PM3125 Lectures 6to9 Heat Transfer

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  • 7/25/2019 PM3125 Lectures 6to9 Heat Transfer

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    Prof. R. Shanthi 1

    PM3125: Lectures 6 to 9

    Content of Lectures 6 to 12:

    Heat transfer:

    -Source of heat

    - Heat transfer- Stea an! e"ectricit# as heatin$ e!ia

    - %eterination of reuireent of aount of

    stea'e"ectrica" ener$#

    - Stea (ressure- Matheatica" (ro)"es on heat transfer

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    Prof. R. Shanthi 2

    *hat is Heat+

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    Prof. R. Shanthi 3

    *hat is Heat+

    Heat is ener$# in transit.

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    Prof. R. Shanthi ,

    nits of Heat /he S unit is theou"e 4

    hich is eua" to 7eton-etre 74.

    Historica""# heat as easure! in ters of the a)i"it#

    to raise the te(erature of ater.

    /he ca"orie ca"4: aount of heat nee!e! to raise the

    te(erature of 1 $rae of ater )# 1 C0fro

    1,.50C to 15.50C4

    n in!ustr# the 8ritish thera" unit 8tu4is sti"" use!:aount of heat nee!e! to raise the te(erature of 1 ")

    of ater )# 1 0fro 630 to 6,04

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    Prof. R. Shanthi 5

    Conersion )eteen !ifferent

    units of heat:

    1 ; 0.23

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    Prof. R. Shanthi 6

    Sensi)"e Heat

    *hat is ?sensi)"e heat@+

    Sensi)"e heat is associate!ith a te(erature chan$e

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    Prof. R. Shanthi A

    S(ecific Heat Ca(acit#

    /o raise the te(erature )# 1 B !ifferentsu)stances nee! !ifferent aount of ener$# )ecause

    su)stances hae !ifferent o"ecu"ar confi$urations

    an! )on!in$ e$: co((er ater oo!4

    /he aount of ener$# nee!e! to raise the

    te(erature of 1 >$ of a su)stance )# 1 B is >non

    as the s(ecific heat ca(acit#

    S(ecific heat ca(acit# is !enote! )# c

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    Prof. R. Shanthi e!

    e=a("es )# R. Shanthini

    (u)"ishe! )# Science !ucation nit acu"t# of Science

    niersit# of Pera!eni#a4

    a"so u("oa!e! at htt(:''.rshanthini.co'PM3125.ht4

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    Prof. R. Shanthi 23

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    -20oC ice

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    Prof. R. Shanthi 2,

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    -20oC ice

    0oC e"tin$ (oint of ice

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    Prof. R. Shanthi 25

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    -20oC ice

    0oC e"tin$ (oint of ice

    120.2oC )oi"in$ (oint of ater at 2 )ar

    8oi"in$ (oint of ater at 1 at (ressure is

    100oC.

    8oi"in$ (oint of ater at 2 )ar is 120.2oC.

    IRefer the Stea /a)"e.J

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    Prof. R. Shanthi 26

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    -20oC ice

    0oC e"tin$ (oint of ice

    120.2oC )oi"in$ (oint of ater at 2 )ar

    150oC su(erheate! stea

    S(ecific heat

    S(ecific heat

    S(ecific heat

    Latent heat

    Latent heat

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    Prof. R. Shanthi 2A

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    S(ecific heat reuire! to raise the te(erature of ice fro -20oCto 0oC

    ; 2 >$4 2.06 >'>$ oC4 I0 - -204JoC ;

    Latent heat reuire! to turn ice into ater at 0oC

    ; 2 >$4 33, >'>$4 ; 66< >

    S(ecific heat reuire! to raise the te(erature of ater fro 0o

    C to120.2oC

    ; 2 >$4 ,.1< >'>$ oC4 I120.2 - 04JoC ; 100,.9 >

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    Prof. R. Shanthi 2$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    Latent heat reuire! to turn ater into stea at 120.2oC an! at 2 )ar

    ; 2 >$4 2202 >'>$4 ; ,,0, >

    ILatent heat of a(ouriEation at 2 )ar is 2202 >'>$ as cou"! )ereferre! to fro the Stea /a)"eJ

    S(ecific heat reuire! to raise the te(erature of stea fro 120.2oC

    to 150oC

    ; 2 >$4 2AA0 K 2A0A4 >'>$ ; 126 >

    Intha"(# at 120.2oC an! 2 )ar is the saturate! stea entha"(# of

    2A0A >'>$ an! the entha"(# at 150oC an! 2 )ar is 2AA0 >'>$ as

    cou"! )e referre! to fro the Stea /a)"eJ

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    Prof. R. Shanthi 29

    *arin$ cure for ater*hat is the aount of heat reuire! to chan$e 2 >$ of ice

    at -20o

    C to stea at 150o

    C at 2 )ar (ressure+

    /ota" aount of heat reuire!

    ; 66< > 100,.9 > ,,0, > 126 >

    ; 62

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    Prof. R. Shanthi 30

    (("ication: Heat =chan$ert is an in!ustria" eui(ent in hich heat is transferre! fro a hot

    f"ui! a "iui! or a $as4 to a co"! f"ui! another "iui! or $as4 ithout

    the to f"ui!s hain$ to i= to$ether or coe into !irect contact.

    Hot f"ui!

    at /Hin Hot f"ui!

    at /Hout

    Co"! f"ui!

    at /Cout

    Co"! f"ui!

    at /Cin

    Heat "ost )# the hot f"ui!

    ; Heat $aine! )# the co"! f"ui!

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    Prof. R. Shanthi 31

    (("ication: Heat =chan$er

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    Prof. R. Shanthi 32

    Heat =chan$er

    hotchot/HinK /Hout4 ; co"!cco"! /CoutK /Cin4. .

    Heat "ost )# the hot f"ui! ; Heat $aine! )# the co"! f"ui!

    ass f"o rate

    of hot f"ui!

    S(ecific heatof hot f"ui!

    ass f"o rate

    of co"! f"ui!

    S(ecific heatof co"! f"ui!

    /e(erature

    !ecrease in the

    hot f"ui!

    /e(erature

    increase in the

    co"! f"ui!

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    Prof. R. Shanthi 33

    Heat =chan$er

    hotchot/HinK /Hout4 ; co"!cco"! /CoutK /Cin4. .

    Heat "ost )# the hot f"ui! ; Heat $aine! )# the co"! f"ui!

    /he a)oe is true on"# un!er the fo""oin$ con!itions:

    14 Heat e=chan$er is e"" insu"ate! so that no heat is "ost to the

    enironent

    24 /here are no (hase chan$es occurrin$ ithin the heate=chan$er.

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    Prof. R. Shanthi 3,

    Heat =chan$er

    Heat "ost )# the hot f"ui! ; Heat $aine! )# the co"! f"ui! Heat "ost to the enironent

    f the heat e=chan$er is 7D/ e"" insu"ate! then

    * > ! " 1 i H h

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    Prof. R. Shanthi 35

    Hi$h (ressure "iui! ater at 10 MPa 100 )ar4 an!

    30oC enters a series of heatin$ tu)es. Su(erheate!stea at 1.5 MPa 15 )ar4 an! 200oC is s(ra#e! oer

    the tu)es an! a""oe! to con!ense. /he con!ense!

    stea turns into saturate! ater hich "eaes the

    heat e=chan$er. /he hi$h (ressure ater is to )e

    heate! u( to 1A0oC. *hat is the ass of stea

    reuire! (er unit ass of incoin$ "iui! ater+

    /he heat e=chan$er is assue! to )e e"" insu"ate!a!ia)atic4.

    *or>e! =a("e 1 in Heat =chan$er

    S " i > ! " 1 i h

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    Prof. R. Shanthi 36

    So"ution to *or>e! =a("e 1 in Heat =chan$er

    S " i * > ! " 1 i H h !

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    Prof. R. Shanthi 3A

    Hi$h (ressure 100 )ar4 ater enters at 30oC an! "eaes at 19'>$ oC4 = 1A0-304oC

    ; 5'>$

    INou cou"! ca"cu"ate the a)oe )# ta>in$ the !ifference in entha"(ies at

    the 2 $ien states fro ta)"es aai"a)"e.J

    So"ution to *or>e! =a("e 1 in Heat =chan$er cont!.

    S " i * > ! " 1 i H h !

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    Prof. R. Shanthi 3e! =a("e 1 in Heat =chan$er cont!.

    S " ti t * > ! " 1 i H t h t!

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    Prof. R. Shanthi 39

    Since there is no heat "oss fro the heater

    Heat "ost )# stea ; Heat $aine! )# hi$h (ressure aterMass f"o rate of stea = 1951 >'>$

    ; Mass f"o rate of ater = 5'>$

    Mass f"o rate of stea ' Mass f"o rate of ater

    ; 5$ of ater

    So"ution to *or>e! =a("e 1 in Heat =chan$er cont!.

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    Prof. R. Shanthi ,0

    Oie the !esi$n of a heat e=chan$erhich has the ost effectie heat

    transfer (ro(erties.

    ssi$nent

    @earning obEecti#es"3& To be able to appreciate heat transfer applications in pharmaceutical

    industry

    1& To become familiar with the wor%ing principles of #arious heateFchangers

    '& To get a mental picture of different heat eFchangers so that sol#ingheat transfer problems in class becomes more interesting

    * > ! " 2 i H t h

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    Prof. R. Shanthi ,1

    Stea enters a heat e=chan$er at 10 )ar an! 200oC an!

    "eaes it as saturate! ater at the sae (ressure. ee!-

    ater enters the heat e=chan$er at 25 )ar an!

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    Prof. R. Shanthi ,2

    - Stea enters at 10 )ar an! 200oC an! "eaes it as saturate! ater at

    the sae (ressure.- Saturation te(erature of ater at 10 )ar is 1A9.9oC.

    - ee!-ater enters the heat e=chan$er at 25 )ar an! $

    Mass f"o of stea ' Mass f"o of fee!-ater

    ; 333.9< ' 2066 ; 0.161A >$ strea ' >$ of ater

    So"ution to *or>e! =a("e 2 in Heat =chan$er

    S " ti t * > ! " 1 i H t h t!

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    Prof. R. Shanthi ,3

    f the fee!-ater "eain$ the heat e=chan$er is fe! !irect"# to a

    )oi"er to )e conerte! to stea at 25 )ar an! 300o

    C fin! the heatreuire! )# the )oi"er (er >$ of fee!-ater.

    -/e(erature of fee!-ater "eain$ the heat e=chan$er is 159.9oC-8oi"in$ (oint of ater at 25 )ar is 221.$

    ; 2,33 >'>$ of fee!-ater

    So"ution to *or>e! =a("e 1 in Heat =chan$er cont!.

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    Prof. R. Shanthi ,,

    Heat Transfer

    is the means by which

    energy mo#es from

    a hotter obEect to

    a colder obEect

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    Prof. R. Shanthi ,5

    9echanisms of Heat Transfer

    onductionis the flow of heat by direct contact between a warmer and acooler body.

    on#ectionis the flow of heat carried by mo#ing gas or li!uid.$warm air rises, gi#es up heat, cools, then falls&

    Gadiationis the flow of heat without need of an inter#ening medium.

    $by infrared radiation, or light&

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    Prof. R. Shanthi ,6

    Latent heat Con!uction

    Conection

    Ra!iation

    9echanisms of Heat Transfer

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    Prof. R. Shanthi ,A

    Con!uction

    HOT

    (lots of vibration)

    COLD

    (not much vibration)

    Heat travels

    along the rod

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    Prof. R. Shanthi , hain$ > ; 1.0, *'.B. /his is coere! on

    the outer surface ith 3 c "a#er of insu"atin$ ateria"

    hain$ > ; 0.0A *'.B. /he innerost surface is at 1000oC

    an! the outerost surface is at ,0oC. Ca"cu"ate the stea!#

    state heat transfer (er area.

    =a("e 1

    /inK /out. T='>4insu"ationT='>4firec"a#

    ;

    So"ution: *e start ith the euation

    =a("e 1 continue!

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    Prof. R. Shanthi 56

    =a("e 1 continue!

    1000K ,04 .

    0.03'0.0A40.21'1.0,4;

    ; 1522.6 *'2.

    =a("e 2

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    Prof. R. Shanthi 5A

    *e ant to re!uce the heat "oss in =a("e 1 to 960 *'2.

    *hat shou"! )e the insu"ation thic>ness+

    =a("e 2

    /inK /out

    .

    T='>4insu"ationT='>4firec"a#;

    So"ution: *e start ith the euation

    1000K ,04

    T=4insu"ation'0.0A40.21'1.0,4;

    .

    ; 960 *'2

    T=4insu"ation ; 5.6 c

    Con!uction throu$h ho""o c#"in!er

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    Prof. R. Shanthi 5L

    ;

    ri

    ro

    /i

    /o

    Con!uction throu$h the co(osite

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    Prof. R. Shanthi 59

    Con!uction throu$h the co(osite

    a"" in a ho""o-c#"in!er

    /iK /o.

    I"nr2'r14J ' 2U>L;

    r1

    r2

    /i

    /o

    r3

    Materia"

    I"nr3'r24J ' 2U>8L

    Materia" 8

    =a("e 3

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    Prof. R. Shanthi 60

    thic> a""e! tu)e of stain"ess stee" > ; 19 *'.B4 ith

    2-c inner !iaeter an! ,-c outer !iaeter is coere!ith a 3-c "a#er of as)estos insu"ation > ; 0.2 *'.B4.

    f the insi!e-a"" te(erature of the (i(e is aintaine! at

    600oC an! the outsi!e of the insu"ation at 100oC ca"cu"ate

    the heat "oss (er eter of "en$th.

    =a("e 3

    /iK /o.

    I"nr2'r14J ' 2U>L;

    I"nr3'r24J ' 2U>8L

    So"ution: *e start ith the euation

    =a("e 3 continue!

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    Prof. R. Shanthi 61

    =a("e 3 continue!

    2 U L 600 K 1004

    .

    I"n2'14J ' 19; I"n5'24J ' 0.2

    .

    L ; 6

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    Prof. R. Shanthi 62

    9echanisms of Heat Transfer

    onductionis the flow of heat by direct contact between a warmer and a

    cooler body.

    on#ection

    is the flow of heat carried by mo#ing gas or li!uid.$warm air rises, gi#es up heat, cools, then falls&

    Gadiationis the flow of heat without need of an inter#ening medium.

    $by infrared radiation, or light&

    on#ection

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    Prof. R. Shanthi 63

    on#ectionConvectionis the (rocess in hich heatis carrie! fro

    ("ace to ("ace )# the )u"> oeent of a fluid $as or

    "iui!4.

    Conection currents are set u( hen

    a (an of ater is heate!.

    on#ection

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    Prof. R. Shanthi 6,

    t e=("ains h# )reeEes coe fro the ocean in the !a#

    an! fro the "an! at ni$ht

    on#ection

    on#ection" B t L @ f li

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    Prof. R. Shanthi 65

    on#ection" BewtonLs @aw of ooling

    .

    con. ; h /surfaceK /f"ui!4

    rea e=(ose!

    Heat transfer coefficientin *'2.B4

    Heate! surface at /surface

    "oin$ f"ui! at /f"ui!

    on#ection" B t L @ f li

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    Prof. R. Shanthi 66

    .

    con.

    /surfaceK /f"ui!

    Heate! surface at /surface

    "oin$ f"ui! at /f"ui!

    ; 1'h4

    Convective heat resistancein B'*4

    on#ection" BewtonLs @aw of ooling

    =a("e ,

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    Prof. R. Shanthi 6A

    /he conection heat transfer coefficient )eteen a surface at 50oC an!

    a)ient air at 30oC is 20 *'2.B. Ca"cu"ate the heat f"u= "eain$ the

    surface )# conection.

    =a("e ,

    So"ution:

    Heate! surface at /surface ; 50oC

    "oin$ f"ui! at /f"ui! ; 30oC

    h ; 20 *'2.B

    .

    con.; h /surfaceK /f"ui!4

    ; 20 *'2.B4 = = 50-304oC

    . con.

    ; 20 = 20 ; ,00 *'2

    Heat f"u= "eain$ the surface:

    se 7etons La of coo"in$ :

    =a("e 5

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    Prof. R. Shanthi 64

    C#erall Heat Transfer through a Mlane Wall

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    Prof. R. Shanthi A3

    g

    . /

    K /1;

    1'h4

    /2

    K /8;

    1'h84

    /1

    K /2;

    T='>4

    . /K /8

    ;1'h4 1'h84 T='>4

    /K /84;

    1' ; 1'h 1'h8 T='>

    here is the oera"" heat transfer coefficient $ien )#

    .

    Dera"" heat transfer throu$h ho""o-c#"in!er

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    Prof. R. Shanthi A,

    $ #

    ri

    ro/i

    /o

    L

    /K /84;

    1' ; 1'hi4 1'h8o4

    .

    "ui! is insi!e the (i(e

    "ui! 8 is outsi!e the (i(e

    /X /8

    "nro'ri4 ' 2U>L

    here

    =a("e 6

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    Prof. R. Shanthi A5

    Stea at 120oC f"os in an insu"ate! (i(e. /he (i(e is

    i"! stee" > ; ,5 *' B4 an! has an insi!e ra!ius of 5c an! an outsi!e ra!ius of 5.5 c. /he (i(e is coere!

    ith a 2.5 c "a#er of ; 0.0A *' B4.

    /he insi!e heat transfer coefficient hi4 is

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    Prof. R. Shanthi A6

    =a("e 6 continue!

    1' ; 1'

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    Prof. R. Shanthi AA

    =a("e 6 continue!

    .

    120 K 354;

    ;

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    Prof. R. Shanthi A