- #1
rabbit44
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Hi, this isn't an actual question, but is a confusion inspired by a question I did (hence me not using the template). I'm having trouble with this example. I'm talking about a solenoid (with core, but doesn't really matter), with n turns per unit length, and a current [itex]I_0 t[/itex] going in. [itex] \vec{z}[/itex] is along the axis of the solenoid, and the current is along [itex]\vec{\theta}[/itex].
Using Ampere we get:
[itex]H=In\hat{z}[/itex]
[itex]B=\mu In \hat{z}[/itex]
Using Faraday we get:
[itex]E=-0.5\mu n I_0 r \hat{\theta}[/itex]
the Poynting Vector is:
[itex]\vec{E} \times \vec{H}[/itex]
Integrating over the surface of some volume inside the solenoid to find the power flowing out, we get:
[itex]\int \vec{N}.\vec{dS} = -\pi \mu n^2 l (I_0)^2 r^2 t[/itex]
Also, the rate of change of energy stored in the magnetic field comes out as:
[itex]\pi \mu n^2 l (I_0)^2 r^2 t = \frac{dU}{dt}[/itex]
Also, work done against field (for that volume):
[itex] - \xi I = \pi \mu n^2 r^2 l (I_0)^2 t = \frac{dW}{dt} [/itex]
These three things don't seem to match up to the energy continuity equation - what am I thinking wrong?
Using Ampere we get:
[itex]H=In\hat{z}[/itex]
[itex]B=\mu In \hat{z}[/itex]
Using Faraday we get:
[itex]E=-0.5\mu n I_0 r \hat{\theta}[/itex]
the Poynting Vector is:
[itex]\vec{E} \times \vec{H}[/itex]
Integrating over the surface of some volume inside the solenoid to find the power flowing out, we get:
[itex]\int \vec{N}.\vec{dS} = -\pi \mu n^2 l (I_0)^2 r^2 t[/itex]
Also, the rate of change of energy stored in the magnetic field comes out as:
[itex]\pi \mu n^2 l (I_0)^2 r^2 t = \frac{dU}{dt}[/itex]
Also, work done against field (for that volume):
[itex] - \xi I = \pi \mu n^2 r^2 l (I_0)^2 t = \frac{dW}{dt} [/itex]
These three things don't seem to match up to the energy continuity equation - what am I thinking wrong?