Vol. 277, Issue 4, H1532-H1539, October 1999
Regional ischemia in hypertrophic
Langendorff-perfused rat hearts
J. F.
Ashruf1,
C.
Ince2, and
H. A.
Bruining1
1 Department of Surgery,
Erasmus University of Rotterdam, 3015 GD Rotterdam; and
2 Department of Anesthesiology,
University of Amsterdam, 1105 AZ Amsterdam, The Netherlands
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ABSTRACT |
Myocardial hypertrophy decreases the muscle
mass-to-vascularization ratio, thereby changing myocardial perfusion.
The effect of these changes on myocardial oxygenation in hypertrophic
Langendorff-perfused rat hearts was measured using epimyocardial NADH
videofluorimetry, whereby ischemic myocardium displays a high
fluorescence intensity. Hypertrophic hearts, in contrast to control
hearts, developed ischemic areas during oxygen-saturated Langendorff
perfusion. Reoxygenation of control hearts after a hypoxic episode
resulted in a swift decrease of fluorescence in a heterogeneous pattern of small, evenly dispersed, highly fluorescent patches. Identical patterns could be evoked by occluding capillaries with microspheres 5.9 µm in diameter. Ten seconds after reoxygenation there were no more
dysoxic areas, whereas reoxygenation in hypertrophic hearts showed
larger ischemic areas that took significantly longer to return to
normoxic fluorescence intensities. Hypothesizing that the larger areas
originate at a vascular level proximal to the capillary network, we
induced hypoxic patterns by embolizing control hearts with microspheres
9.8 and 15 µm in diameter. The frequency distribution histograms of
these dysoxic surface areas matched those of hypertrophic hearts and
differed significantly from those of hearts embolized with 5.9-µm
microspheres. These results suggest the existence of areas in
hypertrophic Langendorff-perfused hearts with suboptimal
vascularization originating at the arteriolar and/or arterial level.
hypertrophy; hypoperfusion; reduced nicotinamide adenine
dinucleotide fluorescence; microspheres; microcirculation
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INTRODUCTION |
HYPERTROPHIC MYOCARDIUM is more susceptible to
ischemic damage than normal myocardium because of, among other
factors, changes in its vascularization (7, 21).
Morphological studies of vasculature in hypertrophic myocardium have
demonstrated profound changes in anatomy and function. In hypertrophic
myocardium, capillary density and coronary vascular reserve decrease,
whereas minimal coronary vascular resistance increases (11, 19, 20).
Hypertrophy also increases diffusion distances from capillaries to
myocytes (22, 24). These changes are not distributed evenly throughout the myocardium, resulting in a diversion of coronary flow from subendocardial to subepicardial layers (1, 8). Many studies have shown
this transmural redistribution of coronary flow in hypertrophy with
changes in the heterogeneity of flow and vascularization between
subsequent transmural myocardial layers (1, 22, 23). Less is known,
however, of the effect of hypertrophy on the local distribution of
oxygen through the myocardial microcirculation. For instance,
measurements of local oxygen consumption and supply did not show any
difference between normal and hypertrophic in situ hearts at rest (25)
and during stress (5, 28), whereas a significant functional impairment
in hypertrophic hearts was demonstrated. An explanation may be that
these hearts were blood-perfused in situ hearts with a physiological
oxygen supply-to-demand ratio as compared with Langendorff-perfused rat
hearts, which are known to have a marginal oxygen supply, resulting in
the development of ischemia when the oxygen supply-to-demand
ratio decreases slightly (13). In a previous study we found that
hypertrophic Langendorff-perfused hearts spontaneously developed
hypoxic areas that could be alleviated by factors influencing oxygen
free radical concentrations through the addition of fatty acids
or superoxide dismutase to the perfusate (12).
The purpose of the present study was to investigate the nature of the
spatial distribution of the hypoxic state in myocardial regions and the
vascular level at which perfusion is disturbed in myocardial
hypertrophy by using epicardial NADH videofluorescence to monitor the
mitochondrial energy state (15). Measurement of the mitochondrial
autofluorescence of reduced pyridine nucleotide (NADH) of the
epimyocardium allows the identification of hypoxic regions because NADH
(which accumulates during hypoxia) fluoresces when exited with
ultraviolet (UV) light and oxidized
NAD+ does not (6). There is also a
fairly linear relationship between the oxygen concentration available
to mitochondria and the NADH fluorescence intensity, as has been shown
in isolated mitochondria (6). In this way the local mitochondrial
energy state of the myocardium can be visualized (2). In normal
Langendorff-perfused rat hearts a stepwise transition from anoxic to
normoxic perfusion was accompanied by a transition from high epicardial
NADH fluorescence intensity to low fluorescence intensity with a
reproducible patchy pattern of high-fluorescence anoxic areas lagging
behind low-fluorescence normoxic areas (15). These areas are
microcirculatory weak units, because in a given heart they were always
at the same location and were the first to become hypoxic during
tachycardia (2, 15). These weak units were also the first to become
hypoxic during inhibition of nitric oxide synthesis in endotoxemic rat hearts (4) and could be the cause of shunting pathways during sepsis
(17). Hypoxic areas of identical size and pattern could also be
elicited by embolization of the capillaries by microspheres whose
diameter corresponded to the capillary diameter (5.9 µm), whereas
embolization of arterioles and arteries by larger microspheres produced
larger hypoxic areas not corresponding to the heterogeneous areas seen
during recovery from hypoxia (15). We hypothesized that in hypertrophic
myocardium this pattern would be altered because of the formerly
mentioned circulatory changes, resulting in suboptimally perfused
myocardial regions. Furthermore, the size of the hypoxic areas in
hypertrophic myocardium could elucidate at which vascular level the
impaired perfusion originated. In this study we analyzed the anatomic
substrate responsible for the appearance of these dysoxic areas in
hypertrophic hearts. Preliminary results were reported elsewhere (3).
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MATERIALS AND METHODS |
Experimental setup.
Male Wistar rats weighing 200-250 g were operated on, undergoing
subdiaphragmatic and suprarenal aortic narrowing to induce left
ventricular hypertrophy (18), and were killed 6 wk later when they
weighed 250-300 g. For control measurements, rats of similar weight were used. Hearts were removed and perfused according to
Langendorff and paced via aortic and right ventricular leads. Mean
coronary flow rates (in
ml · min
1 · g
ventricle wet wt
1) were
measured with an electromagnetic flow probe (Skalar-Medical, Delft, The
Netherlands) placed immediately proximal to the aortic cannula.
Perfusion pressure was measured with a pressure transducer (Hewlett-Packard 8805B corner amplifier) connected to the aortic cannula. The perfusate was a modified Tyrode solution (128 mM NaCl, 4.7 mM KCl, 1 mM MgCl2, 0.4 mM
NaH2PO4,
1.2 mM
Na2SO4,
20.2 mM NaHCO3, and 1.3 mM
CaCl2) containing 11.0 mM
glucose. Perfusate temperature was kept at 37°C and equilibrated
with either 95% O2-5%
CO2 or 95%
N2-5%
CO2. Perfusate pH was kept between
7.35 and 7.45. Hearts were paced at 5 Hz. The left ventricle was
cannulated and communicated with the atmosphere via its apex to prevent
generation of left ventricular pressure (2). In some experiments 10 µM nitroprusside, an endothelium-independent vasodilator, was added to the perfusate. In other experiments microspheres (Polyscience, Warrington, PA) of different diameters were infused into the coronary circulation. When indicated, the oxygen-saturated perfusate contained 10% (vol/vol) fluorocarbon F-43 emulsion (an artificial oxygen carrier) and 1% (wt/vol) fatty acid-free BSA. The stock fluorocarbon emulsion was obtained by sonifying 24 ml of F-43 and 5.6 g of pluronic
F-68 in 150 ml of water at 4°C for 1 h under continuous bubbling of
CO2 through the solution (9).
Chemicals were obtained from Merck (Darmstadt, Germany).
Fluorescence measurements.
The NADH videofluorimeter used has been described previously (2, 15).
The UV light from a 100-W mercury arc lamp (Olympus, Tokyo, Japan) was
selected by means of a UG-1 barrier filter, centered around 365 nm, to
provide the UV light needed for NADH excitation. The NADH fluorescence
signal was selected by means of a band-pass filter centered around 470 ± 20 nm and was placed in front of the camera. An image-intensified
video camera (MXRi, Adimec, Eindhoven, The Netherlands) with a
Micro-Nikkor 105-mm macrolens was used to detect NADH fluorescence
images of the left ventricle of the heart. To enable correction of
images for changes in the sensitivity of the videofluorimeter and
fluctuations in the intensity of the light source, a small piece of
uranyl calibration glass was placed next to the heart within the
excitation field. Images were recorded on a video recorder and were
computer analyzed off-line with the use of image-processing software
(TCLImage, Multihouse, Amsterdam, The Netherlands). Arbitrary units of
NADH fluorescence intensities relative to uranyl fluorescence intensity are expressed as percentages, where 100% is taken as the intensity of
epicardial NADH fluorescence at the end of a 2-min period of perfusion
with nitrogen-saturated medium.
Experimental protocols.
Hearts were allowed at least 15 min of stabilization after the start of
the Langendorff perfusion at a perfusion pressure of 80 mmHg with
oxygen-saturated perfusate before the following experimental protocols
were performed.
To examine the fluorescence patterns in hypertrophic left ventricle
during oxygen-saturated Langendorff perfusion and posthypoxic recovery,
protocol 1 was carried out. After the
stabilization of flow during normoxic perfusion, perfusion
was switched to nitrogen-saturated perfusate for 2 min and then
restored to normoxic perfusion. Because large ischemic areas already
existed during normoxic perfusion at a perfusion pressure of 80 mmHg,
perfusion pressure was increased to 100 and then 120 mmHg for 5 min
each to increase coronary flow and oxygen transport. This did not cause
the ischemic areas to disappear, and perfusion pressure was restored to
80 mmHg. Finally, to ascertain that the ischemic areas already visible
at the beginning of perfusion were reversible [and did not
represent infarcted (fibrotic) highly fluorescent myocardium
(16)], oxygen transport to the myocardium was increased
by either adding 10 µM nitroprusside to the oxygen-saturated
perfusate or switching perfusion to fluorocarbon-containing oxygen-saturated medium.
Protocol 2 was performed to examine
fluorescence patterns in control left ventricle during posthypoxic
recovery and progressive hypoperfusion. After the stabilization of flow
during normoxic perfusion, perfusion pressure was decreased to 60 mmHg
to obtain coronary flows comparable between control hearts and
hypertrophic hearts. As in protocol 1,
control hearts were subjected to a 2-min period of nitrogen-saturated
perfusion, after which perfusion was restored to oxygen-saturated
perfusate. Hereafter, each heart was subjected to stepwise reduction of
perfusion pressure from 60 mmHg to 10 mmHg in steps of 10 mmHg, with
each step lasting 3.5 min.
To determine which vascular level determined the appearance of the
ischemic areas in hypertrophic hearts, control hearts were embolized
with microspheres of different diameters in protocol 3. The frequency distributions of ischemic surface
areas in embolized control hearts were compared with those of
hypertrophic hearts. After the stabilization of flow in control hearts,
heterogeneous fluorescence patterns were elicited by switching
perfusion from oxygen-saturated perfusate to nitrogen-saturated
perfusate (for 2 min) and back. When flow had returned to baseline
values, microspheres emulsified in Tyrode solution were infused at a
rate of 500-1,000 microspheres/min into the coronary flow (15).
Microspheres had fixed diameters of 5.9, 9.8, and 15 µm. Each heart
was perfused with microspheres of one diameter, and infusion was
stopped when flow was decreased to ~75% of the baseline value. The
surfaces of the ischemic areas caused by embolization in control hearts and the surfaces of ischemic areas in hypertrophic hearts during normoxic perfusion were measured in the fluorescence images and expressed in pixels (1 pixel
670 µm2 of myocardial surface). The
transition from a normoxic area to an ischemic area is characterized by
a small transitional zone (26) where fluorescence intensity increases
gradually from normoxic to hypoxic intensity. The surface of an
ischemic area was defined as the number of pixels with a fluorescence
intensity larger than or equal to the intensity halfway between the
intensity of the normoxic surrounding area and the peak intensity of
the ischemic area. Relative frequency distributions were calculated for
six intervals of surface areas (see Fig. 7), and the proportion of total ischemic epicardial surface and the number of ischemic areas were
measured (see Fig. 8).
Data are presented as means ± SE. Mean relative frequencies of
surface areas per interval were tested for differences between groups
using unpaired t-tests. Group means of
other data were also tested for differences, also using unpaired
t-tests. The criterion for
significance was taken to be P < 0.05 for all comparisons.
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RESULTS |
Five hypertrophic Langendorff-perfused hearts (total ventricle wet wt
1.6 ± 0.2 g) were subjected to protocol
1. Hearts instantly developed ischemic areas, indicated
by patches of highly fluorescent myocardium (Fig.
1A).
These ischemic areas were stable in size and time during the entire
period of normoxic perfusion, lasting up to 30 min. After
stabilization, the perfusate was switched to nitrogen-saturated medium
for 2 min, which caused an increase of coronary flow from 13.8 ± 0.4 (at 2 min in Fig.
2A) to
24.4 ± 0.4 ml · min
1 · g
1
(at 4 min in Fig. 2A) and an
increase of NADH fluorescence intensity of the total epicardium from 32 ± 3% (Fig. 1A; at 2 min in Fig. 2B) to 100% (Fig.
1B; at 4 min in Fig.
2B). Restoration to
oxygen-saturated perfusion decreased coronary flow and epicardial
fluorescence intensity (Figs. 1C and
2A). The decrease of NADH
fluorescence intensity was spread in uneven patterns across the
epimyocardial surface with larger areas having a high fluorescence
intensity, persisting even after 20 s of reperfusion (Fig.
1C). Eventually fluorescence
intensity decreased to the baseline level at the start of the
experiment; this took longer than 5 min. To increase oxygen transport
to the myocardium after coronary flow had reached baseline levels,
perfusion pressure was increased to 100 and then 120 mmHg. Coronary
flow increased from 14.1 ± 0.3 to 17.0 ± 0.5 and then 19.8 ± 0.7 ml · min
1 · g
total ventricle wet wt
1,
respectively, but this did not cause ischemic areas to disappear (data
not shown). Perfusion pressure was then restored to 80 mmHg. The
perfusate was switched to oxygen-saturated medium containing nitroprusside to increase oxygen transport by vasodilatation. Flow
increased from 13.5 ± 0.5 to 27.8 ± 1.2 ml · min
1 · g
total ventricle wet wt
1,
and ischemic areas completely disappeared (Fig.
1D). To increase oxygen transport in
a different manner, in three additional hypertrophic hearts (total
ventricle wet wt 1.5 ± 0.1 g) not subjected to this protocol but
which also displayed ischemic areas on commencement of Langendorff
perfusion, the perfusate was switched from oxygen-saturated medium to
fluorocarbon-containing oxygen-saturated medium. Flow decreased from
14.5 ± 0.7 to 12.1 ± 0.6 ml · min
1 · g
total ventricle wet wt
1
(not significant), and the size of ischemic areas dramatically decreased (Fig. 3).

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Fig. 1.
NADH fluorescence images of a hypertrophic heart at the start of
oxygen-saturated perfusion (A), at
the end of nitrogen-saturated perfusion
(B), 20 s after reoxygenation
(C), and during perfusion with
oxygen-saturated nitroprusside-containing medium
(D).
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Fig. 2.
A: coronary flow changes in rat hearts during stepwise changes in
oxygenation. Thick line, mean coronary flow of control heart during
protocol 2 (n = 5); thin line, mean coronary flow
of hypertrophic heart during protocol
1 (n = 5); dashed
lines, ±SE. Horizontal bar indicates period of statistically
significant (P < 0.05) difference in
coronary flow between control and hypertrophic hearts.
B: mean relative NADH fluorescence in
rat hearts during stepwise changes in oxygenation. , NADH
fluorescence of control heart during protocol
2; , NADH fluorescence of hypertrophic heart during
protocol 1. Values are means ± SE.
Steps: 0-2 min, perfusion with oxygen-saturated medium; 2-4
min, perfusion with nitrogen-saturated medium; 4-6 min,
reoxygenation with oxygen-saturated medium. * Statistically
significant (P < 0.05) difference in
mean relative fluorescence between control and hypertrophic hearts.
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Fig. 3.
NADH fluorescence images of a hypertrophic heart during perfusion with
oxygen-saturated medium containing no fluorocarbons
(A) and 3 min after perfusion with
oxygen-saturated medium containing fluorocarbons
(B).
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Control hearts (n = 5, total ventricle
wet wt 1.1 ± 0.1 g) were subjected to protocol
1, which differed from protocol
2 (hypertrophic hearts) in that, at the start of the
protocol, perfusion pressure was decreased to 60 mmHg to obtain
coronary flows comparable to those of the hypertrophic hearts. Coronary
flows of control hearts 2 min before the start of nitrogen-saturated
perfusion did not differ significantly from those of hypertrophic
hearts (Fig. 2A). At the start of
perfusion there were no ischemic areas (Fig.
4A). When the perfusate was switched from oxygen- to nitrogen-saturated medium, NADH fluorescence homogeneously increased over the entire epicardial surface (Figs. 2B and
4B). Also, coronary flow increased from 14.3 ± 0.8 (at 2 min in Fig.
2A) to 28.3 ± 2.0 ml · min
1 · g
1
(at 4 min in Fig. 2A). During
reperfusion with oxygen-saturated medium, NADH fluorescence rapidly
decreased in a heterogeneous pattern (Fig.
4C) of small areas with fluorescence
intensities ranging from a low (normoxic) to a high (hypoxic)
fluorescence intensity, as described previously (15). Ten seconds after
reperfusion, control hearts no longer displayed ischemic areas (data
not shown), whereas in hypertrophic hearts postreperfusion
ischemia persists much longer (compare Fig. 1,
A and
C; 20 s after reperfusion the hypertrophic hearts have ischemic areas that are still larger than they
were at the start of perfusion). This is also shown in Fig.
2B; after reperfusion, mean NADH
fluorescence intensity decreases in both control and hypertrophic
hearts but remains significantly higher in hypertrophic hearts for at
least 2 min. Figure 2A also shows that
after reperfusion, coronary flow decreases faster in hypertrophic
hearts than in control hearts (for instance, 1 min after reperfusion,
coronary flow in the hypertrophic hearts is 15.2 ± 0.7 ml · min
1 · g
1,
whereas in control hearts it is 24.1 ± 1.0 ml · min
1 · g
1).

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Fig. 4.
NADH fluorescence images of a control heart (protocol
2) at the start of oxygen-saturated perfusion
(A), at the end of
nitrogen-saturated perfusion (B),
and 5 s after reoxygenation with oxygen-saturated medium
(C).
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These results suggest that Langendorff-perfused rat hearts that are
hypertrophic are hypoperfused, causing ischemic areas to appear. To
investigate whether hypoperfusion of control hearts causes similar
ischemic areas, perfusion pressure was decreased in a stepwise manner
from 60 to 10 mmHg, with each step lasting 3.5 min
(protocol 2 continued) after flow
returned to baseline levels after the reperfusion experiment. Flow
concomitantly decreased (Fig.
5E) and
stabilized in <2 min after each drop in perfusion pressure. Ischemic
areas grew progressively larger during perfusion pressures of
30 mmHg
(Fig. 5, B-D). The highly
fluorescent ischemic areas were identical in pattern to those seen
after switching from nitrogen- to oxygen-saturated perfusion and were
evenly distributed over the epicardium (compare Figs.
4C and Fig. 5,
B-D). In these experiments,
however, patterns with relatively large ischemic areas coexisting with
large normoxic areas as seen in hypertrophic hearts did not appear.


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Fig. 5.
NADH fluorescence images of a control heart during oxygen-saturated
perfusion (protocol 2) at a
perfusion pressure of 40 (A), 30 (B), 20 (C), and 10 mmHg
(D).
E: coronary flow in control hearts
(n = 5) during stepwise decreases of
perfusion pressure.
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To identify at which level of arteriolar and/or arterial vasculature
the ischemic areas originate in hypertrophic myocardium during
oxygen-saturated perfusion, control hearts were embolized with
microspheres of different diameters according to
protocol 3; five hearts were embolized
with 5.9-µm microspheres, three with 9.8-µm microspheres, and three
with 15-µm microspheres. The larger the diameter, the larger the
ischemic areas, as shown in Figs. 6 and
7. Figure 7 shows the frequency
distribution of ischemic surface areas of hearts embolized with 5.9-, 9.8-, and 15-µm microspheres and of the hypertrophic hearts of
protocol 1. The mean relative frequency distribution of ischemic surface areas in hypertrophic hearts
did not differ significantly from those in control hearts embolized
with 9.8- and 15-µm microspheres (except for the interval from 600 to
800 pixels, where there was a significant difference between
hypertrophic hearts and control hearts embolized with 9.8-µm
microspheres), whereas it did differ significantly from the frequency
distribution of hearts embolized with 5.9-µm microspheres (Fig. 7).
The proportion of ischemic epicardium and number of ischemic areas of
hearts embolized with the different microspheres and of hypertrophic
hearts are shown in Fig. 8.

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Fig. 6.
NADH fluorescence images of control hearts during embolization of
vasculature with microspheres of different diameters: 5.9 µm
(A), 9.8 µm
(B and
C), and 15 µm
(D).
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Fig. 7.
Frequency distribution histogram of ischemic surface area (1 pixel = 670 µm2) in hearts embolized
with microspheres 5.9 (n = 5), 9.8 (n = 3), and 15 µm
(n = 3) in diameter and in
hypertrophic hearts (n = 5). Columns
represent mean frequency and bars represent SE. * Statistically
significant (P < 0.05) different
from 5.9-µm microspheres.
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Fig. 8.
Proportion of ischemic epicardium (open bars) and number of ischemic
areas (filled bars) of hearts embolized with microspheres 5.9 (n = 5), 9.8 (n = 3), and 15 µm
(n = 3) in diameter and in
hypertrophic (hyp) hearts (n = 5).
Columns represent mean values and bars represent SE.
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DISCUSSION |
Earlier work identified hypoperfused ischemic areas in hypertrophic
Langendorff-perfused hearts (12). The present study was performed to
locate the vascular level at which these hypoperfused areas originate.
The main findings of this study were that the ischemic areas in
hypertrophic Langendorff-perfused rat hearts were significantly larger
than ischemic areas evoked by capillary embolization or by normoxic
recovery from nitrogen-saturated perfusion. The ischemic surface areas
had a frequency distribution closely resembling that of normal hearts
embolized at the arteriolar and/or arterial level, suggesting the
existence of hypoperfusion originating at the arteriolar and/or
arterial level.
In this study we used epicardial NADH fluorescence to measure
epicardial ischemia. The definition of ischemia in
terms of fluorescence intensity requires further elaboration. Anoxia
induced in Langendorff-perfused rat hearts leads to a four- to fivefold increase in NADH fluorescence intensity relative to the normoxic NADH
fluorescence intensity (15). In this study we measured the surface
areas of ischemic epicardial zones with a NADH fluorescence intensity
greater than the intensity halfway between the intensities of the
normoxic surrounding area and those of the ischemic epicardial zones.
The NADH fluorescence intensities of the ischemic zones were at
least threefold greater than the NADH fluorescence intensities of
normoxic epicardium. Because fluorescence measurements were made in
beating hearts, we minimized motion artifacts by selecting images from
the hearts in identical positions in the cardiac cycle (2).
The NADH fluorescence intensity is also dependent on the amount of work
output and the mitochondrial state (2, 6). High work output induces a
decrease of the basal normoxic fluorescence intensity. The left
ventricle was cannulated and communicated with the atmosphere in all
experiments to prevent the development of left ventricular pressure
buildup, resulting in similar mitochondrial states in both hypertrophic
and control hearts. This prevented confounding of the fluorescence
measurements by variations in work output (2). Still, differences in
ADP substrate levels between control hearts and hypertrophic hearts
could cause differences in NADH fluorescence intensities. However, as
can be deduced from Refs. 2 and 6, differences in fluorescence induced
by ADP substrate-level variation are not as large as differences
induced by ischemia.
Another factor influencing NADH fluorescence intensity is substrate
availability. It was shown earlier that the normoxic NADH fluorescence
intensity is dependent on the substrate: pyruvate increases normoxic
fluorescence the most, oleate less, and glucose even less (2, 12). In
this study, however, all experiments were performed with 5.5 mM
glucose. Normoxic fluorescence intensity did not differ between
hypertrophic and control hearts (data not shown), and highly
fluorescent areas in hypertrophic hearts disappeared on improvement of
myocardial oxygenation (Figs. 1D and
3B), thereby excluding the
confounding of NADH fluorescence measurements by differences in
substrate availability between control and hypertrophic hearts.
In this study we decreased perfusion pressure in control hearts to
obtain comparable coronary flow rates between control and hypertrophic
hearts. This did not result in qualitatively different NADH
fluorescence patterns in control hearts (data not shown). We did not
increase perfusion pressure in hypertrophic hearts to this end, because
this would have resulted in nonphysiologically high perfusion pressures
in hypertrophic hearts. In all experiments in this study the left
ventricular cavity communicated with the atmosphere via a cannula
inserted through the apex of the left ventricle to ensure the lowest
possible cardiac work output in all hearts, thereby reducing the
confounding of NADH fluorescence measurements by differences in oxygen
consumption (2).
Normal rat hearts Langendorff perfused with oxygen-saturated medium
continuously release lactate in their effluent, indicating that they
are borderline aerobic (13). However, epicardial NADH fluorescence
measurements under these circumstances do not reveal dysoxic areas
(Fig. 4A) (15). Hypertrophic hearts
are known to have a decreased myocardium-to-vascularization ratio (8, 22). Because of this less optimal vascularization, we expected hypertrophic Langendorff-perfused hearts to develop highly
NADH-fluorescent ischemic areas during normoxic perfusion, as shown
earlier (Fig. 1A) (3, 12). That
study had suggested that the development of ischemia was
related to the production of oxygen free radicals and acidosis in
hypoperfused areas of hypertrophic hearts because of the finding that
these ischemic areas could be relieved by perfusion with superoxide
dismutase, a scavenger of oxygen free radicals, or by perfusion with
fatty acids, resulting in a protection from acidosis-initiated loss of
capillary flow. Steenbergen et al. (26) also observed the development
of relatively large ischemic areas induced by acidosis in normal hearts
and suggested that acidosis-induced coronary (arteriolar and/or
arterial) changes were responsible.
Ischemic areas in hypertrophic hearts were elicited at flow rates that
did not cause local ischemia in control hearts, suggesting the
existence of local hypoperfused areas in hypertrophic
Langendorff-perfused rat hearts. To ascertain that these highly
fluorescent areas were still viable areas of myocardium and were
dysoxic because of impaired oxygenation, oxygen transport was increased
in several ways. Adding fluorocarbons or nitroprusside to the perfusate
resulted in either complete disappearance (nitroprusside, Fig.
1A) or significant reduction of
ischemia (fluorocarbons, Fig. 3). Furthermore, histological analysis in formaldehyde-fixed hypertrophic hearts stained with hematoxylin-eosin revealed no evidence of infarction (data not shown).
Increasing coronary flow by increasing perfusion pressure, however, did
not produce a significant decrease in ischemic areas (data not shown)
in hypertrophic hearts. An explanation for this observation could be
that because of the increase in coronary perfusion pressure, oxygen
consumption increases, thereby more or less keeping the ratio between
oxygen supply and demand unchanged (10). Alternatively, enhancing flow
by increasing perfusion pressure could only affect shunting flow,
thereby leaving the hypoperfused areas still dysoxic.
In a previous study (15) we had shown with NADH fluorescence
measurements in normal hearts that occlusion of vessels of increasing
diameter induced patchy ischemic areas of increasing surface area.
Furthermore, normoxic recovery in control hearts from perfusion with
nitrogen-saturated medium was accompanied by a heterogeneous NADH
fluorescence pattern with small, highly fluorescent patches lagging
behind areas with a much faster decrease of fluorescence. These
ischemic areas were shown to be microcirculatory units originating at
the capillary level, which were the last to be reoxygenated during
reperfusion and could also be elicited by occluding capillaries with
microspheres 5.9 µm in diameter (Fig.
6A) (15). A recent histological
study by Vetterlein et al. (27) in normal rat hearts in vivo found that
tissue located within the capillary bed in proximity to the draining
venule is more prone to the development of hypoxia in critical oxygen
supply conditions. Hypoxia develops during hypoperfusion because of a combination of disturbances of perfusion in feeding areas of arterioles and the loss of oxygen lengthwise along capillaries. Apparently the
microcirculatory units described by Ince et al. (15) are located in
capillary beds close to venules. Ischemic areas in hypertrophic hearts
at the start of perfusion are significantly larger than those elicited
by capillary occlusion in normal hearts (compare Figs.
1A and
6A), suggesting that they originate
at a vascular level proximal to the capillaries. This is also supported by the finding that the embolization of increasingly larger vessels (protocol 3) produces increasingly
larger ischemic areas that resemble those of hypertrophic hearts
(compare Figs. 6, B-D, and 1A). One could argue, taking into
account the study of Vetterlein et al. (27), that in hypertrophy the
disturbances of perfusion of certain individual arterioles predominate
over the loss of oxygen lengthwise along capillaries, thereby inducing
larger ischemic areas. Another argument in favor of this hypothesis is
the close resemblance of the frequency distribution histogram of
ischemic surface areas of hypertrophic hearts to that of control hearts with embolized arterioles and/or arteries (Fig. 7).
Reperfusion with oxygen-saturated medium after nitrogen-saturated
perfusion in hypertrophic hearts revealed a significantly different
fluorescence pattern from that of control hearts. Mean fluorescence
intensity decreased significantly slower with, 1 min after reperfusion,
a decline in mean fluorescence intensity of 52 ± 2% in
hypertrophic hearts compared with 40 ± 2% in control hearts (Fig.
2B). This was accompanied by a
significantly faster decrease of flow and thus less oxygen transport
after reperfusion in hypertrophic hearts (15.2 ± 0.7 ml · min
1 · g
1
1 min after reperfusion) compared with control hearts (24.1 ± 1.0 ml · min
1 · g
1
1 min after reperfusion) (Fig. 2B).
Peak flow during nitrogen-saturated perfusion was significantly higher
in control hearts compared with that in hypertrophic hearts (Fig.
2B). These findings indicate a
decreased coronary flow reserve in hypertrophic hearts, as was found in
earlier studies (11, 19, 20). The accompanying fluorescence images
during the reperfusion phase show the persistence of larger ischemic
areas (Fig. 1C) with high
fluorescence even 20 s after reperfusion, whereas in control hearts
fluorescence images reveal no ischemia even before that time.
The ischemic areas persisting in hypertrophic hearts after reperfusion
are also larger than those in control hearts (compare Figs.
1C and 4C) and resemble those after
occlusion of arterioles and/or arteries with microspheres (Fig. 6).
This finding suggests the existence of hypoperfused areas of myocardium
in hypertrophy, originating at the arteriolar and/or arterial level. To
examine the effect of hypoperfusion on control hearts, perfusion
pressure was progressively decreased (protocol
2). This induced ischemic areas that match the
pattern elicited by occluding capillaries (15) and are much smaller in
size than the dysoxic areas seen in hypertrophic hearts. We were never
able to induce patterns of ischemia in control hearts resembling those seen in the hypertrophic hearts. Apparently
hypertrophy produced by the method used in this study induces changes
in arteriolar and/or arterial vascular control that result in
ischemia of myocardial areas during suboptimal coronary
perfusion. Earlier work (12, 14) has shown that a possible mechanism
accounting for such an effect could be scavenging of nitric oxide
(endothelium-derived relaxing factor) by increased oxygen free radical
production in ischemic myocardial areas in hypertrophic hearts.
In conclusion, in this study we found that the pattern of oxygen
transport to the epimyocardium is profoundly altered in hypertrophy. These changes are the result of dysregulation of flow at the arteriolar and/or arterial level. The areas with the slowest reoxygenation after
ischemia in hypertrophy are larger than the microcirculatory units described by Ince et al. (15) and have a surface area distribution matching that of the ischemic areas evoked by arteriolar and/or arterial embolization.
 |
FOOTNOTES |
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: J. F. Ashruf, Dept. of Surgery, Erasmus Univ. of Rotterdam, Dr.
Mole-waterplein 40, 3015 GD Rotterdam, The Netherlands (E-mail:
ashrufpatandin{at}wanadoo.nl).
Received 2 November 1998; accepted in final form 31 May 1999.
 |
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