Xavier
Muñoz-Berbel
*a,
Núria
Vigués
b,
Montserrat
Cortina-Puig
a,
Roger
Escudé
a,
Cristina
García-Aljaro
a,
Jordi
Mas
b and
Francesc Xavier
Muñoz
a
aCentre Nacional de Microelectrònica (IMB-CSIC), Campus Univ. Autònoma de Barcelona, Esfera UAB, 08193,, Bellaterra, Barcelona, Spain. Fax: +34 93 580 14 96; E-mail: fxmber@gmail.com; Fax: +34 93 594 77 00
bGrup de Microbiologia Ambiental, Universitat Autònoma de Barcelona, Campus UAB, E-08193, , Bellaterra, Spain
First published on 28th May 2010
A previously reported methodology is applied to monitor the concentration of bacterial suspensions from an incubator using impedance spectroscopy and platinum electrodes. The interface capacitance, commonly fitted as a constant phase element, CPEi, was found sensitive to the suspended bacteria concentration after short exposure times in a wide range of concentrations (from 102 to 107 colony forming units per mL, CFU mL−1) with a limit of detection of 10 CFU mL−1. The effect of the substances released during bacterial growth (enzymes, toxins, exopolysaccharide, etc.) in the CPEi magnitude was found to be negligible and samples only containing cells washed with saline solutions showed results comparable to those obtained using aliquots directly extracted from the bacterial incubator. This impedimetric approach showed correlation with classical microbiological methods for measuring bacterial concentration such as plating onto agar, optical density and fluorescence microscopy. The impedimetric approach was simplified to a single frequency analysis by selecting the optimal frequency for the measurement.
Conventional methods for the detection of viable bacteria typically rely on the culture-based assays with excessive sample treatment and long incubation times. With the advent of modern molecular biological techniques, many new approaches have been investigated for this purpose, such as bioluminescent assays,4 Fluorescent In Situ Hybridization (FISH),5 optical tweezers,6 nucleic acid amplification method (Polymerase Chain Reaction, PCR),7 Reverse Transcription-Polymerase Chain Reaction (RT-PCR)8,9 and Nucleic Acid Sequence-Based Amplification (NASBA).10 Although these methods can offer high sensitivity, they are either time-consuming or rely on laboratory facilities, which limit their application for rapid operation and on-site analysis. In recent years, a number of new methodologies have been applied to the detection of planktonic bacteria. These include voltamperometry,2 micromechanical oscillators11 and Quartz Crystal Microbalances (QCMs).12 These methods demonstrate good sensitivities (around 102-103 CFU mL−1) with short measurement times. However, the complexity of the assay, which frequently requires the manipulation of fragile or biologically delicate materials, renders this method vulnerable to error.
Recently in our group, a new approach for monitoring bacterial concentration has been developed.13,14 The detection scheme is based on the changes produced in the electrode-solution interface by bacterial attachment in the initial stage of the electrode surface colonization (early reversible bacteria attachment). Previous works of the group showed that bacterial attachment to platinum electrodes could be used for suspended bacteria quantification. Next, this approach was probed to be able to quantify different bacterial species (Pseudomonas aeruginosa and Staphylococcus aureus) and even yeasts (Saccharomyces cerevisiae) following the same measurement protocol.15 In combination with an artificial neural network, this approach was found to be selective enough to distinguish between binary mixtures of microorganisms after a suitable training process.
In this paper, the approach previously described is applied to the monitoring of real bacterial samples from an incubator where Escherichia coli (E. coli) are growing under optimal experimental conditions. Before its application to the control of the bacterial concentration of real samples extracted from the incubator, the influence of the products released during the bacterial metabolism (secreted proteins, such as enzymes or toxins, exopolysaccharide, lipopolysaccharide, cell debris, peptidoglycan or waste products) in the impedimetric measurement is investigated. The impedimetric approach is compared with classical microbiological methods, such as plating onto agar (the classical method for counting bacteria, very accurate but extremely tedious),1 epifluorescence microscopy counting (a standard method, faster than plating but also tedious)16 and optical density (the most employed method for the on-line monitoring of bacterial concentration).1 This approach was also simplified to a single frequency analysis.
For the monitoring of the bacterial growth, 1 mL of the suitable bacterial suspension was inoculated into a 1.5 L water-jacketed glass reactor containing ABMM (under sterile conditions) to achieve the initial concentration of interest. During bacterial growth, the reactor was thermostatically kept at 37 °C with constant agitation [MR 2000 (Heidolph, Germany)] and aeration [BioFlo (New Brunswick Scientific, New Jersey, USA)]. Under these conditions, E. coli grew aerobically with a duplication time experimentally found between 30 and 40 min. After the inoculation, no nutrients were added into the reactor (batch process).
Using the aseptic acquisition system, aliquots of 20 mL were extracted from the incubator at 30 min intervals and directly measured using impedance spectroscopy, optical density and fluorescence microscopy. After 20 min of centrifugation at 4388 × g [Sigma 4–10 centrifuge (Sigma, Switzerland)] the secreted substances (supernatant containing secreted proteins, such as enzymes or toxins, exopolysaccharide, lipopolysaccharide, cell debris, peptidoglycan or waste products from the metabolism) and the suspended cells (pellet cleaned and re-suspended in sterile ABMM) were separately measured using impedance spectroscopy. Biological samples were stored at 4 °C to slow growth until measurement. All of the manipulations were performed under sterile conditions.
Bacterial suspensions were introduced to the electrochemical cell, which was thermostatically kept at 4 °C. Impedance measurements were made after 15 s of exposure for the calibration solutions, direct (non-centrifuged samples), secreted substances or suspended cells samples. After the measurement, the electrochemical cell, including electrodes, was cleaned with water and sterilized with ethanol (Panreac, Spain). Ethanol residues were eliminated by washing another time with water.
Fig. 1 Admittance complex plane plot for bacterial suspensions extracted from the incubator 30 and 270 min after the inoculation of the bacterial starter suspension. Impedance data were fitted using the equivalent circuit shown inset. The experimental impedance spectra (points in the plot) and the ideal impedance spectra from the fitting (line in the plot) are shown. Also the spectra corresponding to the culture medium without bacteria is added in each plot as control (red line). Below, the calculated values and errors of each element from the fitting are detailed. |
Fig. 1 shows the admittance Nyquist plots and the magnitude and errors of each parameter of the electrical equivalent circuit for bacterial suspensions extracted from the incubator 30 and 270 min after the inoculation of the stock bacterial suspension used as starter. Regarding the fitting, from the elements of the equivalent circuit only the magnitude of the CPEi (Ki-T in the figure) was found to change with time as a consequence of bacterial growth in the incubator. The fact that the other parameter of the electrical equivalent circuit related to the CPEi, Ki-P, did not change with bacterial concentration was not surprising since, although this parameter depends on several factors, the roughness of the electrode seems to be one important aspect,20 changing from 1 for ideally flat electrodes to 0.5 for very rough ones.
(1) |
Fig. 2 Representation of the normalized Kiversus the incubation time for total samples containing both cells and released substances (total samples), samples only containing released substances (secreted substance samples), samples containing only cells (washed cell samples) and secreted substance samples after filtration (after filtration). |
A constant RS value was obtained with time for total samples (samples containing both suspended cells and secreted substances), cells samples (samples containing re-suspended bacteria) and secreted molecule samples (samples mainly containing secreted proteins, such as enzymes or toxins, exopolysaccharide, lipopolysaccharide, cell debris, peptidoglycan or waste products from the metabolism) with a magnitude of 445 ± 19 Ω. Sample conductivity was measured separately with a conductance meter and found to be sample invariant, which confirmed that, under the experimental conditions previously exposed, the conductivity of the medium did not vary with the E. coli growth (or with the secretion of molecules and wasting products from the metabolism).
K i -T changed with time in total and cells samples. The increase in CPEi coincided with that reported in previous works of the group where Ki-T was found to correlate very well with the concentration of washed cells between 102 and 107 CFU mL−1.13,14 Briefly, the attachment of bacteria, considered to be behaving as simple charged colloidal particles during the very early attachment stage, was thought to modify the structure of the double layer at the electrode interface. Particularly, bacteria attachment to the electrode surface may decrease the Debye length at the electrode double layer, causing the increase in CPEi. However, the correlation of this change with time, and thus with bacteria growth, was slightly better in the total samples. This is likely due to the centrifugation step used to prepare the cell samples where some bacteria may be lost.
When considering samples only containing secreted molecules, a random oscillation in the CPEi magnitude was recorded, probably caused by the presence of bacteria since the variation decreased after filtration in 0.2 μm pore size GTBP filters. Thus, substances produced and secreted by E. coli during bacteria growth under the experimental conditions discussed herein did not modify the CPEi magnitude either.
Fig. 3 Representation of the normalized Kiversus the logarithm of the suspended concentration of bacteria. This calibration curve was used for converting capacitance values into bacteria concentrations. |
Results from the comparison of both approaches are plotted in Fig. 4. A good method should display comparative lines with high correlation and a slope equal to one with zero intercept. As illustrated in Fig. 4, in both cases impedance spectroscopy measurements showed good correlation with comparison lines practically indistinguishable from the theoretical values. However, better results were obtained in the case of total samples directly extracted from the incubator. As discussed above, this is likely due to the centrifugation step. Some cells remained in suspension after centrifugation, introducing variability in the impedance measurement.
Fig. 4 Representation of the predicted bacteria concentration magnitude (obtained from total (A) and cells samples (B) when using impedance spectroscopy) against the expected ones (from plating onto agar). The dotted line represents the theoretical comparison line y = x. |
Finally, the Student's t-test for paired samples was used for checking whether there were significant differences between the predicted and the expected values, 95% confidence value being considered significant. The tabulated values of the t (ttab), 2.26 and 2.20 for total and cells samples respectively, were always found to be bigger than the calculated ones (0.21 and 0.85 for total and cells samples, respectively). Thus, no significant differences between the predicted and the expected values were obtained. Again, better results were achieved when using total samples directly extracted from the incubator.
Impedance, optical density and epifluorescence microscopy measurements were made as described in Section 2. Impedance spectroscopy suspended concentration values were obtained by correlating the response magnitude with the calibration curve shown in Fig. 3. Optical density suspended concentration values were similarly obtained by correlation with an appropriate calibration curve (data not shown).
The impedance spectroscopy approach showed great fidelity when compared to epifluorescence microscopy (Fig. 5) in a wide range of concentrations (from 102 to 106 CFU mL−1). However, it could not be compared with the optical density method since the linear range of both approaches did not coincide, they were found complementary. The impedimetric approach is faster, simpler and less tedious than the epifluorescence microscopy method, although epifluorescence microscopy is much more accurate (since it is directly proportional to the bacteria concentration while the impedance approach is proportional to the logarithm of the concentration) and has a better limit of detection.
Fig. 5 Representation of the variation of the concentration values from impedance spectroscopy, epifluorescence microscopy and optical density measurements with the incubation time. |
Fig. 6 Representation of the variation of the phase angle (ϕ) with the frequency for a bacterial sample extracted after 60 min of incubation. The slope and the intercept of the comparison plots comparing the predicted bacteria concentration (from impedance spectroscopy) against the expected ones (from plating onto agar) for each frequency under study are also included. |
The phase angle changed from a value close to 0 (at high frequencies) to almost −80 (at low frequencies) with a minimum value at 10 Hz. Considering that the interface capacitance was found sensitive to the bacteria concentration, the ideal frequency for this application would be that one with a phase angle closer to −90. The small differences in the phase angle value in the region from 1 kHz to 10 Hz suggested a deeper analysis. The interface capacitance magnitude at a single frequency was calculated considering that this behaved as an ideal capacitance by using the imaginary magnitude of the impedance at that frequency (Z′′) and the angular frequency (ω) as follows:
(2) |
Recently in our group, a new approach for monitoring bacterial concentration has been developed.13,14 The detection scheme is based on the changes produced in the electrode–solution interface by bacterial attachment in the initial stage of the electrode surface colonization (early reversible bacteria attachment). Previous works of the group showed that bacterial attachment to platinum electrodes could be used for suspended bacteria quantification. Next, this approach was probed to be able to quantify different bacterial species (Pseudomonas aeruginosa and Staphylococcus aureus) and even yeasts (Saccharomyces cerevisiae) following the same measurement protocol.15 In combination with an artificial neural network, this approach was found selective enough to distinguish between binary mixtures of microorganisms after a suitable training process.
This journal is © The Royal Society of Chemistry 2010 |