Abstract
An essential prerequisite for the calculation of FFR from aortic and coronary pressure is to obtain the measurements under conditions of maximum hyperemia. Only in this situation it can be assumed that the resistance of the vascular bed is minimal and therefore equal to the resistance in the same vascular bed but not depending on an epicardial stenosis. This condition has been demonstrated in animals (chapter 7) and in humans (chapter 8). Only when the resistance of the vascular bed depending on an epicardial stenosis equals the resistance of the same vascular bed but without stenosis, these resistances can be cancelled in the calculation of FFR2. It has been shown in animals and in humans, in the physiological range of aortic pressure, that the relation between myocardial flow and driving pressure is linear during maximum microvascular vasodilation3–4 This implies that, during maximum hyperemia, the ratio of two myocardial flows (which corresponds to the definition of FFR) equals the ratio of their respective driving pressures. The key point with respect to FFR is not the slope but the linearity of the pressure-flow relation under conditions of maximum vasodilation. When maximum hyperemia is not achieved the relation between hyperemic flow and driving pressure is curvilinear, and thus, the ratio of these (‘non-hyperemic’) flows does not equal the ratio of their respective driving pressures.
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Pijls, N.H.J., De Bruyne, B. (2000). FFR in Some Specific Conditions. In: Coronary Pressure. Developments in Cardiovascular Medicine, vol 195. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-9564-3_13
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DOI: https://doi.org/10.1007/978-94-015-9564-3_13
Publisher Name: Springer, Dordrecht
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