Biot-Savart Law Difficult Problem

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SUMMARY

The discussion centers on applying the Biot-Savart Law to determine the magnetic field at point P caused by a straight wire segment carrying current I at an angle of 30°. The correct expression for the magnetic field is identified as (μoIlcos30°) / (4π^2). Participants express confusion regarding the integration process and the origin of the π^2 term in the denominator, emphasizing the importance of understanding the geometry and dimensional analysis involved in the Biot-Savart Law.

PREREQUISITES
  • Understanding of the Biot-Savart Law and its application
  • Familiarity with magnetic fields generated by current-carrying conductors
  • Basic knowledge of vector calculus for integration
  • Concept of angles in relation to magnetic field calculations
NEXT STEPS
  • Study the derivation of the Biot-Savart Law in detail
  • Learn how to perform vector integration in magnetic field calculations
  • Explore dimensional analysis in physics equations
  • Investigate the effects of angle variations on magnetic field strength
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Physics students, educators, and anyone interested in electromagnetism, particularly those tackling problems involving the Biot-Savart Law and magnetic fields from current-carrying wires.

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Homework Statement


A short, straight wire segment of length l carries current I and is oriented so that it makes an angle of 30° with the horizontal. Point P is a distance r below the wire segment.

Which expression below is the best approximation for the magnetic field caused by the wire segment at point P?

http://online.physics.uiuc.edu/cgi/courses/shell/common/showme.pl?courses/phys212/oldexams/exam2/fa09/fig15.gif

(a) (μoIlcos30°) / (4π^2)
(b) (μoIlsin30°) / (4π^2)
(c) (μoIl) / (4π^2)

Homework Equations



dB = (μo Idl x r(unit vector)) / (4πr^2)

The Attempt at a Solution



It seems I have to integrate to get the answer, however the geometry behind this problem is really confusing me. I believe I have to integrate r from when it touches the beginning of the wire segment to the end of the wire segment, however I can't figure out how to manipulate the Biot-Svart law to do that. This is what I have so far:

(μo I)/(4π) = S sin(theta)ds/r^2 (S = integral :p)

Now, what do I do with ds?
Can anyone help me out, help would be greatly appreciated :]!

Btw π = pi and μo = mu(0), don't know if you can tell.
 
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You can keep r fixed. Resolve current element I*l into two components, I*l*cos(theta) and I*l*sin(theta). The point P lies on equatorial line to I*l*cos(theta). So it contributes to magnetic field.
The point P lies on axial line to I*l*sin(theta). So it does contributes to magnetic field.
 
Ok, but then where does the pi^2 term come from in the denominator?
Also, the answer is (a) which makes since for the cos, but the pi^2 is what I don't get...
 
Last edited:
There is no integral involved. Just think it through. Which of the three choices gives what you expect when the angle between the wire and the doted line is zero instead of 30o? What about if it is 90o instead of 30o?
 
Ok, I know the answer just by looking at the choices. What I am trying to figure out is where part of that answer comes from. I don't see where that pi^2 in the denominator comes from.
 
I don't see where it comes from either. The posted set of possible answers is dimensionally incorrect. Compare with the law of Biot-Savart equation that you posted. The dimensions should be dimensions of μ0 times dimensions of current divided by Length.
 

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