How Is the Formula for Induced Current in a Coil Derived?

In summary, the conversation discusses a problem involving a single coil in a constant magnetic field and the dimensions of the coil. The formula I = (delta A*B)/(delta t*R) is used to calculate the magnitude of the induced current. It is derived from Faraday's law and Ohm's law. There is a minor disagreement about the equations, but it is clarified.
  • #1
pkossak
52
0
I was wondering about the following problem:

You are looking down on a single coil in a constant magnetic field B = 0.9 T which points directly into of the screen. The dimensions of the coil go from a = 6 cm and b = 15 cm, to a* = 20 cm and b* = 19 cm in t=0.028 seconds. If the coil has resistance that remains constant at 1.7 ohms, what would be the magnitude of the induced current in amperes?

Now, I have the answer, and I was told how to get it. I used the formula I = (delta A*B)/(delta t*R)

What I was wondering was if someone could tell me what rule or law this formula came from? I can't figure out how to derive it from any of the formulas given in this chapter. Thanks a lot.
 
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  • #2
sorry I just realized this was the wrong place to post this question!
 
  • #3
It can be derived using one of the Maxwell equations: Faraday's law:

[tex]\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}[/tex]

or in integral form

[tex]\int \vec{E} \cdot d \vec{l} = -\frac{d}{dt} \int \vec{B} \cdot d \vec{A} = -\frac{d \Phi}{dt}[/tex]

With phi the flux B*A enclosed. The first integral is equivalent to (minus) the voltage across the loop so:

[tex]V = \frac{d \Phi}{dt} = A \frac{d B}{dt} +B\frac{d A}{dt} [/tex]

Or in your case only the last term is nonzero, so

[tex]I=\frac{V}{R}=\frac{dA}{dt} \frac{B}{R}[/tex]
 
  • #4
da_willem said:
[tex]I=\frac{V}{R}=\frac{dA}{dt} \frac{B}{R}[/tex]

I'm afraid I don't agree with you here. You are effetively saying that the induced emf is equal to the induced current :confused:. Also Faraday's law is rate of change of flux, therefore the BA should be enclosed.

I've already replied to your other post pkossak.

-Hoot:smile:
 
  • #5
As far as I made a mistake, you're not too good at explaining where.

Hootenanny said:
You are effetively saying that the induced emf is equal to the induced current

Where? I said I=V/R which is just Ohms law

Hootenanny said:
Also Faraday's law is rate of change of flux, therefore the BA should be enclosed

Ofcourse, I also stated that explicitly

da_willem said:
With phi the flux B*A enclosed

So I'm sorry but I can't really see what's wrong with my derivation...?!
 
  • #6
da_willem said:
So I'm sorry but I can't really see what's wrong with my derivation...?!

Sorry, It just confused me when the flux was in a different fraction. The last point is minor but you say;

[tex]I=\frac{V}{R}=\frac{dA}{dt} \frac{B}{R}[/tex]

[tex]I=\frac{V}{\not R}=\frac{dA}{dt} \frac{B}{\not R}[/tex]
[tex] I = V = \frac{d(AB)}{dt}[/tex]
 
  • #7
Thanks for your reply. Do you mean to say I=V/R should be I=V?

This is not only in conflict wih Ohm's law, it also yields the wrong result. It is the emf that is equal to (minus) the time derivative of the flux, not the current...
 
  • #8
da_willem said:
Thanks for your reply. Do you mean to say I=V/R should be I=V?

This is not only in conflict wih Ohm's law, it also yields the wrong result. It is the emf that is equal to (minus) the time derivative of the flux, not the current...

No, look at the equation you have written;

[tex]I=\frac{V}{R}=\frac{dA}{dt} \frac{B}{R}[/tex]

The two resistances would cancel, leaving you with;

[tex]I=V=\frac{dAB}{dt}[/tex]

Which implies that I = V. I knew what you meant, but at first glance it may be confusing.
 
  • #9
I'm totally lost in what you mean...:confused:

You can't just cancel the R's in the last equality and do noting with the first equality...

[tex]I=\frac{V}{R}=\frac{dA}{dt} \frac{B}{R}[/tex]

Multiplying by R

[tex]IR=V=\frac{dA}{dt} B[/tex]

So IR=V (Not I=V) which is just Ohm's law again!
 
  • #10
Ahh sorry, my mistake I was veiwing them as two separate equations, my apologies da_willem.
 

FAQ: How Is the Formula for Induced Current in a Coil Derived?

What is a coil and how is it used in physics?

A coil is a conducting wire wound in a spiral shape. It is used in physics to create a magnetic field when an electric current is passed through it. This magnetic field can be used for a variety of purposes, such as electromagnets, generators, and inductors.

How is the current in a coil related to its magnetic field?

The strength of the magnetic field produced by a coil is directly proportional to the current passing through it. This means that as the current increases, the magnetic field becomes stronger, and vice versa.

What is the difference between AC and DC current in a coil?

AC (alternating current) in a coil is when the direction of the current changes periodically, usually in the form of a sine wave. DC (direct current) in a coil is when the current flows in one direction only. AC current is used in most household appliances, while DC current is commonly used in batteries and electronic devices.

How does changing the number of turns in a coil affect its magnetic field?

The number of turns in a coil affects the strength of its magnetic field. Increasing the number of turns will increase the strength of the magnetic field, while decreasing the number of turns will decrease the strength of the magnetic field. This is because the more turns there are, the more concentrated the magnetic field becomes.

What is Lenz's Law and how does it relate to coil current?

Lenz's Law states that when a changing magnetic field passes through a coil, an electromagnetic force is induced in the coil that opposes the change in magnetic flux. This means that if the current in a coil is increasing, the induced magnetic field will oppose the increase in current. Similarly, if the current is decreasing, the induced magnetic field will oppose the decrease in current. This is important to consider in applications where a changing magnetic field is used, such as generators and motors.

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