Mutual Inductance between a coil and a long straight wire

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Homework Help Overview

The discussion revolves around the concept of mutual inductance between a coil and a long straight wire, specifically addressing the induced EMF and the role of self-inductance in the context of a differential equation that describes the system.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the assumptions regarding the dimensions of the coil and its proximity to the wire, questioning the necessity of considering self-inductance alongside mutual inductance. They discuss the formulation of the differential equation and the implications of the terms involved.

Discussion Status

The discussion is active, with participants providing insights into the relationship between mutual and self-inductance. Some guidance has been offered regarding the interpretation of the differential equation, and there is an ongoing exploration of the roles of different EMFs in the problem.

Contextual Notes

There is a noted lack of information regarding the dimensions of the coil, which has led to varying assumptions among participants. The discussion also highlights the complexity of the problem due to the interplay of mutual and self-inductance.

harsh22902
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Homework Statement
In the adjacent figure, the mutual inductance of the infinite straight wire and the
coil is M, while the self inductance of the coil is L. The current in infinite wire is
varying according to the relation I = at, where "a" is a constant and t is the time.
The time dependence of current in the coil is .
Relevant Equations
flux = L*i
flux due to a coupled coil = M* current through that coil
sss.jpg


In the given question they have not provided the dimensions of the coil so I assumed it to be very close to the wire and having negligible dimensions compared to the wire . Then EMF induced in the coil due to the current in the wire comes out as M*a . Which when divided by resistance gives option a . But the correct answer is option D. Also the initial change in flux is due to current in the wire so I did not consider self inductance.
 
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You have to consider self inductance for this problem. There are two EMFs in this problem, one due to mutual inductance and one due to self inductance. We have to include both. The correct differential equation that describes this setup is $$M\frac{dI_1}{dt}+L\frac{dI_2}{dt}+I_2R=0$$ where ##I_2## is the current through resistor R, and we have included both EMFs (the EMF due to mutual inductance M ##M\frac{dI_1}{dt}## and the back EMF due to self inductance ##L\frac{dI_2}{dt}##).
)The solution to the above differential equation is indeed none of the options provided.
 
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The current I2 in the equation , is it due to emf induced by mutual inductance?
 
harsh22902 said:
The current I2 in the equation , is it due to emf induced by mutual inductance?
Well the mutual inductance is the primary cause if we can say that, but the self inductance also plays a role in its time dependence as that equation shows.
 
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Also, the term I2*R that is actually the 'net' emf , right?
 
Yes you can view it that way though it is actually the voltage drop in the resistance R but it is equal to the net emf as you say.
 
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Understood it now, thank you !
 
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