Lurdes I. B.
Silva
*a,
Alexandre V.
Panteleitchouk
a,
Ana C.
Freitas
a,
Teresa A. P.
Rocha-Santos
a and
A. C.
Duarte
b
aISEIT/Viseu – Instituto Piaget, Estrada do Alto do Gaio, Galifonge, 3515-776, Lordosa, Viseu, Portugal. E-mail: lsilva@viseu.ipiaget.org; Fax: +351 232910183; Tel: +351 232910100
bCESAM & Department of Chemistry, University of Aveiro, 3810-193, Aveiro, Portugal. Fax: +351 23437084; Tel: +351 23437036
First published on 8th October 2009
Leachates derived from landfill constitute a serious environmental concern as a variety of pollutants can leak from the landfill sites with potential risk of groundwater pollution. Benzene, toluene, ethylbenzene, p-xylene, m-xylene and o-xylene (BTEX) are pollutants widely found in landfill leachate and therefore the development of analytical methodologies which can provide a rapid and simple measurement of these compounds is of great interest. This paper reports an optical fibre (OF) sensor for environmental applications, namely for BTEX determination in landfill leachate samples.Firstly the analytical signal of the developed OF sensor was evaluated regarding some operational variables affecting the deposition of the sensitive siloxane film (type of siloxane cladding, deposition technique, number of cycles for deposition, cure temperature and experimental conditions for stabilization) in order to achieve a high sensitivity of the analytical system. Secondly, the OF based sensor was applied to landfill leachate samples for detection and quantification of BTEX. The obtained results have been compared to the ones obtained by the method based on a gas chromatography-flame ionization detector (GC-FID).The developed OF methodology showed notable analytical advantages, such as high analytical sensitivity and accuracy, good linearity and stability of the analytical signal, and detection limits in the order of a few nanograms (raging from 0.9 to 1.4 ng) for BTEX determination.
Different instrumental methodologies have been implemented to landfill leachate analysis, regarding the determination and characterization of the organic composition of this environmental matrix. Some of the most widely used systems rely on gas chromatography (GC) coupled to: mass spectrometry (MS), electron capture detector (ECD), flame ionization detector (FID) and photoionisation detector (PID).1 These methodologies usually require a sample pre-treatment or analyte pre-concentration. An alternative to the classical liquid–liquid techniques, which requires the use of large quantities of extraction solvents, solid phase extraction (SPE),4purge and trap5 and solid phase microextraction (SPME)6 have been used for analyte extraction of landfill leachates.
The investment in analytical methodologies which provides in situ measurements is imperative for landfill pollution control, since conventional analytical methods can lead to volatile losses during sampling and transport procedures.
Optical fibre (OF) sensors have a great potential for detection and monitoring of volatile organic compounds (VOCs), including BTEX, since they show several analytical advantages, such as low cost compared with the conventional laboratory apparatus, immunity to electromagnetic fields, high sensitivity and accuracy, multiplexing capabilities, ruggedness and portability in a harsh and hazardous environment.7 Additionally, they can also be suitable and advantageous for remote detection, continuous measurements, in situ and real-time monitoring of BTEX at a very high safety level. In this field Silva et al.8 have developed an OF sensor for remote monitoring of BTEX in indoor atmospheres of industrial environments. In summary, OF sensors constitute a very important and useful tool in many technological fields, namely environmental control, with remarkable analytical advantages.9–14
This work aims to develop the application of an OF sensor for direct measurements of BTEX in landfill leachates, with an expected analytical performance comparable to a classical methodology for BTEX measurement based on a gas chromatography-flame ionization detector (GC-FID).
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Fig. 1 Experimental set-up of the OF sensor system (F = flowmeter; IC = injection cell; NR = narrowed region; OC = optical coupler; OF = optical fibre; PC = laptop for data acquisition and processing; PF = fused silica fibre coated with PDMS; TH = tape heater; TT = Teflon tube; V1, V2 and V3 = Valves). |
For the sensor system calibration, the BTEX liquid mixture was injected with a micro-syringe (Hamilton) at the top of a glass cell (injection cell) with a controlled temperature of 150 °C by a coiled tape heater (TH, Cole Parmer). After vaporization the analytes were carried by a continuous stream (25 mL min−1) of nitrogen (N45, Praxair, Portugal), controlled with a flowmeter (Sigma, Spain) to the column and finally to the analytical tube. The miniaturized glass column containing a fused silica fibre coated with a film of polydimethylsiloxane (PDMS) was surrounded by a second tape heater and constitutes the separation or adsorption/desorption system component. At the adsorption step the V1 is open for injection cell-column direction, while V3 is closed for the direction of column-analytical tube way. The valves position allows the adsorption of analytes at the separation component preventing the flow of analytes into the detection component, at this stage. The analyte molecules are thermally desorbed by increasing the temperature of the tape heater, which surrounds the column, by a temperature program controlled with home-made software. The tape heater starts at 25 °C with a program rate of 30 °C min−1 until 75 °C and 10 °C min−1 until 150 °C. The temperature program rate used was previously selected taking into account the best analytical performance (sensitivity and selectivity) of the OF sensor vs. temperature program rate or heating pattern. At this stage V2 is closed and V3 is open in the column-analytical tube direction, allowing the flow of analytes to the detection component of the analytical device.
The detection system component includes:
(a) the sensor head which constitutes a 15 mm long uncladded optical fibre section, onto which a nanometric polymeric film was deposited on the end. The sensor head preparation consisted of: firstly, removing the silicone passive OF cladding on a few millimetres length using a buffer stripper, and then, on the immersion of this OF section in a solvent (dichloromethane); secondly, adjusting the uncladded OF section to 15 mm using a Cleaver V6 (from Future Instrument) precision fibre cleaver and checking the cleanliness of the OF surface by optical microscopy; and finally, on covering the OF with the sensitive film of siloxane. This sensitized OF section was introduced through a Teflon plug inside the 7.7 cm long glass tube with a narrowed region of a few millimetres (analytical tube) centred with the sensor head. The choice of the sensor head length was based on the high analytical signal obtained for a sensor head length of 15 mm, during a study of the sensor behaviour for an analytical system constituting of sensor heads with different lengths (5, 15, 20 and 30 mm). A monomode optical fibre pigtail, core and cladding diameters of 9 and 125 µm, of a directional 50:50 Y coupler were used;
(b) a laser diode (AC/DC power or 9 V battery power, 1 mW output) set at a wavelength of 1550 nm (Oz Optics, Canada) for interrogation signal generation; and
(c) a photodiode (110/220V AC 50/60 Hz Universal power supply or battery power) also from Oz Optics for measurements of the reflected optical power changes.
The optical power guided through the fibre is reflected at the fibre/polymer interface and the exposure of the polymeric film to organic vapours inside the analytical tube causes a change in its refractive index leading to a variation of the light power.
For calibration of the OF device, five repeated measurements were performed for each different amount (40, 50, 60, 70 and 80 ng) of the BTEX standard mixture.
For landfill leachate sampling, the injection cell was replaced by a pump which provides a continuous stream of sample through the separation system component in which adsorption and desorption phases took place, being the experimental lay-out similar to the one described for the calibration step. Thus the analyte molecules are firstly adsorbed onto the PDMS fibre and then thermally adsorbed by increasing the tape heater temperature at the glass column. At the same time the V3 is open in the column-analytical tube direction allowing analyte detection.
For the assessment of the influence of some operational conditions regarding sensitive film deposition in the analytical signal, the experimental set-up was simplified by directly connecting the injection cell to the analytical tube with the main propose of reducing the total time of analysis. Since these studies were carried out using toluene as a proxy of aromatic compound, no selective detection was required.
In this section the OF sensor was tested for three different sensitive coatings: PMTFPS, PDMSHEPMS and PDMS; since different transducing materials promote different sensitive responses to organic compounds. Fig. 2a shows the sensor response obtained for toluene, using an OF sensitized with the three different polymeric coatings. The analytical signal amplitude decreases in the following sequence: PMTFPS > PDMSHEPMS > PDMS. The detection limits were estimated19 as 0.8 ng for a sensor with PMTFPS, and 0.9 ng for a sensor coated with either PDMSHEPMS or PDMS film.
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Fig. 2 Analytical signal (a) and SEM images (b) of an OF surface coated with polymeric films of PMTFPS, PDMSHEPMS and PDMS (OF = coated optical fibre; SS = SEM stage). |
The different polymers used were characterized by scanning electron microscopy (SEM) regarding their film's morphology. The SEM analyses were performed in an Aspex SEM 1200024. The results obtained by SEM analysis, as shown in Fig. 2b, suggest that the OF surface shows different morphological characteristics for the three different polymers under study. The most homogeneous film was obtained for PMTFPS showing a very uniform and regular texture. The PDMSHEPMS film shows a more irregular structure with small beads (dark areas with spherical shape) distributed by the whole covering area. The PDMS film shows some large beads, especially on the outlying OF surface.
The highest analytical signal amplitude of the OF sensor coated with PMTFPS, could be due to the polarizability of this polymeric material. The fluorine atoms in PMTFPS promote polarizability and consequently enhance interactions with polarizable compounds such as toluene, resulting in a higher change of optical power and therefore higher analytical signals. This increase of the analytical signal and sensitivity, due to the use of transducer materials with a high potential for polarizability, has already been reported by Abdelmalek et al.20 during a comparison of the performance of OF sensors sensitized with porous silica films and phenyl-modified porous silica films.
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Fig. 3 Sensor response after injection of 0.05 μg of toluene using an OF coated with a polymeric film deposited by different coating techniques (dip-coating, constant rate, spray) and SEM images of an OF coated with a polymeric film deposited by the three coating techniques (OF = coated optical fibre; SS = SEM stage). |
In summary, from the SEM images shown in Fig. 3 it is possible to infer that the film obtained with the SP technique would lead to an uniform distribution of the polymeric material and consequently to the best analytical signal of the OF sensor.
1 cycle | 3 cycles | |
---|---|---|
Film thickness (nm) | 2 | 8 |
Sensitivity (dB µg−1) | 891 | 305 |
Analytical signal for 0.06 µg of toluene (dB) ± standard deviation of five replicates | 28.6 ± 0.2 | 16.6 ± 0.4 |
Response time (s) | 18 | 22 |
Recovery time (s) | 5 | 8 |
Detection limit (ng) | 0.8 | 1.4 |
The analytical system constituted an OF coated with a polymeric film deposited in 1 coating cycle, shows a higher sensitivity (891 dB µg−1) and lower detection limit (0.8 ng) compared to the values obtained for an analytical system with a polymeric film deposited in 3 coating cycles (sensitivity and detection limit of 305 dB µg−1 and 1.4 ng, respectively). Moreover, the OF sensor coated with a 2 nm polymeric film (1 coating cycle) shows a faster response, and recovery time than the OF sensitized with 3 coating cycles. The results could be explained taking into account how the sensitive film thickness affects the analyte molecules adsorption and interaction which take place at the organic vapour/sensitive film interface.21
The sensing mechanism of the OF sensor is based on the sensitive polymeric film deposited onto the uncladded section of the OF end surface, which suffers a reversible change in its optical properties (refractive index) when exposed to the analyte molecules, leading to a detectable modulation of the light power guided through the OF. Thus the exposure of the polymeric film to the organic vapour inside the analytical tube causes a change in the reflected light power, which was measured as the analytical signal. The reflected optical power is determined by both Fresnel's law21 at the interface fibre core/sensing layer, and evanescent wave20,22 of the light on the 15 mm sensitized fibre.
T = 25 °C | T = 70 °C | T = 140 °C | |
---|---|---|---|
Determination coefficient (r2) | 0.9968 (p < 7.72 × 10−5) | 0.9998 (p < 1.33 × 10−6) | 0.9937 (p < 2.11 × 10−4) |
Standard error | 0.787 | 0.238 | 1.28 |
Sensitivity (dB µg−1) | 760 | 891 | 884 |
Linear working range (µg) | 0.06–0.10 | 0.04–0.08 | 0.08–0.12 |
Detection limit (ng) | 3.1 | 0.8 | 4.3 |
The OF system constituted by a polymeric film cured at 140 °C shows a higher detection limit and standard error, thus it is not adequate for OF sensor purposes. Moreover the optical patch cord showed structural damages maybe due to partial charring after exposure to 140 °C during 24 h, which could lead to light scattering and decrease the patch cord resistance. On the other hand, low temperatures (25 °C) for polymeric film curing, are also not appropriate since this analytical system shows a poor overall analytical performance when compared to a system with a polymeric film cured at moderated temperatures.
A set of experiments were performed in order to establish the operational conditions for stabilization of the polymeric film, which allows the best analytical signal. Firstly, an OF coated with a polymeric film (PMTFPS at 0.01% in DCM) deposited by SP, cured at 70 °C during 24 h was tested immediately for toluene detection, without any stabilization phase. Secondly, an OF also coated with a polymeric film and cured at 70 °C during 24 h was stabilized for another 24 h at room temperature; in this experiment the stabilization phase was performed without gas flow. Thirdly, an OF was prepared in the above mentioned operational conditions for deposition, cure and stabilization, but with a constant flow (14 mL min−1) of nitrogen during the stabilization phase. Fig. 4 shows the OF sensor baseline (optical signal recorded without organic vapours injection) and the SEM images collected for the OF surface produced for each of the above described experiments. It is possible to conclude that smooth polymeric films with high homogeneity—achieved in this experiment by increasing the time of the stabilization phase and introducing a constant flow of an inert gas in this phase—reduces the sensor system noise. In fact the sensor baseline becomes more stable, that is, with no significant optical power changes, as the stabilization conditions have been appropriately chosen.
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Fig. 4 Optical signal and SEM images obtained for an OF surface coated with a polymeric film stabilized at different operational conditions: (a) polymeric film without stabilization; (b) polymeric film stabilized during 24 h without gas flow; (c) polymeric film stabilized during 24 h with a constant gas flow (OF = coated optical fibre; SS = SEM stage). |
The SEM images of the OF surface suggest that: (a) the fibre stabilization time is an important parameter concerning polymeric film uniformity and; (b) the stabilization stage with a nitrogen flow provides a smoother layer at the OF surface with a uniform and regular texture. The OF surface coated with a non stabilized polymeric film showed regions with different topographical contours and spot heights (Fig. 4a), which become less apparent in an OF with a polymeric film stabilized during 24 h without and with gas flow (Fig. 4b, and Fig. 4c, respectively).
The results displayed in Fig. 5 show an analytical system with high sensitivity and linearity (Fig. 5a) in an adequate range of concentrations of BTEX compounds.
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Fig. 5 Sensor response obtained during BTEX analysis: (a) calibration curves obtained with the OF sensor for injections of BTEX between 0.04 and 0.08 µg; (b) optical power decrease obtained for a BTEX mixture of 0.05 µg; (c) sensor response (mean and standard deviation of five repeated evaluations) for 0.06 µg of BTEX during four weeks. |
The total analytical time was found to be 9 min for the seven completely separated compounds detected, as shown in Fig. 5b. The OF system provides a faster BTEX analysis than the one performed by the GC-FID method, which requires an analytical time of around 30 min for each single run. Besides, the GC-FID method requires a large time to perform the sample pre-treatment, as recommended in method 5030B15 by the US EPA.
The developed OF sensor shows different sensitivity for the six aromatic hydrocarbons analysed, increasing in the following order: 751 dB µg−1 for benzene < 892 dB µg−1 for toluene < 933 dB µg−1 for ethylbenzene < 941 dB µg−1 for p-xylene < 949 dB µg−1 for m-xylene < 964 dB µg−1 for o-xylene. The analytical signal depends on the chemical interactions which can take place between the sensitive cladding (polymeric film) and the analyte molecules, modifying the refractive index of the polymeric film and consequently the reflected optical power. The intensity of the modulated reflected signal is proportional to the amount of analyte present at the analytical tube and also depends on the interaction between different physical and chemical factors, such as the waveguide, sensitive cladding and analyte properties, and also the molecular interactions that could occur between the analyte molecules and the sensitive OF cladding. In this way, the different analyte properties, such as the boiling temperature (80.1 °C for benzene < 110.6 °C for toluene < 136.2 °C for ethylbenzene < 138.4 °C for p-xylene < 139.1 °C for m-xylene < 144.4 °C for o-xylene) and vapour pressure (95.2 for benzene > 28.4 for toluene > 9.6 for ethylbenzene > 8.8 for p-xylene > 8.4 for m-xylene > 6.7 for o-xylene, in mmHg at 25 °C) are sufficiently different to explain the significant differences of sensitivities observed for each organic compound analyzed. This observation is in good agreement with the behaviour of the OF polymer based sensors reported by Silva et al.8,17 and Abdelmalek et al.20 for different VOCs detection.
The estimated detection limit values obtained with the reported sensor for benzene, toluene, ethylbenzene, p-xylene, m-xylene and o-xylene were 1.4, 0.8, 1.0, 0.9, 1.0 and 0.9 ng, respectively. These values highlight the high potential of the OF sensor for BTEX monitoring at trace levels.
In order to evaluate the stability of the developed OF methodology an ANOVA was applied, using SigmaStat 3.023 to all data (displayed in Fig. 5c) on benzene, toluene, ethylbenzene, m-xylene, p-xylene and o-xylene, and it showed that there is not a statistically significant difference between weeks (p = 0.267, 0.448, 0.966, 0.658, 0.753 and 0.938 for benzene, toluene, ethylbenzene, p-xylene, m-xylene and o-xylene, respectively), that is, the difference in the mean values among the different weeks is not great enough to exclude the possibility that the difference is just due to random variability in BTEX analysis.
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Fig. 6 Results obtained for five actual samples of landfill leachate analyzed by the OF sensor and the GC-FID method. |
The comparison of the means of the five actual samples analyzed by both the OF sensor and the GC-FID method, shows that there is no statistically significant difference between the results obtained for each sample (p = 0.335, 0.880, 0.810, 0.660, 0.255 and 0.489 for benzene, toluene, ethylbenzene, p-xylene, m-xylene and o-xylene, respectively) by the two analytical systems.
The total BTEX concentration is below 2 µg L−1 for the five analyzed actual samples. The landfill leachate samples were collected in different places at the same Portuguese landfill cell site and therefore it is understandable that there are similar average values of BTEX in the different analyzed samples.
The aromatic compound concentrations found in the analyzed landfill leachate are included in the lower range of BTEX concentrations reported in other studies regarding landfill leachate analysis and chemical characterization.24,25 According to the studies referred to above, the BTEX concentration in landfill leachate can range from centesimal values to thousands of µg L−1, depending on the waste disposal practices, management and landfill technologies, general waste composition, and waste age.25
In order to test the developed OF analyzer for interferences that could be present in the leachate matrix from landfill, the effects of naphthalene and n-propylbenzene, used as an example of interference compounds, on the analytical signal were also evaluated. The compounds tested produce peaks, but in different analytical time windows to the compounds of interest, and therefore did not exhibit any interference in the analytical signal.
The developed methodology showed an analytical performance for BTEX detection in landfill leachates comparable to the GC-FID method. Additionally, the ease of assembling and compact design of the optical device confers high potential for continuous and in situ measuring of BTEX compounds to the developed analytical system.
This journal is © The Royal Society of Chemistry 2009 |