As per the Ampere's circuital law,
The integral of magnetic field along a closed curve equals the sum of the electric current passing thorough the cross-section of the closed curve times permeability.
"\\oint \\overrightarrow{B} \\overrightarrow{dl}=\\mu_oI"
Let I current flowing in a current carrying conductor which have the radius r
Current enclosed in a cross section area "\\pi r^2" is "I_{enclosed}=\\dfrac{\\pi r^2}{\\pi a^2}I=\\dfrac{r^2}{a^2}I"
Taking magnetic field integral along the loop,
"\\oint \\overrightarrow{B}\\overrightarrow{dl}=\\overrightarrow{B}.2\\pi\\overrightarrow{ r}"
So, "\\overrightarrow{B}2\\pi r=\\mu_o\\dfrac{r^2}{a^2}I"
"\\overrightarrow{B}=\\mu_o\\dfrac{rI}{2\\pi a^2}"
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