Step 1: Stokes' law for terminal velocity.
Stokes' law for terminal settling velocity \( v_t \) is given by:
\[
v_t = \frac{2r^2 (\rho_p - \rho_f) g}{9 \mu}
\]
Where:
- \( r \) is the radius of the particle,
- \( \rho_p \) is the particle density (4 times liquid density),
- \( \rho_f \) is the liquid density,
- \( g \) is the acceleration due to gravity,
- \( \mu \) is the dynamic viscosity.
Step 2: Substitute the known values.
Given:
- \( \rho_f = 750 \, \text{kg/m}^3 \),
- \( \rho_p = 4 \times 750 = 3000 \, \text{kg/m}^3 \),
- \( \mu = 9.81 \times 10^{-3} \, \text{Pa.s} \),
- \( g = 9.81 \, \text{m/s}^2 \).
Substitute these values into the equation for \( v_t \):
\[
v_t = \frac{2r^2 (3000 - 750) 9.81}{9 \times 9.81 \times 10^{-3}}
\]
Step 3: Calculate the velocity.
Assume a typical particle size, for example, \( r = 1 \times 10^{-3} \, \text{m} \). After solving the equation, we get the terminal velocity:
\[
v_t = 2 \times 10^{-3} \, \text{m/s}
\]
Final Answer: \[ \boxed{2 \times 10^{-3} \, \text{m/s}} \]
A cube of side 10 cm is suspended from one end of a fine string of length 27 cm, and a mass of 200 grams is connected to the other end of the string. When the cube is half immersed in water, the system remains in balance. Find the density of the cube.
Match List-I with List-II 

