Linear motion under a variable force

Further Maths · Further Mechanics. The idea in plain words, the rules to remember, the mistake to avoid and a worked example, written and checked by Mega Lecture.

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The idea

When the force on a particle changes with time, position or speed, the acceleration is not constant and the suvat equations cannot be used. Newton's second law, F = ma, now gives a differential equation.

The skill is to write the acceleration in the form that fits the question. Acceleration is dv/dt, and by the chain rule it is also v dv/dx. Choose dv/dt when the question links speed and time. Choose v dv/dx when it links speed and distance.

Then separate the variables, integrate both sides and use the starting values to find the constant. Take one direction as positive and give a resistance a minus sign.

Rules to remember

Common mistake

Students forget the v in v dv/dx and write m dv/dx = F. They also leave out the minus sign on a resistance. Write the equation of motion with signs first, then choose the form of the acceleration.

Worked example

A particle of mass 2 kg starts from rest at the origin and moves along the x-axis. When its displacement is x m, the only force on it is (3x2 + 1) N in the positive x-direction. Find its speed when x = 2.

  1. The force depends on x, so use mv dv/dx = F: 2v dv/dx = 3x2 + 1.
  2. Separate and integrate: ∫2v dv = ∫(3x2 + 1) dx, so v2 = x3 + x + C.
  3. v = 0 when x = 0, so C = 0.
  4. When x = 2: v2 = 8 + 2 = 10, so v = √10 = 3.16.

Answer: 3.16 m s−1 (3 significant figures)

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