Q-3 A continuum bcc structure is deformed elastically by x, y, and z directional mechanical forces (Shear type). Find the propagation speed (vs) (for both longitudinal and transverse vibrations) of the elastic waves propagating along [111] direction to dissipate the gained elastic energy through the sample. The necessary equations can be obtained from the equation given below for the displacement vector R = R₂ + R₂ŷ + R₂2 p(0²Rx/t²) = C₁1(@²Rx / x²)+ C44 (0²Rx/y²+ ²Rx /z²)+(C12+C44)(@²Ry/Ox0y+ O²R₂/0x0z) Here, C11, C44, C12 and p are the moduli of elasticity (Stiffness constants) and the mass density of the bcc structure, respectively.

Elements Of Electromagnetics
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Q-3
mechanical forces (Shear type). Find the propagation speed (vs) (for both longitudinal and
transverse vibrations) of the elastic waves propagating along [111] direction to dissipate the
gained elastic energy through the sample. The necessary equations can be obtained from the
equation given below for the displacement vector
A continuum bcc structure is deformed elastically by x, y, and z directional
R = R,& + Ryỹ + R22
p(ô²R/@t) = C11(8²R$ /ôx²)+ C44 (a²R¾/@y²+ ô²Rx /ô z²)+(C12+C4)(ô²Ry/ Ô x ô y+ ô²Rz/@xð z)
Here, C11, C44, C12 and p are the moduli of elasticity (Stiffness constants) and the mass density
of the bcc structure, respectively.
Transcribed Image Text:Q-3 mechanical forces (Shear type). Find the propagation speed (vs) (for both longitudinal and transverse vibrations) of the elastic waves propagating along [111] direction to dissipate the gained elastic energy through the sample. The necessary equations can be obtained from the equation given below for the displacement vector A continuum bcc structure is deformed elastically by x, y, and z directional R = R,& + Ryỹ + R22 p(ô²R/@t) = C11(8²R$ /ôx²)+ C44 (a²R¾/@y²+ ô²Rx /ô z²)+(C12+C4)(ô²Ry/ Ô x ô y+ ô²Rz/@xð z) Here, C11, C44, C12 and p are the moduli of elasticity (Stiffness constants) and the mass density of the bcc structure, respectively.
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