Skip to content
dronacharya.ai
← JEE Advanced 2018 · Paper 2
PhysicsList match+3 / -1Question 18 of 54

JEE Advanced 2018 · Paper 2, Physics question 18

In the List-I below, four different paths of a particle are given as functions of time. In these functions, α\alpha and β\beta are positive constants of appropriate dimensions and α≠β\alpha \ne \beta. In each case, the force acting on the particle is either zero or conservative. In List-II, five physical quantities of the particle are mentioned: p⃗\vec{p} is the linear momentum, L⃗\vec{L} is the angular momentum about the origin, KK is the kinetic energy, UU is the potential energy and EE is the total energy. Match each path in List-I with those quantities in List-II, which are conserved for that path.

LIST-I

  • P
    r⃗(t)=αt i^+βt j^\vec{r}(t) = \alpha t\,\hat{i} + \beta t\,\hat{j}
  • Q
    r⃗(t)=αcos⁡ωt i^+βsin⁡ωt j^\vec{r}(t) = \alpha\cos\omega t\,\hat{i} + \beta\sin\omega t\,\hat{j}
  • R
    r⃗(t)=α(cos⁡ωt i^+sin⁡ωt j^)\vec{r}(t) = \alpha(\cos\omega t\,\hat{i} + \sin\omega t\,\hat{j})
  • S
    r⃗(t)=αt i^+β2t2 j^\vec{r}(t) = \alpha t\,\hat{i} + \dfrac{\beta}{2}t^2\,\hat{j}

LIST-II

  • 1
    p⃗\vec{p}
  • 2
    L⃗\vec{L}
  • 3
    KK
  • 4
    UU
  • 5
    EE
Choose one option
Answer and worked solution

Official answer: A

Find the force from F⃗=mr⃗¨\vec F=m\ddot{\vec r} in each case.

  • P. r⃗=(αt,βt)\vec r=(\alpha t,\beta t): uniform velocity and F⃗=0\vec F=0. r⃗∥v⃗\vec r\parallel\vec v always, so L⃗=mr⃗×v⃗=0\vec L=m\vec r\times\vec v=0, a constant. p⃗\vec p, L⃗\vec L, KK, UU and EE are all conserved: 1, 2, 3, 4, 5.
  • Q. r⃗=(αcos⁡ωt,βsin⁡ωt)\vec r=(\alpha\cos\omega t,\beta\sin\omega t) with α≠β\alpha\ne\beta: F⃗=−mω2r⃗\vec F=-m\omega^2\vec r, a central spring-like force. L⃗\vec L and EE are conserved. The speed and the distance vary, so KK and UU do not stay constant: 2, 5.
  • R. Uniform circular motion with F⃗=−mω2r⃗\vec F=-m\omega^2\vec r: L⃗\vec L, KK, UU (since rr is constant) and EE are conserved. p⃗\vec p is not: 2, 3, 4, 5.
  • S. r⃗=(αt,β2t2)\vec r=(\alpha t,\tfrac\beta2t^2): a constant force mβj^m\beta\hat j, as in a projectile. Only EE is conserved. The torque about the origin, mαβt k^m\alpha\beta t\,\hat k, is nonzero, so L⃗\vec L changes: 5.

(A)