Find magnitude of current of 2 wires separated by an angle

AI Thread Summary
The discussion revolves around calculating the current in two parallel wires carrying equal and opposite currents, which are suspended and separated by an angle of 16 degrees due to magnetic forces. Participants explore relevant equations, including the force between parallel wires and the magnetic field generated by a long straight wire. There is confusion regarding the variables used, particularly the charge (q) and the length of the wires, as well as the appropriate application of the equations. The importance of using a Newtonian approach to analyze the forces acting on the wires is emphasized, with suggestions to derive the necessary formulas. Ultimately, the thread concludes without a definitive solution, indicating a need for further clarification on the physics involved.
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Homework Statement


A telegraph consisted of 2 long straight wires carrying currents equal in magnitude but oppositely directed. Each was suspended by a pair of light-weight and inelastic threads that were about 6cm long. When current flowed through the wires, the magnetic force exerted between them caused them to move apart.

Given that the linear mass density of the wire is 40 g/m, find the magnitude of the current in either wire when the angle separating the threads of the device is 16 degrees.

Homework Equations


Here's a pic of the object: http://i.imgur.com/zwZLzPX.png

F = qv x B = qvBsin(theta)

B = U/2∏ * I/R (Due to a long straight wire) (U is the permeability of empty space.)

The Attempt at a Solution



I tried solving for B from the first equation then plugging it into the 2nd then solving for I.

I = FR2pi/qvsin(theta)

But I'm pretty much stuck. I think I'm missing something really simple but not sure. I know I'm going to need to write an expression of the mag field due to the current in a long straight wire and force on a long straight wire carrying some current though.

Any hints would be great :)
 
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Draw a free-body diagram of one of the wires, showing the magnitudes and directions of the forces involved.

Also, you need to dig up the formula for the force between two parallel wires carrying current. (Or you can derive it from F= qv x B and Ampere's law. You've already stated that law).
 
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Yea the right hand rule is a bit confusing but I think I got it.

The force you are talking about is F1 = B2I1L where L is the length (6cm).

And since the current is equal and with this geometry, the forces are equal. As such, both their magnetic fields should be equal.

Also since it's going about an angle as shown, I can use qB = mv/r I think.

All my work has q in it from F=qvBsin(theta)... would I use a charge of a proton for q?
 
I don't think 6 cm is the length of the wire. They are long straight wires, and the cables that hold them up are 6 cm (it's a radius).

You want forces, but ultimitely you'll have forces acting on an object suspended by a string which can rotate from pi -> 2pi.
 
ichivictus said:
Yea the right hand rule is a bit confusing but I think I got it.

The force you are talking about is F1 = B2I1L where L is the length (6cm).
Right. Except L is not 6 cm, as post 2 indicates. L is arbitrary.
And since the current is equal and with this geometry, the forces are equal. As such, both their magnetic fields should be equal.
The forces are always equal, even if the two fields were not.

Also since it's going about an angle as shown, I can use qB = mv/r I think.
All my work has q in it from F=qvBsin(theta)... would I use a charge of a proton for q?

This formula is totally irrelevant. It describes a charge moving circularly in a B field. No motion here.
 
BiGyElLoWhAt said:
I don't think 6 cm is the length of the wire. They are long straight wires, and the cables that hold them up are 6 cm (it's a radius).

You want forces, but ultimitely you'll have forces acting on an object suspended by a string which can rotate from pi -> 2pi.

Oh right, duh.

Alright so I was probably right in thinking it requires the F = qvBsin(theta). Where theta will probably be 16 degrees.

However, that q in that equation confuses me.

So this is what I got now:

F = BIL = mv^2/r = qvBsin(theta)

I = mv^2/(BLR) = qvsin(theta)/L

So I have a velocity in one and that q and velocity in the other... both of which I don't know. I don't think substituting for one variable and inputting to the other would help at all.
 
ichivictus said:
Oh right, duh.

Alright so I was probably right in thinking it requires the F = qvBsin(theta). Where theta will probably be 16 degrees.

However, that q in that equation confuses me.

So this is what I got now:

F = BIL = mv^2/r = qvBsin(theta)

I = mv^2/(BLR) = qvsin(theta)/L

So I have a velocity in one and that q and velocity in the other... both of which I don't know. I don't think substituting for one variable and inputting to the other would help at all.

I think you're missing the point here. The theta in that equation comes from the fact that it's actually ##qv \times B = F##
Its a cross product between the velocity of the CHARGE and the magnetic field its traveling through. You need to do a Newtonian analysis of the situation, but you don't want F=qv×B. You can do that, but you have to sum up the force on every single electron. Theres a better equation that was mentioned in this thread.

What happens when the 6cm wires make a 16 degree angle from the vertical?

what would happen if you spontaneously removed one of the wires from this equilibrium position? What motion would the remaining wire exibit?
 
did you ever find your answer to this problem??
 
Not sure, they just kinda stopped posting.
 
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