A near real-time system for continuously monitoring airborne subtilisin-type enzymes in the industrial atmosphere

Frederick J. Rowell *a, David Sykes b, Lynsey Grieveson a, Brenden Theaker a, Latha Sundar a and Robert H. Cumming b
aNorth East Biotechnology Centre, School of Health, Natural and Social Sciences, University of Sunderland, Sunderland, UK SR1 3SD. E-mail: frederick.rowell@sunderland.ac.uk; Fax: +44 191 5152502; Tel: +44 191 5152563
bNorth East Biotechnology Centre, School of Science and Technology, University of Teesside, Middlesbrough, UK TS1 3BA

Received 3rd April 2006 , Accepted 13th November 2006

First published on 1st December 2006


Abstract

We describe the development and validation of a portable system comprising an air sampler coupled to an automated flow injection analysis device. The system is able to monitor airborne concentrations of subtilisin-type enzymes in the workplace atmosphere on a continuous basis. Sampling is in two stages: using a sampling head that is designed to mimic human respiration at approx. 1 m s−1 at a sampling rate of 600 l min−1. In the second stage, the captured particles are deposited by impaction from the air stream onto the inner surface of a cyclone that is continuously washed with a jet of buffer solution. Deposited particles are then washed into a reservoir from which samples are taken every 5–6 min and injected automatically into a continuous flow injection analysis system. Proteolytic enzyme in the sample passes through a bioreactor maintained at about 40 °C. This contains a cellulose solid phase matrix on which is covalently immobilised Texas Red-labelled gelatin as substrate. The passing enzyme partially digests the substrate releasing fluorophore that is detected down stream in a flow cell coupled to a fluorimeter. The system is calibrated using enzyme standards and the intensity of the resulting peaks from the ex-air samples is converted to airborne concentrations using a mathematical model programmed into a PC. The system has a limit of detection of 4.8 ng m−3 and a dynamic range of 5–60 ng m−3. The within assay precision (RSD) is 6.3–9.6% over this range. The within batch precision is 20.3% at 20 ng m−3 and the corresponding between batch value is 19.5%. The system has been run for periods up to 8 h in the laboratory and for up to 4 h at a factory site and the values obtained compared with time-averaged values obtained from a conventional Galley sampler and in-house analysis when reasonable agreement of the results was observed. The stability of the system over 21 days of continuous use with standards injected periodically was studied. Linearity was observed for all the standard plots throughout. At the end of 21 days, after a total exposure equivalent to 2395 ng ml−1 of Savinase, the signal due to the 5.0 ng ml−1 standard was still easily detectable.


Introduction

Subtilisin-like protease enzymes are mass-produced and used widely in the detergent and food industries and are also used in animal feeds and leather processing. Care has to be taken in handling the raw material as it is a potential respiratory sensitising agent.1–3 Due this potential risk a maximum exposure limit (MEL) of 40 ng m−3 has been set.4 This requires the employer to reduce exposure to a concentration that is as low as is reasonably practicable and below the MEL.5

Due to the low concentrations involved, routine sampling of industrial air is usually performed with static samplers fitted with filters, such as Galley samplers, and high volume sampling at 600 l min−1 or above is used. Alternatively the exposure of individual workers may be assessed using personal sampling systems attached to the clothing of the worker near their face.5 These are again based on filtration but with low volume sampling at about 2 l min−1.

Both approaches are limited in two respects. Firstly following sampling the filter is removed subjected to extraction and the enzyme concentration in the extract determined. Thus results are obtained hours or days after the sampling is performed. Secondly the results give a time-averaged picture of the airborne levels. This can be less than the MEL even if the MEL is exceeded transiently during an activity within the factory. It is thought that such short-term exposure could be a contributory factor in workplace sensitisation. Hence what is need is a system that can obtain airborne levels in near real-time over an extended monitoring period such as an 8 h shift.

This paper describes our approach to achieving this objective. It combines a high volume air sampler based on a cyclone design with a flow injection system employing a bioreactor containing a fluorescent substrate specific for the proteolytic enzyme. Details of the design and working of the cyclone sampler are given as are the details of the mathematical model used to transform the fluorescence signals from the fluorescence immunoassay (FIA) system into airborne concentrations of enzyme. The FIA-bioreactor system was developed from two bioreactor systems for protease enzymes described previously that were based on fluorescein-labelled porcine thyroglobulin immobilised onto glass beads6 or fluorescein-labelled bovine serum albumin immobilised onto a cellulose support.7 In this paper we describe the development of a new substrate based on gelatin labelled with Texas Red® immobilized on cellulose and its use in a heated bioreactor attached to a fully automated flow injection analysis system. The new analytical system also employs a compact and relatively inexpensive fluorescence detection system. The combined sampling and analysis system has been positioned on a trolley and taken to two sites where proteolytic enzymes are used. The development of the analytical system and the performance of the combined system, both within the laboratory and within the factories, are described.

Experimental

Apparatus

The complete system is shown in Fig. 1. It consisted of a sampler head consisting of a pair of circular metal plates (A) attached via plastic tubing to a glass cyclone (B). Air was sucked through A and B using a commercial vacuum cleaner (C). The rate of airflow was monitored using an orifice plate and adjusted as needed. A needle (D) was attached to B and buffer solution was pumped through its orifice using an adjustable peristaltic pump (E). As air flowed through the cyclone this jet of water covered the inner surface of the cyclone and flowed into a reservoir (F) from which it was recycled via E back into the cyclone. More details of design of the cyclone and its ability to capture the required aerosols are given below.
Schematic representation of the monitoring system (enzyme sniffer) for airborne enzymes.
Fig. 1 Schematic representation of the monitoring system (enzyme sniffer) for airborne enzymes.

Following air sampling, known volumes of buffer are taken periodically from F into an automated flow injection system (G) attached to a bioreactor within a thermostatically controlled column heater (H). Downstream is located an optical flow cell (I) equipped with two optical fibres attached to a light source (J) and a spectrophotometer (K). Phosphate buffered saline is passed through the FIA system using a peristaltic pump (L) and the signal from K recorded using a lap top PC (M). This PC also controlled the automated flow injection system. In both cases the programmes used were those supplied by the manufacturer of these two systems (FIAlab, Medina, WA, USA).

The automated flow injection system (G) was model 3500 from FIAlab Instruments. The column heater (H) was an Eppendorf CH500 heater (Phenomenex, Macclesfield, Cheshire, UK), which was set to operate at an exit buffer temperature of 40 °C at a flow rate of 0.7 ml min−1. The flow cell (I) was model X from FIAlab who also supplied the two stainless steel-coated optical fibres (P400-2), the LS-1 tungsten halogen light source and the S2000 spectrometer (J). The peristaltic pump (K) was model P-1 from Pharmacia (Milton Keynes, Buckinghamshire, UK).

Design and efficiency testing of the cyclone

A glass cyclone of dimensions (40 mm diameter, 20 mm outlet, 30 × 10 mm rectangular inlet, and a main body of 80 mm length and cone of 80 mm length) was constructed which had three pre-drilled holes in the air inlet tube to allow up to three positions of the needle for the introduction of the recycling fluid (see Fig. 2). These holes were positioned at the centre of the inlet tube and 6 mm either side. A stainless steel hypodermic needle was bent at a right angle (10 mm from tip) to allow the recycling fluid to be pumped into the cyclone.
Design of the glass cyclone used in the studies showing the positioning of recycling fluid needle entry points.
Fig. 2 Design of the glass cyclone used in the studies showing the positioning of recycling fluid needle entry points.

The cyclone was tested to measure its grade efficiency by loading fine dust through the cyclone inlet and measuring the difference in particle size and concentration of the dust inputted into the cyclone and that of the dust exiting the cyclone using an aerodynamic particle sizer (APS).

Variable airflows were drawn through the cyclone using a variable flow vacuum pump. The air flow was measured across the entrance to the tubing using a 20 mm diameter bell mouth.

The fine dust, R10 mineral flour (http://www.particletechnology.com) had a particle size of no greater than 10 μm. The dust was aerosolised using a TOPAS SAG 410 (http://www.topas-gmbh.de) into the rig using a pitot tube at approximately 0.1 g min−1.

The air was sampled either side of the cyclone using isokinetic sampling tubes. These were placed at least 10 diameters after any bends, valves or any changes in pipe diameter. Samples were taken using an APS (TSI APS 3320, http://www.tsi.com) at a flow of 5 l min−1.

The APS was set to sample for 20 s with a 10 s interval between samples, the first sample was taken from the isokinetic sampler before the cyclone, the sampling valve was then switched and the next sample was taken from the airflow after the cyclone, following this the sampling valve was switched. This cycle was repeated a total of 10 times with 10 samples taken from the air flow before the cyclone and 10 samples after.

The percentage efficiency of the cyclone at a set flow rate was calculated by subtracting the number of particles at a distinct particle size exiting the cyclone from those entering the cyclone. For example, if at a distinct particle range of 0.523–0.640 μm 10[thin space (1/6-em)]000 particles were sampled from the air entering the cyclone and 9000 particles were measured exiting the cyclone, then the percentage efficiency at that particle range would be 10%.

The grade efficiency for the cyclone at a set flow rate was found by calculating the efficiency across the entire range of the particle sizes measured. This grade efficiency is represented graphically as a curve with percentage efficiency plotted against particle size in microns (not shown).

The d50 of a cyclone at a set flow rate was found by plotting a best fit curve through the points of grade efficiency curve and deriving the particle size where the cyclone is 50% efficient.

Reagents and materials used in the flow injection analysis system

The composition of buffers, sources of enzymes, and chemicals and other materials used in the flow injection system and in bioreactor production are those described previously.6–9 Gelatin type B (about 75 bloom) was from Sigma (Poole, Dorset, UK). Texas Red® succinimidyl ester was from Molecular Probes (Eugene, OR, USA). The serine-type proteolytic enzymes studied were Purafect (Genencor International Inc., Rochester, USA) and Savinase from Novozymes, Bagsvaerd, Denmark, who also supplied the lipase and cellulase enzymes. Papain was from Papayer Latex and supplied by Sigma.
Synthesis of gelatin–Texas Red conjugate. Gelatin (0.105 g) was dissolved in sodium bicarbonate buffer (10 ml of 0.1 M at pH 8.3) with gentle heating (40 °C). Texas Red® succinimidyl ester (5 mg) was dissolved in 500 μl of dimethyl sulfoxide. This mixture was then was then added to the dissolved gelatin solution. The container was covered with tin foil and mixed on a rotator mixer for 1 h at room temperature. When stored at 4 °C, this solution of labelled gelatin is stable for approximately 3–4 weeks.
Synthesis of cellulose–gelatin–Texas Red solid phase. Medium cellulose fibre (5 g) was rinsed in deionised water and centrifuged (2000 rpm for 6 min) prior to removing the supernatant solution. This was repeated three times after which the cellulose was filtered under vacuum using a size 2 sintered glass funnel (BDH Poole, Dorset). Sodium m-periodate solution (80 ml of 0.5 M) was added to the damp cellulose and the mixture rotated for 210 min at room temperature. The activated cellulose was then filtered and washed with 2 l deionised water as above. The activated cellulose was stored at 4 °C in deionised water containing 0.02% sodium azide, and was stable for 3–4 weeks.

Activated cellulose (2.5 g after filtration) was suspended in 0.1 M anhydrous dibasic sodium phosphate buffer (65 ml). To this was added the gelatin–Texas Red conjugate (10 ml). The container was coated in aluminium foil and rotated for 45 min at room temperature prior to the addition of sodium cyanoborohydride (250 mg). The tube was replaced on the rotator and left to mix overnight at room temperature. After coupling, the cellulose–gelatin–Texas Red solid phase was filtered under vacuum as above and washed with 2 l of deionised water. The resulting cellulose–gelatin–Texas Red solid phase was also stable for 3–4 weeks when stored under refrigerated in deionised water containing 0.02% sodium azide. Bioreactors were produced as described in ref. 8.

Development of the flow injection analysis system

Performance of the complete system in-house

FIA conditions. The FIA buffer and that for the enzyme standards were phosphate buffered saline solution (PBST). This contained sodium chloride (7.2 g), anhydrous dibasic sodium phosphate (1.48 g), sodium dihydrogen orthophosphate monohydrate (0.5 g), sodium azide (0.5 g) and polyoxyethylene–sorbitan monolaurate (1.0 ml) (Tween 20® ICI Americas, Inc.) per litre. The FIA flow rate was maintained at 0.7 ml min−1 using small adjustments of the peristaltic pump. The sampling program was compiled using the FIALab for Windows version 5. The sampling volume used was 100 μl, total injection volume 180 μl at a rate of 12 μl s−1. A 590 nm filter was inserted into the path of the light source (J) and the spectrophotometer (K) was set at 612 nm.
Precision. Within assay precision (RSD) was determined from 6 replicate injections of each Purafect standard (0, 5, 10 and 20 ng ml−1 of the active enzyme). Within batch precision was determined by comparing the gradients of the standard curves for standards (0, 10, 20 and 30 ng ml−1 of the active enzyme) for three sequential assays of column material from one batch in three different columns. Between batch variability was performed by comparing the gradients for three assays for the same four standards used in the within batch study on eight columns, prepared from three different batches of solid phase material.
Sensitivity and linearity. The sensitivity of the system, in terms of the limit of detection was determined from a standard curve of peak height versus Purafect concentration. Triplicate injections of Purafect standards (0, 5, 10 and 20 ng ml−1 in PBST) were introduced to the system. The limit of detection was calculated from the resulting standard curve to be the concentration of Purafect corresponding to the mean fluorescence signal of the background plus three times the standard deviation of the background.
Specificity. To test the specificity of the system, three proteolytic enzymes and two non-proteolytic enzymes were studied. Using the same conditions as described for the studies for sensitivity and linearity, replicate injections of 50 ng ml−1 in PBST of Purafect, Savinase, papain, cellulose, and lipase were introduced separately into the column. The peak heights were recorded for n = 6 replicates for each enzyme solution. The resulting mean peak heights were calculated and expressed as a percentage of that of the Purafect standard.
System stability and capacity of the bioreactors. It was possible to retrospectively calculate a value for the total exposure of the column to Purafect standards over several days’ use that significantly decreased the intensity of the calibration peaks. In the first study, a bioreactor was subjected to continuous running of the FIA system over three consecutive days. At the beginning of each day the system was set up as described above under FIA conditions and calibrated with 0, 5, 10 and 20 ng ml−1 triplicate injections of Purafect standards. Two further calibrations were performed each day at the middle and end of each run. The total time of each run was 4.5 h. At the end of the run the system was flushed with FIA buffer, the column heater turned off and the flow rate reduced to 0.2 ml min−1 until the next run was performed. On the following two days the FIA system was set up to operate as described above and the process repeated.

In the second study, an identical bioreactor was used and the system was run continuously for 21 days during which it was calibrated with 0, 5, 10 and 25 ng ml−1 duplicate injections of Savinase standards at the start and end of each daytime run with the same standards injected 6 h after the start but as single standards. At the end of the run the system was flushed with FIA buffer, the column heater turned off and the flow rate reduced to 0.2 ml min−1 until the next run was performed. On the following days, the FIA system was set up to operate as described above and the process repeated. From this experiment it was possible, to calculate the total mass of Purafect and Savinase injected through the respective columns over the test periods.

Calculation of airborne enzyme concentrations. It is necessary to interpolate the signals produced as a result of captured enzyme during air sampling passing through the bioreactor into the detector, into actual airborne concentrations. Hence a mathematical model was needed to relate the concentration of enzyme in the fluid of the cyclone collection vessel to the actual airborne concentration over the collecting period. The equipment and operating variables for using the cyclone as a continuous aerosol collection apparatus is shown in Fig. 3. The concentration of enzyme in the inlet air (C1) is reduced to C2 in the exit air stream. If the cyclone is 100% efficient for the collection of particles, then C2 is zero. If the efficiency is known, C2 can be substituted in the model with C1 (1 − E); where E is the fractional efficiency. The airflow rate leaving the cyclone (F1) is the same as the air flow rate entering the cyclone. A wash fluid is sprayed into the cyclone inlet to sweep the collected enzyme from the cyclone body wall into the collection vessel, where it can be pumped to the FIA measuring system to estimate its enzyme concentration (stream F2). It can be seen that a wash fluid stream is recycled from the collection vessel into the air inlet (F6). A flow of liquid (F5) was necessary to keep the reservoir volume constant, as some fluid is lost through evaporation (F3). It is important to realise that this evaporation loss does not result in loss of enzyme from the system. However, re-entrainment losses from splashes of fluid in the cyclone being captured by the exit air will result in a loss of enzyme from the system (F4). The passage of wash fluid down the cyclone walls and into the collection vessel follows a spiral path. Thus in some conditions, a considerable amount of the collecting fluid could be held on the vessel walls rather than in the collection vessel. This is indicated by the liquid flow F7.
Schematic of fluid flows in the cyclone. F1 air flow rate in; C1 concentration of enzyme in air; C2 concentration of enzyme in air leaving cyclone due to non-capture; F4 liquid flow lost through re-entrainment; C3 concentration of enzyme in collection reservoir and re-entrainment fluid; F3 liquid flow rate lost through evaporation; F7 liquid flow from cyclone walls into collection vessel; V liquid volume of collection reservoir kept constant with top-up flow, F5; F2 liquid flow to enzyme analyser and F6 recycle fluid flow rate.
Fig. 3 Schematic of fluid flows in the cyclone. F1 air flow rate in; C1 concentration of enzyme in air; C2 concentration of enzyme in air leaving cyclone due to non-capture; F4 liquid flow lost through re-entrainment; C3 concentration of enzyme in collection reservoir and re-entrainment fluid; F3 liquid flow rate lost through evaporation; F7 liquid flow from cyclone walls into collection vessel; V liquid volume of collection reservoir kept constant with top-up flow, F5; F2 liquid flow to enzyme analyser and F6 recycle fluid flow rate.
Liquid balances. The top-up fluid has to replace all fluid losses from the collection vessel in order to keep the volume constant, thus:
 
F5 = F2 + F3 + F4(1)
where the liquid (F4) is lost through splashing of the recycle fluid and subsequent re-entrainment in the exit air. This is obviously dependent on the mode of operation of the cyclone. The liquid balance around the cyclone is given by
 
F6 = F3 + F4 + F7(2)
which introduces the idea that some of the collected aerosol may be held-up in the collection fluid on the walls of the cyclone vessel itself. The loss of fluid through evaporation (F3) may be considerable, since the cyclone walls are bathed in a thin liquid film over which there is a high flow rate of air with usually a low humidity. Liquid losses due to re-entrainment will depend on the way the liquid is introduced into the cyclone air inlet as well as airflow rate.
Enzyme balances. The enzyme in the aerosol leaving the cyclone could come from two sources:

(i) Those particles not captured by the cyclone through its design specifications, and

(ii) those particles which have splashed off the wall of the cyclone and have been swept out of the cyclone outlet (re-entrainment). This would be a characteristic for cyclones with a liquid wash stream only.

The aerosol captured by cyclone can thus be calculated as

 
F1 (C1C2) − F4C3(3)
where C1, C2, and C3 are the enzyme concentrations in the inlet air, outlet air and collection vessel, respectively. The enzyme balance in liquid phase (the hold-up liquid) of cyclone body, is given by
 
F6C3 + F1(C1C2) = F7C4 + F4C3(4)
Whereas, the mass balance of the enzyme in collection vessel-assuming ideal mixing is:
 
ugraphic, filename = b615201p-t1.gif(5)
Re-arranging eqn (4):
 
F7C4 = F1(C1C2) + C3(F6F4)(6)
Substituting for F7C4 into eqn (5), gives
 
ugraphic, filename = b615201p-t2.gif(7)
leading to
 
ugraphic, filename = b615201p-t3.gif(8)

Ramifications of the enzyme mass balance. This derivation assumes that the capacity of the cyclone is small compared to the volume of the collection vessel, i.e. all accumulation takes place in the collection vessel. Eqn (8) can be integrated if the cyclone ran in a constant airborne concentration of enzyme (i.e.C1 is constant.). Although this is not expected, it is instructive to do so to reveal the performance of the cyclone in this mode of operation. Eqn (8) can thus be rearranged:
 
ugraphic, filename = b615201p-t4.gif(9)
When t = 0, the enzyme concentration in the collection vessel is zero, i.e.C3 = 0, and eqn (9) can be integrated with respect to t
ugraphic, filename = b615201p-t5.gif
Inverting the logarithms and rearranging to give C3,
 
ugraphic, filename = b615201p-t6.gif(10)
This shows that the concentration of enzyme in the collection vessel would reach a steady state, because as t → ∞, C3ugraphic, filename = b615201p-t7.gif. The characteristic time of the system is, ugraphic, filename = b615201p-t8.gif. To increase the sensitivity of the system t → 0, therefore sensitivity can be increased by a reduction in the size of V, or by increasing the liquid flows from the collection vessel. Of these options, reducing the collection volume is the most practical way of increasing the sensitivity.
Back-calculation of C1. The collection device needs to give the airborne concentration of enzyme in ‘near real-time’. C3 is measured, but C1 is required. Eqn (10) can be rearranged to calculate C1, the constant air inlet concentration:
 
ugraphic, filename = b615201p-t9.gif(11)
Use of the model to predict airborne enzyme concentrations in factory air. The concentrations of enzyme in factory air will fluctuate according to the procedures being carried out and the location of a sampling device. Because the airborne concentration of enzyme in factory air will not be constant, we could use eqn (10) to calculate C1 over a short time interval (e.g. 5 min) with an averaged value of C3 during that time span. This will give a ‘near real-time’ device. Alternatively we could use the differential eqn (8) rather than the integrated eqn (11). Rearrangement of eqn (8) allows calculation of the factory enzyme concentration based on the rate of change (gradient) of the concentration in the collection vessel:
 
ugraphic, filename = b615201p-t10.gif(12)
The slope would be monitored from the output of an enzyme detection device attached to the F2 stream. Since we can calculate the gradient from two successive C3 measurements, the airborne enzyme concentration could again be monitored in near real-time.

The predicted performance of the device was obtained using eqn (8) by taking the gradient of C3t at regular intervals. This is the concentration that the detection system would have to measure. The cyclone concentrates the enzyme in the reservoir as expected, but then the concentration decreases in a linear fashion due to the feed to the detection system and any re-entrainment losses (the reservoir volume is maintained constant through a top-up system of fresh buffer). In practice, a 5 min sampling strategy was adopted because the flow injection analysis of the enzyme needs to include not only a sample injection but a wash phase as well.

The effect of operating conditions of the cyclone on re-entrainment and fluid loss. The principle of the technique is to run the cyclone with a known amount of dye marker material in the reservoir in normal operating conditions but without any aerosol in the inlet air stream. If material is lost from the cyclone, it must be through re-entrainment losses. To simplify the situation, it was assumed that the liquid hold-up volume on the cyclone walls is small compared with the reservoir volume. The situation is shown in Fig. 4, where the notation is as used previously. The reservoir was pre-loaded with a solution of a dye marker substance. The airflow rate leaving the cyclone (F2) is the same as the air flow rate entering the cyclone (F1). A wash fluid is sprayed into the cyclone inlet to sweep the collected material from the cyclone body wall into the collection vessel. It can be seen that a wash fluid stream is recycled from the collection vessel into the air inlet in the body of the cyclone. A flow of liquid (F5) was necessary to keep the reservoir volume constant, as much fluid is lost through evaporation (F3). It is important to realise that this evaporation loss does not result in loss of material from the system. However, re-entrainment losses from splashes of fluid in the cyclone being captured by the exit air will result in a loss of enzyme from the system (F4).
Schematic of the flows for determining re-entrainment losses from the cyclone system. F1 and F2 are the air flow rates entering and leaving the cyclone, respectively; F5 top-up fluid flow rate to keep volume (V) in collection reservoir constant; C3 concentration of dye in reservoir; F3 fluid loss through evaporation and F4 re-entrainment losses.
Fig. 4 Schematic of the flows for determining re-entrainment losses from the cyclone system. F1 and F2 are the air flow rates entering and leaving the cyclone, respectively; F5 top-up fluid flow rate to keep volume (V) in collection reservoir constant; C3 concentration of dye in reservoir; F3 fluid loss through evaporation and F4 re-entrainment losses.
Material balance for determination of the fluid losses. Evaporation losses from the reservoir and subsequent topping-up with fresh fluid will not dilute the marker material in the reservoir. Thus the concentration will not change with running time. However, if there is a re-entrainment loss, then the concentration in the reservoir will fall with time. Remembering that there is no input to the system:
 
ugraphic, filename = b615201p-t11.gif(13)
Which, on integration gives:
 
ugraphic, filename = b615201p-t12.gif(14)
where Ct and C0 are the concentrations in the vessel at time t and time 0, respectively, V is the volume of fluid in the cyclone (ml) and F4 is the liquid flow lost to re-entrainment (ml min−1). Thus a plot of ln (Ct/C0) against t should yield a straight line with a negative gradient of −F4/V; from which F4 can be calculated. Evaporation losses can be calculated by the subtraction of the re-entrainment loss from the total fluid loss.
Determination of fluid losses and proof of model using dye addition to the cyclone. The equipment was as in Fig. 4 and as described above, with air being drawn using a vacuum cleaner at 500 l min−1, liquid pumped into the cyclone sampling system through a syringe needle drawn back into the collection vessel (CV) at a rate of 2 ml min−1 then returning to the pump via an in-line flow cell placed in a spectrophotometer. The cyclone used was a 40 mm rectangular inlet cyclone as described above with injection through the holes in the inlet of the cyclone. The volume within the CV (and whole system) was set at 5 ml, the system was allowed to run to top the CV and tubing within the sampling system. The fluid used was phosphate buffered saline (PBS; PBST minus Tween but containing 0.1% v/v low foaming surfactant Synperonic NCA 840 (Ellis & Everard, Bradford, UK)).

The experiments were carried out by the setting up of the equipment as above with the addition of tartrazine (see experiments below for timings and concentration used), absorbance readings from the spectrophotometer were taken regularly throughout the experiment, and the mass of the liquid reservoir was recorded at time intervals of approximately 10 min.

Fluid loss was investigated by measuring of change in mass in the reservoir bottle over a number of minutes or hours of the experiment, whilst fluid was passed through the cyclone, into the collection vessel and through the flow cell. The change in the concentration of the tartrazine was measured using the absorbance of the dye in the flow cell (λ = 510 nm).

Three sets of experiments were carried out using this equipment and methodology to establish the ability of the model to predict the change in concentration within system given varying concentrations of solute in the system:

(i) A single dose of 10 mg of tartrazine was added at 5 min into the experiment, as an aliquot of 0.1 ml at a concentration of 0.1 g ml−1.

(ii) A constant dose of tartrazine at a rate 0.1 mg min−1 over the experimental run.

(iii) Three doses of 10 mg of tartrazine were added at 5, 65 and 185 min into the experiment as an aliquot of 0.1 ml at a concentration of 0.1 g ml−1.

The resulting data was plotted as tartrazine concentration vs. time, whilst the modelling data was developed from inputting the required values into the method outlined in above. The resulting experimental and modelling data were plotted on the same figures (Fig. 5a, b and c). Several sets of experimental and modelling data are plotted together.


(a) Experimental data of a pulse of solute (tartrazine) added at 5 min to new enzyme sniffer system with modelling data overlaid. (b) Experimental data of constant addition of solute (tartrazine) to enzyme sniffer system with modelling data overlaid. (c) Experimental data of 3 pulses of solute (tartrazine) added to enzyme sniffer system with modelling data overlaid.
Fig. 5 (a) Experimental data of a pulse of solute (tartrazine) added at 5 min to new enzyme sniffer system with modelling data overlaid. (b) Experimental data of constant addition of solute (tartrazine) to enzyme sniffer system with modelling data overlaid. (c) Experimental data of 3 pulses of solute (tartrazine) added to enzyme sniffer system with modelling data overlaid.
Performance of the system in industry. The system was mounted on a trolley for manoeuvrability and transported to an industrial site for testing. There it was run for up to 4 h and the signal recorded at three sites within the factory where proteolytic enzymes were used. The first was a low risk site located at a laboratory, the second a medium risk one where packing machines were located, and the third a high risk site where crude enzyme was tipped and bags containing enzyme stored and changed. At the same time a Galley sampler was set up adjacent to the system and this was run for the same period as the test system. At the end of the sampling, the varying airborne concentrations of Purafect throughout the sampling period were calculated using a computer programme based on the mathematical model described (derived from eqn (14) above) that relates the concentration of enzyme found in the reservoir (F) during the air sampling, to the rate of air sampling, volume of buffer in the reservoir (F), the efficiency of collection, the frequency of injection from F into the FIA system, and the volume of injection of samples from F into the FIA system. Details of this programme are given in ref. 10.

The filters from the Galley samplers were removed and following standard in-house methods of extraction and analysis by used by the company, the time-averaged airborne concentration of Purafect was calculated.

Results

Design of the air sampling system and use of the modelling equation

Testing of the cyclone design and its performance. The cyclone was tested across a range of airflows (nine different airflows from 176 to 732 l min−1), and at 608 l min−1 was shown to have a d50 of approximately 0.77 μm with an SD of 1.1%. The cyclone can be seen to efficiently capture at least 90% of the particles of 1.5 μm and above an air flow of ∼600 l min−1. This establishes that the cyclone is capable of capturing the particle sizes as required by the project and of a similar size to the filters used in Galley samplers which have a 1.2 μm pore size.10
Calculation of re-entrainment losses. As describe above the re-entrainment flow loss is found from subtracting the evaporation loss from the total fluid losses, it can then be expressed as a percentage of the total fluid loss. Fluid loss from the cyclone by re-entrainment was about 16%. The data did not fit a straight line after long run times (not shown). This may be due to the dye crystallising out on the cyclone walls (it could be seen), and will thus remove itself from the system producing a greater apparent re-entrainment loss. A straight line was therefore fitted over the initial part of the curve only.
Determination of fluid losses and proof of model using added tartrazine dye. Fluid losses from the cyclone were studied to determine the optimised flow rates and equipment set-up. The majority of fluid loss was due to evaporation (>90%), which is not surprising since the inner walls of the cyclone have a film of water running over them in the presence of a fast air flow.

With respect to the total fluid loss, the significant parameters (p = 0.05, Student t-tests) were air flow rate and the recycle flow rate; increasing either increased the rate of fluid loss. This is not unexpected, since the higher the air flow rate, the greater will be the evaporation effect. Similarly a high recycle rate will wet more of the cyclone surface and hence cause a higher evaporation loss. In the case of the re-entrainment losses, the significant factors were airflow rate, needle depth and the interaction between these two. By positioning the needle on the cyclone wall, less fluid was lost from the system by re-entrainment at high flow rates than when the needle was releasing the fluid from the axes of the cyclone inlet tube.10

It can be seen in all three figures presented in Fig. 5, that the model predicts the experimental data well. With both pulse experiments (shown in Fig. 5a and c) the model predicts a build up before the actual real data, this may be due to some delay within the real system either computer based or in the collection of the data from the spectrophotometer, the real data also show a larger pulse than that of the modelled data.

Several spikes can be seen towards the end of both experimental data sets in the triple pulse experiments (Fig. 5c). These are caused by delays in the addition of fluid to the system, caused by intermittent foaming during these experiments. Once the foam level drops, the top-up system quickly adds liquid, which subsequently reduces foaming and replenishes the fluid level within in the CV and overall sampling system; this dilutes the exaggerated dye concentration.

The constant build-up experiment (Fig. 5b) represents two different experimental data sets; one when modelled predicts the build-up fairly well throughout the curve (representative within 8% of the real data), whilst the other data set predicts both the beginning and end of the curves better (representative within 10% of the real data, respectively). These differences are most likely due to the variation of the entrainment figure throughout the experiment. The entrainment can vary by a few percent from the beginning of the experiment till the end; this could have this effect on the prediction of real data using the model.

Assay performance

Sensitivity and linearity. The limit of detection was determined to be 4.83 ng ml−1 Purafect at the 99% confidence level. The linearity of the standard curve over the range 0–20 ng ml−1 (n = 4) was good with the correlation coefficient r2 = 0.995 (linear regression analysis). Similar linearity has been observed over larger dynamic ranges up to 0–60 ng ml−1. A typical standard curve is shown in Fig. 6 and a typical profile for an extended run of the FIA system over 2 h with sequential injections of replicates of standards (20 and 60 ng ml−1) is shown in Fig. 7.
Typical calibration curve of fluorescence intensity versus enzyme concentration.
Fig. 6 Typical calibration curve of fluorescence intensity versus enzyme concentration.

Typical response pattern of the FIA system to repeated injections of replicates of Purafect standards (60 ng ml−1n = 5, and 20 ng ml−1n = 21) over an extended run (2 h).
Fig. 7 Typical response pattern of the FIA system to repeated injections of replicates of Purafect standards (60 ng ml−1n = 5, and 20 ng ml−1n = 21) over an extended run (2 h).
Precision. The within assay precision was good with RSD values of 9.6% at 5 ng ml−1, 6.3% at 10 ng ml−1 and 9.0% at 20 ng ml−1 (n = 6 in each case). Within assay variation was between 1.2%–13.5% (n = 8), with six of the 8 columns being less than 10%. Within batch variability was 20.3% and the between-batch variability was calculated as 19.5%.
Specificity. The specificity of the system towards serine-type proteases such as Purafect and Savinase was demonstrated. The relative signal obtained from the Savinase was 157% relative to the Purafect signal at 50 ng ml−1. No significant peaks were observed on the introduction of the non-serine-type protease, papain or for cellulase and lipase.
System stability and capacity of the bioreactors. From the first study it was calculated that a total of 190 ng of Purafect was injected through the bioreactor over the three days of the experiment. It was observed that this exposure resulted in a 50% decrease in the intensity of the peak height from the initial to final calibrations. During the second study, the bioreactor was exposed to Savinase standards during continuous operation for a period of 21 days and a similar progressive decrease in peak intensity was seen. The column was exposed to a total equivalent of 240 ng of Savinase over this period. At the end of the study, a 50% decrease in the intensity of the peak height was observed following exposure to approximately 172 ng of Savinase. A gradual decrease in the gradient of the calibration plots was observed although excellent linearity was seen throughout (r2 = at least 0.990 in each case) (Fig. 8). At the end of the 21 day period, the system was still able to give clear peaks for 5 ng ml−1 standards.
Calibration plots during the continuous operation of the flow injection analysis system over 21 days.
Fig. 8 Calibration plots during the continuous operation of the flow injection analysis system over 21 days.

Performance of the system in industry

No significant signals were produced by the system when it was used on four occasions for up to 4 h at sites 1 and 2. The results from the Galley sampler ranged from 1.3–2.7 ng m−3 for these air samples which are below the LOD for the system. During one further experiment at site 2, no peaks were observed during the first 80 min of sampling. Two samples of crushed washing powder containing enzyme were then thrown into the space between the two samplers at times 85 min and 180 min, when two peaks were then seen at 90 min and 185 min. The time averaged results for the Galley sampler was 5.7 ng m−3 and the corresponding value for the new system was 2.8 ng m−3. Three sampling sessions were undertaken at site 3. In the first, peaks between 5–20 ng m−3 were observed as shown in Fig. 9. This coincided with activities within the factory. As shown in this figure, the system was routinely calibrated at the beginning and end of each run by replicate injections of standards. Fig. 10 shows the corresponding concentrations of enzyme with time for the interpolated airborne concentrations, and the time-averaged airborne concentrations from the Galley samplers. The Galley sampler showed a time-averaged concentration of 0.49 ng m−3 over the 190 min sampling period. The new system exhibited three peaks; a major peak of 21 ng m−3 at the beginning and minor peaks of 8, 7 and 6 ng m−3 thereafter. The calculated time averaged concentration for the new system was 1.73 ng m−3. On the two other occasions, no significant peaks were observed on the first (Galley result of 0.18 ng m−3). On the second occasion no peaks were seen up to 130 min when dust collected from the factory floor and from surfaces was thrown into the gap between the two sampling systems. This produced a large peak of 1200 ng m−3 at 135 min. The time averaged results were 6.9 ng m−3 for the Galley and 25.5 ng m−3 for the new system.
A signal–time response profile obtained during monitoring for airborne proteolytic enzyme at an industrial site. Two sets of standards (25 and 50 ng ml−1) were injected at the beginning (n = 3) and end (n = 5) of the run.
Fig. 9 A signal–time response profile obtained during monitoring for airborne proteolytic enzyme at an industrial site. Two sets of standards (25 and 50 ng ml−1) were injected at the beginning (n = 3) and end (n = 5) of the run.

A concentration–time profile interpolated from results obtained from Fig. 9. The dotted line represents the concentration of proteolytic enzyme in the reservoir/collection vessel of the system (F in Fig. 1) and the continuous line the interpolated concentration of enzyme in the air.
Fig. 10 A concentration–time profile interpolated from results obtained from Fig. 9. The dotted line represents the concentration of proteolytic enzyme in the reservoir/collection vessel of the system (F in Fig. 1) and the continuous line the interpolated concentration of enzyme in the air.

Discussion

We wanted a high-volume sampler (to match current industrial practice) that could deliver the aerosol into a solution which in turn could be pumped to a flow injection enzyme detector. A cyclone air sampler fulfils these requirements. We have already reported the use of a cyclone for the non-continuous monitoring of protease aerosols.7 There are a number of problems associated with the use of a cyclone for continuous sampling, however. These were highlighted in a seminal paper by Errington and Powell11 who used large (350 l min−1) and small (75 l min−1) cyclones to sample aerosols of bacteria and spores. They concluded that the cyclone collection system was as efficient as other samplers (e.g. an impinger) for this application. Griffiths12 and his group have thoroughly investigated and reviewed the use of large throughput cyclones (750 l min−1) to collect bioaerosols in a series of papers and identified parameters that were needed to operate the systems efficiently.

It was concluded from this published work that if we were going to monitor the air borne concentration of enzyme from the concentration in the reservoir on a continuous basis, we either had to measure the volume of collection fluid continuously or keep the collection fluid volume constant. We opted for the latter approach.

Via an iterative experimental process the final cyclone design used in this study was adopted10 and the resulting cyclone connected to an air sampling inlet system that was based on the proven high volume Galley sampler. This is designed to mimic human respiration when operating at an sampling rate of about 600 l min−1 and at an inlet flow of about 1 m s−1.13

The complete cyclone sampler was adapted to operate continuously by:

(i) Using a wash fluid which is recycled from the reservoir;

(ii) Keeping the collection volume constant by adding fresh collection fluid from a storage tank;

(iii) Pumping out some of the reservoir fluid to measure the enzyme concentration continuously or at regular intervals;

(iv) Developing a model to relate the airborne concentration to the reservoir concentration.

The optimisation of the cyclone sampler set-up was a compromise between the need to operate at high air flow rates and the need to minimise fluid losses. In order to collect the enzyme at a high efficiency then the air flow needs to be high, whilst to minimise loss of fluid requires low air flow and low recycling rates. In order to understand the affects of these conflicting requirements on the performance of the cyclone and the entire system, further research was undertaken as described more detail in ref. 10. The operating conditions described herein reflect the outcomes of those studies.

It was demonstrated that the mathematical model developed to calculate the concentration of captured solute during prolonged air sampling was accurate. Thus when tartrazine dye was added under three different conditions (continuous, delayed, and intermittent) to the collection vessel of the air sampling system and the system operated under the normal conditions of air flow, sampling and buffer top up, the concentration of the dye actually measured agreed well with the profile of solute concentration predicted by the model (Fig. 5a, b and c). Thus the prediction from eqn (10), that for a constant enzyme concentration a steady state concentration will be reached, was observed. This gives confidence in the modelling represented above and the use of the model to predict the aerosol concentration of enzymes within the factory experiments.

Within the analytical system a new substrate was used to produce the required signals. Gelatin was conjugated with Texas Red® to produce a fluorescent label that was then covalently immobilised onto a cellulose support matrix. Gelatin was chosen as the substrate because it provides many sites for fluorescent conjugation and potential enzyme hydrolysis. Upon exposure to subtilisin-like protease enzymes, proteolytic cleavage of the immobilised gelatin occurred, resulting in fluorescent signals that were recorded by the spectrophotometer.

The apparatus described constitutes a novel near real-time system for determining the airborne concentration of subtilisin-like protease enzymes in industry. The analytical system has been optimised with respect to sampling volume (100 μl) and flow rates (0.7 ml min−1) to obtain good sensitivity with low sampling time intervals (5 min) when used in combination with the air sampling system.10 The buffer chosen is suitable for maintaining the protease activity of the enzyme and the fluorophore signal. Its use also minimises the leaching of fluorophore, thus extending the lifetime of the bioreactor (data not shown).

The sensitivity of the assay and linearity of the standard curves were good. Linearity of the responses was demonstrated over the enzyme range 5–60 ng ml−1 (equivalent to airborne levels of 5–60 ng m−3)7 and the LOD was calculated to be 4.8 ng ml−1. This is equivalent to an airborne concentration of nearly an order of magnitude below the current MEL for subtilisin-like protease enzymes.

Excellent specificity has been demonstrated for subtilisin-like protease enzymes when compared to other classes of enzyme. No signal was observed with cellulase indicating that hydrolysis of the solid phase support material in the bioreactor did not occur under the conditions use in the FIA system. Also no signals were seen with lipase which, like cellulase, is also used in the detergent industry and thus could be present in the work place atmosphere.

The system has good within-assay precision and reasonable within and between batch variability. The variation stems mainly from inconsistent packing of the columns during manufacture of the bioreactors. This is currently performed manually but an automated system would probably lead to much improved batch consistency.

It was shown that the system became significantly desensitised after exposure of the bioreactor to about 200 ng of Purafect and Savinase. In practice if the system is calibrated with single sets of standards at the beginning and end of each run then it could be run for 18 days if no enzyme is captured from the air. If there is a constant airborne concentration of 6 ng m−3 then the bioreactor will be depleted after 24 h. Transient release of a high airborne concentration of enzyme above 2 μg m−3 will cause a very large signal and immediate depletion of the bioreactor. The inherent stability of the flow injection analysis system with the bioreactor attached was demonstrated by its continuous use for 21 days.

The system is relatively portable and has successfully been demonstrated over extended periods under industrial conditions. However the major advantage of this system over current standard industrial methods is that it provides a near-continuous record of airborne concentrations of enzyme throughout the sampling period. The system is a near time system, with responses of 5 min and a capacity for continuous monitoring over 8 h periods under industrial conditions.

The benefit of the system is clearly demonstrated from the results of the industrial trial. In Fig. 10, the time-averaged airborne concentration seen with the Galley sampler over the 3 h of the run was only 0.49 ng m−3 which is well below the MEL of 40 ng m−3. However the time-airborne concentration profile also shown in Fig. 10 obtained with the new system shows a significant peak of 21 ng m−3 at the beginning of the monitoring period that was detectable for about 10 min. This may have been due to activities that were being undertaken within the factory at that time, but further observations are needed to verify this observation. It is possible that exposure to such transient releases of enzyme within the factory could lead to sensitisation of workers.

The correlation between the time averaged results observed for the new system and the Galley sampler during the industrial sampling was satisfactory since they were within an order of magnitude for the three sets of data obtained. It is not expected that these results will be identical since each sampler may have been exposed to different plumes of air with different concentrations of enzyme. Also the efficiency of collection of the two systems may not be identical and the analytical systems used may not have had the same specificity profiles. Further studies are planned to obtain additional correlation data between these two systems in industry.

Acknowledgements

Partial funding is acknowledged from Unilever, Procter and Gamble, Novozymes and Genencor. The massive contribution to this study of Robert Cumming who died shortly after its completion is acknowledged.

References

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Footnote

We report with regret that Robert Cumming died in 2002.

This journal is © The Royal Society of Chemistry 2007