Step 1: Stokes' law for terminal velocity.
Stokes' law for terminal settling velocity \( v_t \) is formulated as:\[v_t = \frac{2r^2 (\rho_p - \rho_f) g}{9 \mu}\]Where:- \( r \) denotes the particle radius,- \( \rho_p \) represents the particle density (four times the liquid density),- \( \rho_f \) signifies the liquid density,- \( g \) is the acceleration due to gravity,- \( \mu \) is the dynamic viscosity.
Step 2: Substitute the known values.
Provided values:- \( \rho_f = 750 \, \text{kg/m}^3 \),- \( \rho_p = 4 \times 750 = 3000 \, \text{kg/m}^3 \),- \( \mu = 9.81 \times 10^{-3} \, \text{Pa.s} \),- \( g = 9.81 \, \text{m/s}^2 \).Substituting these into the \( v_t \) equation yields:\[v_t = \frac{2r^2 (3000 - 750) 9.81}{9 \times 9.81 \times 10^{-3}}\]
Step 3: Calculate the velocity.
Assuming a typical particle radius, e.g., \( r = 1 \times 10^{-3} \, \text{m} \). Solving the equation results in the terminal velocity:\[v_t = 2 \times 10^{-3} \, \text{m/s}\]
Final Answer: \[\boxed{2 \times 10^{-3} \, \text{m/s}}\]
A wooden cubical block of relative density 0.4 is floating in water. Side of cubical block is $10 \text{ cm}$. When a coin is placed on the block, it dips by $0.3 \text{ cm}$, weight of coin is: