Myogenic tone of the rat testicular subcapsular artery has a role in autoregulation of testicular blood supply

An in vitro method is described for the isolation, cannulation, and pressurization of a 10-mm segment of the adult rat testicular subcapsular artery by use of a 200-microns micropipette connected to an adjustable-height reservoir. External and internal arterial diameters were measured by a digital filar micrometer eyepiece calibrated with a Microcode scaler. Transmural pressure was increased stepwise by 20 mm Hg from 20 to 180 mm Hg at 10-min intervals. The following novel triphasic myogenic response was found: a 22.5% increase in lumen cross-sectional area from 20 to 40 mm Hg (p less than 0.05); a 37.3% decrease in lumen cross-sectional area from 40 to 100 mm Hg (p less than 0.05); and a 72.4% increase in lumen cross-sectional area from 100 to 180 mm Hg (p less than 0.05). Papaverine (0.1 mM) completely blocked the transmural pressure-induced vasoconstriction, indicating an active increase in vascular smooth muscle tone by transmural pressure. The calculated blood flow through the testicular subcapsular artery of the adult rat, from measured internal radii at various transmural pressures ranging from 20 to 180 mm Hg by Poiseuille's equation, was constant from 40 to 100 mm Hg and showed a progressive increase from 100 to 180 mm Hg. These data suggest that the myogenic response of the adult rat testicular subcapsular artery may have an important role in the autoregulation of the testicular blood supply.     

Comparison of norepinephrine and serotonin vasoconstriction of the rat isolated testicular subcapsular artery at physiological and elevated transmural pressures.

This laboratory has previously described an in vitro preparation showing that the isolated testicular subcapsular artery of the adult rat has a novel triphasic transmural pressure-diameter myogenic response curve consisting of vasodilatation from 20 to 40 mm Hg, vasoconstriction from 40 to 100 mm Hg, and vasodilatation from 100 to 180 mm Hg, suggesting that the myogenic response of this artery between 40 and 100 mm Hg may have an important role in the autoregulation of the testicular blood supply. In the present studies, a 10-mm length of the adult rat isolated testicular subcapsular artery was cannulated and pressurized by an adjustable-height reservoir. External and internal arterial diameters were measured by a digital filar micrometer eyepiece. Dose-response curves for norepinephrine and serotonin were generated in a double-bath artery chamber at transmural pressures of 70 and 140 mm Hg, using half of the same artery for each pressure. Norepinephrine (3 x 10(-8) to 1 x 10(-5) M) produced a dose-dependent vasoconstriction at 70 mm Hg, with the highest dose causing a 31.4% decrease in lumen cross-sectional area (p < 0.05). Serotonin (3 x 10(-8) to 1 x 10(-6) M) produced a stronger dose-dependent vasoconstriction at 70 mm Hg, with the highest dose causing a 72.7% decrease in lumen cross-sectional area (p < 0.05). In marked contrast, the same concentration of norepinephrine and serotonin were found to have no statistically significant effect on the lumen cross-sectional area of the isolated testicular subcapsular artery at a transmural pressure of 140 mm Hg.(ABSTRACT TRUNCATED AT 250 WORDS)     

Computational study of LDL mass transport in the artery wall

A two-dimensional (2D) numerical simulation of convective–diffusive transport of LDL in the artery wall, coupled with the wall shear stress gradient (WSSG)-dependent LDL consumption of smooth muscle cells (SMCs) is presented. SMCs are modeled as an array of solid cylindrical pillars embedded in a continuous porous media which represents the interstitial proteoglycan and collagen fiber matrix. The internal elastic lamina (IEL), which separates the artery media from the intima, is modeled as an impermeable barrier to both water and LDL except for the fenestral pores that are assumed to be uniformly distributed over the IEL. The predictions demonstrate a range of interesting features of LDL transport and uptake in the media. For cells immediately below the fenestral pores, LDL uptake of SMCs is highly dependent on WSSG. Moreover, the rate of LDL consumption by SMCs is also affected by the diameter of the fenestral pore. This will be helpful in understanding the involvement of transmural transport processes in the initiation and development of atherosclerosis.     

Transmural gradients of oxygen tension on cerebral microvessels in rats

Using modified oxygen needle microelectrodes, vital microscopy with video-recording facilities, measurements of tissue oxygen tension (PO2) profiles near the cortical arterioles and transmural PO2 gradients on pial arterioles of the rat were performed. At control transmural PO2 gradient averaged 1.17 +/- 0.06 mm Hg/microm (mean +/- SEM, n = 40). Local dilatation of the arteriolar wall (microapplication of sodium nitroprusside approximately 2 x 10(-7) M) resulted in marked drop of the transmural PO2 gradient to 0.68 +/- 0.04 mm Hg/microm (p < 0.001, n = 38). The important finding of the study is the dependence of the transmural PO2 gradient on the vascular tone of pial arterioles. The data presented allow to conclude that O2 consumption of the arteriolar wall lies within the range for surrounding tissue and O2 consumption of the endothelial layer and, apparently, has no substantial impact on transmural PO2 gradient.     

Boundary layer considerations in a multi-layer model for LDL accumulation

Abstract

Boundary layer effects for Low-Density Lipoprotein (LDL) concentration problems in a multi-layer artery model are analyzed in this work. Both a straight artery and aorta-iliac bifurcation are analyzed. Mass, momentum and species governing equations are based on the porous media theory and solved with the commercial finite-element based code COMSOL Multiphysics. For the straight artery, various inlet velocities, arterial sizes and intramural pressure values are investigated. Results are presented in terms of concentration profiles close to the lumen/endothelium interface and boundary layer thickness. It is shown that the boundary layer is affected by all of the three analyzed parameters. The results in this work will further clarify the concentration polarization effects imposed by the arterial wall.     

Intimal hyperplasia and wall shear in arterial bypass graft distal anastomoses: an in vivo model study

The observation of intimal hyperplasia at bypass graft anastomoses has suggested a potential interaction between local hemodynamics and vascular wall response. Wall shear has been particularly implicated because of its known effects upon the endothelium of normal vessels and, thus, was examined as to its possible role in the development of intimal hyperplasia in arterial bypass graft distal anastomoses. Tapered (4-7 mm I.D.) e-PTFE synthetic grafts 6 cm long were placed as bilateral carotid artery bypasses in six adult, mongrel dogs weighing between 25 and 30 kg with distal anastomotic graft-to-artery diameter ratios (DR) of either 1.0 or 1.5. Immediately following implantation, simultaneous axial velocity measurements were made in the toe and artery floor regions in the plane of the anastomosis at radial increments of 0.35 mm, 0.70 mm, and 1.05 mm using a specially designed 20 MHz triple crystal ultrasonic wall shear rate transducer Mean, peak, and pulse amplitude wall shear rates (WSRs), their absolute values, the spatial and temporal wall shear stress gradients (WSSG), and the oscillatory shear index (OSI) were computed from these velocity measurements. All grafts were harvested after 12 weeks implantation and measurements of the degree of intimal hyperplasia (IH) were made along the toe region and the artery floor of the host artery in 1 mm increments. While some IH occurred along the toe region (8.35+/-23.1 microm) and was significantly different between DR groups (p<0.003), the greatest amount occurred along the artery floor (81.6+/-106.5 microm, mean +/- S.D.) (p < 0.001) although no significant differences were found between DR groups. Linear regressions were performed on the paired IH and mean, peak, and pulse amplitude WSR data as well as the absolute mean, peak, and pulse amplitude WSR data from all grafts. The mean and absolute mean WSRs showed a modest correlation with IH (r = -0.406 and -0.370, respectively) with further improvements seen (r = -0.482 and -0.445, respectively) when using an exponential relationship. The overall best correlation was seen against an exponential function of the OSI (r = 0.600). Although these correlation coefficients were not high, they were found to be statistically significant as evidenced by the large F-statistic obtained. Finally, it was observed that over 75 percent of the IH occurred at or below a mean WSR value of 100 s(-1) while approximately 92 percent of the IH occurred at or below a mean WSR equal to one-half that of the native artery. Therefore, while not being the only factor involved, wall shear (and in particular, oscillators wall shear) appears to provide a stimulus for the development of anastomotic intimal hyperplasia.     

Effect of residual stress and heterogeneity on circumferential stress in the arterial wall

Quantifying the stress distribution through the arterial wall is essential to studies of arterial growth and disease. Previous studies have shown that both residual stress, as measured by opening angle, and differing material properties for the media-intima and the adventitial layers affect the transmural circumferential stress (sigma theta) distribution. Because a lack of comprehensive data on a single species and artery has led to combinations from multiple sources, this study determined the sensitivity of sigma theta to published variations in both opening angle and layer thickness data. We fit material properties to previously published experimental data for pressure-diameter relations and opening angles of rabbit carotid artery, and predicted sigma theta through the arterial wall at physiologic conditions. Using a one-layer model, the ratio of sigma theta at the internal wall to the mean sigma theta decreased from 2.34 to 0.98 as the opening angle increased from 60 to 130 deg. In a two-layer model using a 95 deg opening angle, mean sigma theta in the adventitia increased (112 percent for 25 percent adventitia) and mean sigma theta in the media decreased (47 percent for 25 percent adventitia). These results suggest that both residual stress and wall layers have important effects on transmural stress distribution. Thus, experimental measurements of loading curves, opening angles, and wall composition from the same species and artery are needed to accurately predict the transmural stress distribution in the arterial wall.     

Changes of zero-stress state of rat pulmonary arteries in hypoxic hypertension

Zero-stress state of the main pulmonary arteries, from the main trunk to a vessel with a lumen diameter approximately 60 microns, was determined in 25 normal control and 38 hypoxic pulmonary hypertensive rats. Pulmonary hypertension was induced by placing the rats in a hypoxic chamber with 10% O2-90% N2 at atmospheric pressure. The zero-stress state of each vessel was obtained by first cutting the vessel transversely into a series of rings and then cutting each ring radially, whereupon the ring opened into a sector, which is characterized by an opening angle defined as the angle subtended between two lines originating from the midpoint of the inner wall (endothelium) to the tips of the inner wall. Whereas the pulmonary blood pressure increased monotonically during the development of pulmonary hypertension, the opening angle followed a different course; e.g., the values (means +/- SD) of the opening angle at the pulmonary trunk at times 0 (control) and 2, 12, 28, 96, 144, 240, 480, and 720 h after exposure to hypoxia are, respectively, 294 +/- 30 degrees, 378 +/- 24 degrees, 385 +/- 12 degrees, 374 +/- 11 degrees, 246 +/- 63 degrees, 267 +/- 49 degrees, 193 +/- 19 degrees, 195 +/- 83 degrees, and 239 +/- 38 degrees. Trends at other places on the artery are similar, but the magnitudes differ. In this period of time, intimal edema and thickening were found. The intima media thickened rapidly from 48 to 240 h and then more slowly from 240 to 720 h. Adventitia thickened later; its thickness exceeded that of the intima media at approximately 96 h. Thus the changes of zero-stress state of the pulmonary arteries are seen to be related to the nonuniform remodeling of the vessel wall as revealed by the edema, blebs, and thickening of different layers.     

Lack of additional action of oxygen on pulmonary artery pressure at the peak of verapamil or captopril action in pulmonary hypertension secondary to mitral stenosis]

The aim of the study was to investigate whether oxygen causes a further decrease in pulmonary artery pressure after administration of calcium channel blocker-verapamil-or angiotensin converting enzyme inhibitor-captopril-in the secondary pulmonary hypertension. We studied 37 patients with the secondary pulmonary hypertension (mean pulmonary artery systolic pressure = 56.1 mm Hg) due to mitral stenosis. After having completed hemodynamic diagnostic procedures, basal oxygen test was performed and pulmonary artery pressure was recorded at 10 min of oxygen breathing. Then, 10 mg of verapamil was injected into the pulmonary artery of 16 patients and 21 patients received 75 mg of oral captopril. At the peak of vasodilation, 30 min after verapamil and 90 min after captopril administration, pulmonary artery pressure was recorded and oxygen test was repeated. Baseline oxygen test produced a statistically significant decrease in pulmonary artery pressure. Verapamil and captopril also lowered pulmonary artery systolic and diastolic pressures. The second oxygen test did not cause a further decrease in the pulmonary artery pressure; mean pulmonary artery systolic pressure was 52.3 +/- 23.7 mm Hg, pulmonary artery diastolic pressure 22.7 +/- 10.6 mm Hg before and 49.1 +/- 23.8 mm Hg and 23.0 +/- 13.5 mm Hg, respectively after the test in verapamil group, and 47.0 +/- 15.5 mm Hg and 21.7 +/- 8.4 mm Hg before and 46.6 +/- 15.4 mm Hg, respectively in captopril subset. The results may support the thesis that vasodilating effect depends rather on the degree of pulmonary vascular changes than on the vasodilatory mechanism of particular drugs.     

Effects of coronary sinus pressure elevation on coronary blood flow distribution in dogs with normal preload

Coronary sinus pressure (Pcs) elevation shifts the diastolic coronary pressure-flow relation (PFR) of the entire left ventricular myocardium to a higher pressure intercept. This finding suggests that Pcs is one determinant of zero-flow pressure (Pzf) and challenges the existence of a vascular waterfall mechanism in the coronary circulation. To determine whether coronary sinus or tissue pressure is the effective coronary back pressure in different layers of the left ventricular myocardium, the effect of increasing Pcs was studied while left ventricular preload was low. PFRs were determined experimentally by graded constriction of the circumflex coronary artery while measuring flow using a flowmeter. Transmural myocardial blood flow distribution was studied (15-micron radioactive spheres) at steady state, during maximal coronary artery vasodilatation at three points on the linear portion of the circumflex PFR both at low and high diastolic Pcs (7 +/- 3 vs. 22 +/- 5 mmHg; p less than 0.0001) (1 mmHg = 133.322 Pa). In the uninstrumented anterior wall the blood flow measurements were obtained in triplicate at the two Pcs levels. From low to high Pcs, mean aortic (98 +/- 23 mmHg) and left atrial (5 +/- 3 mmHg) pressure, percent diastolic time (49 +/- 7%), percent left ventricular wall thickening (32 +/- 4%), and percent myocardial lactate extraction (15 +/- 12%) were not significantly changed. Increasing Pcs did not alter the slope of the PFR; however, the Pzf increased in the subepicardial layer (p less than 0.0001), whereas in the subendocardial layer Pzf did not change significantly. Similar slopes and Pzf were observed for the PFR of both total myocardial mass and subepicardial region at low and high Pcs. Subendocardial:subepicardial blood flow ratios increased for each set of measurements when Pcs was elevated (p less than 0.0001), owing to a reduction of subepicardial blood flow; however, subendocardial blood flow remained unchanged, while starting in the subepicardium toward midmyocardium blood flow decreased at high Pcs. This pattern was similar for the uninstrumented anterior wall as well as in the posterior wall. Thus as Pcs increases it becomes the effective coronary back pressure with decreasing magnitude from the subepicardium toward the subendocardium of the left ventricle. Assuming that elevating Pcs results in transmural elevation in coronary venous pressure, these findings support the hypothesis of a differential intramyocardial waterfall mechanism with greater subendo- than subepi-cardial tissue pressure.     

A nonlinear axisymmetric model with fluid-wall interactions for steady viscous flow in stenotic elastic tubes.

Arteries with high-grade stenoses may compress under physiologic conditions due to negative transmural pressure caused by high-velocity flow passing through the stenoses. To quantify the compressive conditions near the stenosis, a nonlinear axisymmetric model with fluid-wall interactions is introduced to simulate the viscous flow in a compliant stenotic tube. The nonlinear elastic properties of the tube (tube law) are measured experimentally and used in the model. The model is solved using ADINA (Automatic Dynamic Incremental Nonlinear Analysis), which is a finite element package capable of solving problems with fluid-structure interactions. Our results indicate that severe stenoses cause critical flow conditions such as negative pressure and high and low shear stresses, which may be related to artery compression, plaque cap rupture, platelet activation, and thrombus formation. The pressure filed near a stenosis has a complex pattern not seen in one-dimensional models. Negative transmural pressure as low as -24 mmHg for a 78 percent stenosis by diameter is observed at the throat of the stenosis for a downstream pressure of 30 mmHg. Maximum shear stress as a high as 1860 dyn/cm2 occurs at the throat of the stenoses, while low shear stress with reversed direction is observed right distal to the stenosis. Compressive stresses are observed inside the tube wall. The maximal principal stress and hoop stress in the 78 percent stenosis are 80 percent higher than that from the 50 percent stenosis used in our simulation. Flow rates under different pressure drop conditions are calculated and compared with experimental measurements and reasonable agreement is found for the prebuckling stage.     

Losartan, a nonpeptide angiotensin II (Ang II) receptor antagonist, inhibits neointima formation following balloon injury to rat carotid arteries.

Angiotensin-converting enzyme inhibitors have been shown to inhibit intimal thickening following balloon catheterization of rat carotid arteries. To assess the role of the renin-angiotensin pathway and the angiotensin type-I (AT1) receptor in this effect, the nonpeptide Ang II antagonist losartan (DuP 753) or vehicle was infused continuously i.v. in rats from two days before to two weeks after balloon injury to the left common carotid artery; drug effects upon intimal thickening were examined histologically. Losartan produced a dose-dependent reduction in cross-sectional area of intimal lesions determined two weeks post balloon injury. At 5 mg/kg/day a nonsignificant 23% reduction of intimal area was observed. At the higher dose of 15 mg/kg/day, losartan produced a 48% reduction in intimal area (P less than 0.05) compared to the vehicle-infused group. The cellular density of the neointima was not affected by losartan, indicating a probable effect of the drug upon migration and/or proliferation of smooth muscle cells. In separate groups of non-ballooned rats, losartan infusions of 5 and 15 mg/kg/day produced significant rightward shifts (averaging 6.4- and 55-fold, respectively) in curves relating increases in blood pressure to intravenous Ang II in pithed rats determined between 2 and 16 days following initiation of losartan infusion. Mean arterial blood pressure (determined under alpha-chloralose anesthesia) was reduced following continuous losartan infusion for 6 days from 128 +/- 8 mm Hg (vehicle) to 105 +/- 8 mm Hg at 5 mg/kg/day (P less than 0.05), and 106 +/- 4 mm Hg at 15 mg/kg/day (P less than 0.05). Thus, losartan attenuated the vascular response to balloon catheter injury, and this effect was associated with functional block of vascular AT1 receptors. The results support a role for Ang II, acting via AT1 receptors, in myointimal thickening subsequent to balloon injury of rat carotid arteries.     

Nitric oxide modulates the interaction of pressure-induced wall mechanics and myogenic response of rat intramural coronary arterioles

Interactions between the biomechanical characteristics and pressure-induced active response of coronary microvessels are still not well known. We tested the hypothesis that pressure-dependent biomechanical characteristics of the coronary vascular wall are modulated by the active myogenic response and local vasodilators. We have utilized data obtained previously in isolated rat intramural coronary arterioles (approximately 100 microm in diameter), in which the diameter was investigated as a function of intraluminal pressure (Szekeres et al.: J. Cardiovasc. Pharmacol., 43, 242-249, 2004). To characterize the magnitude of myogenic response, diameter was expressed as percent of passive diameter as a function of pressure (normalized diameter; ND). In addition, circumferential wall stress (WS) and incremental distensibility (ID) were calculated. In control conditions, after an initial increase between 0-30 mm Hg, ND decreased substantially as pressure increased from 30 to 150 mm Hg. Correspondingly, WS gradually increased as a function of pressure (from 0.3 +/- 0.03 to 34.7 +/- 4.4 kPa) exhibiting a plateau phase between 40-80 mm Hg. In contrast, ID decreased and reached negative values (min: -104.9 +/- 21.9 10(-6) m2/N at 50 mm Hg). Inhibition of nitric oxide (NO) synthase by L-NNA decreased basal diameter (approximately 35% at 2 mm Hg), eliminated pressure-induced changes in ND, reduced the slope of pressure-WS curve, and decreased ID at lower pressures. Simultaneous administration of L-NNA and adenosine (which restored initial diameter, i.e. length of smooth muscle) restored--in part--the pressure-induced reduction in ND, reversed the pressure-induced behavior of WS to control, but not that of ID. These results not only confirm that in coronary arterioles wall stress is regulated by the myogenic response, but also suggest that there is interplay between the mechanical behavior of the wall and the myogenic response. Furthermore, the presence of NO seems to be necessary for maintaining a higher distensibility of intramural coronary arterioles allowing increases in diameter to lower pressures, which then activate the myogenic mechanism resulting in constrictions and full development of myogenic tone, as indicated by the presence of negative slope of pressure-diameter curve in the presence of NO.     

Effect of prolonged renal dysfunction on intravascular and extravascular pulmonary fluid volumes during left atrial hypertension

To examine the development of pulmonary edema during experimental renal dysfunction, left atrial pressure was altered in 14 mongrel dogs divided into two groups. Group 1 was composed of seven control animals, and Group 2 was composed of seven animals with surgically induced renal failure (1 week of bilateral ureteral ligation). Data were obtained at two levels of matched transmural pulmonary vascular pressure (defined as mean left atrial pressure less serum protein osmotic pressure). In the animals with renal dysfunction, extravascular lung water (EVLW) (thermal-green dye technique) was higher at moderately (-1 to -2 mm Hg) and severely elevated (11 to 12 mm Hg) vascular driving pressures (11.5 +/- 1.2 cc/kg vs 10.6 +/- 0.8 cc/kg and 14.8 +/- 1.3 cc/kg vs 13.0 +/- 1.9 cc/kg, respectively, both P less than 0.05 vs control). Because protein osmotic pressure was lower in the renal failure group (15.0 +/- 1.8 mm Hg vs 18.4 +/- 1.4 mm Hg, P less than 0.05), greater accumulations of extravascular lung water occurred at lower levels of left atrial pressure (14.2 +/- 1.4 mm Hg vs 17.1 +/- 1.2 mm Hg, P less than 0.05; 26.8 +/- 2.6 mm Hg vs 29.5 +/- 2.3 mm Hg, P less than 0.01). In addition, when the ratio of EVLW/PBV (pulmonary blood volume) was examined in both groups at each stage of the experiment, the ratio was greater in the Group 2 animals at each elevated pressure, suggesting increased permeability with renal dysfunction. In conclusion, pulmonary edema formation occurs at lower left atrial pressures in the setting of sustained renal dysfunction, this phenomenon can be partially explained by lower protein osmotic pressure though altered pulmonary microvascular permeability may contribute to edema formation.     

Red cell egress from the marrow: ? vis-à-tergo

The egress of red cells from the marrow requires their translocation from the hemopoetic space into the marrow sinus lumen. The force for this translocation may be derived from a pressure drop that exists across the marrow sinus wall. Modeling suggests that a pressure gradient of the magnitude estimated to be present in the marrow could drive cells rapidly through pores in the sinus endothelium.     

Computational analysis of coupled blood-wall arterial LDL transport

The transport of macromolecules, such as low density lipoproteins (LDLs), across the artery wall and their accumulation in the wall is a key step in atherogenesis. Our objective was to model fluid flow within both the lumen and wall of a constricted, axisymmetric tube simulating a stenosed artery, and to then use this flow pattern to study LDL mass transport from the blood to the artery wall. Coupled analysis of lumenal blood flow and transmural fluid flow was achieved through the solution of Brinkman's model, which is an extension of the Navier-Stokes equations for porous media. This coupled approach offers advantages over traditional analyses of this problem, which have used possibly unrealistic boundary conditions at the blood-wall interface; instead, we prescribe a more natural pressure boundary condition at the adventitial vasa vasorum, and allow variations in wall permeability due to the occurrence of plaque. Numerical complications due to the convection dominated mass transport process (low LDL diffusivity) are handled by the streamline upwind/Petrov-Galerkin (SUPG) finite element method. This new fluid-plus-porous-wall method was implemented for conditions typical of LDL transport in a stenosed artery with a 75 percent area reduction (Peclet number=2 x 10(8)). The results show an elevated LDL concentration at the downstream side of the stenosis. For the higher Darcian wall permeability thought to occur in regions containing atheromatous lesions, this leads to an increased transendothelial LDL flux downstream of the stenosis. Increased transmural filtration in such regions, when coupled with a concentration-dependent endothelial permeability to LDL, could be an important contributor to LDL infiltration into the arterial wall. Experimental work is needed to confirm these results.     

Diastolic pressure-volume relations and distribution of pressure and fiber extension across the wall of a model left ventricle.

A model for left ventricular diastolic mechanics is formulated that takes into account noneligible wall thickness, incompressibility, finite deformation, nonlinear elastic effects, and the known fiber architecture of the ventricular wall. The model consists of a hollow cylindrical mass of muscle bound between two plates of negligible mass. The wall contains fiber elements that follow a helical course and carry only axial tension. The fiber angle (i.e., helical pitch) is constant along the length of each fiber but varies through the wall in accordance with the known distribution of fiber orientations in the canine left ventricle. To simplify the analysis and reduce the number of degrees of freedom, the anatomic distribution of fiber orientations is divided into a clockwise and counterclockwise system. The reference configuration for the model corresponds to a state in which, by hypothesis, the transmural pressure gradient is zero, the tension is zero for all fibers across the wall, and all fibers are assumed to have a sarcomere length of 1.9 micrometer. This choice of reference configuration is based on the empirical evidence that canine ventricles, fixed in a state of zero transmural pressure gradient and dissected, demonstrate sarcomere lengths between 1.9 and 2.0 micrometer in inner, middle, and outer wall layers, while isolated ventricular muscle bundles are observed to have zero resting tension when the sarcomere length ranges from 1.9 to 2.0 micrometer. An equation representing the global condition for equilibrium is derived and solved numerically. It is found that the model's pressure-volume relation is representative of diastolic filling in vivo over a wide range of filling pressures, and the calculated midwall sarcomere lengths in the model compare favorably with published experimental data. Subendocardial fibers are stretched beyond Lmax even at low filling pressures, i.e., 5 mm Hg, while fibers located between 60-80% of wall thickness extend minimally between 5 and 12 mm Hg. The hydrostatic pressure field within the wall is highly nonlinear. The pressure rises steeply in the subendocardial layers so that the net gain in pressure in the inner third of the wall is 85% of the filling pressure. It is demonstrated that these results are independent of heart size for a family of heart models that are scale models of each other. They are, however, critically dependent on the existence of longitudinally oriented fibers in the endocardial and epicardial regions of heart wall.     

Simultaneous pressure and 19F NMR pH measurements of smooth muscle cells of intact hog carotid arteries at rest and during contractions with norepinephrine

Using 19F NMR we have measured the intracellular pH of the vascular smooth muscle cells of hog carotid arteries at rest and during contractions induced with norepinephrine. Experiments were performed on single, intact arteries closed at both ends, superfused from the lumen and loaded with the 19F NMR pH indicator alpha-difluoromethylalanine. At rest, luminal pressure was maintained at 100 +/- 2 mm Hg and intracellular pH was 7.12 +/- 0.04. Contractions elicited with 10(-5) M norepinephrine were associated with a pressure increase of 18 +/- 6 mm Hg and a decrease in pH of 0.04 +/- 0.02 units.     

Central transmural venous pressure and plasma arginine vasopressin during negative pressure breathing in man

After overnight food and fluid restriction, 8 normal healthy males were examined in the upright sitting position before (prestudy), during and after (recovery) negative pressure breathing (NPB) with a pressure (P = difference between airway pressure and barometric pressure) of -9.6 +/- 0.5 to -10.4 +/- 0.4 mm Hg for 30 min. Plasma arginine vasopressin (pAVP) did not change significantly comparing prestudy with 10 and 30 min of NPB or comparing recovery with NPB at 10, 20 or 30 min. However, at 20 min of NBP, pAVP was slightly lower than at prestudy (p less than 0.05). Central venous pressure (CVP) decreased significantly during NPB, and central transmural venous pressure (CVP-P) increased significantly from -0.9 +/- 0.8 mm Hg to 3.8 +/- 0.7, 4.3 +/- 0.7 and 4.5 +/- 0.6 mm Hg (p less than 0.001) after 10, 20 and 30 min, respectively. Systolic, diastolic and mean arterial pressure and heart rate did not change significantly during NPB. Diuresis, natriuresis, kaliuresis, osmotic excretion and clearance were slightly increased during the recovery hour after NPB compared to prestudy, while urine osmolality decreased during NPB (n = 6). However, none of these changes were significant. There was no significant correlation between CVP-P and pAVP. In conclusion, -10 mm Hg NPB for 30 min in upright sitting subjects did not change pAVP consistently, while CVP-P was significantly increased and HR and arterial pressures were unchanged. This lends support to the concept that arterial baroreceptors and not cardiopulmonary mechanoreceptors are of importance in regulating AVP secretion in man.