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1 Laboratoire de
Physiologie-Groupement d'Intérêt Public Exercice, Heart rate variability is a recognized parameter
for assessing autonomous nervous system activity. Fourier transform,
the most commonly used method to analyze variability, does not offer an
easy assessment of its dynamics because of limitations inherent in its
stationary hypothesis. Conversely, wavelet transform allows analysis of
nonstationary signals. We compared the respective yields of Fourier and
wavelet transforms in analyzing heart rate variability during dynamic
changes in autonomous nervous system balance induced by atropine and
propranolol. Fourier and wavelet transforms were applied to sequences
of heart rate intervals in six subjects receiving increasing doses of
atropine and propranolol. At the lowest doses of atropine administered,
heart rate variability increased, followed by a progressive decrease
with higher doses. With the first dose of propranolol, there was a
significant increase in heart rate variability, which progressively
disappeared after the last dose. Wavelet transform gave significantly
better quantitative analysis of heart rate variability than did Fourier
transform during autonomous nervous system adaptations induced by both
agents and provided novel temporally localized information.
Fourier transform; atropine; propranolol; autonomous nervous system
ADAPTATIONS OF THE ACTIVITY of the autonomous nervous
system have been widely studied through heart rate variability, which was first described by Hales (10) in 1733, by extracting the physiological rhythms embedded in its signal (28). Indeed,
physiological regulations, particularly blood pressure adaptations,
pharmacological responses to many drugs, as well as numerous clinical
applications, have been explored through its use. This interest is
notably reinforced by the known direct relationship between autonomous
nervous system tone and heart rate (20), sinoatrial stretch (12), or
myocardial contractility (6). Different physiological parameters can be addressed, such as respiratory sinus arrhythmia (25) mediated by
parasympathetic activity, thermoregulatory fluctuations in vasomotor
tone (13, 19), and baroreflex control (3, 23). Hon and Lee (11)
appreciated its clinical relevance for the first time in 1965; clinical
applications today also describe the parallelism between the degree of
heart rate variability and health status, including morbidity and
mortality in cardiac diseases (4, 28).
Different mathematical methods have been used to analyze heart rate
variability. Among these, Fourier transform is the one most commonly
chosen (27, 28) but one that is, however, limited to stationary
signals. With this mathematical transform, global representative
indexes of heart rate variability have to be calculated as a set of
cumulate spectrum powers contained in a given number of R wave-to-R
wave (R-R) intervals, which prevents temporal localization of sudden
changes in the behavior of the R-R signal. To overcome these
limitations, we applied wavelet transform, which offers two
complementary interesting features (2, 9, 16, 32). First, wavelet
transform allows a temporally localized sliding analysis of the signal,
thus giving access at any time to the status of heart rate variability,
as, for example, when the balance of autonomous nervous system
equilibrium is suddenly modified by acute clinical situations (15, 16,
29, 32) such as anesthesia or pharmacological interventions (8).
Second, the shape of the wavelet transform-analyzing equation differs
from the fixed sinusoidal shape of the Fourier transform and can be designed to better fit the shape of the analyzed signal, allowing a
better quantitative measurement.
To compare the respective yields of these two mathematical methods in
analyzing heart rate variability, we assessed their respective ability
to quantify, as well as qualify, a shift in autonomous nervous system
equilibrium in response to the administration of increasing doses of
atropine and propranolol.
Subjects.
Six sedentary male subjects, aged 27.7 ± 3.3 yr (mean weight 69.8 ± 8.1 kg, mean height 1.75 ± 0.10 m), received increasing intravenous doses of atropine and of propranolol while being monitored by using a Holter electrocardiogram recorder.
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ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES
![]()
INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES
![]()
METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES
Pharmacological protocol. All subjects were familiarized with the environment of the laboratory. They were requested to avoid alcohol and caffeine before and during the recording periods and to not perform heavy physical exercises during the preceding 24 h. An intravenous catheter was inserted into a large forearm vein 1 h before the beginning of the recordings. The subjects were then recorded in the supine position in a quiet room, which was exclusively reserved for the study. All recordings were started at 8 AM.
During the atropine injection period, an anesthesiologist continuously monitored the subjects and could follow through a monitor the effects of the drug on the electrocardiogram. Each atropine injection was performed in ~5 s and flushed through with 20 ml of normal saline. Four (1 µg/kg), three (2 µg/kg), and five (5 µg/kg) doses of atropine were injected consecutively at 20-min intervals. The doses were chosen to obtain cumulate doses equal to 1, 2, 3, 4, 6, 8, 10, 15, 20, 25, 30, and 35 µg/kg, respectively, without correction for the dilution or elimination of the previous doses. On a different day, a single bolus of 15 µg/kg of atropine was also administrated once in one subject. On another day, three consecutive boluses (50, 50, and 100 µg/kg) of propranolol were injected consecutively at 20-min intervals to progressively obtain complete blockade, given the large volume of distribution and the fast clearance of the drug.Recording procedure. The Holter recording procedures began 1 h before the first injection of atropine or propranolol and were prolonged for a 24-h period. Each intravenous administration was indicated on the Holter tape recorder by pressing the event button. Twenty minutes after the last injection, subjects were allowed to move about the laboratory.
R-R interval analysis. The electrocardiographic Holter system (StrataScan 563, Del Mar Avionics, Irvine, CA) allowed extraction of the list of R-R intervals with a precision of 1/128 s. The length of each R-R interval was manually validated during this step.
The mathematical analysis was made on a PowerMacintosh by using MatLab and the dedicated toolbox software Wavelab.Fourier transform. This analysis is based on the fact that data present with a stationary organization and are a combination of sinusoidal functions (26, 27). Thus the algorithms of analysis are searching for sinusoidal similarities in the signal. Unlike wavelet analysis, which is described below (see Wavelet transform), the search does not indicate the localization of the particular frequency along the observed signal, but, instead, provides a cumulate spectrum power of a particular frequency, i.e., corresponding to the number of occurrences of the given sinusoidal function, without indicating when it occurred. In our study, this analysis was conducted over periods of 256 consecutive R-R intervals. The spectrum power was calculated on ultralow (ULF; 0.0-0.04 Hz), low (LF: 0.04-0.15 Hz), and high (HF; 0.15-0.40 Hz) frequencies, and the low-high index was derived to obtain the autonomic nervous system balance. For the quantification measurements, we separately calculated variability on consecutive 20-min steady-state periods, corresponding to the consecutive doses of atropine and propranolol.
Wavelet transform. This analysis is devoted to the extraction of characteristic frequencies, or specific oscillations, of a signal that, in our study, was composed of the consecutive intervals between R-Rs.
Unlike Fourier, wavelet transform is usually devoted to the analysis of nonstationary signals. Thus there is no prerequisite over the stability of the frequency content along the signal analyzed. Conversely to Fourier, wavelet analysis allows one to follow the temporal evolution of the spectrum of the frequencies contained in the signal. Like Fourier or Laplace transforms, the continuous wavelet transform is an integral transform. The decomposition of a signal by wavelet transform requires a
function adequately regular and localized,
called the "Mother function." Starting from this initial
function, a family of functions is built by dilatation and
translocation, which constitute the so-called "wavelet frame." This frame is defined as follows
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a,b,
i.e.,
f(x) ·
a,b(x) · dx.
The calculation of this scalar product is the analysis of
f by the wavelet
. It allows a
local analysis of f and evidences the
presence of all members of the family, which are all scaled representatives of the Mother function. Indeed, if the Mother wavelet
is 0 out of
[
m,+m],
then
a,b
is 0 out of
[
m|a|+b,
m|a+b],
where m is a real number greater than zero (m
· +). As a
consequence, the value of
Wf(a,b) depends on the value of f near
b, with a weight proportional to a, where
W is wavelet transform.
Quantitatively, the value of Wf(a,b)
is representative of the importance of the concordance of
a,b
to f near
b at the a level. Thus wavelet analysis can be
considered as a local Fourier analysis performed at different separated levels.
The analysis amounts to sliding a window of different weights
(corresponding to different levels) containing the wavelet function all
along the signal. The weight characterizes a family member with a
particular dilatation factor. The calculation of
Wf(a,b) gives a serial list of coefficients called "wavelet
coefficients," which represent the evolution of the correlation
between the signal f and the chosen
wavelet at different levels of analysis (or different ranges of
frequencies) all along the signal f
(24).
A theorical example of wavelet analysis is represented in Fig.
1. The signal to be analyzed (Fig. 1,
top) can be described as
demonstrating three different behaviors; the first part contains a
mixture of high- and low-frequency sinusoidal signals, whereas the last
two parts are made up of a low- and a high-frequency signal,
respectively. The signal is analyzed by using a wavelet base built with
a Mother function called "Daubechies 4," represented in Fig. 1,
bottom right. The wavelet analysis of
this nonstationary signal allows one to follow the evolution of the
presence of each frequency contained in the initial signal through time
(Fig. 1, bottom left). Each wavelet
coefficient is determined at its level. The first levels (2, 4, 8, ...)
correspond to a wavelet analysis conducted with a small value of the
dilatation factor, thus representing high-frequency variations in the
signal. On the contrary, the last levels (..., 32, 64, 128) correspond
to a wavelet analysis conducted with a large value of the dilatation
factor, thus representing low-frequency variations in the signal. At
any level, the larger the coefficients, the greater the correspondence
between the original signal and the analyzing wavelet. This is
illustrated by Fig. 2, which shows the
consecutive 24-h R-R values plotted against time (Fig. 2,
top) in a young normal subject and
the corresponding levels and wavelet coefficients (Fig. 2,
bottom).
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Analysis of the atropine bolus procedure. This was intended to illustrate the response time of wavelet transform vs. Fourier transform after one bolus injection of atropine. First, a set of Fourier analyses was performed on the 256 consecutive R-R intervals before the bolus; then, this 256-R-R-interval window was progressively shifted to incorporate, at each step, 5 new R-R intervals, until all 256 R-R intervals belonged to the postinjection period. Second, a wavelet analysis was performed on the same sequence of R-R intervals.
Statistical analysis. Statistical analyses were performed with the sofware MATLAB, Statview, and SuperANOVA on a PowerMacintosh. A two-factor analysis of variance was performed with subjects and drug doses. P <0.05 was considered significant.
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RESULTS |
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Heart rate evolution.
The first doses of atropine (1-3 µg/kg) determined a
nonsignificant increase in R-R intervals, followed by a progressive
decrease in R-R intervals with the next doses (4-35 µg/kg),
compared with the reference period, which reached significance
(P < 0.05) at the last dose only.
After the last atropine dose, the R-R intervals progressively returned
to a higher value (Table 1). Figure
3, top,
shows the evolution of the R-R intervals of a subject during the
protocol.
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Fourier analysis.
Compared with the reference period, at any frequency analyzed, i.e.,
ULF, LF, and HF, neither the initial increase nor the later decrease in
spectrum power measured during the consecutive steady states reached
statistical significance during atropine administration. Only the LF/HF
ratio showed some significant variations (Fig.
5, bottom
left).
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Wavelet analysis.
At the lowest doses of atropine (1-4 µg/kg or the first 4 steady
states that followed), an initial significant increase in the power
coefficients was observed for the five highest frequency levels, i.e.,
levels 2,
4, 8,
16, and
32 (Fig. 5,
right) compared with the reference
period. After awhile, further increasing the dose of atropine
significantly decreased the power coefficients of the following steady
states. This decrease reached significance first for
levels 2 and
4 at a dose of 6 µg/kg,
then for level 8 at a dose of 10 µg/kg, and finally for level 16 at a
dose of 15 µg/kg (Fig. 5, right).
At each level, the decrease became deeper with the following doses. It
is remarkable that, at any given level, the sooner a significant
decrease was observed, the longer it took for the decrease to
disappear. After the last injection, the order of
reappearance of the coefficients was reversed compared with the order
observed during their disappearance. Then, the power coefficients
calculated during the night after the administration period were all
significantly higher than during the preadministration period. During
atropine administration, the wavelet LF/HF ratio demonstrated an
increase that became significant for a dose of 15 µg/kg and remained
significant 20 min after the last dose of 35 µg/kg (Fig.
7, top).
|
Effect of the single bolus of atropine.
The R-R intervals (Fig.
8A)
demonstrated a shortening and a clear and abrupt decrease in
variability ~15 s after the bolus injection.
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DISCUSSION |
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As hypothesized, wavelet transform performed differently from Fourier transform in analyzing heart rate variability. Two main features can be drawn from their comparison. First, from a qualitative point of view, wavelet analysis, because of its mathematical properties, continuously displayed and calculated the level of heart rate variability. Second, wavelet transform appeared to perform better than Fourier transform from a quantitative point of view in separating different levels of heart rate variability induced by a pharmacological intervention.
Up to now, adaptations of the cardiac autonomous nervous system have most often been evaluated by using Fourier transform of heart rate variability. The need to calculate the representative mean coefficients on a sufficient number of R-R intervals with that transform does not allow a precise detection of a sudden change in autonomous tone, and, thus, does not allow precise localization of one particular event in time (Fig. 8). Actually, because of this averaging process, the power coefficients resulting from that analysis, at a given frequency, are a mixture of events occurring at different times; even if a change occurs during the period analyzed, the mean power coefficients obtained only reflect the average of two different autonomous nervous system equilibriums. In contrast, wavelet analysis is able to calculate, at the highest frequency level, a representative coefficient of heart rate variability for each new set of two consecutive R-R intervals; this gives access to a precise, temporally localized status of heart rate variability for the parasympathetic as well as for the sympathetic drives, which is thus able to immediately reflect a shift in autonomous nervous system equilibrium. By using wavelet analysis, the update of heart rate variability coefficients at the highest frequency level only needs to integrate two new consecutive R-R intervals; the update of the frequency level immediately above must wait until four new R-R intervals have been integrated, and so forth. Thus the strength of wavelet analysis lies in the short delay needed to reflect a change in heart rate variability. This capacity to monitor instantaneous changes in autonomous nervous system tone will undoubtedly lead to new applications in physiology and therapeutics.
Fourier transform compares the shape of the signal to the shape of a sinusoidal function; thus any analyzed shape is always interpreted as a combination of several sinusoidal functions bearing different frequencies. Comparatively, wavelet transform allows the choice of an appropriate shape of the analyzing function to fit any particular signal. In our case, the Daubechies 4 wavelet better fit the point-to-point regulation of the R-R intervals by the autonomous nervous system. This probably explains the better quantitative separation in the power coefficients obtained by wavelet transform, as statistically observed during atropine administration. Undoubtedly, although the same statistical method was used for comparing the quantification represented by the power coefficients obtained from Fourier and wavelet transform of heart rate variability, the statistical differences obtained with the latter analysis were much more important. In any case, wavelet transform, at the highest doses of atropine, showed that the variability coefficients were entirely flattened out at any level. The question remains whether the analyzing shape of the wavelet equation should be adapted when different frequency levels are analyzed: it could be that, when the variability between series of different numbers of R-R intervals is analyzed, the ideal analyzing shape for the given length of a series, for example, 2 R-Rs, could be different from a shape fitting another length of a frequency or series, for example, 64 R-Rs.
Thus the physiological meaning of the wavelet coefficients represents, for the highest frequency, i.e., the variation observed between two consecutive R-R intervals, the ability of the autonomous nervous system to regulate the length of the second interval as an adaptation to the length of the first. As already described, heart rate variability is also assessed for higher combinations of intervals, these combinations being series of 2n intervals. The local analysis allowed by wavelet analysis is, thus, performed for each of these combinations, allowing revelation of a modification in heart rate variability at each frequency and at any time. Furthermore, as shown in Figs. 1, 2, and 8, a clear graphical representation of these progressive temporal changes can be obtained. Levels 2, 4, and 8 represent the frequencies that are attributed to parasympathetic activity, corresponding to the HF of Fourier indexes. The frequency band of the LF, which is an index of both parasympathetic and sympathetic activity, is represented by levels 16 and 32. On the whole, wavelet analysis is able to keep up a precise measurement of autonomous nervous system activity during transitory states (Figs. 6 and 8). Transients of sympathetic activity should also be precisely monitored by using wavelet transform but could be less evidenced than those of parasympathetic activity; this could be related to the fact that the LF power spectrum, and thus the LF/HF ratio, is not a pure index of sympathetic activity (7). Indeed, the LF/HF ratio did not show significant differences during propranolol administration (Fig. 7, bottom).
We followed step by step, in a single experiment, the whole array of the effects of atropine on heart rate variability up to the complete disappearance of these effects, as well as during the whole recovery period. As already shown, we observed that the smallest doses of atropine significantly increased heart rate variability (30). The effect of small doses of atropine on heart rate variability has been attributed to a central effect (17, 18), or a peripheral preference of the muscarinic presynaptic cholinergic receptors, which facilitate acetylcholine release (21). It has been demonstrated that, at higher doses, atropine attenuated or even abolished most of the frequency spectrum components of heart rate variability, as analyzed by Fourier transform (5, 14, 22, 31). Surprisingly, by using Fourier transform, even at the highest doses of atropine, we did not get a statistical difference from the reference level. As a matter of fact, we chose to assess the variations between the different periods by using ANOVA because we had more than two consecutive values to compare and also because we had to follow the variations over time; however, in the literature, the statistical comparison is generally done by using a paired t-test because only two different situations have to be compared, a baseline and an intervention period. Of course, when using paired t-tests on our Fourier transform results to compare the reference value to the intervention values, we got the same statistical differences as those already published; however, even in this case, wavelet transform allowed identification of more significant differences when ANOVA was used than Fourier transform when a paired t-test was used.
In conclusion, the ability to present a local analysis of heart rate variability and to obtain a better quantification of it represents the major advantages of wavelet transform compared with Fourier transform. Fast autonomous nervous system adaptations could be precisely monitored by using the feature of temporally localized analysis. The relationship between parasympathetic tone and cardiac function (6) could probably also be further explored, benefiting both from the quantitative and temporal feature of this mathematical analysis. This additional novel and more precise temporal localization, brought by the ability of wavelet transform to analyze nonstationary signals, makes wavelet transform a promising tool for analyzing other temporary situations, such as progressive adaptations to exercise or progressive effects of pharmacological tests other than atropine, in which it could provide information not easily shown by more traditional methods (1).
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ACKNOWLEDGEMENTS |
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We are indebted to Roland Thomas, Head of the Department of Medical Informatics, Saint-Etienne University Hospital, for valuable help. Del Mar Avionics, Inc., Irvine, CA, made accessible the R-R intervals lists from their Holter system.
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FOOTNOTES |
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This work was supported in part by a grant from the Région Rhône-Alpes (Eurodoc #L086840000).
Address for reprint requests: J.-C. Barthélémy, Laboratoire de Physiologie, CHU Nord-Niveau 6, F-42055 Saint-Etienne cedex 2, France (E-mail: JC.Barthelemy{at}univ-st-etienne.fr).
Received 13 November 1997; accepted in final form 17 October 1998.
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M. Takahashi, K. Matsukawa, T. Nakamoto, H. Tsuchimochi, A. Sakaguchi, K. Kawaguchi, and K. Onari Control of heart rate variability by cardiac parasympathetic nerve activity during voluntary static exercise in humans with tetraplegia J Appl Physiol, November 1, 2007; 103(5): 1669 - 1677. [Abstract] [Full Text] [PDF] |
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R. Barbieri, E. C. Matten, A. A. Alabi, and E. N. Brown A point-process model of human heartbeat intervals: new definitions of heart rate and heart rate variability Am J Physiol Heart Circ Physiol, January 1, 2005; 288(1): H424 - H435. [Abstract] [Full Text] [PDF] |
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F. Roche, V. Pichot, E. Sforza, I. Court-Fortune, D. Duverney, F. Costes, M. Garet, and J-C. Barthelemy Predicting sleep apnoea syndrome from heart period: a time-frequency wavelet analysis Eur. Respir. J., December 1, 2003; 22(6): 937 - 942. [Abstract] [Full Text] [PDF] |
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E. Toledo, O. Gurevitz, H. Hod, M. Eldar, and S. Akselrod Wavelet analysis of instantaneous heart rate: a study of autonomic control during thrombolysis Am J Physiol Regulatory Integrative Comp Physiol, April 1, 2003; 284(4): R1079 - R1091. [Abstract] [Full Text] [PDF] |
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