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Question: A particle is moving in xy-plane with a constant speed $v_0$ such that its y displacement is given b...

A particle is moving in xy-plane with a constant speed v0v_0 such that its y displacement is given by y=αe2vx3v0y = \alpha e^{-\frac{2v_x}{\sqrt{3}v_0}}, where vxv_x is component of velocity along the x-axis. If at some instant x component of it velocity is positive and the slope of the tangent on its path is 13-\frac{1}{\sqrt{3}}, then the displacement of the particle in y-direction at the instant is

A

αe1\alpha e^{-1}

B

αe2\alpha e^{-2}

C

Zero

D

α2e\alpha^2 e

Answer

αe1\alpha e^{-1}

Explanation

Solution

  1. The slope of the tangent is

    dydx=vyvx=13,\frac{dy}{dx} = \frac{v_y}{v_x} = -\frac{1}{\sqrt{3}},

    so vy=vx3v_y = -\frac{v_x}{\sqrt{3}}.

  2. With constant speed v0v_0, we have

    vx2+vy2=v02.v_x^2 + v_y^2 = v_0^2.

    Substituting vy=vx3v_y = -\frac{v_x}{\sqrt{3}} gives:

    vx2+vx23=v024vx23=v02.v_x^2 + \frac{v_x^2}{3} = v_0^2 \quad \Longrightarrow \quad \frac{4v_x^2}{3} = v_0^2.

    Thus,

    vx=32v0(since vx>0).v_x = \frac{\sqrt{3}}{2}\,v_0 \quad (\text{since } v_x>0).
  3. The y-displacement is given by

    y=αexp[2vx3v0].y=\alpha \exp\Bigl[-\frac{2v_x}{\sqrt{3}v_0}\Bigr].

    Substituting vx=32v0v_x = \frac{\sqrt{3}}{2}\,v_0:

    y=αexp[2(32v0)3v0]=αexp(1).y=\alpha\exp\Bigl[-\frac{2\left(\frac{\sqrt{3}}{2}v_0\right)}{\sqrt{3}v_0}\Bigr] = \alpha\exp(-1).