Show that rays in a linear velocity gradient of the form v = a + bz will have ray
paths that are circular. Derive an expression for the radius of the circle in terms of
b and the ray parameter p. (It is also possible to derive a more general constraint,
applying to ray geometries for linear velocity gradients in anisotropic media (see
Shearer and Chapman, 1988); the circular result for isotropic media follows as a
special case.)
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