Infinite wires with current, magnetic field vector

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SUMMARY

The discussion focuses on calculating the magnetic field vector at point A due to three infinitely long straight wires carrying current I, arranged in a square configuration. Participants emphasize using the Biot-Savart law, specifically the equation B = μ₀/4π ∫(IdL/r²), to derive the magnetic field contributions from each wire. The solution involves analyzing the symmetry of the arrangement and applying the right-hand rule to determine the direction of the magnetic fields. The final magnetic field vector is obtained by summing the contributions from the vertical, horizontal, and diagonal wires.

PREREQUISITES
  • Understanding of the Biot-Savart law and its application in calculating magnetic fields.
  • Familiarity with vector addition and the right-hand rule for determining magnetic field directions.
  • Knowledge of integration techniques for evaluating magnetic field contributions from wire segments.
  • Basic concepts of electromagnetism, particularly related to current-carrying conductors.
NEXT STEPS
  • Study the derivation of the magnetic field for a straight current-carrying wire segment using the Biot-Savart law.
  • Learn about vector addition of magnetic fields from multiple sources in electromagnetism.
  • Explore the application of the right-hand rule in determining the direction of magnetic fields in various configurations.
  • Investigate symmetrical arrangements of current-carrying wires and their effects on magnetic field calculations.
USEFUL FOR

Students and educators in physics, particularly those studying electromagnetism, as well as engineers and physicists working with magnetic field calculations in electrical systems.

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Homework Statement



three infinitely long straight wires are arranged in a plane as shown at the left. what is the magnetic field vector at point A(see attach.)? all wires carry current I

Homework Equations



F = IL X B where x indicates cross product, I is current, L is length, B is magnetic field

magnetic field, biot-savart law, B = mu_0/4pi[integral(IdL/r^2)] where mu_0 is constant = 4pi*10^-7, dL is change in length, r is radius/distance, I is current

The Attempt at a Solution



not too sure about how to start, this is what i am thinking of:

first, determine the net magnetic field at the center of the triangle formed by the three wires, and then use the distance from the center of that triangle to point a, as value r in the biot-savart equation.

i have a feeling that since the problem asks for a vector, i need to analyze each wire individually based on their direction, is this a correct assumption?

help appreciated
 

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The wires actually follow the sides and diagonal of a square, which means we can take advantage of some symmetry for this (though not in an obvious way).

What you'll need to derive is the expression for the magnetic field at a point at a perpendicular distance r from the midpoint of a current-carrying wire segment of length L. You use Biot-Savart and the integration is symmetrical around the midpoint of the wire.

You would then use your result for three fields:

1) for the wire on the "vertical" side of the square, you use half your result for a point at a distance a from a segment of length a ;

2) for the "horizontal" side of the square, you use the same value as in (1) above ; and

3) for the diagonal, use the full field value for a point
a/sqrt(2) away from a wire of length a·sqrt(2), but with the field direction pointing the other way. (Use the right-hand rule for the three segments to see why the parts add this way.)

If the magnetic field for a wire segment is already derived in your book, you can just use it; otherwise, the integration isn't too bad...
 

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