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W tym Artykule

  • Podsumowanie
  • Streszczenie
  • Wprowadzenie
  • Protokół
  • Wyniki
  • Dyskusje
  • Ujawnienia
  • Podziękowania
  • Materiały
  • Odniesienia
  • Przedruki i uprawnienia

Podsumowanie

This paper shows an original methodology based on the remote actuation of magnetic particles seeded in a bacterial biofilm and the development of dedicated magnetic tweezers to measure in situ the local mechanical properties of the complex living material built by micro-organisms at interfaces.

Streszczenie

Bacterial adhesion and growth on interfaces lead to the formation of three-dimensional heterogeneous structures so-called biofilms. The cells dwelling in these structures are held together by physical interactions mediated by a network of extracellular polymeric substances. Bacterial biofilms impact many human activities and the understanding of their properties is crucial for a better control of their development — maintenance or eradication — depending on their adverse or beneficial outcome. This paper describes a novel methodology aiming to measure in situ the local physical properties of the biofilm that had been, until now, examined only from a macroscopic and homogeneous material perspective. The experiment described here involves introducing magnetic particles into a growing biofilm to seed local probes that can be remotely actuated without disturbing the structural properties of the biofilm. Dedicated magnetic tweezers were developed to exert a defined force on each particle embedded in the biofilm. The setup is mounted on the stage of a microscope to enable the recording of time-lapse images of the particle-pulling period. The particle trajectories are then extracted from the pulling sequence and the local viscoelastic parameters are derived from each particle displacement curve, thereby providing the 3D-spatial distribution of the parameters. Gaining insights into the biofilm mechanical profile is essential from an engineer's point of view for biofilm control purposes but also from a fundamental perspective to clarify the relationship between the architectural properties and the specific biology of these structures.

Wprowadzenie

Bacterial biofilms are communities of bacteria associated with biological or artificial surfaces1-3. They form by an adhesion-growth mechanism coupled with the production of polysaccharide-rich extracellular matrix that protects and stabilizes the edifice4,5. These biofilms are not simply passive assemblages of cells stuck to surfaces, but organized and dynamic complex biological systems. When bacteria switch from planktonic to biofilm lifestyle, changes in gene expression and cell physiology are observed as well as increased resistance to antimicrobials and host immune defenses being at the origin of many persistent and chronic infections6. However, the controlled development of these living structures also offer opportunities for industrial and environmental applications, such as bioremediation of hazardous waste sites, bio-filtration of industrial water or formation of bio-barriers to protect soil and groundwater from contamination.

While molecular features specific to biofilm way of life are increasingly described, the mechanisms driving the community development and persistence remain unclear. Using the recent advances on microscale measurements using scanning electrochemical or fluorescence microscopy, these living organizations have been shown to exhibit considerable structural, chemical and biological heterogeneity7. Yet, until now, biofilm mechanics have been mainly examined macroscopically. For instance, observation of biofilm streamers deformation due to variations in fluid flow rates8,9,  uniaxial compression of biofilm pieces lift from agar medium or grown on cover slides10,11, shear of biofilm collected from the environment and then transferred to a parallel plate rheometer12,13, atomic force spectroscopy using a glass bead and coated with a bacterial biofilm attached to an AFM cantilever14 or a dedicated microcantilever method for measuring the tensile strength of detached biofilm fragments15,16 have been implemented during the ten last years, providing useful information on the viscoelastic nature of the material17. However, it seems likely that information on in situ biofilm mechanical properties is lost when the material is removed from its native environment, which was often the case in these approaches. Moreover, the treatment of the biofilm as a homogeneous material misses the information on the possible heterogeneity of the physical properties within the community. Therefore, the exact implications of the structure mechanics in the biofilm formation and biological traits such as gene expression patterning or chemical gradients can hardly be recognized. To progress towards a microscale description of the biofilm physical properties, new dedicated tools are required.

This paper details an original approach conceived to achieve measurement of local mechanical parameters in situ, without disturbing the biofilm and enabling drawing of the spatial distribution of the microscale material properties and then the mechanical heterogeneity. The principle of the experiment rests on the doping of a growing biofilm with magnetic microparticles followed by their remote loading using magnetic tweezers in the mature biofilm. Particle displacement under controlled magnetic force application imaged under the microscope enables local viscoelastic parameter derivation, each particle reporting its own local environment. From these data, the 3D mechanical profile of the biofilm can be drawn, revealing spatial and environmental condition dependences. The whole experiment will be shown here on an E. coli biofilm made by a genetically engineered strain carrying a derepressed F-like plasmid. The results detailed in a recent paper18 provide a unique vision of the interior of intact biofilm mechanics.

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Protokół

1. Bacteria Culture and Suspension Preparation

  1. Pick a freshly grown colony from a Lysogeny Broth (LB) agar plate, inoculate it in 5 ml liquid LB medium containing 100 µg/ml ampicillin and 7.5 µg/ml tetracycline and incubate it for 5 to 6 hr at 37 °C on a shaking platform.
  2. Then, add 100 µl of the bacterial culture in 5 ml minimum medium (M63B1) supplemented with 0.4% glucose and the same antibiotic concentrations. Incubate this freshly diluted culture overnight at 37 °C on a shaking platform.
  3. After 16 hr of incubation, add 100 μl the overnight culture to 5 ml M63B1, 0.4% glucose. Keep the tube at 37 °C to the shaking platform until a 0.5 OD is reached. The suspension is then ready for injection into the experiment channel for biofilm formation.

2. Magnetic Particle Preparation

  1. Take 10 μl magnetic particles — 2.8 µm in diameter — from the stock and wash them 3x in 190 μl minimum medium with the aid of a magnetic sample rack.
  2. Adjust the particle concentration to 5 x 106 beads/ml. Typically 50 μl of the washed bead solution is mixed with a further 950 µl of M63B1 with 0.4% glucose.

3. Channel Preparation and Biofilm Growth

  1. Channel Mounting
    1. Cut two square (800 µm side length) borosilicate glass capillaries 10 cm long to obtain two 8 cm long pieces.
    2. Glue the two capillary pieces on two glass slides — cut in half first — 2 cm apart with 1 cm overhang on either end as in Figure 1 using a fast-acting cyanoacrylate glue (so called super-glue).
    3. Autoclave the entire setup and the necessary tubing required for further channel connection.
    4. Gather all the sterile materials under a laminar flow hood: i) the mounted channel and trap 1, ii) the tubing and connectors, iii) the two bubble traps — the bubble filter commonly used to secure children's drip-feeding (trap 1) and the home-made bubble trap as a 4 cm long tube of larger diameter (trap 2), iv) clamps, v) 30 ml syringes filled with M63B1, 0.4% glucose, and vi) the waste bottle.
    5. Connect the whole setup with Luer Lock connecters or junctions in the following order: 50 ml M63B1 syringe controlled by the syringe pump, pediatric bubble filter, homemade bubble trap, capillary (Figure 1, panel B), and the tube to the waste bottle. Then fill the setup with sterile M63B1, 0.4% glucose, turning on the syringe pump at a rate of about 10 ml/hr, higher than the experimental rates. Carefully track and eliminate all the bubbles in the circuit.
    6. Flow the medium through the system for 10-15 min; concurrently mix 1 ml of the bacteria suspension at OD 0.5 from Section 1.3 with 1 ml of the washed bead solution prepared in Section 2.2.
    7. Attach (but don't close) clamps to the tubing at two positions: before and after the capillaries. Switch the flow off.
    8. Introduce the bacterial-bead mixture into the capillary after the home made bubble trap using a 1 ml syringe, taking care to hold up the tube ends to prevent air entry. Re-attach the tubing and then close the clamps.
    9. Repeat the same procedure for the second capillary and check all the tubes for bubbles.
    10. Transfer the apparatus to the microscope and allow it to stand for 15-20 min to enable the bacteria to settle and attach to the surface of the capillary. Install the capillary onto the microscope stage with the waste container at a slightly higher level. Place the syringe pump on the counter top beside the microscope. Elevate the bubble trap before the capillary slightly higher than the capillary plane to capture bubbles.
  2. Biofilm Growth
    1. Adjust the flow rate on the syringe pump and start the flow, the biofilm will now develop on the capillary surface during the required period — usually 24 or 48 hr in these experiments.
    2. Focus on the capillary bottom plane and start the time-lapse recording of the sample images — usually an acquisition frequency of 2 images/min will adequately report the biofilm growth. This video monitors biofilm growth post-control (see extracts in Videos 1, 2 and 3).

4. Magnetic Tweezers Installation

  1. Screw the magnetic tweezers on manually controlled X-Y-Z micromanipulators and screw the micromanipulators on the microscope stage to adjust the position of the tweezers relatively to the capillary. Place the tweezers as in Figure 2 to ensure the appropriate magnetic field gradient is generated in the observation zone.
  2. Connect the tweezers to the function generator via the power amplifier to generate a 40 sec period of time made of 24 sec zero signal and 16 sec of 4 A direct current with a trigger sent to the bright field light shutter after 20 sec for signal synchronization providing a sequence of events as in Figure 3.
    Note: These two operations can be achieved at any time between capillary installation and measurement beginning. See experiment overview sketch in Figure 4.

5. Creep Curve Acquisition

  1. Use the xy movement control of the microscope stage to bring the edge of the left-hand magnetic pole and the left-hand edge of the capillary in the same observation field. Take the origin of the analysis referential at the intersection of x- and y-axes defined by the edge of the capillary and the edge of the pole piece, respectively (see Figure 2).
  2. Adjust the vertical position of the capillary using fine focus control knob of the microscope position. Typically the first examined plane is located between 4 to 7 µm above the capillary bottom. Video 1 corresponds to the xy field that has its top left-hand corner at the origin of the spatial referential.
  3. Trigger the 40 sec sequence of events described in section 4.2 and Figure 3 by switching on the current generator and at the same time, manually trigger the image acquisition sequence of Video 1.
  4. Move the capillary to the neighbor right field by a 250 µm translation of the microscope stage to the left and operate as in section 5.3 to generate Video 2 of slice 2 and so on to obtain the required videos. Typically 3 to 4 fields of 250 x 250 µm2 are collected along the x-axis before changing the plane and repeating same operations for the new plane.

6. Force Calibration

  1. Prepare a glycerol solution by mixing 39.8 g of glycerol with 190 µl of bi-distilled water and 10 μl of magnetic particles at a 2 x 109 particles/ml and fill up an experimental channel with this mixture and place it on the microscope stage as described for the biofilm sample.
  2. After installing the magnetic tweezers as indicated in section 4, apply the magnetic force as indicated in section 5.4 and make time-lapse images to extract each single particle velocity (v) and its position in the capillary to derive the calibration file. This file should contain the applied force as a function of its position in the zone of analysis of the capillary according to stokes law, F = 6πRηv (R: radius of the particle).

7. Analysis

  1. Use a "particle tracker" software to obtain text files with the particle positions in each frame for all the stacks of images acquired as indicated in section 5. Using the image stack acquisition frequency, calculate the particle displacement as a function of time (e.g. Figure 5 and Video 4).
  2. Using the force calibration file, convert the displacement curves to compliance curves (total compliance of the material — J(t)— as a function of time) according to the compliance formula:
    figure-protocol-8399
    which gives the relation between material strain and applied stress for a probe particle of radius R embedded in an incompressible, homogeneous viscoelastic medium as previously established by Schnurr and co-workers19.
  3. Adjust the creep compliance curves to the general Burgers model for viscoelastic materials and derive the viscoelastic parameters, J0, J1, η0, η1 for each particle (Figure 6) according to the Burgers' formula:
    figure-protocol-9067
    Note: This phenomenological analysis has been previously employed for a wide range of materials including biological materials such as biofilms to interpret macroscopic rheology data20-22.

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Wyniki

A typical analysis will provide the spatial distribution of the viscoelastic parameters at the micron scale on a living biofilm without disturbing its original arrangement. Typical results are shown in Figure 7 where the values of J0 — the elastic compliance — are given as a function of the z-axis along the depth and of the y-axis along a lateral dimension of the biofilm. Each point corresponds to a bead which creep curve analysis has provided a J0 value. The data reveal...

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Dyskusje

This magnetic particle seeding and pulling experiment enabled in situ 3D mapping of the viscoelastic parameters of a growing biofilm in its original state. This approach revealed the mechanical heterogeneity of the E. coli biofilm grown here and gave clues to point out the biofilm components supporting the biofilm physical properties, strongly suggesting a fundamental implication of the extracellular matrix and more precisely its degree of cross-linking.

The recognition of me...

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Ujawnienia

We have nothing to disclose.

Podziękowania

This work was in part supported by grants from the Agence Nationale pour la Recherche, PIRIbio program Dynabiofilm and from CNRS Interdisciplinary Risk program. We thank Philippe Thomen for his critical reading of the manuscript and Christophe Beloin for providing the E. coli strain used in this work.

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Materiały

NameCompanyCatalog NumberComments
Table 1: Reagents and cells
Magnetic particlesLife technologies14307DMicrometric magnetic particle, 2.8 µm diameter
Ampicillin (Antibiotic)Sigma-AldrichA9518
Tetracycline (Antibiotic)Sigma-Aldrich87128
Bacterial strain MG1655gfpFUGB, Institut Pasteur, FranceProduces F pili at its surface, resistant to Ampicilllin and tetracycline.
Table 2: Capillaries and tubing
Filters for pediatric perfusionProdimed-Plastimed6932002
Hollow Square CapillariesComposite Metal Scientific8280-100Manufactured in Borosilicate glass. Square 0.8 mm x 0.8 mm
Tubing silicone peroxydeVWR international228-0512Diameter 1 mm
Tubing silicone peroxydeVWR international228-0700Diameter 3 mm
Table 3: Biofilm growth
Lysogeny Broth (LB) solutionAmresco-VWRJ106-10PKStandard medium used to grow bacteria.
M63B1 solutionHome-madeStandard minimum medium used to grow bacteria.
GlucoseSigma-AldrichG8270Used to make M63B1 medium with 0.4% glucose.
Table 4: Electronics
Camera EMCCD  HamamatsuC9100-02
Heater controllerWorld precision instruments300354
Function generatorAgilent technologies33210A
Power amplifierHome-madeIt gives a current signal with amplitudes up to 4 A.
Syringe pumpsKd ScientificKDS-220
ShutterVincent AssociatesUniblitz T132
Magnetic tweezersHome-madeTwo electromagnetic poles, each made of a copper coil with 2,120 turns of 0.56 mm in diameter copper wire and soft magnetic alloy cores (Supra50-Arcelor Mittal, France) square shaped according to the blueprint shown in Figure 10. The two cores are mounted north pole facing south pole, in order to generate a magnetic force in one direction along the length of the capillary. See coil wiring details in Figure 11.
Table 5: Optics
Inverted microscope NikonTE-300
S Fluor x40 Objective (NA 0.9, WD0.3)NikonThis a long working distance objective enabling observation of the biofilm in the depth.
Epifluorescence filters: 1) for green fluorescence: Exc 480/20 nm; DM 495; Em 510/20  2) for Red fluorescence: Exc 540/25 nm; DM 565; Em 605/55Chroma1)#49020 2)#31002Particle displacement upon force application is recorded using the red fluoresecnce filter block.
Table 6: Image analysis
ImageJNIH - particle tracker plugin

Odniesienia

  1. Hall-Stoodley, L., Costerton, J. W., Stoodley, P. Bacterial biofilms: from the natural environment to infectious diseases. Nat Rev Microbiol. 2, 95-108 (2004).
  2. Donlan, R. M. Biofilms: microbial life on surfaces. Emerg Infect Dis. 8, 881-890 (2002).
  3. Costerton, J. W., Stewart, P. S. Battling biofilms. Scientific American. 285, 74-81 (2001).
  4. Branda, S. S., Vik, S., Friedman, L., Kolter, R. Biofilms: the matrix revisited. Trends Microbiol. 13, 20-26 (2005).
  5. Flemming, H. C., Wingender, J. The biofilm matrix. Nat Rev Microbiol. 8, 623-633 (2010).
  6. Costerton, J. W., Stewart, P. S., Greenberg, E. P. Bacterial biofilms: a common cause of persistent infections. Science. 284, 1318-1322 (1999).
  7. Stewart, P. S., Franklin, M. J. Physiological heterogeneity in biofilms. Nat Rev Microbiol. 6, 199-210 (2008).
  8. Stoodley, P., Lewandowski, Z., Boyle, J. D., Lappin-Scott, H. M. Structural deformation of bacterial biofilms caused by short-term fluctuations in fluid shear: an in situ investigation of biofilm rheology. Biotechnology and bioengineering. 65, 83-92 (1999).
  9. Klapper, I., Rupp, C. J., Cargo, R., Purvedorj, B., Stoodley, P. Viscoelastic fluid description of bacterial biofilm material properties. Biotechnol Bioeng. 80, 289-296 (2002).
  10. Korstgens, V., Flemming, H. C., Wingender, J., Borchard, W. Uniaxial compression measurement device for investigation of the mechanical stability of biofilms. Journal of microbiological. 46, 9-17 (2001).
  11. Cense, A. W., et al. Mechanical properties and failure of Streptococcus mutans biofilms, studied using a microindentation device. Journal of microbiological methods. 67, 463-472 (2006).
  12. Shaw, T., Winston, M., Rupp, C. J., Klapper, I., Stoodley, P. Commonality of elastic relaxation times in biofilms. Physical Review Letters. 93, (2004).
  13. Towler, B. W., Rupp, C. J., Cunningham, A. B., Stoodley, P. Viscoelastic properties of a mixed culture biofilm from rheometer creep analysis. Biofouling. 19, 279-285 (2003).
  14. Lau, P. C., Dutcher, J. R., Beveridge, T. J., Lam, J. S. Absolute quantitation of bacterial biofilm adhesion and viscoelasticity by microbead force spectroscopy. Biophysical journal. 96, 2935-2948 (2009).
  15. Poppele, E. H., Hozalski, R. M. Micro-cantilever method for measuring the tensile strength of biofilms and microbial flocs. Journal of microbiological methods. 55, 607-615 (2003).
  16. Aggarwal, S., Poppele, E. H., Hozalski, R. M. Development and testing of a novel microcantilever technique for measuring the cohesive strength of intact biofilms. Biotechnology and bioengineering. 105, 924-934 (2010).
  17. Guélon, T., Mathias, J. -D., Stoodley, P. Biofilm Highlights. Series on Biofilms (eds Hans-Curt Flemming, Jost Wingender, & Ulrich Szewzyk). 5, Springer. Berlin Heidelberg. (2011).
  18. Galy, O., et al. Mapping of Bacterial Biofilm Local Mechanics by Magnetic Microparticle Actuation. Biophysical journal. 103, 1-9 (2012).
  19. Schnurr, B., Gittes, F., MacKintosh, F. C., Schmidt, C. F. Determining Microscopic Viscoelasticity in Flexible and Semiflexible Polymer Networks from Thermal Fluctuations. Macromolecules. 30, 7781-7792 (1997).
  20. Aggarwal, S., Hozalski, R. M. Effect of Strain Rate on the Mechanical Properties of Staphylococcus epidermidis Biofilms. Langmuir. 28, 2812-2816 (2012).
  21. Towler, B. W., Cunningham, A., Stoodley, P., McKittrick, L. A model of fluid-biofilm interaction using a Burger material law. Biotechnol Bioeng. 96, 259-271 (2007).
  22. Jones, W. L., Sutton, M. P., McKittrick, L., Stewart, P. S. Chemical and antimicrobial treatments change the viscoelastic properties of bacterial biofilms. Biofouling. 27, 207-215 (2011).
  23. Apgar, J., et al. Multiple-particle tracking measurements of heterogeneities in solutions of actin filaments and actin bundles. Biophysical journal. 79, 1095-1106 (2000).

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