How Should Voltage Across an Inductor Be Treated in Circuit Analysis?

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Homework Help Overview

The discussion revolves around the treatment of voltage across an inductor in a circuit analysis context, specifically involving a series circuit with a battery and resistor. Participants are exploring the implications of Kirchhoff's loop law and the behavior of inductors in both charging and discharging scenarios.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants are questioning whether to consider the potential across the inductor as positive or negative, particularly in relation to the opposing emf of the battery. There is also discussion about the implications of initial conditions in the circuit and the role of induced emf in the inductor.

Discussion Status

Some participants have offered guidance on applying Kirchhoff's laws and the nature of induced emf in inductors. There is an ongoing exploration of the reasoning behind the sign of the voltage across the inductor, with various interpretations being discussed.

Contextual Notes

There is mention of the need for clarity regarding the treatment of voltage in discharging LR circuits, as well as the foundational principles of electrodynamics that govern the behavior of inductors.

cupid.callin
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Homework Statement


suppose there is a inductor connected to a battery and resistor in series ...

i need to find the current in circuit at some time t
i suppose i could use Kirchhoff's loop law but i don't know weather to take potential across inductor (L di/dt) as positive or negative.
i suppose i should use it as negative because it is opposing the emf of battery but i am not sure

but this thing will not work in case of discharging LR circuit ... some help please ... ... ... ...
 
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cupid.callin said:

Homework Statement


suppose there is a inductor connected to a battery and resistor in series ...

i need to find the current in circuit at some time t
i suppose i could use Kirchhoff's loop law but i don't know weather to take potential across inductor (L di/dt) as positive or negative.
i suppose i should use it as negative because it is opposing the emf of battery but i am not sure

but this thing will not work in case of discharging LR circuit ... some help please ... ... ... ...
You can figure this out. :smile:

Suppose there is no initial current. In other words, suppose the circuit is such that at time t = 0, the circuit is closed and i0 = 0 (at that instant in time).

Now sum the voltages all the way around in a loop. You'll have to calculate the voltage drop across R, but that should be pretty easy since at this instant in time, i = 0. Then note that the sum of all the voltage drops, all the way around the loop should equal zero, per one of Kirchhoff's laws.

So what polarity does the voltage across the inductor have to be to insure that Kirchhoff's law(s) are satisfied?
 
cupid.callin said:
i don't know weather to take potential across inductor (L di/dt) as positive or negative.
i suppose i should use it as negative because it is opposing the emf of battery but i am not sure



The potential refers to a point. Potential difference is "across".
In an inductor, an is emf induced due to changing current. It is -L dI/dt. You can consider it as an additional voltage source that has opposite sign as that of the "real" source.

ehild
 
collinsmark said:
You can figure this out. :smile:

Suppose there is no initial current. In other words, suppose the circuit is such that at time t = 0, the circuit is closed and i0 = 0 (at that instant in time).

Now sum the voltages all the way around in a loop. You'll have to calculate the voltage drop across R, but that should be pretty easy since at this instant in time, i = 0. Then note that the sum of all the voltage drops, all the way around the loop should equal zero, per one of Kirchhoff's laws.

So what polarity does the voltage across the inductor have to be to insure that Kirchhoff's law(s) are satisfied?

ehild said:
The potential refers to a point. Potential difference is "across".
In an inductor, an is emf induced due to changing current. It is -L dI/dt. You can consider it as an additional voltage source that has opposite sign as that of the "real" source.

ehild

i can do this to find the sign but i need the reason that why is sign like that ...

and sorry for late reply ...
 
It is the consequence of Maxwell's laws. They are the fundamental laws of electrodynamics, based on experimental facts. You cannot ask, why.

ehild
 
why not ... everything in physics has a reason ,,, weather we know it or not
 
Well, you can think that in case the opposite were true, and positive electromotive force were induced by a changing current, the induced emf would rise the current even more in a circuit and the circuit would blow away. If such law existed in the history of the universe in some world, that world would not have been stable and can not exist now.

ehild
 

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