JEE PYQ: Motion in a Plane - Question ID 95b3b5edff5a (JEE Main 2020)

ID: 95b3b5edff5aJEE Main 2020Single Correct MCQ
When a car is at rest, its driver sees rain drops falling on it vertically. When driving the car with speed v, he sees that rain drops are coming at an angle 60° from the horizontal. On further increasing the speed of the car to (1 + β\beta)v, this angle changes to 45o. The value of β\beta is close to :
JEE Question illustration 95b3b5edff5a

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Step-by-step Explanation

Core Formula & Concept:

In this problem, we analyze the motion of raindrops relative to a moving car. The key concept is relative velocity. When the car is stationary, the driver observes the raindrops falling vertically downward. However, when the car moves, the driver perceives the raindrops as approaching at an angle due to the combination of the car's horizontal velocity and the raindrops' vertical velocity.

Let:

  • vrv_r = velocity of raindrops relative to the ground (vertical, downward).
  • vv = speed of the car (horizontal, forward).
  • θ\theta = angle at which the driver sees the raindrops relative to the horizontal.

The relative velocity of the raindrops with respect to the car is: vr/c=vrvc\vec{v}_{r/c} = \vec{v}_r - \vec{v}_c Since vr\vec{v}_r is vertical and vc\vec{v}_c is horizontal, the magnitude of the relative velocity is: vr/c=vr2+v2|\vec{v}_{r/c}| = \sqrt{v_r^2 + v^2} The angle θ\theta that the relative velocity makes with the horizontal is given by: tanθ=vrv\tan \theta = \frac{v_r}{v} This is because the vertical component of the relative velocity is vrv_r (downward), and the horizontal component is vv (opposite to the car's motion).

Step-by-Step Derivation:

Step 1: Analyze the first scenario (car moving at speed vv)
When the car moves at speed vv, the driver sees the raindrops at an angle 6060^\circ from the horizontal. Using the relative velocity concept: tan60=vrv\tan 60^\circ = \frac{v_r}{v} We know tan60=3\tan 60^\circ = \sqrt{3}, so: 3=vrv    vr=v3\sqrt{3} = \frac{v_r}{v} \implies v_r = v \sqrt{3}

Step 2: Analyze the second scenario (car moving at speed (1+β)v(1 + \beta)v)
When the car's speed increases to (1+β)v(1 + \beta)v, the angle changes to 4545^\circ. Again, using the relative velocity concept: tan45=vr(1+β)v\tan 45^\circ = \frac{v_r}{(1 + \beta)v} We know tan45=1\tan 45^\circ = 1, so: 1=vr(1+β)v    vr=(1+β)v1 = \frac{v_r}{(1 + \beta)v} \implies v_r = (1 + \beta)v

Step 3: Equate the two expressions for vrv_r
From Step 1 and Step 2, we have: v3=(1+β)vv \sqrt{3} = (1 + \beta)v The vv terms cancel out: 3=1+β\sqrt{3} = 1 + \beta Solving for β\beta: β=31\beta = \sqrt{3} - 1

Step 4: Calculate the numerical value of β\beta
We know 31.732\sqrt{3} \approx 1.732, so: β=1.7321=0.732\beta = 1.732 - 1 = 0.732 This value is close to 0.730.73, which corresponds to option B.

Common Traps & Exam Tip:

  1. Misidentifying the angle: Students often confuse whether the angle is measured from the vertical or horizontal. Here, the angle is given from the horizontal, so tanθ=vrv\tan \theta = \frac{v_r}{v} is correct. If misread as from the vertical, the formula would incorrectly become tanθ=vvr\tan \theta = \frac{v}{v_r}.
  2. Incorrect relative velocity direction: The relative velocity of the raindrops with respect to the car is vrvc\vec{v}_r - \vec{v}_c, not vcvr\vec{v}_c - \vec{v}_r. Mixing up the order leads to the wrong angle calculation.
  3. Algebraic errors: When solving for β\beta, students might incorrectly cancel terms or misapply the tangent function. Always double-check the trigonometric identities and algebraic manipulations.
  4. Approximation errors: While 31.732\sqrt{3} \approx 1.732 is standard, some students might use a rougher approximation (e.g., 1.71.7), leading to an incorrect β\beta value. Use precise values for such calculations.

Exam Tip: Always draw a velocity vector diagram to visualize the relative motion. Label the directions clearly (e.g., car moving right, raindrops falling down). This helps avoid confusion about the angle and the components of velocity.