Convection:Force and free convectionPhysicle mechanism of convectionWhat is h and determination of h?Velocity boundry layerThermal boundry layers Nuselt number Prandtl numberCritical Reynolds numberForced convection in tubes- Dittus and boelter co-relation-sieder and coalter co-relationForced convection outside the tubesChurchill and berstein co-relationWheitkher co-relationExample 7.5 and 7.6Flow across tube banksOverall heat transfer cofficient for plane and cylindricle wallsProblem 12.3Log mean temperature difference for co current and counter currentExample 9.1 Problem 9.5 and 9.6Examples 5.1,5.2,5.3 and 5.4Problem 5.1,5.2,5.3 and 5.4Problem 11.3

hto s-1.

conduction convection and radiation introduction example 1.1fourier la of heat conductionexample 1.5example 9.2 coulsonthermal conductivitythermal diffusivityexample 1.8general heat conduction equationexample 2.3one dimensional steady state conduction through plane wallexample 2.11one dimensional steady state conduction through composite wallthermal resistantproblem 2.23

example 9.3 coulsonexample 2.4example 3.1one dimensional steady state through conduction in cylinderone dimensional steady state conduction through steady state sphericle coordinateexample 2.15example 2.16criticle radius derivation

HTO S-3 SYALLABUS.....

caloric and wall temperatureintroduction of double pipe,compact ,shell and tube and plate frame heat exchangerDOUBLE PIPE HEAT EXCHANGERCALCULATION OF RENYOLD NUMBER FOR INNER PIPE FLOWING FLUIDFOULING FACTOR of DIRT FACTORPRELIMANRY DESIGN STEPS FOR HEAT EXCHANGEREXAMPLE #6.1 D Q KERNSHELL AND TUBE HEAT EXCHANGEREXAMPLE 7.3 D Q KERNEFFECTIVENESS -NTU (CENGEL CHAPTER 13 ) TOPIC 13.5EXAMPLE 13.7 AND 13.5 FROM CENGELEXAMPLE #9.29 FROM COULSON VOLUME 1...EVAPORATION ...... TYPES ARE IMPORTANT EXAMPLE 16.2 FORM MECAB AND SMITH