The velocity components in the x and y directions of a two dimensional potential flow are u and v, respectively. Then $\frac{\partial u}{\rho y}$ is equal to
(a) $\frac{\partial v}{\rho x}$ (b)$-\frac{\partial v}{\rho x}$
(c) $\frac{\partial v}{\rho y}$ (d) $-\frac{\partial v}{\rho y}$
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