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: \[ \boxed{2 \times 10^{-3} \, \text{m/s}} \]

