Work in
Physics
Understand how forces transfer energy when they act over a distance: the scalar quantity \( W = Fd\cos\theta \).
What is Work?
In physics, work measures the energy transferred to or from an object when a force acts on it through a displacement. Unlike everyday language, work has a precise definition: it requires both a force and a displacement in the direction of that force.
Three Ingredients of Work
Force, Displacement, and Angle
The Work Equation
Special Cases of \( \theta \)
Force is parallel to displacement.
Maximum positive work: \( W = Fd \)
Force is perpendicular to displacement.
Zero work: \( W = 0 \)
Force opposes displacement.
Negative work: \( W = -Fd \)
Positive vs. Negative Work
Work as Area Under the \( F \)-\( d \) Curve
Net Work and the Work-Energy Theorem
The net work done on an object equals its change in kinetic energy. This is the Work-Energy Theorem: it links the total work from all forces to how the object speeds up or slows down.
Additional worked example
The following is a separate example from the long-form lesson. Its values may differ from the example already on this slide.
A child pulls a 15 kg sled across a flat, snowy field with a rope that makes a 30° angle above the horizontal. The child exerts a constant 40 N tension on the rope, and the coefficient of kinetic friction between the sled and snow is μₖ = 0.10. The sled is pulled a horizontal distance of 20 m. Find (a) the work done by the tension, (b) the work done by friction, (c) the work done by gravity, (d) the net work, and (e) the final speed if the sled starts from rest.
Show answer and explanation
Step 1 — Identify Given Values: m = 15 kg, T = 40 N, θ = 30°, d = 20 m, μₖ = 0.10, v_(i) = 0 m/s, g = 9.8 m/s². Step 2 — Work Done by Tension: W_(T) = T d cos θ = (40)(20) cos 30° = (800)(0.866). W_T = 693 J Step 3 — Find Normal Force: In the vertical direction the sled is in equilibrium: N + T sin θ − mg = 0, so N = mg − T sin θ = (15)(9.8) − (40) sin 30° = 147 − 20 = 127 N. N = 127 N Step 4 — Work Done by Friction: fₖ = μₖ N = (0.10)(127) = 12.7 N. Friction opposes displacement, so θ = 180°: W_(f) = fₖ d cos 180° = (12.7)(20)(−1). W_f = −254 J Step 5 — Work Done by Gravity and Normal Force: Both gravity (downward) and the normal force (upward) are perpendicular to the horizontal displacement. Therefore W_(g) = 0 J and W_(N) = 0 J. Step 6 — Net Work and Final Speed: Wₙₑₜ = W_(T) + W_(f) + W_(g) + W_(N) = 693 + (−254) + 0 + 0 = 439 J. By the work-energy theorem, Wₙₑₜ = ½mv² − 0, so v = √(2Wₙₑₜ/m) = √(2 × 439 / 15) = √(58.5) ≈ 7.65 m/s. W_net = 439 J, v_f ≈ 7.65 m/s

Work vs. Energy vs. Power
| Work | Energy | Power | |
|---|---|---|---|
| Definition | Force acting over a distance | Capacity to do work | Rate of doing work |
| Formula | \( Fd\cos\theta \) | \( \frac{1}{2}mv^2 \), \( mgh \) | \( \frac{W}{t} \) |
| Unit | Joule (J) | Joule (J) | Watt (W) |
| Scalar/Vector | Scalar | Scalar | Scalar |
| Can be negative? | Yes | KE: No | Yes |
How to Solve Work Problems
Example 1: Pushing a Crate
Example 2: Pulling at an Angle
Example 3: Work by Friction
Common Mistakes
Summary of Work Concepts
| Scenario | \( \theta \) | \( \cos\theta \) | Work |
|---|---|---|---|
| Push along motion | \( 0^\circ \) | +1 | +Fd |
| Pull at angle | \( 0^\circ < \theta < 90^\circ \) | + (fraction) | + (reduced) |
| Carry horizontally (gravity) | \( 90^\circ \) | 0 | 0 |
| Push against motion (brake) | \( 90^\circ < \theta < 180^\circ \) | - (fraction) | - (reduced) |
| Friction / direct opposition | \( 180^\circ \) | -1 | -Fd |
Question 1 of 5
A student pushes a box with a force of 40 N over a distance of 5 m along a flat floor. The force is applied parallel to the floor. How much work is done?
Question 2 of 5
A person carries a 10 kg backpack while walking 50 m on a level path. How much work does the gravitational force do on the backpack?
Question 3 of 5
A rope pulls a sled with a force of 80 N at an angle of 60° above the horizontal over a displacement of 12 m. What is the work done by the rope?
Question 4 of 5
A 3 kg object moving at 4 m/s is brought to rest by friction over 2 m. What is the net work done on the object?
Question 5 of 5
Which of the following situations involves zero net work done on the object?