International Union for Vacuum Science, Technique and Applications

Slides:



Advertisements
Similar presentations
Union Internationale pour la Science,la Technique et les Applications du Vide International Union for Vacuum Science, Technique and Applications Internationale.
Advertisements

CFCs/HCFCs Warrington Williams – Thanks to John Meyer Environmental Affairs Director John Morrell & Company.
E VERY L IFE H AS A P URPOSE… Chemgard TM Infrared Gas Monitor.
QUALITY ASSURANCE OF LARGE AREA RPC DETECTOR : TECHNIQUES FOR MEASUREMENT OF GAS LEAK RATE By Avinash V. Joshi Alpha Pneumatics, Mumbai (India)
Chapter 10 Chemical Quantities
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
Phases of Matter Properties of a Gas Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
Amedeo Avogadro In order to state that equal volumes of all gases at the same temperature and pressure contain the same number of molecules, Amedeo Avogadro.
Measuring Pressure. Atmospheric Pressure Recall: Caused by the weight of the air molecules above us. Typically kPa or Pa Measured using.
1 Chapter 4 - Gases Movie – phase diagrams Kinetic Theory Pressure Measurement –Units –Unit Conversions Boyle & Charles Combined Gas Law.
Pressure and particles
Empirical and Molecular Formulas
Automotive Heating and Air Conditioning, Fifth Edition By Tom Birch © 2010 Pearson Higher Education, Inc. Pearson Prentice Hall - Upper Saddle River, NJ.
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.
PHYSICS 225, 2 ND YEAR LAB VACUUM TECHNOLOGY G.F. West Thurs, Jan. 12.
AOSC 634 Air Sampling and Analysis
The SEM and Ion Pumps. UHV Systems UHV – Ultra High Vacuum Pressures of less than 10^-11 mbar Pumps at an “atomic level”
High-Vacuum Technology Course
1 Air Conditioning EPA Core. 2 Effects of Ozone Depletion Skin Cancer Cataracts Crop loss Immune system deficiencies. Skin Cancer Cataracts Crop loss.
Vacuum tests Problem description Valve presentation Test setup Measurements & Results Conclusions.
PIMS IN INSTITUTE FOR NUCLEAR STUDIES Brazing Andrzej Soltan Institute for Nuclear Studies.
The Nuclear Atom Rutherford modified Thomson’s model: –assume the atom is spherical but the positive charge must be located at the center (it’s small and.
Section 10.3 Percent Composition and Chemical Formulas n n OBJECTIVES: – –Describe how to calculate the percent by mass of an element in a compound.
Vacuum Fundamentals High-Vacuum Technology Course Week 7 Paul Nash HE Subject Leader (Engineering)
Automotive Heating and Air Conditioning, Fifth Edition By Tom Birch © 2010 Pearson Higher Education, Inc. Pearson Prentice Hall - Upper Saddle River, NJ.
Ideal Gases Physics – Molecular Kinetic Theory , &
The ideal gas equation. Room temperature and pressure, RTP Limitations At RTP, 1 mol of gas molecules occupies 24.0 dm 3 Conditions are not always room.
Concept of Humidity What is the relationship between water vapor holding and temperature? Air hold more water vapour at higher temperature.
Review Label which units are pressure and which are volume: Atm ________cm^3 ________ L _________ torr _________.
Leak tests G. Apeldoorn, P. Vankov , NIKHEF.
Unit 10: Gases Section 1: Combined Gas Law. Introduction Molecules in a gas behave uniquely…  Gas molecules move rapidly and expand to fill their space.
Gases II Dr. Ron Rusay. Experimentally Determining The Moles & Molar Mass of Hydrogen Applying Avogadro’s Law Using the Ideal Gas Law & Partial Pressures.
Leak Detection method for Vacuum Systems Alexander Permogorov
Thin Film Technology - Student Talk Sophie Chauvin 02/02/16 Leak Detection method for Vacuum Systems 1.
Take your periodic table out. What is atomic mass of Carbon Point where you can find it in the periodic table! 6 is atomic number not atomic mass Atomic.
Percent Composition, Empirical Formulas, & Molecular Formulas Section 10.4.
3. Climate Control Systems Service Automotive – Heating & Air Conditioning Topics covered in this presentation: Gauge set and refrigerant Service ports.
Prepared by:- B.S.Bhandari Faculty HNBGU.  Refrigeration is a science of producing and maintaining temperature below that of the surrounding temperature.
Chapter 4 Training Package HCFC Phase-out RACSS – UNEP 2014 Servicing of HCFC/HFC Based Air-conditioners.
Vacuum Leak Exercises CAS VACUUM, 6-16 June 2107
General Physics: Ideal Gas Law and Kinetic Theory
Climate Control Systems Service Air Conditioning System Service
Sub-system integration for the VBOX
Gases.
Vacuum At LLO 2016 SURF Udochu, Ogbonnaya LIGO-T
Introduction to Food Engineering
Process and Process Variables
Chapter 6 Gases 6.1 Properties of Gases 6.2 Gas Pressure.
Section 9.3—Analysis of a Chemical Formula
Chemistry 13.1.
Gas Law Calculations.
General, Organic, and Biological Chemistry
Chapter 10 – Chemical Quantities
Gases.
The ideal gas equation.
Section 8 References & Acknowledgements
Chemistry 13.1.
Basic Chemistry Chapter 11 Gases Chapter 11 Lecture
Mole Map Representative Volume of Gas Particles (STP) 0o C 1 atm
VISUAL AIDS for instruction in VACUUM TECHNOLOGY AND APPLICATIONS
Chapter 19 Avogadro’s Principle.
Physics 2 – Feb 10, 2017 P3 Challenge – A 1.25 kg sample of copper (c=386 J/kgK) is heated to 100.0C and then transferred to a Styrofoam calorimeter.
Section 3 Methods of leak detection
Atmosphere and Climate Change
The Mole Mole: convenient measure of chemical quantities.
Chapter 8 Gases The Gas Laws of Boyle, Charles and Avogadro
Physics 2 – Mar 14, 2019 Do Now: If not yet, go to and sign up.
Vacuum System Design for the Target Monolith System
Presentation transcript:

International Union for Vacuum Science, Technique and Applications VISUAL AIDS PROGRAM of the International Union for Vacuum Science, Technique and Applications Module 6 LEAK DETECTION © 2004. IUVSTA 1.00

Section 1 Introduction to leak detection © 2004. IUVSTA 1.01

Leak detection has many applications ICs LCD Displays Medicine Industry Automotive Aviation Semiconductor technology © 2004. IUVSTA 1.02

Small defect sizes cause leakages Typical leakage 10-2 mbar l/s Typical leakage 10-7 mbar l/s A micron- sized hole Cross-section of a human hair © 2004. IUVSTA 1.03

Typical leak rate ranges for detectors Pressure drop Pressure rise Ultrasonic - Bubbletest He – sniffing leak detection He – vacuum leak detection Bubbletest 10-12 10-11 10-10 10-9 10-7 10-8 10-6 10-5 10-4 10-3 10-2 10-1 100 101 H2 - sniffing leak detection SF6 – vacuum leak detection SF6 – sniffing leak detection Notes 1/ This slide was taken from the 1st Edition slide 06-038 augmented by some special modern methods. © 2004. IUVSTA 1.04

Acceptable leakage rates for bike tyres? Want a maximum pressure drop of 1000 mbar over 175 days before repumping tyre! Volume = about 1.5 Litre 175 days = 1.5 x 107 seconds What then is the maximum acceptable Leak rate? © 2004. IUVSTA 1.05

Example: a tyre leak rate in mbar l/s Formula: Unit: = mbar l s-1 qL=[V * (p2 - p1)] / t [qL] = mbar l s-1 – Leak rate [V] = l - Volume Test part [p1] = mbar – pressure at the start of the (measurement) period [p2] = mbar - pressure at the end of the elapsed (measurement) period t - s © 2004. IUVSTA 1.06

Leak rate conversion tables UNIT mbar l/s Pa l/s Torr l/s lusec cm3/s cm3 /hour kg/hour Air g/year R12 1 100 0.75 751 3560 4.3E-3 1.55E5 0.01 7.5E-3 7.51 0.99E-2 35.6 4.3E-5 1.55E3 1.33 133 1000 1.32 4738 5.7E-3 2.1E5 1.33E-3 0.133 1E-3 1.32E-3 4.74 5.7E-6 2.1E2 1.01 101 0.76 759 3600 cm3 /hour 2.81E-4 2.81E-2 2.11E-4 2.11E-1 2.7E-4 1.21E-6 4.30E1 230 23000 175 1.75E5 8.29E5 - 6.4E-6 6.4E-4 4.90E-6 4.80-3 2.3E-2 Notes 1/ This table derives directly from the 1st Edition of the IUVSTA Visual Aids Module 6, slide 06-039, with additional comments on the CFC replacement of R12 by the present author. 2/ The conversion table assumes units of Pressure x Volume / Time are at normal temperature (Tn), while the units of Volume / Time are at both Tn and normal pressure Pn=1013mbar. The table shows that 1mbar.l/s (Tn) = 0.99 cm3/s. (Tn.Pn). In actual practice one generally uses 1mbar.l/s = 1 cm3/s (Tn.Pn) = 1 std.cc/s. 3/ The temperature of the Air in the conversion table is 20°C 4/ R12 is Freon 12, chemical formula CCl3F. This material is banned under the Montreal Protocols on CFC elimination. Other refrigerants, blowing agents and propellants are now used in their stead, for which the g/year value will be different by the scaling factor provided by the inverse ratio of their molecular weights to R12 (Mol weight= 135.5). Thus R134a, which is an HFA molecule containing no chlorine atoms, having Mol weight= 102, has higher g/year for the given Pressure x Volume / Time unit by the scaling factor = 135.5/102 © 2004. IUVSTA 1.07

Typical limits for vacuum components Absolute Pressure range in Vacuum leak tightness units = mbarl/s Components used in systems Rough vacuum 1000 to 1 mbar < 10-5 Backing valves roughing valves Medium vacuum 1 to 10-3 mbar < 10-7 Vapour boosters foreline traps High vacuum 10-3 to 10-7 mbar < 10-9 Secondary pump bodies & valves Ultra-high vacuum < 10-7 mbar < 10-10 Bakeable valves; UHV component Notes 1/ This slide was taken from Mass Spectrometer leak detectors published by Edwards High Vacuum International. The material was gleaned from production tests and is merely indicative of the scale of leak tightness tested. © 2004. IUVSTA 1.08