Topic 4 of 4
Falling with air resistance
A falling body's weight can stay constant while its acceleration changes. As drag grows, the resultant force decreases; at terminal speed the body keeps moving while the forces balance.
Consider a body released from rest in still air. Use a uniform gravitational field, constant mass and negligible buoyancy. Its shape and the surrounding air conditions remain unchanged, and drag increases with its speed relative to the air.
For this fall, choose downward as positive. This differs from the upward-positive convention used for the projectile examples. Let D be the upward drag magnitude:
adown = g - D/m
Unchanged weight, increasing upward drag
One body is released from rest in still air. Weight is constant and buoyancy is neglected. Purple arrows are forces on the body; the separate blue arrow shows velocity.
1. Just released from rest
Acceleration is g downward.
2. Falling faster, still speeding up
Downward acceleration is less than g.
3. Terminal speed
Resultant force = 0; acceleration = 0.
All weight arrows have the same length; the terminal drag arrow has that same length. The middle drag arrow only means smaller than weight, not a specified fraction. Velocity arrows have different units and are not on the force scale.
At terminal speed, kinetic energy stays constant, but gravitational potential energy still decreases and energy continues to enter internal stores of the body and air.
- Just released: relative air speed is zero, so drag is zero in this model. The downward resultant is mg and downward acceleration is g.
- Speed increasing: drag acts upward and grows. It is smaller than weight, so the body still accelerates downward, but its acceleration is less than g.
- Terminal motion: drag balances weight. The resultant and acceleration are zero while the body continues downward at a nonzero constant speed.
For these falling graphs, downward is positive
This convention differs from the upward-positive launch graphs. The same body falls in unchanged still-air conditions. These are qualitative trends, with no numerical time scale or assumed drag formula.
Downward speed approaches a limit
The slope gets smaller as acceleration decreases. The curve approaches terminal speed without crossing above it under these unchanged conditions.
Downward acceleration approaches zero
As upward drag grows towards weight, downward resultant force and acceleration approach zero. Acceleration stays downward throughout this approach.
The curves show approach to a limit, not a measured settling time. Zero acceleration at terminal speed means constant downward velocity, not rest.
The speed-time gradient is the downward acceleration during this downward motion. The curve becomes less steep as drag grows and tends to a horizontal line at terminal speed. The body does not stop there. The unchanged-condition model does not predict a speed overshoot followed by an upward acceleration.
The constant-acceleration equations cannot be used across the whole drag-dominated fall: a = g - D/m changes as D changes. Near terminal motion, acceleration is approximately zero even though gravitational field strength remains nonzero.
Follow the energy as well as the forces
Before terminal speed, decreasing gravitational potential energy supplies both increasing kinetic energy and increasing internal energy of the body and air. The kinetic-energy increase is smaller than the gravitational decrease when energy is dissipated.
At terminal speed, kinetic energy is constant, but the body continues descending. Gravitational potential energy continues to decrease, and energy continues transferring to internal stores. A zero resultant is not zero work by each individual force.
Worked terminal-motion account
Continuing transfer at constant speed
In a supplied model, a body's weight is 600 N and its steady downward speed is 50 m/s. Upward drag is therefore also 600 N.
Power of drag = -600 × 50 = -30000 W = -30 kW
The net kinetic-energy change rate is zero. Gravitational energy decreases at 30 kW, while energy transfers to internal stores of the body and air at the same rate under this model. The two forces' work does not vanish merely because their sum is zero.
Optional check A body of weight 600 N falls at a steady terminal speed of 50 m/s in still air. Buoyancy is negligible. Which energy statement is correct?
If the drag conditions change
Opening a parachute changes the relationship between drag and speed. Immediately after opening, the upward drag may exceed weight while the body is still moving down. The upward resultant slows its downward motion; it does not make velocity reverse instantly.
As speed decreases, drag falls towards a new balance at a lower terminal speed. With downward positive, the slowing stage has negative acceleration. This changed-condition example differs from the earlier approach to terminal speed for an unchanged body.