Bragg's Law

NSDL National Science Digital Library

It may be beneficial to have students perform the Wave Interference activity prior to engaging them in this activity. The following handouts are identical, with the exception that one is in Word format, while the other is in PDF format. The students should perform the exercise in a computer laboratory. Before proceeding through the questions, they should be given an opportunity to review the material on this web page. Bragg\\'s Law Activity Sheet (Acrobat (PDF) 73kB Mar2 10) Bragg\\'s Law Activity Sheet for Word (Microsoft Word 37kB Feb25 10) The following Powerpoint presentation can be used as an introduction to Bragg's Law. Bragg\\'s Law Powerpoint Presentation (PowerPoint 974kB Feb25 10) Wave Interference Activity Prior to investigating Bragg's law through this activity, it may be helpful to explore interference of sinusoidal waveforms by following the link below. Wave Interference Activity Bragg's Law Applet Java Applet created by Konstantin Lukin with supervision by Glenn A. Richard, Project Java Webmaster Original Bragg's Law Applet page on Mineral Physics Institute web server at Stony Brook University: Project Java - Bragg's Law and Diffraction: How waves reveal the atomic structure of crystals Bragg's Law refers to the simple equation: nÃ = 2d sinÃ derived by the English physicists Sir W.H. Bragg and his son Sir W.L. Bragg in 1913 to explain why the cleavage faces of crystals appear to reflect X-ray beams at certain angles of incidence (Ã, Ã). The variable d is the distance between atomic layers in a crystal, and the variable lambda is the wavelength of the incident X-ray beam (see applet); n is an integer. This observation is an example of X-ray wave interference (Roentgenstrahlinterferenzen), commonly known as X-ray diffraction (XRD), and was direct evidence for the periodic atomic structure of crystals postulated for several centuries. The Braggs were awarded the Nobel Prize in physics in 1915 for their work in determining crystal structures beginning with NaCl, ZnS and diamond. Although Bragg's law was used to explain the interference pattern of X-rays scattered by crystals, diffraction has been developed to study the structure of all states of matter with any beam, e.g., ions, electrons, neutrons, and protons, with a wavelength similar to the distance between the atomic or molecular structures of interest. How to Use this Applet The applet shows two rays incident on two atomic layers of a crystal, e.g., atoms, ions, and molecules, separated by the distance d. The layers look like rows because the layers are projected onto two dimensions and your view is parallel to the layers. The applet begins with the scattered rays in phase and interferring constructively. Bragg's Law is satisfied and diffraction is occurring. The meter indicates how well the phases of the two rays match. The small light on the meter is green when Bragg's equation is satisfied and red when it is not satisfied. The meter can be observed while the three variables in Bragg's are changed by clicking on the scroll-bar arrows and by typing the values in the boxes. The d and Ã variables can be changed by dragging on the arrows provided on the crystal layers and scattered beam, respectively. Bragg's Law Applet with details meter activated, but no constructive interference. Note that the peaks and troughs on the scattered beams are not aligned. Bragg's Law Applet with constructive interference and n = 2. Note that the peaks and troughs on the scattered beams are aligned. Deriving Bragg's Law by Paul Schields Bragg's Law can easily be derived by considering the conditions necessary to make the phases of the beams coincide when the incident angle equals and reflecting angle. The rays of the incident beam are always in phase and parallel up to the point at which the top beam strikes the top layer at atom z (Fig. 1). The second beam continues to the next layer where it is scattered by atom B. The second beam must travel the extra distance AB + BC if the two beams are to continue traveling adjacent and parallel. This extra distance must be an integral (n) multiple of the wavelength (Ã) for the phases of the two beams to be the same: nÃ = AB +BC (2). Fig. 1 Deriving Bragg's Law using the reflection geometry and applying trigonometry. The lower beam must travel the extra distance (AB + BC) to continue traveling parallel and adjacent to the top beam. Recognizing d as the hypotenuse of the right triangle Abz, we can use trigonometry to relate d and Ã to the distance (AB + BC). The distance AB is opposite Ã so, AB = d sinÃ(3). Because AB = BC eq. (2) becomes, nÃ = 2AB (4) Substituting eq. (3) in eq. (4) we have, nÃ = 2 d sinÃ, (1) and Bragg's Law has been derived. The location of the surface does not change the derivation of Bragg's Law. Experimental Diffraction Patterns The following figures show experimental x-ray diffraction patterns of cubic SiC using synchrotron radiation. Detail from previous image Players in the Discovery of X-ray Diffraction Friedrich and Knipping first observed Roentgenstrahlinterferenzen in 1912 after a hint from their research advisor, Max von Laue, at the University of Munich. Bragg's Law greatly simplified von Laue's description of X-ray interference. The Braggs used crystals in the reflection geometry to analyze the intensity and wavelengths of X-rays (spectra) generated by different materials. Their apparatus for characterizing X-ray spectra was the Bragg spectrometer. Laue knew that X-rays had wavelengths on the order of 1 Ã. After learning that Paul Ewald's optical theories had approximated the distance between atoms in a crystal by the same length, Laue postulated that X-rays would diffract, by analogy to the diffraction of light from small periodic scratches drawn on a solid surface (an optical diffraction grating). In 1918 Ewald constructed a theory, in a form similar to his optical theory, quantitatively explaining the fundamental physical interactions associated with XRD. Elements of Ewald's eloquent theory continue to be useful for many applications in physics. Kennedy Walker split cylinder apparatus in the Mineral Physics Institute High Pressure Laboratory at Stony Brook University Do We Have Diamonds? If we perform a high pressure experiment in a press, such as the Kennedy-Walker split cylinder apparatus, to convert graphite into diamonds, we can use X-ray diffraction techniques to determine whether we achieved the intended result. The carbon atoms in graphite are arranged into planes that are separated by d-spacings of 3.35Ã. If we use X-rays with a wavelength (Ã) of 1.54Ã, and we have diamonds in the material we are testing, we will find peaks on our X-ray pattern at Ã values that correspond to each of the d-spacings that characterize diamond. These d-spacings are 1.075Ã, 1.261Ã, and 2.06Ã. To discover where to expect peaks if diamond, graphite, or both are present, you can set Ã to 1.54Ã in the applet, and set distance to one of the d-spacings. Then start with Ã at 6 degrees, and vary it until you find a Bragg's condition. Do the same with each of the remaining d-spacings. Remember that in the applet, you are varying Ã, while on the X-ray pattern printout, the angles are given as 2Ã. Consequently, when the applet indicates a Bragg's condition at a particular angle, you must multiply that angle by 2 to locate the angle on the X-ray pattern printout where you would expect a peak. First stage anvils in the Kennedy Walker split cylinder apparatus