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3.2.2Dynamics, forces and pressure

Terminal Velocity

5 min read 10 parts Lesson 10 of 24 1 quiz

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3.2.2 Terminal Velocity — AS PHYSICS 9702 notes: Explain the stages of a fall with drag, the shape of the velocity-time graph and the idea of terminal velocity.With no air resistance, as on the Moon — the only force is weight, the resultant force equals weight and the body accele…

  • With air resistance, as on Earth
  • The body accelerates according to F = ma
  • When drag equals weight
  • At terminal velocity the resultant force is zero
  • In symbols (air, upthrust ignored)
  • If drag is kv2

Section 1 of 10Free fall with and without air resistance

1With no air resistance, as on the Moon
  • With no air resistance, as on the Moon the only force is weight, the resultant force equals weight and the body accelerates at g.
2With air resistance, as on Earth
  • With air resistance, as on Earth weight is greater than drag at first, so the resultant force is in the direction of motion.
3The body accelerates according to F = ma
  • The body accelerates according to F = ma as velocity increases the drag increases and the acceleration decreases.
4When drag equals weight
  • When drag equals weight the resultant force is zero and the body falls at constant velocity.

Section 2 of 10Terminal velocity

Terminal velocity
Terminal velocity
Terminal velocity the constant maximum velocity reached when the resistive forces balance the weight.
At terminal velocity the resultant force is zero
  • At terminal velocity the resultant force is zero so by the first law the acceleration is zero.
In symbols (air, upthrust ignored)
  • In symbols (air, upthrust ignored) mg = Fd at v = vt.
If drag is kv2
  • If drag is kv2 vt = √(mg ÷ k).
A heavier object, or a smaller area or more streamlined shape (smaller k)
  • A heavier object, or a smaller area or more streamlined shape (smaller k) has a higher terminal velocity.

Section 3 of 10Stages of the fall

1
At release (v = 0) there is no drag, the resultant force is the weight and the acceleration is g.
2
As v increases the drag increases, so the resultant force (weight minus drag, minus upthrust in a liquid) decreases.
3
The object keeps speeding up, but more slowly, as the acceleration decreases.
4
At terminal velocity drag (plus upthrust) equals weight, so the resultant force is zero, a = 0 and v is constant.

Section 4 of 10The velocity-time graph

The graph starts at the origin
  • The graph starts at the origin with gradient g = 9.8 m s-2.
The gradient decreases steadily
  • The gradient decreases steadily showing the acceleration falls from g toward zero.
The graph levels off to a horizontal line
  • The graph levels off to a horizontal line at the terminal velocity, approached asymptotically.
The gradient at any point
  • The gradient at any point is the acceleration, found with a tangent.
The area under the graph
  • The area under the graph gives the distance fallen.

Section 5 of 10A skydiver's two terminal velocities

1Arms and legs spread
  • Arms and legs spread terminal speed about 55 m s-1.
2After the parachute opens
  • After the parachute opens the area is much larger, so drag at 55 m s-1 far exceeds the weight.
3The resultant force is upward
  • The resultant force is upward so the skydiver decelerates and the drag falls as the speed falls.
    • (upward acceleration)
4Drag equals weight again at a much lower terminal velocity
  • Drag equals weight again at a much lower terminal velocity about 5 m s-1, which allows a safe landing.
5The skydiver does not move upwards when the parachute opens
  • The skydiver does not move upwards when the parachute opens they decelerate to a lower terminal velocity.
6A more massive skydiver of the same shape
  • A more massive skydiver of the same shape has a larger terminal velocity, so should jump later than a lighter skydiver if they want to meet.

Section 6 of 10Falling in a liquid

Falling in a liquid
Three forces act on a sphere in a viscous liquid
  • Three forces act on a sphere in a viscous liquid weight mg down, upthrust U up and drag Fd up.
At terminal velocity mg = U + Fd.
Time the sphere between two marks on a tall tube
  • Time the sphere between two marks on a tall tube after it has reached steady speed, to find the terminal velocity.
This method gives the viscosity of liquids such as oil
  • This method gives the viscosity of liquids such as oil a more viscous liquid gives a lower terminal velocity.
A bigger or denser sphere falls faster.

Section 7 of 10Describing the graph precisely

1At the start the speed is zero
  • At the start the speed is zero so there is no drag, the resultant force equals the weight and the acceleration is g.
2As the speed increases the drag increases
  • As the speed increases the drag increases so the resultant force and the acceleration decrease and the gradient decreases.
3When drag equals weight
  • When drag equals weight the resultant force is zero, the acceleration is zero and the graph is horizontal.
4Use the words resultant force and gradient
  • Use the words resultant force and gradient not gravity cancels.

Section 8 of 10More from the specification

More from the specification
Forces acting on falling bodies
  • A body falling through fluid experiences downward gravitational weight opposed by upward drag and buoyancy;
    • resultant force determines acceleration: Fnet = W - Fdrag - Fbuoy.
Attainment of terminal velocity
  • As velocity increases, viscous drag force increases until the sum of upward forces equals downward weight,
  • resulting in zero net force and constant terminal velocity.
Velocity-time graphs of falling objects
  • The gradient of a velocity-time graph represents acceleration;
    • the curve starts with gradient g and flattens asymptotically to a horizontal line at terminal speed.
Fluid resistance drag
  • Fluid resistance drag frictional resistive forces acting on a body moving through a fluid increase in magnitude with higher speeds.
Terminal velocity condition
  • Terminal velocity condition occurs when upward fluid drag forces equal downward weight, causing resultant force and acceleration to become zero.
Streamlining bodies
  • Streamlining bodies aerodynamic shaping reduces fluid drag magnitude,
    • allowing vehicles to reach higher speeds before resistive forces balance driving power.
Driving force
  • Force applied by an engine or motor to produce motion.

Section 9 of 10Key terms

TermMeaning
Terminal velocityThe constant maximum velocity reached when the resistive force equals the weight.
Drag forceA resistive force opposing motion through a fluid.
Resultant forceThe vector sum of the forces on the object, zero at terminal velocity.
UpthrustThe upward force from the fluid on an immersed object.
Free fallFalling under the action of gravity alone.
ViscosityThe resistance of a fluid to flow.
AsymptoteA level that a curve approaches but never reaches.
StreamlinedShaped to reduce drag.

Section 10 of 10Exam technique

1
Saying that at terminal velocity there are no forces — the forces balance and the resultant is zero.
2
Thinking the object stops accelerating because gravity stops acting.
3
Drawing the v-t graph as a straight line then a sharp kink — it is a smooth curve.
4
Forgetting upthrust when the object falls in a liquid.
5
Saying terminal velocity means zero velocity.
Physics 0625 & 9702 SUVAT Mastery Graph Interpretation

Constant Acceleration Equations (SUVAT) & Slopes

v = u + at  |  s = ut + ½at2  |  v2 = u2 + 2as  |  s = ½(u + v)t

  • Displacement-Time Graph: Gradient = Velocity (curve = accelerating).
  • Velocity-Time Graph: Gradient = Acceleration; Area under curve = Distance travelled / Displacement.
  • Free Fall in vacuum: a = g ≈ 9.81 m/s2 downwards (air resistance negligible).