The Stoke’s Law states that when a spherical object of radius \(R\) is falling at velocity \(v\) in a fluid, the resistance force \(F\) acting on the sphere is given by
\(F=-6\pi \eta Rv\),
where \(\eta \) is the coefficient of viscosity of the fluid. The following table shows the coefficients of viscosity of various fluids at \({{25}^{{}^\circ }}\mathrm{C}\):
| Fluid | Coefficient of viscosity, \(\eta\text{ kg m}^{-1}\text{ s}^{-1}\) |
|---|---|
| Acetone | \(3.06 \times 10^{-4}\) |
| Benzene | \(1.81 \times 10^{-5}\) |
| Castor Oil | \(0.985\) |
| Corn Syrup | \(1.3806\) |
| Ethanol | \(1.074 \times 10^{-3}\) |
| Methanol | \(5.44 \times 10^{-4}\) |
| Olive Oil | \(8.1 \times 10^{-2}\) |
A spherical ball of radius \(0.05\) m and mass \(0.2\) kg is released from rest in a huge container filled with corn syrup at \({{25}^{{}^\circ }}\mathrm{C}\). It can be shown that as the ball falls through the corn syrup, the velocity \(v\) in \(\mathrm{m}{{\mathrm{s}}^{-1}}\) at time \(t\) seconds after release satisfies the differential equation:
\(\frac{\mathrm{d}v}{\mathrm{d}t}+\frac{6\pi \,\eta \,R}{m}v=g\),
where \(g=9.780\)ms\(^{-2}\) is the acceleration due to gravity and \(m\) kg is the mass of the ball.
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