Forces

The Physics Hypertextbook
© 1998-2008 by Glenn Elert -- A Work in Progress
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Discussion

Truth is ever to be found in simplicity,
& not in ye multiplicity & confusion of things.
Isaac Newton. Treatise on the Apocalypse.

The first chapter of this book dealt with the topic of kinematics -- the mathematical description of motion. With the exception of falling bodies and projectiles (which involve some mysterious thing called gravity) the factors affecting this motion were never discussed. It is now time to expand our studies to include the quantities that affect motion -- mass and force. The mathematical description of motion that includes these quantities is called dynamics.

Many introductory textbooks often define a force as "a push or a pull". This is a reasonable informal definition to help you conceptualize a force, but it is a terrible operational definition. What exactly is "a push or a pull"? How would you measure such a thing? Most importantly, how does "a push or a pull" relate to the other quantities already defined in this book?

Physics, like mathematics, is axiomatic. Each new topic begins with elemental concepts, called axioms, that are so simple that they cannot be made any simpler or are so generally well understood that an explanation would not help people to understand them any better. The two quantities that play this role in kinematics are distance and time. No real attempt was made to define either of these quantities formally in this book (so far) and none was needed. Nearly everyone on the planet knows what distance and time mean.

So a force is "a push or a pull". That's a pretty poor definition even for an informal definition. How about we build up the concept of force with real world examples? Here we go …

Isaac Newton (1642-1727) England. Did most of the work during the plague years of 1665 & 1666. Philosophiæ Naturalis Principia Mathematica (The Mathematical Principles of Natural Philosophy) published in 1687 (20+ year lag!) at Halley's expense.

Lex. I.   Law I.
Corpus omne perſeverare in ſtatu ſuo quieſcendi vel movendi uniformiter in directum, niſi quatennus illud a viribus impreſſi cogitur ſtatum suum mutare.   Every body perseveres in its state of rest, or of uniform motion in a right line, unless it is compelled to change that state by forces impressed thereon.
   
Projectilia perſeverant in motibus ſuis, niſi quatenus a reſiſtentia aëris retardantur, & vi gravitatis impelluntur deorſum. Trochus, cujus partes cohærendo perpetuo retrahunt ſeſe a motibus rectilineis, non ceſſat rotari, niſi quatenus ab aëre retardantur. Majora autem planetarum & cometarum corpora motus ſuos & progreſſivos & circulares in ſpatiis minus reſiſtentibus factos conſervant diutius.   Projectiles continue in their motions, so far as they are not retarded by the resistance of the air, or impelled downwards by the force of gravity. A top, whose parts by their cohesion are continually drawn aside from rectilinear motions, does not cease its rotations, otherwise than it is retarded by the air. The greater bodies of the planets and comets, meeting with less resistance in freer spaces, persevere in their motions both progressive and circular for a much longer time.

(Newton, interpreted by Elert)

An object at rest tends to remain at rest and an object in motion tends to continue moving with constant velocity unless compelled by a net external force to act otherwise.

This rather complicated sentence says quite a bit. A common misconception is that moving objects contain a quantity called "go" (or something like that -- in the old days they called it "impetus") and they eventually stop since they run out of "go".

If no forces act on a body, its speed and direction of motion remain constant.

Motion is just as natural a state as is rest.

Motion (or the lack of motion) doesn't need a cause, but a change in motion does.

Definitio. III.   Definition III.
Materiæ vis insita est potentia resistendi, qua corpus unumquodque, quantum in se est, perseverat in statu suo vel quiescendi vel movendi uniformiter in directum.   The vis insita, or innate force of matter, is a power of resisting, by which every body endeavours to persevere in its present state, whether it be of rest, or of moving uniformly forward in a right line.
 
     
Definitio. IV.   Definition IV.
Vis impressa est actio in corpus exercita, ad mutandum ejus statum vel quiescendi vel movendi uniformiter in directum.   An impressed force is an action exerted upon a body, in order to change its state, either of rest, or of moving uniformly forward in a right line.
     
Consistit hæc vis in actione sola, neque post actionem permanet in corpore. Perserverat enim corpus in statu omni novo per solam vim inertiæ. Est autem vis impresa diversarum originum, ut ex ictu, ex pressione, ex vi centripeta.   This force consists in the action only; and remains no longer in the body when the action is over. For a body maintains every new state it acquires, by its vis inertiæ only. Impressed forces are of different origins as from percussion, from pressure, from centripetal force.

In general, inertia is resistance to change. In mechanics, inertia is the resistance to change in velocity or, if you prefer, the resistance to acceleration.

In general, a force is an interaction that causes a change. In mechanics, a force is that which causes a change in velocity or, if you prefer, that which causes an acceleration.

When more than one force acts on an object it is the net force that is important. Since force is a vector quantity, use geometry instead of arithmetic when combining forces.

External force: For a force to accelerate an object it must come from outside it. You can't pull yourself up by your own bootstraps. Anyone who says you can is literally wrong.

Summary


Some Common Forces
name/symbol(s) when/where direction
weight W, Fg due to gravity down
normal N, Fn surfaces in contact normal to surface
friction ƒ, Fƒ surfaces in contact tangent to surface
tension T, Ft strings, ropes, cables, etc along the axis
elasticity Fs, Fe springs, elastic bands, etc. along the axis
buoyancy B, Fb immersed in a fluid up
drag R, D, Fd moving through a fluid opposite velocity of object
lift L moving through a fluid perpendicular to flow
thrust T pushing a fluid opposite velocity of fluid

Problems

practice

  1. Draw a free body diagram of …
    1. a book lying on a level table.
    2. a person floating in still water.
    3. a wrecking ball hanging vertically from a cable.
    4. a helicopter hovering in place.
    Solutions …
    1. Answer it.
    2. Answer it.
    3. Answer it.
    4. Answer it.
  2. Draw a free body diagram of a child pushing a wagon on level ground.
    Solution …
    • Answer it.
  3. Write something different.
    • Answer it.
  4. Write something completely different.
    • Answer it.

conceptual

  1. Draw a free body diagram for each of the following situations …
    1. a car that …
      1. accelerates forward,
      2. cruises with a constant velocity, and then
      3. brakes to a stop
    2. a passenger in an elevator that …
      1. ascends from the lobby,
      2. cruises upwards, and then
      3. slows to a stop at the 35th floor
    3. a passenger in an elevator that …
      1. descends from the 35th floor,
      2. cruises downwards, and then
      3. slows to a stop at the lobby
    4. an airplane that …
      1. climbs to cruising altitude,
      2. cruises horizontally, and then
      3. descends to a landing …
      all with a constant velocity
    5. a child pulling a sled by a rope
    6. a home owner pushing a lawn mower
    7. a stationary crate on a ramp inclined 30° to the horizontal
    8. a child pushing a wagon up a ramp inclined 30° to the horizontal
    9. a laboratory pendulum held at an angle …
      1. before and
      2. after …
      being released by a student
  2. The physicist and author Dr. John Fontanella in the first chapter of his book The Physics of Basketball claims to have identified "The Final Four". It's more than just a clever reference for fans of college basketball in the US. Mr. Fontanella has identified the four forces that affect the trajectory of a basketball. Determine these four forces and draw a free body diagram for a basketball as it leaves the hands of a player throwing a free throw. Assume a launch angle of 51° with backspin -- an initial condition that Dr. Fontanella says "results in the softest shot".

worksheets

  1. The Physics Teacher has published several articles containing free body diagram worksheets. They are available free to members of the American Association of Physics Teachers (AAPT). Everyone else has to pay.
    1. Free-body diagrams revisited — I. James E. Court. The Physics Teacher. Vol. 37, No. 7 (October 1999): 427-433. Note: pages 428-431 are relevant to this topic.
    2. Exercises in drawing and utilizing free-body diagrams. Kurt Fisher. The Physics Teacher. Vol. 37, No. 7 (October 1999): 434-435.
    3. Free-body diagrams. James E. Court. The Physics Teacher. Vol. 31, No. 2 (February 1993): 104-108. Note: Questions 1-19 are relevant to this topic.

Resources


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