| Nanopore Unitary Permeability Measured by Electrochemical and Optical Single Transporter Recording Biophysical Journal, Volume 88, Issue 6, 1 June 2005, Pages 4000-4007 Roland Hemmler, Guido Böse, Richard Wagner and Reiner Peters Abstract For the analysis of membrane transport processes two single molecule methods are available that differ profoundly in data acquisition principle, achievable information, and application range: the widely employed electrical single channel recording and the more recently established optical single transporter recording. In this study dense arrays of microscopic horizontal bilayer membranes between 0.8m and 50m in diameter were created in transparent foils containing either microholes or microcavities. Prototypic protein nanopores were formed in bilayer membranes by addition of -hemolysin (-HL). Microhole arrays were used to monitor the formation of bilayer membranes and single -HL pores by confocal microscopy and electrical recording. Microcavity arrays were used to characterize the formation of bilayer membranes and the flux of fluorescent substrates and inorganic ions through single transporters by confocal microscopy. Thus, the unitary permeability of the -HL pore was determined for calcein and Ca ions. The study paves the way for an amalgamation of electrical and optical single transporter recording. Electro-optical single transporter recording could provide so far unresolved kinetic data of a large number of cellular transporters, leading to an extension of the nanopore sensor approach to the single molecule analysis of peptide transport by translocases. Abstract | Full Text | PDF (482 kb) |
| Modeling Transmembrane Transport through Cell Membrane Wounds Created by Acoustic Cavitation Biophysical Journal, Volume 95, Issue 9, 1 November 2008, Pages 4124-4138 Vladimir Zarnitsyn, Christina A. Rostad and Mark R. Prausnitz Abstract Cells exposed to acoustic cavitation and other mechanical stresses can be transiently permeabilized to permit intracellular uptake of molecules, including drugs, proteins, and genes. Microscopic imaging and other studies suggest that intracellular loading occurs through plasma membrane wounds of submicrometer radius that reseal over time through the aggregation and fusion of lipid vesicles trafficked to the wound site. The goal of this study was to 1), determine the size of membrane wounds as a function of time after in vitro sonication of DU145 prostate cancer cells under conditions that caused extensive acoustic cavitation; and 2), theoretically model transport processes leading to intracellular loading. Our overall hypothesis was that intracellular loading is governed by passive diffusion through porous membrane wounds of up to 300-nm radius containing pores that permit entry of molecules up to at least 28-nm radius over a timescale of minutes. Experimental measurements showed intracellular loading of molecules with radii from 0.6 to 28nm, where most loading occurred after sonication over a timescale up to minutes and where smaller molecules were taken up to a greater extent and over a longer timescale than larger molecules. Theoretical modeling predicted that membrane wounds would have a 300-nm radius initially and then would shrink, with a half life of 20 to 50s. Uptake was shown to occur predominantly by diffusion and the increasing levels of uptake with decreasing molecular size was explained primarily by differences in molecular diffusivity and, for the largest molecule, geometrical hindrance within the wound. Mathematical modeling was simplified, because transport through porous wounds of possibly complex internal nanostructure was governed largely by transport at the edge of the wound, and depended only weakly on the size, number, and distribution of nanopores within the wound under the conditions relevant to this study. Overall, this study developed a theoretical framework for analysis of transmembrane transport through cell membrane wounds and thereby provided quantitative estimates of their size and lifetime. Abstract | Full Text | PDF (302 kb) |
| Negative Contrast Imaging of Mitochondria by Confocal Microscopy Biophysical Journal, Volume 77, Issue 3, 1 September 1999, Pages 1747-1748 John J. Lemasters, Ting Qian and Anna-Liisa Nieminen Full Text | PDF (58 kb) |
Copyright © 2007 The Biophysical Society. All rights reserved.
Biophysical Journal, Volume 92, Issue 1, L04-L06, 1 January 2007
doi:10.1529/biophysj.106.096743
Biophysical Letters
Susanne Zibek*, Alfred Stett*, Peter Koltay†, Min Hu†, Roland Zengerle†, Wilfried Nisch* and Martin Stelzle*,
, 
* Natural and Medical Sciences Institute, D-72770 Reutlingen, Germany
† Institute of Microsystem Technology IMTEK, D-79110 Freiburg, Germany
Address reprint requests and inquiries to Dr. Martin Stelzle, Natural and Medical Sciences Institute, Tel.: 49-7121-5153075; Fax: 49-7121-5153062.Electrostimulation has been the method of choice for almost all neurostimulation devices in use to date. As it relies solely on membrane depolarization by electric fields to induce a cellular response, it lacks, however, the cell type selectivity and spatial resolution in principle achievable by chemical stimulation. Several microfabricated drug delivery systems for controlled release of biochemically active compounds have been proposed 1,2,3. Earlier attempts to use microfluidic devices for chemical stimulation of cells suffered from the problem of uncontrolled leakage from open microapertures into the medium and consequently undefined concentration conditions 4,5. In contrast, our novel “air gap”-scheme 6 (Fig. 1) avoids such leakage completely. It facilitates the precise positioning of the application spot directly under or at a lateral distance with respect to cells of interest. Either calcein-AM or acetylcholine was used for stimulation. Concentration gradients develop along the surface of the cell layer eliciting specific cellular responses.
Tissue chambers consisting of a glass ring with a Nucleopore membrane (Whatman International, Maidstone, UK) with pore sizes ranging from 50nm to 1μm glued to their bottom were homemade and treated in an air plasma (30s) before cultivation of TE 671 muscle sarcoma cells. Dulbecco's modified Eagle's medium (4.5 g/l glucose) supplemented with 10% fetal calf serum, 2mM glutamine, penicillin, and streptomycin was used. A commercially available bubble jet print head was used to apply single or multiple droplets of ∼25 pl volume to the bottom face of the membrane (Fig. 1) 6.
Mixtures of calcein-AM (0.25mM, nonfluorescent) and eosin Y dye (0.1mM) and of acetylcholine (1mM) and eosin Y dye (10μM) were used. Eosin Y served to indicate the distribution and the diffusive transport of the active, yet invisible substance (calcein-AM or acetylcholine, respectively) in the medium. Cellular response was recorded using a Zeiss Axiophot fluorescence microscope (Zeiss, Göttingen, Germany) fitted with a Hamamatsu C2400-08 video camera (Hamamatsu Photonics, Herrsching, Germany) employing 485nm excitation and 515 - 585nm emission filters. Calcein AM becomes fluorescent after enzymatic hydrolysis of ester residues after its incorporation into cells. To monitor excitation by acetylcholine, cells were first loaded with Ca2+-sensitive fluo-4-AM dye (Invitrogen, Karlsruhe, Germany) by incubation for 30min at a concentration of 2.3μM. Subsequently the medium was changed to remove extracellular fluo-4-AM dye and cells were incubated for another hour at 37°C. Upon excitation, intracellular Ca2+ concentration increases resulting in an increase of fluorescence intensity. The latter is determined using Image J software in regions of interest of 10μm diameter manually specified for each cell (cf. Fig. 3, t=5s).
Application of calcein-AM/eosin Y: TE 671 cells were cultivated on nanoporous membranes (pore size, 1μm) and stained with Hoechst 33342 dye (nucleus staining) to track cell location in the membrane (Figure 2A). The calcein-AM/eosin Y mixture (5 droplets, 125 pl total volume) was applied resulting in a transient fluorescence signal indicating the spot size (≈60μm) where substance was actually delivered to the cell layer. Control experiments with eosin Y did not show any uptake of this dye into TE 671 cells. Rather, eosin Y fluorescence vanishes over a period of several minutes to invisibility due to diffusion in the medium (Figure 2D). After this time period, only cells appear fluorescent, which is attributed to the incorporation and enzymatic hydrolysis of calcein-AM by the cells (Figure 2D). At the concentration employed here (0.25mM), only cells located directly above the application spot were sufficiently loaded by calcein to show appreciable fluorescence. Variation of concentration and droplet volume thus determines effective spatial resolution achievable by this chemical stimulation scheme.
Acetylcholine stimulation: single droplets of a mixture of acetylcholine (1mM) and eosin Y (10μM) were applied to the bottom of a nanoporous membrane (pore size, 50nm). Fig. 3 shows a panel of fluorescence micrographs of the cell culture after the application of the droplet (at t=0s). The eosin Y fluorescence indicates the location of the application spot (center). Subsequently, fluorescence of TE 671 cells appears and shows a wave of excitation progressing from the application spot to the periphery in a circular symmetry. In the figure inset, the effective radius of excitation is given as indicated by arrows in the micrographs. After 30s, fluorescence has almost completely decayed. Fluorescence intensity traces of the cells indicated by circles in Fig. 3 (t=5s) were analyzed in detail (Fig. 4, Table 1). The delay, τ, of cellular response with respect to droplet delivery varies proportional to the square of the distance, d, between the rim of the application spot and the location of the cell under investigation as is expected for diffusive transport (Fig. 4inset, Table 1).
The apparent lag time of 1.5s between stimulation and onset of excitation of cells (inset, Fig. 4) is attributed to intracellular signaling in agreement with earlier reports 7. The low level of fluorescence intensity at t<1.5s confirms that contribution of eosin Y to overall fluorescence is negligible outside the application spot. Interestingly, cells showed different maximum intensities, even if located at similar distances d. This may be due to different degrees of loading with fluo-4-AM dye. The origin of the modulation in some of the fluorescence signals (for example, cell 5, Fig. 4) is yet unknown.
The response time as it may be determined from the initial slope (from 10% to 50% of the final fluorescence signal intensity seems to show a tendency toward an increase with increasing d). This would point to a dose/response relationship as acetylcholine concentration is expected to decrease with increasing d. However, further study in cell cultures with a larger field of view will be necessary to confirm this preliminary finding. At lower concentration of acetylcholine, excitation is limited to a smaller area or even precisely to the application spot (data not shown). This finding is as expected, since half spherical diffusive transport of acetylcholine in the space above the cell layer will result in progressive dilution of the neurotransmitter. At a certain distance from the application spot, the concentration will be lower than the threshold level required to induce excitation of cells. Also, the use of smaller droplets would further enhance spatial resolution.
Functional chemical stimulation of adherent cells may be achieved in a well-controlled and versatile fashion by utilizing nanoporous membranes as support and localized substance application by bubble jet technology. By variation of concentration and/or volume of the fluid, spatial resolution and range of excitation may be controlled. Future research will be directed toward numerical simulation of concentration profiles along the surface of the cell layer considering the application spot as extended drainable reservoir and the measurement of complete dose/response curves from experiments as demonstrated in this Letter. As the cellular response reflects the local concentration, this approach should allow for rapid determination of dose/response curves in a single experiment as opposed to the multi-well plate approach commonly used today.
Funding for this research was obtained from the Landesstiftung Baden-Württemberg under grant “Artificial Synapse”.
1. (2003). Microfabricated drug delivery systems: from particles to pores. Adv. Drug Deliv. Rev. 55, 315–328. CrossRef | PubMed
2. (2004). Electronic MEMS for triggered delivery. Adv. Drug Deliv. Rev. 56, 173–184. CrossRef | PubMed
3. (2001). Microfabricated drug delivery systems: concepts to improve clinical benefit. Biomed. Microdevices 3, 97–108. CrossRef | PubMed
4. (2004). Localized chemical release from an artificial synapse chip. Proc. Natl. Acad. Sci. USA 101, 9951–9954. CrossRef | PubMed
5. (2003). Towards a neurotransmitter-based retinal prosthesis using an inkjet print-head. Biomed. Microdevices 5, 195–199. CrossRef | PubMed
6. (2006). Discrete chemical release from a microfluidic chip. Proc. In IEEE-MEMS International Conference on Micro Electro Mechanical Systems. (Istanbul: Institute of Electrical and Electronics Engineers), pp. 28–31. PubMed
7. (1999). Probing intracellular dynamics in living cells with near-field optics. J. Neurosci. Methods 89, 9–15. CrossRef | PubMed