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Starting from rest a body slides down a ...

Starting from rest a body slides down a `45^(@)` inclined plane in twice the time it takes to slide down the same distance in the absence of friction. The coefficient of the body and the inclined plane is :

A

0.2

B

0.25

C

0.75

D

0.5

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To solve the problem of finding the coefficient of friction between a body and a 45-degree inclined plane, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Problem:** - We have a body sliding down a 45-degree inclined plane. - The body starts from rest and takes twice the time to slide down the same distance when friction is present compared to when it is absent. 2. **Case 1: Frictionless Incline** - When there is no friction, the only force acting on the body is the component of gravitational force along the incline. - The acceleration \( a_1 \) of the body is given by: \[ a_1 = g \sin \theta \] where \( \theta = 45^\circ \). Thus, \( \sin 45^\circ = \frac{1}{\sqrt{2}} \), and we have: \[ a_1 = g \cdot \frac{1}{\sqrt{2}} = \frac{g}{\sqrt{2}} \] 3. **Using the Equation of Motion:** - The distance \( s \) covered in time \( t \) can be expressed as: \[ s = ut + \frac{1}{2} a_1 t^2 \] Since the body starts from rest, \( u = 0 \): \[ s = \frac{1}{2} a_1 t^2 = \frac{1}{2} \cdot \frac{g}{\sqrt{2}} t^2 \] 4. **Case 2: Incline with Friction** - When friction is present, the net force acting on the body is: \[ F = mg \sin \theta - \mu mg \cos \theta \] - The acceleration \( a_2 \) can be expressed as: \[ a_2 = g \sin \theta - \mu g \cos \theta \] Substituting \( \theta = 45^\circ \): \[ a_2 = g \cdot \frac{1}{\sqrt{2}} - \mu g \cdot \frac{1}{\sqrt{2}} = \frac{g}{\sqrt{2}}(1 - \mu) \] 5. **Using the Equation of Motion for Case 2:** - The time taken to slide down with friction is \( 2t \): \[ s = u(2t) + \frac{1}{2} a_2 (2t)^2 \] Again, since \( u = 0 \): \[ s = \frac{1}{2} a_2 (2t)^2 = 2 a_2 t^2 \] - Substituting for \( a_2 \): \[ s = 2 \left(\frac{g}{\sqrt{2}}(1 - \mu)\right) t^2 \] 6. **Equating Distances:** - Since both cases cover the same distance \( s \): \[ \frac{1}{2} \cdot \frac{g}{\sqrt{2}} t^2 = 2 \left(\frac{g}{\sqrt{2}}(1 - \mu)\right) t^2 \] - Simplifying gives: \[ \frac{1}{2} = 4(1 - \mu) \] - Rearranging: \[ 1 - \mu = \frac{1}{8} \] \[ \mu = 1 - \frac{1}{8} = \frac{7}{8} \] 7. **Final Calculation:** - The coefficient of friction \( \mu \) is: \[ \mu = 0.875 \] ### Conclusion: The coefficient of friction between the body and the inclined plane is \( \mu = 0.875 \).

To solve the problem of finding the coefficient of friction between a body and a 45-degree inclined plane, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Problem:** - We have a body sliding down a 45-degree inclined plane. - The body starts from rest and takes twice the time to slide down the same distance when friction is present compared to when it is absent. ...
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