AcademyOne-Dimensional Motion

Academy

Position and Velocity from Calculus

Level 1 - Physics topic page in One-Dimensional Motion.

Principle

Calculus links motion quantities by differentiation and integration. Derivatives describe local rates, while integrals accumulate signed changes over an interval.

Notation

\(x(t)\)
position function
\(\mathrm{m}\)
\(v_x(t)\)
velocity function
\(\mathrm{m\,s^{-1}}\)
\(a_x(t)\)
acceleration function
\(\mathrm{m\,s^{-2}}\)
\(t\)
time
\(\mathrm{s}\)

Method

Velocity is slope
\[v_x(t)=\frac{dx}{dt}\]
Differentiate position to get the local rate of position change.
Acceleration is slope
\[a_x(t)=\frac{dv_x}{dt}\]
Differentiate velocity to get the local rate of velocity change.
Accumulate velocity
\[\Delta x=\int_{t_i}^{t_f}v_x(t)\,dt\]
Signed area under velocity gives displacement.
Accumulate acceleration
\[\Delta v_x=\int_{t_i}^{t_f}a_x(t)\,dt\]
Signed area under acceleration gives velocity change.

The graph below combines the two views: slope turns a position history into velocity, and area under a velocity history gives displacement.

0123450246810tx or vxx(t)vx(t)
Slope connects position to velocity; area under velocity gives displacement.

When velocity changes sign, split an integral before calculating distance; a single signed integral gives displacement.

Rules

These are the compact results from the method above.

Velocity from position
\[v_x(t) = \frac{dx}{dt}\]
Acceleration from velocity
\[a_x(t) = \frac{dv_x}{dt}\]
Displacement from velocity
\[\Delta x = \int_{t_i}^{t_f} v_x(t)\,dt\]
Velocity change
\[\Delta v_x = \int_{t_i}^{t_f} a_x(t)\,dt\]

Examples

Question
For
\[x(t)=t^3-2t\]
find
\[v_x(t)\]
\[a_x(t)\]
and both values at
\[t=2\]
Answer
\[v_x=3t^2-2\]
\[a_x=6t\]
At
\[t=2\]
\[v_x=10\,\text{m s}^{-1}\]
\[a_x=12\,\text{m s}^{-2}\]

Checks

  • Derivatives give instantaneous rates.
  • Integrals give accumulated change.
  • Initial conditions fix constants.
  • Graph area has physical units.