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Measuring Strain Using X-Ray Diffraction
By: James Belasco
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What is Strain? When a force is applied materials deform in two ways
It will deform and then revert to its original shape (reversible) Change its shape permanently (irreversible)
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The Structure of Materials
At the local level, solids are composed o crystalline lattices Atoms in these crystal structures are arranged in different crystal shapes depending on the material
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Lattice Under Stress In reversible strain the bonds act like springs
Strain “stretches” the bonds in the lattice without breaking them
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Who’s More Flexible?
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How does a polycrystalline material distribute strain?
1 2 1 2 + = ? or
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Polycrystalline Materials
Nanocrystalline structures are made of a large number of randomly oriented crystals How does the bulk property of the material relate to the individual crystallites?
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Figure Compliments of Matt Bibee, SULI 2006
The Value of X-Ray Diffraction Normal Space Diffraction Space d0 d0 d0 d2* d1* Strained Sample Strain d2* d1* Figure Compliments of Matt Bibee, SULI 2006
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Strain Equations x y z x a = y z
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The Apparatus Detector Sample Beam
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Straining Iron [110] [200] Sets of crystals oriented in a particular direction from their own ring Iron produces three rings [211]
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To Have Cake Diffraction images are transformed to a different coordinate system or “caked” One Ring χ Q χ Transformation Q
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Straining Iron Strain Direction The slopes of the lines give us the elastic modulus in a crystallographic direction [200]: 152.3 Error: 6.05 [211]: 207.3 Error: 9.2 [110]: 177.5 Error: 10.9
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The polycrystalline sample exhibits properties of the single crystal
How far can you stretch? Single Crystal Values 110 210 GPa 200 125 GPa 211 210 GPa Measured Values 110 177 ± 11 GPa 200 152 ± 6 GPa 211 207 ± 9 GPa ~ ~ The polycrystalline sample exhibits properties of the single crystal
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So what Really Happens? 1 2 + = ?
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Acknowledgements Department of Energy, SLAC, and SSRL Apurva Mehta
David Bronfenbrenner
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