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Performance analysis of cryogenic system and cryomodules for the complete superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf.

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Presentation on theme: "Performance analysis of cryogenic system and cryomodules for the complete superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf."— Presentation transcript:

1 Performance analysis of cryogenic system and cryomodules for the complete superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf of Cryogenics & Applied Superconductivity Group) Inter- University Accelerator Centre. New Delhi India CEC-ICMC2015 Tucson (T S Datta)

2 Superconducting LINAC at IUAC, Delhi
CRYOGENIC SYSTEM QWR Nb Cavity ( 97 MHz) 27 Nos Ti = 160 MeV Ti = 300 MeV CEC-ICMC2015 Tucson (T S Datta)

3 IUAC SUPERCONDUCTING CAVITY
Accelerating Structure 200 ß = .08c f= 97MHz, Leff = 16 cm, Eacc= 0.6MV Cold Mass= 50 kg Q.Rs=18 Outer SS Jacket LIQUID HELIUM OUTER NIOBIUM 800 mm approx.. BEAM PORT SLOW TUNER CENTRAL NIOBIUM Operating Temperature : 4.2 K and Frequency : 97 MHz CEC-ICMC2015 Tucson (T S Datta)

4 IUAC SUPERCONDUCTING CAVITY
First lot ( 8 Nos) of QWR was developed at USA in Collaboration with ANL. Remaining 20 cavities were developed in house at IUAC Performance Curve of a Cavity CEC-ICMC2015 Tucson (T S Datta) Courtesy ; P N Prakash

5 CEC-ICMC2015 Tucson (T S Datta)
Partial Linac was operated with one Linac module ( LC-1) along with Buncher (SBC) , Rebuncher (RBC). and old Refrigerator ( Make CCI, USA) till 2012 SBC Full Linac with the addition of LC-2 & LC-3 ( 16 Cavities) and with New Refrigerator ( Linde) is under operational since 2013 CRYO MODULE LC-1 LOW ENERGY FROM PELLETRON BEAM LINE LC-2 LC-3 LN2 LINE CRYO LINE OLD HE REF RBC HIGH ENERGY New Line NEW HE REFIGERAOR CEC-ICMC2015 Tucson (T S Datta)

6 Beam acceleration by all 22 Cavities in (LC-1, LC-2 & LC-3)
Year Beam Energy From Pelletron (MeV) Energy After Linac ( MeV) Gain MeV Gain/ Charge 2013 Ti+14 162 270 108 7.7 2014 275 113 8.07 2015 Ti+15 168 300 132 8.78 Improvement Average Field : 3.5 MV/ m at 5 W Power CEC-ICMC2015 Tucson (T S Datta)

7 CEC-ICMC2015 Tucson (T S Datta)
TOTAL LINAC COOLING WITH NEW REFRIGERATOR LC2+LC3 LC1 RBC SBC Total 5 days required to cool the linac module in Batch with liquid Helium CEC-ICMC2015 Tucson (T S Datta)

8 CEC-ICMC2015 Tucson (T S Datta)
Cooling Philosophy of linac is changed : Because New Refrigerator Cooling schematic different from earlier Effective Radiation Cooling Minor Modification on LC-2 & LC-3 Vacuum Nb SS304L LHe Thermal Shield Helium Vessel Resonator In Out JT Pr Driving Force : Dewar Pr CEC-ICMC2015 Tucson (T S Datta)

9 Cooling Performance comparison between Earlier and present
No Liquid Nitrogen Precooling required Earlier: 3 Stages Now : 2 stages Radiation Cooling Helps to Reduce the cavity Temperature from 210 to 175 K CEC-ICMC2015 Tucson (T S Datta)

10 REDUCED WITH NEW REFRIGERATOR RF LOCKS ARE VERY STABLE
Helium Pressure fluctuation in Cryomodules REDUCED WITH NEW REFRIGERATOR RF LOCKS ARE VERY STABLE CCI Refrigerator a) CEC-ICMC2015 Tucson (T S Datta)

11 OPERATION PARAMETERS OF LINDE REFRIGERATOR WITH VARIABLE LOAD FROM LINAC
Cavity Problem Refrigeration load : 280 W to 440 W Discharge Pressure : to bar Mass flow rate : 53 g/s to 63 g/s Power : 150 kW to 180 kW CEC-ICMC2015 Tucson (T S Datta)

12 Preliminary Heat load ( 4.2 K) contribution by each system :
Total Load ~ W . Refrigeration capacity : 550 W ( W/0 LN2) Cryogenic Load Distribution of LINAC Operating Range Measured load of Linac CEC-ICMC2015 Tucson (T S Datta)

13 CEC-ICMC2015 Tucson (T S Datta)
Complete Automation of Cryogen Distribution system LN2 VESSELS LHe & LN2 LEVEL/ Pressure In Cryomodule He Gas CEC-ICMC2015 Tucson (T S Datta)

14 Two Modes of LHe Supply Valves operation of Cryomodule
CEC-ICMC2015 Tucson (T S Datta)

15 Power Supply in India is not very Stable
Main system like Helium Compressor, Cold box, control system are connected through UPS and back up Generator.. Auxiliary system like chiller air supply are not with emergency power Compressor of when water inlet temp crosses 45 C CEC-ICMC2015 Tucson (T S Datta)

16 Temperature Sensor : DT- 470 Good Cavity : Fluctuation less
Temperature Reading Fluctuation Good Cavity Temperature Sensor : DT- 470 Fluctuation starts : Once cavity Comes out from Multipactoring Barrier Noted Good Cavity : Fluctuation less Reduced by Twisted cable, Filter Yet to be solved ???? Poor Performance CEC-ICMC2015 Tucson (T S Datta)

17 CEC-ICMC2015 Tucson (T S Datta)
CONCLUSION Superconducting Linac is being operational for expt with high energy heavy ion beam with almost double energy At present Load, Linac run can be managed on running Linde refrigerator ( LR 280) without LN2 Cooling Radiation Cooling is much more effective for the recent cryomodules and liquid nitrogen precooling stage is discarded Helium Pressure fluctuation is reduced and RF lock is very stable Power cut is common problem In India. Precaution are taken with UPS and back up generator Shortly High Current Injector will be the another source for LINAC. CEC-ICMC2015 Tucson (T S Datta)

18 ICEC 26 - ICMC 2016 Thank You http://www.ICEC 26 - ICMC 2016.org
March 7-11, 2016 Manekshaw Centre, New Delhi, India Thank You Welcome to Delhi Hosted by Inter-University Accelerator Centre Indian Cryogenics Council ICMC 2016.org Abstract submission open : August 17, 2015 CEC-ICMC2015 Tucson (T S Datta) Contact :


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