Ampere's Law on Current Carrying Loop

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SUMMARY

The discussion centers on the application of Ampere's Law to derive the magnetic field density (B) for a current-carrying loop. While Ampere's Law yields the formula B = μI / (2πr), the Biot-Savart Law provides a different result, B = μI / (2r). The inconsistency arises because, unlike a long straight wire where B is constant along the Amperian loop, the magnetic field around a current-carrying ring varies, making Ampere's Law less practical in this scenario. Consequently, the Biot-Savart Law is preferred for calculating magnetic fields in more complex geometries.

PREREQUISITES
  • Understanding of Ampere's Law and its mathematical formulation
  • Familiarity with the Biot-Savart Law and its application
  • Basic knowledge of magnetic field concepts and units
  • Geometry of magnetic fields around current-carrying conductors
NEXT STEPS
  • Study the derivation of Ampere's Law and its limitations in various geometries
  • Explore the Biot-Savart Law in detail, including its derivation and applications
  • Investigate the concept of magnetic field lines and their behavior around different current configurations
  • Learn about advanced topics such as magnetic field simulations using software tools
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Physics students, electrical engineers, and anyone interested in electromagnetism and the behavior of magnetic fields in various configurations.

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I haven't seen anyone derive the magnetic field density (B) using ampere's law, only using Biot-Savart Law
any reason why?

if we cut the loop and loop at one end (of the new cut) and treat it as if it was a current carrying wire, then by ampere's law we'd get:

B = u*I / 2*pi*r

but however by the Biot-Savart Law we actually get

B = u*I / 2*r

anyone know why?
 
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Ampere's law tells you that (line integral of B.dl along the loop) = μ0 * (flux of I through the loop). If you know from the geometry of the situation that B is constant along the loop, then calculating the line integral of B along the loop is easy. This is the case with a long straight wire. Here we draw a loop at a distance R from the wire. We know from symmetry that the value of B is everywhere constant along the loop, so the line integral of B along the loop is just 2*pi*R*B. In the case of a current carrying ring, no matter how you draw your Amperian loop, there is no way to draw it so that B is constant. So, while Ampere's law still holds, it is not very useful, since you don't know how to calculate the line integral. So you use the Biot-Savart law, which is more amenable to a general situation.
 

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