Forces of a straight wire on a semi-circular wire loop (Magnetism)

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Homework Help Overview

The discussion revolves around the forces acting on a semi-circular wire loop due to an infinitely long straight wire carrying a current. The loop, which also carries a current, is partially surrounded by the straight wire, and participants are exploring the implications of these interactions, particularly focusing on the force exerted on the loop and whether this force induces rotation.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the calculation of forces on different segments of the wire loop and question how these forces relate to the concept of torque and rotation. There is an exploration of the magnetic fields generated by the currents and how they influence the forces acting on the loop.

Discussion Status

The conversation has progressed through various attempts to analyze the forces and their effects. Some participants have offered insights into the relationship between force and torque, while others are questioning the conditions under which rotation would occur. There is an ongoing exploration of the implications of the forces acting through the axis of rotation.

Contextual Notes

Participants are working within the constraints of a homework problem, which may limit the information available for analysis. The discussion includes considerations of how to express magnetic fields in terms of known variables and the geometric relationships relevant to torque calculations.

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Homework Statement


An ideal, infinitely long straight wire carries a current I1 and is partially surrounded by a loop of current as shown below (image attached). The loop has length L, parallel to the infinitely long wire. The loop carries current I2.
A) Calculate the magnitude and direction of the force exerted on the entire loop.
B) Does this force tend to cause rotation of the loop?

Homework Equations


Fwire=ILxB= ILBsinθ (The F, L, and B are all vectors, once you do the cross product they are no longer vectors)

The Attempt at a Solution


A)
Each wire is creating its own magnetic field at the location of the other wire. I broke the semicircular curved wire into 4 segments, labeled them a-d (segments.jpg).
The magnetic field from the infinitely long wire on segment "a" and "c" of the curved semicircular wire loop is everywhere parallel or anti parallel to the current traveling through those segments. Therefore the force on those wires is zero. The only segments that are affected by the infinitely long wire are segments "b" and "d" of our loop. Segment "b" feels a force towards the center of its circular shape (to the right) and segment "d" feels a force to the right.

Fwire d=I1LxB1=I1LB1(i hat direction)
Fwire b=I1LxB1=I1LB1(i hat direction)

So the force exerted on the entire loop is
2[I1LB1(i hat direction)]

B) Not sure how to approach part b, any advice?

Thanks in advanced! As always I appreciate the help!
 

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For part a, the givens are I1, I2, not I1, B1.

For part b, what do you think? How does a force on an object cause it to rotate about an axis? What axis do you think they mean?
 
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haruspex said:
For part a, the givens are I1, I2, not I1, B1.

For part b, what do you think? How does a force on an object cause it to rotate about an axis? What axis do you think they mean?
Hmmm, okay.
So are you saying since it gave me I1 and I2 I need to write my magnetic field in terms of I2?
The equation I am tempted to use if the one in my above post which states Fwire=ILxB. So are you saying write that B in terms of known variables?

The reason I used B1 is because the infinite wire with current I1 creates a magnetic field (which makes sense to label B1) at the position of the loop.

The only thing I can think about rotational motion would be some sort of Torque equation, would this be the right avenue to explore?

Thanks
 
haruspex said:
For part a, the givens are I1, I2, not I1, B1.

For part b, what do you think? How does a force on an object cause it to rotate about an axis? What axis do you think they mean?
I believe I've figured out what you are saying, attempt below:

Fwire b=I2LxB1=I2LB1 (i hat)
Fwire d=I2LxB1=I2LB1 (i hat)

Ftotal=2(I2LB1) (i hat)

B1=Bwire=Magnetic field that wire with current I1 is creating at location of wire 2 (the loop) with current
I2= (μ0I1)/(2πd) (d being distance from one wire to the other)

Ftotal=(2I20I1)/(2πd) (i hat) = (I2I10)/(πd) (i hat)
 
cookiemnstr510510 said:
I believe I've figured out what you are saying, attempt below:

Fwire b=I2LxB1=I2LB1 (i hat)
Fwire d=I2LxB1=I2LB1 (i hat)

Ftotal=2(I2LB1) (i hat)

B1=Bwire=Magnetic field that wire with current I1 is creating at location of wire 2 (the loop) with current
I2= (μ0I1)/(2πd) (d being distance from one wire to the other)

Ftotal=(2I20I1)/(2πd) (i hat) = (I2I10)/(πd) (i hat)
Yes, that's what I think they want.
cookiemnstr510510 said:
The only thing I can think about rotational motion would be some sort of Torque equation
Right. So what torque do these forces exert about the central axis?
 
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haruspex said:
Right. So what torque do these forces exert about the central axis?
τ=Fwire b(R) + Fwire d (R), R=lever arm. I am stuck here.

This is a 3-D shape, both forces are in the positive "i" direction. I would think that at least a component of some force would have to be in the negative j direction (picture attached of my coordinates) for there to be any rotation around the axis, that's just my first thought...
 

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cookiemnstr510510 said:
R=lever arm
The lever arm is the perpendicular distance from the line of action of the force to the axis, i.e., if you follow the line of action of the force, how much does it miss the axis by at its closest approach?
 
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haruspex said:
The lever arm is the perpendicular distance from the line of action of the force to the axis, i.e., if you follow the line of action of the force, how much does it miss the axis by at its closest approach?
I feel like the line of action goes directly through the the axis (axis meaning the infinitely long wire)
 
cookiemnstr510510 said:
I feel like the line of action goes directly through the the axis (axis meaning the infinitely long wire)
Right. So how long does that make the lever arm, and what does that tell you about torque?
 
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  • #10
haruspex said:
Right. So how long does that make the lever arm, and what does that tell you about torque?
The lever arms length would be the radius of curvature, R. But there is no component of force that is perpendicular to the lever arm, so it won't rotate?
 
  • #11
cookiemnstr510510 said:
The lever arms length would be the radius of curvature, R
No. I asked: "if you follow the line of action of the force, how much does it miss the axis by at its closest approach?", and you answered, correctly,
cookiemnstr510510 said:
the line of action goes directly through the the axis
So how much does it miss by?
 
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  • #12
haruspex said:
So how much does it miss by?
It misses it by 0?
 
  • #13
cookiemnstr510510 said:
It misses it by 0?
Right. So what can you say about the torque it exerts about that axis?
 
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  • #14
haruspex said:
Right. So what can you say about the torque it exerts about that axis?
That there is no torque about the axis?
 
  • #15
cookiemnstr510510 said:
That there is no torque about the axis?
Yes!
 
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  • #16
haruspex said:
Yes!
Cool!
So since there is no torque about the axis this means that there is no rotation, correct?
From looking at the problem initially my intuition was that since the force was only in one direction how could there be rotation? Does that logic make sense?
 
  • #17
cookiemnstr510510 said:
since there is no torque about the axis this means that there is no rotation, correct?
Right.
cookiemnstr510510 said:
initially my intuition was that since the force was only in one direction how could there be rotation?
No, that does not follow. Rotations are always in the context of a specified axis. If the net force acts through that axis then there is no torque about it.
But consider observing someone push a trolley past you (from rest). If you take yourself as axis then the force exerted on the trolley does have a torque about you, and indeed the trolley does acquire an angular velocity about you. You might not think of that as rotating about you, because the distance is changing; but technically it does acquire a rotation about you, i.e. a tangential motion, as well as a radial motion.
 
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  • #18
haruspex said:
No, that does not follow. Rotations are always in the context of a specified axis. If the net force acts through that axis then there is no torque about it.
But consider observing someone push a trolley past you (from rest). If you take yourself as axis then the force exerted on the trolley does have a torque about you, and indeed the trolley does acquire an angular velocity about you. You might not think of that as rotating about you, because the distance is changing; but technically it does acquire a rotation about you, i.e. a tangential motion, as well as a radial motion.
Okay, thanks for the insight!
Greatly appreciated!
 

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