Previous Article | Next Article ![]()
Applied and Environmental Microbiology, November 2004, p. 6871-6874, Vol. 70, No. 11
0099-2240/04/$08.00+0 DOI: 10.1128/AEM.70.11.6871-6874.2004
Copyright © 2004, American Society for Microbiology. All Rights Reserved.
Department of Biomedical Engineering, University of Groningen, Groningen, The Netherlands
Received 18 May 2004/ Accepted 4 July 2004
|
|
|---|
|
|
|---|
Biofilm formation commences with the adhesion of microorganisms to an implant surface. This initial microbial adhesion has been extensively studied and is generally believed to depend on the physicochemical properties of the microbial and biomaterial surfaces, such as hydrophobicity and charge (10). Previously, it was demonstrated that >75% of initially adhering staphylococci could be stimulated to detach from surgical stainless steel by the application of an electric current of <100 µA, either a direct current (DC) or block current, while yielding a 2-log reduction in the viability of the remaining organisms (20). It was suggested that the reason for the higher detachment percentage was caused by electroosmotic fluid flow directed to and from the surface (17). The alternating field causes the hydrated ions to move along the applied field, dragging water with them. This fluid flow causes an extra force that stimulates detachment.
The influence of electric currents on the detachment of microorganisms from conducting surfaces during the growth stage of biofilm formation has not yet been studied, but it could be entirely different from the effects seen on initially adhering organisms. During growth, not only do microorganisms multiply in large numbers, but adhesion also proceeds from a more reversible to a more irreversible state through the excretion of extracellular polymeric substances (EPS), which act as a glue between the biofilm and the substratum surface, by the adhering organisms.
Therefore, the aim of this study was to determine whether it is possible to stimulate bacterial detachment of a growing Staphylococcus epidermidis biofilm from surgical stainless steel by using DCs and block currents (50% duty cycle, 1 Hz) of 60 and 100 µA.
|
|
|---|
Stainless steel.
AISI 316 LVM stainless steel (Stryker Corp., Kiel, Germany) was ground down to grit number 1200 and subsequently polished with 6- and 3-µm-diameter water-based diamond suspensions (Metadi 3- and 6-µm-diameter diamond suspension and Trident polishing cloth; Buehler, Lake Bluff, Ill.) for 3 and 1.5 min, respectively. Grinding and polishing were done with a polishing machine with a 30-N load and oppositely rotating axes (Phoenix Beta and Vector grinder-polisher; Buehler). The polished steel was cleaned by a 5-min sonication in 2% alkaline cleaning agent (RBS35 in water; Omniclean) followed by a thorough rinsing with tap water, sonication in ethanol, and rinsing in Millipore-filtered demineralized water. After being cleaned, the steel was passivated according to American Society for Testing and Materials standard F86-91, thoroughly rinsed with Millipore-filtered demineralized water, and dried in an oven at 80°C prior to being used as an electrode surface.
Parallel plate flow chamber and surface growth and detachment experiments.
Bacterial adhesion and biofilm growth as well as subsequent detachment were studied in a parallel plate flow chamber with a distance of 0.6 mm between the top and bottom plates (19). The bottom plate consisted of the surgical stainless steel electrode (area, 21 cm2), while the top plate, employed as a counterelectrode, was made of an indium tin oxide (ITO), DC-sputtered glass (Philips Natlab, Eindhoven, The Netherlands). The ITO-coated glass plates were cleaned in the same way as the stainless steel, and an electrical wire was glued to the surface with silver dag (Electrodag 1415; Acheson, Port Huron, Mich.). Before the flow chamber and electrodes were assembled, each part was sterilized by being submerged in 70% (vol/vol) ethanol. All other parts requiring sterility were autoclaved prior to assembly.
The flow chamber was equipped with a heating element attached to a nickel-coated brass block placed directly in contact with the stainless steel bottom plate. The temperature of the block was kept constant at 36.5°C throughout the entire experiment. Adhering bacteria were observed with a CCD-MXR camera mounted on a metallurgical microscope equipped with a 40x ultra-long-working-distance objective. All fluids used were circulated through the camber by use of a peristaltic pump at a flow rate of 0.012 ml/s (shear rate, 10 s1). PBS was first flowed through the chamber for 40 min, followed by the bacterial suspension, until 106 bacteria cm2 were found adhering to the stainless steel bottom plate, which took approximately 25 min under the experimental conditions applied. Subsequently, the chamber was perfused for 40 min with cell-free PBS to remove planktonic bacteria from the system, followed by the perfusion of growth medium (tryptic soy broth) for 200 min. After perfusion of the growth medium, 10 mM potassium phosphate buffer (pH 7) was directed through the system for 400 min, during the course of which a specific current was applied through the anode and the cathode. The electric current was kept constant during the final 360 min of the experiment with the aid of an LM334Z semiconductor (National Semiconductor Corp., Santa Clara, Calif.) and was driven by a voltage that varied in both frequency and duty cycle, with the stainless steel bottom plate acting as a cathode. The voltage and current applied to the electrodes were both observed with conventional multimeters. The LM334Z output potential was adapted continuously to meet the required and adjusted current, irrespective of the applied voltage to the integrated circuit (IC). The following currents were tested: a 100-µA DC, a 60-µA DC, a 100-µA (50% duty cycle, 1 Hz) block current, and a 60-µA (50% duty cycle, 1 Hz) block current. The limited space in the parallel plate flow chamber did not allow the use of a reference electrode to measure the surface potential. Additionally, a control experiment was done in which the electric current was omitted.
During each experiment, images were taken of bacteria adhering to the stainless steel bottom plate and were stored in the computer to obtain the number of adhering bacteria per unit area versus time during the application of the electric current. All experiments were done in triplicate with separately cultured bacteria and freshly prepared top and bottom plates.
Viability staining.
In order to determine possible effects of the electric current on the viability of the staphylococci that remained adherent after the current application, we operated two parallel plate flow chambers simultaneously with bacterial suspensions taken from the same culture. One flow chamber was used as a control in the absence of an electric current, while the second flow chamber was connected to the current source. During the time of current application, the control flow chamber was perfused with 10 mM potassium phosphate buffer. After the experiment, both chambers were disconnected, filled with staining fluid (Live/Dead Baclight bacterial viability kit; Molecular Probes, Leiden, The Netherlands), and incubated for 15 min in the dark. On different, randomly chosen locations on each surface, micrographs were taken with a confocal laser scanning microscope (CLSM) with a 40x ultra-long-working-distance objective, with the microscope set for fluorescein isothiocyanate (excitation at 488 nm and emission at 500 to 600 nm) and tetramethylrhodamine isocyanate (excitation at 543 nm and emission at 560 to 700 nm) to show dead and live bacteria, respectively. Results were expressed as percentages of dead bacteria.
|
|
|---|
![]() View larger version (16K): [in a new window] |
FIG. 1. Examples of time series involved in the adhesion and growth of S. epidermidis HBH276 biofilms and their detachment from stainless steel by the use of two different currents ( , 100-µA DC; , 100-µA [50% duty cycle, 1 Hz] block current) in 10 mM potassium phosphate buffer. The four dashed lines indicate the four consecutive phases of the experiments. (A) Bacterial deposition (25 min); (B) perfusion with buffer (40 min); (C) growth medium (200 min); (D) perfusion with buffer (40 min); and (E) application of electric current during perfusion with buffer (360 min).
|
|
View this table: [in a new window] |
TABLE 1. Voltage differences between the cathode and the anode and total detachment percentages and detachment rates of S. epidermidis HBH276 biofilm upon the application of different electric currents in a 10 mM potassium phosphate buffer after 200 min of growth
|
![]() View larger version (10K): [in a new window] |
FIG. 2. Total detachment versus voltage difference between the cathode (stainless steel) and the anode (ITO-coated glass) during electric current-stimulated detachment of S. epidermidis HBH276 biofilms. Error bars denote the standard errors for three experiments with separately cultured bacteria and freshly prepared plates.
|
![]() View larger version (45K): [in a new window] |
FIG. 3. CLSM micrographs of bacteria adhering to stainless steel and stained with a live-dead stain after experiments with and without the application of an electric field. Green, live cells; red, dead cells. (A) Control experiment with no electric current; (B) 100-µA block current; and (C) 100-µA DC.
|
|
|
|---|
Previously, it was shown that initially adhering bacteria, which interact solely through Lifshitz-Van der Waals, electrostatic, and acid-base interactions, could be stimulated to detach by the use of DCs and block currents. The block currents yielded higher detachment percentages than DCs due to the electroosmotic fluid flow (17). However, when biofilm bacteria are concerned, DCs cause higher detachment percentages than their counterpart block currents. This suggests that the influence of electroosmotic fluid flow on biofilm bacteria is absent. When adhering bacteria start to grow and excrete EPS, adhering bacteria become trapped in a more-or-less gel-like structure (6, 9, 12). The EPS matrix prevents water and entrapped particles, such as hydrated ions, to move freely. Because the ions are limited in their movement, the electroosmotic fluid flow is small or even absent, despite the applied electric field, and thus will not cause additional detachment. However, the absence of electroosmotic fluid flow cannot explain the fact that the detachment stimulated by block currents is less than that stimulated by DCs. It is likely that the decrease in detachment percentage with decreasing potentials (Fig. 2) is a direct consequence of a decrease in the Stern potential and therefore in the Gibbs interaction energy, as outlined in the DLVO (Derjaguin, Landau, Verseug, and Overbeek) theory (13).
The potential varied linearly with the applied current, yielding an electric resistance of the biofilm of 7,700 ± 500
. This resistance was constant throughout each experiment, regardless of subsequent bacterial detachment, suggesting that the electric resistance is mainly caused by EPS remaining on the substratum surface after detachment of the adhering bacteria (7).
To summarize, we have described a method by which bacterial biofilms can be stimulated to detach from surgical stainless steel by use of a small electric current to disconnect the link between the biofilm and the conducting substratum (9, 10). This method may have an application in the medical field, as it can be used in combination with conventional pin site care to prevent or cure infections by applying the current between a circular electrode placed around the pin and the pin itself. The conventional cleaning technique with water and soap can provide the flow needed for bacterial transportation, and between cleanings the current can kill the adhering bacteria.
|
|
|---|
This article has been cited by other articles:
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Copyright © 2009 by the American Society for Microbiology. For an alternate route to Journals.ASM.org, visit: http://intl-journals.asm.org | More Info»