Nusc
- 752
- 2
em
In a certain region, the magnetic field as a linear function of time is given by
[tex] B = Bo \frac{t}{/tau} z hat[/tex]
Bo and tau constants.
A)FInd a simple expression for the vector potential which will yield this field.
B)Assuming the scalar potential is a constant, find E from the above result for the vector potential. Check that your answer is consistent with the diff form of faradays law
[tex] \nabla^2 \mathbf{A} - \mu_0 \epsilon_0 \frac{\partial^2 \mathbf{A}}{\partial t^2} = -\mu_0 \mathbf{J}[/tex]
[tex] \mathbf{A} = \frac{\mu_0}{4 \pi} \int \frac{\mathbf{J}(\mathbf{rsingle-quote},t_r)}{\cal{R}} d\tausingle-quote[/tex]
[tex] t_r \equiv t - \frac{\cal{R}}{c}[/tex]
[tex] B= \nabla \times A [/tex]
We take the curl of B on the LHS and on the RHS we have
[tex] \nabla \times (\nabla \times A )[/tex]
Eventually we will get to this [tex] \nabla^2 \mathbf{A} - \mu_0 \epsilon_0 \frac{\partial^2 \mathbf{A}}{\partial t^2} = -\mu_0 \mathbf{J}[/tex]This is assuming were in the Lorentz Gauge, we don't know if we are. Or do we assume we are? We have to satisfy E = -delV -dA/dt but we don't know either of those quantities.
Homework Statement
In a certain region, the magnetic field as a linear function of time is given by
[tex] B = Bo \frac{t}{/tau} z hat[/tex]
Bo and tau constants.
A)FInd a simple expression for the vector potential which will yield this field.
B)Assuming the scalar potential is a constant, find E from the above result for the vector potential. Check that your answer is consistent with the diff form of faradays law
Homework Equations
[tex] \nabla^2 \mathbf{A} - \mu_0 \epsilon_0 \frac{\partial^2 \mathbf{A}}{\partial t^2} = -\mu_0 \mathbf{J}[/tex]
[tex] \mathbf{A} = \frac{\mu_0}{4 \pi} \int \frac{\mathbf{J}(\mathbf{rsingle-quote},t_r)}{\cal{R}} d\tausingle-quote[/tex]
[tex] t_r \equiv t - \frac{\cal{R}}{c}[/tex]
The Attempt at a Solution
[tex] B= \nabla \times A [/tex]
We take the curl of B on the LHS and on the RHS we have
[tex] \nabla \times (\nabla \times A )[/tex]
Eventually we will get to this [tex] \nabla^2 \mathbf{A} - \mu_0 \epsilon_0 \frac{\partial^2 \mathbf{A}}{\partial t^2} = -\mu_0 \mathbf{J}[/tex]This is assuming were in the Lorentz Gauge, we don't know if we are. Or do we assume we are? We have to satisfy E = -delV -dA/dt but we don't know either of those quantities.