B-field for a half-infinitely long wire

In summary, the solution to this problem is to use the Biot-Savart Law. However, you need to consider the r^2 term when calculating the limits of integration, as the wire is infinitely long.
  • #1
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Homework Statement
Please see below
Relevant Equations
Please see below
For this problem,
1674757975575.png

The solution is
1674757999684.png


However, I would like to understand how to solve this using Biot–Savart Law.

So far my working is:

## \vec {dB} = \frac {\mu_0Ids\sin\theta} {4\pi r^2}##

However, I'm not sure what to do about the ## r^2 ## since the wire is infinitely long. I am thinking about having the limits of integration to be ## \theta_1 = 0 ## and ## \theta_2 = \frac {\pi} {2} ##

Many thanks!
 
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  • #2
Callumnc1 said:
.So far my working is:

## \vec {dB} = \frac {\mu_0Ids\sin\theta} {4\pi r^2}##
Knowing a formula is of no value unless you know what all the variables mean and in what context the formula applies.
Please state what those variables mean here. From that you should be able to answer your question.
 
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  • #3
As your LHS is vector, RHS should be vector also. Check it out.
 
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  • #4
haruspex said:
Knowing a formula is of no value unless you know what all the variables mean and in what context the formula applies.
Please state what those variables mean here. From that you should be able to answer your question.
Thank you for your reply @haruspex!

##\mu_0## is the magnetic permeability of free space
##I## is the current in the vertical wire
## ds ## is the length element of the wire
## r^2 ## is the distance from each ##ds## to point ##P##

I think the thing that was tripping me up was that I thinking that we could call the infinite length to be ##a## which would mean that ##\tan\theta = \frac {x} {a} ## however this would be zero since ## a \rightarrow \infty ## then ##\tan \theta \rightarrow 0 ##. I was then going to solve for ##\theta## and have limits of integration to be angles ## \theta_1 = 0 ## and ## \theta_2 = \frac {\pi} {2} ##. However now I think I should get ## r ## in terms of ## \sin\theta ##. I will try to solve that now. Is my reasoning correct so far?
 
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  • #5
anuttarasammyak said:
As your LHS is vector, RHS should be vector also. Check it out.
Thanks @anuttarasammyak ! Sorry both sides should have ##-\hat k## as the direction.
 
  • #6
Callumnc1 said:
I should get ## r ## in terms of ## \sin\theta ##.
Yes.
 
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  • #7
1674778111259.png

1674778179068.png

1674778209637.png
 
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  • #8
haruspex said:
Yes.
Thank you @haruspex !
 
  • #10
Callumnc1 said:
Thank you for your solution @Alex Schaller! :)
You are welcome
 
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FAQ: B-field for a half-infinitely long wire

What is the B-field of a half-infinitely long wire?

The B-field (magnetic field) of a half-infinitely long wire can be calculated using the Biot-Savart Law or Ampère's Law. For a wire extending from a point and going to infinity, the magnetic field at a distance \( r \) from the wire is given by \( B = \frac{\mu_0 I}{4 \pi r} \), where \( \mu_0 \) is the permeability of free space and \( I \) is the current through the wire.

How does the B-field of a half-infinitely long wire differ from that of an infinitely long wire?

The B-field of a half-infinitely long wire is essentially half of that of an infinitely long wire at the same distance \( r \). For an infinitely long wire, the B-field is \( B = \frac{\mu_0 I}{2 \pi r} \), while for a half-infinitely long wire, it is \( B = \frac{\mu_0 I}{4 \pi r} \).

What direction does the B-field of a half-infinitely long wire point?

The direction of the B-field around a half-infinitely long wire follows the right-hand rule. If you point the thumb of your right hand in the direction of the current, the curl of your fingers shows the direction of the magnetic field, which forms concentric circles around the wire.

Can the B-field of a half-infinitely long wire be calculated using Ampère's Law?

Yes, the B-field of a half-infinitely long wire can be calculated using Ampère's Law, but it requires considering the boundary conditions appropriately. Ampère's Law states that \( \oint \mathbf{B} \cdot d\mathbf{l} = \mu_0 I_{\text{enc}} \). For a half-infinite wire, the enclosed current is \( I/2 \), leading to \( B = \frac{\mu_0 I}{4 \pi r} \).

What assumptions are made when calculating the B-field of a half-infinitely long wire?

The primary assumptions include that the wire is perfectly straight and extends infinitely in one direction, the current is steady (DC), and the medium around the wire is homogeneous and isotropic (usually vacuum or air). These assumptions simplify the calculations and allow the use of symmetry in applying the Biot-Savart Law or Ampère's Law.

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