What is the work-energy theorem?

The work-energy theorem is a fundamental physics principle stating that the net work done on an object is exactly equal to the change in its kinetic energy. In equation form, it is written as Wnet=ΔKW_{\text{net}} = \Delta K. Think of your bank account: the net money you deposit or withdraw (work) exactly equals the change in your account balance (kinetic energy). If you push a shopping cart forward (doing positive work), its speed increases. If friction drags against the cart (doing negative work), its speed decreases.

What it is: Defining the terms

To use this theorem, we need to understand its two pieces. Net work (WnetW_{\text{net}}) is the sum of all the work done by every force acting on the object. Kinetic energy (KK) is the energy an object has due to its motion, calculated using the formula K=12mv2K = \frac{1}{2}mv^2. The theorem simply says that whenever forces act on an object over a distance, the total effort (work) translates directly into a change in the object's motion energy.

Why it works: The connection to forces

This theorem isn't just a coincidence; it is born directly from Newton's second law (F=maF = ma) and the equations of motion (kinematics). When a net force pushes an object over a certain distance, it causes the object to accelerate. That acceleration means the object's velocity is changing. By multiplying the net force by the distance, we are effectively calculating exactly how much the kinetic energy has changed.

Where students slip: Net work vs. single work

The most common mistake students make is calculating the work done by just one force (like a person pushing a box) and setting that equal to the change in kinetic energy. You must account for all forces! If you push a box but friction is pushing back, you must subtract the work done by friction to find the true net work. Only the net work equals ΔK\Delta K.

Worked through

A 1000 kg car is traveling at 10 m/s. The driver applies the brakes, which exert a steady net frictional force of -2000 N over a distance of 20 m. What is the final speed of the car?

First, we calculate the net work done on the car. Wnet=Fnet×d=2000 N×20 m=40,000 JW_{\text{net}} = F_{\text{net}} \times d = -2000 \text{ N} \times 20 \text{ m} = -40,000 \text{ J}. Next, we find the initial kinetic energy: Ki=12mv2=12(1000 kg)(10 m/s)2=50,000 JK_i = \frac{1}{2}mv^2 = \frac{1}{2}(1000 \text{ kg})(10 \text{ m/s})^2 = 50,000 \text{ J}. Using the work-energy theorem, Wnet=KfKiW_{\text{net}} = K_f - K_i. Plugging in our numbers: 40,000 J=Kf50,000 J-40,000 \text{ J} = K_f - 50,000 \text{ J}. Solving for final kinetic energy gives Kf=10,000 JK_f = 10,000 \text{ J}. Finally, we use the kinetic energy formula to find the final speed: 10,000=12(1000)vf210,000 = \frac{1}{2}(1000)v_f^2. This simplifies to 10,000=500vf210,000 = 500v_f^2, so vf2=20v_f^2 = 20. Taking the square root, vf4.47 m/sv_f \approx 4.47 \text{ m/s}.

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Where this comes from: OpenStax University Physics Volume 1 · Khan Academy AP Physics 1

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