chapter 7 - conservation of energy and momentum

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    UNIT 3Momentum & Energy

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    EFFICIENCY

    Efficiency is the ratio of useful energy or work

    output to the total energy or work output.

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    EFFICIENCY

    A model rocket engine contains explosives storing

    3.5*10^3J of chemical potential energy. The stores

    energy is transformed into gravitational potential

    energy at the top of a rockets flight path. Calculate

    how efficiently the rocket transforms storedchemical energy into gravitational potential energy

    if the 0.500kg rocket is propelled to a height of

    1.00*10^2m.

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    EFFICIENCY

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    CHAPTER 17CONSERVATION OF

    ENERGY AND MOMENTUM

    Law of conservation of energy: Energy can not becreated or destroyed, or may only be transformed.

    Thus, the total energy of an isolated system must

    be constant over time.

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    ENERGY TRANSFORMATIONS

    Youve talked about kinetic, potential, and

    gravitational energyall mechanical energies. Now

    we will talk about what happens to the energy after

    youve done work on the object.

    If you shoot a hockey puck down an ice surface,

    what will eventually happen?

    It has lost the mechanical energy that weve given

    it!

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    CONSERVATIVE AND NON-

    CONSERVATIVE FORCES

    If you lift a book one meter above a table and

    release it, what happens?

    If you push a book across a table, will itautomatically return to its original spot?

    What are we doing work against in the first case?

    And the second?

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    CONSERVATIVE AND NON-

    CONSERVATIVE FORCES

    Now, if you lift the book one meter above the table,

    and then carry it across the room, have you done

    more work on the book than in the first case?

    If you push the book from one side to the other, and

    then push it back to its original position, have you

    done more work than before?

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    CONSERVATION OF MECHANICAL

    ENERGY

    When all of the work done throughout a process is

    done by conservative forces, the total mechanical

    energy of the system before the process is equal to

    the total mechanical energy at the end of the

    process.

    Ek + Eg + Ee= Ek + Eg + Ee

    k = kinetic

    g = gravitational

    e = elastic

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    CONSERVATION OF MECHANICAL

    ENERGY

    What kind of energy transformation is happening if

    you drop a rock?

    What happens the total energy?

    What is happening to the different energies

    throughout the process?

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    CONSERVATION OF MECHANICAL

    ENERGY

    A skier is gliding along with a speed of 2.00m/s at

    the top of a ski hill, 40.0m high. The skier then

    begins to slide down the icy (frictionless) hill.

    a. What will be the skiers speed at a height of 25.0m?

    b. At what height will the skier have a speed of 10.0m/s?

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    CONSERVATION OF MECHANICAL

    ENERGY

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    CONSERVATION OF MECHANICAL

    ENERGY

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    CONSERVATION OF MECHANICAL

    ENERGY

    Homework problems: pg. 287, #1-4

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    ELASTIC POTENTIAL ENERGY AND

    KINETIC ENERGY

    Youve leaned what elastic potential energy is and

    how to express it when stored in a stretched or

    compressed spring:

    Now, what are some practical examples of

    transforming elastic potential energy into kinetic

    energy?

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    ELASTIC POTENTIAL ENERGY AND

    KINETIC ENERGY

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    ELASTIC POTENTIAL ENERGY AND

    KINETIC ENERGY

    A low friction cart with a mass of 0.25kg travels

    along a horizontal track and collides head on with a

    spring that has a spring constant of

    155N/m. If the spring was compressed by 6.0cm,

    how fast was the cart initially travelling?

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF TOTAL ENERGY

    A system is any object or group of objects.

    An internal force is any force exerted on any objectin the system due to another object in the system.

    An external force is any force exerted by an object

    that is not a part of the system on an object withinthe system.

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    CONSERVATION OF TOTAL ENERGY

    An open system can exchange both matter and

    energy with its surroundings.

    A closed system can exchange energy, but notmatter, with its surroundings.

    An isolated system can not exchange energy or

    matter with its surroundings - nothing can enter orleave.

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF TOTAL ENERGY

    You often hear that a system lost energy. Since

    the energy can not be created or destroyed, what

    happens to the energy?

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    CONSERVATION OF TOTAL ENERGY

    We can now state the law of conservation of energy

    mathematically:

    The work done by non-conservative forces is the

    difference between the final mechanical energy andthe initial mechanical energy of a system.

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    CONSERVATION OF TOTAL ENERGY

    A roller-coaster with a mass of 200.0kg is moving to the right at a

    speed of 4.00m/s at point A, 15.00m above the ground. The

    car then heads down the slope towards point B, 6.00m above

    the ground. If 3.40*10^3J of work are done by friction between

    points A and B, determine the speed of the car at point B.

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF TOTAL ENERGY

    Example: A 65.0kg skydiver steps out from a hot air

    balloon that is 5.00*10^2m above the ground. After

    free-falling a short distance, she deploys her

    parachute, finally reaching the ground with a

    velocity of 8.00m/s.

    a. What is the gravitational potential energy

    of the skydiver, relative to the ground,

    before she jumps?b. What is the kinetic energy just before she

    lands on the ground?

    c. How much work did the non-conservative

    frictional force do?

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF TOTAL ENERGY

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    CONSERVATION OF MOMENTUM

    Elastic collisionskinetic energy is conserved.

    Inelastic collisionskinetic energy is not

    conserved.

    Newtons third law of motion states that for every

    action force on object B due to object A, there is a

    reaction force equal in magnitude (but opposite

    direction) acting on object A due to object B.

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    CONSERVATION OF MOMENTUM

    So how do we derive the conservation of

    momentum law from Newtons third law? We use

    the impulse-momentum theorem!

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    CONSERVATION OF MOMENTUM

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    CONSERVATION OF MOMENTUM

    The conservation of momentum law states that the

    total momentum of two objects before a collision is

    the same as the total momentum of the same two

    objects after the collision.

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    CONSERVATION OF MOMENTUM

    We all know that systems are rarely perfectly

    isolated, and that immediately after a collision,

    frictional forces and interactions with other objects

    change the momentum of the objects.

    So is this law still useful?

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    CONSERVATION OF MOMENTUM

    Yes! We can still use the conservation of

    momentum law to describe a system from the

    instant before to the instant after a collision.

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    CONSERVATION OF MOMENTUM

    A 1.75*10^4kg boxcar is rolling down a track toward

    a stationary boxcar that has a mass of 2.00*10^4kg.

    Just before the collision, the first boxcar is moving

    east at 5.45m/s. When the boxcars collide, they

    lock together and continue down the track. What isthe velocity of the two boxcars after the collision?

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    CONSERVATION OF MOMENTUM

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    CONSERVATION OF MOMENTUM

    A 0.250kg billiard ball moving at 5.00m/s collides

    head-on with a stationary, 0.800kg steel ball. If the

    billiard ball bounces directly backwards at 2.62m/s,

    was the collision elastic?

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    REAL LIFE EXAMPLES

    What are some examples that make this important

    for everyday events?

    Homework: pg. 327 # 2,7,8

    pg. 332 # 38, 42, 44, 46, 49