solving process problems at the molecular flux level
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Solving Process Problems at the Molecular Flux Level
Working from pressure readings alone can mislead and misdirect a search forprocess problems, but reaching down a layer further into the molecularflux level can provide real solutions.
Every vacuum process hassome sort of specifiedparameters that must be
met if the process is to beeither initiated or carried outsuccessfully. Most
commonly, theseparameters state that acertain vacuum level beachieved or maintained,
and these levels are usuallydenoted in either totalpressure or in partialpressures of specific gases.
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Although parametricspecificity at this level isoften sufficient, there are all
too many cases whereprocess problems erupteven though the vacuumspecs appear to be met orexceeded. This result, then,often causes the vacuumpractitioner to question the
original specifications eventhough they had alreadyproved to be apparentlyworkable and practical.
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What's really missing in this
situation is the awarenessthat all technologies, andvacuum in particular, existin layers of detail and
complexity. In this case, wecan assumeoverdependence on thefundamentalvacuumrelationshipQ=SP.Getting to the root of the problem
Although the Q=SPrelationship is an extremelyimportant tool in
The process gas enters the chamber,but most of it goes directly into thepump, and this provides a wrongpressure measurement.
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understanding the behavior
of vacuum systems, it does,however, have a built-intrap that can interfere with adeeper understanding if we
let it. We have to assumean equilibrium condition anda uniformity of gas load,pressure, and identity ofgas species throughout asystem to make use of it.When process or design
problems require us toreach into a deeper level ofunderstanding, it becomesapparent that the
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assumptions applied to the
Q=SP relationships aren'tnecessarily true at thislevel.
For example, the idea of alarge number of gasmolecules bouncing aroundwithin a chamber in purelyrandom and mutuallyequidistant motion begins tobreak down. The Q=SP
relationship is a bit of anabstraction that is useful forcalculating andunderstanding overall
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performance, but it cannot
take into account the actualdetailed motion ofmolecules within thechamber. This level is
where many problems areto be found. Specificsources of gas, often in theform of molecular beams,and specific gas sinks needto beconsidered and
analyzed.A modern day example
If we look at acommonly encountered
The process gas enters the chamber,but most of it goes into the gauge,which renders an incorrect pressuremeasurement.
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problem such as a tiny
pinhole leak, we can easilyconstruct a mental pictureof an expanding beam ofmolecules entering the
chamber from the leak site.If we know the leak rate incommon terms, such astorr-L/sec, we can do aQ=SP calculation anddetermine the chamberpressure change produced
by the leak providing weknow the pumping speed. Ifwe know the change inchamber pressure, we can
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calculate the leak rate
instead. A beam of non-polar air gases such asnitrogen (N2 ) or oxygen (O2) will enter an empty
chamber, continuallyrebound from surfaces,reach an equilibriumconcentration, and bepumped away.
But, working at a lower
level, we can see that thebeam of chemically activegas could easily pass rightthrough a work volume or
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impact a work surface. This
would have the same effecton the process as a totalpressure many orders ofmagnitude higher. Process
problems could then beencountered even thoughthe pressure reading(s) wasstill within the approvedprocess parameters.hinking in molecules
Thinking in molecular flux
not only allows us toquantify the numbers ofmolecules acting andinteracting within the
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system but also begins to
allow us to build mentalpictures of the performanceof the system. Out of thisability to construct mental
pictures will, in time anduse, allow the vacuumpractitioner to grow thepriceless ability to "feel" asystem perform. Thispainfully acquired skill canhave many important
practical applications inboth troubleshooting adesign or process and in
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the original system design
or process development.Calculating units
In the Q=SP relationship,we make our calculations in
units that are convenient forthe abstract relationship butare difficult to think in. Gasloads (Q) in mass flowterms of torr-L/sec are veryhard to picture mentally, buta stated number of
molecules/sec is mucheasier to handle effectively.After all, pressure is reallythe number of molecules in
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a given volume to anyone
working in the molecularflow regime where thenormal concept of pressureis essentially meaningless
anyway. In manyprocesses, the number ofmolecules passing througha process volume orimpacting upon a processsurface is key tounderstanding that process.
Granted, the number ofmolecules/L/torr is a
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mindboggling number, but it
does give us something towork with. This can becalculated with the followingequation: (torr) x (3.54 x
1019 ) = molecules/L. Thiskind of calculation can beuseful when comparing thenumber of molecules in avolume and then adding ina particular beam-borne fluxof molecules from
something like a leak.
It is even more useful tothink (mental picture again)
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of the number of molecules
impacting a surface.Assuming that all theresidual molecules are N2 ,we can calculate the
number of collisions: (torr) x(3.95 x 1020 ) = number ofcollisions/cm2 /sec. This canbe compared to the numberof collisions/sec that wouldresult from an impactingbeam of molecules. The
same system can beapplied to the number ofmolecules passing througha process volume by merely
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calculating the surface area
of the volume.What's it good for?
Molecular flux concepts canbe applied in either a
qualitative or quantitativefashion. Qualitatively, wecan use the surface impactcalculations alreadydiscussed to determine theeffects.
For example, a freshlydeposited film of activemetal will react with theresidual gases as they
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impact on the surface, so it
becomes possible to makestoichiometric calculationsof the chemical changes onthe surface. That might well
be to determine how longthe fresh film can beexposed before aninsulating film results.
Before the quantitativecalculations become
important, though, we needto learn to think a system'spossible performancethrough using molecular flux
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thinking techniques to
determine whether therewould be any additionaleffects to the obviousresidual gas impacts.
We can then begin to thinkabout, and mentally picture,what might occur when aprocess gas is introducedinto a vacuum chamber.When a stream of gas is
allowed to flow from acontrolled leak valve intothe chamber, it will tend toform an expanding
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molecular beam that
traverses the chambervolume, and usually theprocess volume, inessentially a straight line.
The beam's diameter willincrease with distance andform a continuous cone withthe molecular populationgreatest at the cone'scenter in a condition calledcosine distribution. If a
pump is located directlyacross the chamber fromthe leak valve, the greatestportion of the gas will be
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directed into the pump's
throat with only the outlyingportion of the beam strikingthe chamber wall. If thegauge sensor head is
located 90o from the linebetween valve and pump, itwill only detect the gas thatdoesn't enter the pump as itscatters away from thechamber wall. This meansthat more gas is passing
through the chamber andthe process than would beexpected from the gauge'spressure reading. If the
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gauge and pump positions
are reversed, though, thegauge would detect aseemingly higher gas fluxthan would actually be the
case.
These two practicalexamples represent twocommon design mistakesthat lead to processproblems that aren't
immediately apparent whenthe process is monitored bypressure readings alone.
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Molecular flux thinking
allows us to take identifiedgas load sources andpicture, or calculate, theeffects of the resultant flux.
For example, a large O-ringon a door seal can easilyallow a diffusive flux fromthe O-ring's outgassing andpermeation of water vapor.This can result in the build-up of sorbed water vapor on
surfaces close to the O-ringthat can later be a problemfor a process if the surfacedesorption rate is too high.The outcome
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The number of examples
and possible uses for thistype of thinking and
analysis is endless, but
learning to use it on simpleand fairly standard
applications can help
master the technique andmake it a standard mental
reflex when considering a
design or trouble-shooting a
system. The Q=SP
relationship is a powerful
tool and should never be
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ignored, but any vacuum
practitioner should beconstantly ready to peel
back another layer in the
technology and thinkmolecular flux.
Phil Danielson
The Vacuum LabDowners Grove, Ill. 630-
434-1681
www.vacuumlab.com