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Work Power and Energy question

2014 · Shift 1 · Q44
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Work Power and Energy question

2014 · Shift 1 · Q44

JEE AdvancedPhysicsWork Power and EnergyNumerical+3 / −1
Consider an elliptically shaped rail PQ in the vertical plane with OP = 3 m and OQ = 4 m. A block of mass 1 kg is pulled along the rail from P to Q with a force of 18 N, which is always parallel to line PQ (see the figure given). Assuming no frictional losses, the kinetic energy of the block when it reaches Q is (n × 10) Joules. The value of n is (take acceleration due to gravity = 10 ms–2) JEE Advanced 2014 Paper 1 Offline Physics - Work Power & Energy Question 17 English
Numerical answer
View written solutionFree

Correct answer: 12

Step-by-step Solution

  1. Understand the Setup and Identify Forces

    • The system is a block of mass m = 1 kg.
    • The block moves on a vertical elliptical rail from point P to point Q.
    • The coordinates of the points are P = (0, 3 m) and Q = (4 m, 0), taking O as the origin.
    • The forces acting on the block are:
      • Gravitational force, Fg=mgF_g = mgFg​=mg, acting downwards.
      • An applied force, F = 18 N, which is always parallel to the line PQ.
      • The normal force from the rail, N, which is always perpendicular to the path. Since it's perpendicular to the displacement, it does no work.
    • We assume the block starts from rest, so its initial kinetic energy KEP=0KE_P = 0KEP​=0.
    • We need to find the final kinetic energy KEQKE_QKEQ​.
  2. Apply the Work-Energy Theorem The work-energy theorem states that the net work done on an object equals its change in kinetic energy. Wnet=ΔKE=KEQ−KEPW_{net} = \Delta KE = KE_Q - KE_PWnet​=ΔKE=KEQ​−KEP​ The net work is the sum of the work done by all forces: Wnet=WF+Wg+WNW_{net} = W_F + W_g + W_NWnet​=WF​+Wg​+WN​ Since WN=0W_N = 0WN​=0 and KEP=0KE_P = 0KEP​=0: KEQ=WF+WgKE_Q = W_F + W_gKEQ​=WF​+Wg​

  3. Calculate the Work Done by Gravity (W_g) The work done by the conservative gravitational force is the negative change in gravitational potential energy. Wg=−ΔUg=−(Ug,Q−Ug,P)W_g = -\Delta U_g = -(U_{g,Q} - U_{g,P})Wg​=−ΔUg​=−(Ug,Q​−Ug,P​) Let the potential energy be zero at the ground level (y=0). The initial height at P is hP=3h_P = 3hP​=3 m and the final height at Q is hQ=0h_Q = 0hQ​=0 m. Ug,P=mghP=(1 kg)(10 m/s2)(3 m)=30 JU_{g,P} = mgh_P = (1 \text{ kg})(10 \text{ m/s}^2)(3 \text{ m}) = 30 \text{ J}Ug,P​=mghP​=(1 kg)(10 m/s2)(3 m)=30 J Ug,Q=mghQ=(1 kg)(10 m/s2)(0 m)=0 JU_{g,Q} = mgh_Q = (1 \text{ kg})(10 \text{ m/s}^2)(0 \text{ m}) = 0 \text{ J}Ug,Q​=mghQ​=(1 kg)(10 m/s2)(0 m)=0 J Therefore, the work done by gravity is: Wg=−(0−30) J=30 JW_g = -(0 - 30) \text{ J} = 30 \text{ J}Wg​=−(0−30) J=30 J Alternatively, since the block's vertical displacement is 3 m downwards, gravity does positive work: Wg=mgΔh=(1)(10)(3)=30W_g = mg\Delta h = (1)(10)(3) = 30Wg​=mgΔh=(1)(10)(3)=30 J.

  4. Calculate the Work Done by the Applied Force (W_F) The applied force F has a constant magnitude of 18 N and is always parallel to the line PQ. This means the force vector F⃗\vec{F}F is constant in both magnitude and direction throughout the motion.

    • The displacement vector from P to Q is d⃗=r⃗Q−r⃗P=(4i^+0j^)−(0i^+3j^)=4i^−3j^\vec{d} = \vec{r}_Q - \vec{r}_P = (4\hat{i} + 0\hat{j}) - (0\hat{i} + 3\hat{j}) = 4\hat{i} - 3\hat{j}d=rQ​−rP​=(4i^+0j^​)−(0i^+3j^​)=4i^−3j^​.
    • The magnitude of the displacement vector is ∣d⃗∣=∣PQ⃗∣=42+(−3)2=16+9=25=5|\vec{d}| = |\vec{PQ}| = \sqrt{4^2 + (-3)^2} = \sqrt{16 + 9} = \sqrt{25} = 5∣d∣=∣PQ​∣=42+(−3)2​=16+9​=25​=5 m.
    • The force F⃗\vec{F}F is in the same direction as the displacement vector d⃗\vec{d}d. The work done by a constant force is given by WF=F⃗⋅d⃗W_F = \vec{F} \cdot \vec{d}WF​=F⋅d. Since F⃗\vec{F}F is parallel to d⃗\vec{d}d, the dot product simplifies to the product of their magnitudes. WF=F×∣d⃗∣W_F = F \times |\vec{d}|WF​=F×∣d∣ WF=18 N×5 m=90 JW_F = 18 \text{ N} \times 5 \text{ m} = 90 \text{ J}WF​=18 N×5 m=90 J It is important to note that for a constant force, the work done is independent of the path taken between the initial and final points.
  5. Calculate the Final Kinetic Energy (KE_Q) Now, we substitute the calculated work values into the work-energy theorem equation: KEQ=WF+Wg=90 J+30 J=120 JKE_Q = W_F + W_g = 90 \text{ J} + 30 \text{ J} = 120 \text{ J}KEQ​=WF​+Wg​=90 J+30 J=120 J

  6. Determine the value of n The problem states that the final kinetic energy is KEQ=(n×10)KE_Q = (n \times 10)KEQ​=(n×10) Joules. 120=n×10120 = n \times 10120=n×10 n=12010=12n = \frac{120}{10} = 12n=10120​=12

Conclusion and Comparison with Stored Answer

The derived value for n is 12. The stored correct answer is 5. There is a disagreement.

Let's analyze the discrepancy. The solution derived above is based on a straightforward application of the work-energy theorem. The calculations for work done by gravity (30 J) and the applied force (90 J) are robust based on the problem statement.

If we assume the stored answer n=5 is correct, the final kinetic energy would be KEQ=5×10=50KE_Q = 5 \times 10 = 50KEQ​=5×10=50 J. Using the work-energy theorem, KEQ=WF+WgKE_Q = W_F + W_gKEQ​=WF​+Wg​, we would have: 50J=WF+30J50 J = W_F + 30 J50J=WF​+30J This implies that the work done by the applied force should be WF=20W_F = 20WF​=20 J.

For WFW_FWF​ to be 20 J, given that the force acts over a displacement whose component along the force is 5 m, the magnitude of the force would need to be: F=WF/d=20J/5m=4F = W_F / d = 20 J / 5 m = 4F=WF​/d=20J/5m=4 N.

This suggests that the question likely contains a typo, and the applied force should have been 4 N instead of 18 N. However, solving the problem as stated gives n=12.

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