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Simple Harmonic Motion Chapter 15

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Title: Simple Harmonic Motion Chapter 15


1
Lecture 22

2
Simple Harmonic MotionChapter 15
3
  • A block of mass 1 kg is attached to a spring with
    k100 N/m and free to move on a frictionless
    horizontal surface. At t0, the spring is
    extended 5 cm beyond its equilibrium position and
    the block is moving to the left with a speed of
    1 m/s. What is the displacement of the block as a
    function of time?

4
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5
  • Three 10,000 kg ore cars are held at rest on a
    30o incline using a cable. The cable stretches 15
    cm just before a coupling breaks detaching one of
    the cars. Find (a) the frequency of the resulting
    oscillation of the remaining two cars and (b) the
    amplitude of the oscillation.

6
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7
  • A 10 g bullet strikes a 1 kg pendulum bob that is
    suspended from a 10 m long string. After the
    collision the two objects stick together and the
    pendulum swings with an amplitude of 10o.
  • What was the speed of the bullet when it hit the
    bob?

10o
10 g
v?
8
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9
CO2 molecule
  • Carbon dioxide is a linear molecule. The C-O
    bonds act like springs. This molecule can vibrate
    such that the oxygen atoms move symmetrically in
    and out, while the carbon atom is at rest. The
    frequency of this vibration is observed to be
    2.83x1013 Hz.
  • What is the spring constant of the C-O bond?
  • In which other way can the molecule vibrate and
    at what frequency?
  • If the amplitude is the same, in which mode is
    the energy of the molecule higher?

10
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11
Driven Harmonic Oscillator
  • What happens if you have an oscillator, such as a
    mass on a spring, where an external force is
    acting on the system?
  • Example Motion of a building or bridge during an
    earthquake
  • Essentially all objects have one or more natural
    frequencies that they will oscillate at if they
    are initially displaced from equilibrium
  • Example mass on a spring has a natural frequency
    given by
  • If an oscillating external force is applied with
    angular frequency w close to the natural
    frequency w0, the results can be dramatic

12
Driven Harmonic Oscillator
  • To get motion, use Newtons 2nd law
  • Suppose the external force is sinusoidal
  • Eventually, the objects motion will oscillate
    with frequency ? since thats the frequency of
    the applied force

13
Driven Harmonic Oscillator
  • Solution for driven harmonic oscillator is
    somewhat more complicated than what we have done
    so far in Physics 5
  • With some effort, one can solve the equation of
    motion
  • where the frequency and amplitude are given by

14
Driven Harmonic Oscillator
  • Example Mass on spring
  • Notice how amplitude and phase change as the
    frequency of the external force crosses the
    natural frequency
  • Example Vibrations of a solid object
  • Solid objects typically have one or more natural
    frequencies that they oscillate at
  • If the damping is small, large oscillations occur
    when driven at these natural frequencies
  • These vibrations can be a considerable source of
    stress on the object!

15
Oscillations Summary
  • We get periodic motion when force acts to push
    object back towards equilibrium position
  • Many problems exhibit simple harmonic motion
  • Energy exchanged between kinetic and potential
    energy, total mech. energy unchanged for undamped
    oscillations
  • Correspondence between simple harmonic motion and
    uniform circular motion
  • Amplitude of oscillations decays with a damping
    force
  • Driven oscillations exhibit a resonance at the
    natural frequency
  • (ex Tacoma Narrows bridge collapse video)

16
Fluids Chapter 14
17
Fluids
  • What is a fluid?
  • A substance that flows
  • Examples include liquid, gas, plasma, etc
  • A simple fluid can withstand pressure but not
    shear
  • Density
  • Density
  • Unit kg/m3
  • Examples density of water 1000 kg/m3 air 1.21
    kg/m3
  • A materials specific gravity is the ratio of the
    density of the material to the density of water
    at 4C.
  • What is special about water at 4C?
  • Water is most dense at that temperature.
  • Aluminum has a specific gravity of 2.7 it is
    2.7 times more denser than water at 4C.

18
A table of densities
19
Pressure
  • Pressure
  • Unit pascal (Pa)N/m2
  • Examples 1 atm1.01x105 Pa760 torr14.7 lb/in2
  • Torricelli (torr) is defined as the pressure of
    mm Hg. Blood pressure 70/120 torr
  • At any point in a fluid at rest, the pressure is
    the same in all directions.
  • If this were not true there would be a net force
    on the fluid and it could not be at rest.
  • The force due to fluid pressure acts
    perpendicular to any surface.
  • Else there would be a force component along the
    surface which would accelerate the fluid.

20
Atmospheric pressure
  • At atmospheric pressure, every square meter has a
    force of 100,000 N exerted on it, coming from air
    molecules bouncing off it!
  • Why dont we, and other things, collapse because
    of this pressure?

21
Fluid-Statics
  • Static equilibrium
  • A simpler expression
  • Where p0 is the pressure at the surface, and h is
    depth of the liquid
  • The pressure at any point in a fluid is
    determined by the density of the fluid and the
    depth. It does not depend on any horizontal
    dimension of the fluid or its container. It also
    does not depend on the shape of the container.
    (example pascal vases)

22
Measuring pressure
  • The relationship between pressure and depth is
    exploited in manometers (or barometers) that
    measure pressure.
  • A standard barometer is a tube with one end
    sealed.
  • The sealed end is close to zero pressure, while
    the other end is open to the atmosphere.
  • The pressure difference between the two ends of
    the tube can maintain a column of fluid in the
    tube, with the height of the column being
    proportional to the pressure difference.
  • pressure at bottom of column atmospheric
    pressure

23
Mercury/Water barometer
  • Mercury
  • atmospheric pressure pushes Hg column up ? unit
    mm-Hg (torr)
  • Thus Atmospheric pressure pushes the Hg column
    up by
  • 101.3 kPa/133 Pa/mm 760 mm
  • Water
  • Thus atmospheric pressure pushes the water column
    up by
  • 101.3 kPa/9.8 Pa/mm 10.3 m
  • another unit 1 bar 105 N/m2
  • in calculations only use N/m2 Pa (SI unit)

24
Gauge Pressure
  • Gauges measure pressure relative to atmospheric
    pressure absolute pressure gauge pressure
    atmospheric pressure
  • manometer (height of column of liquid measures
    gauge pressure)

25
Blood pressure
  • A typical reading for blood pressure is 120 over
    80.
  • What do the two numbers represent?
  • What units are they in?

26
Water pressure
  • At the surface of a body of water, the pressure
    you experience is atmospheric pressure. Estimate
    how deep you have to dive to experience a
    pressure of 2 atmospheres.
  • .

27
Blaise Pascal (1623-1662)
  • A change in the pressure applied to an enclosed
    incompressible fluid is transmitted undiminished
    everywhere in the fluid and to the walls of the
    container

28
Pascals Principle
  • Hydraulic lever (see diagram on right)
  • Something has to give
  • Since the liquid is incompressible, the volume
    drop on the left is equal to the volume increase
    on the right, ie.

29
  • Pascal placed a long thin tube vertically into a
    wine barrel. When the barrel and tube were filled
    with water to a height of 12 m, the barrel burst.
  • (a) what is the mass of the water in the tube?
  • (b) what is the net force exerted onto the lid of
    the barrel?

30
The Buoyant Force
  • With fluids, we bring in a new force.
  • The buoyant force is generally an upward force
    exerted by a fluid on an object that is either
    fully or partly immersed in that fluid.
  • Lets survey your initial ideas about the buoyant
    force.

31
The Buoyant Force
  • A wooden block with a weight of 100 N floats
    exactly 50 submerged in a particular fluid. The
    upward buoyant force exerted on the block by the
    fluid
  • has a magnitude of 100 N
  • has a magnitude of 50 N
  • depends on the density of the fluid
  • depends on the density of the block
  • depends on both the density of the fluid and
    the density of the block

32
Apply Newtons Second Law
  • Even though we are dealing with a new topic,
    fluids, we can still apply Newtons second law to
    find the buoyant force.

33
  • A block of weight mg 45.0 N has part of its
    volume submerged in a beaker of water. The block
    is partially supported by a string of fixed
    length. When 80.0 of the blocks volume is
    submerged, the tension in the string is 5.00 N.
    What is the magnitude of the buoyant force acting
    on the block?

34
  • Water is steadily removed from the beaker,
    causing the block to become less submerged. The
    string breaks when its tension exceeds 35.0 N.
    What percent of the blocks volume is submerged
    at the moment the string breaks?

35
  • After the string breaks and the block comes to a
    new equilibrium position in the beaker, what
    percent of the blocks volume is submerged?
  • what does the free-body diagram look like now?

36
Archimedes Principle
  • While it is true that the buoyant force acting on
    an object is proportional to the volume of fluid
    displaced by that object.
  • Example cartesian diver
  • But, we can say more than that. The buoyant force
    acting on an object is equal to the weight of
    fluid displaced by that object. This is
    Archimedes Principle.

37
A Floating Object
  • When an object floats in a fluid, the downward
    force of gravity acting on the object is balanced
    by the upward buoyant force.
  • Looking at the fraction of the object submerged
    in the fluid tells us how the density of the
    object compares to that of the fluid. (example
    density blocks, coke cans)

38
The origin of the buoyant force
  • The net upward buoyant force is the vector sum of
    the various forces from the fluid pressure.
  • Because the fluid pressure increases with depth,
    the upward force on the bottom surface is larger
    than the downward force on the upper surface of
    the immersed object.
  • This is for a fully immersed object. For a
    floating object, h is the height below the water
    level, so we get

39
When the object goes deeper
  • If the fluid density does not change with depth,
    all the forces increase by the same amount,
    leaving the buoyant force unchanged!

40
Archimedes Principle
  • Buoyant force
  • Objects that float
  • Dry wood, ice, some plastics, oil, wax
    (candles)
  • Boats made of woods, ceramic, steel, or any other
    materials, as long as they are hollow enough
  • Objects that sink
  • Rocks, sands, clay, metal, etc.
  • Any material with density larger than water
  • Apparent weight (example submerged object weighs
    less)
  • Apparent weightactual weight - buoyant force
  • What is your apparent weight in water? (no more
    than a few pounds!)

41
Unbalancing the forces
  • If we remove the balance between forces, we can
    produce some interesting effects. Demonstrations
    of this include
  • The Magdeburg hemispheres (see below)
  • Crushing a can

42
Crush a can
  • Remember that this is just the collective effect
    of a bunch of air molecules!

43
Summary
  • Density and pressure of fluids
  • Air pressure, blood pressure and underwater
    pressure
  • Pascals Principle
  • Archimedes Principle
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