Direction and magnitude of electric field produced by current change

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Homework Help Overview

The discussion revolves around the direction and magnitude of the electric field produced by changes in current, specifically in the context of solenoids and induced electromotive force (emf). Participants are examining the implications of Faraday's Law and the characteristics of magnetic fields within solenoids.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants question the absence of certain terms in the provided answers, such as the lack of ##\cos \theta## in the first answer and the absence of the number of turns ##N## in the second. They explore the relationship between magnetic flux and induced current, referencing Faraday's Law.

Discussion Status

Several participants are actively engaging with the questions posed, offering insights and analogies to clarify the concepts. There is a recognition of the need to understand the assumptions behind the equations used, particularly regarding the geometry of the solenoid and the orientation of the loops involved.

Contextual Notes

Participants are navigating through the implications of the geometry of the solenoid and the definitions of magnetic flux and electric field in relation to the problem. There is an ongoing examination of how the number of turns and the length of the solenoid affect the magnetic field and induced emf.

songoku
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Homework Statement
Please see below
Relevant Equations
Faraday Law
1745680139587.png

The answer key is:
a) ##\frac{\mu_o \pi nar_{1}^{2}}{R}##

b) ##-\frac{\mu_o abn}{2}##

My questions:
1) Why is there no ##\cos \theta## in answer (a)?
$$\text{induced current}=\frac{\varepsilon}{R}$$

When calculating induced emf ##\varepsilon=-\frac{d\Phi}{dt}=-\frac{d(\vec B . \vec A)}{dt}##, wouldn't the magnetic field produced by the solenoid making angle ##\theta## with respect to normal of plane of loop of wire so the rate of change of magnetic flux experienced by the loop is ##\mu_o an \pi r_{1}^{2} \cos \theta##?


2) Why is there no ##N## in answer (b), where ##N## is number of turns of the solenoid?
$$\int \vec E . d\vec s=-\frac{d\Phi}{dt}$$

##\Phi## is magnetic flux linkage so shouldn't ##\Phi=N\phi## so there is ##N## in the final answer?

3) Is the direction of electric field at distance ##b## in positive y direction?

Thanks
 
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songoku said:
My questions:
1) Why is there no cos⁡θ in answer (a)?
Because whoever wrote the answer didn't put it in?

Clearly, if θ = 90°, there will be no changing flux through the loop and hence no induced current.

songoku said:
Why is there no N in answer (b), where N is number of turns of the solenoid?
Because the magnetic field inside a very long solenoid of ##N## turns and length ##L## is approximated as ##B=\mu_0 n I## where ##n=\dfrac{N}{L}## is the number of turns per unit length.
 
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songoku said:
1) Why is there no cos⁡θ in answer (a)?
The induced current is the result of the magnetic flux that couples (i.e. flows through) the wire loops in the solenoid and the outer sensing coil. This is Faraday's Law. The solenoid flux in one direction is essentially entirely contained within the solenoid.
1745693681954.png



So if the sensing coil wraps around the solenoid (sort of tightly*) the angle doesn't matter, the flux through it will be the same.

An analogy is if you were counting cars on a freeway that pass through an imaginary plane, it wouldn't matter if that plane was tilted, as long as every car had to pass through it somewhere.

* You don't want that outer coil to capture much of the returning flux. A gigantic outer coil might not see any net flux, it could all (mostly) cancel.
 
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kuruman said:
Because the magnetic field inside a very long solenoid of ##N## turns and length ##L## is approximated as ##B=\mu_0 n I## where ##n=\dfrac{N}{L}## is the number of turns per unit length.
I mean why for the flux it is not ##\frac{\mu_o N^2 I}{L}##. I saw something similar to this when calculating self inductance of solenoid; I need to multiply the flux to get total flux linkage so the self inductance can be ##\frac{\mu_o N^2 \pi r^2}{L}##

DaveE said:
The induced current is the result of the magnetic flux that couples (i.e. flows through) the wire loops in the solenoid and the outer sensing coil. This is Faraday's Law. The solenoid flux in one direction is essentially entirely contained within the solenoid.
View attachment 360418


So if the sensing coil wraps around the solenoid (sort of tightly*) the angle doesn't matter, the flux through it will be the same.

An analogy is if you were counting cars on a freeway that pass through an imaginary plane, it wouldn't matter if that plane was tilted, as long as every car had to pass through it somewhere.

* You don't want that outer coil to capture much of the returning flux. A gigantic outer coil might not see any net flux, it could all (mostly) cancel.
I understand
 
kuruman said:
Because the magnetic field inside a very long solenoid of ##N## turns and length ##L## is approximated as ##B=\mu_0 n I## where ##n=\dfrac{N}{L}## is the number of turns per unit length.
For electric field in question (b), the correct answer is ##-\frac{\mu_o abn}{2}## or ##-\frac{\mu_o abnN}{2}##?

Thanks
 
songoku said:
For electric field in question (b), the correct answer is ##-\frac{\mu_o abn}{2}## or ##-\frac{\mu_o abnN}{2}##?
What is the expression for the magnetic field ##B## inside a solenoid?
What is the expression for the flux through the single loop in this problem?
 
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songoku said:
For electric field in question (b), the correct answer is ##-\frac{\mu_o abn}{2}## or ##-\frac{\mu_o abnN}{2}##?

Thanks
Since n=N/L, you are effectively asking whether it is ##-\frac{\mu_o abN}{2L}## or ##-\frac{\mu_o abN^2}{2L}##.
Perhaps you meant should it be ##-\frac{\mu_o abn}{2}## or ##-\frac{\mu_o abN}{2}##? If so, to put it another way, would the result be different if the solenoid were longer, but still the same winding density?
Well, what do you think?
 
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haruspex said:
Since n=N/L, you are effectively asking whether it is ##-\frac{\mu_o abN}{2L}## or ##-\frac{\mu_o abN^2}{2L}##.
Perhaps you meant should it be is ##-\frac{\mu_o abn}{2}## or ##-\frac{\mu_o abN}{2}##? If so, to put it another way, would the result be different if the solenoid were longer, but still the same winding density?
Well, what do you think?
I am actually asking whether it is ##-\frac{\mu_o abN}{2L}## or ##-\frac{\mu_o abN^2}{2L}## but I think now I know why I am wrong.

kuruman said:
What is the expression for the magnetic field ##B## inside a solenoid?
What is the expression for the flux through the single loop in this problem?
I was mistaken when taking which object to consider. I thought I need to consider the number of turns of solenoid. It turns out I need to consider the loop.


Thank you very much for all the help and explanation kuruman, DaveE, haruspex
 

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