Fundamentals Of Leak Detection - Leybold

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PrefaceFundamentalsof leak detectionEditor: Leybold GmbHCat. No. 199 79 VA.02Authors:Leybold GmbHBonner Str. 498 · D-50968 KölnT 49 (0) 221-347-0F 49 (0) 221-347-1250info@leybold.comwww.leybold.com19979 LV Umschlag HandbuchLD EN 426x297.indd 1BICOM 13619.13810.19979 VA.020.2.12.16mzsPrinted in Germany on chlorine-free bleached paper     Technical alterations reservedHans RottländerWalter UmrathGerhard Voss01.12.16 16:13

Fundamentals of Leak DetectionPrefaceLeybold, a member of the globally active industrialAtlas Copco Group of companies has developed into theworld market leader in the area of vacuum technology.In this leading position, we recognize that our customersaround the world count on Leybold to deliver technicalsuperiority and maximum value for all our products andservices.This brochure is meant to provide an easy to read overview covering the entire range of vacuum technologyand is independent of the current Leybold productportfolio. The presented product diagrams and dataare provided to help promote a more comprehensiveunderstanding of vacuum technology and are not offeredas an implied warranty.To us, partnership-like customer relationships are afundamental component of our corporate culture as wellas the continued investments we are making in researchand development for our next generation of innovativevacuum technology products.In the course of our over 165 year-long corporate history,Leybold developed a comprehensive understanding ofprocess and application know-how in the field of vacuumtechnology. Jointly with our partners and customers, weplan to continue our efforts to open up further markets,implement new ideas and develop pioneering products.Leybold GmbHCologne, December 20161

Fundamentals of Leak DetectionTable of ContentsIntroduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .41Types of leaks . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .42Leak rate, leak size, (gas) mass flow . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .52.1Helium standard leakrate . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 82.2Conversion formulas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 83Terms and definitions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .4Leak detection methods without leak detector . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 114.1Pressure rise test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .4.2Pressure drop test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 124.3Leak test using vacuum gauges which are sensitive to the type of gas . . . . . . . . . . . . . . . . . . . .4.4Bubble immersion test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 124.5Foam-spray test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 134.6Vacuum box check bubble . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .134.7Krypton 85 test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .134.8High-frequency vacuum test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 134.9Test with chemical reactions and dye penetration . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .5Leak detectors and how they work . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 155.1Halogen leak detectors . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .155.1.1Halogen diode principle . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .155.1.2Infrared principle (HLD 5000) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 155.2Leak detectors with mass spectrometers (MS) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 155.2.1The operating principle of a leak detector with mass spectrometer . . . . . . . . . . . . . . . . . . . . . .165.2.2Detection limit, background, gas storage in oil (gas ballast),floating zero-point suppression . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .175.2.3Calibrating leak detectors; calibration leaks . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .185.2.4Leak detectors with quadrupole mass spectrometer . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 215.2.5Leak detectors with 180 sector field mass spectrometer . . . . . . . . . . . . . . . . . . . . . . . . . . . 215.2.6Direct-flow and counter-flow leak detectors . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 225.2.7Counter-flow leak detector in partial-flow operation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .5.2.8Connection to vacuum systems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 245.2.9Time constant . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 266Limit values / specifications for the leak detector . . . . . . . . . . . . . . . . . . . . . . . . . . . . .277Leak detection techniques using vacuum leak detectors . . . . . . . . . . . . . . . . . . . . . . . . .277.1Vacuum method – spray technique (local leak test) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .277.2Positive pressure method – sniffer technique (local leak test) . . . . . . . . . . . . . . . . . . . . . . . . .297.3Envelope test (integral leak test) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 297.3.1Envelope test according to the positive pressure method . . . . . . . . . . . . . . . . . . . . . . . . . . . 297.3.2Envelope test according to the vacuum method . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 307.4"Bombing" test, "storage under pressure" . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 302911121324

Fundamentals of Leak Detection8Industrial leak test . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .9Formulary for leak detection technique . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 329.1Pressure of a gas and pressure units . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .9.1.1Partial pressure - total pressure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 329.2Gas quantity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 339.2.1Equation of state for ideal gases . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 339.3Gas flow . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 339.3.1(Gas) mass flow . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .339.4Pumping speed . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .349.5Leak rate . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 349.5.1Leak rate for pressure rise/pressure drop measurement . . . . . . . . . . . . . . . . . . . . . . . . . . . . 349.6Concentration of the test gas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .359.6.1Leak rate in case of decreased test gas concentration . . . . . . . . . . . . . . . . . . . . . . . . . . . .359.7"Temperature adjustment" (test temperature conversion) . . . . . . . . . . . . . . . . . . . . . . . . . . .359.8"Pressure adjustment" (test pressure conversion) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .369.9Change of gas type . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .369.10Conversion of liquid leak rate to gas leak rate . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 379.10.1 Matter constant c . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .9.11303238Partial-flow ratio . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 389.11.1 Response time . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 399.12Pump-down time . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .399.12.1 Required pumping speed . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .409.13Conversion of pressure units . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 419.14Conversion of gas flow/leak rate units . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 429.15Conversion of Anglo-American units . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 439.16Conversion of temperature units . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 449.17Temperature comparison . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .9.18Compilation of the most important gas laws (continuum theory) . . . . . . . . . . . . . . . . . . . . . . . . 46453

Fundamentals of Leak DetectionIntroduction1 Types of leaksIn addition to the actual vacuum systems and theirindividual components (vacuum vessel, lines, valves,measuring devices, etc.) there are numerous othersystems and products in the fields industry andresearch with high requirements regarding tightnessor so-called "hermetic sealing". These include,in particular, assemblies for the automotive andrefrigeration industry.The simplest definition for the term "leak" is:Generalized statements often made, such as“no detectable leaks” or “leak rate zero”, do notrepresent an adequate basis for acceptance testing.Every experienced engineer knows that properlyformulated acceptance specifications will indicatea certain leak rate under defined conditions.Which leak rate is acceptable is also determinedby the application itself.A leak is an "opening" in a (separating) wall or barrierthrough which solids, liquids or gases can undesirablyenter or exit.Depending on the type of material or joining fault,the following leak types are differentiated: Leaks in detachable connections:Flanges, ground mating surfaces, covers Leaks in permanent connections:Solder and welding seams, glued joints Leaks due to porosity:particularly following mechanical deformation (bending!)or thermal processing of polycrystallinematerials and cast components Thermal leaks:opening up at extreme temperature loading(heat/ cold), above all at solder joints Apparent (virtual) leaks:leaks: quantities of gas will be liberated from hollowsand cavities inside cast parts, blind holes and joints(also due to the evaporation of liquids). Indirect leaks:leaking supply lines in vacuum systems or furnaces(water, compressed air, brine) "Serial leaks":this is the leak at the end of several "spaces connectedin series", e.g. a leak in the oil-filled sectionof the oil pan in a rotary vane pump "One-way leaks":these will allow gas to pass in one direction but aretight in the other direction (very seldom)An area which is not gas-tight but which is not leakyin the sense that a defect is present would be the Permeationnaturally permeability of gas through materials suchas rubber hoses, elastomer seals, etc. (unless theseparts have become brittle and thus "leaky").4

Fundamentals of Leak Detection2 Leak rate, leak size(gas) mass flowNo vacuum device or system can ever be absolutelyvacuum-tight and it does not actually need to be. Thesimple essential is that the leak rate must be low enoughthat the required operating pressure, gas balance andultimate pressure in the vacuum container are not influenced.It follows that the requirements in regard to the gastightness of an apparatus are the more stringentthe lower the required pressure level is.In order to be able to register leaks quantitatively, theconcept of the "leak rate" with the symbol qL and theunit mbar l/s was introduced.A leak rate of qL 1 mbar·l/s is present when in anenclosed, evacuated vessel with a volume of 1 l the pressurerises by 1 mbar per second or, where there is positivepressure in the container, pressure drops by 1 mbar.The leak rate of a vessel indicates the amount of gas flowwhich escapes through the walls of the vessel. It must benoted, however, that the leak rate for a leak dependson the type of gas.If the gas temperature T and the molar mass M of a gasG is known, the gas mass flow can be calculated from theleak rate qL suing the equation of state for ideal gases viathe relationship(1) m/ t (qL·M)/(R·T)Unit: g/swithR 83.14 (mbar·l)/(mol·K)T Gas temperature in K M Molar mass in g/mol m Mass in g t Time span in sThe relationship (1) is used toa) to determine the mass flow m/ t at a known leak rate of qL(in this context, see example at 4.1)orb) to determine the leak rate qL at a known gas mass flow m/ t(see example below).Example for b):A refrigeration system using the refrigerant R134a( Freon) exhibits a refrigerant loss of 1 g per yearat 25 C.How large is the Freon leak rate qL(Freon)?With T (273 25) K 298 K and M(R134a) 102.03g/mol, the Freon leak rate is qL(Freon) 6.5·10-6 mbar·l/sin accordance with (1).For high-vacuum systems, the following rule of thumbapplies:qL(air) 10-6 mbar·l/s System is "very tight"qL(air) 10-5 mbar·l/s System is "sufficiently tight"qL(air) 10-4 mbar·l/s System is "leaky"A leak can in fact be compensated by a vacuum pumpof sufficient capacity since the following applies to thereachable ultimate (operating) pressure pult:(2) pult qL/SeffwithqL Leak rate in mbar l/sSeff Effective pumping speed of the vacuum pumpat the vacuum vessel in l/sIf Seff is increased sufficiently, it is therefore alwayspossible to reach a specified ultimate (operating)pressure pult independent of the leak rate qL.In practice, however, a desired increase of Seff maynot be realizable due to economic and design reasons(high investment costs, high space requirement).If the desired ultimate pressure is not reached ina vacuum system, there are usually two causes for this:1. the presence of leaksand/or2. the gas liberation from the vessel walls andseal outgassing.In order to differentiate between the two causes, a partialpressure analysis with a mass spectrometer or the timerelated pressure rise test may be used. Since it is onlypossible to determine the existence of a leak and not itsposition in the system when using the pressure rise test, itis recommended to use a helium leak detector with whichthe leaks may also be localized significantly faster.5

Fundamentals of Leak DetectionIn order to achieve an overview of the correlation betweenthe geometric size of the hole and the associated leakrate it is possible to operate on the basis of the following,rough estimate:A circular hole with a diameter D 1 cm in the wall ofa vacuum vessel is closed with a valve. Atmosphericpressure (p 1013 mbar) prevails outside, a vacuuminside. When the valve is opened, the air flowsat the speed of sound (vS 330 m/s) through theopening cross section of A p·(D2/4) – 0.79 cm2 into thevessel. The air quantity flowing into the vessel amounts toqL(air) p·vS·A – 2.6·104 mbar·l/s.If all other conditions are kept identical and helium isallowed to flow into the hole at its speed of sound of970 m/s, then the helium leak rateqL (helium) is – 7.7·104 mbar·l/s, so the leak rate issignificantly higher.This greater "sensitivity" for helium is used in leakdetection and has resulted in the development and massproduction of highly sensitive helium-based leak detectors(see Section 5.2).Shown in Fig. 1 is the correlation between the hole sizeand leak rate for air, with the approximate value of qL (air) 104 mbar·l/s for the "1 cm hole".The table shows that when the hole diameter D is reducedto 1 mm 0.001 mm ( reduction of D by the factor10000) the leak rate will amount to 1.0·10-4 mbar·l/s,a value which in vacuum technology already representsa major leak (see the rule of thumb above).A leak rate of 1.0·10-12 mbar·l/s corresponds to holediameter of 1 angstrom (Å);this is the lower detection limit for modern helium leakdetectors. Since the grid constants for many solids amountto several Å and the diameter of smaller molecules (H2,He) are about 1 Å, inherent permeation through solids canbe registered metrologically using helium leak detectors.This has led to the development of calibrated test leakswith very small leak rates. This is a measurable "lack oftightness" but not a "leak" in the sense of being a defectin the material or joint.Correlation between hole diameter and leak rate, estimation for air p 1013 mbar, hole diameter d 1 cmGas speed speed of sound in air 330ms32m 1 · π · cm2 26 · 103 cm 26Volume/second: 330 s ·ss44 mbar ·4 mbar ·10Quantity/second: 1013 mbar · 26 s 2,6 · 10ssDiameter10-2-310-410-510m m m m 1,0 cm1,0 mm0,1 mm0,01 mm10 m 1,0 µm-6-710-810-910-1010m m m m 0,1 µm0,01 µm1,0 nm1,0 AngströmLeak rate in mbar ·s410210010( 1)-21010-4-610-810-1010-1210Fig. 1: Correlation between hole diameter and leak rate, estimation for air6(Detection limit of helium leak detectors)

Fundamentals of Leak DetectionEstimates or measurements of the sizes of atoms,molecules, viruses, bacteria, etc. have often given rise toeveryday terms such as “watertight” or “bacteria-tight”(see Table 1).qL (mbar · l/s)Concept / criterionCommentRelevant particle sizeWater-tight*)Droplets 10–2Vapor-tight"Sweating" 10–3Bacteria-tight*)(cocci)(rod-shaped) 10–4Oil-tight 10–5Virus-tight*)(vaccines e. g. pox)(smallest viruses, bacteriophages)(viroids, RNA) 10–6 10–8 10–10Gas-tight 10–7"Absolutely tight" 10–10Technical 1 µm 0.5 - 1 µm, 2 - 10 µm long*) As opposed to vapor, it is necessary to differentiate between hydrophilic and hydrophobic solids.This also applies to bacteria and viruses since they are transported primarily in solutions.Table 1: Correlation between tightness criteria and leak rates qLCompiled in Fig. 2 are the nature and detectionlimits of frequently used leak detection methods.Helium leak detector PHOENIXL300 dryPressure rise e testPressure drop test10-9 10-10 10-11 10-12 mbar ·· s-1Positive pressure methodHe leak detector (sniffer method)Vacuum methodHelium leak detector PHOENIXL300, PHOENIXL300 modulFig. 2: Nature and detection limits of frequently used leak detection methods7

Fundamentals of Leak Detection2.1 Helium standard leakrateRequired for unequivocal definition of a leak are thepressures prevailing on either side of the (vessel) walland the nature of the medium passing through that wall(viscosity, molar mass). For the case where the test iscarried out with helium4 at a pressure difference of1 bar from the atmosphere pressure (external) tothe vacuum(p 1 mbar, internal), which is frequently found inpractice, the designation "helium standard leak rate"has been introduced in the standard DIN EN 1330-8.In order to indicate the rejection rate for a test usinghelium under standard helium conditions it is necessaryfirst to convert the real test conditions of use to heliumstandard conditions (see 2.2). Some examples of suchconversions are shown in Fig. 3.Quantity of substance per time unit through holeLeakStandard helium conditions:p1 1 bar, p2 1 mbar ( p 1 bar)Test gas Helium Known leaks:Leaking quantity of substance:Standard helium leak rate:Water faucet drippingmg34 s Water0,17 6,45 mbars · Airmbar ·He Stds4 mm ø, 1 Hz, p 4 barmbar ·AirsHair lies on seal10 –2Bicycle tube in water(bubble test)2 mm ø, 1 Hz, p 0,1 bar4,19 · 10–3Ncm 3mbar ·Air 4,24 · 10 –3ssCar tire looses air25 l, 6 Mo: 1,8 -- 1,6 bar3,18 · 10–4mbar ·Airs2.2 Conversion formulasRegarding the conversion of pressure and gas type(viscosity, molar mass), it must be noted that differentformulas apply to laminar viscous and molecularflow. The boundary between these areas is very difficultto determine. As a guideline, the following can beassumed: at leak ratesq L 10–4 mbar·l/slaminar viscous flowand at leak ratesq L 10–6 mbar·l/smbar ·He Stds0,9 · 10 –21,88 · 10 –24,3 · 10 –5mbar ·He Stdsmbar ·He StdsFig. 3:Examples for theconversion of leak ratesto helium standard leakratesIn the intermediate range the manufacturer (who is liableunder the guarantee terms) must assume values on thesafe side.The equations are listed in Table 2.Here indices "I" and "II" refer to the one or the other pressureratio and indices "1" and "2" reference the inside andoutside of the leak point, respectively. For a sensible useof the formulas, the pressure p1 must always be the higherpressure ( p1 p2 ).molecular flowFlowLaminar viscousMolecularPressureq I · ( p 1 2 p 2 2 ) II q II · ( p 1 2 p 2 2 ) Iq I ·(p 1 p 2 ) II q II ·(p 1 p 2 ) IGas typeq G a s A · h G a s A q G a s B · h G a sB q G a sA ·(M G a sA ) 1/2q G a sB ·(M G a sB ) 1/2Table 2:Formulae for the conversion of pressure and gas type, p pressure, q gas flow (leak rate), h viscosity, M molar mass8

Fundamentals of Leak Detection3 Terms and definitionsWhen searching for leaks one will generally have todistinguish between two tasks:1. locating leaks and2. measuring the leak rateIn addition, we distinguish, based on the direction of flowfor the fluid, between thea. vacuum method(sometimes known as an "outside-in leak"), where thedirection of flow is into the test object; the pressure insidethe test object is less than ambient pressureand theb. positive pressure method(often referred to as the “inside-out leak”), where theflow takes place from inside the test object outward; thepressure inside the test object is higher than the ambientpressure.The test objects should wherever possible be examined ina configuration corresponding to their later application, i.e.components for vacuum applications using the vacuummethod and using the positive pressure method for partswhich will be pressurized on the inside.When measuring leak rates, we differentiate betweenregisteringa. individual leaks (local measurement), Fig. 4band 4d,and registeringb. the total of all leaks in the test object (integralmeasurement) Fig. 4a and 4c.The smallest leak rate which is no longer tolerable inaccordance with the acceptance specifications is knownas the rejection rate. Its calculation is based on thecondition that the test object may not fail during itsplanned utilization period due to faults caused by leaks,and this to a certain degree of certainty.situation in regard to the pressures inside and outside thetest object and the type of gas (or liquid) being handled.Where a vacuum is present inside the test object (p 1 mbar),atmospheric pressure outside, and helium4 is used atthe test gas, one refers to standard helium conditions.Standard helium conditions are always present duringhelium leak detection for a vacuum system when thesystem is connected to a leak detector, if the system ispumped down to p less than 1 mbar and if it is sprayedwith helium4 (spray technique) (see Fig. 4b).If the test object is evacuated solely by the leak detector,then one would say that the leak detector is operating inthe direct-flow mode of the leak detector (LD).If the test object is itself a complete vacuum system withits own vacuum pump and if the leak detector is operatedin parallel to the system’s pumps, then one refers topartial-flow mode of the leak detector. One also refersto partial-flow mode when a separate auxiliary pump isused parallel to the leak detector.When using the positive pressure method it is sometimeseither impractical or in fact impossible to measure theleakage rate directly while it could certainly be sensedin an envelope which encloses the test specimen. Themeasurement can be made by connecting that envelopeto the leak detector or by accumulation ( increasingthe concentration) of the test gas inside the envelope(see Fig. 4c). The bombing test is a special version ofthe accumulation test (see 7.4).In the so-called sniffer technique, another variationof the of the positive pressure technique, the (test) gasissuing from leaks is collected (extracted) by a specialapparatus and fed to the leak detector (see Fig. 4d).This procedure can be carried out using either heliumor refrigerants or SF6 as the test gas.Often it is not the leak rate for the test object undernormal operating conditions which is determined, butrather the throughput rate of a test gas under similarconditions. The achieved measuring values have to beconverted to correspond to the actual application9

Fundamentals of Leak Detectiona:c:b:d:Fig. 4:Usage options for a vacuum leak detector based on the vacuum method (a, b) and based on the positive pressure method (c, d)10Vacuum methodPositive pressure method Vacuum inside specimen Pressurized test gas inside specimena: Enclosure test (integral leak detection)c: Enclosure test (integral leak detection)b: Spray technique (local leak detection)d: Sniffer technique (local leak detection)

Fundamentals of Leak Detection4 Leak detection methods withoutleak detectorThe most sensible differentiation between the test methodsused is the differentiation as to whether or not special leakdetection equipment is used.In the simplest case a leak can be determined qualitativelyand, when using certain test techniques, quantitatively as well(this being the leak rate) without the assistance of a specialleak detector.For example, the quantity of water dripping from aleaking water faucet over a certain period of time canbe determined by collecting the water with a measuringvessel. In this case, however, one would hardly refer tothis as a leak detector.In those cases where the leak rate can be determinedduring leak detection without using a leak detector, thisleak rate will often be converted to the helium standardleak rate (see 2.1). The helium standard leak rate is oftenrequired for issuing acceptance certificates but can alsobe of service when comparing leak rate values determinedvia helium leak detector devices.constant, then a leak is present, assuming that the waitingperiod between the two pressure rise measurements waslong enough. The appropriate length of the waiting perioddepends on the nature and size of the device. If the timefor the pressure rise Δp increases, this effect is most likelycaused by a reduced gas liberation on the inside of theapparatus.One may also attempt to differentiate between leaks andcontamination by interpreting the curve depicting the risein pressure ( pressure as a function of time).Plotted on a graph with linear scales, the curve for the risein pressure must be a straight line where a leak is present,even at higher pressures.If the pressure rise is due to gas being liberated from thewalls, then the pressure rise will gradually taper off andwill approach a final and stable value. In most cases bothphenomena will occur simultaneously so that separating thetwo causes is often difficult if not impossible.These r

Fundamentals of Leak Detection In order to achieve an overview of the correlation between the geometric size of the hole and the associated leak rate it is possible to operate on the basis of the following, rough estimate: A circular hole with a diameter D 1 cm in the wa

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