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1. The equation of continuity of a pure fluid is given as др at + V.pv = 0 a) In performing a derivation in fluid mechanics,

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Answer #1

Given

Continuity equation

\frac{\partial \rho}{\partial t}+\triangledown .\rho v=0

Where

\\ v=v_x i+v_yj+v_zk\ \ \ i,j,k\ are \ unit \ vector \ in \ x \ y \ z\ direction \\ \triangledown .\rho v=\frac{\partial \rho v_x }{\partial x}+\frac{\partial \rho v_y }{\partial y}+\frac{\partial \rho v_z }{\partial z} \\Applying\ product \ rule \\ \triangledown .\rho v=v.\triangledown \rho+\rho \triangledown .v=v_x\frac{\partial \rho }{\partial x}+ v_y\frac{\partial \rho }{\partial y}+v_z \frac{\partial \rho }{\partial z}+\rho (\frac{\partial v_x }{\partial x}+\frac{\partial v_y }{\partial y}+\frac{\partial v_z }{\partial z})

Applying in the continuity equation

\\ \frac{\partial \rho}{\partial t}+v.\triangledown \rho+\rho \triangledown .v=0 \ \ Eq1 \\ The \ total\ derivative\ of \rho \\ \frac{\mathrm{D}\rho }{\mathrm{D} t}=\frac{\partial \rho}{\partial t}+v_x\frac{\partial \rho }{\partial x}+ v_y\frac{\partial \rho }{\partial y}+v_z \frac{\partial \rho }{\partial z}=\frac{\partial \rho}{\partial t}+v.\triangledown \rho \\ Applying \ in \ Eq1 \\ \frac{\mathrm{D} \rho}{\mathrm{D} t}+\rho\triangledown .v=0 \\ \frac{\mathrm{D} \rho}{\mathrm{D} t}=-\rho\triangledown .v\ \ \ Eq2

We need to find

\\ \frac{\mathrm{D} ln \rho }{\mathrm{D} x} \\ Applying \ chain\ rule \\ \frac{\mathrm{D} ln \rho }{\mathrm{D} t}=\frac{\partial ln\rho}{\partial \rho}* \frac{\mathrm{D} \rho }{\mathrm{D} t}=\frac{1}{\rho} \frac{\mathrm{D} \rho }{\mathrm{D} t} \\ Using \ Eq2 \\ \frac{\mathrm{D} ln \rho }{\mathrm{D} t}=\frac{1}{\rho}*-\rho\triangledown .v=-\triangledown .v

So the solution is

\\ \frac{\mathrm{D} ln \rho }{\mathrm{D} t}=-\triangledown .v=-(\frac{\partial v_x }{\partial x}+\frac{\partial v_y }{\partial y}+\frac{\partial v_z }{\partial z})

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