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Constant power P is supplied to a partic...

Constant power P is supplied to a particle having mass `m` and initially at rest. choose correct graph.

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To solve the problem of determining the correct graph for a particle under constant power, we can follow these steps: ### Step 1: Understand the relationship between power, work, and kinetic energy Given that constant power \( P \) is supplied to a particle of mass \( m \) that starts from rest, we can relate power to kinetic energy. The work done by the power over time \( t \) is equal to the change in kinetic energy. ### Step 2: Relate power to kinetic energy The work done \( W \) by the power over time \( t \) can be expressed as: \[ W = P \cdot t \] This work is equal to the kinetic energy \( KE \) of the particle: \[ W = \frac{1}{2} m v^2 \] Setting these two equations equal gives: \[ P \cdot t = \frac{1}{2} m v^2 \] ### Step 3: Solve for velocity \( v \) Rearranging the equation for \( v \): \[ v^2 = \frac{2Pt}{m} \] Taking the square root gives: \[ v = \sqrt{\frac{2P}{m} t} \] ### Step 4: Find the relationship between distance \( s \) and time \( t \) The distance \( s \) traveled by the particle can be found by integrating the velocity over time: \[ s = \int_0^t v \, dt \] Substituting the expression for \( v \): \[ s = \int_0^t \sqrt{\frac{2P}{m} t'} \, dt' \] ### Step 5: Perform the integration The integral can be computed as follows: \[ s = \sqrt{\frac{2P}{m}} \int_0^t (t')^{1/2} \, dt' \] The integral of \( (t')^{1/2} \) is: \[ \int (t')^{1/2} \, dt' = \frac{2}{3} (t')^{3/2} \] Evaluating this from 0 to \( t \) gives: \[ s = \sqrt{\frac{2P}{m}} \cdot \frac{2}{3} t^{3/2} \] Thus, we have: \[ s = \frac{2}{3} \sqrt{\frac{2P}{m}} t^{3/2} \] ### Step 6: Determine the relationship between \( s \) and \( t \) From the final expression, we can see that: \[ s \propto t^{3/2} \] This indicates that the graph of \( s \) versus \( t \) will be a curve that is concave upward, resembling a parabola. ### Conclusion The correct graph representing the relationship between distance \( s \) and time \( t \) is a concave upward parabola. ---
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