Helmholtz Coil Problem: Analyzing Magnetic Field at Point Z

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SUMMARY

The discussion focuses on analyzing the magnetic field at point Z, located midway between two identical Helmholtz coils. Each coil consists of N loops carrying current I, with a radius R and separated by a distance R. The magnetic field strength B at point Z is derived using the equation B = (4/5)^(3/2) * (μNI/R), and it is established that both the first and second derivatives of B with respect to z are zero at point Z (z = -R/2), indicating minimal variation in the magnetic field at this location.

PREREQUISITES
  • Understanding of Helmholtz coil configuration and its properties
  • Familiarity with magnetic field equations, specifically dB_z = (μ₀I/4π)(dl/r²)cos(θ)
  • Knowledge of calculus, particularly differentiation and integration
  • Basic principles of superposition in electromagnetic theory
NEXT STEPS
  • Study the derivation of the magnetic field for a single current loop
  • Learn about the application of superposition in calculating magnetic fields from multiple sources
  • Explore the implications of magnetic field uniformity in Helmholtz coils
  • Investigate the effects of varying coil parameters (N, I, R) on magnetic field strength
USEFUL FOR

Physics students, electrical engineers, and researchers interested in electromagnetism and magnetic field analysis, particularly those studying Helmholtz coils and their applications.

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Homework Statement



The diagram illustrates a Helmholtz coil, consisting of two identical circular coils of wire, each one having N loops and carrying the same current I. The radius of each coil is R, and the two coils are R meters apart. (a) What are the direction and strength of the magnetic field at the point Z, midway between the two coils? (b) Express B as a function of the variable z, taking the origin for z to be at the center of the left-hand coil and the positive z direction to be to the left. (c) Find the first and second derivatives of the magnetic field strength B with respect to z, dB/dz and d 2B/dz2. Show that they are both zero at point Z (where z = −R/2). This shows that the magnetic field varies very little at the point Z.

http://i40.tinypic.com/k4b5ag.jpg

that link should have the picture.

Homework Equations



I think the equation for a Helmholtz coil is (4/5)3/2 (uNI/R)


The Attempt at a Solution



For part a, I think it's to the left. I could really use some direction for parts B and C. Thanks!
 
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Start by finding the differential field at any point on the z axis for one current loop:

dB_z=\frac{\mu_0I}{4\pi}\frac{dl}{r^2}cos\theta

where theta is the angle made by the radius of the loop and the line from the current element on the loop to the point on the z axis. Intergrate to determine the field contributions from all the dl elements. Then multiply by the factor N to find all the loop contributions. Do the same for the second coil. Express the cosine function in terms of the loop radius and the distance from one of the loop centers to the point in question. Finish by using superposition.
 

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