Applying the Work-Energy Theorem to Solve Problems

Physics · Work, Energy And Power · NEET

The work-energy theorem says the net work done on a body equals its change in kinetic energy: W(net) = Kf - Ki = (1/2)m v^2 - (1/2)m u^2. To solve a numerical, find the net work (or use W = F d for a single force), set it equal to the change in kinetic energy, and solve for the unknown. Memory hook: "Net work changes the speed" - only the total work by all forces matters, not any single force.
Work-Energy Theorem: Net Work Changes Kinetic EnergymumvF (applied)friction (-)displacement dW(net) = Kf - Ki(1/2)m v^2 - (1/2)m u^2
Only the net work of all forces (applied force minus friction) equals the change in kinetic energy as the block moves from speed u to speed v over displacement d.

Your doubts, answered

Do I plug in the net force or a single force into W = F d?

You must use the NET work, meaning the sum of work done by every force. The theorem is W(net) = Kf - Ki. If a box is pushed with 50 N while friction resists with 20 N over 4 m, W(net) = (50 - 20)(4) = 120 J, not 50(4). A common mistake is using only the applied force and forgetting friction or gravity. When one force alone acts, then W(net) equals that force's work.

How do I find the final speed of a body using the work-energy theorem?

Compute the net work W, then write W = (1/2)m v^2 - (1/2)m u^2 and solve for v. Rearranged, v = sqrt(u^2 + 2W/m). Example: a 2 kg body at rest (u = 0) gains 100 J of net work, so 100 = (1/2)(2)v^2, giving v^2 = 100 and v = 10 m/s. This works even when the force is not constant, as long as you know the total work done.

Why is the work done by friction taken as negative when a car stops?

Friction acts opposite to the motion, so the angle between force and displacement is 180 degrees and cos 180 = -1. This makes W(friction) = -F d, a negative value. In a stopping problem the car's kinetic energy falls to zero, so W(net) = 0 - Ki, which is negative. Setting -F d = -Ki gives F d = Ki, the neat result that the braking work removes all the starting kinetic energy.

When should I use the work-energy theorem instead of v^2 = u^2 + 2as?

Use the work-energy theorem when the force is variable, when several forces act, or when the path is curved (like a circle or an incline). Kinematics equations only work for constant acceleration along a straight line. The theorem still gives the right speed even if acceleration changes, because it deals with total energy, not step-by-step motion. For simple constant-force straight-line cases both give the same answer.

Does the work-energy theorem work on a curved or circular path?

Yes. Kinetic energy depends only on speed, not direction, so the theorem holds on any path. For a particle speeding up on a circle, the net work equals the change in (1/2)m v^2. In the NEET 2016 circular-motion PYQ, the tangential force does work over the arc length travelled (two revolutions), and that work equals the gained kinetic energy. The centripetal force does zero work because it is always perpendicular to the velocity.

⚠️ The NEET trap
Using only the applied (pushing) force to compute work and equating it to the change in kinetic energy.
Use the NET work of all forces: W(net) = W(applied) + W(friction) + W(gravity) = Kf - Ki.
🧠 The theorem uses NET work, not one force. Always add friction and gravity work with their correct signs before equating to the kinetic energy change.

Real NEET questions

NEET 2025

The kinetic energies of two similar cars A and B are 100 J and 225 J respectively. On applying brakes, car A stops after 1000 m and car B stops after 1500 m. If F(A) and F(B) are the braking forces on cars A and B respectively, then the ratio F(A)/F(B) is

A · 1/3
B · 1/2
C · 3/2
D · 2/3
Solution: By the work-energy theorem, the braking work removes all the kinetic energy: F d = KE, so F = KE / d. For car A, F(A) = 100 / 1000 = 0.10 N. For car B, F(B) = 225 / 1500 = 0.15 N. The ratio F(A)/F(B) = 0.10 / 0.15 = 2/3. Answer: 2/3 (option D).
NEET 2017

Consider a drop of rain water having mass 1 g falling from a height of 1 km. It hits the ground with a speed of 50 m/s. Take g = 10 m/s^2. The work done by the (i) gravitational force and the (ii) resistive force of air is

A · (i) 1.25 J (ii) -8.25 J
B · (i) 100 J (ii) 8.75 J
C · (i) -10 J (ii) -8.25 J
D · (i) 10 J (ii) -8.75 J
Solution: Mass m = 1 g = 10^-3 kg, h = 1 km = 1000 m. Work by gravity: W(grav) = m g h = 10^-3 x 10 x 1000 = 10 J. Change in kinetic energy: delta KE = (1/2)m v^2 = (1/2)(10^-3)(50)^2 = 1.25 J. Work-energy theorem (net work = delta KE): W(grav) + W(air) = delta KE, so W(air) = 1.25 - 10 = -8.75 J. Answer: (i) 10 J (ii) -8.75 J (option D).
NEET 2016 Phase 1

A particle of mass 10 g moves along a circle of radius 6.4 cm with a constant tangential acceleration. The magnitude of this acceleration, if the kinetic energy of the particle becomes equal to 8 x 10^-4 J by the end of the second revolution after the beginning of the motion, is

A · 0.15 m/s^2
B · 0.18 m/s^2
C · 0.1 m/s^2
D · 0.2 m/s^2
Solution: From kinetic energy, find v: (1/2)m v^2 = 8 x 10^-4, so v^2 = 2(8 x 10^-4)/0.01 = 0.16. The particle travels 2 full circles, so arc length s = 2(2 pi r) = 4 pi (0.064) = 0.804 m. Using v^2 = 2 a(t) s along the path (work-energy theorem for the tangential force), a(t) = v^2 / (2s) = 0.16 / 1.608 = 0.1 m/s^2. Answer: 0.1 m/s^2 (option C).

Solved Work, Energy And Power NEET PYQs

Try the real previous-year questions from this chapter — each with the answer and a full solution.

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Frequently asked

What is the formula used to solve work-energy theorem numericals?

W(net) = Kf - Ki = (1/2)m v^2 - (1/2)m u^2, where W(net) is the total work by all forces, u is initial speed and v is final speed.

Can the work-energy theorem give a negative answer?

Yes. If the body slows down, Kf is less than Ki, so W(net) is negative. This happens when resistive forces like friction or air drag do more negative work than any positive work.

Is the work-energy theorem valid for variable forces?

Yes. The theorem holds for constant and variable forces. For a variable force you find the total work by integration or as the area under a force-displacement graph, then equate it to the change in kinetic energy.

Why is the work-energy theorem important for NEET?

Many NEET problems ask for final speed, stopping distance, or an unknown force. The theorem skips finding acceleration and time, giving a fast one-step link between force, distance and speed - a big time saver in the exam.

Does gravity do positive or negative work on a falling body?

Positive. A falling body moves in the same direction as gravity, so W(grav) = m g h is positive. For a body rising, gravity does negative work equal to -m g h.