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Laws of Motion question

2020 · 5 Sep · Shift 2 · Q53
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  5. /2020 · 5 Sep · Shift 2 · Q53

Laws of Motion question

2020 · 5 Sep · Shift 2 · Q53

JEE MainPhysicsLaws of MotionMCQ+4 / −1
A spaceship in space sweeps stationary interplanetary dust. As a result, its mass increases at a rate dM(t)dt{{dM\left( t \right)} \over {dt}}dtdM(t)​ = bv2(t), where v(t) is its instantaneous velocity. The instantaneous acceleration of the satellite is :
  1. A
    -bv3(t)
  2. B
    −2bv3M(t)- {{2b{v^3}} \over {M\left( t \right)}}−M(t)2bv3​
  3. C
    −bv3M(t)- {{b{v^3}} \over {M\left( t \right)}}−M(t)bv3​
  4. D
    −bv32M(t)- {{b{v^3}} \over {2M\left( t \right)}}−2M(t)bv3​
View written solutionFree

Correct answer: C

  1. Given data

A spaceship is moving in space and sweeps up stationary interplanetary dust. Its mass increases as

dMdt=bv2(t)\frac{dM}{dt} = b v^2(t)dtdM​=bv2(t)

We need the instantaneous acceleration a=dvdta = \dfrac{dv}{dt}a=dtdv​.


  1. Use conservation of momentum for variable mass system

In time interval dtdtdt:

  • spaceship mass changes from MMM to M+dMM+dMM+dM
  • velocity changes from vvv to v+dvv+dvv+dv
  • dust collected was initially at rest

Since there is no external force, total momentum is conserved.

Initial momentum:

Pi=MvP_i = MvPi​=Mv

Final momentum:

Pf=(M+dM)(v+dv)P_f = (M+dM)(v+dv)Pf​=(M+dM)(v+dv)

Because the dust was initially stationary, it contributed zero initial momentum.

So,

Mv=(M+dM)(v+dv)Mv = (M+dM)(v+dv)Mv=(M+dM)(v+dv)

Expanding and neglecting second-order small term dM dvdM\,dvdMdv:

Mv=Mv+M dv+v dMMv = Mv + M\,dv + v\,dMMv=Mv+Mdv+vdM

Thus,

M dv+v dM=0M\,dv + v\,dM = 0Mdv+vdM=0

Divide by dtdtdt:

Mdvdt+vdMdt=0M\frac{dv}{dt} + v\frac{dM}{dt} = 0Mdtdv​+vdtdM​=0

Hence,

dvdt=−vMdMdt\frac{dv}{dt} = -\frac{v}{M}\frac{dM}{dt}dtdv​=−Mv​dtdM​
  1. Substitute the given rate of mass increase

Given,

dMdt=bv2\frac{dM}{dt} = b v^2dtdM​=bv2

Therefore,

dvdt=−vM(bv2)\frac{dv}{dt} = -\frac{v}{M}(b v^2)dtdv​=−Mv​(bv2) dvdt=−bv3M\frac{dv}{dt} = -\frac{b v^3}{M}dtdv​=−Mbv3​

So the instantaneous acceleration is

−bv3(t)M(t)\boxed{-\frac{b v^3(t)}{M(t)}}−M(t)bv3(t)​​
  1. Option check
  • A: −bv3(t)-bv^3(t)−bv3(t) — missing division by mass, incorrect.
  • B: −2bv3M(t)-\dfrac{2bv^3}{M(t)}−M(t)2bv3​ — extra factor of 2, incorrect.
  • C: −bv3M(t)-\dfrac{bv^3}{M(t)}−M(t)bv3​ — correct.
  • D: −bv32M(t)-\dfrac{bv^3}{2M(t)}−2M(t)bv3​ — incorrect factor.

  1. Comparison with stored answer

Stored correct answer: C

Derived answer: C

They match.

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