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PERSPECTIVES IN PHARMACOLOGY
Department of Pharmaceutical Sciences, University at Buffalo, the State University of New York, Buffalo, New York (D.E.M.); and National Institute on Aging, National Institutes of Health, Gerontology Research Center, Baltimore, Maryland (D.R.A.)
Received September 27, 2006; accepted November 30, 2006.
| Abstract |
|---|
High-frequency measurement of drug effects allows development of concepts of pharmacodynamic systems analysis and drug effects based on integrated signaling networks. There are many challenges to this approach; however, recognition of the basic tenets of the complexity, robustness, emergent properties, and intrinsic noise of biological signaling networks provide insight for their analysis (Weng et al., 1999
; Aderem, 2005
). Current approaches attempting to characterize such interactions in mechanistic terms include deterministic systems such as ordinary differential equations (e.g., chemical kinetics and compartmental models) and partial differential equations (e.g., reaction-diffusion models), stochastic systems (frequently used for species existing in small numbers), and hybrid systems that combine deterministic and stochastic components (Eungdamrong and Iyengar, 2004
).
Mathematical transforms are required to interpret time-series data of nonlinear systems and instances in which the frequency content of a signal is more informative than the original waveform. Fourier transforms of various biomedical signals have identified primary frequency regions that reflect the interplay between physiological control systems, the understanding of which may be exploited to characterize the intensity and time course of in vivo drug effects. Wavelet transforms are an extension of Fourier-type spectral analysis; however, they localize in both time and frequency domains and have properties that may have utility for analyzing pharmacodynamic data. It is important to recognize that mathematical transforms do not represent techniques that are mutually exclusive from current modeling paradigms (i.e., deterministic and stochastic systems). Wavelet and Fourier transforms may be used to describe specific functions within these models, characterize biological system properties that are subject to modeling, explore interconnections of system components, and/or qualify properties of existing models. Here we provide a brief overview of the fundamentals of Fourier and wavelet analyses, present example applications in pharmacodynamic research, and discuss their potential for analysis of complex pharmacological systems.
| The Fast Fourier Transform |
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![]() | (1) |
. The inverse Fourier transform is defined as:
![]() | (2) |
This shifts the time domain to a frequency domain. This transform also may be applied to space and position signals (e.g., imaging data), with H as a function of inverse wavelength (cycles per distance measure). For periodic functions, the original waveform may be reconstructed from the sinusoidal components by application of the Fourier transform:
![]() | (3) |
A useful feature of the Fourier transform (Brigham, 1988
; Press et al., 1992
) is to correlate two functions (g and h), defined as:
![]() | (4) |
leading to a Fourier transform pair:
![]() | (5) |
![]() | (6) |
A second useful feature of the Fourier transform is the computation of total power (TP) within a signal:
![]() | (7) |
A discrete Fourier transform is often used for signals composed of data sampled at evenly spaced intervals. A continuous signal may be reconstructed without information loss if the sampling frequency (fs) is greater than twice the highest frequency component in the signal (Nyquist critical frequency) (Semmlow, 2004
). The discrete Fourier transform is defined by the equation:
![]() | (8) |
|
| FFT and Spectral Analysis in Pharmacodynamics |
|---|
To model circadian cortisol concentrations, Krzyzanski et al. (2000
) developed an algorithm that uses Fourier series analysis to derive periodic, time-dependent input functions for basic turnover pharmacodynamic models that have been coded as a Fortran executable program called FOUR-PHARM. The rate of change of a biological substance (R) undergoing periodic secretion can be described by the following equation:
![]() | (9) |
![]() | (10) |
![]() | (11) |
![]() | (12) |
![]() | (13) |
With the input function defined, the baseline equation (eq. 9) can be integrated into indirect pharmacodynamic response models, where drug concentrations may serve to inhibit or stimulate the production or loss of the response variable. For cortisol, the pharmacokinetics of exogenous corticosteroids serve as driving functions for inhibiting Kin(t). This is achieved by multiplying Kin(t) in eq. 9 by the following inhibition function:
![]() | (14) |
1), and IC50 is the plasma steroid concentration producing 50% Imax. Model parameters (kout, Imax, and IC50) are estimated from fitting eqs. 9 to 14 to temporal cortisol profiles using nonlinear regression analysis. The Fourier coefficients may be fixed to values determined using the L2-norm approximation algorithm or, alternatively, could be estimated. This method improves on previous techniques for modeling circadian cortisol dynamics and has been extended to jointly model the combined effects of cortisol and exogenous corticosteroids on lymphocyte trafficking (Mager et al., 2003| Markers of Pharmacological Effect from Spectral Analysis |
|---|
-adrenergic, and renin-angiotensin system blockade alters specific components of the power spectrum of beat-to-beat heart rate fluctuations. Frequency-domain based methods for computing the power spectral density of heart rate variability (HRV) data include the FFT and parametric autoregressive modeling (Task Force of the European Society of Cardiology and the North American Society of Pacing and Electrophysiology, 1996
The paradoxical effect of atropine on parasympathetic cardiovascular control, where low doses of the drug cause an increase in vagal tone (shown as an increase in the HF band of the power spectrum) and high doses can result in complete parasympathetic blockade (Alcalay et al., 1992
), was demonstrated using FFT analysis. However, frequency-domain techniques are limited by loss of temporal information (Fig. 1B). One method for exploring the time course of frequency content of signals is to divide the signal into shorter segments of equal length and determine the frequency band power in each segment from the FFT (termed short-time Fourier transform or STFT) (Fig. 1C). Parametric techniques, such as autoregressive modeling, are an alternative to using the FFT to calculate power spectra and may also be used with this segmenting approach (Semmlow, 2004
). The time epochs must be of sufficient duration to identify the frequency range of interest but short enough to allow good temporal resolution. Scheinin et al. (1999
) applied this window technique to monitor the parasympatholytic effects of atropine, glycopyrrolate, and scopolamine. The parasympathetic tone in short segments of approximately 5 min was defined by the Hayano index (HI) (Hayano et al., 1990
):
![]() | (15) |
To address the intrinsic noise of HRV spectra using a cumulative plot approach, peak values of the power spectrum in the HF range for male Sabra rats (1.352.65 Hz) were obtained from autoregressive modeling of 2-min epochs of interbeat intervals following intravenous injection of saline, scopolamine, or a range of atropine doses (Perlstein and Hoffmann, 2000
). Although these HF peak values fluctuate significantly over time, a plot of the cumulative HF peak values as a function of time under placebo conditions reveals a constant positive slope, suggesting stationary vagal tone. Cumulative plots after low-dose scopolamine and atropine show an increase in this slope, whereas high atropine doses produce less steep curves, both gradually returning to predose values as drugs are eliminated. Thus, in this instance, the cumulative plot of spectral measures provided a relatively simple and rapid means of monitoring the time course of pharmacological effects of drugs on the autonomic nervous system. The parasympatholytic effects of atropine were then modeled using an indirect response model [eqs. 9 and 12 with Kin(t) replaced by a constant zero-order rate constant defined as Kin = kout x R(0)], with the slope of the cumulative plot representing the pharmacodynamic response variable (Perlstein et al., 2001
). Hoffman and co-workers also developed a model to characterize the increase in vagal tone induced by low doses of scopolamine and atropine (Perlstein et al., 2002
), where a significant delay in the onset of effects required the use of a time-dependent transduction model (Mager and Jusko, 2001
).
Similar short-time frequency analysis methods have been applied to EEG signals for quantifying the pharmacodynamics of drugs for the central nervous system, including benzodiazepines, neuroactive steroids, and other GABAA receptor modulators, antipsychotics, synthetic opiates, and adenosine A1 agonists (Mandema and Danhof, 1992
; Danhof, 2002
). An example of mechanism-based modeling of spectral measures of central nervous system drug effects utilized measurement of the average amplitudes in the
-frequency band (11.530 Hz) of 1-min EEG signals. These signals, obtained using FFT, were measured in male Wistar rats following 5-min intravenous infusions of one of nine study drugs, including six benzodiazepines, zolpidem, zopiclone, and a
-carboline compound (Visser et al., 2003
). The final pharmacodynamic model represents a modified form of the operational models of agonism described by Black and Leff (1983
), where the ultimate effect is defined by the two distinct processes of drug-receptor interaction and subsequent signal transduction. The estimated in vivo pharmacodynamic parameters were well correlated with those obtained from in vitro bioassays.
| Functional Image Analysis |
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![]() | (16) |
![]() | (17) |
As with the one-dimensional discrete Fourier transform, the FFT can be used to efficiently compute the transform coefficients of h(k1,k2).
Use of FFT to describe cellular dynamics may be approached by extending principles of fluorescence correlation spectroscopy. Petersen et al. (1993
) have developed image correlation spectroscopy for the quantitative analysis of images generated from confocal scanning laser microscopy. Consider a one-dimensional autocorrelation function (eq. 4) specified in the spatial domain:
![]() | (18) |
represents a spatial shift. An important property of this function is that the variance of the fluctuations in the original signal can be defined by eq. 18 as
0, which is inversely proportional to the number of fluorescent particles. Analogous to eq. 6, the two-dimensional FFT can be used to calculate a 2-D autocorrelation function. A 2-D Gaussian function is fitted to the normalized autocorrelation function using standard nonlinear regression analysis, and the number and density of fluorescent particles are calculated from model parameter estimates. Changes in the aggregation state and distribution of receptors for platelet-derived growth factor on human foreskin fibroblasts were detected using this approach (Petersen et al., 1993
5-integrin in migrating cells. | Visualization of Multi-Dimensional Datasets |
|---|
|
![]() | (19) |
| Continuous Wavelet Transform |
|---|
![]() | (20) |
) represents the sliding window function. However, only limited time resolution is obtained using this technique that is dependent on the size of the fixed window used to analyze the signal and the density of the measurements. The STFT is recognized as providing either good time or frequency resolution but not both (Wiklund et al., 1997
The continuous wavelet transform (CWT) represents a natural extension of Fourier analysis and provides a windowing technique of variable-sized regions based on frequency (see Fig. 1C). Similar to the FFT, the wavelet transform denotes a shift in data representation from the time domain of the original signal to an alternate domain. The CWT is defined as:
![]() | (21) |
is a wavelet basis function. Thus, scale or frequency information is obtained, whereas the function simultaneously localizes in the time domain. Similar to Fourier analysis, where a signal is decomposed into a series of sin and cos functions, the CWT is the sum over all time of a signal multiplied by scaled (a) and shifted (b) versions of the chosen wavelet basis function. The calculated coefficients, W(a,b), reflect the correlation between the original signal, h(t), and the wavelet basis function at specific scales (or frequencies) as a function of time. There are several families of wavelets, and although each has specific features that might enable certain applications, the final choice of the basis function is often made experimentally. The Morlet wavelet is an example of those defined by explicit functions over all time:
![]() | (22) |
Wavelet analysis of a simulated signal exhibiting a change in frequency content at a specific point in time is shown in Fig. 1D. The signal represents a simple sinusoid with a frequency of 15 Hz for the first 2 s and 5 Hz for times thereafter (Fig. 1A). The power spectrum of this signal calculated with the FFT shows no indication of the temporal aspects of the signal. The square of the wavelet coefficients as a function of scale and time is shown in Fig. 1D. For point of reference, scales 23 and 70 correspond to frequencies of 15.3 and 5.0 Hz, as described by the relationship:
![]() | (23) |
is the sampling period. The time course and change in frequency content of the simulated signal are clearly detected using wavelet analysis (Fig. 1D). | Wavelet Analysis in Pharmacodynamics |
|---|
| Parametric Wavelet Transforms in Medical Imaging |
|---|
![]() | (24) |
Turkheimer et al. (2000
) developed algorithms for characterizing the time-varying spatial pattern of radioactivity in PET studies that include multiresolution analysis and linear modeling in the wavelet domain. The overall procedure involves: 1) the application of the DWT to each 2-D image in a time-lapse sequence, 2) kinetic modeling of the time course of each wavelet coefficient to obtain a parametric wavelet transform and associated standard error, 3) utilization of the parametric wavelet transform to threshold the coefficients, and 4) application of the inverse DWT to the remaining coefficients to obtain the final spatial mapping. This technique may be applied to 4-D data sets (3-D images in time) and has been extended to provide variance estimates of the spatial mapping from an analysis of the residuals of the kinetic modeling in the wavelet domain (Aston et al., 2005
). Applications of the DWT for analyzing magnetic resonance imaging studies have also been reviewed previously (Bullmore et al., 2004
). Whitcher et al. (2005
) propose to group voxels according to a wavelet-based clustering algorithm. This technique involves applying the DWT to each voxel time series within user-selected regions. A subset of coefficients is selected as a means of dimension reduction, and members of the final set are grouped by k-means clustering. The algorithm was successfully applied to several data sets, including phantom data, contrast-enhanced perfusion-weighted imaging, and the pharmacokinetic analysis of an i.v. contrast agent injected into rats.
| Identification of Cellular Signaling Microdomains |
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|
| Potential Role in Integrative Pharmacology |
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In summary, the fast Fourier and wavelet transforms are widely used for the analysis of complex nonlinear dynamical systems in bioengineering and many other fields of study. Many signals of physiological and pharmacological processes exhibit such properties, where significant information may be contained in the time-frequency domain as opposed to the original waveform. Although the FFT and other spectral methods have been integrated into traditional methods of pharmacodynamic systems analysis, the use of wavelet transforms is more preliminary. Further development of these mathematical transforms may better incorporate time and space parameters into pharmacodynamic analysis.
| Footnotes |
|---|
This work was funded in part by the Intramural Research Program of the National Institute on Aging.
Article, publication date, and citation information can be found at http://jpet.aspetjournals.org.
ABBREVIATIONS: FFT, fast Fourier transform; CWT, continuous wavelet transform; DWT, discrete wavelet transform; EEG, electroencephalogram; 1-D, 2-D, 3-D, and 4-D, one-, two-, three-, and four-dimensional, respectively; STFT, short-time Fourier transform; FFHP, first Fourier harmonic projection; FRET, fluorescence energy resonance transfer; HRV, heart rate variability; HF, high-frequency; PET, positron emission tomography.
Address correspondence to: Dr. Darrell R. Abernethy, National Institute on Aging, Gerontology Research Center, 5600 Nathan Shock Drive, Baltimore, MD 21224. E-mail: abernethyd{at}grc.nia.nih.gov
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