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A small wooden block of density 400 kg//...

A small wooden block of density `400 kg//m^(3)` is released from rest inside a swimming pool filled with water of density `10^(3)kg//m^(3)`. The acceleration of the block just after it is released is __________ `m//s^(2) (g=10 m//s^(2))`

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To find the acceleration of the wooden block just after it is released in water, we can follow these steps: ### Step 1: Identify the Given Data - Density of the wooden block, \( \rho_b = 400 \, \text{kg/m}^3 \) - Density of water, \( \rho_w = 1000 \, \text{kg/m}^3 \) - Acceleration due to gravity, \( g = 10 \, \text{m/s}^2 \) ### Step 2: Determine the Forces Acting on the Block When the block is submerged in water, two main forces act on it: 1. The weight of the block (\( W \)) acting downwards: \[ W = mg = \rho_b V g \] where \( V \) is the volume of the block. 2. The buoyant force (\( F_b \)) acting upwards, which is equal to the weight of the water displaced by the block: \[ F_b = \rho_w V g \] ### Step 3: Calculate the Net Force Acting on the Block The net force (\( F_{net} \)) acting on the block can be calculated as: \[ F_{net} = F_b - W \] Substituting the expressions for \( F_b \) and \( W \): \[ F_{net} = \rho_w V g - \rho_b V g \] Factoring out \( Vg \): \[ F_{net} = Vg (\rho_w - \rho_b) \] ### Step 4: Apply Newton's Second Law According to Newton's second law, the net force is also equal to the mass of the block times its acceleration (\( a \)): \[ F_{net} = ma \] The mass of the block (\( m \)) is given by: \[ m = \rho_b V \] Thus, we can write: \[ Vg (\rho_w - \rho_b) = \rho_b V a \] ### Step 5: Simplify the Equation Dividing both sides by \( V \) (assuming \( V \neq 0 \)): \[ g (\rho_w - \rho_b) = \rho_b a \] Now, solving for \( a \): \[ a = \frac{g (\rho_w - \rho_b)}{\rho_b} \] ### Step 6: Substitute the Values Substituting the known values: \[ a = \frac{10 \, \text{m/s}^2 \times (1000 \, \text{kg/m}^3 - 400 \, \text{kg/m}^3)}{400 \, \text{kg/m}^3} \] \[ a = \frac{10 \, \text{m/s}^2 \times 600 \, \text{kg/m}^3}{400 \, \text{kg/m}^3} \] \[ a = \frac{6000 \, \text{m/s}^2}{400} \] \[ a = 15 \, \text{m/s}^2 \] ### Final Answer The acceleration of the block just after it is released is \( 15 \, \text{m/s}^2 \). ---

To find the acceleration of the wooden block just after it is released in water, we can follow these steps: ### Step 1: Identify the Given Data - Density of the wooden block, \( \rho_b = 400 \, \text{kg/m}^3 \) - Density of water, \( \rho_w = 1000 \, \text{kg/m}^3 \) - Acceleration due to gravity, \( g = 10 \, \text{m/s}^2 \) ### Step 2: Determine the Forces Acting on the Block ...
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Knowledge Check

  • A wooden block of mass 1kg and density 800 Kg m^(-3) is held stationery, with the help of a string, in a container filled with water of density 1000 kg m^(-3) as shown in the figure. If the container is moved upwards with an acceleration of 2 m s^(-2) , then the tension in the string will be ( take g=10ms^(-2) )

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    2N
    B
    3N
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  • A wooden block of density 860 kg//m^(3) at 0^(@)C is floating on bezene liquid of density 900 kg/m^(3) at 0^(@)C . The temperature at which the block just submerge in benzene is [gamma_(wo od)=8xx10^(-5//@)c, gamma_("benzene")=12xx10^(-4//@)c]

    A
    `24^(@)c`
    B
    `42^(@)c`
    C
    `16^(@)c`
    D
    `32^(@)c`
  • A sphere of radius 10cm and density 500kg//m^(3) is under water of density 1000kg//m^(3) The acceleration of the sphere is 9.80m//s^(2) upward viscosity of water is 1.0 centipoise if g=9.81m//s^(2) the velocity of the sphere is

    A
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    B
    `10m//s`
    C
    `11m//s`
    D
    `12m//s`
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