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Departments of 1Biomedical Engineering, 2Cellular and Integrative Physiology, and 3Surgery, Indiana University Purdue University, Indianapolis, Indiana
Submitted 22 August 2006 ; accepted in final form 16 November 2006
| ABSTRACT |
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vessel wall; vascular tree; scaling laws
The best-recognized minimum dissipation principle was proposed by Murray (8), in which the metabolic consumption in a single vessel segment is proportional to the blood volume. Murray's law, which states that the cube of the radius of a parent vessel equals the sum of the cube of the radii of the daughters, has been considered in various bifurcations of different organs (5, 7, 10, 11, 1315). On the basis of angiographic data of vascular tress, there has been important progress to establish more global relationships between morphological parameters in an entire tree and its subtrees (6). Zhou et al. (16) (ZKM model) extended Murray's cost form to stem-crown units (SCU), and they deduced a set of scaling laws that describe the optimal structure-function relationships in vascular trees. Briefly, a vessel segment was defined as a stem, and the tree distal to the stem was defined as a crown. Although the form of these scaling laws has been validated in numerous trees (3), the theory only considers the metabolic consumption of the blood. There was no consideration of the metabolic requirements of the vessel wall (passive and active).
At first glance, the volume of blood to the volume of vessel wall scales as
R2L/2
RHL or R/2H, where R and H are the radius of the vessel and wall thickness, respectively. For large vessels, this ratio is large, implying that the blood volume term dominates the wall volume. For smaller vessels, however, this term decreases and the volume of the vessel wall becomes significant. More importantly, vasoactive properties of the vessel wall require substantially more metabolism compared with passive properties and may be significantly larger than the blood contribution.
Taber (12) considered a cost form that includes the vessel wall basal metabolism and vasomotor tone. It was shown that the optimal geometry of a vessel segment leads to a flow shear that increases with the blood pressure, in contrast to being constant as implied by Murray's law (5). It was also shown that the metabolic cost in a vessel segment is no longer proportional to the blood volume as required in Murray's formulation; instead, it appears to depend on the local wall thickness and pressure.
Although Taber's extension of Murray's hypothesis is useful for a single vessel segment, it must be extended to an entire tree as an integrated system. Here, we extended Taber's formulation to a vascular tree and the SCUs in the framework of the ZKM model. Our results show that the relation between metabolic dissipation and volume of the tree and SCUs remains proportional as additional metabolic sources are considered. This implies that the previously validated scaling relations hold under the conditions of dissipations of blood and vessel wall. This increases the biological realism of the validated ZKM model.
| Glossary |
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= H/R


a
| METHODS |
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![]() | (1) |
Metabolism in vessel wall.
There are two major sources of energy cost to maintain the vessel wall (12). For a vessel segment with radius R, length L, and wall thickness H, the basal metabolic energy is assumed proportional to the volume of vessel wall; i.e., Pwp =
·2
RLH, where
is a passive metabolic parameter. There are also smooth muscle cells that generate active contraction stress
a to balance the blood pressure p (9, 12). According to Laplace's law and assuming
a contributes f (0 < f
1) of the total wall stress, Taber (12) formulated the cost due to vasomotor tone as Pwa = f
p·2
R2L, where
is an active metabolic parameter. Thus the metabolic consumption in a vessel wall segment is given by:
![]() | (2) |
= H/R denotes the thickness-to-radius ratio.
For the ZKM, the total metabolism of a SCU with N vessel segments is thus the sum over all the segments, as
![]() | (3) |
n,
n, and fn may vary among all the vessel segments in a SCU.
Metabolism in SCU.
The total metabolic cost in a SCU is thus the sum of Pb and Pw. Whereas Pb (Eq. 1) is proportional to the crown volume V, the form of Pw (Eq. 3) is more complex and does not necessarily obey proportionality. For the passive basal metabolism, the wall thickness has been found to depend linearly on the radius along a vascular tree (1). For instance, H = 8.22 x 103 R + 3.2 (in µm) was reported by Guo and Kassab (2) for pig left anterior descending. Metabolic parameter
depends on the composition of the wall and may change along the tree. In the absence of experimental data, it is assumed that
n in Eq. 3 is relatively uniform over the three orders of magnitude variation in diameter over the vascular tree, i.e.,
n
. Thus the basal metabolic cost of a SCU is rewritten as:
![]() | (4) |
![]() |
is constant, and thus kwp = 2
is also a constant, showing that Pwp is approximately proportional to the arterial volume V. In Eq. 4, kwp may vary along a vascular tree, because the relation between thickness and radius is no longer proportional.
Next, we further consider Pwa due to active wall stress. Similarly to Eq. 4, it is rewritten as:
![]() | (5) |
n and fn in a SCU. Therefore, Eq. 5 does not indicate that Pwa is proportional to the arterial volume V. In the following experimentally based calculations, however, we find that kwa is nearly constant for all SCUs in a vascular tree under certain assumptions. Thus the total metabolic consumption in a SCU is formulated as:
![]() | (6) |
| RESULTS |
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Basal metabolic coefficient kwp.
To estimate kwp, we need the value of parameter
. Taber (12) estimated
as 2.88 x 103 (in dyn·cm2·s1) for rat portal vein, 1.21 x 103 for bovine mesenteric vein, and 7.64 x 103 for porcine carotid artery. In general,
can be estimated in the range of 103
104. Here, we calculated kwp for the pig left common coronary artery (LCCA). The morphometric data and blood pressure are taken from our previous studies (2, 4). As in Table 1, the pig LCCA consists of 11 orders of vessel segments. For each order, the average diameter R, length L, wall thickness H, and the number of vessels nv are given, as well as the previously computed longitudinal blood pressure p. SCUs of 10 orders are considered, as in Table 2. Order 10 is the entire LCCA, order 9 is a second largest SCU, and so on, until order 1, which is a smallest SCU with only two capillary branches. We assume
= 5.0 x 103 for the entire LCCA. It is found that kwp increases from 887 (dyn·cm2·s1) for the entire LCCA to 4,500 for the smallest SCUs (Table 2). When compared with kb for blood, kwp is on the same or even higher order of magnitude, which means that the basal metabolism in vessel wall cannot be ignored when the structure-function relationships are considered.
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also depends on the type and composition of vessel wall. It is estimated as 0.158 (in s1) for rat portal vein, 0.00872 for porcine carotid artery, and 0.0177 for bovine mesenteric vein (12). Therefore, the range of
is very large.
We calculated kwa for the pig LCCA. Since the values of f and
are lacking, we estimate f = 1.0 and
= 0.01 (12) for all vessel segments. The results are given in Table 2. It is found that kwa remains nearly uniform for large SCUs (orders 6
10) at about 2,500 and then gradually decreases to about 1,000 for the smallest SCUs of order 1. The degree of variation is relatively small given the three orders of magnitude change of diameter. Furthermore, the degree of active contraction for smaller vessels is significantly higher than that of larger arteries (by as much as factor 3), which implies a significantly higher f for the smaller vessels. This could serve to further reduce the variation of kwa over the entire range of SCUs.
Total metabolic coefficient.
As in Eq. 6, kmeta is the sum of blood metabolic coefficient kb and wall metabolic coefficient kw, which is the sum of active and passive coefficients kwa and kwp. Given that kb is constant in a vascular tree, kmeta is nearly constant over the entire range of SCUs only when kw is approximately constant. Whereas kwa and kwp both show variation from large SCUs to small ones (Table 2), it is interesting to determine the variation of their sum kw. In the absence of experimental data on the metabolic parameter
, we calculated kw with
= 1,000, 2,000,..., 6,000 (dyn ·cm2·s1), respectively. For a given
, the mean, standard deviation (SD), and coefficient of variance [CV = (SD/mean) x 100] of kw are computed over the SCUs. The variations of kwa and kwp, quantified with CV, are 30.7% and 64.2%, respectively. Note that CV for kwp does not change with
. It is found that the variations of kwa and kwp counterbalance each other when summed together. For example, CV of kw is 17.9% with
= 5,000, which is significantly lower than the CV of kwa and kwp individually. With
= 2,000 and 3,000, CV of kw further reduces to as low as 2.3% and 6.7%, respectively, meaning kwp is highly uniform for all the SCUs. If 1,000
5,000 for the pig LCCA, we expect that the total metabolic consumption (kmeta in Eq. 6) is approximately constant for all SCUs in a vascular tree.
| DISCUSSION |
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It may be noted that the metabolic coefficient kmeta must be large to confer a good fit to experimental data (unpublished observations). The blood metabolic coefficient kb, with typical value around 1,000 dyn·cm2·s1, does not meet the requirement. The present finding that the total metabolic consumption due to multiple sources can be estimated as proportional to the arterial volume is encouraging. In fact, when basal and vasomotor tone consumptions are taken into account, the value of kmeta is significantly increased.
The present study is based on several assumptions that may be verified when more experimental data become available. Whereas we use exact wall thickness data of pig LCCA (2), instead of previous approximation of uniform
(12), we assume uniform
along the entire vascular tree, which does not reflect the variation of composition of vessel wall in the tree. For the vasomotor tone, we also approximate that f and
are constant. We expect a proportional relationship by summing up the passive and active metabolic consumption in the vessel wall assuming that active stress in smaller vessels contributes more to the total wall stress than in larger vessels. The latter assumption has a physiological basis as smaller vessels have a stronger tone. However, experimental measurements on the metabolic parameters
, f, and
along a vascular tree are needed to more definitively establish the theory.
In summary, this study considers the total metabolic consumption in the SCUs of vascular trees, including blood metabolism and basal and vasomotor tone consumptions in the vessel wall. On the basis of previous experimental measurements, we estimated that the total metabolic consumption in any SCU is nearly proportional to the arterial volume, which provides further physical realism to the validated scaling laws of vascular trees.
| FOOTNOTES |
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The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
| REFERENCES |
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This article has been cited by other articles:
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Y. Liu, C. Dang, M. Garcia, H. Gregersen, and G. S. Kassab Surrounding tissues affect the passive mechanics of the vessel wall: theory and experiment Am J Physiol Heart Circ Physiol, December 1, 2007; 293(6): H3290 - H3300. [Abstract] [Full Text] [PDF] |
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