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Motion in A Plane question

2020 · 8 Jan · Shift 2 · Q39
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  5. /2020 · 8 Jan · Shift 2 · Q39

Motion in A Plane question

2020 · 8 Jan · Shift 2 · Q39

JEE MainPhysicsMotion in A PlaneMCQ+4 / −1
A particle moves such that its position vector r→(t)=cos⁡ωti^+sin⁡ωtj^\overrightarrow r \left( t \right) = \cos \omega t\widehat i + \sin \omega t\widehat jr(t)=cosωti+sinωtj​ where ω\omegaω is a constant and t is time. Then which of the following statements is true for the velocity v→(t)\overrightarrow v \left( t \right)v(t) and acceleration a→(t)\overrightarrow a \left( t \right)a(t) of the particle :
  1. A
    v→\overrightarrow vv and a→\overrightarrow aa both are perpendicular to r→\overrightarrow rr
  2. B
    v→\overrightarrow vv and a→\overrightarrow aa both are parallel to r→\overrightarrow rr
  3. C
    v→\overrightarrow vv is perpendicular to r→\overrightarrow rr and a→\overrightarrow aa is directed towards the origin
  4. D
    v→\overrightarrow vv is perpendicular to r→\overrightarrow rr and a→\overrightarrow aa is directed away from the origin
View written solutionFree

Correct answer: C

  1. Given position vector

    r⃗(t)=cos⁡ωt i^+sin⁡ωt j^\vec r(t)=\cos \omega t\,\hat i+\sin \omega t\,\hat jr(t)=cosωti^+sinωtj^​

    This represents motion on a circle of radius 111 centered at the origin, since

    ∣r⃗∣=cos⁡2ωt+sin⁡2ωt=1|\vec r|=\sqrt{\cos^2\omega t+\sin^2\omega t}=1∣r∣=cos2ωt+sin2ωt​=1

  2. Find velocity

    Velocity is the time derivative of position:

    v⃗(t)=dr⃗dt=−ωsin⁡ωt i^+ωcos⁡ωt j^\vec v(t)=\frac{d\vec r}{dt}=-\omega \sin \omega t\,\hat i+\omega \cos \omega t\,\hat jv(t)=dtdr​=−ωsinωti^+ωcosωtj^​

  3. Check whether v⃗\vec vv is perpendicular to r⃗\vec rr

    Compute the dot product:

    r⃗⋅v⃗=(cos⁡ωt)(−ωsin⁡ωt)+(sin⁡ωt)(ωcos⁡ωt)=0\vec r\cdot \vec v=(\cos \omega t)(-\omega \sin \omega t)+(\sin \omega t)(\omega \cos \omega t)=0r⋅v=(cosωt)(−ωsinωt)+(sinωt)(ωcosωt)=0

    Hence,

    v⃗⊥r⃗\vec v \perp \vec rv⊥r

  4. Find acceleration

    Acceleration is the time derivative of velocity:

    a⃗(t)=dv⃗dt=−ω2cos⁡ωt i^−ω2sin⁡ωt j^\vec a(t)=\frac{d\vec v}{dt}=-\omega^2\cos \omega t\,\hat i-\omega^2\sin \omega t\,\hat ja(t)=dtdv​=−ω2cosωti^−ω2sinωtj^​

    Factorizing:

    a⃗(t)=−ω2(cos⁡ωt i^+sin⁡ωt j^)=−ω2r⃗(t)\vec a(t)=-\omega^2\left(\cos \omega t\,\hat i+\sin \omega t\,\hat j\right)=-\omega^2\vec r(t)a(t)=−ω2(cosωti^+sinωtj^​)=−ω2r(t)

  5. Interpret acceleration

    Since

    a⃗=−ω2r⃗\vec a=-\omega^2\vec ra=−ω2r

    acceleration is opposite to r⃗\vec rr. Because r⃗\vec rr points from the origin to the particle, −r⃗-\vec r−r points towards the origin.

  6. Evaluate options

    • A: False, because a⃗\vec aa is not perpendicular to r⃗\vec rr; it is anti-parallel to it.
    • B: False, because v⃗\vec vv is perpendicular to r⃗\vec rr.
    • C: True, because v⃗⊥r⃗\vec v \perp \vec rv⊥r and a⃗\vec aa is directed towards the origin.
    • D: False, because a⃗\vec aa is not directed away from the origin.

Therefore, the correct option is C.

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