Vacuum Technology-2 Concepts and Key Points Jim Jr-Min Lin 林志民 Institute of Atomic and Molecular Sciences Academia Sinica, Taipei, Taiwan 106 原分所 Department.

Slides:



Advertisements
Similar presentations
Vacuum Science and Technology in Accelerators
Advertisements

Sampling and Measurement for Volatile Organic Compounds
Machine Tools And Devices For Special Technologies Electrochemical machining Slovak University of Technology Faculty of Material Science and Technology.
First Law of Thermodynamics
Chapter 11 “Stoichiometry”
Machine Tools And Devices For Special Technologies Plasma machining Slovak University of Technology Faculty of Material Science and Technology in Trnava.
Vacuum System Design Considerations Materials Plumbing –Pumping –Throughput Ultimate pressure –Dynamic equilibrium –Pumping speed –Leaks.
Chapter 22 Solutions.
Overview of Vacuum Systems Tejas Deshpande 24 July, 2014.
ASHOKA INSTITUTE OF TECHNOLOGY & MANAGEMENT AKTHA, SARNATH VARANASI
Vacuum Fundamentals High-Vacuum Technology Course Week 8 Paul Nash HE Subject Leader (Engineering)
High-Vacuum Technology Course
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Vacuum Fundamentals Lecture 5 G.J. Mankey
Ch. 6 Thermal Energy. 6.1: Temperature and Heat Temperature  measure of the average kinetic energy of the particles in a sample of matter.
SSRF1 ALUMINUM ALLOY VACUUM CHAMBERS FOR SSRF L.X. Yin, D.K. Jiang, H.W. Du, X.L. Jiang SSRF Vacuum Group Shanghai National Synchrotron Radiation Center.
Vacuum equipment. Pumps Rotary vane pumps Rotary piston pumps Roots pumps Turbo molecular pumps Diffusion pumps Getter pumps –Sublimation pumps.
Vacuum Technology Need for Vacuum Environment
1 Boyle’s Law (T and n constant) Charles’ Law (p and n constant) Combined Gas Law (n constant) Summary of Gas Laws p 1 ×V 1 = p 2 ×V 2.
Basics of Vacuum Technology Unit: Pa = N/m 2 = J/m 3 UnitPa or N/m 2 bar10 5 mbar100 atm= 760 torr x 10 5.
The Deposition Process
Engine Friction Dr Jehad Yamin.
Photoelectron Spectroscopy Lecture 5 – instrumental details –General spectrometer design –Vacuum generation and measurement.
High-Vacuum Technology Course
實況 與 經驗 Practical Considerations of Pulsed Molecular Beam
Pressure 1 atmosphere ~ 1 bar ~ 760 mm Hg ~ 760 torr ~ 100,000 Pa Ion gauges read in mbar i.e. 1x mbar = 1x atm. Sometimes ion gauges read.
Solar Cell conductive grid and back contact
Phases of Matter.
GAS LAWS. Properties of Gases  Composed of randomly scattered particles  No definite _________ or ___________  Spread out to fill the space of their.
Oxyfuel Cutting And Welding. Introduction  Oxyfuel: the process of combining pure oxygen with a combustible fuel gas to produce a flame  Can be used.
Vacuum science.
Reference book: Building Scientific Apparatus A practical guide to design and construction by John H. Moore, C. C. Davis and M. A. Coplan 2ed or 3rd edition.
Vacuum Fundamentals 1 atmosphere = 760 mm Hg = kPa 1 torr = 1 mm Hg vacuum range pressure range low 760 ~ 25 torr medium 25~ high ~ 10.
Chapter 13 States of Matter
PHYSICS 225, 2 ND YEAR LAB VACUUM TECHNOLOGY G.F. West Thurs, Jan. 12.
Techniques of Vacuum and Basics of High Voltage (2/3) Pauli Heikkinen Jyväskylä University.
Chapter 22 Solutions.
Matter & Change. What is matter? Matter is anything that has mass and takes up space. Quantifying Matter – Measuring Matter Mass – measure of the amount.
Vacuum Fundamentals High-Vacuum Technology Course Week 6 Paul Nash HE Subject Leader (Engineering)
Vacuum Fundamentals 1 atmosphere = 760 mm Hg = kPa 1 torr = 1 mm Hg vacuum range pressure range low 760 ~ 25 torr medium 25~ high ~ 10.
Metals, Making Electricity and Corrosion. Metals The job that a metal is used for is determined by its physical and chemical properties. Physical properties.
High-Vacuum Technology Course
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Vacuum Systems Lecture 6 G.J. Mankey
Chapter Gases: Mixtures and Movements. The surface of a latex balloon has tiny pores through which gas particles can pass. The rate at which.
Energy and the Environment Fall 2013 Instructor: Xiaodong Chu : Office Tel.:
2009/1/16-18 ILD09 Seoul 1 Notes for ILD Beam Pipe (Technical Aspect) Y. Suetsugu, KEK Parasitic loss Vacuum pressure profile Some comments for beam pipe.
Vacuum Technology.
Solar Cells need a top side conductor to collect the current generated They also need a conductive film on the backside.
Chapter 8 Substances, Mixtures, and Solubility. I. Substances A. Atoms and Elements A substance is matter that has the same fixed composition and properties;
Outgassing Test and the Getter Specification
States of Matter and Mixtures and Solutions Carl Wozniak Northern Michigan University.
1. Which of the following is NOT a conversion factor for 1 mole of a substance? A. 1.0 g B. molar mass C X particles D L E. Avogadro’s.
Vacuum Technology and Components for Cryogenics
Copyright ©2008 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Introductory Chemistry: Concepts & Connections, Fifth.
Matter & Change 1. What is matter? Matter is anything that has mass and takes up space. Quantifying Matter – Measuring Matter Mass – measure of the amount.
6/14/20161 Chapter 10- Causes of Change Heat and Chemical change.
Leak Detection method for Vacuum Systems Alexander Permogorov
CH4: Gases and their Properties NOTES #5. Diffusion  Caused by random motion!!! And collision of molecules  Random motion of molecules and their collisions.
Phase Changes & Solids AP Chemistry. Phase Changes.
Jari Koskinen 1 Thin Film Technology Lecture 2 Vacuum Surface Engineering Jari Koskinen 2014.
Vacuum Systems for Electron Microscopy Constraints on Specimens Specimens placed in the electron microscope must be able to withstand very high vacuum.
Holders and Pumps Summary
7.5 – NOTES Inappropriate Levels in Water
Thermal Outgassing Rate for Various Beam Line Materials
-Honors Thesis Defense- In Situ Ellipsometry of Surfaces in an Ultrahigh Vacuum Thin Film Deposition Chamber Joseph Choi Department of Physics and Astronomy,
VIII. Production of Vacuum
properties & structure
CHAPTER 16 Solids and Liquids 16.3 Metals and Alloys.
BASIC VACUUM PRACTICE.
Chapter 2 Chemistry of Life
Presentation transcript:

Vacuum Technology-2 Concepts and Key Points Jim Jr-Min Lin 林志民 Institute of Atomic and Molecular Sciences Academia Sinica, Taipei, Taiwan 106 原分所 Department of Applied Chemistry National Chiao Tung University, Hsinchu, Taiwan 300 交大應化系

1 Mean Free Path of gas molecules: Viscose flow Vs. Molecular flow Gas flow: Throughput, Conductance, Pumping speed Pumps: Mechanical, Roots, Turbo, Diffusion, Dry, Ion, Cryo, Gauges: Mechanical, Thermal conductance, Ionization, Chambers: Joints (metal, elastomer), parts 2 Practical concerns: Surface Material: SUS, Al alloy, ceramic, plastic, Baking Virtual leak Leak test UHV Outlines:

Surface Outgas Concern example: mol H 2 O, 18 mg, liquid 1.8x10 -2 cm 3 ; gas 2.4x10 -2 ℓ at 1 atm If mol H 2 O in chamber surface and if the outgas pressure is torr, how long it takes to pump down to torr when the pumping speed is 1000 ℓ /s? Initial pumping throughput is torr * 1000 ℓ /s = torr ℓ /s Total amount of water is 1 atm * 2.4x10 -2 ℓ = 760 torr * 2.4x10 -2 ℓ = 1.8 x 10 1 torr ℓ Assume: outgas rate ∝ water amount ∝ P, i.e. ∝ pump out throughput Q=PS i.e. first order rate equation

example of exponential decay same area under both curves

2.3  = 115 hr to reduce 10x pressure Often for a chamber with big surface area Pump out time constant =  Big chamber ≠ big surface area

How to minimize surface area Remove thick surface oxide: electro polish SUS chamber and parts basic wash (NaOH solution) Al alloy acid wash copper/brass parts sand blast Oxide could be porous Dirty surface is thicker Strong detergent is much more efficient than solvent Cleaning

Estimate the effect of Baking When temperature rises by 100 o C, outgas rate rises by roughly two orders of magnitude, i.e., torr instead of torr Initial pumping throughput is torr * 1000 ℓ /s = torr ℓ /s to P = torr, P 0 /P = 10 5 Practically, it takes a little bit longer ( ≲ 100 hr) ∵ Single exponential delay is only an approximation Deeper water has smaller outgas rate, thus longer 

bake uniformly is important to avoid distortion Don’t bake oily surface. oil  tar Aluminum foil on SUS chamber, heating tape on the aluminum foil, another layer of aluminum foil to reduce heat loss Degas ion gauge during baking Clean ion gauge and its surrounding by excess heating

Estimate the effect of using plastic parts plastic may absorb H 2 O to 1~2 % w/w Assume 100 g plastic can absorb ~1.8 g H 2 O = 0.1 mol If the initial outgas pressure is torr,  = 5000 hr If the initial outgas pressure is torr,  = 500 hr more troublesome is that most plastics cannot be baked Use only Inert material: Teflon, PE, PP, Kel-F, Viton, Teflon insulated wire High temperature material : polyimide (Vespel, Kapton), Kalrez (O-ring) Less absorption Bakable to 200 o C less inert than Teflon

Material outgas (volume outgas) SUS: H 2 & CO. SUS316L can be vacuum firing at 1000 o C to remove deeper contaminants Al alloy: less H 2 & CO. Bakable to 120 o C Zn & Cd alloy have high vapor pressure High temperature increase bake out Cooling can reduce use It lasts forever! More than your life!

Metal seal: copper gasket & ConFlat flange are preferred Sealing Concern: 100% seal low outgas bakable O-ring seal: Viton O-ring bakable to 100 o C 15 ~ 18 % compression to seal volume compression is not allowed sealing surface polish is important small leak is possible ( Hard to find small leaks) convenient non-consuming Careful to use viton gasket on conflat flanges very easy to leak for size larger than 4.5” two surfaces may fuse together use silver plated screws in SUS taps not cheap

Dynamic Seal a virtual leak without differential pumping 760 torr * L = torr * 1000 ℓ/s L = 1.3 x10 -7 ℓ/s 760 torr torr 1000 ℓ/s 760 torr P2P2 0.1 ℓ/s P3P3 with differential pumping 760 torr * L = P 2 * 0.1 ℓ/s P 2 = 1 x10 -3 torr P 2 *L=P 3 *1000 ℓ/s P 3 = 1.3x torr O-ring: 15  2 % compression + Grease polished surfaces to have the above leak rate careless work makes 1~2 orders worse O-ring may trap gas & water ⇒ Virtual leak rotatable or translational

Virtual Leak: Gas trapped in a vacuum system, can’t be found from outside 1 cc at 1 atm = 760 x 10 7 cc at torr = 7.6 x 10 6 ℓ at torr pressure drop takes 2.3  Estimate pump down time constant if leak out rate is 1.32x10 -7 ℓ/s and the chamber is pumped at 1000 ℓ/s, that is, 760 torr x 1.32x10 -7 ℓ/s = torr x 1000 ℓ/s O-ring can trap small bubbles and release them when being moved. leak: 1.32x10 -7 ℓ/s 1 cc at 1 atm pumped at 1000 ℓ/s, 1x10 -7 torr

Leak Check Spread CH 3 OH or C 2 H 5 OH on a possible leak to see if pressure rises Acetone is OK for metal, bad for O-ring, bad for health Response rise time ~ few seconds, Don’t move too fast. It takes very long to dry out the solvent. Very long fall time From lower spots to higher spots. Helium leak check: Spread He to see if P He rises MASS is required. RGA or He leak detector fast ≲ 1 sec ∵ light mass ∴ fast speed He is fast to escape, fast to pump down low background inert from higher spots to lower spots He is easy to reach a nearby spot. ⇒ isolation

high m28/m32 (4:1) indicate air leak daughter ion is useful. CO + C + O + Vs. N 2 + N + Don’t make vacuum chamber wet, especially at a rainy day H 2 O is very common RGA provide very important information

Good vacuum practices No leak Clean: traps for oil pumps: molecular sieve, LN2 Metal & non-porous ceramic is excellent Plastic and grease: as less as possible Confident sealing. Finding a leak is labor consuming. Bakable for torr or better Good local conductance for pumping speed Gas composition (partial pressure) is often more important than the total pressure, as most vacuum parameters are species dependent. e.g. surface laser burn, background masses RGA is very nice to have

Example of utilizing a sorption pump to recycle isotope gases, see §3.4.3 pump 2 turbo pump ℓ /s P 1 = 1x10 -5 torr O 2 ( 18 O, 97%, > NT$10000/ ℓ ) ℓ: std liter (1 ℓ at standard condition, i.e. 298K, 760 torr) If pump 2 = mechanical pump, O 2 will be mixed with air and oil. If pump 2 = molecular sieve sorption pump, O 2 can be absorbed at liquid nitrogen temperature and retrieved at room temperature. molecular sieve gas inlet Question: How much O 2 (in atm ℓ ) is used per hour?  25mm  6mm

Quiz: Write answer on a page of A4 paper A mixture of 10% C 4 H 10 in He flows into a vacuum chamber pumped by a turbo pump. The Ion Gauge reading is 5x10 -6 torr. (a) What is the true pressure? (b) What is the pressure reading for a 20% mixture at the same flow rate? Note: Given that the relative electron impact cross section:  (N 2 )=1,  (He)=0.15,  (C 4 H 10 )=5

Untra High Vacuum < 1x torr Example of 1 x torr Practically clean chamber, turbo pump, not baked, torr clean chamber, 2 serial turbo pumps, baked, torr (compression ratio for H 2 )

LN2 78K <10K 50K He cold head (remove displacer to bake) room temperature 5x torr LN2 3x torr (much cleaner) cold head 1x torr

How to make Ultra High Vacuum (UHV): Outgas rate = pumping speed x pressure 100 ℓ/ s x torr Ultimate pressure of pumps Outgas rate Effective pumping speed 2 serial Turbo Pumps: torr, H 2 compression ratio Ion Pumps : torr, small pumping speed, memory effect Getter Pumps: Titanium Sublimation pump, Non-evaporative getter Cryopump: torr, not-bakable, memory effect Materials: Stainless Steel, Al alloy, OFHC copper, ceramic, teflon, kapton S -1 = S S 2 -1 Bake & Contamination: Firing, porous oxides, oil→tar→charcoal Virtual Leaks Low temperature: LN2, cryohead Surfaces: mechanical polish (glue on sand paper!), electro polish, acid, base

Turbo pumps: 400 ℓ /s, 600 ℓ /s compression ratio: 10 4 for H 2, 10 6 for He,10 9 for N o C Oil, grease, or magnetic bearing and insulated wires Fore line back stream when Electric shutdown Getter pumps: Ion, Ti, NEG No foreline needed, no continuous electricity needed 250 o C, 400 o C Not for every gas, memory effect Low maintenances for low load systems

Cryopumps: >1500 ℓ /s, bake to 70 o C, Not for every gas, memory effect Outgas due to activated carbon absorber Electric shutdown Cryopump + turbo pump: Very high pumping speed even for H 2 at torr Bakable Cryohead without absorber: high pumping speed for H 2 at < torr Low outgas  torr

SUS304, SUS304L: Cr 18%, Ni 10%, Fe, C<0.2 % or Low carbon < 0.08% SUS316, SUS316L: Cr 18%, Ni 10%, Mo 2-3%, std and Low carbon Sand ballasting, basic detergent, Acid dip, Electro polish, DI water Easy to be welded, Bake to 250 o C, SUS316L: Fire at 1000 o C at torr Major outgas: H 2, CO Al alloy 6061-T6, and others Low H 2, CO outgas Welding at outside, must clean before welding NaOH(aq), HNO 3 (aq), Al 2 O 3 is porous. Mirror finish parts is available (Japan) 120 o C, high temperature will change tempering condition

Plastic: gas/water permittivity is high Teflon absorb water 10 times less than usual plastics, but still too much for UHV Teflon, PE, PP, might be OK for torr, others are only good to torr. polyimide (Kapton) is bakable, torr Oxygen Free High Conductance copper, Beryllium copper Brass and bronze could be dirty (zinc, phosphor) Special (strong) acid brightening Ceramic could be porous Al 2 O 3 (alumina) (thermal conductance better than SUS) Vacuum firing