Effect of pulsed and reversing electric fields on the orientation of linear and supercoiled DNA molecules in agarose gels

When linear or supercoiled DNA molecules are imbedded in agarose gels and subjected to electric fields, they become oriented in the gel matrix and give rise to an electric birefringence signal. The sign of the birefringence is negative, indicating that the DNA molecules are oriented parallel to the electric field lines. If the DNA molecules are larger than about 1.5 kilobase pairs, a delay is observed before the birefringence signal appears. This time lag, which is roughly independent of DNA molecular weight, decreases with increasing electric field strength. The field-free decay of the birefringence is much slower for the DNA molecules imbedded in agarose gels than observed in free solution, indicating that orientation in the gel is accompanied by stretching. Both linear and supercoiled molecules become stretched, although the apparent change in conformation is much less pronounced for supercoiled molecules. When the electric field is rapidly reversed in polarity, very little change in the birefringence signal is observed for linear or supercoiled DNAs if the equilibrium orientation (i.e., birefringence) had been reached before field reversal. Apparently, completely stretched, oriented DNA molecules are able to reverse their direction of migration with little or no loss of orientation. If the steady-state birefringence had not been reached before the field reversal, complicated orientation patterns are observed after field reversal. Very large, partially stretched DNA molecules exhibit a rapid decrease in orientation at field reversal. The rate of decrease of the birefringence signal in the reversing field is faster than the field-free decay of the birefringence and is approximately equal to the rate of orientation in the field (after the lag period).(ABSTRACT TRUNCATED AT 250 WORDS)     

Orientation of DNA in agarose gels.

An orientation of the lambda DNA during the electrophoresis in agarose gels was measured by a microscopic linear dichroism technique. The method involved staining the DNA with the dye ethidium bromide and measuring under the microscope the polarization properties of the fluorescence field around the electrophoretic band containing the nucleic acid. It was first established that the fluorescence properties of the ethidium bromide-DNA complex were the same in agarose gel and in a solution. Then the linear dichroism method was used to measure the dichroism of the absorption dipole of EB dye bound to lambda DNA. In a typical experiment the orientation of two-tenth of a picogram (2 x 10(-13)g) of DNA was measured. When the electric field was turned on, the dichroism developed rapidly and assumed a steady state value which increased with the strength of the field and with the size of DNA. A linear dichroism equation related the measured dichroism of fluorescence to the mean orientation of the absorption dipole of ethidium bromide and to an extent to which the orientation of this dipole deviated from the mean. The observed development of dichroism in the presence of an electric field was interpreted as an alignment of DNA along the direction of the field. The increase in the steady state value of dichroism with the rise in the strength of the field and with the increase of the size of DNA was interpreted as a better alignment of DNA along the direction of the field and as a smaller deviation from its mean orientation.     

An electro-optical study of the mechanisms of DNA condensation induced by spermine

Condensation of DNA by spermine has been studied by electric dichroism, electric birefringence and rotational relaxation times at 1 mM ionic strength. Using Manning's theory, we found that condensation occurs for a fraction of neutralized phosphate charges (r) equal to 0.90, in good agreement with previous studies using spermidine, synthetic polyamines and trivalent cations (e.g. Co(NH3)36 +, Tb3 +). Our results are compatible with the presence in solution of torus-shaped condensed structures in a narrow range of spermine concentration; further addition of the polyamine produced precipitation due to the self-aggregation of several toroids. For spermine concentrations lower than that required for collapse, important changes of the orientation mechanism in the electric field and of DNA stiffness were observed. Whereas free DNA was mainly oriented by a fast-induced polarizability mechanism, DNA-spermine complexes displayed an important permanent dipole component, in the spermine concentration range where extension of the DNA molecules was present. The birefringence relaxation times suggested that, in the first step, the stiffness of the DNA molecules increased, and then, at higher spermine concentration, bending of the DNA molecules occurred so that condensation into toroidal particles became possible.     

Electric birefringence of restriction enzyme fragments of DNA: optical factor and electric polarizability as a function of molecular weight

The electric birefringence of restriction enzyme fragments of DNA has been investigated as a function of DNA concentration, buffer concentration, and molecular weight, covering a molecular weight range from 80 to 4364 base pairs (bp) (6 × 10⁴–3 × 10⁶ daltons). The specific birefringence of the DNA fragments is independent of DNA concentration below 20 μg DNA/ml, but decreases with increasing buffer concentration, or conductivity, of the solvent. At sufficiently low field strengths, the Kerr law is obeyed for all fragments. The electric field at which the Kerr law ends is inversely proportional to molecular weight. In the Kerr law region the rise of the birefringence is accurately symmetrical with the decay for fragments ≤ 389 bp, indicating an induced dipole orientation mechanism. The optical factor calculated from a 1/E extrapolation of the high field birefringence data is ?0.028, independent of molecular weight; if a 1/E² extrapolation is used, the optical factor is ?0.023. The induced polarizability, calculated from the Kerr constant and the optical factor, is proportional to the square of the length of the DNA fragments, and inversely proportional to temperature. Saturation curves for DNA fragments ≤ 161 bp can be described by theoretical saturation curves for induced dipole orientation. The saturation curves of larger fragments are broadened, because of a polarization term which is approximately linear in E, possibly related to the saturation of the induced dipole in high electric fields. This “saturated induced dipole” is found to be 6400 D, independent of molecular weight. The melting temperature of a 216-bp sample is decreased 6°C in an electric field of 8 kV/cm, because the lower charge density of the coil form of DNA makes it more stable in an electric field than the helix form.     

Electric shock-mediated transfection of cells. Characterization and optimization of electrical parameters.

The effect of various parameters on the electric shock-mediated permeabilization and transfection of CHO cells has been investigated. Up to 70% of the cells can be maintained transiently permeable to erythrosin B for periods of at least 1 h at 20 degrees C. Electrical conditions optimal for transient permeabilization were also optimal for efficient DNA transfection by pSV2neo. However, the DNA must be present during exposure to the electric field for efficient transformation. The same requirement existed for voltage-induced DNA toxicity. The results suggest that DNA moves into the cells by electrophoresis, not by simple diffusion. Based on these observations a simple, rapid procedure for optimizing the conditions for electric shock-mediated DNA transfer into cells has been developed.     

Transient electric birefringence of agarose gels. I. Unidirectional electric fields

The orientation of agarose gels in pulsed electric fields has been studied by the technique of transient electric birefringence. The unidirectional electric fields ranged from 2 to 20 V/cm in amplitude and 1 to 100 s in duration, values within the range typically used for pulsed field gel electrophoresis (PFGE). Agarose gels varying in concentration from 0.3 to 2.0% agarose were studied. The sign of the birefringence varied randomly from one gel to another, as described previously [J. Stellwagen & N. C. Stellwagen (1989), Nucleic Acids Research, Vol. 17, 1537–1548]. The sign and amplitude of the birefringence also varied randomly at different locations within each gel, indicating that agarose gels contain multiple subdomains that orient independently in the electric field. Three or four relaxation times of alternating sign were observed during the decay of the birefringence. The various relaxation times, which range from 1 to ～ 120 s, can be attributed to hierarchies of aggregates that orient in different directions in the applied electric field. The orienting domains range up to ～ 22 μm in size, depending on the pulsing conditions. The absolute amplitude of the birefringence of the agarose gels increased approximately as the square of the electric field strength. The measured Ker constants are ～ 5 orders of magnitude larger than those observed when short, high-voltage pulses are applied to agarose gels. The increase in the Kerr constants in the low-voltage regime parallels the increase in the relaxation times in low-voltage electric fields. Birefringence saturation saturation curves in both the low- and high-voltage regimes can be fitted by theoretical curves for permanent dipole orientation. The apparent permanent dipole moment increase approximately as the 1.6 power of fiber length, consistent with the presence of overlapping agarose helices in the large fiber bundles orienting in low-voltage electric fields, the optical factor is approximately independent of fiber length. Therefore, the marked increase in the Kerr constants observed in the low-voltage regime is due to the large increase in the electrical orientation factor, which is due in turn to the increased length of the fiber bundles and domains orienting in low-voltage electric fields. Since the size of the fiber bundles and domains approximates the size of the DNA molecules being separated by PFGE, the orientation of the agarose matrix in the applied electric field may facilitate the migration of large DNA molecules during PFGE. © 1994 John Wiley & Sons, Inc.     

Interactions of nucleic acid double helices induced by electric field pulses

Electric field pulses induce a substantial increase of the light scattering intensity of double-helical DNA. The relative change of light scattering and also the reciprocal relaxation time constants under electric field pulses increase with increasing nucleotide concentration. These observations, together with a large difference between dichroism orientation time constants and light scattering time constants under electric field pulses, demonstrate that the main part of the light scattering effect is due not to field-induced orientation but to interactions between DNA helices. From the concentration dependence of the light scattering time constants we obtain, according to an isodesmic reaction model, association rate constants in the range 3 × 10¹⁰ M^?1 helices s^?1 for DNA with approx. 300 base-pairs. These values are at the limit of a diffusion-controlled DNA association and do not show any dependence upon the field strength. The dissociation rate constants k_d decrease strongly with increasing field strength E and thus demonstrate that the interactions between the helices are induced by the electric field. This conclusion is consistent with independent measurements which do not reveal any DNA association at zero field strength. The observed linear relation between log(k_d) and E² suggests a field-induced reaction driven by dipole changes. According to this interpretation the change of dipole moment should be in the range of approx. 1400 debye. The dissociation rates for DNA helices with approx. 300 to approx. 800 base-pairs strongly increase with increasing sail concentration (measured in the range 1–5 mM ionic strength), whereas the association rate constants remain virtually unchanged. Measurements of the linear dichroism in the same range of DNA chain length demonstrate that for long field pulses of e.g., 40 μs, the amplitude approaches a maximum value and then decreases. The dichroism relaxation curves observed after long field pulses exhibit a component with a positive dichroism and an increased decay time. These observations suggest the formation of a DNA aggregate with an unusual arrangement of the bases.     

Conformation changes in rRNA induced by electric impulses

We have investigated the effects of electric field pulses (of about 44 kV/cm magnitude and 30 μsec duration) on E. coli ribosomal RNA in solution (5 × 10^?4 M sodium cacodylate buffer, pH 7, 20° C). The time course of changes in ultraviolet absorbance and electric dichroism can be resolved into contributions from orientational and conformational changes. The fast part of the relaxation spectrum (completed in less than 1 μs) is attributed to alignment of double-helical segments of rRNA with the external electric field; the slower part (relaxation times in the ms and μs range) is shown to be due to changes in orientation of the entire τRNA molecule, concomitant with electric field-induced helix-coil transitions of oligomeric base-paired regions.     

Electric properties and structure of DNA-restriction fragments from measurements of the electric dichroism

The electric dichroism of 17 homogeneous DNA fragments, ranging in size from 43 to 4362 base-pairs, has been analyzed in high electric fields. The orientation of the small fragments can be described in terms of an induced dipole moment, whereas the large fragments are oriented according to a constant dipole mechanism. In the intermediate size range, DNA orients according to an induced dipole mechanism at low field strengths and according to a constant dipole mechanism at high field strengths. From these observations we propose an orientation mechanism with a saturating induced dipole. The induced dipole observed at low field strengths is saturated at a field strength Eo within a transition range Em to give a constant dipole moment at high field strengths. These parameters together with the polarizability and the limit reduced dichroism are evaluated by a least-squares analysis of the experimental data. Eo and Em are found to decrease with increasing chain length from Eo approximately 40 kV/cm (Em approximately 14 kV/cm) at 65 base-pairs to 10 kV/cm (6 kV/cm) at 194 base-pairs. The polarizability is found to increase with the square of the chain length, whereas the saturated dipole increases with chain length N at low N and goes to a limit value at high N. The temperature dependence of the orientation parameters is found to be very small. The values obtained for the limit dichroism are between -1.0 and -1.3 for chain lengths between 60 and 1000 base-pairs, whereas values around -1.4 are observed at chain lengths greater than 1000 base-pairs. These data indicate that electric fields extend the contour of DNA strands at high chain lengths from a weakly bent to a more linear form. The variations of the limit dichroism observed for short fragments suggest sequence-dependent differences in the secondary structure of the helix. The experimental results are compared with numerical calculations based on simple polyelectrolyte models. For short fragments the magnitude of several electrochemical parameters can be adequately explained by a polarization of the ion cloud around the DNA molecules. However, these polyelectrolyte models do not adequately describe the observed chain length dependence of the orientation phenomena.     

Theory of linear dichroism of DNA and DNA-containing structures

Analysis has been made of the relationship between the dichroic ratio of DNA polymers and the orientation of their transition dipoles. The molecules may be aligned in a mechanical shear or electric field. The effect of the shear or electric field on the orientation factor has been shown. The results of dipole moments and their dependence on the strength of the electric field have been discussed. Higher orders of coiling, flat packing and their various combinations cause the optical and electrical dichroic ratio to change characteristically, so that the electric and optical anisotropy of DNA can be utilized to study the DNA arrangement in DNA-containing structures.     

Electric dichroism of poly(riboadenylic acid)

Electric dichroism measurements on poly(A) in low-ionic-strength solution demonstrate that below a molecular weight of 130,000 the double-stranded polymer is hydrodynamically rigid and above that molecular weight becomes increasingly flexible. At 500,000 it is considerably more flexible than DNA of the same molecular weight, with a mean end-to-end distance of about 1150 Å compared to approximately 1600 Å for DNA. The fully extended length for both DNA and poly(A) of this molecular weight is about 2750 Å. It is further shown that the orientation of these polyelectrolytes in an electric field is consistent with theoretical treatments of the counter-ion distribution and a preliminary model based on the additivity of classical valence charge anisotropy and counter-ion polarization is postulated for the orientation mechanism. Single-stranded pol (A) is shown not only to retain its base stacking in the presence of the electric field but to extend the persistent regions of stacked bases so that it attains a rodlike structure very similar to the one in the double-stranded polymer is found to be less than that expected from consideration of the x-ray structure. An explanation for this result is sought in the electric asymmetry of the helical polymer.     

Exploitation of the electro-optical characteristics of microbial suspensions for determining p-nitrophenol and microbial degradative activity

The effect of p-nitrophenol metabolism on the electrophysical properties of a microbial cell suspension of Acinetobacter calcoaceticum was investigated. The dependence of the suspension's optical density changes due to the orientation of the electric field on the frequency of an orienting electric field (orientational spectra) over the range 10–10 000 kHz was used. Upon optimization of cell culture conditions, followed by orientational spectrum measurements, it was found that the most dramatic changes in orientation spectrum associated with p-nitrophenol metabolism took place over the frequency range 10–1000 kHz. Additionally, a linear dependence of the magnitude of the electrooptical effect on p-nitrophenol concentrations of 0.1–0.8 mM was established. The minimum p-nitrophenol concentration detectable by this calibration was 0.1 mM.     

Dielectric behavior of polyelectrolytes. VI. Dynamic response of cylindrical biopolymers to electric fields

The time dependence of the orientation of a cylindrical biopolymer and the configuration of its counterion complement in the presence of an external electric field is found by solving a model forced diffusion equation. The solution is a high temperature expansion in the external field strength and is used to predict the nature of the dielectric relaxation and the dynamic Kerr effect for such systems. Specific application is made to the dynamic Kerr effect of a DNA oligomer for which experimental data appear in the literature. The analysis yields a value for the surface diffusion coefficient of a sodium ion on DNA at 20 degrees C of 3.8 x 10(-10) m2 s-1.     

Nonsequence-specific arginine interactions in the nucleosome core particle

We have analyzed the relative orientation of basic amino acid side chains towards DNA in the nucleosome core particle. The electric field created by DNA phosphates has no apparent preferential orientation: no favored orientation of the arginine guanidinium group is found. Arginine may be either directly hydrogen bonded to a phosphate oxygen or stabilized in the minor groove by van der Waals contacts and the local negative electric field. On the other hand, the phosphate oxygen atoms hydrogen bonded to arginines are always found close to the plane defined by the guanidinium group. Thus it can be concluded that the interactions of arginine are strongly directional, those of phosphate are not. We also find that a highly charged fragment of histone H2B, which is placed between two DNA turns, has a very variable conformation. An increase in protein positive charge density apparently allows multiple nonspecific protein conformations when interacting with DNA.     

Transient orientation of linear DNA molecules during pulsed-field gel electrophoresis.

The transient orientation of lambda DNA and lambda-DNA oligomers has been measured during pulsed field gel electrophoresis. The DNA becomes substantially aligned parallel to the electric field E. In response to a single rectangular pulse, orientation shows an overshoot with a peak at 1 second, then a small undershoot, and finally a plateau. When the field is turned off, the orientation dissipates in two distinct exponential phases. Field inversion leads to periods of orientation with intervening periods of reduced orientation as the chains reverse direction. Field inversion pulses applied to linear oligomers of lambda-DNA show that orientation responses slow down but increase in amplitude as molecular weight increases, for a given field. Because DNA stretching and alignment parallel to E are expected to correlate with DNA velocity, the velocity in response to a pulsed field is also expected to exhibit an overshoot.     

Perinatal essential fatty acid deficiency influences body weight and bone parameters in adult male rats

Electropermeabilization designates the use of electric pulses to overcome the barrier of the cell membrane. This physical method is used to transfer anticancer drugs or genes into living cells. Its mechanism remains to be elucidated. A position-dependent modulation of the membrane potential difference is induced, leading to a transient and reversible local membrane alteration. Electropermeabilization allows a fast exchange of small hydrophilic molecules across the membrane. It occurs at the positions of the cell facing the two electrodes on an asymmetrical way. In the case of DNA transfer, a complex process is present, involving a key step of electrophoretically driven association of DNA only with the destabilized membrane facing the cathode. We report here at the membrane level, by using fluorescence microscopy, the visualization of the effect of the polarity and the orientation of electric pulses on membrane permeabilization and gene transfer. Membrane permeabilization depends on electric field orientation. Moreover, at a given electric field orientation, it becomes symmetrical for pulses of reversed polarities. The area of cell membrane where DNA interacts is increased by applying electric pulses with different orientations and polarities, leading to an increase in gene expression. Interestingly, under reversed polarity conditions, part of the DNA associated with the membrane can be removed, showing some evidence for two states of DNA in interaction with the membrane: DNA reversibly associated and DNA irreversibly inserted.     

Effect of electrical corrosion protection of oil pipelines on fish migration

Effect of the dc electric field of the corrosion protection of oil pipelines crossing the Ob River on the behavioral response of fish was investigated. It was shown by calculations and measurements that, at the bottom level, the electric field strength was 0.6 V/m, and at a depth of 2 m from the surface, it was 0.4-0.1 V/m and extended to a distance of 50-100 m from the oil pipeline. It was established that the electric field of oil pipelines lowered the migration activities of fish, resulting in a growth of fish number in regions of increased electric field strength.     

Linear contour length dependence of electrical polarizability of nucleosomal DNA fragments: implications for the flexibility of DNA

The transient electric birefringence of monodisperse oligonucleosomal DNA ranging from 145 to 990 base pairs has been studied. The orientation of fragments can be described in terms of an induced dipole moment with a small contribution of a permanent dipole. The electrical polarizability delta alpha was found to increase linearly with the DNA contour length. This unexpected dependence might result from a bent structure of DNA already considerable for very short segments. The observed delta alpha values agree with a segmental orientation of rigid subunits of length 13-18 nm as estimated in the elastic model of DNA with a kink angle of about 41 degrees.     

The mechanism of ion polarisation along DNA double helices

The orientation curves of short DNA fragments induced by electric field pulses are measured with high time resolution and analysed by efficient deconvolution techniques. A small, but clearly detectable delay of the 'on-field' orientation can be described accurately by the superposition of two exponential processes with opposite amplitudes. The time constant of the faster process is around 10 ns and the slower one in the range 50-1000 ns depending upon the electric field strength and chain length of the DNA fragment. The relation between amplitudes and time constants observed for each curve corresponds exactly to that expected for a convolution of two processes, where the first process is without optical response and becomes detectable only via the optical response of the second process. These results indicate that the first process reflects the polarisation of the ion atmosphere required for the second process of the orientation. Measurements at different ion concentrations c demonstrate that the reciprocal time constant of the fast process is a linear function of c and thus is consistent with an association reaction. The association rate constant evaluated from this dependence according to a simple bimolecular reaction model is 8 X 10(9) M-1 s-1 for a 95 base-pair fragment and is consistent with binding of Na+ to the helix, a reaction close to the limit of diffusion control. The association rate constant is almost independent of the electric field strength E, while the dissociation rate constant k- strongly increases with E, indicating dissociation of ions at high E values. The data suggest a linear correlation between log(k-) and E2 corresponding to a reaction driven by a dipole change. The apparent dipole change evaluated from this dependence is in the order of magnitude estimated for an elementary step of ion dissociation at one end of the helices. The combined results obtained from the polarisation and the orientation mechanism can be explained by dissociation of surprisingly few counterions biased towards one end of the helices. The experimental data obtained for a 76 base-pair fragment are analogous to those for the 95 base-pair fragment, whereas the 'slow' ion polarisation has not been detected for a fragment with 27 base-pairs. This result together with those obtained for the longer fragments at low field strengths indicate that there is a fast polarisation mechanism without 'ion dissociation' at low chain lengths and for low electric field strengths. This mechanism is replaced at high chain lengths and/or high electric field strengths by the ion dissociation mechanism.(ABSTRACT TRUNCATED AT 400 WORDS)     

Intracellular effect of ultrashort electrical pulses

A simple electrical model for biological cells predicts an increasing probability for electric field interactions with cell substructures of prokaryotic and eukaryotic cells when the electric pulse duration is reduced into the sub-microsecond range. The validity of this hypothesis was verified experimentally by applying electrical pulses with electric field intensities of up to 5.3 MV/m to human eosinophils in vitro. When 3-5 pulses of 60 ns duration were applied to human eosinophils, intracellular granules were modified without permanent disruption of the plasma membrane. In spite of the extreme electrical power levels applied to the cells thermal effects could be neglected because of the ultrashort pulse duration. The intracellular effect extends conventional electroporation to cellular substructures and opens the potential for new applications in apoptosis induction, gene delivery to the nucleus, or altered cell functions, depending on the electrical pulse conditions.