Analysis of subcellular surface structure, function and dynamics.

Analytics of single biological cells allows quantitative investigation from a structural, functional and dynamical point of view and opens novel possibilities to an unamplified subcellular analysis. In this article, we report on three different experimental methods and their applications to single cellular systems with a subcellular sensitivity down to the single molecule level. First, the subcellular surface structure of living bacteria (Corynebacterium glutamicum) was investigated with atomic force microscopy (AFM) at the resolution of individual surface layer (S-layer) proteins; discrimination of bacterial strains that lack the expression of hexagonally packed surface layer proteins was possible. Second, quantitative measurement of individual recognition events of membrane-bound receptors on living B-cells was achieved in single cell manipulation and probing experiments with optical tweezers (OT) force spectroscopy. And third, intracellular dynamics of translocating photoactivatable GFP in plant protoplasts (Nicotiana tabacum BY-2) was quantitatively monitored by two-photon laser scanning microscopy (2PLSM).

Electroporative fast pore-flickering of the annexin V-lipid surface complex, a novel gating concept for ion transport.

In contact with lipid bilayers and Ca2+-ions, the intracellular protein human annexin V (wild-type), Mr = 35,800, forms two types of cation-selective channels for the transport of Ca2+-, K+-, Na+- and Mg2+-ions, depending on the protein concentration [AN]. Type (I) channel events are large and predominant at high values [AN] > or = K = 5 nM at 296 K. At 50 mM Ca2+, symmetrical on both membrane sides, AN added at the cis side, the conductance is gCa(I) = 22 +/- 2 pS and at symmetrical 0.1 M K+-conditions: gK(I) = 32 +/- 3 pS, associated with two mean open-times tau1(I) = 0.68 +/- 0.2 ms and tau2(I) = 31 +/- 2 ms. Monoclonal anti-AN antibodies added to the trans-side first increase the mean open-times and then abolish the channel activity, suggesting that type (I) channels refer to a membrane spanning protein complex, probably a trimer T, which at [AN] > K changes its membrane organization to a higher oligomer, probably to the side-by-side double-trimer T2. The smaller type (II) channel events are predominant at low [AN] < or = K and refer to the (electroporative) adsorption complex of the monomer. The conductances g(i)(II) for symmetrical concentrations depend non-linearly on the voltage Um = Uext + U(AN), where U(AN) = 0.02 +/- 0.002 V is the electrostatic contribution of the Ca2+-AN complex and Uext the externally applied voltage. There is only one mean open-time tau(o)(II) which is voltage-dependent according to a functional of b x Um2 where b = 113.9 +/- 15 V(-2), yielding an activation Gibbs free energy of Ga = RT x b x Um2. The conformational flicker probability f(i)(II) in g(i)(II) = g(i)0(II) x gamma(i) x f(i)(II) is non-linearly voltage-dependent according to a functional of a x Um2. The Nernst term gamma(i) refers to asymmetrical ion concentrations. From a = 50 V(-2), independent of the ion type, we obtain f(i)0(II) = 0.03 +/- 0.002 and the conductances for the fully open-channel states: gCa0(II) = 69 +/- 3 pS (0.05 M Ca2+) and gK0(II) = 131 +/- 5 pS (1.2 M K+). From the electroporation term a = pi[r(p)2]epsilon0(epsilon(w) - epsilon(m))/(2 kTd) we determine the mean pore radius of the complex in its fully open state as r(p)= 0.86 +/- 0.05 nm. The adsorbed annexin V (Ca2+) monomer appears to electrostatically facilitate the electric pore formation at the contact interface between the protein and the lipid phase. The complex rapidly flickers and thus limits the ion transport in a voltage-dependent manner.

Principles of membrane electroporation and transport of macromolecules.

The phenomenon of membrane electroporation (ME) methodologically comprises an electric technique to render lipid and lipid-protein membranes porous and permeable, transiently and reversibly, by electric voltage pulses. It is of great practical importance that the primary structural changes induced by ME, condition the electroporated membrane for a variety of secondary processes, such as, for instance, the permeation of otherwise impermeable substances.

Fundamentals of electroporative delivery of drugs and genes.

Electrooptical and conductometrical relaxation methods have given a new insight in the molecular mechanisms of the electroporative delivery of drug-like dyes and genes (DNA) to cells and tissues. Key findings are: (1) Membrane electroporation (ME) and hence the electroporative transmembrane transport of macromolecules are facilitated by a higher curvature of the membrane as well as by a gradient of the ionic strength across charged membranes, affecting the spontaneous curvature. (2) The degree of pore formation as the primary field response increases continuously without a threshold field strength, whereas secondary phenomena, such as a dramatic increase in the membrane permeability to drug-like dyes and DNA (also called electropermeabilization), indicate threshold field strength ranges. (3) The transfer of DNA by ME requires surface adsorption and surface insertion of the permeant molecule or part of it. The diffusion coefficient for the translocation of DNA (M(r) approximately 3.5 x 10(6)) through the electroporated membrane is Dm = 6.7 x 10(-13) cm2 s-1 and Dm for the drug-like dye Serva Blue G (M(r) approximately 854) is Dm = 2.0 x 10(-12) cm2 s-1. The slow electroporative transport of both DNA and drugs across the electroporated membrane reflects highly interactive (electro-) diffusion, involving many small pores coalesced into large, but transiently occluded pores (DNA). The data on mouse B-cells and yeast cells provide directly the flow and permeability coefficients of Serva blue G and plasmid DNA at different electroporation protocols. The physico-chemical theory of ME and electroporative transport in terms of time-dependent flow coefficients has been developed to such a degree that analytical expressions are available to handle curvature and ionic strength effects on ME and transport. The theory presents further useful tools for the optimization of the ME techniques in biotechnology and medicine, in particular in the new field of electroporative delivery of drugs (electrochemotherapy) and of DNA transfer and gene therapy.

Mechanism of electroporative dye uptake by mouse B cells.

The color change of electroporated intact immunoglobulin G receptor (Fc gammaR-) mouse B cells (line IIA1.6) after direct electroporative transfer of the dye SERVA blue G (Mr 854) into the cell interior is shown to be dominantly due to diffusion of the dye after the electric field pulse. Hence the dye transport is described by Fick's first law, where, as a novelty, time-integrated flow coefficients are introduced. The chemical-kinetic analysis uses three different pore states (P) in the reaction cascade (C <==> P1 <==> P2 <==> P3), to model the sigmoid kinetics of pore formation as well as the biphasic pore resealing. The rate coefficient for pore formation k(p) is dependent on the external electric field strength E and pulse duration tE. At E = 2.1 kV cm(-1) and tE = 200 micros, k(p) = (2.4 +/- 0.2) x 10(3) s(-1) at T = 293 K; the respective (field-dependent) flow coefficient and permeability coefficient are k(f)0 = (1.0 +/- 0.1) x 10(-2) s(-1) and P0 = 2 cm s(-1), respectively. The maximum value of the fractional surface area of the dye-conductive pores is 0.035 +/- 0.003%, and the maximum pore number is Np = (1.5 +/- 0.1) x 10(5) per average cell. The diffusion coefficient for SERVA blue G, D = 10(-6) cm2 s(-1), is slightly smaller than that of free dye diffusion, indicating transient interaction of the dye with the pore lipids during translocation. The mean radii of the three pore states are r(P1) = 0.7 +/- 0.1 nm, r(P2) = 1.0 +/- 0.1 nm, and r(P3) = 1.2 +/- 0.1 nm, respectively. The resealing rate coefficients are k(-2) = (4.0 +/- 0.5) x 10(-2) s(-1) and k(-3) = (4.5 +/- 0.5) x 10)(-3) s(-1), independent of E. At zero field, the equilibrium constant of the pore states (P) relative to closed membrane states (C) is K(p)0 = [(P)]/[C] = 0.02 +/- 0.002, indicating 2.0 +/- 0.2% water associated with the lipid membrane. Finally, the results of SERVA blue G cell coloring and the new analytical framework may also serve as a guideline for the optimization of the electroporative delivery of drugs that are similar in structure to SERVA blue G, for instance, bleomycin, which has been used successfully in the new discipline of electrochemotherapy.

Membrane electroporation and electromechanical deformation of vesicles and cells.

Analysis of the reduced turbidity (delta T-/T0) and absorbance (delta A-/A0) relaxations of unilamellar lipid vesicles, doped with the diphenylhexatrienyl-phosphatidylcholine (beta-DPH pPC) lipids in high-voltage rectangular electrical field pulses, demonstrates that the major part of the turbidity and absorbance dichroism is caused by vesicle elongation under electric Maxwell stress. The kinetics of this electrochemomechanical shape deformation (time constants 0.1 < or = tau/microsecond < or = 3) is determined both by the entrance of water and ions into the bulk membrane phase to form local electropores, and by the faster processes of membrane stretching and smoothing of thermal undulations. Moreover, the absorbance dichroism indicates local displacements of the chromophore relative to the membrane normal in the field. The slightly slower relaxations of the chemical turbidity (delta T+/T0) and absorbance (delta A+/A0) modes are both associated with the entrance of solvent into the interface membrane/medium, caused by the alignment of the bipolar lipid head groups in one of the leaflets at the pole caps of the vesicle bilayer. In addition, (delta T+/T0) indicates changes in vesicle shape and volume. The results for lipid vesicles provide guidelines for the analysis of electroporative deformations of biological cells.