; Rampal, Pierre; Lavergne, Thomas; Aaboe, Signe</p> <p>2017-04-01</p> <p>Sea <span class="hlt">Ice</span> Age is one of the components of the Sea <span class="hlt">Ice</span> ECV as defined by the Global Climate Observing System (GCOS) [WMO, 2015]. It is an important climate indicator describing the sea <span class="hlt">ice</span> state in addition to sea <span class="hlt">ice</span> concentration (SIC) and thickness (SIT). The amount of old/thick <span class="hlt">ice</span> in the Arctic Ocean has been decreasing dramatically [Perovich et al. 2015]. Kwok et al. [2009] reported significant decline in the MYI share and consequent loss of thickness and therefore volume. Today, there is only one acknowledged sea <span class="hlt">ice</span> age climate data record [Tschudi, et al. 2015], based on Maslanik et al. [2011] provided by National Snow and <span class="hlt">Ice</span> Data Center (NSIDC) [http://nsidc.org/data/docs/daac/nsidc0611-sea-<span class="hlt">ice</span>-age/]. The sea <span class="hlt">ice</span> age algorithm [Fowler et al., 2004] is using satellite-derived <span class="hlt">ice</span> drift for Lagrangian tracking of individual <span class="hlt">ice</span> parcels (12-km grid cells) defined by areas of sea <span class="hlt">ice</span> concentration > 15% [Maslanik et al., 2011], i.e. sea <span class="hlt">ice</span> extent, according to the NASA Team algorithm [Cavalieri et al., 1984]. This approach has several drawbacks. (1) Using sea <span class="hlt">ice</span> extent instead of sea <span class="hlt">ice</span> concentration leads to overestimation of the amount of older <span class="hlt">ice</span>. (2) The individual <span class="hlt">ice</span> parcels are not advected uniformly over (long) time. This leads to undersampling in areas of consistent <span class="hlt">ice</span> divergence. (3) The end product grid cells are assigned the age of the oldest <span class="hlt">ice</span> parcel within that cell, and the frequency distribution of the <span class="hlt">ice</span> age is not taken into account. In addition, the base sea <span class="hlt">ice</span> drift product (https://nsidc.org/data/docs/daac/nsidc0116_icemotion.gd.html) is known to exhibit greatly reduced accuracy during the summer season [Sumata et al 2014, Szanyi, 2016] as it only relies on a combination of sea <span class="hlt">ice</span> drifter trajectories and wind-driven "free-drift" motion during summer. This results in a significant overestimate of old-<span class="hlt">ice</span> content, incorrect shape of the old-<span class="hlt">ice</span> <span class="hlt">pack</span>, and lack of information about the <span class="hlt">ice</span> age distribution within the grid cells. We</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA133158','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA133158"><span>Evaluation of Type II Fast <span class="hlt">Packs</span> for Electrostatic Discharge Properties.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-08-01</p> <p>34 x 8" x 1 3/4") consisting of a reclosable cushioned carrier which mates into an outer fiberboard sleeve. A cushioning insert is used consisting of a... RECLOSABLE CUSHIONED CARRIER <span class="hlt">TEST</span> LOAD FIGURE 1: Cancel Caddy <span class="hlt">Pack</span> * CONVOLUTED 4* CUSHIONED I FIGURE 2: Type II Fast <span class="hlt">Pack</span> (PPP-B-1672) TYPE II FAST <span class="hlt">PACK</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120014612','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120014612"><span>Scaling of Lift Degradation Due to Anti-<span class="hlt">Icing</span> Fluids Based Upon the Aerodynamic Acceptance <span class="hlt">Test</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Broeren, Andy P.; Riley, James T.</p> <p>2012-01-01</p> <p>In recent years, the FAA has worked with Transport Canada, National Research Council Canada (NRC) and APS Aviation, Inc. to develop allowance times for aircraft operations in <span class="hlt">ice</span>-pellet precipitation. These allowance times are critical to ensure safety and efficient operation of commercial and cargo flights. Wind-tunnel <span class="hlt">testing</span> with uncontaminated anti-<span class="hlt">icing</span> fluids and fluids contaminated with simulated <span class="hlt">ice</span> pellets had been carried out at the NRC Propulsion and <span class="hlt">Icing</span> Wind Tunnel (PIWT) to better understand the flowoff characteristics and resulting aerodynamic effects. The percent lift loss on the thin, high-performance wing model <span class="hlt">tested</span> in the PIWT was determined at 8 angle of attack and used as one of the evaluation criteria in determining the allowance times. Because it was unclear as to how performance degradations measured on this model were relevant to an actual airplane configuration, some means of interpreting the wing model lift loss was deemed necessary. This paper describes how the lift loss was related to the loss in maximum lift of a Boeing 737-200ADV airplane through the Aerodynamic Acceptance <span class="hlt">Test</span> (AAT) performed for fluids qualification. A loss in maximum lift coefficient of 5.24 percent on the B737-200ADV airplane (which was adopted as the threshold in the AAT) corresponds to a lift loss of 7.3 percent on the PIWT model at 8 angle of attack. There is significant scatter in the data used to develop the correlation related to varying effects of the anti-<span class="hlt">icing</span> fluids that were <span class="hlt">tested</span> and other factors. A statistical analysis indicated the upper limit of lift loss on the PIWT model was 9.2 percent. Therefore, for cases resulting in PIWT model lift loss from 7.3 to 9.2 percent, extra scrutiny of the visual observations is required in evaluating fluid performance with contamination.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120018061','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120018061"><span>Scaling of Lift Degradation Due to Anti-<span class="hlt">Icing</span> Fluids Based Upon the Aerodynamic Acceptance <span class="hlt">Test</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Broeren, Andy; Riley, Jim</p> <p>2012-01-01</p> <p>In recent years, the FAA has worked with Transport Canada, National Research Council Canada (NRC) and APS Aviation, Inc. to develop allowance times for aircraft operations in <span class="hlt">ice</span>-pellet precipitation. These allowance times are critical to ensure safety and efficient operation of commercial and cargo flights. Wind-tunnel <span class="hlt">testing</span> with uncontaminated anti-<span class="hlt">icing</span> fluids and fluids contaminated with simulated <span class="hlt">ice</span> pellets had been carried out at the NRC Propulsion and <span class="hlt">Icing</span> Wind Tunnel (PIWT) to better understand the flow-off characteristics and resulting aerodynamic effects. The percent lift loss on the thin, high-performance wing model <span class="hlt">tested</span> in the PIWT was determined at 8 deg. angle of attack and used as one of the evaluation criteria in determining the allowance times. Because it was unclear as to how performance degradations measured on this model were relevant to an actual airplane configuration, some means of interpreting the wing model lift loss was deemed necessary. This paper describes how the lift loss was related to the loss in maximum lift of a Boeing 737-200ADV airplane through the Aerodynamic Acceptance <span class="hlt">Test</span> (AAT) performed for fluids qualification. A loss in maximum lift coefficient of 5.24% on the B737-200ADV airplane (which was adopted as the threshold in the AAT) corresponds to a lift loss of 7.3% on the PIWT model at 8 deg. angle of attack. There is significant scatter in the data used to develop the correlation related to varying effects of the anti-<span class="hlt">icing</span> fluids that were <span class="hlt">tested</span> and other factors. A statistical analysis indicated the upper limit of lift loss on the PIWT model was 9.2%. Therefore, for cases resulting in PIWT model lift loss from 7.3% to 9.2%, extra scrutiny of the visual observations is required in evaluating fluid performance with contamination.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.C41A0504B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.C41A0504B"><span>Managing <span class="hlt">Ice</span>Bridge Airborne Mission Data at the National Snow and <span class="hlt">Ice</span> Data Center</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brodzik, M.; Kaminski, M. L.; Deems, J. S.; Scambos, T. A.</p> <p>2010-12-01</p> <p>Operation <span class="hlt">Ice</span>Bridge (OIB) is a NASA airborne geophysical survey mission conducting laser altimetry, <span class="hlt">ice</span>-penetrating radar profiling, gravimetry and other geophysical measurements to monitor and characterize the Earth's cryosphere. The <span class="hlt">Ice</span>Bridge mission will operate from 2009 until after the launch of ICESat-II (currently planned for 2015), and provides continuity of measurements between that mission and its predecessor. Data collection sites include the Greenland and Antarctic <span class="hlt">Ice</span> Sheets and the sea <span class="hlt">ice</span> <span class="hlt">pack</span> regions of both poles. These regions include some of the most rapidly changing areas of the cryosphere. <span class="hlt">Ice</span>Bridge is also collecting data in East Antarctica via the University of Texas ICECAP program and in Alaska via the University of Alaska, Fairbanks glacier mapping program. The NSIDC Distributed Active Archive Center at the University of Colorado at Boulder provides data archive and distribution support for the <span class="hlt">Ice</span>Bridge mission. Our <span class="hlt">Ice</span>Bridge work is based on two guiding principles: ensuring preservation of the data, and maximizing usage of the data. This broadens our work beyond the typical scope of a data archive. In addition to the necessary data management, discovery, distribution, and outreach functions, we are also developing tools that will enable broader use of the data, and integrating diverse data types to enable new science research. Researchers require expeditious access to data collected from the <span class="hlt">Ice</span>Bridge missions; our archive approach balances that need with our long-term preservation goal. We have adopted a "fast-track" approach to publish data quickly after collection and make it available via FTP download. Subsequently, data sets are archived in the NASA EOSDIS ECS system, which enables data discovery and distribution with the appropriate backup, documentation, and metadata to assure its availability for future research purposes. NSIDC is designing an <span class="hlt">Ice</span>Bridge data portal to allow interactive data search, exploration, and subsetting via</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990063739','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990063739"><span>New <span class="hlt">Icing</span> Cloud Simulation System at the NASA Glenn Research Center <span class="hlt">Icing</span> Research Tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Irvine, Thomas B.; Oldenburg, John R.; Sheldon, David W.</p> <p>1999-01-01</p> <p>A new spray bar system was designed, fabricated, and installed in the NASA Glenn Research Center's <span class="hlt">Icing</span> Research Tunnel (IRT). This system is key to the IRT's ability to do aircraft in-flight <span class="hlt">icing</span> cloud simulation. The performance goals and requirements levied on the design of the new spray bar system included increased size of the uniform <span class="hlt">icing</span> cloud in the IRT <span class="hlt">test</span> section, faster system response time, and increased coverage of <span class="hlt">icing</span> conditions as defined in Appendix C of the Federal Aviation Regulation (FAR), Part 25 and Part 29. Through significant changes to the mechanical and electrical designs of the previous-generation spray bar system, the performance goals and requirements were realized. Postinstallation aerodynamic and <span class="hlt">icing</span> cloud calibrations were performed to quantify the changes and improvements made to the IRT <span class="hlt">test</span> section flow quality and <span class="hlt">icing</span> cloud characteristics. The new and improved capability to simulate aircraft encounters with in-flight <span class="hlt">icing</span> clouds ensures that the 1RT will continue to provide a satisfactory <span class="hlt">icing</span> ground-<span class="hlt">test</span> simulation method to the aeronautics community.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007903','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007903"><span>Mixed Phase Modeling in Glenn<span class="hlt">ICE</span> with Application to Engine <span class="hlt">Icing</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wright, William B.; Jorgenson, Philip C. E.; Veres, Joseph P.</p> <p>2011-01-01</p> <p>A capability for modeling <span class="hlt">ice</span> crystals and mixed phase <span class="hlt">icing</span> has been added to Glenn<span class="hlt">ICE</span>. Modifications have been made to the particle trajectory algorithm and energy balance to model this behavior. This capability has been added as part of a larger effort to model <span class="hlt">ice</span> crystal ingestion in aircraft engines. Comparisons have been made to four mixed phase <span class="hlt">ice</span> accretions performed in the Cox <span class="hlt">icing</span> tunnel in order to calibrate an <span class="hlt">ice</span> erosion model. A sample <span class="hlt">ice</span> ingestion case was performed using the Energy Efficient Engine (E3) model in order to illustrate current capabilities. Engine performance characteristics were supplied using the Numerical Propulsion System Simulation (NPSS) model for this <span class="hlt">test</span> case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12208033','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12208033"><span>Influence of <span class="hlt">ice</span> and snow covers on the UV exposure of terrestrial microbial communities: dosimetric studies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cockell, Charles S; Rettberg, Petra; Horneck, Gerda; Wynn-Williams, David D; Scherer, Kerstin; Gugg-Helminger, Anton</p> <p>2002-08-01</p> <p>Bacillus subtilis spore biological dosimeters and electronic dosimeters were used to investigate the exposure of terrestrial microbial communities in micro-habitats covered by snow and <span class="hlt">ice</span> in Antarctica. The melting of snow covers of between 5- and 15-cm thickness, depending on age and heterogeneity, could increase B. subtilis spore inactivation by up to an order of magnitude, a relative increase twice that caused by a 50% ozone depletion. Within the snow-<span class="hlt">pack</span> at depths of less than approximately 3 cm snow algae could receive two to three times the DNA-weighted irradiance they would receive on bare ground. At the edge of the snow-<span class="hlt">pack</span>, warming of low albedo soils resulted in the formation of overhangs that provided transient UV protection to thawed and growing microbial communities on the soils underneath. In shallow aquatic habitats, thin layers of heterogeneous <span class="hlt">ice</span> of a few millimetres thickness were found to reduce DNA-weighted irradiances by up to 55% compared to full-sky values with equivalent DNA-weighted diffuse attenuation coefficients (K(DNA)) of >200 m(-1). A 2-mm snow-encrusted <span class="hlt">ice</span> cover on a pond was equivalent to 10 cm of <span class="hlt">ice</span> on a perennially <span class="hlt">ice</span> covered lake. <span class="hlt">Ice</span> covers also had the effect of stabilizing the UV exposure, which was often subject to rapid variations of up to 33% of the mean value caused by wind-rippling of the water surface. These data show that changing <span class="hlt">ice</span> and snow covers cause relative changes in microbial UV exposure at least as great as those caused by changing ozone column abundance. Copyright 2002 Elsevier Science B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGC13I0797F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGC13I0797F"><span><span class="hlt">ICE</span>911 Research: Preserving and Rebuilding Reflective <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, L. A.; Chetty, S.; Manzara, A.; Venkatesh, S.</p> <p>2014-12-01</p> <p>We have developed a localized surface albedo modification technique that shows promise as a method to increase reflective multi-year <span class="hlt">ice</span> using floating materials, chosen so as to have low subsidiary environmental impact. It is now well-known that multi-year reflective <span class="hlt">ice</span> has diminished rapidly in the Arctic over the past 3 decades and this plays a part in the continuing rapid decrease of summer-time <span class="hlt">ice</span>. As summer-time bright <span class="hlt">ice</span> disappears, the Arctic is losing its ability to reflect summer insolation, and this has widespread climatic effects, as well as a direct effect on sea level rise, as oceans heat and once-land-based <span class="hlt">ice</span> melts into the sea. We have <span class="hlt">tested</span> the albedo modification technique on a small scale over six Winter/Spring seasons at sites including California's Sierra Nevada Mountains, a Canadian lake, and a small man-made lake in Minnesota, using various materials and an evolving array of instrumentation. The materials can float and can be made to minimize effects on marine habitat and species. The instrumentation is designed to be deployed in harsh and remote locations. Localized snow and <span class="hlt">ice</span> preservation, and reductions in water heating, have been quantified in small-scale <span class="hlt">testing</span>. We have continued to refine our material and deployment approaches, and we have had laboratory confirmation by NASA. In the field, the materials were successfully deployed to shield underlying snow and <span class="hlt">ice</span> from melting; applications of granular materials remained stable in the face of local wind and storms. We are evaluating the effects of snow and <span class="hlt">ice</span> preservation for protection of infrastructure and habitat stabilization, and we are concurrently developing our techniques to aid in water conservation. Localized albedo modification options such as those being studied in this work may act to preserve <span class="hlt">ice</span>, glaciers, permafrost and seasonal snow areas, and perhaps aid natural <span class="hlt">ice</span> formation processes. If this method is deployed on a large enough scale, it could conceivably</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1352756-anisotropic-thermal-response-packed-copper-wire','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1352756-anisotropic-thermal-response-packed-copper-wire"><span>Anisotropic Thermal Response of <span class="hlt">Packed</span> Copper Wire</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wereszczak, Andrew A.; Emily Cousineau, J.; Bennion, Kevin; ...</p> <p>2017-04-19</p> <p>The apparent thermal conductivity of <span class="hlt">packed</span> copper wire <span class="hlt">test</span> specimens was measured parallel and perpendicular to the axis of the wire using laser flash, transient plane source, and transmittance <span class="hlt">test</span> methods. Approximately 50% wire <span class="hlt">packing</span> efficiency was produced in the specimens using either 670- or 925-μm-diameter copper wires that both had an insulation coating thickness of 37 μm. The interstices were filled with a conventional varnish material and also contained some remnant porosity. The apparent thermal conductivity perpendicular to the wire axis was about 0.5–1 W/mK, whereas it was over 200 W/mK in the parallel direction. The Kanzaki model andmore » an finite element analysis (FEA) model were found to reasonably predict the apparent thermal conductivity perpendicular to the wires but thermal conductivity percolation from nonideal wire-<span class="hlt">packing</span> may result in their underestimation of it.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5324094','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5324094"><span>Variability in sea <span class="hlt">ice</span> cover and climate elicit sex specific responses in an Antarctic predator</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Labrousse, Sara; Sallée, Jean-Baptiste; Fraser, Alexander D.; Massom, Rob A.; Reid, Phillip; Hobbs, William; Guinet, Christophe; Harcourt, Robert; McMahon, Clive; Authier, Matthieu; Bailleul, Frédéric; Hindell, Mark A.; Charrassin, Jean-Benoit</p> <p>2017-01-01</p> <p>Contrasting regional changes in Southern Ocean sea <span class="hlt">ice</span> have occurred over the last 30 years with distinct regional effects on ecosystem structure and function. Quantifying how Antarctic predators respond to such changes provides the context for predicting how climate variability/change will affect these assemblages into the future. Over an 11-year time-series, we examine how inter-annual variability in sea <span class="hlt">ice</span> concentration and advance affect the foraging behaviour of a top Antarctic predator, the southern elephant seal. Females foraged longer in <span class="hlt">pack</span> <span class="hlt">ice</span> in years with greatest sea <span class="hlt">ice</span> concentration and earliest sea <span class="hlt">ice</span> advance, while males foraged longer in polynyas in years of lowest sea <span class="hlt">ice</span> concentration. There was a positive relationship between near-surface meridional wind anomalies and female foraging effort, but not for males. This study reveals the complexities of foraging responses to climate forcing by a poleward migratory predator through varying sea <span class="hlt">ice</span> property and dynamic anomalies. PMID:28233791</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28233791','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28233791"><span>Variability in sea <span class="hlt">ice</span> cover and climate elicit sex specific responses in an Antarctic predator.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Labrousse, Sara; Sallée, Jean-Baptiste; Fraser, Alexander D; Massom, Rob A; Reid, Phillip; Hobbs, William; Guinet, Christophe; Harcourt, Robert; McMahon, Clive; Authier, Matthieu; Bailleul, Frédéric; Hindell, Mark A; Charrassin, Jean-Benoit</p> <p>2017-02-24</p> <p>Contrasting regional changes in Southern Ocean sea <span class="hlt">ice</span> have occurred over the last 30 years with distinct regional effects on ecosystem structure and function. Quantifying how Antarctic predators respond to such changes provides the context for predicting how climate variability/change will affect these assemblages into the future. Over an 11-year time-series, we examine how inter-annual variability in sea <span class="hlt">ice</span> concentration and advance affect the foraging behaviour of a top Antarctic predator, the southern elephant seal. Females foraged longer in <span class="hlt">pack</span> <span class="hlt">ice</span> in years with greatest sea <span class="hlt">ice</span> concentration and earliest sea <span class="hlt">ice</span> advance, while males foraged longer in polynyas in years of lowest sea <span class="hlt">ice</span> concentration. There was a positive relationship between near-surface meridional wind anomalies and female foraging effort, but not for males. This study reveals the complexities of foraging responses to climate forcing by a poleward migratory predator through varying sea <span class="hlt">ice</span> property and dynamic anomalies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920013291','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920013291"><span>The NASA aircraft <span class="hlt">icing</span> research program</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shaw, Robert J.; Reinmann, John J.</p> <p>1990-01-01</p> <p>The objective of the NASA aircraft <span class="hlt">icing</span> research program is to develop and make available to industry <span class="hlt">icing</span> technology to support the needs and requirements for all-weather aircraft designs. Research is being done for both fixed wing and rotary wing applications. The NASA program emphasizes technology development in two areas, advanced <span class="hlt">ice</span> protection concepts and <span class="hlt">icing</span> simulation. Reviewed here are the computer code development/validation, <span class="hlt">icing</span> wind tunnel <span class="hlt">testing</span>, and <span class="hlt">icing</span> flight <span class="hlt">testing</span> efforts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120011129','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120011129"><span>Fundamental <span class="hlt">Ice</span> Crystal Accretion Physics Studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter M.; Broeren, Andy P.; Tsao, Jen-Ching; Vargas, Mario; Wright, William B.; Currie, Tom; Knezevici, Danny; Fuleki, Dan</p> <p>2012-01-01</p> <p>Due to numerous engine power-loss events associated with high-altitude convective weather, <span class="hlt">ice</span> accretion within an engine due to <span class="hlt">ice</span> crystal ingestion is being investigated. The National Aeronautics and Space Administration (NASA) and the National Research Council (NRC) of Canada are starting to examine the physical mechanisms of <span class="hlt">ice</span> accretion on surfaces exposed to <span class="hlt">ice</span>-crystal and mixed-phase conditions. In November 2010, two weeks of <span class="hlt">testing</span> occurred at the NRC Research Altitude Facility utilizing a single wedge-type airfoil designed to facilitate fundamental studies while retaining critical features of a compressor stator blade or guide vane. The airfoil was placed in the NRC cascade wind tunnel for both aerodynamic and <span class="hlt">icing</span> <span class="hlt">tests</span>. Aerodynamic <span class="hlt">testing</span> showed excellent agreement compared with CFD data on the <span class="hlt">icing</span> pressure surface and allowed calculation of heat transfer coefficients at various airfoil locations. <span class="hlt">Icing</span> <span class="hlt">tests</span> were performed at Mach numbers of 0.2 to 0.3, total pressures from 93 to 45 kPa, and total temperatures from 5 to 15 C. <span class="hlt">Ice</span> and liquid water contents ranged up to 20 and 3 g/m3, respectively. The <span class="hlt">ice</span> appeared well adhered to the surface in the lowest pressure <span class="hlt">tests</span> (45 kPa) and, in a particular case, showed continuous leading-edge <span class="hlt">ice</span> growth to a thickness greater than 15 mm in 3 min. Such widespread deposits were not observed in the highest pressure <span class="hlt">tests</span>, where the accretions were limited to a small area around the leading edge. The suction surface was typically <span class="hlt">ice</span>-free in the <span class="hlt">tests</span> at high pressure, but not at low pressure. The <span class="hlt">icing</span> behavior at high and low pressure appeared to be correlated with the wet-bulb temperature, which was estimated to be above 0 C in <span class="hlt">tests</span> at 93 kPa and below 0 C in <span class="hlt">tests</span> at lower pressure, the latter enhanced by more evaporative cooling of water. The authors believe that the large <span class="hlt">ice</span> accretions observed in the low pressure <span class="hlt">tests</span> would undoubtedly cause the aerodynamic performance of a compressor component</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120004044','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120004044"><span>Fundamental <span class="hlt">Ice</span> Crystal Accretion Physics Studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Currie, Tom; Knezevici, Danny; Fuleki, Dan; Struk, Peter M.; Broeren, Andy P.; Tsao, Jen-ching; Vargas, Mario; Wright, William</p> <p>2011-01-01</p> <p>Due to numerous engine power-loss events associated with high-altitude convective weather, <span class="hlt">ice</span> accretion within an engine due to <span class="hlt">ice</span>-crystal ingestion is being investigated. The National Aeronautics and Space Administration (NASA) and the National Research Council (NRC) of Canada are starting to examine the physical mechanisms of <span class="hlt">ice</span> accretion on surfaces exposed to <span class="hlt">ice</span>-crystal and mixed-phase conditions. In November 2010, two weeks of <span class="hlt">testing</span> occurred at the NRC Research Altitude Facility utilizing a single wedge-type airfoil designed to facilitate fundamental studies while retaining critical features of a compressor stator blade or guide vane. The airfoil was placed in the NRC cascade wind tunnel for both aerodynamic and <span class="hlt">icing</span> <span class="hlt">tests</span>. Aerodynamic <span class="hlt">testing</span> showed excellent agreement compared with CFD data on the <span class="hlt">icing</span> pressure surface and allowed calculation of heat transfer coefficients at various airfoil locations. <span class="hlt">Icing</span> <span class="hlt">tests</span> were performed at Mach numbers of 0.2 to 0.3, total pressures from 93 to 45 kPa, and total temperatures from 5 to 15 C. <span class="hlt">Ice</span> and liquid water contents ranged up to 20 and 3 grams per cubic meter, respectively. The <span class="hlt">ice</span> appeared well adhered to the surface in the lowest pressure <span class="hlt">tests</span> (45 kPa) and, in a particular case, showed continuous leading-edge <span class="hlt">ice</span> growth to a thickness greater than 15 millimeters in 3 minutes. Such widespread deposits were not observed in the highest pressure <span class="hlt">tests</span>, where the accretions were limited to a small area around the leading edge. The suction surface was typically <span class="hlt">ice</span>-free in the <span class="hlt">tests</span> at high pressure, but not at low pressure. The <span class="hlt">icing</span> behavior at high and low pressure appeared to be correlated with the wet-bulb temperature, which was estimated to be above 0 C in <span class="hlt">tests</span> at 93 kPa and below 0 C in <span class="hlt">tests</span> at lower pressure, the latter enhanced by more evaporative cooling of water. The authors believe that the large <span class="hlt">ice</span> accretions observed in the low pressure <span class="hlt">tests</span> would undoubtedly cause the aerodynamic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26336338','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26336338"><span>Multiple Off-<span class="hlt">Ice</span> Performance Variables Predict On-<span class="hlt">Ice</span> Skating Performance in Male and Female Division III <span class="hlt">Ice</span> Hockey Players.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Janot, Jeffrey M; Beltz, Nicholas M; Dalleck, Lance D</p> <p>2015-09-01</p> <p>The purpose of this study was to determine if off-<span class="hlt">ice</span> performance variables could predict on-<span class="hlt">ice</span> skating performance in Division III collegiate hockey players. Both men (n = 15) and women (n = 11) hockey players (age = 20.5 ± 1.4 years) participated in the study. The skating <span class="hlt">tests</span> were agility cornering S-turn, 6.10 m acceleration, 44.80 m speed, modified repeat skate, and 15.20 m full speed. Off-<span class="hlt">ice</span> variables assessed were years of playing experience, height, weight and percent body fat and off-<span class="hlt">ice</span> performance variables included vertical jump (VJ), 40-yd dash (36.58m), 1-RM squat, pro-agility, Wingate peak power and peak power percentage drop (% drop), and 1.5 mile (2.4km) run. Results indicated that 40-yd dash (36.58m), VJ, 1.5 mile (2.4km) run, and % drop were significant predictors of skating performance for repeat skate (slowest, fastest, and average time) and 44.80 m speed time, respectively. Four predictive equations were derived from multiple regression analyses: 1) slowest repeat skate time = 2.362 + (1.68 x 40-yd dash time) + (0.005 x 1.5 mile run), 2) fastest repeat skate time = 9.762 - (0.089 x VJ) - (0.998 x 40-yd dash time), 3) average repeat skate time = 7.770 + (1.041 x 40-yd dash time) - (0.63 x VJ) + (0.003 x 1.5 mile time), and 4) 47.85 m speed <span class="hlt">test</span> = 7.707 - (0.050 x VJ) - (0.01 x % drop). It was concluded that selected off-<span class="hlt">ice</span> <span class="hlt">tests</span> could be used to predict on-<span class="hlt">ice</span> performance regarding speed and recovery ability in Division III male and female hockey players. Key pointsThe 40-yd dash (36.58m) and vertical jump <span class="hlt">tests</span> are significant predictors of on-<span class="hlt">ice</span> skating performance specific to speed.In addition to 40-yd dash and vertical jump, the 1.5 mile (2.4km) run for time and percent power drop from the Wingate anaerobic power <span class="hlt">test</span> were also significant predictors of skating performance that incorporates the aspect of recovery from skating activity.Due to the specificity of selected off-<span class="hlt">ice</span> variables as predictors of on-<span class="hlt">ice</span> performance, coaches can</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4541115','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4541115"><span>Multiple Off-<span class="hlt">Ice</span> Performance Variables Predict On-<span class="hlt">Ice</span> Skating Performance in Male and Female Division III <span class="hlt">Ice</span> Hockey Players</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Janot, Jeffrey M.; Beltz, Nicholas M.; Dalleck, Lance D.</p> <p>2015-01-01</p> <p>The purpose of this study was to determine if off-<span class="hlt">ice</span> performance variables could predict on-<span class="hlt">ice</span> skating performance in Division III collegiate hockey players. Both men (n = 15) and women (n = 11) hockey players (age = 20.5 ± 1.4 years) participated in the study. The skating <span class="hlt">tests</span> were agility cornering S-turn, 6.10 m acceleration, 44.80 m speed, modified repeat skate, and 15.20 m full speed. Off-<span class="hlt">ice</span> variables assessed were years of playing experience, height, weight and percent body fat and off-<span class="hlt">ice</span> performance variables included vertical jump (VJ), 40-yd dash (36.58m), 1-RM squat, pro-agility, Wingate peak power and peak power percentage drop (% drop), and 1.5 mile (2.4km) run. Results indicated that 40-yd dash (36.58m), VJ, 1.5 mile (2.4km) run, and % drop were significant predictors of skating performance for repeat skate (slowest, fastest, and average time) and 44.80 m speed time, respectively. Four predictive equations were derived from multiple regression analyses: 1) slowest repeat skate time = 2.362 + (1.68 x 40-yd dash time) + (0.005 x 1.5 mile run), 2) fastest repeat skate time = 9.762 - (0.089 x VJ) - (0.998 x 40-yd dash time), 3) average repeat skate time = 7.770 + (1.041 x 40-yd dash time) - (0.63 x VJ) + (0.003 x 1.5 mile time), and 4) 47.85 m speed <span class="hlt">test</span> = 7.707 - (0.050 x VJ) - (0.01 x % drop). It was concluded that selected off-<span class="hlt">ice</span> <span class="hlt">tests</span> could be used to predict on-<span class="hlt">ice</span> performance regarding speed and recovery ability in Division III male and female hockey players. Key points The 40-yd dash (36.58m) and vertical jump <span class="hlt">tests</span> are significant predictors of on-<span class="hlt">ice</span> skating performance specific to speed. In addition to 40-yd dash and vertical jump, the 1.5 mile (2.4km) run for time and percent power drop from the Wingate anaerobic power <span class="hlt">test</span> were also significant predictors of skating performance that incorporates the aspect of recovery from skating activity. Due to the specificity of selected off-<span class="hlt">ice</span> variables as predictors of on-<span class="hlt">ice</span> performance, coaches</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=267860&Lab=OTAQ&keyword=lithium+AND+ion+AND+battery&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=267860&Lab=OTAQ&keyword=lithium+AND+ion+AND+battery&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>HIL Development and Validation of Lithium-ion Battery <span class="hlt">Packs</span> (SAE 2014-01-1863)</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>A Battery <span class="hlt">Test</span> Facility (BTF) has been constructed at United States Environmental Protection Agency (EPA) to <span class="hlt">test</span> various automotive battery <span class="hlt">packs</span> for HEV, PHEV, and EV vehicles. Battery <span class="hlt">pack</span> <span class="hlt">tests</span> were performed in the BTF using a battery cycler, <span class="hlt">testing</span> controllers, battery pa...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/27475','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/27475"><span>Development of a mechanical rocker <span class="hlt">test</span> procedure for <span class="hlt">ice</span> melting capacity evaluation.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-06-01</p> <p>During Phase 2 of the NDOR deicing chemicals performance evaluation project (No. SPR-P1(10) P328), a : simple and economical <span class="hlt">test</span> using a martini shaker to evaluate <span class="hlt">ice</span> melting capacity of liquid deicers showed : good potential to become a standardiz...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740002260','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740002260"><span>Microwave maps of the polar <span class="hlt">ice</span> of the earth. [from Nimbus-5 satellite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gloersen, P.; Wilheit, T. T.; Chang, T. C.; Nordberg, W.; Campbell, W. J.</p> <p>1973-01-01</p> <p>Synoptic views of the entire polar regions of earth were obtained free of the usual persistent cloud cover using a scanning microwave radiometer operating at a wavelength of 1.55 cm on board the Nimbus-5 satellite. Three different views at each pole are presented utilizing data obtained at approximately one-month intervals during the winter of 1972-1973. The major discoveries resulting from an analysis of these data are as follows: (1) Large discrepancies exist between the climatic norm <span class="hlt">ice</span> cover depicted in various atlases and the actual extent of the canopies. (2) The distribution of multiyear <span class="hlt">ice</span> in the north polar region is markedly different from that predicted by existing <span class="hlt">ice</span> dynamics models. (3) Irregularities in the edge of the Antarctic sea <span class="hlt">ice</span> <span class="hlt">pack</span> occur that have neither been observed previously nor anticipated. (4) The brightness temperatures of the Greenland and Antarctica glaciers show interesting contours probably related to the <span class="hlt">ice</span> and snow morphologic structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMPP13D1106W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMPP13D1106W"><span>Wave inhibition by sea <span class="hlt">ice</span> enables trans-Atlantic <span class="hlt">ice</span> rafting of debris during Heinrich Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wagner, T. J. W.; Dell, R.; Eisenman, I.; Keeling, R. F.; Padman, L.; Severinghaus, J. P.</p> <p>2017-12-01</p> <p>The thickness of the <span class="hlt">ice</span>-rafted debris (IRD) layers that signal Heinrich Events declines far more gradually with distance from the iceberg sources than would be expected based on present-day iceberg trajectories. Here we model icebergs as passive Lagrangian tracers driven by ocean currents, winds, and sea surface temperatures. The icebergs are released in a comprehensive climate model simulation of the last glacial maximum (LGM), as well as a simulation of the modern climate. The two simulated climates result in qualitatively similar distributions of iceberg meltwater and hence debris, with the colder temperatures of the LGM having only a relatively small effect on meltwater spread. In both scenarios, meltwater flux falls off rapidly with zonal distance from the source, in contrast with the more uniform spread of IRD in sediment cores. In order to address this discrepancy, we propose a physical mechanism that could have prolonged the lifetime of icebergs during Heinrich events. The mechanism involves a surface layer of cold and fresh meltwater formed from, and retained around, densely <span class="hlt">packed</span> armadas of icebergs. This leads to wintertime sea <span class="hlt">ice</span> formation even in relatively low latitudes. The sea <span class="hlt">ice</span> in turn shields the icebergs from wave erosion, which is the main source of iceberg ablation. We find that allowing sea <span class="hlt">ice</span> to form around all icebergs during four months each winter causes the model to approximately agree with the distribution of IRD in sediment cores.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130011782','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130011782"><span>Aero-Thermal Calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (2012 <span class="hlt">Tests</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pastor-Barsi, Christine; Allen, Arrington E.</p> <p>2013-01-01</p> <p>A full aero-thermal calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (IRT) was completed in 2012 following the major modifications to the facility that included replacement of the refrigeration plant and heat exchanger. The calibration <span class="hlt">test</span> provided data used to fully document the aero-thermal flow quality in the IRT <span class="hlt">test</span> section and to construct calibration curves for the operation of the IRT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.C33A0684F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.C33A0684F"><span><span class="hlt">Ice</span>911 Research: Preserving and Rebuilding Multi-Year <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, L. A.; Chetty, S.; Manzara, A.</p> <p>2013-12-01</p> <p>A localized surface albedo modification technique is being developed that shows promise as a method to increase multi-year <span class="hlt">ice</span> using reflective floating materials, chosen so as to have low subsidiary environmental impact. Multi-year <span class="hlt">ice</span> has diminished rapidly in the Arctic over the past 3 decades (Riihela et al, Nature Climate Change, August 4, 2013) and this plays a part in the continuing rapid decrease of summer-time <span class="hlt">ice</span>. As summer-time <span class="hlt">ice</span> disappears, the Arctic is losing its ability to act as the earth's refrigeration system, and this has widespread climatic effects, as well as a direct effect on sea level rise, as oceans heat, and once-land-based <span class="hlt">ice</span> melts into the sea. We have <span class="hlt">tested</span> the albedo modification technique on a small scale over five Winter/Spring seasons at sites including California's Sierra Nevada Mountains, a Canadian lake, and a small man-made lake in Minnesota, using various materials and an evolving array of instrumentation. The materials can float and can be made to minimize effects on marine habitat and species. The instrumentation is designed to be deployed in harsh and remote locations. Localized snow and <span class="hlt">ice</span> preservation, and reductions in water heating, have been quantified in small-scale <span class="hlt">testing</span>. Climate modeling is underway to analyze the effects of this method of surface albedo modification in key areas on the rate of oceanic and atmospheric temperature rise. We are also evaluating the effects of snow and <span class="hlt">ice</span> preservation for protection of infrastructure and habitat stabilization. This paper will also discuss a possible reduction of sea level rise with an eye to quantification of cost/benefit. The most recent season's experimentation on a man-made private lake in Minnesota saw further evolution in the material and deployment approach. The materials were successfully deployed to shield underlying snow and <span class="hlt">ice</span> from melting; applications of granular materials remained stable in the face of local wind and storms. Localized albedo</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......484S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......484S"><span>Sea-<span class="hlt">ice</span> habitat preference of the Pacific walrus (Odobenus rosmarus divergens) in the Bering Sea: A multiscaled approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sacco, Alexander Edward</p> <p></p> <p>, walruses were preferentially occupying fragmented <span class="hlt">pack</span> <span class="hlt">ice</span> seascapes range 50 -- 89% of the time, when, all throughout the Bering Sea, only range 41 -- 46% of seascapes consisted of fragmented <span class="hlt">pack</span> <span class="hlt">ice</span>. Traditional knowledge of a walrus' use of sea <span class="hlt">ice</span> is investigated through semi-directed interviews conducted with subsistence hunters and elders from Savoonga and Gambell, two Alaskan Native communities on St. Lawrence Island, Alaska. Informants were provided with a large nautical map of the land and ocean surrounding St. Lawrence Island and 45 printed large-format aerial photographs of walruses on sea <span class="hlt">ice</span> to stimulate discussion as questions were asked to direct the topics of conversation. Informants discussed change in sea <span class="hlt">ice</span> conditions over time, walrus behaviors during the fall and spring subsistence hunts, and sea-<span class="hlt">ice</span> characteristics that walruses typically occupy. These observations are compared with <span class="hlt">ice</span>-patch preferences analyzed from aerial imagery. Floe size was found to agree with remotely-sensed <span class="hlt">ice</span>-patch analysis results, while floe shape was not distinguishable to informants during the hunt. <span class="hlt">Ice</span>-patch arrangement descriptors concentration and density generally agreed with <span class="hlt">ice</span>-patch analysis results. Results include possible preference of <span class="hlt">ice</span>-patch descriptors at the <span class="hlt">ice</span>-patch scale and fragmented <span class="hlt">pack</span> <span class="hlt">ice</span> preference at the seascape scale. Traditional knowledge suggests large <span class="hlt">ice</span> ridges are preferential sea-<span class="hlt">ice</span> features at the <span class="hlt">ice</span>-patch scale, which are rapidly becoming less common during the fall and spring migration of sea <span class="hlt">ice</span> through the Bering Sea. Traditional knowledge, combined with a scientific analysis and field work to study species habitat preferences and, ultimately, habitat partitioning, can stem from these results. Future work includes increased sophistication of the synthetic aperture radar classification algorithm, experimentation with various spatial scales to determine the optimal scale for walrus' life-cycle events, and incorporation of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26317706','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26317706"><span><span class="hlt">Testing</span> the Dark Matter Scenario for PeV Neutrinos Observed in <span class="hlt">Ice</span>Cube.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Murase, Kohta; Laha, Ranjan; Ando, Shin'ichiro; Ahlers, Markus</p> <p>2015-08-14</p> <p>Late time decay of very heavy dark matter is considered as one of the possible explanations for diffuse PeV neutrinos observed in <span class="hlt">Ice</span>Cube. We consider implications of multimessenger constraints, and show that proposed models are marginally consistent with the diffuse γ-ray background data. Critical <span class="hlt">tests</span> are possible by a detailed analysis and identification of the sub-TeV isotropic diffuse γ-ray data observed by Fermi and future observations of sub-PeV γ rays by observatories like HAWC or Tibet AS+MD. In addition, with several-year observations by next-generation telescopes such as <span class="hlt">Ice</span>Cube-Gen2, muon neutrino searches for nearby dark matter halos such as the Virgo cluster should allow us to rule out or support the dark matter models, independently of γ-ray and anisotropy <span class="hlt">tests</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70176362','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70176362"><span>The study of fresh-water lake <span class="hlt">ice</span> using multiplexed imaging radar</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Leonard, Bryan M.; Larson, R.W.</p> <p>1975-01-01</p> <p>The study of <span class="hlt">ice</span> in the upper Great Lakes, both from the operational and the scientific points of view, is receiving continued attention. Quantitative and qualitative field work is being conducted to provide the needed background for accurate interpretation of remotely sensed data. The data under discussion in this paper were obtained by a side-looking multiplexed airborne radar (SLAR) supplemented with ground-truth data.Because of its ability to penetrate adverse weather, radar is an especially important instrument for monitoring <span class="hlt">ice</span> in the upper Great Lakes. It has previously been shown that imaging radars can provide maps of <span class="hlt">ice</span> cover in these areas. However, questions concerning both the nature of the surfaces reflecting radar energy and the interpretation of the radar imagery continually arise.Our analysis of <span class="hlt">ice</span> in Whitefish Bay (Lake Superior) indicates that the combination of the <span class="hlt">ice</span>/water interlace and the <span class="hlt">ice</span>/air interface is the major contributor to the radar backscatter as seen on the imagery At these frequencies the <span class="hlt">ice</span> has a very low relative dielectric permittivity (< 3.0) and a low loss tangent Thus, this <span class="hlt">ice</span> is somewhat transparent to the energy used by the imaging SLAR system. The <span class="hlt">ice</span> types studied include newly formed black <span class="hlt">ice</span>, pancake <span class="hlt">ice</span>, and frozen and consolidated <span class="hlt">pack</span> and brash <span class="hlt">ice</span>.Although <span class="hlt">ice</span> thickness cannot be measured directly from the received signals, it is suspected that by combining the information pertaining to radar backscatter with data on the meteorological and sea-state history of the area, together with some basic ground truth, better estimates of the <span class="hlt">ice</span> thickness may be provided. In addition, certain <span class="hlt">ice</span> features (e.g. ridges, <span class="hlt">ice</span>-foot formation, areas of brash <span class="hlt">ice</span>) may be identified with reasonable confidence. There is a continued need for additional ground work to verify the validity of imaging radars for these types of interpretations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA128219','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA128219"><span>Properties of Urea-Doped <span class="hlt">Ice</span> in the CRREL <span class="hlt">Test</span> Basin,</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-03-01</p> <p>thickness versus initial <span class="hlt">ice</span> thickness at start of warm-up ................ 7 9. Thin sections of urea-doped <span class="hlt">ice</span>...following section ) on the mechanical properties of the tank, essential for achieving an <span class="hlt">ice</span> sheet of uni- the model <span class="hlt">ice</span> was investigated. In particular...Figure 1. elastic foundation: Measurements ~i 7 A 1 f 2 Temperature As mentioned in the preceding section , water and temperature was measured with a 1/50</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990019485','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990019485"><span>NASA/FAA Tailplane <span class="hlt">Icing</span> Program Overview</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ratvasky, Thomas P.; VanZante, Judith Foss; Riley, James T.</p> <p>1999-01-01</p> <p>The effects of tailplane <span class="hlt">icing</span> were investigated in a four-year NASA/FAA Tailplane <span class="hlt">Icing</span>, Program (TIP). This research program was developed to improve the understanding, of <span class="hlt">iced</span> tailplane aeroperformance and aircraft aerodynamics, and to develop design and training aides to help reduce the number of incidents and accidents caused by tailplane <span class="hlt">icing</span>. To do this, the TIP was constructed with elements that included <span class="hlt">icing</span>, wind tunnel <span class="hlt">testing</span>, dry-air aerodynamic wind tunnel <span class="hlt">testing</span>, flight <span class="hlt">tests</span>, and analytical code development. This paper provides an overview of the entire program demonstrating the interconnectivity of the program elements and reports on current accomplishments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70186594','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70186594"><span>Diminishing sea <span class="hlt">ice</span> in the western Arctic Ocean</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Stone, R.S.; Belchansky, G.I.; Drobot, Sheldon; Douglas, David C.; Levinson, D.H.; Waple, A.M.</p> <p>2004-01-01</p> <p>Since the advent of satellite passive microwave radiometry (1978), variations in sea <span class="hlt">ice</span> extent and concentration have been carefully monitored from space. An estimated 7.4% decrease in sea <span class="hlt">ice</span> extent has occurred in the last 25 yr (Johannessen et al. 2004), with recent record minima (e.g., Maslanik et al. 1999; Serreze et al. 2003) accounting for much of the decline. Comparisons between the time series of Arctic sea <span class="hlt">ice</span> melt dynamics and snowmelt dates at the NOAA–CMDL Barrow Observatory (BRW) reveal intriguing correlations.Melt-onset dates over sea <span class="hlt">ice</span> (Drobot and Anderson 2001) were cross correlated with the melt-date time series from BRW, and a prominent region of high correlation between snowmelt onset over sea <span class="hlt">ice</span> and the BRW record of melt dates was approximately aligned with the climatological center of the Beaufort Sea Anticyclone (BSA). The BSA induces anticyclonic <span class="hlt">ice</span> motion in the region, effectively forcing the Beaufort gyre. A weak gyre caused by a breakdown of the BSA diminishes transport of multiyear <span class="hlt">ice</span> into this region (Drobot and Maslanik 2003). Similarly, the annual snow cycle at BRW varies with the position and intensity of the BSA (Stone et al. 2002, their Fig. 6). Thus, variations in the BSA appear to have far-reaching effects on the annual accumulation and subsequent melt of snow over a large region of the western Arctic.A dramatic increase in melt season duration (Belchansky et al. 2004) was also observed within the same region of high correlation between onset of melt over the <span class="hlt">ice</span> <span class="hlt">pack</span> and snowmelt at BRW (Fig. 5.7). By inference, this suggests linkages between factors that modulate the annual cycle of snow on land and processes that influence melting of snow and <span class="hlt">ice</span> in the western Arctic Ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130000327','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130000327"><span>Aero-Thermal Calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (2012 <span class="hlt">Test</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pastor-Barsi, Christine M.; Arrington, E. Allen; VanZante, Judith Foss</p> <p>2012-01-01</p> <p>A major modification of the refrigeration plant and heat exchanger at the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (IRT) occurred in autumn of 2011. It is standard practice at NASA Glenn to perform a full aero-thermal calibration of the <span class="hlt">test</span> section of a wind tunnel facility upon completion of major modifications. This paper will discuss the tools and techniques used to complete an aero-thermal calibration of the IRT and the results that were acquired. The goal of this <span class="hlt">test</span> entry was to complete a flow quality survey and aero-thermal calibration measurements in the <span class="hlt">test</span> section of the IRT. <span class="hlt">Test</span> hardware that was used includes the 2D Resistive Temperature Detector (RTD) array, 9-ft pressure survey rake, hot wire survey rake, and the quick check survey rake. This <span class="hlt">test</span> hardware provides a map of the velocity, Mach number, total and static pressure, total temperature, flow angle and turbulence intensity. The data acquired were then reduced to examine pressure, temperature, velocity, flow angle, and turbulence intensity. Reduced data has been evaluated to assess how the facility meets flow quality goals. No <span class="hlt">icing</span> conditions were <span class="hlt">tested</span> as part of the aero-thermal calibration. However, the effects of the spray bar air injections on the flow quality and aero-thermal calibration measurements were examined as part of this calibration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC43H1161F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC43H1161F"><span><span class="hlt">Ice</span>911 Research: A Reversible Localized Geo-Engineering Technique to Mitigate Climate Change Effects: Field <span class="hlt">Testing</span>, Instrumentation and Climate Modeling Results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, L. A.; Sholtz, A.; Chetty, S.; Manzara, A.; Johnson, D.; Christodoulou, E.; Decca, R.; Walter, P.; Katuri, K.; Bhattacharyya, S.; Ivanova, D.; Mlaker, V.; Perovich, D. K.</p> <p>2017-12-01</p> <p>This work uses ecologically benign surface treatment of silica-based materials in carefully selected, limited areas to reduce polar <span class="hlt">ice</span> melt by reflecting energy from summertime polar sun to attempt to slow <span class="hlt">ice</span> loss due to the <span class="hlt">Ice</span>-Albedo Feedback Effect. Application of <span class="hlt">Ice</span>911's materials can be accomplished within a season, at a comparatively low cost, and with far less secondary environmental impact than many other proposed geo-engineering solutions. Field <span class="hlt">testing</span>, instrumentation, safety <span class="hlt">testing</span>, data-handling and modeling results will be presented. The albedo modification has been <span class="hlt">tested</span> over a number of melt seasons with an evolving array of instrumentation, at multiple sites and on progressively larger scales, most recently in a small artificial pond in Minnesota and in a lake in Barrow, Alaska's BEO (Barrow Experimental Observatory) area. The <span class="hlt">test</span> data show that the glass bubbles can provide an effective material for increasing albedo, significantly reducing the melting rate of <span class="hlt">ice</span>. Using NCAR's CESM package the environmental impact of the approach of surface albedo modification was studied. During two separate runs, region-wide Arctic albedo modification as well as more targeted localized treatments were modeled and compared. The parameters of a surface snow layer are used as a proxy to simulate <span class="hlt">Ice</span>911's high-albedo materials, and the modification is started in January over selected <span class="hlt">ice</span>/snow regions in the Arctic. Preliminary results show promising possibilities of enhancements in surface albedo, sea <span class="hlt">ice</span> area and sea-<span class="hlt">ice</span> concentration, as well as temperature reductions of .5 to 3 degree Kelvin in the Arctic, and global average temperature reductions of .5 to 1 degrees.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950034736&hterms=typing&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtyping','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950034736&hterms=typing&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtyping"><span>Feasibility of sea <span class="hlt">ice</span> typing with synthetic aperture radar (SAR): Merging of Landsat thematic mapper and ERS 1 SAR satellite imagery</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steffen, Konrad; Heinrichs, John</p> <p>1994-01-01</p> <p>Earth Remote-Sensing Satellite (ERS) 1 synthetic aperture radar (SAR) and Landsat thematic mapper (TM) images were acquired for the same area in the Beaufort Sea, April 16 and 18, 1992. The two image pairs were colocated to the same grid (25-m resolution), and a supervised <span class="hlt">ice</span> type classification was performed on the TM images in order to classify <span class="hlt">ice</span> free, nilas, gray <span class="hlt">ice</span>, gray-white <span class="hlt">ice</span>, thin first-year <span class="hlt">ice</span>, medium and thick first-year <span class="hlt">ice</span>, and old <span class="hlt">ice</span>. Comparison of the collocated SAR pixels showed that <span class="hlt">ice</span>-free areas can only be classified under calm wind conditions (less than 3 m/s) and for surface winds greater than 10 m/s based on the backscattering coefficient alone. This is true for <span class="hlt">pack</span> <span class="hlt">ice</span> regions during the cold months of the year where <span class="hlt">ice</span>-free areas are spatially limited and where the capillary waves that cause SAR backscatter are dampened by entrained <span class="hlt">ice</span> crystals. For nilas, two distinct backscatter classes were found at -17 dB and at -10 dB. The higher backscattering coefficient is attributed to the presence of frost flowers on light nilas. Gray and gray-white <span class="hlt">ice</span> have a backscatter signature similar to first-year <span class="hlt">ice</span> and therefore cannot be distinguished by SAR alone. First-year and old <span class="hlt">ice</span> can be clearly separated based on their backscattering coefficient. The performance of the Geophysical Processor System <span class="hlt">ice</span> classifier was <span class="hlt">tested</span> against the Landsat derived <span class="hlt">ice</span> products. It was found that smooth first-year <span class="hlt">ice</span> and rough first-year <span class="hlt">ice</span> were not significantly different in the backscatter domain. <span class="hlt">Ice</span> concentration estimates based on ERS 1 C band SAR showed an error range of 5 to 8% for high <span class="hlt">ice</span> concentration regions, mainly due to misclassified <span class="hlt">ice</span>-free and smooth first-year <span class="hlt">ice</span> areas. This error is expected to increase for areas of lower <span class="hlt">ice</span> concentration. The combination of C band SAR and TM channels 2, 4, and 6 resulted in <span class="hlt">ice</span> typing performance with an estimated accuracy of 90% for all seven <span class="hlt">ice</span> classes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdAtS..35..106Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdAtS..35..106Z"><span>Record low sea-<span class="hlt">ice</span> concentration in the central Arctic during summer 2010</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Jinping; Barber, David; Zhang, Shugang; Yang, Qinghua; Wang, Xiaoyu; Xie, Hongjie</p> <p>2018-01-01</p> <p>The Arctic sea-<span class="hlt">ice</span> extent has shown a declining trend over the past 30 years. <span class="hlt">Ice</span> coverage reached historic minima in 2007 and again in 2012. This trend has recently been assessed to be unique over at least the last 1450 years. In the summer of 2010, a very low sea-<span class="hlt">ice</span> concentration (SIC) appeared at high Arctic latitudes—even lower than that of surrounding <span class="hlt">pack</span> <span class="hlt">ice</span> at lower latitudes. This striking low <span class="hlt">ice</span> concentration—referred to here as a record low <span class="hlt">ice</span> concentration in the central Arctic (CARLIC)—is unique in our analysis period of 2003-15, and has not been previously reported in the literature. The CARLIC was not the result of <span class="hlt">ice</span> melt, because sea <span class="hlt">ice</span> was still quite thick based on in-situ <span class="hlt">ice</span> thickness measurements. Instead, divergent <span class="hlt">ice</span> drift appears to have been responsible for the CARLIC. A high correlation between SIC and wind stress curl suggests that the sea <span class="hlt">ice</span> drift during the summer of 2010 responded strongly to the regional wind forcing. The drift trajectories of <span class="hlt">ice</span> buoys exhibited a transpolar drift in the Atlantic sector and an eastward drift in the Pacific sector, which appeared to benefit the CARLIC in 2010. Under these conditions, more solar energy can penetrate into the open water, increasing melt through increased heat flux to the ocean. We speculate that this divergence of sea <span class="hlt">ice</span> could occur more often in the coming decades, and impact on hemispheric SIC and feed back to the climate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950048358&hterms=Frost&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DFrost','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950048358&hterms=Frost&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DFrost"><span>Measurements of thermal infrared spectral reflectance of frost, snow, and <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Salisbury, John W.; D'Aria, Dana M.; Wald, Andrew</p> <p>1994-01-01</p> <p>Because much of Earth's surface is covered by frost, snow, and <span class="hlt">ice</span>, the spectral emissivities of these materials are a significant input to radiation balance calculations in global atmospheric circulation and climate change models. Until now, however, spectral emissivities of frost and snow have been calculated from the optical constants of <span class="hlt">ice</span>. We have measured directional hemispherical reflectance spectra of frost, snow, and <span class="hlt">ice</span> from which emissivities can be predicted using Kirchhoff's law (e = 1-R). These measured spectra show that contrary to conclusions about the emissivity of snow drawn from previously calculated spectra, snow emissivity departs significantly from blackbody behavior in the 8-14 micrometer region of the spectrum; snow emissivity decreases with both increasing particle size and increasing density due to <span class="hlt">packing</span> or grain welding; while snow emissivity increases due to the presence of meltwater.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011437','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011437"><span>Preparation for Scaling Studies of <span class="hlt">Ice</span>-Crystal <span class="hlt">Icing</span> at the NRC Research Altitude <span class="hlt">Test</span> Facility</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter M.; Bencic, Timothy J.; Tsao, Jen-Ching; Fuleki, Dan; Knezevici, Daniel C.</p> <p>2013-01-01</p> <p>This paper describes experiments conducted at the National Research Council (NRC) of Canadas Research Altitiude <span class="hlt">Test</span> Facility between March 26 and April 11, 2012. The <span class="hlt">tests</span>, conducted collaboratively between NASA and NRC, focus on three key aspects in preparation for later scaling work to be conducted with a NACA 0012 airfoil model in the NRC Cascade rig: (1) cloud characterization, (2) scaling model development, and (3) <span class="hlt">ice</span>-shape profile measurements. Regarding cloud characterization, the experiments focus on particle spectra measurements using two shadowgraphy methods, cloud uniformity via particle scattering from a laser sheet, and characterization of the SEA Multi-Element probe. Overviews of each aspect as well as detailed information on the diagnostic method are presented. Select results from the measurements and interpretation are presented which will help guide future work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080013293','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080013293"><span>Airfoil <span class="hlt">Ice</span>-Accretion Aerodynamics Simulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bragg, Michael B.; Broeren, Andy P.; Addy, Harold E.; Potapczuk, Mark G.; Guffond, Didier; Montreuil, E.</p> <p>2007-01-01</p> <p>NASA Glenn Research Center, ONERA, and the University of Illinois are conducting a major research program whose goal is to improve our understanding of the aerodynamic scaling of <span class="hlt">ice</span> accretions on airfoils. The program when it is completed will result in validated scaled simulation methods that produce the essential aerodynamic features of the full-scale <span class="hlt">iced</span>-airfoil. This research will provide some of the first, high-fidelity, full-scale, <span class="hlt">iced</span>-airfoil aerodynamic data. An initial study classified <span class="hlt">ice</span> accretions based on their aerodynamics into four types: roughness, streamwise <span class="hlt">ice</span>, horn <span class="hlt">ice</span>, and spanwise-ridge <span class="hlt">ice</span>. Subscale <span class="hlt">testing</span> using a NACA 23012 airfoil was performed in the NASA IRT and University of Illinois wind tunnel to better understand the aerodynamics of these <span class="hlt">ice</span> types and to <span class="hlt">test</span> various levels of <span class="hlt">ice</span> simulation fidelity. These studies are briefly reviewed here and have been presented in more detail in other papers. Based on these results, full-scale <span class="hlt">testing</span> at the ONERA F1 tunnel using cast <span class="hlt">ice</span> shapes obtained from molds taken in the IRT will provide full-scale <span class="hlt">iced</span> airfoil data from full-scale <span class="hlt">ice</span> accretions. Using these data as a baseline, the final step is to validate the simulation methods in scale in the Illinois wind tunnel. Computational <span class="hlt">ice</span> accretion methods including LEWICE and ONICE have been used to guide the experiments and are briefly described and results shown. When full-scale and simulation aerodynamic results are available, these data will be used to further develop computational tools. Thus the purpose of the paper is to present an overview of the program and key results to date.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...837...56M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...837...56M"><span>Identification of Accretion as Grain Growth Mechanism in Astrophysically Relevant Water&<span class="hlt">ice</span> Dusty Plasma Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marshall, Ryan S.; Chai, Kil-Byoung; Bellan, Paul M.</p> <p>2017-03-01</p> <p>The grain growth process in the Caltech water-<span class="hlt">ice</span> dusty plasma experiment has been studied using a high-speed camera and a long-distance microscope lens. It is observed that (I) the <span class="hlt">ice</span> grain number density decreases fourfold as the average grain major axis increases from 20 to 80 μm, (II) the major axis length has a log-normal distribution rather than a power-law dependence, and (III) no collisions between <span class="hlt">ice</span> grains are apparent. The grains have a large negative charge resulting in strong mutual repulsion and this, combined with the fractal character of the <span class="hlt">ice</span> grains, prevents them from agglomerating. In order for the grain kinetic energy to be sufficiently small to prevent collisions between <span class="hlt">ice</span> grains, the volumetric <span class="hlt">packing</span> factor (I.e., ratio of the actual volume to the volume of a circumscribing ellipsoid) of the <span class="hlt">ice</span> grains must be less than ˜0.1 depending on the exact relative velocity of the grains in question. Thus, it is concluded that direct accretion of water molecules is very likely to dominate the observed <span class="hlt">ice</span> grain growth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=63179&keyword=air+AND+company&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=63179&keyword=air+AND+company&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>ENVIRONMENTAL TECHNOLOGY VERIFICATION REPORT, FRANCE COMPRESSOR PRODUCTS EMISSIONS <span class="hlt">PACKING</span>, PHASE I REPORT</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>The report presents results of a Phase I <span class="hlt">test</span> of emissions <span class="hlt">packing</span> technology offered by France Compressor Products which is designed to reduce methane leaks from compressor rod <span class="hlt">packing</span> when a compressor is in a standby and pressurized state. This Phase I <span class="hlt">test</span> was executed betwee...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1245128','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1245128"><span>Battery <span class="hlt">Pack</span> Life Estimation through Cell Degradation Data and <span class="hlt">Pack</span> Thermal Modeling for BAS+ Li-Ion Batteries. Cooperative Research and Development Final Report, CRADA Number CRD-12-489</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Smith, Kandler</p> <p></p> <p>Battery Life estimation is one of the key inputs required for Hybrid applications for all GM Hybrid/EV/EREV/PHEV programs. For each Hybrid vehicle program, GM has instituted multi-parameter Design of Experiments generating <span class="hlt">test</span> data at Cell level and also <span class="hlt">Pack</span> level on a reduced basis. Based on experience, generating <span class="hlt">test</span> data on a <span class="hlt">pack</span> level is found to be very expensive, resource intensive and sometimes less reliable. The proposed collaborative project will focus on a methodology to estimate Battery life based on cell degradation data combined with <span class="hlt">pack</span> thermal modeling. NREL has previously developed cell-level battery aging models and <span class="hlt">pack</span>-level thermal/electricalmore » network models, though these models are currently not integrated. When coupled together, the models are expected to describe <span class="hlt">pack</span>-level thermal and aging response of individual cells. GM and NREL will use data collected for GM's Bas+ battery system for evaluation of the proposed methodology and assess to what degree these models can replace <span class="hlt">pack</span>-level aging experiments in the future.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12..350D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12..350D"><span>Modelling the climate and <span class="hlt">ice</span> sheets of the mid-Pliocene warm period: a <span class="hlt">test</span> of model dependency</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dolan, Aisling; Haywood, Alan; Lunt, Daniel; Hill, Daniel</p> <p>2010-05-01</p> <p> British Antarctic Survey thermomechanically coupled <span class="hlt">ice</span> sheet model (BASISM) to <span class="hlt">test</span> the extent to which equilibrium state <span class="hlt">ice</span> sheets in the Northern Hemisphere are GCM dependent. Initial results which do not use GCM-specific topography suggest that employing different GCM climatologies with only small differences in surface air temperature and precipitation has a dramatic effect on the resultant Greenland <span class="hlt">ice</span> sheet, where the end-member <span class="hlt">ice</span> sheets vary from near modern to almost zero <span class="hlt">ice</span> volume. As an extension of this analysis, we will also present results using a second <span class="hlt">ice</span> sheet model (Glimmer), with a view to <span class="hlt">testing</span> the degree to which end-member <span class="hlt">ice</span> sheets are <span class="hlt">ice</span> sheet model dependent, something which has not previously been addressed. Initially, BASISM and Glimmer will be internally optimised for performance, but we will also present a comparison where BASISM will be configured to the Glimmer model setup in a further <span class="hlt">test</span> of <span class="hlt">ice</span> sheet model dependency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-PIA01786.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-PIA01786.html"><span>Space Radar Image of Weddell Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>1999-04-15</p> <p>This is the first calibrated, multi-frequency, multi-polarization spaceborne radar image of the seasonal sea-<span class="hlt">ice</span> cover in the Weddell Sea, Antarctica. The multi-channel data provide scientists with details about the <span class="hlt">ice</span> <span class="hlt">pack</span> they cannot see any other way and indicates that the large expanse of sea-<span class="hlt">ice</span> is, in fact, comprised of many smaller rounded <span class="hlt">ice</span> floes, shown in blue-gray. These data are particularly useful in helping scientists estimate the thickness of the <span class="hlt">ice</span> cover which is often extremely difficult to measure with other remote sensing systems. The extent, and especially thickness, of the polar ocean's sea-<span class="hlt">ice</span> cover together have important implications for global climate by regulating the loss of heat from the ocean to the cold polar atmosphere. The image was acquired on October 3, 1994, by the Spaceborne Imaging Radar-C/X-Band Synthetic Aperture Radar (SIR-C/X-SAR) onboard the space shuttle Endeavour. This image is produced by overlaying three channels of radar data in the following colors: red (C-band, HH-polarization), green (L-band HV-polarization), and blue (L-band, HH-polarization). The image is oriented almost east-west with a center location of 58.2 degrees South and 21.6 degrees East. Image dimensions are 45 kilometers by 18 kilometers (28 miles by 11 miles). Most of the <span class="hlt">ice</span> cover is composed of rounded, undeformed blue-gray floes, about 0.7 meters (2 feet) thick, which are surrounded by a jumble of red-tinged deformed <span class="hlt">ice</span> pieces which are up to 2 meters (7 feet) thick. The winter cycle of <span class="hlt">ice</span> growth and deformation often causes this <span class="hlt">ice</span> cover to split apart, exposing open water or "leads." <span class="hlt">Ice</span> growth within these openings is rapid due to the cold, brisk Antarctic atmosphere. Different stages of new-<span class="hlt">ice</span> growth can be seen within the linear leads, resulting from continuous opening and closing. The blue lines within the leads are open water areas in new fractures which are roughened by wind. The bright red lines are an intermediate stage of new-<span class="hlt">ice</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C34B..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C34B..02B"><span>Constraining <span class="hlt">ice</span> sheet history in the Weddell Sea, West Antarctica, using <span class="hlt">ice</span> fabric at Korff <span class="hlt">Ice</span> Rise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brisbourne, A.; Smith, A.; Kendall, J. M.; Baird, A. F.; Martin, C.; Kingslake, J.</p> <p>2017-12-01</p> <p>The grounding history of <span class="hlt">ice</span> rises (grounded area of independent flow regime within a floating <span class="hlt">ice</span> shelf) can be used to constrain large scale <span class="hlt">ice</span> sheet history: <span class="hlt">ice</span> fabric, resulting from the preferred orientation of <span class="hlt">ice</span> crystals due to the stress regime, can be used to infer this grounding history. With the aim of measuring the present day <span class="hlt">ice</span> fabric at Korff <span class="hlt">Ice</span> Rise, West Antarctica, a multi-azimuth wide-angle seismic experiment was undertaken. Three wide-angle common-midpoint gathers were acquired centred on the apex of the <span class="hlt">ice</span> rise, at azimuths of 60 degrees to one another, to measure variation in seismic properties with offset and azimuth. Both vertical and horizontal receivers were used to record P and S arrivals including converted phases. Measurements of the variation with offset and azimuth of seismic traveltimes, seismic attenuation and shear wave splitting have been used to quantify seismic anisotropy in the <span class="hlt">ice</span> column. The observations cannot be reproduced using an isotropic <span class="hlt">ice</span> column model. Anisotropic ray tracing has been used to <span class="hlt">test</span> likely models of <span class="hlt">ice</span> fabric by comparison with the data. A model with a weak girdle fabric overlying a strong cluster fabric provides the best fit to the observations. Fabric of this nature is consistent with Korff <span class="hlt">Ice</span> Rise having been stable for the order of 10,000 years without any ungrounding or significant change in the <span class="hlt">ice</span> flow configuration across the <span class="hlt">ice</span> rise for this period. This observation has significant implications for the <span class="hlt">ice</span> sheet history of the Weddell Sea sector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70033649','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70033649"><span>Extent of the last <span class="hlt">ice</span> sheet in northern Scotland <span class="hlt">tested</span> with cosmogenic 10Be exposure ages</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Phillips, W.M.; Hall, A.M.; Ballantyne, C.K.; Binnie, S.; Kubik, P.W.; Freeman, S.</p> <p>2008-01-01</p> <p>The extent of the last British-Irish <span class="hlt">Ice</span> Sheet (BIIS) in northern Scotland is disputed. A restricted <span class="hlt">ice</span> sheet model holds that at the global Last Glacial Maximum (LGM; ca. 23-19 ka) the BIIS terminated on land in northern Scotland, leaving Buchan, Caithness and the Orkney Islands <span class="hlt">ice</span>-free. An alternative model implies that these three areas were <span class="hlt">ice</span>-covered at the LGM, with the BIIS extending offshore onto the adjacent shelves. We <span class="hlt">test</span> the two models using cosmogenic 10Be surface exposure dating of erratic boulders and glacially eroded bedrock from the three areas. Our results indicate that the last BIIS covered all of northern Scotland during the LGM, but that widespread deglaciation of Caithness and Orkney occurred prior to rapid warming at ca. 14.5 ka. Copyright ?? 2008 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29208255','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29208255"><span>Using <span class="hlt">Ice</span> Cream for Diagnosis of Diabetes Mellitus and Impaired Glucose Tolerance: An Alternative to the Oral Glucose Tolerance <span class="hlt">Test</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chanprasertpinyo, Wandee; Bhirommuang, Nattapimon; Surawattanawiset, Titiporn; Tangsermwong, Thanwarin; Phanachet, Pariya; Sriphrapradang, Chutintorn</p> <p>2017-12-01</p> <p>Oral glucose tolerance <span class="hlt">test</span> (OGTT) is a sensitive and reliable <span class="hlt">test</span> for diabetes mellitus and impaired glucose tolerance (IGT). However, poor patient tolerance of glucose solutions is common. We aim to compare the diagnostic value of an <span class="hlt">ice</span> cream <span class="hlt">test</span> with a standard OGTT. A total of 104 healthy adults were randomly assigned to either 75-g OGTT or <span class="hlt">ice</span> cream, followed by a crossover to the other <span class="hlt">test</span>. Most patients were females (71%). Mean age was 37 ± 12 years, and body mass index was 24.2 ± 3.9kg/m 2 . Diabetes mellitus and IGT, as diagnosed by 75-g OGTT, were 4.8% and 6.7%, respectively. The 2-hour plasma glucose levels were 110 ± 55.5mg/dL with 75-g glucose and 97.52 ± 40.7mg/dL with <span class="hlt">ice</span> cream. The correlation coefficient of 2-hour plasma glucose for the 2 <span class="hlt">tests</span> was 0.82 (95% CI: 0.75-0.87; P < 0.001). Discordant diagnostic results, based on 2-hour plasma glucose levels, were 9.61%. By using a combination of fasting plasma glucose and 2-hour plasma glucose values, the <span class="hlt">ice</span> cream <span class="hlt">test</span> would have missed 5.76% of those at high risk for diabetes mellitus (impaired fasting glucose and IGT) or diabetes. An <span class="hlt">ice</span> cream <span class="hlt">test</span> may serve as an alternative to a 75-g OGTT. Before applying this <span class="hlt">test</span> in clinical practice, it needs to be validated in a larger population. Copyright © 2017 Southern Society for Clinical Investigation. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.P21B1223L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.P21B1223L"><span>Laboratory measurements of <span class="hlt">ice</span> tensile strength dependence on density and concentration of silicate and polymer impurities at low temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Litwin, K. L.; Beyeler, J. D.; Polito, P. J.; Zygielbaum, B. R.; Sklar, L. S.; Collins, G. C.</p> <p>2009-12-01</p> <p>The tensile strength of <span class="hlt">ice</span> bedrock on Titan should strongly influence the effectiveness of the erosional processes responsible for carving the extensive fluvial drainage networks and other surface features visible in images returned by the Cassini and Huygens probes. Recent measurements of the effect of temperature on the tensile strength of low-porosity, polycrystalline <span class="hlt">ice</span>, without impurities, suggest that <span class="hlt">ice</span> bedrock at the Titan surface temperature of 93 K may be as much as five times stronger than <span class="hlt">ice</span> at terrestrial surface temperatures. However, <span class="hlt">ice</span> bedrock on Titan and other outer solar system bodies may have significant porosity, and impurities such silicates or polymers are possible in such <span class="hlt">ices</span>. In this laboratory investigation we are exploring the dependence of tensile strength on the density and concentration of impurities, for polycrystalline <span class="hlt">ice</span> across a wide range of temperatures. We use the Brazilian tensile splitting <span class="hlt">test</span> to measure strength, and control temperature with dry <span class="hlt">ice</span> and liquid nitrogen. The 50 mm diameter <span class="hlt">ice</span> cores are made from a log-normally distributed seed crystal mixture with a median size of 1.4 mm. To control <span class="hlt">ice</span> density and porosity we vary the <span class="hlt">packing</span> density of the seed grains in core molds and vary the degree of saturation of the matrix with added near-freezing distilled water. We also vary <span class="hlt">ice</span> density by blending in a similarly-sized mixture of angular fragments of two types of impurities, a fine-grained volcanic rock and a polyethylene polymer. Because both types of impurities have greater tensile strength than <span class="hlt">ice</span> at Earth surface temperatures, we expect higher concentrations of impurities to correlate with increased strength for <span class="hlt">ice</span>-rock and <span class="hlt">ice</span>-polymer mixtures. However, at the ultra-cold temperatures of the outer planets, we expect significant divergence in the temperature dependence of <span class="hlt">ice</span> tensile strength for the various mixtures and resulting densities. These measurements will help constrain the range of possible</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018HMT...tmp..130X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018HMT...tmp..130X"><span>Numerical simulation of flow and melting characteristics of seawater-<span class="hlt">ice</span> crystals two-phase flow in inlet straight pipe of shell and tube heat exchanger of polar ship</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Li; Huang, Chang-Xu; Huang, Zhen-Fei; Sun, Qiang; Li, Jie</p> <p>2018-05-01</p> <p>The <span class="hlt">ice</span> crystal particles are easy to enter into the seawater cooling system of polar ship together with seawater when it sails in the Arctic. They are easy to accumulate in the pipeline, causing serious blockage of the cooling pipe. In this study, the flow and melting characteristics of <span class="hlt">ice</span> particles-seawater two-phase flow in inlet straight pipe of shell-and-tube heat exchanger were numerically simulated by using Eulerian-Eulerian two-fluid model coupled with the interphase heat and mass transfer model. The influences of inlet <span class="hlt">ice</span> <span class="hlt">packing</span> factor, <span class="hlt">ice</span> crystal particle diameter, and inlet velocity on the distribution and melting characteristics of <span class="hlt">ice</span> crystals were investigated. The degree of asymmetry of the distribution of <span class="hlt">ice</span> crystals in the cross section decreases gradually when the IPF changes from 5 to 15%. The volume fractions of <span class="hlt">ice</span> crystals near the top of the outlet cross section are 19.59, 19.51, and 22.24% respectively for <span class="hlt">ice</span> <span class="hlt">packing</span> factor of 5, 10 and 15%. When the particle diameter is 0.5 mm, the <span class="hlt">ice</span> crystals are gradually stratified during the flow process. With particle diameters of 1.0 and 2.0 mm, the region with the highest volume fraction of <span class="hlt">ice</span> crystals is a small circle and the contours in the cloud map are compact. The greater the inlet flow velocity, the less stratified the <span class="hlt">ice</span> crystals and the more obvious the turbulence on the outlet cross section. The average volume fraction of <span class="hlt">ice</span> crystals along the flow direction is firstly rapidly reduced and then stabilized after 300 mm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060017059','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060017059"><span>Dynamic Wind-Tunnel <span class="hlt">Testing</span> of a Sub-Scale <span class="hlt">Iced</span> Business Jet</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Sam; Barnhart, Billy P.; Ratvasky, Thomas P.; Dickes, Edward; Thacker, Michael</p> <p>2006-01-01</p> <p>The effect of <span class="hlt">ice</span> accretion on a 1/12-scale complete aircraft model of a business jet was studied in a rotary-balance wind tunnel. Three types of <span class="hlt">ice</span> accretions were considered: <span class="hlt">ice</span> protection system failure shape, pre-activation roughness, and runback shapes that form downstream of the thermal <span class="hlt">ice</span> protection system. The results were compared with those from a 1/12-scale semi-span wing of the same aircraft at similar Reynolds number. The data showed that the full aircraft and the semi-span wing models showed similar characteristics, especially post stall behavior under <span class="hlt">iced</span> configuration. However, there were also some discrepancies, such as the magnitude in the reductions in the maximum lift coefficient. Most of the <span class="hlt">ice</span>-induced effects were limited to longitudinal forces. Rotational and forced oscillation studies showed that the effects of <span class="hlt">ice</span> on lateral forces were relatively minor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23574610','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23574610"><span>Impact of early and late winter <span class="hlt">icing</span> events on sub-arctic dwarf shrubs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Preece, C; Phoenix, G K</p> <p>2014-01-01</p> <p>Polar regions are predicted to undergo large increases in winter temperature and an increased frequency of freeze-thaw cycles, which can cause <span class="hlt">ice</span> layers in the snow <span class="hlt">pack</span> and <span class="hlt">ice</span> encasement of vegetation. Early or late winter timing of <span class="hlt">ice</span> encasement could, however, modify the extent of damage caused to plants. To determine impacts of the date of <span class="hlt">ice</span> encasement, a novel field experiment was established in sub-arctic Sweden, with <span class="hlt">icing</span> events simulated in January and March 2008 and 2009. In the subsequent summers, reproduction, phenology, growth and mortality, as well as physiological indicators of leaf damage were measured in the three dominant dwarf shrubs: Vaccinium uliginosum, Vaccinium vitis-idaea and Empetrum nigrum. It was hypothesised that January <span class="hlt">icing</span> would be more damaging compared to March <span class="hlt">icing</span> due to the longer duration of <span class="hlt">ice</span> encasement. Following 2 years of <span class="hlt">icing</span>, E. nigrum berry production was 83% lower in January-<span class="hlt">iced</span> plots compared to controls, and V. vitis-idaea electrolyte leakage was increased by 69%. Conversely, electrolyte leakage of E. nigrum was 25% lower and leaf emergence of V. vitis-idaea commenced 11 days earlier in March-<span class="hlt">iced</span> plots compared to control plots in 2009. There was no effect of <span class="hlt">icing</span> on any of the other parameters measured, indicating that overall these study species have moderate to high tolerance to <span class="hlt">ice</span> encasement. Even much longer exposure under the January <span class="hlt">icing</span> treatment does not clearly increase damage. © 2013 German Botanical Society and The Royal Botanical Society of the Netherlands.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11049062','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11049062"><span>Rheological properties of <span class="hlt">ice</span> cream mixes and frozen <span class="hlt">ice</span> creams containing fat and fat replacers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Adapa, S; Dingeldein, H; Schmidt, K A; Herald, T J</p> <p>2000-10-01</p> <p><span class="hlt">Ice</span> cream mixes and frozen <span class="hlt">ice</span> creams at milk fat levels of 12%, 8%, 6%, 6% plus a protein-based fat replacer, and 6% plus a carbohydrate-based fat replacer were evaluated for viscoelastic properties by dynamic <span class="hlt">testing</span> with sinusoidal oscillatory <span class="hlt">tests</span> at various frequencies. The storage modulus (G'), loss modulus (G"), and tan delta (G"/G') were calculated for all the treatments to determine changes in the viscous and elastic properties of the mixes and frozen <span class="hlt">ice</span> creams due to fat content. In <span class="hlt">ice</span> cream mixes, G' and G" exhibited a strong frequency dependence. The G" was higher than G' throughout the frequency range (1 to 8 Hz) examined, without any crossover, except for the 12% mix. Elastic properties of the <span class="hlt">ice</span> cream mixes decreased as fat content decreased. Tan delta values indicated that fat replacers did not enhance the elastic properties of the <span class="hlt">ice</span> cream mixes. In all frozen <span class="hlt">ice</span> creams, G' and G" again showed a frequency dependence throughout the range <span class="hlt">tested</span> (0.5 to 10 Hz). The amount of fat in <span class="hlt">ice</span> creams and the degree of fat destabilization affected the elasticity in the frozen product. Even though the <span class="hlt">ice</span> creams did not have significant elastic properties, when compared as a group the samples with higher fat content had higher elastic properties. The addition of protein-based and carbohydrate-based fat replacers did not enhance the elastic properties of the <span class="hlt">ice</span> creams but did increase the viscous properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013707','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013707"><span>Evolution of the Marginal <span class="hlt">Ice</span> Zone: Adaptive Sampling with Autonomous Gliders</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>kinetic energy (ε). Gliders also sampled dissolved oxygen, optical backscatter ( chlorophyll and CDOM fluorescence) and multi-spectral downwelling...Fig. 2). In the <span class="hlt">pack</span>, Pacific Summer Water and a deep chlorophyll maximum form distinct layers at roughly 60 m and 80 m, respectively, which become...Sections across the <span class="hlt">ice</span> edge just prior to recovery, during freeze-up, reveal elevated chlorophyll fluorescence throughout the mixed layer (Fig. 4</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050186848&hterms=Running+beneficial&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DRunning%2Bbeneficial','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050186848&hterms=Running+beneficial&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DRunning%2Bbeneficial"><span>Surface Modeling and Grid Generation for <span class="hlt">Iced</span> Airfoils (Smagg<span class="hlt">Ice</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hammond, Brandy M.</p> <p>2004-01-01</p> <p>Many of the troubles associated with problem solving are alleviated when there is a model that can be used to represent the problem. Through the Advanced Graphics and Visualization (G-VIS) Laboratory and other facilities located within the Research Analysis Center, the Computer Services Division (CSD) is able to develop and maintain programs and software that allow for the modeling of various situations. For example, the <span class="hlt">Icing</span> Research Branch is devoted to investigating the effect of <span class="hlt">ice</span> that forms on the wings and other airfoils of airplanes while in flight. While running <span class="hlt">tests</span> that physically generate <span class="hlt">ice</span> and wind on airfoils within the laboratories and wind tunnels on site are done, it would be beneficial if most of the preliminary work could be done outside of the lab. Therefore, individuals from within CSD have collaborated with <span class="hlt">Icing</span> Research in order to create Smagg<span class="hlt">Ice</span>. This software allows users to create <span class="hlt">ice</span> patterns on clean airfoils or open files containing a variety of <span class="hlt">icing</span> situations, manipulate and measure these forms, generate, divide, and merge grids around these elements for more explicit analysis, and specify and rediscretize subcurves. With the projected completion date of Summer 2005, the majority of the focus of the Smagglce team is user-functionality and error handling. My primary responsibility is to <span class="hlt">test</span> the Graphical User Interface (GUI) in Smagg<span class="hlt">Ice</span> in order to ensure the usability and verify the expected results of the events (buttons, menus, etc.) within the program. However, there is no standardized, systematic way in which to <span class="hlt">test</span> all the possible combinations or permutations of events, not to mention unsolicited events such as errors. Moreover, scripting <span class="hlt">tests</span>, if not done properly and with a view towards inevitable revision, can result in more apparent errors within the software and in effect become useless whenever the developers of the program make a slight change in the way a specific process is executed. My task therefore</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150019659','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150019659"><span>Recent Advances in the LEWICE <span class="hlt">Icing</span> Model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wright, William B.; Addy, Gene; Struk, Peter; Bartkus, Tadas</p> <p>2015-01-01</p> <p>This paper will describe two recent modifications to the Glenn <span class="hlt">ICE</span> software. First, a capability for modeling <span class="hlt">ice</span> crystals and mixed phase <span class="hlt">icing</span> has been modified based on recent experimental data. Modifications have been made to the <span class="hlt">ice</span> particle bouncing and erosion model. This capability has been added as part of a larger effort to model <span class="hlt">ice</span> crystal ingestion in aircraft engines. Comparisons have been made to <span class="hlt">ice</span> crystal <span class="hlt">ice</span> accretions performed in the NRC Research Altitude <span class="hlt">Test</span> Facility (RATFac). Second, modifications were made to the run back model based on data and observations from thermal scaling <span class="hlt">tests</span> performed in the NRC Altitude <span class="hlt">Icing</span> Tunnel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140008934','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140008934"><span>Evaluation of Arctic Sea <span class="hlt">Ice</span> Thickness Simulated by Arctic Ocean Model Intercomparison Project Models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, Mark; Proshuntinsky, Andrew; Aksenov, Yevgeny; Nguyen, An T.; Lindsay, Ron; Haas, Christian; Zhang, Jinlun; Diansky, Nikolay; Kwok, Ron; Maslowski, Wieslaw; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140008934'); toggleEditAbsImage('author_20140008934_show'); toggleEditAbsImage('author_20140008934_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140008934_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140008934_hide"></p> <p>2012-01-01</p> <p>Six Arctic Ocean Model Intercomparison Project model simulations are compared with estimates of sea <span class="hlt">ice</span> thickness derived from pan-Arctic satellite freeboard measurements (2004-2008); airborne electromagnetic measurements (2001-2009); <span class="hlt">ice</span> draft data from moored instruments in Fram Strait, the Greenland Sea, and the Beaufort Sea (1992-2008) and from submarines (1975-2000); and drill hole data from the Arctic basin, Laptev, and East Siberian marginal seas (1982-1986) and coastal stations (1998-2009). Despite an assessment of six models that differ in numerical methods, resolution, domain, forcing, and boundary conditions, the models generally overestimate the thickness of measured <span class="hlt">ice</span> thinner than approximately 2 mand underestimate the thickness of <span class="hlt">ice</span> measured thicker than about approximately 2m. In the regions of flat immobile landfast <span class="hlt">ice</span> (shallow Siberian Seas with depths less than 25-30 m), the models generally overestimate both the total observed sea <span class="hlt">ice</span> thickness and rates of September and October <span class="hlt">ice</span> growth from observations by more than 4 times and more than one standard deviation, respectively. The models do not reproduce conditions of fast <span class="hlt">ice</span> formation and growth. Instead, the modeled fast <span class="hlt">ice</span> is replaced with <span class="hlt">pack</span> <span class="hlt">ice</span> which drifts, generating ridges of increasing <span class="hlt">ice</span> thickness, in addition to thermodynamic <span class="hlt">ice</span> growth. Considering all observational data sets, the better correlations and smaller differences from observations are from the Estimating the Circulation and Climate of the Ocean, Phase II and Pan-Arctic <span class="hlt">Ice</span> Ocean Modeling and Assimilation System models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940007284&hterms=holt+winters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dholt%2Bwinters','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940007284&hterms=holt+winters&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dholt%2Bwinters"><span>Sea <span class="hlt">ice</span> radar signatures from ERS-1 SAR during late Summer and Fall in the Beaufort and Chukchi Seas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holt, Benjamin; Cunningham, Glenn; Kwok, Ron</p> <p>1993-01-01</p> <p>A study which examines ERS-1 C band SAR (Synthetic Aperture Radar) imagery of sea <span class="hlt">ice</span> obtained in the Beaufort and Chukchi Seas from mid Summer through Fall freeze up and early Winter in 1991 is presented. Radar backscatter statistics of sea <span class="hlt">ice</span> were obtained from the imagery, using common floes tracked through consecutive repeat images whenever possible. During the Summer months, strong fluctuations in <span class="hlt">ice</span> signatures of several dB are observed over 2 to 3 day periods, which are found to be closely related to air temperature excursions above and below freezing that alters the phase of the <span class="hlt">ice</span> surface. As air temperatures drop steadily below freezing in the Fall, the signatures of the <span class="hlt">pack</span> <span class="hlt">ice</span> increase in brightness and become more stable with time. Multiyear <span class="hlt">ice</span> is distinguished from rough and smooth first year <span class="hlt">ice</span>. There are also variations in the multiyear signatures with latitude. Large variations are seen in new <span class="hlt">ice</span> and open water contained within leads which results in ambiguous classification.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17868292','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17868292"><span>Sea <span class="hlt">ice</span> occurrence predicts genetic isolation in the Arctic fox.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Geffen, Eli; Waidyaratne, Sitara; Dalén, Love; Angerbjörn, Anders; Vila, Carles; Hersteinsson, Pall; Fuglei, Eva; White, Paula A; Goltsman, Michael; Kapel, Christian M O; Wayne, Robert K</p> <p>2007-10-01</p> <p>Unlike Oceanic islands, the islands of the Arctic Sea are not completely isolated from migration by terrestrial vertebrates. The <span class="hlt">pack</span> <span class="hlt">ice</span> connects many Arctic Sea islands to the mainland during winter months. The Arctic fox (Alopex lagopus), which has a circumpolar distribution, populates numerous islands in the Arctic Sea. In this study, we used genetic data from 20 different populations, spanning the entire distribution of the Arctic fox, to identify barriers to dispersal. Specifically, we considered geographical distance, occurrence of sea <span class="hlt">ice</span>, winter temperature, ecotype, and the presence of red fox and polar bear as nonexclusive factors that influence the dispersal behaviour of individuals. Using distance-based redundancy analysis and the BIOENV procedure, we showed that occurrence of sea <span class="hlt">ice</span> is the key predictor and explained 40-60% of the genetic distance among populations. In addition, our analysis identified the Commander and Pribilof Islands Arctic populations as genetically unique suggesting they deserve special attention from a conservation perspective.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C21A0650P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C21A0650P"><span>Sea <span class="hlt">Ice</span> Summer Camp: Bringing Together Arctic Sea <span class="hlt">Ice</span> Modelers and Observers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Perovich, D. K.; Holland, M. M.</p> <p>2016-12-01</p> <p>The Arctic sea <span class="hlt">ice</span> has undergone dramatic change and numerical models project this to continue for the foreseeable future. Understanding the mechanisms behind sea <span class="hlt">ice</span> loss and its consequences for the larger Arctic and global systems is of critical importance if we are to anticipate and plan for the future. One impediment to progress is a disconnect between the observational and modeling communities. A sea <span class="hlt">ice</span> summer camp was held in Barrow Alaska from 26 May to 1 June 2016 to overcome this impediment and better integrate the sea <span class="hlt">ice</span> community. The 25 participants were a mix of modelers and observers from 13 different institutions at career stages from graduate student to senior scientist. The summer camp provided an accelerated program on sea <span class="hlt">ice</span> observations and models and also fostered future collaborative interdisciplinary activities. Each morning was spent in the classroom with a daily lecture on an aspect of modeling or remote sensing followed by practical exercises. Topics included using models to assess sensitivity, to <span class="hlt">test</span> hypotheses and to explore sources of uncertainty in future Arctic sea <span class="hlt">ice</span> loss. The afternoons were spent on the <span class="hlt">ice</span> making observations. There were four observational activities; albedo observations, <span class="hlt">ice</span> thickness measurements, <span class="hlt">ice</span> coring and physical properties, and <span class="hlt">ice</span> morphology surveys. The last field day consisted of a grand challenge where the group formulated a hypothesis, developed an observational and modeling strategy to <span class="hlt">test</span> the hypothesis, and then integrated the observations and model results. The impacts of changing sea <span class="hlt">ice</span> are being felt today in Barrow Alaska. We opened a dialog with Barrow community members to further understand these changes. This included an evening discussion with two Barrow sea <span class="hlt">ice</span> experts and a community presentation of our work in a public lecture at the Inupiat Heritage Center.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110011418','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110011418"><span>The ISS Increments 3 and 4 <span class="hlt">Test</span> Report: For the Active Rack Isolation System ISS Characterization Experiment (ARIS-<span class="hlt">ICE</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Quraishi, Naveed; Allen, Jim; Bushnell, Glenn; Fialho, Ian</p> <p>2003-01-01</p> <p>The purpose of ARIS-<span class="hlt">ICE</span> is to improve, optimize then operationally <span class="hlt">test</span> and document the performance of the ARIS system on the International Space Station. The <span class="hlt">ICE</span> program required <span class="hlt">testing</span> across a full 3 increments (2 through 4). This paper represents the operational report summarizing our accomplishments through the third and fourth increment of <span class="hlt">testing</span>. The main objectives and results of the increment two <span class="hlt">testing</span> are discussed in The Increment two Operational Report. This report can be obtained from the ISS Payloads Office or from (http://iss-www.isc.nasa.gov/sslissapt/payofc/OZ3/ARIS.html). In summary these were to ensure the smooth and successful activation of the system and correct operational issues related to long term <span class="hlt">testing</span>. Then the follow on increment 3 & 4 <span class="hlt">testing</span> encompassed the majority of the on orbit performance assessments and improvements made to the ARIS system. The intent here is to report these preliminary results of the increment 3 & 4 ARIS-<span class="hlt">ICE</span> <span class="hlt">testing</span> as well as the ARIS system improvements made for our users and customers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070021400&hterms=relationships&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D50%26Ntt%3Drelationships','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070021400&hterms=relationships&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D50%26Ntt%3Drelationships"><span>Spatial Variability of Barrow-Area Shore-Fast Sea <span class="hlt">Ice</span> and Its Relationships to Passive Microwave Emissivity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Maslanik, J. A.; Rivas, M. Belmonte; Holmgren, J.; Gasiewski, A. J.; Heinrichs, J. F.; Stroeve, J. C.; Klein, M.; Markus, T.; Perovich, D. K.; Sonntag, J. G.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20070021400'); toggleEditAbsImage('author_20070021400_show'); toggleEditAbsImage('author_20070021400_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20070021400_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20070021400_hide"></p> <p>2006-01-01</p> <p>Aircraft-acquired passive microwave data, laser radar height observations, RADARSAT synthetic aperture radar imagery, and in situ measurements obtained during the AMSR-<span class="hlt">Ice</span>03 experiment are used to investigate relationships between microwave emission and <span class="hlt">ice</span> characteristics over several space scales. The data fusion allows delineation of the shore-fast <span class="hlt">ice</span> and <span class="hlt">pack</span> <span class="hlt">ice</span> in the Barrow area, AK, into several <span class="hlt">ice</span> classes. Results show good agreement between observed and Polarimetric Scanning Radiometer (PSR)-derived snow depths over relatively smooth <span class="hlt">ice</span>, with larger differences over ridged and rubbled <span class="hlt">ice</span>. The PSR results are consistent with the effects on snow depth of the spatial distribution and nature of <span class="hlt">ice</span> roughness, ridging, and other factors such as <span class="hlt">ice</span> age. Apparent relationships exist between <span class="hlt">ice</span> roughness and the degree of depolarization of emission at 10,19, and 37 GHz. This depolarization .would yield overestimates of total <span class="hlt">ice</span> concentration using polarization-based algorithms, with indications of this seen when the NT-2 algorithm is applied to the PSR data. Other characteristics of the microwave data, such as effects of grounding of sea <span class="hlt">ice</span> and large contrast between sea <span class="hlt">ice</span> and adjacent land, are also apparent in the PSR data. Overall, the results further demonstrate the importance of macroscale <span class="hlt">ice</span> roughness conditions such as ridging and rubbling on snow depth and microwave emissivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1917705S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1917705S"><span><span class="hlt">Ice</span> particle collisions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sampara, Naresh; Turnbull, Barbara; Hill, Richard; Swift, Michael</p> <p>2017-04-01</p> <p> becomes more likely when the particles are new and rough, but also after they have been through many collisions. Experiment 2: To create an even higher collision density and to understand the collective behaviour of these <span class="hlt">ice</span> particles, a sample of them were placed to cover the tray of an electromagnetic shaker, mounted in an environment controlled chamber at -2°C. Continuous shaking of this system permitted observation of a spontaneous transition from dry granular behaviour to that of wetted granules. Vibrating with a fixed acceleration, image sequences were recorded every 10 min to show that at early stage (<15min) the particles adopted the dry granular flow (particles are free to bounce on the vibrating plate). After circa 40 min 90% particles became spontaneously immobile in an approximately hexagonally <span class="hlt">packed</span> 2 dimensional sheet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900007135','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900007135"><span>Parallel algorithm for determining motion vectors in <span class="hlt">ice</span> floe images by matching edge features</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Manohar, M.; Ramapriyan, H. K.; Strong, J. P.</p> <p>1988-01-01</p> <p>A parallel algorithm is described to determine motion vectors of <span class="hlt">ice</span> floes using time sequences of images of the Arctic ocean obtained from the Synthetic Aperture Radar (SAR) instrument flown on-board the SEASAT spacecraft. Researchers describe a parallel algorithm which is implemented on the MPP for locating corresponding objects based on their translationally and rotationally invariant features. The algorithm first approximates the edges in the images by polygons or sets of connected straight-line segments. Each such edge structure is then reduced to a seed point. Associated with each seed point are the descriptions (lengths, orientations and sequence numbers) of the lines constituting the corresponding edge structure. A parallel matching algorithm is used to match <span class="hlt">packed</span> arrays of such descriptions to identify corresponding seed points in the two images. The matching algorithm is designed such that fragmentation and merging of <span class="hlt">ice</span> floes are taken into account by accepting partial matches. The technique has been demonstrated to work on synthetic <span class="hlt">test</span> patterns and real image pairs from SEASAT in times ranging from .5 to 0.7 seconds for 128 x 128 images.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880015729','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880015729"><span>National plans for aircraft <span class="hlt">icing</span> and improved aircraft <span class="hlt">icing</span> forecasts and associated warning services</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pass, Ralph P.</p> <p>1988-01-01</p> <p>Recently, the United States has increased its activities related to aircraft <span class="hlt">icing</span> in numerous fields: <span class="hlt">ice</span> phobics, revised characterization of <span class="hlt">icing</span> conditions, instrument development/evaluation, de-<span class="hlt">ice/anti-ice</span> devices, simulated supercooled clouds, computer simulation and flight <span class="hlt">tests</span>. The Federal Coordinator for Meteorology is involved in two efforts, one a National Plan on Aircraft <span class="hlt">Icing</span> and the other a plan for Improved Aircraft <span class="hlt">Icing</span> Forecasts and Associated Warning Services. These two plans will provide an approved structure for future U.S. activities related to aircraft <span class="hlt">icing</span>. The recommended activities will significantly improve the position of government agencies to perform mandated activities and to enable U.S. manufacturers to be competitive in the world market.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830005852','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830005852"><span>Development and <span class="hlt">test</span> of a Microwave <span class="hlt">Ice</span> Accretion Measurement Instrument (MIAMI)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Magenheim, B.; Rocks, J. K.</p> <p>1982-01-01</p> <p>The development of an <span class="hlt">ice</span> accretion measurement instrument that is a highly sensitive, accurate, rugged and reliable microprocessor controlled device using low level microwave energy for non-instrusive real time measurement and recording of <span class="hlt">ice</span> growth history, including <span class="hlt">ice</span> thickness and accretion rate is discussed. Data is displayed and recorded digitally. New experimental data is presented, obtained with the instrument, which demonstrates its ability to measure <span class="hlt">ice</span> growth on a two-dimensional airfoil. The device is suitable for aircraft <span class="hlt">icing</span> protection. It may be mounted flush, non-intrusively, on any part of an aircraft skin including rotor blades and engine inlets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol8/pdf/CFR-2011-title7-vol8-sec906-340.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol8/pdf/CFR-2011-title7-vol8-sec906-340.pdf"><span>7 CFR 906.340 - Container, <span class="hlt">pack</span>, and container marking regulations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... committee for <span class="hlt">testing</span> in connection with a research project conducted by or in cooperation with the... requirements of standard sizing: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of... sizes in Table II: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of Grapefruit...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol8/pdf/CFR-2012-title7-vol8-sec906-340.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol8/pdf/CFR-2012-title7-vol8-sec906-340.pdf"><span>7 CFR 906.340 - Container, <span class="hlt">pack</span>, and container marking regulations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... committee for <span class="hlt">testing</span> in connection with a research project conducted by or in cooperation with the... requirements of standard sizing: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of... sizes in Table II: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of Grapefruit...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol8/pdf/CFR-2014-title7-vol8-sec906-340.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol8/pdf/CFR-2014-title7-vol8-sec906-340.pdf"><span>7 CFR 906.340 - Container, <span class="hlt">pack</span>, and container marking regulations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... committee for <span class="hlt">testing</span> in connection with a research project conducted by or in cooperation with the... requirements of standard sizing: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of... sizes in Table II: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of Grapefruit...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol8/pdf/CFR-2013-title7-vol8-sec906-340.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol8/pdf/CFR-2013-title7-vol8-sec906-340.pdf"><span>7 CFR 906.340 - Container, <span class="hlt">pack</span>, and container marking regulations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... committee for <span class="hlt">testing</span> in connection with a research project conducted by or in cooperation with the... requirements of standard sizing: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of... sizes in Table II: Provided, That the <span class="hlt">packing</span> tolerances in the U.S. Standards for Grades of Grapefruit...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010049676','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010049676"><span>Aero-thermal Calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (2000 <span class="hlt">Tests</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gonsalez, Jose C.; Arrington, E. Allen; Curry, Monroe R., III</p> <p>2001-01-01</p> <p>Aerothermal calibration measurements and flow quality surveys were made in the <span class="hlt">test</span> section of the <span class="hlt">Icing</span> Research Tunnel at the NASA Glenn Research Center. These surveys were made following major facility modifications including widening of the heat exchanger tunnel section, replacement of the heat exchanger, installation of new turning vanes, and installation of new fan exit guide vanes. Standard practice at NASA Glenn requires that <span class="hlt">test</span> section calibration and flow quality surveys be performed following such major facility modifications. A single horizontally oriented rake was used to survey the flow field at several vertical positions within a single cross-sectional plane of the <span class="hlt">test</span> section. These surveys provided a detailed mapping of the total and static pressure, total temperature, Mach number, velocity, flow angle and turbulence intensity. Data were acquired over the entire velocity and total temperature range of the facility. No <span class="hlt">icing</span> conditions were <span class="hlt">tested</span>; however, the effects of air sprayed through the water injecting spray bars were assessed. All data indicate good flow quality. Mach number standard deviations were less than 0.0017, flow angle standard deviations were between 0.3 deg and 0.8 deg, total temperature standard deviations were between 0.5 and 1.8 F for subfreezing conditions, axial turbulence intensities varied between 0.3 and 1.0 percent, and transverse turbulence intensities varied between 0.3 and 1.5 percent. Measurement uncertainties were also quantified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25714114','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25714114"><span>Fire <span class="hlt">Tests</span> on E-vehicle Battery Cells and <span class="hlt">Packs</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sturk, David; Hoffmann, Lars; Ahlberg Tidblad, Annika</p> <p>2015-01-01</p> <p>The purpose of this study was to investigate the effects of abuse conditions, including realistic crash scenarios, on Li ion battery systems in E-vehicles in order to develop safe practices and priorities when responding to accidents involving E-vehicles. External fire <span class="hlt">tests</span> using a single burning item equipment were performed on commercial Li ion battery cells and battery <span class="hlt">packs</span> for electric vehicle (E-vehicle) application. The 2 most common battery cell technologies were <span class="hlt">tested</span>: Lithium iron phosphate (LFP) and mixed transition metal oxide (lithium nickel manganese cobalt oxide, NMC) cathodes against graphite anodes, respectively. The cell types investigated were "pouch" cells, with similar physical dimensions, but the NMC cells have double the electric capacity of the LFP cells due to the higher energy density of the NMC chemistry, 7 and 14 Ah, respectively. Heat release rate (HRR) data and concentrations of toxic gases were acquired by oxygen consumption calorimetry and Fourier transform infrared spectroscopy (FTIR), respectively. The <span class="hlt">test</span> results indicate that the state of charge (SOC) affects the HRR as well as the amount of toxic hydrogen fluoride (HF) gas formed during combustion. A larger number of cells increases the amount of HF formed per cell. There are significant differences in response to the fire exposure between the NMC and LFP cells in this study. The LFP cells generate a lot more HF per cell, but the overall reactivity of the NMC cells is higher. However, the total energy released by both batteries during combustion was independent of SOC, which indicates that the electric energy content of the <span class="hlt">test</span> object contributes to the activation energy of the thermal and heat release process, whereas the chemical energy stored in the materials is the main source of thermal energy in the batteries. The results imply that it is difficult to draw conclusions about higher order system behavior with respect to HF emissions based on data from <span class="hlt">tests</span> on single</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22935858','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22935858"><span>Comparing the efficacy of mature mud <span class="hlt">pack</span> and hot <span class="hlt">pack</span> treatments for knee osteoarthritis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sarsan, Ayşe; Akkaya, Nuray; Ozgen, Merih; Yildiz, Necmettin; Atalay, Nilgun Simsir; Ardic, Fusun</p> <p>2012-01-01</p> <p>The objective of this study is to compare the efficacy of mature mud <span class="hlt">pack</span> and hot <span class="hlt">pack</span> therapies on patients with knee osteoarthritis. This study was designed as a prospective, randomized-controlled, and single-blinded clinical trial. Twenty-seven patients with clinical and radiologic evidence of knee osteoarthritis were randomly assigned into two groups and were treated with mature mud <span class="hlt">packs</span> (n 15) or hot <span class="hlt">packs</span> (n=12). Patients were evaluated for pain [based on the visual analog scale (VAS)], function (WOMAC, 6 min walking distance), quality of life [Short Form-36 (SF-36)], and serum levels of tumor necrosis factor-alpha (TNF-α), interleukin-6 (IL-6), and insulin-like growth factor-1 (IGF-1) at baseline, post-treatment, and 3 and 6~months after treatment. The mud <span class="hlt">pack</span> group shows a significant improvement in VAS, pain, stifness, and physical function domains of WOMAC. The difference between groups of pain and physical activity domains is significant at post-treatment in favor of mud <span class="hlt">pack</span>. For a 6 min walking distance, mud <span class="hlt">pack</span> shows significant improvement, and the difference is significant between groups in favor of mud <span class="hlt">pack</span> at post-treatment and 3 and 6 months after treatment. Mud <span class="hlt">pack</span> shows significant improvement in the pain subscale of SF-36 at the third month continuing until the sixth month after the treatment. Significant improvements are found for the social function, vitality/energy, physical role disability, and general health subscales of SF-36 in favor of the mud <span class="hlt">pack</span> compared with the hot <span class="hlt">pack</span> group at post-treatment. A significant increase is detected for IGF-1 in the mud <span class="hlt">pack</span> group 3 months after treatment compared with the baseline, and the difference is significant between groups 3 months after the treatment. Mud <span class="hlt">pack</span> is a favorable option compared with hotpack for pain relief and for the improvement of functional conditions in treating patients with knee osteoarthritis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890013198','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890013198"><span>NASA's program on <span class="hlt">icing</span> research and technology</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reinmann, John J.; Shaw, Robert J.; Ranaudo, Richard J.</p> <p>1989-01-01</p> <p>NASA's program in aircraft <span class="hlt">icing</span> research and technology is reviewed. The program relies heavily on computer codes and modern applied physics technology in seeking <span class="hlt">icing</span> solutions on a finer scale than those offered in earlier programs. Three major goals of this program are to offer new approaches to <span class="hlt">ice</span> protection, to improve our ability to model the response of an aircraft to an <span class="hlt">icing</span> encounter, and to provide improved techniques and facilities for ground and flight <span class="hlt">testing</span>. This paper reviews the following program elements: (1) new approaches to <span class="hlt">ice</span> protection; (2) numerical codes for deicer analysis; (3) measurement and prediction of <span class="hlt">ice</span> accretion and its effect on aircraft and aircraft components; (4) special wind tunnel <span class="hlt">test</span> techniques for rotorcraft <span class="hlt">icing</span>; (5) improvements of <span class="hlt">icing</span> wind tunnels and research aircraft; (6) ground de-<span class="hlt">icing</span> fluids used in winter operation; (7) fundamental studies in <span class="hlt">icing</span>; and (8) droplet sizing instruments for <span class="hlt">icing</span> clouds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM31C..05B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM31C..05B"><span>Simulating Extraterrestrial <span class="hlt">Ices</span> in the Laboratory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berisford, D. F.; Carey, E. M.; Hand, K. P.; Choukroun, M.</p> <p>2017-12-01</p> <p>Several ongoing experiments at JPL attempt to simulate the <span class="hlt">ice</span> environment for various regimes associated with icy moons. The Europa Penitent <span class="hlt">Ice</span> Experiment (EPIX) simulates the surface environment of an icy moon, to investigate the physics of <span class="hlt">ice</span> surface morphology growth. This experiment features half-meter-scale cryogenic <span class="hlt">ice</span> samples, cryogenic radiative sink environment, vacuum conditions, and diurnal cycling solar simulation. The experiment also includes several smaller fixed-geometry vacuum chambers for <span class="hlt">ice</span> simulation at Earth-like and intermediate temperature and vacuum conditions for development of surface morphology growth scaling relations. Additionally, an <span class="hlt">ice</span> cutting facility built on a similar platform provides qualitative data on the mechanical behavior of cryogenic <span class="hlt">ice</span> with impurities under vacuum, and allows <span class="hlt">testing</span> of <span class="hlt">ice</span> cutting/sampling tools relevant for landing spacecraft. A larger cutting facility is under construction at JPL, which will provide more quantitative data and allow full-scale sampling tool <span class="hlt">tests</span>. Another facility, the JPL <span class="hlt">Ice</span> Physics Laboratory, features icy analog simulant preparation abilities that range icy solar system objects such as Mars, Ceres and the icy satellites of Saturn and Jupiter. In addition, the <span class="hlt">Ice</span> Physics Lab has unique facilities for Icy Analog Tidal Simulation and Rheological Studies of Cryogenic Icy Slurries, as well as equipment to perform thermal and mechanical properties <span class="hlt">testing</span> on icy analog materials and their response to sinusoidal tidal stresses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARH51007W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARH51007W"><span>Non-equilibrium Statistical Mechanics and the Sea <span class="hlt">Ice</span> Thickness Distribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wettlaufer, John; Toppaladoddi, Srikanth</p> <p></p> <p>We use concepts from non-equilibrium statistical physics to transform the original evolution equation for the sea <span class="hlt">ice</span> thickness distribution g (h) due to Thorndike et al., (1975) into a Fokker-Planck like conservation law. The steady solution is g (h) = calN (q) hqe - h / H , where q and H are expressible in terms of moments over the transition probabilities between thickness categories. The solution exhibits the functional form used in observational fits and shows that for h << 1 , g (h) is controlled by both thermodynamics and mechanics, whereas for h >> 1 only mechanics controls g (h) . Finally, we derive the underlying Langevin equation governing the dynamics of the <span class="hlt">ice</span> thickness h, from which we predict the observed g (h) . This allows us to demonstrate that the <span class="hlt">ice</span> thickness field is ergodic. The genericity of our approach provides a framework for studying the geophysical scale structure of the <span class="hlt">ice</span> <span class="hlt">pack</span> using methods of broad relevance in statistical mechanics. Swedish Research Council Grant No. 638-2013-9243, NASA Grant NNH13ZDA001N-CRYO and the National Science Foundation and the Office of Naval Research under OCE-1332750 for support.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28607400','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28607400"><span>Arctic sea <span class="hlt">ice</span> melt leads to atmospheric new particle formation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dall Osto, M; Beddows, D C S; Tunved, P; Krejci, R; Ström, J; Hansson, H-C; Yoon, Y J; Park, Ki-Tae; Becagli, S; Udisti, R; Onasch, T; O Dowd, C D; Simó, R; Harrison, Roy M</p> <p>2017-06-12</p> <p>Atmospheric new particle formation (NPF) and growth significantly influences climate by supplying new seeds for cloud condensation and brightness. Currently, there is a lack of understanding of whether and how marine biota emissions affect aerosol-cloud-climate interactions in the Arctic. Here, the aerosol population was categorised via cluster analysis of aerosol size distributions taken at Mt Zeppelin (Svalbard) during a 11 year record. The daily temporal occurrence of NPF events likely caused by nucleation in the polar marine boundary layer was quantified annually as 18%, with a peak of 51% during summer months. Air mass trajectory analysis and atmospheric nitrogen and sulphur tracers link these frequent nucleation events to biogenic precursors released by open water and melting sea <span class="hlt">ice</span> regions. The occurrence of such events across a full decade was anti-correlated with sea <span class="hlt">ice</span> extent. New particles originating from open water and open <span class="hlt">pack</span> <span class="hlt">ice</span> increased the cloud condensation nuclei concentration background by at least ca. 20%, supporting a marine biosphere-climate link through sea <span class="hlt">ice</span> melt and low altitude clouds that may have contributed to accelerate Arctic warming. Our results prompt a better representation of biogenic aerosol sources in Arctic climate models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050232832','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050232832"><span>Experimental Investigation of <span class="hlt">Ice</span> Accretion Effects on a Swept Wing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wong, S. C.; Vargas, M.; Papadakis, M.; Yeong, H. W.; Potapczuk, M.</p> <p>2005-01-01</p> <p>An experimental investigation was conducted to study the effects of 2-, 5-, 10-, and 22.5-min <span class="hlt">ice</span> accretions on the aerodynamic performance of a swept finite wing. The <span class="hlt">ice</span> shapes <span class="hlt">tested</span> included castings of <span class="hlt">ice</span> accretions obtained from <span class="hlt">icing</span> <span class="hlt">tests</span> at the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (IRT) and simulated <span class="hlt">ice</span> shapes obtained with the LEWICE 2.0 <span class="hlt">ice</span> accretion code. The conditions used for the <span class="hlt">icing</span> <span class="hlt">tests</span> were selected to provide five glaze <span class="hlt">ice</span> shapes with complete and incomplete scallop features and a small rime <span class="hlt">ice</span> shape. The LEWICE <span class="hlt">ice</span> shapes were defined for the same conditions as those used in the <span class="hlt">icing</span> <span class="hlt">tests</span>. All aerodynamic performance <span class="hlt">tests</span> were conducted in the 7- x 10-ft Low-Speed Wind Tunnel Facility at Wichita State University. Six component force and moment measurements, aileron hinge moments, and surface pressures were obtained for a Reynolds number of 1.8 million based on mean aerodynamic chord and aileron deflections in the range of -15o to 20o. <span class="hlt">Tests</span> were performed with the clean wing, six IRT <span class="hlt">ice</span> shape castings, seven smooth LEWICE <span class="hlt">ice</span> shapes, and seven rough LEWICE <span class="hlt">ice</span> shapes. Roughness for the LEWICE <span class="hlt">ice</span> shapes was simulated with 36-size grit. The experiments conducted showed that the glaze <span class="hlt">ice</span> castings reduced the maximum lift coefficient of the clean wing by 11.5% to 93.6%, while the 5-min rime <span class="hlt">ice</span> casting increased maximum lift by 3.4%. Minimum <span class="hlt">iced</span> wing drag was 133% to 3533% greater with respect to the clean case. The drag of the <span class="hlt">iced</span> wing near the clean wing stall angle of attack was 17% to 104% higher than that of the clean case. In general, the aileron remained effective in changing the lift of the clean and <span class="hlt">iced</span> wings for all angles of attack and aileron deflections <span class="hlt">tested</span>. Aileron hinge moments for the <span class="hlt">iced</span> wing cases remained within the maximum and minimum limits defined by the clean wing hinge moments. <span class="hlt">Tests</span> conducted with the LEWICE <span class="hlt">ice</span> shapes showed that in general the trends in aerodynamic performance degradation of the wing with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007302','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007302"><span>An Initial Study of the Fundamentals of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter; Bartkus, Tadas; Tsao, Jen-Ching; Bencic, Timothy; King, Michael; Ratvasky, Thomas; Van Zante, Judith</p> <p>2017-01-01</p> <p>This presentation shows results from an initial study of the fundamental physics of <span class="hlt">ice</span>-crystal <span class="hlt">ice</span> accretion using the NASA Propulsion Systems Lab (PSL). <span class="hlt">Ice</span> accretion due to the ingestion of <span class="hlt">ice</span>-crystals is being attributed to numerous jet-engine power-loss events. The NASA PSL is an altitude jet-engine <span class="hlt">test</span> facility which has recently added a capability to inject <span class="hlt">ice</span> particles into the flow. NASA is evaluating whether this facility, in addition to full-engine and motor-driven-rig <span class="hlt">tests</span>, can be used for more fundamental <span class="hlt">ice</span>-accretion studies that simulate the different mixed-phase <span class="hlt">icing</span> conditions along the core flow passage of a turbo-fan engine compressor. The data from such fundamental accretion <span class="hlt">tests</span> will be used to help develop and validate models of the accretion process. The present study utilized a NACA0012 airfoil. The mixed-phase conditions were generated by partially freezing the liquid-water droplets ejected from the spray bars. This presentation shows data regarding (1) the freeze out characteristics of the cloud, (2) changes in aerothermal conditions due to the presence of the cloud, and (3) the <span class="hlt">ice</span> accretion characteristics observed on the airfoil model. The primary variable in this <span class="hlt">test</span> was the PSL plenum humidity which was systematically varied for two duct-exit-plane velocities (85 and 135 ms) as well as two particle size clouds (15 and 50 m MVDi). The observed clouds ranged from fully glaciated to fully liquid, where the liquid clouds were at least partially supercooled. The air total temperature decreased at the <span class="hlt">test</span> section when the cloud was activated due to evaporation. The <span class="hlt">ice</span> accretions observed ranged from sharp arrow-like accretions, characteristic of <span class="hlt">ice</span>-crystal erosion, to cases with double-horn shapes, characteristic of supercooled water accretions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007924','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007924"><span>An Initial Study of the Fundamentals of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter M.; Ratvasky, Thomas P.; Bencic, Timothy J.; Van Zante, Judith F.; King, Michael C.; Tsao, Jen-Ching; Bartkus, Tadas P.</p> <p>2017-01-01</p> <p>This paper presents results from an initial study of the fundamental physics of <span class="hlt">ice</span>-crystal <span class="hlt">ice</span> accretion using the NASA Propulsion Systems Lab (PSL). <span class="hlt">Ice</span> accretion due to the ingestion of <span class="hlt">ice</span>-crystals is being attributed to numerous jet-engine power-loss events. The NASA PSL is an altitude jet-engine <span class="hlt">test</span> facility which has recently added a capability to inject <span class="hlt">ice</span> particles into the flow. NASA is evaluating whether this facility, in addition to full-engine and motor-driven-rig <span class="hlt">tests</span>, can be used for more fundamental <span class="hlt">ice</span>-accretion studies that simulate the different mixed-phase <span class="hlt">icing</span> conditions along the core flow passage of a turbo-fan engine compressor. The data from such fundamental accretion <span class="hlt">tests</span> will be used to help develop and validate models of the accretion process. The present study utilized a NACA0012 airfoil. The mixed-phase conditions were generated by partially freezing the liquid-water droplets ejected from the spray bars. This paper presents data regarding (1) the freeze out characteristics of the cloud, (2) changes in aerothermal conditions due to the presence of the cloud, and (3) the <span class="hlt">ice</span> accretion characteristics observed on the airfoil model. The primary variable in this <span class="hlt">test</span> was the PSL plenum humidity which was systematically varied for two duct-exit-plane velocities (85 and 135 ms) as well as two particle size clouds (15 and 50 m MVDi). The observed clouds ranged from fully glaciated to fully liquid, where the liquid clouds were at least partially supercooled. The air total temperature decreased at the <span class="hlt">test</span> section when the cloud was activated due to evaporation. The <span class="hlt">ice</span> accretions observed ranged from sharp arrow-like accretions, characteristic of <span class="hlt">ice</span>-crystal erosion, to cases with double-horn shapes, characteristic of supercooled water accretions.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/121524-application-booth-kautzmann-method-determination-packing-leakage','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/121524-application-booth-kautzmann-method-determination-packing-leakage"><span>Application of the Booth-Kautzmann method for the determination of N-2 <span class="hlt">packing</span> leakage</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Burkhart, D.M.; Milton, J.W.; Fawcett, S.T.</p> <p>1995-06-01</p> <p>To accurately determine turbine cycle heat rate, leakage past the N-2 steam seal <span class="hlt">packing</span> must be determined on turbines with both HP and IP turbines contained within a common high pressure casing. N-2 <span class="hlt">packing</span> leakage can be determined by the Booth-Kautzmann Method with instrumentation commonly used to determine the HP and IP turbine efficiency. The only additional requirements are changes to the main steam and/or hot reheat steam conditions. This paper discusses the actual <span class="hlt">test</span> results using the Booth-Kautzmann <span class="hlt">test</span> procedure on three natural gas fired units. The <span class="hlt">test</span> results demonstrate the added advantage of having at least three N-2more » <span class="hlt">test</span> runs, stability requirements for repeatable <span class="hlt">test</span> runs and <span class="hlt">test</span> procedures used to determine leakage results. Discussion of the sensitivity of the assumed N-2 enthalpy are also addressed. Utilizing Martins Formula with a series of N-2 Leakage <span class="hlt">test</span> runs is shown to be a leakage prediction tool and a <span class="hlt">packing</span> clearance approximation tool. It is concluded that the Booth-Kautzmann Method for determination of N-2 <span class="hlt">packing</span> leakage should be utilized whenever HP and Ip turbine efficiency is determined. The two or three additional hours invested in the <span class="hlt">test</span> runs is well worth the information gained on the performance of the N-2 <span class="hlt">packing</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMOS14A..04Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMOS14A..04Z"><span>Local Effects of <span class="hlt">Ice</span> Floes on Skin Sea Surface Temperature in the Marginal <span class="hlt">Ice</span> Zone from UAVs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zappa, C. J.; Brown, S.; Emery, W. J.; Adler, J.; Wick, G. A.; Steele, M.; Palo, S. E.; Walker, G.; Maslanik, J. A.</p> <p>2013-12-01</p> <p> downstream the skin SST is mixed within the turbulent wake over 10s of meters. We compare the structure of circulation and mixing of the influx of cold skin SST driven by surface currents and wind. In-situ temperature measurements provide the context for the vertical structure of the mixing and its impact on the skin SST. Furthermore, comparisons to satellite-derived sea surface temperature of the region are presented. The accuracy of satellite derived SST products and how well the observed skin SSTs represent ocean bulk temperatures in polar regions is not well understood, due in part to lack of observations. Estimated error in the polar seas is relatively high at up to 0.4 deg. C compared to less than 0.2 deg. C for other areas. The goal of these and future analyses of the MIZOPEX data set is to elucidate a basic question that is significant for the entire Earth system. Have these regions passed a tipping point, such that they are now essentially acting as sub-Arctic seas where <span class="hlt">ice</span> disappears in summer, or instead whether the changes are transient, with the potential for the <span class="hlt">ice</span> <span class="hlt">pack</span> to recover?</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2575336','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2575336"><span>Southern Ocean frontal structure and sea-<span class="hlt">ice</span> formation rates revealed by elephant seals</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Charrassin, J.-B.; Hindell, M.; Rintoul, S. R.; Roquet, F.; Sokolov, S.; Biuw, M.; Costa, D.; Boehme, L.; Lovell, P.; Coleman, R.; Timmermann, R.; Meijers, A.; Meredith, M.; Park, Y.-H.; Bailleul, F.; Goebel, M.; Tremblay, Y.; Bost, C.-A.; McMahon, C. R.; Field, I. C.; Fedak, M. A.; Guinet, C.</p> <p>2008-01-01</p> <p>Polar regions are particularly sensitive to climate change, with the potential for significant feedbacks between ocean circulation, sea <span class="hlt">ice</span>, and the ocean carbon cycle. However, the difficulty in obtaining in situ data means that our ability to detect and interpret change is very limited, especially in the Southern Ocean, where the ocean beneath the sea <span class="hlt">ice</span> remains almost entirely unobserved and the rate of sea-<span class="hlt">ice</span> formation is poorly known. Here, we show that southern elephant seals (Mirounga leonina) equipped with oceanographic sensors can measure ocean structure and water mass changes in regions and seasons rarely observed with traditional oceanographic platforms. In particular, seals provided a 30-fold increase in hydrographic profiles from the sea-<span class="hlt">ice</span> zone, allowing the major fronts to be mapped south of 60°S and sea-<span class="hlt">ice</span> formation rates to be inferred from changes in upper ocean salinity. Sea-<span class="hlt">ice</span> production rates peaked in early winter (April–May) during the rapid northward expansion of the <span class="hlt">pack</span> <span class="hlt">ice</span> and declined by a factor of 2 to 3 between May and August, in agreement with a three-dimensional coupled ocean–sea-<span class="hlt">ice</span> model. By measuring the high-latitude ocean during winter, elephant seals fill a “blind spot” in our sampling coverage, enabling the establishment of a truly global ocean-observing system. PMID:18695241</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ISPAr42.3.2419Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ISPAr42.3.2419Z"><span>Sea <span class="hlt">Ice</span> Drift Monitoring in the Bohai Sea Based on GF4 Satellite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Y.; Wei, P.; Zhu, H.; Xing, B.</p> <p>2018-04-01</p> <p>The Bohai Sea is the inland sea with the highest latitude in China. In winter, the phenomenon of freezing occurs in the Bohai Sea due to frequent cold wave influx. According to historical records, there have been three serious <span class="hlt">ice</span> <span class="hlt">packs</span> in the Bohai Sea in the past 50 years which caused heavy losses to our economy. Therefore, it is of great significance to monitor the drift of sea <span class="hlt">ice</span> and sea <span class="hlt">ice</span> in the Bohai Sea. The GF4 image has the advantages of short imaging time and high spatial resolution. Based on the GF4 satellite images, the three methods of SIFT (Scale invariant feature - the transform and Scale invariant feature transform), MCC (maximum cross-correlation method) and sift combined with MCC are used to monitor sea <span class="hlt">ice</span> drift and calculate the speed and direction of sea <span class="hlt">ice</span> drift, the three calculation results are compared and analyzed by using expert interpretation and historical statistical data to carry out remote sensing monitoring of sea <span class="hlt">ice</span> drift results. The experimental results show that the experimental results of the three methods are in accordance with expert interpretation and historical statistics. Therefore, the GF4 remote sensing satellite images have the ability to monitor sea <span class="hlt">ice</span> drift and can be used for drift monitoring of sea <span class="hlt">ice</span> in the Bohai Sea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20072039','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20072039"><span>The development and reliability of a repeated anaerobic cycling <span class="hlt">test</span> in female <span class="hlt">ice</span> hockey players.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wilson, Kier; Snydmiller, Gary; Game, Alex; Quinney, Art; Bell, Gordon</p> <p>2010-02-01</p> <p>The purpose of this study was to develop and assess the reliability of a repeated anaerobic power cycling <span class="hlt">test</span> designed to mimic the repeated sprinting nature of the sport of <span class="hlt">ice</span> hockey. Nineteen female varsity <span class="hlt">ice</span> hockey players (mean X +/- SD age, height and body mass = 21 +/- 2 yr, 166.6 +/- 6.3 cm and 62.3 +/- 7.3) completed 3 trials of a repeated anaerobic power <span class="hlt">test</span> on a Monark cycle ergometer on different days. The <span class="hlt">test</span> consisted of "all-out" cycling for 5 seconds separated by 10 seconds of low-intensity cycling, repeated 4 times. The relative load factor used for the resistance setting was equal to 0.095 kg per kilogram body mass. There was no significant difference between the peak 5-second power output (PO), mean PO, or the fatigue index (%) among the 3 different trials. The peak 5-second PO was 702.6 +/- 114.8 w and 11.3 +/- 1.1 w x kg, whereas the mean PO across the 4 repeats was 647.1 +/- 96.3 w and 10.4 +/- 1.0 w x kg averaged for the 3 different <span class="hlt">tests</span>. The fatigue index averaged 17.8 +/- 6.5%. The intraclass correlation coefficient for peak 5-second, mean PO, and fatigue index was 0.82, 0.86, and 0.82, respectively. This study reports the methodology of a repeated anaerobic power cycling <span class="hlt">test</span> that was reliable for the measurement of PO and calculated fatigue index in varsity women <span class="hlt">ice</span> hockey players and can be used as a laboratory-based assessment of repeated anaerobic fitness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AnGla..44..253U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AnGla..44..253U"><span>Ship-borne electromagnetic induction sounding of sea-<span class="hlt">ice</span> thickness in the southern Sea of Okhotsk</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uto, Shotaro; Toyota, Takenobu; Shimoda, Haruhito; Tateyama, Kazutaka; Shirasawa, Kunio</p> <p></p> <p>Recent observations have revealed that dynamical thickening is dominant in the growth process of sea <span class="hlt">ice</span> in the southern Sea of Okhotsk. That indicates the importance of understanding the nature of thick deformed <span class="hlt">ice</span> in this area. The objective of the present paper is to establish a ship-based method for observing the thickness of deformed <span class="hlt">ice</span> with reasonable accuracy. Since February 2003, one of the authors has engaged in the core sampling using a small basket from the icebreaker Soya. Based on these results, we developed a new model which expressed the internal structure of <span class="hlt">pack</span> <span class="hlt">ice</span> in the southern Sea of Okhotsk, as a one-dimensional multilayered structure. Since 2004, the electromagnetic (EM) inductive sounding of sea-<span class="hlt">ice</span> thickness has been conducted on board Soya. By combining the model and theoretical calculations, a new algorithm was developed for transforming the output of the EM inductive instrument to <span class="hlt">ice</span> + snow thickness (total thickness). Comparison with total thickness by drillhole observations showed fair agreement. The probability density functions of total thickness in 2004 and 2005 showed some difference, which reflected the difference of fractions of thick deformed <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980000580','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980000580"><span>Scaling Methods for Simulating Aircraft In-Flight <span class="hlt">Icing</span> Encounters</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anderson, David N.; Ruff, Gary A.</p> <p>1997-01-01</p> <p>This paper discusses scaling methods which permit the use of subscale models in <span class="hlt">icing</span> wind tunnels to simulate natural flight in <span class="hlt">icing</span>. Natural <span class="hlt">icing</span> conditions exist when air temperatures are below freezing but cloud water droplets are super-cooled liquid. Aircraft flying through such clouds are susceptible to the accretion of <span class="hlt">ice</span> on the leading edges of unprotected components such as wings, tailplane and engine inlets. To establish the aerodynamic penalties of such <span class="hlt">ice</span> accretion and to determine what parts need to be protected from <span class="hlt">ice</span> accretion (by heating, for example), extensive flight and wind-tunnel <span class="hlt">testing</span> is necessary for new aircraft and components. <span class="hlt">Testing</span> in <span class="hlt">icing</span> tunnels is less expensive than flight <span class="hlt">testing</span>, is safer, and permits better control of the <span class="hlt">test</span> conditions. However, because of limitations on both model size and operating conditions in wind tunnels, it is often necessary to perform <span class="hlt">tests</span> with either size or <span class="hlt">test</span> conditions scaled. This paper describes the theoretical background to the development of <span class="hlt">icing</span> scaling methods, discusses four methods, and presents results of <span class="hlt">tests</span> to validate them.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170007301','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170007301"><span>Evaluation of Alternative Altitude Scaling Methods for Thermal <span class="hlt">Ice</span> Protection System in NASA <span class="hlt">Icing</span> Research Tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Sam; Addy, Harold; Broeren, Andy P.; Orchard, David M.</p> <p>2017-01-01</p> <p>A <span class="hlt">test</span> was conducted at NASA <span class="hlt">Icing</span> Research Tunnel to evaluate altitude scaling methods for thermal <span class="hlt">ice</span> protection system. Two scaling methods based on Weber number were compared against a method based on the Reynolds number. The results generally agreed with the previous set of <span class="hlt">tests</span> conducted in NRCC Altitude <span class="hlt">Icing</span> Wind Tunnel. The Weber number based scaling methods resulted in smaller runback <span class="hlt">ice</span> mass than the Reynolds number based scaling method. The <span class="hlt">ice</span> accretions from the Weber number based scaling method also formed farther upstream. However there were large differences in the accreted <span class="hlt">ice</span> mass between the two Weber number based scaling methods. The difference became greater when the speed was increased. This indicated that there may be some Reynolds number effects that isnt fully accounted for and warrants further study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850005139','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850005139"><span>Dynamics of coupled <span class="hlt">ice</span>-ocean system in the marginal <span class="hlt">ice</span> zone: Study of the mesoscale processes and of constitutive equations for sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hakkinen, S.</p> <p>1984-01-01</p> <p>This study is aimed at the modelling of mesoscale processed such as up/downwelling and <span class="hlt">ice</span> edge eddies in the marginal <span class="hlt">ice</span> zones. A 2-dimensional coupled <span class="hlt">ice</span>-ocean model is used for the study. The <span class="hlt">ice</span> model is coupled to the reduced gravity ocean model (f-plane) through interfacial stresses. The constitutive equations of the sea <span class="hlt">ice</span> are formulated on the basis of the Reiner-Rivlin theory. The internal <span class="hlt">ice</span> stresses are important only at high <span class="hlt">ice</span> concentrations (90-100%), otherwise the <span class="hlt">ice</span> motion is essentially free drift, where the air-<span class="hlt">ice</span> stress is balanced by the <span class="hlt">ice</span>-water stress. The model was <span class="hlt">tested</span> by studying the upwelling dynamics. Winds parallel to the <span class="hlt">ice</span> edge with the <span class="hlt">ice</span> on the right produce upwilling because the air-<span class="hlt">ice</span> momentum flux is much greater that air-ocean momentum flux, and thus the Ekman transport is bigger under the <span class="hlt">ice</span> than in the open water. The upwelling simulation was extended to include temporally varying forcing, which was chosen to vary sinusoidally with a 4 day period. This forcing resembles successive cyclone passings. In the model with a thin oceanic upper layer, <span class="hlt">ice</span> bands were formed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990026767&hterms=vertigo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dvertigo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990026767&hterms=vertigo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dvertigo"><span><span class="hlt">Ice</span> as a Construction Material</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zuppero, Anthony; Lewis, J.</p> <p>1998-01-01</p> <p>This presentation shows how water and <span class="hlt">ice</span> can enable exceptionally simple ways to construct structures in deep space. Practicality is underscored by applying advanced tank methods being developed for Mars missions. Water or <span class="hlt">ice</span> is now known to be present or abundant on most objects in the solar system, starting with the planet Mercury. Thermal processes alone can be used to melt <span class="hlt">ice</span> . The cold of space can refreeze water back into <span class="hlt">ice</span>. The anomalous low vapor pressure of water, about 7 mm Hg, permits bladder containers. Tanks or bladders made with modern polymer fiber and film can exhibit very small (<0.1 %) equivalent tankage and ullage fractions and thus hold thousands of tons of water per ton bladder. Injecting water into a bladder whose shape when inflated is the desired final shape, such as a space vehicle, provides a convenient way to construct large structures. In space, structures of 1O,OOO-T mass become feasible because the bladder mass is low enough to be launched. The bladder can weigh 1OOO times less than its contents, or 10 T. The bladder would be <span class="hlt">packed</span> like a parachute. Shaped memory materials and/or gas inflation could reestablish the desired structure shape after unpacking. The water comes from space resources. An example examines construction of torus space vehicle with 100-m nominal dimension. People would live inside the torus. A torus, like a tire on an automobile, would spin and provide synthetic gravity at its inner surface. A torus of order 100 m across would provide a gravity with gradients low enough to mitigate against vertigo.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987RaPC...29..325N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987RaPC...29..325N"><span>Preliminary investigations on a new method of retaining the colour of shucked cockles ( Anadara Granosa), and the extension of shelflife by gamma irradiation and vacuum <span class="hlt">packing</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ng, Cher Siang; Low, Lai Kim; Chia, Lawrence H. L.</p> <p></p> <p>Live cockles were incubated in atmospheres containing different concentrations of carbon monoxide. Since CO combines more readily with myoglobin and haemoglobin than oxygen, the formation of in vivo deoxygenated haemoglobins and post mortem formation of methaemoglobin were retarded by the more stable carboxyhaemoglobin (HbCO). The bright red colour of the stable HbCO is retained during storage, giving the desired colour to the cockles. The colour of normal, chilled cockle meat deteriorated after 3 days <span class="hlt">ice</span> storage while those treated with 50 and 100% CO retained the bright deep orange colour up to 10 days storage. Irradiation caused faster colour deterioration in both CO and non-CO treated samples. Vacuum <span class="hlt">packing</span> influenced the colour of the cockles with irradiation and with CO treatments. In non-CO treated, irradiated samples, the effect of vacuum <span class="hlt">packing</span> was not obvious. In CO treated, irradiated samples, vacuum <span class="hlt">packing</span> retarded the deterioration of colour. Odour developments were influenced by irradiation, vacuum <span class="hlt">packing</span> and storage temperature, and were not influenced by CO treatments. Irradiation suppressed the development of odour for the first 11 days storage (0°C) while vacuum <span class="hlt">packing</span> depressed the odour by lowering its intensity instead. Odour development was slowed down by lowering the storage temperature. The odour of shucked cockles was rejected within one day at room temperature (26-28°C) while at 0°C the odour of the shucked cockles was still acceptable after 10 days. Suitable chemical indices for quality are K value and TVBN. Treatment with CO did not influence the K value development. Vacuum <span class="hlt">packing</span> produced the highest K values after 19 days storage (0°C), while irradiated samples had higher K values than non-irradiated samples. The TVBN increased with storage and is an indicator of the odour development. The use of CO treatment extended the shelflife of the cockles based on appearance. A combination of CO treatment, vacuum <span class="hlt">packing</span>, <span class="hlt">ice</span> storage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.3278P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.3278P"><span><span class="hlt">Testing</span> the reliability of <span class="hlt">ice</span>-cream cone model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pan, Zonghao; Shen, Chenglong; Wang, Chuanbing; Liu, Kai; Xue, Xianghui; Wang, Yuming; Wang, Shui</p> <p>2015-04-01</p> <p>Coronal Mass Ejections (CME)'s properties are important to not only the physical scene itself but space-weather prediction. Several models (such as cone model, GCS model, and so on) have been raised to get rid of the projection effects within the properties observed by spacecraft. According to SOHO/ LASCO observations, we obtain the 'real' 3D parameters of all the FFHCMEs (front-side full halo Coronal Mass Ejections) within the 24th solar cycle till July 2012, by the <span class="hlt">ice</span>-cream cone model. Considering that the method to obtain 3D parameters from the CME observations by multi-satellite and multi-angle has higher accuracy, we use the GCS model to obtain the real propagation parameters of these CMEs in 3D space and compare the results with which by <span class="hlt">ice</span>-cream cone model. Then we could discuss the reliability of the <span class="hlt">ice</span>-cream cone model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JGRC..115.2005V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JGRC..115.2005V"><span>Modeling brine and nutrient dynamics in Antarctic sea <span class="hlt">ice</span>: The case of dissolved silica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vancoppenolle, Martin; Goosse, Hugues; de Montety, Anne; Fichefet, Thierry; Tremblay, Bruno; Tison, Jean-Louis</p> <p>2010-02-01</p> <p>Sea <span class="hlt">ice</span> ecosystems are characterized by microalgae living in brine inclusions. The growth rate of <span class="hlt">ice</span> algae depends on light and nutrient supply. Here, the interactions between nutrients and brine dynamics under the influence of algae are investigated using a one-dimensional model. The model includes snow and <span class="hlt">ice</span> thermodynamics with brine physics and an idealized sea <span class="hlt">ice</span> biological component, characterized by one nutrient, namely, dissolved silica (DSi). In the model, DSi follows brine motion and is consumed by <span class="hlt">ice</span> algae. Depending on physical <span class="hlt">ice</span> characteristics, the brine flow is either advective, diffusive, or turbulent. The vertical profiles of <span class="hlt">ice</span> salinity and DSi concentration are solutions of advection-diffusion equations. The model is configured to simulate the typical thermodynamic regimes of first-year Antarctic <span class="hlt">pack</span> <span class="hlt">ice</span>. The simulated vertical profiles of salinity and DSi qualitatively reproduce observations. Analysis of results highlights the role of convection in the lowermost 5-10 cm of <span class="hlt">ice</span>. Convection mixes saline, nutrient-poor brine with comparatively fresh, nutrient-rich seawater. This implies a rejection of salt to the ocean and a flux of DSi to the <span class="hlt">ice</span>. In the presence of growing algae, the simulated ocean-to-<span class="hlt">ice</span> DSi flux increases by 0-115% compared to an abiotic situation. In turn, primary production and brine convection act in synergy to form a nutrient pump. The other important processes are the flooding of the surface by seawater and the percolation of meltwater. The former refills nutrients near the <span class="hlt">ice</span> surface in spring. The latter, if present, tends to expell nutrients from the <span class="hlt">ice</span> in summer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29324580','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29324580"><span>Relationship Between Skating Economy and Performance During a Repeated-Shift <span class="hlt">Test</span> in Elite and Subelite <span class="hlt">Ice</span> Hockey Players.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lamoureux, Nicholas R; Tomkinson, Grant R; Peterson, Benjamin J; Fitzgerald, John S</p> <p>2018-04-01</p> <p>Lamoureux, NR, Tomkinson, GR, Peterson, BJ, and Fitzgerald, JS. Relationship between skating economy and performance during a repeated-shift <span class="hlt">test</span> in elite and subelite <span class="hlt">ice</span> hockey players. J Strength Cond Res 32(4): 1109-1113, 2018-The purpose of this study was to determine the importance of skating economy to fatigue during repeated high-intensity efforts of a simulated <span class="hlt">ice</span> hockey shift. Forty-five collegiate and Junior A male <span class="hlt">ice</span> hockey players (aged 18-24 years) performed a continuous graded exercise <span class="hlt">test</span> using a skate treadmill. Breath-by-breath data for oxygen consumption (V[Combining Dot Above]O2) and respiratory exchange ratio were collected and used to derive energy expenditure (EE) averaged over the final 10 seconds of each stage. Economy was determined as the slope of the regression line relating V[Combining Dot Above]O2 and EE against skating speed separately. Participants also completed 8 bouts of maximal <span class="hlt">ice</span> skating through a course designed to simulate typical shift, with timing gates determining first half, second half, and total fatigue decrement, calculated by a percent decrement score. Partial correlation was used to determine the association between economy measures and decrement during the repeated-shift <span class="hlt">test</span>. Twenty-six participants met inclusion criteria and were included in data analysis. Skating economy measures (both relative V[Combining Dot Above]O2 and EE) were very likely moderate positive correlates of total fatigue decrement (r [95% confidence interval]: V[Combining Dot Above]O2, 0.46 [0.09, 0.72] and EE, 0.44, [0.06, 0.71]) but not with first or second gate decrement. Our results indicate that skating economy plays an important role in fatigue resistance over repeated on-<span class="hlt">ice</span> sprints designed to simulate a typical shift. This supports the use of technical skating coaching and training techniques to enhance skating economy as a means of improving <span class="hlt">ice</span> hockey performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940007290&hterms=SSM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSSM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940007290&hterms=SSM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSSM"><span>Summer Arctic <span class="hlt">ice</span> concentrations and characteristics from SAR and SSM/I data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Comiso, Joey C.; Kwok, Ron</p> <p>1993-01-01</p> <p>The extent and concentration of the Summer minima provide indirect information about the long term ability of the perennial portion of the <span class="hlt">ice</span> <span class="hlt">pack</span> to survive the Arctic atmosphere and ocean system. Both active and passive microwave data were used with some success for monitoring the <span class="hlt">ice</span> cover during the Summer, but they both suffer from similar problems caused by the presence of meltponding, surface wetness, flooding, and freeze/thaw cycles associated with periodic changes in surface air temperatures. A comparative analysis of <span class="hlt">ice</span> conditions in the Arctic region using coregistered ERS-1 SAR (Synthetic Aperture Radar) and SSM/I (Special Sensor Microwave/Imager) data was made. The analysis benefits from complementary information from the two systems, the good spatial resolution of SAR data, and the good time resolution of and global coverage by SSM/I data. The results show that in many areas <span class="hlt">ice</span> concentrations derived from SAR data are significantly different (usually higher) than those derived from passive microwave data. Additional insights about surface conditions can be inferred depending on the nature of the discrepancies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4281296','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4281296"><span>cell<span class="hlt">PACK</span>: A Virtual Mesoscope to Model and Visualize Structural Systems Biology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Johnson, Graham T.; Autin, Ludovic; Al-Alusi, Mostafa; Goodsell, David S.; Sanner, Michel F.; Olson, Arthur J.</p> <p>2014-01-01</p> <p>cell<span class="hlt">PACK</span> assembles computational models of the biological mesoscale, an intermediate scale (10−7–10−8m) between molecular and cellular biology. cellPACK’s modular architecture unites existing and novel <span class="hlt">packing</span> algorithms to generate, visualize and analyze comprehensive 3D models of complex biological environments that integrate data from multiple experimental systems biology and structural biology sources. cell<span class="hlt">PACK</span> is currently available as open source code, with tools for validation of models and with recipes and models for five biological systems: blood plasma, cytoplasm, synaptic vesicles, HIV and a mycoplasma cell. We have applied cell<span class="hlt">PACK</span> to model distributions of HIV envelope protein to <span class="hlt">test</span> several hypotheses for consistency with experimental observations. Biologists, educators, and outreach specialists can interact with cell<span class="hlt">PACK</span> models, develop new recipes and perform <span class="hlt">packing</span> experiments through scripting and graphical user interfaces at http://cell<span class="hlt">PACK</span>.org. PMID:25437435</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33M..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33M..02W"><span>Upper-Tropospheric Cloud <span class="hlt">Ice</span> from <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, D. L.</p> <p>2017-12-01</p> <p>Cloud <span class="hlt">ice</span> plays important roles in Earth's energy budget and cloud-precipitation processes. Knowledge of global cloud <span class="hlt">ice</span> and its properties is critical for understanding and quantifying its roles in Earth's atmospheric system. It remains a great challenge to measure these variables accurately from space. Submillimeter (submm) wave remote sensing has capability of penetrating clouds and measuring <span class="hlt">ice</span> mass and microphysical properties. In particular, the 883-GHz frequency is a highest spectral window in microwave frequencies that can be used to fill a sensitivity gap between thermal infrared (IR) and mm-wave sensors in current spaceborne cloud <span class="hlt">ice</span> observations. <span class="hlt">Ice</span>Cube is a cubesat spaceflight demonstration of 883-GHz radiometer technology. Its primary objective is to raise the technology readiness level (TRL) of 883-GHz cloud radiometer for future Earth science missions. By flying a commercial receiver on a 3U cubesat, <span class="hlt">Ice</span>Cube is able to achieve fast-track maturation of space technology, by completing its development, integration and <span class="hlt">testing</span> in 2.5 years. <span class="hlt">Ice</span>Cube was successfully delivered to ISS in April 2017 and jettisoned from the International Space Station (ISS) in May 2017. The <span class="hlt">Ice</span>Cube cloud-<span class="hlt">ice</span> radiometer (ICIR) has been acquiring data since the jettison on a daytime-only operation. <span class="hlt">Ice</span>Cube adopted a simple design without payload mechanism. It makes maximum utilization of solar power by spinning the spacecraft continuously about the Sun vector at a rate of 1.2° per second. As a result, the ICIR is operated under the limited resources (8.6 W without heater) and largely-varying (18°C-28°C) thermal environments. The spinning cubesat also allows ICIR to have periodical views between the Earth (atmosphere and clouds) and cold space (calibration), from which the first 883-GHz cloud map is obtained. The 883-GHz cloud radiance, sensitive to <span class="hlt">ice</span> particle scattering, is proportional to cloud <span class="hlt">ice</span> amount above 10 km. The ICIR cloud map acquired during June 20-July 2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110020439','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110020439"><span>Preparing and Analyzing <span class="hlt">Iced</span> Airfoils</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vickerman, Mary B.; Baez, Marivell; Braun, Donald C.; Cotton, Barbara J.; Choo, Yung K.; Coroneos, Rula M.; Pennline, James A.; Hackenberg, Anthony W.; Schilling, Herbert W.; Slater, John W.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20110020439'); toggleEditAbsImage('author_20110020439_show'); toggleEditAbsImage('author_20110020439_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20110020439_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20110020439_hide"></p> <p>2004-01-01</p> <p>Smagg<span class="hlt">Ice</span> version 1.2 is a computer program for preparing and analyzing <span class="hlt">iced</span> airfoils. It includes interactive tools for (1) measuring <span class="hlt">ice</span>-shape characteristics, (2) controlled smoothing of <span class="hlt">ice</span> shapes, (3) curve discretization, (4) generation of artificial <span class="hlt">ice</span> shapes, and (5) detection and correction of input errors. Measurements of <span class="hlt">ice</span> shapes are essential for establishing relationships between characteristics of <span class="hlt">ice</span> and effects of <span class="hlt">ice</span> on airfoil performance. The shape-smoothing tool helps prepare <span class="hlt">ice</span> shapes for use with already available grid-generation and computational-fluid-dynamics software for studying the aerodynamic effects of smoothed <span class="hlt">ice</span> on airfoils. The artificial <span class="hlt">ice</span>-shape generation tool supports parametric studies since <span class="hlt">ice</span>-shape parameters can easily be controlled with the artificial <span class="hlt">ice</span>. In such studies, artificial shapes generated by this program can supplement simulated <span class="hlt">ice</span> obtained from <span class="hlt">icing</span> research tunnels and real <span class="hlt">ice</span> obtained from flight <span class="hlt">test</span> under <span class="hlt">icing</span> weather condition. Smagg<span class="hlt">Ice</span> also automatically detects geometry errors such as tangles or duplicate points in the boundary which may be introduced by digitization and provides tools to correct these. By use of interactive tools included in Smagg<span class="hlt">Ice</span> version 1.2, one can easily characterize <span class="hlt">ice</span> shapes and prepare <span class="hlt">iced</span> airfoils for grid generation and flow simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA474414','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA474414"><span>CJ2 <span class="hlt">Icing</span> Effects Simulator. Delivery Order 0019: Development of an <span class="hlt">Icing</span> Effects Simulation for a Typical Business Jet Configuration</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2007-08-01</p> <p>considered were: - <span class="hlt">Icing</span> protection system failure <span class="hlt">ice</span> - Inter-cycle (roughness) <span class="hlt">ice</span> - Run-back <span class="hlt">ice</span>. The study entailed wind tunnel <span class="hlt">tests</span> of different...jet that incorporates the effects of various forms of <span class="hlt">ice</span>. The <span class="hlt">ice</span> conditions considered were:  <span class="hlt">Icing</span> protection system failure <span class="hlt">ice</span>  Inter-cycle...accretions. These were pre-activation roughness, runback shapes that form downstream of the thermal wing <span class="hlt">ice</span> protection system , and a wing <span class="hlt">ice</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPCM...29C3001G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPCM...29C3001G"><span><span class="hlt">Packing</span> in protein cores</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaines, J. C.; Clark, A. H.; Regan, L.; O'Hern, C. S.</p> <p>2017-07-01</p> <p>Proteins are biological polymers that underlie all cellular functions. The first high-resolution protein structures were determined by x-ray crystallography in the 1960s. Since then, there has been continued interest in understanding and predicting protein structure and stability. It is well-established that a large contribution to protein stability originates from the sequestration from solvent of hydrophobic residues in the protein core. How are such hydrophobic residues arranged in the core; how can one best model the <span class="hlt">packing</span> of these residues, and are residues loosely <span class="hlt">packed</span> with multiple allowed side chain conformations or densely <span class="hlt">packed</span> with a single allowed side chain conformation? Here we show that to properly model the <span class="hlt">packing</span> of residues in protein cores it is essential that amino acids are represented by appropriately calibrated atom sizes, and that hydrogen atoms are explicitly included. We show that protein cores possess a <span class="hlt">packing</span> fraction of φ ≈ 0.56 , which is significantly less than the typically quoted value of 0.74 obtained using the extended atom representation. We also compare the results for the <span class="hlt">packing</span> of amino acids in protein cores to results obtained for jammed <span class="hlt">packings</span> from discrete element simulations of spheres, elongated particles, and composite particles with bumpy surfaces. We show that amino acids in protein cores <span class="hlt">pack</span> as densely as disordered jammed <span class="hlt">packings</span> of particles with similar values for the aspect ratio and bumpiness as found for amino acids. Knowing the structural properties of protein cores is of both fundamental and practical importance. Practically, it enables the assessment of changes in the structure and stability of proteins arising from amino acid mutations (such as those identified as a result of the massive human genome sequencing efforts) and the design of new folded, stable proteins and protein-protein interactions with tunable specificity and affinity.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5043326','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5043326"><span><span class="hlt">Packing</span> and deploying Soft Origami to and from cylindrical volumes with application to automotive airbags</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nelson, Todd G.; Zimmerman, Trent K.; Fernelius, Janette D.; Magleby, Spencer P.; Howell, Larry L.</p> <p>2016-01-01</p> <p><span class="hlt">Packing</span> soft-sheet materials of approximately zero bending stiffness using Soft Origami (origami patterns applied to soft-sheet materials) into cylindrical volumes and their deployment via mechanisms or internal pressure (inflation) is of interest in fields including automobile airbags, deployable heart stents, inflatable space habitats, and dirigible and parachute <span class="hlt">packing</span>. This paper explores twofold patterns, the ‘flasher’ and the ‘inverted-cone fold’, for <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes. Two initial <span class="hlt">packing</span> methods and mechanisms are examined for each of the flasher and inverted-cone fold patterns. An application to driver’s side automobile airbags is performed, and deployment <span class="hlt">tests</span> are completed to compare the influence of <span class="hlt">packing</span> method and origami pattern on deployment performance. Following deployment <span class="hlt">tests</span>, two additional <span class="hlt">packing</span> methods for the inverted-cone fold pattern are explored and applied to automobile airbags. It is shown that modifying the <span class="hlt">packing</span> method (using different methods to impose the same base pattern on the soft-sheet material) can lead to different deployment performance. In total, two origami patterns and six <span class="hlt">packing</span> methods are examined, and the benefits of using Soft Origami patterns and <span class="hlt">packing</span> methods are discussed. Soft Origami is presented as a viable method for efficiently <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes. PMID:27703707</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016RSOS....360429B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RSOS....360429B"><span><span class="hlt">Packing</span> and deploying Soft Origami to and from cylindrical volumes with application to automotive airbags</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bruton, Jared T.; Nelson, Todd G.; Zimmerman, Trent K.; Fernelius, Janette D.; Magleby, Spencer P.; Howell, Larry L.</p> <p>2016-09-01</p> <p><span class="hlt">Packing</span> soft-sheet materials of approximately zero bending stiffness using Soft Origami (origami patterns applied to soft-sheet materials) into cylindrical volumes and their deployment via mechanisms or internal pressure (inflation) is of interest in fields including automobile airbags, deployable heart stents, inflatable space habitats, and dirigible and parachute <span class="hlt">packing</span>. This paper explores twofold patterns, the `flasher' and the `inverted-cone fold', for <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes. Two initial <span class="hlt">packing</span> methods and mechanisms are examined for each of the flasher and inverted-cone fold patterns. An application to driver's side automobile airbags is performed, and deployment <span class="hlt">tests</span> are completed to compare the influence of <span class="hlt">packing</span> method and origami pattern on deployment performance. Following deployment <span class="hlt">tests</span>, two additional <span class="hlt">packing</span> methods for the inverted-cone fold pattern are explored and applied to automobile airbags. It is shown that modifying the <span class="hlt">packing</span> method (using different methods to impose the same base pattern on the soft-sheet material) can lead to different deployment performance. In total, two origami patterns and six <span class="hlt">packing</span> methods are examined, and the benefits of using Soft Origami patterns and <span class="hlt">packing</span> methods are discussed. Soft Origami is presented as a viable method for efficiently <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27703707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27703707"><span><span class="hlt">Packing</span> and deploying Soft Origami to and from cylindrical volumes with application to automotive airbags.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bruton, Jared T; Nelson, Todd G; Zimmerman, Trent K; Fernelius, Janette D; Magleby, Spencer P; Howell, Larry L</p> <p>2016-09-01</p> <p><span class="hlt">Packing</span> soft-sheet materials of approximately zero bending stiffness using Soft Origami (origami patterns applied to soft-sheet materials) into cylindrical volumes and their deployment via mechanisms or internal pressure (inflation) is of interest in fields including automobile airbags, deployable heart stents, inflatable space habitats, and dirigible and parachute <span class="hlt">packing</span>. This paper explores twofold patterns, the 'flasher' and the 'inverted-cone fold', for <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes. Two initial <span class="hlt">packing</span> methods and mechanisms are examined for each of the flasher and inverted-cone fold patterns. An application to driver's side automobile airbags is performed, and deployment <span class="hlt">tests</span> are completed to compare the influence of <span class="hlt">packing</span> method and origami pattern on deployment performance. Following deployment <span class="hlt">tests</span>, two additional <span class="hlt">packing</span> methods for the inverted-cone fold pattern are explored and applied to automobile airbags. It is shown that modifying the <span class="hlt">packing</span> method (using different methods to impose the same base pattern on the soft-sheet material) can lead to different deployment performance. In total, two origami patterns and six <span class="hlt">packing</span> methods are examined, and the benefits of using Soft Origami patterns and <span class="hlt">packing</span> methods are discussed. Soft Origami is presented as a viable method for efficiently <span class="hlt">packing</span> soft-sheet materials into cylindrical volumes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AIPC.1542..341Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AIPC.1542..341Y"><span>The theory of granular <span class="hlt">packings</span> for coarse soils</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yanqui, Calixtro</p> <p>2013-06-01</p> <p>Coarse soils are substances made of grains of different shape, size and orientation. In this paper, new massive-measurable grain indexes are defined to develop a simple and systematic theory for the ideal <span class="hlt">packing</span> of grains. First, a linear relationship between an assemblage of monodisperse spheres and an assemblage of polydisperse grains is deduced. Then, a general formula for the porosity of linearly ordered <span class="hlt">packings</span> of spheres in contact is settled down by the appropriated choosing of eight neighboring spheres located at the vertices of the unit parallelepiped. The porosity of axisymmetric <span class="hlt">packings</span> of grains, related to sand piles and axisymmetric compression <span class="hlt">tests</span>, is proposed to be determined averaging the respective linear parameters. Since they can be <span class="hlt">tested</span> experimentally, porosities of the densest state and the loosest state of a granular soil can be used to verify the accuracy of the present theory. Diagrams for these extreme quantities show a good agreement between the theoretical lines and the experimental data, no matter the dependency on the protocols and mineral composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12..761D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12..761D"><span>Compression experiments on artificial, alpine and marine <span class="hlt">ice</span>: implications for <span class="hlt">ice</span>-shelf/continental interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dierckx, Marie; Goossens, Thomas; Samyn, Denis; Tison, Jean-Louis</p> <p>2010-05-01</p> <p>Antarctic <span class="hlt">ice</span> shelves are important components of continental <span class="hlt">ice</span> dynamics, in that they control grounded <span class="hlt">ice</span> flow towards the ocean. As such, Antarctic <span class="hlt">ice</span> shelves are a key parameter to the stability of the Antarctic <span class="hlt">ice</span> sheet in the context of global change. Marine <span class="hlt">ice</span>, formed by sea water accretion beneath some <span class="hlt">ice</span> shelves, displays distinct physical (grain textures, bubble content, ...) and chemical (salinity, isotopic composition, ...) characteristics as compared to glacier <span class="hlt">ice</span> and sea <span class="hlt">ice</span>. The aim is to refine Glen's flow relation (generally used for <span class="hlt">ice</span> behaviour in deformation) under various parameters (temperature, salinity, debris, grain size ...) to improve deformation laws used in dynamic <span class="hlt">ice</span> shelf models, which would then give more accurate and / or realistic predictions on <span class="hlt">ice</span> shelf stability. To better understand the mechanical properties of natural <span class="hlt">ice</span>, deformation experiments were performed on <span class="hlt">ice</span> samples in laboratory, using a pneumatic compression device. To do so, we developed a custom built compression rig operated by pneumatic drives. It has been designed for performing uniaxial compression <span class="hlt">tests</span> at constant load and under unconfined conditions. The operating pressure ranges from about 0.5 to 10 Bars. This allows modifying the experimental conditions to match the conditions found at the grounding zone (in the 1 Bar range). To maintain the <span class="hlt">ice</span> at low temperature, the samples are immersed in a Silicone oil bath connected to an external refrigeration system. During the experiments, the vertical displacement of the piston and the applied force is measured by sensors which are connected to a digital acquisition system. We started our experiments with artificial <span class="hlt">ice</span> and went on with continental <span class="hlt">ice</span> samples from glaciers in the Alps. The first results allowed us to acquire realistic mechanical data for natural <span class="hlt">ice</span>. <span class="hlt">Ice</span> viscosity was calculated for different types of artificial <span class="hlt">ice</span>, using Glen's flow law, and showed the importance of impurities</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.5905M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.5905M"><span><span class="hlt">Testing</span> a common <span class="hlt">ice</span>-ocean parameterization with laboratory experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McConnochie, C. D.; Kerr, R. C.</p> <p>2017-07-01</p> <p>Numerical models of <span class="hlt">ice</span>-ocean interactions typically rely upon a parameterization for the transport of heat and salt to the <span class="hlt">ice</span> face that has not been satisfactorily validated by observational or experimental data. We compare laboratory experiments of <span class="hlt">ice</span>-saltwater interactions to a common numerical parameterization and find a significant disagreement in the dependence of the melt rate on the fluid velocity. We suggest a resolution to this disagreement based on a theoretical analysis of the boundary layer next to a vertical heated plate, which results in a threshold fluid velocity of approximately 4 cm/s at driving temperatures between 0.5 and 4°C, above which the form of the parameterization should be valid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160005836','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160005836"><span><span class="hlt">Ice</span> Accretions and Full-Scale <span class="hlt">Iced</span> Aerodynamic Performance Data for a Two-Dimensional NACA 23012 Airfoil</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Addy, Harold E., Jr.; Broeren, Andy P.; Potapczuk, Mark G.; Lee, Sam; Guffond, Didier; Montreuil, Emmanuel; Moens, Frederic</p> <p>2016-01-01</p> <p>This report documents the data collected during the large wind tunnel campaigns conducted as part of the SUNSET project (StUdies oN Scaling EffecTs due to <span class="hlt">ice</span>) also known as the <span class="hlt">Ice</span>-Accretion Aerodynamics Simulation study: a joint effort by NASA, the Office National d'Etudes et Recherches Aérospatiales (ONERA), and the University of Illinois. These data form a benchmark database of full-scale <span class="hlt">ice</span> accretions and corresponding <span class="hlt">ice</span>-contaminated aerodynamic performance data for a two-dimensional (2D) NACA 23012 airfoil. The wider research effort also included an analysis of <span class="hlt">ice</span>-contaminated aerodynamics that categorized <span class="hlt">ice</span> accretions by aerodynamic effects and an investigation of subscale, low- Reynolds-number <span class="hlt">ice</span>-contaminated aerodynamics for the NACA 23012 airfoil. The low-Reynolds-number investigation included an analysis of the geometric fidelity needed to reliably assess aerodynamic effects of airfoil <span class="hlt">icing</span> using artificial <span class="hlt">ice</span> shapes. Included herein are records of the <span class="hlt">ice</span> accreted during campaigns in NASA Glenn Research Center's <span class="hlt">Icing</span> Research Tunnel (IRT). Two different 2D NACA 23012 airfoil models were used during these campaigns; an 18-in. (45.7-cm) chord (subscale) model and a 72-in. (182.9-cm) chord (full-scale) model. The aircraft <span class="hlt">icing</span> conditions used during these campaigns were selected from the Federal Aviation Administration's (FAA's) Code of Federal Regulations (CFR) Part 25 Appendix C <span class="hlt">icing</span> envelopes. The records include the <span class="hlt">test</span> conditions, photographs of the <span class="hlt">ice</span> accreted, tracings of the <span class="hlt">ice</span>, and <span class="hlt">ice</span> depth measurements. Model coordinates and pressure tap locations are also presented. Also included herein are the data recorded during a wind tunnel campaign conducted in the F1 Subsonic Pressurized Wind Tunnel of ONERA. The F1 tunnel is a pressured, high- Reynolds-number facility that could accommodate the full-scale (72-in. (182.9-cm) chord) 2D NACA 23012 model. Molds were made of the <span class="hlt">ice</span> accreted during selected <span class="hlt">test</span> runs of the full-scale model</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol2/pdf/CFR-2011-title7-vol2-sec51-310.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol2/pdf/CFR-2011-title7-vol2-sec51-310.pdf"><span>7 CFR 51.310 - <span class="hlt">Packing</span> requirements.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... STANDARDS) United States Standards for Grades of Apples <span class="hlt">Packing</span> Requirements § 51.310 <span class="hlt">Packing</span> requirements. (a) Apples tray <span class="hlt">packed</span> or cell <span class="hlt">packed</span> in cartons shall be arranged according to approved and... that apples are of the proper size for molds or cell compartments in which they are <span class="hlt">packed</span>, and that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol2/pdf/CFR-2012-title7-vol2-sec51-310.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol2/pdf/CFR-2012-title7-vol2-sec51-310.pdf"><span>7 CFR 51.310 - <span class="hlt">Packing</span> requirements.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... STANDARDS) United States Standards for Grades of Apples <span class="hlt">Packing</span> Requirements § 51.310 <span class="hlt">Packing</span> requirements. (a) Apples tray <span class="hlt">packed</span> or cell <span class="hlt">packed</span> in cartons shall be arranged according to approved and... that apples are of the proper size for molds or cell compartments in which they are <span class="hlt">packed</span>, and that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860022116','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860022116"><span>Turbulent dispersion of the <span class="hlt">icing</span> cloud from spray nozzles used in <span class="hlt">icing</span> tunnels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marek, C. J.; Olsen, W. A., Jr.</p> <p>1986-01-01</p> <p>To correctly simulate flight in natural <span class="hlt">icing</span> conditions, the turbulence in an <span class="hlt">icing</span> simulator must be as low as possible. But some turbulence is required to mix the droplets from the spray nozzles and achieve an <span class="hlt">icing</span> cloud of uniform liquid water content. The goal for any spray system is to obtain the widest possible spray cloud with the lowest possible turbulence in the <span class="hlt">test</span> section of a <span class="hlt">icing</span> tunnel. This investigation reports the measurement of turbulence and the three-dimensional spread of the cloud from a single spray nozzle. The task was to determine how the air turbulence and cloud width are affected by spray bars of quite different drag coefficients, by changes in the turbulence upstream of the spray, the droplet size, and the atomizing air. An <span class="hlt">ice</span> accretion grid, located 6.3 m downstream of the single spray nozzle, was used to measure cloud spread. Both the spray bar and the grid were located in the constant velocity <span class="hlt">test</span> section. Three spray bar shapes were <span class="hlt">tested</span>: the short blunt spray bar used in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel, a thin 14.6 cm chord airfoil, and a 53 cm chord NACA 0012 airfoil. At the low airspeed (56 km/hr) the <span class="hlt">ice</span> accretion pattern was axisymmetric and was not affected by the shape of the spray bar. At the high airspeed (169 km/hr) the spread was 30 percent smaller than at the low airspeed. For the widest cloud the spray bars should be located as far upstream in the low velocity plenum of the <span class="hlt">icing</span> tunnel. Good comparison is obtained between the cloud spread data and predicitons from a two-dimensional cloud mixing computer code using the two equation turbulence (k epsilon g) model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.C41C0467V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.C41C0467V"><span>Modeling brine and nutrient dynamics in Antarctic sea <span class="hlt">ice</span>: the case of dissolved silica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vancoppenolle, M.; Goosse, H.; de Montety, A.; Fichefet, T.; Tremblay, B.; Tison, J.</p> <p>2009-12-01</p> <p>Sea <span class="hlt">ice</span> ecosystems are characterized by micro-algae living in brine inclusions. The growth rate of <span class="hlt">ice</span> algae depends on light and nutrient supply. Here, the interactions between nutrients and brine dynamics under the influence of algae are investigated using a one-dimensional model. The model includes snow and <span class="hlt">ice</span> thermodynamics with brine physics and an idealized sea <span class="hlt">ice</span> biological component, characterized by one nutrient, namely dissolved silica (DSi). In the model, DSi follows brine motion and is consumed by <span class="hlt">ice</span> algae. Depending on physical <span class="hlt">ice</span> characteristics, the brine flow is either advective, diffusive or turbulent. The vertical profiles of <span class="hlt">ice</span> salinity and DSi concentration are solutions of advection-diffusion equations. The model is configured to simulate the typical thermodynamic regimes of first-year Antarctic <span class="hlt">pack</span> <span class="hlt">ice</span>. The simulated vertical profiles of salinity and DSi qualitatively reproduce observations. Analysis of results highlights the role of convection in the lowermost 5-10 cm of <span class="hlt">ice</span>. Convection mixes saline, nutrient-poor brine with comparatively fresh, nutrient-rich seawater. This implies a rejection of salt to the ocean and a flux of DSi to the <span class="hlt">ice</span>. In presence of growing algae, the simulated ocean-to-<span class="hlt">ice</span> DSi flux increases by 0-115% compared to an abiotic situation. In turn, primary production and brine convection act in synergy to form a nutrient pump. The other important processes are the flooding of the surface by seawater and the percolation of meltwater. The former refills nutrients near the <span class="hlt">ice</span> surface in spring. The latter, if present, tends to expell nutrients from the <span class="hlt">ice</span> in summer. Sketch of salt (left) and nutrient (right) exchanges at the <span class="hlt">ice</span>-ocean interface proposed in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27170707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27170707"><span>American Spirit <span class="hlt">Pack</span> Descriptors and Perceptions of Harm: A Crowdsourced Comparison of Modified <span class="hlt">Packs</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pearson, Jennifer L; Richardson, Amanda; Feirman, Shari P; Villanti, Andrea C; Cantrell, Jennifer; Cohn, Amy; Tacelosky, Michael; Kirchner, Thomas R</p> <p>2016-08-01</p> <p>In 2015, the Food and Drug Administration issued warnings to three tobacco manufacturers who label their cigarettes as "additive-free" and/or "natural" on the grounds that they make unauthorized reduced risk claims. The goal of this study was to examine US adults' perceptions of three American Spirit (AS) <span class="hlt">pack</span> descriptors ("Made with Organic Tobacco," "100% Additive-Free," and "100% US Grown Tobacco") to assess if they communicate reduced risk. In September 2012, three cross-sectional surveys were posted on Amazon Mechanical Turk. Adult participants evaluated the relative harm of a Marlboro Red <span class="hlt">pack</span> versus three different AS <span class="hlt">packs</span> with the descriptors "Made with Organic Tobacco," "100% Additive-Free," or "100% US Grown Tobacco" (Survey 1; n = 461); a Marlboro Red <span class="hlt">pack</span> versus these AS <span class="hlt">packs</span> modified to exclude descriptors (Survey 2; n = 857); and unmodified versus modified AS <span class="hlt">pack</span> images (Survey 3; n = 1001). The majority of Survey 1 participants rated the unmodified AS <span class="hlt">packs</span> as less harmful than the Marlboro Red <span class="hlt">pack</span>; 35.4%-58.8% of Survey 2 participants also rated the modified (no claims) <span class="hlt">packs</span> as less harmful than Marlboro Red. In these surveys, prior use of AS cigarettes was associated with reduced perceptions of risk (adjusted odds ratio [AOR] 1.59-2.40). "Made with Organic Tobacco" and "100% Additive-Free" were associated with reduced perceptions of risk when comparing the modified versus the unmodified AS <span class="hlt">packs</span> (Survey 3). Data suggest that these AS <span class="hlt">pack</span> descriptors communicate reduced harm messages to consumers. Findings have implications for regulatory actions related to product labeling and packaging. These findings provide additional evidence that the "Made with Organic Tobacco," "100% Additive-Free," and "100% US Grown" descriptors, as well as other aspects of the AS <span class="hlt">pack</span> design, communicate reduced harm to non-, current, and former smokers. Additionally, they provide support for the importance of FDA's 2015 warning to Santa Fe Natural Tobacco Company on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880003414','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880003414"><span>Measured performance of the heat exchanger in the NASA <span class="hlt">icing</span> research tunnel under severe <span class="hlt">icing</span> and dry-air conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, W.; Vanfossen, J.; Nussle, R.</p> <p>1987-01-01</p> <p>Measurements were made of the pressure drop and thermal perfomance of the unique refrigeration heat exchanger in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel (IRT) under severe <span class="hlt">icing</span> and frosting conditions and also with dry air. This data will be useful to those planning to use or extend the capability of the IRT and other <span class="hlt">icing</span> facilities (e.g., the Altitude Wind Tunnel-AWT). The IRT heat exchanger and refrigeration system is able to cool air passing through the <span class="hlt">test</span> section down to at least a total temperature of -30 C (well below <span class="hlt">icing</span> requirements), and usually up to -2 C. The system maintains a uniform temperature across the <span class="hlt">test</span> section at all airspeeds, which is more difficult and time consuming at low airspeeds, at high temperatures, and on hot, humid days when the cooling towers are less efficient. The very small surfaces of the heat exchanger prevent any <span class="hlt">icing</span> cloud droplets from passing through it and going through the <span class="hlt">tests</span> section again. The IRT heat exchanger was originally designed not to be adversely affected by severe <span class="hlt">icing</span>. During a worst-case <span class="hlt">icing</span> <span class="hlt">test</span> the heat exchanger <span class="hlt">iced</span> up enough so that the temperature uniformaity was no worse than about +/- 1 deg C. The conclusion is that the heat exchanger design performs well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060022142','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060022142"><span><span class="hlt">Test</span> and Analysis Correlation of High Speed Impacts of <span class="hlt">Ice</span> Cylinders</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fasanella, Edwin L.; Boitnott, Richard L.; Kellas, Sotiris</p> <p>2006-01-01</p> <p>During the space shuttle return-to-flight preparations following the Columbia accident, finite element models were needed that could predict the threshold of critical damage to the orbiter s wing leading edge from <span class="hlt">ice</span> debris impacts. Hence, an experimental program was initiated to provide crushing data from impacted <span class="hlt">ice</span> for use in dynamic finite element material models. A high-speed drop tower was configured to capture force time-histories of <span class="hlt">ice</span> cylinders for impacts up to approximately 100 ft/s. At low velocity, the force-time history depended heavily on the internal crystalline structure of the <span class="hlt">ice</span>. However, for velocities of 100 ft/s and above, the <span class="hlt">ice</span> fractured on impact, behaved more like a fluid, and the subsequent force-time history curves were much less dependent on the internal crystalline structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910032594&hterms=helicopter+water&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dhelicopter%2Bwater','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910032594&hterms=helicopter+water&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dhelicopter%2Bwater"><span>Passive infrared <span class="hlt">ice</span> detection for helicopter applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dershowitz, Adam L.; Hansman, R. John, Jr.</p> <p>1990-01-01</p> <p>A technique is proposed to remotely detect rotor <span class="hlt">icing</span> on helicopters by using passive IR thermometry to detect the warming caused by latent heat release as supercooled water freezes. During <span class="hlt">icing</span>, the <span class="hlt">ice</span> accretion region will be warmer than the uniced trailing edge, resulting in a characteristic chordwise temperature profile. Preliminary <span class="hlt">tests</span> were conducted on a static model in the NASA <span class="hlt">Icing</span> Research Tunnel for a variety of wet (glaze) and dry (rime) <span class="hlt">ice</span> conditions. The chordwise temperature profiles were confirmed by observation with an IR thermal video system and thermocouple observations. The IR observations were consistent with predictions of the LEWICE <span class="hlt">ice</span> accretion code, which was used to extrapolate the observations to rotor <span class="hlt">icing</span> conditions. Based on the static observations, the passive IR <span class="hlt">ice</span> detection technique appears promising; however, further <span class="hlt">testing</span> or rotating blades is required.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017TCry...11.2033D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017TCry...11.2033D"><span><span class="hlt">Ice</span> bridges and ridges in the Maxwell-EB sea <span class="hlt">ice</span> rheology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dansereau, Véronique; Weiss, Jérôme; Saramito, Pierre; Lattes, Philippe; Coche, Edmond</p> <p>2017-09-01</p> <p>This paper presents a first implementation of a new rheological model for sea <span class="hlt">ice</span> on geophysical scales. This continuum model, called Maxwell elasto-brittle (Maxwell-EB), is based on a Maxwell constitutive law, a progressive damage mechanism that is coupled to both the elastic modulus and apparent viscosity of the <span class="hlt">ice</span> cover and a Mohr-Coulomb damage criterion that allows for pure (uniaxial and biaxial) tensile strength. The model is <span class="hlt">tested</span> on the basis of its capability to reproduce the complex mechanical and dynamical behaviour of sea <span class="hlt">ice</span> drifting through a narrow passage. Idealized as well as realistic simulations of the flow of <span class="hlt">ice</span> through Nares Strait are presented. These demonstrate that the model reproduces the formation of stable <span class="hlt">ice</span> bridges as well as the stoppage of the flow, a phenomenon occurring within numerous channels of the Arctic. In agreement with observations, the model captures the propagation of damage along narrow arch-like kinematic features, the discontinuities in the velocity field across these features dividing the <span class="hlt">ice</span> cover into floes, the strong spatial localization of the thickest, ridged <span class="hlt">ice</span>, the presence of landfast <span class="hlt">ice</span> in bays and fjords and the opening of polynyas downstream of the strait. The model represents various dynamical behaviours linked to an overall weakening of the <span class="hlt">ice</span> cover and to the shorter lifespan of <span class="hlt">ice</span> bridges, with implications in terms of increased <span class="hlt">ice</span> export through narrow outflow pathways of the Arctic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090042816','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090042816"><span>Impact <span class="hlt">Testing</span> on Reinforced Carbon-Carbon Flat Panels with <span class="hlt">Ice</span> Projectiles for the Space Shuttle Return to Flight Program</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Melis, Matthew E.; Revilock, Duane M.; Pereira, Michael J.; Lyle, Karen H.</p> <p>2009-01-01</p> <p>Following the tragedy of the Orbiter Columbia (STS-107) on February 1, 2003, a major effort commenced to develop a better understanding of debris impacts and their effect on the space shuttle subsystems. An initiative to develop and validate physics-based computer models to predict damage from such impacts was a fundamental component of this effort. To develop the models it was necessary to physically characterize reinforced carbon-carbon (RCC) along with <span class="hlt">ice</span> and foam debris materials, which could shed on ascent and impact the orbiter RCC leading edges. The validated models enabled the launch system community to use the impact analysis software LS-DYNA (Livermore Software Technology Corp.) to predict damage by potential and actual impact events on the orbiter leading edge and nose cap thermal protection systems. Validation of the material models was done through a three-level approach: Level 1--fundamental <span class="hlt">tests</span> to obtain independent static and dynamic constitutive model properties of materials of interest, Level 2--subcomponent impact <span class="hlt">tests</span> to provide highly controlled impact <span class="hlt">test</span> data for the correlation and validation of the models, and Level 3--full-scale orbiter leading-edge impact <span class="hlt">tests</span> to establish the final level of confidence for the analysis methodology. This report discusses the Level 2 <span class="hlt">test</span> program conducted in the NASA Glenn Research Center (GRC) Ballistic Impact Laboratory with <span class="hlt">ice</span> projectile impact <span class="hlt">tests</span> on flat RCC panels, and presents the data observed. The Level 2 <span class="hlt">testing</span> consisted of 54 impact <span class="hlt">tests</span> in the NASA GRC Ballistic Impact Laboratory on 6- by 6-in. and 6- by 12-in. flat plates of RCC and evaluated three types of debris projectiles: Single-crystal, polycrystal, and "soft" <span class="hlt">ice</span>. These impact <span class="hlt">tests</span> helped determine the level of damage generated in the RCC flat plates by each projectile and validated the use of the <span class="hlt">ice</span> and RCC models for use in LS-DYNA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=76463&keyword=ice&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=76463&keyword=ice&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>CTEPP STANDARD OPERATING PROCEDURE FOR <span class="hlt">PACKING</span> AND SHIPPING STUDY SAMPLES (SOP-3.11)</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>This SOP describes the methods for <span class="hlt">packing</span> and shipping study samples. These methods are for <span class="hlt">packing</span> and shipping biological and environmental samples. The methods have been <span class="hlt">tested</span> and used in the previous pilot studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090038754&hterms=heat+exchanger&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dheat%2Bexchanger','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090038754&hterms=heat+exchanger&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dheat%2Bexchanger"><span>Development, <span class="hlt">Testing</span>, and Failure Mechanisms of a Replicative <span class="hlt">Ice</span> Phase Change Material Heat Exchanger</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Leimkuehler, Thomas O.; Hansen, Scott; Stephan, Ryan A.</p> <p>2009-01-01</p> <p>Phase change materials (PCM) may be useful for thermal control systems that involve cyclical heat loads or cyclical thermal environments such as Low Earth Orbit (LEO) and Low Lunar Orbit (LLO). Thermal energy can be stored in the PCM during peak heat loads or in adverse thermal environments. The stored thermal energy can then be released later during minimum heat loads or in more favorable thermal environments. One advantage that PCM s have over evaporators in this scenario is that they do not use a consumable. Wax PCM units have been baselined for the Orion thermal control system and also provide risk mitigation for the Altair Lander. However, the use of water as a PCM has the potential for significant mass reduction since the latent heat of formation of water is approximately 70% greater than that of wax. One of the potential drawbacks of using <span class="hlt">ice</span> as a PCM is its potential to rupture its container as water expands upon freezing. In order to develop a space qualified <span class="hlt">ice</span> PCM heat exchanger, failure mechanisms must first be understood. Therefore, a methodical experimental investigation has been undertaken to demonstrate and document specific failure mechanisms due to <span class="hlt">ice</span> expansion in the PCM. An <span class="hlt">ice</span> PCM heat exchanger that replicates the thermal energy storage capacity of an existing wax PCM unit was fabricated and <span class="hlt">tested</span>. Additionally, methods for controlling void location in order to reduce the risk of damage due to <span class="hlt">ice</span> expansion are investigated. This paper presents the results to date of this investigation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100017225','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100017225"><span>Development, <span class="hlt">Testing</span>, and Failure Mechanisms of a Replicative <span class="hlt">Ice</span> Phase Change Material Heat Exchanger</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Leimkuehler, Thomas O.; Hansen, Scott; Stephan, Ryan A.</p> <p>2010-01-01</p> <p>Phase change materials (PCM) may be useful for thermal control systems that involve cyclical heat loads or cyclical thermal environments such as Low Earth Orbit (LEO) and Low Lunar Orbit (LLO). Thermal energy can be stored in the PCM during peak heat loads or in adverse thermal environments. The stored thermal energy can then be released later during minimum heat loads or in more favorable thermal environments. One advantage that PCM's have over evaporators in this scenario is that they do not use a consumable. Wax PCM units have been baselined for the Orion thermal control system and also provide risk mitigation for the Altair Lander. However, the use of water as a PCM has the potential for significant mass reduction since the latent heat of formation of water is approximately 70% greater than that of wax. One of the potential drawbacks of using <span class="hlt">ice</span> as a PCM is its potential to rupture its container as water expands upon freezing. In order to develop a space qualified <span class="hlt">ice</span> PCM heat exchanger, failure mechanisms must first be understood. Therefore, a methodical experimental investigation has been undertaken to demonstrate and document specific failure mechanisms due to <span class="hlt">ice</span> expansion in the PCM. An <span class="hlt">ice</span> PCM heat exchanger that replicates the thermal energy storage capacity of an existing wax PCM unit was fabricated and <span class="hlt">tested</span>. Additionally, methods for controlling void location in order to reduce the risk of damage due to <span class="hlt">ice</span> expansion are investigated. This paper presents the results to date of this investigation. Nomenclature</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23705008','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23705008"><span>Change and variability in East antarctic sea <span class="hlt">ice</span> seasonality, 1979/80-2009/10.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Massom, Robert; Reid, Philip; Stammerjohn, Sharon; Raymond, Ben; Fraser, Alexander; Ushio, Shuki</p> <p>2013-01-01</p> <p>Recent analyses have shown that significant changes have occurred in patterns of sea <span class="hlt">ice</span> seasonality in West Antarctica since 1979, with wide-ranging climatic, biological and biogeochemical consequences. Here, we provide the first detailed report on long-term change and variability in annual timings of sea <span class="hlt">ice</span> advance, retreat and resultant <span class="hlt">ice</span> season duration in East Antarctica. These were calculated from satellite-derived <span class="hlt">ice</span> concentration data for the period 1979/80 to 2009/10. The pattern of change in sea <span class="hlt">ice</span> seasonality off East Antarctica comprises mixed signals on regional to local scales, with pockets of strongly positive and negative trends occurring in near juxtaposition in certain regions e.g., Prydz Bay. This pattern strongly reflects change and variability in different elements of the marine "icescape", including fast <span class="hlt">ice</span>, polynyas and the marginal <span class="hlt">ice</span> zone. A trend towards shorter sea-<span class="hlt">ice</span> duration (of 1 to 3 days per annum) occurs in fairly isolated pockets in the outer <span class="hlt">pack</span> from∼95-110°E, and in various near-coastal areas that include an area of particularly strong and persistent change near Australia's Davis Station and between the Amery and West <span class="hlt">Ice</span> Shelves. These areas are largely associated with coastal polynyas that are important as sites of enhanced sea <span class="hlt">ice</span> production/melt. Areas of positive trend in <span class="hlt">ice</span> season duration are more extensive, and include an extensive zone from 160-170°E (i.e., the western Ross Sea sector) and the near-coastal zone between 40-100°E. The East Antarctic pattern is considerably more complex than the well-documented trends in West Antarctica e.g., in the Antarctic Peninsula-Bellingshausen Sea and western Ross Sea sectors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060043803&hterms=soil+environment&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsoil%2Benvironment','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060043803&hterms=soil+environment&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsoil%2Benvironment"><span>USDC based rapid penetrator of <span class="hlt">packed</span> soil</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bao, Xiaoqi; Bar-Cohen, Yoseph; Chang, Zensheu; Sherrit, Stewart; Badescu, Mircea</p> <p>2006-01-01</p> <p>Environment protection requires more <span class="hlt">testing</span> and analysis tools. To detect buried chemical containers or other objects embedded in soil and avoid possible damages of them, a penetrator of <span class="hlt">packed</span> soil operated using low pushing force was developed. The design was based on a novel driving mechanism of the ultrasonic/sonic driller/corer (USDC) device developed in the NDEAA lab at JPL [Bar-Cohen et al 2001, Bao et al 2003]. In the penetrator, a small free-flying mass is energized by a piezoelectric transducer and impacts a rod probe on its shoulder at frequencies of hundreds times per second. The impacts help the probe to penetrate the <span class="hlt">packed</span> soil rapidly. A great reduction of the needed pushing force for penetration was achieved. The details of the design of the prototype penetrator and the results of performance <span class="hlt">tests</span> are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.C51A0683R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.C51A0683R"><span>Inter-comparison of isotropic and anisotropic sea <span class="hlt">ice</span> rheology in a fully coupled model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roberts, A.; Cassano, J. J.; Maslowski, W.; Osinski, R.; Seefeldt, M. W.; Hughes, M.; Duvivier, A.; Nijssen, B.; Hamman, J.; Hutchings, J. K.; Hunke, E. C.</p> <p>2015-12-01</p> <p>We present the sea <span class="hlt">ice</span> climate of the Regional Arctic System Model (RASM), using a suite of new physics available in the Los Alamos Sea <span class="hlt">Ice</span> Model (CICE5). RASM is a high-resolution fully coupled pan-Arctic model that also includes the Parallel Ocean Program (POP), the Weather Research and Forecasting Model (WRF) and Variable Infiltration Capacity (VIC) land model. The model domain extends from ~45˚N to the North Pole and is configured to run at ~9km resolution for the <span class="hlt">ice</span> and ocean components, coupled to 50km resolution atmosphere and land models. The baseline sea <span class="hlt">ice</span> model configuration includes mushy-layer sea <span class="hlt">ice</span> thermodynamics and level-<span class="hlt">ice</span> melt ponds. Using this configuration, we compare the use of isotropic and anisotropic sea <span class="hlt">ice</span> mechanics, and evaluate model performance using these two variants against observations including Arctic buoy drift and deformation, satellite-derived drift and deformation, and sea <span class="hlt">ice</span> volume estimates from ICESat. We find that the isotropic rheology better approximates spatial patterns of thickness observed across the Arctic, but that both rheologies closely approximate scaling laws observed in the <span class="hlt">pack</span> using buoys and RGPS data. A fundamental component of both <span class="hlt">ice</span> mechanics variants, the so called Elastic-Viscous-Plastic (EVP) and Anisotropic-Elastic-Plastic (EAP), is that they are highly sensitive to the timestep used for elastic sub-cycling in an inertial-resolving coupled framework, and this has a significant affect on surface fluxes in the fully coupled framework.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol3/pdf/CFR-2013-title7-vol3-sec91-20.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol3/pdf/CFR-2013-title7-vol3-sec91-20.pdf"><span>7 CFR 91.20 - Shipping.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... refrigerated samples should contain <span class="hlt">ice</span> or <span class="hlt">ice</span> <span class="hlt">packs</span> to maintain temperatures of 0° to 5 °C, unless a different temperature is required for the sample to be <span class="hlt">tested</span>. (d) Containers for frozen samples should contain dry <span class="hlt">ice</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol3/pdf/CFR-2012-title7-vol3-sec91-20.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol3/pdf/CFR-2012-title7-vol3-sec91-20.pdf"><span>7 CFR 91.20 - Shipping.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... refrigerated samples should contain <span class="hlt">ice</span> or <span class="hlt">ice</span> <span class="hlt">packs</span> to maintain temperatures of 0° to 5 °C, unless a different temperature is required for the sample to be <span class="hlt">tested</span>. (d) Containers for frozen samples should contain dry <span class="hlt">ice</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol3/pdf/CFR-2014-title7-vol3-sec91-20.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol3/pdf/CFR-2014-title7-vol3-sec91-20.pdf"><span>7 CFR 91.20 - Shipping.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... refrigerated samples should contain <span class="hlt">ice</span> or <span class="hlt">ice</span> <span class="hlt">packs</span> to maintain temperatures of 0° to 5 °C, unless a different temperature is required for the sample to be <span class="hlt">tested</span>. (d) Containers for frozen samples should contain dry <span class="hlt">ice</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol3/pdf/CFR-2011-title7-vol3-sec91-20.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title7-vol3/pdf/CFR-2011-title7-vol3-sec91-20.pdf"><span>7 CFR 91.20 - Shipping.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... refrigerated samples should contain <span class="hlt">ice</span> or <span class="hlt">ice</span> <span class="hlt">packs</span> to maintain temperatures of 0° to 5 °C, unless a different temperature is required for the sample to be <span class="hlt">tested</span>. (d) Containers for frozen samples should contain dry <span class="hlt">ice</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol3/pdf/CFR-2010-title7-vol3-sec91-20.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol3/pdf/CFR-2010-title7-vol3-sec91-20.pdf"><span>7 CFR 91.20 - Shipping.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... refrigerated samples should contain <span class="hlt">ice</span> or <span class="hlt">ice</span> <span class="hlt">packs</span> to maintain temperatures of 0° to 5 °C, unless a different temperature is required for the sample to be <span class="hlt">tested</span>. (d) Containers for frozen samples should contain dry <span class="hlt">ice</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930016861','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930016861"><span>Radar backscatter measurements from Arctic sea <span class="hlt">ice</span> during the fall freeze-up</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Beaven, S.; Gogineni, S. P.; Shanableh, M.; Gow, A.; Tucker, W.; Jezek, K.</p> <p>1993-01-01</p> <p>Radar backscatter measurements from sea <span class="hlt">ice</span> during the fall freeze-up were performed by the United States Coast Guard Icebreaker Polar Star as a part of the International Arctic Ocean Expedition (IAOE'91) from Aug. to Sep. 1991. The U.S. portion of the experiment took place on board the Polar Star and was referred to as TRAPOLEX '91 (Transpolar expedition) by some investigators. Before prematurely aborting its mission because of mechanical failure of her port shaft, the Polar Star reached 84 deg 57 min N latitude at 35 deg E longitude. The ship was in the <span class="hlt">ice</span> (greater than 50 percent coverage) from 14 Aug. until 3 Sep. and was operational for all but 6 days due to two instances of mechanical problems with the port shaft. The second was fatal to the ship's participation in the expedition. During the expedition, radar backscatter was measured at C-band under a variety of conditions. These included measurements from young <span class="hlt">ice</span> types as well as from multiyear and first-/second-year sea <span class="hlt">ice</span> during the fall freeze-up. The sea <span class="hlt">ice</span> types were determined by measurement of the <span class="hlt">ice</span> properties at several of the stations and by visual inspection on others. Radar backscatter measurements were performed over a large portion of the ship's transit into the Arctic <span class="hlt">ice</span> <span class="hlt">pack</span>. These were accompanied by in situ sea <span class="hlt">ice</span> property characterization by the U.S. Army Cold Regions Research and Engineering Laboratory (CRREL) at several stations and, when snow was present, its properties were documented by The Microwave Group, Ottawa River (MWG).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780007288','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780007288"><span>Kinetics of <span class="hlt">pack</span> aluminization of nickel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Seigle, L. L.; Gupta, B. K.; Shankar, R.; Sarkhel, A. K.</p> <p>1978-01-01</p> <p>The kinetics of <span class="hlt">pack</span> aluminization of unalloyed nickel in <span class="hlt">packs</span> of varying aluminum activity with various halide activators were studied. Surface compositions of the coatings as functions of time, temperature, and <span class="hlt">pack</span> composition were obtained in order to establish the boundary conditions for diffusion in the system. The structure of the <span class="hlt">packs</span> was also examined in order to clarify the mechanism of aluminum transport. The results indicate that the kinetics of <span class="hlt">pack</span> aluminization are controlled jointly by gas diffusion in the <span class="hlt">pack</span> and solid diffusion in the coating. Levine and Caves' model for gas diffusion was combined with calculations of rates of diffusion in the solid to formulate a more complete theory for the kinetics of <span class="hlt">pack</span> aluminization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TRACE...6..221S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TRACE...6..221S"><span>Fundamental Research on Heat Transfer Characteristics in Shell & Tube Type <span class="hlt">Ice</span> Forming Cold Energy Storage</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saito, Akio; Utaka, Yoshio; Okawa, Seiji; Ishibashi, Hiroaki</p> <p></p> <p>Investigation of heat transfer characteristics in an <span class="hlt">ice</span> making cold energy storage using a set of horizontal cooling pipes was carried out experimentally. Cooling pipe arrangement, number of pipes used and initial water temperature were varied, and temperature distribution in the tank and the volume of <span class="hlt">ice</span> formed around the pipe were measured. Natural convection was also observed visually. During the experiment, two kinds of layers were observed. One is the layer where <span class="hlt">ice</span> forming is interfered by natural convection and its temperature decreases rapidly with an almost uniform temperature distribution, and the other is the layer where <span class="hlt">ice</span> forms steadily under a stagnant water condition. The former was called that the layer is under a cooling process and the latter that the layer is under an <span class="hlt">ice</span> forming process. The effect of the experimental parameters, such as the arrangement of the cooling pipes, the number of pipes, the initial water temperature and the flow rate of the cooling medium, on the cooling process and the <span class="hlt">ice</span> forming process were discussed. Approximate analysis was also carried out and compared with the experimental results. Finally, the relationship between the <span class="hlt">ice</span> <span class="hlt">packing</span> factor, which is significant in preventing the blockade, and experimental parameters was discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA955001','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA955001"><span>Man in the Arctic, The Changing Nature of His Quest for Food and Water as Related to Snow, <span class="hlt">Ice</span>, and Permafrost</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1962-01-01</p> <p>Sub- marines have been used under the <span class="hlt">ice</span> <span class="hlt">pack</span>. The most systematic and concerted effort has bet that conducted in Greenland where data from nearly...ml -’ -•- <span class="hlt">ice</span> individually, chronic thirst was a common complaint. In fact, one cause of dehydration ex- haustion was seen .15 The problem of...made by truck or sledge and bar- rel. For example, at Hay River water is supplied under franchise by a trucker. This water is drawn from the river and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.213...17B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.213...17B"><span>Gypsum and hydrohalite dynamics in sea <span class="hlt">ice</span> brines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Butler, Benjamin M.; Papadimitriou, Stathys; Day, Sarah J.; Kennedy, Hilary</p> <p>2017-09-01</p> <p> experimental solubility in this system. Incorporation of hydrohalite solubility into a 1D thermodynamic model of the growth of first-year Arctic sea <span class="hlt">ice</span> showed its precipitation to initiate once the incoming shortwave radiation dropped to 0 W m-2, and that it can reach concentrations of 9.9 g kg-1 within the upper and coldest layers of the <span class="hlt">ice</span> <span class="hlt">pack</span>. This suggests a limited effect of hydrohalite on the albedo of sea <span class="hlt">ice</span>. The insights provided by the solubility measurements into the behaviour of gypsum and hydrohalite in the <span class="hlt">ice</span>-brine system cannot be gleaned from field investigations at present.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRC..119.4168M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRC..119.4168M"><span>Calibration of sea <span class="hlt">ice</span> dynamic parameters in an ocean-sea <span class="hlt">ice</span> model using an ensemble Kalman filter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Massonnet, F.; Goosse, H.; Fichefet, T.; Counillon, F.</p> <p>2014-07-01</p> <p>The choice of parameter values is crucial in the course of sea <span class="hlt">ice</span> model development, since parameters largely affect the modeled mean sea <span class="hlt">ice</span> state. Manual tuning of parameters will soon become impractical, as sea <span class="hlt">ice</span> models will likely include more parameters to calibrate, leading to an exponential increase of the number of possible combinations to <span class="hlt">test</span>. Objective and automatic methods for parameter calibration are thus progressively called on to replace the traditional heuristic, "trial-and-error" recipes. Here a method for calibration of parameters based on the ensemble Kalman filter is implemented, <span class="hlt">tested</span> and validated in the ocean-sea <span class="hlt">ice</span> model NEMO-LIM3. Three dynamic parameters are calibrated: the <span class="hlt">ice</span> strength parameter P*, the ocean-sea <span class="hlt">ice</span> drag parameter Cw, and the atmosphere-sea <span class="hlt">ice</span> drag parameter Ca. In twin, perfect-model experiments, the default parameter values are retrieved within 1 year of simulation. Using 2007-2012 real sea <span class="hlt">ice</span> drift data, the calibration of the <span class="hlt">ice</span> strength parameter P* and the oceanic drag parameter Cw improves clearly the Arctic sea <span class="hlt">ice</span> drift properties. It is found that the estimation of the atmospheric drag Ca is not necessary if P* and Cw are already estimated. The large reduction in the sea <span class="hlt">ice</span> speed bias with calibrated parameters comes with a slight overestimation of the winter sea <span class="hlt">ice</span> areal export through Fram Strait and a slight improvement in the sea <span class="hlt">ice</span> thickness distribution. Overall, the estimation of parameters with the ensemble Kalman filter represents an encouraging alternative to manual tuning for ocean-sea <span class="hlt">ice</span> models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/3116836','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/3116836"><span>Lactose digestion from flavored and frozen yogurts, <span class="hlt">ice</span> milk, and <span class="hlt">ice</span> cream by lactase-deficient persons.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martini, M C; Smith, D E; Savaiano, D A</p> <p>1987-10-01</p> <p>Lactose digestion from and tolerance to flavored and frozen yogurts, <span class="hlt">ice</span> cream, and <span class="hlt">ice</span> milk were evaluated (20 g lactose/meal) in lactase-deficient subjects by use of breath hydrogen techniques. Unflavored yogurt caused significantly less hydrogen production than milk (37 vs 185 delta ppm X h, n = 9). Flavored yogurt was intermediate (77 delta ppm X h). Subjects were free of symptoms after consuming flavored and unflavored yogurts. Of seven commercial yogurts <span class="hlt">tested</span>, all contained significant levels of microbial beta-galactosidase (beta-gal). In addition, eight subjects were fed meals of milk, <span class="hlt">ice</span> milk, <span class="hlt">ice</span> cream, and frozen yogurts with and without cultures containing high levels of beta-gal. Peak hydrogen excretion after consumption of frozen yogurt with high beta-gal was less than one-half of that observed after the other five <span class="hlt">test</span> meals and intolerance symptoms were absent. Tolerance to frozen yogurt, produced under usual commercial procedures, was found to be similar to that of <span class="hlt">ice</span> milk and <span class="hlt">ice</span> cream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.C53B0574L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.C53B0574L"><span><span class="hlt">Ice</span> Shelf-Ocean Interactions Near <span class="hlt">Ice</span> Rises and <span class="hlt">Ice</span> Rumples</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lange, M. A.; Rückamp, M.; Kleiner, T.</p> <p>2013-12-01</p> <p>The stability of <span class="hlt">ice</span> shelves depends on the existence of embayments and is largely influenced by <span class="hlt">ice</span> rises and <span class="hlt">ice</span> rumples, which act as 'pinning-points' for <span class="hlt">ice</span> shelf movement. Of additional critical importance are interactions between <span class="hlt">ice</span> shelves and the water masses underlying them in <span class="hlt">ice</span> shelf cavities, particularly melting and refreezing processes. The present study aims to elucidate the role of <span class="hlt">ice</span> rises and <span class="hlt">ice</span> rumples in the context of climate change impacts on Antarctic <span class="hlt">ice</span> shelves. However, due to their smaller spatial extent, <span class="hlt">ice</span> rumples react more sensitively to climate change than <span class="hlt">ice</span> rises. Different forcings are at work and need to be considered separately as well as synergistically. In order to address these issues, we have decided to deal with the following three issues explicitly: oceanographic-, cryospheric and general topics. In so doing, we paid particular attention to possible interrelationships and feedbacks in a coupled <span class="hlt">ice</span>-shelf-ocean system. With regard to oceanographic issues, we have applied the ocean circulation model ROMBAX to ocean water masses adjacent to and underneath a number of idealized <span class="hlt">ice</span> shelf configurations: wide and narrow as well as laterally restrained and unrestrained <span class="hlt">ice</span> shelves. Simulations were performed with and without small <span class="hlt">ice</span> rises located close to the calving front. For larger configurations, the impact of the <span class="hlt">ice</span> rises on melt rates at the <span class="hlt">ice</span> shelf base is negligible, while for smaller configurations net melting rates at the <span class="hlt">ice</span>-shelf base differ by a factor of up to eight depending on whether <span class="hlt">ice</span> rises are considered or not. We employed the thermo-coupled <span class="hlt">ice</span> flow model TIM-FD3 to simulate the effects of several <span class="hlt">ice</span> rises and one <span class="hlt">ice</span> rumple on the dynamics of <span class="hlt">ice</span> shelf flow. We considered the complete un-grounding of the <span class="hlt">ice</span> shelf in order to investigate the effect of pinning points of different characteristics (interior or near calving front, small and medium sized) on the resulting flow and stress fields</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090030609','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090030609"><span>An <span class="hlt">Ice</span> Protection and Detection Systems Manufacturer's Perspective</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sweet, Dave</p> <p>2009-01-01</p> <p>Accomplishments include: World Class Aircraft <span class="hlt">Icing</span> Research Center and Facility. Primary Sponsor/Partner - Aircraft <span class="hlt">Icing</span> Consortia/Meetings. <span class="hlt">Icing</span> Research Tunnel. <span class="hlt">Icing</span> <span class="hlt">Test</span> Aircraft. <span class="hlt">Icing</span> Codes - LEWICE/Scaling, et al. Development of New Technologies (SBIR, STTR, et al). Example: Look Ahead <span class="hlt">Ice</span> Detection. Pilot Training Materials. Full Cooperation with Academia, Government and Industry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100040661','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100040661"><span><span class="hlt">Packing</span> Optimization of an Intentionally Stratified Sorbent Bed Containing Dissimilar Media Types</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kidd, Jessica; Guttromson, Jayleen; Holland, Nathan</p> <p>2010-01-01</p> <p>The Fire Cartridge is a <span class="hlt">packed</span> bed air filter with two different and separate layers of media designed to provide respiratory protection from combustion products after a fire event on the International Space Station (ISS). The first layer of media is a carbon monoxide catalyst made from gold nanoparticles dispersed on iron oxide. The second layer of media is universal carbon, commonly used in commercial respirator filters. Each layer must be optimally <span class="hlt">packed</span> to effectively remove contaminants from the air. Optimal <span class="hlt">packing</span> is achieved by vibratory agitations. However, if post-<span class="hlt">packing</span> movement of the media within the cartridge occurs, mixing of the bed layers, air voids, and channeling could cause preferential air flow and allow contaminants to pass. Several iterations of prototype fire cartridges were developed to reduce post-<span class="hlt">packing</span> movement of the media within each layer (settling), and to prevent mixing of the two media types. Both types of movement of the media contribute to decreased fire cartridge performance. Each iteration of the fire cartridge design was <span class="hlt">tested</span> to demonstrate mechanical loads required to cause detrimental movement within the bed, and resulting level of functionality of the media beds after movement was detected. In order to optimally <span class="hlt">pack</span> each layer, vertical, horizontal, and orbital agitations were <span class="hlt">tested</span> and a final <span class="hlt">packed</span> bulk density was calculated for each method. <span class="hlt">Packed</span> bulk density must be calculated for each lot of catalyst to accommodate variations in particle size, shape, and density. In addition, a physical divider sheet between each type of media was added within the fire cartridge design to further inhibit intermixing of the bed layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA180863','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA180863"><span>An Analytical Study of <span class="hlt">Icing</span> Similitude for Aircraft Engine <span class="hlt">Testing</span>. Revision</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1987-02-01</p> <p>MODELING GEOMETRIES Component Cowl Spinner Fan Blade Fan Stator Exit Vane Probe Approximating Geometry NACA 0012 Airfoil Sphere NACA 0012...DOT/FAA/CT·86/35 AEDC·TR·86·26 An Analytical Study of <span class="hlt">Icing</span> Similitude for Aircraft Engine <span class="hlt">Testing</span> c. Scott Bartlett Sverdrup Technology, Inc...8217~,feCa.ORI A n AnalYtical Study )f Icin~ Similitude for Aircraft Engine Tes t tu~ 12. PERSONAL AUTHOR/S) B a r t l e t t , C. Scot t , Sverdrup</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019574','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019574"><span>Rime-, mixed- and glaze-<span class="hlt">ice</span> evaluations of three scaling laws</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anderson, David N.</p> <p>1994-01-01</p> <p>This report presents the results of <span class="hlt">tests</span> at NASA Lewis to evaluate three <span class="hlt">icing</span> scaling relationships or 'laws' for an unheated model. The laws were LWC x time = constant, one proposed by a Swedish-Russian group and one used at ONERA in France. <span class="hlt">Icing</span> <span class="hlt">tests</span> were performed in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel (IRT) with cylinders ranging from 2.5- to 15.2-cm diameter. Reference conditions were chosen to provide rime, mixed and glaze <span class="hlt">ice</span>. Scaled conditions were <span class="hlt">tested</span> for several scenarios of size and velocity scaling, and the resulting <span class="hlt">ice</span> shapes compared. For rime-<span class="hlt">ice</span> conditions, all three of the scaling laws provided scaled <span class="hlt">ice</span> shapes which closely matched reference <span class="hlt">ice</span> shapes. For mixed <span class="hlt">ice</span> and for glaze <span class="hlt">ice</span> none of the scaling laws produced consistently good simulation of the reference <span class="hlt">ice</span> shapes. Explanations for the observed results are proposed, and scaling issues requiring further study are identified.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28753208','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28753208"><span><span class="hlt">Ice</span> nucleation active bacteria in precipitation are genetically diverse and nucleate <span class="hlt">ice</span> by employing different mechanisms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Failor, K C; Schmale, D G; Vinatzer, B A; Monteil, C L</p> <p>2017-12-01</p> <p>A growing body of circumstantial evidence suggests that <span class="hlt">ice</span> nucleation active (<span class="hlt">Ice</span> + ) bacteria contribute to the initiation of precipitation by heterologous freezing of super-cooled water in clouds. However, little is known about the concentration of <span class="hlt">Ice</span> + bacteria in precipitation, their genetic and phenotypic diversity, and their relationship to air mass trajectories and precipitation chemistry. In this study, 23 precipitation events were collected over 15 months in Virginia, USA. Air mass trajectories and water chemistry were determined and 33 134 isolates were screened for <span class="hlt">ice</span> nucleation activity (INA) at -8 °C. Of 1144 isolates that <span class="hlt">tested</span> positive during initial screening, 593 had confirmed INA at -8 °C in repeated <span class="hlt">tests</span>. Concentrations of <span class="hlt">Ice</span> + strains in precipitation were found to range from 0 to 13 219 colony forming units per liter, with a mean of 384±147. Most <span class="hlt">Ice</span> + bacteria were identified as members of known and unknown <span class="hlt">Ice</span> + species in the Pseudomonadaceae, Enterobacteriaceae and Xanthomonadaceae families, which nucleate <span class="hlt">ice</span> employing the well-characterized membrane-bound INA protein. Two <span class="hlt">Ice</span> + strains, however, were identified as Lysinibacillus, a Gram-positive genus not previously known to include <span class="hlt">Ice</span> + bacteria. INA of the Lysinibacillus strains is due to a nanometer-sized molecule that is heat resistant, lysozyme and proteinase resistant, and secreted. <span class="hlt">Ice</span> + bacteria and the INA mechanisms they employ are thus more diverse than expected. We discuss to what extent the concentration of culturable <span class="hlt">Ice</span> + bacteria in precipitation and the identification of a new heat-resistant biological INA mechanism support a role for <span class="hlt">Ice</span> + bacteria in the initiation of precipitation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2774433','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2774433"><span>Relating protein conformational changes to <span class="hlt">packing</span> efficiency and disorder</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bhardwaj, Nitin; Gerstein, Mark</p> <p>2009-01-01</p> <p> that between the two conformations, the cores of the proteins remain mostly intact, whereas the interfaces display the most elasticity, both in terms of disorder and change in <span class="hlt">packing</span> efficiency. By doing a variety of <span class="hlt">tests</span>, we also show that our observations are robust to the solvation state of the proteins. PMID:19472340</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED187850.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED187850.pdf"><span>Career Action <span class="hlt">Pack</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Blum, Robert E.; Raymond, Carolyn D.</p> <p></p> <p>One of five McDonald's Action <span class="hlt">Packs</span>, these instructional materials for ninth and tenth graders (and more able sixth and seventh graders) have incorporated ideas around three career development goals--subject relevance, career awareness, and self-awareness. The action <span class="hlt">pack</span> contains six units--three units each in the subject areas of language arts…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994ESRv...36...59R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994ESRv...36...59R"><span>Particle <span class="hlt">packing</span> from an earth science viewpoint</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rogers, C. D. F.; Dijkstra, T. A.; Smalley, I. J.</p> <p>1994-04-01</p> <p>Particle <span class="hlt">packings</span> are relevant to many aspects of the Earth sciences, and there is a long history of the study of <span class="hlt">packings</span> from an Earth science viewpoint. <span class="hlt">Packings</span> have also been studied in connection with other subjects and disciplines. Allen (1982) produced a major review which provides a solid base for Earth science related studies. This review complements Allen's work and in particular focuses on advances in the study of random <span class="hlt">packings</span> over the last ten years. Transitions from <span class="hlt">packing</span> to <span class="hlt">packing</span> may be as important as the <span class="hlt">packings</span> themselves, and possibly easier to model. This paper places emphasis on certain neglected works, in particular Morrow and Graves (1969) and the <span class="hlt">packing</span> transition envelope, Kahn (1956) and the measurement of <span class="hlt">packing</span> parameters, Griffiths (1962) on <span class="hlt">packings</span> in one-dimension, and Getis and Boots (1978) on <span class="hlt">packings</span> in two dimensions. Certain <span class="hlt">packing</span> problems are relevant to current areas of study including structure collapse in loess (hydroconsolidation), flowslides in very sensitive soils, wind erosion, jewel quality in opals and the structure and functions of sand dunes. The region where interparticle forces become active (particles < 200 μm) is considered and the implications for <span class="hlt">packing</span> are examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JTST...26..150K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JTST...26..150K"><span>Anti-<span class="hlt">icing</span> Behavior of Thermally Sprayed Polymer Coatings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koivuluoto, Heli; Stenroos, Christian; Kylmälahti, Mikko; Apostol, Marian; Kiilakoski, Jarkko; Vuoristo, Petri</p> <p>2017-01-01</p> <p>Surface engineering shows an increasing potential to provide a sustainable approach to <span class="hlt">icing</span> problems. Currently, several passive anti-<span class="hlt">ice</span> properties adoptable to coatings are known, but further research is required to proceed for practical applications. This is due to the fact that <span class="hlt">icing</span> reduces safety, operational tempo, productivity and reliability of logistics, industry and infrastructure. An <span class="hlt">icing</span> wind tunnel and a centrifugal <span class="hlt">ice</span> adhesion <span class="hlt">test</span> equipment can be used to evaluate and develop anti-<span class="hlt">icing</span> and icephobic coatings for a potential use in various arctic environments, e.g., in wind power generation, oil drilling, mining and logistic industries. The present study deals with evaluation of <span class="hlt">icing</span> properties of flame-sprayed polyethylene (PE)-based polymer coatings. In the laboratory-scale <span class="hlt">icing</span> <span class="hlt">tests</span>, thermally sprayed polymer coatings showed low <span class="hlt">ice</span> adhesion compared with metals such as aluminum and stainless steel. The <span class="hlt">ice</span> adhesion strength of the flame-sprayed PE coating was found to have approximately seven times lower <span class="hlt">ice</span> adhesion values compared with metallic aluminum, indicating a very promising anti-<span class="hlt">icing</span> behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010124078','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010124078"><span>Towards GPS Surface Reflection Remote Sensing of Sea <span class="hlt">Ice</span> Conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Komjathy, A.; Maslanik, J. A.; Zavorotny, V. U.; Axelrad, P.; Katzberg, S. J.</p> <p>2000-01-01</p> <p>This paper describes the research to extend the application of Global Positioning System (GPS) signal reflections, received by airborne instruments, to cryospheric remote sensing. The characteristics of the GPS signals and equipment afford the possibility of new measurements not possible with existing radar and passive microwave systems. In particular, the GPS receiving systems are small and light-weight, and as such are particularly well suited to be deployed on small aircraft or satellite platforms with minimal impact. Our preliminary models and experimental results indicate that reflected GPS signals have potential to provide information on the presence and condition of sea and fresh-water <span class="hlt">ice</span> as well as the freeze/thaw state of frozen ground. In this paper we show results from aircraft experiments over the <span class="hlt">ice</span> <span class="hlt">pack</span> near Barrow, Alaska suggesting correlation between forward scattered GPS returns and RADARSAT backscattered signals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.C21C0622M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.C21C0622M"><span>Meteorological conditions influencing the formation of level <span class="hlt">ice</span> within the Baltic Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazur, A. K.; Krezel, A.</p> <p>2012-12-01</p> <p>The Baltic Sea is covered by <span class="hlt">ice</span> every winter and on average, the <span class="hlt">ice</span>-covered area is 45% of the total area of the Baltic Sea. The beginning of <span class="hlt">ice</span> season usually starts in the end of November, <span class="hlt">ice</span> extent is the largest between mid-February and mid-March and sea <span class="hlt">ice</span> disappears completely in May. The <span class="hlt">ice</span> covered areas during a typical winter are the Gulf of Bothnia, the Gulf of Finland and the Gulf of Riga. The studies of sea <span class="hlt">ice</span> in the Baltic Sea are related to two aspects: climate and marine transport. Depending on the local weather conditions during the winter different types of sea <span class="hlt">ice</span> can be formed. From the point of winter shipping it is important to locate level and deformed <span class="hlt">ice</span> areas (rafted <span class="hlt">ice</span>, ridged <span class="hlt">ice</span>, and hummocked <span class="hlt">ice</span>). Because of cloud and daylight independency as well as good spatial resolution, SAR data seems to be the most suitable source of data for sea <span class="hlt">ice</span> observation in the comparatively small area of the Baltic Sea. We used ASAR Wide Swath Mode data with spatial resolution 150 m. We analyzed data from the three winter seasons which were examples of severe, typical and mild winters. To remove the speckle effect the data were resampled to 250 m pixel size and filtred using Frost filter 5x5. To detect edges we used Sobel filter. The data were also converted into grayscale. Sea <span class="hlt">ice</span> classification was based on Object-Based Image Analysis (OBIA). Object-based methods are not a common tool in sea <span class="hlt">ice</span> studies but they seem to accurately separate level <span class="hlt">ice</span> within the <span class="hlt">ice</span> <span class="hlt">pack</span>. The data were segmented and classified using eCognition Developer software. Level <span class="hlt">ice</span> were classified based on texture features defined by Haralick (Grey Level Co-Occurrence Matrix homogeneity, GLCM contrast, GLCM entropy and GLCM correlation). The long-term changes of the Baltic Sea <span class="hlt">ice</span> conditions have been already studied. They include date of freezing, date of break-up, sea <span class="hlt">ice</span> extent and some of work also <span class="hlt">ice</span> thickness. There is a little knowledge about the relationship of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C23D..04M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C23D..04M"><span>Role of <span class="hlt">ice</span> sheet dynamics in the collapse of the early-Holocene Laurentide <span class="hlt">Ice</span> Sheet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matero, I. S. O.; Gregoire, L. J.; Cornford, S. L.; Ivanovic, R. F.</p> <p>2017-12-01</p> <p>The last stage of the deglaciation of the Laurentide <span class="hlt">Ice</span> Sheet (LIS) during the early Holocene Thermal Maximum ( 9000 to 7000 years ago) provides an analogy and insight to the possible responses of contemporary <span class="hlt">ice</span> sheets in a warming climate. What makes LIS particularly interesting is that meltwater from the collapse of an <span class="hlt">ice</span> saddle over Hudson Bay was recently shown to be the primary forcing for the period of abrupt northern hemisphere cooling known as the 8.2 ka event. The evolution of the LIS during this period was likely influenced by its interaction with marginal lakes and the ocean, and its major <span class="hlt">ice</span> stream, which exported <span class="hlt">ice</span> towards Hudson Strait. Accurately simulating the early Holocene LIS evolution thus requires a model such as BISICLES, capable of accurately and efficiently resolving <span class="hlt">ice</span> stream dynamics and grounding line migration thanks to the combined use of higher order physics and adaptive mesh refinement. We drive the BISICLES model using a positive degree day mass balance scheme with monthly precipitation and temperature from the HadCM3 climate model under climatic conditions from 10,000 to 8,000 years ago. We <span class="hlt">test</span> the effect of varying the initial topographies and <span class="hlt">ice</span> thicknesses from different timeslices in the <span class="hlt">ICE</span>-6Gc reconstruction. We also <span class="hlt">test</span> different parameterisations for the basal friction based on the thicknesses of the underlying sediments. These simulations evaluate the role of the Hudson Strait <span class="hlt">ice</span> stream, <span class="hlt">ice</span> sheet dynamics and interactions with the adjacent proglacial Lake Agassiz and North Atlantic Ocean in the collapse of the LIS. Our results highlight that the choice of parameterisation for basal friction has major effects on <span class="hlt">ice</span> sheet dynamics and evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C33C1202F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C33C1202F"><span>Determination of a Critical Sea <span class="hlt">Ice</span> Thickness Threshold for the Central Arctic Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ford, V.; Frauenfeld, O. W.; Nowotarski, C. J.</p> <p>2017-12-01</p> <p>While sea <span class="hlt">ice</span> extent is readily measurable from satellite observations and can be used to assess the overall survivability of the Arctic sea <span class="hlt">ice</span> <span class="hlt">pack</span>, determining the spatial variability of sea <span class="hlt">ice</span> thickness remains a challenge. Turbulent and conductive heat fluxes are extremely sensitive to <span class="hlt">ice</span> thickness but are dominated by the sensible heat flux, with energy exchange expected to increase with thinner <span class="hlt">ice</span> cover. Fluxes over open water are strongest and have the greatest influence on the atmosphere, while fluxes over thick sea <span class="hlt">ice</span> are minimal as heat conduction from the ocean through thick <span class="hlt">ice</span> cannot reach the atmosphere. We know that turbulent energy fluxes are strongest over open ocean, but is there a "critical thickness of <span class="hlt">ice</span>" where fluxes are considered non-negligible? Through polar-optimized Weather Research and Forecasting model simulations, this study assesses how the wintertime Arctic surface boundary layer, via sensible heat flux exchange and surface air temperature, responds to sea <span class="hlt">ice</span> thinning. The region immediately north of Franz Josef Land is characterized by a thickness gradient where sea <span class="hlt">ice</span> transitions from the thickest multi-year <span class="hlt">ice</span> to the very thin marginal <span class="hlt">ice</span> seas. This provides an ideal location to simulate how the diminishing Arctic sea <span class="hlt">ice</span> interacts with a warming atmosphere. Scenarios include both fixed sea surface temperature domains for idealized thickness variability, and fixed <span class="hlt">ice</span> fields to detect changes in the ocean-<span class="hlt">ice</span>-atmosphere energy exchange. Results indicate that a critical thickness threshold exists below 1 meter. The threshold is between 0.4-1 meters thinner than the critical thickness for melt season survival - the difference between first year and multi-year <span class="hlt">ice</span>. Turbulent heat fluxes and surface air temperature increase as sea <span class="hlt">ice</span> thickness transitions from perennial <span class="hlt">ice</span> to seasonal <span class="hlt">ice</span>. While models predict a sea <span class="hlt">ice</span> free Arctic at the end of the warm season in future decades, sea <span class="hlt">ice</span> will continue to transform</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990084033&hterms=divergent+series&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Ddivergent%2Bseries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990084033&hterms=divergent+series&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Ddivergent%2Bseries"><span>C-Band Backscatter Measurements of Winter Sea-<span class="hlt">Ice</span> in the Weddell Sea, Antarctica</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Drinkwater, M. R.; Hosseinmostafa, R.; Gogineni, P.</p> <p>1995-01-01</p> <p>During the 1992 Winter Weddell Gyre Study, a C-band scatterometer was used from the German <span class="hlt">ice</span>-breaker R/V Polarstern to obtain detailed shipborne measurement scans of Antarctic sea-<span class="hlt">ice</span>. The frequency-modulated continuous-wave (FM-CW) radar operated at 4-3 GHz and acquired like- (VV) and cross polarization (HV) data at a variety of incidence angles (10-75 deg). Calibrated backscatter data were recorded for several <span class="hlt">ice</span> types as the icebreaker crossed the Weddell Sea and detailed measurements were made of corresponding snow and sea-<span class="hlt">ice</span> characteristics at each measurement site, together with meteorological information, radiation budget and oceanographic data. The primary scattering contributions under cold winter conditions arise from the air/snow and snow/<span class="hlt">ice</span> interfaces. Observations indicate so e similarities with Arctic sea-<span class="hlt">ice</span> scattering signatures, although the main difference is generally lower mean backscattering coefficients in the Weddell Sea. This is due to the younger mean <span class="hlt">ice</span> age and thickness, and correspondingly higher mean salinities. In particular, smooth white <span class="hlt">ice</span> found in 1992 in divergent areas within the Weddell Gyre <span class="hlt">ice</span> <span class="hlt">pack</span> was generally extremely smooth and undeformed. Comparisons of field scatterometer data with calibrated 20-26 deg incidence ERS-1 radar image data show close correspondence, and indicate that rough Antarctic first-year and older second-year <span class="hlt">ice</span> forms do not produce as distinctively different scattering signatures as observed in the Arctic. Thick deformed first-year and second-year <span class="hlt">ice</span> on the other hand are clearly discriminated from younger undeformed <span class="hlt">ice</span>. thereby allowing successful separation of thick and thin <span class="hlt">ice</span>. Time-series data also indicate that C-band is sensitive to changes in snow and <span class="hlt">ice</span> conditions resulting from atmospheric and oceanographic forcing and the local heat flux environment. Variations of several dB in 45 deg incidence backscatter occur in response to a combination of thermally-regulated parameters</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RSPTA.37550354S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RSPTA.37550354S"><span>Micromechanics of sea <span class="hlt">ice</span> frictional slip from <span class="hlt">test</span> basin scale experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sammonds, Peter R.; Hatton, Daniel C.; Feltham, Daniel L.</p> <p>2017-02-01</p> <p>We have conducted a series of high-resolution friction experiments on large floating saline <span class="hlt">ice</span> floes in an environmental <span class="hlt">test</span> basin. In these experiments, a central <span class="hlt">ice</span> floe was pushed between two other floes, sliding along two interfacial faults. The frictional motion was predominantly stick-slip. Shear stresses, normal stresses, local strains and slip displacement were measured along the sliding faults, and acoustic emissions were monitored. High-resolution measurements during a single stick-slip cycle at several positions along the fault allowed us to identify two phases of frictional slip: a nucleation phase, where a nucleation zone begins to slip before the rest of the fault, and a propagation phase when the entire fault is slipping. This is slip-weakening behaviour. We have therefore characterized what we consider to be a key deformation mechanism in Arctic Ocean dynamics. In order to understand the micromechanics of sea <span class="hlt">ice</span> friction, we have employed a theoretical constitutive relation (i.e. an equation for shear stress in terms of temperature, normal load, acceleration, velocity and slip displacement) derived from the physics of asperity-asperity contact and sliding (Hatton et al. 2009 Phil. Mag. 89, 2771-2799 (doi:10.1080/14786430903113769)). We find that our experimental data conform reasonably with this frictional law once slip weakening is introduced. We find that the constitutive relation follows Archard's law rather than Amontons' law, with ? (where τ is the shear stress and σn is the normal stress) and n = 26/27, with a fractal asperity distribution, where the frictional shear stress, τ = ffractal Tmlws, where ffractal is the fractal asperity height distribution, Tml is the shear strength for frictional melting and lubrication and ws is the slip weakening. We can therefore deduce that the interfacial faults failed in shear for these experimental conditions through processes of brittle failure of asperities in shear, and, at higher velocities</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030054467','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030054467"><span><span class="hlt">Iced</span> Aircraft Flight Data for Flight Simulator Validation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ratvasky, Thomas P.; Blankenship, Kurt; Rieke, William; Brinker, David J.</p> <p>2003-01-01</p> <p>NASA is developing and validating technology to incorporate aircraft <span class="hlt">icing</span> effects into a flight training device concept demonstrator. Flight simulation models of a DHC-6 Twin Otter were developed from wind tunnel data using a subscale, complete aircraft model with and without simulated <span class="hlt">ice</span>, and from previously acquired flight data. The validation of the simulation models required additional aircraft response time histories of the airplane configured with simulated <span class="hlt">ice</span> similar to the subscale model <span class="hlt">testing</span>. Therefore, a flight <span class="hlt">test</span> was conducted using the NASA Twin Otter <span class="hlt">Icing</span> Research Aircraft. Over 500 maneuvers of various types were conducted in this flight <span class="hlt">test</span>. The validation data consisted of aircraft state parameters, pilot inputs, propulsion, weight, center of gravity, and moments of inertia with the airplane configured with different amounts of simulated <span class="hlt">ice</span>. Emphasis was made to acquire data at wing stall and tailplane stall since these events are of primary interest to model accurately in the flight training device. Analyses of several datasets are described regarding wing and tailplane stall. Key findings from these analyses are that the simulated wing <span class="hlt">ice</span> shapes significantly reduced the C , max, while the simulated tail <span class="hlt">ice</span> caused elevator control force anomalies and tailplane stall when flaps were deflected 30 deg or greater. This effectively reduced the safe operating margins between <span class="hlt">iced</span> wing and <span class="hlt">iced</span> tail stall as flap deflection and thrust were increased. This flight <span class="hlt">test</span> demonstrated that the critical aspects to be modeled in the <span class="hlt">icing</span> effects flight training device include: <span class="hlt">iced</span> wing and tail stall speeds, flap and thrust effects, control forces, and control effectiveness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.4193S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.4193S"><span>Trend analysis of Arctic sea <span class="hlt">ice</span> extent</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Silva, M. E.; Barbosa, S. M.; Antunes, Luís; Rocha, Conceição</p> <p>2009-04-01</p> <p>The extent of Arctic sea <span class="hlt">ice</span> is a fundamental parameter of Arctic climate variability. In the context of climate change, the area covered by <span class="hlt">ice</span> in the Arctic is a particularly useful indicator of recent changes in the Arctic environment. Climate models are in near universal agreement that Arctic sea <span class="hlt">ice</span> extent will decline through the 21st century as a consequence of global warming and many studies predict a <span class="hlt">ice</span> free Arctic as soon as 2012. Time series of satellite passive microwave observations allow to assess the temporal changes in the extent of Arctic sea <span class="hlt">ice</span>. Much of the analysis of the <span class="hlt">ice</span> extent time series, as in most climate studies from observational data, have been focussed on the computation of deterministic linear trends by ordinary least squares. However, many different processes, including deterministic, unit root and long-range dependent processes can engender trend like features in a time series. Several parametric <span class="hlt">tests</span> have been developed, mainly in econometrics, to discriminate between stationarity (no trend), deterministic trend and stochastic trends. Here, these <span class="hlt">tests</span> are applied in the trend analysis of the sea <span class="hlt">ice</span> extent time series available at National Snow and <span class="hlt">Ice</span> Data Center. The parametric stationary <span class="hlt">tests</span>, Augmented Dickey-Fuller (ADF), Phillips-Perron (PP) and the KPSS, do not support an overall deterministic trend in the time series of Arctic sea <span class="hlt">ice</span> extent. Therefore, alternative parametrizations such as long-range dependence should be considered for characterising long-term Arctic sea <span class="hlt">ice</span> variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870008688','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870008688"><span>Structural properties of impact <span class="hlt">ices</span> accreted on aircraft structures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scavuzzo, R. J.; Chu, M. L.</p> <p>1987-01-01</p> <p>The structural properties of <span class="hlt">ice</span> accretions formed on aircraft surfaces are studied. The overall objectives are to measure basic structural properties of impact <span class="hlt">ices</span> and to develop finite element analytical procedures for use in the design of all deicing systems. The <span class="hlt">Icing</span> Research Tunnel (IRT) was used to produce simulated natural <span class="hlt">ice</span> accretion over a wide range of <span class="hlt">icing</span> conditions. Two different <span class="hlt">test</span> apparatus were used to measure each of the three basic mechanical properties: tensile, shear, and peeling. Data was obtained on both adhesive shear strength of impact <span class="hlt">ices</span> and peeling forces for various <span class="hlt">icing</span> conditions. The influences of various <span class="hlt">icing</span> parameters such as tunnel air temperature and velocity, <span class="hlt">icing</span> cloud drop size, material substrate, surface temperature at <span class="hlt">ice</span>/material interface, and <span class="hlt">ice</span> thickness were studied. A finite element analysis of the shear <span class="hlt">test</span> apparatus was developed in order to gain more insight in the evaluation of the <span class="hlt">test</span> data. A comparison with other investigators was made. The result shows that the adhesive shear strength of impact <span class="hlt">ice</span> typically varies between 40 and 50 psi, with peak strength reaching 120 psi and is not dependent on the kind of substrate used, the thickness of accreted <span class="hlt">ice</span>, and tunnel temperature below 4 C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19888714','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19888714"><span><span class="hlt">Ice</span> nucleation onto Arizona <span class="hlt">test</span> dust at cirrus temperatures: effect of temperature and aerosol size on onset relative humidity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kanji, Z A; Abbatt, J P D</p> <p>2010-01-21</p> <p>The University of Toronto Continuous Flow Diffusion Chamber (UT-CFDC) was used to study <span class="hlt">ice</span> formation onto monodisperse Arizona <span class="hlt">Test</span> Dust (ATD) particles. The onset relative humidity with respect to <span class="hlt">ice</span> (RH(i)) was measured as a function of temperature in the range 251-223 K for 100 nm ATD particles. It was found that for 0.1% of the particles to freeze, water saturation was required at all temperatures except 223 K where particles activated at RH(i) below water saturation. At this temperature, where deposition mode freezing is occurring, we find that the larger the particle size, the lower the onset RH(i). We also demonstrate that the total number of particles present may influence the onset RH(i) observed. The surface area for <span class="hlt">ice</span> activation, aerosol size, and temperature must all be considered when reporting onset values of <span class="hlt">ice</span> formation onto ATD mineral dust particles. In addition, we calculate nucleation rates and contact angles of <span class="hlt">ice</span> germs with ATD aerosols which indicate that there exists a range of active sites on the surface with different efficiencies for activating <span class="hlt">ice</span> formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009fpc..book..407I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009fpc..book..407I"><span>Fully Dynamic Bin <span class="hlt">Packing</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivković, Zoran; Lloyd, Errol L.</p> <p></p> <p>Classic bin <span class="hlt">packing</span> seeks to <span class="hlt">pack</span> a given set of items of possibly varying sizes into a minimum number of identical sized bins. A number of approximation algorithms have been proposed for this NP-hard problem for both the on-line and off-line cases. In this chapter we discuss fully dynamic bin <span class="hlt">packing</span>, where items may arrive (Insert) and depart (Delete) dynamically. In accordance with standard practice for fully dynamic algorithms, it is assumed that the <span class="hlt">packing</span> may be arbitrarily rearranged to accommodate arriving and departing items. The goal is to maintain an approximately optimal solution of provably high quality in a total amount of time comparable to that used by an off-line algorithm delivering a solution of the same quality.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA112582','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA112582"><span>Limited Artificial and Natural <span class="hlt">Icing</span> <span class="hlt">Tests</span> Production UH-60A Helicopter (Re-Evaluation).</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1981-08-01</p> <p>parameters , and definitions of <span class="hlt">icing</span> types and severities are presented in appendix D. 2 RESULTS AND DISCUSSION GENERAL 9. Artificial and natural <span class="hlt">icing</span> flight...anti-<span class="hlt">ice</span> off, the system may be reactivated by cycling the appropriate windshield anti-<span class="hlt">ice</span> switch. The windshield anti-<span class="hlt">ice</span> system is fully operational...is off, then the fault monitor illuminates the respective PWR light on its front panel. The light informs the crew that further action is requied to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAMES...9..854K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAMES...9..854K"><span>LIVVkit: An extensible, python-based, land <span class="hlt">ice</span> verification and validation toolkit for <span class="hlt">ice</span> sheet models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kennedy, Joseph H.; Bennett, Andrew R.; Evans, Katherine J.; Price, Stephen; Hoffman, Matthew; Lipscomb, William H.; Fyke, Jeremy; Vargo, Lauren; Boghozian, Adrianna; Norman, Matthew; Worley, Patrick H.</p> <p>2017-06-01</p> <p>To address the pressing need to better understand the behavior and complex interaction of <span class="hlt">ice</span> sheets within the global Earth system, significant development of continental-scale, dynamical <span class="hlt">ice</span> sheet models is underway. Concurrent to the development of the Community <span class="hlt">Ice</span> Sheet Model (CISM), the corresponding verification and validation (V&V) process is being coordinated through a new, robust, Python-based extensible software package, the Land <span class="hlt">Ice</span> Verification and Validation toolkit (LIVVkit). Incorporated into the typical <span class="hlt">ice</span> sheet model development cycle, it provides robust and automated numerical verification, software verification, performance validation, and physical validation analyses on a variety of platforms, from personal laptops to the largest supercomputers. LIVVkit operates on sets of regression <span class="hlt">test</span> and reference data sets, and provides comparisons for a suite of community prioritized <span class="hlt">tests</span>, including configuration and parameter variations, bit-for-bit evaluation, and plots of model variables to indicate where differences occur. LIVVkit also provides an easily extensible framework to incorporate and analyze results of new intercomparison projects, new observation data, and new computing platforms. LIVVkit is designed for quick adaptation to additional <span class="hlt">ice</span> sheet models via abstraction of model specific code, functions, and configurations into an <span class="hlt">ice</span> sheet model description bundle outside the main LIVVkit structure. Ultimately, through shareable and accessible analysis output, LIVVkit is intended to help developers build confidence in their models and enhance the credibility of <span class="hlt">ice</span> sheet models overall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://dx.doi.org/10.1016/S0163-1047(80)91932-9','USGSPUBS'); return false;" href="http://dx.doi.org/10.1016/S0163-1047(80)91932-9"><span>Sleeping distance in wild wolf <span class="hlt">packs</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Knick, S.T.; Mech, L.D.</p> <p>1980-01-01</p> <p>Sleeping distances were observed among members of 13 wild wolf (Canis lupus) <span class="hlt">packs</span> and 11 pairs in northeastern Minnesota to determine if the distances correlated with <span class="hlt">pack</span> size and composition. The study utilized aerial radio-tracking and observation during winter. <span class="hlt">Pack</span> size and number of adults per <span class="hlt">pack</span> were inversely related to <span class="hlt">pack</span> average sleeping distance and variability. No correlation between sleeping distance and microclimate was observed. Possible relationships between social bonding and our results are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27216342','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27216342"><span>Electrocauterization and no <span class="hlt">packing</span> may be comparable with nasal <span class="hlt">packing</span> for postoperative hemorrhage after endoscopic sinus surgery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Dong-Kyu; Rhee, Chae Seo; Kim, Jeong-Whun</p> <p>2016-05-01</p> <p>Nasal <span class="hlt">packing</span> is commonly performed after functional endoscopic sinus surgery (FESS). However, nasal <span class="hlt">packing</span> is associated with higher cost (owing to the cost of <span class="hlt">packing</span> materials), patient discomfort, delayed wound healing, and concern about toxic shock syndrome. Some surgeons have been performing FESS without <span class="hlt">packing</span>, but there are few studies that show its safety. The purpose of this study was to evaluate the safety of electrocauterization and no <span class="hlt">packing</span>. A total of 490 patients who underwent bilateral FESS for chronic rhinosinusitis were included in this retrospective study, 242 in the nasal <span class="hlt">packing</span> group and 248 in the electrocauterization and no-<span class="hlt">packing</span> group. Electrocauterization was performed by using a suction coagulator. Rates of immediate (first 24 hours after surgery) and delayed postoperative bleeding were compared. Patient characteristics, including concomitant disease and medication history, and Lund-Mackay computed tomography score were also assessed Results: There were no significant differences in age; sex; Lund-Mackay score; use of anticoagulant drugs; or prevalence of hypertension, diabetes, or asthma between the two groups. In the electrocauterization and no-<span class="hlt">packing</span> group, there were fewer patients with allergic rhinitis and more smokers. Primary bleeding did not occur in the nasal <span class="hlt">packing</span> group, but 11 patients (4.4%) had delayed bleeding. Primary bleeding occurred in four patients (1.7%) in the electrocauterization and no-<span class="hlt">packing</span> group, and five patients (2.1%) had delayed bleeding. There were no significant differences in primary (p = 0.058) and secondary bleeding (p = 0.142) between the two groups. All bleeding was minor and easily controlled. Multivariate logistic regression analysis ruled out significant correlation between no <span class="hlt">packing</span> and postoperative bleeding. This study provided evidence that, in terms of postoperative hemorrhage, the safety of the electrocauterization and no-<span class="hlt">packing</span> technique after FESS was comparable with that of</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JCHyd.164..230F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JCHyd.164..230F"><span>Consideration of grain <span class="hlt">packing</span> in granular iron treatability studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Firdous, R.; Devlin, J. F.</p> <p>2014-08-01</p> <p>Commercial granular iron (GI) is light steel that is used in Permeable Reactive Barriers (PRBs). Investigations into the reactivity of GI have focused on its chemical nature and relatively little direct work has been done to account for the effects of grain shape and <span class="hlt">packing</span>. Both of these factors are expected to influence available grain surface area, which is known to correlate to reactivity. Commercial granular iron grains are platy and therefore <span class="hlt">pack</span> in preferential orientations that could affect solution access to the surface. Three <span class="hlt">packing</span> variations were investigated using Connelly Iron and trichloroethylene (TCE). Experimental kinetic data showed reaction rates 2-4 times higher when grains were <span class="hlt">packed</span> with long axes preferentially parallel to flow (VP) compared to <span class="hlt">packings</span> with long axes preferentially perpendicular to flow (HP) or randomly arranged (RP). The variations were found to be explainable by variations in reactive sorption capacities, i.e., sorption to sites where chemical transformations took place. The possibility that the different reactive sorption capacities were related to physical pore-scale differences was assessed by conducting an image analysis of the pore structure of sectioned columns. The analyses suggested that pore-scale factors - in particular the grain surface availability, reflected in the sorption capacity terms of the kinetic model used - could only account for a fraction of the observed reactivity differences between <span class="hlt">packing</span> types. It is concluded that <span class="hlt">packing</span> does affect observable reaction rates but that micro-scale features on the grain surfaces, rather than the pore scale characteristics, account for most of the apparent reactivity differences. This result suggests that treatability <span class="hlt">tests</span> should consider the <span class="hlt">packing</span> of columns carefully if they are to mimic field performance of PRBs to the greatest extent possible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol2/pdf/CFR-2014-title7-vol2-sec51-310.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol2/pdf/CFR-2014-title7-vol2-sec51-310.pdf"><span>7 CFR 51.310 - <span class="hlt">Packing</span> requirements.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... (INSPECTION, CERTIFICATION, AND STANDARDS) United States Standards for Grades of Apples <span class="hlt">Packing</span> Requirements § 51.310 <span class="hlt">Packing</span> requirements. (a) Apples tray <span class="hlt">packed</span> or cell <span class="hlt">packed</span> in cartons shall be arranged.... 3 2 “Fairly tight” means that apples are of the proper size for molds or cell compartments in which...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol2/pdf/CFR-2013-title7-vol2-sec51-310.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol2/pdf/CFR-2013-title7-vol2-sec51-310.pdf"><span>7 CFR 51.310 - <span class="hlt">Packing</span> requirements.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... (INSPECTION, CERTIFICATION, AND STANDARDS) United States Standards for Grades of Apples <span class="hlt">Packing</span> Requirements § 51.310 <span class="hlt">Packing</span> requirements. (a) Apples tray <span class="hlt">packed</span> or cell <span class="hlt">packed</span> in cartons shall be arranged.... 3 2 “Fairly tight” means that apples are of the proper size for molds or cell compartments in which...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4653172','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4653172"><span>Producing desired <span class="hlt">ice</span> faces</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shultz, Mary Jane; Brumberg, Alexandra; Bisson, Patrick J.; Shultz, Ryan</p> <p>2015-01-01</p> <p>The ability to prepare single-crystal faces has become central to developing and <span class="hlt">testing</span> models for chemistry at interfaces, spectacularly demonstrated by heterogeneous catalysis and nanoscience. This ability has been hampered for hexagonal <span class="hlt">ice</span>, Ih––a fundamental hydrogen-bonded surface––due to two characteristics of <span class="hlt">ice</span>: <span class="hlt">ice</span> does not readily cleave along a crystal lattice plane and properties of <span class="hlt">ice</span> grown on a substrate can differ significantly from those of neat <span class="hlt">ice</span>. This work describes laboratory-based methods both to determine the Ih crystal lattice orientation relative to a surface and to use that orientation to prepare any desired face. The work builds on previous results attaining nearly 100% yield of high-quality, single-crystal boules. With these methods, researchers can prepare authentic, single-crystal <span class="hlt">ice</span> surfaces for numerous studies including uptake measurements, surface reactivity, and catalytic activity of this ubiquitous, fundamental solid. PMID:26512102</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26347538','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26347538"><span>Processes controlling surface, bottom and lateral melt of Arctic sea <span class="hlt">ice</span> in a state of the art sea <span class="hlt">ice</span> model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tsamados, Michel; Feltham, Daniel; Petty, Alek; Schroeder, David; Flocco, Daniela</p> <p>2015-10-13</p> <p>We present a modelling study of processes controlling the summer melt of the Arctic sea <span class="hlt">ice</span> cover. We perform a sensitivity study and focus our interest on the thermodynamics at the <span class="hlt">ice</span>-atmosphere and <span class="hlt">ice</span>-ocean interfaces. We use the Los Alamos community sea <span class="hlt">ice</span> model CICE, and additionally implement and <span class="hlt">test</span> three new parametrization schemes: (i) a prognostic mixed layer; (ii) a three equation boundary condition for the salt and heat flux at the <span class="hlt">ice</span>-ocean interface; and (iii) a new lateral melt parametrization. Recent additions to the CICE model are also <span class="hlt">tested</span>, including explicit melt ponds, a form drag parametrization and a halodynamic brine drainage scheme. The various sea <span class="hlt">ice</span> parametrizations <span class="hlt">tested</span> in this sensitivity study introduce a wide spread in the simulated sea <span class="hlt">ice</span> characteristics. For each simulation, the total melt is decomposed into its surface, bottom and lateral melt components to assess the processes driving melt and how this varies regionally and temporally. Because this study quantifies the relative importance of several processes in driving the summer melt of sea <span class="hlt">ice</span>, this work can serve as a guide for future research priorities. © 2015 The Author(s).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28518108','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28518108"><span>Identification of Plant <span class="hlt">Ice</span>-binding Proteins Through Assessment of <span class="hlt">Ice</span>-recrystallization Inhibition and Isolation Using <span class="hlt">Ice</span>-affinity Purification.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bredow, Melissa; Tomalty, Heather E; Walker, Virginia K</p> <p>2017-05-05</p> <p><span class="hlt">Ice</span>-binding proteins (IBPs) belong to a family of stress-induced proteins that are synthesized by certain organisms exposed to subzero temperatures. In plants, freeze damage occurs when extracellular <span class="hlt">ice</span> crystals grow, resulting in the rupture of plasma membranes and possible cell death. Adsorption of IBPs to <span class="hlt">ice</span> crystals restricts further growth by a process known as <span class="hlt">ice</span>-recrystallization inhibition (IRI), thereby reducing cellular damage. IBPs also demonstrate the ability to depress the freezing point of a solution below the equilibrium melting point, a property known as thermal hysteresis (TH) activity. These protective properties have raised interest in the identification of novel IBPs due to their potential use in industrial, medical and agricultural applications. This paper describes the identification of plant IBPs through 1) the induction and extraction of IBPs in plant tissue, 2) the screening of extracts for IRI activity, and 3) the isolation and purification of IBPs. Following the induction of IBPs by low temperature exposure, extracts are <span class="hlt">tested</span> for IRI activity using a 'splat assay', which allows the observation of <span class="hlt">ice</span> crystal growth using a standard light microscope. This assay requires a low protein concentration and generates results that are quickly obtained and easily interpreted, providing an initial screen for <span class="hlt">ice</span> binding activity. IBPs can then be isolated from contaminating proteins by utilizing the property of IBPs to adsorb to <span class="hlt">ice</span>, through a technique called '<span class="hlt">ice</span>-affinity purification'. Using cell lysates collected from plant extracts, an <span class="hlt">ice</span> hemisphere can be slowly grown on a brass probe. This incorporates IBPs into the crystalline structure of the polycrystalline <span class="hlt">ice</span>. Requiring no a priori biochemical or structural knowledge of the IBP, this method allows for recovery of active protein. <span class="hlt">Ice</span>-purified protein fractions can be used for downstream applications including the identification of peptide sequences by mass spectrometry and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol8/pdf/CFR-2010-title7-vol8-sec966-11.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol8/pdf/CFR-2010-title7-vol8-sec966-11.pdf"><span>7 CFR 966.11 - <span class="hlt">Pack</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... Orders; Fruits, Vegetables, Nuts), DEPARTMENT OF AGRICULTURE TOMATOES GROWN IN FLORIDA Order Regulating Handling Definitions § 966.11 <span class="hlt">Pack</span>. <span class="hlt">Pack</span> means any of the <span class="hlt">packs</span> of tomatoes as defined and set forth in the United States Standards for Fresh Tomatoes issued by the United States Department of Agriculture (§§ 51...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170000875','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170000875"><span>Plans and Preliminary Results of Fundamental Studies of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter; Tsao, Jen-Ching; Bartkus, Tadas</p> <p>2017-01-01</p> <p>This paper describes plans and preliminary results for using the NASA Propulsion Systems Lab (PSL) to experimentally study the fundamental physics of <span class="hlt">ice</span>-crystal <span class="hlt">ice</span> accretion. NASA is evaluating whether this facility, in addition to full-engine and motor-driven-rig <span class="hlt">tests</span>, can be used for more fundamental <span class="hlt">ice</span>-accretion studies that simulate the different mixed-phase <span class="hlt">icing</span> conditions along the core flow passage of a turbo-fan engine compressor. The data from such fundamental accretion <span class="hlt">tests</span> will be used to help develop and validate models of the accretion process. This paper presents data from some preliminary <span class="hlt">testing</span> performed in May 2015 which examined how a mixed-phase cloud could be generated at PSL using evaporative cooling in a warmer-than-freezing environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170001732','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170001732"><span>Plans and Preliminary Results of Fundamental Studies of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics in the NASA Propulsion Systems Laboratory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Struk, Peter; Tsao, Jen-Ching; Bartkus, Tadas</p> <p>2016-01-01</p> <p>This presentation accompanies the paper titled Plans and Preliminary Results of Fundamental Studies of <span class="hlt">Ice</span> Crystal <span class="hlt">Icing</span> Physics in the NASA Propulsion Systems Laboratory. NASA is evaluating whether PSL, in addition to full-engine and motor-driven-rig <span class="hlt">tests</span>, can be used for more fundamental <span class="hlt">ice</span>-accretion studies that simulate the different mixed-phase <span class="hlt">icing</span> conditions along the core flow passage of a turbo-fan engine compressor. The data from such fundamental accretion <span class="hlt">tests</span> will be used to help develop and validate models of the accretion process. This presentation (and accompanying paper) presents data from some preliminary <span class="hlt">testing</span> performed in May 2015 which examined how a mixed-phase cloud could be generated at PSL using evaporative cooling in a warmer-than-freezing environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920013862','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920013862"><span>NASA's aircraft <span class="hlt">icing</span> technology program</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reinmann, John J.</p> <p>1991-01-01</p> <p>NASA' Aircraft <span class="hlt">Icing</span> Technology program is aimed at developing innovative technologies for safe and efficient flight into forecasted <span class="hlt">icing</span>. The program addresses the needs of all aircraft classes and supports both commercial and military applications. The program is guided by three key strategic objectives: (1) numerically simulate an aircraft's response to an in-flight <span class="hlt">icing</span> encounter, (2) provide improved experimental <span class="hlt">icing</span> simulation facilities and <span class="hlt">testing</span> techniques, and (3) offer innovative approaches to <span class="hlt">ice</span> protection. Our research focuses on topics that directly support stated industry needs, and we work closely with industry to assure a rapid and smooth transfer of technology. This paper presents selected results that illustrate progress towards the three strategic objectives, and it provides a comprehensive list of references on the NASA <span class="hlt">icing</span> program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3199821','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3199821"><span>Nasal <span class="hlt">packing</span> and stenting</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Weber, Rainer K.</p> <p>2011-01-01</p> <p>Nasal <span class="hlt">packs</span> are indispensable in ENT practice. This study reviews current indications, effectiveness and risks of nasal <span class="hlt">packs</span> and stents. In endoscopic surgery, nasal <span class="hlt">packs</span> should always have smooth surfaces to minimize mucosal damage, improve wound healing and increase patient comfort. Functional endoscopic endonasal sinus surgery allows the use of modern nasal <span class="hlt">packs</span>, since pressure is no longer required. So called hemostatic/resorbable materials are a first step in this direction. However, they may lead to adhesions and foreign body reactions in mucosal membranes. Simple occlusion is an effective method for creating a moist milieu for improved wound healing and avoiding dryness. Stenting of the frontal sinus is recommended if surgery fails to produce a wide, physiologically shaped drainage path that is sufficiently covered by intact tissue. PMID:22073095</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050217460','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050217460"><span>Smagg<span class="hlt">Ice</span> 2D Version 1.8: Software Toolkit Developed for Aerodynamic Simulation Over <span class="hlt">Iced</span> Airfoils</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Choo, Yung K.; Vickerman, Mary B.</p> <p>2005-01-01</p> <p>Smagg<span class="hlt">Ice</span> 2D version 1.8 is a software toolkit developed at the NASA Glenn Research Center that consists of tools for modeling the geometry of and generating the grids for clean and <span class="hlt">iced</span> airfoils. Plans call for the completed Smagg<span class="hlt">Ice</span> 2D version 2.0 to streamline the entire aerodynamic simulation process--the characterization and modeling of <span class="hlt">ice</span> shapes, grid generation, and flow simulation--and to be closely coupled with the public-domain application flow solver, WIND. Grid generated using version 1.8, however, can be used by other flow solvers. Smagg<span class="hlt">Ice</span> 2D will help researchers and engineers study the effects of <span class="hlt">ice</span> accretion on airfoil performance, which is difficult to do with existing software tools because of complex <span class="hlt">ice</span> shapes. Using Smagg<span class="hlt">Ice</span> 2D, when fully developed, to simulate flow over an <span class="hlt">iced</span> airfoil will help to reduce the cost of performing flight and wind-tunnel <span class="hlt">tests</span> for certifying aircraft in natural and simulated <span class="hlt">icing</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120009185','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009185"><span>Further Evaluation of Scaling Methods for Rotorcraft <span class="hlt">Icing</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsao, Jen-Ching; Kreeger, Richard E.</p> <p>2012-01-01</p> <p>The paper will present experimental results from two recent <span class="hlt">icing</span> <span class="hlt">tests</span> in the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (IRT). The first <span class="hlt">test</span>, conducted in February 2009, was to evaluate the current recommended scaling methods for fixed wing on representative rotor airfoils at fixed angle of attack. For this <span class="hlt">test</span>, scaling was based on the modified Ruff method with scale velocity determined by constant Weber number and water film Weber number. Models were un-swept NACA 0012 wing sections. The reference model had a chord of 91.4 cm and scale model had a chord of 35.6 cm. Reference <span class="hlt">tests</span> were conducted with velocity of 100 kt (52 m/s), droplet medium volume diameter (MVD) 195 m, and stagnation-point freezing fractions of 0.3 and 0.5 at angle of attack of 5deg and 7deg . It was shown that good <span class="hlt">ice</span> shape scaling was achieved with constant Weber number for NACA 0012 airfoils with angle of attack up to 7deg . The second <span class="hlt">test</span>, completed in May 2010, was primarily focused on obtaining transient and steady-state <span class="hlt">iced</span> aerodynamics, <span class="hlt">ice</span> accretion and shedding, and thermal <span class="hlt">icing</span> validation data from an oscillating airfoil section over some selected ranges of <span class="hlt">icing</span> conditions and blade assembly operational configurations. The model used was a 38.1-cm chord Sikorsky SC2110 airfoil section installed on an airfoil <span class="hlt">test</span> apparatus with oscillating capability in the IRT. For two <span class="hlt">test</span> conditions, size and condition scaling were performed. It was shown that good <span class="hlt">ice</span> shape scaling was achieved for SC2110 airfoil at dynamic pitching motion. The data obtained will be applicable for future main rotor blade and tail rotor blade applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050177166','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050177166"><span>Scale Model <span class="hlt">Icing</span> Research Tunnel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Canacci, Victor A.</p> <p>1997-01-01</p> <p>NASA Lewis Research Center's <span class="hlt">Icing</span> Research Tunnel (IRT) is the world's largest refrigerated wind tunnel and one of only three <span class="hlt">icing</span> wind tunnel facilities in the United States. The IRT was constructed in the 1940's and has been operated continually since it was built. In this facility, natural <span class="hlt">icing</span> conditions are duplicated to <span class="hlt">test</span> the effects of inflight <span class="hlt">icing</span> on actual aircraft components as well as on models of airplanes and helicopters. IRT <span class="hlt">tests</span> have been used successfully to reduce flight <span class="hlt">test</span> hours for the certification of <span class="hlt">ice</span>-detection instrumentation and <span class="hlt">ice</span> protection systems. To ensure that the IRT will remain the world's premier <span class="hlt">icing</span> facility well into the next century, Lewis is making some renovations and is planning others. These improvements include modernizing the control room, replacing the fan blades with new ones to increase the <span class="hlt">test</span> section maximum velocity to 430 mph, installing new spray bars to increase the size and uniformity of the artificial <span class="hlt">icing</span> cloud, and replacing the facility heat exchanger. Most of the improvements will have a first-order effect on the IRT's airflow quality. To help us understand these effects and evaluate potential improvements to the flow characteristics of the IRT, we built a modular 1/10th-scale aerodynamic model of the facility. This closed-loop scale-model pilot tunnel was fabricated onsite in the various shops of Lewis' Fabrication Support Division. The tunnel's rectangular sections are composed of acrylic walls supported by an aluminum angle framework. Its turning vanes are made of tubing machined to the contour of the IRT turning vanes. The fan leg of the tunnel, which transitions from rectangular to circular and back to rectangular cross sections, is fabricated of fiberglass sections. The contraction section of the tunnel is constructed from sheet aluminum. A 12-bladed aluminum fan is coupled to a turbine powered by high-pressure air capable of driving the maximum <span class="hlt">test</span> section velocity to 550 ft</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100026660','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100026660"><span>Aero-Thermal Calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel (2004 and 2005 <span class="hlt">Tests</span>)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Arrington, E. Allen; Pastor, Christine M.; Gonsalez, Jose C.; Curry, Monroe R., III</p> <p>2010-01-01</p> <p>A full aero-thermal calibration of the NASA Glenn <span class="hlt">Icing</span> Research Tunnel was completed in 2004 following the replacement of the inlet guide vanes upstream of the tunnel drive system and improvement to the facility total temperature instrumentation. This calibration <span class="hlt">test</span> provided data used to fully document the aero-thermal flow quality in the IRT <span class="hlt">test</span> section and to construct calibration curves for the operation of the IRT. The 2004 <span class="hlt">test</span> was also the first to use the 2-D RTD array, an improved total temperature calibration measurement platform.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995AtmRe..36..207M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995AtmRe..36..207M"><span>A comparison of selected models for estimating cable <span class="hlt">icing</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McComber, Pierre; Druez, Jacques; Laflamme, Jean</p> <p></p> <p>In many cold climate countries, it is becoming increasingly important to monitor transmission line <span class="hlt">icing</span>. Indeed, by knowing in advance of localized danger for <span class="hlt">icing</span> overloads, electric utilities can take measures in time to prevent generalized failure of the power transmission network. Recently in Canada, a study was made to compare the estimation of a few <span class="hlt">icing</span> models working from meteorological data in estimating <span class="hlt">ice</span> loads for freezing rain events. The models <span class="hlt">tested</span> were using only standard meteorological parameters, i.e. wind speed and direction, temperature and precipitation rate. This study has shown that standard meteorological parameters can only achieve very limited accuracy, especially for longer <span class="hlt">icing</span> events. However, with the help of an additional instrument monitoring the <span class="hlt">icing</span> rate intensity, a significant improvement in model prediction might be achieved. The <span class="hlt">icing</span> rate meter (IRM) which counts <span class="hlt">icing</span> and de-<span class="hlt">icing</span> cycles per unit time on a standard probe can be used to estimate the <span class="hlt">icing</span> intensity. A cable <span class="hlt">icing</span> estimation is then made by taking into consideration the accretion size, temperature, wind speed and direction, and precipitation rate. In this paper, a comparison is made between the predictions of two previously <span class="hlt">tested</span> models (one obtained and the other reconstructed from their description in the public literature) and of a model based on the <span class="hlt">icing</span> rate meter readings. The models are <span class="hlt">tested</span> against nineteen events recorded on an <span class="hlt">icing</span> <span class="hlt">test</span> line at Mt. Valin, Canada, during the winter season 1991-1992. These events are mostly rime resulting from in-cloud <span class="hlt">icing</span>. However, freezing rain and wet snow events were also recorded. Results indicate that a significant improvement in the estimation is attained by using the <span class="hlt">icing</span> rate meter data together with the other standard meteorological parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28894785','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28894785"><span>Experimental Study of a <span class="hlt">Pack</span> of Supercapacitors Used in Electric Vehicles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mansour, Amari; Mohamed Hedi, Chabchoub; Faouzi, Bacha</p> <p>2017-01-01</p> <p>Electric vehicles have recently attracted research interest. An electric vehicle is composed of two energy sources, such as fuel cells and ultracapacitors, which are employed to provide, respectively, the steady-state and transient power demanded by the vehicle. A bidirectional DC-DC converter is needed to interface the ultracapacitor to a DC bus. The <span class="hlt">pack</span> of ultracapacitor consists of many cells in series and possibly also in parallel. In this regard, this paper introduces a comparative study between two <span class="hlt">packs</span> of supercapacitors. The first supercapacitor <span class="hlt">pack</span> is composed of ten cells in series but the second supercapacitor <span class="hlt">pack</span> is composed of five cells in series and two parallel circuits. Each cell is characterized by 2.5 V and 100 F. A number of practical <span class="hlt">tests</span> are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5574307','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5574307"><span>Experimental Study of a <span class="hlt">Pack</span> of Supercapacitors Used in Electric Vehicles</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Mohamed Hedi, Chabchoub</p> <p>2017-01-01</p> <p>Electric vehicles have recently attracted research interest. An electric vehicle is composed of two energy sources, such as fuel cells and ultracapacitors, which are employed to provide, respectively, the steady-state and transient power demanded by the vehicle. A bidirectional DC-DC converter is needed to interface the ultracapacitor to a DC bus. The <span class="hlt">pack</span> of ultracapacitor consists of many cells in series and possibly also in parallel. In this regard, this paper introduces a comparative study between two <span class="hlt">packs</span> of supercapacitors. The first supercapacitor <span class="hlt">pack</span> is composed of ten cells in series but the second supercapacitor <span class="hlt">pack</span> is composed of five cells in series and two parallel circuits. Each cell is characterized by 2.5 V and 100 F. A number of practical <span class="hlt">tests</span> are presented. PMID:28894785</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED564244.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED564244.pdf"><span>TLC <span class="hlt">Pack</span> Unpacked</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Oberhofer, Margret; Colpaert, Jozef</p> <p>2015-01-01</p> <p>TLC <span class="hlt">Pack</span> stands for Teaching Languages to Caregivers and is a course designed to support migrants working or hoping to work in the caregiving sector. The TLC <span class="hlt">Pack</span> resources range from A2 to B2 level of the Common European Framework of Reference for Languages (CEFR), and will be made available online in the six project languages: Dutch, English,…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018TCry...12.1921M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018TCry...12.1921M"><span>Reflective properties of melt ponds on sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malinka, Aleksey; Zege, Eleonora; Istomina, Larysa; Heygster, Georg; Spreen, Gunnar; Perovich, Donald; Polashenski, Chris</p> <p>2018-06-01</p> <p>Melt ponds occupy a large part of the Arctic sea <span class="hlt">ice</span> in summer and strongly affect the radiative budget of the atmosphere-<span class="hlt">ice</span>-ocean system. In this study, the melt pond reflectance is considered in the framework of radiative transfer theory. The melt pond is modeled as a plane-parallel layer of pure water upon a layer of sea <span class="hlt">ice</span> (the pond bottom). We consider pond reflection as comprising Fresnel reflection by the water surface and multiple reflections between the pond surface and its bottom, which is assumed to be Lambertian. In order to give a description of how to find the pond bottom albedo, we investigate the inherent optical properties of sea <span class="hlt">ice</span>. Using the Wentzel-Kramers-Brillouin approximation approach to light scattering by non-spherical particles (brine inclusions) and Mie solution for spherical particles (air bubbles), we conclude that the transport scattering coefficient in sea <span class="hlt">ice</span> is a spectrally independent value. Then, within the two-stream approximation of the radiative transfer theory, we show that the under-pond <span class="hlt">ice</span> spectral albedo is determined by two independent scalar values: the transport scattering coefficient and <span class="hlt">ice</span> layer thickness. Given the pond depth and bottom albedo values, the bidirectional reflectance factor (BRF) and albedo of a pond can be calculated with analytical formulas. Thus, the main reflective properties of the melt pond, including their spectral dependence, are determined by only three independent parameters: pond depth z, <span class="hlt">ice</span> layer thickness H, and transport scattering coefficient of <span class="hlt">ice</span> σt.The effects of the incident conditions and the atmosphere state are examined. It is clearly shown that atmospheric correction is necessary even for in situ measurements. The atmospheric correction procedure has been used in the model verification. The optical model developed is verified with data from in situ measurements made during three field campaigns performed on landfast and <span class="hlt">pack</span> <span class="hlt">ice</span> in the Arctic. The measured pond albedo</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930019963','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930019963"><span>A passive infrared <span class="hlt">ice</span> detection technique for helicopter applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dershowitz, Adam L.; Hansman, R. John, Jr.</p> <p>1991-01-01</p> <p>A technique has been developed, and successfully <span class="hlt">tested</span>, to detect <span class="hlt">icing</span> remotely on helicopter rotor blades. Using passive infrared (IR) thermometry it is possible to detect the warming caused by latent heat released as supercooled water freezes. During <span class="hlt">icing</span>, the <span class="hlt">ice</span> accretion region on the leading edge of the blade is found to be warmer than the uniced trailing edge resulting in a chordwise temperature profile characteristic of <span class="hlt">icing</span>. Preliminary <span class="hlt">tests</span>, using an IR Thermal video system, were conducted on a static model in the NASA <span class="hlt">Icing</span> Research Tunnel (IRT) for a variety of wet (glaze) and dry (rime) <span class="hlt">ice</span> conditions. A prototype detector system was built consisting of a single point IR pyrometer, and experiments were run on a small scale rotor model. Using this prototype detector, the characteristic chordwise temperature profiles were again observed for a range of <span class="hlt">icing</span> conditions. Several signal processing methods were investigated, to allow automatic recognition of the <span class="hlt">icing</span> signature. Additionally, several implementation issues were considered. Based on both the static and subscale rotor <span class="hlt">tests</span>, where <span class="hlt">ice</span> was successfully detected, the passive IR technique appears to be promising for rotor <span class="hlt">ice</span> detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ResPh...6..851Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ResPh...6..851Z"><span>Yield surface evolution for columnar <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Zhiwei; Ma, Wei; Zhang, Shujuan; Mu, Yanhu; Zhao, Shunpin; Li, Guoyu</p> <p></p> <p>A series of triaxial compression <span class="hlt">tests</span>, which has capable of measuring the volumetric strain of the sample, were conducted on columnar <span class="hlt">ice</span>. A new <span class="hlt">testing</span> approach of probing the experimental yield surface was performed from a single sample in order to investigate yield and hardening behaviors of the columnar <span class="hlt">ice</span> under complex stress states. Based on the characteristic of the volumetric strain, a new method of defined the multiaxial yield strengths of the columnar <span class="hlt">ice</span> is proposed. The experimental yield surface remains elliptical shape in the stress space of effective stress versus mean stress. The effect of temperature, loading rate and loading path in the initial yield surface and deformation properties of the columnar <span class="hlt">ice</span> were also studied. Subsequent yield surfaces of the columnar <span class="hlt">ice</span> have been explored by using uniaxial and hydrostatic paths. The evolution of the subsequent yield surface exhibits significant path-dependent characteristics. The multiaxial hardening law of the columnar <span class="hlt">ice</span> was established experimentally. A phenomenological yield criterion was presented for multiaxial yield and hardening behaviors of the columnar <span class="hlt">ice</span>. The comparisons between the theoretical and measured results indicate that this current model is capable of giving a reasonable prediction for the multiaxial yield and post-yield properties of the columnar <span class="hlt">ice</span> subjected to different temperature, loading rate and path conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C33E..07F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C33E..07F"><span>Routine Mapping of the Snow Depth Distribution on Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Farrell, S. L.; Newman, T.; Richter-Menge, J.; Dattler, M.; Paden, J. D.; Yan, S.; Li, J.; Leuschen, C.</p> <p>2016-12-01</p> <p>The annual growth and retreat of the polar sea <span class="hlt">ice</span> cover is influenced by the seasonal accumulation, redistribution and melt of snow on sea <span class="hlt">ice</span>. Due to its high albedo and low thermal conductivity, snow is also a controlling parameter in the mass and energy budgets of the polar climate system. Under a changing climate scenario it is critical to obtain reliable and routine measurements of snow depth, across basin scales, and long time periods, so as to understand regional, seasonal and inter-annual variability, and the subsequent impacts on the sea <span class="hlt">ice</span> cover itself. Moreover the snow depth distribution remains a significant source of uncertainty in the derivation of sea <span class="hlt">ice</span> thickness from remote sensing measurements, as well as in numerical model predictions of future climate state. Radar altimeter systems flown onboard NASA's Operation <span class="hlt">Ice</span>Bridge (OIB) mission now provide annual measurements of snow across both the Arctic and Southern Ocean <span class="hlt">ice</span> <span class="hlt">packs</span>. We describe recent advances in the processing techniques used to interpret airborne radar waveforms and produce accurate and robust snow depth results. As a consequence of instrument effects and data quality issues associated with the initial release of the OIB airborne radar data, the entire data set was reprocessed to remove coherent noise and sidelobes in the radar echograms. These reprocessed data were released to the community in early 2016, and are available for improved derivation of snow depth. Here, using the reprocessed data, we present the results of seven years of radar measurements collected over Arctic sea <span class="hlt">ice</span> at the end of winter, just prior to melt. Our analysis provides the snow depth distribution on both seasonal and multi-year sea <span class="hlt">ice</span>. We present the inter-annual variability in snow depth for both the Central Arctic and the Beaufort/Chukchi Seas. We validate our results via comparison with temporally and spatially coincident in situ measurements gathered during many of the OIB surveys. The results</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3322824','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3322824"><span>Structural Basis for Antifreeze Activity of <span class="hlt">Ice</span>-binding Protein from Arctic Yeast*</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lee, Jun Hyuck; Park, Ae Kyung; Do, Hackwon; Park, Kyoung Sun; Moh, Sang Hyun; Chi, Young Min; Kim, Hak Jun</p> <p>2012-01-01</p> <p>Arctic yeast Leucosporidium sp. produces a glycosylated <span class="hlt">ice</span>-binding protein (LeIBP) with a molecular mass of ∼25 kDa, which can lower the freezing point below the melting point once it binds to <span class="hlt">ice</span>. LeIBP is a member of a large class of <span class="hlt">ice</span>-binding proteins, the structures of which are unknown. Here, we report the crystal structures of non-glycosylated LeIBP and glycosylated LeIBP at 1.57- and 2.43-Å resolution, respectively. Structural analysis of the LeIBPs revealed a dimeric right-handed β-helix fold, which is composed of three parts: a large coiled structural domain, a long helix region (residues 96–115 form a long α-helix that <span class="hlt">packs</span> along one face of the β-helix), and a C-terminal hydrophobic loop region (243PFVPAPEVV251). Unexpectedly, the C-terminal hydrophobic loop region has an extended conformation pointing away from the body of the coiled structural domain and forms intertwined dimer interactions. In addition, structural analysis of glycosylated LeIBP with sugar moieties attached to Asn185 provides a basis for interpreting previous biochemical analyses as well as the increased stability and secretion of glycosylated LeIBP. We also determined that the aligned Thr/Ser/Ala residues are critical for <span class="hlt">ice</span> binding within the B face of LeIBP using site-directed mutagenesis. Although LeIBP has a common β-helical fold similar to that of canonical hyperactive antifreeze proteins, the <span class="hlt">ice</span>-binding site is more complex and does not have a simple <span class="hlt">ice</span>-binding motif. In conclusion, we could identify the <span class="hlt">ice</span>-binding site of LeIBP and discuss differences in the <span class="hlt">ice</span>-binding modes compared with other known antifreeze proteins and <span class="hlt">ice</span>-binding proteins. PMID:22303017</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1352451-livvkit-extensible-python-based-land-ice-verification-validation-toolkit-ice-sheet-models','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1352451-livvkit-extensible-python-based-land-ice-verification-validation-toolkit-ice-sheet-models"><span>LIVVkit: An extensible, python-based, land <span class="hlt">ice</span> verification and validation toolkit for <span class="hlt">ice</span> sheet models</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kennedy, Joseph H.; Bennett, Andrew R.; Evans, Katherine J.</p> <p></p> <p>To address the pressing need to better understand the behavior and complex interaction of <span class="hlt">ice</span> sheets within the global Earth system, significant development of continental-scale, dynamical <span class="hlt">ice</span> sheet models is underway. Concurrent to the development of the Community <span class="hlt">Ice</span> Sheet Model (CISM), the corresponding verification and validation (V&V) process is being coordinated through a new, robust, Python-based extensible software package, the Land <span class="hlt">Ice</span> Verification and Validation toolkit (LIVVkit). Incorporated into the typical <span class="hlt">ice</span> sheet model development cycle, it provides robust and automated numerical verification, software verification, performance validation, and physical validation analyses on a variety of platforms, from personal laptopsmore » to the largest supercomputers. LIVVkit operates on sets of regression <span class="hlt">test</span> and reference data sets, and provides comparisons for a suite of community prioritized <span class="hlt">tests</span>, including configuration and parameter variations, bit-for-bit evaluation, and plots of model variables to indicate where differences occur. LIVVkit also provides an easily extensible framework to incorporate and analyze results of new intercomparison projects, new observation data, and new computing platforms. LIVVkit is designed for quick adaptation to additional <span class="hlt">ice</span> sheet models via abstraction of model specific code, functions, and configurations into an <span class="hlt">ice</span> sheet model description bundle outside the main LIVVkit structure. Furthermore, through shareable and accessible analysis output, LIVVkit is intended to help developers build confidence in their models and enhance the credibility of <span class="hlt">ice</span> sheet models overall.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1352451-livvkit-extensible-python-based-land-ice-verification-validation-toolkit-ice-sheet-models','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1352451-livvkit-extensible-python-based-land-ice-verification-validation-toolkit-ice-sheet-models"><span>LIVVkit: An extensible, python-based, land <span class="hlt">ice</span> verification and validation toolkit for <span class="hlt">ice</span> sheet models</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kennedy, Joseph H.; Bennett, Andrew R.; Evans, Katherine J.; ...</p> <p>2017-03-23</p> <p>To address the pressing need to better understand the behavior and complex interaction of <span class="hlt">ice</span> sheets within the global Earth system, significant development of continental-scale, dynamical <span class="hlt">ice</span> sheet models is underway. Concurrent to the development of the Community <span class="hlt">Ice</span> Sheet Model (CISM), the corresponding verification and validation (V&V) process is being coordinated through a new, robust, Python-based extensible software package, the Land <span class="hlt">Ice</span> Verification and Validation toolkit (LIVVkit). Incorporated into the typical <span class="hlt">ice</span> sheet model development cycle, it provides robust and automated numerical verification, software verification, performance validation, and physical validation analyses on a variety of platforms, from personal laptopsmore » to the largest supercomputers. LIVVkit operates on sets of regression <span class="hlt">test</span> and reference data sets, and provides comparisons for a suite of community prioritized <span class="hlt">tests</span>, including configuration and parameter variations, bit-for-bit evaluation, and plots of model variables to indicate where differences occur. LIVVkit also provides an easily extensible framework to incorporate and analyze results of new intercomparison projects, new observation data, and new computing platforms. LIVVkit is designed for quick adaptation to additional <span class="hlt">ice</span> sheet models via abstraction of model specific code, functions, and configurations into an <span class="hlt">ice</span> sheet model description bundle outside the main LIVVkit structure. Furthermore, through shareable and accessible analysis output, LIVVkit is intended to help developers build confidence in their models and enhance the credibility of <span class="hlt">ice</span> sheet models overall.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000023203','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000023203"><span>Laboratory Investigation of Direct Measurement of <span class="hlt">Ice</span> Water Content, <span class="hlt">Ice</span> Surface Area, and Effective Radius of <span class="hlt">Ice</span> Crystals Using a Laser-Diffraction Instrument</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gerber, H.; DeMott, P. J.; Rogers, D. C.</p> <p>1995-01-01</p> <p>The aircraft microphysics probe, PVM-100A, was <span class="hlt">tested</span> in the Colorado State University dynamic cloud chamber to establish its ability to measure <span class="hlt">ice</span> water content (IWC), PSA, and Re in <span class="hlt">ice</span> clouds. Its response was compared to other means of measuring those <span class="hlt">ice</span>-cloud parameters that included using FSSP-100 and 230-X 1-D optical probes for <span class="hlt">ice</span>-crystal concentrations, a film-loop microscope for <span class="hlt">ice</span>-crystal habits and dimensions, and an in-situ microscope for determining <span class="hlt">ice</span>-crystal orientation. Intercomparisons were made in <span class="hlt">ice</span> clouds containing <span class="hlt">ice</span> crystals ranging in size from about 10 microns to 150 microns diameter, and <span class="hlt">ice</span> crystals with plate, columnar, dendritic, and spherical shapes. It was not possible to determine conclusively that the PVM accurately measures IWC, PSA, and Re of <span class="hlt">ice</span> crystals, because heat from the PVM evaporated in part the crystals in its vicinity in the chamber thus affecting its measurements. Similarities in the operating principle of the FSSP and PVM, and a comparison between Re measured by both instruments, suggest, however, that the PVM can make those measurements. The resolution limit of the PVM for IWC measurements was found to be on the order of 0.001 g/cubic m. Algorithms for correcting IWC measured by FSSP and PVM were developed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017391','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017391"><span><span class="hlt">Ice</span> Shapes on a Tail Rotor</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kreeger, Richard E.; Tsao, Jen-Ching</p> <p>2014-01-01</p> <p><span class="hlt">Testing</span> of a thermally-protected helicopter rotor in the <span class="hlt">Icing</span> Research Tunnel (IRT) was completed. Data included inter-cycle and cold blade <span class="hlt">ice</span> shapes. Accreted <span class="hlt">ice</span> shapes were thoroughly documented, including tracing, scanning and photographing. This was the first time this scanning capability was used outside of NASA. This type of data has never been obtained for a rotorcraft before. This data will now be used to validate the latest generation of <span class="hlt">icing</span> analysis tools.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1714301S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714301S"><span>Validating Cryosat-2 elevation estimates with airborne laser scanner data for the Greenland <span class="hlt">ice</span> sheet, Austfonna and Devon <span class="hlt">ice</span> caps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simonsen, Sebastian B.; Sandberg Sørensen, Louise; Nilsson, Johan; Helm, Veit; Langley, Kirsty A.; Forsberg, Rene; Hvidegaard, Sine M.; Skourup, Henriette</p> <p>2015-04-01</p> <p>The ESA CryoSat-2 satellite, launched in late 2010, carries a new type of radar altimeter especially designed for monitoring changes of sea and land <span class="hlt">ice</span>. The radar signal might penetrate into the snow <span class="hlt">pack</span> and the depth of the radar reflecting surface depends on the ratio between the surface and the volume backscatter, which is a function of several different properties such as snow density, crystal structure and surface roughness. In case of large volume scatter, the radar waveforms become broad and the determination of the range (surface elevation) becomes more difficult. Different algorithms (retrackers) are used for the range determination, and estimated surface penetration is highly dependent on the applied retracker. As part of the ESA-CryoVEx/CryoVal-Land <span class="hlt">Ice</span> projects, DTU Space has gathered accurate airborne laser scanner elevation measurements. Sites on the Greenland <span class="hlt">ice</span> sheet, Austfonna and Devon <span class="hlt">ice</span> caps, has been surveyed repeatedly, aligned with Cryosat-2 ground tracks and surface experiments. Here, we utilize elevation estimates from available Cryosat-2 retrackers (ESA level-2 retracker, DTU retracker, etc.) and validate the elevation measurements against ESA-CryoVEx campaigns. A difference between laser and radar elevations is expected due to radar penetration issues, however an inter-comparison between retrackers will shed light on individual performances and biases. Additionally, the geo-location of the radar return will also be a determining factor for the precision. Ultimately, the use of multiple retrackers can provide information about subsurface conditions and utilize more of the waveform information than presently used in radar altimetry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880059050&hterms=europa+ice&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Deuropa%2Bice','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880059050&hterms=europa+ice&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Deuropa%2Bice"><span>Friction of <span class="hlt">ice</span>. [on Ganymede, Callisto, and Europa surfaces</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Beeman, M.; Durham, W. B.; Kirby, S. H.</p> <p>1988-01-01</p> <p>Frictional sliding experiments were performed on saw-cut samples of laboratory-made polycrystalline water <span class="hlt">ice</span>, prepared in the same way as the material used by Kirby et al. (1987) in <span class="hlt">ice</span> deformation experiments. The data show that the maximum frictional stress is a function of the normal stress but is not measurably dependent on temperature or sliding rate over the ranges covered in these experiments (77-115 K and 0.0003-0.03 mm/s, respectively). The sliding behavior was invariably stick slip, with the sliding surfaces exhibiting only minor gouge development. In samples with anomalously low strength, a curious arrangement of densely <span class="hlt">packed</span> short vertical fractures was observed. The results of these experiments were applied to a model of near-surface tectonic activity on Ganymede, one of Jupiter's icy moons. The results indicate that a global expansion on Ganymede of 3 linear percent will cause extensional movement on preexisting faults at depths to 7 + or - 3 km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090030606','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090030606"><span>Airframe <span class="hlt">Icing</span> Research Gaps: NASA Perspective</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Potapczuk, Mark</p> <p>2009-01-01</p> <p>qCurrent Airframe <span class="hlt">Icing</span> Technology Gaps: Development of a full 3D <span class="hlt">ice</span> accretion simulation model. Development of an improved simulation model for SLD conditions. CFD modeling of stall behavior for <span class="hlt">ice</span>-contaminated wings/tails. Computational methods for simulation of stability and control parameters. Analysis of thermal <span class="hlt">ice</span> protection system performance. Quantification of 3D <span class="hlt">ice</span> shape geometric characteristics Development of accurate ground-based simulation of SLD conditions. Development of scaling methods for SLD conditions. Development of advanced diagnostic techniques for assessment of tunnel cloud conditions. Identification of critical <span class="hlt">ice</span> shapes for aerodynamic performance degradation. Aerodynamic scaling issues associated with <span class="hlt">testing</span> scale model <span class="hlt">ice</span> shape geometries. Development of altitude scaling methods for thermal <span class="hlt">ice</span> protections systems. Development of accurate parameter identification methods. Measurement of stability and control parameters for an <span class="hlt">ice</span>-contaminated swept wing aircraft. Creation of control law modifications to prevent loss of control during <span class="hlt">icing</span> encounters. 3D <span class="hlt">ice</span> shape geometries. Collection efficiency data for <span class="hlt">ice</span> shape geometries. SLD <span class="hlt">ice</span> shape data, in-flight and ground-based, for simulation verification. Aerodynamic performance data for 3D geometries and various <span class="hlt">icing</span> conditions. Stability and control parameter data for <span class="hlt">iced</span> aircraft configurations. Thermal <span class="hlt">ice</span> protection system data for simulation validation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100001611','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100001611"><span>Selection of Environmentally Friendly Solvents for the Extravehicular Mobility Unit Secondary Oxygen <span class="hlt">Pack</span> Cold Trap <span class="hlt">Testing</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steele, John; Chullen, Cinda; Morenz, Jesse; Stephenson, Curtis</p> <p>2010-01-01</p> <p>Freon-113(TradeMark) has been used as a chemistry lab sampling solvent at NASA/JSC for EMU (extravehicular Mobility Unit) SOP (Secondary Oxygen <span class="hlt">Pack</span>) oxygen <span class="hlt">testing</span> Cold Traps utilized at the USA (United Space Alliance) Houston facility. Similar <span class="hlt">testing</span> has occurred at the HSWL (Hamilton Sundstrand Windsor Locks) facility. A NASA Executive Order bans the procurement of all ODS (ozone depleting substances), including Freon-113 by the end of 2009. In order to comply with NASA direction, HSWL began evaluating viable solvents to replace Freon-113 . The study and <span class="hlt">testing</span> effort to find Freon-113 replacements used for Cold Trap sampling is the subject of this paper. <span class="hlt">Test</span> results have shown HFE-7100 (a 3M fluorinated ether) to be an adequate replacement for Freon-113 as a solvent to remove and measure the non-volatile residue collected in a Cold Trap during oxygen <span class="hlt">testing</span>. Furthermore, S-316 (a Horiba Instruments Inc. high molecular weight, non-ODS chlorofluorocarbon) was found to be an adequate replacement for Freon-113 as a solvent to reconstitute non-volatile residue removed from a Cold Trap during oxygen <span class="hlt">testing</span> for subsequent HC (hydrocarbon) analysis via FTIR (Fourier Transform Infrared Spectroscopy).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010027899','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010027899"><span>Studies of Antarctic Sea <span class="hlt">Ice</span> Concentrations from Satellite Data and Their Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Comiso, Josefino C.; Steffen, Konrad; Zukor, Dorothy J. (Technical Monitor)</p> <p>2001-01-01</p> <p>Large changes in the sea <span class="hlt">ice</span> cover have been observed recently. Because of the relevance of such changes to climate change studies it is important that key <span class="hlt">ice</span> concentration data sets used for evaluating such changes are interpreted properly. High and medium resolution visible and infrared satellite data are used in conjunction with passive microwave data to study the true characteristics of the Antarctic sea <span class="hlt">ice</span> cover, assess errors in currently available <span class="hlt">ice</span> concentration products, and evaluate the applications and limitations of the latter in polar process studies. Cloud-free high resolution data provide valuable information about the natural distribution, stage of formation, and composition of the <span class="hlt">ice</span> cover that enables interpretation of the large spatial and temporal variability of the microwave emissivity of Antarctic sea <span class="hlt">ice</span>. Comparative analyses of co-registered visible, infrared and microwave data were used to evaluate <span class="hlt">ice</span> concentrations derived from standard <span class="hlt">ice</span> algorithms (i.e., Bootstrap and Team) and investigate the 10 to 35% difference in derived values from large areas within the <span class="hlt">ice</span> <span class="hlt">pack</span>, especially in the Weddell Sea, Amundsen Sea, and Ross Sea regions. Landsat and OLS data show a predominance of thick consolidated <span class="hlt">ice</span> in these areas and show good agreement with the Bootstrap Algorithm. While direct measurements were not possible, the lower values from the Team Algorithm results are likely due to layering within the <span class="hlt">ice</span> and snow and/or surface flooding, which are known to affect the polarization ratio. In predominantly new <span class="hlt">ice</span> regions, the derived <span class="hlt">ice</span> concentration from passive microwave data is usually lower than the true percentage because the emissivity of new <span class="hlt">ice</span> changes with age and thickness and is lower than that of thick <span class="hlt">ice</span>. However, the product provides a more realistic characterization of the sea <span class="hlt">ice</span> cover, and are more useful in polar process studies since it allows for the identification of areas of significant divergence and polynya</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26339489','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26339489"><span><span class="hlt">Ice</span> swimming - '<span class="hlt">Ice</span> Mile' and '1 km <span class="hlt">Ice</span> event'.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Knechtle, Beat; Rosemann, Thomas; Rüst, Christoph A</p> <p>2015-01-01</p> <p><span class="hlt">Ice</span> swimming for 1 mile and 1 km is a new discipline in open-water swimming since 2009. This study examined female and male performances in swimming 1 mile ('<span class="hlt">Ice</span> Mile') and 1 km ('1 km <span class="hlt">Ice</span> event') in water of 5 °C or colder between 2009 and 2015 with the hypothesis that women would be faster than men. Between 2009 and 2015, 113 men and 38 women completed one '<span class="hlt">Ice</span> Mile' and 26 men and 13 completed one '1 km <span class="hlt">Ice</span> event' in water colder than +5 °C following the rules of International <span class="hlt">Ice</span> Swimming Association (IISA). Differences in performance between women and men were determined. Sex difference (%) was calculated using the equation ([time for women] - [time for men]/[time for men] × 100). For '<span class="hlt">Ice</span> Mile', a mixed-effects regression model with interaction analyses was used to investigate the influence of sex and environmental conditions on swimming speed. The association between water temperature and swimming speed was assessed using Pearson correlation analyses. For '<span class="hlt">Ice</span> Mile' and '1 km <span class="hlt">Ice</span> event', the best men were faster than the best women. In '<span class="hlt">Ice</span> Mile', calendar year, number of attempts, water temperature and wind chill showed no association with swimming speed for both women and men. For both women and men, water temperature was not correlated to swimming speed in both '<span class="hlt">Ice</span> Mile' and '1 km <span class="hlt">Ice</span> event'. In water colder than 5 °C, men were faster than women in '<span class="hlt">Ice</span> Mile' and '1 km <span class="hlt">Ice</span> event'. Water temperature showed no correlation to swimming speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970009335','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970009335"><span>Validation of NASA Thermal <span class="hlt">Ice</span> Protection Computer Codes. Part 1; Program Overview</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, Dean; Bond, Thomas; Sheldon, David; Wright, William; Langhals, Tammy; Al-Khalil, Kamel; Broughton, Howard</p> <p>1996-01-01</p> <p>The <span class="hlt">Icing</span> Technology Branch at NASA Lewis has been involved in an effort to validate two thermal <span class="hlt">ice</span> protection codes developed at the NASA Lewis Research Center. LEWICE/Thermal (electrothermal deicing & anti-<span class="hlt">icing</span>), and ANTICE (hot-gas & electrothermal anti-<span class="hlt">icing</span>). The Thermal Code Validation effort was designated as a priority during a 1994 'peer review' of the NASA Lewis <span class="hlt">Icing</span> program, and was implemented as a cooperative effort with industry. During April 1996, the first of a series of experimental validation <span class="hlt">tests</span> was conducted in the NASA Lewis <span class="hlt">Icing</span> Research Tunnel(IRT). The purpose of the April 96 <span class="hlt">test</span> was to validate the electrothermal predictive capabilities of both LEWICE/Thermal, and ANTICE. A heavily instrumented <span class="hlt">test</span> article was designed and fabricated for this <span class="hlt">test</span>, with the capability of simulating electrothermal de-<span class="hlt">icing</span> and anti-<span class="hlt">icing</span> modes of operation. Thermal measurements were then obtained over a range of <span class="hlt">test</span> conditions, for comparison with analytical predictions. This paper will present an overview of the <span class="hlt">test</span>, including a detailed description of: (1) the validation process; (2) <span class="hlt">test</span> article design; (3) <span class="hlt">test</span> matrix development; and (4) <span class="hlt">test</span> procedures. Selected experimental results will be presented for de-<span class="hlt">icing</span> and anti-<span class="hlt">icing</span> modes of operation. Finally, the status of the validation effort at this point will be summarized. Detailed comparisons between analytical predictions and experimental results are contained in the following two papers: 'Validation of NASA Thermal <span class="hlt">Ice</span> Protection Computer Codes: Part 2- The Validation of LEWICE/Thermal' and 'Validation of NASA Thermal <span class="hlt">Ice</span> Protection Computer Codes: Part 3-The Validation of ANTICE'</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26186271','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26186271"><span>Adhesive loose <span class="hlt">packings</span> of small dry particles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Wenwei; Li, Shuiqing; Baule, Adrian; Makse, Hernán A</p> <p>2015-08-28</p> <p>We explore adhesive loose <span class="hlt">packings</span> of small dry spherical particles of micrometer size using 3D discrete-element simulations with adhesive contact mechanics and statistical ensemble theory. A dimensionless adhesion parameter (Ad) successfully combines the effects of particle velocities, sizes and the work of adhesion, identifying a universal regime of adhesive <span class="hlt">packings</span> for Ad > 1. The structural properties of the <span class="hlt">packings</span> in this regime are well described by an ensemble approach based on a coarse-grained volume function that includes the correlation between bulk and contact spheres. Our theoretical and numerical results predict: (i) an equation of state for adhesive loose <span class="hlt">packings</span> that appear as a continuation from the frictionless random close <span class="hlt">packing</span> (RCP) point in the jamming phase diagram and (ii) the existence of an asymptotic adhesive loose <span class="hlt">packing</span> point at a coordination number Z = 2 and a <span class="hlt">packing</span> fraction ϕ = 1/2(3). Our results highlight that adhesion leads to a universal <span class="hlt">packing</span> regime at <span class="hlt">packing</span> fractions much smaller than the random loose <span class="hlt">packing</span> (RLP), which can be described within a statistical mechanical framework. We present a general phase diagram of jammed matter comprising frictionless, frictional, adhesive as well as non-spherical particles, providing a classification of <span class="hlt">packings</span> in terms of their continuation from the spherical frictionless RCP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMGC33A1268F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMGC33A1268F"><span><span class="hlt">ICE</span>911 Research: Floating Safe Inert Materials to Preserve <span class="hlt">Ice</span> and Conserve Water in Order to Mitigate Climate Change Impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, L. A.; Manzara, A.; Chetty, S.; Venkatesh, S.; Scholtz, A.</p> <p>2015-12-01</p> <p><span class="hlt">Ice</span>911 Research has conducted years of field <span class="hlt">testing</span> to develop and <span class="hlt">test</span> localized reversible engineering techniques to mitigate the negative impacts of polar <span class="hlt">ice</span> melt. The technology uses environmentally safe materials to reflect energy in carefully selected, limited areas from summertime polar sun. The technology is now being adapted to help with California's drought. We have <span class="hlt">tested</span> the albedo modification technique on a small scale over seven Winter/Spring seasons at sites including California's Sierra Nevada Mountains, a Canadian lake, and a small artificial pond in Minnesota about 100 ft in diameter and 6 ft deep at the center, using various materials and an evolving array of instrumentation. On the pond in Minnesota, this year's <span class="hlt">test</span> results for <span class="hlt">ice</span> preservation, using hollow glass spheres deployed over our largest <span class="hlt">test</span> areas yet, showed that glass bubbles can provide an effective material for increasing albedo, significantly reducing the melting rate of <span class="hlt">ice</span>. This year <span class="hlt">Ice</span>911 also undertook its first small Arctic field <span class="hlt">test</span> in Barrow, Alaska on a lake in Barrow's BEO area, and results are still coming in. The technology that <span class="hlt">Ice</span>911 has been developing for <span class="hlt">ice</span> preservation has also been shown to keep small <span class="hlt">test</span> areas of water cooler, in various small-scale <span class="hlt">tests</span> spanning years. We believe that with some adaptations of the technology, the materials can be applied to reservoirs and lakes to help stretch these precious resources further in California's ongoing drought. There are several distinct advantages for this method over alternatives such as large reverse osmosis projects or building new reservoirs, which could possibly allow a drought-stricken state to build fewer of these more-costly alternatives. First, applying an ecologically benign surface treatment of <span class="hlt">Ice</span>911's materials can be accomplished within a season, at a lower cost, with far less secondary environmental impact, than such capital-and-time-intensive infrastructure projects. Second, keeping</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-200910220008HQ.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-200910220008HQ.html"><span><span class="hlt">Ice</span> Bridge Antarctic Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2009-10-21</p> <p>Sea <span class="hlt">ice</span> is seen out the window of NASA's DC-8 research aircraft as it flies 2,000 feet above the Bellingshausen Sea in West Antarctica on Wednesday, Oct., 21, 2009. This was the fourth science flight of NASA’s Operation <span class="hlt">Ice</span> Bridge airborne Earth science mission to study Antarctic <span class="hlt">ice</span> sheets, sea <span class="hlt">ice</span>, and <span class="hlt">ice</span> shelves. Photo Credit: (NASA/Jane Peterson)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23218187','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23218187"><span>Colloidal aspects and <span class="hlt">packing</span> behaviour of charged microparticulates in high efficiency ion chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wahab, M Farooq; Pohl, Christopher A; Lucy, Charles A</p> <p>2012-12-28</p> <p>The development of small particles in ion chromatography (IC) is a recent phenomenon. Very few studies are available on <span class="hlt">packing</span> polymeric particles bearing ionizable functional groups. This study explores the colloidal and rheological properties that govern slurry <span class="hlt">packing</span> to form high efficiency IC columns. The polymeric substrate used was non-porous 4.4 μm sulfonated ethylvinylbenzene–divinylbenzene (1.4 mequiv. SO(3)H/g resin) with 55% crosslink. We developed simple <span class="hlt">tests</span> optical microscopy and sedimentation <span class="hlt">tests</span> for predicting the quality of <span class="hlt">packed</span> columns. The negatively charged particles (zeta potential: −52 mV in water) behave like colloids. The influence of counter-ion charge (Al(3+), Mg(2+), Na(+)) and ionic strength on column efficiency followed the Schulze–Hardy rule. Highly flocculating slurries give poorly <span class="hlt">packed</span> columns with N ~ 900 whereas under non-agglomerating slurry conditions efficiencies up to N > 10,000 can be achieved. A non-agglomerating slurry also shows non-Newtonian behaviour, specifically shear thickening. <span class="hlt">Packing</span> at lower flow rate (<1 mL/min) or higher temperature (>50 °C) reduces the shear thickening and produces higher efficiency columns. The <span class="hlt">packed</span> sulfonated resin column is coated with 72 nm quaternary ammonium bearing latex (AS4A) and used in the separation of F(−), Cl(−), NO(2)(−), Br(−), and NO(3)(−) yielding a reduced plate height of 1.9 under optimum conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001118.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001118.html"><span>Persistent <span class="hlt">Ice</span> on Lake Superior</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-12-08</p> <p>Though North America is a full month into astronomical spring, the Great Lakes have been slow to give up on winter. As of April 22, 2014, the Great Lakes were 33.9 percent <span class="hlt">ice</span> covered. The lake they call Superior dominated the <span class="hlt">pack</span>. In the early afternoon on April 20, 2014, the Moderate Resolution Imaging Spectroradiometer (MODIS) on NASA’s Aqua satellite captured this natural-color image of Lake Superior, which straddles the United States–Canada border. At the time Aqua passed over, the lake was 63.5 percent <span class="hlt">ice</span> covered, according to the NOAA Great Lakes Environmental Research Lab (GLERL). Averaged across Lake Superior, <span class="hlt">ice</span> was 22.6 centimeters (8.9 inches) thick; it was as much as twice that thickness in some locations. GLERL researcher George Leshkevich affirmed that <span class="hlt">ice</span> cover this spring is significantly above normal. For comparison, Lake Superior had 3.6 percent <span class="hlt">ice</span> cover on April 20, 2013; in 2012, <span class="hlt">ice</span> was completely gone by April 12. In the last winter that <span class="hlt">ice</span> cover grew so thick on Lake Superior (2009), it reached 93.7 percent on March 2 but was down to 6.7 percent by April 21. Average water temperatures on all of the Great Lakes have been rising over the past 30 to 40 years and <span class="hlt">ice</span> cover has generally been shrinking. (Lake Superior <span class="hlt">ice</span> was down about 79 percent since the 1970s.) But chilled by persistent polar air masses throughout the 2013-14 winter, <span class="hlt">ice</span> cover reached 88.4 percent on February 13 and 92.2 percent on March 6, 2014, the second highest level in four decades of record-keeping. Air temperatures in the Great Lakes region were well below normal for March, and the cool pattern is being reinforced along the coasts because the water is absorbing less sunlight and warming less than in typical spring conditions. The graph below, based on data from Environment Canada, shows the 2014 conditions for all of the Great Lakes in mid-April compared to the past 33 years. Lake Superior <span class="hlt">ice</span> cover got as high as 95.3 percent on March 19. By April 22, it was</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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