Magnetic Flux, Equator and flying bullets

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Homework Help Overview

The problem involves calculating the electromotive force (EMF) induced in a bullet shot horizontally at the equator, where the Earth's magnetic field is present. The bullet's speed, dimensions, and the magnetic field strength are provided, with an emphasis on understanding the relationship between motion and magnetic fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Faraday's law and the relationship between magnetic fields and moving charges. There is an exploration of the EMF calculation and the implications of the bullet's direction of travel on the induced EMF.

Discussion Status

Some participants have provided feedback on the calculations and terminology used, while others are questioning the implications of the bullet's direction on the induced EMF. There is an ongoing exploration of the concepts involved, particularly regarding the effects of motion parallel to the magnetic field.

Contextual Notes

Participants are navigating potential confusion regarding the relationship between the Lorentz force and induced EMF, particularly when the bullet travels parallel to the magnetic field. There are also considerations about the assumptions made in the problem setup.

TFM
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Homework Statement



At the equator, the earth’s magnetic field is approximately horizontal, is directed towards the north and has a value of [tex]8 × 10^{-5}[/tex] T.

(i)

Estimate the EMF induced between the top and bottom of a bullet shot horizontally at a target on the equator if the bullet is shot east. Assume the bullet has length of 1 cm, a diameter of 0.4 cm and travels at a speed of 300 m/s (for simplicity, one can assume that the bullet has a square cross-section).


Homework Equations



[tex]\epsilon = -\frac{d\Phi}{dt}[/tex]

[tex]\Phi = \int B da = BHx[/tex]

The Attempt at a Solution



I think I have done this question, but would like to check to see it I have done it correctly...

[tex]\Phi = BHx[/tex]

[tex]\epsilon = -\frac{d\Phi}{dt}[/tex]

[tex]\epsilon = -\frac{dBHx}{dt}[/tex]

B and H are constants:

[tex]\epsilon = -BH\frac{dx}{dt}[/tex]

since:

[tex]\frac{dx}{dt} = v[/tex]

[tex]\epsilon = -BHv[/tex]

we know:

B = [tex]8 × 10^{-5}[/tex]
H = 0.004
v = 300

thus inserting the values I get:

[tex]\epsilon = -9.6 \time 10^{-5}[/tex] Volts

Does this look correct?

TFM
 
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Does this look like the right solution?

TFM
 
Does it look like I have attempted the question in the correct way? Does it look right?

?

TFM
 
Hi TFM,

Your answer looks good to me, although I wouldn't use H as a variable when considering B-fields since it could be confused with the auxillary field H. This question is familar to a hall effect question, although the circumstances are different you get the same final equation. I geuss when it comes down to it though you still have moving charges in a B-field, so in essence it's the same. Odd.
 
Ok that's good. For the second part,

(ii)

What is the EMF if the bullet was traveling South?

I am assuming that the same equation will be used, which should give the same value, since none of the variables appear to have changed. The only real difference is that the bullet is no longer traveling perpendicular, but it does have a perpendicular surface (to the current). Does this sound right?

TFM
 
If the bullet is traveling south then all the charges inside it are also traveling south. The velocity of the charges will be parallel to the magnetic field. What is the force on a charge when moving parallel to a magnetic field?
 
Well the formula is:

[tex]Q(v \times B)[/tex]

which is a cross product, so the force will be 0?

TFM
 
Does this look right? If so, how would this force connect to the EMF force, [tex]\epsilon[/tex]?

TFM
 
note: emf isn't a force.

The two methods (Faraday and Lorentz) should lead to the same answer. However I am now confused, since when the bullet moves south there is still a surface parallel to B (so B.da is non zero) which will sweep out an area and lead to an emf. However the Lorentz force law contradicts this, because it says that since all the charges are now moving parallel to B the force on them must be zero.

Please can someone explain this odd inconsistency? I think I have something obvious mixed up somewhere.
 
  • #10
I think that as the bullet is now traveling parallel to the B-field there will be no change in magnetic flux through any of it's surfaces or open surfaces, since there will be as much B-field going in as there is coming out and it's not cutting any field lines. Does that make sense?
 
  • #11
That does indeed make sense.

TFM
 

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