Calculating Magnetic Field in a Square with Varying Resistances

Click For Summary

Homework Help Overview

The problem involves calculating the magnetic field at the center of a square with sides of varying resistances when a potential difference is applied between specific points. The subject area includes concepts from electromagnetism and circuit analysis.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the equivalent resistance and current distribution in the circuit. Questions arise regarding the appropriate application of Ampere's law and whether the symmetry of the magnetic field allows for its use. There is also consideration of using Biot-Savart's law and its applicability in the context of a variable electric field.

Discussion Status

The discussion is active, with participants exploring different laws to apply for calculating the magnetic field. Some guidance has been offered regarding the use of Biot-Savart's law, and there is acknowledgment of the limitations posed by variable electric fields.

Contextual Notes

Participants are navigating the complexities of applying electromagnetic laws in a scenario with non-uniform resistances and potential changes in electric fields. There is an indication of uncertainty regarding the assumptions necessary for the application of these laws.

arpon
Messages
234
Reaction score
16

Homework Statement


Untitled2.png
[/B]
Consider a square whose successive sides of length [itex]L[/itex] has resistances [itex]R, 2R, 2R, R[/itex] respectively. If a potential difference [itex]V[/itex] is applied between the points (call them , say , A and B) where the sides with R and 2R meet. Find the magnetic field [itex]B[/itex] at the center of the square.

Homework Equations


[itex]R_s = R_1 + R_2 + R_3 + ... + R_n[/itex]
[itex]\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + ... + \frac{1}{R_n}[/itex]
[itex]V = iR[/itex]
[itex]\oint \vec B \cdot d \vec s = \mu _0 i[/itex]

The Attempt at a Solution


The equivalent resistance of this combination is [itex]\frac{4R}{3}[/itex] . So, the current through [itex]R , 2R[/itex] are [itex]\frac{V}{2R} , \frac{V}{4R}[/itex] respectively. But, to calculate the magnetic field, what will be the amperian loop to imagine?
 
Physics news on Phys.org
Does the magnetic field pattern have enough symmetry to use Ampere's law? If not, can you think of a different law that you can use?
 
So, I should use Biot-Savart's law. But another question, can I use Biot-Savart's Law in case of variable electric field?
 
Last edited by a moderator:
  • Like
Likes   Reactions: arpon
arpon said:
So, I should use Biot-Savart's law.

Yes.
 

Similar threads

Replies
6
Views
1K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
Replies
2
Views
1K
Replies
11
Views
2K
Replies
8
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
Replies
12
Views
2K
Replies
4
Views
2K
  • · Replies 17 ·
Replies
17
Views
2K