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Circulation Research. 2000;87:474-479

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(Circulation Research. 2000;87:474.)
© 2000 American Heart Association, Inc.


Integrative Physiology

Electrical Coupling Between Endothelial Cells and Smooth Muscle Cells in Hamster Feed Arteries

Role in Vasomotor Control

Geoffrey G. Emerson, Steven S. Segal

From The John B. Pierce Laboratory and Department of Cellular and Molecular Physiology, Yale University School of Medicine, New Haven, Conn.

Correspondence to Steven S. Segal, PhD, The John B. Pierce Laboratory, Yale University School of Medicine, 290 Congress Ave, New Haven, CT 06519. E-mail sssegal{at}jbpierce.org


*    Abstract
up arrowTop
*Abstract
down arrowIntroduction
down arrowMaterials and Methods
down arrowResults
down arrowDiscussion
down arrowReferences
 
Abstract—Endothelial cells (ECs) govern smooth muscle cell (SMC) tone via the release of paracrine factors (eg, NO and metabolites of arachidonic acid). We tested the hypothesis that ECs can promote SMC relaxation or contraction via direct electrical coupling. Vessels (resting diameter, 57±3 µm; length, 4 mm) were isolated, cannulated, and pressurized (75 mm Hg; 37°C). Two microelectrodes were used to simultaneously impale 2 cells (ECs or SMCs) in the vessel wall separated by 500 µm. Impalements of one EC and one SMC (n=26) displayed equivalent membrane potentials at rest, during spontaneous oscillations, and during hyperpolarization and vasodilation to acetylcholine. Injection of -0.8 nA into an EC caused hyperpolarization ({approx}5 mV) and relaxation of SMCs (dilation, {approx}5 µm) along the vessel segment. In a reciprocal manner, +0.8 nA caused depolarization ({approx}2 mV) of SMCs with constriction ({approx}2 µm). Current injection into SMCs while recording from ECs produced similar results. We conclude that ECs and SMCs are electrically coupled to each other in these vessels, such that electrical signals conducted along the endothelium can be directly transmitted to the surrounding smooth muscle to evoke vasomotor responses.


Key Words: endothelium • smooth muscle • electrical coupling • resistance artery • conduction


*    Introduction
up arrowTop
up arrowAbstract
*Introduction
down arrowMaterials and Methods
down arrowResults
down arrowDiscussion
down arrowReferences
 
Endothelial cells (ECs) promote smooth muscle relaxation through the release of NO,1 prostaglandins,2 and endothelium-derived hyperpolarizing factors (EDHFs).3 4 These paracrine factors promote K+ efflux from smooth muscle cells (SMCs), with ensuing relaxation.4 5 Recent evidence suggests that ECs may also effect SMC relaxation via direct myoendothelial coupling.

Electron microscopic studies demonstrate regions of close apposition between endothelium and smooth muscle.6 7 8 9 10 11 These regions are believed to contain myoendothelial gap junctions7 8 11 12 that promote the direct transfer of electrical and chemical signals between ECs and SMCs.13 14 15 16 17 18 19 In previous studies, membrane potential has typically been measured in a single cell, with electrical coupling inferred between respective cell types. A definitive measure of electrical coupling entails simultaneous recording20 from endothelium and smooth muscle, once demonstrated in strips of coronary artery, albeit in the absence of vasomotor responses.21 Dual simultaneous recordings have not been obtained from intact vessels that control oxygen delivery to target tissues. Therefore, it is not known whether electrical coupling between ECs and SMCs is of functional significance with respect to blood flow control.

In this study, we tested the hypothesis that ECs and SMCs are electrically coupled in resistance microvessels. Experiments were performed using feed arteries from the hamster retractor muscle, because these vessels are known to control blood flow to downstream tissue22 23 and have wall morphology (a single layer of ECs surrounded by a single layer of SMCs) that is conducive to intracellular recording.24 Electrophysiological responses were induced and recorded simultaneously from defined ECs and SMCs during vasodilation and vasoconstriction. Our data demonstrate that endothelium and smooth muscle are electrically coupled to each other and that such myoendothelial coupling plays a key role in coordinating vasomotor activity.


*    Materials and Methods
up arrowTop
up arrowAbstract
up arrowIntroduction
*Materials and Methods
down arrowResults
down arrowDiscussion
down arrowReferences
 
General
Procedures were approved by the Animal Care and Use Committee of The John B. Pierce Laboratory. Male Golden hamsters (n=28; 80 to 90 g) were anesthetized with sodium pentobarbital (65 mg/kg IP), and feed arteries supplying the retractor muscle were isolated.24 In a chamber (1 mL) containing physiological saline, the vessel was cannulated and in vivo pressure (75 mm Hg) was restored. Spontaneous tone developed during equilibration for 30 minutes at 37°C. EC and SMC viability was tested with microiontophoresis of acetylcholine (ACh) and phenylephrine, respectively.24 25

Electrophysiology
For mechanical stability, the vessel was positioned on a Sylgard block submerged at the bottom of the vessel chamber. Two glass microelectrodes containing 1% propidium iodide in 2 mol/L KCl (resistance, 100 to 150 M{Omega}), each connected to an intracellular electrometer, were aligned with the vessel axis at a penetration angle of 60°. In 5 recordings, one microelectrode contained 4% Lucifer yellow in 135 mmol/L LiCl2 (resistance, 400 to 600 M{Omega}) to determine whether recordings were affected by the type of intracellular dye used. Both dyes are membrane-impermeant; however, dye can diffuse from an EC to its neighbors through gap junctions.14 24 25 26 To impale a cell, each microelectrode was advanced slowly into the vessel wall, and the base of the micromanipulator was gently tapped.24 When tip potential rapidly dropped to {approx}-30 mV24 25 and remained stable for >1 minute, the other microelectrode was advanced similarly into another cell at a separation distance of 500 µm. When both microelectrodes were lodged in cells simultaneously, the vessel was stimulated (see below). At the end of each recording, it was confirmed that tip potential returned rapidly to 0±2 mV on withdrawal from the cell. Vessels were then viewed using fluorescence microscopy to identify the cell type recorded from on the basis of the pattern of dye staining.24

Vessel Stimulation
During dual-cell impalements, current (<=±1.6 nA; 1.5 seconds) was injected into one electrode, or ACh was microiontophoresed onto the distal end of the vessel. The vasomotor response was measured using video calipers positioned at the recording electrode farthest from the stimulus. Electrical and vasomotor responses (resolutions, 1 mV and 1 µm, respectively) were acquired at 400 Hz.

Pharmacology
To inhibit the effects of NO, cytochrome P-450 metabolites, or metabolites of arachidonic acid, vessels were incubated with N{omega}-nitro-L-arginine (L-NNA; 100 µmol/L, 30 minutes), 17-octadecynoic acid (ODYA; 10 µmol/L, 30 minutes), or indomethacin (10 µmol/L, 15 minutes).27

Electron Microscopy
Feed arteries were fixed in situ with Karnovsky’s fixative for 10 minutes. The tissue was excised, postfixed for 20 minutes, and stored in 0.1 mol/L sodium cacodylate buffer with 7% sucrose for 4 days. Vessels were osmicated, stained en bloc with 3% uranyl acetate, and embedded in epoxy resin. Tissue was sectioned at {approx}50 nm thickness, stained with uranyl acetate and lead citrate, and examined on a Zeiss 109T transmission electron microscope.

Data Analysis
Representative tracings were selected to illustrate typical responses. Summary data are presented as mean±SEM. Statistical analyses are given in context.


*    Results
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
*Results
down arrowDiscussion
down arrowReferences
 
On pressurization, feed arteries (n=28) initially dilated to their maximal diameter (82±3 µm). Spontaneous tone developed during equilibration (resting diameter, 57±3 µm) and persisted throughout the experiment (3 to 5 hours). All vessels dilated to ACh and constricted to phenylephrine.

Recorded cells were identified by dye (propidium iodide or Lucifer yellow) that diffused from the microelectrode during intracellular recording.24 Because there is typically one SMC layer in these vessels, intracellular microelectrodes readily penetrated to ECs ({approx}50% of impalements) with no apparent damage to (or labeling of) surrounding SMCs. During EC impalement, multiple ECs (oriented parallel to vessel axis, Figure 1ADown) were labeled, regardless of the dye used. In contrast, smooth muscle labeling was confined to the impaled cell (oriented perpendicular to the vessel axis, Figure 1BDown). Moreover, dye did not spread from ECs to SMCs or vice versa. Propidium iodide labeled cell nuclei, whereas Lucifer yellow labeled the entire cell (Figure 1CDown). Electrophysiological responses were similar whether electrodes contained propidium iodide or Lucifer yellow. Resting membrane potential and electrophysiological responses were unchanged throughout a given impalement (up to 1.5 hours); vasomotor responses were unchanged in the impaled region throughout the experiment (up to 5 hours).



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Figure 1. Intracellular labeling of ECs and SMCs. During intracellular recording, propidium iodide or Lucifer yellow dye diffused from the microelectrode into the impaled cell. After each recording, impaled sites were identified with fluorescence microscopy. A, EC nuclei stained with propidium iodide. Nuclei are oriented parallel to the vessel axis (white lines depict vessel boundaries), with multiple cells stained after impalement of a single EC. B, SMC nucleus stained with propidium iodide. A single SMC nucleus, oriented perpendicular to the vessel axis, is stained. A and B, Cells that correspond to recordings in Figure 2Up. C, EC nuclei stained with propidium iodide (red) with nearby SMC stained with Lucifer yellow (green). Note lack of dye transfer between ECs and SMCs. Scale bars=15 µm (A), 15 µm (B), and 10 µm (C).

Two to five simultaneous dual-cell recordings were obtained from each vessel. During recordings from one EC and one SMC (n=26), membrane potential in both cells was identical (–28±1 mV), and oscillations in membrane potential were simultaneous and equivalent (Figure 2Down). Injection of negative (hyperpolarizing) current into the EC resulted in simultaneous hyperpolarization of the SMC, with ensuing vasodilation (lag time between onset of hyperpolarization and onset of vasodilation, 1.7±0.1 seconds). Conversely, injection of negative current into the SMC caused simultaneous hyperpolarization of the EC, with ensuing vasodilation (lag time, 1.6±0.1 seconds). When ACh was microiontophoresed onto the downstream end of the vessel, simultaneous hyperpolarization of both cell types ensued (Figure 2BDown), and vasodilation conducted along the entire vessel (n=8). Addition of L-NNA decreased resting diameter (n=7; 75±4 versus 67±3 µm; P<0.05, paired t test; reversed with 1 mmol/L L-arginine) but did not alter the vasodilatory response to ACh. Further, indomethacin (n=4), 17-ODYA (n=3), or L-NNA and 17-ODYA in combination (n=3) had no effect on the vasodilatory response to ACh. These findings argue against a role for NO or metabolites of arachidonic acid in mediating responses to ACh. Electron microscopy revealed regions of electron-dense apposition between ECs and SMCs (Figure 2CDown), indicating the presence of myoendothelial gap junctions.11



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Figure 2. Simultaneous recording of membrane potential (Em) from an EC and an SMC. A, Illustration of an isolated vessel with microelectrodes impaled in an EC and an SMC. A micropipette filled with ACh is positioned at the downstream end of the vessel (with respect to superfusion of physiological saline; Flow) to trigger hyperpolarization and vasodilation, which conduct along the entire vessel. Scale bar=250 µm. B, Simultaneous recording of diameter, membrane potential of EC, and membrane potential of SMC. During the recording, 3 stimuli were applied, as follows: -0.8 nA was injected into EC (solid bar), -0.8 nA was injected into SMC (open bar), and ACh was delivered by microiontophoresis ({uparrow}; 500 nA, 500 ms). Each stimulus evoked dilation along the entire vessel; diameter was recorded at site of SMC impalement. Note simultaneous oscillations in membrane potential (magnified inset). This record is representative of n=26 dual-cell recordings from ECs and SMCs. Scale bar=5 seconds. C, Electron micrograph of feed artery wall in cross section. EC (with prominent nucleus, adjacent to the vessel lumen, L) and SMC (underlying the adventitia, A) are separated by internal elastic lamina except in the region of EC:SMC contact, where electron-dense regions characteristic of myoendothelial gap junctions11 are present (arrowhead). Scale bar=0.2 µm.

To test whether electrical coupling within the endothelium is greater than electrical coupling between ECs and SMCs, current was injected into one cell while the electrical response in the other cell was recorded.20 Each combination of cell-cell coupling was evaluated, as follows: (1) endothelial-endothelial, (2) endothelial-smooth muscle, (3) smooth muscle-endothelial, and (4) smooth muscle-smooth muscle (Figures 3Down and 4Down). For all combinations, injection of -0.8 nA evoked simultaneous hyperpolarization of the second cell and vasodilation that conducted along the entire feed artery. In a complementary manner, injection of +0.8 nA evoked depolarization and constriction that conducted along the vessel. In each case, the electrical response of the noninjected cell was instantaneous in onset and offset for both hyperpolarization and depolarization. The magnitudes of electrical and vasomotor responses were similar for all cell-cell combinations (Figures 3Down and 4Down), as were the delays between the onset of hyperpolarization and the onset of vasodilation (1.7±0.1 seconds) and between depolarization and vasoconstriction (1.3±0.1 seconds).



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Figure 3. Diameter and electrophysiological responses to current injection. Two cells in the vessel wall were impaled simultaneously (microelectrode separation, 500 µm). -0.8 nA (solid bar) and +0.8 nA (open bar) were injected for 1.5 seconds into an EC (A and B) or an SMC (C and D) while recording from an EC (A and C) or an SMC (B and D). For all combinations, negative current evoked hyperpolarization and vasodilation at the recording site, whereas positive current evoked depolarization (or changed the electrical baseline) and vasoconstriction. A through D, Bottom tracing indicates membrane potential of the injected cell; middle tracing, membrane potential of the recorded cell; and top tracing, diameter at the recorded cell. Cell type identified as in Figure 1Up. Note simultaneous oscillations of membrane potential in panel D. These 1-Hz oscillations are more rapid than vasomotor responses, which are typically delayed ({approx}2 seconds) and prolonged (5 to 10 seconds) with respect to electrical events.



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Figure 4. Summary data (n=6 to 13) of electrophysiological (A) and diameter (B) responses to negative (hatched columns) and positive (open columns) current injection. Response magnitudes were calculated as peak minus resting value (error bars indicate SEM) and were not different between conditions (ANOVA). Cell type was identified as in Figure 1Up. The transfer resistance (defined as the change in voltage at the recording electrode divided by the current injected) was not different (ANOVA) between EC-EC (6.5±0.5 M{Omega}), EC-SMC (6.7±0.6 M{Omega}), SMC-EC (6.8±0.8 M{Omega}), and SMC-SMC (5.6±0.6 M{Omega}), indicating that electrical coupling between the 2 cells was similar in all combinations.

In all cell-cell combinations, responses to -0.8 nA were consistently greater than responses to +0.8 nA (Figures 3Up and 4Up). To further explore this relationship, the current intensity was varied between –1.6 and +1.6 nA (Figure 5Down). Throughout this range, pooled for all cells that compose the conduction pathway, the "transfer resistance" (Figure 4Up, legend) for positive current was {approx}25% of that for negative current (1.3±0.5 versus 6.0±0.5 M{Omega}, respectively; P<0.01, paired t test). Nevertheless, for ECs as well as SMCs, the relationship between electrophysiological and vasomotor responses was approximately linear ({approx}1 µm/mV; Figure 5CDown). This proportionality between electrical and mechanical responses to current injection is consistent with electromechanical coupling.25 28 For rapid ({approx}1-Hz) oscillations in membrane potential (eg, Figures 2BUp and 3DUp), electrical events were presumably too brief to be accompanied by corresponding mechanical events.



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Figure 5. Current, voltage, and diameter relationships during current injection. During dual-cell impalements (n=35), current pulses (±0.4 to 1.6 nA, 1.5 seconds) were injected into one cell and recorded in the other cell. A, Current-voltage relationship demonstrating that electrical response to current injection is intensity-dependent. Note that responses to positive current were significantly smaller than responses to equal negative current. B, Current-diameter relationship demonstrating that the mechanical response ({Delta} Diameter) to the injection of current (nA) is intensity-dependent. C, Voltage-diameter relationship demonstrating linearity between change in membrane potential ({Delta} Em) and change in diameter. This relationship was similar whether recording from ECs ({circ}) or SMCs (•).

Controls were performed for current injection as follows. (1) Throughout experiments, stimuli were delivered with microelectrodes positioned in the bath to confirm that the bridge of the electrometer was balanced similarly for positive and negative current injections. (2) Current injection into the bath adjacent to the vessel failed to evoke vasomotor or electrophysiological responses (n=6). (3) Injection of current into a cell failed to evoke a response from a recording electrode positioned in the bath adjacent to the vessel (n=7). (4) During simultaneous impalements, increasing stimulus duration (eg, to 15 seconds) correspondingly prolonged electrical responses and enhanced changes in vessel diameter (n=5; data not shown).


*    Discussion
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
up arrowResults
*Discussion
down arrowReferences
 
We present the first dual simultaneous electrophysiological recordings obtained concomitant with vasomotor responses. Our findings demonstrate that ECs and SMCs are electrically coupled to each other in resistance microvessels that control blood flow to the hamster retractor muscle. Instantaneous, bidirectional transmission of electrical signals between endothelium and smooth muscle ensures that both cell types consistently display equivalent membrane potential. Thus, myoendothelial coupling enables electrical responses originating in either the endothelium or the smooth muscle to evoke robust vasomotor responses along the entire vessel segment.

Endothelium-dependent agonists (eg, ACh) can hyperpolarize and relax SMCs by a mechanism independent of NO, EDHFs, and prostaglandins.15 16 29 Conversely, SMC-specific agonists (eg, phenylephrine) can alter EC calcium13 and membrane potential.17 18 28 30 Electron microscopy has revealed electron-dense regions of membrane apposition between SMCs and ECs in conduit vessels,8 9 resistance arteries,11 and arterioles.6 7 Such regions of membranous contact (eg, Figure 2CUp) are believed to contain gap junctions. Whereas putative gap junction antagonists can inhibit responses that depend on cell coupling,15 16 17 18 19 there is a paucity of direct evidence21 that electrical signals spread freely between ECs and SMCs. Moreover, the role of myoendothelial electrical coupling in governing vascular resistance has not been defined.

Hyperpolarization and depolarization evoke vasodilation and vasoconstriction, respectively, through electromechanical coupling (Figure 5CUp). This behavior is consistent with voltage-operated calcium channels in SMCs.31 However, the present findings demonstrate that injection of current into an EC evokes vasodilation or vasoconstriction (according to polarity) and that EC membrane potential itself is a powerful determinant of electromechanical coupling within the smooth muscle layer (Figure 5CUp). Both electrical and mechanical responses to negative current were consistently larger than those to equivalent positive current (Figures 3Up and 4Up), and depolarizations were frequently followed by a slight, transient hyperpolarization (eg, Figure 3Up). These features of the response to positive current are consistent with the presence of voltage-activated potassium channels.32

Myoendothelial coupling promotes synchronization of cells in the vessel wall.33 In arterioles and feed arteries, cells are organized such that each EC spans {approx}20 SMCs and each SMC spans {approx}20 ECs.24 25 34 This wall morphology promotes heterologous cell-to-cell contact. Further, homologous coupling within the endothelium14 25 26 35 36 promotes electrical conduction along the vessel axis.24 34 The integrity of the EC layer is required for conducting hyperpolarization and vasodilation along hamster feed arteries, indicating relatively poor coupling between SMCs.24 Here we demonstrate in the same vessels that myoendothelial coupling is of similar electrical resistance to that within the endothelium (Figure 4Up). In turn, myoendothelial coupling ensures that SMCs are electrically coupled to each other (albeit indirectly) via the endothelium (Figures 3Up and 4Up).

The importance of NO,1 37 EDHFs,3 4 27 and prostaglandins2 during endothelium-dependent vasodilation is well demonstrated. Although we cannot rule out a contribution of these paracrine agents to current-induced vasodilation, their involvement is unlikely given the instantaneous and bidirectional nature of electrical transmission and the failure of established pharmacological interventions to block responses to ACh.

The present study was performed in vitro rather than in vivo because dual-cell intracellular recording requires absolute mechanical stability; this condition cannot be achieved when feed arteries pulse with arterial pressure. However, the electrical behavior of vessels studied in vitro may differ from that in vivo.25 28 Further, the rapid (<2-hour) turnover of connexin molecules38 implies that the properties of cell-to-cell coupling within a vessel may change over time. To minimize the potential for such effects, we restored isolated vessels to in vivo length and transmural pressure. The resting diameter and vasomotor responses of feed arteries in vitro24 are similar to those in vivo,39 indicating that functional integrity is preserved throughout our experimental procedures. Whereas the resting membrane potential ({approx}–30 mV) of cells in our preparation is depolarized relative to unpressurized arterioles in vitro,28 40 it is similar to that reported for arterioles in vivo.25 27 We attribute this difference in membrane potential to the restoration of physiological transmural pressure and the depolarizing effect of the myogenic response.41

In summary, we present the first simultaneous measurements of EC membrane potential, SMC membrane potential, and diameter responses. Our data establish that electrical signals travel freely and bidirectionally between ECs and SMCs to evoke robust vasomotor responses. We conclude that myoendothelial coupling can serve as a rapid, integral component of blood flow control.


*    Acknowledgments
 
This study was supported by NIH Grants RO1-HL41026 and RO1-HL56786, Yale Diabetes and Endocrinology Research Center grant P30-DK45735, and Medical Scientist Training Program Fellowship GM07205 (to G.G.E.). Beth Doran provided expert technical assistance in preparing electron micrographs.

Received June 7, 2000; revision received July 13, 2000; accepted July 17, 2000.


*    References
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMaterials and Methods
up arrowResults
up arrowDiscussion
*References
 
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Am. J. Physiol. Heart Circ. Physiol.Home page
B. Rodenwaldt, U. Pohl, and C. de Wit
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T. R. Uhrenholt, T. L. Domeier, and S. S. Segal
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T. L. Domeier and S. S. Segal
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Am. J. Physiol. Regul. Integr. Comp. Physiol.Home page
Q. Zhang, C. Cao, M. Mangano, Z. Zhang, E. P. Silldorff, W. Lee-Kwon, K. Payne, and T. L. Pallone
Descending vasa recta endothelium is an electrical syncytium
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HypertensionHome page
X. F. Figueroa, B. E. Isakson, and B. R. Duling
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Hypertension, November 1, 2006; 48(5): 804 - 811.
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M. C. Jantzi, S. E. Brett, W. F. Jackson, R. Corteling, E. J. Vigmond, and D. G. Welsh
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S. Earley and M. T. Nelson
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J. F. Brekke, W. F. Jackson, and S. S. Segal
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V. V. Matchkov, A. Rahman, L. M. Bakker, T. M. Griffith, H. Nilsson, and C. Aalkjaer
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E. M. Sokoya, A. R. Burns, C. T. Setiawan, H. A. Coleman, H. C. Parkington, and M. Tare
Evidence for the involvement of myoendothelial gap junctions in EDHF-mediated relaxation in the rat middle cerebral artery
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Arterioscler. Thromb. Vasc. Bio.Home page
M. Feletou and P. M. Vanhoutte
Endothelium-Derived Hyperpolarizing Factor: Where Are We Now?
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N. I. Gokina and T. Goecks
Upregulation of endothelial cell Ca2+ signaling contributes to pregnancy-enhanced vasodilation of rat uteroplacental arteries
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Silent Inward Rectifier K+ Channels in Hypercholesterolemia
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A. Radaelli, P. Castiglioni, M. Centola, F. Cesana, G. Balestri, A. U. Ferrari, and M. Di Rienzo
Adrenergic origin of very low-frequency blood pressure oscillations in the unanesthetized rat
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Myoendothelial Coupling Is Not Prominent in Arterioles Within the Mouse Cremaster Microcirculation In Vivo
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S. J Haug and S. S Segal
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J.-A. Haefliger, P. Nicod, and P. Meda
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S. P. Marrelli, M. S. Eckmann, and M. S. Hunte
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E. Bussemaker, R. Popp, B. Fisslthaler, C. M. Larson, I. Fleming, R. Busse, and R. P. Brandes
Aged Spontaneously Hypertensive Rats Exhibit a Selective Loss of EDHF-Mediated Relaxation in the Renal Artery
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G. G. Emerson, T. O. Neild, and S. S. Segal
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H. Li, S. Brodsky, S. Kumari, V. Valiunas, P. Brink, J.-I. Kaide, A. Nasjletti, and M. S. Goligorsky
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CirculationHome page
R. J. Rivers, T. W. Hein, C. Zhang, and L. Kuo
Activation of Barium-Sensitive Inward Rectifier Potassium Channels Mediates Remote Dilation of Coronary Arterioles
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S. P. Marrelli
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S. Budel, A. Schuster, N. Stergiopoulos, J.-J. Meister, and J.-L. Beny
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H.-Z. Wang, N. Day, M. Valcic, K. Hsieh, S. Serels, P. R. Brink, and G. J. Christ
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Am. J. Physiol. Heart Circ. Physiol.Home page
H. A. Coleman, M. Tare, and H. C. Parkington
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Am J Physiol Heart Circ Physiol, June 1, 2001; 280(6): H2478 - H2483.
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Am. J. Physiol. Heart Circ. Physiol.Home page
G. G. Emerson and S. S. Segal
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Am J Physiol Heart Circ Physiol, January 1, 2001; 280(1): H160 - H167.
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Am. J. Physiol. Renal Physiol.Home page
X. Wang and R. Loutzenhiser
Determinants of renal microvascular response to ACh: afferent and efferent arteriolar actions of EDHF
Am J Physiol Renal Physiol, January 1, 2002; 282(1): F124 - F132.
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Am. J. Physiol. Heart Circ. Physiol.Home page
H. Li, S. Brodsky, S. Kumari, V. Valiunas, P. Brink, J.-I. Kaide, A. Nasjletti, and M. S. Goligorsky
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P. Vequaud and E. Thorin
Endothelial G Protein {beta}-Subunits Trigger Nitric Oxide- but not Endothelium-Derived Hyperpolarizing Factor-Dependent Dilation in Rabbit Resistance Arteries
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R. Popp, R. P. Brandes, G. Ott, R. Busse, and I. Fleming
Dynamic Modulation of Interendothelial Gap Junctional Communication by 11,12-Epoxyeicosatrienoic Acid
Circ. Res., April 19, 2002; 90(7): 800 - 806.
[Abstract] [Full Text] [PDF]


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