PhysicsChapter 5: Work and Kinetic Energy
Work Done by a Constant Force
Explanation level
Overview
In physics, work is done when a force causes an object to move through a displacement.
Work depends on:
- Magnitude of the force
- Magnitude of displacement
- Angle between force and displacement
For a constant force:
W = F⃗ · d⃗
or:
W = Fd cos θ
Learning Outcomes
Students should be able to:
- Define work scientifically.
- Explain why work is a scalar quantity.
- Calculate work done by a constant force.
- Resolve force into parallel and perpendicular components.
- Differentiate between positive, negative and zero work.
- Calculate work done by several forces.
- State the SI unit and dimensions of work.
1. Definition of Work
Work done on an object is the scalar or dot product of force and displacement:
W = F⃗ · d⃗
Its magnitude is:
W = Fd cos θ
Where:
- W = work done
- F = magnitude of constant force
- d = magnitude of displacement
- θ = angle between force and displacement
Work is a scalar quantity because a dot product produces a scalar.
2. Conditions Necessary for Work
For mechanical work to be done:
- A force must act on the object.
- The object must undergo displacement.
- The force must have a component along the displacement.
If any of these conditions is missing, the work done is zero.
3. Effective Component of Force
Suppose a force F acts at angle θ to horizontal displacement d.
The force has two components:
Parallel component
F∥ = F cos θ
This component acts along the displacement and performs work.
Perpendicular component
F⊥ = F sin θ
This component is perpendicular to the displacement and performs no work.
Therefore:
W = F∥ d W = (F cos θ) d
Work Done by a Constant Force

Intermediate Level
4. Positive Work
Work is positive when force has a component in the direction of displacement.
The angle lies in the range:
0° ≤ θ < 90°
In this range:
cos θ > 0
Therefore:
W > 0
Maximum positive work
When force and displacement act in the same direction:
θ = 0° W = Fd cos 0° W = Fd
Examples include:
- Pulling a box forward
- Gravity acting on a falling object
- An engine moving a vehicle forward
5. Negative Work
Work is negative when force has a component opposite to displacement.
The angle lies in the range:
90° < θ ≤ 180°
In this range:
cos θ < 0
Therefore:
W < 0
When force acts directly opposite to displacement:
θ = 180° W = Fd cos 180° W = −Fd
Examples include:
- Friction acting on a sliding object
- Braking force acting on a moving vehicle
- Air resistance opposing motion
Negative work generally removes mechanical energy from an object.
6. Zero Work
Work is zero when force is perpendicular to displacement:
θ = 90°
Therefore:
W = Fd cos 90° W = 0
Work is also zero when:
F = 0
or:
d = 0
Examples include:
- Normal reaction on an object moving horizontally
- Gravitational force on an object moving horizontally
- Holding a stationary object
- Centripetal force in uniform circular motion
7. Work and Angle
Work and Angle
| Angle θ | Value of cos θ | Type of work |
|---|---|---|
| 0° | 1 | Maximum positive |
| Between 0° and 90° | Positive | Positive |
| 90° | 0 | Zero |
| Between 90° and 180° | Negative | Negative |
| 180° | −1 | Maximum negative |
8. Net Work Done by Several Forces
If several constant forces act on an object, calculate the work performed by each force separately.
W₁ = F₁ d cos θ₁ W₂ = F₂ d cos θ₂ W₃ = F₃ d cos θ₃
The net work is:
Wnet = W₁ + W₂ + W₃ + ⋯
or:
Wnet = Σᵢ Fᵢ d cos θᵢ
For horizontal displacement:
- Horizontal forces may perform positive or negative work.
- Weight performs zero work.
- Normal reaction performs zero work.
9. SI Unit of Work
From:
W = Fd
The unit of force is newton and the unit of displacement is metre.
Therefore:
[W] = N m
The SI unit of work is the joule:
1 J = 1 N m
Using:
1 N = 1 kg m s⁻²
Therefore:
1 J = 1 kg m s⁻² × 1 m 1 J = 1 kg m² s⁻²
10. Dimensions of Work
W = Fd
Dimensions of force are:
[F] = [MLT⁻²]
Therefore:
[W] = [MLT⁻²][L] [W] = [ML²T⁻²]
Work and energy have the same unit and dimensions because work represents energy transferred by a force.
11. Work Is Not the Same as Effort
In everyday language, holding a heavy object may feel like hard work. However, if the object does not move:
d = 0
Therefore:
W = F(0) cos θ W = 0
Mechanical work may be zero even though the person uses biological energy.
Formula Summary
Formula Summary
| Situation | Formula |
|---|---|
| General constant force | W = Fd cos θ |
| Force parallel to displacement | W = Fd |
| Force opposite to displacement | W = −Fd |
| Force perpendicular to displacement | W = 0 |
| Several forces | Wnet = Σ Wᵢ |
| Parallel force component | F∥ = F cos θ |
| Perpendicular component | F⊥ = F sin θ |
Solved Examples
Example 1: Force Along Displacement
A constant force of 20 N moves a box through 5 m in the same direction. Calculate the work done.
Given:
F = 20 N d = 5 m θ = 0°
Formula:
W = Fd cos θ
Solution:
W = (20)(5) cos 0° W = (20)(5)(1) W = 100 J
Final answer:
W = 100 J
Example 2: Force Acting at an Angle
A 50 N force moves an object through 3 m. The force makes an angle of 60° with the displacement.
Formula:
W = Fd cos θ
Solution:
W = (50)(3) cos 60° W = (50)(3)(0.5) W = 75 J
Final answer:
W = 75 J
Example 3: Negative Work by Friction
A frictional force of 8 N opposes an object moving through 6 m.
Given:
F = 8 N d = 6 m θ = 180°
Formula:
W = Fd cos θ
Solution:
W = (8)(6) cos 180° W = (8)(6)(−1) W = −48 J
Final answer:
W = −48 J
Example 4: Textbook Suitcase Example
A suitcase is pulled through 4.90 m by a constant force of 16.8 N acting at 30° above the horizontal. A frictional force of 0.170 N opposes its motion.
Part A: Work done by applied force
WM = FM d cos θM WM = (16.8)(4.90) cos 30° WM = (16.8)(4.90)(0.866) WM = 71.3 J WM = 71.3 J
Part B: Work done by friction
Wf = Ff d cos θf Wf = (0.170)(4.90) cos 180° Wf = (0.170)(4.90)(−1) Wf = −0.833 J Wf = −0.833 J
Part C: Work by weight and normal reaction
Both forces are perpendicular to horizontal displacement:
θ = 90°
Therefore:
Wg = 0 WN = 0
Part D: Net work
Wnet = WM + Wf + Wg + WN Wnet = 71.3 − 0.833 + 0 + 0 Wnet = 70.467 J Wnet ≈ 70.5 J
Scientist Connection
The SI unit of work is named after James Prescott Joule, whose experiments helped establish that heat is a form of energy transfer.
1 joule = 1 newton-metre
Important Exam Facts
- Work is the dot product of force and displacement.
- Work is a scalar quantity.
- Only F cos θ performs work along displacement.
- Work is positive when force supports motion.
- Work is negative when force opposes motion.
- Work is zero when force and displacement are perpendicular.
- No displacement means no mechanical work.
- Net work is the sum of work done by all forces.
- The SI unit is joule.
- The dimensions are [ML²T⁻²].
Common Mistakes
- Using W = Fd when the force acts at an angle.
- Using F sin θ instead of F cos θ.
- Measuring θ from the wrong direction.
- Ignoring the negative sign of frictional work.
- Thinking every acting force performs work.
- Including weight in horizontal motion without checking the angle.
- Confusing work with force or power.
- Writing joule per second as the unit of work.
- Forgetting that work is a scalar.
MCQs with Answers
1. Work done by a constant force is: A. Fd sin θ B. Fd cos θ C. Fd D. Fd² Answer: B — W = Fd cos θ.
2. Work is a: A. Vector quantity B. Scalar quantity C. Base quantity D. Dimensionless quantity Answer: B — Work is obtained from a dot product.
3. Work is zero when force and displacement are: A. Parallel B. Opposite C. Perpendicular D. Equal Answer: C — cos 90° = 0.
4. Friction usually performs: A. Positive work B. Negative work C. Zero work in every case D. Infinite work Answer: B — Friction generally acts opposite to displacement.
5. The SI unit of work is: A. Watt B. Newton C. Joule D. Pascal Answer: C — Joule.
Short-Question Preparation
Short-Question Preparation
Q. Define work and state its formula.
A. Work is the scalar product of force and displacement. For a constant force: W = F⃗ · d⃗ = Fd cos θ. Only the component of force parallel to displacement performs work.
Q. Why does a perpendicular force perform zero work?
A. When force is perpendicular to displacement, the angle is 90°. Since cos 90° = 0, the force has no component along the displacement and performs zero work.
Q. Differentiate between positive and negative work.
A. Positive work occurs when force has a component in the direction of displacement. Negative work occurs when force has a component opposite to displacement. Positive work normally adds energy, while negative work normally removes it.
Long-Question Preparation
A complete answer should include:
- Definition of work.
- Vector expression W = F⃗ · d⃗.
- Scalar expression W = Fd cos θ.
- Meaning of F, d and θ.
- Resolution of force into components.
- Explanation of F cos θ.
- Explanation of why F sin θ does no work.
- Conditions for positive work.
- Conditions for negative work.
- Conditions for zero work.
- Maximum positive work.
- Maximum negative work.
- SI unit of work.
- Relationship 1 J = 1 N m.
- Dimensional formula.
- Work done by several forces.
- Definition of net work.
- Suitable real-life examples.
Sticky Notes
Sticky Notes
- Main formula: W = Fd cos θ
- Component rule: Only the force component parallel to displacement performs work.
- Sign rule: Same direction is positive; opposite direction is negative.
- Zero-work rule: Perpendicular force or zero displacement means zero work.
- Exam warning: Always identify the angle between force and displacement.
Ask-the-Tutor Modes
Students may select:
- Explain work in simpler words.
- Determine whether work is positive, negative or zero.
- Resolve force into useful components.
- Check a numerical solution one step per line.
- Explain why a particular force performs no work.
60-Second Revision
W = F⃗ · d⃗ W = Fd cos θ 1 J = 1 N m [W] = [ML²T⁻²] θ = 0°: maximum positive work θ = 90°: zero work θ = 180°: maximum negative work Work is scalar. Net work is the sum of work done by all forces.
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Exam preparation
Exam Focus
Important points
- Work is the dot product of force and displacement.
- Work is a scalar quantity.
- Only F cos θ performs work along displacement.
- Work is positive when force supports motion.
- Work is negative when force opposes motion.
- Work is zero when force and displacement are perpendicular.
Common mistakes
- Using W = Fd when the force acts at an angle.
- Using F sin θ instead of F cos θ.
- Measuring θ from the wrong direction.
- Ignoring the negative sign of frictional work.
- Thinking every acting force performs work.
- Including weight in horizontal motion without checking the angle.
- Confusing work with force or power.
- Writing joule per second as the unit of work.
- Forgetting that work is a scalar.
Quick revision
Revision Zone
Review the key facts, formulas and checks before you move on.Work Done by a Constant Force
Sticky Notes · Quick Revision
Core ideas
- Main formula: W = Fd cos θ
- Component rule: Only the force component parallel to displacement performs work.
- Sign rule: Same direction is positive; opposite direction is negative.
Exam tips
- Zero-work rule: Perpendicular force or zero displacement means zero work.
- Exam warning: Always identify the angle between force and displacement.
Ready to test yourself?
You've completed the learning section.
- 5 concept questions
- Easy → Medium → Hard
- Explanation after each answer
Exam Practice
Important Short Question
Q1. Define work and state its formula.
Important Short Question
Q2. Why does a perpendicular force perform zero work?
Important Short Question
Q3. Differentiate between positive and negative work.
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