referring to fig1 a sample collection system 10 includes a saturator 12 into which an aerosol 14 ( the ambient air ) is first drawn at a sampling flow rate of 200 l / min and mixed with steam 16 injected radially through a porous walled tube 18 of the saturator 12 to achieve saturation of the aerosol . an ambient temperature and the steam flow rate of 6 l / min ( or less ) is generally adequate to saturate the aerosol . to insure mixing of the ambient air and the steam , the aerosol / steam mixture is delivered to a saturator chamber which consists of a tube 18 approximately 29 cm long and 2 . 7 cm in diameter to provide a residence time of about 1 ms which should guarantee saturation of the sampled air . the tube 18 is kept at a temperature of 35c . with a heater 20 controlled by a control circuit 22 . subsequently , the saturated air from the saturator 12 is drawn through a pair of condensers 24 that allow the fine particles delivered into the saturator to grow to a diameter in the range of 0 . 7 - 10 μm . the sub - system including the saturator 12 and the condenser 24 grows the particles by condensing water on them ( thus , creating large droplets ). the condensers 24 consist of two coaxial glass tubes 28 , 30 , having approximate dimensions 97 cm in length and diameters of 3 . 4 cm . and incorporate an exit chamber configured to remove excess water lost to the walls .. the design and dimensions are directed to a system which provides for a residence time in the condensers 24 of about 0 . 6 seconds for a flow of 200 l / min . across the condenser 24 and maximize the efficiency of the supersaturation process . the condenser 28 , 30 are maintained at temperature 0 . 5 ° c . with a refrigerant cooler 32 . the particle growth through the vapor condensation is the basic principle used in the saturator / condenser sub - system . the degree of supersaturation required depends on particle size which for hydrophobic particles & lt ; 0 . 1 μm in diameter , is given by the kelvin equation : supersaturation = p p s = exp  ( 4   σ   m ρ   r   t   d p ) ( 3 ) p s is the saturation vapor pressure at a given temperature ; m , ρ and σ are the molecular weight , density , and surface tension of the condensing liquid ; d p is the critical particle diameter , also called kelvin diameter . the kelvin diameter defines the critical equilibrium diameter at which a pure droplet is stable at the critical saturation ratio needed for equilibrium . at the critical saturation ratio , particles larger than the critical diameter will grow by condensation , while smaller particles will evaporate . conversely , smaller critical diameters will be achieved by applying higher saturation ratios , i . e ., resulting in particle growth by condensation , while at lower saturation ratios , the particle will evaporate . equation 3 is only valid for a pure liquid surface . when dissolved salts ( e . g . ammonium sulfate and nitrate in atmospheric aerosols ) are present , the equilibrium vapor pressure above the droplet surface is reduced . this reduces the required saturation ratio for condensational growth to occur compared to a pure liquid . adding the correction for a dissolved salt , and after particles have grown substantially , equation 2 now becomes ( hinds , w . c . aerosol technology : properties , behavior , and measurement of airborne particles , 1982 , john wiley & amp ; sons , new york .) s = p p s = ( 1 + 6  i   m   m v m s  ρπ   d 3 ) - 1  exp  ( 4  γ   m v ρ   rtd ) ( 3 ) where m and m s are the mass and molecular weight of the salt , and i is the number of ions per salt molecule . a supersaturation of 1 . 24 is required to condense water on 0 . 01 μm particles . the ultimate size to which particles grow depends on the time of exposure to the saturated vapor . as the dynamics of condensation dictate that small particles grow rapidly and large particles grow slowly , the resulting size distribution becomes quite nearly unimodal . it is possible to grow particles , in a near uniform manner to a size of 12 μm . enlarged particles ( i . e ., now droplets ) of this size may be easily separated at a low pressure drop with the virtual impactor 26 having a cutpoint of 0 . 7 μm ( aerodynamic particle diameter ). as the particles tend to are grow to a uniform size , losses in the device tend to be independent of the original size . the target supersaturation ratio to be achieved is on the order of 3 . 0 to insure activation of all particles . the choice of parameters such as the temperature of the saturator 12 and condenser 24 is generally determined empirically . from the kelvin equation ( 3 ), supersaturation 10 is adequate for activating a water droplet as small as 0 . 003 μm ( m = 18 g / mole , σ = 72 dyn / cm , ρ = 1 g / cm 3 ). nevertheless , a supersaturation value as high as 300 % may be chosen to account for excess moisture is required to account for condensation of water vapor occurring onto the cold walls of the condenser and the complexity of condensational growth for real polydisperse , multimodal , multicomponent aerosol . for droplets smaller than the mean free path of the gas ( about 0 . 066 μm for air ), the rate of growth in this region is determined by random molecular collisions , given by the kinetic theory of gases as ( hinds , w . c . ( 1982 ) aerosol technology : properties , behavior , and measurement of airborne particles , john wiley & amp ; sons , new york .)  d p  t = 2   m v  ( p ∞ - p d ) ρ p  n a  2  π   m v  k   t ( 4 ) where p d is the vapor pressure at the droplet surface , given by the equation 3 , p oo is the vapor pressure away from the droplet , n α is avagadro &# 39 ; s number , m v is the mass of a vapor molecule , and k is boltzmann &# 39 ; s constant . the growth rate for particles smaller than the mean free path of the gas is , therefore , independent of the particle size . for particles larger than the mean free path of the gas , the rate of growth is governed by the rate of diffusion of vapor to the particle surface given by ( hinds , w . c . ( 1982 ) aerosol technology : properties , behavior , and measurement of airborne particles , john wiley & amp ; sons , new york .)  d p  t = 4  d v  m v r   ρ p  d p  ( p ∞ t ∞ - p d t d ) ( 5 ) where d v is the diffusion coefficient for the condensing vapor . thus , the growth rate for particles larger than the mean free path of the gas is inversely proportional to the particle size . this will cause all particles larger than the kelvin diameter to approach an equilibrium size , determined by the time and amount of vapor available for condensation . the two equations for growth can be combined into a single expression by applying the fuchs and sutugin ( fuchs , n . a . and sutugin , a . g . ( 1970 ) highly dispersed aerosols , ann arbor science publishers , ann arbor , mich .) correction factor , ƒ ( kn ), to equation 5  d p  t = 4  d v  m v r   ρ p  d p  ( p ∞ t ∞ - p d t d )  f  ( λ , d p ) ( 6 ) f  ( λ , d p ) = d p + 2  λ d p + 3 . 42  λ + 5 . 33  ( λ 2 d p ) ( 7 ) where λ is the mean free path of the vapor or gas molecules . since vapor is condensing onto the droplet surface , an additional correction must be applied to account for heating of the droplet due to the latent heat of condensation and the heat lost by conduction to the cooler surrounding air . the resulting temperature correction is given by ( ahn , k .- h . and liu , b . y . h . ( 1990 ) particle activation and droplet growth processes in condensation nucleus counter - i . background . j . aerosol sci ., 21 , 249 - 261 .) t d - t ∞ = d v  m v  h r   k v  ( p d t d - p ∞ t ∞ )  f  ( λ v , d p ) f  ( λ g , d p ) ( 8 ) where h is the latent heat of condensation , and k v is the thermal conductivity of the condensing vapor . to determine the time required for condensational growth , equations 6 - 8 must be solved iteratively and integrated over the initial to final particle sizes . during growth , the saturation ratio will be decreasing due to loss of vapor by condensation to the walls of the condenser as well as to the particles . to a lesser extent , the saturation ratio will also be lowered due to the effects of latent heat production on the particles . these factors make theoretical growth rate calculations suitable only as a guideline for experimental characterization . for growth to occur on particles as small as 0 . 01 μm in diameter , equation 2 predicts a critical saturation ratio of 1 . 24 . the maximum time required for condensational growth may then be estimated by assuming a saturation ratio of 1 . 25 . since dissolved salts will only serve to aid condensational growth , the particles are assumed to be insoluble and equation 3 may , therefore , be ignored . from equation 4 , approximately 0 . 1 ms is needed for particles to grow from 0 . 01 μm to 0 . 1 μm in diameter , when growth by diffusion of water vapor becomes dominant . equation 5 predicts an additional 30 ms is required for growth from 0 . 1 μm to 5 μm diameter . after applying the correction factors in equations 6 - 8 , the estimated time for particle growth from 0 . 01 μm to 5 μm in diameter is 33 ms , i . e ., much less than the residence time of aerosol in the condensors . after passing through the condenser 24 , the aerosol is drawn through a virtual impactor 26 with a 0 . 7 μm cutpoint . the physical principle of operation of a virtual impactor is similar to that of an inertial impactor , as both methods use particle inertia to separate particles from gases . a jet of particle - laden air is deflected abruptly by an impaction plate , which causes an abrupt deflection of the air streamlines . particles larger than a critical size ( the so - called cutpoint of the impactor ) cross the air streamlines and , in the case of an inertial impactor , are collected on the impaction plate , while particles smaller than the critical size follow the deflected streamlines . the main difference between an inertial and a virtual impactor is that in the latter , particles are directed into a collection nozzle rather than onto a collection plate . to separate larger particles continuously from the collection probe , a fraction of the total flow , referred to as the minor flow ( typically 10 %- 20 % of the total flow ), is allowed to pass through the probe , leaving particles larger than the cutpoint contained in a small fraction of the gas . particles larger than the cutpoint from the collection probe , a fraction of the total flow , referred to as the minor flow ( typically 10 %- 20 % of the total flow ), is allowed to pass through the probe , leaving particles larger than the cutpoint contained in a small fraction of the gas . particles larger than the cutpoint are , therefore , concentrated into the minor flow , nominally by a factor of the inverse of the minor flow ratio ( i . e ., particles are concentrated 20 - fold for a minor flow of 5 l . min − 1 and total flow of 100 l . min 31 1 ). the impactors 26 have single circular acceleration nozzles with diameters of 3 mm and tapered circular collection nozzles 4 . 5 mm in diameter . acceleration and collection nozzle spacing is 4 mm , and other critical dimensions include inlet and exit chamber diameters ( 31 mm and 9 mm , respectively ), and the impactor body diameter , 45 mm . the impactors 26 operate at a minor flow ratio of approximately 10 l / min with major flow of 160 l / min . although operation of virtual impactors at such low minor flow ratios often implies excessive particle losses within the impactor , these losses are typically associated with particles close to the cutpoint . as particles passing through the saturator / condenser unit are expected to grow to sizes two - to - three times larger in diameter than the cutpoint of the impactor , much smaller losses would occur . even at very low minor - to - total flow ratios ( 2 - 5 %), particle losses become minimum at sizes larger than the cutpoint . a major advantage of the condensational growth method employed in the system of the present invention is that particles grow to approximately the same size , thus particle losses , if any , are generally independent of the initial particle size . tests of the sample collection system 10 , also referred herein to as the particle concentrator , have proven the ability to activate and grow by condensation , particles smaller than 0 . 1 μm in diameter . suspensions of 0 . 084 , 0 . 209 , 0 . 495 , 0 . 930 , 1 . 881 , 2 . 977 , and 5 . 895 μm diameter psl particles were prepared by diluting a 50 - μl aliquot of each stock solution to 100 ml with high - purity water . these suspensions were nebulized with a commercial nebulizer 34 ( micro - mist model 4650d , devilbis , somerset , pa .) operated at 200 kpa to create the test aerosol . hydrophobic psl particles have been shown ( sioutas , c . and koutrakis , p . ( 1996 ) inertial separation of ultrafine particles using a condensational growth / virtual impaction system . aerosol sci . technol ., 25 , 424 - 436 .) to be grown by condensation of water vapor to the same extent as hygroscopic atmospheric aerosol particles such as ammonium sulfate and potassium nitrate . the aerosol was first mixed with dry air to form dry test particles , then mixed with filtered room air to make up the total flow needed prior to sampling . following efficiency tests made with fluorescent particles , the liquid samples were vacuum dried overnight at room temperature . the fluorescein dye on the reference filters and dried samples was extracted with 10 - ml aliquots of ethyl acetate . to determine losses within individual components of the system , each component was washed with ethyl acetate and 2 - propanol because ethyl acetate alone is not miscible with water . the washes were collected , dried , and re - dissolved with 10 ml of ethyl acetate . the fluorescence intensity of each sample was determined with a spectrofluorophotometer ( model rf - 5301pc , shimadzu corp ., columbia , md .) using an excitation wavelength of 440 nm and integrating the emission intensity from 450 to 600 mn . the collection efficiency is calculated as eff = f s / q s f r / q r ( 10 ) where f is the integrated fluorescence intensity , q is the flow rate , and the subscripts s and r refer to the downstream sample and upstream reference filters , respectively . the size distributions for the test psl particles were measured before and after condensational growth using a micro - orifice impactor to segregate the aerosol into nine size ranges from 0 . 01 to 15 μm aerodynamic diameter . the particle concentrations were kept as low as practical to reduce agglomeration , while still being detectable in a 30 - min sample , but the effects of agglomeration are still evident for particles & lt ; 0 . 5 μm in diameter . fig4 shows fluorescence vs . particle size spectra for 0 . 084 μm particles before and after condensational growth . the relatively high concentration for 0 . 084 μm particles results in multiple particles becoming entrained in each nebulizer droplet , which increases the mean dry particle diameter to about 0 . 3 μm . this agglomeration effect is greatly reduced for 0 . 209 μm diameter particles and negligible for larger particles . following condensational growth , the mean size of the grown droplets increases to about 4 μm , with 65 % of the droplets & gt ; 3 μm in diameter . the efficiencies for the virtual and real impactors were measured using dry psl particles with no condensational growth . the transmission efficiency versus particle size curve for the virtual impactor ( fig5 ) for dry particles ranging in size from 0 . 1 to 6 μm indicates a 50 % cutpoint of about 1 . 8 μm in diameter . this corresponds to a stokes number of 1 . 4 . the entire system is made from glass , teflon , and nylon , to prevent contamination of the collected slurry samples . the system is mounted vertically to prevent losses by particle sedimentation . the aerosol concentrator system 10 can be mated with a perkin elmer simaa 6000 graphite furnace instrument 44 . as a compromise between high temporal resolution and collection of adequate sample , target sampling times of about 10 min were investigated . analysis times for solid materials were typically of the order of 30 s for ashing and 3 or 4 seconds for atomization . one or two additional firings may be required to clean out the graphite furnace . thus , the sample throughput rate is expected to be controlled by the sampling time rather than by the analysis time . the principles of the gfaa based multi - element analysis is well known to those skilled in the art , and therefore , are not intended to be discussed herein in detail . in the system of the present invention , particles ( e . g ., droplets ) associated with the 10 l / min aerosol flow from the concentrator can be delivered directly into the furnace 44 with a single , circular jet , real or inertial impactor 46 , as best shown in fig2 . the largest impactor jet diameter which can be inserted into the graphite furnace port is 1 . 5 mm . at a flow rate of 10 l / min , it is calculated that the cutpoint of the impactor 46 is about 0 . 7 μm , i . e ., far smaller than needed to collect the supermicrometer - size droplets emerging from the concentrator . the impactor 46 ( best shown in fig1 ) consists of a body 48 with internal diameter smoothly tapering from about 9 mm at the inlet 50 to 1 mm at the outlet 52 over a distance of the order of about 10 cm . both the virtual impactor 26 and the impactor 46 can be machined from high - purity aluminum . the impactor nozzle is machined from high - purity tantalum or like material . assuming an initial aerosol concentration at the inlet 54 of the concentrator system 10 of 50 μg m 31 3 , initial particle size of 0 . 5 μm , and final droplet size of 10 μm , then about 200 μl of water associated with the droplets enter the graphite furnace 48 during a 10 - minute sampling period . only about 3 ml of water is associated with the droplets if all of the original aerosol mass were contained in 0 . 2 - μm particles . either of these amounts of water can easily be controlled by changing the condenser temperature and by heating the furnace during collection . the impaction probe may be heated slightly to prevent condensation of the 2 ml of water vapor associated with the ( saturated ) 100 l of air ( i . e ., 10 l / min for 10 min ) sampled during this period . to aspirate the aerosol into the graphite furnace 44 , optical - quality quartz end caps are installed to seal the furnace 44 . this can be accomplished without substantial reduction in beam intensity . the pressure drop required by the impactor 46 is about 0 . 05 atm ( i . e ., 5 cm of hg ) and is achieved by withdrawing air from a port in the edge of the quartz endcaps with a small leak - free diaphragm pump . the flow rate is monitored with a precision flow meter mounted at the exit of the pump . with large droplets , the impactor nozzle 52 does not need to be inserted much past the wall of the furnace tube , although , optimum positioning is established experimentally , by aspirating fluorescent monodisperse test particles of the proper size and measuring the collection efficiency using the method described in above paragraphs . it is envisioned that an adequate seal can be achieved ( although none may be needed ) between the impaction probe and the graphite furnace port by friction . the impaction probe may be attached to a mechanical retractor to remove it before firing the furnace 44 . this will permit additions of standards and matrix modifiers using the systems auto sampler and will prevent clogging and damage to the impaction probe . a switching valve 98 is used to divert the sample flow during analysis periods . the retracting impactor nozzle can be plumbed to the concentrator outlet 56 with a piece of flexible tubing using teflon or like material , such that the length of tubing is straight and vertical during sampling . the concentrations of respirable aerosol particles typically varies between 20 and about 50 μg m − 3 . at the target sampling rate and time ( 200 l / min for 10 min ), the total aerosol mass delivered to the furnace 44 at the higher concentration is only 100 μg , i . e ., an amount well below the 1 or 2 mg introduced in slurry analyses described above . under these conditions , memory effects ( associated with heating regimes of the furnace 44 ) of the gfaa are likely to be less of a problem than experienced in other solids analyses . clearly , larger mass loadings might be tolerated , provided they are delivered by the concentrator system 10 of the present invention . should memory effects be important , experimentation with matrix modifiers , e . g ., chlorides , which may be introduced into the furnace 44 with the autosampler and fired between analyses can be accomplished . the conditions of the graphite furnace 44 are dictated by the elements to be analyzed . the atomization temperature must be high enough so that even the least volatile element is atomized , however ashing temperature must be low enough that most of the volatile elements are not volatilized prior to analysis . recommended furnace conditions for individual analysis of a wide range of elements are shown in table 1 . the data suggest that ag , cd , pb , and zn may be determined simultaneously , or similarly , as , sb , se , and mn ; and al , co , cr , cu , fe , ni , and s . however , fe , for example , is so abundant in aerosol particles that the determination may be made at conditions far from the optimum . the choice of elements that can be determined simultaneously depends on the atmosphere to be sampled . instrument calibration for solid sample analyses has been done by running standard solutions , in this case , multielement standards ; and with standard addition techniques in which the sample is spiked with a known amount of the element ( s ) to be determined . referring to fig2 the set - up for testing of the overall system 58 is schematically presented . test aerosol is generated by nebulizing a suspension of monodisperse florescent polystyrene latex ( psl ) particles ( polysciences , inc ., warrington , pa .) with the commercial nebulizer 34 ( micro - mist model 4650d , devilbis , somerset , pa .). suspensions of 0 . 084 , 0 . 209 , 0 . 495 , 0 . 930 , 1 . 881 , 2 . 977 , and 5 . 895 μm diameter psl are prepared by diluting a 50 μl aliquot of each stock solution to 100 ml with 18 . 2 mω water . hydrophobic psl particles are known to be grown by condensational growth to the same extent as hygroscopic atmospheric aerosol particles such as ammonium sulfate and potassium nitrate . the aerosol is initially mixed in a chamber 60 to form dry test particles , then mixed in the mixing chamber 64 with room air 66 to make up the total flow 68 prior to entering the saturator / condenser / virtual impactor system 10 . the airflow 68 is split into 3 equal flows 70 , 72 , 74 of 85 l / min for the reference filter 76 and two condensational growth columns 78 , 80 . the reference filter 76 is a 47 - mm diameter teflon filter ( teflo , 2 μm pore , gelman laboratory , ann arbor , mich .) which provides a measure of the particle concentration prior to entering the system 10 . steam is generated by steam generator 82 by delivering 18 . 2 mω water with a multichannel peristaltic pump 84 ( minipuls 3 , gilson , inc ., middleton , wis .) to heated flasks . the steam 86 is then injected coaxially into the airstream through a coarse - fritted glass collar in each steam injector 88 , 90 , which represents a cylindrical glass tube 27 mm in diameter and 450 mm in length . turbulence within the steam injector 88 , 90 causes rapid mixing of the steam 86 and air which becomes saturated at approximately 35 ° c . the saturated air then enters the condensers 24 , which include cylindrical glass tubes approximately 33 mm in diameter and 970 mm in length , which are maintained at 0 . 5 ° c . by a recirculating chiller 92 ( polystat model 12910 - 10 , cole - parmer instrument co ., vernon hills , ill .). a water trap built into the bottom of each condenser collects and removes water that condenses on the walls . within the condensers 24 , the air is rapidly cooled to about 25 ° c ., giving a maximum theoretical saturation ratio of 1 . 8 . vapor loss due to condensation on the walls of the condenser and onto the particles reduces the actual saturation ratio to some extent . a saturation ratio of only 1 . 25 is needed to grow hydrophobic particles as small as 0 . 01 μm by condensational growth . the grown particles in the form of droplets , are concentrated using a 2 - nozzle glass virtual impactor 26 operating at a major flow of 160 l / min and a minor flow of 10 l / min . the 3 mm diameter acceleration nozzle and 4 . 5 mm diameter collection nozzle produce a 50 % cutpoint of approximately 2 μm at a pressure drop of 24 kpa . a glass single - jet real impactor 46 with a 1 . 9 mm diameter jet and 50 % cutpoint of 1 μm is used to separate the concentrated droplets from the airflow . the droplets accumulate in the bottom of the real impactor 46 in a liquid slurry at about 0 . 2 ml / min . following a 30 minute collection period , the slurry is hydraulically delivered to an x - y fraction collector 94 ( foxy , isco , lincoln , nebr .) and stored in glass sample vials for subsequent analysis . it is also possible and is contemplated in the scope of the present invention , to deliver the liquid slurry directly into the graphite furnace 44 for on - line analysis . extensive control and automation of the collection process of the present invention is accomplished using a computer - controller datalogger ( model cr23x , campbell scientific , inc ., logan , utah ). volumetric air flow rates are precisely maintained using control valves and mass flow meters corrected to ambient temperature and pressure . the steam injection rate is determined by the datalogger based on ambient temperature and relative humidity and the desired saturation ratio , with the peristaltic pump speed automatically updated every 10 s . at the end of a sample collection period , ball valves are closed to isolate the real impactor 46 , which is then pressurized using compressed air to expel the accumulated slurry . the fraction collector 94 automatically advances to the next sample collection vial after the slurry is dispensed , and the next sample collection begins . following efficiency tests made with fluorescent particles , the liquid samples were vacuum dried overnight at room temperature . the fluorescein dye on the reference filters 76 and dried samples may be extracted with 10 ml aliquots of ethyl acetate . to determine losses within individual components of the system , each component was washed with ethyl acetate and 2 - propanol , with the washes collected , dried , and dissolved with 10 ml ethyl acetate . the fluorescence intensity of each sample may be determined with a spectrofluorophotometer ( model rf - 5301pc , shimadzu corporation , columbia , md .) using an excitation wavelength of 440 nm and integrating the emission intensity from 450 to 600 nm . the collection efficiency is calculated as eff = f s / o s f r / o r ( 6 ) to determine the system blank for various potential analytes , an absolute fluted filter capsule ( 3 - μm pore model 12116 , gelman laboratory , ann arbor , mich .) may be installed at the sampler inlet and the system operated for two 30 - minute periods and the resulting aqueous samples acidified to achieve a 0 . 5 % concentration of nitric acid and analyzed by direct injection into a multi - element gfaas 96 with zeeman background correction ( simaa 6000 , perkin elmer corp ., danbury , conn .) for al , as , cd , cr , cu , fe , mn , ni , pb , sb , se , zn . the size distributions for the rest psl particles are measured before and after condensational growth using a micro - orifice impactor to segregate the aerosol into 9 size ranges from 0 . 01 to 15 μm . the particle concentrations are kept as low as practical to reduce agglomeration , while still being detectable in a 30 minute sample , but the effects are still evident for particles & lt ; 0 . 5 μm . [ 0107 ] fig3 shows fluorescence vs . particle size spectra for 0 . 084 μm particles before and after condensational growth . the relatively high concentration for 0 . 084 μm particles results in multiple particles becoming entrained in each nebulizer droplet , which increases the mean dry particle diameter to about 0 . 3 μm . this agglomeration effect is greatly reduced for 0 . 209 μm particles and negligible for larger particles . following condensational growth , the mean size increases to about 4 μm , with 65 % of the droplets & gt ; 3 μm . the collection efficiencies for the virtual and real or inertial impactors were measured using dry psl particles with no condensational growth . the collection efficiency vs . particle size curve for the virtual impactor ( shown in fig4 ) for dry particles ranging in size from 0 . 1 to 6 μm indicates a 50 % cutpoint of about 1 . 8 μm . for particles 3 μm and larger , the collection efficiency is 80 %, which results in a concentration factor of 13 . 6 for large particles in the minor flow . the collection efficiency curve for the real impactor for dry particles ranging in size from 0 . 1 to 3 μm , shown in fig5 indicates a 50 % cutpoint of about 0 . 4 μm . the collection efficiency for the entire system 58 ( i . e ., steam injectors , condensers , virtual impactor , real impactor , and transfer lines to the fraction collector ) was measured using psl particles ( 0 . 1 to 3 μm ) and is shown in fig6 . for input particles & lt ; 0 . 5 μm , the collection efficiency is about 40 % and is independent of particle size . for particles & gt ; 0 . 5 μm , the collection efficiency gradually increases with size to 68 % for 2 . 977 μm input particles . the lower efficiency for small particles is due to incomplete growth of those particles , as seen in fig3 . a mass balance for particle collection and loss performed for 0 . 084 μm particles through the entire condensational growth system is shown in a summarized manner in table 2 . each component was washed before and after the tests to determine losses . the overall collection efficiency for the grown droplets was 32 %, with the virtual impactor major flow and condensers being the major sources of loss , accounting for 26 % and 25 % of the input particles , respectively . based on ambient concentrations measured in college park , md ., a non - industrial suburb of washington , d . c ., average aqueous system blanks ( al , 3 ; as , 0 . 06 ; cd , 0 . 03 ; cr , 0 . 4 ; cu , 0 . 2 ; fe , 1 . 5 ; mn , 0 . 4 ; ni , 0 . 1 ; pb , 0 . 4 ; sb , 0 . 3 ; se , 0 . 08 ; and zn , 1 . 2 ng ml - − 1 ) are adequate to achieve average sample - to - blank ratios ranging from & gt ; 3 to & gt ; 30 for all but cr and ni ( for which s : b ratios are in the range of 1 to 5 ) in the current system . although this invention has been described in connection with specific forms and embodiments thereof , it will be appreciated that various modifications other than those discussed above may be resorted to without departing from the spirit or scope of the invention . for example , equivalent elements may be substituted for those specifically shown and described , certain features may be used independently of other features , and in certain cases , particular locations of elements may be reversed or interposed , all without departing from the spirit or scope of the invention as defined in the appended claims .