Law for magnetic field due to solenoid

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The discussion centers on the formula for calculating the magnetic field (B) in a solenoid, specifically the interpretation of 'n' in the equation B = 4pi * 10^-7 * n * I/L. Participants clarify that 'n' refers to the total number of loops, not just those in a single layer, and emphasize that the formula is intended to calculate the magnetic field at the center of the solenoid. They note that while the formula provides an approximate value, the magnetic field strength varies along the length of the solenoid, being strongest at the center. The conversation also touches on the importance of understanding the underlying principles of the formula rather than just memorizing it. Overall, the key takeaway is that for a solenoid with multiple layers, the total number of loops should be used in the calculation.
NooDota
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Homework Statement



Just a quick clarification about the law: B = 4pi * 10^-7 * n *I/LDoes n refer to total number of loops, or just the number of loops in a single layer?

Like, If I have a solenoid that's made up of 4 layers and 1000 total loops, do I plug in 1000 or 250?

Homework Equations

The Attempt at a Solution

 
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NooDota said:
Just a quick clarification about the law: B = 4pi * 10^-7 * n *I/L
Let me rewrite it:

B = μ0*H

It looks like an attempt to calculate the B-Field in the center of a solenoide. Thus:

By "n/L", turns per length is meant, so you could write it:

Bcenter = μ0 * I * ( ΔN / ΔL ).

n = ΔN , L = ΔL ( if you understand what I mean ) :wink:
 
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Your formula is made from the figure beneath with Amperes law:

upload_2015-6-13_0-26-53.jpeg
 
NooDota said:

Homework Statement



Just a quick clarification about the law: B = 4pi * 10^-7 * n *I/L
Does n refer to total number of loops, or just the number of loops in a single layer?
Like, If I have a solenoid that's made up of 4 layers and 1000 total loops, do I plug in 1000 or 250?
1000.
n refers to the total number of loops in that formula.
However, conventionally n is used to mean "loops per unit length"; in SI that would be loops per meter.
It doesn't matter whether loops are in 1st or 2nd or 3rd or 4th layer, or any other layers.
 
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Okay, thank you all.
 
rude man said:
n refers to the total number of loops in that formula.
However, conventionally n is used to mean "loops per unit length";

I don't think you are right here. It is not just a convention, but a premise. The intension of the formula is to calculate the H or B field at a distinct location ( the center ) in the solenoide.

Of symmetrical reasons you can only find the H and B fields at the center: Amperes law just tells you what the mean values will be, following the circulation path. Now calling the lower left corner of the rectangle ( circulation path ) in the figure in #3, A, then clockwise the other corners B, C, D. If AB and CD are very close to each other, the H fields parallel to AB and CD will be zero, because the H-field will be perpendicular to AB and CD due to symmetry. Making BC and DA longer ( or not centered ), the H-field will no longer be perpendicular to AB and CD. The lengths of AB and CD are assumed infinite, so that the H-field along BC is zero.

Therefore the formula can only find the H-field at the center of the solenoid, and thus DA must be kept very small. That's why n = ΔN / ΔL, ( not N/L ).

I know that the result will be the same, no matter if you use n or N. I'm just speaking of the premises as for the formula, and that the H-field is calculated at the center of the solenoid.
http://h2physics.org/wp-content/uploads/2010/05/solenoid2.jpg
 
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Hesch said:
I don't think you are right here. It is not just a convention, but a premise. The intension of the formula is to calculate the H or B field at a distinct location ( the center ) in the solenoide.

Of symmetrical reasons you can only find the H and B fields at the center: Amperes law just tells you what the mean values will be, following the circulation path. Now calling the lower left corner of the rectangle ( circulation path ) in the figure in #3, A, then clockwise the other corners B, C, D. If AB and CD are very close to each other, the H fields parallel to AB and CD will be zero, because the H-field will be perpendicular to AB and CD due to symmetry. Making BC and DA longer ( or not centered ), the H-field will no longer be perpendicular to AB and CD. The lengths of AB and CD are assumed infinite, so that the H-field along BC is zero.

Therefore the formula can only find the H-field at the center of the solenoid, and thus DA must be kept very small. That's why n = ΔN / ΔL, ( not N/L ).

I know that the result will be the same, no matter if you use n or N. I'm just speaking of the premises as for the formula, and that the H-field is calculated at the center of the solenoid.
http://h2physics.org/wp-content/uploads/2010/05/solenoid2.jpg
As before, I am confused by your riposte, feeling it to be inapposite.
 
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Ahh, I don't know any of the stuff you're talking about. I've only studied magnetic fields in my school and they just gave us direct laws to calculate them. (Straight line, solenoid, and a circular circuit or whatever you call it)
 
NooDota said:
Ahh, I don't know any of the stuff you're talking about. I've only studied magnetic fields in my school and they just gave us direct laws to calculate them. (Straight line, solenoid, and a circular circuit or whatever you call it)
I wouldn't worry about it! :smile: (BTW your 'circular circuit' is probably a one-turn loop or a toroid).
 
  • #10
rude man said:
I am confused by your riposte, feeling it to be inapposite.
Why?

It's important to understand, that the H-field is not constant along a solenoid ( the H-field has most strength at the center ). As for other locations in/nearby the solenoid, Biot-Savart law must be used.

I'm just specifying that, as it is not mentioned in post #1.

How come that you are confused about that? Why is it inapposite?

This is the "wrong" sketch:

sol3.gif

I've picked out the sketch in #6.
 
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  • #11
Hesch said:
Why?.
Because you did not address the OP's question (post #1). Th OP's formula is the prima facie formula for axial B in a finite-length solenoid. The main purpose of its derivation is to show the multifarious utility of Ampere's law, and is always accompanied by a statement that the so computed field is approximate. I don't think the OP wanted to go beyond that point. I pointed out that the formula does not discriminate among windings from different layers. Thus, my answer of "1000" which is all he asked for.

For a more accurate computation of the axial B field inside or outside the solenoid one invokes the Biot-Savart law, applied to each winding individually and then summed for all windings. The ensuing summation is more simply replaced by the appropriate integral. Theodoros.mihos has recently posted a site which shows one way of accomplishing this:

 
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  • #12
That's why n = ΔN / ΔL, ( not N/L ).
Same thing, unless the spacings are uneven!
 
  • #13
rude man said:
Same thing, unless the spacings are uneven!
Its the same result, but not the same "thing".
Hesch said:
Of symmetrical reasons you can only find the H and B fields at the center: Amperes law just tells you what the mean values will be, following the circulation path.
I've written this of educational reasons, so that the OP ( what does that mean? ) won't have to remember the formula. The OP has just to remember the principle in where the formula has derived from. Having understood that, and if the OP can somehow place a symmetric circulation path through a toroid, the OP can see through how the formula must be as for a toroid. ( H = N * I / 2πr ). I think it's more constructive to explain the idea ( how to find the H-field in the center of a toroid ) in the formula, than to reply with a "1000".

My english is not excellent, but I've found help here:

http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html

( Same idea ).
 

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