The velocity profile in fully developed laminar flow in a pipe of diameter D is given by u = u0(1 – 4r2 / D2), where r is the radial distance from the centre. If the viscosity of the fluid is m, the pressure drop across a length L of the pipe is
(a) $\frac{\mu \mu _{0}}{D_{2}}$ (b) $\frac{4\mu \mu _{0}}{D_{2}}$
(c)$\frac{8\mu \mu _{0}}{D_{2}}$ (d)$\frac{16\mu \mu _{0}}{D_{2}}$