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A horizontal force applied on a body on ...

A horizontal force applied on a body on a rough horizontal surface produces an acceleration 'a'. If coefficient of friction between the body & surface which is m is reduced to m/3, the accele-ration increases by 2 units. The value of m is

A

2/3kg

B

3/2kg

C

3/g

D

1/g

Text Solution

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The correct Answer is:
To solve the problem step by step, we will analyze the forces acting on the body and use Newton's second law of motion. ### Step 1: Understand the forces acting on the body When a horizontal force \( F \) is applied to a body on a rough surface, the frictional force \( f \) opposes the motion. The frictional force can be expressed as: \[ f = \mu N \] where \( \mu \) is the coefficient of friction and \( N \) is the normal force. For a horizontal surface, \( N = mg \), where \( m \) is the mass of the body and \( g \) is the acceleration due to gravity. ### Step 2: Set up the equations for the two cases 1. **Case 1**: When the coefficient of friction is \( \mu = m \), the acceleration \( a \) is given by: \[ F - f = ma \] Substituting for \( f \): \[ F - \mu mg = ma \quad \text{(1)} \] 2. **Case 2**: When the coefficient of friction is reduced to \( \mu = \frac{m}{3} \), the new acceleration becomes \( a + 2 \): \[ F - f' = m(a + 2) \] where \( f' = \frac{m}{3} mg \): \[ F - \frac{m}{3} mg = m(a + 2) \quad \text{(2)} \] ### Step 3: Rearranging the equations From equation (1): \[ F = ma + \mu mg \] From equation (2): \[ F = m(a + 2) + \frac{m}{3} mg \] ### Step 4: Equate the two expressions for \( F \) Setting the two expressions for \( F \) equal to each other: \[ ma + \mu mg = m(a + 2) + \frac{m}{3} mg \] ### Step 5: Substitute \( \mu \) and simplify Substituting \( \mu = m \): \[ ma + m \cdot mg = m(a + 2) + \frac{m}{3} mg \] This simplifies to: \[ ma + m^2g = ma + 2m + \frac{m}{3}g \] Cancelling \( ma \) from both sides: \[ m^2g = 2m + \frac{m}{3}g \] ### Step 6: Combine like terms Rearranging gives: \[ m^2g - \frac{m}{3}g = 2m \] Factoring out \( g \): \[ g\left(m^2 - \frac{m}{3}\right) = 2m \] ### Step 7: Solve for \( m \) Dividing through by \( m \) (assuming \( m \neq 0 \)): \[ g\left(m - \frac{1}{3}\right) = 2 \] Rearranging gives: \[ m - \frac{1}{3} = \frac{2}{g} \] Thus: \[ m = \frac{2}{g} + \frac{1}{3} \] ### Step 8: Find a common denominator and simplify To combine the fractions: \[ m = \frac{6}{3g} + \frac{1}{3} = \frac{6 + 1g}{3g} \] Thus: \[ m = \frac{6 + g}{3g} \] ### Final Answer To find the specific value of \( m \), we can substitute \( g \) with \( 9.8 \, \text{m/s}^2 \) or leave it in terms of \( g \) for a general solution.
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Knowledge Check

  • Two blocks A and B of masses 10 kg and 15 kg are placed in contact with each other rest on a rough horizontal surface as shown in the figure. The coefficient of friction between the blocks and surface is 0.2. A horizontal force of 200 N is applied to block A. The acceleration of the system is ("Take g"=10ms^(-2))

    A
    `4"ms"^(-2)`
    B
    `6"ms"^(-2)`
    C
    `8"ms"^(-2)`
    D
    `10"ms"^(-2)`
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