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- https://phys.libretexts.org/Courses/Joliet_Junior_College/JJC_-_PHYS_110/09%3A_A_Physics_Formulary/9.01%3A_Physics_Formulas_(Wevers)/9.1.01%3A_MechanicsClassical mechanics from Newton to Hamilton, Lagrange and Liouville.
- https://phys.libretexts.org/Learning_Objects/A_Physics_Formulary/Physics/01%3A_MechanicsClassical mechanics from Newton to Hamilton, Lagrange and Liouville.
- https://phys.libretexts.org/Courses/Prince_Georges_Community_College/General_Physics_I%3A_Classical_Mechanics/08%3A_Kinematics_in_One_Dimension/8.01%3A_PositionFor one-dimensional motion, we align the x axis with the direction of the motion, and we are free to choose the origin at any place that’s convenient. If a particle is at at position \(x_{1}\) at some...For one-dimensional motion, we align the x axis with the direction of the motion, and we are free to choose the origin at any place that’s convenient. If a particle is at at position \(x_{1}\) at some time \(t_{1}\), then at position \(x_{2}\) at some later time \(t_{2}\), then the particle has undergone a displacement
- https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Introductory_Physics_II_(1112)/zz%3A_Back_Matter/10%3A_13.1%3A_Appendix_J-_Physics_Formulas_(Wevers)/1.01%3A_MechanicsClassical mechanics from Newton to Hamilton, Lagrange and Liouville.
- https://phys.libretexts.org/Courses/Prince_Georges_Community_College/General_Physics_I%3A_Classical_Mechanics/11%3A_Kinematics_in_Two_or_Three_Dimensions/11.01%3A_Position_Velocity_Accelerationwhere \(\Delta \mathbf{r}=\mathbf{r}_{2}-\mathbf{r}_{1}\) is the difference in the position vectors \(\mathbf{r}_{1}\) and \(\mathbf{r}_{2}\) at two closely spaced times \(t_{1}\) and \(t_{2}\), respe...where \(\Delta \mathbf{r}=\mathbf{r}_{2}-\mathbf{r}_{1}\) is the difference in the position vectors \(\mathbf{r}_{1}\) and \(\mathbf{r}_{2}\) at two closely spaced times \(t_{1}\) and \(t_{2}\), respectively. where \(\Delta \mathbf{v}=\mathbf{v}_{2}-\mathbf{v}_{1}\) is the difference in the velocity vectors \(\mathbf{v}_{1}\) and \(\mathbf{v}_{2}\) at two closely spaced times \(t_{1}\) and \(t_{2}\), respectively.