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A particle of mass mm is driven by a machine that delivers a constant power of kk watts. If the particle starts from rest, the force on the particle at the time tt is:

A

mk2t1/2\sqrt{\frac{mk}{2}} t^{-1/2}

B

mkt1/2\sqrt{mk} t^{-1/2}

C

2mkt1/2\sqrt{2mk} t^{-1/2}

D

12mkt1/2\frac{1}{2} \sqrt{mk} t^{-1/2}

Step-by-Step Solution

To find the force as a function of time, we utilize the relationship between power, work, and kinetic energy:

  1. Work-Energy Theorem: Since the machine delivers constant power kk, the work done (WW) on the particle in time tt is W=P×t=ktW = P \times t = kt . According to the work-energy theorem, this work is equal to the change in kinetic energy: kt=12mv20kt = \frac{1}{2}mv^2 - 0 .
  2. Velocity Calculation: From the energy equation, we solve for velocity (vv): v2=2ktm    v=2ktmv^2 = \frac{2kt}{m} \implies v = \sqrt{\frac{2kt}{m}} .
  3. Force Calculation: Power is defined as the product of force and velocity (P=FvP = F \cdot v) . Therefore, F=PvF = \frac{P}{v}.
  4. Substitution: Substituting the expressions for PP and vv: F=k2ktm=k2m2kt=mk2t1/2F = \frac{k}{\sqrt{\frac{2kt}{m}}} = \sqrt{\frac{k^2 \cdot m}{2kt}} = \sqrt{\frac{mk}{2}} t^{-1/2}

Thus, the force acting on the particle at time tt is mk2t1/2\sqrt{\frac{mk}{2}} t^{-1/2}.

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