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Motion question

2020 · Shift 2 · Q48
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Motion question

2020 · Shift 2 · Q48

JEE AdvancedPhysicsMotionMultiple correct+4 / −2
Starting at time t = 0 from the origin with speed 1 ms-1, a particle follows a two-dimensional trajectory in the x-y plane so that its coordinates are related by the equation y=x22y = {{{x^2}} \over 2}y=2x2​. The x and y components of its acceleration are denoted by ax and ay, respectively. Then
  1. A
    ax = 1 ms-2 implies that when the particle is at the origin, ay = 1 ms-2
  2. B
    ax = 0 implies ay = 1 ms-2 at all times
  3. C
    at t = 0, the particle's velocity points in the x-direction
  4. D
    ax = 0 implies that at t = 1s, the angle between the particle's velocity and the x axis is 45 ∘^\circ∘
View written solutionFree

Correct answer: A, B, C, D

  1. Given trajectory

    The particle moves such that y=x22.y = \frac{x^2}{2}.y=2x2​.

    Since motion is in the plane, let x=x(t),y=y(t)=x(t)22.x = x(t), \qquad y = y(t)=\frac{x(t)^2}{2}.x=x(t),y=y(t)=2x(t)2​.

  2. Velocity components

    Differentiate with respect to time: y˙=xx˙.\dot y = x\dot x.y˙​=xx˙. Hence, vx=x˙,vy=y˙=xx˙.v_x = \dot x, \qquad v_y = \dot y = x\dot x.vx​=x˙,vy​=y˙​=xx˙.

    So the velocity vector is v⃗=(x˙, xx˙).\vec v = (\dot x,\, x\dot x).v=(x˙,xx˙).

  3. Use the initial speed condition

    At t=0t=0t=0, the particle starts from the origin, so x(0)=0,y(0)=0.x(0)=0, \qquad y(0)=0.x(0)=0,y(0)=0.

    Initial speed is 1 m s−11\,\text{m s}^{-1}1m s−1, so ∣v⃗(0)∣=1.|\vec v(0)| = 1.∣v(0)∣=1.

    But at x=0x=0x=0, vy(0)=x(0)x˙(0)=0.v_y(0)=x(0)\dot x(0)=0.vy​(0)=x(0)x˙(0)=0. Therefore, ∣v⃗(0)∣=∣vx(0)∣=∣x˙(0)∣=1.|\vec v(0)| = |v_x(0)| = |\dot x(0)| = 1.∣v(0)∣=∣vx​(0)∣=∣x˙(0)∣=1.

    So initially the velocity is entirely along the x-axis (either +x+x+x or −x-x−x direction).

    Hence Option C is correct.

  4. Acceleration components

    Differentiate y˙=xx˙\dot y = x\dot xy˙​=xx˙ again: y¨=x˙2+xx¨.\ddot y = \dot x^2 + x\ddot x.y¨​=x˙2+xx¨.

    Therefore, ax=x¨,ay=x˙2+xx¨.a_x = \ddot x, \qquad a_y = \dot x^2 + x\ddot x.ax​=x¨,ay​=x˙2+xx¨.

    So ay=vx2+xax.a_y = v_x^2 + x a_x.ay​=vx2​+xax​.


  1. Check Option A

    Option A states: if ax=1 m s−2a_x=1\,\text{m s}^{-2}ax​=1m s−2, then when the particle is at the origin, ay=1 m s−2a_y=1\,\text{m s}^{-2}ay​=1m s−2.

    At the origin, x=0x=0x=0, so ay=x˙2+xx¨=x˙2.a_y = \dot x^2 + x\ddot x = \dot x^2.ay​=x˙2+xx¨=x˙2.

    At t=0t=0t=0 (starting from origin), we already found ∣x˙(0)∣=1  ⟹  x˙(0)2=1.|\dot x(0)|=1 \implies \dot x(0)^2=1.∣x˙(0)∣=1⟹x˙(0)2=1.

    Thus, ay(0)=1 m s−2.a_y(0)=1\,\text{m s}^{-2}.ay​(0)=1m s−2.

    This is true irrespective of the sign of x˙(0)\dot x(0)x˙(0), and the given condition ax=1a_x=1ax​=1 is consistent.

    Hence Option A is correct.


  1. Check Option B

    If ax=0a_x=0ax​=0, then x¨=0  ⟹  x˙=constant.\ddot x=0 \implies \dot x=\text{constant}.x¨=0⟹x˙=constant.

    Since initial speed at the origin is 111 and initially velocity is along x-axis, ∣x˙∣=1.|\dot x|=1.∣x˙∣=1. Therefore, x˙2=1for all times.\dot x^2=1 \quad \text{for all times}.x˙2=1for all times.

    Now using ay=x˙2+xax,a_y = \dot x^2 + x a_x,ay​=x˙2+xax​, with ax=0a_x=0ax​=0, ay=x˙2=1.a_y = \dot x^2 = 1.ay​=x˙2=1.

    So at all times, ay=1 m s−2.a_y=1\,\text{m s}^{-2}.ay​=1m s−2.

    Hence Option B is correct.


  1. Check Option D

    Again, if ax=0a_x=0ax​=0, then x˙\dot xx˙ is constant with magnitude 111.

    Taking the usual positive-x start, x˙=1\dot x=1x˙=1, so x=tx=tx=t because x(0)=0x(0)=0x(0)=0.

    Then vy=xx˙=t⋅1=t.v_y = x\dot x = t\cdot 1 = t.vy​=xx˙=t⋅1=t.

    At t=1 st=1\,\text{s}t=1s, vx=1,vy=1.v_x=1, \qquad v_y=1.vx​=1,vy​=1.

    Therefore, tan⁡θ=vyvx=1  ⟹  θ=45∘.\tan\theta = \frac{v_y}{v_x} = 1 \implies \theta=45^\circ.tanθ=vx​vy​​=1⟹θ=45∘.

    Hence Option D is correct.


  1. Final conclusion

    All four statements are correct: A,B,C,D\boxed{A, B, C, D}A,B,C,D​

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