Magnetic field in the open loop

AI Thread Summary
To find the magnetic field at a specific point using the Biot-Savart law, it's suggested to divide the wire into segments and analyze the contributions from each segment. The integration variable can be set to theta, simplifying the calculations. It is important to consider the symmetry of the system, as the contributions from opposite sides may cancel out. The limits for the integral should be determined by the geometry of the setup, and in this case, angles from -π/4 to π/4 are appropriate. The discussion emphasizes the need for careful arithmetic to validate any assumptions made during the calculations.
tomfrank
Messages
37
Reaction score
0

Homework Statement


I am trying to find the magnetic field at the point in the middle of the picture can someone give a hint on how to approach the problem?


Homework Equations





The Attempt at a Solution

 

Attachments

  • magne.jpg
    magne.jpg
    4.6 KB · Views: 492
Physics news on Phys.org
Attachments Pending Approval...
 
any help?
 
tomfrank said:

Homework Statement


I am trying to find the magnetic field at the point in the middle of the picture can someone give a hint on how to approach the problem?


Homework Equations





The Attempt at a Solution


The hint is to use the Biot-Savart law... (Hint: it often simplifies the integration to make your variable of integration theta...)
 
you should divide the wire into some parts and find m.f created by these parts.
 
would the left and the right side cancel out...

So I have to do it just for the bottom side?
 
so thus this integral work :

B= (\mu*I)/(4*pi*x)\int between(-pi/4) and (pi/4) of cos (\theta) d\theta
 
tomfrank said:
would the left and the right side cancel out...

So I have to do it just for the bottom side?

I believe so (though I might be wrong). In all cases you should prove it via arithmetic so don't use this shortcut if you are not sure.
 
tomfrank said:
so thus this integral work :

B= (\mu*I)/(4*pi*x)\int between(-pi/4) and (pi/4) of cos (\theta) d\theta

No. Biot-Savart:

<br /> dB = \frac{\mu_0 I}{4 \pi} \frac{dl sin\theta}{r^2}<br />

With \theta is angle between dl and r. imo, you can use symmetry property to make life easier.
 
  • #10
so i stil do not quite get it...does the two side cancel out?

<br /> <br /> dB = \frac{\mu_0 I}{4\pi r^2} {dl sin\theta}<br /> <br />

will the angle be (-pi/4) to (pi/4)
 
  • #11
No. r is changing with theta. Can you find relationship between sin(theta) and r? and between r and x?

About two sides, you can say that they cancel out.
 
  • #12
i see how you are looking at the picture.

basically the

sin (theta) dl = cos (theta') dl

and

1/r^2 = cos^2(theta')/ x^2
when i put all of them in the integral reduce down to

dB = \frac{\mu_0 I}{4\pi x} {dl cos\theta}<br /> <br />

i do not know yet what boundary to use for the integral
 
  • #13
1/r^2 = cos^2(theta')/ x^2

from this, i guess theta and theta' as shown in fig below:

http://img149.imageshack.us/img149/6568/88285645.jpg

is that right?
 
Last edited by a moderator:
  • #14
dB = μo/4π*I*di*sinθ/r^2
where sinθ = x/r = x/sqrt( x^2 + l^2)
Take the limits of integration from -x/2 to +x/2.
 
  • #15
yes the picture with the angle is exactly what I was thinking...what are the limits for the integral angles?
 
  • #16
tomfrank said:
yes the picture with the angle is exactly what I was thinking...what are the limits for the integral angles?

The limits come from the geometry of the diagram. You really should be able to figure that part out.

And on your PM question to me, know, the B-field contributions from the two sides on the left and right do not cancel out.
 
  • #17
i did to -45 to 45...will that work?
 
  • #18
tomfrank said:
i did to -45 to 45...will that work?

Based on your initial drawing, yes.
 
  • #19
thank you
 
Back
Top