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Laws of Motion question

2020 · 4 Sep · Shift 2 · Q58
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Laws of Motion question

2020 · 4 Sep · Shift 2 · Q58

JEE MainPhysicsLaws of MotionMCQ+4 / −1
A small ball of mass m is thrown upward with velocity u from the ground. The ball experiences a resistive force mkv2 where v is its speed. The maximum height attained by the ball is :
  1. A
    1ktan⁡−1ku22g{1 \over k}{\tan ^{ - 1}}{{k{u^2}} \over {2g}}k1​tan−12gku2​
  2. B
    12ktan⁡−1ku2g{1 \over {2k}}{\tan ^{ - 1}}{{k{u^2}} \over g}2k1​tan−1gku2​
  3. C
    12kln⁡(1+ku2g){1 \over {2k}}\ln \left( {1 + {{k{u^2}} \over g}} \right)2k1​ln(1+gku2​)
  4. D
    1kln⁡(1+ku22g){1 \over k}\ln \left( {1 + {{k{u^2}} \over {2g}}} \right)k1​ln(1+2gku2​)
View written solutionFree

Correct answer: C

  1. Forces during upward motion

When the ball moves upward, both forces act downward:

  • Weight: mgmgmg
  • Resistive force: mkv2mk v^2mkv2

So, taking upward as positive, mdvdt=−mg−mkv2m\frac{dv}{dt}=-mg-mkv^2mdtdv​=−mg−mkv2

Dividing by mmm, dvdt=−(g+kv2)\frac{dv}{dt}=-(g+kv^2)dtdv​=−(g+kv2)


  1. Use the relation between acceleration and displacement

We need maximum height, so use dvdt=vdvdx\frac{dv}{dt}=v\frac{dv}{dx}dtdv​=vdxdv​

Thus, vdvdx=−(g+kv2)v\frac{dv}{dx}=-(g+kv^2)vdxdv​=−(g+kv2)

Rearranging, dx=−v dvg+kv2dx=-\frac{v\,dv}{g+kv^2}dx=−g+kv2vdv​


  1. Apply limits

At launch:

  • x=0x=0x=0, v=uv=uv=u

At maximum height:

  • x=Hx=Hx=H, v=0v=0v=0

So,

=\int_0^u \frac{v\,dv}{g+kv^2}$$ --- 4. **Evaluate the integral** $$H=\int_0^u \frac{v\,dv}{g+kv^2}$$ Let $$t=g+kv^2 \Rightarrow dt=2kv\,dv$$ So, $$v\,dv=\frac{dt}{2k}$$ Hence, $$H=\frac{1}{2k}\int_{g}^{g+ku^2}\frac{dt}{t}$$ $$H=\frac{1}{2k}\left[\ln t\right]_{g}^{g+ku^2}$$ $$H=\frac{1}{2k}\ln\left(\frac{g+ku^2}{g}\right)$$ $$H=\frac{1}{2k}\ln\left(1+\frac{ku^2}{g}\right)$$ --- 5. **Match with the options** This is exactly: $$\boxed{\frac{1}{2k}\ln\left(1+\frac{ku^2}{g}\right)}$$ So the correct option is **C**. --- 6. **Comparison with stored answer** Stored correct answer: **C** Our derived answer: **C** They match.
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