How to Calculate Magnetic Flux with a Long Wire and Rotated Plane

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Homework Help Overview

The problem involves calculating the magnetic flux through a rotated plane defined by specific radial and vertical limits, with a current flowing along a long wire. The context includes the application of magnetic field concepts and integration to find the flux.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the integral definition of magnetic flux and express uncertainty about the geometry of the problem. There are attempts to clarify the setup, including considerations of cylindrical coordinates and the relationship between the magnetic field and the area element.

Discussion Status

The discussion is ongoing, with participants seeking clarification on the geometry and the application of relevant laws. Some have proposed interpretations of the problem, while others are waiting for further input from the original poster.

Contextual Notes

Participants note the lack of a clear visual representation of the problem and express confusion regarding the angle between the magnetic field and the area element. There is also mention of the need for additional information to fully understand the setup.

hd28cw
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Find the magnetic flux crossing the portion of the plane
theta = x/4 defined by 0.01 m < r <0.05 m and 0 m < z < 2 m. A current of 2.50 A is flowing along z-axis along a very long wire.

in drawing the picture i know that there is a long thin wire with a current of 2.5 amps flowing positively on the z-axis and the plane is lying rotated at an angle of pi/4 with the magnetic field flowing in a counter clockwise direction.

How do I go about finding the magnetic flux.
Please help.
 
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The magnetic flux through the surface is the integral

[tex]\int_S \vec B \cdot \hat n dA[/tex]

where [itex]\hat n[/itex] is a unit vector normal to the element of area dA.

From your description I don't have a clear picture of the geometry.
 
Tide said:
The magnetic flux through the surface is the integral

[tex]\int_S \vec B \cdot \hat n dA[/tex]

where [itex]\hat n[/itex] is a unit vector normal to the element of area dA.

From your description I don't have a clear picture of the geometry.
Me neither.I saw this problem 2 hours ago,but i couldnt' figure out the geometry and how would flux definition and Ampère's law fit in.Let's hope (for his sake) he comes up with a drawing or with the original text.

EDIT:Maybe i got it.He's obviously using cylindrical coordinates and that domain should be a rectangle perpendicular to the OXY plane with one of the sides lying in the OXY plane.So i guess,be should find that,since magnetic field lines are perpendicular to the rectangle,the angle between the magnetic field and \vec<n should be zero.At constant z,the field is varying inversly proportional with "r" as stated by Ampèere's law.So the surface integral would splin in 2,the integral along the "z" gives the magnitude of "z" and along "r" smth about natural logarithm.
I guess that does it.Yet where does the XY angle "theta" come in...??Or am i missing something??Like a different from pi over 2 angle between the field and the rectangle??Anyway...Tide,i let u give your opinion.
 
Last edited:
Dexter,

That makes sense. I think I'll wait for hd28cw to offer clarification!
 

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