JEE PYQ: Motion in a Straight Line - Question ID 1ad94d5642e1 (JEE Main 2022)

ID: 1ad94d5642e1JEE Main 2022Single Correct MCQ

The velocity of the bullet becomes one third after it penetrates 4 cm in a wooden block. Assuming that bullet is facing a constant resistance during its motion in the block. The bullet stops completely after travelling at (4 + x) cm inside the block. The value of x is :

Select Option

Step-by-step Explanation

Core Formula & Concept:

This problem involves the motion of a bullet under a constant resistive force inside a wooden block. The key physics concepts and formulas are:

  • Work-Energy Theorem: When a constant force FF acts on a body, the work done by the force equals the change in kinetic energy of the body. W=ΔK=KfKiW = \Delta K = K_f - K_i Here, the resistive force FF does negative work (since it opposes motion), so: Fs=12mvf212mvi2-F \cdot s = \frac{1}{2} m v_f^2 - \frac{1}{2} m v_i^2 where ss is the displacement, mm is the mass of the bullet, and viv_i, vfv_f are initial and final velocities.
  • Constant Resistance Implies Constant Deceleration: Since the resistive force is constant, the deceleration aa is also constant. We can use kinematic equations for uniformly decelerated motion: vf2=vi2+2asv_f^2 = v_i^2 + 2 a s Here, aa is negative (deceleration), so: vf2=vi22asv_f^2 = v_i^2 - 2 |a| s

We are given: - After penetrating s1=4 cms_1 = 4 \text{ cm}, velocity becomes v1=v03v_1 = \frac{v_0}{3}, where v0v_0 is the initial velocity. - The bullet stops after travelling a total distance stotal=4+x cms_{\text{total}} = 4 + x \text{ cm}. We need to find xx.

--- Step-by-Step Derivation:

Step 1: Apply Work-Energy Theorem for the first 4 cm

Let mm = mass of bullet, v0v_0 = initial velocity, v1=v03v_1 = \frac{v_0}{3} = velocity after 4 cm. Work done by resistive force FF over distance s1=4 cms_1 = 4 \text{ cm}: Fs1=12mv1212mv02-F \cdot s_1 = \frac{1}{2} m v_1^2 - \frac{1}{2} m v_0^2 Substitute v1=v03v_1 = \frac{v_0}{3}: F4=12m(v03)212mv02-F \cdot 4 = \frac{1}{2} m \left(\frac{v_0}{3}\right)^2 - \frac{1}{2} m v_0^2 4F=12m(v029v02)-4F = \frac{1}{2} m \left(\frac{v_0^2}{9} - v_0^2\right) 4F=12mv02(191)-4F = \frac{1}{2} m v_0^2 \left(\frac{1}{9} - 1\right) 4F=12mv02(89)-4F = \frac{1}{2} m v_0^2 \left(-\frac{8}{9}\right) 4F=49mv02-4F = -\frac{4}{9} m v_0^2 Multiply both sides by 1-1: 4F=49mv024F = \frac{4}{9} m v_0^2 Divide both sides by 4: F=19mv02(Equation 1)F = \frac{1}{9} m v_0^2 \quad \text{(Equation 1)}

Step 2: Apply Work-Energy Theorem until bullet stops

Total distance travelled before stopping: stotal=4+xs_{\text{total}} = 4 + x Final velocity vf=0v_f = 0 Work done by resistive force over total distance: Fstotal=12m0212mv02-F \cdot s_{\text{total}} = \frac{1}{2} m \cdot 0^2 - \frac{1}{2} m v_0^2 F(4+x)=12mv02-F (4 + x) = -\frac{1}{2} m v_0^2 Multiply both sides by 1-1: F(4+x)=12mv02(Equation 2)F (4 + x) = \frac{1}{2} m v_0^2 \quad \text{(Equation 2)}

Step 3: Substitute FF from Equation 1 into Equation 2

From Equation 1: F=19mv02F = \frac{1}{9} m v_0^2 Substitute into Equation 2: 19mv02(4+x)=12mv02\frac{1}{9} m v_0^2 (4 + x) = \frac{1}{2} m v_0^2 Cancel mv02m v_0^2 from both sides (assuming m0m \neq 0, v00v_0 \neq 0): 19(4+x)=12\frac{1}{9} (4 + x) = \frac{1}{2} Multiply both sides by 9: 4+x=924 + x = \frac{9}{2} 4+x=4.54 + x = 4.5 Subtract 4: x=0.5x = 0.5

Conclusion: The value of xx is 0.50.5 cm, which corresponds to option C.

--- Common Traps & Exam Tip:

Trap 1: Misapplying Kinematic Equations Without Considering Signs
Students often forget that deceleration is negative acceleration. If they use vf2=vi2+2asv_f^2 = v_i^2 + 2 a s without accounting for the negative sign of aa, they get incorrect results. Always define deceleration as a-|a|.

Trap 2: Incorrect Use of Work-Energy Theorem
Some students forget that the work done by a resistive force is negative. They write Fs=ΔKF \cdot s = \Delta K instead of Fs=ΔK-F \cdot s = \Delta K. This leads to sign errors and wrong answers.

Trap 3: Assuming Linear Velocity-Distance Relationship
Students sometimes assume velocity decreases linearly with distance, which is incorrect under constant deceleration. Velocity decreases quadratically with distance (v2sv^2 \propto s), not linearly.

Exam Tip:
Always start by writing down known quantities and the physics principle to apply. In this case, since force is constant, the work-energy theorem is the most straightforward approach. Avoid unnecessary use of kinematic equations unless explicitly required.

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