The <str<strong>on</strong>g>12th</str<strong>on</strong>g> <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g> <strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong> <strong>Cooling</strong>,September 5 th to September 7 th , 2010, Tallinn, Est<strong>on</strong>iaThe governing equati<strong>on</strong>s then change to:[8]Table 8 Pipe temperature predicati<strong>on</strong> comparis<strong>on</strong> (supplyoutlet temperature is c<strong>on</strong>trolled at 50 o C)WhereThe boundary c<strong>on</strong>diti<strong>on</strong>s change to :[9]The system linear ordinary differential equati<strong>on</strong>s can besolved with Eigen value method or with Laplacetransformati<strong>on</strong>. The Laplace transformati<strong>on</strong> wasapplied in this study. Eq. 8 is transformed to:The final soluti<strong>on</strong>s are given as:Where :[10][11][12], [13], [14]Tws- DN32, which is the l<strong>on</strong>gest main pipe in HE ofcase 1, is selected for the assessment with U 1 =0.141<strong>and</strong> U 2 =0.0523. The pipe length is assumed 500 m.Ground temperature ranges from 0 to 15 o C. The inletof supply <strong>and</strong> return temperatures are known as 55 o C<strong>and</strong> 22 o C respectively. The outlet temperature ofsupply pipe is c<strong>on</strong>trolled as 50 o C <strong>and</strong> 45 o C,respectively.Table 8 shows the temperature predicti<strong>on</strong> based <strong>on</strong>single pipe simplificati<strong>on</strong> <strong>and</strong> the coupled pipeequati<strong>on</strong>s. T_Difference represents the coupledsoluti<strong>on</strong> minus the single pipe soluti<strong>on</strong>. When thetemperature drop al<strong>on</strong>g the supply pipe is c<strong>on</strong>trolled at5 o C, the predicti<strong>on</strong> between the single pipe <strong>and</strong> thecoupled pipe is very close. The predicti<strong>on</strong> errorsincrease with increase the ground temperature. Thesingle pipe approach predicts lower supply watertemperature <strong>and</strong> higher return temperature than thoseof coupled pipe soluti<strong>on</strong>s. It was also observed thatwhen the ground temperature is higher than 4 o C, thenet heat transfer effect in the return pipe is to absorbheat to the surrounding.79The by-pass water temperature in this study was set ina c<strong>on</strong>servative way. In many practices, the by-passwater can be set 10 °C lower than the supply watertemperature. Even lower by-pass temperature isproposed for the low temperature district heatingnetwork [3]. Table 9 shows the simulati<strong>on</strong> results based<strong>on</strong> a10 °C temperature drop al<strong>on</strong>g the supply pipe. Itshows the predicti<strong>on</strong> errors increase in both supply <strong>and</strong>return pipes. The heat transfer was predicted in areverse trend in the return pipe at 4 °C. C<strong>on</strong>siderablepredicti<strong>on</strong> error was found in the return pipe at highground temperature.It is worth to be noted that the increase of supplytemperature drop has more influence <strong>on</strong> the return pipetemperature predicti<strong>on</strong> than that of supply pipe. Thereas<strong>on</strong> can be explained from the expressi<strong>on</strong> of U s <strong>and</strong>U r in Eq. 1–2. As the magnitude of T s -T g is higher thanT r -T g , the same amount of return water temperaturevariati<strong>on</strong> will have more influence <strong>on</strong> U r than U s ,therefore causes a larger predicti<strong>on</strong> error in the returnpipe than in the supply pipe.Table 9 Pipe temperature predicati<strong>on</strong> comparis<strong>on</strong> (supplyoutlet temperature is c<strong>on</strong>trolled at 45 o C)CONCLUSIONIn this paper, a preliminary study was c<strong>on</strong>ducted <strong>on</strong> theinfluence of by-pass flow <strong>on</strong> the network return watertemperature in a designed low temperature DHnetwork. The c<strong>on</strong>cept of supply water recirculati<strong>on</strong> was
The <str<strong>on</strong>g>12th</str<strong>on</strong>g> <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g> <strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong> <strong>Cooling</strong>,September 5 th to September 7 th , 2010, Tallinn, Est<strong>on</strong>iaintroduced to avoid the mixing of by-pass water to thereturn water. Double pipe water supply c<strong>on</strong>cept wastested to use the recirculati<strong>on</strong> pipe supply water duringwinter seas<strong>on</strong>. Two different house installati<strong>on</strong> modeswere c<strong>on</strong>sidered in the analysis.The by-pass water significantly increases the returnwater temperature in the traditi<strong>on</strong>al design. The mixedreturn temperature can reach 35.5 o C for HE <strong>and</strong>45.6 o C for DHWS. With applying the by-pass waterrecirculati<strong>on</strong>, this return temperature can be maintainedat 22 o C, while the re-circulated by-pass water can bekept as high as 44 o C <strong>and</strong> 53.5 o C for HE <strong>and</strong> DHWS atthe plant, respectively. It was found that the doublepipe supply leads to the highest network heat loss.However, the c<strong>on</strong>clusi<strong>on</strong> that whether the c<strong>on</strong>cept ofdouble pipe supply is inferior to other network designmethods can <strong>on</strong>ly be drawn after further networkthermal-ec<strong>on</strong>omic optimizati<strong>on</strong>.The simulati<strong>on</strong> program simplifies the twin pipe heattransfer predicti<strong>on</strong> as a single pipe, <strong>and</strong> neglects thereturn pipe heat loss when the return pipe absorbs heatfrom the surroundings. The temperature predicti<strong>on</strong>errors due to the single pipe assumpti<strong>on</strong> were analyzedthrough solving the coupled supply/return pipedifferential energy equati<strong>on</strong>s. The predicti<strong>on</strong> errorsincrease with increase the allowable temperature dropin the network. C<strong>on</strong>siderable error was found for thereturn pipe at high ground temperature.NOMENCLATUREc p = specific heat capacity [ J/kg.K]q = Heat transfer rate [kW / m]s = Laplace transform variableT = Temperature [ K]U = Overall heat transfer coefficient [ kW /m.K]U ij = Linear thermal transmittance [kW/m.K]= mass flow rate [ kg/s]Greek Letter = Dimensi<strong>on</strong>less temperatureSubscriptsg = Undistributed groundr = Returns = Supplyu = Upstreamd = DownstreamAbbreviati<strong>on</strong>DH = <strong>District</strong> heatingHE = Heat exchangerDHWS = Domestic hot water storage tankREFERENCE[1] H. Lund, B. Moller, B. V. Mathiesen, A. Dyrelund, ―The role of district heating in future renewableenergy systems‖, Energy, 35, pp. 1381-1390,2010.[2] Charlotte Reidhav, Sven Werner, ―Profitability ofsparse district heating‖, Appliced Energy, 85, pp.867-877.[3] ―Udvikling og Dem<strong>on</strong>strati<strong>on</strong> af Lavenergifjernvarmetil Lavenergibyggeri‖, EFP 2007.[4] TERMIS Help Manual, Versi<strong>on</strong> 2.093,7-Technologies A/S.[5] Dansk St<strong>and</strong>ard DS 439, 2000. Norm forv<strong>and</strong>installati<strong>on</strong>er, Code of Practice for domesticwater supply installati<strong>on</strong>s, 3. udgave, www.ds.dk.[6] Otto Paulsen, Jianhua Fan, Sim<strong>on</strong> Furbo, Jan EricThorsen, ―C<strong>on</strong>sumer Unit for Low Energy <strong>District</strong><strong>Heating</strong> Net‖, The 11th <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g><strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong> <strong>Cooling</strong>, 2008, Icel<strong>and</strong>.[7] P. K. Olsen, et.al, ―A new low-temperature districtheating system for low energy buildings‖, the 11th<str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g> <str<strong>on</strong>g>Symposium</str<strong>on</strong>g> <strong>on</strong> <strong>District</strong> <strong>Heating</strong> <strong>and</strong><strong>Cooling</strong>, Icel<strong>and</strong>, 2008.[8] Logstor. http://www.logstor.com/[9] Benny Bohm, Halldor Kristjanss<strong>on</strong>, ―Single, twin<strong>and</strong> triple buried heating pipes: <strong>on</strong> potentialsavings in heat losses <strong>and</strong> costs‖, <str<strong>on</strong>g>Internati<strong>on</strong>al</str<strong>on</strong>g>Journal of Energy Research, 29, pp. 1301-1312,2005.[10] P.Walleten, ―Steady-state heat loss from insulatedpipes‖, Thesis, Lund Institute of Technology,Sweden, 1991.80
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academic access is facilitated as t
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