Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 1 Cryolab Cooling of electrically insulated.

Slides:



Advertisements
Similar presentations
Boiling heat transfer of liquid nitrogen in the presence of electric fields P Wang, P L Lewin, D J Swaffield and G Chen University of Southampton, Southampton,
Advertisements

Materials properties at low temperature
Quiz – An organic liquid enters a in. ID horizontal steel tube, 3.5 ft long, at a rate of 5000 lb/hr. You are given that the specific.
Electro-Hydro-Dynamics Enhancement of Multi-phase Heat Transfer
Energy in Thermal Processes
Analysis of Simple Cases in Heat Transfer P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Gaining Experience !!!
Inverse Heat Conduction Problem (IHCP) Applied to a High Pressure Gas Turbine Vane David Wasserman MEAE 6630 Conduction Heat Transfer Prof. Ernesto Gutierrez-Miravete.
Electric cooling from room temperature down to 200 mK M.Tarasov, L.Kuzmin, and I.Agulo, Chalmers University of Technology, S41296, Göteborg, Sweden V.Mikheev,
1 Model 4: Heat flow in an electrical conductor A copper conductor is sheathed in an insulator material. The insulator also stops heat from escaping. Imagine.
CHE/ME 109 Heat Transfer in Electronics
Conduction. Transfer Mechanisms  Conduction Energy flow from direct thermal contactEnergy flow from direct thermal contact  Radiation Energy radiating.
One Dimensional Polar Geometries For Conduction with Heat Generation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A.
The Heat Conduction Equation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi An Easy Solution to Industrial Heat Transfer.
One Dimensional Steady Heat Conduction problems P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Simple ideas for complex.
Solutions of the Conduction Equation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi An Idea Generates More Mathematics….
Boyce/DiPrima 10th ed, Ch 10.5: Separation of Variables; Heat Conduction in a Rod Elementary Differential Equations and Boundary Value Problems, 10th.
Feasibility Analysis h T1 T2 T3 T4 T5 One Dimensional Transient Analysis One Dimensional Finite Difference Steady State Analysis T1 and T5 will be known.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
MECHANISMS OF HEAT TRANSFER
PRESENTED BY ALBERT.N Under the guidance of Mr.N.RAMANUJAM M.E (Ph.d) (Associate Prof/Hod- Mech) DEPARTMENT OF MECHANICAL ENGINEERING E.G.S.PILLAY ENGINEERING.
Presented by Anas Mazady, Cameron Fulton, Nicholas Williams University of Connecticut Department of Electrical and Computer Engineering Thursday, April.
STEADY HEAT TRANSFER AND THERMAL RESISTANCE NETWORKS
Workshop on Beam losses, heat deposition and quench levels for LHC magnets, Geneva, 3-4 March 2005 Liquid helium heat transfer in superconducting cable.
Methods of Energy Transfer
Research at Welding Equipment and Engineering Department Speaker: Andrey Batranin, PhD. Student Tomsk Polytechnic University Non-destructive Testing Institute.
Anharmonic Effects. Any real crystal resists compression to a smaller volume than its equilibrium value more strongly than expansion to a larger volume.
University of Miskolc Department of Mechanical Engineering Modelling of Laser Surface Treatment Tutor: Dr. Mária Kocsis Báan Consultant: Mr. Reza Roshan.
CBE 150A – Transport Spring Semester 2014 Non-Steady State Conduction.
Hyperbolic Heat Equation 1-D BTE assume Integrate over velocity space assuming that  is an averaged relaxation time (4.63a) (4.64) or.
Yoon kichul Department of Mechanical Engineering Seoul National University Multi-scale Heat Conduction.
Russian Research Center” Kurchatov Institute” Theoretical Modeling of Track Formation in Materials under Heavy Ion Irradiation Alexander Ryazanov “Basic.
5 장 Dielectrics and Insulators. Preface ‘ Ceramic dielectrics and insulators ’ is a wide-ranging and complex topic embracing many types of ceramic, physical.
Studies of the Cryogenic Part with Load Lock System T. Eisel, F. Haug CERN TE-CRG-CI October 19 th, 2011, Page 1 Superconductivity years Heike Kamerlingh.
7.1.1 Hyperbolic Heat Equation
HEAT TRANSFER FINITE ELEMENT FORMULATION
Unsteady State Heat Conduction
L. Serio COPING WITH TRANSIENTS L. SERIO CERN, Geneva (Switzerland)
Chapter 6 Overview. Maxwell’s Equations In this chapter, we will examine Faraday’s and Ampère’s laws.
Modelling and Simulation of Passive Optical Devices João Geraldo P. T. dos Reis and Henrique J. A. da Silva Introduction Integrated Optics is a field of.
Russian Research Center” Kurchatov Institute” Shock wave propagation near 450 GeV and 7 TeV proton beams in LHC collimator materials Alexander Ryazanov.
CRYOGENICS FOR MLC Cryogenic Principle of the Module Eric Smith External Review of MLC October 03, October 2012Cryogenics for MLC1.
Cooling of GEM detector CFD _GEM 2012/03/06 E. Da RivaCFD _GEM1.
ERT 206/4 THERMODYNAMICS SEM 2 (2011/2012). light Energy can exist in numerous forms: Thermal Mechanical Kinetic Potential Electric Magnetic Chemical.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
Simulation of Phase transformation behavior of NiTi doped with Cu during loading using classical molecular dynamics S. Aich, A. Behera and S. Ghosh Department.
Ch. 12 Partial Differential Equations
CERN Cryolab CO 2 cooling for pixel detectors Investigation of heat transfer Christopher Franke, Torsten Köttig, Jihao Wu, Friedrich Haug TE-CRG-CI.
Some considerations about design and technology AE IS DT Science-Techno Tea meeting Diego Perini
Contents: Computer Code
Thermal Physics Energy meter Thermometer Immersion heater
Tutorial 2b: Thermo-physical properties
CERN co-worker: Thomas Eisel (lecturer) Diego Perini Friedrich Haug
Cryogenic Safety- HSE seminar CERN,
Organization of proposed cryolab collaboration with AEGIS
Chapter 2: Introduction to Conduction
Nathaniel Garceau, Wei Guo, Thomas Dodamead
Simulated thermal performance of triple vacuum glazing
Building Energy Analysis
MiniGRAIL “Extreme Make-over” Giorgio Frossati
UNIT - 4 HEAT TRANSFER.
HIGH VOLTAGE ENGINEERING. ACTIVE LEARNING ASSIGNMENT : CONDUCTION AND BREAKDOWN IN COMMERCIAL LIQUIDS. PREPARED BY : JOBIN ABRAHAM.
4.6 Anharmonic Effects Any real crystal resists compression to a smaller volume than its equilibrium value more strongly than expansion due to a larger.
Nanofluids: A Review Wednesday, 3rd March 2010.
Chapter One Thermal-fluid sciences involve the transfer, transport, and conversion of energy, usually studied under the subcategories of thermodynamics,
Conduction thermal resistance in different coordinate system
Table 3. Main properties of the thin brass electrode
Source of variation Degrees of freedom Sum of squares Mean square
Cryogenic management of the LHC Run 2 dynamic heat loads
Temperature Distribution Study of Composite Germanium Detector
Presentation transcript:

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 1 Cryolab Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements Eisel T., Bremer J., Burghart G., Feigl S., Haug F., Koettig T. CERN, 1211 Geneva 23, Switzerland

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 2 Cryolab Electrodes integrated in AEgIS Cooling source: Dilution Refrigerator (DR) Cooling design: Sandwich Theory of dynamic measurements Simulation Results of dynamic measurements Discussion/ conclusion Content Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 3 Cryolab AEgIS 1 experiment at CERN Scientific goal: influence of g upon antimatter Penning trap at 100 mK  deceleration of particles AEgIS Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements DRMC 1

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 4 Cryolab Standard cooling source: DR 1 – (0.002 to ~ 0.5) K – Continuous operation – Dilution of 3 He in 4 He – 0.05 K Dilution Refrigerator Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements 1

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 5 Cryolab Sandwich Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements 1 G. Frossati. Experimental Techniques: Methods for Cooling Below 300 mK. Journal of Low Temperature Physics, Vol. 87, Nos. 3/4, 1992

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 6 Cryolab Antimatter creation/ annihilation (Illuminati) is periodically (200 s) Dynamic measurements – Information on how fast inserted heat can be transferred – Key property which determines the propagation-speed of a heat wave in an homogeneous material: material’s thermal diffusivity a ( m 2 / s )... thermal conductivity ρ... density c p... specific heat capacity Theory of dyn. meas. Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements Sandwich’s thermal diffusivity a*

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 7 Cryolab Theory of dyn. meas. Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements Semi-infinite rod (one dimensional) One end imposed temp. function T H =f(t) (sin, pulse ) T C =f(t) at certain distance  Alteration of the original function (phase shift, attenuation ) material’s thermal diffusivity a can be analytically solved

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 8 Cryolab Simulation Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements Sandwich is not a semi-infinite rod (T MC =const) Imposed temp. function T H is not sinusoidal (square heat wave)  Simulation (MATLAB ®,pdepe): – T H (t)=T H,meas (t) – T MC =T MC,meas – x S =x Sapphire – T C,sim =T C,meas x therm Sandwich’s thermal diffusivity a*

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 9 Cryolab Results Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements

Studies of the Cryogenic Part with Load Lock System T. Eisel, CERN TE-CRG-CI AEgIS November 11 th, 2010 Page 10 Cryolab For temperatures > 30 mK an indium deposition improves the diffusivity significantly (about a factor of 2) The surface roughness influences the diffusivity only minor  contrary to static measurements 1 ; conclusion: heat transfer mechanisms of dynamic and static measurements are different Discussion/ conclusion Cooling of electrically insulated high voltage electrodes down to 30 mK – Dynamic measurements 1 Eisel T., Bremer J., Burghart G., Feigl S., Haug F., Koettig T., Cooling of electrically insulated high voltage electrodes down to 30 mK. Proceedings of the twenty third cryogenic engineering conference, Poland; Sandwich’s thermal diffusivity is more than 6 orders of magnitude smaller than the thermal diffusivity of copper or sapphire  thermal boundary resistance The diffusivity is not constant, it diminishes with reduced temperature  thermal boundary resistance  The fastest heat propagation could be achieved along a Sandwich using indium deposited and polished sapphire plates