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1 Department of Cardiology, Wales Heart Research Institute, University of Wales College of Medicine, Heath Park, Cardiff CF14 4XN; and 2 Physiological Flow Studies Group, Department of Bioengineering, Imperial College for Science, Technology and Medicine, London SW7 2AZ, United Kingdom
A continuing focus on subcellular processes could
result in neglect of the framework through which these small processes
are integrated. This focus could be particularly problematic in the cardiovascular system in which a patient's clinical condition depends
on the function of the whole system, specifically the pumping of blood
and its distribution. These are currently less fashionable
areas of research. However, the ability to characterize the intact
system, for example during and after pharmacological or genetic
perturbation, must be retained to realize the potential of molecular
biology. Paradoxically, and unusually in medicine, the integrating
processes within the circulation may be best understood by adopting a
reductionist approach. Such an approach involves breaking down blood
flow into its constituent elements. In this short editorial, we outline
recent work on wavefronts, mathematically derived elemental forces in
arterial flow that appear to provide a new perspective on the
integrated system for clinicians and basic scientists alike. Although
clinical applications remain to be elucidated, we speculate on likely
areas of interest.
The problem for intact system research is that elements are
interdependent and are not easily held constant. There are many examples, e.g., cardiac output depends on the heart and the arteries but they are linked through afterload, coronary flow depends on aortic
pressure and ventricular contraction and they interact, etc. In a
system of tubes, the challenge frequently is how to resolve the
directional basis of a perturbation, does it originate upstream or
downstream, or both? How can interaction between constituent parts be
considered as an interchange of energy? In the circulation, how do
arteries serve as cables or transmission lines? It has long been
recognized that the answers may be found in the mechanics of arterial
wave travel (41), an area that has been mathematically redefined during the last few years (26). A wave-intensity
analysis of forward and backward wave travel has the potential to
quantify the amplitude and direction of energy transfer in the systemic (11, 12), pulmonary (9), or coronary arterial
systems (32). This theoretical approach also has practical
implications, because there is increasing evidence that
upstream-downstream cardiovascular interactions have real prognostic
(1) and therapeutic significance (24) for
cardiology patients in the clinic. The disadvantageous development of
left ventricular hypertrophy in hypertension and the advantageous use
of vasodilators in heart failure serve as testimony to the importance
of ventriculoarterial interaction.
In the circulation, wave travel results from the exchange of
energy between the kinetic energy of the flowing blood and the potential energy of the elastic vascular wall (4). For the case of the aorta, a pressure increase associated with left ventricular ejection leads to and is buffered by aortic expansion. Elastic recoil
accounts for a limited pressure increase, however, and thus blood flows
by expansion and contraction along the vessel wall. In situations
associated with arterial stiffening, such as atherosclerotic disease,
hypertension, or aging, the systolic pressure change increases as
vessel expansion decreases. The pulse wave travels as this interchange
of energy spreads through the system. The speed of wave travel
increases as the wall becomes stiffer, or less distensible, so that the
state of a vessel can be described functionally by the pulse-wave
velocity (PWV) along it. As for other variables associated with the
elasticity of the arterial wall, PWV is pressure dependent, varying
nonlinearly with pressure as distension shifts the load between
different wall components (7). Medial smooth
muscle is viscoelastic and contributes variably depending on its state
of activation and the pressure range. Vasorelaxation tends to reduce
PWV (27) and vice versa.
Since the pioneering work of Taylor and MacDonald in the 1950s using
Fourier transform methods, it has been a valuable approach to think of
arterial waves as combinations of sinusoidal wave trains of different
amplitudes and frequencies (3, 20). This may seem natural,
because everything that we see and hear reaches us as sinusoidal wave
trains. The problems with this form of analysis are that it assumes
linearity and periodicity, and it has been difficult for clinicians to
understand instinctively. There are other forms of waves that could be
used to describe the observed arterial waves. One choice, particularly
useful in gas dynamics, is to consider the propagation of discrete
wavefronts, elemental waves that cause a step change in pressure and
velocity as they pass. One distinct and practical advantage of these
wavefronts is that they can be located in time and space unlike
sinusoidal waveforms that have only a phase and a frequency.
Furthermore, if we consider infinitesimal, or transient, wavefronts
that either increase the pressure (compression waves) or decrease it
(expansion waves), it is possible to build up any observed waveform
from a time-dependent succession of wavefronts. These infinitesimal wavefronts are convected with the blood velocity and travel forward and
backward in the artery with a wave speed usually referred to as the PWV.
A measured pressure or flow waveform generally results from coincident
successions of forward and backward wavefronts. In the aorta, forward
wavefronts arise in the heart, and backward wavefronts arise from
reflection in the systemic periphery. In a pulmonary vein, backward
wavefronts originate in the left atrium (31). In a
coronary artery, forward wavefronts originate in the left ventricular
cavity and backward wavefronts originate in the small vessels within
the relaxing or contracting myocardium (32). The
physiologically important point is that the wave travel in any given
direction carries information about its initiating event.
Pressure and flow change together in forward wavefronts but in opposite
ways in backward, reflected wavefronts (Fig.
1). Thus reflected compression wavefronts
arriving in the aorta increase pressure but decelerate flow.
Conversely, in a coronary artery, a backward expansion wave caused by
myocardial relaxation decreases pressure but accelerates the flow along
the vessel (Fig. 2). The nature of a wave
reflection will depend on the nature of the reflecting site; a positive
pressure change will reflect as a positive pressure change from a
closed end but becomes a negative pressure change when reflected from
an opening or expansion. This gives rise to four possibilities: forward
and backward compression and expansion wavefronts (Fig. 1). Most
reflecting sites in the normal systemic arterial system are closed end
in type, but this appears not to be the case for the pulmonary
circulation (9), in which the daughter vessels have
greater area than the main vessel and is probably not the case for an
aneurysmal aorta. The different relations between pressure and flow in
forward and backward wavefronts allow their mathematical separation so
that upstream and downstream information can be distinguished from a
single set of measurements at an accessible site remote from where the
waves were initiated (12).
![]()
THE PROBLEM WITH FASHION
TOP
THE PROBLEM WITH FASHION
HOW DO WAVES TRAVEL?
HOW ARE WAVES ASSESSED?
WHY ARE WAVES IMPORTANT?
CONCLUSIONS
REFERENCES
![]()
HOW DO WAVES TRAVEL?
TOP
THE PROBLEM WITH FASHION
HOW DO WAVES TRAVEL?
HOW ARE WAVES ASSESSED?
WHY ARE WAVES IMPORTANT?
CONCLUSIONS
REFERENCES

View larger version (16K):
[in a new window]
Fig. 1.
A sketch representation of the impact on the pressure
waveform and the flow (velocity) waveform, measured at any specific
site in the vascular system, by the passage of each of the four types
of wavefronts (forward traveling compression or expansion waves or
backward traveling compression or expansion waves).

View larger version (57K):
[in a new window]
Fig. 2.
A diagrammatic representation of an epicardial coronary
artery and a section of myocardium. Solid arrows represent myocardial
fiber lengthening in early diastole. Interrupted arrow represents the
resultant backward traveling expansion wave, which decreases pressure
but accelerates coronary flow.
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HOW ARE WAVES ASSESSED? |
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Impedance Analysis
For the last half century, arterial waves have been envisioned almost exclusively in terms of sinusoidal wave trains. The well-known theorem of Fourier tells us that any time series, arterial pressure and flow, for example, can be represented exactly as the superposition of harmonic waves with the appropriate frequencies and magnitudes and phase shifts. This Fourier analysis has been the basis of the vast majority of studies on arterial haemodynamics, but the standard textbooks tend not to mention that it can be useful to analyze waves in other ways (20, 21).Fourier analysis has contributed much to our understanding of arterial hemodynamics, but it is not necessarily the most convenient mode of analysis. The principle drawback is that it is a frequency-domain analysis in which it is fundamentally impossible to relate events occurring at specific times in the cardiac cycle to particular features of the frequency spectrum; each Fourier component is determined by its fit over a periodic cardiac waveform. Thus, for example, an intervention that affects only systole will affect the Fourier components of all frequencies to some extent. Second, Fourier analysis is essentially a steady-state analysis that cannot be used to study transient or nonperiodic events. Practically, this means that an irregular rhythm such as atrial fibrillation can only be approximated and that short-lived changes following intervention cannot be properly assessed. Finally, in its most common form, impedance analysis, Fourier analysis makes the generally unwarranted assumption that pressure and flow are linearly related through an Ohms law for each frequency component: pressure = impedance × flow.
Generally, clinical cardiologists find it difficult to follow the meaning of results explained in terms of phase and frequency and would prefer a more intuitive, time-dependent approach.
Wave-Intensity Analysis
There is another way to analyze waves that might lead to more readily understandable information. This alternative approach has its origins in gas dynamics and takes infinitesimal discrete wavefronts as its basic elements. The basic one-dimensional equations describing the conservation of mass and momentum in an elastic tube can be solved by using the method of characteristics (26, 30). The solution process is rather complicated, but the results are surprisingly simple. Any disturbance applied to the tube will propagate downstream and upstream with velocity, U ± c, where U is the velocity of the fluid and c is the wave speed determined by D, the distensibility of the tube, and
is the density of the fluid, c = (1/
· D)1/2.
In a nonlinear analysis, wave speed is allowed to be a function of
pressure and therefore to change during the cardiac cycle. If the
disturbance is a transient wavefront, then there is a simple relationship between the change in pressure across the wavefront (dP)
and the change in velocity (dU):
dP = ±
· c · dU,
where the + sign refers to the forward direction and the
sign is to the backward direction. For each direction, there are two
types of wavefronts: compression wavefronts that increase pressure
(generated by "blowing") and expansion wavefronts that decrease
pressure (generated by "sucking"). These wavefronts are the
elemental waves of this approach to wave mechanics, and any complex
wave can be synthesized from a succession of compression and expansion
wavefronts. The simplest way to imagine this synthesis of a complex
wave is to consider measuring the wave at short, discrete time
intervals as in analog-to-digital sampling. The change in pressure
between successive sampling times (dP) is the size of the pressure
wavefront at each time of sampling. When all of these waves are added
together, the original wave is generated.
The four possibilities of forward and backward compression and expansion waves, each potentially occurring simultaneously in the artery, mean that the interpretation of measured waveforms can be challenging. Fortunately, this task is made simpler by the mathematical observation that the wave intensity, the product of the change in pressure, and the change in velocity is positive for forward waves and negative for backward waves. Furthermore, the wave intensity calculated from a measured pressure and velocity at any time is equal to the algebraic sum of the wave intensities of the forward and backward waves intersecting at the site and time of measurement. Because of the importance of the wave intensity, this approach to the study of arterial hemodynamics is now generally known as wave-intensity analysis.
This approach has several physiological advantages. It is carried out in the time domain instead of the frequency domain, and therefore temporal events in the cardiac cycle can be interpreted directly in terms of wavefronts arriving at specific times. This allows the identification and quantification of upstream and downstream events. For example, waves arriving at the ascending aorta before and after the closure of the aortic valve can be identified and their impact on (or isolation from) the ventricle can be assessed. In addition, the method does not assume linearity between pressure and velocity and easily accommodates the main nonlinearities in the arteries, the change in wave speed with pressure, and the essential nonlinearity of the convective derivative in the conservation equations (11). The detailed mechanics have been published elsewhere and do not require repetition herein.
The most direct application of this analysis is the calculation of the wave intensity throughout the cardiac cycle from simultaneous measurements of pressure (or diameter) and velocity (or flow). The measurement of the pressure waveform generally requires an invasive approach, but this can be substituted by a wall displacement waveform measured noninvasively. The sign and magnitude of the measured wave intensity indicate the net effect of the forward and backward waves. Wave intensity is positive if the forward wave is larger than the backward wave and negative if the backward wave is larger than the forward wave. Zero wave intensity indicates either an absence of wave travel or that the forward and backward waves are of similar magnitude at the time of measurement. This simple calculation can tell us much about the amplitude and timing of reflected waves.
It is also possible to use wave-intensity analysis to separate the
measured pressure and velocity waveforms into their forward and
backward components, if one assumes that the forward and backward waves
are linearly additive. This separation is formally equivalent to the
separation based on the measurement of characteristic impedance proposed by Van den Bos et al. (34). This method depends
on the knowledge of the local pulse-wave velocity. The basic wave equations allow the wave speed to be calculated as a function of
pressure from pressure and velocity waveforms (pressure-velocity loop)
measured during the short period in early systole when forward wave
travel is predominant (13) (Fig.
3). These separated wave intensities give
an even more detailed description of the pattern of forward and
backward waves, which determines the pressure and flow that can be
measured in the artery.
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WHY ARE WAVES IMPORTANT? |
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Because waves are blood-borne mediators of energy transfer, a wave
pattern will inform about all the mechanical factors that influence the
pressure or flow. One example in disease is in hypertension, in which
reflected waves assume central importance. In the elderly or other
individuals with stiff or diseased large arteries, wave reflections are
increased and arrive early due to an increased PWV (22).
Early and accentuated reflections in the aorta account primarily for
late systolic pressure augmentation and thus the absolute systolic
pressure level (14, 23). Reflected waves also account for
isolated systolic hypertension (24). Early arriving wave
reflections are the major determinant of the systolic-diastolic pressure difference, and recent evidence points to pulse pressure as a
more powerful determinant of adverse events and mortality than either
systolic or diastolic pressures alone (16). Systolic ventricular loading by early and accentuated wave reflections can
result in left ventricular hypertrophy and left ventricular failure
(5). Reversal of systolic hypertension with reduction of
pulse pressure and ventricular hypertrophy brings outcome benefit and
points to large conduit arteries as a target for therapeutic intervention. Evidence is already accumulating that different blood
pressure-lowering agents exert differential effects on PWV and central
arterial wave reflections. Pannier et al. (25) showed that, despite causing similar decreases in systolic and diastolic blood
pressures, an angiotensin-converting enzyme inhibitor reduced aortic
wave reflections more than a
-adrenergic antagonist, but only the
latter reduced central aortic stiffness. Because the measurable
contribution of wave reflections to hypertension varies between
patients, these findings offer the opportunity for closer matching of
therapy to phenotype in the future. Care must be taken in the clinic
environment, however, because the increasing amplitude of reflections
in the periphery results in peripheral pressures that are higher than
central pressures, and these may be affected differently by vasoactive
interventions (35). These differences have led some to
advocate a peripheral measurement with computation of central pressure
using a transfer function (38).
Conduit artery stiffening resulting in increased PWV has thus become a powerful indicator of adverse prognosis. PWV generally increases with neurohumorally mediated vasoconstriction and decreases with endothelium-dependent dilatation (27). PWV is independently associated with cardiovascular and all-cause mortality in hypertensives (15). PWV has long been known to be increased in patients with Type I diabetes (28). More recently, PWV has been shown to be increased in patients with Type II diabetes and their first-degree relatives (10). In these patients, arterial compliance decreases as fasting glucose increases and accordingly may be seen before any changes in mean blood pressure (19). In patients with diabetes, PWV correlates positively with intima-media thickness (33), and the elastic behavior of arteries varies with blood glucose control (19). Sustained hyperglycemia results in the irreversible glycation of proteins, including collagen and other matrix and plasma proteins, to form advanced glycation end products (AGEs) (2). Elastin and collagen may be glycated with a corresponding increase in vascular stiffness in vitro (39). Glycation and intimal and medial cross-links account for the increased vascular stiffness seen in patients with diabetes (29). AGE cross-link breakers reverse the diabetes-induced increase in arterial stiffness in vitro (40). They also increase arterial compliance and tend to decrease PWV in elderly nondiabetic patients. The pressure-velocity loop approach to PWV measurement developed from wave-intensity analysis is a relatively easy way of assessing PWV in clinical studies. Furthermore, this single-site approach to local wave speed measurement provides greater precision than the time delay method applied to measurements at different sites, which usually results in a PWV averaged over a segment of artery containing widely differing wall characteristics (13). Because local wave speed reflects local wall elastic properties, it has potential utility for the longitudinal assessment of therapy directed at large artery stiffness and pulse pressure augmentation in patients with systemic hypertension and perhaps chronic heart failure.
Not all systems are as simple as the systemic arteries, in which backward traveling waves result from the passive reflection of actively generated forward waves. In more complex systems, waves can be generated from either direction. Wave intensity has been shown to reveal the net direction of wave travel at any instant in any structure in which one-dimensional blood flow can be assumed. One such complex system is the coronary circulation, in which flow is determined by waves generated actively by both upstream and downstream events (32). Wave-intensity analysis has been applied to measurements derived from the canine coronary circulation at rest and during atrial pacing. During isovolumic contraction, negative values of wave intensity in coronary arteries indicate backward compression waves generated by the compression of the intramyocardial vessels that increase coronary pressure but decrease coronary flow. During early systole, increasing aortic pressure initiates forward waves, indicated by positive values of wave intensity that increase both coronary pressure and flow, despite continuing high left ventricular pressure. Similarly, the relaxation of the myocardium during diastole generates a backward expansion wave that initiates the diastolic coronary flow. These new concepts, yet to be measured in the cardiac catheter laboratory, could be a possible means of assessing the functional significance of coronary stenoses and their response to intervention.
A different complex system is the pulmonary venous circulation where there has been debate about the origin of changes in pulmonary venous flow; does systolic forward flow result from left atrial "suction" or transmission of the right ventricular pressure pulse through the pulmonary vascular bed? An analysis of recent measurements shows that the wave intensity is negative in early systole, indicating a dominant backward traveling wave that decreases pressure and increases forward flow velocity (31). The backward traveling wave in this case results from atrial events. Thus backward traveling waves impose opposite effects on pressure in the coronary arterial and pulmonary venous circulations. In a pulmonary vein, a backward traveling expansion wave manifests "suction" from within the left atrium, caused by atrial relaxation and the downward apical shift of the atrioventricular ring caused by left ventricular contraction. The next event in the pulmonary venous cardiac cycle is a forward traveling wave in later systole, which originates in the right ventricle. Finally, during early diastole, pulmonary forward flow into the atrium is motivated by a further backward traveling expansion wave, this time caused by the reduction of left atrial pressure that follows mitral valve opening.
The wave intensity approach has also been adapted for the study of diastolic left ventricular filling by assuming one-dimensional blood flow between the left ventricle and atrium during the filling interval (17). As for the pulmonary veins, suction is apparent as a backward traveling expansion wave, in this case generated by left ventricular relaxation and falling left ventricular pressure. Every detail of the diastolic mitral inflow trace is explained in terms of forward or backward waves generated by the pressure changes occurring within either the left ventricular or left atrial cavities. Wave-intensity analysis has also allowed the calculation of left ventricular wave speed, a measure of myocardial compressibility that varies throughout the cardiac cycle, in animal experiments (36). The clinical assessment of diastolic filling, in particular, may be advanced by echocardiographic assessment of intraventricular wave speed and the direction of wave travel.
Finally, PWV can be measured noninvasively in rats and mice, and variations with vasoactive medications have been confirmed (8). Apolipoprotein E-knockout mice demonstrate reduced endothelium-dependent dilatation and increased atherosclerosis and, as expected, increased aortic PWV (6), despite unchanged blood pressure. This change is probably caused by decreased endothelial NO-dependent dilatation and by fragmentation of the elastic arterial lamina (37). This study advances our understanding of wave travel in transgenic mice by detailed consideration of changes in aortic velocity and acceleration waveforms. Increased PWV coincides with an early systolic inflection of the blood velocity signal in the upper descending aorta. This is consistent with a reflection from the carotid bifurcation traveling in the direction of aortic blood flow. The acceleration caused by the reflection exhibits a time delay consistent with the distance to the reflecting site and the wave speed. The authors speculate whether the same waveform may be seen in patients with severe atherosclerosis. This finding of increased peripheral wave reflection suggests widespread abnormalities of conduit vessels and smaller peripheral branching arteries in this animal model. A transgenic mouse model of Marfan syndrome with underexpression of fibrillin exhibits increased thoracoabdominal PWV (18). The wave mechanics of small animals can therefore change independently of blood pressure and may be used to monitor genetic and therapeutic manipulation.
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CONCLUSIONS |
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Hemodynamic studies are unfashionable in this era of molecular and genetic biology. However, we will increasingly need to understand how the elemental building blocks of life are incorporated into complex systems in intact organs and organisms. In the intact circulation, traveling wavefronts represent elemental units of energy transmitted within and between blood vessels and the heart. Energy transfer within traveling wavefronts represents a powerful integrating, or "messaging," mechanism operating through blood flow. Wave patterns, analyzed mathematically, inform about the upstream and downstream events that influence the flow, and the speed of wave travel informs about the mechanical state of the blood vessel in the locality. The measurement of pulse-wave velocity has physiological and potentially clinical significance in animals and humans and can be determined noninvasively and used to monitor treatment. Wave-intensity analysis, a relatively new approach, can explain the forces underlying blood flow in such complex systems as the coronary and pulmonary circulations and the diastolic heart. Despite its ease of measurement and interpretation, it has not yet been used extensively in the clinical environment. Indeed, the work referred to in this editorial has been preliminary.
Further study will be needed before we can "catch the wave" and realize its full potential on the catwalk of contemporary cardiovascular medicine and physiology. However, most fashions turn full circle in the fullness of time; this editorial shows how arterial hemodynamics has recently been redesigned. It may yet have its day.
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ACKNOWLEDGEMENTS |
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The contributions of Dr. A. Khir and Dr. A. Zambinini to the figures are greatly appreciated.
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FOOTNOTES |
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C. J. H. Jones and R. A. Bleasdale are funded by the British Heart Foundation.
Address for reprint requests and other correspondence: C. J. H. Jones, Wales Heart Research Institute, Heath Park, Cardiff CF14 4XN, UK (E-mail: jonescj4{at}cf.ac.uk).
10.1152/ajpheart.00070.2003
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