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PubMed1986

Histologic changes and arrhythmogenicity after discharge through transseptal catheter electrode.

Ventricular tachycardia commonly arises within the intraventricular septum and successful catheter ablation of septal tachycardia might be enhanced by transseptal electrode placement. We have evaluated the safety of a transseptal ablation procedure. Arrhythmogenicity and histology were examined after high-energy capacitor discharges were delivered to an intracavitary cathode-anode pair placed on opposite sides of the interventricular septum in pentobarbital-anesthetized dogs. After two discharges of 200 or 100 J proved lethal, paired discharges of 30 or 50 J (10 dogs) or a single discharge of 100 J (four dogs) was used to induce 28 lesions. Acute rhythm changes and risk of induction of ventricular tachycardia by programmed stimulation were measures of arrhythmogenicity. Gross and histologic examination of the hearts after 20 min to 28 days allowed characterization of the evolution of lesions. The conduction system in nearby and remote locations was extensively examined in four dogs. Refractory ventricular fibrillation developed with paired shocks at 200 or 100 J. At lower energy levels, acute ventricular fibrillation occurred with 12 of 20 shocks (60%), but defibrillation was consistently achieved. After ablation, no dog had ventricular tachycardia or fibrillation induced with programmed stimulation. Matching anodal and cathodal lesions spanned the septum without perforation in 10 of 16 dogs, and the lesions were of similar histology. Each contained central areas of hemorrhage surrounded by a region of coagulation necrosis merging with normal myocytes peripherally. There was necrosis and edema without inflammation at 20 min, acute inflammatory cell infiltration at 1 to 2 days, and myocyte replacement by granulation tissue after 6 days.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1992

Cardiac potential and potential gradient fields generated by single, combined, and sequential shocks during ventricular defibrillation.

BACKGROUND: Potential gradient field determination may be a helpful means of describing the effects of defibrillation shocks; however, potential gradient field requirements for defibrillation with different electrode configurations have not been established. METHODS AND RESULTS: To evaluate the field requirements for defibrillation, potential fields during defibrillation shocks and the following ventricular activations were recorded with 74 epicardial electrodes in 12 open-chest dogs with the use of a computerized mapping system. Shock electrodes (2.64 cm2) were attached to the lateral right atrium (R), lateral left ventricular base (L), and left ventricular apex (V). Four electrode configurations were tested: single shocks of 14-msec duration given to two single anode-single cathode configurations, R:V and L:V, and to one dual anode-single cathode configuration, (R+L):V; and sequential 7-msec shocks separated by 1 msec given to R:V and L:V (R:V----L:V). Defibrillation threshold (DFT) current was significantly lower for R:V----L:V than for the other configurations and markedly higher for L:V. Despite these differences, the minimum potential gradients measured at DFT were not significantly different (approximately 6-7 V/cm for each electrode configuration). Potential gradient fields generated by the electrode configurations were markedly uneven, with a 15-27-fold change from lowest to highest gradient, with the greatest decrease in gradient occurring near the shock electrodes. Although gradient fields varied with the electrode configuration, all configurations produced weak fields along the right ventricular base. Early sites of epicardial activation after all unsuccessful shocks occurred in areas in which the field was weak; 87% occurred at sites with gradients less than 15 V/cm. Ventricular tachycardia originating in high gradient areas near shock electrodes followed 11 of 67 successful shocks. CONCLUSIONS: These data suggest that 1) defibrillation fields created by small epicardial electrodes are very uneven; 2) achievement of a certain minimum potential gradient over both ventricles is necessary for ventricular defibrillation; 3) the difference in shock strengths required to achieve this minimum gradient over both ventricles may explain the differences in DFTs for various electrode configurations; and 4) high gradient areas in the uneven fields can induce ectopic activation after successful shocks.

Animals↗
PubMed1994

Prospective, randomized comparison in humans of a unipolar defibrillation system with that using an additional superior vena cava electrode.

BACKGROUND: A unipolar defibrillation system using a single right ventricular (RV) electrode and the active shell or "CAN" of the implantable cardioverter-defibrillator itself situated in a left infraclavicular pocket has been shown to be as efficient in defibrillation as an epicardial lead system. The purpose of this study was to determine whether defibrillation efficacy can be improved further by adding a superior vena cava (SVC) electrode to this already efficient defibrillation system. METHODS AND RESULTS: We prospectively and randomly compared the defibrillation efficacy of a simplified unipolar defibrillation system, RV-->CAN, with that of one incorporating a high SVC electrode, RV-->SVC + CAN, in 15 consecutive cardiac arrest survivors undergoing implantation of a presently available transvenous defibrillation system. The RV defibrillation electrode was a 5-cm coil located on a 10.5F lead used as the anode in both lead configurations examined. The active CAN was a 108-cm2 surface area shell of a titanium alloy pulse generator used as the cathode in both configurations and placed in a left infraclavicular pocket. The SVC electrode was a 6F 5-cm-long coil and was used as an additional cathode positioned at the junction of the SVC and the left innominate vein. The defibrillation pulse used was a 65% tilt, asymmetric biphasic waveform delivered from a 120-microF capacitor. The defibrillation threshold (DFT) stored energy, leading edge voltage, current, and pulsing resistance were measured for both lead systems. The single-lead unipolar system, RV-->CAN, resulted in a stored energy DFT of 7.4 +/- 5.2 J, and the three-electrode dual pathway system, RV-->SVC + CAN, resulted in a DFT of 6.0 +/- 3.4 J (P = .20). There was no difference in defibrillation efficacy with the more complicated three-electrode system over the unipolar system despite a decrease in pulsing resistance to 48.6 +/- 3.5 omega compared with 61.2 +/- 5.9 omega for the unipolar system (P < .0001) and a slight rise in delivered current to 6.3 +/- 1.8 A compared with 5.5 +/- 2.0 A for the unipolar system (P = .062). CONCLUSIONS: The unipolar single-lead transvenous defibrillation system provides defibrillation at energy levels comparable to that reported with present epicardial lead systems. Coupling of this lead system to a third SVC electrode increases system complexity but offers little defibrillation advantage despite a large decrease in pulsing resistance and a modest increase in delivered current.

Defibrillators, Implantable↗
PubMed1988

Extracellular field required for excitation in three-dimensional anisotropic canine myocardium.

It is not known how well potential gradient, current density, and energy correlate with excitation by extracellular stimulation in the in situ heart. Additionally, the influence of fiber orientation and stimulus polarity on the extracellular thresholds for stimulation expressed in terms of these factors has not been assessed. To answer these questions for myocardium in electrical diastole, extracellular excitation thresholds were determined from measurements of stimulus potentials and activation patterns recorded from 120 transmural electrodes in a 35 X 20 X 5-mm region of the right ventricular outflow tract in six open-chest dogs. Extracellular potential gradients, current densities, energies, and their components longitudinal and transverse to the local fiber orientation at each recording site were calculated from the stimulus potentials produced by 3-msec constant-current stimuli. The resulting values in regions directly excited by the stimulus field were compared with the values in regions not directly excited but activated by the spread of wavefronts conducting away from the directly excited region. Magnitudes of 3.66 mA/cm2 for current density, 9.7 microJ/cm3 for energy, and 804 mV/cm for potential gradient yielded minimum misclassifications of 8%, 13%, and 17%, respectively, of sites directly and not directly excited. A linear bivariate combination of the longitudinal (l) and transverse (t) components of the potential gradient yielded 7% misclassification (threshold ratio t/l of 2.88), and linear combination of corresponding current density components yielded 8% misclassification (threshold ratio t/l of 1.04). Anodal and cathodal thresholds were not significantly different (p = 0.39). Potential gradient, current density, and energy strength-duration curves were constructed for pulse durations (D) of 0.2-20 msec. The best fit hyperbolic curve for current density magnitude (Jm) was Jm = 3.97/D + 3.15, where Jm is in mA/cm2, and D is in msec. Thus, for stimulation during electrical diastole 1) both current density magnitude and longitudinal and transverse components of the potential gradient are closely correlated with excitation, 2) the extracellular potential gradient along cardiac cells has a lower threshold than across cells, while current density thresholds along and across cells are similar, 3) anodal and cathodal thresholds are approximately equal for stimuli greater than or equal to 5 mA, and 4) the extracellular potential gradient, current density, and energy excitation thresholds can be expressed by strength-duration equations.

Action Potentials↗
PubMed1994

The mechanism of termination of reentrant activity in ventricular fibrillation.

The reentrant wave fronts in ventricular fibrillation (VF) have only a limited life span. The mechanisms by which these reentrant wave fronts terminate are unknown. We performed computerized mapping studies in six open-chest dogs before and after right ventricular subendocardial ablation with Lugol's solution. Recordings were made with 56 bipolar electrodes separated by 3 mm. Baseline pacing was performed on the right side of the tissue to create parallel activation wave fronts. A premature 50-V shock of either anodal or cathodal polarity was given to a bar electrode on the upper edge of the tissue. Counterclockwise reentrant wave fronts and VF were induced both before (60 episodes) and after (57 episodes) subendocardial ablation with either anodal or cathodal shocks. Among these reentrant wave fronts, 8 episodes before and 10 episodes after ablation had over 10 rotations (P = NS). The reentrant wave fronts in other episodes terminated with an average of 3.2 +/- 1.9 rotations before and 3.1 +/- 1.8 rotations after the ablation (P = NS). The reentrant wave-front cycle length was 118 +/- 19 milliseconds before and 124 +/- 20 milliseconds after ablation (P = .001). Conduction block occurred when the wave front was traveling across the myocardial fibers. When conduction was blocked in these episodes, the leading edge of the reentrant wave front encountered tissue that had been excited within the past 58 +/- 12 milliseconds (range, 28 to 77 milliseconds), which corresponded to 47 +/- 12% of the preceding VF cycle length. This period was significantly shorter than the recovery period in the same region that had allowed conduction (91 +/- 19 milliseconds; range, 48 to 137 milliseconds), which corresponded to 72 +/- 18% of the preceding VF cycle length (P < .001). In nine episodes, reentrant wave-front activity terminated when wave fronts that had originated from outside the mapped tissue interfered with the reentrant pathways. Conclusions are as follows: (1) The refractory period of fibrillating ventricular muscle ranges from 48 to 77 milliseconds. Because the refractory period is much shorter than the VF cycle length, a large excitable gap is present in the reentrant circuit. The presence of a large excitable gap contributes to reentrant wave-front termination. (2) Myocardial fiber orientation is an important determinant of the site of conduction block. (3) Although subendocardial ablation slowed the wave-front propagation, it did not prevent the generation and the maintenance of reentry and VF.

Animals↗
PubMed1998

Spatial changes in the transmembrane potential during extracellular electric stimulation.

The purpose of this study was to determine the spatial changes in the transmembrane potential caused by extracellular electric field stimulation. The transmembrane potential was recorded in 10 guinea pig papillary muscles in a tissue bath using a double-barrel microelectrode. After 20 S1 stimuli, a 10-ms square wave S2 shock field with a 30-ms S1-S2 coupling interval was given via patch shock electrodes 1 cm on either side of the tissue during the action potential plateau. Two shock strengths (2.1+/-0.2 and 6.5+/-0.6 V/cm) were tested with both shock polarities. The recording site was moved across the tissue along fibers with either 200 micrometer (macroscopic group [n=5], 12 consecutive recording sites over a 2. 2-mm tissue length in each muscle) or 20 micrometer (microscopic group [n=5], 21 consecutive recording sites over a 0.4-mm tissue length in each muscle) between adjacent recording sites. In the macroscopic group, the portion of the tissue toward the anode was hyperpolarized, whereas the portion toward the cathode was depolarized, with 1 zero-potential crossing from hyperpolarization to depolarization present near the center of the tissue. In the microscopic group, only 1 zero-potential crossing was observed in the center region of the tissue, whereas, away from the center, only hyperpolarization was observed toward the anode and depolarization toward the cathode. Although these results are consistent with predictions from field stimulation of continuous representations of myocardial structure, ie, the bidomain and cable equation models, they are not consistent with the prediction of depolarization-hyperpolarization oscillation from representations based on cellular-level resistive discontinuities associated with gap junctions, ie, the sawtooth model.

Animals↗
PubMed2002

Fabrication and properties of spray-dried nanofeatured spherical Ni(OH)2 materials.

Spherical agglomerates of nanostructured beta-phase Ni(OH)2 with the general formula Ni1-xCox(OH)2 (x = 0, 0.1, 0.3) for use as cathode materials were produced by a modified method including coprecipitation of Ni or Ni composite hydroxide and further spray drying of the precipitated and washed slurry. This process leads to the formation of spherical agglomerate particles with a narrow Gaussian-type distribution range. The method permits faster and cheaper production of cathode materials with a higher specific surface area and similar or better capacity and cycle life compared with the materials prepared via conventional technology.

Aerosols↗
PubMed2006

Nanomaterials for lithium-ion rechargeable batteries.

In lithium-ion batteries, nanocrystalline intermetallic alloys, nanosized composite materials, carbon nanotubes, and nanosized transition-metal oxides are all promising new anode materials, while nanosized LiCoO2, LiFePO4, LiMn2O4, and LiMn2O4 show higher capacity and better cycle life as cathode materials than their usual larger-particle equivalents. The addition of nanosized metal-oxide powders to polymer electrolyte improves the performance of the polymer electrolyte for all solid-state lithium rechargeable batteries. To meet the challenge of global warming, a new generation of lithium rechargeable batteries with excellent safety, reliability, and cycling life is needed, i.e., not only for applications in consumer electronics, but especially for clean energy storage and for use in hybrid electric vehicles and aerospace. Nanomaterials and nanotechnologies can lead to a new generation of lithium secondary batteries. The aim of this paper is to review the recent developments on nanomaterials and nanotechniques used for anode, cathode, and electrolyte materials, the impact of nanomaterials on the performance of lithium batteries, and the modes of action of the nanomaterials in lithium rechargeable batteries.

Electric Power Supplies↗
PubMed2006

Modeling of the anodic arc discharge and conditions for single-wall carbon nanotube growth.

A model of the arc discharge used for a single wall carbon nanotube (SWNT) synthesis is developed. Coupling solution of the non-equilibrium, Knudsen layer, with hydrodynamic layer and discharge column provides self-consistent solution for the ablation rate and plasma parameter distribution. It is predicted that the interelectrode gap decreases with the background pressure increase. Conditions for single wall carbon nanotube formation in the arc discharge method of nanotube synthesis are described. Carbon nanotube seed formation and charging in the interelectrode gap are found to be very important effects that may alter carbon nanotube formation in the cathode region. This model predicts that the long carbon nanotubes in the high pressure Helium environment can be deposited on the cathode surface. Model predictions are found to be in agreement with experiment.

Carbon↗
PubMed1989

Identification of a single nucleotide change in the hypoxanthine-guanine phosphoribosyltransferase gene (HPRTYale) responsible for Lesch-Nyhan syndrome.

Complete deficiency of hypoxanthine-guanine phosphoribosyltransferase (HPRT) causes the Lesch-Nyhan syndrome. Previous characterization of a mutant form of HPRT, HPRTYale, from a subject with the Lesch-Nyhan syndrome revealed normal mRNA and protein concentrations, no residual catalytic activity, and cathodal migration upon PAGE. We have cloned and sequenced HPRTYale cDNA. The nucleotide sequence of full-length HPRTYale cDNA revealed a single nucleotide substitution compared with normal HPRT cDNA: G----C at nucleotide position 211. This transversion predicts substitution of arginine for glycine at amino acid position 71, explaining the cathodal migration of HPRTYale. Chou-Fasman secondary structure analysis predicts a change in the probability of beta-turn formation in the region containing the mutation. Inclusion of the bulky arginine side chain in place of glycine probably disrupts protein folding as well. Cloning mutant forms of cDNA allows identification of specific mutations, provides insight into mutational mechanisms, and facilitates structure-function analysis of mutant proteins.

DNA↗
PubMedDate not supplied

In vivo effects of direct current in the mandible.

The application of low level direct current (3 to 5 mua in situ, that is, 50 mua/cm2), within the mandible of mature Beagle dogs results in an increased osteogenesis at the cathode (negative electrode) when compared to responses about nonactive (control) packs within the same dog. The increased osteogenesis suggests a stimulation of cellular activity rather than the electrophoretic migration of cells. Significant differences observed between platinum-iridium and stainless-steel electrodes seem to suggest that faradaic results play little or no role in the osteogenic response at the platinum-iridium cathode. Conversely, at all other electrodes, faradaic reactions compete to some extent with an osteogenic response. Careful consideration of current density and electrode composition must be taken into account when direct current stimulation is to be used.

Animals↗
PubMedDate not supplied

Clinical application and dosimetric calibration procedure of the superficial and orthovoltage therapy unit Therapax DXT300.

AIMS AND BACKGROUND: The aim of this study was to configure a new superficial and orthovoltage therapy unit for clinical use and discuss the clinical indications for this kind of energy. There is renewed interest in radiotherapy using photon beams in the range from 40 to 300 kVp, in particular for the treatment of non-neoplastic diseases and superficial lesions. This is due to the fact that the latest units are of good quality, relatively cheap and reliable in comparison with alternative equipment. It is therefore necessary to document the steps involved in the clinical application of this therapeutic equipment. METHODS: The calibration procedure for a new superficial/orthovoltage therapy unit, Therapax DXT300 (Pantak, USA), installed at the Radiotherapy Department of the Mauriziano Hospital in Turin, was carried out by measurement of beam quality (half-value layer, HVL), percentage depth dose (PDD), profiles, internal dosimetry system, dose rate calibration and output factors. The Therapax DXT300 can be programmed to stop treatment either by time or dose, like a linear accelerator. It is equipped with one adjustable collimator (2 x 2 divided by 20 x 20 cm2) for orthovoltage therapy (focus skin distance, FSD = 50 cm) and six fixed applicators for superficial and orthovoltage therapy (FSD = 30 and 50 cm, respectively). Up to eight combinations of generating potential, tube current and added beam filter can be set. RESULTS: In the range of accelerating potentials from 40 to 300 kVp the Therapax provides beams with HVL ranging from 1.48 mm Al to 3.68 mm Cu. As regards the PDD curves, a slight difference between PDD values has been observed with potentials ranging from 200 to 300 kVp. The beam symmetry and flatness are almost the same in Y and X plane directions for accelerating potentials of less than 200 kVp. At higher kVp values these parameters are significantly worse in the anode-cathode axis direction, because the useful X-ray beam is extracted perpendicular to the anode-cathode axis direction: as the energy increases, the bremsstrahlung becomes more forward directed, resulting in a higher dose rate on the anode side. CONCLUSION: The present paper suggests a methodological approach for the clinical application of an orthovoltage/superficial therapy unit and discusses its current indications. It is necessary to maintain the performance of the equipment within predefined limits in order to meet the requirements of an efficient quality assurance program. This unit is particularly useful in the treatment of superficial lesions and non-neoplastic diseases and in palliative care (eg for bone metastases).

Calibration↗
PubMed2005

Bifrontal transcranial direct current stimulation slows reaction time in a working memory task.

BACKGROUND: Weak transcortical direct current stimulation (tDCS) applied to the cortex can shift the membrane potential of superficial neurons thereby modulating cortical excitability and activity. Here we test the possibility of modifying ongoing activity associated with working memory by tDCS. The concept of working memory applies to a system that is capable of transiently storing and manipulating information, as an integral part of the human memory system. We applied anodal and cathodal transcranial direct current (tDCS) stimulation (260 microA) bilaterally at fronto-cortical electrode sites on the scalp over 15 min repeatedly (15 sec-on/15 sec-off) as well as sham-tDCS while subjects performed a modified Sternberg task. RESULTS: Reaction time linearly increased with increasing set size. The slope of this increase was closely comparable for real and sham stimulation indicating that our real stimulation did not effect time required for memory scanning. However, reaction time was slowed during both anodal and cathodal stimulation as compared to placebo (p < 0.05) indicating that real stimulation hampered neuronal processing related to response selection and preparation. CONCLUSION: Intermittent tDCS over lateral prefrontal cortex during a working memory task impairs central nervous processing related to response selection and preparation. We conclude that this decrease in performance by our protocol of intermittent stimulation results from an interference mainly with the temporal dynamics of cortical processing as indexed by event-related sustained and oscillatory EEG activity such as theta.

Adult↗
PubMed2005

Safety and cognitive effect of frontal DC brain polarization in healthy individuals.

BACKGROUND: Data from the human motor cortex suggest that, depending on polarity, direct current (DC) brain polarization can depress or activate cortical neurons. Activating effects on the frontal lobe might be beneficial for patients with frontal lobe disorders. This phase 1 study tested the safety of frontal DC, including its effects on frontal and other brain functions. METHODS: The authors applied 20 minutes of anodal, cathodal, or sham DC to the left prefrontal cortex in three groups of right-handed subjects and looked for effects on global measures of processing and psychomotor speed, emotion, and verbal fluency, a measure of local cortical function. In one experiment (n = 30), the authors tested before and after 1 mA DC and monitored EEG in 9 subjects. In two other experiments using 1 mA (n = 43) and 2 mA (n = 30), the authors tested before and then starting 5 minutes after the onset of DC. RESULTS: All subjects tolerated DC well. There were no significant effects on performance with 1 mA DC. At 2 mA, verbal fluency improved significantly with anodal and decreased mildly with cathodal DC. There were no clinically significant effects on the other measures. CONCLUSIONS: Limited exposure to direct current polarization of the prefrontal cortex is safe and can enhance verbal fluency selectively in healthy subjects. As such, it deserves consideration as a procedure to improve frontal lobe function in patients.

Adult↗
PubMed1975

Chronic cerebellar stimulation in the monkey. Electron microscopic and biochemical observations.

The effects of chronic electrical stimulation to the surface of cerebellum in the Macaca mulatta monkey were studied with morphologic and biochemical techniques. There was considerable damage and loss of Purkinje cells in all specimens examined, including an area without electrodes, but the greatest changes appeared in tissue beneath the cathode and anode. Despite the damage, normal appearing synapses persisted in the molecular layer of all specimens. Fibrous glial processes were more numerous beneath the cathode. There were abnormalities in gamma-amino butyric acid (GABA) and polyamine concentrations in virtually all specimens, consistent with the morphologic evidence of widespread tissue damage.

Animals↗
PubMed2004

Roles of microtubules, cell polarity and adhesion in electric-field-mediated motility of 3T3 fibroblasts.

Direct-current electric fields mediate motility (galvanotaxis) of many cell types. In 3T3 fibroblasts, electric fields increased the proportion, speed and cathodal directionality of motile cells. Analogous to fibroblasts' spontaneous migration, we initially hypothesized that reorientation of microtubule components modulates galvanotaxis. However, cells with intact microtubules did not reorient them in the field and cells without microtubules still migrated, albeit slowly, thus disproving the hypothesis. We next proposed that, in monolayers wounded and placed in an electric field, reorientation of microtubule organizing centers and stable, detyrosinated microtubules towards the wound edge is necessary and/or sufficient for migration. This hypothesis was negated because field exposure mediated migration of unoriented, cathode-facing cells and curtailed migration of oriented, anode-facing cells. This led us to propose that ablating microtubule detyrosination would not affect galvanotaxis. Surprisingly, preventing microtubule detyrosination increased motility speed, suggesting that detyrosination inhibits galvanotaxis. Microtubules might enhance adhesion/de-adhesion remodeling during galvanotaxis; thus, electric fields might more effectively mediate motility of cells poorly or dynamically attached to substrata. Consistent with this hypothesis, incompletely spread cells migrated more rapidly than fully spread cells. Also, overexpression of PAK4, a Cdc42-activated kinase that decreases adhesion, enhanced galvanotaxis speed, whereas its lack decreased speed. Thus, electric fields mediate fibroblast migration via participation of microtubules and adhesive components, but their participation differs from that during spontaneous motility.

Animals↗
PubMed2004

Cellular mechanisms of direct-current electric field effects: galvanotaxis and metastatic disease.

Endogenous direct-current electric fields (dcEFs) occur in vivo in the form of epithelial transcellular potentials or neuronal field potentials, and a variety of cells respond to dcEFs in vitro by directional movement. This is termed galvanotaxis. The passive influx of Ca(2+) on the anodal side should increase the local intracellular Ca(2+) concentration, whereas passive efflux and/or intracellular redistribution decrease the local intracellular Ca(2+) concentration on the cathodal side. These changes could give rise to 'push-pull' effects, causing net movement of cells towards the cathode. However, such effects would be complicated in cells that possess voltage-gated Ca(2+) channels and/or intracellular Ca(2+) stores. Moreover, voltage-gated Na(+) channels, protein kinases, growth factors, surface charge and electrophoresis of proteins have been found to be involved in galvanotaxis. Galvanotactic mechanisms might operate in both the short term (seconds to minutes) and the long term (minutes to hours), and recent work has shown that they might be involved in metastatic disease. The galvanotactic responses of strongly metastatic prostate and breast cancer cells are much more prominent, and the cells move in the opposite direction compared with corresponding weakly metastatic cells. This could have important implications for the metastatic process and has clinical implications. Galvanotaxis could thus play a significant role in both cellular physiology and pathophysiology.

Animals↗
PubMed1997

Integrated interactions between chondroitin sulphate proteoglycans and weak dc electric fields regulate nerve growth cone guidance in vitro.

During development and regenerative growth, neuronal pathways are defined in part by several endogenous cues that collectively determine directed growth. The interactions between such cues largely are unknown. To address potential interactions, we have examined in vitro the combined effect on nerve growth of two endogenous growth cone guidance cues: chondroitin sulphate proteoglycans and weak dc electric fields. Addition to the culture medium of a chondroitin 6-sulphate/keratan sulphate containing PG (BNC-PG) markedly enhanced the cathodal re-orientation of embryonic Xenopus neurites in an electric field, whereas a proteoglycan containing chondroitin 4-sulphate (RC-PG) was inhibitory. These effects of BNC-PG and RC-PG were reproduced by their chondroitin sulphate glycosaminoglycan side chains alone. Chondroitin 6-sulphate or chondroitin 4-sulphate, respectively, enhanced and inhibited cathodally-directed nerve re-orientation. This was dependent on the integrity of the glycosaminoglycan chain structure; when digested into their disaccharide subunits both molecules became inactive. Keratan sulphate, a minor component of BNC-PG, was found to be inhibitory, whereas dermatan sulphate, an epimer of chondroitin 4-sulphate, had no effect. We conclude that in vitro specific interactions between these two nerve guidance cues do occur and that the specificity of the response is critically dependent on the charge pattern of the proteoglycans chondroitin sulphate side chains. The expression of a host of proteoglycans with differing glycosaminoglycan side chains varies in both time and place in the developing nervous system, thus the scope is vast for spatial and temporal modulation of nerve guidance by interacting cues.

Animals↗