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A spherical ball of radius 3xx10^(-4)m a...

A spherical ball of radius `3xx10^(-4)`m and density `10^(4)kg//m^(3)` falls freely under gravity through a distance h before entering a tank of water. If after entering the water the velocity of the ball does not change, find h the viscosity of water is `9.8xx10^(-6)N-s//m^(2)`

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To solve the problem step by step, we need to follow these steps: ### Step 1: Understand the Forces Acting on the Ball When the spherical ball enters the water, three forces act on it: 1. The gravitational force (weight) acting downwards: \( F_g = mg \) 2. The buoyant force acting upwards: \( F_b = \rho_w V g \) 3. The viscous force acting upwards: \( F_v = 6 \pi r \eta v_t \) At terminal velocity, the net force acting on the ball is zero, which means: \[ F_g - F_b - F_v = 0 \] ### Step 2: Calculate the Mass of the Ball The mass \( m \) of the ball can be calculated using its density and volume: \[ m = \rho_b V \] Where: - \( \rho_b = 10^4 \, \text{kg/m}^3 \) (density of the ball) - \( V = \frac{4}{3} \pi r^3 \) (volume of the sphere) Given \( r = 3 \times 10^{-4} \, \text{m} \): \[ V = \frac{4}{3} \pi (3 \times 10^{-4})^3 = \frac{4}{3} \pi (27 \times 10^{-12}) = 36 \pi \times 10^{-12} \, \text{m}^3 \] Now, substituting in the mass: \[ m = 10^4 \times 36 \pi \times 10^{-12} = 36 \pi \times 10^{-8} \, \text{kg} \] ### Step 3: Calculate the Gravitational Force The gravitational force acting on the ball is: \[ F_g = mg = (36 \pi \times 10^{-8}) g \] Using \( g = 10 \, \text{m/s}^2 \): \[ F_g = 36 \pi \times 10^{-8} \times 10 = 36 \pi \times 10^{-7} \, \text{N} \] ### Step 4: Calculate the Buoyant Force The buoyant force is given by: \[ F_b = \rho_w V g \] Where: - \( \rho_w = 10^3 \, \text{kg/m}^3 \) (density of water) - \( V = 36 \pi \times 10^{-12} \, \text{m}^3 \) Thus, \[ F_b = 10^3 \times 36 \pi \times 10^{-12} \times 10 = 36 \pi \times 10^{-9} \, \text{N} \] ### Step 5: Set Up the Equation for Terminal Velocity At terminal velocity, the forces balance: \[ F_g - F_b - F_v = 0 \] Substituting the forces: \[ 36 \pi \times 10^{-7} - 36 \pi \times 10^{-9} - 6 \pi r \eta v_t = 0 \] ### Step 6: Solve for Terminal Velocity Rearranging gives: \[ 36 \pi \times 10^{-7} - 36 \pi \times 10^{-9} = 6 \pi (3 \times 10^{-4}) (9.8 \times 10^{-6}) v_t \] Factoring out \( 36 \pi \): \[ 36 \pi (10^{-7} - 10^{-9}) = 6 \pi (3 \times 10^{-4}) (9.8 \times 10^{-6}) v_t \] Cancel \( \pi \) and simplify: \[ 36 (10^{-7} - 10^{-9}) = 6 (3 \times 10^{-4}) (9.8 \times 10^{-6}) v_t \] Calculating \( 10^{-7} - 10^{-9} = 0.099 \times 10^{-7} \): \[ 36 \times 0.099 \times 10^{-7} = 6 \times 3 \times 10^{-4} \times 9.8 \times 10^{-6} v_t \] ### Step 7: Calculate Terminal Velocity Solving for \( v_t \): \[ v_t = \frac{36 \times 0.099 \times 10^{-7}}{6 \times 3 \times 10^{-4} \times 9.8 \times 10^{-6}} \] Calculating gives: \[ v_t \approx 0.1836 \, \text{m/s} \] ### Step 8: Calculate the Height \( h \) Using the equation of motion: \[ v^2 = u^2 + 2gh \] Where \( u = 0 \): \[ (0.1836)^2 = 0 + 2 \times 10 \times h \] \[ h = \frac{(0.1836)^2}{20} \] Calculating gives: \[ h \approx 0.16868 \, \text{m} \] ### Final Answer Thus, the height \( h \) from which the ball fell is approximately: \[ h \approx 1.6868 \, \text{m} \] ---
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