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A body starts from rest on a long inclin...

A body starts from rest on a long inclined plane of slope `45^(@)` . The coefficient of friction between the body and the plane varies as `mu = 0.3 x` , where x is the distance travelled down the plane. The body will have maximum speed (for `g = 10 m//s^(2)` ) when x =

A

9.8 m

B

12 m

C

12 m

D

3.33 m

Text Solution

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The correct Answer is:
To solve the problem, we need to analyze the forces acting on the body as it moves down the inclined plane. Here’s a step-by-step solution: ### Step 1: Identify the forces acting on the body The forces acting on the body are: 1. The gravitational force acting down the slope: \( F_{\text{gravity}} = mg \sin \theta \) 2. The normal force acting perpendicular to the slope: \( F_{\text{normal}} = mg \cos \theta \) 3. The frictional force acting up the slope: \( F_{\text{friction}} = \mu F_{\text{normal}} = \mu mg \cos \theta \) ### Step 2: Write the expression for the net force The net force acting on the body as it moves down the incline can be expressed as: \[ F_{\text{net}} = F_{\text{gravity}} - F_{\text{friction}} = mg \sin \theta - \mu mg \cos \theta \] ### Step 3: Substitute the values Given that the angle of inclination \( \theta = 45^\circ \), we know: - \( \sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}} \) - The coefficient of friction is given as \( \mu = 0.3x \) Substituting these values into the net force equation: \[ F_{\text{net}} = mg \left( \frac{1}{\sqrt{2}} \right) - (0.3x) mg \left( \frac{1}{\sqrt{2}} \right) \] Factoring out \( mg \frac{1}{\sqrt{2}} \): \[ F_{\text{net}} = mg \frac{1}{\sqrt{2}} \left( 1 - 0.3x \right) \] ### Step 4: Relate net force to acceleration According to Newton's second law, \( F_{\text{net}} = ma \), where \( a \) is the acceleration of the body. Thus: \[ ma = mg \frac{1}{\sqrt{2}} \left( 1 - 0.3x \right) \] Dividing both sides by \( m \): \[ a = g \frac{1}{\sqrt{2}} \left( 1 - 0.3x \right) \] ### Step 5: Set the acceleration to zero for maximum speed The body will reach maximum speed when the acceleration becomes zero: \[ 0 = g \frac{1}{\sqrt{2}} \left( 1 - 0.3x \right) \] This implies: \[ 1 - 0.3x = 0 \] Solving for \( x \): \[ 0.3x = 1 \implies x = \frac{1}{0.3} = \frac{10}{3} \approx 3.33 \text{ meters} \] ### Conclusion The body will have maximum speed when \( x = 3.33 \) meters.

To solve the problem, we need to analyze the forces acting on the body as it moves down the inclined plane. Here’s a step-by-step solution: ### Step 1: Identify the forces acting on the body The forces acting on the body are: 1. The gravitational force acting down the slope: \( F_{\text{gravity}} = mg \sin \theta \) 2. The normal force acting perpendicular to the slope: \( F_{\text{normal}} = mg \cos \theta \) 3. The frictional force acting up the slope: \( F_{\text{friction}} = \mu F_{\text{normal}} = \mu mg \cos \theta \) ...
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