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J Appl Physiol 89: 1633-1635, 2000;
8750-7587/00 $5.00
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Vol. 89, Issue 4, 1633-1635, October 2000

INVITED EDITORIAL
Brief commentary on coronary wave-intensity analysis

Julien I. E. Hoffman1 and William M. Chilian2

1 Department of Pediatrics, Cardiovascular Research Institute, University of California, San Francisco, California 94143; and 2 Department of Physiology, Cardiovascular Research Center, Medical College of Wisconsin, Milwaukee, Wisconsin 53226


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CORONARY PRESSURE-FLOW RELATIONS have long interested physiologists but are so complex that even today they have still not been completely unraveled. Early investigators like Rebatel in 1872 (Ref. 33; cited by van der Meer), Anrep and von Saalfeld in 1933 (1), Gregg and Green in 1940 (17), and Wiggers in 1954 (39) observed that, when aortic pressures were high in systole, coronary flow was low; conversely, when aortic pressures were low in diastole, coronary flows increased. They attributed this inverse relationship to the impediment to myocardial flow occurring during systole, although there were differences in their detailed views on the mechanisms. All of these studies were done with relatively crude instruments, and the more modern studies of coronary pressure-flow relations can be regarded as beginning in 1965 with the use of electromagnetic flowmeters [by Gregg and colleagues (18)]. Not only were high-frequency recordings of coronary flow and pressure obtained, often in conscious chronically instrumented dogs, but also the careful attention to detail together with simple manipulations of cardiac function allowed these investigators to make inferences from minor changes in the complex flow signals from the left and right coronary arteries.

At this point, the belief was that, because of assumed differences in intramyocardial pressure across the wall of the left ventricle, the systolic coronary flow perfused the outer or subepicardial muscle, but the deeper or subendocardial muscle could be perfused only in diastole. These inferences were based on mathematical models of the myocardium by bioengineers (27, 28) and on the results of direct measurements of intramyocardial pressures (4, 5, 16, 24, 44). Unfortunately, these different studies often disagreed, sometimes markedly, about the exact pressures in different regions of the ventricle. Some of the disagreement stemmed from unrealistic assumptions and lack of computational power for the models and from artifacts caused by introducing finite-sized probes into the dense myocardium (32). With time, many of these difficulties were overcome, and, eventually, models and experiments began to agree closely (6, 7, 25, 26, 32, 38). There was general agreement that, in systole, intramyocardial pressures were close to cavity pressures beneath the endocardium of the left ventricle and decreased almost linearly to near atmospheric beneath the epicardium. To this extent, the inferences of Gregg et al. (18) seemed to have been correct.

A change in thought was required when investigators began to take the capacitance of the extramural coronary arteries into account. Douglas and Greenfield (13) concluded that all of the systolic flow into the origins of the canine left coronary artery could be stored in the extramural arteries so that there might be no systolic perfusion of the subepicardial muscle. This argument was reinforced when Chilian and Marcus (9) showed that, in the absence of any capacitance in the extramural coronary arteries (septal artery, distal branch just before myocardial penetration), there was reverse systolic coronary flow. In addition, retrograde flow in the extramural coronary arteries was also demonstrated by Kajiya et al. (20).

None of the above-mentioned studies measured regional flows, which could be studied by diffusible indicators (11, 19, 26, 30) or radioactive microspheres (12). These methods soon brought out the importance of subendocardial underperfusion in various models of heart disease (4, 19, 29). It took many years, however, before the likely mechanism for this selective regional underperfusion was elucidated (14, 15).

While these studies were in progress, newer microscopic techniques were used to evaluate regional vascular reactivity (2, 3, 5-8, 10, 16, 21, 31, 40, 41). These studies confirmed the narrowing of the subendocardial arterioles during systole and also showed variations in vascular reactivity in arterioles of different sizes and different locations. Others explored the role of the intramyocardial blood volume in regulating regional flows in systole and diastole (34-37); eventually, the elastance concept was applied to the coronary vascular bed (22-25).

Many of these studies were done with at least two artificial constraints. The coronary arteries were usually cannulated so that their pressure could be controlled independent of left ventricular pressure and work. In addition, because most of the techniques used required a steady state, many of the studies were done with maximally vasodilated coronary vessels. Although these studies revealed many things about the coronary circulation, it was difficult to predict what results would have been obtained without these constraints. Some investigators used beat-by-beat analysis (38), but this required cannulation and some interpretation of the data.

The new approach introduced by wave-intensity analysis helps to overcome some of the existing problems. It does not require coronary arterial cannulation and obtains results beat by beat, thus not requiring a long steady state. So far, however, it has not produced new insights into the coronary circulation because it has only begun to be applied, but it promises to be a powerful new tool. One caveat is needed: methods such as this yield global information and so far are not capable of exploring regional differences. This caveat is also a criticism of the elastance concept of coronary flow, treating as it does the intramyocardial circulation as a single entity with all its components responding in the same way. One of the future challenges will be to adapt this method to investigate regional relationships.


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3.   Ashikawa, K, Kanatsuka H, Suzuki T, and Takishima T. Phasic blood flow velocity pattern in epimyocardial microvessels in the beating canine left ventricle. Circ Res 59: 704-711, 1986[Abstract/Free Full Text].

4.   Buckberg, GD, Fixler DE, Archie JP, and Hoffman JIE Experimental subendocardial ischemia in dogs with normal coronary arteries. Circ Res 30: 67-81, 1972[Abstract/Free Full Text].

5.   Chilian, WM. Microvascular pressures and resistances in the left ventricular subepicardium and subendocardium. Circ Res 69: 561-570, 1991[Abstract/Free Full Text].

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8.   Chilian, WM, Eastham CL, and Marcus ML. Microvascular distribution of coronary vascular resistance in beating left ventricle. Am J Physiol Heart Circ Physiol 251: H779-H788, 1986[Abstract/Free Full Text].

9.   Chilian, WM, and Marcus ML. Effects of coronary and extravascular pressure on intramyocardial and epicardial blood velocity. Am J Physiol Heart Circ Physiol 248: H170-H178, 1985[Abstract/Free Full Text].

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J APPL PHYSIOL 89(4):1633-1635
8750-7587/00 $5.00 Copyright © 2000 the American Physiological Society



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