COOLING & VENTILATION FOR THE DRIVE BEAM TUNNEL M Nonis – EN/CV – 16/9/2009 CLIC TWO BEAM MODULES REVIEW - 2009.

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Presentation transcript:

COOLING & VENTILATION FOR THE DRIVE BEAM TUNNEL M Nonis – EN/CV – 16/9/2009 CLIC TWO BEAM MODULES REVIEW

Agenda -Tunnel cross section -Ventilation: - main parameters - improvements, pending issue -proposed solution - Cooling: -main parameters -proposed solution -pending issues

Tunnel cross section

90 kW 250 kW 200 kW Ventilation main parameters: heat dissipation in the air Heat dissipation in the tunnel: 250 kW / DB sector 1250 kW between two shafts Drive Beam sector = 250 kW UTRA cavern = 200 kW Loop = 90 kW Heat dissipation in the Loops & UTRA: 290 kW / DB sector 1450 kW between two shafts

200 kW 90 kW UTRA Loop Ventilation of UTRA and loop: local cooling solution Chilled water pipe from shaft?

Ventilation working parameters: Cooling power: 1250 kW Delta T: 20 °C  °C Flow rate: 180’000 m3/h If v= 12 m/s  Cross section:4.1 m 2 If cross section 1.2 m 2  v= 41 m/s

a) Reduce the cooling power removed by air Cross section ducts: 1.2 m 2 Flow rate: 52’000 m 3 /h Cooling power:360 kW b) Using pre-alignment shafts for ventilation shall allow a reduction in the dimensions of AHU on surface Possible improvements

c) Validate the delta temperature Supply and extraction temperatures are average values at louvers position. Effective temperatures close to equipment are related to the heat load in each component and local air speed:HOT SPOTS Define the maximum acceptable temperature for equipment Pending issue

Semi transversal principle SHAFT POINT Extraction Air supply NEXT SHAFT POINT Extraction Air supply Possible fire resistance sectors with two emergency exits per sector 1 Smoke extraction trap per sector 1 supply and extraction grille per 30 mtrs. Optimisation of the air flow rate Low air speed in the tunnel Optimisation of the gradient temperature Reversible and redundant operation possible Energy recovery possible, recycling of air Proposed solution

UserPower [MW] Delta T [°C] Flow rate [m3/h] Circuit A Demineralized water Modules ’350 Circuit B Demineralized water UTRA, UTRC, loop, beam dump Circuit C Raw water Fire fightingn.a. 35 Circuit D Compressed air Regulationn.a. 760 Drain systemPumps in each UTRA; raised in each shaft Water cooling main parameters

WITH EXISTING CROSS SECTION Flow rate [m3/h] NDPressure loss [bars/km] Circuit A Demineralized water 3’350600~ 1.13 Circuit B Demineralized water ~ 0.8 Impossible to regulate the pressure at each delivery point for modules with such a pressure difference along the supply pipe Water cooling main parameters

Use of booster pumps along the tunnel to have lower working pressure, Increase of pipes diameters: ND600  ND800 ND300  ND400 Use of cooling towers every 4.4 km, Doubling the circuits to reduce the flow rate and working pressures. Possible solutions

Space needed in the cross section to pass from ND600 to delivery point (ND50? T.b.c.) Temperatures are at outlet of cooling station: stability in lenght still to be analysed Stability of temperature in time: local heating. Cooling with water from lake: reduce inlet temperature Pending issues

Conclusions AIR -Thermal charges removed by air to be confirmed -Validate working temperatures for air WATER -Pressure loss on cooling circuit to be reduced; -Temperature stability in time and length -Study of connection between main collector and cooling pipe for module -Ratio air/water heat dissipation confirmed? -Evaluate the impact on tunnel cross section -All this figures require the use of non standard manifacturing, tooling and equipment: increase of costs. Still to be discussed: heat dissipations in Exp. Caverns, LINACS etc.….