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Br^{2}=\frac{1}{4}r^{2}\pi ^{-1}\mu _{0}\times \frac{I}{r^{2}}\sin(\alpha )\times 2\pi a
Multiply both sides of the equation by r^{2}.
Br^{2}=\frac{1}{2}r^{2}\pi ^{-1}\mu _{0}\times \frac{I}{r^{2}}\sin(\alpha )\pi a
Multiply \frac{1}{4} and 2 to get \frac{1}{2}.
Br^{2}=\frac{I}{2r^{2}}r^{2}\pi ^{-1}\mu _{0}\sin(\alpha )\pi a
Multiply \frac{1}{2} times \frac{I}{r^{2}} by multiplying numerator times numerator and denominator times denominator.
Br^{2}=\frac{I\sin(\alpha )}{2r^{2}}r^{2}\pi ^{-1}\mu _{0}\pi a
Express \frac{I}{2r^{2}}\sin(\alpha ) as a single fraction.
Br^{2}=\frac{I\sin(\alpha )\pi }{2r^{2}}r^{2}\pi ^{-1}\mu _{0}a
Express \frac{I\sin(\alpha )}{2r^{2}}\pi as a single fraction.
Br^{2}=\frac{I\sin(\alpha )\pi a}{2r^{2}}r^{2}\pi ^{-1}\mu _{0}
Express \frac{I\sin(\alpha )\pi }{2r^{2}}a as a single fraction.
Br^{2}=\frac{I\sin(\alpha )\pi ar^{2}}{2r^{2}}\pi ^{-1}\mu _{0}
Express \frac{I\sin(\alpha )\pi a}{2r^{2}}r^{2} as a single fraction.
Br^{2}=\frac{\pi Ia\sin(\alpha )}{2}\pi ^{-1}\mu _{0}
Cancel out r^{2} in both numerator and denominator.
Br^{2}=\frac{\pi Ia\sin(\alpha )\pi ^{-1}}{2}\mu _{0}
Express \frac{\pi Ia\sin(\alpha )}{2}\pi ^{-1} as a single fraction.
Br^{2}=\frac{\pi Ia\sin(\alpha )\pi ^{-1}\mu _{0}}{2}
Express \frac{\pi Ia\sin(\alpha )\pi ^{-1}}{2}\mu _{0} as a single fraction.
\frac{\pi Ia\sin(\alpha )\pi ^{-1}\mu _{0}}{2}=Br^{2}
Swap sides so that all variable terms are on the left hand side.
\pi Ia\sin(\alpha )\pi ^{-1}\mu _{0}=2Br^{2}
Multiply both sides of the equation by 2.
a\mu _{0}\sin(\alpha )I=2Br^{2}
The equation is in standard form.
\frac{a\mu _{0}\sin(\alpha )I}{a\mu _{0}\sin(\alpha )}=\frac{2Br^{2}}{a\mu _{0}\sin(\alpha )}
Divide both sides by a\sin(\alpha )\mu _{0}.
I=\frac{2Br^{2}}{a\mu _{0}\sin(\alpha )}
Dividing by a\sin(\alpha )\mu _{0} undoes the multiplication by a\sin(\alpha )\mu _{0}.