- #1
Nusc
- 760
- 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.