Magnetic Field Due To Wire Of Semi-Circular Cross Section

AI Thread Summary
The discussion centers on calculating the magnetic field due to a wire with a semi-circular cross-section. The initial calculations involve integrating the current density over the wire's area, but participants point out that the wire should be treated as a thin arc rather than a volume, leading to confusion about the current distribution. The correct approach is to consider the current density as uniform along the arc, simplifying the integration to account for its geometry. Participants emphasize that the vertical component of the magnetic field should integrate to zero due to symmetry. The terminology used in the question is criticized for being misleading, as it refers to the wire as a "semicircular ring."
Aurelius120
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Homework Statement
An infinite wire has semi-circular cross section with radius R. It carries current I. Then the magnitude of magnetic induction along its axis
Relevant Equations
Field due to infinite wire=##\frac{\mu_○I}{2\pi d}##
1000016287.jpg

I proceeded as follows
Current in sector ##d\theta=## is:
$$dI=\int_{x=0}^{x=R}{\frac{I}{\pi R^2/2}\times\frac{d\theta}{2\pi}\times 2\pi x dx}$$
Field due to sector ##d\theta## is therefore
$$dB=\int^{x=R}_{x=0}{\frac{\mu_○}{2\pi x}\times\frac{I}{\pi R^2/2}\times\frac{d\theta}{2\pi}\times 2\pi x dx}$$
$$\implies dB=\frac{\mu_○IR}{\pi^2R^2}d\theta$$
1000016289.jpg
For the entire wire:
$$B_{net}=\int^{\pi}_0{dB \cos(\theta-\pi/2) \hat i} + \int^{\pi}_0{dB \sin(\theta-\pi/2) \hat j}$$
Finally$$ B_{net}=\frac{2\mu_○I}{\pi^2R}$$

This is double the correct value? What did I do wrong ? Why does the book give this answer?
1000016289.jpg
 
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I don't understand what you are doing here: $$dI=\int_{x=0}^{x=R}{\frac{I}{\pi R^2/2}\times\frac{d\theta}{2\pi}\times 2\pi x dx}.$$ The semicircular ring of radius ##R## is very thin and there should be no ##\pi R^2## term to consider. Assume that the current is uniformly distributed over the ring. An arc ##ds=R ~d\theta## has current $$dI=\frac{I}{\pi R}ds=\frac{1}{\pi}I~d\theta.$$ Consider that as an infinitely long wire, find the two components of its contribution ##dB_x## and ##dB_y## at the center and integrate over ##\theta##. The vertical component is expected to integrate to zero by symmetry. That's how one adds vectors.
 
kuruman said:
I don't understand what you are doing here: $$dI=\int_{x=0}^{x=R}{\frac{I}{\pi R^2/2}\times\frac{d\theta}{2\pi}\times 2\pi x dx}.$$ The semicircular ring of radius ##R## is very thin and there should be no ##\pi R^2## term to consider.
The wire has semi-circular cross section. Therefore it has current distributed throughout its volume . It is a half cylinder with area ##\pi R^2/2## so current density is calculate by dividing current by area. So what is wrong with how I did it?
Why are you dividing current with circumference to find current density?
 
Aurelius120 said:
It is a half cylinder
The text says "semicircular ring", so just an arc of negligible width.
 
haruspex said:
The text says "semicircular ring", so just an arc of negligible width.
So how does that look like?
 
@Aurelius120 (just in case you're still not clear) based on the Post #1 diagram the conductor is shaped like this
gutter.gif

(but infinitely long and made of material of negligible thickness).

The use of the terms 'wire'and 'ring' in the question, is not ideal IMO.
 
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