Solve for Q
Q=4\pi E\epsilon _{0}\epsilon _{α}r^{2}
\epsilon _{α}\neq 0\text{ and }r\neq 0\text{ and }\epsilon _{0}\neq 0
Solve for E
E=\frac{Q}{4\pi \epsilon _{0}\epsilon _{α}r^{2}}
\epsilon _{α}\neq 0\text{ and }r\neq 0\text{ and }\epsilon _{0}\neq 0
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\frac{Q}{4\pi \epsilon _{0}\epsilon _{α}r^{2}}=E
Swap sides so that all variable terms are on the left hand side.
\frac{1}{4\pi \epsilon _{0}\epsilon _{α}r^{2}}Q=E
The equation is in standard form.
\frac{\frac{1}{4\pi \epsilon _{0}\epsilon _{α}r^{2}}Q\times 4\pi \epsilon _{0}\epsilon _{α}r^{2}}{1}=\frac{E\times 4\pi \epsilon _{0}\epsilon _{α}r^{2}}{1}
Divide both sides by \frac{1}{4}\pi ^{-1}\epsilon _{0}^{-1}\epsilon _{α}^{-1}r^{-2}.
Q=\frac{E\times 4\pi \epsilon _{0}\epsilon _{α}r^{2}}{1}
Dividing by \frac{1}{4}\pi ^{-1}\epsilon _{0}^{-1}\epsilon _{α}^{-1}r^{-2} undoes the multiplication by \frac{1}{4}\pi ^{-1}\epsilon _{0}^{-1}\epsilon _{α}^{-1}r^{-2}.
Q=4\pi E\epsilon _{0}\epsilon _{α}r^{2}
Divide E by \frac{1}{4}\pi ^{-1}\epsilon _{0}^{-1}\epsilon _{α}^{-1}r^{-2}.
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