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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>iaCO 2 Emissi<strong>on</strong> CoefficientThe CO 2 rating is d<strong>on</strong>e by calculating CO 2 emissi<strong>on</strong>coefficients (c CO2 ) that quantify the total amount of fossilfuel derived CO 2 , emitted to the atmosphere, per unitdelivered energy. As for the primary energy factor thesystem boundary comprises of power plants <strong>and</strong> DHN.Also the power b<strong>on</strong>us method is applied for calculatingthe DHN‘s specific CO 2 emissi<strong>on</strong>s. For the sake ofcompleteness it must be menti<strong>on</strong>ed that CO 2 -equivalentemissi<strong>on</strong>s of other greenhouse gases can opti<strong>on</strong>ally beincluded. However this has not been implemented intothis study, due to a lack of data. Similarly to the PEF theCO 2 emissi<strong>on</strong> coefficients for the base case arecalculated as:cCO2, DHiEF , icCO2, F , iQDHAnd for the modified plant as:cCO2, DHiEF , i cCO2, F , i P c P cQCO2, El .CO2, El .DH. EPyro cCO2, PyroE F,i , E Pyro , P <strong>and</strong> Q DH represent heat in fuels, heat inpyrolysis slurry <strong>and</strong> co-generated electricity <strong>and</strong> DHrespectively. Accordingly, c CO2,F,i , c CO2,Pyro , c CO2,El. <strong>and</strong>c CO2,DH are the related CO 2 emissi<strong>on</strong> coefficients. Thecorresp<strong>on</strong>ding values are given in table 2.RESULTSIn table 3, three simulati<strong>on</strong> cases are presented: thebase case (case 1), pyrolysis integrati<strong>on</strong> with the sameoperati<strong>on</strong> hours (case 2) <strong>and</strong> the maximum pyrolysisslurry producti<strong>on</strong> (case 3) with prol<strong>on</strong>ged operati<strong>on</strong>.hours <strong>and</strong> a DH load as low as 30% (matching 18% ofthe total DH load). It can be seen from the table that forall cases the DH output is the same for the 100-50%operating points. This results, in the first two cases, inan identical total DH output of 70.85 GWh. Thiscorresp<strong>on</strong>ds with 75% of the total yearly DH load. Dueto steam extracted to the dryer, the enthalpy flowthrough the turbine in part load is decreased, whichresults in a lower electricity producti<strong>on</strong> in part load forthe cases 2 <strong>and</strong> 3. Already for the sec<strong>on</strong>d casepyrolysis slurry with an energy c<strong>on</strong>tent in the samerange as the DH load can be produced. Fuel input,which is defined as wood burned in the boiler <strong>and</strong> woodentering the dryer for subsequent pyrolysis, increaseswith falling load for load levels 60% <strong>and</strong> higher. In thosecases the boiler combusti<strong>on</strong> power is 100%, but it isdecreased for lower load levels as explained above. Ifoperati<strong>on</strong> hours are extended by supplying lower DHloads with the CHP plant (case 3), total pyrolysis slurryproducti<strong>on</strong> can be increased by approximately 55%,electricity producti<strong>on</strong> by 7.8% compared to the basecase. Further DH producti<strong>on</strong> is increased byapproximately 14.7%, covering now 86% of the total DHdem<strong>and</strong>. This directly decreases the fossil fuelledbackup power as shown in table 4. The needed backupheat is almost cut in half. Together with the additi<strong>on</strong>allyproduced electricity this substantially improves theprimary energy factor to 0.68 which certainly will have apositive influence <strong>on</strong> the PEF of the buildings c<strong>on</strong>nectedto the DHN. For case 2 the improvement is marginal.The CO 2 emissi<strong>on</strong> coefficient changes somewhatc<strong>on</strong>troversially by increasing in the 2 nd case. This isbecause the loss in electricity b<strong>on</strong>us cannot becompensated by the produced pyrolysis slurry, since theCO 2 emissi<strong>on</strong> coefficients differ widely. However forcase 3 specific CO 2 emissi<strong>on</strong>s become even negative.The negative value is very unlikely to reach <strong>and</strong> can beexplained with the not fully accounted fuel producti<strong>on</strong>chain. Nevertheless, it is obvious that the DHN‘s CO 2emissi<strong>on</strong> factors can be c<strong>on</strong>siderably reduced with thepresented integrati<strong>on</strong> c<strong>on</strong>cept.173

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