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 calculated end method states the ends of theservice pipe shall be insulated with a known thermalc<strong>on</strong>ductivity as shown in Fig 2.X, L: distance to next measuring point from the middle,sample lengthT 0m ,T 0X ,∆T 0m ,T 2 : pipe temperature at the middle of thetest secti<strong>on</strong>, temperature at distance X of the middle,temperature correcti<strong>on</strong>, temperature at insulati<strong>on</strong>surface.Fig 2, C<strong>on</strong>figurati<strong>on</strong> calculated end cap.The service pipe is heated, using a heating elementwith <strong>on</strong>ly <strong>on</strong>e secti<strong>on</strong>. During the tests a thermal profileis made of the outer casing of the sample, showinglower values at the ends. After testing the heat loss iscompensated for the end loss with the van Rinsum orNukiyama theory. For this investigati<strong>on</strong> <strong>on</strong>ly the vanRinsum theory is used <strong>and</strong> therefore described.According to the van Rinsum theory, the axial heat losscauses a decrease in temperature not <strong>on</strong>ly towards theends of the service pipe, but in the test secti<strong>on</strong> as well.With the use of the equati<strong>on</strong>s (1), (2), (3) thistemperature decrease in the test secti<strong>on</strong> can becalculated <strong>and</strong> added to the measured value,compensating the end loss. This corrected temperatureis used in equati<strong>on</strong> (4) to calculate the overall thermalc<strong>on</strong>ductivity. This method is used by <strong>on</strong>e of theGerman institutes. calcc D 2 lnD 0 2LT 0m T 2 2 calc DA 1 1 A 2 2 2 lnD 0 T 0m T 0XT 0m cosh Xc 2 D 2 lnD 0 LT 0m T 0m T 2 λ calc : approximate value of thermal c<strong>on</strong>ductivity(1)(2)(3)(4)D 2 /D 0 : outer/inner diameters of casing <strong>and</strong> service pipeA 1 , A 2 : areas of the heating probe, inner service pipeλ 1 , λ 2 , λ: thermal c<strong>on</strong>ductivity of heating probe, thermalc<strong>on</strong>ductivity of medium in the service pipe, thermalc<strong>on</strong>ductivity total sample.251VERIFICATION OF SAMPLESTo verify the outcome of the Thermaflex heat lossequipment <strong>and</strong> the laboratory tests, three samples ofthe Flexalen 600 piping system are tested <strong>on</strong> theiroverall heat loss. These samples c<strong>on</strong>sist of 2 or 3 m ofthe pre-insulated piping system. More informati<strong>on</strong>about the Flexalen 600 system can be found in “Heatloss of flexible plastic pipe systems analysis <strong>and</strong>optimizati<strong>on</strong>” (E. van der Ven et Al.) [4]. Furthermore,method comparis<strong>on</strong> tests are performed <strong>on</strong> competitivepre-insulated piping systems, a comparis<strong>on</strong> of theproducts themselves is given in “Performance of preinsulated pipes” (I. Smits et Al.) [6].The tests <strong>on</strong> the Flexalen 600 products are performedby Thermaflex <strong>and</strong> by <strong>on</strong>e of the acknowledgedinstitutes, using the different methods. To ensure theeffect of ageing in the Flexalen 600 system is the sameduring all tests, the Flexalen 600 samples are testedsimultaneously. To exclude effects of the producti<strong>on</strong>process both tested samples are half of a 6 meter stick.An alternative method is used for Flexalen 50A25 <strong>and</strong>competitive products. Here the same sample is testedat the different test facilities.The comparis<strong>on</strong> of the results is based <strong>on</strong> the outcomeof heat loss per meter, calculated as described in theEuropean st<strong>and</strong>ard [1]. This loss per meter is <strong>on</strong>lyc<strong>on</strong>clusive <strong>on</strong> a very small part of the entire system.Therefore the complete Flexalen 600 system will becovered in paper “Heat loss system optimisati<strong>on</strong>” (J.Korsman et Al.) [3] <strong>and</strong> ‗‟New ec<strong>on</strong>omical c<strong>on</strong>necti<strong>on</strong>soluti<strong>on</strong>s for flexible piping systems” (C. Engel et Al.)[5].In this report the following diameters of the Flexalen600 piping systems are used for comparis<strong>on</strong> of themeasurements: Flexalen 600: 50A25, two guarded end tests* <strong>and</strong> calculated endtest. 160A90, <strong>on</strong>e guarded end test* <strong>and</strong> calculated endtest. 200A110, <strong>on</strong>e guarded end test* <strong>and</strong> calculatedend test.Competitive products: Sample 1 two guarded end tests Sample 2 two guarded end tests**At the time of writing the sec<strong>on</strong>d test results were notyet available.
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>iaTHERMAFLEX HEAT LOSS EQUIPMENT 600The Thermaflex heat loss equipment is speciallydesigned for the Thermaflex Flexalen 600 series. Oneof the major design goals was to develop a fast <strong>and</strong>easy to use test rig with the precisi<strong>on</strong> of a laboratorialtest. These goals have resulted in a test rig that is ableto measure heat loss in a few hours, allowing directoptimizati<strong>on</strong> during the producti<strong>on</strong> process, <strong>and</strong> isoperable by the producti<strong>on</strong> staff without the loss ofaccuracyPhysical test facilityThe physical part of the Thermaflex heat lossequipment c<strong>on</strong>sists of three segments.The first is the water cooled compartment in which alltests are performed. This compartment is kept at ac<strong>on</strong>stant temperature, (23 °C), during eachmeasurement.The sec<strong>on</strong>d is a heat source, for which heating probesare used. These heating probes are custom made byequipping a two meter Thermaflex piping segment, ofall available diameters, with three heating coils.The third part of the heat loss equipment is the c<strong>on</strong>trolunit. Here the heating probe is powered <strong>and</strong> all thermalreadings are d<strong>on</strong>e. By applying custom made softwareall desired readings can be d<strong>on</strong>e. The final output is theactual heat loss in W/m through the entire pre-insulatedFlexalen pipe, c<strong>on</strong>sisting of the service pipe, insulati<strong>on</strong><strong>and</strong> outer casing.secti<strong>on</strong>. With this method it is possible to measure theheat loss by measuring the power needed to maintain ac<strong>on</strong>stant temperature of the test sample. Inc<strong>on</strong>tradicti<strong>on</strong> to the measurements at the test institutes,the Thermaflex heating probes temperature isregulated by PID c<strong>on</strong>trolled power supplies. In the testresults Graph 2 the power c<strong>on</strong>sumpti<strong>on</strong> versus testtime is shown. This variable power supply makes itpossible to pre-heat the probes in a short period oftime, shortening waiting times c<strong>on</strong>siderably.Furthermore the use of the actual pipe material as aheating probe increases the accuracy. Moreover iteliminates all additi<strong>on</strong>al heat loss by c<strong>on</strong>vecti<strong>on</strong> thatwill be present with the use of smaller, not inner servicepipe c<strong>on</strong>necting heating probes.For testing competitive products with differentdiameters these advantages are lost. However by theuse of thermal compartments in the service pipe thetest results can be guaranteed.Thermaflex method of testingFor testing, the heating probe with the appropriatediameter is inserted in the insulati<strong>on</strong> covered with outercasing, <strong>and</strong> inserted in the cooled test secti<strong>on</strong>. Afterc<strong>on</strong>necting the probe to the c<strong>on</strong>trol unit themeasurement can be started. Different testingc<strong>on</strong>diti<strong>on</strong>s can be entered at this point such as theinner pipe temperature, representing the internalmedium. When the test is started the heating coils heatthe inner side of the probe until the desiredtemperature is reached. When the inner temperature isc<strong>on</strong>sidered c<strong>on</strong>stant <strong>and</strong> uniform throughout the threeheating coils, the actual measurement is started. Toensure a c<strong>on</strong>stant temperature in the probe, a waitingtime is built in the software that will reset themeasurement if temperature exceeds presettemperature values.Fig 3, Thermaflex heat loss equipment 600.Measurement principle ThermaflexThe Thermaflex test rig is designed in compliance withthe European st<strong>and</strong>ard [1] <strong>and</strong> also the tests arecarried out according to ISO 8497 <strong>and</strong> EN 15632. Inthe design of the heating probes the most realisticmethod, the guarded end method, is used. Accordingto this method the heating probes are equipped withthree heating coils with separate power supply. Asshown in Figure 2, two 400 mm heating coils located ateach end of the 1000 mm test secti<strong>on</strong>. These twosecti<strong>on</strong>s provide a thermal insulati<strong>on</strong> at both ends ofthe test secti<strong>on</strong> since all three are kept under uniformtemperature, eliminating axial heat loss of the test252The heat loss measurement is d<strong>on</strong>e by measuring theenergy required to keep the probe at a c<strong>on</strong>stanttemperature, by measuring the current at c<strong>on</strong>stantvoltage in the heating coils, <strong>and</strong> calculating the powerc<strong>on</strong>sumpti<strong>on</strong>. Since the middle/testing coil is exactly<strong>on</strong>e meter in length the required energy represents theexact heat loss through <strong>on</strong>e meter of piping <strong>and</strong>insulati<strong>on</strong> in W/m. Since the actual piping material isused during the measurement, there are no otherlosses, nor advantages, than there will be in practise,ensuring an objective measurement. Furthermore arealistic fit of the insulati<strong>on</strong> material is guaranteed. Asstated in the foregoing paragraph these advantagesare lost for divergent diameters. However during thisinvestigati<strong>on</strong> the probes have proven suitable fortesting, as both testing institutes also use smallerheating probes.
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