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A particle of mass m initially moving wi...

A particle of mass m initially moving with speed v.A force acts on the particle f=kx where x is the distance travelled by the particle and k is constant. Find the speed of the particle when the work done by the force equals W.

A

`sqrt((k)/(m)+v^(2))`

B

`sqrt((2W)/(m)+v^(2))`

C

`sqrt((2W)/(k)+v^(2))`

D

`sqrt((W)/(2m)+v^(2))`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the speed of a particle of mass \( m \) when the work done by the force \( F = kx \) equals \( W \). Here are the steps to derive the solution: ### Step 1: Understand the Work Done by the Force The work done \( W \) by a variable force can be expressed as: \[ W = \int F \, dx \] In this case, the force \( F \) is given by \( F = kx \). Therefore, the work done as the particle moves from \( 0 \) to \( x \) is: \[ W = \int_0^x kx' \, dx' = \left[ \frac{k}{2} (x')^2 \right]_0^x = \frac{k}{2} x^2 \] ### Step 2: Relate Work Done to the Given Work \( W \) Setting the expression for work done equal to \( W \): \[ W = \frac{k}{2} x^2 \] From this, we can solve for \( k \): \[ k = \frac{2W}{x^2} \] ### Step 3: Use the Work-Energy Principle The work-energy principle states that the work done on an object is equal to the change in its kinetic energy. The initial kinetic energy \( KE_i \) is: \[ KE_i = \frac{1}{2} mv^2 \] The final kinetic energy \( KE_f \) when the speed is \( v_f \) is: \[ KE_f = \frac{1}{2} mv_f^2 \] The work done \( W \) is equal to the change in kinetic energy: \[ W = KE_f - KE_i \] Substituting the expressions for kinetic energy: \[ W = \frac{1}{2} mv_f^2 - \frac{1}{2} mv^2 \] Rearranging this gives: \[ \frac{1}{2} mv_f^2 = W + \frac{1}{2} mv^2 \] ### Step 4: Solve for Final Speed \( v_f \) Multiplying through by 2 to eliminate the fraction: \[ mv_f^2 = 2W + mv^2 \] Now, divide by \( m \): \[ v_f^2 = \frac{2W}{m} + v^2 \] Taking the square root gives us the final speed: \[ v_f = \sqrt{v^2 + \frac{2W}{m}} \] ### Final Answer The speed of the particle when the work done by the force equals \( W \) is: \[ v_f = \sqrt{v^2 + \frac{2W}{m}} \]
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