How Does the Biot-Savart Law Apply to a Wire Shaped in Two Half Circles?

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Homework Help Overview

The problem involves a wire shaped into two half circles connected by straight sections, with a current flowing through it. Participants are tasked with determining the magnetic field at the center of the configuration and the magnetic dipole moment of the circuit using the Biot-Savart Law.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the Biot-Savart Law and its implications for calculating the magnetic field from the two half circles. There are attempts to derive the magnetic field contributions from each section of the wire, with some participants questioning how to combine these contributions. Others inquire about the magnetic field of a circular loop as a reference point.

Discussion Status

The discussion is ongoing, with various approaches being explored. Some participants have provided equations and insights into the contributions of the half circles, while others are clarifying the setup and assumptions involved in the calculations. There is no explicit consensus yet on the final expression for the magnetic field.

Contextual Notes

Participants are working under the constraints of applying the Biot-Savart Law and considering the geometry of the wire. There is a focus on the contributions from different sections of the wire, and some assumptions about the behavior of the magnetic field in relation to the straight sections are being discussed.

Kyousik
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Homework Statement


"A wire is formed into the shape of two half circles connected by equal-length straight sections. A current I flows in the circuit clockwise as shown. Determine (a) The magnitude and the direction of the magnetic field at the center, C, and (b) the magnetic dipole moment of the circuit"

http://img225.imageshack.us/img225/4218/untitled1mm6.jpg

Homework Equations


Biot-Savart Law -> dB = (Mu * I * dL) / (4 * Pi * R^2)

The Attempt at a Solution


The answer is

( Mu * I * [R1 + R2] )/ (4 * R1 * R2)

Not sure how they get it, I'm seeing it as two half circles and you minus them from each other.

B = ( Mu * I * [2 * Pi * R1 / 2] ) / (4 * Pi * R1^2)
B1 = (Mu * I) / (2 * R1)

B2 = (Mu * I) / (2 * R2)

Bt = B1 + B2 ?
 
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Hello,

Do you know the magnetic field in the center of a circle loop with radius a and current i ?


Regards
 
B = (Mu * I) / (2 * Pi * a); where R = a; I = Ienclosed.
 
What i know is
[tex]B=\frac{\mu_0I}{2a}[/tex]

The magnetic field in the question is the superposition of contributions of two half-circle loops.


Best regards
 
This question uses the Biot-Savart Law:

[tex]B = \frac{\mu_0 I}{4\pi}\int \frac{d\vec{l} \times \hat{r}}{r^2}[/tex]

In this case, use cylindrical co-ordinates to find your field for the two radii. For the straight parts, the current is parallel to the r-hat vector, and as such the B-field is zero on those sections. For the two radii:

[tex]dl = rd\phi \hat{\phi}; \hat{r} = \hat{s}[/tex]

Use the cross product and integrate over the angle to get your expression. Do this for the two different radii and add together to give your final magnetic field.
 

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