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Published byQuentin Long Modified over 9 years ago
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X-ray diffraction Biophysics
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W. K. Röntgen (1845 – 1923) Wife’s hand
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Ruhmkorff inductor
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X-ray tube with rotating anode
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Syncrotron in Grenoble
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X-ray spectrum of rhodium Λ min K series Å (Duane – Hunt limit) White radiation Bremsstrahlung
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Moseley-law σ= 1 for K lines σ= 7.4 for L lines
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Diffractometer Note: diffraction is a special geometry dependent spectroscopy
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X-ray diffraction facility
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Laue diagram Condition for constructive interference: Δ = AD - BC Incident beam X Z Y α0α0 β0β0 γ0γ0
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Diffraction pattern of a crystal
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X-ray pattern of whale myoglobin
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Debye-Scherrer method
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Bragg scattering condition kλ= 2dsinδ
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Diffraction from 2-D lattice Incident beam Reflected beam
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Sources of secondary X rays zero order 0 1 3 2 -2 -3 third order P Row of scatterers 1 1’ Note: If the number of scatterers increases the diffraction pattern becomes sharper
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Continuous helix
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Diffraction pattern of continuous helix 1 2 3 1/P P: pitch of helix
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X-ray diffraction of helix structure 1/R +1 1/p
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Generation of diffraction pattern 14.3 nm
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Striated muscle Relaxed state Rigor state
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Sarcoplasmatic reticulum
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I4-1 supernova
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