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Ewald sphere
Limiting sphere
P (
hkl
)
P ¢ H hkl
b*
s / l
2 q
O
C
s 0 / l
a*
1/ l
2/ l
FIGURE 1.14 Limiting sphere for the powder diffraction.
in Figure 1.15. The end of s/l vector forms a circle on the Ewald sphere passing
through the reciprocal lattice point P(hkl ), P 0 (hkl ), and all equivalent reciprocal
lattice points. The diffracted beams form a conewith the incident beamon the rotation
axis. This cone is referred to as diffraction cone. The 2u angle can take values from0 to
Diffraction vector cone
Diffraction cone
Ewald sphere
P (
hkl
)
s / l
H hkl
X-ray
2 2 q
C
O
s 0 / l
H hkl
s / l
P
¢
( hkl )
FIGURE 1.15 Diffraction cone and diffraction vector cone illustrated on the Ewald sphere.
 
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