∣ z − z 0 ∣ = r \left|\text{z} - {\text{z}}_{0}\right| = \text{r} ∣ z − z 0 ∣ = r \left|\text{z} - {\text{z}}_{0}\right| = 2 \text{r}
< b r / > ∣ α − z 0 ∣ = r <br />\left|\alpha - {\text{z}}_{0}\right| = \text{r} < b r / > ∣ α − z 0 ∣ = r \left|1\overset{¯}{\alpha} - {\text{z}}_{0}\right| = 2\text{r}\alpha\overset{¯}{\alpha} = {\left|\alpha\right|}^{2}
< b r / > ∣ α ∣ α ∣ 2 − z 0 ∣ = 2 r <br />\left|\dfrac{\alpha}{{\left|\alpha\right|}^{2}} - {\text{z}}_{0}\right| = 2 \text{r} < b r / > ∣ α ∣ 2 α − z 0 = 2 r \left(\alpha - {\text{z}}_{0}\right) \left(\overset{¯}{\alpha} - {\overset{¯}{\text{z}}}_{0}\right) = {\text{r}}^{2} ⇒ {\left|\alpha\right|}^{2} - {\text{z}}_{0} \overset{¯}{\alpha} - \alpha {\overset{¯}{\text{z}}}_{0} + {\left|{\text{z}}_{0}\right|}^{2} = {\text{r}}^{2}
< b r / > ( α ∣ α ∣ 2 − z 0 ) ( α ¯ ∣ α ∣ 2 − z ¯ 0 ) = 4 r 2 ⇒ ∣ α ∣ 2 ∣ α ∣ 4 − z ¯ 0 α ∣ α ∣ 2 − z ¯ 0 α ∣ α ∣ 2 + ∣ z 0 ∣ 2 = 4 r 2 <br />\left(\dfrac{\alpha}{{\left|\alpha\right|}^{2}} - {\text{z}}_{0}\right) \left(\dfrac{\overset{¯}{\alpha}}{{\left|\alpha\right|}^{2}} - {\overset{¯}{\text{z}}}_{0}\right) = 4 {\text{r}}^{2} ⇒ \dfrac{{\left|\alpha\right|}^{2}}{{\left|\alpha\right|}^{4}} - \dfrac{{\overset{¯}{\text{z}}}_{0} \alpha}{{\left|\alpha\right|}^{2}} - \dfrac{{\overset{¯}{\text{z}}}_{0} \alpha}{{\left|\alpha\right|}^{2}} + {\left|{\text{z}}_{0}\right|}^{2} = 4 {\text{r}}^{2} < b r / > ( ∣ α ∣ 2 α − z 0 ) ( ∣ α ∣ 2 α ¯ − z ¯ 0 ) = 4 r 2 ⇒ ∣ α ∣ 4 ∣ α ∣ 2 − ∣ α ∣ 2 z ¯ 0 α − ∣ α ∣ 2 z ¯ 0 α + ∣ z 0 ∣ 2 = 4 r 2 1 − z 0 α ¯ − z ¯ 0 α + ∣ z 0 ∣ 2 ∣ α ∣ 2 = 4 r 2 ∣ α ∣ 2 1 - {\text{z}}_{0} \overset{¯}{\alpha} - {\overset{¯}{\text{z}}}_{0} \alpha + {\left|{\text{z}}_{0}\right|}^{2} {\left|\alpha\right|}^{2} = 4 {\text{r}}^{2} {\left|\alpha\right|}^{2} 1 − z 0 α ¯ − z ¯ 0 α + ∣ z 0 ∣ 2 ∣ α ∣ 2 = 4 r 2 ∣ α ∣ 2 ⇒ ( ∣ α 2 ∣ − 1 ) + ∣ z 0 ∣ 2 ( 1 − ∣ α ∣ 2 ) = r 2 ( 1 − 4 α 2 ) ⇒ \left(\left|{\alpha}^{2}\right| - 1\right) + {\left|{\text{z}}_{0}\right|}^{2} \left(1 - {\left|\alpha\right|}^{2}\right) = {\text{r}}^{2} \left(1 - 4 {\alpha}^{2}\right) ⇒ ( α 2 − 1 ) + ∣ z 0 ∣ 2 ( 1 − ∣ α ∣ 2 ) = r 2 ( 1 − 4 α 2 ) \left({\left|\alpha\right|}^{2} - 1\right) \left(1 - \dfrac{{\text{r}}^{2} + 2}{2}\right) = {\text{r}}^{2} \left(1 - 4 {\left|\alpha\right|}^{2}\right)
< b r / > ( ∣ α ∣ 2 − 1 ) ( − r 2 2 ) = r 2 ( 1 − 4 ∣ α ∣ 2 ) <br />\left({\left|\alpha\right|}^{2} - 1\right) \left(\dfrac{- {\text{r}}^{2}}{2}\right) = {\text{r}}^{2} \left(1 - 4 {\left|\alpha\right|}^{2}\right) < b r / > ( ∣ α ∣ 2 − 1 ) ( 2 − r 2 ) = r 2 ( 1 − 4 ∣ α ∣ 2 ) ∣ α ∣ 2 − 1 = − 2 + 8 ∣ α ∣ 2 {\left|\alpha\right|}^{2} - 1 = - 2 + 8 {\left|\alpha\right|}^{2} ∣ α ∣ 2 − 1 = − 2 + 8 ∣ α ∣ 2 1 = 7 ∣ α ∣ 2 ⇒ ∣ α ∣ = 1 7 1 = 7 {\left|\alpha\right|}^{2} ⇒ \left|\alpha\right| = \dfrac{1}{\sqrt{7}} 1 = 7 ∣ α ∣ 2 ⇒ ∣ α ∣ = 7 1