Consider a body moving in a straight line with constant acceleration aa. Between two events A and B, four equations hold, each of which links three of the four kinematic quantities.

Equations of uniformly accelerated motion

sBsA=vA(tBtA)+12a(tBtA)2s_B - s_A = v_A\,(t_B - t_A) + \frac{1}{2}\,a\,(t_B - t_A)^2 vBvA=a(tBtA)v_B - v_A = a\,(t_B - t_A) vA+vB2=sBsAtBtA\frac{v_A + v_B}{2} = \frac{s_B - s_A}{t_B - t_A} vB2vA2=2a(sBsA)v_B^2 - v_A^2 = 2\,a\,(s_B - s_A)

The way to use them is always the same: look at which data are known and choose the equation that contains a single unknown. Here is what each one links:

What each equation links

  • displacement: links ss, vAv_A, aa, tt;
  • velocity: links vv, aa, tt;
  • average velocity: links ss, vAv_A, vBv_B, tt;
  • time-free: links vv, aa, ssno tt!

The last equation, vB2vA2=2a(sBsA)v_B^2 - v_A^2 = 2a(s_B - s_A), is particularly valuable: it is the only one in which time does not appear. When time is not known and is not of interest, it allows velocity, acceleration and displacement to be linked directly without having to calculate time as an intermediate step.

Topics: Kinematics Concepts: Uniformly accelerated motion Skills: Symbolic setup

Related exercises: Carlo’s journey · Stopping distance (reaction and braking) · Proof of the time-free equation