Bioelectrical parameters of the whole human body obtained through bioelectrical impedance analysis

Knowledge of electrical properties of body tissues across the frequency spectrum is useful for tissue characterization. The bioelectric impedance analysis method, operating from 1 to 250 kHz (multi-frequency), was used in 23 normal male human subjects between the ages of 21 and 52 years, for estimation of their bioelectrical parameters. Amplitude of the output current was set to 800 microA(RMS). The experimental data showed that bioelectric parameters were highly dependent on frequency and the presence of a threshold frequency around 4 kHz. In order to explain the unusual features observed in our experimental data, the human body was simulated through the Cole-Fricke-Cole model (RC circuit) and the Extended Cole-Fricke-Cole model (RLC circuit). The simulated data showed that the Extended Cole-Fricke-Cole model had a higher accuracy than the traditional Cole-Fricke-Cole model. These results suggest that the unusual features could be due to the possible existence of inductive effects in biological cells and body tissues and that the inductive parameter and the threshold frequency could be used for characterizing the healthy tissues as well as the traditional bioelectric parameters.     

Total body water and ECFV measured using bioelectrical impedance analysis and indicator dilution in horses.

The purposes of this study were 1) to determine the compartmentation of body water in horses by using indicator dilution techniques and 2) to simultaneously measure bioelectrical impedance to current flow at impulse current frequencies of 5 and 200 kHz to formulate predictive equations that could be used to estimate total body water (TBW), extracellular fluid volume (ECFV), and intracellular fluid volume (ICFV). Eight horses and ponies weighing from 214 to 636 kg had catheters placed into the left and right jugular veins. Deuterium oxide, sodium thiocyanate, and Evans blue were infused for the measurement of TBW, ECFV, and plasma volume (PV), respectively. Bioelectrical impedance was measured by using a tetrapolar electrode configuration, with electrode pairs secured above the knee and hock. Measured TBW, ECFV, and PV were 0.677 +/- 0.022, 0.253 +/- 0.006, and 0.040 +/- 0.002 l/kg body mass, respectively. Strong linear correlations were determined among measured variables that allowed for the prediction of TBW, ECFV, ICFV, and PV from measures of horse length or height and impedance. It is concluded that bioelectrical impedance analysis (BIA) can be used to improve the predictive accuracy of noninvasive estimates of ECFV and PV in euhydrated horses at rest.     

Linear electrical properties of passive and active currents in spherical heart cell clusters.

Impedance studies were performed on small spherical clusters of embryonic chick heart cells grown in tissue culture. Each syncytial cluster was impaled with two microelectrodes; one injected low amplitude stochastic current and the other recorded the resulting perturbation of intracellular potential. The current and potential records were digitized, decomposed into their sinusoidal components, and the frequency domain impedance of the cluster was determined. The impedance data were compared with a theory for current flow in a spherical syncytium and values were derived for parameters describing the membranes and intercellular clefts of the tissue. The clusters were spontaneously active but usually became temporarily quiescent when impaled with two electrodes. The potential stabilized at a value close to -30 mV. At this depolarized potential, active slow currents, presumably present in the cardiac action potential, contributed noticeably to the linear impedance, producing a resonant peak in the magnitude of the impedance at a frequency of 1-3 Hz. The linearized impedance functions for these currents were characterized in the presence and absence of tetrodotoxin (TTX) and D-600. TTX had no noticeable effect on the impedance but D-600 essentially abolished the active currents. Although the ionic basis of these currents is not known, frequency domain analysis appears to be a viable technique for studying slow currents in heart muscle.     

Heptaminol hydrochloride as an epithelium transporter

Electrophysiological and transport effects induced by heptaminol hydrochloride were studied in frog epithelium. This tissue, which can easily be maintained in vitro, is a valuable model for studying sodium active transport with hormone-dependent characteristics that reproduce mammalian nephron behavior (notably in areas with tight gap junctions). The two following techniques were used: the Ussing short-circuit current method and the swept-frequency impedance measurement method. Our findings indicate the following. (i) Heptaminol hydrochloride significantly increases the short-circuit current and transepithelial polarization. (ii) This effect develops progressively as the molecule is introduced on the serous side (3Na+/2K+ active countertransport sites). Time to maximum development is approximately 20 min and the electrophysiological effect lasts from 60 to 90 min. (iii) The mean equivalent cationic current rise is larger in sulfate-Ringer (+23 +/- 4.6 microA, p less than 0.01) than in chloride-Ringer (+14 +/- 4.9 microA, p less than 0.05). The increase in short-circuit current is approximately 0.9 muequiv. cm-2 h-1 in sulfate-Ringer. (iv) The increase in mean polarization is greater in chloride (+21 +/- 6.2 mV, p less than 0.02) than in sulfate (+6 +/- 1.5 mV, p less than 0.01) following a diphasic effect on potential. (v) Changes in apical impedance Z are small (-454 +/- 323 omega, nonsignificant) compared with transepithelial resistance in sulfate (-1065 +/- 359 omega, p less than 0.05). (vi) Changes in membrane capacitance reflect changes in the membrane surface. However, no significant capacitance changes are produced in sulfate and chloride solution by heptaminol hydrochloride (-0.04 +/- 0.11 microF and 0.05 +/- 0.11 microF, respectively).(ABSTRACT TRUNCATED AT 250 WORDS)     

Evidence for a central role for electro-osmosis in fluid transport by corneal endothelium

The mechanism of transepithelial fluid transport remains unclear. The prevailing explanation is that transport of electrolytes across cell membranes results in local concentration gradients and transcellular osmosis. However, when transporting fluid, the corneal endothelium spontaneously generates a locally circulating current of approximately 25 microA cm(-2), and we report here that electrical currents (0 to +/-15 microA cm(-2)) imposed across this layer induce fluid movements linear with the currents. As the imposed currents must be approximately 98% paracellular, the direction of induced fluid movements and the rapidity with which they follow current imposition (rise time < or =3 sec) is consistent with electro-osmosis driven by sodium movement across the paracellular pathway. The value of the coupling coefficient between current and fluid movements found here (2.37 +/- 0.11 microm cm(2) hr(-1) microA (-1), suggests that: 1) the local endothelial current accounts for spontaneous transendothelial fluid transport; 2) the fluid transported becomes isotonically equilibrated. Ca(++)-free solutions or endothelial damage eliminate the coupling, pointing to the cells and particularly their intercellular junctions as a main site of electro-osmosis. The polycation polylysine, which is expected to affect surface charges, reverses the direction of current-induced fluid movements. Fluid transport is proportional to the electrical resistance of the ambient medium. Taken together, the results suggest that electro-osmosis through the intercellular junctions is the primary process in a sequence of events that results in fluid transport across this preparation.     

ATP crossing the cell plasma membrane generates an ionic current in xenopus oocytes

The presence of ATP within cells is well established. However, ATP also operates as an intercellular signal via specific purinoceptors. Furthermore, nonsecretory cells can release ATP under certain experimental conditions. To measure ATP release and membrane currents from a single cell simultaneously, we used Xenopus oocytes. We simultaneously recorded membrane currents and luminescence. Here, we show that ATP release can be triggered in Xenopus oocytes by hyperpolarizing pulses. ATP release (3.2 +/- 0.3 pmol/oocyte) generated a slow inward current (2.3 +/- 0.1 microA). During hyperpolarizing pulses, the permeability for ATP(4-) was more than 4000 times higher than that for Cl(-). The sensitivity to GdCl(3) (0. 2 mm) of hyperpolarization-induced ionic current, ATP release and E-ATPase activity suggests their dependence on stretch-activated ion channels. The pharmacological profile of the current inhibition coincides with the inhibition of ecto-ATPase activity. This enzyme is highly conserved among species, and in humans, it has been cloned and characterized as CD39. The translation, in Xenopus oocytes, of human CD39 mRNA encoding enhances the ATP-supported current, indicating that CD39 is directly or indirectly responsible for the electrodiffusion of ATP.     

Endogenous chloride channels of insect sf9 cells. Evidence for coordinated activity of small elementary channel units

The endogenous Cl- conductance of Spodoptera frugiperda (Sf9) cells was studied 20-35 h after plating out of either uninfected cells or cells infected by a baculovirus vector carrying the cloned beta-galactosidase gene (beta-Gal cells). With the cation Tris+ in the pipette and Na+ in the bath, the reversal potential of whole-cell currents was governed by the prevailing Cl- equilibrium potential and could be fitted by the Goldman-Hodgkin-Katz equation with similar permeabilities for uninfected and beta-Gal cells. In the frequency range 0.12 < f < 300 Hz, the power density spectrum of whole-cell Cl- currents could be fitted by three Lorentzians. Independent of membrane potential, >50% of the total variance of whole-cell current fluctuations was accounted for by the low frequency Lorentzian (fc = 0.40 +/- 0.03 Hz, n = 6). Single-Cl- channels showed complex gating kinetics with long lasting (seconds) openings interrupted by similar long closures. In the open state, channels exhibited fast burst-like closures. Since the patches normally contained more than a single channel, it was not possible to measure open and closed dwell-time distributions for comparing single-Cl- channel activity with the kinetic features of whole-cell currents. However, the power density spectrum of Cl- currents of cell-attached and excised outside-out patches contained both high and low frequency Lorentzian components, with the corner frequency of the slow component (fc = 0.40 +/- 0.02 Hz, n = 4) similar to that of whole-cell current fluctuations. Chloride channels exhibited multiple conductance states with similar Goldman-Hodgkin-Katz-type rectification. Single-channel permeabilities covered the range from approximately 0.6.10(-14) cm5/s to approximately 6.10(-14) cm3/s, corresponding to a limiting conductance (gamma 150/150) of approximately 3.5 pS and approximately 35 pS, respectively. All states reversed near the same membrane potential, and they exhibited similar halide ion selectivity, P1 > PCl approximately PBr. Accordingly, Cl- current amplitudes larger than current flow through the smallest channel unit resolved seem to result from simultaneous open/shut events of two or more channel units.     

Presumptive neurons derived by differentiation of a human embryonal carcinoma cell line exhibit tetrodotoxin-sensitive sodium currents and the capacity for regenerative responses

Cloned human embryonal carcinoma cells (NTERA-2 cl.D1) differentiate into neuron-like cells upon exposure to retinoic acid. Using whole-cell patch-clamp techniques, these putative neurons exhibited rapidly activating and inactivating inward currents upon depolarization as well as outward currents. The electrical characteristics and tetrodotoxin (TTX) sensitivity of the inward currents suggest that they were sodium currents. By contrast, only outward potassium currents were seen in the undifferentiated stem cells. Under current clamp conditions, the neuron-like cells showed regenerative responses. The peaks of these responses never exceeded the O-mV level, perhaps due to the low mean inward current density of 93.8 +/- 17.8 (SEM) microA/cm2:n = 9. The electrophysiological characteristics of these human teratocarcinoma-derived neuron-like cells were consistent with our previous identification of these cells as neurons, but suggest that they may resemble immature embryonic, rather than adult, neurons.     

Artificial gills for robots: MFC behaviour in water

This paper reports on the first stage in developing microbial fuel cells (MFCs) which can operate underwater by utilizing dissolved oxygen. In this context, the cathodic half-cell is likened to an artificial gill. Such an underwater power generator has obvious potential for autonomous underwater robots. The electrical power from these devices increased proportionately with water flow rate, temperature and salinity. The current output at ambient temperature (null condition) was 32 microA and this increased by 200% (approximately 100 microA) as a result of a corresponding temperature increase (DeltaT) of 52 degrees C. Similarly, the effect of increasing the water flow rate resulted in an increase in the MFC output ranging from 135% to 150%. Furthermore, the same positive effect was recorded when artificial seawater was used instead, in which case the increase in the MFC current output was >100% (from 32 to 65 microA). There was a distinct difference in the MFC performance when operated under low turbulent as opposed to high turbulent flow rates. These findings can be advantageous in the design of underwater autonomous robots.     

Effect of an electric field on the motility of Entamoeba histolytica examined by multiple-beam interference microscopy

A recently developed multiple-beam interference microscopic technique has been used to visualize submicroscopic structures of Entamoeba histolytica and their movements in applied external electric fields. The movements were videorecorded and it was found that at low current (120 microA) pseudopods are filled with hyaline ectoplasm. At slightly higher current (about 150 microA), the amoeba stops extending the pseudopods and loosens its attachment to the surface. At higher currents (200 microA), it forms a cyst and remains immobile for a time. Before this stage is reached a narrow ring is formed around the nucleus due to alterations in the proteins to protect it.     

Equation for estimating total body water by bioelectrical impedance measurements in Japanese subjects]

This article reports a study in which the equation for total body water (TBW) estimated from deuterium (2H2O)-dilution method and bioelectrical impedance measurement (BIM) is described. Subjects were 60 healthy males aged 30 +/- 18.3 yr (18-74) and 31 healthy females aged 37 +/- 17.5 yr (19-70). Total body water determined by the analysis of the dilution of orally ingested deuterium oxide (1g2H2O, 99.75 atom % excess/kg body weight) in urine. Bioelectrical impedance was measured for each subjects in a supine position using an electrical impedance analyzer (500 microA, 50kHz, T-1988K, Toyo Physical Inc.) with a four electrodes (Y-250, Nihon Kohden). The mean values of total body water and the impedance in males and females subjects were 34.1 +/- 4.27 l and 25.7 +/- 2.42 l, 567 +/- 28.5 omega and 562 +/- 32.5 omega, respectively. Height squared divided by resistance (Ht2/R) correlated well with TBW as measured by 2H2 O, r = 0.530 (p less than 0.001) in males and r = 0.782 (p less than 0.001) in females. The best-fitting regression equation to predict TBW comprised Ht2/R(X1) and body weight (X2) (R = 0.915, SEE = 1.70 l in males and R = 0.834, SEE = 1.28 l in females). Equations were provided with BIM instrument for the prediction of TBW: for males TBW, l = 0.1983X1 + 0.4004X2 - 0.7938 and for females TBW, l = 0.3536X1 + 0.1269X2 + 3.3417. These results suggest that bioelectrical impedance measurement is a useful measure of total body water in Japanese subjects.     

Improved frequency response of pneumotachometers by digital compensation

To measure impedance one measures or estimates flow, which is commonly done by measuring the pressure drop across a pneumotachometer. The frequency response characteristics of standard pneumotachometer/pressure transducers (PPT) limit their use to relatively low frequencies. Also, the frequency response of PPTs has been reported to be "load" dependent. Thus, the frequency response characteristics measured under "no-load" conditions, which theoretically could be used to compensate subsequent measurements, may not be appropriate for measurements made under loaded conditions. Another method of measuring impedance exists which depends on a reference impedance element other than a pneumotachometer. In this method, an oscillatory flow signal with known amplitude is generated and used to force the system being tested. Unlike PPTs, this oscillatory flow generator (OFG) is a closed system that allows measurements to be made only during breath holding. Our objective was to determine whether the frequency response of a PPT could be compensated using measurements made under no-load conditions, such that it accurately measured an impedance load. The frequency response of the PPT under no-load conditions was measured by the OFG and used to compensate the output of the PPT in subsequent impedance measurements. The compensated PPT was used to measure the impedance of a mechanical structure and the impedances of four human subjects. The impedances of the mechanical structure and the subjects were also measured using the OFG.(ABSTRACT TRUNCATED AT 250 WORDS)     

Induced current measurements in whole body exposure condition to radio frequency electric fields.

The current induced in a human exposed to radio frequency electric fields has been studied by the use of a stripline, in which whole body exposure to vertical electric fields (3-27 MHz) can be produced. We have examined two different techniques to measure the induced current; parallel plate meters and current probes. When the subject has good connection to the ground, the choice of measurement technique is not crucial, since there are only minor differences in readings between the instruments. But when the subject is wearing shoes and/or standing on a wooden plate, the difference between the instruments increases considerably. The difference can mainly be explained by the capacitive coupling between the parallel plate meters and the ground; therefore, the current probes are preferred when the subject does not have perfect contact with the ground. Since the International Commission on Non-Ionizing Radiation Protection guidelines demand measurements of induced current in humans exposed to radio frequency fields in the range of 10-110 MHz, the importance of finding an appropriate measurement procedure becomes apparent.     

Electric field induced desorption of bacteria from a conditioning film covered substratum.

Desorption of three oral bacterial strains from a salivary conditioning film on an indium tin oxide electrode during application of a positive (bacterial adhesion to the anode) or a negative electric current was studied in a parallel plate flow chamber. Bacterial adhesion was from a flowing suspension of high ionic strength, after which the bacterial suspension was replaced by a low ionic strength solution without bacteria and currents ranging from -800 to +800 microA were applied. Streptococcus oralis J22 desorbed during application of a positive and negative electric current with a desorption probability that increased with increasing electric current. Two actinomyces strains, however, could not be stimulated to desorb by the electric currents applied. The desorption forces acting on adhering bacteria are electroosmotic in origin and working parallel to the electrode surface in case of a positive current, whereas they are electrophoretic and electrostatic in origin and working perpendicular to the surface in case of a negative current. By comparison of the effect of positive and negative electric currents, it can be concluded that parallel forces are more effective in stimulating bacterial desorption than perpendicular forces. The results of this study point to a new pathway of cleaning industrial and biomedical surfaces without the use of detergents or biocides.     

Ionic current of an identifiable giant neurone, d-RPLN, of an African giant snail (Achatina fulica Férussac), measured under voltage clamping--II. Outward currents

1. The outward currents of d-RPLN (dorsal-right parietal large neurone), one of the largest identifiable neurones of an African giant snail, were studied. 2. At the holding potential (-90 mV) and at the command voltage (Vc20 mV), the current values were 3.05 +/- 0.13 microA (M +/- SE) for the peak (n = 38), and 1.96 +/- 0.10 microA for the plateau (n = 37). 3. The peak time constant (Vc = 0 mV) was 2.05 +/- 0.08 msec. 4. Tetraethylammonium at 50 mM reduced the plateau value up to 50-55% of the normal, but had little effect on the peak. 5. 5-Aminopyridine at 5.0 mM diminished the peak value to about 50-55%, and delayed the peak time. 6. Quinine at 0.25 mM decreased both the peak and the plateau approximately to 55-65% of their controls, but shortened the peak time when Vc was beyond 0 mV, in contrast to the case of 4-AP. 7. The calcium-free state (replaced with cobalt) reduced these currents to about 75% of the normal, and evidently delayed the peak time.     

Measuring Visceral and Hepatic Fat in Clinical Practice and Clinical Research

ObjectiveTo review how visceral and hepatic fat are measured in clinical practice and clinical research.MethodsWe examine different methods employed to assess visceral and hepatic fat in the literature.ResultsFat in the human body is located in 2 main compartments: subcutaneous and visceral, which also includes liver fat. Visceral and liver fats are associated with the metabolic complications of obesity like hypertension, diabetes, and atherosclerosis. Therefore, there is a need to detect those fats early in life before the development of cardiometabolic syndrome (CMS). Many modalities have been proposed to measure visceral and liver fat. Indirect measurements can be done through waist circumference (WC), dual-energy X-ray absorptiometry (DEXA), ultrasound, and bioelectric impedance, whereas direct methods include computed tomography (CT) and magnetic resonance imaging (MRI). An ideal measurement method should be noninvasive, reliable, suitable for all body sizes, widely available, cost and time effective, show low variability, and have no or limited radiation exposure.ConclusionMeasuring visceral and liver fat is not a straightforward procedure in clinical practice or research; several variables may affect measure accuracy and validity. (Endocr Pract. 2013;19:587-595)     

Flow-activated chloride channels in vascular endothelium. Shear stress sensitivity, desensitization dynamics, and physiological implications

Although activation of outward rectifying Cl(-) channels is one of the fastest responses of endothelial cells (ECs) to shear stress, little is known about these channels. In this study, we used whole-cell patch clamp recordings to characterize the flow-activated Cl(-) current in bovine aortic ECs (BAECs). Application of shear stress induced rapid development of a Cl(-) current that was effectively blocked by the Cl(-) channel antagonist 5-nitro-2-(3-phenopropylamino)benzoic acid (100 microM). The current initiated at a shear stress as low as 0.3 dyne/cm(2), attained its peak within minutes of flow onset, and saturated above 3.5 dynes/cm(2) approximately 2.5-3.5-fold increase over pre-flow levels). The Cl(-) current desensitized slowly in response to sustained flow, and step increases in shear stress elicited increased current only if the shear stress levels were below the 3.5 dynes/cm(2) saturation level. Oscillatory flow with a physiological oscillation frequency of 1 Hz, as occurs in disturbed flow zones prone to atherosclerosis, failed to elicit the Cl(-) current, whereas lower oscillation frequencies led to partial recovery of the current. Nonreversing pulsatile flow, generally considered protective of atherosclerosis, was as effective in eliciting the current as steady flow. Measurements using fluids of different viscosities indicated that the Cl(-) current is responsive to shear stress rather than shear rate. Blocking the flow-activated Cl(-) current abolished flow-induced Akt phosphorylation in BAECs, whereas blocking flow-sensitive K(+) currents had no effect, suggesting that flow-activated Cl(-) channels play an important role in regulating EC flow signaling.     

Quantitative measurements of NO reaction kinetics with a Clark-type electrode.

Nitric oxide (NO) plays important physiological roles in the body. Knowledge regarding the kinetics of NO catabolism is important for understanding the biological functions of NO. Clark-type NO electrodes have been frequently employed in measuring the kinetics of NO reactions; however, the slow response time of these electrodes can cause measurement errors and limit the application of the electrode in measurements of fast NO reactions. In this study, a simplified diffusion model is given for describing the response process of the NO electrode to the change of NO concentration. The least-square method is used in fitting the currents calculated from the diffusion equation to the experimental curves for determining the diffusion parameters and rate constants. The calculated currents are in excellent accordance with the experimental curves for different NO reaction kinetics. It has been demonstrated that when using an NO electrode with a response time of approximately 6 s to measure fast NO reactions with a half-life of approximately 1s, the response currents of the electrode have large differences compared to the curve of actual NO concentration in the solution; however, the rate constant of NO decay can still be accurately determined by computer simulations with the simplified diffusion model. Theoretical analysis shows that an NO electrode with a response time of 6 s (D/L2=0.06 s-1) and the lowest detection limit of 1 nM NO can be used in measuring kinetics of extremely rapid NO reactions with a half-life below 10 ms.     

The AC Impedance of Frog Skin and Its Relation to Active Transport

The AC electrical impedance of frog skin was measured in the range 1 cycle/second to 50 kc/second by injecting current sinusoidally at low current density. The behavior of the skin was found to be linear so the usual concepts of impedance could be validly employed. In the range 1 cycle/second to 5 kc/second, the impedance traces out a circular arc locus with its center off the real axis; thus the skin could be represented by a series resistance and a parallel combination of a conductance and a phase shift element. The phase shift element has an impedance angle of about 80 degrees , current leading voltage, with an equivalent capacitance of about 2 muf/cm(2). The phase shift and the equivalent capacitance were independent of the experimental conditions. The parallel conductance, which was responsible for most of the low frequency impedance, could be subdivided into two approximately equal conductances, one associated with sodium ion current and the other associated with chloride ion current. Both currents were determined mainly by the concentrations of the respective ions bathing the outside of the skin. The response to changes in concentration and the response to CO(2) indicated that the chloride current was passive, but the sodium current appeared to be associated with the active transport mechanism; little sodium could pass through the skin unless associated with active transport.     

Endogenous electrical currents and the resultant voltage gradients in the chick embryo

We have studied some of the electrophysiological properties of 2 1/2- to 4-day-old (stage 14-22) chick embryos. Using a recently developed two-dimensional vibrating probe, large currents were found to exit the posterior intestinal portal (p.i.p.) during the period of tail gut reduction. During this period, epithelial cells lining cloacal regions of the hindgut are dying, thus creating a low-resistance pathway for current flow out of the embryo. Currents entered the intact epithelium over other regions of the embryo. The outward currents at the p.i.p. were first detected at stage 15 and reached their average maximum current density of 112 +/- 10 microA/cm2 at stage 17. After stage 17, the magnitude of the currents decreased, dropping to 16 +/- 0.3 microA/cm2 by stage 22. The currents were reversibly reduced by about 50% when Na+ was replaced by choline in the bathing solution. The magnitude of the currents leaving the p.i.p. suggested the existence of a measurable intraembryonic voltage gradient. The transepithelial potential (TEP) of stage 14-21 embryos was measured lateral to the neural tube through the dorsal ectoderm. For all stages, the combined average TEP was 16 +/- 0.5 mV. Differences in the TEP between various regions of the embryo were used to calculate an intraembryonic voltage gradient. At stage 14, before outward current was found at the p.i.p., no significant intraembryonic voltage gradient was detected. At stage 17, when the outward current at the p.i.p. was maximum, a voltage gradient of 21 +/- 5 mV/mm (mean +/- SEM; N = 6) was measured in the caudal end of the embryo. This gradient in some cases was as steep as 33 mV/mm. This is well above the minimum level needed to affect the direction of embryonic cell migration in vitro. We hypothesize that this endogenous electrical field acts as a directional cue for neural crest cell movements in the developing chick embryo.