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12th International Symposium on District Heating and Cooling

12th International Symposium on District Heating and Cooling

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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>iac<strong>on</strong>trol logics for building automati<strong>on</strong>, which are todayoften used for c<strong>on</strong>trolling DH substati<strong>on</strong>s. The c<strong>on</strong>trolmethod suggests how the flow can be determined foreach heat load. The flow is regulated by adjusting thepump‘s rotating speed. Speed-c<strong>on</strong>trolled pumps arecomm<strong>on</strong>ly used nowadays <strong>and</strong> they provide a superiorc<strong>on</strong>trollability [1], [10].Table 1: A summary of flow-weighted mean primary returntemperatures (bold) <strong>and</strong> resulting reducti<strong>on</strong> for varioustemperature programmes.Let us first study an example of an optimal c<strong>on</strong>trolcurve for a 100 % oversized system. Such a curve ispresented in Fig. 1, which also shows the relativemagnitude of the varying radiator flow in relati<strong>on</strong> to therequired flow. The blue dashed line in the diagramcorresp<strong>on</strong>ds to the primary return temperature. For thesake of comparis<strong>on</strong>, the primary return temperature fora 55/45 °C system is also shown (gray dashed line).Temperature [ C]Rel. flow [%]10090807060504030755025Primary return temperature reducti<strong>on</strong>0-15 -10 -5 0 5 10 15Outdoor temperature [C]T p,sT p,r,optT s,s,optT s,r,optT p,r,55/45Fig. 1 Temperatures with an optimised temperature curve<strong>and</strong> a variable flow in a 100% oversized system. Theprimary return temperature from a 55/45 °C programme isshown for comparis<strong>on</strong>.Flow-weighted, yearly mean primary returntemperatures from the radiator HEX have beencalculated with regard to the outdoor temperaturedurati<strong>on</strong>. Above the dashed line in Table 1, results areshown for a correctly dimensi<strong>on</strong>ed system, with an80/60°C programme as well as with an optimisedprogramme. The gain is estimated to just under twodegrees C. The last column shows how the primaryreturn temperature is affected when the length of theHEX is doubled. This comparis<strong>on</strong> can be justified bythe fact that the primary return temperature issignificantly influenced by the lower sec<strong>on</strong>dary flow thatthe optimisati<strong>on</strong> entails, while the pressure drop <strong>and</strong>heat transfer rate in the HEX can remain at amagnitude close to the original <strong>on</strong>es.m sUnder the dashed line, results are shown for a systemthat is oversized by 100 %. The first three temperatureprogrammes are 55/45, 60/40 <strong>and</strong> 80/30 °C, whereasthe last two are optimised <strong>on</strong>es with variable flow.The following c<strong>on</strong>clusi<strong>on</strong>s could be drawn from thetable: The oversizing of a radiator system leads, in itself,to a significant reducti<strong>on</strong> of the primary returntemperature, provided that some kind ofcompensati<strong>on</strong> has been made in order for thesystem to work properly, i.e., that an accurateindoor temperature has been provided. By optimising the system (through the use of avariable sec<strong>on</strong>dary flow), the primary returntemperature can be further reduced, especially ifthe system is oversized. By extending the radiator HEX, the returntemperature can be further reduced with thetemperature programmes that employ a relativelylow flow. Regardless of the degree of oversizing, acombinati<strong>on</strong> of an optimised temperatureprogramme <strong>and</strong> an extended HEX provides asubstantially reduced primary return temperature.The values presented in the table have been calculated<strong>on</strong>ly for the radiator HEX. When c<strong>on</strong>sidering thesubstati<strong>on</strong>‘s total return temperature, it can be said tobe smoothed by the DHW c<strong>on</strong>sumpti<strong>on</strong>. Calculati<strong>on</strong>scorresp<strong>on</strong>ding to those in Table 1 for a parallel <strong>and</strong> a 2-stage substati<strong>on</strong> for 20 flats (based <strong>on</strong> the Swedish<strong>District</strong> <strong>Heating</strong> Associati<strong>on</strong>‘s recommendati<strong>on</strong>s forsizing) result in reducti<strong>on</strong>s in the return temperaturethat are approximately 20 % lower than the valuesshown in the table. The difference between the parallel<strong>and</strong> the 2-stage c<strong>on</strong>necti<strong>on</strong> is negligible when thereturn temperature from the radiator HEX is low ormoderate, a fact that has been previously207

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