JEE PYQ: Motion in a Plane - Question ID 3aed4f8d2a22 (JEE Main 2020)

ID: 3aed4f8d2a22JEE Main 2020Single Correct MCQ
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 j where ω\omega 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) and acceleration a→(t)\overrightarrow a \left( t \right) of the particle :

Select Option

Step-by-step Explanation

Core Formula & Concept:

In plane motion, the position vector r→(t)\overrightarrow{r}(t) describes the trajectory of a particle. The velocity v→(t)\overrightarrow{v}(t) and acceleration a→(t)\overrightarrow{a}(t) are obtained by differentiating r→(t)\overrightarrow{r}(t) with respect to time:

  • v→(t)=dr→dt\overrightarrow{v}(t) = \frac{d\overrightarrow{r}}{dt}
  • a→(t)=dv→dt=d2r→dt2\overrightarrow{a}(t) = \frac{d\overrightarrow{v}}{dt} = \frac{d^2\overrightarrow{r}}{dt^2}

Two vectors A→\overrightarrow{A} and B→\overrightarrow{B} are perpendicular if their dot product vanishes: A→⋅B→=0\overrightarrow{A} \cdot \overrightarrow{B} = 0. A vector A→\overrightarrow{A} is directed toward the origin if it is antiparallel to the position vector r→\overrightarrow{r}, i.e. A→=−k r→\overrightarrow{A} = -k\,\overrightarrow{r} for some positive scalar kk.

Step-by-Step Derivation:

Step 1: Compute the velocity vector

Given r→(t)=cos⁡(ωt) i^+sin⁡(ωt) j^\displaystyle \overrightarrow{r}(t) = \cos(\omega t)\,\widehat{i} + \sin(\omega t)\,\widehat{j}, we differentiate with respect to tt:

v→(t)=dr→dt=ddt[cos⁡(ωt)] i^+ddt[sin⁡(ωt)] j^=−ωsin⁡(ωt) i^+ωcos⁡(ωt) j^.\overrightarrow{v}(t) = \frac{d\overrightarrow{r}}{dt} = \frac{d}{dt}\bigl[\cos(\omega t)\bigr]\,\widehat{i} + \frac{d}{dt}\bigl[\sin(\omega t)\bigr]\,\widehat{j} = -\omega\sin(\omega t)\,\widehat{i} + \omega\cos(\omega t)\,\widehat{j}.

Step 2: Check orthogonality of v→\overrightarrow{v} and r→\overrightarrow{r}

Form the dot product:

v→⋅r→=[−ωsin⁡(ωt)][cos⁡(ωt)]+[ωcos⁡(ωt)][sin⁡(ωt)]=−ωsin⁡(ωt)cos⁡(ωt)+ωcos⁡(ωt)sin⁡(ωt)=0.\overrightarrow{v}\cdot\overrightarrow{r} = \bigl[-\omega\sin(\omega t)\bigr]\bigl[\cos(\omega t)\bigr] + \bigl[\omega\cos(\omega t)\bigr]\bigl[\sin(\omega t)\bigr] = -\omega\sin(\omega t)\cos(\omega t) + \omega\cos(\omega t)\sin(\omega t) = 0.

Since the dot product is zero, v→\overrightarrow{v} is perpendicular to r→\overrightarrow{r}.

Step 3: Compute the acceleration vector

Differentiate v→(t)\overrightarrow{v}(t):

a→(t)=dv→dt=ddt[−ωsin⁡(ωt)] i^+ddt[ωcos⁡(ωt)] j^=−ω2cos⁡(ωt) i^−ω2sin⁡(ωt) j^=−ω2[cos⁡(ωt) i^+sin⁡(ωt) j^]=−ω2 r→(t).\overrightarrow{a}(t) = \frac{d\overrightarrow{v}}{dt} = \frac{d}{dt}\bigl[-\omega\sin(\omega t)\bigr]\,\widehat{i} + \frac{d}{dt}\bigl[\omega\cos(\omega t)\bigr]\,\widehat{j} = -\omega^2\cos(\omega t)\,\widehat{i} - \omega^2\sin(\omega t)\,\widehat{j} = -\omega^2\bigl[\cos(\omega t)\,\widehat{i} + \sin(\omega t)\,\widehat{j}\bigr] = -\omega^2\,\overrightarrow{r}(t).

Step 4: Interpret the direction of a→\overrightarrow{a}

The acceleration is a negative scalar multiple of r→\overrightarrow{r}: a→=−ω2 r→\overrightarrow{a} = -\omega^2\,\overrightarrow{r}. This means a→\overrightarrow{a} points exactly opposite to r→\overrightarrow{r}, i.e. toward the origin.

Step 5: Match with the given options

  • Option A claims both v→\overrightarrow{v} and a→\overrightarrow{a} are perpendicular to r→\overrightarrow{r}. We found a→\overrightarrow{a} is antiparallel, not perpendicular.
  • Option B claims both are parallel to r→\overrightarrow{r}. That is false for v→\overrightarrow{v}.
  • Option C states v→\overrightarrow{v} is perpendicular to r→\overrightarrow{r} and a→\overrightarrow{a} is directed toward the origin. This matches our results.
  • Option D says a→\overrightarrow{a} is directed away from the origin, which is incorrect.

Therefore the correct choice is C.

Common Traps & Exam Tip:

1. Sign error in differentiation: Students often forget the negative sign when differentiating cos⁡(ωt)\cos(\omega t) or sin⁡(ωt)\sin(\omega t), leading to wrong velocity or acceleration expressions. 2. Misinterpreting antiparallel as perpendicular: The acceleration a→=−ω2r→\overrightarrow{a} = -\omega^2\overrightarrow{r} is collinear with r→\overrightarrow{r} but points inward. Some confuse this with perpendicularity. 3. Skipping the dot-product check: Without computing v→⋅r→\overrightarrow{v}\cdot\overrightarrow{r}, one might guess that both vectors are either parallel or perpendicular. Always compute the dot product explicitly.

Exam Tip: Whenever you see a position vector of the form cos⁡(ωt) i^+sin⁡(ωt) j^\cos(\omega t)\,\widehat{i} + \sin(\omega t)\,\widehat{j}, recognize it as uniform circular motion. In such motion the velocity is always tangent (perpendicular to radius) and the acceleration is centripetal (directed toward the center).