Superconduttivita` e Criogenia per LHC
Transcript
Superconduttivita` e Criogenia per LHC
Superconduttivita’ e Criogenia XXII Giornate di Studio sui Rivelatori Torino, 15 Giugno 2012 Amalia Ballarino European Organization for Nuclear Research (CERN), Geneva Introduction Superconductivity for high energy physics Part I Cryogenics for LHC Part II Superconductivity in LHC PART III Superconductivity & Cryogenics in LHC Upgrades Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Superconductivity for high energy physics Part I Cryogenics for LHC Part II Superconductivity in LHC PART III Superconductivity & Cryogenics in LHC Upgrades Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction What is cryogenics ? Cryogenic: for Greek “kryos", which means cold or freezing, and "genes" meaning born or produced. “In physics, cryogenics is the study of the production of very low eye temperature (below –150 °C, –238 °F or 123 K) and the behavior of materials at those temperatures” from Wikipedia The lowest natural temperature ever recorded on earth was in 1983 in Antartica: -89.2 oC or 183.8 K What is superconductivity ? “Superconductivity is a phenomenon occurring in certain materials at very low temperatures , characterized by exactly zero electrical resistance and the exclusion of the interior magnetic field (the Meissner effect) from Wikipedia Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Resistance (Ohm) vs Temperature (K) of Hg – K. Onnes, 1911 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Cryogenics Particles accelerator Superconductivity Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Accelerator: Instrument of High Energy Physics h/p 1 TeV 10-18 m Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Accelerator Energy and Magnetic Field Particles are produced by converting the collision energy into mass Synchrotron: E[GeV]=0.29979 B[T] R[m] High energy High field magnets Energy (TeV) 100.00 r=10 km LHC 10.00 r=1 km r=0.3 km 1.00 Tevatron SSC UNK LHC 0.10 Colliding beams: ECM~2E r=3 km HERA RHIC LEP 0.01 0 5 10 15 Dipole field (T) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Resistive magnets The most economical designs are iron-dominated; The upper field limit for iron-dominated magnets is ~2 T due to iron saturation; Most resistive accelerator magnet rings are operated at low field (~ 1 T), to limit power consumption ( B R). Superconducting magnets Significant reduction in power consumption (cryogenic power R); Higher current density in the magnet coils. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Economical savings due to superconductivity The LHC has a circumference of 27 km, out of which some 20 km of main superconducting magnets operating at 8.3 T and 1.9 K. Cryogenics will consume about 40 MW electrical power from the grid. If the LHC were not superconducting: Using resistive magnets operating at 1.8 T (limited by iron saturation), the circumference should be about 100 km, and the electrical consumption 900 MW, leading to prohibitive capital and operation costs. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction The Energy Frontier Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Large Superconducting Accelerators Tevatron FermiLab HERA DESY RHIC BNL LEP CERN LHC CERN Type p -p e-p Heavy ion e+ - e- p-p Radius (m) 768 569 98 2801 2801 Energy per beam (TeV) 1 0.9 0.1 0.104* 7 Op. temperature (K) 4.6 4.5 4.6 RT-4.5 K* 1.9 Dipole field (T) 4.4 4.68 3.46 0.135 8.33 Dipole Current (kA) 4.4 5.03 5.09 4.5 11.8 Commissioning 1883 1990 19992000 1989 20072008 * Upgrade with sc cavities to achieve the mass of the pair of W particles Amalia Ballarino XXII Giornate di Studio sui Rivelatori Introduction Superconductivity for high energy physics Part I Cryogenics for LHC Part II Superconductivity for LHC PART III Superconductivity & Cryogenics for LHC Upgrades Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Cryo-history 1848: Determination of existence of zero absolute (Lord Kelvin) 1853: Discovery of Joule-Thomson effect (cool-down of a compressed gas during adiabatic expansion) 1877: Liquefaction of oxygen below 320 atmospheres (R. P., Pictet) 1895: First liquefaction of air (Carl von Linde) 1898: Liquefaction of hydrogen (Dewar) 1908: Liquefaction of helium @ 4.2 K (*K. Onnes, Leiden Univ., ND) 1911: Discovery of superconductivity (K. Onnes) 1938 : Discovery of superfluid helium (He II). 1978: Kapitza, Nobel Price in Physics 1971: Use of superfluid helium at atmospheric pressure (Roubeau) 1990: Use of pressurized superfluid helium in large-scale projects (Claudet and Aymar) 2008: Start-up of LHC, with the world’s largest cryogenic system (superfluid helium for cooling the superconducting magnets) *1913:Noble Price in Physics “for his investigations on the properties of matter at low temperatures which led, inter alia, to the production of liquid helium” Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Standard P-T and T-v Phase diagrams Cryogenic fluids Cryogen Triple point (K) Normal Boiling point (K) Critical point (K) Oxygen 54.4 90.2 154.6 Argon 83.8 87.2 150.9 Nitrogen 63.1 77.3 126.2 Saturated Vapor/liquid Temperature 24.6 27.1 44.4 Hydrogen 13.8 20.4 33.2 Neon Helium 2.2 4.2 (-point) 5.2 Saturated vapor curve Saturated liquid curve Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Helium Second lightest elemental gas, after hydrogen Smallest of all molecules Colorless, odorless, inert and non-toxic Lowest boiling point of any element (-268.9°C, 4.2 K) Helium is produced continually by the radioactive decay of uranium and other elements, gradually working its way into the atmosphere Commercial extraction from air is impractical because helium's concentration is only about five parts per billion. Commercially, helium is obtained from the small fraction of natural gas deposits that contain helium volumes of 0.3 percent or higher Unusual characteristics: Helium remains liquid to absolute zero At 2.1 K, liquid helium exhibits super fluidity or virtually zero viscosity (Helium II), defies gravity to flow up container walls and becomes nearly a perfect heat conductor Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Phase diagram of helium (He4) 10000 SOLID Pressure [kPa] 1000 -line He II SUPERCRITICAL He I CRITICAL POINT Tc=5.19 K SATURATED He I pc=2.2 bar 100 PRESSURIZED He II (Subcooled liquid) 10 VAPOUR T=2.17 K p=50 mbar -point SATURATED He II 1 0 1 2 3 4 5 6 Temperature [K] Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Specific heat of saturated helium Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Viscosity of He II Allen and Misener Keesom Two fluid model: rn, n, sn rs, s=0, ss=0 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Equivalent thermal conductivity of He II 2000 Helium II Y(T) ± 5% KT,q q 2.4 YT 1500 dT q 3.4 dX Y(T) 1000 q in W / cm2 T in K X in cm 500 T OFHC copper 0 1.3 1.4 1.5 1.6 1.8 1.7 1.9 2 2.1 2.2 T [K] Conduction in a tubular conduit Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Superconductor performance at 4.2 K and 1.9 K Critical current density of NbTi as a function of Magnetic field at 4.2 K and 1.9 K Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Saturated and pressurized He II at 1.9 K 10000 SOLID Pressure [kPa] 1000 -line He II SUPERCRITICAL He I CRITICAL POINT 100 PRESSURIZED He II (Subcooled liquid) SATURATED He I 10 VAPOUR -point SATURATED He II 1 0 1 2 3 4 5 6 Temperature [K] Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Large scale He II systems Use of saturated superfluid helium. By lowering the pressure of the vapor when pumping on LHe, the boiling temperature is reduced. Liquid helium vapor pressure equilibrium and latent heat of vaporization T (K) 1.6 1.7 1.8 1.9 2 2.1 2.17 4.22 P (kPa) 0.74 1.12 1.63 2.29 3.12 4.14 5.04 101.32 L (J g-1) 22.93 23.19 23.36 23.44 23.4 23.19 - 20.72 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Large scale He II systems Sat. He Pres. He Air inleak prevention - + Dielectric strength - + Pump-down time - + Enthalpy margin for transient - + Technical simplicity + - 10000 SOLID Pressure [kPa] 1000 -line He II SUPERCRITICAL He I CRITICAL POINT 100 PRESSURIZED He II (Subcooled liquid) SATURATED He I 10 VAPOUR -point SATURATED He II 1 0 1 2 3 4 5 6 Temperature [K] Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Refrigeration Refrigerator: machine that extracts heat (Qc) from a low temperature source (Tc) by adsorbing mechanical work (W); by doing so, it rejects heat (Qh) to the high temperature source (Th, usually equal to room temperature) W = Qh-Qc COP = benefit/cost = Qc/W = 1/((Qh/Qc)-1) COP ≤ Tc/(Th-Tc) COP= Cofficient of Performance Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Carnot cycle The Carnot cycle is the most efficient refrigeration cycle operating between two temperature levels COP = Tc/(Th-Tc) Tc (K) 77 (LN2) 20 (LH2) 4.2 (LHe) 1.8 (LHe) W/Qc* 2.8 13.5 68.7 161.8 COP 0.3 0.07 0.004 0.0006 Tc/(Th-Tc) 0 Tc 0 *Figure of merit 1-2 2-3 3-4 4-1 Isothermal expansion Isentropic compression Isothermal compression Isentropic expansion T QH 4 1 3 2 QC s Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Hypothetical Carnot cycle for He refrigeration Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Claudet cycle Widely used in refrigeration technology. It combines isenthalpic and isentropic expansion. A refrigerator based on the Claudet cycle comprises a compressor at RT, a series of heat exchangers, an expansion turbine and a Joule-Thomson valve. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Refrigeration Cooling methods: Heat transfer – counter flow heat exchangers External work – engine work (usually via turbine expanders, with reduction of the gas temperature and pressure) Isenthalpic expansion (Joule-Thomson effect) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Joule-Thompson inversion temperature: temperature above which expansion at constant enthalpy causes the temperature to rise, and below which such expansion causes cooling Joule–Thomson (Kelvin) coefficient: JT=(T/p)h (K/Pa) JT > 0 JT < 0 T<Tin T>Tin Joule-Thomson effect: adiabatic expansion of a gas (constant enthalpy) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Efficiency of refrigerators and liquefiers as a function refrigeration capacity 30 (W/Qc)CARNOT,4.2K = 68.7 (Q/Qc) = 68.7/0.3 230 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I The cryogenic system for the LHC machine 0.999999991c Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I LHC layout Sector=3.3 km SSS=528 m Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I From the LEP to the LHC machine 8000 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Layout of LHC cryogenic system • 5 Cryogenic islands • 8 Refrigerators: - 2 at P4, P6 and P8 - 1 at P2 - 1 at P1.8 • 1 Refrigerator serves 1 Sector (3.3 km) • Possibility of coupling two refrigerators via the interconnection box Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Performance of 4.5 K refrigerators at CERN LHC: COP= 230 W/W = 29 CARNOT Electrical input power installed 4.5 MW/refrigerator Amalia Ballarino XXII Giornate di Studio sui Rivelatori Gas storage tanks Part I Cooling the LHC ring Total refrigeration capacity: 144 kW at 4.5 K (8×18 kW @ 4.5 K, 600 kW liquid nitrogen pre-cooler liquid used during cool-down) and 20 kW at 1.9 K (82.4 kW @ 1.9 K) distributed around the ring. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Principle of LHC cooling scheme In the LHC, heat is conducted from the superfluid helium to the a heat exchanger pipe containing a mixture of saturated vapor and superfluid helium (p16 mbar) arranged in a series of 107 m cooling loops all around the ring. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Schematic of cooling system SHe supply (4.6 K, 3 bar) GHe pumping (15 to 19 mbar) Bayonet heat exchanger Saturated LHeII TT Hydraulic plug TT TT Magnet TT TT Ps0 TT Wetted length (Lw) Magnet cell (107 m) Amalia Ballarino TT JT TT Dried length (Ld) Pressurised LHeII Slope XXII Giornate di Studio sui Rivelatori Part I Cryogenic flow scheme of an LHC cell (107 m) 107 m Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Temperature levels in the LHC cryogenic system In view of the high cost of refrigeration at 1.8 K, the main heat influx in intercepted at higher temperatures. The temperature levels are: 50 K to 75 K for thermal shielding of the cold masses; 4.6 K to 20 K for cooling of the beam screens and lower temperature interception; 1.9 K quasi-isothermal superfluid helium for the magnets; 4 K helium at very low pressure for transporting the superheated helium flow coming from the 1.8 K heat exchanger tubes across the sector length to the 1.8 K refrigeration unit; 4.5 K saturated helium for some insertion magnets, RF cavities, and the bottom end of the HTS leads; 20 K to 300 K cooling for the resistive upper section of the HTS leads. Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Cryogenic block diagram 4 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Thermodynamic states of He in LHC cryogenic system Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Process flow diagram of LHC 18 kW cryoplant E1 T1 E3 E4 T2 20 K - 280 K loads M Pa M Pa 0. 1 1. 9 LN2 Precooler 0. 4 M Pa (LHC current leads) 201 K 50 K - 75 K loads E6 T1 T3 from LHC loads (LHC shields) T2 E7 75 K T3 E8 T4 49 K Adsorber LHC shields 32 K E9a T4 20 K E9b 13 K 10 K E10 4.5 K - 20 K loads T5 T7 from LHC loads T7 (magnets + leads + cavities) T6 9K T8 4.4 K 0. 3 M Pa E11 T5 To LHC loads E12 T6 E13 Amalia Ballarino T8 XXII Giornate di Studio sui Rivelatori Part I Adsorbers Turblne CCB WCS 4.5 K Refrigerator Cold compressors 1.8 K Refrigeration Unit 1.8 K He refrigeration system D C 0.13 MPa, 20 -30 K 0.3 MPa 4.6 K B LHC Sector Load LHe 1.8 K Q1.8K Installed pumping capacity 125 g/s at 15 mbar (i.e. ~2.4 kW @ 1.8 K) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I LHC Distribution system The refrigerating helium of the magnets and cavities have to be distributed over the 27 km of the accelerator, in the LHC tunnel, 100 m below ground level. Due to the size of the experiment, ultra high performance cryogenic lines have been specially designed for the LHC project. The achieved performance of the line is: about 0.05 W/m on each of the 4.5 K tubes of the transfer line, a performance around 10 times better than usually achieved Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I LHC Cryogenic line in the LHC tunnel Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Connection via service module and jumper Supply and recovery of helium with 26 km long cryogenic distribution line Static bath of superfluid helium at 1.9 K in cooling loops of 110 m length Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Transverse cross section of the LHC tunnel Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Cool-down of LHC machine Removal of air in circuit by evacuation and He filling (1 week); Removal of dust and debris by flushing the helium circuits with high helium flow at 300 K (1 to 2 week per sector) ; Cool-down of 4625 t per sector over 3.3 km: From 300 to 80 K: 600 kW pre-cooling with LN2, up to ~5 t/h, 6 LN2 trailer per day during 10 days (1250 t of LN2 in total); From 80 to 5 K: Cryoplant turbo-expander cooling; LHe filling: 15 t of LHe in total (4 trailers); LHe filling and cool-down completion by using the 1.8 K refrigeration unit (1 week/sector) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Cool-down of Sector 7-8 80 K 20 K Temperature evolution during cool-down of the first LHC Sector From RT to 80 K, from 80 K to 20 K, from 20 K to 4.5 K, from 4.5 K to 1.9 K with LHe filling. Electrical test are performed at each plateau. The time for cooling one Sector is about 3 weeks (3.3 km, 1250 tons LN2, 18 tons of He, 800 g/s of He, 4600 tons of material in the Sector) Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Cryogenic instrumentation Type Thermometers (Cernox 1.7 - 300 K) Thermometers (Pt100, Thermocouple) Quantity 700* 500* Location Magnet cold mass, QRL, DFB Current lead, cryo-heater, thermal shield SSS phase separator, DFB, standalone magnet Magnet cold mass, DFB, QRL, beam screen Level gauges 70 Cryo-heaters 300 Cryogenic control valves 180 QRL Warm control valves (DFB) 150 Current lead Total per sector 1900 Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Heat load and cryostat design Heat inleaks – Radiation – Residual gas conduction – Solid conduction Joule heating – Superconductor splices 70 K shield, MLI Vacuum < 10-4 Pa Non-metallic supports Heat intercepts Resistance < a few nW Beam-induced heating – Synchrotron radiation (0.6 W/m) – Beam image currents (0.8 W/m) – Localized heat due to loss of particles (e.g particles escaping collimations) Amalia Ballarino } } 5-20 K beam screens } XXII Giornate di Studio sui Rivelatori Part I Cryostat of LHC dipole Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Thermal shield Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Multi-layer insulation Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I Horizontal tanks for storage of He gas (250 m3) at 2 MPa Vertical dewars (100 m3) for liquid nitrogen He gas Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I LHC Control Room Amalia Ballarino XXII Giornate di Studio sui Rivelatori Part I The CERN accelerator network Amalia Ballarino XXII Giornate di Studio sui Rivelatori