Electroporation is the use of a transmembrane electric field pulse to
induce microscopic pathways (pores) in a bio-membrane. These pores are
sometimes called "electropores." Their presence allows molecules,
ions, and water to pass from one side of the membrane to the other. As
the right side bar shows, the electropores are located primarily on the
surfaces of cells which are closest to the electrodes. If the electric
field pulse has the proper parameters, then the "electroporated" cells
can recover (the electropores reseal spontaneously), and the cells can
continue to grow. The time for the pathways to form is about one microsecond.
The time to reseal is minutes.
The use of electroporation was described by Neumann in the early 1980.
The routine use of electroporation became very popular with researchers
through the 1980s because it was found to be a practical way to place
drugs, or other molecules into cells. In the late 1980s, scientists began
to use electroporation for applications in multi-cellular tissue.
In the early 1990's Lluis Mir of the Institute Gustave-Roussy was the
first to use electroporation in a human trial to treat external tumors.
Research has shown that the induction of electropores is affected by
three major factors. First, cell-to-cell biological variability causes
some cells to be more sensitive to electroporation than other cells.
Second, for electropores to be induced, the product of the pulse amplitude
and the pulse duration has to be above a lower limit threshold. Third,
the number of pores and effective pore diameter increase with the product
of "amplitude" and "duration." Although other factors
are involved, this threshold is now understood to be largely dependent
on a fourth factor, the reciprocal of cell size. If the upper limit threshold
is reached pore diameter and total pore area are too large for the cell
to repair by any spontaneous or biological process. The result is irreversible
damage to the cell or cell lyses. Because the mechanism of electroporation
is not well understood, the development of protocols for a particular
application has usually been achieved empirically, by adjusting pulse
parameters (amplitude, duration, number, and inter-pulse interval).
Early research on electro-pore-mediated transport across membranes assumed
that simple thermal motion (i.e. diffusion) propelled molecules through
electropores.
Research in the late 1980s and early 1990s showed that certain experimental
conditions and parameters of electrical pulses may be capable of causing
many more molecules to move per unit time than simple diffusion. For
example, there is good evidence (Dimitrov and Sowers, 1990) [1] that
molecular flow is in the direction of the arrow in the sidebar but there
is also good evidence (Sukharev, et al., 1992) [2] that DNA movement
is in the opposite direction of the arrow in the sidebar. This implies
that electroporation has polarity dependence. Although this apparent
contradiction will have to be resolved by future basic research, it clearly
suggests that pulse generators with polarity-adjustable electrical parameters
are necessary for protocol development.
An additional important consideration is that during the electroporation
pulse, the electric field causes electrical current to flow through the
cell suspension or tissue. Biologically relevant buffers for cells, bathing
media, and fluid in extra-cellular space in tissues contain ionic species
at concentrations high enough to cause high electric currents to flow.
These currents can lead to dramatic heating which is biologically unacceptable.
Principles of physics suggest that the early part of exponentially decaying
pulses does most of the membrane porating but the late part continues
to heat the medium.
There have been two main waveform categories of "porating" pulses:
exponentially decaying, and rectangular (square) wave. These waveform
qualities were a matter of customary electrical engineering principles
and the fact that pulse generators designed for one waveform usually
could not deliver the other waveform. Moreover, only a few side-by-side
studies were conducted which showed a fundamental and universal superiority
of one waveform over another. In cases where there is evidence that an
exponentially decaying pulse may have an advantage for a particular application,
a protocol which delivers two pulses, one which is high in amplitude
and short in duration followed by a second which is low in amplitude
but long in duration, may simulate the effects of the exponentially-decaying
pulse or even provide an improved result. Indeed, the Pulse
Agile® capability
of Cyto Pulse pulsers has more pulse flexibility than any other currently
available instruments.
[1] Dimitrov, D.S., and Sowers, A.E., (1990) Membrane electroporation
- fast molecular exchange by electroosmosis. Biochimica et Biophysica
Acta 1022: 381-392.
[2] Sukharev SI, Klenchin VA, Serov SM, Chernomordik LV and Chizmadzhev
YA, (1992) Electroporation, and electrophoretic DNA transfer into cells:
The effect of DNA interaction with electropores, 1992, Biophys J. 63:
1320-1327.
References, General Electroporation
Books
Nickoloff, Jac A., ed. (1995) Electroporation Protocols for Microorganisms,
Methods in Molecular Biology, Volume 47, (Humana Press, Totowa, New Jersey),
372 pp.
Nickoloff, Jac A., ed. (1995) Animal Cell Electroporation and Electrofusion
Protocols, Methods in Molecular Biology, Volume 48. (Humana Press, Totowa,
New Jersey). 369 pp.
Nickoloff, Jac A., ed. (1995) Plant Cell Electroporation and Electrofusion
Protocols, Methods in Molecular Biology, Volume 55. (Humana Press, Totowa,
New Jersey). 205 pp.
E. A. Disalvo and S.A. Simon, eds. (1995) Permeability and Stability
of Lipid Bilayers (CRC Press, Boca Raton), p 105-121.
Chang, D.C., Chassy, B.M., Saunders, J.A. and
Sowers, A.E., eds. (1992)
Guide to Electroporation and Electrofusion, (Academic press, San Diego),
581 pp.
Neuman, E., Sowers, A.E., and Jordan, C.A.., eds. (1989) Electroporation
and Electrofusion in Cell Biology, (Plenum Press, New York) 581 pp.
Journal Articles
Bartoletti, D. C., Harrison, G. I., & Weaver, J. C. (1989). The
number of molecules taken up by electroporated cells: quantitative determination.
FEBS Lett., 256, 4-10.
Canatella, P. J., Karr, J. F., Petros, J. A., & Prausnitz,
M. R. (2001). Quantitative study of electroporation-mediated molecular uptake
and cell viability. Biophys.J, 80, 755-764.
Djuzenova, C. S., Zimmermann, U., Frank, H., Sukhorukov,
V. L., Richter, E., & Fuhr, G. (1996). Effect of medium conductivity and composition
on the uptake of propidium iodide into electropermeabilized myeloma cells.
Biochim.Biophys.Acta, 1284, 143-152.
Klenchin VA, Sukharev SM, Chernomordik LV, Chizmadzhev
YA, Electricaly
induced DNA uptake by cells is a fast process involving DNA electrophoresis,
1991, Biophys J. 60:804-811
Neumann, E., Kakorin, S., & Toensing, K. (1999). Fundamentals of
electroporative delivery of drugs and genes. Bioelectrochem.Bioenerg.,
48, 3-16.
Neumann, E., Toensing, K., Kakorin, S., Budde,
P., & Frey, J. (1998).
Mechanism of electroporative dye uptake by mouse B cells. Biophys.J.,
74, 98-108.
Sukharev, S. I., Klenchin, V. A., Serov, S. M.,
Chernomordik, L. V., & Chizmadzhev,
Y. (1992). Electroporation and electrophoretic DNA transfer into cells.
The effect of DNA interaction with electropores. Biophys.J., 63, 1320-1327.
Wolf, H., Rols, M. P., Boldt, E., Neumann, E., & Teissie,
J. (1994).
Control by pulse parameters of electric field-mediated gene transfer
in mammalian cells. Biophys.J., 66, 524-531.
Zerbib, D., Amalric, F., & Teissie, J. (1985). Electric field mediated
transformation: isolation and characterization of a TK+ subclone. Biochem.Biophys.Res.Commun.,
129, 611-618.