(Circulation. 1998;98:1912-1920.)
© 1998 American Heart Association, Inc.
Basic Science Reports |
From the Cardiovascular Division, University of Virginia School of Medicine, Charlottesville, Va.
Correspondence to Sanjiv Kaul, MD, Cardiovascular Division, Box 158, University of Virginia Medical Center, Charlottesville, VA 22908. E-mail sk{at}virginia.edu
| Abstract |
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Methods and ResultsWe studied 12 dogs before and after creation of left anterior descending coronary artery stenoses both at rest and during hyperemia (n=62 stages). Microbubbles were administered as a constant infusion, and myocardial contrast echocardiography (MCE) was performed with the use of different pulsing intervals. The video intensity versus pulsing interval plots derived from each myocardial pixel were fitted to an exponential function: y=A(1-eßt), where A reflects microvascular cross-sectional area (or myocardial blood volume), and ß reflects mean myocardial microbubble velocity. The product A · ß represents myocardial blood flow (MBF). Average values for these parameters were derived from the endocardial and epicardial regions of interest placed over the left anterior descending coronary artery bed. Radiolabeled microspherederived MBF was also measured from the same regions. There was poor correlation between radiolabeled microspherederived MBF and A-endocardial/epicardial ratios (EER) (r=0.46). The correlation with ß-EER was better (r=0.69, P<0.01). The best correlation with radiolabeled microspherederived MBF-EER was noted with A · ß-EER (r=0.88, P<0.01).
ConclusionsThe transmural distribution of myocardial perfusion can be accurately assessed with MCE with the use of our newly described method of tissue replenishment of microbubbles after their ultrasound-induced destruction. In the model studied, an uncoupling of the transmural distribution of MBF and myocardial blood volume was observed during reversal of the MBF-EER.
Key Words: echocardiography perfusion myocardium blood flow
| Introduction |
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Commonly used techniques for myocardial perfusion imaging such as single-photon and positron emission tomography do not have the spatial resolution to discriminate between endocardial and epicardial MBF.7 Myocardial contrast echocardiography (MCE), which uses intravascular injection of microbubbles for the assessment of myocardial perfusion,8 has good spatial resolution, particularly in the axial direction.9 We have previously demonstrated that myocardial peak video intensity (VI) with the use of this technique reflects myocardial blood volume (MBV),10 90% of which is present in myocardial capillaries.11 12 Damage to endocardial capillaries with subendocardial infarction results in a reduction of endocardial MBV and therefore of MBF. We have shown that in such a situation, the myocardial peak VIendocardial/epicardial ratio (VI-EER) correlates well with radiolabeled microsphere (RM)-derived MBF-EER.13
In the absence of microvascular damage, however, we were unable to find any relation between MCE-derived parameters during intracoronary and aortic root injections of microbubbles and RM-derived MBF-EER in several models of coronary stenosis.14 Because no correlation was found between the peak VI-EER and RM-derived MBF-EER in that study, we postulated that in the setting of coronary stenosis, the spatial distribution of MBV and MBF may not be coupled.14 In those experiments, we also found no correlation between mean microbubble transit rate, which reflects the MBF/coronary blood volume (volume of blood in the entire coronary circulation, including epicardial vessels) ratio and RM-derived MBF-EER. We postulated that this finding was probably related to the stenosis-induced changes in both MBF and coronary blood volume.14
We have recently developed a new method for the quantification of myocardial perfusion with MCE.15 Microbubbles are destroyed as they enter a myocardial region during steady state achieved with continuous venous infusion. The rate at which they replenish the region after their destruction is then measured, which provides an estimate of mean microbubble velocity. The VI measured after complete replenishment of the region provides an estimate of MBV. Thus unlike the situation with bolus injections, continuous infusions of microbubbles can be used to derive estimates of both MBV and MBF. Using our new method, we were able to determine transmural MBF accurately.15 We therefore hypothesized that this method could be used to measure perfusion in the different layers of the myocardium in the presence of coronary stenoses, even when there is no microvascular damage.
| Methods |
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A left lateral thoracotomy was performed and the heart was suspended in a pericardial cradle. A 7F catheter was placed in the left atrium for injection of RM. A similar catheter was placed in the ascending aorta through the right carotid artery for measurement of aortic pressure. The proximal portion of the left anterior descending coronary artery (LAD) was dissected free from the surrounding tissue, and an ultrasonic time-of-flight flow probe (series SB, Transonics) was placed around it and connected to a digital flowmeter (model T206, Transonics). A custom-designed screw occluder was placed distal to the flow probe, and a 20 gauge Teflon catheter (Critikon) was introduced into the LAD distal to the occluder through a side branch of the artery.
Hemodynamics
All fluid-filled catheters were connected to fluid-filled
pressure transducers, which, like the flowmeter and the
micromanometer-tipped catheter, were connected to a
multichannel recorder (model ES 2000, Gould Electronics). LAD flow
and all pressure data were acquired digitally at 200 Hz into an
80386-based personal computer by an 8-channel analog-to-digital
converter (Metrabyte). The signals were displayed on-line with the use
of a Labtech Notebook (Laboratory Technologies). The severity of each
stenosis was judged by the gradient between the mean aortic and
distal LAD pressures. LAD driving pressure was calculated by
subtracting the mean right atrial pressure from the mean distal LAD
pressure.16 Microvascular resistance in the
LAD bed was calculated by dividing the LAD flow by the LAD driving
pressure and converting the value into dyne · s ·
cm-5.
Radiolabeled Microsphere MBF Measurement
MBF was measured with left atrial injections of
2 ·
106 11-µm RM (DuPont Medical Products)
suspended in 4 mL of 0.9% saline and 0.01%
Tween-80.17 Duplicate reference blood samples (10
mL each) were withdrawn from the femoral arteries over 130 seconds with
a constant rate withdrawal pump (model 944, Harvard
Apparatus). At the end of the experiment, the left
ventricular short-axis slice corresponding to the MCE image
was cut into 16 wedge-shaped pieces, excluding the papillary muscles,
and each piece was further divided into epicardial, midcardial, and
endocardial segments. The tissue and reference blood samples were
counted in a well counter with a multichannel analyzer (model
1282, LKB Wallac). Corrections were made for activity spilling from 1
energy window to another with the use of a custom-designed program. MBF
to each epicardial, midcardial, and endocardial segment was calculated
from the equation
Qm=(Cm ·
Qr)/Cr, where
Qm is blood flow to the myocardial segment
(mL · min-1), Cm is
tissue counts, Qr is rate of arterial
sample withdrawal (mL · min-1), and
Cr is arterial reference sample
counts.17
Absolute epicardial, midcardial, and endocardial MBF (mL · min-1 · g-1) to each of the 48 pieces was calculated as the quotient of the flows and the weight of the segment. Mean transmural as well as endocardial and epicardial MBF were calculated by averaging MBF to the segments within the LAD bed at the level of the MCE imaging plane. These segments were identified by positive staining with monastral blue, which was injected into the LAD before termination of the experiment (see "Protocol"). Segments at the border that only partially stained blue were excluded from analysis. Of the 16 segments in an imaging plane, data from 3 to 7 were averaged to derive LAD MBF.
MBF in each segment within the LAD bed was also represented with a parametric image with color coding to display the magnitude of MBF. This custom-designed program uses colors ranging from black (low flow) to bright orange (high flow). All values are normalized to the highest MBF within the LAD bed. MBF between adjacent segments are averaged and interpolated to allow a smoother transition of color.
Myocardial Contrast Echocardiography
A prototype Sonos 2500 system (Hewlett Packard) was used for
MCE.15 18 Imaging was performed in the harmonic
mode, in which ultrasound is transmitted at 2 MHz and received at 4
MHz. A saline bath served as an acoustic interface between the heart
and the ultrasound transducer, which was fixed in position with a clamp
attached to the procedure table. Imaging was performed at the mid
papillary muscle, short-axis level. To improve the spatial resolution
of MCE, the depth setting was adjusted so that only the anterior
myocardium was visualized. The maximal dynamic range (60
dB) was used. The transmit power, focus, overall gain, and image depth
were held constant between experiments. Up to 8 end-systolic
images were acquired at each pulsing interval and stored on 1.25-cm
videotape with the use of an S-VHS recorder (Panasonic AG-MD830,
Matsushita Electrical).
Imaging was performed with the use of 2 triggers. Although both triggers resulted in microbubble destruction and myocardial opacification, the first was used only for the purpose of microbubble destruction. We have previously shown that at concentrations used in this experiment, almost all bubbles are destroyed by a single ultrasound pulse.15 The second trigger was used only for the assessment of myocardial opacification in end-systole.15 18 The interval between the 2 triggers was progressively increased from an initial value of 250 to 350 ms (depending on heart rate) to every 1, 2, 3, 5, 8, 10, and 20 cardiac cycles to allow incremental microbubble replenishment of the ultrasound beam elevation.15
Imagent US (AFO150, Alliance Pharmaceutical Corp) was used as the contrast agent.18 It consists of surfactant-coated microbubbles containing perfluorohexane and nitrogen. These microbubbles have a mean diameter of 5 µm and a mean concentration of 5 · 108 mL-1. The partial pressures within the bubbles are designed to remain constant at all times, so there is no spontaneous change in their size after they mix with blood. A solution consisting of 4 mL of this agent was mixed with 46 mL of 0.9% saline and administered as a continuous infusion at approximately 2 mL · min-1 with a volumetric pump (IVAC). This infusion rate was periodically adjusted to obtain optimal myocardial opacification.
MCE images were analyzed as previously described.15 19 20 They were transferred from videotape to the memory of a computer at 30 Hz in a 320x240x8 bit matrix. Five precontrast images and a similar number of contrast-enhanced images from each of the 9 pulsing intervals were selected for analysis. The precontrast and contrast-enhanced images from each pulsing interval were aligned by means of computer cross-correlation. Each set of images (both precontrast and contrast-enhanced for each pulsing interval) was separately averaged. The averaged precontrast image was digitally subtracted from the averaged contrast-enhanced image. VI was measured in each pixel within the digitally subtracted images at each pulsing interval, and the resulting pulsing interval versus VI plot was fitted to an exponential function: y=A(1-eßt), where y is VI at pulsing interval t, A represents microvascular cross-sectional area (or MBV), and ß represents the mean myocardial microbubble velocity.15
The values of A, ß, and A · ß derived from the fitted function obtained from each pixel were represented in color as separate parametric images. For the parametric image depicting A, each pixel was assigned a hue of red, with dark to bright red indicating increasing values of A. Similarly, for the parametric image illustrating ß, each pixel was assigned a color scheme representing a ripening mango, in which increases in ß were represented as changes in color from green to yellow to orange. Finally, a similar procedure was adopted for the parametric image showing A · ß, in which each pixel was relegated a color representing the rainbow (increasing A · ß represented as change in color from black to red to green to white to blue). Mosaic colors were used in which the correlation coefficient for fitting the function in any pixel was <0.90, which was mostly caused by noise. These parametric images allowed a simple and easy way to visualize complex data obtained from many frames and cardiac cycles in an intuitive 2-dimensional image. Regions of interest were then placed over endocardial and epicardial areas of the LAD bed to derive average values of A, ß, and A · ß in these regions. Any pixel showing mosaic colors was not included in the region of interest. For optimal data registration, the LAD bed was defined by monastral blue staining of the heart.
Experimental Protocol
A total of 5 to 6 stages were attempted in each dog, including
baseline and hyperemia both before and after placement of
different stenoses, which were nonflow limiting at rest. The
severity of each stenosis was judged by the pressure drop
across it. Hyperemia was induced by venous infusion of 0.04
µg · kg-1 ·
min-1 of WRC-0470 (Discovery Therapeutics), a
selective adenosine A2a receptor agonist,
which causes minimal hypotension in anesthetized
dogs.21 Hemodynamic data were
averaged from values acquired just before and after MCE at each stage.
The respirator was shut off for brief periods (10 to 20 seconds) during
MCE, which did not result in any hemodynamic changes.
At each stage, MCE was followed by injection of RM. At the end of the
experiment, the LAD was occluded and monastral blue dye (Sigma
Chemical) was injected into it through the distal catheter to define
the LAD bed. The dog was then euthanized with an overdose of
pentobarbital and KCl, and the heart was removed from the chest cavity.
It was cut into 5 short-axis slices of equal thickness, and the slice
corresponding to the MCE imaging plane was processed for the RM-derived
MBF analysis.
Statistical Methods
Data are expressed as mean±1 SD. Comparisons between
nonhyperemia and hyperemia stages were performed with
either the paired or the unpaired Student t test.
Correlations were performed with least-squares-fit linear regression
analysis. For differences, a value of P<0.05
(2-sided) was considered significant.
| Results |
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Table 1
depicts the mean hemodynamic and MBF data in
the presence of hyperemia before (n=11) and after placement of
a stenosis (n=24). The mean aortic pressure remained unchanged
after the placement of a stenosis, whereas the mean heart rate,
coronary driving pressure, and transmural MBF decreased
significantly. Importantly, the mean myocardial microvascular
resistance increased after stenosis placement. The MBF-EER,
ß-EER, and A · ß-EER decreased
significantly (P<0.01) after stenosis placement,
whereas the A-EER remained unchanged (Table 2
).
Figure 1
illustrates the
parametric RM-derived MBF and the corresponding MCE images
(representing the values A, ß, and
A · ß) during hyperemia from 1 of the dogs
in the absence of any stenosis. Note the uniform spatial
distribution of colors in the anterior myocardium denoting
a relatively homogeneous perfusion across the entire
myocardial thickness.
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Figure 2
illustrates parametric
images of RM-derived MBF and the corresponding MCE data during
hyperemia in 1 of the dogs after stenosis placement. A
decrease in RM-derived MBF-EER is noted, with a proportionate decrease
in ß-EER and A · ß-EER. The
A-EER does not appear to be reduced to the same extent.
Figure 3
depicts RM-derived MBF and the
corresponding MCE data in a dog with a moderate stenosis that
has not been subjected to hyperemia. There is equal reduction
in A-EER, ß-EER, and A ·
ß-EER. During the same stenosis, the magnitude and
spatial extent of reduced RM-derived MBF, ß, and
A · ß is greater during hyperemia, without
any alteration in the magnitude and extent of abnormal A
(Figure 4
).
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Figure 5
(B and C) illustrates pulsing
interval versus VI curves obtained by placing regions of interest over
the endocardial and epicardial portions of the parametric
images shown in Figures 3
and 4
. These curves represent the
average of the values obtained from pixels within the epicardial and
endocardial regions of interest. It is apparent that the quantitative
information reflects what is qualitatively observed in the
parametric images. Figure 5A
depicts MCE data from the same dog
during baseline when the RM-derived MBF-EER was normal.
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In most instances, although reduction in RM-derived MBF-EER was
associated with a decrease in both ß-EER and A
· ß-EER, the A-EER remained unchanged (Table 2
). Of
the few instances (14 of the 62 stages) in which A-EER was
reduced (
0.75), it was associated with a significantly lower mean
absolute endocardial ß than when it was not reduced
(0.41±0.16 versus 0.63±0.32, P=0.02). The absolute
endocardial MBF in these instances also tended to be lower (0.85±0.83
versus 1.12±0.96 mL · min-1 ·
g-1, P=0.12).
Thus, whereas ß-EER and A · ß-EER
always mimicked RM-derived MBF-EER, A-EER did not. This
phenomenon is graphically depicted in Figure 6
, in which A-EER,
ß-EER, and A · ß-EER from all 62
stages are plotted against the RM-derived MBF-EER. There is poor
correlation between the A-EER and the RM-derived MBF-EER
(Figure 6A
). Although the relation between the ß-EER and
the RM-derived EER is better (P<0.01, Figure 6B
), that
between the A · ß-EER and the RM-derived EER is the
best (P<0.01, Figure 6C
).
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| Discussion |
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There has been controversy regarding the ability of MCE to determine the MBF-EER,12 22 23 24 25 some of which may be due to differences in methodologies. For instance, some investigators used microbubbles made by sonicating radio-opaque dyes,23 which tend to produce larger bubbles that transiently block the microcirculation, whereas others20 used flow tracers that behave like red blood cells within the microcirculation.26 27 28 Some studies were performed in patients in whom the presence of selective reduction in endocardial MBF could not be independently confirmed.23 24 In other studies with animals, the limited lateral resolution of ultrasound was a confounding problem in the lateral wall supplied by a stenotic left circumflex coronary artery.22 25 In these experiments, although decreases in peak VI were noted in the presence of reduction in endocardial MBF during coronary hyperemia, no correlation between VI and endocardial MBF was demonstrated.25
In an extensive study with 21 dogs and 3 different models of ischemia, we were unable to demonstrate any correlation between peak VI-EER and MBF-EER as well as between mean microbubble transit rate-EER and RM-derived MBF-EER.14 In these experiments, we injected the microbubbles either directly into the coronary artery or the aorta with a constant input function during both rest and hyperemia.
Because peak VI reflects MBV,10 we postulated that the lack of correlation between peak VI-EER and RM-derived MBF-EER noted in our study indicated an uncoupling of the transmural distribution of MBF and MBV distal to a stenosis.14 The results of our present study support this notion. In only a few cases, endocardial VI decreased when MBF-EER reversed. In these cases, the absolute endocardial microbubble velocity (ß) and endocardial MBF were significantly lower. These data imply that when endocardial MBF is very low, complete replenishment of the ultrasound beam by microbubbles may not have occurred within the endocardium even at 12 seconds (the longest pulsing interval used in the study), resulting in an apparent decrease in the A-EER. When MBF is normal, beam replenishment is complete in 5 seconds.
In our previous study, we also found no relation between mean microbubble transit rate-EER and RM-derived EER.14 Because the mean microbubble transit rate reflects MBF/coronary blood volume (which, in distinction to MBV, is the volume of blood in the entire coronary tree), our results implied that changes in coronary blood volume occurring distal to a stenosis were not coupled with the transmural distribution of MBF. In the present study, we found a good correlation between ß-EER and MBF-EER. It is important not to confuse mean microbubble velocity (ß) with mean microbubble transit rate. The former is measured only over the myocardium and is not influenced by the entire coronary blood volume, whereas the latter is significantly influenced by it.
The results of the present study confirm our previous observations15 18 that in the presence of hyperemia, myocardial microvascular resistance increases after placement of a coronary stenosis. We have also shown that this increase in myocardial microvascular resistance is associated with a decrease in MBV (or capillary density).18 A constant capillary hydrostatic pressure is essential for homeostasis.29 In the presence of coronary stenosis, the coronary driving pressure decreases and capillary hydrostatic pressure is maintained by an appropriate degree of vasodilation of the arterioles. When hyperemia is induced, however, vasomotor tone is lost, which in the absence of other adaptive mechanisms could result in an increase in capillary hydrostatic pressure. We have postulated that under these circumstances, the capillaries "derecruit" in order to maintain a constant hydrostatic pressure.18 The mechanism of this "derecruitment" is unknown at present.
At first glance, it may appear surprising that the transmural distribution of RM-derived MBF and MBV do not correlate with each other, particularly during hyperemia. We, however, interpret our results as indicating that because capillaries constitute 90% of MBV,11 the uniform transmural decrease in MBV in the presence of a coronary stenosis during hyperemia indicates a uniform transmural "derecruitment" of capillaries, all of which experience the same coronary driving pressure. The transmural differences in MBF distal to a stenosis occur from changes in dimensions of arterioles supplying these regions. Because the blood within these arterioles constitutes only 5% to 7% of MBV11 and because many of these arterioles are not present inside the myocardium, changes in their dimensions are not likely to be reflected in the measured VI across the myocardial wall.14
The best assessment of the transmural distribution of MBF with MCE occurred when we used the product of mean microbubble velocity (ß) and capillary cross-sectional area (A), which represents MBF.15 The method of microbubble destruction and ultrasound beam replenishment has the advantage of simultaneously depicting the spatial distribution of both MBF and MBV. As seen in this study, the assessment of both MBF and MBV provides greater insight into myocardial perfusion than measuring either alone. These independent assessments provide insights into the vascular sites of MBF control.
The spatial resolution of MCE is <1 mm in the axial direction. In
comparison, the spatial resolution of the RM technique is limited by
the number of segments into which each myocardial slice is divided.
Because an adequate number of microspheres need to be
present in each tissue sample for the count statistics to be
robust, each slice is generally divided into 16 segments, as was done
in our study. Thus, as seen in Figures 1 to 4![]()
![]()
![]()
, the fine gradations and
heterogeneities in MBF are much more likely to be discerned with MCE
than with the RM technique.
In this article, we have also described a new method of depicting mean microbubble velocity (ß) and microvascular cross-sectional area (A) on a pixel-by-pixel basis. On one hand, this method could introduce noise because of the stochastic nature of ultrasound or because of even minor misalignment of images acquired at different pulsing intervals. On the other hand, if the data are of superior quality (well-aligned and averaged), the curve fitting could potentially reduce noise and provide greater insights into heterogeneities of regional MBV and MBF seen under physiological and pathological conditions. Although the large number of mathematical calculations required makes the method time-consuming at present, it can be made more efficient.
We performed the experiments under the most optimal conditions. We used open chest dogs with a saline bath serving as a nonattenuating acoustic interface between the heart and ultrasound transducer. We abolished respiration-induced motion artifacts by temporarily shutting off the respirator for a few seconds during image acquisition. We imaged at a low depth setting so that the sector contained only the anterior myocardium, and we could place large regions of interest over the epicardial and endocardial areas, which result in more accurate measurements of VI.30 We used the superior axial resolution of ultrasound by imaging the myocardium most perpendicular to the beam.
It is unlikely that we can obtain similar results from patients at the current time unless the image quality is excellent, such as during transesophageal echocardiography. It is possible that advances in transducer design and signal processing may allow the assessment of transmural distribution of MBF and MBV by MCE in the future even with transthoracic echocardiography. This study provides the proof of principle and discusses the physiological basis for using MCE for the noninvasive assessment of the transmural distribution of myocardial perfusion. It also highlights the independent importance of determining both MBF and MBV in the overall assessment of myocardial perfusion.
| Acknowledgments |
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| Footnotes |
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Received March 6, 1998; revision received June 4, 1998; accepted June 5, 1998.
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