Resistive Forces
A short lesson with diagrams, a worked example, a problem to try, and a quick check. Then quiz yourself on 5 practice questions.
A drag force grows with speed. For linear drag, F = −bv. A falling object speeds up until drag balances gravity at the terminal speed vT = mg/b. It approaches vT exponentially: v = vT(1 − e−t/τ), with τ = m/b.
1. Falling with drag
2. Solving the differential equation
Separate the variables: dv/(g − bv/m) = dt. Integrate from 0 to v and from 0 to t:
−(m/b) ln(1 − v/vT) = t, which gives v = vT(1 − e−bt/m).
After τ: 63% of vT. After 3τ: 95%. The object never quite reaches vT, but gets as close as you like.
Heavier objects (same shape) fall faster: vT ∝ m for linear drag, ∝ √m for quadratic drag.
3. Example, then try it
A 0.20 kg ball falls with linear drag, b = 0.50 kg/s. Find its terminal speed and time constant.
vT = mg/b = (0.20)(10) ÷ 0.50 = 4.0 m/s.
τ = m/b = 0.20 ÷ 0.50 = 0.40 s.
For that ball, dropped from rest, find its speed at t = 0.40 s and t = 1.2 s, and its acceleration at the moment its speed is 2.0 m/s.
At t = τ = 0.40 s: v = 4.0(1 − e−1) ≈ 4.0(0.63) ≈ 2.5 m/s.
At t = 3τ = 1.2 s: v = 4.0(1 − e−3) ≈ 4.0(0.95) ≈ 3.8 m/s.
At v = 2.0 m/s: a = (mg − bv)/m = (2.0 − 1.0) ÷ 0.20 = 5.0 m/s², half of g.
Answer: 2.5 m/s, 3.8 m/s; 5.0 m/s² at 2.0 m/s.
4. Common mistakes
Two balls with the same size and shape fall with linear drag F = bv. One has twice the mass. How do their terminal speeds compare?
vT = mg/b. Same shape means the same b, so doubling m doubles vT.
Ready to practice?
5 questions on Resistive Forces, each with a hint and an explanation for every wrong answer.
