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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>iafind potential frost acti<strong>on</strong> damages. The inspecti<strong>on</strong>swere documented with photos.3. RESULTS3.1 Test results from deformati<strong>on</strong> of the pipe overtimeThe measured pipe deformati<strong>on</strong>s during the test periodturned out to be very small. The diagram in Fig. 13describes the measured changes in the casing sinceinstallati<strong>on</strong> <strong>and</strong> average air temperatures during thetest period. All three displacement gauges were set tozero before the installati<strong>on</strong>. The diagram shows thatthe casing of the test pipe during the installati<strong>on</strong> wassqueezed out up to 0.5 mm at the three measurementpoints. The deformati<strong>on</strong>s in the casing are most likelycaused by the packing of the backfill surrounding thepipe.After the installati<strong>on</strong> during the test period the resultsindicate that the upper side (violet curve in thediagram) of the test pipe casing have been pressed in0.2 mm. The side of the test pipe casing havesqueezed out approximately 0.1 mm. The under side(red curve) was squeezed out approximately 0.1 mmduring the period between the first <strong>and</strong> sec<strong>on</strong>dmeasurement results. During the rest of the test periodthe casing have been pressed back in 0.1 mm.It is to be observed that these measured changes arevery small relative to the test pipe casing diameter.Compared to the zero values in the laboratory themeasured changes are not more than 0.3 % relative tothe casing diameter.In Fig. 16 <strong>and</strong> 17 the diagrams show the vibrati<strong>on</strong>velocity (m/s) in the ground when a heavy lorry passover the test area at a speed of 40 km/h. The vibrati<strong>on</strong>velocity is calculated from the accelerati<strong>on</strong> signal byintegrati<strong>on</strong>.The diagrams in Fig. 18 <strong>and</strong> 19 show the maximumamplitude of the accelerati<strong>on</strong> in the ground as afuncti<strong>on</strong> of the speed of the lorry when it passes overthe test area in 20 km/h <strong>and</strong> 40 km/h, respectively themaximum vibrati<strong>on</strong> velocity as a functi<strong>on</strong> of the speedof the lorry.200 mm below surface, vehicle speed 40 km/hTime (s)Fig. 14 Vertical accelerati<strong>on</strong> 200 mm below the roadsurface when a lorry passes at 40 km/h.600 mm below surface, vehicle speed 40 km/hmm0,90,80,70,60,50,40,30,20,10-1000 100 200 300 400Days since installati<strong>on</strong>Average temperatures (°C)Under SideUpper SideFig. 13 Average air temperatures <strong>and</strong> changes in casingat installati<strong>on</strong> <strong>and</strong> during test period.3.2 Test results from instant deformati<strong>on</strong> of thepipe <strong>and</strong> accelerati<strong>on</strong>s from traffic loadThe diagrams in Fig. 14 <strong>and</strong> 15 describe the vibrati<strong>on</strong>sprocess at 200 mm, the same depth as the test pipe,<strong>and</strong> 600 mm below the road surface as accelerati<strong>on</strong>(m/s2) in the ground when a heavy lorry pass over thetest area at a speed of 40 km/h.Side200-20-40-60-80Time (s)Fig. 15 Vertical accelerati<strong>on</strong> 600 mm below the roadsurface when a lorry passes at 40 km/h.Velocity (mm/s)200 mm below surface, vehicle speed 40 km/hTime (s)Fig. 16 Vibrati<strong>on</strong> velocity 200 mm below the road surfacewhen lorry passes at 40 km/h.100

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