The rate of flow of liquid through a capillary tube is governed by the formula: \[ Q = \frac{\pi r^4 \Delta P}{8 \eta L} \] where: - \( Q \) is the rate of flow, - \( r \) is the radius of the capillary, - \( \Delta P \) is the pressure difference, - \( \eta \) is the viscosity of the liquid, - \( L \) is the length of the capillary tube.
Step 1: If the radius \( r \) is increased by 25%, the new radius \( r' \) will be: \[ r' = 1.25r \]
Step 2: The rate of flow \( Q \) is proportional to the fourth power of the radius, so the new rate of flow \( Q' \) will be: \[ Q' = \frac{\pi (r')^4 \Delta P}{8 \eta L} = \frac{\pi (1.25r)^4 \Delta P}{8 \eta L} \]
Step 3: Simplifying: \[ Q' = Q \times (1.25)^4 \] \[ (1.25)^4 = 2.4414 \] Thus, the new rate of flow will be approximately 144% of the original rate of flow. Hence, the rate of flow will change by \( \boxed{144\%} \).
A metal plate of area 10-2m2 rests on a layer of castor oil, 2 × 10-3m thick, whose viscosity coefficient is 1.55 Ns/m2. The approximate horizontal force required to move the plate with a uniform speed of 3 × 10-2ms-1 is: