Experimental Study and Investigation of Helical Pipe Heat Exchanger with Varying Pitch

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Experimental Study and Investigation of Helical Pipe Heat Exchanger with Varying Pitch

1M.Tech student, Thermal Engineering, Department of Mechanical Engineering, Newton’s Institute of Science & Technology, Macherla, A.P.

2Assistant Professor, Department of Mechanical Engineering, Newton’s Institute of Science & Technology, Macherla, A.P.

3 Assistant Professor & HOD, Department of Mechanical Engineering, Newton’s Institute of Science & Technology, Macherla, A.P.

Abstract -

Heat exchangers are the most researched and constantly evolved devices in the research industry. This projectisanattemptonexperimentalinvestigationofhelical coilheatexchangersanditsbesteffectivenessfordifferent pitchvaluesbuttherestofthedimensionskeptconstant.In theprocessofenhancingtheheattransfercapacityofheat exchangersthehelicalpipeheatexchangershavecomeinas apassivemethodofheatenhancement.Thereasonforthis wouldbethattheflowinthehelicalcoilsalwaysproducesa secondary flow component to the radial velocity. This additionalcomponentistheresultofcentrifugalforcedueto flowinthecurvature.

Present research work is to understand more behavioraleffectsonthehelicalpipeheatexchangeronthe pitch of the helix is selected. Normal design procedure is followedtodesigntheheatexchangerbuttheoptiontovary thepitchofthehelixisprovided.

Thehelicalcoilisenclosedinavesseltosimulatetheshell side of heat exchanger. The cold fluid enters the shell throughthebottomconnectionandflowsup.Itleavesthe shell through the outlet at the top. The coil is welded to a bottomflangeplateinsuchawaythatcoilassemblyremains fixedatthebottomoftheassembly.Byvaryingtheflowrates ofthehotandcoldwaterexperimentwasconductedforall thepithselected.Theeffectivenesswascalculatedforeach case.Resultsandplotswererecorded

Key Words: helicalpipeheatexchanger,helixpitch

1. INTRODUCTION

Heatexchangersarethemostresearchedandconstantly evolved devices in the research industry. Basically a Heat exchangerisadevicethataccommodatesthetransferofheat from one fluid to other. It basically consists of an arrangementtoallow twofluids;usuallyliquids to flow in twodifferentpassagesmaybeconcentrictubesoranyother pattern.

Asweknowheatexchangerisadeviceinwhichtheheat energyintheformofenthalpyistransferredfromonefluidto another fluid through the solid medium with or without externalworkinvolved.Majorapplicationofheatexchangers involve the heat transfer between the two fluids either evaporation or condensation or just controlling the temperature of the fluid of concern. In many medical or chemicalindustryrelatedapplicationsitwouldbewith an intentionofsterilizing,pasteurizing,distilling,fractionating, crystallizingoralso controlprocessthefluid.

1.1 Shell And Tube Heat Exchanger

Ashellandtubeheatexchangerisoneoftheclassesofheat exchangertypes.Itisthemostcommonlyusedtypeofheat exchangerinchemicalprocessesandotheroilrefineries.This typeofheatexchangerisbestsuitedforhigh-pressureand high-temperatureapplications.Thistypeofheatexchanger basicallyconsistsofashell(alargeenclosuretowithstand pressure)withasingleorbundleoftubesenclosed.Amongst the two fluids, one flows through the shell and the other through the tubes. The surface of the tubes helps the heat transferfromtheouterflowingfluidtotheinsidefluidorvice versadependingonthetemperaturegradientbetweenthe twofluids.Ifasetoftubesisenclosedintheshellthenthat setiscalledbundleoftubes.Atubebundlemaybecomposed bydifferenttypesoftubeswithorwithoutfinslongitudinally attachedtothetubes.Thefigurebelowshowsatypicalshell andtubeheatexchangers.

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 03 | Mar 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page93
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Fig1.1:TypicalShellAndTubeHeatExchanger

1.2 Helical Pipe Heat Exchanger

Inthistypeofheatexchangerthetubeisformedintothe helical pipe and placed inside the shell. This provides a secondaryflowtothefluidflowinginthispipe.Aschematic ofthehelicalpipeheatexchangerisshowninthefollowing figure.

Fig1.2:HelicalPipeHeatExchanger

Intheprocessofenhancingtheheattransfercapacityof heatexchangersthehelicalpipeheatexchangershavecome inasapassivemethodofheatenhancement.Thereasonfor this would be that the flow in the helical coils always producesasecondaryflowcomponenttotheradialvelocity. Thisadditionalcomponentistheresultofcentrifugalforce duetoflowinthecurvature.

Aslotofliteratureisavailabletoproveabouttheflowpattern thatisgeneratedinthehelicalandothercurvedchannels.It isalsoseenthatasymmetricalpairedvorticesusuallyaffects the main flow stream of thefluid. Also the details of these flowcharacteristicsarediscussedintheliteraturesurvey.

2. EXPERIMENTAL SETUP

Thepipeusedtoconstructthehelicalsectionhas10mm inside diameter and 12.7mm outer diameter. The tube materialiscopper.ThePitchCircleDiameter(PCD)ofthecoil is80mmandtubepitchis20mm.Theremainingpartsofthe setuparemadeofmildsteel.Thehelicalcoilisenclosedina vesseltosimulatetheshellsideofheatexchanger.Thecold fluid enters the shell through the bottom connection and flowsup.Itleavestheshellthroughtheoutletatthetop.The coilisweldedtoabottomflangeplateinsuchawaythatcoil assembly remains fixed at the bottom of the assembly. A manuallycontrolledmechanismisprovidedtopushandpull thecoilaccordingtotheneed.

The helical coil test section is connected to a loop, which providesthenecessaryflowthroughthetubeandshellside ofthetestsectionandtherequiredinstrumentation.Atank with electric heater is provided to heat the water to be circulated through the helical coil with a total power of 2000W.Themanufacturedexperimentalsetupisasshownin thefollowingfigure.

Intheprocessofenhancingtheheattransfercapacityofa heatexchangersthehelicalpipeheatexchangershavecome inasapassivemethodofheatenhancement.Thereasonfor this would be that the flow in the helical coils always producesasecondaryflowcomponenttotheradialvelocity.

3. METHODOLOGY

3.1

Design Procedure

Thedesignwascalculatedasperthefollowingequations

1)ThecoiltubelengthLforNnumberofturns

2)Thevolumeutilizedbythecoil,Vc:

(π/4)d20L (2)

3)Annulusvolumeavailable,Va:

π/4)(C2–B2)��N (3)

4)Theavailablevolumeforthefluidtoflowintheannulus, Vf:

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 03 | Mar 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page94
Fig2.1:experimentalsetup Fig3.1:sectionalviewofthehelicalcoilheatexchanger
��=��√(2����)2
��2 (1)
+
Vc=
Va=
(
Vf=����–��c
(4)

5)Equivalentdiameterofthecoiledtubeforshell-side, De:

����=4����/�������� (5)

3.2 Design Calculations

AssumedNumberofcoilsN=10

Radiusofthehelicalisr=80mm

Pitchofthehelicalisp=20mm

do=80+6.35=86.35mm

di=80-6.35=73.65mm

B=73.35–6.35=67.3mm

C=86.35+(1.5∗12.7)=105.4mm

Therefore:

��=10√(2��80)2+202=2016mm=2.016m

Vc=(π/4)86.352∗2016=1470m3

Va=(π/4)(105.42–67.32)20∗10=1.033m3

����=14.70−1.033=13.667m3

����=(4∗13.667∗106)/(π∗86.35∗2016)=99.96mm

4. RESULTS AND DISCUSSION

The experiment was conducted for different parameters.Theresultsaretabulatedasfollows.

Case 1: Full Length

4.1 Gap between Coils = 20 Mm, Parallel Flow & Full Length

4.1.1ForConstantColdwaterflowas1LPM

Sample Calculation

Heat Flow capacity of cold water:

Cc=mcCpcwhereforwaterCpc=4.187kJ/kgK

mc=1LPM=(1000*10-6*1000)/60=0.0167kg/s

∴Cc=0.0167*4.187=69.91121kJ/K

Heat Flow capacity of Hot water:

Ch=mhCphwhereforwaterCph=4.187kJ/kgK

.mh=1LPM=(600*106*1000)/60=0.01kg/s

∴Ch=0.0167*4.187=41.87kJ/K

Fromtheabovewecanseethat:

Cmin=41.87kJ/KandCmax=69.91121kJ/K

Maximum Heat transfer theoretically:

Qmax=Cmin(th1–tc1)=41.87(69–38)=1297.753kJ /s

Heat Transfer in Cold water:

Qc=mc(tc2–tc1)=0.0167(43–38)=349.5978kJ/s

Heat Transfer in hot water:

Qh=mh

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 03 | Mar 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page95
Table4.1Temperaturesrecordedfor20mmgapbetween coils1LPMColdwaterconstantflow Table4.2:CalculatedEffectivenessfor20mmgapbetween coils1LPMColdwaterconstantflow Fig4.1:Plotforeffectiveness20mmgapbetweencoils, Parallelflow,ColdwaterFlowrate1LPM
(th1
th2
=0.01(69–46)=1608.15kJ/s HotWater Temperature0C ColdWater Temperature0C FlowRateOf HotWater (kg/s) FlowRateOf ColdWater (kg/s) Inlet Outlet Inlet Outlet 0.01 0.0167 69 46 38 43 0.0133 0.0167 69 57 39 47 0.0167 0.0167 69 56 38 47 Ch Cc Cmin Qmax Qh Qc Q Ε 41.86 69.91 41.86 1297.75 1608.15 349.59 978.87 0.75 55.67 69.91 55.67 1670.33 839.03 559.35 699.19 0.41 69.91 69.91 69.91 2167.24 908.95 629.27 769.11 0.35
)

Average Heat transfer:

Q=(Qh+Qc)/2=(1608.15+359.5978)/2=978.8738

Effectiveness:

ε=(Q/Qavg)=978.8738/1297.753

ε=0.754284

4.1.2 For Constant Hot water flow as 1 LPM

Fig4.3Plotforeffectiveness20mmGapbetweencoils, Counterflow,ColdwaterFlowrate1LPM

4.2.2 For Constant Hot water flow as 1 LPM

Fig4.2:Plotforeffectiveness20mmGapbetweencoils, Parallelflow,HotwaterFlowrate1LPM

4.2 Gap between Coils = 20 Mm, Counter Flow & Full Length

Fig4.4:Plotforeffectiveness20mmGapbetweencoils, Counterflow, HotwaterFlowrate1LPM

Similarlytheworkwascontinuedfor10mmpitchand0mm pitchforfulllengthpipewithsameflowconditionsincold andhotflowandtheresultsareshownbelow.

Table4.3:Temperaturesrecordedfor20mmgapbetween coils1LPMColdwaterconstantflow

4.2.1 For Constant Cold water flow as 1 LPM

Table4.4:CalculatedEffectivenessfor20mmgapbetween coils1LPMColdwaterconstantflow

© 2023, IRJET | Impact Factor value: 8.226

Fig4.5:PlotforeffectivenessVsMassflowrate consolidatedforparallelflow(coldwaterflowrate1LPM)

International
of
and
(IRJET) e-ISSN: 2395-0056 Volume:
Issue:
| Mar 2023 www.irjet.net p-ISSN: 2395-0072
| ISO 9001:2008 Certified Journal | Page96
Research Journal
Engineering
Technology
10
03
HotWater Temperature 0C ColdWater Temperature 0C FlowRateOf HotWater (kg/s) FlowRateOf ColdWater (kg/s) Inlet Outlet Inlet Outlet 0.01 0.0167 70 53 36 49 0.0133 0.0167 69 56 38 50 0.0167 0.0167 69 57 37 50 Ch Cc Cmin Qmax Qh Qc Q Ε 41.86 69.91 41.86 142334 1188.63 908.95 1048.79 0.73 55.67 69.91 55.67 1781.68 978.87 839.03 908.95 0.51 69.91 69.91 69.91 2237.15 839.03 908.95 873.99 0.39

1LPM)

For half length:

1LPM)

Fig

foreffectivenessVsMassflowrate

forparallelflow,forhalflength(coldwater flowrate1LPM)

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 03 | Mar 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page97
Fig4.6:PlotforeffectivenessVsMassflowrate consolidatedforcounterflow.(coldwaterflowrate1LPM) Fig4.7:PlotforeffectivenessVsMassflowrate consolidatedforParallelflow(Hotwaterflowrate Fig4.8:PlotforeffectivenessVsMassflowrate consolidatedforcounterflow(Hotwaterflowrate 4.9:Plot consolidated Fig4.10:PlotforeffectivenessVsMassflowrate consolidatedforcounterflow,forhalflength(coldwater flowrate1LPM) Fig4.11:PlotforeffectivenessVsMassflowrate consolidatedforParallelflow,forhalflength(Hotwater flowrate1LPM)

5. CONCLUSIONS

Theheatexchangerwasdesignedfirstaccordingtothe normal design procedure. The heat exchanger was manufacturedasthedimensionsobtainedfromthedesign. Thesamewasrepeatedforthedifferentflowratesofthecold water,keepingthehotwaterflowrateconstant.Effectiveness wascalculatedforalltheflowrates.Theworkwasdonefor

pitch of 20 mm,10 mm,0 mm in full lengthand halflength conditions.

Weobservethattheeffectivenessingeneralreduceswiththe increaseofthemassflowrateirrespectiveofthepitch.

Fromtheresearchitcanbeeasilyconcludefromtheresults thatwhenthegapbetweenthecoilswas10mmand0mm theeffectivenesswasconsistentforbothparallelandcounter flow arrangements, in both half length and full length readings.

The consolidated graphs plotted also reveal for the half length readings that the length chosen according to the designi.e.2misaccurateandthelengthofthecopperpipe cannotbereducedfurther.

Itisbeenobservedthatwhenpowerlosseswerecalculated and plotted accordingly, the maximum power loss has occurredwhentheflowrateofcoldfluidwas0.6kg/sat10 mm gap between the coils for counter flow. And the value was 72.76%. It is also observed that the minimum power losses are occurred at when the hot fluid flow rate was maintainedat0.6kg/swhentherewasnogapbetweenthe coils for parallel flow arrangement. And the value was 25.58%.

REFERENCES

[1] “Numericalandexperimentalstudiesofadoublepipe helical heat exchanger” by Timothy j. Rennie department of bioresource engineering, mcgill university, montreal, submitted august 2004, a thesis submitted to mcgilluniversityinpartialfulfillmentoftherequirementsof thedegreeofdoctorofphilosophy.

[2] “Helically Coiled Heat Exchangers - Basic design Applications” by J. S. Jayakumar Professor, Dept. of Mechanical Engineering, Amrita Vishwa Vidyapeetham, AmritaSchoolofEngineering,Amritapuri,Kollam,India.

[3] “FabricationandAnalysisofTube-In-TubeHelical Coil Heat Exchanger” by Mrunal P.Kshirsagar, Trupti J. Kansara, Swapnil M. Aher, International Journal of EngineeringResearchandGeneralScienceVolume2,Issue3, April-May2014ISSN2091-2730.

[4] “ Thermal Analysis of a Helical Coil Heat Exchanger”by Amol Andhare, V M Kriplani, J P Modak, International Journal of Innovative Research in Advanced Engineering(IJIRAE)ISSN:2349-2163

[5] “Thermal Analysis Validation for Different Design TubesinaHeatExchanger”byRoshan.V.MarodeandAshok. J.Keche,InternationalJournalofEngineeringResearchand GeneralScienceVolume3,Issue1,January-February,2015, ISSN2091-2730.

International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 03 | Mar 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page98
Fig4.12:PlotforeffectivenessVsMassflowrate consolidatedforcounterflowforhalflength(Hotwater flowrate1LPM) 4.3 POWER LOSSES Fig4.13:losseswhencoldwaterflowratemaintainedat 0.0167kg/s. Fig4.13:losseswhenhotwaterflowratemaintainedat 0.0167kg/s

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