The velocity components in the x and y directions are given by U= $\lambda$xy3 – x2y, $v=xy^{2}-\frac{3}{4}y^{4}.$ . The value of $\lambda$ for a possible flow field involving an incompressible fluid is
(a) -$\frac{3}{4}$ (b)-$\frac{4}{3}$ (c)$\frac{4}{3}$ (d) 3
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