Right option is (c) \(\frac{∂τ_{xz}}{∂x} +\frac{∂τ_{yz}}{∂y} +\frac{∂σ_z}{∂z} +Z=0\)
Explanation: The sum of forces acting on the element in the z-direction is given by,
\(\{(σ_z+\frac{∂σ_z}{∂z}\frac{dz}{2})dx.dy-(σ_z-\frac{∂σ_z}{∂z} \frac{dz}{2})dx.dy\} +
\{(τ_{zx}+\frac{∂τ_{zx}}{∂x} \frac{dx}{2})dz.dy-(τ_{zx}-\frac{∂τ_{zx}}{∂x}\frac{dx}{2})dz.dy\} +\)
\( \{(τ_{yz}+\frac{∂τ_{yz}}{∂y} \frac{dy}{2})dz.dx-(τ_{yz}-\frac{∂τ_{yz}}{∂y}\frac{dy}{2})dz.dx\} + Zdx.dy.dz = 0\)
Now dividing all the terms by dx.dy.dz we get,
\(\frac{∂τ_{xz}}{∂x} +\frac{∂τ_{yz}}{∂y} +\frac{∂σ_z}{∂z} +Z=0.\)