Understanding Magnetic Induction Field B on Circular Coil Axis

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Homework Help Overview

The discussion revolves around understanding the magnetic induction field B on the axis of a circular coil, specifically addressing the relationship between the differential length element (dl) and the position vector (r) in the context of the Biot-Savart law.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster questions the relationship between angles in the context of the cross product, specifically why (dlxr) becomes dlrsin(alpha) and whether alpha is indeed the correct angle to use.

Discussion Status

Participants are exploring the definitions and relationships of angles in the problem, with some suggesting clarifications on notation and others defending the use of the angle alpha. There is an ongoing examination of the assumptions regarding the geometry involved.

Contextual Notes

There is a mention of potential confusion arising from the use of variable names and notation, which may impact the clarity of the discussion. The reference to the Biot-Savart law indicates the theoretical framework being applied.

retupmoc
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Just a quick question about finding the magnetic induction field B on the axis of a circular coil shown on page 7 on http://www.physics.gla.ac.uk/~dland/ELMAG305/Elmag305txt5.pdf
I understand why the field must be along the x-axis but why does (dlxr )x become dlrsin(alpha)? alpha doesn't seem to be the angle between the dl and r, dlxr would equal |dl|| r |sin(x) where x would be the angle between the dl and r. My problem is x and alpha don't seem to be the same angle so i don't know how to advance with this problem. Any help?
 
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You can't denote the angle with "x",one of the axis with "Ox" and the sign for a vector/cross product with "x"...Let the angle be "alpha",the axis "Ox" and the sign [tex]\times[/tex].

Daniel.
 
I don't see why alpha wouldn't be that angle. What angle are you suggesting?

A is the radius of the circle, and r is the line drawn from the center of the loop at a distance x_i away. You are integrating I along every dl, during which the radius A rides along its resident circle once.
 
Oh,and it should be Biot-Savart-Laplace law...Laplace was the mathematician who made the formula up,while the other guys fooled around with magnets.

The same story with Stefan-Boltzmann law...Boltzmann was the theorist,and Stefan the experimentalist.

Daniel.
 

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