JEE PYQ: Motion in a Straight Line - Question ID 779846aea1be (JEE Main 2024)

ID: 779846aea1beJEE Main 2024Single Correct MCQ

The relation between time 'tt' and distance 'xx' is t=αx2+βxt=\alpha x^2+\beta x, where α\alpha and β\beta are constants. The relation between acceleration (a)(a) and velocity (v)(v) is :

Select Option

Step-by-step Explanation

Core Formula & Concept:

In kinematics, when the position xx is given as a function of time tt, we can find velocity vv and acceleration aa by successive differentiation:

  • Velocity is the first derivative of position with respect to time: v=dxdtv = \frac{dx}{dt}.
  • Acceleration is the first derivative of velocity with respect to time: a=dvdt=d2xdt2a = \frac{dv}{dt} = \frac{d^2x}{dt^2}.

However, in this problem, time tt is expressed as a function of position xx, i.e., t=αx2+βxt = \alpha x^2 + \beta x. To find velocity and acceleration, we must use implicit differentiation with respect to time.

Key formulas used:

  • v=dxdtv = \frac{dx}{dt}
  • a=dvdt=vdvdxa = \frac{dv}{dt} = v \frac{dv}{dx} (chain rule)
Step-by-Step Derivation:

Step 1: Express dt/dxdt/dx

Given: t=αx2+βxt = \alpha x^2 + \beta x Differentiate both sides with respect to xx: dtdx=2αx+β\frac{dt}{dx} = 2\alpha x + \beta

Step 2: Find velocity v=dx/dtv = dx/dt

Since v=dxdtv = \frac{dx}{dt}, we have: v=1dtdx=12αx+βv = \frac{1}{\frac{dt}{dx}} = \frac{1}{2\alpha x + \beta}

Step 3: Express xx in terms of vv

From above: v=12αx+β    2αx+β=1vv = \frac{1}{2\alpha x + \beta} \implies 2\alpha x + \beta = \frac{1}{v} Solve for xx: 2αx=1vβ    x=1βv2αv2\alpha x = \frac{1}{v} - \beta \implies x = \frac{1 - \beta v}{2\alpha v}

Step 4: Find acceleration a=dv/dta = dv/dt using chain rule

We use: a=dvdt=dvdxdxdt=vdvdxa = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} = v \frac{dv}{dx} So, we need dvdx\frac{dv}{dx}.

From Step 2: v=(2αx+β)1v = (2\alpha x + \beta)^{-1} Differentiate with respect to xx: dvdx=1(2αx+β)22α=2α(2αx+β)2\frac{dv}{dx} = -1 \cdot (2\alpha x + \beta)^{-2} \cdot 2\alpha = -\frac{2\alpha}{(2\alpha x + \beta)^2} But 2αx+β=1v2\alpha x + \beta = \frac{1}{v}, so: dvdx=2α(1v)2=2αv2\frac{dv}{dx} = -\frac{2\alpha}{\left(\frac{1}{v}\right)^2} = -2\alpha v^2

Step 5: Compute acceleration aa

Now: a=vdvdx=v(2αv2)=2αv3a = v \frac{dv}{dx} = v \cdot (-2\alpha v^2) = -2\alpha v^3

Step 6: Match with given options

We have derived: a=2αv3a = -2\alpha v^3 This matches Option C.

Common Traps & Exam Tip:

Common Mistake 1: Students often try to differentiate tt with respect to tt directly, leading to confusion. Remember: tt is given as a function of xx, so dt/dxdt/dx is the correct starting point.

Common Mistake 2: Forgetting to use the chain rule a=vdvdxa = v \frac{dv}{dx} and instead trying to differentiate vv with respect to tt directly, which is not straightforward here.

Exam Tip: When time is given as a function of position, always invert the relationship to find dx/dtdx/dt, then proceed carefully using implicit differentiation. Keep track of powers of vv — the final expression must be in terms of vv and constants only.

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