The magnetic field caused by a element of circular wire "dl" can be found as following
"\\displaystyle dB = \\frac{\\mu_0}{4 \\pi} \\frac{I dl}{r^2}"
To find B(z) we need to integrate dB for the whole circle. Vector dB has 2 components relative to z-axis: parallel and perpendicular. Because of circular symmetry, all "dB_\\perp" compensate each other. So field B at any point of z-axis is directed along this axis.
"\\displaystyle dB_z = |dB| \\cos \\beta = |dB| \\frac{R}{R^2+z^2} = \\frac{\\mu I_0}{4 \\pi} \\frac{R}{(R^2+z^2)^{3\/2}} dl"
After integration we get
"\\displaystyle B = \\frac{\\mu I_0}{2 } \\frac{R^2}{(R^2+z^2)^{3\/2}}"
For R=1cm, z=2cm and I = 1 A, the value of B is
"\\displaystyle B = \\frac{1.26 \\cdot 10^{-6}}{2 } \\frac{10^{-4}}{(5 \\cdot 10^{-4})^{3\/2}} = \\frac{1.26 \\cdot 10^{-6}}{2 } \\frac{10^{-4}}{1.11 \\cdot 10^{-5}}=0.57 \\cdot 10^{-5} = 5.7 \\; \\mu T"
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