Forces between parallel currents
Key idea: Parallel currents in the same direction attract; opposite currents repel. Each wire feels the other's field, with equal and opposite forces proportional to I₁I₂ and inversely to separation.
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Guided lessons · coming soon
Guided lesson
Guided steps
- Predict the directions and compare the forces on the two wires.
- Find the neighbour’s field direction, then the force direction.
- Find the field at the wire, then calculate the force.
- Explain why neither wire has zero force.
- Follow the field calculation and the force calculation.
- Find the force after reversing one current and doubling separation.
- Find and compare the forces with unequal currents.
- Draw the arrows and explain how doubling one current changes them.
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ContinueTwo wires carrying currents side by side pull together or push apart, even with no magnet nearby. Each wire sits in the magnetic field of the other, so each feels a force. Putting together the field of a straight wire and the force on a current explains the direction of these forces and how big they are.
Check your understanding 1 Before drawing the forces
Two long parallel wires carry currents in the same direction, one twice as large as the other. Predict whether the wires attract or repel, and compare the force magnitudes on equal lengths of the wires.
Show answer
The wires attract. Their force magnitudes are equal on equal lengths, even though the currents differ. Work through the field directions below to see why the force points towards the other wire.
Why parallel currents attract or repel
To find the force on one wire, find the field that the other wire produces where it is, then apply Fleming’s left-hand rule to its own current. For this interaction, use the neighbour’s field as the external field acting on the wire.
Take two long parallel wires, both carrying current out of the page, with wire 1 on the left. By the right-hand grip rule, wire 1’s field circles anticlockwise, so at wire 2 it points up the page. With the current in wire 2 out of the page and the field up, Fleming’s left-hand rule gives a force on wire 2 to the left, towards wire 1. Repeating this for wire 1 in the field of wire 2 gives a force to the right. The wires attract.
- Currents in the same direction attract.
- Currents in opposite directions repel.
The two forces are a Newton’s third law pair: equal in size and opposite in direction, even when the currents are different. Note that the rule is the opposite of the one for electric charges, where like charges repel.
Check your understanding 2 Which field, and where?
Two long wires 0.080 m apart each carry 4.0 A in the same direction. Their resultant field at the midpoint is zero. A student concludes that they exert no force on one another. Find the field that one wire produces at the other, then calculate the force magnitude on a 0.50 m length of each wire.
Show the steps Optional working
Show answer
Each wire experiences its neighbour’s non-zero field at the wire, not the resultant field at the midpoint. That field is B = (4π × 10⁻⁷)(4.0)/(2π × 0.080) = 1.0 × 10⁻⁵ T. Each wire feels F = BIl = (1.0 × 10⁻⁵)(4.0)(0.50) = 2.0 × 10⁻⁵ N towards the other wire. The equal and opposite forces act on different wires and do not cancel on either one.
Check your understanding 3 Why zero at the midpoint is not enough
For those two wires, explain why zero resultant field at the midpoint does not make the force on either wire zero. Explain also why the equal and opposite forces do not cancel on either wire.
Show answer
Check that you identify where the field is needed and which body each force acts on. Each wire lies in its neighbour’s non-zero field at the full separation d, not in the zero field at the midpoint. The magnetic forces point towards each other but act on different wires. They cancel when both wires are included in one system; they do not cancel on either wire separately.
The size of the force
At a distance d, the field of wire 1 is B₁ = μ₀I₁/(2π d), at right angles to wire 2. So the force on a length l of wire 2 is F = B₁I₂l, and the force per unit length is
Swapping the labels gives the same expression for the force on wire 1, which is why the forces are equal: both contain the product I₁I₂.
Worked example 1
Two equal currents
Problem
Two long parallel wires 0.050 m apart each carry 6.0 A in the same direction. Find the force on a 0.20 m length of either wire.
Show full solution
Field of one wire at the other
Method
Use B = μ₀I/(2π d) at the position of the other wire.Reason
The force on a wire comes from its neighbour’s field, not its own.Working
Answer
B₁ = ((4π × 10⁻⁷)(6.0))/2π(0.050) = 2.4 × 10⁻⁵ T
Force
Working
Answer
F = B₁I₂l = (2.4 × 10⁻⁵)(6.0)(0.20) = 2.9 × 10⁻⁵ N, towards the other wire
Quick check
The currents are in the same direction, so the force is an attraction. It is tiny: everyday currents need very long wires or very small gaps before the force matters.
Guided practice 2
Wider apart, one current reversed
Problem
Two parallel wires attract each other with a force of 1.2 × 10⁻⁴ N per metre. The separation is doubled and one of the currents is reversed, keeping its size. Find the new force per metre, and say whether the wires now attract or repel.
Find the new force per metre
Hints
Hint 1
size and direction separately
Which change affects the field strength, and which changes its direction?
Show full solution
New force
Working
Answer
Doubling d halves the force per metre to 6.0 × 10⁻⁵ N m⁻¹. With one current reversed, the currents are opposite, so the wires repel.
Try it yourself 3
Unequal currents
Problem
Two long parallel wires 0.040 m apart carry currents of 8.0 A and 2.0 A in opposite directions. Find the force per metre on the wire carrying 2.0 A, state its direction relative to the other wire, and compare its magnitude with the force per metre on the other wire.
Find and compare the forces
Show the steps Optional working
Hints
Hint 1
which field
Find the field acting on each wire: which current produces it?
Show solution step by step
Force on the 2.0 A wire
Reason
It is in the field of the 8.0 A wire.Working
Answer
F/l = ((4π × 10⁻⁷)(8.0)(2.0))/2π(0.040) = 8.0 × 10⁻⁵ N m⁻¹, away from the other wire
Comparison
Working
Answer
The same. The 8.0 A wire sits in a field four times weaker, but carries four times the current, so the product I₁I₂ is unchanged.
Exam-style question 1
Opposite currents
Examination question
Two long parallel wires are seen end-on. Wire 1, on the left, carries a current into the page. Wire 2, on the right, carries a current out of the page.
(a) State the direction of the magnetic field of wire 1 at wire 2, and hence the direction of the force on wire 2. [2 marks]
(b) State the direction of the force on wire 1, and explain why it has the same size as the force on wire 2. [2 marks]
(c) The current in wire 1 is doubled. State the effect on the force on each wire. [1 mark]
Write your answer before viewing the mark scheme
Show solution step by step
(a) Field and force at wire 2
2 marksMethod
Use the grip rule for wire 1, then the left-hand rule for wire 2.Reason
The force on wire 2 comes from wire 1’s field at wire 2.Working
Answer
Wire 1’s field circles clockwise, so at wire 2 it points down the page. With current out of the page, the force on wire 2 is to the right, away from wire 1.
(b) Force on wire 1
2 marksReason
The forces are a third-law pair, and both equal μ₀I₁I₂l/(2π d).Working
Answer
To the left, away from wire 2: the wires repel, with forces of equal size.
(c) Doubling current 1
1 markWorking
Answer
Both forces double, because both depend on I₁I₂.
Self-mark with the mark scheme
Tick each mark point that your answer includes.
Tick each point only if your answer states it clearly.
Common mistakes
- Using the field at the midpoint, at d/2, instead of the field of one wire at the other.
- Applying the electrostatic rule: parallel currents in the same direction attract, not repel.
- Thinking the wire with the larger current feels the larger force.
- Adding the two forces on the two wires as if they acted on one object.
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Syllabus and review details
- GCE A-Level H2 Physics 2027 · 2027
Content Overview, PDF pages 9–10; Subject Content, PDF pages 11–30
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