## Elements of X-Ray Diffraction |

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Page 89

In such a case, there is simply no diffracted beam at the angle predicted by an

equation of the type of Eqs. (3-10) and (3-11). It is in this sense that equations of

this kind predict all possible diffracted beams. 3-6 Diffraction methods. I^ra^

In such a case, there is simply no diffracted beam at the angle predicted by an

equation of the type of Eqs. (3-10) and (3-11). It is in this sense that equations of

this kind predict all possible diffracted beams. 3-6 Diffraction methods. I^ra^

**tion**...Page 107

The equa-

square of the distance from the scattering atom, as one would expect, and that

the scattered beam is stronger in forward or backward directions than in a

direction ...

The equa-

**tion**also shows that the scattered intensity decreases as the inversesquare of the distance from the scattering atom, as one would expect, and that

the scattered beam is stronger in forward or backward directions than in a

direction ...

Page 424

Variation of transmitted intensity with wavelength near an ubsor|>-

this particular curve, three thicknesses of photographic film were used as an

absorber and the absorption edge shown is the K edge of the silver 'in the

emulsion ...

Variation of transmitted intensity with wavelength near an ubsor|>-

**tion**edge. (Forthis particular curve, three thicknesses of photographic film were used as an

absorber and the absorption edge shown is the K edge of the silver 'in the

emulsion ...

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#### LibraryThing Review

User Review - ron_benson - LibraryThingExcellent reference book. Needs some updating in terms of advances in detector technology. Read full review

### Contents

PROPERTIES OF XRAYS | 1 |

THE GEOMETRY OF CRYSTALS | 29 |

THE DIRECTIONS OF DIFFRACTED BEAMS | 78 |

Copyright | |

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### Common terms and phrases

absorption coefficient absorption edge alloy atomic number austenite axes axis back-reflection Bragg angle Bragg law Bravais lattice calculated camera chart circle composition constant copper cos2 counter counting rate cubic curve Debye ring Debye-Scherrer decreases density determined diffracted beam diffraction lines diffraction pattern diffractometer direction distance electrons elements equation error example face-centered face-centered cubic factor film filter given grain hexagonal incident beam indices integrated intensity lattice parameter Laue method located martensite measured metal normal obtained orthorhombic parallel percent phase photograph pinhole plotted point lattice pole figure position powder pattern preferred orientation produced pulses rays reciprocal lattice reflecting planes relative rhombohedral rotation sample scattering shown in Fig sin2 6 values slit solid solution spacing specimen sphere stereographic projection stress structure substance surface symmetry temperature tetragonal thickness tion transmission twin twin band unit cell vector voltage wave wavelength x-ray diffraction x-ray tube zero zone