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7.8 Scaling Laws of Blood Flow Rate, Vessel Blood Volume, Vascular... 475
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Fig. 7.11 Relationship between normalized stem ow (Qs/Q capillaries (N scatter plot. RCA right coronary artery, LAD left anterior descending artery, LCx left circumex artery, PA pulmonary artery, PV pulmonary vein, SMA sartorius muscle arteries, MA mesentery arteries, OV omentum veins, BCA bulbar conjunctiva arteries, BCV bulbar conjunctiva veins, RMA retractor muscle artery. Reproduced from Razavi et al. (2018)
) for the symmetric trees of various species and organs shown in a log-log
c/Nc,max
) and normalized number of
s,max
malnutrition, atrophy, or apoptosis of cells. Conversely, the number density of capillaries may be increased in exercise or tumors in line with increase in blood ow to enhance the growth of the tissue. The number density can be determined from histological sections of biopsy specimens of animals and patients.
The ow perfusion-number density scaling relation can also be used for drug dose determination. The dose can be titrated b etween species as the number density reects perfusion (ow per mass) of tissue. Adequate perfusion (volumetric ow per mass of tissue) is essential for any organ because it affects its health and function. The linearity between stem ow and the number of capillaries the functional capillary density can be obtained from the length of vascular network noninvasively from standard medical imaging.
7.8.2 Crown Volume Scales with Capillary Number
Since crown volume (Vc) is cumulative blood volume within a network, a derivation based on the average branching ratio and scaling of vessel diameters and lengths in
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each branching level results in a relationship between crown volume and number of capillaries as shown in Appendix 13. If we normalize Eq. (7.94) in Appendix 13, with respect to maximum crown volume and number of capillaries in the entire vascular network, a general form of scaling relationship is obtained as:
where V
c,max
and N
V
V
c, max
are the total crown volume and the total number of
c,max

c
N
N
c
c, max
λ
capillaries in a vascular system, respectively.
The crown volume obeys a power-law (Eq. 7.15) as shown by analysis of morphometric data of full asymmetric arterial trees of porcine RCA, LAD, and LCx (Fig. 7.12). The scaling exponents (λ) are 1.48 (R (R
2
2
2
total numbe r of data points shown in Figs. 7.12a–c are the same as those in Figs. 7.10a–c; respectively.
The exponents in the symmetric analys is for the RCA, LAD, and LCx are 1.45 (R
2
2
2
similar to the asymmetric tree analysis and close to the theoretical value of 3/2 (Fig. 7.13). The mean exponent across various species and organs are 1.37 0.166
2
(R
> 0.92), which is within the theoretical range predicted by 2/3and 3/4
scaling laws. The scaling exponents, condence intervals, and R
2
associated with
scaling exponent for various species and organs are summarized in Appendix 12.
7.8.3 Crown Length Scales with Capillary Number
Since crown length is simply cumulative length of blood vessels of all branching levels within the network, a derivation based on the average branching ratio and scaling of average length of blood vessels in each level of branching (Huo & Kassab,
2012), results in a direct relationship between crown length and number of capil-
laries (Appendix 13). If Eq. (7.92) of Appendix 13 is normalized with respect to an entire tree, the following relation holds:
where L
c, max
capillaries in the entire tree. The hypothesis that λ is equal to 1 is conrmed below.
The crown length linearly scales with the number of capillaries for all stem-crown units of the full asymmetric coronar y arterial trees (Fig. 7.14). The values of scaling exponent λ (Eq. 7.16) obtained from Figs. 7.14a–c were 1.03 (R
2
(R respectively (as compared to a theoretical value of unit y, Eq. (7.16)).
and N
L
L
c, max
are the maximum crown length and the number of
c, max
2

c
N
N
c
c, max
λ
2
7.8 Scaling Laws of Blood Flow Rate, Vessel Blood Volume, Vascular... 477
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Fig. 7.12 Relationship between normalized crown volume (V
c/Vc,max
) and normalized number of capillaries (N
c/Nc,max
) for the full asymmetric porcine arterial tree shown in a log-log density plot: (a) RCA right coronary artery; (b) LAD left anterior descending artery; (c) LCx left circumex artery. The total number of data points are the same as those in Fig. 7.11. Reproduced from Razavi et al. (2018) with permission
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Fig. 7.13 Relationship between normalized crown volume (Vc/V capillaries (N scatter plot. RCA right coronary artery, LAD left anterior descending artery, LCx left circumex artery, PA pulmonary artery, PV pulmonary vein, SMA sartorius muscle arteries, MA mesentery arteries, OV omentum veins, BCA bulbar conjunctiva arteries, BCV bulbar conjunctiva veins, RMA retractor muscle artery. Reproduced from Razavi et al. (2018) with permission
The exponents in the symmetric analysis for the RCA, LAD, and LCx is 1.02
2
(R
) for the symmetric trees of various species and organs shown in a log-log
c/Nc,max
2
2
) and normalized number of
c,max
similar to the asymmetric tree analysis and close to the theoretical unity (Fig. 7.15). The average scaling exponent (Eq. 7.16) for all species and organs is 1.08 0.102
2
(R
> 0.9). Table 7.9 (Appendix 12) summarizes the least squares power-law
relation for each of the vascular trees, including exponent, condence interval, and
2
R
. The exponents are nearly unity and the R2is highly signicant.
The conformity between scaling of crown length and number of capillaries among various species and organs reveals another salient proportionality law between form and function of the vascular system. The blood vessels are known to adapt to physiological demands and altered homeostatic conditions. The capability of vascular trees to deliver oxygen tissue and nutrients to serve metabolism strongly depends on the number of capillaries. The capillary density changes in response to conditions like hypoxia. In the context of new blood vessel formation and vascular sprouting, length of the perfused blood vessel is a key determinant of growth and development. It has been shown that length of blood vessels adapts to changes in homeostatic conditions (Humphrey, Eberth, Dye, & Gleason, 2009; Lehman, Owens, Kassell, & Hongo, 1991; Sho et al., 2004). The scaling law links vascular length to respective capillaries through a structure–function relation.
7.8 Scaling Laws of Blood Flow Rate, Vessel Blood Volume, Vascular... 479
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Fig. 7.14 Relationship between the normalized crown length (L
c/Lc,max
) and normalized number of capillaries (N
c/Nc,max
) for the full asymmetric porcine arterial tree shown in a log-log scatter plot: (a) RCA right coronary artery, LAD left anterior descending artery, LCx left circumex artery. The total number of data points are the same as those in Fig. 7.10. Reproduced from Razavi et al. (2018) with permission
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Fig. 7.15 Relationship between the normalized crown length (Lc/L capillaries (N RCA right coronary artery, LAD left anterior descending artery, LCx left circumex artery, PA pulmonary artery, PV pulmonary vein, SMA sartorius muscle arteries, MA mesentery arteries, OV omentum veins, BCA bulbar conjunctiva arteries, BCV bulbar conjunctiva veins, RMA retractor muscle artery. Reproduced from Razavi et al. (2018) with permission
) for the full asymmetric porcine arterial tree shown in a log-log scatter plot.
c/Nc,max
) and normalized number of
c,max
7.8.4 Transit Time Scales with Crown Volume and Length
Because of the structural heterogeneity of vascular networks and hence heteroge­neous perfusions, the particles traverse various paths in the network. Hence, the mean transit time (T vascular network over period of time. Appendix 14 demonstrates a derivation for a relation between mean transit time and crown volume and length (i.e., Eq. 7.97). Equation (7.97) (Appendix 14) can be presented in a general normalized form as:
where T
c, max
, L
volume in the entire tree, respectively.
The crown volume and the product of crown length and mean transit time of
asymmetric coronary arterial trees follows a scaling relationship (Fig. 7.16). The
) is the average time required for blood to travel through the
c
c, max

T
T
c, max
, and V
c, max
c

L
c
L
c, max

V
V
c
c, max
λ
are the crow n transit time, crown length, and crown
7.9 Other Design Features of Vascular Trees 481
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scaling exponent λ (Eq. 7.17) are 0.981 (R
2
2
2
for the porcine RCA, LAD, and LCx, respectively, as compared to a theoretical value of unity reected by Eq. (7.17).
The transit time is a fundamental physiological parameter in biological transport phenomena and has critical implications for vascular disease. Too low or too high of transit times may not be physiological. For example, no-capillary ow and altered blood volume conditions occur under pathophysiological conditions. The scaling relation between mean transit time, blood volume, and the number capillaries can be used as a theoretical basis to understand the distribution of oxygen and nutrients under physiological conditions and microvascular failure under pathological condi­tions. It was shown by Razavi et al. (2018) that the estimation of transit time based on the crown length and volume hold for proximal trees (down to 1 mm diameter vessels which can be observed in angiograms). Hence, standard clinical imaging of blood vessel anatomy may yield functional data on the transit times through the organ of interest.
Similarly, the exponents in the symmetric analysis were 1.01 (R
2
(R similar to the exponents related to the asymmetric data (Fig. 7.17). The mean exponents for all species and organs is 1.03 0.082 (R data). The exponents for various species and organs along with the associated condence interval and R
2
2
2
were summarized in Table 7.9 (Appendix 12).
2
> 0.98 for symmetric
7.9 Other Design Features of Vascular Trees
Hortons law states that there exists a geometric relationship between the number of vessels of a given order and the corresponding order where the parameter of this geometric relationship is the branching ratio (Chap. 2). Although biological trees do not strictly obey Hortons law because the various branching ratios vary somewhat with order number (Kassab, Lin, & Fung, 1994), a mean ratio may be dened over the entire range of orders such that Hortons law is a good approximation. Table 7.8 (Appendix 8) shows the mean diameter, length, and number ratios over a range of order numbers for various organs and species. Horseld (1980) suggested that for laminar ow with minimal resistance and minimal entropy production, the number ratio should be equal to the cube of the diameter ratio R ratio should be equal the diameter ratio (R
L
that the length ratio is within 10% of the diameter ratio for most organs and species, while the number ratio deviates signicantly from the cube of the diameter ratio. Barker, Cumming, and Horseld (1973) observed that the quotient of the diameter and number ratios is 0.5 for the human pulmonary arterial and bronchial trees and birch trees. The mean SD of the R
ratio for the various organs and species
D/RN
listed in Table 7.8 is 0.48 0.057. This implies a coefcient of variance

). Table 7.8 (Appendix 8) shows
D
3
N
, and the length
D
482 7 Scaling Laws of Coronary Vasculature
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Fig. 7.16 Relationship between normalized crown volume (V
c/Vc,max
) and multiplication of crown mean transit time and crown length (T
s/Ts,max*Ls/Ls,max
) for the full asymmetric porcine arterial tree shown in a log-log density plot: (a) RCA right coronary artery; (b) LAD left anterior descending artery; (c) LCx left circumex artery. The total number of data points are the same as those in Fig. 7.10. Reproduced from Razavi et al. (2018) with permission
7.10 Fractal Description of Branching Pattern 483
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Fig. 7.17 Relationship between normalized crown volume (Vc/V mean transit time and crown length (T and organs shown in a log-log scatter plot. RCA right coronary artery, LAD left anterior descending artery, LCx left circumex artery, PA pulmonary artery, PV pulmonary vein, SMA sartorius muscle arteries, MA mesentery arteries, OV omentum veins, BCA bulbar conjunctiva arteries, BCV bulbar conjunctiva veins, RMA retractor muscle artery. Reproduced from Razavi et al. (2018) with permission
s/Ts,max*Ls/Ls,max
) for the symmetric trees of various species
) and multiplication of crown
c,max
(SD/mean 100) of approxi mately 10% over a wide variety of organs and species. The constancy of this ratio is suggestive of a design criterion for tree structures.
7.10 Fractal Description of Branching Pattern
A system obeying Hortons law is said to be fractalaccording to the mathematical terminology introduced by Mandelbrot (1977). Mandelbrot classied fractals according to their dimensions. A fractal structure exhibits a power-law relationship between total length of a morp hological feature (e.g., total length of elements or sum of diameters of elements) and basic length of measuring unit (e.g., length or diameter of a single element). Nelson (1988) has shown that for a tree structure, the fractal dimension can be computed as one minus the exponent of the power-law relation­ship. Gan, Tian, Yen, and Kassab (1993) have determined that the fractal dimensions of diameter and length are 2.49 and 2.99, respectively, for the dog pulmonary venous tree. Huang et al. (1996) obtained diameter and length fractal dimensions of 2.71 and
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2.97, respectively, for the human pulmonary arterial trees; the corresponding fractal dimensions for the human pulmonary venous trees are 2.64 and 2.86, respectively. The coronary data show that the diameter fractal dimensions for the RCA, LAD, and LCx are 2.09, 2.06, and 1.99, respectively, while the corresponding length fractional dimensions are 1.89, 1.96, and 1.78, respectively. These and other results summa­rized in Table 7.8 (Appendix 8) suggest that the various vascular trees possess the characteristics of a fractal structure.
7.11 Intraspecic Scaling Laws of Vascular Trees
The fractal dimension dened by Mandelbrot has been shown to characterize natural phenomena with remarkable simplicity (Mandelbrot, 1977). Vascular (Bassingthwaighte, Van Beek, & King, 1990; Family, Masters, & Platt, 1989; Matsuo, Okeda, Takahashi, & Funata, 1990; Sernetz, Wübbeke, & Wlczek, 1992), bronchial (Kitaoka & Itoh, 1991; Nelson & Manchester, 1988), and botanical trees (Kamiya & Takahashi, 2007; Matsuo, Nakakubo, & Yamamoto, 1997; Morse, Lowton, Dodson, & Williamson, 1985; Shibusawa, 1994) have been found to have fractal-like features. West et al. (1997) proposed a mathematical model referred to as the WBE (West, Brown, and Enquist) model to support the allometric 3/4 scaling law of metabolism for interspecic (from species to species) scaling, based on three major assumptions in a fractal-like cardiovascular system:
1. Area-preservation for branching patterns of vessel diameter >1 mm and cubed-
law for smaller vessels as wel l as space-lling branching pattern.
2. Size-invariant capillaries.
3. Minimum energy loss.
In the process, they assumed that the fractal-like networks in life have a fourth spatial dimension (West, Brown, & Enquist, 1999), which served as the basis of the WBE model (West et al., 1997). There is much debate on the WBE model, however, especially for the assumption of the space-lling branching pattern in the cardiovas­cular system (i.e., LR ¼ BR
1 3
, where BR and LR are the branching ratio and length
ratio, respectively. Kozlowski and Konarzewski (2004, 2005).
To derive the scaling laws within a species (intraspecic scaling, within an organ of given species), the branching ratio, diameter ratio, and length ratio in a fractal-like tree structure are dened as: BR ¼ n where n i ¼ 1, ... , N
, Di, and Liare the number, diameter, and length of vessels in level i,
i
(Huo & Kassab, 2012). Level 0 is the most proximal stem for an
total
entire tree or a stem for the stem-crown unit and level N arterioles or venules. Based on the assumptions of LR ¼ BR
i/ni  1
,DR¼ Di/D
, and LR ¼ Li/L
i  1
refers to the smallest
total
1
3γ
and DR ¼ BR
i  1
2þE
(where γ ¼ 0 represents space-lling, γ ¼ 1 area-lling, and γ ¼ 2 length­preservation; ε ¼ 0 represents area-preservation and ε ¼ 1 Murray s law) for a tree structure, fundamental derivations of the volume–diameter and ow–length
,
1