Variable acceleration: the calculus way
When a is not constant, integrate: v = ∫a dt, x = ∫v dt — with the constants from initial conditions.
In this lesson
- When a is not constant, integrate: v = ∫a dt, x = ∫v dt — with the constants from initial conditions.
a = 6t is not constant — the SUVAT equations die here; calculus takes over.
v(t) = v₀ + ∫a dt; x(t) = x₀ + ∫v dt. When a is a function of x instead, use v dv = a dx (the chain-rule form) — a JEE favourite.
Always write the integration constants explicitly using t = 0 conditions.
Acceleration in the v–x form
Worked example
The acceleration of a body starting from rest is a = 2 m/s² for 4 s, then zero for 2 s. Find its velocity at t = 6 s.
- Area under the a–t graph = change in velocity.
- Area = 2 m/s² × 4 s = 8 m/s (the last 2 s add nothing).
Answer: 8
Transcript (0 min)
WEBVTT 1 00:00:00.000 --> 00:00:05.000 Variable acceleration: the calculus way — FemtoLearn. 2 00:00:05.000 --> 00:00:15.000 When a is not constant, integrate: v = ∫a dt, x = ∫v dt — with the constants from initial conditions.
Practice
Free · 4 questions with full solutions- Q1 · Numerical · difficulty 2/5
The acceleration of a body starting from rest is a = 2 m/s² for 4 s, then zero for 2 s. Find its velocity at t = 6 s.
- Q2 · Numerical · difficulty 2/5
A body moves with v = 10 m/s for 3 s, then v = 5 m/s for 2 s in the same direction. Find the total distance.
- Q3 · Numerical · difficulty 2/5
A body starts from rest with a = 4 m/s². Find the displacement in the 5th second.
- Q4 · MCQ · difficulty 2/5
A particle moves with constant velocity. Which a–t graph describes it?
- A horizontal line at a = 0
- A horizontal line at a = 2 m/s²
- A straight line through the origin
- A parabola