Direction of Magnetic Field for a Charged Rotating Disc

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SUMMARY

The discussion focuses on determining the direction of the magnetic field generated by a charged rotating disc. The key equation used is the curl of the electric field, expressed as \nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}. The magnetic field exhibits two components, \hat{r} and \hat{\theta}, which are dependent on the measurement location, particularly along the z-axis. The field lines resemble those of a circular loop of current, indicating that the disc can be conceptualized as a collection of thin circular loops.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically Maxwell's equations.
  • Familiarity with vector calculus, particularly curl operations.
  • Knowledge of magnetic field concepts related to charged rotating bodies.
  • Basic principles of electric fields and their relationship to magnetic fields.
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  • Study the application of Maxwell's equations in dynamic systems.
  • Learn about the Biot-Savart Law and its relation to magnetic fields from current loops.
  • Explore the concept of magnetic field lines and their visualization in three dimensions.
  • Investigate the effects of charge distribution on magnetic field generation in rotating systems.
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Students and professionals in physics, particularly those specializing in electromagnetism, electrical engineers, and anyone studying the behavior of magnetic fields in rotating systems.

Rahmuss
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Homework Statement


The question actually asks for the equation for the magnetic field for the rotating disc; but all I'm after is the direction of the magnetic field.


Homework Equations


None were given; but I've been using:
\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}


The Attempt at a Solution


When I use the above equation I get two components to the magnetic field: \hat{r} and \hat{\theta}. That doesn't really make a lot of sense to me. What am I missing?
 
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The cross product will give you the direction.
 
Rahmuss said:

Homework Statement


The question actually asks for the equation for the magnetic field for the rotating disc; but all I'm after is the direction of the magnetic field.


Homework Equations


None were given; but I've been using:
\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}


The Attempt at a Solution


When I use the above equation I get two components to the magnetic field: \hat{r} and \hat{\theta}. That doesn't really make a lot of sense to me. What am I missing?

The direction of the field depends on where you are measuring it at. If you measure the field along the axis of the disk (presumably the z-axis--- where \theta=0), then the field should point along the axis (assuming the disk is uniformly charged). It may help you to note that \hat{z}=\cos\theta\hat{r}-\sin\theta\hat{\theta}=\hat{r} along the z-axis.
 
what - Thanks. And that part I understand just fine. There is only a z-component of the electric field, so when I do a cross product, I get both an r-component and a theta-component.

gabbagabbahey - So the way you're describing it, the magnetic field seems to come up at the center of the disk, and then moves out and around to the bottom circling back up along the z-axis again?
 
Rahmuss said:
gabbagabbahey - So the way you're describing it, the magnetic field seems to come up at the center of the disk, and then moves out and around to the bottom circling back up along the z-axis again?

Yes, the field lines are very similar to those of a circular loop of current. After all, the disk can be thought of as a superposition of a very large number of thin circular loops of various radii.
 

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