Magnetic field outside a solenoid crossed by a current.

AI Thread Summary
The discussion centers on calculating the magnetic field outside a solenoid with 320 turns of wire and a current of 4.20 A. The student initially struggles with integrating the relevant equations, particularly the Biot-Savart Law and Ampère's Law, to find the magnetic field at a distance along the z-axis. Clarification is provided that "axial distance" refers to measuring from the center of the solenoid. The student derives the magnetic field formula for a single coil and then extends it to the solenoid, ultimately simplifying it for the case where z is much greater than the radius. The final step involves solving for z using the known magnetic field strength of 5.0 μT.
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Homework Statement


A student makes an electromagnet by winding 320 turns of wire around a wooden cylinder of diameter 4,80 cm. The coil is connected to a battery producing a current of 4.20 A in the wire. At what axial distance z>>d will the magnetic field of this dipole be 5.0 μT?

Homework Equations


Biot-Savard Law: (in vector form) B=(μ/4π) i(L x u)/r^2
Maybe Ampère's Law: ∫Bds=μi

The Attempt at a Solution


Unfortunately I can't even imagine how to integrate...
I tried by using Ampère's Law on a circular path around the solenoid. I mean: imagine the solenoid and an imaginary circumference that lays on the same plane of the coils, then inside this circumference there's the current i. I actually treated it as a straight wire because the result is the same and it's wrong...

mhh, help?
 
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Well... I did it...
I got confused by "the axial distance", it meant measuring the distance along the z axis starting from the center of the coil (solenoid).
Let's start from the general formula for a circular wire carrying a current i, B=\frac{µ_{0}iR^{2}}{2\left( R^{2}+z^{2} \right)^{\frac{3}{2}}}. Then, we approximate this formula to the case z>>R, so that B=\frac{µ_{0}iR^{2}}{2z^{3}}. This is the result for a singular coil, our solenoid is made by 320 coils whose magnetic dipole we can know. So, I get to B=\frac{µ_{0}i\pi R^{2}}{2\pi z^{3}}=\frac{µ_{0}i}{2\pi }\frac{Nµ}{z^{3}}. From here it's easy to get z because we know B.
 
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