Grade 12 Electromagnetic Problem

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SUMMARY

The discussion focuses on calculating the current required in a bottom wire to support a top wire carrying a current of 40A at a height of 4.0 cm, given a linear mass density of 150g/m. The magnetic field generated by the top wire is described by the formula B = (μ₀I)/(2πr), while the force acting on the wires is derived from the Lorentz force law, F_mag = qvB. By equating the magnetic force to the gravitational force, the necessary current in the bottom wire is determined using the equation I₂ = (μ 2πrg)/(μ₀I₁).

PREREQUISITES
  • Understanding of electromagnetic theory, specifically the Lorentz force law.
  • Familiarity with magnetic fields generated by current-carrying wires.
  • Knowledge of Newton's Second Law and its application to forces.
  • Ability to apply the right-hand rule for determining magnetic field direction.
NEXT STEPS
  • Study the derivation of the magnetic field around a long straight wire using Ampère's Law.
  • Learn about the applications of the right-hand rule in electromagnetic contexts.
  • Explore the relationship between current, magnetic fields, and forces in parallel wire systems.
  • Investigate the effects of varying linear mass density on wire stability in electromagnetic setups.
USEFUL FOR

Students and educators in physics, particularly those studying electromagnetism, as well as engineers working with electromagnetic systems and applications involving current-carrying conductors.

Dan17
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A wire, whose linear mass density is 150g/m, carries a current of 40A (supplied by a flexible negligible weight). This wire lies parallel to, and on top of, another horizontal wire on a table. What current must flow through the bottom wire in order to repel and support the top wire at a height of 4.0 cm above it? The top wire is held in place by frictionless guide plates.

Thanks,

...Dan
 
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The field due to a wire is

[tex]B=\frac{\mu_{0}I}{2\pi r}[/tex]

and the direction can be determined by use of the right hand rule. The force associated with these fields is given by the lorentz force law

[tex]F_{mag}=qvB[/tex]

when the field and the motion are perpendicular. Let's look at this another way... let's say that the lorentz force law read

[tex]F_{mag}=\frac{qLB}{\Delta t}[/tex]

we can then move that [tex]\Delta t[/tex] over to [tex]q[/tex] and get somthing that looks like this

[tex]F_{mag}=ILB=\frac{\mu_{0}I_{1}I_{2}}{2\pi r}L[/tex]

Utilizing Newton's Second law, in order for one wire to repel and support the other the forces must be equal.

[tex]0=F_{mag}-F_{grav}[/tex]

so we set the forces equal. ([tex]\mu[/tex] and [tex]\mu_{0}[/tex] are not related in any kind of way,[tex]\mu[/tex] is the linear mass density)

[tex]\mu gL=\frac{\mu_{0}I_{1}I_{2}}{2\pi r}L[/tex]

and we get a result that is only dependent on the second current

[tex]I_{2}=\frac{\mu 2\pi rg}{\mu_{0}I_{1}}[/tex]

Before you start putting numbers in make sure you understand what I have said here. And remember to give the current the proper polarity as indicated by the right hand rule.
 
Last edited:
Thanks for the help
 

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