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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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- 374 -<br />

define the axes u, v and w where w is the projection of m into the specimen<br />

surface. The angles * and 0 define the orientation of m, u, v<br />

relative to x, y and z.<br />

The elastic strain along m is<br />

d d-d d-d<br />

n m _ in o „, m o<br />

G s j_n<br />

m d d d<br />

o o<br />

where: dm is the interplanar spacing along m,<br />

d0 is the interplanar spacing with no stress and<br />

the change from the exact value d0 to the approximate value<br />

d, causes only a small error in era.<br />

Then:<br />

em = ew(cos 2 ip) YUW cosipsini|/<br />

and, for material exhibiting isotroplc elasticity:<br />

uw<br />

uw<br />

G<br />

where: ew, eu, yuw are normal and shear strains in the u,<br />

v, w coordinate system,<br />

a u> a v> a w anc ' T uw are n 01 "" 13 ! an( l shear stresses<br />

in the u, v, w coordinate system<br />

E, v, G are Young's modulus, Poisson's ratio and the shear<br />

modulus.<br />

The X-rays normally sample only a thin surface layer in which<br />

stress and structure gradients are small. With no surface tractions<br />

= Tuw = 0<br />

Eq.<br />

Eq. 3<br />

Eq. 3a<br />

Eq. 3b<br />

Eq. 3c

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