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Chapter 11 Simple Harmonic Motion

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Title: Chapter 11 Simple Harmonic Motion


1
Chapter 11Simple Harmonic Motion
2
Hookes Law
Chapter 11
  • One type of periodic motion is the motion of a
    mass attached to a spring.
  • The direction of the force acting on the mass
    (Felastic) is always opposite the direction of
    the masss displacement from equilibrium (x 0).

3
Hookes Law, continued
Chapter 11
  • At equilibrium
  • The spring force and the masss acceleration
    become zero.
  • The speed reaches a maximum.
  • At maximum displacement
  • The spring force and the masss acceleration
    reach a maximum.
  • The speed becomes zero.

4
Hookes Law, continued
Chapter 11
  • Measurements show that the spring force, or
    restoring force, is directly proportional to the
    displacement of the mass.
  • This relationship is known as Hookes Law
  • Felastic kx
  • spring force (spring constant ? displacement)
  • The quantity k is a positive constant called the
    spring constant.

5
The Simple Pendulum
Section 1 Simple Harmonic Motion
Chapter 11
  • A simple pendulum consists of a mass called a
    bob, which is attached to a fixed string.
  • The x component (Fg,x Fg sin q) is the only
    force acting on the bob in the direction of its
    motion and thus is the restoring force.

6
Measures of Simple Harmonic Motion
Chapter 11
7
Simple Harmonic Motion
Chapter 11
8
Period and Frequency
  • Period and frequency are inversely related
  • Any time you have a value for period or
    frequency, you can calculate the other value.

9
Period of a Simple Pendulum in SHM
Chapter 11
  • The period of a simple pendulum depends on the
    length and on the free-fall acceleration.
  • The period does not depend on the mass of the bob
    or on the amplitude (for small angles).

10
Period of a Mass-Spring System in SHM
  • The period of an ideal mass-spring system depends
    on the mass and on the spring constant.
  • The period does not depend on the amplitude.
  • This equation applies only for systems in which
    the spring obeys Hookes law.

11
Wave Motion
Chapter 11
Section 3 Properties of Waves
  • A wave is the motion of a disturbance.
  • A medium is a physical environment through which
    a disturbance can travel. For example, water is
    the medium for ripple waves in a pond.
  • Waves that require a medium through which to
    travel are called mechanical waves. Water waves
    and sound waves are mechanical waves.
  • Electromagnetic waves such as visible light do
    not require a medium.

12
Relationship Between SHM and Wave Motion
Chapter 11
As the sine wave created by this vibrating blade
travels to the right, a single point on the
string vibrates up and down with simple harmonic
motion.
13
Wave Types
  • A wave that consists of a single traveling pulse
    is called a pulse wave.
  • Whenever the source of a waves motion is a
    periodic motion, such as the motion of your hand
    moving up and down repeatedly, a periodic wave is
    produced.
  • A wave whose source vibrates with simple harmonic
    motion is called a sine wave. Thus, a sine wave
    is a special case of a periodic wave in which the
    periodic motion is simple harmonic.

14
Wave Types
Chapter 11
  • A transverse wave is a wave whose particles
    vibrate perpendicularly to the direction of the
    wave motion.
  • The crest is the highest point above the
    equilibrium position, and the trough is the
    lowest point below the equilibrium position.
  • The wavelength (l) is the distance between two
    adjacent similar points of a wave.

v f?
15
Wave Types
Chapter 11
  • A longitudinal wave is a wave whose particles
    vibrate parallel to the direction the wave is
    traveling.
  • A longitudinal wave on a spring at some instant t
    can be represented by a graph. The crests
    correspond to compressed regions, and the troughs
    correspond to stretched regions.
  • The crests are regions of high density and
    pressure (relative to the equilibrium density or
    pressure of the medium), and the troughs are
    regions of low density and pressure.

16
Fig. 21.22, p.675
17
The Electromagnetic Spectrum
Section 1 Characteristics of Light
Chapter 13
18
Crab NebulaX-ray image
19
Crab NebulaOptical image
20
  • The most famous and conspicuous supernova
    remnant. The Crab Nebula is the centuries-old
    wreckage of a stellar explosion, or supernova,
    first noted by Chinese astronomers on July 4,
    1054, and that reached a peak magnitude of -6
    (about four times brighter than Venus). According
    to the Chinese records, it was visible in
    daylight for 23 days and in the night sky to the
    unaided eye for 653 days. Petroglyphs found in
    Navaho Canyon and White Mesa (both Arizona) and
    in the Chaco Canyon National Park (New Mexico)
    appear to be depictions of the event by Anasazi
    Indian artists. The Crab Nebula lies about
    6,300 light-years away in the constellation
    Taurus, measures roughly 10 light-years across,
    and is expanding at an average speed of 1,800
    km/s. Surprisingly, its expansion rate seems to
    be accelerating, driven by radiation from the
    central pulsar. Its luminosity at visible
    wavelengths exceeds 1,000 times that of the Sun

21
Crab NebulaInfrared image
22
Crab NebulaRadio image
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