Www.minigrail.nl Materials and Cooling Techniques G. Frossati, A.de Waard, L.Gottardi and O.Usenko Kamerlingh Onnes Laboratory Leiden, The Netherlands.

Slides:



Advertisements
Similar presentations
Basic Refrigeration, Its Components, and Its Cycle
Advertisements

Piero Rapagnani I.N.F.N. Sezione di Roma
STREGA C2:Cryogenic suspension system for advanced resonant detectors (5 MIN) Task -C2: development and construction of advanced cryogenic system for resonant.
Io ILIAS - STREGA MEETING
Using Heat Chapter 16.3.
Participants: C-1:Cryogenic last-stage suspensions (interferometers) (F.Ricci-G.Frossati) Objectives: -Design new suspension elements for the last stage.
Current status of AMoRE-10 cryostat
The Use of Small Coolers for Hydrogen and Helium Liquefaction
Patricia Aguar Bartolomé Institut für Kernphysik, Universität Mainz PSTP 2013 Workshop, Charlottesville 11th September 2013.
Kendra Passow M.S. Graduate Student Mechanical Engineering
R. D. Foster, C. R. Gould, D. G. Haase, J. H. Kelley, D. M. Markoff, (North Carolina State University and TUNL), W. Tornow (Duke University and TUNL) Supported.
1 Technical Arguments in Favor of using the Cryomech PT-415 Cooler for Cooling the LH 2 Experiment Michael A. Green Lawrence Berkeley Laboratory Berkeley.
How many joules are needed to change 120.g of
Raffael‘s Sixtinische Madonna in der Galerie Alte Meister in Dresden.
1 Absorber Heat Transfer and Other Issues A Comparison between MICE and the Forced Flow Absorber System Michael A. Green Lawrence Berkeley National Laboratory.
Phase Changes Melting Vaporization Condensation Freezing Sublimation.
ILIAS meeting Mallorca 2005 V. Fafone Viviana Fafone INFN - LNF Future plans for resonant detectors
DISTRIBUTED CRYOGENIC COOLING WITH MINIATURIZED FLUID CIRCUITS Steffen Grohmann, ETT/TT RD39 Collaboration ST Workshop 2003 CERN, April 01-03, 2003.
TOTEM Collaboration Meeting, Feb. 2005, F. Haug, CERN Cooling System for TOTEM Friedrich Haug and Jihao Wu Cryogenics for Experiments CERN TOTEM Collaboration.
Pacific School Of Engineering. Guided By:- Asst.Prof.Vatsal patel Submitted by:-  Kotadiya Reshma :  Ladva Piyush : 
RLSCamera Cooling1 Camera Cooling Discussion Richard L. Schmitt Fermilab July 14, 2006.
Content 1 Introduction to Cryocoolers
Aim: Students will be able to measure the amount of heat released or absorbed in a chemical reaction. Do Now: What is the difference between potential.
An Autonomous Dilution Microcryostat- Insert for Nano Physics V. S. Edelman, Institute for Physical Problems RAS, Moscow, Russia The cryostat with base.
Thermal Energy (Heat) Temperature (°C) Notes: Thermal Energy and Phase Changes.
Using Dilution Refrigerator Technology to perform experiments on MoS2 Mateusz Zuba, Chen, Yung-Fu, State University of New York at Oswego  Motivation.
Temperature ( o C) Heat (J) Solid Liquid Gas Heat = mass x ΔT x C l Heat = mass x H Fusion Heat = mass x H Vaporization s ↔ l l ↔ g H Vaporization H Fusion.
Refrigeration Basics 101.
GWDAW 9 - December 15 th, 2004 STATUS OF EXPLORER AND NAUTILUS INFN – LN Frascati, LN Gran Sasso, Sez. Roma 1, Roma 2 and Genova Universities “La Sapienza”
CRYOGENICS FOR MLC Cryogenic Cooldown Scheme Eric Smith External Review of MLC October 03, October 2012Cryogenics for MLC1.
Large Area Microcalorimeters of the Diffuse X-ray Background Sarah Bank Towson University August 5, 2004.
Ultra-cryogenics for advanced resonant detectors (C2) G.Frossati Kamerlingh Onnes Laboratory Leiden, The Netherlands Second ILIAS-GW Meeting.
1 NEDM 4 He Purifier and Other Cryogenic Issues David G. Haase North Carolina State University Update on Cryovessel Engineering Evaporative Purification.
Heat Diagram of H2O.
Duke nEDM Collaboration Meeting The status of 3 He Relaxation Time Measurement at ~400mK Q. Ye, D. Dutta, H. Gao, W. Zheng, X. Zhu Duke University R. Golub,
Xkcd. Cryogenics Tyler Brewer Overview History of cryogenics Uses Methods of Cooling Materials Considerations Vibration Issues.
R&D on thermal noise in Europe: the STREGA Project Geppo Cagnoli University of Glasgow AMALDI 6 – Okinawa - Japan June
„Cryogen-free“ Dilution Refrigerators
Phase Changes.
50 Years of Dilution Refrigeration
He3 dilution refrigerator
Bryant Mueller M.S. Student Mechanical Engineering Room: 1335 ERB Hometown: Two Rivers, WI.
Chemistry 1011 Slot 5 Chemistry 1011 TOPIC Thermochemistry TEXT REFERENCE Masterton and Hurley Chapter 8.
Removal of 3 He from 4 He (R&D) David Haase, Franklin Dubose, Travis McCaw and Paul Huffman North Carolina State University.
a magnetic refrigeration stage
Energy Changes & Phase Changes Heating & Cooling Curves.
Lesson 7: Just A Phase Key Terms. Solid A solid has definite volume and definite shape. The particles in a solid are closely packed and vibrate in relation.
Transport of 3 He by heat flush measurement of 3 He concentration tests of heat flush George Seidel Brown University.
1 Small Coolers for MICE Michael A. Green University of Oxford Department of Physics Oxford OX1 3RH, UK MICE Collaboration Meeting RAL.
CRYOGENICS FOR MLC Cryogenic Principle of the Module Eric Smith External Review of MLC October 03, October 2012Cryogenics for MLC1.
ILIAS WG1 - April 7 th, 2005 G.W. ANTENNA NAUTILUS LNF - FRASCATI G.W. ANTENNA EXPLORER CERN - GENEVA Bar Al 5056 M = 2270 kg L = 2.97 m Ø = 0.6 m A =
Dilution Refrigerators with Superconducting Magnets
1 Cryogenic Design and the 4 He Evaporative Purifier David G. Haase, et al., North Carolina State University.
Liquid xenon cryogenic system at KEK. LXe cryogenic system at KEK Xe cylinder Recovery Bottle(3.75L) SAES Getter Monotor 0.75m 3 Tank Circulation Pump.
Important Terms & Notes Feb , Energy Flow During Phase Changes of Matter Energy must be ABSORBED by matter when the phase changes from: –
VAPOUR ABSORPTION REFRIGERATION SYSTEM
Liquids By:MaKenzie,Lei-Lani,Isis & Noah. Definition: Liquids: have a definite volume and takes the shape of a container. Fluid: a substance that can.
Honors Chemistry Podcast 2.3 Joule Problems Q = mc  T.
Initial Tests of the JLab Frozen Spin Target Chris Keith Target Group Jefferson Lab September 13, 2007 Brookhaven National Lab.
Aalto University, Espoo, Finland
The Development of the Dilution Insert and some Tunneling Experiments
1 K thermal model for QUBIC
Refrigeration & air conditioning
NATURAL GAS LIQUIDS RECOVERY
MiniGRAIL “Extreme Make-over” Giorgio Frossati
Production and measurement Techniques of Very low temperature
Changes in states of matter pt.1
Changes in states of matter pt.1
Phase Changes in Matter
Changes in states of matter pt.1
Presentation transcript:

Materials and Cooling Techniques G. Frossati, A.de Waard, L.Gottardi and O.Usenko Kamerlingh Onnes Laboratory Leiden, The Netherlands ESF exploratory workshop: Toward a 3 rd generation European Gravitational Wave Observatory Perugia, Sept. 2005

Sensitivity Minimum detectable energy T eff =T/  Q +2T N For a SQUID noise energy of one quantum Need  ~0.05; Q~2x10 6 : T~30 mK

material properties Dissipation is mainly caused by the mobility of defects  defects freeze out at low temperature  Q-factor increases with reducing temperature

H for several spheres

MiniGRAIL Cryogenics; The dilution refrigerator still (700 mK) 50 mK plate mixing chamber (10 mK)

MiniGRAIL Cryogenics

Next: 33 ton sphere ? Project together with the Roma group to be submitted to INFN h QL ≈4x /√Hz h QL ≈4x /√Hz

Cooling from 300K Fill liquid helium

Forced flow MiniGRAIL 1.4 ton N L 600 L He SFERA ton N L He ! Use 4 GM cryocoolers For pre-cooling from 300K to 20K 4 PT410 for cooling to 4K and for the dilution refrigerator GM600 (Cryomech) 1200W at 250K PT400 60W at 60K and 1W at 4.2k Heat to remove ~70J/gm ~2.8x10 9 J Cool-down time ~2 weeks to 4k

Liquid mixtures of 3 He and 4 He He concentration T (K) Superfluid 3 He/ 4 He Normal 3 He/ 4 He -line Two-phase region

Dilution Refrigeration as an upside-down evaporation VAPOR LIQUID 3 He out 3 He in diluted phase

Dilution Refrigeration; Schematic view CIRCULATION SYSTEM  STILL  HEAT EXCHANGER  M IXING CHAMBER  HEAT ABSORPTION REGION 1k POT HEAT FLOW T MC

Pulsed tube dilution refrigerator Joule Thompson heat exchanger replaces the 1K pot: No need for Helium bath JT Heat exchanger PTR Mixing Chamber 50K 4K 600 mK 60 mK 10 mK

Strain sensitivity 2m CuAl6% sphere  f=1000 Hz  f=100 Hz  f=10 Hz MiniGRAIL