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01 / CHAPTER 05

Constant-acceleration motion

Derive the familiar one-dimensional equations and know the assumptions behind them.

Kinematics: original course diagram
A visual model for this course. Read it as a prompt for the assumptions behind the chapter.

ANCHOR EQUATION

Constant-acceleration velocity

v=v0+at

In symbols: v = v₀ + at

This is the slope-based companion to the position equation.

Constant acceleration comes from equal velocity changes

Constant acceleration means velocity gains the same vector increment in every equal time interval. It is an approximation, not a universal property of motion; it works when the net force is effectively constant for the interval of interest.

Integrate once, then again

Start with a = dv/dt constant. Rearranging gives dv = a dt; integrating from 0 to t gives v − v₀ = at, hence v(t) = v₀ + at. Since v = dx/dt, integrate dx = (v₀ + at)dt from 0 to t: x − x₀ = v₀t + ½at². The factor ½ appears because velocity grows linearly, so its average over the interval is (v₀ + v)/2 = v₀ + ½at.

A car with v₀ = 5.0 m/s and a = 2.0 m/s² travels in 4.0 s: v = 13 m/s and Δx = 5(4) + ½(2)(16) = 36 m. Units check: m/s·s and m/s²·s² both give metres.

When the formula stops being exact

The equations require one-dimensional motion with acceleration constant in time. If a depends on x or v, integrate the actual function instead. If acceleration varies only mildly, the formula may still be a useful local estimate, but the error grows with the interval.

Work it: A train moving at 18 m/s brakes at −1.5 m/s². Derive its stopping time from v = 0 and its stopping distance from x(t), then check the distance using average velocity.