JEE PYQ: Motion in a Straight Line - Question ID 468afadeb4a1 (JEE Main 2021)

ID: 468afadeb4a1JEE Main 2021Single Correct MCQ
The velocity-displacement graph describing the motion of bicycle is shown in the figure.

JEE Main 2021 (Online) 16th March Morning Shift Physics - Motion in a Straight Line Question 83 English
The acceleration-displacement graph of the bicycle's motion is best described by :
JEE Question illustration 468afadeb4a1

Select Option

Step-by-step Explanation

Core Formula & Concept:

To convert a velocity-displacement (vv vs xx) graph into an acceleration-displacement (aa vs xx) graph, we use the chain rule of calculus: a=dvdt=dvdxdxdt=vdvdx.a = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} = v \cdot \frac{dv}{dx}. Here, vv is the velocity at displacement xx, and dvdx\frac{dv}{dx} is the slope of the vvxx graph at that point.

Key observations from the given vvxx graph (a straight line with negative slope):

  • The slope dvdx\frac{dv}{dx} is constant and negative.
  • The velocity vv decreases linearly from a positive value at x=0x=0 to zero at some x=x0x=x_0.

Hence, a=vdvdxa = v \cdot \frac{dv}{dx} will be negative throughout and will vary linearly with xx (since vv itself is linear in xx).

Step-by-Step Derivation:

Step 1: Express vv as a function of xx.

From the graph, vv decreases linearly from v0v_0 at x=0x=0 to 00 at x=x0x=x_0. Thus v(x)=v0(1xx0).v(x) = v_0 \Bigl(1 - \frac{x}{x_0}\Bigr).

Step 2: Compute dvdx\frac{dv}{dx}.

Differentiating, dvdx=v0x0.\frac{dv}{dx} = -\frac{v_0}{x_0}. This slope is constant and negative.

Step 3: Compute a(x)a(x).

Using a=vdvdxa = v\,\frac{dv}{dx}, a(x)=v(x)dvdx=v0(1xx0)(v0x0)=v02x0(1xx0).a(x) = v(x)\,\frac{dv}{dx} = v_0\Bigl(1 - \frac{x}{x_0}\Bigr)\Bigl(-\frac{v_0}{x_0}\Bigr) = -\frac{v_0^2}{x_0}\Bigl(1 - \frac{x}{x_0}\Bigr). This is a linear function of xx that starts at a(0)=v02x0a(0)=-\frac{v_0^2}{x_0} and increases to a(x0)=0a(x_0)=0.

Step 4: Sketch aa vs xx.

The acceleration-displacement graph is a straight line with negative intercept at x=0x=0 and rising to zero at x=x0x=x_0. This matches option A.

Common Traps & Exam Tip:

1. Misapplying a=dvdta = \frac{dv}{dt} directly. Students often forget to use the chain rule a=vdvdxa = v\,\frac{dv}{dx} and instead try to read dvdt\frac{dv}{dt} from the vvxx graph, which is incorrect. 2. Sign errors. The negative slope of vv vs xx leads to a negative acceleration, but one must track how aa varies with xx. 3. Confusing intercepts. The acceleration does not start at zero; it starts at a negative value and increases linearly to zero.

Exam Tip: Always write down a=vdvdxa = v\,\frac{dv}{dx} explicitly when converting vvxx to aaxx. Then substitute the algebraic form of v(x)v(x) and differentiate.

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