GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Present Design of LCGT Cryogenic Payload - Status of Cryogenic Design - N. KIMURA*, Y. SAKAKIBARA**,

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Presentation transcript:

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Present Design of LCGT Cryogenic Payload - Status of Cryogenic Design - N. KIMURA*, Y. SAKAKIBARA**, S. KOIKE*, T. OHMORI***, T. SUZUKI*, H. YAMAOKA*, and LCGT Collaboration * High Energy Accelerator Research Organization (KEK) ** University of Tokyo *** Teikyo University

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA 2 Outline Design of the LCGT cryogenics Structure of the cryostat Cryostat response to ground motion at CLIO/Kamioka mine Thermal Budget of the cryostat Estimation of heat load of the Mirror from the beam duct shields (by Mr. SAKAKIBARA) Summary

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Vacuum duct  800 with radiation shield Gate valve Connection Port to SAS Mirror a cryostat Location of Four Mirror Cryostats with the Cryo-coolers for the LCGT Mozumi-End Atotsu-End X-Front Room Y-Front Room Vacuum duct  800 with radiation shield L=~20 m

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Production plan of LCGT mirror cryostats and peripheral components Manufacture components Assemble and factory test with cryo-coolers Transport to Kamioka Custody at Kamioka 2011 Jfy2012 Jfy2013 Jfy ‘12.3‘13.3‘14.3‘11.3 Design by KEK Bidding We are here Four Mirror Cryostats Cryo-cooler units Design by KEK 1st Prot-type Cryo-cooler unit test Production of seven cryo-cooler units Production of nine cryo- cooler units Transport to Kamioka Custody at Kamioka Performance test Duct shield units Design by KEK Production of Prot-type ducts shield units with cryo-coolers Performance test

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Basic requirements from LCGT cryogenic Temperature of the test mass/mirror : 20 [K] Inner radiation shield have to be cooled to < 8 K The mirror have to be cooled without introducing excess noise, especially vibration due to cryocoolers. Easy access and enough capacity to installation work around the mirror. Satisfy ultra high vacuum specification < Pa Requirements and Answers Answer to the requirements Adopt Pulse Tube-type Cryo-cooler units with very low vibration mount based on the CLIO type cooler. Adopt  2200 of inner diameter of flanges for installation work of the mirror and suspension. Analysed the cryostat response to ground motion at Kamioka-mine. Heat load from components as low as possible. Develop very low out gas super insulation system for radiation heat load for ultra high vacuum specification < Pa

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Main beam (1200mm FL) to SAS View ports Remote valve Low vibration cryocooler unit Main LASER beam  2.4m ~3.8m Cryostat Stainless steel t20mm Diameter 2.4m Height ~3.8m M ~ 10 ton Cryocoolers Pulse tube, 60Hz 0.9 W at 4K (2nd) 36 W at 50K (1st) Drawn by S. Koike (KEK) Cryostat accompany with four cryocooler units Structure of Mirror Cryostat

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA The interior of the cryostat Double radiation shields with hinged doors Support rods View Ports Heat path to cryocooler Drawn by S. Koike (KEK)

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Structure of Radiation Shields Outer Shields Inner Shields Flame made by A6000 Aluminum Secure stiffness and conductivity of the radiation shields

Cryo-top Cryo-L Cryo-F Input Cryo-R X-directionY-direction X 方向 Y 方向 Response to ground motion resonant frequency

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA 10 An Estimated Break Down List of Thermal Budget Outer Shield (W) ◦ Eleven View Ports 22 ◦ Radiation From 300 K 70 ◦ Support post and Rods 24 ◦ Electrical wires 3 x Total 116 W/unit 29 Inner Shield (W) ◦ Duct Shields* < 0.05 (Beam and SAS) ◦ Eleven View Ports 0.4 ◦ Radiation From 80 K 2.2 ◦ Support post and Rods 2.4 ◦ Electrical wires 3 x ◦ Mirror Deposition 0.9 ◦ Scattering Light ? Total5.9 W/unit1.5 *Heat Load of Duct Shields will be told by Mr. Sakakibara 1 st Cold stage2 nd Cold stage

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA 11 Estimated Thermal Budget Estimated Heat Loads at the radiation shields and Support posts and rods 70 W by the radiation at 80 K outer shield 2.2 W by the radiation at 8 K inner shield 24 W by the radiation and conduction (support posts and tension rods) at 80 K 2.4 W by the radiation and conduction (support posts and tension rods) at 8 K Low Vibration Cryo-cooler unit Very High Purity Aluminum Conductor (5N8) Connection point with IM dT 2nd =0.5 K 94 K at the top of the 80 K outer shield 7.4 K at the top of the 8 K inner shield 47 K at 1 st cold stage of Cryo-cooler 6.5 K at 2nd cold stage of Cryo- cooler dT 1st = 26 K

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA 12 Outline Concept of the LCGT cryogenics Structure and Response to ground motion at CLIO/Kamioka mine Thermal Budget of the cryostat Estimation of heat load of the Mirror from the beam duct shields (by Mr. SAKAKIBARA) Summary

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Thermal radiation from opening of 500 mm in diameter Cooling power 3.6 W at 4 K (inner shield, 4 pulse tube cryo-coolers of 0.9 W at 4 K) Thermal radiation appears to be reduced by reducing solid angle 13 Estimation of heat load from the beam duct shields of the Mirror in the Cryostat

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Problem experienced in CLIO Thermal radiation reflected by metal shield pipe Incident power (calculated using ray trace model, experimentally verified by T. Tomaru, et al ) Very large compared with solid angle 14 animation 300 K 4 K mirror

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Reducing heat load by baffles Incident power calculated using ray trace model by counting up number of reflections 15 animation (Aluminum of A1070 measured at 10  m, 100 K) 300 K4 K

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Result of calculation 16 R=0.94±0.02 Worse case R=0.96 P=52.4 mW Better case R=0.92 P=17.6 mW R= K4 K mirror The better result for the case that intervals of baffles are not equal to each other – If intervals of baffles are equal, ray whose angle passes through one baffle also passes the other baffles x=20 m x=0 m

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Diamond Like Carbon coating Baffles whose room temperature sides are coated with DLC Assuming reflectivity 0.35 (measured at 1  m at room temperature by T. Tomaru, et al. 2005) Preparation for measurement at 10  m, cryogenic temperature is now underway 17 DLC coating Heat absorbed by baffles Heat load becomes smaller

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Summary 1 18 Sum of heat load from openings of cryostat can be sufficiently reduced by baffles ◦ 37 mW (18.4 mW x2) ◦ Problem in CLIO solved One prototype duct shield will be constructed until the end of March, The duct shield will be tested to verify this calculation with the mirror cryostat.

GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Summary 2 19 The design of the mirror cryostat for LCGT satisfying requirements was almost finished. The production of the components for the cryostat will be started after decided contractor. Performance of the first cryostat will be demonstrated at the factory of the contractor on the mid of 2012 Jfy. We would like to discuss the detailed design process of the cryostat with participants of GWADW conference after this talk.