KinEqn1_vat
One-dimensional motion with constant acceleration is described by the equation $v_2=v_1 + a (t_2-t_1)$, where $v_2$ is the velocity at time $t_2$, $v_1$ is the velocity at time $t_1$, and $a$ is the acceleration.
KinEqn2_dvt
One-dimensional motion with constant acceleration is described by the equation $x_\text{2}=x_\text{1} + \frac{1}{2} (v_\text{1}+v_\text{2}) (t_\text{2}-t_\text{1})$, where $x_\text{2}$ is the position at time $t_\text{2}$, $x_\text{1}$ is the position at time $t_\text{1}$, $v_\text{2}$ is the velocity at time $t_\text{2}$, and $v_\text{1}$ is the velocity at time $t_\text{1}$.
KinEqn3_dv_plus_at^2
One-dimensional motion with constant acceleration is described by the equation $x_2=x_1 + v_1 (t_2-t_1)+\frac{1}{2} a (t_2-t_1)^2$, where $x_2$ is the position at time $t_2$, $x_1$ is the position at time $t_1$, $v_1$ is the velocity at time $t_1$, and $a$ is the acceleration.
KinEqn4_2adv^2
One-dimensional motion with constant acceleration is described by the equation $v_2^2=v_1^2 + 2 a (x_2-x_1)$, where $v_2$ is the velocity at time $t_2$, $v_1$ is the velocity at time $t_1$, $a$ is the acceleration, $x_2$ is the position at time $t_2$, and $x_1$ is the position at time $t_1$.
KinEqn5_dv_minus_at^2
One-dimensional motion with constant acceleration is described by the equation $x_2=x_1 + v_2 (t_2-t_1)-\frac{1}{2} a (t_2-t_1)^2$, where $x_2$ is the position at time $t_2$, $x_1$ is the position at time $t_1$, $v_2$ is the velocity at time $t_2$, and $a$ is the acceleration.
