The magnetic flux density at point P between parallel wires

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SUMMARY

The magnetic flux density at point P between two parallel wires carrying currents of 15 A and 32 A, separated by 5.3 cm, is calculated using the formula B = μ₀(I/2πr). The total magnetic flux density at point P is determined to be approximately 0.19 mT, aligning with the answer provided in the reference book. The calculation involves using the Pythagorean theorem to combine the contributions from both wires, as the magnetic fields are orthogonal. The final result is derived from the equation B_total = √(B_B² + B_A²).

PREREQUISITES
  • Understanding of magnetic flux density and its calculation.
  • Familiarity with the right-hand rule for determining magnetic field direction.
  • Knowledge of the Pythagorean theorem for vector addition.
  • Proficiency in using the permeability of free space (μ₀) in calculations.
NEXT STEPS
  • Review the derivation of the magnetic flux density formula B = μ₀(I/2πr).
  • Explore vector addition of magnetic fields, particularly in orthogonal configurations.
  • Study the application of the right-hand rule in different current configurations.
  • Investigate the effects of varying current magnitudes on magnetic flux density.
USEFUL FOR

Students studying electromagnetism, physics educators, and anyone involved in electrical engineering or related fields seeking to understand magnetic field interactions between current-carrying conductors.

whatdoido
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Homework Statement


In the picture at points A and B are two thin parallel wires, where traveling currents are 15 A and 32 A to opposite directions. The distance between wires is 5.3 cm. Point's P distances from A and B are the same. Calculate the magnetic flux density at point P.
magndens1.png


Homework Equations


##B=\mu_0\frac{I}{2\pi r}##

The Attempt at a Solution



##I_1=15A##
##I_2=32A##
##x=5.3cm=0.053m##
##\mu_0=4\pi *10^-7 Tm/A##

I solved length L with Pythagorean equation

##L^2+L^2=x^2##

##L=\frac{x}{\sqrt{2}}##

With right-hand-rule the directions of magnetic flux density can be deduced. The magnetic flux density at point P generated from point B is to the direction of point A. From point A the generated magnetic flux density at point P is towards point B.

magndens2.png


To add both ##B_B## and ##B_A## they need to be turned downward by ##\theta## which is ##\theta=\frac{90^o}{2}=45^o##. This should be reasonable, right? The total magnetic flux density at point P is then:

##B_{total}=sin\theta B_B+sin\theta B_A=sin\theta\mu_0\frac{I_1}{2\pi \frac{x}{\sqrt{2}}}+sin\theta\mu_0\frac{I_2}{2\pi \frac{x}{\sqrt{2}}}=sin\theta(I_1+I_2)\frac{\mu_0}{\sqrt{2}\pi x}=1.773...*10^-4 T \approx 0.17mT##

This problem is from a book and it gives answer 0.19mT. I checked multiple times where I could have made a mistake but I cannot find it. The calculation is rather straightforward so there is not much to check. Thus it looks like there is some conceptual error? Thanks for reading and any help is appreciated
 

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whatdoido said:
To add both ##B_B## and ##B_A## they need to be turned downward by θ
That will give you the PX component of each, but since they are of different magnitudes their resultant also has an AB component.
Since the two flux density vectors are orthogonal, it is much simpler to add them without resolving into PX and AB components.
 
Okay simply with Pythagorean style:

##B_{total}=\sqrt{B_B^2+B_A^2}=\sqrt{(\frac{μ_0 I_1}{√2πx})^2+(\frac{μ_0 I_2}{√2πx})^2}=1.886...*10^{-4} T \approx 0.19mT##

Thanks!
 
Last edited:

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