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Page 38
The orientation of planes in a lattice may also be represented symbolically ,
according to a system popularized by the English crystallographer Miller . In the
general case , the given plane will be tilted with respect to the crystallographic
axes ...
The orientation of planes in a lattice may also be represented symbolically ,
according to a system popularized by the English crystallographer Miller . In the
general case , the given plane will be tilted with respect to the crystallographic
axes ...
Page 60
The orientation of any plane in a crystal can be just as well represented by the
inclination of the normal to that plane relative to some reference plane as ... All
the planes in a crystal can thus be represented by a set of plane normals
radiating ...
The orientation of any plane in a crystal can be just as well represented by the
inclination of the normal to that plane relative to some reference plane as ... All
the planes in a crystal can thus be represented by a set of plane normals
radiating ...
Page 217
The beam reflected by the plane shown strikes the film at S. The normal to this
reflecting plane is CN and the plane ... If we imagine this plane to rotate about the
zone axis , it will pass through all the positions at which planes of this zone in an
...
The beam reflected by the plane shown strikes the film at S. The normal to this
reflecting plane is CN and the plane ... If we imagine this plane to rotate about the
zone axis , it will pass through all the positions at which planes of this zone in an
...
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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 | |
21 other sections not shown
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Elements of X-ray Diffraction Bernard Dennis Cullity,Stuart R. Stock,Stuart R.. Stock Snippet view - 2001 |
Common terms and phrases
absorption alloy angle applied atoms axis Bragg calculated called camera cause circle composition consider constant contains copper counter counting crystal cubic curve decreases depends described determined diffracted beam diffraction lines diffractometer direction distance effect electrons elements energy equal equation error example factor Figure film fluorescent given gives grain hexagonal incident beam increases indices intensity involved kind known lattice Laue length located material means measured metal method normal observed obtained occur orientation parallel parameter particular pattern percent phase photograph plane plotted pole position possible powder produced projection proportional pulses radiation rays reference reflection relation relative result rotation sample scattering shown shown in Fig shows simple single slit solid solution spacing specimen stress structure substance surface temperature thickness tion tube twin unit cell usually vector voltage wave wavelength x-ray