Is the Work Done in Charging an Inductor Different in Non-Quasistatic Scenarios?

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The work done in charging an inductor is typically calculated using the quasistatic approximation, resulting in the formula W = 1/2LI². In non-quasistatic scenarios, such as when current changes rapidly, the work done may exceed this value due to energy losses from radiation. However, if the charging process is extremely slow, approaching an infinite time T, the work done will converge to 1/2LI². The discussion also highlights that while LC circuits are often described as lossless, they do experience some energy losses, both resistive and radiative, which are quantified by the quality factor Q. Ultimately, the presence of DC versus AC current influences the potential for electromagnetic radiation during the charging process.
mayank pathak
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As we know, work done by an outside agency in creating some current ''I" in an inductor 'L' is 1/2LI2. Now this result is derived by quasistatic approximation if I am not wrong. Now, I am assuming that in non quasistatic (real) scenarios, the work done by outside agency would be different(If you actually calculate by using Poynting Vector, there would be some radiation flying off ...). Am I right till here ?

My question is :Let W be the work done in charging inductor to current I in time T (at a rate of I/T amperes per second) without making qusi static approximations. Is W > 1/2LI2 ? Also, if T approaches infinity (i.e. the rate of increasing current is too darned slow), will W approach 1/2LI2 ?

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To help answer your question ## L=\frac{\Phi}{I} ## , and for a long cylinder ## B=n \mu_o I ##. The result is with ## E=(1/2)LI^2 ## and with ## \Phi=nL( BA) ## that ## E=(1/2) \frac{B^2}{\mu_o} V ##. This assumes nothing gets radiated away=otherwise, yes, there is power that is lost and not described by these basic equations. It is still correct that ## E=(1/2) LI^2 ##. That part of the energy is recoverable.
 
Charles Link said:
To help answer your question ## L=\frac{\Phi}{I} ## , and for a long cylinder ## B=n \mu_o I ##. The result is with ## E=(1/2)LI^2 ## and with ## \Phi=nL( BA) ## that ## E=(1/2) \frac{B^2}{\mu_o} V ##. This assumes nothing gets radiated away=otherwise, yes, there is power that is lost and not described by these basic equations. It is still correct that ## E=(1/2) LI^2 ##. That part of the energy is recoverable.

Yes. Thanks. I think I get it now.

Also, is my assumption about super-slow process true(will W= 1/2LI^2 in that limiting case where T approaches infinity)
 
mayank pathak said:
Also, is my assumption about super-slow process true(will W= 1/2LI^2 in that limiting case where T approaches infinity)
Yes
 
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Khashishi said:
Yes
One more question : then how can an lossless LC circuit exist ? It should lose energy by means of radiation since current in the circuit is definitely greater than zero(hence quasistatic approximation certainly doesnot hold)
 
mayank pathak said:
One more question : then how can an lossless LC circuit exist ? It should lose energy by means of radiation since current in the circuit is definitely greater than zero(hence quasistatic approximation certainly doesnot hold)
I don't know that anyone ever said that an LC circuit is completely lossless. Normally, LC circuits come with a quality factor ## Q ##, and the higher the ## Q ##, the smaller the losses. The losses can be both resistive and radiative, and it can be somewhat difficult to determine how much is resistive and how much is radiative.
 
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Charles Link said:
I don't know that anyone ever said that an LC circuit is completely lossless. Normally, LC circuits come with a quality factor ## Q ##, and the higher the ## Q ##, the smaller the losses. The losses can be both resistive and radiative, and it can be somewhat difficult to determine how much is resistive and how much is radiative.

Thanks. "Lossless" word stuck with me and I guess I never cared so deeply about these questions until now. Maxwell equations has certainly enlightened me. I almost see the whole picture now. Thanks again :)
 
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mayank pathak said:
Thanks. "Lossless" word stuck with me and I guess I never cared so deeply about these questions until now. Maxwell equations has certainly enlightened me. I almost see the whole picture now. Thanks again :)
It sounds as if you are charging the inductor from a DC source such as a battery.
Any EM wave radiated would then have to be unidirectional. The usual view is that this is not possible.
So it looks as if the radiated energy may be zero for this case.
 
tech99 said:
It sounds as if you are charging the inductor from a DC source such as a battery.
Any EM wave radiated would then have to be unidirectional. The usual view is that this is not possible.
So it looks as if the radiated energy may be zero for this case.

I didn't understand. Can you elaborate more ?
 
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mayank pathak said:
I didn't understand. Can you elaborate more ?
In order to obtain EM radiation, we require an alternating current. You are using a DC supply so there is no alternating current.
If the inductor is connected to AC, then there will be some radiated energy, depending on the dimensions and the size of the current.
 
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