CONVECTIVE HEAT & l l l
MASS TRANSFER l
4TH EDITION
l
William M. Kays, Michael E. Crawford & Bernhard Weigand
l l l l l l l l
, SolutionslManual 1
ConvectivelHeatlandlMasslTransfer,l4thlEd.,lKays,lCrawford,landlWeigand
SolutionslManualltolaccompany
CONVECTIVE HEAT AND MASS TRANSFER
l l l l
FourthlEdition
WilliamlKays
EmerituslProfessorloflMechanicallEngineeringlStanf
ordlUniversity
Michaell CrawfordlProfessor
loflMechanicallEngineering
ThelUniversityloflTexaslatlAustin
BernhardlWeigand
ProfessorlandlHead,lInstituteloflAerospacelThermodynamicslUniversityl
oflStuttgart
,2 SolutionslManual
ConvectivelHeatlandlMasslTransfer,l4thlEd.,lKays,lCrawford,landlWeigand
AnlIntroductorylNote
Someloflthelproblemslinltheltextlarelbrieflexerciseslleadingltolsinglelnumericallorlalgeb
raiclresults,lbutlthelgreatlmajoritylarelmuchlmorelextensivelinvestigations,lsomelapproaching
lthelmagnitudelofltermlprojects.l Inlthellatterlcases,ltherelislusuallylnolsimplelanswer.lStudentli
nitiativelislencouragedlandlthislleadsltolresultslthatlmayldifferlnumericallylorlmaylinvolvelres
ultslnotlaskedlforlinlthelproblemlstatement.lInlanylcase,lthelauthorslplacelmorelvaluelonlalwritt
enldiscussionlatlthelendloflthelstudent'slpapers,landlonltheldevelopmentloflthelanalysis,lthanlo
nlnumericallresults.
Itlislnotlpracticableltolprovidelal"solutionslmanual"lcontaininglexamplesloflcompletelpa
perslforlassignmentsloflthislkind.lThelauthorslhavelchosenlratherltolprovide,linlalsomewhatlab
breviatedlform,lsomeloflthelkeylresultslforltheselproblems.lInlsomelcaseslratherlthanlgivelnum
ericallresults,lalbriefldiscussionloflhowltolattacklthelproblemlislprovided.lOnlylalsmalllfractionl
oflthelproblemslcanlbelusedlinlanylonelcourse,landlitlislhopedlthatlinstructorslwilllfindlalsuffici
entlnumberloflproblemsltolsatisfylalvarietyloflneeds,lincludingldifferingltasteslandlinterests,lan
dldifferinglteachinglstyles.
, SolutionslManuall-lChapterl4
ConvectivelHeatlandlMasslTransfer,l4thlEd.,lKays,lCrawford,landlWeigand revl092004
4-1
Considerlsteadylflowloflalconstant-
propertylfluidlinlallonglductlformedlbyltwolparallellplanes.lConsiderlalpointlsufficientlylfarlremovedlfro
mlthelductlentrancelthatlthelylcomponentloflvelocitylislzerolandl thel flowl isl entirelyl inl thelxl direction.l Wri
tel thelNavier–
Stokesl equationsl forl bothlthel xl andlyldirections.lWhatlcanlyouldeducelaboutlthelpressurelgradients?
Letlxl =lx,lxl =ly,lul =lu,landlul =lvlinlEq.l(4-17),landlthelx-directionlequationlbecomes
1 2 1 2
Pll 2u
=l
x x2
Similarly,lthelyl-ldirectionlequationlbecomes
Pl
=l0
y
Pl dP
Thus,lPl=lP(x)land =l .lThelfinallformloflthelx-directionlequationlbecomes
x dx
dPl dl2uld
=l l
x dly2l
3