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Physics 2211, Spring 2002

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In this work, he proposed three 'laws' of motion: Law 1: An object subject to no external forces ... If m1 and m2 are glued together and the same force F acts ... – PowerPoint PPT presentation

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Title: Physics 2211, Spring 2002


1
Physics 2211 Lecture 8Todays Agenda
  • Newtons Laws (Particle Dynamics)
  • How and why do objects move?

2
(No Transcript)
3
Dynamics
  • Isaac Newton (1643 - 1727) published Principia
    Mathematica in 1687. In this work, he proposed
    three laws of motion
  • Law 1 An object subject to no external forces
    is at rest or moves with a constant
    velocity if viewed from an inertial reference
    frame.

4
Newtons First Law
  • An object subject to no external forces is at
    rest or moves with a constant velocity if viewed
    from an inertial reference frame.
  • If no forces act, there is no acceleration.
  • The following statements can be thought of as the
    definition of inertial reference frames.
  • An IRF is a reference frame that is not
    accelerating (or rotating) with respect to the
    fixed stars.
  • If one IRF exists, infinitely many exist since
    they are related by any arbitrary constant
    velocity vector!

5
Is Atlanta a good IRF?
  • Is Atlanta accelerating?
  • YES!
  • Atlanta is on the Earth.
  • The Earth is rotating.
  • What is the acceleration (centripetal) of Atlanta?
  • T 1 day 8.64 x 104 sec,
  • R RE 6.4 x 106 meters .
  • Plug this in aatl 0.034 m/s2 ( 1/300 g)
  • Close enough to zero that we will ignore it.
  • Atlanta is a pretty good IRF.

6
Newtons Second Law
  • The constant of proportionality is called mass,
    denoted m.
  • This is the definition of mass.
  • The mass of an object is a constant property of
    thatobject and is independent of external
    influences.
  • Force has units of M x L / T2 kg m/s2 N
    (Newton)

7
Newtons Second Law
  • What is a force?
  • A Force is a push or a pull.
  • A Force has magnitude direction (vector).
  • Adding forces is just like adding vectors.

8
Newtons Second Law
  • Again, we can treat the three dimensions
    independently!
  • Suppose we know m and FX , we can solve for aX
    and apply the things we learned about kinematics
    over the last few weeks. For example, if aX is
    constant

9
Example Pushing a Box on Ice.
  • A skater is pushing a heavy box (mass m 100 kg)
    across a sheet of ice (horizontal
    frictionless). She applies a force of 50 N in
    the x-direction. If the box starts at rest,
    what is its speed v after being pushed a distance
    d 10 m ?

10
Example Pushing a Box on Ice.
  • A skater is pushing a heavy box (mass m 100 kg)
    across a sheet of ice (horizontal
    frictionless). She applies a force of 50 N in
    the x-direction. If the box starts at rest,
    what is its speed v after being pushed a distance
    d 10 m ?

v
F
a
m
x
d
11
Example Pushing a Box on Ice.
  • Start with F ma.
  • a F / m.
  • Recall that v2 - v02 2a(x - x0 )
  • So v2 2Fd / m

12
Example Pushing a Box on Ice.
  • Plug in F 50 N, d 10 m, m 100 kg Find v
    3.2 m/s.

13
ExampleForce and acceleration
  • A force F acting on a mass m1 results in an
    acceleration a1.The same force acting on a
    different mass m2 results in an acceleration a2
    2a1.

m1
m2
F
a1
F
a2 2a1
  • If m1 and m2 are glued together and the same
    force F acts on this combination, what is the
    resulting acceleration?

m1
m2
F
a ?
(a) 2/3 a1 (b) 3/2 a1 (c) 3/4
a1
14
ExampleForce and acceleration
  • Since a2 2a1 for the same applied force, m2
    (1/2)m1 !
  • m1 m2 3m1 /2
  • So a (2/3)F / m1

15
Forces
  • We will consider two kinds of forces
  • Empirical (contact) forces
  • This is the most familiar kind.
  • I push on the desk.
  • The ground pushes on the chair...
  • Fundamental (action-at-a-distance) forces
  • Gravity
  • Electric Magnetic (Electromagnetic)

16
Overview of Physics
Laws of Motion Newtons Laws
  • Observables
  • Fundamental (M,L,T,Q)
  • Derived
  • Forces/Fields
  • Fundamental
  • Gravitational
  • Electromagnetic
  • Strong
  • Empirical (Contact)

electroweak
17
Empirical (Contact) Forces(examples)
  • Linear Restoring Force
  • Friction Force
  • Fluid Force

Characterized by variable, experimentally determin
ed constants k, m, b, etc.
These forces are all electromagnetic in origin.
18
Contact forces
  • Objects in contact exert forces.

This is not a universal convention
19
Gravitational Force(only fundamental force well
study this semester)
20
Gravitation Force(Courtesy of Newton)
  • Newton found that amoon / g 0.000278
  • and noticed that RE2 / R2 0.000273
  • This inspired him to propose the Universal Law
    of Gravitation

where G 6.67 x 10 -11 m3 kg-1 s-2
21
Gravitation Force
22
Gravitation Force
  • Near the Earths surface
  • R12 RE
  • Wont change much if we stay near the Earth's
    surface.
  • i.e. since RE gtgt h, RE h RE.

23
Gravitation Force
  • Near the Earths surface...

24
Example gravity problem
  • What is the force of gravity exerted by the earth
    on a typical physics student?
  • Typical student mass m 55kg
  • g 9.8 m/s2.
  • Fg mg (55 kg)x(9.8 m/s2 )
  • Fg 539 N
  • The force that gravity exerts on any object is
    called its weight
  • W 539 N ( 121 lbs.)

25
Newtons Third Law
  • For every action there is an equal and opposite
    reaction.
  • We have already seen this in the case of gravity

26
Newton's Third Law
27
Example of Fuzzy Thinking
28
Example of Good Thinking
  • Consider only forces on the box!
  • Free Body Diagram (next time).

29
ExampleNewtons 3rd Law
  • Two blocks are stacked on the ground. How many
    action-reaction pairs of forces are present in
    this system?

(a) 2 (b) 3 (c) 4
a
b
30
ExampleNewtons 3rd Law
(c) 4
31
Recap of todays lecture
  • Newtons Three Laws (Text 4-1 to
    4-4)
  • Law 1 An object subject to no external forces
    is at rest or moves with a constant velocity if
    viewed from an inertial reference frame.
  • Law 2 For any object,
  • Law 3 Forces occur in pairs
  • For next time Read Chapter 4.5 - 4.7 in Tipler.
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