Physics 1Motion in One Dimension

Motion Without the Time

v² = v₀² + 2aΔx links speeds and displacement when the time isn't known.

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Sometimes the time is neither given nor wanted: a car's braking distance, a jet's runway length. You could find $t$ first from the constant-acceleration equations, but one more equation skips that step.

Key idea

$v^2 = v_0^2 + 2a\Delta x$ links the speeds and the displacement without the time. It also needs constant acceleration.

Why it works

Start from the area under the straight $v$–$t$ line: a trapezoid, $\Delta x = \tfrac12(v_0 + v)\,t$. The first equation gives $t = \dfrac{v - v_0}{a}$. Substitute: $$\Delta x = \dfrac{(v + v_0)(v - v_0)}{2a} = \dfrac{v^2 - v_0^2}{2a}.$$ Multiply both sides by $2a$ and the time is gone: $v^2 = v_0^2 + 2a\Delta x$.
A car braking from 20 m/s at 5 m/s²: the triangle under the v–t line is the 40 m stopping distance.

Worked examples

Worked example: Stopping distance

A car moving at $25\ \text{m/s}$ brakes at $5\ \text{m/s}^2$. How far does it go while stopping?
  1. Take the motion as positive: $v_0 = 25$, $v = 0$, $a = -5\ \text{m/s}^2$.
  2. $0 = 25^2 + 2(-5)\Delta x$, so $\Delta x = \dfrac{625}{10} = 62.5\ \text{m}$.

Answer: $62.5\ \text{m}$

Worked example: Speed after a stretch

A skier at $4\ \text{m/s}$ speeds up at $2\ \text{m/s}^2$ over $30\ \text{m}$ of slope. Find the final speed.
  1. $$v^2 = 4^2 + 2(2)(30) = 16 + 120 = 136.$$
  2. $v = \sqrt{136} \approx 11.7\ \text{m/s}$.

Answer: about $11.7\ \text{m/s}$

Worked example: Required acceleration

A jet must reach $70\ \text{m/s}$ from rest on a $1{,}400\ \text{m}$ runway. What acceleration does it need?
  1. $70^2 = 0 + 2a(1400)$.
  2. $a = \dfrac{4900}{2800} = 1.75\ \text{m/s}^2$.

Answer: $1.75\ \text{m/s}^2$

The four constant-acceleration equations. Pick the one that leaves out the quantity you neither know nor want.
EquationLeaves out
$v = v_0 + at$$\Delta x$
$\Delta x = v_0 t + \tfrac12 a t^2$$v$
$v^2 = v_0^2 + 2a\Delta x$$t$
$\Delta x = \tfrac12(v_0 + v)\,t$$a$
Because $\Delta x = \dfrac{v_0^2}{2|a|}$ when stopping, doubling the speed makes the braking distance four times as long, not twice. Traffic engineers build that square into stopping-distance tables.

Common mistake

Forgetting the 2 in $2a\Delta x$, or stopping at $v^2$ and forgetting the square root. Also, the square root only gives a size: $v^2 = 36$ means $v = +6$ or $-6\ \text{m/s}$, and you choose the sign from the direction of motion. Check: units of $2a\Delta x$ are $\text{m}^2/\text{s}^2$, the same as $v^2$.

Practice

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Sources and further reading

  • OpenStax College Physics 2e, Section 2.5 Motion Equations for Constant Acceleration in One Dimension
  • OpenStax University Physics Volume 1, Section 3.4 Motion with Constant Acceleration
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