…\end{gathered} kde \begin{gathered} \eta_\text{h}=\frac{4{,}6\cdot h}{L(z_\text{s})}\cdot f_\text{L}(z_\text{s}{,}n_{1,\text{x}})=\frac{4{,}6\cdot3}{104{,}875}\cdot5{,}983=0{,}787 \end{gathered} \begin{gathered} \eta_\text{b}=\frac{4{,}6\cdot b}{L(z_\text{s})}\cdot f_\text{L}(z_\text{s}{,}n_{1,\text{x}})=\frac{4{,}6\cdot31{,}7}{104{,}875}\cdot5{,}983=8{,}319 \end{gathered} \begin{gathered} R_\text{h}=\frac{1}{\eta_\text{h}}-\frac{1}{2\cdot\eta_\text{h}^2}\cdot(1-e^{-2\eta_\text{h}})=\frac{1}{0{,}787}-\frac{1}{2\cdot0{,}787^2}\cdot(1-e^{-2\cdot0{,}787})=0{,}631 \end{gathered} \begin{gathered} R_\text{b}=\frac{1}{\eta_\text{b}}-\frac{1}{2\cdot\eta_\text{b}^2}\cdot(1-e^{-2\eta_\text{b}})=\frac{1}{8{,}319}-\frac{1}{2\cdot8{,}319^2}\cdot(1-e^{-2\cdot8{,}319})=0{,}113 \end{gathered} \begin{gathered} R^2=\frac{\pi^2}{2\cdot0{,}056}\cdot0{,}042\cdot0{,}631\cdot0{,}113=0{,}264 \end{gathered} Frekvence přechodů s kladnou směrnicí, podle B.2 (4) [1]: \begin{gathered}…