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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>iaapplicati<strong>on</strong>s. Low-temperature district heating systemsare defined as networks where fluids at a temperaturebelow 50 °C are used, while a medium-temperaturedistrict heating system is defined as using fluids attemperatures not higher than 70 °C [11, 12].Steady-state heat losses from pre-insulated buriedpipes are generally treated by use of the followingequati<strong>on</strong> [10], which is valid for each pipe-i:where Uij is the heat transfer coefficient between pipe-i<strong>and</strong> pipe-j, Tj is the temperature of the water in pipe-j<strong>and</strong> T0 is the temperature of the ground. In case of twoburied pipes, which is the most comm<strong>on</strong> applicati<strong>on</strong> inthe DH sector, the heat losses can be calculated asfollows, respectively for the supply pipe <strong>and</strong> the returnpipe, where T1 is the supply temperature <strong>and</strong> T2 is thereturn temperature.(1)Supply pipe: (2)Return pipe: (3)Equati<strong>on</strong>s (2) <strong>and</strong> (3) show how the heat transfer fromeach pipe can be seen as linear superimpositi<strong>on</strong> of twoheat fluxes, the first <strong>on</strong>e describing the heat transferbetween the pipe <strong>and</strong> the ground, the sec<strong>on</strong>d <strong>on</strong>erepresenting the heat transfer between the supply pipe<strong>and</strong> the return pipe. The equati<strong>on</strong>s can also bere-arranged in the following way:thermal coefficient, which is functi<strong>on</strong> of the temperaturein this case. U-values are dependent both <strong>on</strong>temperature <strong>and</strong> time. If the time-dependency due tothe ageing of the foam can be restrained by introducingeffective diffusi<strong>on</strong> barriers, that is not true for theintrinsic dependency <strong>on</strong> temperature. It is practice toevaluate the steady state heat loss applying a thermalc<strong>on</strong>ductivity value that corresp<strong>on</strong>ds to a hypothesizedmean temperature of the insulati<strong>on</strong>. Nevertheless weneed models based, for example, <strong>on</strong> the finite elementmethod (FEM) when complex geometries or a highdegree of detail are requested.Temperature dependant thermal c<strong>on</strong>ductivity ofPUR insulati<strong>on</strong> foamIn this paragraph the authors want to explain <strong>and</strong>dem<strong>on</strong>strate the importance of taking into account thetemperature-dependency of the thermal c<strong>on</strong>ductivity ofthe insulati<strong>on</strong> (lambda-value). The temperaturegradient in the insulati<strong>on</strong> foam in the radial directi<strong>on</strong> isoften higher then 10 °C/cm, meaning that the thermalc<strong>on</strong>ductivity of the material locally varies remarkably. Inthe example shown Figure 2, it varies more than 10%of the prescribed mean value. This affects themagnitude of the heat transfer. C<strong>on</strong>sidering a life cycleassessment of a DH system, the main impact to theenvir<strong>on</strong>ment is represented by heat losses [13]. Thethermal c<strong>on</strong>ductivity of the insulati<strong>on</strong> material inpre-insulated DH pipes is usually stated at atemperature of 50 °C. The lambda-coefficients werechosen according to the available data at the end of2009; the lambda-value at 50 °C for straight pipes,axial c<strong>on</strong>tinuous producti<strong>on</strong> was set to 0.024 W/(mK)<strong>and</strong> for flexible pipes to 0.023 W/(mK). Since April 2010new results are available [14]. It is preferable to have amodel that takes into account the temperaturedependencyof the thermal c<strong>on</strong>ductivity of theinsulati<strong>on</strong> foam. The calculati<strong>on</strong>s in this paper use thefollowing expressi<strong>on</strong>, if not differently stated. It derivesfrom experimental data [15]:λ(T) = 0.0196734 + 8.0747308 . 10-5.T [W/(mK)] (1)Supply pipe: (4)Return pipe: (5)Equati<strong>on</strong>s (4) <strong>and</strong> (5) show how the heat transfer fromeach pipe can be calculated by use of <strong>on</strong>ly <strong>on</strong>e linearFigure 2: Thermal c<strong>on</strong>ductivity in the insulati<strong>on</strong>, horiz<strong>on</strong>talcross-secti<strong>on</strong> of the pipe. Pipe: Aluflex 16-16/110,temperatures supply/return/ground 55/25/8 °C.83

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