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4. Cons of ME

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    UNIT 1: CONSERVATION LAWS

    Lesson 4:

    Conservation of Mechanical Energy

    CENTRE HIGH: PHYSICS 30

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    D. Conservation of Energy

    Recommended Reading:

    Ladner pp. 16 - 17

    Heath pp. 291 - 292, 300

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    D. Conservation of Energy

    Recall:

    There are two major advantages to the energetics perspective:

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    D. Conservation of Energy

    Recall:

    There are two major advantages to the energetics perspective:

    1. Energy is a scalar

    - does not have direction

    - no need for vector math

    2. It is conserved

    We will now analyze situations where total mechanical energyis conserved.

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    D1. Total Mechanical Energy (MET)

    MET = sum of all mechanical energies= KE + PEg (+ Ee)

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    Ex. 1 mcar = 400 kg

    20 m/s

    Aconstant speed

    16 m 20 m/s

    B

    If the car's PEg is zero at A, then find MET at B (in kJ).

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    Solution

    A Ref h (h = 0)

    -16 m 20 m/s

    B

    Since the height is zero at A,

    then location B is below the reference height

    So, the height at B is negative

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    Solution

    A Ref h (h = 0)

    -16 m 20 m/s

    B

    PEgB = m g h

    = (400 kg) (9.81 N/kg) (-16 m) = -62,784 J

    KEB = 0.5 mv2

    = 0.5 (400 kg) (20 m/s)2 = 80,000 J

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    MET = PEgB + KEB

    = -62,784 J + 80,000 J

    = 17, 216 JUnit you want

    MET = 17, 216 J x 1 kJ

    1000 J

    Unit to cancel

    = 17 kJ

    Check:

    2 sig digs; units

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    D2. Energy Conversions

    Recall W =

    E

    - there are two ways that energy can change:

    1. Energy Transformation

    2. Energy Transfer

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    1. Energy Transformations

    - when energy changes from one form (or type)

    to another

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    e.g. Dropping a ball:

    Rest

    Ref h

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    Since the object is losing height,

    it is losing PEg All PEg Rest

    Where does this energy go?

    No PEg Ref h

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    Since the object is losing height,

    it is losing PEg All PEg Rest

    No KEAt the same time, the object is

    gaining speed.

    Thus, it gains KE.

    No PEg Ref h

    All KE

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    Since the object is losing height,

    it is losing PEg All PEg Rest

    No KEAt the same time, the object is

    gaining speed.

    Thus, it gains KE.

    No PEg Ref h

    All KE

    We say that the PEg has transformed

    into KE.

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    2. Energy Transfer

    When energy goes from one object to another.

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    e.g. Car colliding with another stationary car:

    moving car stationary car

    (KE) (no KE)

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    KE No KE

    Both have KE

    After the collision, the blue car has gained kinetic energy.

    Where did the energy come from?

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    KE No KE

    Both have KE

    Some kinetic energy has transferred from the first car

    to the second

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    D3. Conservation of Mechanical Energy

    - total mechanical energy stays constant (conserved) when:* the system is closed

    - no objects are added / lost

    * no friction

    * only mechanical forms of energy change

    - only Fg and Fs do work on the object

    - mechanical energy can convert only to another

    form of mechanical energy

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    Equations:

    If mechanical energy is conserved, then you can use two

    equations:

    1. MET remains constant

    METi = METfPEgi + KEi = PEgf + KEf

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    2. No overall change in energy

    PEg +

    KE = 0

    PEg = - KE

    That is,

    if PEg increases by 100 J,

    then KE decreases by 100 J (no overall change)

    So, one form of mechanical energy transforms intoanother form of mechanical energy

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    e.g. Consider an object thrown downward (No air resistance)

    PEgi = 600 J

    KEi = 200 J

    PEgf Ref h (h = 0)

    KEf

    What is the total mechanical energy at the start?

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    METi PEgi = 600 J

    800 J KEi = 200 J

    PEgf Ref h (h = 0)

    KEf

    What is the total mechanical energy at the end?

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    METi PEgi = 600 J

    800 J KEi = 200 J

    METi = METf

    METf PEgf Ref h (h = 0)

    800 J KEf

    So, what is its kinetic energy at the end?

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    METi PEgi = 600 J

    800 J KEi = 200 J

    METf PEgf= 0 Ref h (h = 0)

    800 J KEf = 800 J

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    PEgi = 600 J

    KEi = 200 J

    Calculate and interpret:

    - the change in PEg

    - the change in KE

    PEgf = 0

    KEf = 800 J

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    PEgi = 600 J

    KEi = 200 J PEg = PEgf - PEgi

    = 0 - 600 J= - 600 J

    object loses 600 J of PEgPEgf = 0 (since it loses height)

    KEf = 800 J

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    PEgi = 600 J

    KEi = 200 J KE = KEf - KEi

    = 800 J - 200 J= + 600 J

    object gains 600 J of KEPEgf = 0 (since it gains speed)

    KEf = 800 J

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    PEgi = 600 J

    KEi = 200 J

    The object loses 600 J of PEg,but it gains 600 J of KE

    We say that the PEg has

    transformed into KE.PEgf = 0

    KEf = 800 J

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    Animations:

    1. Dropped object:

    http://departments.weber.edu/physics/amiri/director/dcrfiles/energy/FallingBallS.dcr

    Can you explain what happens in the animation?

    http://departments.weber.edu/physics/amiri/director/dcrfiles/energy/FallingBallS.dcrhttp://departments.weber.edu/physics/amiri/director/dcrfiles/energy/FallingBallS.dcrhttp://departments.weber.edu/physics/amiri/director/dcrfiles/energy/FallingBallS.dcrhttp://departments.weber.edu/physics/amiri/director/dcrfiles/energy/FallingBallS.dcr
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    You should have noticed:

    The PEg goes down by 1078 J,

    but at the same time, the KE goes up by 1078 J

    That is, the PEg has transformed entirely into KE

    Thus, the total mechanical energy will remain the samethroughout the entire motion

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    Other animations showing conservation of energy:

    2. Pendulum:

    http://www.phy.ntnu.edu.tw/ntnujava/viewtopic.php?t=27

    3. Rollercoaster:

    http://www.glenbrook.k12.il.us/gbssci/phys/mmedia/qt/energy/

    coastwin.html

    http://www.phy.ntnu.edu.tw/ntnujava/viewtopic.php?t=27http://www.glenbrook.k12.il.us/gbssci/phys/mmedia/qt/energy/coastwin.htmlhttp://www.glenbrook.k12.il.us/gbssci/phys/mmedia/qt/energy/coastwin.htmlhttp://www.glenbrook.k12.il.us/gbssci/phys/mmedia/qt/energy/coastwin.htmlhttp://www.glenbrook.k12.il.us/gbssci/phys/mmedia/qt/energy/coastwin.htmlhttp://www.phy.ntnu.edu.tw/ntnujava/viewtopic.php?t=27
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    Ex. 2 A ball is dropped from a height H and it lands with a

    speed of 7.0 m/s. If the system is conservative,

    a) find H

    b) sketch a PEg vs t, KE vs t, and a MET vs t graph

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    a) METi = METf Rest

    PEgi+ KE

    i= PEg

    f+ KE

    f

    Ref h (h = 0)

    Be certain to state 7.0 m/s

    where the height is zero

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    a) METi = METf Rest

    PEgi+ KE

    i= PEg

    f+ KE

    f

    Ref h (h = 0)

    7.0 m/s

    Since it starts at rest, KEi = 0Since it has no height at the end, PEgf = 0

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    METi = METf

    PEgi + KEi = PEgf+ KEf

    mghi = 0.5 mvf2

    ghi = 0.5 vf2

    If you divide both sides of the equation by m,

    the mass cancels

    Thus, the answer does not depend on mass.

    i.e. It is true for any mass

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    METi = METf

    PEgi + KEi = PEgf+ KEf

    mghi = 0.5 mvf2

    ghi = 0.5 vf2

    hi = 0.5 vf2 = 0.5 (7.0 m/s)2

    g 9.81 m/s2

    H = 2.5 m

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    b) PEg KE

    t t

    MET

    t

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    b) PEg KE

    height speed

    decreases increases

    t t

    MET constant

    t

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    Ex. 3 A 1.20 kg car travels the following path. No friction.

    A 6.70 m/s

    v ?

    C

    8.70 m B4.20 m

    1.90 m

    D

    Find its speed at C.

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    A 6.70 m/s

    v ?

    C

    8.70 m B

    4.20 m

    1.90 mD (h = 0)

    The reference height (h = 0) is at D,

    the lowest location in the diagram

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    A 6.70 m/s

    v ?

    C

    8.70 m B

    4.20 m

    1.90 mD (h = 0)

    Total mechanical energy remains the same.

    So, META

    = METC

    PEgA + KEA = PEgC + KEC

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    Ref h = D

    PEgA = mghA

    = (1.20 kg) (9.81 N/kg) (8.70 m) = 102.42 J

    KEA = 0.5mvA2

    = 0.5 (1.20 kg) (6.70 m/s)2 = 26.93 J

    PEgC = mghC

    = (1.20 kg) (9.81 N/kg) (4.20 m) = 49.44 J

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    Find KEC:

    META = METB

    PEgA + KEA = PEgC + KEC

    102.42 J + 26.93 J = 49.44 J + KEC

    KEC = 79.908 J

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    Find speed at C:

    KEC

    = 0.5 mv2

    v2 = KEC

    0.5 m

    v = KEC = 79.908 J = 11.5 m/s0.5 m 0.5 (1.20 kg)

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    Ex. 4

    A 14.0 kg object is currently moving at a height of 75.0 cm. If

    it then loses 92.0 J of KE, find the object's new height.

    Assume a conservative system.

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    Solution

    The total mechanical energy must remain the same

    So, if the object loses 92.0 J of KE,

    it must gain 92.0 J of PEg

    That is, the KE converts (transforms) into PEg

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    Find PEgi:

    PEgi

    = mghi

    = (14.0 kg) (9.81 N/kg) (0.750 m)

    = 103.0 J

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    Find PEgf:

    Since PEg

    must increase by 92.0 J,

    PEgf = PEgi + 92.0 J

    = 103.0 J + 92.0 J

    = 195.0 J

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    Find the final height:

    PEgf

    = mghf

    hf = PEgf = 195.0 J = 1.42 m

    mg (14.0 kg) (9.81 N/kg)

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    Practice Problems:

    Try:

    Ladner p.19 #1 - 10, 13

    Heath p.304 #3, 4

    Challenge:

    Ladner p.19 #11, 12

    Heath p. 344 #38

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    SUMMARY

    1. Identify the 3 conditions for MET to remain constant.

    2. An object experiences a gain of 700 J of PEg. If the system is

    conservative, describe what happens to:

    a) its KE b) MET

    3. A ball is thrown vertically upward to a maximum height. If

    there is no AR, sketch the following graphs:

    a) PEg vs t b) KE vs t c) MET vs t

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    SUMMARY

    1. Identify the 3 conditions for MET to remain constant.

    Closed system

    - no objects lost, added

    No friction

    Only mechanical energy can change

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    2. An object experiences a gain of 700 J of PEg. If the system is

    conservative, describe what happens to:

    a) KE b) MET

    a) KE must decrease by 700 J

    KE = - PEg

    b) MET remains constant

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    3. A ball is thrown vertically upward to a maximum height. If

    there is no AR, sketch the following graphs:

    a) PEg vs t b) KE vs t c) MET vs t

    a) PEg b) KE c) MET

    t t theight speed


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