Animated Solution for Physics - Magnetic Effects of Current: Two thin long parallel wires separated by a distance b are carrying a current i ampere each. The magnitude of the force per unit length exerted by one wire on the other is
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Visualized Solution
Setup&Variables
Two parallel wires carrying current i
Separation distance =b
MagneticField(B1)
B1=2πbμ0i
MagneticForce(F)
F=iLB1sin(90∘)
ForceperUnitLength
LF=iB1
Substitution
LF=i(2πbμ0i)
FinalAnswer
LF=2πbμ0i2
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The Sigma Insight: Magnetic Force on Current
Solution Diagram
The interaction between two parallel current-carrying wires is a classic and fundamental concept in electromagnetism. It beautifully bridges two core ideas: how a current creates a magnetic field, and how a magnetic field exerts a force on a moving charge (or current).
Analyzing the Setup
Imagine two infinitely long, thin, parallel wires separated by a distance b. Both wires are carrying an identical current i. We want to find the force per unit length that one wire exerts on the other.
To solve this, we break the problem into two logical steps. First, we calculate the magnetic field produced by one wire at the location of the second wire. Then, we calculate the force that this magnetic field exerts on the second wire.
The Magnetic Field
Let's focus on the first wire. According to Ampere's Law, a long straight wire carrying a current i generates a magnetic field around it. At a perpendicular distance b from the wire, the magnitude of this magnetic field B1 is given by:
B1=2πbμ0i
Using the right-hand grip rule, if we point our thumb in the direction of the current in the first wire, our fingers curl in the direction of the magnetic field. At the position of the second wire, this magnetic field points perpendicularly into (or out of, depending on the relative orientation) the plane containing the two wires.
The Lorentz Force
Now, consider the second wire. It is carrying a current i and is immersed in the external magnetic field B1 created by the first wire. The magnetic force F on a straight segment of wire of length L carrying current i in a uniform magnetic field B is given by the Lorentz force equation for currents:
F=i(L×B)
Since the second wire is parallel to the first wire, it is perpendicular to the magnetic field B1 (which forms concentric circles around the first wire). Therefore, the angle between L and B1 is 90∘, and sin(90∘)=1. The magnitude of the force is simply:
F=iLB1
Final Calculation
The question asks for the force per unit length, which is LF. Rearranging our force equation gives:
LF=iB1
Now, we substitute the expression for B1 that we derived earlier:
LF=i(2πbμ0i)
Multiplying the terms together, we arrive at our final, elegant result:
LF=2πbμ0i2
This tells us that the force per unit length is directly proportional to the square of the current and inversely proportional to the distance between the wires. If the currents are in the same direction, the force is attractive; if they are in opposite directions, the force is repulsive. In this problem, we only needed the magnitude, which perfectly matches option (b).