JEE PYQ: Motion in a Plane - Question ID 01b44822f4b3 (JEE Main 2019)

ID: 01b44822f4b3JEE Main 2019Single Correct MCQ
The position co-ordinates of a particle moving in a 3-D coordinate system is given by
x = a cosω\omegat
y = a sinω\omegat and
z = aω\omegat

The speed of the particle is :

Select Option

Step-by-step Explanation

Core Formula & Concept:

To determine the speed of a particle moving in three-dimensional space, we rely on the following fundamental concepts:

  • Position Vector: The position of the particle at any time tt is given by the vector r(t)=x(t)i^+y(t)j^+z(t)k^\vec{r}(t) = x(t) \hat{i} + y(t) \hat{j} + z(t) \hat{k} where x(t)x(t), y(t)y(t), and z(t)z(t) are the time-dependent coordinates.
  • Velocity Vector: The velocity of the particle is the time derivative of the position vector: v(t)=drdt=dxdti^+dydtj^+dzdtk^\vec{v}(t) = \frac{d\vec{r}}{dt} = \frac{dx}{dt} \hat{i} + \frac{dy}{dt} \hat{j} + \frac{dz}{dt} \hat{k}
  • Speed: The speed of the particle is the magnitude of the velocity vector: v=v(t)=(dxdt)2+(dydt)2+(dzdt)2v = |\vec{v}(t)| = \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2 + \left(\frac{dz}{dt}\right)^2}

In this problem, the coordinates are given as: x=acos(ωt),y=asin(ωt),z=aωtx = a \cos(\omega t), \quad y = a \sin(\omega t), \quad z = a \omega t We will compute the velocity components by differentiating these expressions with respect to time and then find the magnitude of the velocity vector to obtain the speed.

--- Step-by-Step Derivation:

Step 1: Compute the velocity components

Differentiate each coordinate with respect to time tt:

  • x=acos(ωt)x = a \cos(\omega t) dxdt=aωsin(ωt)\frac{dx}{dt} = -a \omega \sin(\omega t)
  • y=asin(ωt)y = a \sin(\omega t) dydt=aωcos(ωt)\frac{dy}{dt} = a \omega \cos(\omega t)
  • z=aωtz = a \omega t dzdt=aω\frac{dz}{dt} = a \omega

Step 2: Write the velocity vector

The velocity vector is: v(t)=dxdti^+dydtj^+dzdtk^\vec{v}(t) = \frac{dx}{dt} \hat{i} + \frac{dy}{dt} \hat{j} + \frac{dz}{dt} \hat{k} v(t)=aωsin(ωt)i^+aωcos(ωt)j^+aωk^\vec{v}(t) = -a \omega \sin(\omega t) \hat{i} + a \omega \cos(\omega t) \hat{j} + a \omega \hat{k}

Step 3: Compute the magnitude of the velocity vector (speed)

The speed vv is: v=v(t)=(dxdt)2+(dydt)2+(dzdt)2v = |\vec{v}(t)| = \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2 + \left(\frac{dz}{dt}\right)^2} Substitute the derivatives: v=(aωsin(ωt))2+(aωcos(ωt))2+(aω)2v = \sqrt{(-a \omega \sin(\omega t))^2 + (a \omega \cos(\omega t))^2 + (a \omega)^2} Simplify each term: v=a2ω2sin2(ωt)+a2ω2cos2(ωt)+a2ω2v = \sqrt{a^2 \omega^2 \sin^2(\omega t) + a^2 \omega^2 \cos^2(\omega t) + a^2 \omega^2} Factor out a2ω2a^2 \omega^2: v=a2ω2(sin2(ωt)+cos2(ωt))+a2ω2v = \sqrt{a^2 \omega^2 (\sin^2(\omega t) + \cos^2(\omega t)) + a^2 \omega^2} Use the trigonometric identity sin2θ+cos2θ=1\sin^2 \theta + \cos^2 \theta = 1: v=a2ω2(1)+a2ω2=a2ω2+a2ω2v = \sqrt{a^2 \omega^2 (1) + a^2 \omega^2} = \sqrt{a^2 \omega^2 + a^2 \omega^2} v=2a2ω2=2aωv = \sqrt{2 a^2 \omega^2} = \sqrt{2} a \omega

Step 4: Match with the given options

The speed of the particle is 2aω\sqrt{2} a \omega, which corresponds to option A.

--- Common Traps & Exam Tip:

Students often make the following mistakes in this type of problem:

  • Forgetting to differentiate the z-coordinate: Some students only consider the xx and yy components, ignoring the zz-component, leading to an incorrect speed of aωa \omega (option B).
  • Incorrectly squaring the derivatives: Misapplying the square operation on the derivatives can lead to wrong magnitudes. Always ensure that each component is squared individually before summing.
  • Overlooking the trigonometric identity: Failing to use sin2θ+cos2θ=1\sin^2 \theta + \cos^2 \theta = 1 can complicate the expression unnecessarily. This identity simplifies the calculation significantly.
  • Confusing speed with velocity: Speed is a scalar quantity (magnitude of velocity), while velocity is a vector. Ensure you compute the magnitude, not just the components.

Exam Tip: Always double-check that you have included all components of motion (especially in 3D problems) and applied differentiation correctly. Simplify expressions using trigonometric identities to avoid errors.