Work-Energy Theorem for a Variable Force

Physics · Work, Energy And Power · NEET

The work-energy theorem still holds even when the force keeps changing: the total work done by a variable force equals the change in kinetic energy, W = integral of F dx = K_f - K_i. So you find the work by integrating F(x) over displacement (or taking the area under the F-x graph), then set it equal to (1/2)m v_f^2 - (1/2)m v_i^2. Memory hook: "Area under F-x = change in KE" - the shape of the force does not matter, only the area it sweeps.
Work = Area under F-x graph = change in KExFW (positive area)negative area (F backward, KE drops)x_ix=8x=12W = integral F dx = K_f - K_i
Work done by a variable force is the net signed area under the force-displacement (F-x) graph. Areas above the axis add kinetic energy; areas below (where the force acts backward) remove it. The total area equals K_f - K_i.

Your doubts, answered

Does the work-energy theorem work when the force is not constant?

Yes. This is the key point for NEET. Whether the force is constant or variable, the theorem W = K_f - K_i is always true. For a constant force you compute W = F d cos theta; for a variable force you compute W = integral of F dx (the area under the force-displacement graph). The right side, change in kinetic energy, stays exactly the same. NCERT proves it starting from dK/dt = m v (dv/dt) = F v = F (dx/dt), which gives dK = F dx, and integrating both sides gives K_f - K_i = integral of F dx = W.

How do I find final velocity from a force-displacement (F-x) graph?

Three steps. Step 1: find the work done W = area under the F-x graph between the start and end positions (add positive areas, subtract areas below the x-axis where force is negative). Step 2: this area equals the change in kinetic energy, so W = (1/2) m v_f^2 - (1/2) m v_i^2. Step 3: solve for v_f. If the body starts from rest, v_i = 0, so v_f = square root of (2W/m). You never need the exact force formula, only the area.

When do I integrate and when do I take the area under the graph?

They are the same operation. If the problem gives you a formula like F = 20 + 10y, integrate: W = integral of F dy. If the problem gives you a graph of F versus x, find the geometric area (triangles and rectangles). Both give the work done, and both equal the change in kinetic energy. Use whichever the question hands you.

What does 'integral form of Newton's second law' mean?

NCERT says the work-energy theorem is an integral form of Newton's second law. Newton's second law F = m a tells you the force at one instant. When you multiply by dx and add up (integrate) over the whole path, the acceleration information turns into a change in kinetic energy. So the theorem does not give the full instant-by-instant motion, but it directly connects total work to the change in speed, which is often all you need.

Does the force being variable change the units or the final formula?

No. The work is still in joules and kinetic energy is still (1/2) m v^2 in joules. Only the method of getting W changes (integration or area instead of a simple multiplication). The final relation W = change in KE is identical.

⚠️ The NEET trap
Reading final velocity straight off the F-x graph, or using only the positive part of the area and ignoring the region where the force acts backward (below the x-axis).
Work = net signed area under the F-x graph. Add areas where F is positive, subtract areas where F is negative, then set that net work equal to the change in kinetic energy to solve for v.
🧠 In the NEET 2019 graph PYQ the speed goes DOWN from x = 8 m to x = 12 m because the force turns negative there and removes energy.

Real NEET questions

NEET 2019

A force F = 20 + 10y acts on a particle in the y-direction, where F is in newton and y is in metre. The work done by this force to move the particle from y = 0 to y = 1 m is:

A · 20 J
B · 30 J
C · 5 J
D · 25 J
Solution: The force varies with position, so integrate. W = integral from 0 to 1 of (20 + 10y) dy. Doing the integration: W = [20y + 5y^2] from 0 to 1 = (20(1) + 5(1)^2) - 0 = 20 + 5 = 25 J. By the work-energy theorem this 25 J also equals the gain in kinetic energy of the particle. Answer: D (25 J).
NEET 2019

An object of mass 500 g, initially at rest, is acted upon by a variable force whose X-component varies with X as shown in the graph. The velocities of the object at the points X = 8 m and X = 12 m would be, respectively (nearly):

A · 18 m/s and 24.4 m/s
B · 23 m/s and 24.4 m/s
C · 23 m/s and 20.6 m/s
D · 18 m/s and 20.6 m/s
Solution: Work = area under the F-x graph = change in kinetic energy. Mass m = 500 g = 0.5 kg, starting from rest (v_i = 0), so W = (1/2)(0.5)v^2. Up to x = 8 m the net area is about +130 J, so (1/2)(0.5)v^2 = 130, giving v^2 = 520 and v = about 22.8 m/s, nearly 23 m/s. From x = 8 m to x = 12 m the force is negative, so it removes energy; the net area up to x = 12 m drops to about +106 J, giving v = about 20.6 m/s. The speed falls because of the negative-force region. Answer: C (23 m/s and 20.6 m/s).

Solved Work, Energy And Power NEET PYQs

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Frequently asked

What is the statement of the work-energy theorem for a variable force?

The net work done by a variable force on a body equals the change in its kinetic energy: W = integral of F dx = K_f - K_i, where K = (1/2) m v^2. It is valid for any force, constant or variable.

How is the theorem derived in NCERT?

Start with the rate of change of kinetic energy: dK/dt = d/dt[(1/2)m v^2] = m v (dv/dt). By Newton's second law m (dv/dt) = F, so dK/dt = F v = F (dx/dt). This gives dK = F dx. Integrating from initial to final position: K_f - K_i = integral of F dx = W.

Is the work-energy theorem the same as Newton's second law?

It is the integral form of Newton's second law. Newton's law relates force and acceleration at each instant; the work-energy theorem sums the effect over a path, so it does not carry the full instant-by-instant information but directly links total work to change in speed.

Can the kinetic energy decrease under a variable force?

Yes. If the net work (net signed area under the F-x graph, or the integral of F dx) is negative, the kinetic energy decreases and the body slows down. This happens whenever the force acts opposite to the displacement over part of the path.

Why is this concept important for NEET?

NEET regularly gives problems where you must find work by integrating a position-dependent force or by taking the area under an F-x graph, then use W = change in KE to get the final speed. It rewards students who remember that the theorem holds even when the force is not constant.