Use of Biot-Savart Law for Square Loop

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SUMMARY

The discussion focuses on the application of the Biot-Savart Law to calculate the magnetic field at the center of a square loop. The user, Sekonda, successfully integrated the differential magnetic field element for each of the four sides of the loop, accounting for angle variations between 45 and -45 degrees. The resulting magnetic field expression is confirmed as B = (√2μ₀I)/(πa), which is accurate. The conversation highlights the connection between this scenario and the magnetic field of an infinite straight wire.

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Sekonda
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Hey,

My question concerns the integration of the biot savart law of a differential magnetic field element to find the magnetic field at the center of a square loop. The question is part (c) (using info from (b)) of the image below:

electromagnetism3.png


I want to check if what I did was right, but what I did was to integrate the differential magnetic field element separately for each of the 4 sides, using the fact the angle varies between 45 and -45 degrees for each side. So basically I multiplied the integral of the differential magnetic field by 4 and integrated across the limits of 45 degrees and -45 degrees to attain:

B=\frac{\sqrt{2}\mu _{0}I}{\pi a}

Is this right?

Many thanks for any help/comments!
SK
 
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Hey Sekonda! :wink:

Yup, looks ok. :smile:

(btw, [3] is the differential form of the usual (µo/4πa)(sinθ1 - sinθ2), = µo/2πa for an infinite straight wire :wink:)
 
Cheers thanks, and so it is; I always miss the ''intricate'' relations between scenario's in electromagnetism.

Thanks again,
SK
 

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