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Buoyancy and Stability

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    BUOYANCY AND STABILITY

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    BUOYANCYDEFINITION

    Itis an upward force exerted by a fluid that

    opposes the weight of an immersed object. In a

    column of fluid pressure increases with depth as a

    result of the weight of the o!erlying fluid.

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    Buoyant Force

    " The force remains evenwithout the origina !ui"#

    " It must $aance theweight that wou" have$een there#

    " This is the buoyantforce#

    # %&uas the fuidweight

    # Directe" u'war"

    # Acts on the voume

    Fb = mg

    VgFbuoy =

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    Sin(ing an" )ising

    " An o$*ect in a !ui""is'aces a voume thatha" some mass#

    " If the o$*ect is heavierthan the !ui" it sin(s#

    " If the o$*ect is ighter itrises#

    Fb = Vg

    W= mg

    Fb = Vg

    W= mg

    mmgVgamgVgFnet

    /)( =

    =

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    Archime"es+ ,rinci'e

    " An o$*ect sus'en"e" in a !ui" hasess a''arent weight "ue to$uoyancy#

    Fb = Vg

    W= mg

    FT = mg -

    Vg

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    Ice$erg

    " An ice$erg has an average"ensity of -./ ofseawater#

    " 0hat fraction of theice$erg is un"erwater1

    The $uoyant force is theweight of water "is'ace"$y the ice$erg2 Fb3

    waterVsubg#

    The weight is the totaweight of the ice2 Wi3

    iceViceg#

    Fin" the ratio of Vsub/Vice 0e (now the ratio ice4water

    waterVsubg = iceViceg

    Vsub/Vice3 ice4water3 5#-.

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    Center of Buoyancy

    " The force of $uoyancy acts at thecenter of mass of the missing !ui"#

    " The "is'acing o$*ect has a center ofgravity at its center of mass#

    " The two forces may not act at thesame 'oint#

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    Ti''y Canoe

    " If a forces on an o$*ectact at "i6erent 'ointsthere is a tor&ue#

    " Buoyant force a$ove thecenter of mass is sta$e#

    # The tor&ue moves it$ac( to the center

    " Buoyant force $eow thecenter of mass isunsta$e#

    # The tor&ue moves itaway from the center

    ne7t

    http://var/www/apps/conversion/tmp/scratch_7/p210_09c.ppthttp://var/www/apps/conversion/tmp/scratch_7/p210_09c.ppt
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    STABILITY

    " A !oating o$*ect is sta$e if it ten"sto restore itsef to an e&uii$rium'osition after a sma "is'acement#

    For e7am'e8 !oating o$*ects wigeneray have vertica sta$iity8 as ifthe o$*ect is 'ushe" "own sighty8

    this wi create a greater $uoyancyforce8 which8 un$aance" $y theweight force8 wi 'ush the o$*ect

    $ac( u'

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    Stability o Immersed and Floating

    Bodies9Centers of $uoyancy an" gravity "o not coinci"e9 A sma rotation can resut in either a restoring or

    overturning cou'e#

    9 Sta$iity is im'ortant for !oating $o"ies

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    Stability o an immersed body

    Sta$iity of acom'etey

    immerse" $o"y :center

    of gravity $eowentroi"#

    Sta$iity of a com'eteyimmerse" $o"y : centerof gravity a$ovecentroi"#

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    Stability o a foating body

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    %CONO;IC ,I,% DIA;%T%)

    The "iameter of the 'i'e strongyin!uences the 'resent vaue of the'ant8 through $oth the annua cost of

    eectric 'ower an" the instaation costof the 'i'ing system

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    %conomic 'i'e seection metho"

    " Intro"uction

    " The economic 'i'e seection metho" is use to$aance >7e" cost of 'i'e with annua energy

    cost for 'um'ing" 0ith arge 'i'e si?es8 the average !ow veocityfor a given "ischarge "ecreases8 causing acorres'on"ing "ecrease in friction oss

    " This re"uces the hea" on the 'um' an" energycan $e save"

    " @owever8 arger 'i'es are e7'ensive

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    " To $aance these costs an" to >n" theminimum cost8 we wi annuaise the

    >7e" costs8 com'are" with annuaenergy costs#

    " 0e wi ta(e into account interestrates an" in!ation rates to ma(e thecom'arison

    " This is $asicay an engineeringeconomics 'ro$em s'eciay a"a'te"to ma(e the seection of 'i'e si?es

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    ,rinci'e ste's

    " Determine the e&uivaent annuacost for 'urchasing each avaia$e'i'e si?e

    " Determine the annua energy cost of'um'ing

    " Baance the annua cost for a"*acent

    'i'e si?e

    " Construct a gra'h of system !owrate v4s section !ow rate

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    ,i'e si?e vs cost


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