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    8$oatin! Head STHE TEMA T

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    A Ne) 9art/+ 7n$# for SHTE

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    Cross Baff$es

    ' Baff$es ser,e t)o *ur*oses5

    ' Divert (direct) the flow across the %und$e to o%tain a hi!herheat transfer coefficient+' Support the tubes for structura$ ri!idit#0 *re,entin! tu%e

    ,i%ration and sa!!in!+

    ' When the tube bundle employs baffles 0' the heat transfer coefficient is hi!her than the coefficient for

    undistur%ed f$o) around tu%es )ithout %aff$es+' 8or a %aff$ed heat e chan!er the hi!her heat transfer

    coefficients resu$t fro( the increased turbulence +' the velocity of fluid fluctuates %ecause of the constricted area

    %et)een ad1acent tu%es across the %und$e+

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    T#*es of Baff$e 9$ates 5 Se!(enta$ Cut Baff$es

    ' The sin!$e and dou%$e se!(enta$ %aff$es are (ost frequent$# used+

    ' The# di,ert the f$o) (ost effecti,e$# across the tu%es+

    ' The %aff$e s*acin! (ust %e chosen )ith care+

    ' 7*ti(a$ %aff$e s*acin! is so(e)here %et)een :;< - =;< of the

    she$$ dia(eter+' Baff$e cut of >?

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    T#*es of Baff$e 9$ates

    Tri*$e Se!(enta$ Baff$es

    Dou%$e Se!(enta$ Baff$es

    The triple segmental bafes are used or lowpressure applications.

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    T#*es of Baff$e 9$ates

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    T#*es of Baff$e 9$ates

    Disc and ring bafes are composed o alternating outerrings and inner discs, which direct the ow radially

    across the tube eld. The potential bundle-to-shell bypass stream is

    eliminated

    This bafe type is very e ective in pressure drop toheat trans er conversion

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    T#*es of Baff$e 9$ates

    n an ori ce bafe shell-side- uid ows through theclearance between tube outside diameter andbafe-hole diameter.

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    Therm-!ydraulic "nalysis o !eat#$changer

    ' nitia$ Decisions+' Tu%e side Ther(a$ Ana$#sis+

    ' Ther(a$ ana$#sis for She$$ side+' 7,era$$ Heat Transfer coefficient+' H#drau$ic Ana$#sis of Tu%e side+' H#drau$ic Ana$#sis of She$$ side+

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    "luid Allo#ation $ %ube Side

    ' Tu%e side is *referred under these circu(stances5' 8$uids )hich are *rone to fou$' The hi!her ,e$ocities )i$$ reduce %ui$du*' Mechanica$ c$eanin! is a$so (uch (ore *ractica$ for tu%es than for

    she$$s+' Corrosi,e f$uids are usua$$# %est in tu%es' Tu%es are chea*er to fa%ricate fro( e otic (ateria$s' This is a$so true for ,er# hi!h te(*erature f$uids requirin! a$$o#

    construction' To ic f$uids to increase contain(ent' Strea(s )ith $o) f$o) rates to o%tain increased ,e$ocities and

    tur%u$ence' Hi!h *ressure strea(s since tu%es are $ess e *ensi,e to %ui$d stron!+

    ' Strea(s )ith a $o) a$$o)a%$e *ressure dro*

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    8$uid A$$ocation 5 She$$ Side

    ' She$$ side is *referred under these circu(stances5' iscous f$uids !o on the she$$ side0 since this )i$$ usua$$#

    i(*ro,e the rate of heat transfer+

    ' 7n the other hand0 *$acin! the( on the tu%e side )i$$usua$$# $ead to $o)er *ressure dro*s+ ud!(ent is needed+

    ' Low heat transfer coefficient: ' Strea( )hich has an inherent$# $o) heat transfer coefficient

    such as $o) *ressure !ases or ,iscous $iquids 0 this strea(is *referentia$$# *ut on the she$$-side so that e tendedsurface (a# %e used to reduce the tota$ cost of the heate chan!er+

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    Options for Shell-Side Thermal nalysis

    ' !ern"s inte#ral method

    ' $ell-Delaware method

    ' Stream analysis method

    ' %ecent &ethods

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    !ern &ethod ofS' LL- D-T*$ ' T +,' % nalysis

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    no)$ed!e for So$,in! True ndustria$ 9ro%$e(s 5Dona$d F ern

    ' True %e$ie,er of *ro,idin! 2no)$ed!e for use of so$,in!run-of-the-(i$$ *ro%$e(s+

    ' Donald ./ !ern ward: 0,h /' n honor of Dona$d F+ ern0 *ioneer in *rocess heat

    transfer0 the Di,ision reco!ni.es an indi,idua$ s e *ertise ina !i,en fie$d of heat transfer or ener!# con,ersion+

    ' There is no true f$o) area %# )hich the she$$-side (ass,e$ocit# can %e co(*uted+

    ' 8ictitious ,a$ues for equi,a$ent dia(eter and (ass ,e$ocit#are to %e defined+

    ' These are %orne out %# e *eri(ent+

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    8$o) 9ast Tu%e Bund$es 5 7utside 8i$( Coefficient

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    ern s nte!ra$ Method

    ' The initia$ atte(*ts to *ro,ide (ethods for ca$cu$atin! she$$-side *ressure dro* and heat transfer coefficient )ere %ased one *eri(enta$ data for t#*ica$ heat e chan!ers+

    ' 7ne of these (ethods is the )e$$-2no)n ern (ethod0 )hich)as an atte(*t to corre$ate data for standard e chan!ers %# asi(*$e equation ana$o!ous to equations for f$o) in tu%es+

    ' This (ethod is restricted to a fi ed %aff$e cut >?< andcannot adequate$# account for %aff$e-to-she$$ and tu%e-to-

    %aff$e $ea2a!es+

    ' A$thou!h the ern equation is not *articu$ar$# accurate0 it doesa$$o) a ,er# si(*$e and ra*id ca$cu$ation of she$$-sidecoefficients and *ressure dro* to %e carried out

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    Ma1or Ste*s in Desi!n

    ' nitia$ Decisions+' Tu%e side Ther(a$ Ana$#sis+

    ' Ther(a$ ana$#sis for She$$ side f$o)+' 7,era$$ Heat Transfer coefficient+' H#drau$ic Ana$#sis of Tu%e side+' H#drau$ic Ana$#sis of She$$ side+

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    nitia$ Decisions

    ' S*atia$ a$$ocation of f$uid+' Deter(ination of f$o) ,e$ocit#+

    ' nitia$ !uess for nu(%er of tu%es+' Correction for standard tu%e dia(eter+' Effect of nu(%er of tu%es on tu%e $en!th/+