Uniform and Variable Acceleration: MDCAT Physics notes
Uniform and Variable Acceleration for MDCAT: definitions, direction of acceleration when slowing, equations of motion and free fall with g = 9.8 m/s².
Uniform and variable acceleration
Uniform acceleration: the velocity changes by equal amounts in equal intervals of time, however small the intervals. Its velocity–time graph is a straight line of constant slope.
Variable acceleration: the velocity changes by unequal amounts in equal intervals of time. The v–t graph is a curve; its slope differs from point to point, so the acceleration is changing.
- Average acceleration: $a_{av} = \Delta v/\Delta t$ over a finite interval.
- Instantaneous acceleration: the limit of $\Delta v/\Delta t$ as $\Delta t \to 0$, i.e. the slope of the tangent to the v–t graph at that instant.
- For uniform acceleration, average and instantaneous accelerations are equal.
Direction of acceleration
Acceleration is a vector. Its direction is the direction of the change in velocity, not necessarily the direction of motion.
| Motion | Velocity | Acceleration |
|---|---|---|
| Speeding up along +x | +x | +x |
| Slowing down along +x | +x | −x |
| Speeding up along −x | −x | −x |
| Slowing down along −x | −x | +x |
Rule: when a body slows down, its acceleration points opposite to its velocity. This is called deceleration or retardation; in calculations it enters as a negative value.
Key formulas (uniform acceleration only)
$$v_f = v_i + at$$
$$S = v_i t + \tfrac12 a t^2$$
$$2aS = v_f^2 - v_i^2$$
$$S = \frac{v_i + v_f}{2}\,t$$
For free fall near the Earth, $a = g = 9.8\ \mathrm{m\,s^{-2}}$ downward. A body dropped from rest ($v_i = 0$) falls
$$S = \tfrac12 g t^2 = 4.9\,t^2 \ \text{metres}$$
and has speed $v = gt$ or $v = \sqrt{2gh}$ after falling a height $h$.
Worked examples
1. Starting from rest. A bike starts from rest with uniform acceleration $2\ \mathrm{m\,s^{-2}}$. After 6 s: $v_f = 0 + 2\times6 = 12\ \mathrm{m\,s^{-1}}$; distance $= \tfrac12\times2\times6^2 = 36$ m.
2. Braking. A car moving at $20\ \mathrm{m\,s^{-1}}$ must stop within 25 m. Using $v_f^2 = v_i^2 + 2aS$: $0 = 400 + 2a(25)$, so $a = -8\ \mathrm{m\,s^{-2}}$. The magnitude of deceleration is $8\ \mathrm{m\,s^{-2}}$.
3. Partway through a fall. A ball is released from rest 10 m above the ground. Its speed when it is 5 m above the ground depends only on the height fallen so far, 5 m: $v = \sqrt{2\times9.8\times5} = \sqrt{98} \approx 9.9\ \mathrm{m\,s^{-1}}$. The mass does not matter.
4. Free-fall distance. In 3 s a dropped stone falls $4.9\times3^2 = 44.1$ m.
Common MDCAT traps
- "Unequal changes in velocity in equal times" means variable acceleration, not uniform.
- For a body slowing along −x, acceleration is along +x.
- In free-fall problems use the height actually fallen, not the height above the ground.
- $S = 4.9t^2$ comes from $\tfrac12 g$; do not use $9.8t^2$.
- A changing slope on a v–t graph means changing acceleration, not uniform velocity.
Quick revision
- Uniform acceleration: straight v–t line.
- Variable acceleration: curved v–t line.
- Deceleration: acceleration opposite to velocity.
- $g = 9.8\ \mathrm{m\,s^{-2}}$; dropped body falls $4.9t^2$ m.
- Equations of motion apply only for uniform acceleration.