Buoyancy des

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    Archimedes Principle

    An object immersed in a liquid

    has an upward buoyant force

    equal to the weight of the liquiddisplaced by the object.

    An object will float if the

    upward buoyant force is greaterthan the objects weight.

    Archimedes

    287 211 BC

    (courtesy F. Remer)

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    Archimedes Principle Square bubble

    of gas in a tank

    of water

    (courtesy F. Remer)

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    Archimedes Principle Water pressure

    in tank increases

    with depth

    p = pressure

    h = depth

    ph

    (courtesy F. Remer)

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    Archimedes Principle Horizontal Pressure

    Differences Balance

    (courtesy F. Remer)

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    Archimedes Principle Force on bottom of

    bubble

    Fbottom

    pbottom !Fbottom

    A

    ApF bottombottom !

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    Archimedes Principle Force on top of

    bubble

    Fbottom

    Ftop

    A

    Fp

    top

    top !

    ApF toptop !

    (courtesy F. Remer)

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    Archimedes Principle

    Buoyancy Force

    Fbottom

    Ftop

    FB ! (pbottom ptop ) A

    FB

    FB

    ! Fbottom

    Ftop

    FB ! (pA

    (courtesy F. Remer)

    FB ! Apbottom Aptop

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    Archimedes Principle

    Pressure Difference

    Between Top & Bottom

    Negative by convention pbottom

    ptop

    h

    (p

    h! Vg

    (p ! Vgh

    (courtesy F. Remer)

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    Archimedes Principle

    Combine Equations

    pbottom

    ptop

    h

    (p ! Vgh

    B

    B ! (pA

    FB ! VghA

    FB ! VgV

    V ! hA

    (courtesy F. Remer)

    Note: Density () = density of liquid

    Volume = displaced volume of liquid = volume of object

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    Archimedes Principle

    The net force on the object is thus thedifference between the objects weight and

    the buoyancy force of the displaced fluid.

    If the buoyancy of an object exceeds itsweight, it tends to rise. An object whose

    weight exceeds its buoyancy tends to sink.

    Fnet ! mg VVgWeight of

    object

    Buoyant

    Force of displaced

    fluid

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    Archimedes Principle

    Cartoon here??Archimedes

    287 211 BC

    At the moment of Archimedes famous discovery.

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    Example

    What is the buoyancy in seawater of a piece ofwood that weighs 10,000 N & measures 3m x

    1m x 2m?

    The weight of wood = 10,000 N The volume of wood = 3m x 2m x 1m= 6 m3

    The corresponding weight of an equal volume of

    seawater: 6 m

    3

    x 10300N/m

    3

    = 61,800Nweight of water displaced = upward force = 61,800Nweight of wood = downward force = 10,000N

    Net Force = 51,800N up

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    Example 2 A fully suited diver weighs 200 pounds. This diver

    displaces a volume of 3.0 cubic feet of seawater.Will the diver float or sink?

    weight of equal volume of seawater:

    3.0 ft3

    x 64 lb/ft3

    . = 192 lb.Weight of diver = down force = 200 lbs

    Displaced weight of sea water = up force = 192 lb

    net force = 8 lbsdown

    The diver will sink. This diver weighs 8 pounds in

    the water and is over-weighted. Removal of eight

    pounds will allow the diver to hover.

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    Buoyancy

    Similar to parcel of air

    in atmosphere

    At Equilibrium

    Density of Parcel Same

    as Density of

    Environment

    pVeV

    pe V!V

    (courtesy F. Remer)

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    Archimedes Principle

    Translation:

    objects more dense than water will sink -

    negatively buoyant ;

    objects less dense than water will float -

    positively buoyant;

    objects of the same density will remain at the

    same level and neither sink nor float -

    neutrally buoyant.

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    Buoyancy Density Difference

    Results in Net

    Buoyancy Force

    pVeVpe V"V

    B

    (courtesy F. Remer)

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    Buoyancy Density Difference

    Results in Net

    Buoyancy Force

    pVeVpe VV

    B

    (courtesy F. Remer)

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    Buoyancy Net Buoyancy Force

    pVeV

    BgV)(B pe VV!

    (courtesy F. Remer)

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    Archimedes Principle Water is in hydrostatic

    equilibrium

    = density

    g = acceleration ofgravity

    B

    (p

    (h! Vg

    (p

    (h

    gV

    (courtesy F. Remer)

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    Buoyancy How is air displaced?

    Two methods

    1.) Forced Ascent

    2.) Auto-Convective Ascent

    (courtesy F. Remer)

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    Forced Ascent Some mechanism forces air aloft

    CoolAirCoolAir

    Cold airCold airWarm airWarm air

    (courtesy F. Remer)

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    Auto-Convective Ascent Air becomes buoyant

    by contact with warm

    ground

    HotHotCoolCool CoolCool(courtesy F. Remer)

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    Buoyancy As Parcel Rises Parcel Temperature

    Changes and it expands.

    Unsaturated?

    (courtesy F. Remer)

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    Stability As Parcel of Air Rises The Parcel Temperature

    Changes and expands.

    Saturated? Gaseous water condenses to rain

    (courtesy F. Remer)

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