Question #51238

Derive an expression for the velocity of the transverse wave in the [100] direction in a
cubic crystal.
1

Expert's answer

2015-04-02T02:38:21-0400

Answer on Question #51238-Physics-Solid State Physics

Derive an expression for the velocity of the transverse wave in the [100] direction in a cubic crystal.

Solution

The equation of motion in the xx direction is


ρ2ut2=C112ux2+C44(2uy2+2uz2)+(C12+C44)(2vxy+2wxz).(a)\rho \frac {\partial^ {2} u}{\partial t ^ {2}} = C _ {1 1} \frac {\partial^ {2} u}{\partial x ^ {2}} + C _ {4 4} \left(\frac {\partial^ {2} u}{\partial y ^ {2}} + \frac {\partial^ {2} u}{\partial z ^ {2}}\right) + \left(C _ {1 2} + C _ {4 4}\right) \left(\frac {\partial^ {2} v}{\partial x \partial y} + \frac {\partial^ {2} w}{\partial x \partial z}\right). \quad (a)


The equation of motion in the yy direction is


ρ2vt2=C112vx2+C44(2vy2+2vz2)+(C12+C44)(2uxy+2wyz).(b)\rho \frac {\partial^ {2} v}{\partial t ^ {2}} = C _ {1 1} \frac {\partial^ {2} v}{\partial x ^ {2}} + C _ {4 4} \left(\frac {\partial^ {2} v}{\partial y ^ {2}} + \frac {\partial^ {2} v}{\partial z ^ {2}}\right) + \left(C _ {1 2} + C _ {4 4}\right) \left(\frac {\partial^ {2} u}{\partial x \partial y} + \frac {\partial^ {2} w}{\partial y \partial z}\right). \quad (b)


The equation of motion in the zz direction is


ρ2wt2=C112wx2+C44(2wy2+2wz2)+(C12+C44)(2uxz+2vyz).(c)\rho \frac {\partial^ {2} w}{\partial t ^ {2}} = C _ {1 1} \frac {\partial^ {2} w}{\partial x ^ {2}} + C _ {4 4} \left(\frac {\partial^ {2} w}{\partial y ^ {2}} + \frac {\partial^ {2} w}{\partial z ^ {2}}\right) + \left(C _ {1 2} + C _ {4 4}\right) \left(\frac {\partial^ {2} u}{\partial x \partial z} + \frac {\partial^ {2} v}{\partial y \partial z}\right). \quad (c)


here ρ\rho is the density and u,v,wu, v, w are the components of the displacement, CabC_{ab} are the elastic stiffness constants.

Consider a transverse or shear wave with the wavevector along the xx cube edge and with the particle displacement vv in the yy direction:


v=v0ei(Kxωt).v = v _ {0} e ^ {i (K x - \omega t)}.


On substitution in (b) this gives the dispersion relation


ω2ρ=C44K2;\omega^ {2} \rho = C _ {4 4} K ^ {2};


thus the velocity ωK\frac{\omega}{K} of a transverse wave in the [100] direction is


vs=(C44ρ)2.v _ {s} = \left(\frac {C _ {4 4}}{\rho}\right) ^ {2}.


The identical velocity is obtained if the particle displacement is in the zz direction.

Thus for KK parallel to [100] the two independent shear waves have equal velocities. This is not true for KK in a general direction in the crystal.

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