JEE PYQ: Motion in a Straight Line - Question ID de5a28d2d9f5 (JEE Main 2006)

ID: de5a28d2d9f5JEE Main 2006Single Correct MCQ
A particle located at x = 0 at time t = 0, starts moving along the positive x-direction with a velocity 'v' that varies as v=αxv = \alpha \sqrt x. The displacement of the particle varies with time as

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Step-by-step Explanation

Core Formula & Concept:

In kinematics, when a particle moves along a straight line, its velocity vv is defined as the time derivative of its displacement xx: v=dxdt.v = \frac{dx}{dt}. The problem gives the velocity as a function of position: v=αx,v = \alpha \sqrt{x}, where α\alpha is a positive constant. Our goal is to find how the displacement xx varies with time tt, starting from x=0x = 0 at t=0t = 0.

Step-by-Step Derivation:

Step 1: Express the differential equation
Given v=dxdt=αxv = \frac{dx}{dt} = \alpha \sqrt{x}, we rewrite this as: dxdt=αx1/2.\frac{dx}{dt} = \alpha x^{1/2}. This is a separable first-order ordinary differential equation.

Step 2: Separate variables
Rearrange the equation to isolate xx and tt: dxx1/2=αdt.\frac{dx}{x^{1/2}} = \alpha \, dt.

Step 3: Integrate both sides
Integrate the left side with respect to xx and the right side with respect to tt: x1/2dx=αdt.\int x^{-1/2} \, dx = \int \alpha \, dt. The integrals evaluate to: 2x1/2=αt+C,2 x^{1/2} = \alpha t + C, where CC is the constant of integration.

Step 4: Apply the initial condition
At t=0t = 0, x=0x = 0. Substituting these values: 201/2=α0+C    C=0.2 \cdot 0^{1/2} = \alpha \cdot 0 + C \implies C = 0. Thus, the equation simplifies to: 2x1/2=αt.2 x^{1/2} = \alpha t.

Step 5: Solve for xx
Square both sides to eliminate the square root: (2x1/2)2=(αt)2    4x=α2t2.(2 x^{1/2})^2 = (\alpha t)^2 \implies 4 x = \alpha^2 t^2. Therefore, x=α24t2.x = \frac{\alpha^2}{4} t^2. This shows that the displacement xx varies as t2t^2.

Common Traps & Exam Tip:

Students often make the following mistakes:

  • Incorrect separation of variables: Forgetting to separate dxdx and dtdt properly, leading to incorrect integration.
  • Ignoring the initial condition: Failing to apply x=0x = 0 at t=0t = 0, which results in an incorrect constant of integration.
  • Misinterpreting the velocity expression: Assuming v=αxv = \alpha \sqrt{x} implies constant acceleration, which is not the case here. The acceleration is not constant.
  • Algebraic errors in solving for xx: Squaring both sides incorrectly or forgetting to divide by the coefficient of xx.
Exam Tip: Always verify units and dimensions. Here, α\alpha must have units of [L1/2T1][L^{1/2} T^{-1}] to ensure v=αxv = \alpha \sqrt{x} has units of velocity. The final expression xt2x \propto t^2 is dimensionally consistent.

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