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Am J Physiol Heart Circ Physiol 277: H756-H762, 1999;
0363-6135/99 $5.00
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Vol. 277, Issue 2, H756-H762, August 1999

Effects of long-term, high-altitude hypoxia on the capillarity of the ovine fetal heart

A. M. Lewis1, O. Mathieu-Costello2, P. J. McMillan1, and R. D. Gilbert1

1 Center for Perinatal Biology, Loma Linda University, Loma Linda 92350; and 2 Department of Physiology, School of Medicine, University of California, San Diego, La Jolla, California 92093


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

To determine the effect of chronic hypoxia on myocardial capillarity, we exposed pregnant ewes to an altitude of 3,820 m from day 30 to day 139 of gestation and compared the fetus to low-altitude (~300 m) controls. We hypothesized that capillarity would increase in the hypoxic myocardium to optimize oxygen and metabolite flux to hypoxic tissues. Fetal hearts were fixed by retrograde aortic perfusion and processed for microscopy and stereological evaluation. Fiber cross-sectional area and capillary density were measured and standardized to sarcomere length. Capillary volume density and capillary diameter were measured, capillary-to-fiber ratio and capillary length density were calculated, and the capillary anisotropy coefficient was obtained from a table of known values. Capillary-to-fiber ratio, capillary volume density, and the capillary anisotropy coefficient were not different between hypoxia and control groups. Capillary diameter was significantly larger in the right compared with the left ventricle of hypoxic but not control hearts; fiber cross-sectional area tended to be larger in the right ventricle of both groups, but this was not significant. As a result of larger fiber size, capillary density and capillary length density were significantly smaller in the right ventricle of hypoxic but not control fetal hearts. Contrary to our hypothesis, the ovine fetus does not show morphological adaptation in the myocardium after ~109 days of high-altitude hypoxic stress.

light microscopy; morphometry; angiogenesis


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

PREGNANCY COMPLICATED WITH high-altitude hypoxemic stress has been shown to elevate risk for preeclampsia and low maternal blood volume (34) and contribute to low birth weight and increased fetal mortality rates (21, 22, 32). In previous experiments, our laboratory examined the effects of long-term, high-altitude hypoxemia (3,820 m) on ovine fetal cardiac output and reported a 34 and 38% decrease in right and left ventricular outputs, respectively, after 14 days of hypoxia (12). After 90 days of fetal hypoxia, a substantial reduction in right and combined ventricular outputs were found with no significant difference in left ventricular output (11). Despite this profound deficit in flow, a redistribution of blood flow was observed to favor the heart and brain (10), at the expense of the rest of the tissues, maintaining physiological oxygen delivery to these vital organs.

We also found that chronic hypoxia significantly reduced the inotropic response to calcium (4) in ovine fetal papillary muscles, and it elevated cardiac enzymes such as citrate synthase and lactate dehydrogenase (23). Left and right ventricular function was significantly depressed with prolonged hypoxemia (1, 11, 12).

In addition to potential hypoxic influences on myocyte function, we hypothesized that morphological adaptations may have occurred that altered cardiac function. It is well known that substantial right ventricular hypertrophy occurs at moderate elevations after only a few days in the adult. Significant right and left ventricular hypertrophy is seen in fetal and young rats (7, 25, 30), young guinea pigs (13), calves (15), pigs (8), and human children (2), whereas myocardial hypotrophy has been found in developing chick hearts (14) exposed to gestational hypoxia. It has been speculated that, in the face of myocyte hypertrophy, tissue oxygenation is threatened, and compensatory angiogenesis has been found to occur in the right or in both ventricles of rats (7, 30), guinea pigs (13, 33), calves (15), and puppies (3) born at moderate to high altitudes.

To our knowledge there has been no comprehensive morphological study quantitating the cardiac adaptations to gestational hypoxia in the near-term sheep fetus. We therefore sought to identify the changes in microvasculature and myocyte structure of the developing ovine myocardium after prolonged gestational high-altitude hypoxia using light microscopy and stereological analysis. We hypothesized that capillary proliferation would occur to offset probable fiber hypertrophy and, therefore, maintain proper oxygenation in an hypoxic environment.


    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Isolation of fetal sheep heart. Time-dated pregnant ewes of a homogeneous-mixed Western breed were obtained from a single supplier (Nebeker Ranch, Lancaster, CA) and randomly allocated to long-term hypoxic or control groups. The control group (n = 5) remained at Nebeker Ranch, altitude ~300 m, until ~138 days of gestation. At 30 days of gestation, we transported the long-term hypoxic group (n = 6) to the Barcroft Laboratory (White Mountain Research Station, Bishop, CA; altitude 3,820 m), where they remained until ~138 days of gestation. In a previous study we reported that arterial PO2 was 102 ± 2 mmHg at Nebeker Ranch and 64 ± 2 mmHg at the White Mountain Research Station (barometric pressure ~480 Torr) (24). Both high- and low-altitude ewes were kept in a sheltered pen and provided with alfalfa pellets, mineral supplements, and clean water ad libitum. We transported animals (~7-h trip) from either location to our laboratory at Loma Linda University, where they either underwent immediate study or, in the case of hypoxic ewes awaiting study, were surgically implanted with a nonocclusive tracheal catheter (6) for nitrogen gas administration to reestablish hypoxemia immediately after arrival at our laboratory. On the experimental day, animals ranged from 139 to 142 days of gestation (control: 139.3 ± 0.2 days; hypoxic: 140.4 ± 0.7 days). The ewes were sedated intravenously with thiamylal (10 mg/kg), intubated, and kept under surgical anesthesia (halothane 5% in oxygen) while we delivered the fetuses through a midline laparotomy. After fetal weights were recorded, the fetal heart was quickly removed via a midline thoracotomy and immersed in heparinized saline.

Tissue preparation. Within 1 min of removal of the heart, the aorta was secured to a cannula, which was connected to a perfusion pump. The heart was immediately flushed with heparinized saline and 0.1% sodium nitrite at a nonpulsatile flow rate of 50 ml/min until the exudate was clear of red blood cells (~90 s). The apex of the left ventricle (LV) was pierced for outflow. Retrograde aortic perfusion was then switched to 6.25% glutaraldehyde in 0.1 M sodium cacodylate buffer, pH 7.4, 1,125 mosmol, for 20 min at continuous flow rate. The physiological flow rate was calculated to be 50-55 ml/min for these fetuses. A pressure transducer was calibrated before each experiment and connected to the perfusion line to measure changes in perfusion pressure. Hearts were dissected free of the great vessels and weighed. Right ventricle (RV) and LV plus septum (LV + S) weights were also obtained. RV and LV samples were taken from the entire thickness of the central portion of the ventricle free wall, 50% of the distance from apex to base. From the same area the wall thickness of both ventricles was measured under a dissecting microscope. Tissue from each ventricle was subsampled into subepicardium and subendocardium portions of equal size, and the midwall section was discarded. Subepicardium and subendocardium were subsequently cut into 1 × 1 × 3 mm blocks and immersed in glutaraldehyde fixative for at least 1 day. Blocks were rinsed in 0.1 M sodium cacodylate buffer, postfixed for 2 h in 1% osmium tetroxide solution in cacodylate buffer, dehydrated in increasing concentrations (70-100%) of ethanol, rinsed in propylene oxide, and embedded in Araldite.

Tissue sectioning. Sections 1 µm in thickness were cut using an LKB Ultrotome III and stained with aqueous 0.1% toluidine blue solution. For each subsample, 24 blocks were embedded, and from those, 4 transverse and 4 longitudinal blocks were randomly selected from each subepicardial and subendocardial sample. Transverse sections were cut (1 µm) with the muscle fiber axis at an orientation perpendicular to the microtome knife. As sections were cut and examined under the light microscope, they were determined to be transverse when changing the sectioning angle by 5° in either direction produced smaller A-band spacing within the fiber sections. For longitudinal sections, at least three sections were obtained, after the sectioning angle was changed by 1°, with muscle fibers parallel to the microtome knife, and sarcomere length was measured (mean of 10 measurements) in each section. Longitudinal sections were identified as those with the shortest sarcomere length compared with that in sections obtained at a sectioning angle altered by 1° in either direction. Because of the interwoven network of myocytes characteristic of the heart, sections often contained areas of longitudinally as well as obliquely or transversely oriented fibers. In these cases, a specific area was chosen as nearly longitudinal, and the above procedure of systematically altering the section angle was performed until a longitudinal subsample was obtained.

Morphometric analysis. Morphometric data were collected from the 1-µm sections of subepicardium and subendocardium from the LV and RV. Mean fiber cross-sectional area [<OVL><IT>a</IT></OVL>(f)], mean fiber cross-sectional perimeter [<OVL><IT>b</IT></OVL>(f)], and mean number of capillaries around a fiber (NCAF) were measured with an image analyzer (Videometric 150, American Innovision, San Diego, CA) on transverse sections. An average of 167 fibers were measured per subsample at ×400 magnification. Capillary diameter [<OVL><IT>d</IT></OVL>(c)] was measured on transverse sections using image analysis (560 capillaries/subsample) by identifying circular profiles on transverse sections with a diameter <= 8 µm and a difference between the shortest and longest diameters not exceeding 15%. This excluded small venules of ~10 µm in diameter.

Capillary numerical density was determined on transverse [QA(0)] and longitudinal [QA(pi /2)] sections (4 blocks each, ×400 magnification) with an average of three and six fields sampled per section, respectively. Because of the effect of sarcomere length on fiber cross-sectional area, we normalized fiber cross-sectional area and capillary density to a 1.9-µm sarcomere length, a value close to the mean of each group. Points were collected and stored on an Apple computer (17). Capillary-to-fiber ratio [NN(c, f)], was calculated as the product of capillary number per fiber area in transverse section and fiber cross-sectional area. The number of fibers sharing one capillary (SF) was calculated as NCAF/NN(c, f). Capillary length density [JV(c, f)], the capillary orientation parameter (K), and its coefficient [c(K, 0)], which represents the contribution of tortuosity and branching to capillary length, were estimated using the method developed by Mathieu et al. (16). Briefly, it was demonstrated that the Fisher axial distribution model is suitable for estimation of capillary anisotropy in rat heart muscle (26). Thus the capillary length density is related to capillary numerical density in transverse and longitudinal sections by the following equations
J<SUB>V</SUB>(c, f) = <IT>c</IT>(<IT>K</IT>, 0) · Q<SUB>A</SUB>(0) (1)
and
J<SUB>V</SUB>(c, f) = <IT>c</IT>(<IT>K</IT>, &pgr;/2) · Q<SUB>A</SUB>(&pgr;/2) (2)
where c(K, 0) and c(K, pi /2) are capillary anisotropy coefficients for transverse and longitudinal sections, respectively. Combining and rearranging Eqs. 1 and 2 gives the relationship between capillary densities and the anisotropy coefficient for transverse and longitudinal sections
Q<SUB>A</SUB>(0)/Q<SUB>A</SUB>(&pgr;/2) = <IT>c</IT>(<IT>K</IT>, &pgr;/2)/<IT>c</IT>(<IT>K</IT>, 0) (3)
In the Fisher axial distribution model, the ratio c(K, pi /2)/c(K, 0) is a uniform and monotonic function of K and thus can be used to estimate K and c(K, 0) from a table of known coefficients (16). JV(c, f) is then estimated from Eq. 1 or 2.

When capillaries are anisotropic (straight and parallel) with respect to muscle fibers, K = infinity  and c(K, 0) = 1. For isotropic (randomly oriented) capillaries, K = 0 and c(K, 0) = 2. Estimates of capillarity in each sample were expressed per unit of muscle fiber area as reference space. This prevents error due to fixation influences on extracellular space (17). Capillary volume density [VV(c, f)] was estimated using a standard point-counting procedure on transverse sections.

Statistical analysis. Differences between subepicardium and subendocardium, LV and RV, and hypoxic and control hearts were assessed using three-way ANOVA and Duncan's multiple-range test for post hoc differences. When differences between subendocardium and subepicardium were absent, the data were pooled. Subsequently, when further comparison of RV and LV showed no statistical significance, these data were also pooled. Student's t-test was used for comparison between control and hypoxic hearts. Results are presented as means ± SE, and significance was accepted at P < 0.05.


    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Gross morphology. Representative low-power light micrographs of transverse and longitudinal sections of heart muscle are shown in Fig. 1. Retrograde aortic perfusion provided optimum preservation of myocardial ultrastructure with no contracture. Pressure transducer recordings indicated no changes in perfusion pressure of any animals, as indicated by the flow rate (50-55 ml/min), other than the negligible rise in pressure observed caused by gradual hardening of the tissue with fixation.





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Fig. 1.   Light micrographs of portions of myocardium in transverse (A and C) and longitudinal (B and D) sections from control (A and B) and hypoxic (C and D) fetal heart. Bar, 20 µm.

Fetal weight in the hypoxic group was not statistically different from that in the control group (Table 1). There were no significant differences in heart weight, LV + S weight, and RV weight between hypoxic and control fetuses (Table 1). Sarcomere length in the hypoxic animals was not statistically different from that in controls (Table 2), and it is therefore assumed that animals were perfusion fixed at comparable levels of diastole. Wall thickness in the LV and RV (Table 1) was not significantly different in hypoxic myocardium compared with those in controls.

                              
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Table 1.   Age, heart weights, and wall thickness in control and hypoxic fetuses


                              
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Table 2.   Light microscopic data from control and long-term hypoxic fetal myocardium

Light microscopy. Mean sarcomere length varied from 1.90 to 1.99 µm and from 1.89 to 1.93 µm (Table 2) in subendocardial and subepicardial regions of control and hypoxia, respectively, and there was no significant difference between regions. No systematic differences were found between control and hypoxic groups in capillary-to-fiber ratio, number of capillaries around a fiber, capillary anisotropy coefficient, number of fibers sharing one capillary, mean fiber cross-sectional area, and capillary volume density (Table 2).

Although capillary diameter was not significantly different between control and hypoxia, it was significantly greater in the RV (4.81 ± 0.08 µm) than in the LV of hypoxic fetuses (4.46 ± 0.06 µm, P < 0.05) (Fig. 2) but not in controls (RV, 4.71 ± 0.16 µm; LV, 4.44 ± 0.12 µm). Similarly, capillary numerical density did not differ between control and hypoxia, whereas it was significantly lower in the RV (5,867 ± 167 capillaries/mm2) than in the LV of hypoxic animals (7,144 ± 355 capillaries/mm2, P < 0.05) (Fig. 3). This is consistent with the tendency for fiber cross-sectional area to be greater in the RV (control, 42.5 ± 3.6 µm; hypoxic, 47.3 ± 3.8 µm) than in the LV (control, 35.5 ± 1.9 µm; hypoxic, 37.3 ± 4.0 µm; P = not significant). Capillary numerical density was not significantly different between control ventricles (RV, 6,358 ± 423 capillaries/mm2; LV, 7,427 ± 626 capillaries/mm2) (Fig. 3).


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Fig. 2.   Comparison of capillary diameter [<OVL><IT>d</IT></OVL>(c)] in right (open bars) and left ventricle (filled bars) of control (n = 5) and high-altitude (n = 6) fetal hearts. * Significantly different (P < 0.05) from right ventricle.



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Fig. 3.   Comparison of capillary number per fiber cross-sectional area between right (open bars) and left ventricle (filled bars) of control (n = 5) and hypoxic (n = 6) fetal myocardium. * Significantly different (P < 0.05) from left ventricle.

Capillary length density was not significantly different between hypoxic and control animals (Fig. 4). It was significantly smaller in hypoxic RV (6,339 ± 288 mm-2) than hypoxic LV (7,477 ± 362 mm-2; P < 0.05) (Fig. 4), consistent with the decreased capillary density and unchanged anisotropy coefficient in the hypoxic RV. Capillary length density was not significantly different in control hearts (RV, 7,046 ± 400 mm-2; LV, 7,969 ± 546 mm-2). Capillary volume density was not significantly different between hypoxic and control animals (Table 2).


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Fig. 4.   Comparison of capillary length density [JV(c, f)] in right (open bars) and left ventricle (filled bars) of control (n = 5) and hypoxic (n = 6) ovine fetal myocardium. * Significantly different (P < 0.05) from left ventricle.


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Blood gases and pH. Blood gases were not measured in fetuses for this study because of the immediate, rapid removal of the heart. However, in a previous study (11), arterial PO2 averaged 23.3 ± 0.5 Torr in controls compared with 19.3 ± 0.8 Torr (P < 0.01) in high-altitude animals. Similarly, PCO2 was reduced from 48.9 ± 1.2 Torr in controls to 39.9 ± 0.9 Torr (P < 0.01) in hypoxic fetuses. However, pH remained unchanged between hypoxic (7.35 ± 0.01) and control animals (7.33 ± 0.01), and fetal lactate was also unchanged. Oxyhemoglobin concentration was significantly reduced from 59.2 ± 1.7% in controls to 49.8 ± 3.6% (P < 0.05) in the hypoxic group. However, because of the elevated hemoglobin concentration with hypoxia, oxygen content did not differ significantly between the two groups (11).

Gross weights. The sheep fetuses in this study do not exhibit low birth weight after ~109 days of development at 3,820 m. We report comparable birth weights for control and high-altitude sheep fetuses (Table 1). Growth retardation in high-altitude native human infants was reported after development at an altitude range of 2,740-3,100 m (22), and in another study, trends toward low birth weights were reported at 3,100 m (34). Despite the higher altitude in our study (3,820 m), we may speculate that the influence of hypoxic stress on birth weight is attenuated in the sheep, representing a unique adaptive characteristic. In addition, Jacobs et al. (9) reported significant growth retardation in the ovine fetus exposed to 4,572 m from day 30 to day 135 of gestation. It is possible that, despite profound physiological adaptation in our model at 3,820 m, the critical stimulus for morphological adjustments to hypoxia in the ovine model occurs somewhere between our altitude of 3,820 m and that of 4,572 m reported by Jacobs et al. (9).

Gross measurements of whole heart weights, ventricular weights, and wall thicknesses were similar for control and hypoxic fetuses (Table 1), indicating a lack of the hypertrophy commonly seen in developing hearts after altitude exposure (2, 8, 13, 15, 25). These data are supported further by the unchanged fiber cross-sectional area in hypoxic compared with control myocardium (Table 2). Fiber cross-sectional area tended to be greater in the RV than LV in control and hypoxic myocardium. This might suggest that the fetal heart is in early stages of anatomic acclimatization at 3,820 m. Because extreme RV hypertrophy and capillary proliferation were reported in several animal models after equivalent high-altitude exposure, and because we did not find significant changes in capillarity, we speculate that fetal sheep offer a suitable model for altitude tolerance.

Capillarity. Contrary to our hypothesis, this level of hypoxic stress was insufficient to stimulate angiogenesis (Table 2 and Fig. 3) and/or fiber hypertrophy (Tables 1 and 2) in the developing ovine fetal heart. Arias-Stella and Recavarren (2) found substantial RV hypertrophy in human infants and children born at altitudes ranging from 3,107 to 4,360 m as well as a retardation in the shift from RV to LV dominance commonly observed in the human heart after birth. In rats born at 3,500 (7) and 5,000 m (30), profound RV and LV hypertrophy has been seen with concomitant angiogenesis. RV hypertrophy and capillary growth has also been observed in young guinea pigs after simulated altitude exposure (fractional inspired oxygen 10%) (13). Because these models (7, 13, 30) exhibit angiogenesis accompanied by fiber hypertrophy, it may be that the lack of ventricular fiber hypertrophy in our model removes an essential angiogenic stimulus. If this is true, then we may predict that a direct angiogenic stimulus may also originate from surrounding tissue made hypoxic by the hypertrophic adaptive response to altitude and not directly from low arterial PO2. Furthermore, morphological adaptation could occur subsequent to the physiological changes associated with birth.

Elevated arterial pressure (afterload) and/or increased workload are speculated to be causative agents for ventricular fiber hypertrophy rather a than direct hypoxic influence. In a previous study from our laboratory (11), hypoxic fetal sheep were shown to exhibit a 17% rise in arterial pressure, a potentially strong hypertrophic stimulus. However, our previous data (11, 12) showed that this level of arterial pressure increase plus hypoxia is not an effective hypertrophic influence and that the hypoxic fetal heart is less sensitive to increased arterial pressure. Thus the sheep fetus compensates for the higher systemic pressure at altitude, possibly preventing hypertrophy.

In large mammals such as calves (19-21 wk), altitude exposure (3,500 m) for 53 days produced RV hypertrophy as well as capillary growth (15). These calves exhibited an elevated arterial pressure and reduced oxygen content. The oxygen content for our sheep was not different from that for controls (11). Oxygen delivery to the myocardium of our fetal sheep could have remained within a physiological range because of the favorable redistribution of blood flow and maintenance of oxygen content. Also, the reduction in ventricular arterial pressure sensitivity prevents the fetal heart from expending additional energy in the face of higher arterial pressure at altitude. Thus physiological adjustments could occur without morphological adaptation at this altitude.

In an acute hypoxic model, in the 122-day ovine fetus, Fisher et al. (5) reported that myocardial blood flow was 160% of control after 15 min of hypoxia (PO2 14 ± 1 Torr), and Reller et al. (28) reported that blood flows were 154% of control in 128-day fetuses after 5-8 days of hypoxia (PO2 <18 Torr). Both authors suggested that remodeling of the ovine fetal coronary vascular tree occurred to accommodate these increased flows. Because we found no evidence of capillary growth (Table 2), we may speculate that recruitment, rather than growth of new vessels, accommodated the enhanced coronary flow observed at altitude. It has also been shown (29) that a threefold coronary flow reserve exists at physiological arterial pressure in late-gestation fetal sheep. This large reserve capacity would be sufficient to accommodate the flow increases reported by Fisher et al. (5) and Reller et al. (28) as well as our own results (10). However, Reller et al. (28) showed higher maximal myocardial blood flows with adenosine infusion (induced maximal vasodilatation) after 5-8 days of hypoxia (PO2 <18 Torr) in the ovine fetus compared with controls, suggesting some degree of capillary proliferation.

Capillary diameter in hypoxia was significantly larger in the RV compared with that in the LV (Fig. 2), and the same trend was seen in controls. The reverse was seen for capillary density (Fig. 3). As reported previously by Smolich et al. (31), these characteristics of the sheep fetus are similar to those of humans, for whom the fetal RV is dominant (27) and is matched by larger capillaries and a smaller capillary density. With normal growth after birth, the LV assumes the dominant role, and the capillary size and density relationships are reversed. These findings suggested that the hypoxic myocardium exhibits normal growth patterns despite high-altitude stress.

In addition to angiogenesis, the contribution of capillary tortuosity and branching to capillary length may have been enhanced with altitude exposure to increase capillary and fiber surface contact and, therefore, oxygen delivery. We found the anisotropy coefficient c(K, 0) to be similar in both hypoxic and control fetal myocardium, and thus there was no evidence of increased tortuosity and branching. In hindlimb muscles of deer mice living at 3,820 m, Mathieu-Costello (18) reported no change in capillary number or capillary tortuosity and branching, whereas the intensely aerobic flight muscle of birds showed increased capillary number and altered capillary tortuosity and branching with adaptation to the same altitude (19, 20).

In conclusion, these studies demonstrated that, after ~109 days of high-altitude (3,820 m) hypoxemia, myofiber hypertrophy and capillary growth did not occur in the ovine fetal myocardium. This is demonstrated by the lack of changes in capillary-to-fiber ratio, fiber cross-sectional area, capillary diameter, and capillary density between hypoxic and control fetuses. Similarly, capillary length and volume density remained unchanged between the two groups. The degree of capillary tortuosity and branching was not affected by high altitude. Thus reduced ventricular contractility and cardiac output observed in ovine fetuses at 3,820 m cannot be explained by morphological changes in either fiber size or capillarization.


    ACKNOWLEDGEMENTS

We thank Virginia Stiffel, Thomas Smith, Larnele Hazelwood, Peter Agey, and Ernest Whitter for technical support.


    FOOTNOTES

This work was supported by National Institutes of Health Grants HD-31226 and 5P0-HL-17731.

The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.

Address for reprint requests and other correspondence: A. M. Lewis, Center for Perinatal Biology, Loma Linda University, Loma Linda, CA 92350 (E-mail: dmlewis{at}budgetblinds.com).

Received 24 December 1998; accepted in final form 23 March 1999.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

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16.   Mathieu, O., L. M. Cruz Orive, H. Hoppeler, and E. R. Weibel. Estimating length density and quantifying anisotropy in skeletal muscle capillaries. J. Microsc. 131: 131-146, 1983[Medline].

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Am J Physiol Heart Circ Physiol 277(2):H756-H762
0002-9513/99 $5.00 Copyright © 1999 the American Physiological Society



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