Siła ciężkości, siła sprężystości i siła tarcia

$F_{g} = G \frac{m_{1} \cdot m_{2}}{r^{2}}$

$\vec{γ} = \frac{{\vec{F}}_{g}}{m}$

$E_{p} = - G \frac{m_{1} \cdot m_{2}}{r}$

$Δ E_{p} = m \cdot g \cdot Δ h$

$v_{I} = \sqrt{\frac{G \cdot M_{z}}{R_{z}}} = 7,9 \frac{km}{s}$ $v_{II} = \sqrt{\frac{2 \cdot G \cdot M_{z}}{R_{z}}} = 11,2 \frac{km}{s}$

$\frac{{T_{1}}^{2}}{{R_{1}}^{3}} = \frac{{T_{2}}^{2}}{{R_{2}}^{3}} = const$

${\vec{F}}_{s} = - k \cdot \vec{x}$

$E_{pot} = \frac{1}{2} k \cdot x^{2}$

$T_{k} = μ_{k} \cdot F_{N}$

$T_{s} \leq μ_{s} \cdot F_{N}$