M3.1 - Further kinematics
- Syllabus
- 2019
- Topic
- M3.1
- Level
- A2
For motion along a straight line, displacement x, signed velocity v and signed acceleration a are linked by derivatives. Choose the form whose independent variable matches the information given; this avoids introducing an unnecessary unknown function.
v=dtdx,a=dtdv=vdxdv
| Information given | Equation to set up | First result after integration |
|---|---|---|
| a=f(t) | dtdv=f(t) | v as a function of t |
| a=f(x) | vdxdv=f(x) | 21v2 as a function of x |
| v=f(x) | dtdx=f(x), so dt=f(x)dx | t as a function of x |
| v=f(t) | dtdx=f(t) | x as a function of t |
The displacement form of acceleration follows from the chain rule:dtdv=dxdvdtdx=vdxdv.Use it when acceleration or velocity is expressed in terms of x. If the required quantity is time and v=f(x), separate variables instead: dt=dx/v(x).
Every indefinite integration needs a constant. Apply a stated condition such as x=x0 and v=v0 at t=t0 only after integrating, or use definite integrals with those values as limits. Keep v signed: a negative velocity represents motion in the negative x-direction, while speed is ∣v∣.
Suppose v=12/(x+2) metres per second and x=1 when t=0. First,a=vdxdv=x+212(−(x+2)212)=−(x+2)3144.At x=4, a=−2/3ms−2. For the elapsed time to reach x=4,t=∫14vdx=∫1412x+2dx=[24x2+6x]14=89 s.The negative acceleration means velocity is decreasing here; the deceleration magnitude is 2/3ms−2.
Check that the final variable matches the question, substitute the initial condition back into the integrated relation, and verify units: v has units ms−1 and a has units ms−2. If a derivation divides by v or by another expression that can be zero, solve on intervals where that division is valid and inspect the zero case separately.
Do not use constant-acceleration formulae when a varies, replace a by dv/dx without the factor v, discard an integration constant, or report a negative acceleration automatically as a positive deceleration. Acceleration and velocity signs must be interpreted together.