Calculating EMF Induced by Moving Rectangular Loop

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SUMMARY

The discussion centers on calculating the electromotive force (EMF) induced in a rectangular loop of wire moving away from a straight wire carrying a current of 2 amps. The relevant equations include the magnetic field formula B = μ0I/2πr and the EMF calculation EMF = -dΦ/dt. Participants clarify that while the area (A) of the loop remains constant, the magnetic field (B) decreases as the loop moves away from the wire. The preferred method for calculating EMF in this scenario is using the Blv law, which states that EMF = (B x l).v, where l is the length of the wire and v is the velocity of the loop.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically Faraday's law of induction
  • Familiarity with the Biot-Savart law for calculating magnetic fields
  • Knowledge of the Blv law for induced EMF in moving conductors
  • Basic proficiency in calculus for differentiating magnetic flux
NEXT STEPS
  • Study the application of Faraday's law in dynamic systems
  • Explore the Biot-Savart law for calculating magnetic fields around current-carrying wires
  • Learn about the implications of the Blv law in various electromagnetic scenarios
  • Investigate the effects of loop orientation on induced EMF calculations
USEFUL FOR

Physics students, electrical engineers, and anyone interested in understanding electromagnetic induction and its applications in moving conductors.

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Homework Statement



A rectangular loop of wire, of sides 5 and 3 cm moves away from a a long straight wire at 4ms-1 carrying a current of 2 amps. What is the EMF induced in the moving loop, when the near side of the loop is 3cm away from the wire?

Homework Equations



B = μ0I/2πr
EMF = -dΦ/dt

The Attempt at a Solution



EMF = -dΦ/dt = -dAB/dt where A is the area, and B is the field.

I am not sure what to do now as the answers I have seen treat A (the area) as changing?

As I see it the area of the loop (A) is constant, and B changes as the loop moves out along the radius (the field gets weaker). Can anyone clarify which is right?
 
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A stays the same.
What's unclear to me is which of the two (3 cm or 5 cm) sides is parallel to the current wire ...
 
You can also use the Blv law. That is actually preferred since for moving media emf = -dΦ/dt doesn't always hold.

The Blv law is emf = (B x l).v
or more generally
d(emf) = (B x dl).v
l = length of wire
v = velocity of wire
Apply the formula to both loop lengths (parallel to the wire) and subtract.
 

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