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The co-efficient of friction ( both stat...

The co-efficient of friction ( both static and kinetic ), between the inclined plane and the block A of mass 1kg is `1 //sqrt(3)` whereas there is not friction between block B( 1 kg ) and the inclined plane. The system starts from rest. When the system covers a distance s=30m on the inclined plane,the cord between A and B is burnt off. The velocity of A when it coerse a further distance of 20m on the inclined plane is

A. zero
B. `sqrt( 120 ) m//s`
C. `sqrt( 150 ) m//s`
D. `sqrt( 300) m//s`

A

zero

B

`sqrt( 120 ) m//s`

C

`sqrt( 150 ) m//s`

D

`sqrt( 300) m//s`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, let's break it down into manageable parts. ### Step 1: Understanding the System We have two blocks, A and B, both with a mass of 1 kg. Block A is on an inclined plane with a coefficient of friction of \( \frac{1}{\sqrt{3}} \), while block B has no friction with the plane. The system starts from rest and travels a distance of 30 m before the cord connecting the two blocks is burnt. ### Step 2: Determine the Forces Acting on the Blocks 1. **For Block A**: - The forces acting on block A are: - Gravitational force down the incline: \( mg \sin \theta \) - Frictional force opposing the motion: \( f = \mu mg \cos \theta \) - Tension in the cord (before it is burnt): \( T \) 2. **For Block B**: - The only force acting on block B is the gravitational force down the incline: \( mg \sin \theta \). ### Step 3: Set Up the Equations of Motion 1. For Block B: \[ mg \sin \theta - T = ma \quad \text{(1)} \] 2. For Block A: \[ mg \sin \theta + T - f = ma \quad \text{(2)} \] where \( f = \mu mg \cos \theta \). ### Step 4: Combine the Equations Adding equations (1) and (2): \[ mg \sin \theta - T + mg \sin \theta + T - f = 2ma \] This simplifies to: \[ 2mg \sin \theta - f = 2ma \] Substituting \( f = \mu mg \cos \theta \): \[ 2mg \sin \theta - \mu mg \cos \theta = 2ma \] Dividing through by \( 2m \): \[ g \sin \theta - \frac{\mu g \cos \theta}{2} = a \] ### Step 5: Calculate the Acceleration Given \( g = 10 \, \text{m/s}^2 \), \( \mu = \frac{1}{\sqrt{3}} \), and \( \theta = 30^\circ \): - \( \sin 30^\circ = \frac{1}{2} \) - \( \cos 30^\circ = \frac{\sqrt{3}}{2} \) Substituting these values: \[ a = 10 \cdot \frac{1}{2} - \frac{\frac{1}{\sqrt{3}} \cdot 10 \cdot \frac{\sqrt{3}}{2}}{2} \] \[ = 5 - \frac{5}{2} = 5 - 2.5 = 2.5 \, \text{m/s}^2 \] ### Step 6: Find the Velocity After 30 m Using the equation of motion: \[ v^2 = u^2 + 2as \] where \( u = 0 \) (starts from rest), \( a = 2.5 \, \text{m/s}^2 \), and \( s = 30 \, \text{m} \): \[ v^2 = 0 + 2 \cdot 2.5 \cdot 30 = 150 \] Thus, \[ v = \sqrt{150} \, \text{m/s} \] ### Step 7: Analyze the Situation After the Cord is Burnt After the cord is burnt, block A continues to move under the influence of gravity and friction. The net force on block A is: \[ F_{\text{net}} = mg \sin \theta - f \] Substituting the values: \[ F_{\text{net}} = mg \sin \theta - \mu mg \cos \theta \] This results in zero net force, meaning block A will continue with the same velocity of \( \sqrt{150} \, \text{m/s} \) as it travels an additional 20 m. ### Conclusion The velocity of block A after it travels a further distance of 20 m is: \[ \sqrt{150} \, \text{m/s} \] ### Final Answer **Option C: \( \sqrt{150} \, \text{m/s} \)**
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