Fluctuations and power laws in pulmonary physiology
Fluctuations and power laws in pulmonary physiology
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DOI:
10.1164/rccm.200202-152pp
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发表时间:
2002-07-15
影响因子:
24.7
通讯作者:
Suki, B
中科院分区:
文献类型:
--
作者:
Suki, B
Fluctuations of a variable can be characterized by the probability density distribution, which specifies the likelihood of finding a particular value of the variable within a small range. To estimate the distribution, we first construct a histogram of the measured values, and then we normalize the histogram so that the area under it is in unity. Often the distribution N (x) of a variable x follows a power law form: N (x) x d, which says that the relative frequency with which the variable takes a value x is proportional to x raised to the power d. The logarithm of this relationship is log (N) d log (x), a linear relationship between log (N) and log (x). Thus, to estimate the exponent d, we plot N (x) on a double-logarithmic graph, and d is the negative slope of a straight-line fit to N. An important feature of the power law is that its tail is very long compared with familiar distributions such as a Gaussian. The tail of a distribution is representative of the relative frequency of occurrence of large events. Because the tail of a power law can be orders of magnitude larger than the tail of a Gaussian, the probability that a large or rare event occurs in the power law model is also orders of magnitude higher. Most distributions have a typical or “characteristic” value, such as the value corresponding to the peak of the Gaussian. Power law distributions, however, do not have a characteristic value or scale that would be largely preferred over other scales. Thus, the process or structure that the power law describes is said to be “scale free”(3, 4). The implications are important. For example, the power law tail of the distribution in Figure 1C implies that the statistical risk for long periods of insufficient breathing is significantly larger than if the distribution were Gaussian. Power laws are closely related to fractals introduced by Mandelbrot (3). Fractals are self-similar objects because small parts of the structure at increasing magnifications appear similar to the entire object (4). The three-dimensional structure of the airways is a classic example in which the branching pattern repeats itself over multiple length scales (5). The trachea branches to the main bronchi at a scale of centimeters, whereas the peripheral airways show a similar branching pattern at a scale of 0.2 mm. The fluctuations in the size of a structure, for example, variability of airway diameter, depend on the size of the ruler, in this case airway generation. Furthermore, the distribution of measured sizes is a power law with an exponent that describes how the measured feature changes under successive magnifications. Dynamic processes (eg, acoustic or electric waves) propagating over fractal structures also exhibit fluctuations in time that follow power law distributions (6). In addition, power laws appear in spatial and temporal fluctuations studied using various correlation techniques (4, 7, 8). Examples of power law behavior include fluctuations in heart rate (8), respiratory rate (9), lung volume (10), ventilation and perfusion (11), tidal volume, oxygen and carbon dioxide (12), blood flow (13, 14), or the mechanics of cells (15) and lung tissues (16, 17). Nevertheless, fractals are not the only source of