\(\displaystyle v=\frac{S}{t}\)
\(\displaystyle a=\frac{\Delta v}{\Delta t}\)
\(\displaystyle S=v_0t+\frac{at^2}{2}\)
\(\displaystyle \omega=\frac{\Delta\varphi}{t}\)
\(\displaystyle \Delta\varphi=\omega_0t+\frac{\varepsilon t^2}{2}\)
\(\displaystyle \omega=2\pi\nu\)
\(\displaystyle v=\omega r\)
\(\displaystyle T\cdot\nu=1\)
\(\displaystyle v=v_0\pm gt\)
\(\displaystyle h=v_0t\pm\frac{gt^2}{2}\)
\(\displaystyle v_x=v_0\cos\alpha\)
\(\displaystyle v_{0y}=v_0\sin\alpha\)
\(\displaystyle t_u=\frac{2v_{0y}}{g}\)
\(\displaystyle h_{max}=\frac{v_{0y}^2}{2g}\)
\(\displaystyle S=v_x\cdot t\)
\(\displaystyle \vec a=\vec a_t+\vec a_n\)
\(\displaystyle a_n=\frac{v^2}{r}\)
\(\displaystyle m=\rho V\)
\(\displaystyle a=\frac{F}{m}\)
\(\displaystyle \vec F_1=-\vec F_2\)
\(\displaystyle F_{el}=-k\Delta l\)
\(\displaystyle a=g(\sin\alpha\pm\mu\cos\alpha)\)
\(\displaystyle p=mv\)
\(\displaystyle \Delta p=F\cdot t\)
\(\displaystyle E_k=\frac{mv^2}{2}\)
\(\displaystyle M=F\cdot l\)
\(\displaystyle F_1l_1=F_2l_2\)
\(\displaystyle F_{ish}=\mu N\)
\(\displaystyle N=\frac{A}{t}=F\cdot v\)
\(\displaystyle A=F\cdot S\cdot\cos\alpha\)
\(\displaystyle E_p=mgh\)
\(\displaystyle E_k+E_p=const\)
\(\displaystyle P=m(g-a)\)
\(\displaystyle g=\frac{GM}{R^2}\)
\(\displaystyle v_1=\sqrt{gR}\)
\(\displaystyle v_2=\sqrt{2gR}\)
\(\displaystyle v=x'\)
\(\displaystyle a=v'\)
\(\displaystyle x=A\cdot\sin(\omega t+\varphi_0)\)
\(\displaystyle v=A\omega\cdot\cos(\omega t+\varphi_0)\)
\(\displaystyle a=-x\cdot\omega^2\)
\(\displaystyle v=\lambda\nu\)
\(\displaystyle v=\sqrt{\frac{T}{\rho_{ch}}}\)
\(\displaystyle v=\sqrt{\frac{E}{\rho}}\)
\(\displaystyle \omega=\sqrt{\frac{k}{m}}\)
\(\displaystyle T=2\pi\sqrt{\frac{m}{k}}\)
\(\displaystyle \omega=\sqrt{\frac{g}{l}}\)
\(\displaystyle T=2\pi\sqrt{\frac{l}{g}}\)
\(\displaystyle \Delta l=l-l_0\)
\(\displaystyle \varepsilon=\frac{\Delta l}{l_0}\)
\(\displaystyle k=\frac{ES}{l_0}\)
\(\displaystyle F_A=\rho_s V_b g\)
\(\displaystyle P=\rho gh\)
\(\displaystyle S_1v_1=S_2v_2\)
\(\displaystyle V_b=\frac{\rho_j V_j}{\rho_s}\)
\(\displaystyle p+\frac{\rho v^2}{2}+\rho gh=const\)