Confusion regarding line integrals

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SUMMARY

The discussion clarifies the difference between line integrals in two contexts: the force on a closed loop of current-carrying wire in a uniform magnetic field and the evaluation of an Amperian loop using Ampere's Law. The line integral for the current loop results in zero due to the cancellation of forces in various directions, while the Amperian loop integral yields a non-zero value because the magnetic field is tangent to the loop, allowing for constructive summation of the terms. Understanding these distinctions is crucial for applying calculus in electromagnetism.

PREREQUISITES
  • Basic understanding of line integrals in calculus
  • Familiarity with Ampere's Law
  • Knowledge of magnetic fields and their properties
  • Concept of closed loops in physics
NEXT STEPS
  • Study the application of Ampere's Law in various geometries
  • Explore the concept of magnetic fields and their interactions with current-carrying conductors
  • Learn about the principles of vector calculus as applied to electromagnetism
  • Investigate the physical interpretation of line integrals in different contexts
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Students of physics, electrical engineers, and anyone interested in understanding the principles of electromagnetism and line integrals.

rahularvind06
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Sorry if this is the wrong place to post this, but I wasn't sure where exactly to put it.
When we calculate the force on a closed loop of current-carrying wire in a uniform magnetic field,
We calculate the line integral of the loop to be 0.
However, when we evaluate the line integral for an Amperian loop while using Ampere's law, we integrate from 0 to 2π.
Why is there a difference? I'm not very advanced with calculus, so some intuition is all I request.
 
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I am not sure I understand what you are asking. Both line integrals are taken over closed loops, so if your variable of integration is some angle θ, then the limits of integration would be from 0 to 2π. The fact that the net force on a current loop in a uniform magnetic filed is zero is a different issue. Think of the integral as a sum. In the current loop case you are adding a whole bunch of elements ##d \vec{F}## that point in all sorts of directions so that their sum is zero regardless of the shape of the loop. In the Amperian loop case, you choose the loop so that the B-field is tangent to the loop in which case all the ##\vec{B}\cdot d\vec{\mathcal l}## terms add together to give a non-zero value.

I hope I answered your question.
 

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