Solenoid & Energy: Solenoid Dynamics & Power Flow

In summary, the conversation discusses the use of Ampere's and Faraday's laws to calculate the magnetic field and energy in a solenoid. The Poynting vector is used to determine the power flowing out of the solenoid, and it is shown that the rate of change of magnetic field energy is equal to the negative of the surface integral of the Poynting vector. This leads to the conclusion that there is no electromagnetic radiation present in this scenario. The conversation also discusses the energy continuity equation and how it relates to the Poynting vector and magnetic field energy. Ultimately, it is concluded that considering the Poynting vector alone is sufficient for conservation of energy, as it includes the necessary terms.
  • #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?
 
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  • #2
If we consider the surface of the solenoid, the Poynting vector is directed inwards - this represents the transfer of energy to the magnetic field.

Hence, it is no coincidence that the rate of change of magnetic field energy is equal to the negative of the surface integral of the Poynting vector.

If the consider a surface just outside the (infinite) solenoid, H = 0, and hence the Poynting vector is 0. Ie. There is no electromagnetic radiation whatsoever to consider.

Hence,
[itex]
\int \vec{N}.\vec{dS} = -\pi \mu n^2 l (I_0)^2 r^2 t
[/itex] represents the same thing as [itex] \pi \mu n^2 l (I_0)^2 r^2 t = \frac{dU}{dt}
[/itex], which is equal to [itex]
- \xi I = \pi \mu n^2 r^2 l (I_0)^2 t = \frac{dW}{dt}
[/itex].

It is not necessary to add both the surface integral and magnetic field energy terms together.

On the other hand, if there was electromagnetic radiation, considering the Poynting vector alone would give the right answer for conservation of energy, as the Energy Flux integral would necessarily include the [itex]
\frac{dU}{dt}
[/itex] term.

I hope this answers the question.
 
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FAQ: Solenoid & Energy: Solenoid Dynamics & Power Flow

What is a solenoid?

A solenoid is a coil of wire that is tightly wound into a cylindrical shape. It is usually made of copper or aluminum and is used to create a magnetic field when an electric current is passed through it.

How does a solenoid work?

When an electric current is passed through the coil, it creates a magnetic field. The strength of the magnetic field depends on the number of turns in the coil, the current passing through it, and the material of the core. The magnetic field produced by the solenoid can be used to attract or repel other magnetic materials.

What is the purpose of a solenoid?

Solenoids have a variety of uses in various industries. They are commonly used in electromechanical devices such as valves, switches, and relays. They can also be used in electric motors, generators, and transformers.

How is energy transferred in a solenoid?

Energy is transferred in a solenoid through the magnetic field that is created when an electric current flows through the coil. This magnetic field can interact with other magnetic materials and transfer energy to them, causing them to move or perform work.

How can the power flow in a solenoid be controlled?

The power flow in a solenoid can be controlled by varying the current passing through the coil, changing the number of turns in the coil, or using a different material for the core. Additionally, the direction of the current can also be changed to control the power flow in a solenoid.

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