Changing velocity on a plane
Displacement and velocity for motion on a horizontal plane, finding change in velocity by vector subtraction when the direction changes, average acceleration in two dimensions, and why turning at constant speed is acceleration.
Drive round a roundabout at a steady 30 km/h and the speedometer needle never moves. You are still accelerating the whole way round, and your coffee knows it. Velocity has a direction, and changing direction changes velocity.
In a straight line, the change in velocity is just $v - u$ with signs. When the direction changes on a plane, $v - u$ has to be done as a vector subtraction. This page shows how, and how to get the average acceleration from it. It's also the starting point for circular motion in Year 12.
Change in velocity
$$\Delta\vec v = \vec v - \vec u = \vec v + (-\vec u)$$Method for a vector diagram:
- Draw $\vec v$.
- From its head, draw $-\vec u$ (same length as $\vec u$, opposite direction).
- $\Delta\vec v$ goes from the tail of $\vec v$ to the head of $-\vec u$.
Then the average acceleration is in the same direction as $\Delta\vec v$:
$$\vec a_{\text{avg}} = \frac{\Delta\vec v}{\Delta t}$$A car travelling north at 15.0 m s⁻¹ turns a corner and is then travelling west at 15.0 m s⁻¹. The turn takes 4.0 s. Find the change in velocity and the average acceleration.
A tennis ball hits a wall at 8.0 m s⁻¹ east and rebounds at 6.0 m s⁻¹ west. It is in contact with the wall for 0.050 s. Find its average acceleration.
Using components instead
For awkward angles, find $\Delta v_x = v_x - u_x$ and $\Delta v_y = v_y - u_y$ separately, then recombine with Pythagoras and inverse tan. This is the same component method as 1F, applied to the subtraction.
A yacht sailing at 6.0 m s⁻¹ on a bearing of 000° changes to 8.0 m s⁻¹ on a bearing of 060° over 20 s. Find its average acceleration.
Displacement on a plane
Displacement on a plane follows the same rules. Add each leg of a journey as a vector, and average velocity is total displacement ÷ total time, in the direction of the displacement. For example, a car driving round three-quarters of a circular track of radius 50 m has travelled $\tfrac34 \times 2\pi(50) = 236$ m, but its displacement is a chord of length $\sqrt{50^2 + 50^2} = 70.7$ m.
- Choose 90° left turn. Check: Δv is 21.2 m/s towards 225° and the average acceleration is 5.30 m/s², with no change in speed.
- Choose U-turn (10 m/s north to 10 m/s south in 6 s). Why is the acceleration 3.33 m/s² south, when the speed is the same at the start and the end?
- Choose Ball bouncing off a wall: 280 m/s² west. Increase the time to 0.10 s. What happens to the acceleration?
- Use the sliders for the yacht example: 6 m/s at 000° to 8 m/s at 060° in 20 s. Check 7.2 m/s and 0.36 m/s².
- Keep the speed fixed at 15 m/s and make the turn sharper and sharper. How does |Δv| change?
Test yourself
A car goes round a bend at a constant 20 m s⁻¹. Which statement is correct?
The direction changes, so the velocity changes; the size stays at 20 m s⁻¹.
A puck moving at 4.0 m s⁻¹ east is hit and moves off at 3.0 m s⁻¹ north. Its change in velocity is
$\Delta\vec v = 3.0$ N $+ 4.0$ W, size 5.0 m s⁻¹. Angle from north: $\tan^{-1}(4.0/3.0) = 53°$ towards the west.
A ball hits a floor at 5.0 m s⁻¹ downwards and bounces up at 4.0 m s⁻¹. Contact lasts 0.020 s. The average acceleration during contact is
Up positive: $\Delta v = 4.0 - (-5.0) = 9.0$ m s⁻¹, so $a = 9.0 / 0.020 = 450$ m s⁻² up.
The average acceleration of an object always points in the direction of
$\vec a_{\text{avg}} = \Delta\vec v / \Delta t$, and $\Delta t$ is a positive scalar.
Label the car turning the corner and its vector diagram.
Does the velocity change?
Change in velocity is found by vector : $\vec v - \vec u$. On a diagram, reverse $\vec u$ and add it to $\vec v$ head to . Average acceleration has the same direction as the change in . An object moving at constant speed around a bend is .
A cyclist travelling at 6.0 m s⁻¹ east turns and travels at 8.0 m s⁻¹ south. The turn takes 2.5 s. Using a vector diagram, calculate the cyclist's average acceleration, and explain why it is not $(8.0 - 6.0)/2.5$.
$\Delta\vec v = \vec v + (-\vec u)$: 8.0 m s⁻¹ south plus 6.0 m s⁻¹ west, at right angles.
$|\Delta\vec v| = \sqrt{8.0^2 + 6.0^2} = 10$ m s⁻¹. Its angle from south is $\tan^{-1}(6.0/8.0) = 37°$ towards the west, so S37°W (bearing 217°).
$a = 10 \div 2.5 = 4.0$ m s⁻², on a bearing of 217°.
$(8.0 - 6.0)/2.5 = 0.8$ m s⁻² only uses the change in speed. Velocity is a vector, and the cyclist's direction changed by 90°, so the velocity changed by much more than the speed did.
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