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A time varying force, F=2t is acting on ...

A time varying force, `F=2t` is acting on a particle of mass `2kg` moving along x-axis. velocity of the particle is `4m//s` along negative x-axis at time `t=0`. Find the velocity of the particle at the end of 4s.

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To solve the problem step by step, we will use the impulse-momentum theorem, which states that the impulse applied to an object is equal to the change in its momentum. ### Step-by-Step Solution: 1. **Identify the Given Values:** - Time-varying force: \( F(t) = 2t \) - Mass of the particle: \( m = 2 \, \text{kg} \) - Initial velocity at \( t = 0 \): \( v_0 = -4 \, \text{m/s} \) (negative indicates direction along the negative x-axis) - Time interval: \( t = 4 \, \text{s} \) 2. **Calculate the Impulse:** - Impulse \( J \) is given by the integral of force over time: \[ J = \int_{0}^{4} F(t) \, dt = \int_{0}^{4} 2t \, dt \] - Evaluating the integral: \[ J = 2 \int_{0}^{4} t \, dt = 2 \left[ \frac{t^2}{2} \right]_{0}^{4} = 2 \left[ \frac{4^2}{2} - \frac{0^2}{2} \right] = 2 \left[ \frac{16}{2} \right] = 2 \times 8 = 16 \, \text{Ns} \] 3. **Relate Impulse to Change in Momentum:** - The change in momentum \( \Delta p \) is given by: \[ J = \Delta p = m(v_f - v_0) \] - Substituting the known values: \[ 16 = 2(v_f - (-4)) \] - Simplifying: \[ 16 = 2(v_f + 4) \] \[ 8 = v_f + 4 \] \[ v_f = 8 - 4 = 4 \, \text{m/s} \] 4. **Final Result:** - The final velocity of the particle at \( t = 4 \, \text{s} \) is \( v_f = 4 \, \text{m/s} \).

To solve the problem step by step, we will use the impulse-momentum theorem, which states that the impulse applied to an object is equal to the change in its momentum. ### Step-by-Step Solution: 1. **Identify the Given Values:** - Time-varying force: \( F(t) = 2t \) - Mass of the particle: \( m = 2 \, \text{kg} \) - Initial velocity at \( t = 0 \): \( v_0 = -4 \, \text{m/s} \) (negative indicates direction along the negative x-axis) ...
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DC PANDEY ENGLISH-CENTRE OF MASS, LINEAR MOMENTUM AND COLLISION-Level 2 Subjective
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