Magnetic Field of Three Circular loops

In summary, In the first and the second case the plane of the circle is parallel to the straight wire segments, in the third case the plane of the circle is perpendicular to the straight segments. The straight segments are very long in all three cases in both directions.
  • #1
arl146
343
1

Homework Statement


The radius of the circular loop is R = 21.2 cm and the wire carries the same electric current I = 19.3 A in all three cases. In the first and in the second case the plane of the circle is parallel to the straight wire segments, in the third case the plane of the circle is perpendicular to the straight segments. The straight segments are very long in all three cases in both directions.

(i.) What is the size of the magnetic field at the center of the circle in the first case?
(ii.) 2nd case
(iii.) 3rd case

Homework Equations


For the first one I used B= (mu*i) / (2*pi*R) for the straight part and B= (mu*i) / (2R) for the loop. Which at the end I added the two together.

The Attempt at a Solution



First answer is 7.54×10^(-5) T. I got that correct. The 2nd I'm confused about because of the break in the loop and the 3rd I just don't know what to do with it since the loop is positioned differently. For the second wouldn't it be really similar to the first?
 

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  • #2
In the second case, find the direction of the field due to the straight conductor and the loop?
Are they in the same direction?
similarly, what are the directions of the fields in the third case?
 
  • #3
In the 2nd case, yea, wouldn't they be the same? It would be pointing out of the page?
So, in all 3 cases, the straight part's field is pointing out of the page? And in the 3rd case, the loop part is towards like the +y direction?

I ask those all as questions because I'm not very confident in those answers but that's what I'm getting with the right hand rule
 
  • #4
In the 2nd case field due to wire goes into the page and due to the loop fiedl comes out of the page.
In all the case, the field due to the wire is out of the page on left side of the wire and that into the page towards right of the wire.
 
  • #5
I don't get it? how does the 2nd case of the straight wire go into the page?
 
  • #6
arl146 said:
I don't get it? how does the 2nd case of the straight wire go into the page?
If you candider the gap is very small, the direction of the current in the vertical wire is in upward direction.
If you hold it in your right hand pointing your thumb in the direction of the current, field is going into the page in the right side of the wire.
 
  • #7
rl.bhat said:
In all the case, the field due to the wire is out of the page on left side of the wire and that into the page towards right of the wire.

okay i guess i get that, but how come on the loop you wrap your fingers in the direction of the current but on the straight part you use your thumb? just because its in one direction unlike the loop in which is curving? and can you explain this quote a little more i don't understand the left and right side part, is it because the current would go up the wire and come back down it? that confuses me
 
  • #8
can someone help, I am confused on this ?
 
  • #9
In fact you can use the right hand rule for both, straight conductor and the loop.
Consider the straight conductor and the loop separately close to each other. Apply the right hand rule to the points on the straight conductor and loop close to each other. You can see that the fields dut to these points at the center are in the opposite direction.
 
  • #10
im so confused. can you start from the beginning and be like real clear because I am really not following ..
 
  • #11
You can find the field at any point due to a current carrying straight wire by using right hand clasp rule. According to that, thumb indicates the direction of the current in the conductor and the finger tips indicate the direction of the field.
In the current loop, finger tips of the right hand indicate the direction of the current and thumb indicates the direction of the field.
Second method is identical to the first method if you apply the first method to a small section of the loop which you can treat as a straight conductor and sum it up to get the total field at the center.
 
  • #12
oh okay, that makes sense, i thought that's what you were getting at. i still don't understand why you said this "In all the case, the field due to the wire is out of the page on left side of the wire and that into the page towards right of the wire." how can the wire have a different field on the left side and right side, how would you know that, you were talking about the straight wire right? how can it have it both ways? so what now?
 
  • #13
okay, disregard that last post. i completely understand everything now. http://www.matter.org.uk/schools/content/magneticfields/fields_2.html this website helped a bit and reading back over what you said, made a lot of sense. So, in the 2nd case, we said that the B field due to the straight wire is both into and out of the page depending on the side of the wire. We also said for the loop on the 2nd case, that the B field is out of the page. So, the 3rd case, same thing for straight wire but the loop is going straight up. I got all that now. So what do I do next then?
 
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  • #14
Can someone please help me with this problem? much appreciated ! The gap in the second one confuses me a little and the third one it throws me off because of the axis it lays on!
 
  • #15
In the second case, if the straight conductor is very long, you can neglect the gap. And field due to it at the center of the circular coil is μο*I/(2πr). The direction is into the page.
The magnetic field at the center of the circular loop carrying current will be μο*I/(2r) and the direction is out of the page. So the net field will be difference of these fields.
In the third case, the same two fields mentioned above are perpendicular to each other. So find the resultant field.
 
  • #16
I got the second one, stupid mistake that I was doing ! Yea that's where I'm confused, what does that mean if the fields are perpendicular? I wouldn't add/subract them right so what would I do? multiply them or something?
 
  • #17
arl146 said:
I got the second one, stupid mistake that I was doing ! Yea that's where I'm confused, what does that mean if the fields are perpendicular? I wouldn't add/subract them right so what would I do? multiply them or something?
If two vectors X and Y are perpendicular to each other then, the resultant vector R will be written as
R^2 = X2 + Y2
 
  • #18
ohh, yea duhh ... i always over think this stuff. thanks so much, got it !
 

FAQ: Magnetic Field of Three Circular loops

What is a magnetic field?

A magnetic field is an invisible force that surrounds a magnetic material or a moving electric charge. It exerts a force on other magnetic materials or moving electric charges.

How is a magnetic field created?

A magnetic field is created by the movement of charged particles, such as electrons, within a material or electric current. The spinning of electrons creates a magnetic dipole, which is the basic unit of a magnetic field.

What are three circular loops?

Three circular loops refer to three concentric circles that are placed one inside the other, with the same center point. Each loop carries an electric current and creates its own magnetic field.

How do the magnetic fields of three circular loops interact?

The magnetic fields of three circular loops interact with each other through a phenomenon known as superposition. This means that the total magnetic field at any point is the sum of the individual magnetic fields created by each loop.

What are some real-life applications of three circular loops?

Three circular loops are used in various applications such as electric motors, generators, speakers, and MRI machines. They are also used in scientific experiments to study the behavior of magnetic fields and their interactions.

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