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)=cosωti^+sinωtj^\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)=drdt\overrightarrow{v}(t) = \frac{d\overrightarrow{r}}{dt}
  • a(t)=dvdt=d2rdt2\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: AB=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=kr\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)=drdt=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:

vr=[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)=dvdt=ddt[ωsin(ωt)]i^+ddt[ωcos(ωt)]j^=ω2cos(ωt)i^ω2sin(ωt)j^=ω2[cos(ωt)i^+sin(ωt)j^]=ω2r(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=ω2r\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 vr\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).