Direction of Magnetic Field for a Charged Rotating Disc

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Homework Help Overview

The discussion centers on determining the direction of the magnetic field generated by a charged rotating disc. Participants are exploring the relationship between the electric field and magnetic field in this context.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the use of the curl of the electric field to derive components of the magnetic field, questioning the meaning of the resulting radial and angular components. There is also a consideration of how the magnetic field direction varies based on measurement location, particularly along the axis of the disc.

Discussion Status

Some participants have provided insights into the relationship between the electric and magnetic fields, suggesting that the magnetic field behaves similarly to that of a circular loop of current. However, there is no explicit consensus on the interpretation of the components or the overall direction of the magnetic field.

Contextual Notes

Participants are working under the assumption that the disc is uniformly charged and are considering the implications of this on the magnetic field's direction. There is an acknowledgment of the complexity involved in visualizing the field lines and their behavior around the disc.

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:
[tex]\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}[/tex]


The Attempt at a Solution


When I use the above equation I get two components to the magnetic field: [tex]\hat{r}[/tex] and [tex]\hat{\theta}[/tex]. 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:
[tex]\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}[/tex]


The Attempt at a Solution


When I use the above equation I get two components to the magnetic field: [tex]\hat{r}[/tex] and [tex]\hat{\theta}[/tex]. 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 [itex]\theta=0[/itex]), then the field should point along the axis (assuming the disk is uniformly charged). It may help you to note that [itex]\hat{z}=\cos\theta\hat{r}-\sin\theta\hat{\theta}=\hat{r}[/itex] 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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