Solving Biot-Savart Law for a Ring of Charge

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The discussion focuses on solving the Biot-Savart Law for a ring of charge, specifically analyzing the magnetic field along the X-axis from the center of the ring. The problem involves a current flowing counterclockwise in a ring located in the Y-Z plane, with participants clarifying the definitions of the coordinate system and variables used in the calculations. There are concerns about the clarity of the problem description, particularly regarding the orientation of the ring and the meaning of certain variables. Corrections were made to the expressions for the infinitesimal length element and the unit vector, leading to a resolution of the mathematical discrepancies. The final consensus indicates that the calculations are now correct, and the problem has been resolved.
Maxwellkid
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This is a simple problem if you work with only magnitude and consider the symmetry of a ring. However, I am taking a detailed approach, and I am not getting the correct answer. Could you please look over my math?

a evenly distributed ring of charge on the positive Y-Z plane has a current, I, flowing counterclockwise or flowing from positive Z direction on top and -Z direction on bottom of ring. Figure out the magnetic field along the X axis of this ring of charge from the center of the ring.

d \vec{B} = \frac {\mu_{o} I}{4\pi} \frac {d\vec{l} \times \hat{r}}{r^2}

below are pictures of the ring of charge. left picture is the sideway view with theta being constant. right picture is the frontal view with phi.

d\vec{l} = <0 , dl cos\phi , dl sin\phi>
\hat{r} = <cos\theta , -w/r sin\phi , w/r cos\phi>

{d\vec{l} \times \hat{r} = \frac{w}{r} cos^2\phi dl \cdot \hat{i} + \frac{w}{r} sin^2\phi dl \cdot \hat{i} + cos\theta sin\phi dl \cdot \hat{j} - cos\theta cos\phi dl \cdot \hat{k}

\frac {d\vec{l} \times \hat{r}}{r^2} =\frac{w}{r^3} 1 dl \cdot \hat{i} +\frac{1}{r^2} cos\theta sin\phi dl \cdot \hat{j} - \frac{1}{r^2} cos\theta cos\phi dl \cdot \hat{k}

dl = w d\phi

\frac {d\vec{l} \times \hat{r}}{r^2} = \frac{w^2}{r^3} 1 d\phi \cdot \hat{i} +\frac{w}{r^2} cos\theta sin\phi d\phi \cdot \hat{j} - \frac{w}{r^2} cos\theta cos\phi d\phi \cdot \hat{k}

ARE ALL MY STEPS CORRECT SO FAR?
 

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Maxwellkid said:
a evenly distributed ring of charge on the positive Z plane has a current, I, flowing counterclockwise or flowing from positive Z direction on top and -Z direction on bottom of ring. Figure out the magnetic field along the X axis of this ring of charge from the center of the ring.

This problem description is not at all clear to me. For starters, what is 'the z plane'? There is such a thing as a z axis, but not a z plane. Do you mean the plane defined by the equation z=0 (AKA the x-y plane)? Or do you mean the y-z plane (x=0) as your pictures would leave me to believe? Or perhaps you mean something else entirely?

Also, the 'top' and 'bottom' of the ring are not well defined. Which direction is up, and which direction is down?

I also see the variable w in your calculations, but no explanation as to what it represents.
 
gabbagabbahey said:
This problem description is not at all clear to me. For starters, what is 'the z plane'? There is such a thing as a z axis, but not a z plane. Do you mean the plane defined by the equation z=0 (AKA the x-y plane)? Or do you mean the y-z plane (x=0) as your pictures would leave me to believe? Or perhaps you mean something else entirely?

Also, the 'top' and 'bottom' of the ring are not well defined. Which direction is up, and which direction is down?

I also see the variable w in your calculations, but no explanation as to what it represents.

z plane refers to the z-y plane. w is the radius of the ring of charge. positive z direction current on top of ring and negative z direction current on bottom of ring (counterclockwise current flow)
 
Maxwellkid said:
z plane refers to the z-y plane. w is the radius of the ring of charge. positive z direction current on top of ring and negative z direction current on bottom of ring (counterclockwise current flow)

Okay, and by 'top' you mean the point (0,w,0)?

Maxwellkid said:
d\vec{l} = <-dl sin\phi , dl cos \phi , 0>

d\vec{l} is an infinitesimal piece of the ring, right? If the ring is entirely in the y-z plane, why does your expression have a non-zero x-coordinate?

\hat{r} = <cos\theta , -w/r sin\phi , w/r cos\phi>

Are you sure about the sign of the z-coordinate?

Also, I'm not sure why you would bother introducing a new variable \theta here...why not just work with the variables given ion the problem statement x and w?

\vec{r}=<x,-w\sin\phi,-w\cos\phi>

\implies r=\sqrt{x^2+w^2}

\implies\hat{r}=<\frac{x}{\sqrt{x^2+w^2}},\frac{-w\sin\phi}{\sqrt{x^2+w^2}},\frac{-w\cos\phi}{\sqrt{x^2+w^2}}>
 
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gabbagabbahey said:
Okay, and by 'top' you mean the point (0,w,0)?

d\vec{l} is an infinitesimal piece of the ring, right? If the ring is entirely in the y-z plane, why does your expression have a non-zero x-coordinate?
i think you're right
gabbagabbahey said:
This doesn't look like a unit vector to me, its magnitude does not equal 1.

To properly find \hat{r}, Start by finding an expression for \vec{r}, and then divide by its magnitude.
it is a unit vector. try taking the absolute value of it...it comes out to 1
 
i've made the dl correction in the original post. THANKS. however, the math still comes out to be a bit off...i'm off by a half.
 
Maxwellkid said:
it is a unit vector. try taking the absolute value of it...it comes out to 1

Yes, I realized after I posted that \cos^2\theta+\frac{w^2}{r^2}=1 from looking at your picture.
 
okay...it's been corrected...i'll check back in a couple of hours...need to be away from computer
 
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Hmmm... looking at your picture it seems that you have defined \phi such that z=w\cos\phi, but looking at you calculations it seems as though you are using z=-w\cos\phi...which is it?
 
  • #10
i got it...came out correctly...

thank you!
 

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