All revision notes topics

Variable acceleration in one dimensionEdexcel A-Level Further Maths: Revision notes

Section 1

Calculus and motion

When acceleration is not constant, the suvat equations no longer apply. Use calculus instead: v=dxdt,a=dvdt=d2xdt2.v=\frac{dx}{dt},\qquad a=\frac{dv}{dt}=\frac{d^2x}{dt^2}. Going from acceleration to velocity to displacement means integrating; going the other way means differentiating. Every indefinite integral needs a constant of integration, found from the initial conditions (for example v=9v=9 and x=0x=0 at t=0t=0).

Key termsvariable accelerationconstant of integration
Common mistake

Using v=u+atv=u+at or s=ut+12at2s=ut+\frac12at^2 when acceleration varies. They give wrong answers.

Section 2

Acceleration as a function of time: dv/dt = f(t)

Integrate a=f(t)a=f(t) to get vv, then integrate vv to get xx. Example: a=6t−12a=6t-12, v=9v=9 and x=0x=0 at t=0t=0. v=3t2−12t+9,x=t3−6t2+9t.v=3t^2-12t+9,\qquad x=t^3-6t^2+9t. At t=2t=2: v=−3v=-3 m s⁻¹ and x=2x=2 m. The particle is instantaneously at rest when v=0v=0: 3(t−1)(t−3)=03(t-1)(t-3)=0, so t=1t=1 and t=3t=3. A negative velocity means the particle moves in the negative direction.

Exam tip

Instantaneous rest means v=0v=0, not a=0a=0. Maximum displacement occurs when v=0v=0.

Section 3

Velocity as a function of time: dx/dt = f(t)

If the velocity is given, integrate for displacement and differentiate for acceleration. Trigonometric and exponential functions appear: ∫cos⁡kt dt=1ksin⁡kt\int\cos kt\,dt=\frac1k\sin kt and ∫ekt dt=1kekt\int e^{kt}\,dt=\frac1ke^{kt}. Use radians. Example: v=6cos⁡2tv=6\cos2t, x=1x=1 at t=0t=0. Then x=3sin⁡2t+1x=3\sin2t+1, a=−12sin⁡2ta=-12\sin2t, and the greatest displacement is 4 (when sin⁡2t=1\sin2t=1). Distance travelled is not the same as displacement if the particle reverses.

Section 4

Acceleration as a function of velocity: dv/dt = f(v)

When the acceleration depends on vv, separate the variables: ∫dvf(v)=∫dt\int\frac{dv}{f(v)}=\int dt. Then use the initial condition to find the constant. Example: dvdt=60−v20\frac{dv}{dt}=\frac{60-v}{20} from rest. ∫dv60−v=∫dt20\int\frac{dv}{60-v}=\int\frac{dt}{20} gives −ln⁡(60−v)=t20+c-\ln(60-v)=\frac{t}{20}+c, and v=0v=0 at t=0t=0 gives v=60(1−e−0.05t)v=60\left(1-e^{-0.05t}\right). The speed tends to the limiting speed 60 as t→∞t\to\infty. Example: deceleration 0.02v20.02v^2 from 10 m s⁻¹: ∫dvv2=−0.02∫dt\int\frac{dv}{v^2}=-0.02\int dt, so 1v=0.02t+0.1\frac1v=0.02t+0.1 and v=101+0.2tv=\frac{10}{1+0.2t}.

Key termsseparate the variableslimiting speed
Common mistake

Dropping the minus sign for a deceleration. A deceleration kv2kv^2 means dvdt=−kv2\frac{dv}{dt}=-kv^2.

Section 5

Further forms (A Level Further Maths only)

The full specification also allows acceleration to depend on displacement: vdvdx=f(x)v\frac{dv}{dx}=f(x) or f(v)f(v), and dxdt=f(x)\frac{dx}{dt}=f(x). These use the chain-rule form a=vdvdxa=v\frac{dv}{dx} and are examined in the A2 content. At AS, questions use only dvdt=f(t)\frac{dv}{dt}=f(t), dvdt=f(v)\frac{dv}{dt}=f(v) and dxdt=f(t)\frac{dx}{dt}=f(t).

Section 6

Exam approach

Decide what you are given (a function of tt or of vv) and what is asked. Write the differential equation first, with correct signs. Separate or integrate, include the constant, and use initial conditions straight away. Check your final expression with the initial values. Give answers to 3 significant figures and state units.

That's the notes covered.

Carry on to the next subtopic.

Exam questions on Variable acceleration in one dimension

  1. A particle PP moves in a straight line. At time tt seconds, where t≥0t\ge0, its acceleration is (6t−12)(6t-12) m s⁻² in the positive direction. At t=0t=0, PP is at the origin OO with velocity 9 m s⁻¹ in the positive direction.
    Find the times at which PP is instantaneously at rest.2 marks
  2. A sports car accelerates from rest along a straight, level track. At time tt seconds its velocity is vv m s⁻¹ and its acceleration is 60−v20\frac{60-v}{20} m s⁻².
    Find the time taken for the car to reach 90% of its limiting speed.2 marks
  3. A particle PP moves along the xx-axis. At time tt seconds its velocity in the positive xx-direction is 6cos⁡2t6\cos2t m s⁻¹. At t=0t=0, PP is at the point with coordinate x=1x=1. Angles are in radians.
    Find an expression for xx in terms of tt.3 marks
See the full worksheet

Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).