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[parent] loop example of Biot-Savart law (Example)

Here we will examine two examples of the Biot-Savart law, one simple and the other more challenging. To begin we will find the magnetic field at the center of a current carrying loop as shown in figure 1

PIC

Figure 1:Figure 1: Current Loop

this setup is the same as the quater loop example of Biot-Savart law where we have

dl × ˆr = dlsin(π∕2)

dl = rd 𝜃

giving us a similar integral, except from 0 to 2 π and the lack of a minus sign since the current is going in the opposite direction so the magnetic field will be out of the web browser

          ∫
     ˆμ0I-   2π
B =  k4πr      d𝜃
            0

taking the integral gives the magnetic field at the center of the loop

     μ0Iˆk
B =  -----
      2r

The second more challenging example is the magnetic field at a point z above the loop as shown in figure 2

PIC

Figure 2:Figure 2: Current Loop

The not so obvious hint is the direction of dB. The cross product of r with dl leads to a vector perpendicular to both of them and as you go around the loop, dB will always be off the z axis by an angle ϕ. This makes all the horizontal components of dB cancel leaving just the vertical so

dl × ˆr = dlcos(ϕ )ˆk

once again the differential is given as

dl = Rd 𝜃

, so the integral to get the magnetic field is

      μ IR  ∫ 2π
B = kˆ-0--2-     cos(ϕ)d𝜃
      4 πr   0

From the geometry of the problem we see that

r2 = R2  + z2

         R
cos(ϕ) = --
          r

this leads to

    √ --2---2-
r =   R  + z

             R
cos(ϕ) =  √--2----2-
           R   + z

substituting these relations into the integral

          μ IR2     ∫ 2π
B  = ˆk-----0------3      d𝜃
      4 π(R2 + z2)2  0

Finally, taking the integral gives us the magnetic field

       μ IR2  ˆk
B  = ---0-------3
     2(R2 +  z2)2

"loop example of Biot-Savart law" is owned by bloftin.
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Cross-references: relations, vector, cross product, magnetic field, Biot-Savart law
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This is version 4 of loop example of Biot-Savart law, born on 2006-01-14, modified 2011-01-18.
Object id is 105, canonical name is LoopExampleOfBiotSavartLaw.
Accessed 11557 times total.

Classification:
Physics Classification41.20.Gz (Magnetostatics; magnetic shielding, magnetic induction, boundary-value problems)
Pending Errata and Addenda
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Discussion
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Question about B-field at center of loop by evanm3 on 2011-01-17 17:15:44
I have a quick question about the answer posted for the magnetic field at the center of a current loop. Everything makes sense up to the final answer, where I believe the factor of pi on the denominator should vanish. When you do the integral of dtheta, from 0 -> 2*pi, you get 2*pi, and thus the two pis cancel out giving (mu-naught*I / 2*r). Please let me know if I am thinking about this properly. Thanks in advance.
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