01 / CHAPTER 05
Constant-acceleration motion
Derive the familiar one-dimensional equations and know the assumptions behind them.
ANCHOR EQUATION
Constant-acceleration velocity
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.