Magnetic field of off center triangle - Biot Savart Law

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The discussion focuses on calculating the magnetic field at point P due to a wire shaped as an isosceles right triangle carrying current I. The key equation used is the Biot-Savart Law, which requires evaluating the magnetic field contributions from each segment of the triangle. It is clarified that while different coordinate systems can be considered for each segment, a single coordinate system is sufficient for the calculation. The contributions from two segments must be added, with one segment contributing a field based on its length a and the other based on length √2a. The overall magnetic field direction is consistent, pointing into the screen.
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1. Homework Statement

A piece of wire is bent into an isosceles right triangle whose shorter sides have length a The wire carries current I. Calculate the magnetic field for point P. Point P is located on the Y-axis ( 0, √2a). Two corners of the triangle are are located at (0,0), (√2a,0).

Homework Equations


I have to use the definition of the magnetic field for each side.
dB = (u/4π) (Ids x r(unit vector))/r^2

The Attempt at a Solution


My problem is more conceptual. Can I split the triangle into three different parts and have different coordinate systems for them? I was thinking of setting one side to be along x axis, and rotate the other side. Pic included. Can I add the magnetic field for each side if they had different coordinate systems?
 

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All segments produce fields in the same direction, into the screen. One coordinate system is sufficient for all. As you pointed out, one segment contributes nothing. Note that both of the other two segments produce fields that are at a perpendicular distance from their end that is equal to their length. One length is ##a## and the other ##\sqrt{2}a##. So basically you need to find the field from the end of a segment of distance L at perpendicular distance L from its end, then add two contributions one with ##L=a## and one with ##L=\sqrt{2}a##.
 
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