scholarly journals Active and passive electrical properties of single bullfrog atrial cells.

1981 ◽  
Vol 78 (1) ◽  
pp. 19-42 ◽  
Author(s):  
J R Hume ◽  
W Giles
Keyword(s):  
Rana Catesbeiana ◽  
Single Cells ◽  
Input Resistance ◽  
Isolated Cells ◽  
Atrial Cells ◽  
Long Duration ◽  
Electrophysiological Measurements ◽  
3 Omega ◽  
Passive Electrical Properties ◽  
Atrial Cell

Single cells from the bullfrog (Rana catesbeiana) atrium have been prepared by using a modification of the enzymatic dispersion procedure described by Bagby et al. (1971. Nature [Long.]. 234:351--352) and Fay and Delise (1973. Proc. Natl. Acad. Sci. U.S.A. 70:641--645). Visualization of relaxed cells via phase-contrast or Nomarski optics (magnification, 400--600) indicates that cells range between 150 and 350 micrometers in length and 4 and 7 micrometers in diameter. The mean sarcomere length in relaxed, quiescent atrial cells in 2.05 micrometer. Conventional electrophysiological measurements have been made. In normal Ringer's solution (2.5 mM K+, 2.5 mM Ca++) acceptable cells have stable resting potentials of about -88 mV, and large (125 mV) long-duration (approximately 720 ms) action potentials can be elicited. The Vm vs. log[K+]0 relation obtained from isolated cells is similar to that of the intact atrium. The depolarizing phase of the action potential of isolated atrial myocytes exhibits two pharmacologically separable components: tetrodotoxin (10(-6) g/ml) markedly suppresses the initial regenerative depolarization, whereas verapamil (3 x 10(-6) M) inhibits the secondary depolarization and reduce the plateau height. A bridge circuit was used to estimate the input resistance (220 +/- 7 M omega) and time constant 20 +/- 7 ms) of these cells. Two-microelectrode experiments have revealed small differences in the electrotonic potentials recorded simultaneously at two different sites within a single cell. The equations for a linear, short cable were used to calculate the electrical constants of relaxed, single atrial cells: lambda = 921.3 +/- 29.5 micrometers; Ri = 118.1 +/- 24.5 omega cm; Rm = 7.9 +/- 1.2 x 10(3) omega cm2; Cm = 2.2 +/- 0.3 mu Fcm-2. These results and the atrial cell morphology suggest that this preparation may be particularly suitable for voltage-clamp studies.

Electrical interactions between a rabbit atrial cell and a nodal cell model

1998 ◽  
Vol 274 (6) ◽  
pp. H2152-H2162 ◽  
Author(s):  
Ronald W. Joyner ◽  
Rajiv Kumar ◽  
David A. Golod ◽  
Ronald Wilders ◽  
Habo J. Jongsma ◽  
...  
Keyword(s):  
Action Potentials ◽  
Cycle Length ◽  
Cell Model ◽  
Stimulus Frequency ◽  
Input Resistance ◽  
Sa Node ◽  
Atrial Cells ◽  
Model Cell ◽  
Atrial Cell ◽  
Basic Cycle Length

Atrial activation involves interactions between cells with automaticity and slow-response action potentials with cells that are intrinsically quiescent with fast-response action potentials. Understanding normal and abnormal atrial activity requires an understanding of this process. We studied interactions of a cell with spontaneous activity, represented by a “real-time” simulation of a model of the rabbit sinoatrial (SA) node cell, simultaneously being electrically coupled via our “coupling clamp” circuit to a real, isolated atrial myocyte with variations in coupling conductance ( G c) or stimulus frequency. The atrial cells were able to be driven at a regular rate by a single SA node model (SAN model) cell. Critical G c for entrainment of the SAN model cell to a nonstimulated atrial cell was 0.55 ± 0.05 nS ( n = 7), and the critical G c that allowed entrainment when the atrial cell was directly paced at a basic cycle length of 300 ms was 0.32 ± 0.01 nS ( n = 7). For each atrial cell we found periodic phenomena of synchronization other than 1:1 entrainment when G c was between 0.1 and 0.3 nS, below the value required for frequency entrainment, when the atrial cell was directly driven at a basic cycle length of either 300 or 600 ms. In conclusion, the high input resistance of the atrial cells allows successful entrainment of nodal and atrial cells at low values of G c, but further uncoupling produces arrhythmic interactions.

scholarly journals The use of a slide spinner in the analysis of cell dispersion.

1976 ◽  
Vol 24 (1) ◽  
pp. 11-15 ◽  
Author(s):  
R C Wolley ◽  
H M Dembitzer ◽  
F Herz ◽  
K Schreiber ◽  
L G Koss
Keyword(s):  
Cell Suspension ◽  
Single Cells ◽  
Cell Loss ◽  
Optimum Conditions ◽  
Isolated Cells ◽  
Cell Dispersion ◽  
Cervical Cancer Cells ◽  
A Cell ◽  
Human Cervical Cancer Cells ◽  
Human Cervical Cancer

A simple and reliable method of determining the degree of dispersion of a cell suspension has been developed using the Perkin-Elmer Uni-Smear Spinner. Optimum conditions regarding rate and duration of spin, etc., were first ascertained using dispersed cell cultures including human cervical cancer cells as well as gynecologic samples. After spinning, single cells in suspension appeared as isolated cells on the slides. Cell aggregates, on the other hand, remained together. Therefore, the distribution of cells in various sized aggregates could be easily quantitated and the slides retained for future review. This method was used to evaluate the dispersing effects of trypsin, ethylenediaminetetraacetate and and syringing human on human gynecology samples obtained by routine cervical scrapes. None of the dispersion methods has, so far, produced an adequate monodispersed cell suspension without unacceptable cell loss.

scholarly journals "Creep currents" in single frog atrial cells may be generated by electrogenic Na/Ca exchange.

1986 ◽  
Vol 87 (6) ◽  
pp. 857-884 ◽  
Author(s):  
J R Hume ◽  
A Uehara
Keyword(s):  
Voltage Clamp ◽  
Time Course ◽  
Single Cells ◽  
Mechanical Activity ◽  
Common Mechanism ◽  
Mechanical Relaxation ◽  
Equilibrium Conditions ◽  
Atrial Cells ◽  
Current Voltage ◽  
Wide Range

The objective of these experiments was to test the hypothesis that the "creep currents" induced by Na loading of single frog atrial cells (Hume, J. R., and A. Uehara. 1986. Journal of General Physiology. 87:833) may be generated by an electrogenic Na/Ca exchanger. Creep currents induced by Na loading were examined over a wide range of membrane potentials. During depolarizing voltage-clamp pulses, outward creep currents were observed, followed by inward creep currents upon the return to the holding potential. During hyperpolarizing voltage-clamp pulses, creep currents of the opposite polarity were observed: inward creep currents were observed during the pulses, followed by outward creep currents upon the return to the holding potential. The current-voltage relations for inward and outward creep currents in response to depolarizing or hyperpolarizing voltage displacements away from the holding potential all intersect the voltage axis at a common potential, which indicates that inward and outward creep currents may have a common reversal potential under equilibrium conditions and may therefore be generated by a common mechanism. Measurements of inward creep currents confirm that voltage displacements away from the holding potential rapidly alter equilibrium conditions. Current-voltage relationships of inward creep currents after depolarizing voltage-clamp pulses are extremely labile and depend critically upon the amplitude and duration of outward creep currents elicited during preceding voltage-clamp pulses. An optical monitor of mechanical activity in single cells revealed (a) a similar voltage dependence for the outward creep currents induced by Na loading and tonic contraction, and (b) a close correlation between the time course of the decay of the inward creep current and the time course of mechanical relaxation. A mathematical model of electrogenic Na/Ca exchange (Mullins, L.J. 1979. Federation Proceedings. 35:2583; Noble, D. 1986. Cardiac Muscle. 171-200) can adequately account for many of the properties of creep currents. It is concluded that creep currents in single frog atrial cells may be attributed to the operation of an electrogenic Na/Ca exchange mechanism.

Basal ganglia precursors found in aggregates following embryonic transplantation adopt a striatal phenotype in heterotopic locations

Development ◽  
1998 ◽  
Vol 125 (15) ◽  
pp. 2847-2855
Author(s):  
L. Magrassi ◽  
M.E. Ehrlich ◽  
G. Butti ◽  
S. Pezzotta ◽  
S. Govoni ◽  
...  
Keyword(s):  
Basal Ganglia ◽  
Single Cells ◽  
Heterologous Host ◽  
Isolated Cells ◽  
Neuronal Progenitors ◽  
Spiny Neurons ◽  
Donor Cells ◽  
Powerful Approach ◽  
Dissociated Cells ◽  
The Brain

Transplantation of immature CNS-derived cells into the developing brain is a powerful approach to investigate the factors that regulate neuronal position and phenotype. CNS progenitor cells dissociated from the embryonic striatum and implanted into the brain of embryos of the same species generate cells that reaggregate to form easily recognizable structures that we previously called clusters and cells that disperse and integrate as single cells into the host brain. We sought to determine if the neurons in the clusters differentiate according to their final location or acquire a striatal phenotype in heterotopic positions. We transplanted dissociated cells from the E14 rat medial and lateral ganglionic eminences, either combined or in isolation, into the E16 embryonic rat brain. At all time points, we found clusters of BrdU- and DiI-labelled donor cells located in the forebrain and hindbrain, without any apparent preference for striatum. Immunocytochemical analyses revealed that cells in the clusters expressed DARPP-32 and ARPP-21, two antigens typically co-expressed in striatal medium-sized spiny neurons. In agreement with observations previously noted by several groups, isolated cells integrated into heterologous host areas do not express basal ganglia phenotypes. These data imply that immature striatal neuronal progenitors exert a community effect on each other that is permissive and/or instructive for development of a striatal phenotype in heterotopic locations.

Correlation between electrical and morphological properties of canine pyloric circular muscle

1991 ◽  
Vol 260 (3) ◽  
pp. G390-G398 ◽  
Author(s):  
F. Vogalis ◽  
S. M. Ward ◽  
K. M. Sanders
Keyword(s):  
Single Cells ◽  
Electrical Coupling ◽  
Circular Muscle ◽  
Muscle Layer ◽  
Morphological Properties ◽  
Morphological Examination ◽  
Isolated Cells ◽  
Time Constants ◽  
Morphological Studies ◽  
Cable Properties

Electrical slow waves decay in amplitude as they conduct from the myenteric to the submucosal regions of the circular muscle layer in the canine pyloric sphincter. We used the partitioned chamber method to study the passive and active properties of pyloric muscles, and we found that length constants of circular muscles of myenteric region were significantly longer than muscles near the submucosal surface. These data suggested differences in either membrane resistance, junctional resistance, or cytoplasmic resistance. The first parameter was evaluated by measuring time constants in intact tissues and single cells isolated from the submucosal and myenteric regions. Membrane time constants were not different in the two regions, nor were differences found in the input resistances of isolated cells. Morphological studies failed to demonstrate differences in cell diameters in the two regions suggesting that cytoplasmic resistances are similar. These findings suggest that the different cable properties in the two regions may be due to differences in electrical coupling. Morphological examination revealed similar numbers of gap junctions between cells in the two regions, but large differences were noted in the size of muscular bundles. Muscles of the myenteric region were arranged into large, tightly packed bundles, whereas muscles of the submucosal region consisted of small bundles with an extensive extracellular space filled with connective tissue. We suggest that the difference in cable properties may be due to differences in electrical coupling between bundles. These data suggest that submucosal muscles function more like a multiunit smooth muscle, whereas myenteric muscles behave as a single unit.

Electrotonic structure of olfactory sensory neurons analyzed by intracellular and whole cell patch techniques

1991 ◽  
Vol 65 (3) ◽  
pp. 747-758 ◽  
Author(s):  
F. Pongracz ◽  
S. Firestein ◽  
G. M. Shepherd
Keyword(s):  
Sensory Neurons ◽  
Information Transfer ◽  
Experimental Studies ◽  
Input Resistance ◽  
Resting Membrane Potential ◽  
Ambystoma Tigrinum ◽  
Olfactory Sensory Neurons ◽  
Isolated Cells ◽  
Whole Cell

1. Experimental studies employing whole cell patch recordings from freshly isolated olfactory sensory neurons of the salamander (Ambystoma tigrinum) yield much higher estimates of specific membrane resistance (Rm) than studies using conventional intracellular recordings from in situ neurons. Because Rm is critical for understanding information transfer in these cells, we have used computational methods to analyze the possible reasons for this difference. 2. Compartmental models were constructed for both the in situ and isolated neurons, using SABER, a general-purpose simulation program. For Rm in the in situ cell, we used a high value of 100,000 omega.cm2, as estimated in the whole cell recordings from isolated cells. A shunt across the cell membrane caused by the penetrating microelectrode was simulated by several types of shunt mechanisms, and its effects on lowering the apparent value of resting membrane potential (MP), input resistance (RN), and membrane time constant (tau m) and increasing the electrotonic length (L) were analyzed. 3. A good approximation of the electrotonic properties recorded intracellularly was obtained in the in situ model with high Rm combined with an electrode shunt consisting of Na and K conductances. A raised K conductance (1-5 nS) helps to maintain the resting MP while contributing to the increased conductance, which lowers RN and shortens the apparent tau m toward the experimental values. 4. Combined shunt resistances of 0.1-0.2 G omega (5-10 nS) gave the best fits with the experimental data. These shunts were two to three orders of magnitude smaller than the values reported from intracellular penetrations in muscle cells and motoneurons. This may be correlated with the smaller electrode tips used in the recordings from these small neurons. We thus confirm the prediction that even small values of electrode shunt have relatively large effects on the recorded electrotonic properties of small neurons, because of their high RN (2-5 G omega). 5. We have further explored the effects on electrotonic structure of a nonuniform Rm by giving higher Rm values to the distally located cilia compared with the proximal soma-dendritic region, as indicated by recent experiments. For the same RN, large increases in ciliary Rm above 100,000 omega.cm2 can be balanced by relatively small decreases below that value in soma-dendritic Rm. A high ciliary Rm appears to be a specialization for transduction of the sensory input, as reported also in photoreceptors and hair cells.

Isolation of smooth muscle cells from swine carotid artery by digestion with papain

1986 ◽  
Vol 251 (3) ◽  
pp. C474-C481 ◽  
Author(s):  
S. P. Driska ◽  
R. Porter
Keyword(s):  
Smooth Muscle ◽  
Carotid Artery ◽  
Smooth Muscle Cells ◽  
Single Cells ◽  
Calcium Ionophore ◽  
Muscle Cells ◽  
Ionophore A23187 ◽  
Free Solution ◽  
Isolated Cells ◽  
Viable Cells

A new method is described for the preparation of viable, elongated smooth muscle cells from the swine carotid artery. Cells were prepared by papain digestion of pressurized arteries in calcium-free solution. After digestion, the arteries were everted, and fine strips were teased from the intimal surface of the media in calcium-free solution, releasing single cells. Viability was assessed by exclusion of trypan blue and by appearance under phase-contrast microscopy. By these criteria, approximately 20% of the isolated cells were viable. The most distinguishing and unexpected characteristic of these cells was their length. Mean length of the relaxed viable cells was 240.4 +/- 47.4 microns (SD, n = 76), which is much longer than previously reported for arterial smooth muscle cells. Calcium (1.6 mM) caused most of the viable cells to contract slightly, and the mean cell length in calcium was 194.4 +/- 57.7 microns. Cells in 1.6 mM calcium contracted substantially in response to 10 microM histamine or the calcium ionophore A23187 (10 microM), demonstrating that histamine receptors and the contractile apparatus were still functional.

Electrotonic suppression of early afterdepolarizations in isolated rabbit Purkinje myocytes

2000 ◽  
Vol 279 (1) ◽  
pp. H250-H259 ◽  
Author(s):  
Delilah J. Huelsing ◽  
Kenneth W. Spitzer ◽  
Andrew E. Pollard
Keyword(s):  
Ventricular Myocytes ◽  
Single Cells ◽  
Late Phase ◽  
Input Resistance ◽  
Membrane Resistance ◽  
Early Afterdepolarizations ◽  
Model Cell ◽  
Triggered Arrhythmias ◽  
Electrotonic Interactions ◽  
Coupling Current

Many studies suggest that early afterdepolarizations (EADs) arising from Purkinje fibers initiate triggered arrhythmias under pathological conditions. However, electrotonic interactions between Purkinje and ventricular myocytes may either facilitate or suppress EAD formation at the Purkinje-ventricular interface. To determine conditions that facilitated or suppressed EADs during Purkinje-ventricular interactions, we coupled single Purkinje myocytes and aggregates isolated from rabbit hearts to a passive model cell via an electronic circuit with junctional resistance ( R j). The model cell had input resistance ( R m,v) of 50 MΩ, capacitance of 39 pF, and a variable rest potential ( V rest,v). EADs were induced in Purkinje myocytes during superfusion with 1 μM isoproterenol. Coupling at high R j to normally polarized V rest,v established a repolarizing coupling current during all phases of the Purkinje action potential. This coupling current preferentially suppressed EADs in single cells with mean membrane resistance ( R m,p) of 297 MΩ, whereas EAD suppression in larger aggregates with mean R m,p of 80 MΩ required larger coupling currents. In contrast, coupling to elevated V rest,v established a depolarizing coupling current during late phase 2, phase 3, and phase 4 that facilitated EAD formation and induced spontaneous activity in single Purkinje myocytes and aggregates. These results have important implications for arrhythmogenesis in the infarcted heart when reduction of the ventricular mass due to scarring alters the R m,p-to- R m,v ratio and in the ischemic heart when injury currents are established during coupling between polarized Purkinje myocytes and depolarized ventricular myocytes.

Determinants of action potential initiation in isolated rabbit atrial and ventricular myocytes

1998 ◽  
Vol 274 (6) ◽  
pp. H1902-H1913 ◽  
Author(s):  
David A. Golod ◽  
Rajiv Kumar ◽  
Ronald W. Joyner
Keyword(s):  
Action Potential ◽  
Ventricular Myocytes ◽  
Cell Types ◽  
Membrane Properties ◽  
Resting Membrane Potential ◽  
Isolated Cells ◽  
Atrial Cells ◽  
Ventricular Cells ◽  
Action Potential Initiation ◽  
Potential Initiation

Action potential conduction through the atrium and the ventricle of the heart depends on the membrane properties of the atrial and ventricular cells, particularly with respect to the determinants of the initiation of action potentials in each cell type. We have utilized both current- and voltage-clamp techniques on isolated cells to examine biophysical properties of the two cell types at physiological temperature. The resting membrane potential, action potential amplitude, current threshold, voltage threshold, and maximum rate of rise measured from atrial cells (−80 ± 1 mV, 109 ± 3 mV, 0.69 ± 0.05 nA, −59 ± 1 mV, and 206 ± 17 V/s, respectively; means ± SE) differed significantly ( P < 0.05) from those values measured from ventricular cells (−82.7 ± 0.4 mV, 127 ± 1 mV, 2.45 ± 0.13 nA, −46 ± 2 mV, and 395 ± 21 V/s, respectively). Input impedance, capacitance, time constant, and critical depolarization for activation also were significantly different between atrial (341 ± 41 MΩ, 70 ± 4 pF, 23.8 ± 2.3 ms, and 19 ± 1 mV, respectively) and ventricular (16.5 ± 5.4 MΩ, 99 ± 4.3 pF, 1.56 ± 0.32 ms, and 36 ± 1 mV, respectively) cells. The major mechanism of these differences is the much greater magnitude of the inward rectifying potassium current in ventricular cells compared with that in atrial cells, with an additional difference of an apparently lower availability of inward Na current in atrial cells. These differences in the two cell types may be important in allowing the atrial cells to be driven successfully by normal regions of automaticity (e.g., the sinoatrial node), whereas ventricular cells would suppress action potential initiation from a region of automaticity (e.g., an ectopic focus).

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