Field, contact and elastic forces
Key idea: Forces describe interactions. Identify what is interacting with the chosen body before deciding the force type or direction.
Continue where you stopped
The core idea
H1 Physics 8867 · Lesson 1 of 3
Check your understandingBy the end of this lesson, you should be able to
- Describe gravitational, electric and magnetic field forces on the appropriate object.
- Recognise normal, frictional and viscous contact forces without using out-of-scope coefficients.
- Apply Hooke’s law within the proportional region.
Learn the idea
Big question: Which interaction produces each force, and what determines that force’s direction?
Choose the body before naming forces
A force diagram answers one question: what forces act on this chosen body? Weight is exerted by a gravitational field on mass; electric force by an electric field on charge; magnetic force by a magnetic field on a current-carrying conductor. Contact forces arise only where the body touches a surface, spring or fluid.
Naming the agent prevents invented forces. A flying ball has weight and perhaps drag, but it does not retain a forward force from the hand after contact ends.
Check your understanding: Why is a normal force not automatically equal to weight?
Its size is set by the complete force balance perpendicular to the surface; other forces or acceleration can make it different from weight.
Separate motion from force direction
Drag and friction oppose relative motion between contacting bodies or fluid layers. A spring force instead opposes deformation: a stretched spring pulls and a compressed spring pushes towards its natural length. Neither rule says that force must oppose the object’s instantaneous velocity.
Check your understanding: A compressed spring launches a block forward. Can spring force and velocity point the same way?
Yes. While the spring expands, its restoring force can accelerate the already forward-moving block in the same direction.
Key ideas
- Name the agent exerting each force.
- Draw only forces acting on the chosen body.
- The spring constant k is the gradient of a straight F–x graph.
Relationships to know
weight W = mgelectric force F = QEspring force magnitude F = kx
Follow the reasoning
Worked example
Use Hooke’s law inside an equilibrium argument
Question: A 0.60 kg block rests on a rough horizontal table. A spring of force constant 80 N m⁻¹ attached on the right is stretched by 0.050 m. Find the friction force and describe all other forces.
Step 1: Calculate the spring interaction
Why: The extension is within the stated proportional regime, so Hooke’s law applies.
Working: Fspring = kx = 80(0.050) = 4.0 N to the right.
Step 2: Apply horizontal equilibrium
Why: The resting block has zero resultant horizontal force.
Working: Ffriction + 4.0 = 0, so friction is 4.0 N to the left.
Step 3: Complete the vertical model
Why: A free-body account must include every external force, even those not needed numerically.
Working: Weight = 0.60g downward and normal contact = 0.60g upward.
Answer: Static friction is 4.0 N left. Weight and normal contact are equal and opposite vertically; spring force and friction are equal and opposite horizontally.
Check: Both component resultants are zero, consistent with the block remaining at rest.
Now try it with support
Practise with support
A 2.0 N force extends a spring by 4.0 cm. Find k and predict the extension for 3.0 N if the spring remains proportional.
Hints
- Convert 4.0 cm to metres.
- Use the same k only because proportional behaviour is stated.
View the guided answer
k = 2.0/0.040 = 50 N m⁻¹. For 3.0 N, x = 3.0/50 = 0.060 m = 6.0 cm.
Your turn
Practise independently
A 0.60 kg block rests on a rough horizontal table and is attached to a spring of force constant 80 N m⁻¹ stretched by 0.050 m. Draw the forces and find the friction needed for equilibrium.
Check your answer
The forces are weight 0.60g downward, normal contact upward, spring force kx = 80(0.050) = 4.0 N towards the spring, and static friction 4.0 N opposite the spring force. Vertical forces balance and the horizontal resultant is zero.
Common mistakes and exam guidance
Watch out for
- Drawing a continuing ‘push’ after an object has left the hand.
- Applying F = kx after the force–extension graph has stopped being linear.
In an exam
- A force label should include its type and, where useful, the agent.
- If the question asks for a free-body diagram, do not add velocity or acceleration arrows as forces.
Put the ideas together
Exam-style practice [6 marks]
For each situation, name the force and state its direction: (i) a positive charge in an eastward electric field; (ii) a current-carrying wire that experiences an upward magnetic force; (iii) a sphere falling through oil below terminal speed. For the sphere, explain how the forces change as speed rises.
Plan before you answer
- Identify the object responding to each field or contact interaction.
- Use the field definition or relative-motion rule for direction.
- For the sphere, connect rising speed to viscous force and resultant force.
View the marking points and model answer
Marking points
- Positive charge: electric force east.
- Wire: magnetic force upward as stated, acting on the current-carrying conductor.
- Sphere: weight downward.
- Sphere: viscous drag upward, opposing motion.
- Drag increases as speed rises while weight remains approximately constant.
- Downward resultant and acceleration decrease towards zero.
Model answer
The positive charge experiences electric force east, along the electric field. The wire experiences magnetic force upward. The falling sphere has weight downward and viscous drag upward. As its speed increases, drag increases while weight is nearly constant, so the downward resultant and acceleration decrease. At terminal speed the two forces become equal.
Finish from memory
Three-question recap
What interaction produces a normal force?
Check
Contact between a body and a surface.
When is F = kx valid?
Check
Within the region where force is proportional to extension or compression.
Does friction always oppose velocity?
Check
It opposes relative slipping or the tendency to slip at the contact, not necessarily the body’s overall velocity.
Continue with the next resource in this course.
Course and syllabus information
- Course
- GCE A-Level H1 Physics
- Edition
- GCE A-Level H1 Physics 2027