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¶ 3. Mathematical Representation of Crystal Orientation, Misorientation

¶ 3. Mathematical Representation of Crystal Orientation, Misorientation

¶ 3. Mathematical Representation of Crystal Orientation, Misorientation

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Analysis. He labels the crystal axes as K A and the crystal axes as K B; the specimen axes<br />

are X, Y & Z, and the crystal axes are X’, Y’ & Z’.<br />

<strong>3.</strong>C.2 Correspondence between Matrices<br />

Given the orientation matrix derived from Euler angles and the matrix derived from<br />

direction cosines, one can immediately see how to convert between the various<br />

descriptions because each pair <strong>of</strong> corresponding entries must be identical to each other.<br />

That is to say, b 1 in the first matrix = cosφ 1 cosφ 2− sinφ 1 sinφ 2 cosΦ, etc.<br />

b1 Sample<br />

t1 n1 ⎛ ⎞<br />

⎜ ⎟<br />

aij = <strong>Crystal</strong><br />

⎜<br />

b2 t2 n2 ⎟<br />

⎜ ⎟<br />

⎝ b3 t3 n3 ⎠<br />

⎛ cosϕ1 cosϕ 2 − sinϕ1 sinϕ 2 cosΦ sinϕ1 cosϕ 2 + cosϕ1 sinϕ 2 cosΦ<br />

⎜<br />

≡<br />

⎜<br />

−cosϕ1 sinϕ 2 − sinϕ1 cosϕ 2 cosΦ −sinϕ1 sinϕ 2 + cosϕ1 cosϕ 2 cosΦ<br />

⎜<br />

€<br />

⎝ sinϕ1 sinΦ −cosϕ1 sinΦ<br />

sinϕ 2 sinΦ⎞<br />

⎟<br />

cosϕ 2 sinΦ<br />

⎟<br />

cosΦ ⎠<br />

This permit Euler angles to be converted to Miller indices by extracting the first and third<br />

€ columns <strong>of</strong> the orientation matrix, and re-scaling each (unit) vector to have suitable<br />

integer values.<br />

More conversions are given below.<br />

<strong>3.</strong>C.3 Other definitions € <strong>of</strong> Euler angles<br />

h = n sin Φ sinϕ 2<br />

k = n sin Φ cosϕ 2<br />

l = n cosΦ<br />

( )<br />

u = n ′ cosϕ1 cosϕ 2 − sinϕ1 sinϕ 2 cosΦ<br />

v = n ′ ( − cosϕ1 sinϕ 2 − sinϕ1 cosϕ 2 cosΦ)<br />

w = n ′ sin Φ sinϕ1 The other conventions are those <strong>of</strong> Roe [Roe, R. J. (1965). “Description <strong>of</strong><br />

<strong>Crystal</strong>lite <strong>Orientation</strong> in Polycrystalline Materials. <strong>3.</strong> General Solution to Pole Figure<br />

Inversion”, Journal <strong>of</strong> Applied Physics 36 2024], who developed an analysis in parallel<br />

with Bunge), Matthies and Kocks. The main difference between the Bunge convention<br />

and the others is that the second rotation (Θ above) is about the (rotated) X-axis, whereas<br />

in all the other conventions it is about the (rotated) Y-axis. From the (Russian) physics<br />

literature, Borisenko and Tarapov (Vector and Tensor Analysis, Dover) call them the<br />

precession, nutation and pure rotation angles, respectively, and follow the Bunge<br />

convention. Other physics literature follows the Roe convention; it would be interesting<br />

to know how the west and east came to take different approaches to Euler angles!<br />

8/27/09 8

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