A spherical ball of radius \(1\) mm and density \(10.5\) g/cc is dropped in glycerine of coefficient of viscosity \(9.8\) poise and density \(1.5\) g/cc. Viscous force on the ball when it attains constant velocity is \(3696\times 10^{-x}\) N. The value of \(x\) is (Given, \(g = 9.8\text{ m}/\text{s}^2\) and \(π = \frac{22}{7}\))
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At constant velocity the viscous force equals the weight minus the buoyant force.