Concept:
Continutiy equation in Three-Dimension
\(\frac{{\partial {\rm{\rho }}}}{{\partial {\rm{t}}}} + \frac{{\partial \left( {{\rm{\rho U}}} \right)}}{{\partial {\rm{X}}}} + \frac{{\partial \left( {{\rm{\rho V}}} \right)}}{{\partial {\rm{Y}}}} + \frac{{\partial \left( {{\rm{\rho W}}} \right)}}{{\partial {\rm{Z}}}} = 0{\rm{;}}\)
Where,
U, V, and W are components of velocity in X, Y and Z direction respectively
When the flow is steady\(,;;\frac{{\partial {\bf{\rho }}}}{{\partial {\bf{t}}}} = 0\)
\(\therefore \frac{{{\rm{\partial }}\left( {{\rm{\rho U}}} \right)}}{{{\rm{\partial X}}}} + \frac{{{\rm{\partial }}\left( {{\rm{\rho V}}} \right)}}{{{\rm{\partial Y}}}} + \frac{{{\rm{\partial }}\left( {{\rm{\rho W}}} \right)}}{{{\rm{\partial Z}}}} = 0\)
When flow is steady and incompressible, ρ = constant
\(\therefore \frac{{\partial {\rm{U}}}}{{\partial {\rm{X}}}} + \frac{{\partial {\rm{V}}}}{{\partial {\rm{Y}}}} + \frac{{\partial {\rm{W}}}}{{\partial {\rm{Z}}}} = 0{\rm{;}}\)
When the flow is steady, incompressible and 2-D, \(\frac{{\partial {\bf{W}}}}{{\partial {\bf{Z}}}} = 0\)
\(\therefore \frac{{\partial {\rm{U}}}}{{\partial {\rm{X}}}} + \frac{{\partial {\rm{V}}}}{{\partial {\rm{Y}}}} = 0{\rm{;}}\)
For flow being irrotational
\( \frac{{\partial {\rm{V}}}}{{\partial {\rm{X}}}} - \frac{{\partial {\rm{U}}}}{{\partial {\rm{Y}}}} = 0{\rm{;}}\)
Calculation:
Given:
\(\begin{array}{l} U = \frac{{{y^3}}}{3} + 2x - {x^2}y\ V = x{y^2} - 2y - \frac{{{x^3}}}{3} \end{array}\)
As per continuity equation, for flow to occur
\(\therefore \frac{{\partial {\rm{U}}}}{{\partial {\rm{X}}}} + \frac{{\partial {\rm{V}}}}{{\partial {\rm{Y}}}} = 0{\rm{;}}\)
\(\begin{array}{l} \frac{{\partial {\rm{U}}}}{{\partial {\rm{X}}}} = 2 - 2xy\ \frac{{\partial {\rm{V}}}}{{\partial {\rm{Y}}}} = 2xy - 2 \end{array}\)
2 - 2xy + 2xy - 2 = 0
Since, \(\frac{{\partial {\rm{U}}}}{{\partial {\rm{X}}}} + \frac{{\partial {\rm{V}}}}{{\partial {\rm{Y}}}} = 0{\rm{;}}\), then flow is incompressible.
For irrational flow
\(\begin{array}{l} \frac{{\partial {\rm{V}}}}{{\partial {\rm{X}}}} = {y^2} - {x^2}\ \frac{{\partial {\rm{U}}}}{{\partial {\rm{Y}}}} = {y^2} - {x^2} \end{array}\)
\( \frac{{\partial {\rm{V}}}}{{\partial {\rm{X}}}} - \frac{{\partial {\rm{U}}}}{{\partial {\rm{Y}}}} = 0{\rm{;}}\)
So, flow is irrotational also.