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Circular Motion question

2010 · Shift 0 · Q76
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  5. /2010 · Shift 0 · Q76

Circular Motion question

2010 · Shift 0 · Q76

JEE MainPhysicsCircular MotionMCQ+4 / −1
For a particle in uniform circular motion the acceleration a→\overrightarrow aa at a point P(R, θ) on the circle of radius R is (here θ is measured from the x–axis)
  1. A
    −v2Rcos⁡θi^+v2Rsin⁡θj^- {{{v^2}} \over R}\cos \theta \widehat i + {{{v^2}} \over R}\sin \theta \widehat j−Rv2​cosθi+Rv2​sinθj​
  2. B
    −v2Rsin⁡θi^+v2Rcos⁡θj^- {{{v^2}} \over R}\sin \theta \widehat i + {{{v^2}} \over R}\cos \theta \widehat j−Rv2​sinθi+Rv2​cosθj​
  3. C
    −v2Rcos⁡θi^−v2Rsin⁡θj^- {{{v^2}} \over R}\cos \theta \widehat i - {{{v^2}} \over R}\sin \theta \widehat j−Rv2​cosθi−Rv2​sinθj​
  4. D
    v2Ri^+v2Rj^{{{v^2}} \over R}\widehat i + {{{v^2}} \over R}\widehat jRv2​i+Rv2​j​
View written solutionFree

Correct answer: C

  1. Position vector of the particle

For a point P(R,θ)P(R,\theta)P(R,θ) on a circle of radius RRR, measured from the xxx-axis,

r⃗=Rcos⁡θ i^+Rsin⁡θ j^\vec r = R\cos\theta\,\hat i + R\sin\theta\,\hat jr=Rcosθi^+Rsinθj^​

  1. Direction of acceleration in uniform circular motion

In uniform circular motion, the speed is constant, but the velocity direction changes continuously.

Hence the acceleration is centripetal, i.e. directed towards the center.

Its magnitude is

a=v2Ra = \frac{v^2}{R}a=Rv2​

and its direction is opposite to the radial unit vector.

  1. Radial unit vector

The outward radial unit vector at angle θ\thetaθ is

r^=cos⁡θ i^+sin⁡θ j^\hat r = \cos\theta\,\hat i + \sin\theta\,\hat jr^=cosθi^+sinθj^​

Therefore, inward direction is

−r^=−cos⁡θ i^−sin⁡θ j^-\hat r = -\cos\theta\,\hat i - \sin\theta\,\hat j−r^=−cosθi^−sinθj^​

  1. Acceleration vector

Thus,

a⃗=v2R(−r^)\vec a = \frac{v^2}{R}(-\hat r)a=Rv2​(−r^)

a⃗=−v2Rcos⁡θ i^−v2Rsin⁡θ j^\vec a = -\frac{v^2}{R}\cos\theta\,\hat i - \frac{v^2}{R}\sin\theta\,\hat ja=−Rv2​cosθi^−Rv2​sinθj^​

  1. Compare with options
  • A: −v2Rcos⁡θ i^+v2Rsin⁡θ j^-\dfrac{v^2}{R}\cos\theta\,\hat i + \dfrac{v^2}{R}\sin\theta\,\hat j−Rv2​cosθi^+Rv2​sinθj^​ ❌
  • B: −v2Rsin⁡θ i^+v2Rcos⁡θ j^-\dfrac{v^2}{R}\sin\theta\,\hat i + \dfrac{v^2}{R}\cos\theta\,\hat j−Rv2​sinθi^+Rv2​cosθj^​ ❌
  • C: −v2Rcos⁡θ i^−v2Rsin⁡θ j^-\dfrac{v^2}{R}\cos\theta\,\hat i - \dfrac{v^2}{R}\sin\theta\,\hat j−Rv2​cosθi^−Rv2​sinθj^​ ✅
  • D: v2Ri^+v2Rj^\dfrac{v^2}{R}\hat i + \dfrac{v^2}{R}\hat jRv2​i^+Rv2​j^​ ❌

Therefore, the correct option is C.

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