Biot Savart Law with a surface current

Click For Summary
SUMMARY

The discussion focuses on applying the Biot-Savart Law to a rotating disc with a uniformly distributed charge Q and radius R. The surface current density K(x,y) is derived as K = Q(w × R) / (πR²). Participants explore the implications of this current density on the magnetic field at specific points, ultimately discovering that the application of the Biot-Savart Law yields a zero magnetic field under certain conditions. This conclusion prompts further examination of the calculations involved in determining the current density and magnetic field.

PREREQUISITES
  • Understanding of the Biot-Savart Law
  • Knowledge of angular momentum and its implications in electromagnetism
  • Familiarity with surface current density concepts
  • Basic calculus for modeling current loops
NEXT STEPS
  • Explore advanced applications of the Biot-Savart Law in different geometries
  • Study the effects of varying charge distributions on magnetic fields
  • Investigate the relationship between angular velocity and magnetic field generation
  • Learn about the implications of zero magnetic fields in practical scenarios
USEFUL FOR

Students and professionals in physics, particularly those studying electromagnetism and magnetic fields generated by rotating charged bodies.

OmarRod
Messages
3
Reaction score
0

Homework Statement


There is a disc with radius R which has a uniformly-distributed total charge Q, rotating with a constant angular velocity w.

(a) in a coordinate system arranged so that the disc lies in the xy plane with its center at the origin, and so that the angular momentum point in the positive z direction, the local current density can be written J(x,y,z) = K(x,y) d(z). determine the surface current K(x,y) in terms of Q, w, and R.

(b) using the Biot Savart law, determine the magnetic field at point r=sk, k is the vector direction. find the same for r=-sk.


Homework Equations


Biot Savart Law


The Attempt at a Solution



I obtained K= Q(w X R) / pi*R squared for part A, but I'm not sure how that's supposed to fit into the Biot Savart Law.
 
Physics news on Phys.org
Note that the velocity of the current is not equal for charges at R/2 as it is for charges at R (the angular velocity is the same, but the radii are different). Try modeling the solution as a sum of current loops of width dr, with approximately equal radius (and thus velocity)

This answer would then be the current, which can be modeled with the Biot-Savart law.

~Lyuokdea
 
Lyuokdea said:
Note that the velocity of the current is not equal for charges at R/2 as it is for charges at R (the angular velocity is the same, but the radii are different). Try modeling the solution as a sum of current loops of width dr, with approximately equal radius (and thus velocity)

This answer would then be the current, which can be modeled with the Biot-Savart law.

Ok, I've done this and after applying Biot Savart's Law, I get a zero magnetic field. This can't be right can it?
 
that doesn't sound right...what did you get for J, and how did you include this into the biot savart law?

~Lyuokdea
 
nevermind, i looked at it again and found my mistake. thanks!
 

Similar threads

  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 7 ·
Replies
7
Views
318
Replies
8
Views
1K
  • · Replies 6 ·
Replies
6
Views
3K
Replies
4
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 13 ·
Replies
13
Views
2K