AJP - Heart Calcium Transients and Cell-Sarcomere
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Am J Physiol Heart Circ Physiol 290: H657-H664, 2006. First published September 19, 2005; doi:10.1152/ajpheart.00803.2005
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Axial nonuniformity of geometric and mechanical properties of mouse aorta is increased during postnatal growth

Yi Huang, Xiaomei Guo, and Ghassan S. Kassab

Department of Biomedical Engineering, University of California, Irvine, California

Submitted 28 July 2005 ; accepted in final form 12 September 2005


    ABSTRACT
 TOP
 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 
The hemodynamic conditions of aorta are relatively uniform prenatally and become more heterogeneous postnatally. Our objective was to quantify the heterogeneity of geometry and mechanical properties during growth and development. To accomplish this objective, we obtained a systematic set of data on the geometry and mechanical properties along the length of mouse aorta during postnatal development. C57BL/6 mice of ages 1–33 days were studied. The ascending aorta was cannulated in situ and preconditioned with several cyclic changes in pressure. We investigated the axial variations of geometry (diameter and length) and mechanical properties (stress-stain relation, elastic modulus and compliance) of the mouse aorta from the aortic valve to the common iliac. Our results show that the arterial blood pressure of mice increased from ~30 to 80 mmHg during the first 2 wk of life. The stretch ratio, diameter, wall (intima-media) thickness, and total lumen volume of mouse aorta increased with age. The aorta was transformed from a cylindrical tube at birth to a tapered structure during growth. Furthermore, we found the mechanical properties were fairly uniform along the length of the aorta at birth and become more nonuniform with age. We conclude that the rapid change of blood pressure and blood flow after birth alter the geometric and mechanical properties differentially along the length of the aorta. Hence, the axial nonuniformity of the aorta increases as the organ becomes more specialized during growth and development.

development; wall thickness; compliance; stress-strain relation; elastic modulus


AT THE TIME OF BIRTH, the major hemodynamic changes include an increase of cardiac output and its heterogeneity along the aorta, as well as an immediate increase in systemic blood pressure (13). During early growth and development, the peripheral tissues continuously increase demand for blood flow as the blood pressure increases to accommodate those flows for several weeks (16, 17, 35). During postnatal growth and development, the mammalian aorta undergoes rapid remodeling in response to the hemodynamic changes.

The study of the change of the geometry and mechanical properties during the postnatal development is particularly important to understand the mechanisms of vascular adaptation in response to changes in physical stress. The pressure-induced circumferential wall tension and flow-induced wall shear stress regulate the remodeling of the wall thickness and the diameter of the aorta, respectively (17). Numerous studies have investigated the morphological, structural, and biochemical changes of the aorta during development as well as the relation between these changes and the mechanics of the aorta (1, 3, 15, 16, 24, 31, 33, 34, 36). These studies confirm the aorta to increase its lumen, wall thickness, and mechanical stiffness during development. Most of these studies, however, have focused mainly on the proximal aorta, and none have systematically characterized the geometric and mechanical properties along the entire length of the aorta.

Our major objective was to quantify the heterogeneity of geometry and mechanical properties along the length of aorta as the organ becomes more specialized during growth and development. Hence, we systematically documented the geometry and the mechanical properties along the length of the mouse aorta at different age groups. We chose the mouse model because the mouse is being widely used in experimental studies of many aspects of cardiovascular health and disease. We focused on the C57BL/6J strain because it is the most widely used and best known of all inbred strains. Furthermore, it has substrains that are predisposed to hypertension, diabetes, and hypercholesterolemia, all of which are important risk factors for cardiovascular disease (6, 30). Our results show that the heterogeneity of geometry and material properties increases during development and underscore the structure-function relationship of the aorta during the postnatal period. Furthermore, the present data will serve as a reference state that defines normal growth for future studies of cardiovascular diseases in genetically manipulated mice.


    METHODS
 TOP
 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 
Animal preparation. All experiments were performed in accordance with national and local ethical guidelines, including the Institute for Laboratory Animal Research Guide, National Institutes of Health Policy, Animal Welfare Act, and University of California Institutional policies regarding the use of animal in research.

Forty-nine homozygous inbred mice of both sexes (C57BL/6 strain) from ages 1 to 33 days were used in this study. The mice were divided into eight groups according to age. The mice were anesthetized with intraperitoneal injections of ketamine (80 mg/kg) and xylazine (8 mg/kg). The mice were placed on a heating pad to maintain body temperature. The carotid artery was cannulated for blood pressure measurement by using a heating, stretched catheter as previously reported (26, 28). Heparin (200 U/ml) was used to prevent blood clots in the heart and blood vessels via the carotid artery catheter. The mice were euthanized with an overdose of the combination of ketamine and xylazine, and the apex of the hearts was excised.

Pressure-diameter-length relationship. The ascending aorta was cannulated through the apex of the left ventricle. The aorta was then carefully exposed and perfused with 6% dextran solution to flush out the blood. Cab-O-Sil (Eastman Kodak; concentration range 0.25–0.36%) was then mixed into the dextran solution to prevent flow through the microvessels and, hence, to attain a zero-flow condition. Water-resistant carbon particles were used to mark the aorta, dividing it into a series of 10–15 short segments. The aorta was preconditioned with five cyclic changes in pressure from 0 to the maximum in vivo pressure for each age group. The perfusion pressure was increased in 10- to 20-mmHg increments. The external geometry of the aorta, at different pressurized states, was photographed to obtain the loaded outer diameter along the trunk of the aorta. The outer diameter-length-pressure relationship for each of the segments was measured serially. A local dimensional coordinate, x, was introduced along the loaded vessel trunk, with x = 0 at the aortic valve and x = 1 at the point of common iliac bifurcation, as described by Guo and Kassab (11).

No-load and zero-stress state. After the distension protocol, the aorta was then dissected and placed into Ca2+-free Krebs solution (composition in mM: 11 D-glucose, 4.7 KCl, 120 NaCl, 25 NaHCO3, 1.2 KH2PO4, 1.2 MgSO4, and 0.026 EDTA). The entire length of the aorta was then cut into 50–70 rings. Each ring was transferred to Ca2+-free Krebs solution, aerated with 95%O2 and 5% CO2, and photographed in the no-load state. Each ring was then cut radially at the anterior position labeled with carbon black particles. The ring opened to a sector and gradually approached a constant opening angle defined as the angle subtended by two radii connecting the midpoint of the inner wall. The cross section of the sectors was photographed 30 min after the radial cut was made. The morphological measurements of inner and outer circumference, medial wall thickness (bounded by internal and external elastic lamina), and area in the no-load and zero-stress states were made from the images by using a morphometric analysis system (Sigma Scan). We made four measurements at equal distance along the circumference of the ring and the sector to determine the medial wall thickness.

A local dimensional coordinate, a, was introduced along the unloaded vessel trunk, with a = 0 at the aortic valve and a = 1 at the point of common iliac bifurcation. The coordinates x and a were referred to as the fractional longitudinal position (FLP) in the loaded and no-load states, respectively (11).

Biomechanical analysis. The characterization of biomechanical properties along the length of aorta has been previously described in detail (11). Briefly, the incompressibility condition was used to compute the inner radius as

(1a)
where ro and ri are the outer and inner radii at the loaded state, respectively. {lambda}z = l/l0 is the axial stretch ratio, where l and l0 are the vessel lengths in the loaded and zero-stress states, respectively, and A0 is the wall area in the no-load state. The wall thickness (h) was computed as

(1b)
The wall thickness was computed based on measured quantities r0, A0, and {lambda}z for the intima-media.

The circumferential deformation of the artery may be described by Green strain ({varepsilon}) as

(2a)
where {lambda}{theta} is the midwall circumferential stretch ratio ({lambda}{theta} = Cm/CmZS). Cm refers to the midwall circumference (average of inner and outer circumference) of the vessel in the loaded or no-load state, and CmZS refers to the midwall circumference in the zero-stress state as described in No-load and zero-stress state. The axial Green strain ({varepsilon}z) is given as

(2b)
where {lambda}z is defined as above. At an equilibrium condition, the average circumferential Cauchy and Kirchhoff stresses in the vessel wall were computed as

(3a)
where P is the luminal pressure and {lambda}{theta} and h are the circumferential stretch ratio and wall thickness of the vessel, respectively. The axial Kirchhoff stress is given as

(3b)
The elastic modulus in circumferential direction was computed as

(4)
The value was constant for all pressures, because the stress-strain relationship was found to be linear.

The lumen cross-sectional area (CSA) and the lumen volume (V) at different distention pressures were computed as CSA = {pi}ri2 and

(5)
where ri is the inner radii at the loaded state and L is the total length of the aorta (aortic valve to common iliac bifurcation). Similarly, the wall area (WA) and the wall volume (V) of the aorta at loaded state were computed as WA = 2{pi}rih and

(6)
The CSA compliance, CCSA, of the aorta is given as the slope of the pressure-volume relationship; i.e., CCSA = {Delta}CSA/{Delta}P. The volume compliance, CV, was defined similarly as CV = {Delta}V/{Delta}P.

Wall shear stress. The wall shear stress, WSS, can be evaluated if the diameter and flow rate are known under certain assumptions. The volumetric flow rate is proportional to the cube of the vessel radius, assuming a laminar, incompressible Newtonian flow through a rigid cylindrical vessel as given by the following relationship:

(7)
where Q and D represent the volumetric flow rate and diameter of vessel and µ denotes the viscosity of blood. If we combine the present data on the diameter of the proximal aorta with the data on cardiac output (CO) or flow of the same mouse strain (35), we can determine the WSS. Using MRI, Wiesmann et al. (35) showed that the CO increased linearly in the first 4 wk, which was 1.1 ml/min at 3 days of age and 5.3 ml/min at 10 days (CO = 0.32t + 1.1; R2 = 0.998, where CO and t have units of ml/s and days, respectively). Similarly, the inner diameter of the ascending aorta, from the present study, was found to vary linearly with time and were curve fitted accordingly. If we assume a constant blood viscosity of 4 cP, we can compute the WSS at various time points of development, given the diameter and flow.

Data analysis. The position along the aorta was normalized with respect to the total length. The results were expressed in terms of the FLP, ranging from 0 to 1. We further divided the aorta according to anatomic regions; i.e., the thoracic aorta was divided into proximal, middle, and distal regions, whereas the abdominal aorta was divided into proximal and distal regions. Anatomically, the proximal, middle, and distal thoracic aorta correspond to the segment from the aortic valve to the first pair of intercostals arteries, from the first to the sixth pair of intercostal arteries, and from the sixth pair of intercostal arteries to the subcostal artery (diaphragm), respectively (11). The proximal and distal abdominal aorta corresponds to the segment from the subcostal artery to the left renal artery and from the left renal artery to the common iliac artery, respectively.

Statistical analysis. Either linear or nonlinear regression was used to curve fit the data. One-way and two-way ANOVA and Student’s t-test were used to detect the possible difference between different positions and groups of animals.


    RESULTS
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 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 
Figure 1 shows the increase of body weight, which has a linear relationship with age in the first 30 days of growth. The growth rate is 0.5 g/day, as summarized in Table 1. The mean arterial blood pressure of the mice increased from 30.6 ± 3.9 to 78.8 ± 10.3 mmHg (means ± SD) during the first 2 wk of development and tended to stabilize thereafter, as shown in Fig. 2.



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Fig. 1. Variation in mouse body weight with age.

 

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Table 1. Growth rate for various parameters of mouse and aorta for the first 30 days of life

 


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Fig. 2. Variation of mouse mean arterial blood pressure with age.

 
The variation of outer diameter and wall thickness for the various segments of the aorta at loaded state are shown in Fig. 3, A and B, respectively. The outer diameter of the mouse aorta increases linearly with age during the first 4 wk of life, with the proximal thoracic aorta growing the fastest (26.7 µm/day) and the distal abdominal aorta growing the slowest (9.7 µm/day). The wall thickness of the mouse aorta increases rapidly during the first 2 wk of life but grows more slowly thereafter. Similarly, the proximal thoracic aorta grows the fastest, whereas the distal abdominal aorta grows the slowest. During growth and development, the body length (distance from nose to anus), coelom length (distance from clavicle to anus), and aorta length (distance from valve to common iliac bifurcation) at the loaded state increases linearly with an increase in age, as shown in Fig. 4A. The body length grew the fastest (1.64 mm/day), whereas the aorta grew the slowest (0.72 mm/day), as shown in Table 1. The global stretch ratio is taken as the total length of the aorta at physiological pressure normalized with respect to the in vitro length at the no-load state (approximately equivalent to zero-stress state) as shown in Fig. 4B. The global stretch ratio of mice did not change significantly during the first 2 wk of life (P > 0.05), but it did so when the mice were 3–4 wk old (P < 0.05).



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Fig. 3. Variation of outer diameter (A) and medial wall thickness (B) along the longitudinal location of the mouse aorta with age. PTh, proximal thoracic aorta; MTh, middle thoracic aorta; DTh, distal thoracic aorta; PAb, proximal abdominal aorta; DAb, distal abdominal aorta.

 


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Fig. 4. Variation of mouse body, coelom, and aorta length (A) and global axial stretch ratio (B) with age. *P < 0.05 compared with other groups.

 
The lumen volume of the aorta increased linearly with age, as shown in Fig. 5A, at a rate of 1.09 mm3/day. The wall volume growth of the aorta also increased linearly at a rate of 0.14 mm3/day, as shown in Fig. 5B. If the density of the aorta remains constant, this would represent the growth rate of the aorta (mass/time).



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Fig. 5. Lumen volume (A) and wall volume (B) of the mouse aorta at the loaded state.

 
Figure 6 shows the variation of the Green strain and Cauchy stress with age at physiological pressure. The Green strain was uniform during the first 3 days of life and began to decrease thereafter, as shown in Fig. 6A. It reached a constant value when the mice were more than 2 wk old. The Green strain of the thoracic and abdominal aorta tended to be uniform when the mice were <2 wk old but became significantly different when the mice were >2 wk old, albeit the differences are relatively small. Conversely, the Cauchy stress of the aorta increased gradually with age. When the mice were 3 days old, the stress was uniform along the length of the aorta. The Cauchy stress of proximal aorta tended to be higher than the distal after 3 days of age (P < 0.05).



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Fig. 6. Variation of circumferential Green strain (A) and Cauchy stress (B) in mouse aorta with age. Th, thoracic aorta; Ab, abdominal aorta. *Significant difference compared with different segments along the aorta. #Significant difference for thoracic compared with abdominal aorta.

 
The variation of the circumferential and axial Green strain and Kirchhoff stress with pressure were computed for various segments of the aorta. The relationships were found to be linear up to physiological pressures. The variation of the circumferential elastic modulus showed no significant difference along the aorta (P > 0.05), and it increased with age, as shown in Fig. 7A. The modulus was low when the mice were younger (age within 3 days) and reached a plateau when the mice were older than 2 wk of age. The variation of lumen CSA with pressure for the various segments of aorta also was found to be linear. Figure 7B shows the CSA compliance of the aortic segments (i.e., slope of the P-CSA relationship). The CSA compliance was relatively uniform along the length of the aorta when the mice were younger (first 2 age groups, P > 0.05) and became significantly different later in age (P < 0.01).



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Fig. 7. Circumferential elastic modulus (A) and cross-sectional area compliance (B) for different segments of mouse aorta. *Significant difference compared with different segments along the aorta. #Significant difference compared with other age groups.

 
The variation of lumen volume with pressure for the various segments of aorta also was found to be linear. Hence, the volume compliance was computed as the slope of the pressure-volume relationship, as shown in Fig. 8A. The volume compliance of various segments of aorta was relatively uniform in the first 3 days and became significantly different later in age (P < 0.01). Figure 8B shows the volume compliance of thoracic (sum of proximal, middle, and distal thoracic aorta) and abdominal aorta (sum of proximal and distal abdominal aorta). It is clear that the difference in volume compliance of thoracic and abdominal aorta increases with age.



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Fig. 8. Volume compliance for different segments of the mouse aorta (A) and for the thoracic and abdominal aorta (B). *Significant difference when compared with different segments along the aorta.

 
The strain measurements were based on the circumferences in the zero-stress state. Correspondingly, the opening angle of the zero-stress state was measured in the various age groups. In the thoracic aorta, the opening angles varied from 106.9 ± 7.2 to 85.0 ± 4.0° at 6 to 30 days of age, respectively. The opening angles of the abdominal aorta did not vary significantly at ~110° during the same period of time. The measurements of opening angle were less accurate for the first several days because of the softness and twisting of the tissue.

The WSS was computed according to Eq. 7 and is shown in Fig. 9. The linearity of the change of WSS during development is quite apparent. The rate of change of WSS is summarized in Table 1. The negative sign denotes a decrease in WSS during development.



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Fig. 9. Change in wall shear stress in mouse aorta with age during development.

 

    DISCUSSION
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 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 
The results of this study both support and extend the previous studies on the remodeling of aortic geometry and mechanical properties during postnatal growth and development (1, 2, 4, 15). Changes of pressure and flow in arterial tissue introduce deformations in the axial, circumferential, and radial directions (17, 32). Hence, the aorta should manifest growth and remodeling in length, diameter, and wall thickness during development. The heterogeneity of those parameters along the entire length of the aorta, which has previously not been documented, was the primary focus of this study.

One to two wk of age: pressure- and flow-induced remodeling. The first 2 wk of the mouse life are characterized by simultaneous changes of blood pressure and CO. Our data show that the mean arterial pressure of the C57BL/6 mouse increased from ~30 to 80 mmHg during postnatal development and reached the adult value at 2 wk of age (Fig. 2). Study of CO of the same strain of mouse with MRI showed that the CO increased linearly in the first 4 wk of life and was 1.1 ml/min at 3 days of age and 5.3 ml/min at 10 days age (35). Hence, in addition to the hormonal changes in the first 2 wk of life, the C57BL/6 mouse aorta experiences stress-induced remodeling introduced by changes in both blood pressure and blood flow, with the changes in flow (382% increase) being significantly higher than those in pressure (167%).

Numerous studies have demonstrated that changes in blood pressure are associated with changes in wall thickness. Aortic wall thickening was observed during development (3, 24, 27), which was attributed to the medial tissue accumulation of elastin, collagen, and smooth muscle cells. The wall thickness increases rapidly during the first 2 wk of the C57BL/6 mouse. We found that the growth of the wall thickness is not uniform along the aorta during development. The thoracic aorta grows faster than the abdominal aorta, where the proximal aorta grows the fastest and the distal aorta grows the slowest.

The major flow changes at the time of birth include a dramatic increase in pulmonary blood flow because of the postnatal loss of the placental circulation. Furthermore, there is a dramatic decline in blood flow in the abdominal aorta because of the closure of the umbilical arteries at birth (13). Langille et al. (18) found that the abdominal aortic external diameter in the period between 4 and 14 days postpartum was reduced significantly compared with in utero values. Our data show a linear relationship in the outer diameter (Fig. 3A) and the inner diameter of the aorta (data not shown) with age. The growth rates of both the outer and the inner diameters of thoracic and abdominal aorta are different during the first 2 wk of life. The thoracic aorta grows faster than the abdominal, where the proximal grows the fastest and the distal aorta grows the slowest, as shown in Table 1.

Three to four wk of age: flow-induced remodeling. The mean blood pressure reached the adult value when the mouse was 2 wk old, as shown in Fig. 2. Interestingly, Fig. 3B shows that the growth of the wall thickness of the aorta levels off when the mouse reaches 2 wk of age. This observation is consistent with hypertension-induced wall hypertrophy verified by previous studies (19, 25). Similarly, we found that the growth of the wall thickness is not uniform along the aorta during development, where the proximal aorta grows the fastest and the distal grows the slowest, as shown in Table 1. It has been previously demonstrated that the growth rates of the medial CSA between the thoracic and the abdominal aorta were different (18). This suggests that the aorta radially transforms from a relatively thin cylindrical tube to a thicker structure, where the thickness tapers along the length of the aorta during postnatal growth.

Although the blood pressure plateaus, the CO continues to increase linearly through 3 (8.7 ml/min) and 4 wk of age (9.3 ml/min) (35). Figure 3A shows that the outer diameter of the aorta increases linearly with age within the first 4 wk of life. Similarly, we found that the growth of the diameter of the aorta is not uniform along the aorta during development, where the proximal aorta grows the fastest and the distal aorta grows the slowest (Table 1). This implies that the blood flow increases the most at the proximal aorta. This difference in flow circumferentially transforms the aorta from a relatively cylindrical tube to a tapering structure after birth.

These mice are fully mature sexually at 63–70 days, and their average life span is ~900 days (20). Hence, at 10 wk, it is unlikely that there are additional significant changes in hemodynamic parameters. The MRI measurements of CO by Wiesmann et al. (35) showed values of 15.7 and 14.3 at 10 and 16 wk, respectively. These differences were not statistically significant. Hence, the increase in the various parameters (body weight, diameter, length, lumen volume, and wall volume of aorta) would plateau because the hemodynamic stimuli become uniform. The remodeling process in senescence is, of course, a different issue.

Axial growth and remodeling. The length of the aorta increases linearly with age during normal development (Fig. 4B). It is well known that arteries are under axial traction and that the percent vessel retraction increases linearly with age (4). The retraction is due to axial prestretch that is imposed by attachments to contiguous tissue. Our data show that the variation in global stretch ratios of the aorta was not significantly different in the first 2 wk (P > 0.05). The global stretch ratio increased significantly, however, when the mice were >3 wk of age. During development, the body length grows faster than the aorta, as shown in Fig. 4A. This implies that the aorta is subjected to a distending axial force during growth that becomes significant after 3 wk of age.

In a recent study, Zhang et al. (37) showed that an increase in axial stretch tends to increase the axial stress and strain much more significantly than their circumferential and radial counterparts for both the porcine left anterior descending coronary (LAD) artery and rabbit aorta. For the coronary artery, a stretch ratio of 1.5 results in identical circumferential and axial stresses and strains. This is interesting, because the axial prestretch ratio for the LAD artery is ~1.4 (22). These results indicate that the circumferential and axial wall stresses and strains in the LAD artery become more uniform as the axial prestretch ratio increases. In other words, under the same physiological pressure, a more homogeneous stress state may be obtained by prestretching the vessel. Hence, the axial prestretch at the in vivo state may play a role similar to that of the circumferential residual strain, i.e., making the stress and strain more homogeneous in the vessel wall. Future studies should consider the effect of change in prestretch on the intramural stress and strain distribution during development.

Changes in opening angle during postnatal development. The zero-stress state often has been characterized by the opening angle, which is defined as the angle subtended by two radii connecting the midpoint of the inner wall (10). Fung (10) previously proposed that the remodeling of the zero-stress state is an index of the nonuniformity of growth and remodeling. Fung and Liu (8, 9, 21) showed that hypertension induces growth of intima that exceeds that of the adventitia. Consequently, the vessel sector, in the zero-stress state, shows an outward bend and, hence, an increase in the opening angle. Conversely, Lu et al. (23) showed that flow overload induces growth of adventitia that exceeds that of intima. Hence, the vessel sector bends inward and decreases the opening angle. In summary, hypertension and flow overload have opposing effects on the opening angle. In models of simultaneous hypertension and flow overload, the effects of opening angle are nearly conciliatory (14).

Our present results are consistent with the previous findings if we consider the changes in pressure and flow. In the thoracic aorta, the change in flow dominates the change in pressure, and hence the opening angle decreases during development (from 107° to 85°). In the abdominal aorta, however, the changes in pressure and flow are fairly similar (approximately constant at 110°), and hence the effect is conciliatory. In future studies, it would be interesting to consider the effect of change in zero-stress state on the transmural distribution of intramural stress and strain.

Physiological implications of mechanical remodeling. Elastin, collagen, and smooth muscle cells are the main components of aorta. The elastin and collagen are thought to contribute to the elastic properties at low and moderate blood pressures and at high pressures, respectively (1, 32). The principal source of viscoelasticity is attributed to smooth muscle cells (34). During development, there was an uneven growth of each of the microstructured components, with increases in collagen > elastic laminae > muscle cells (27). The collagen content was higher and the elastic fiber content was lower in the thoracic compared with the abdominal aorta, which implies the thoracic aorta is more compliant than the abdominal aorta (7). The present data show that the stress-strain relationship of the mouse aorta is linear within the physiological pressure range in all age groups (10–50 mmHg for the newborn, 30–100 mmHg from >3 wk old); the relationship becomes nonlinear beyond the physiological pressure range. These results are consistent with our study on adult mice (11). The lines shift upward and to the left during development, suggesting increased stiffness.

At birth, when the pressure is low, the elastic modulus (Fig. 7A) and the compliance (Figs. 7B and 8, A and B) are small and fairly uniform along the entire length of the aorta. As the pressure increases, the aorta becomes more elastic. Furthermore, the aorta becomes mechanically heterogeneous, with the proximal region near the heart being the most compliant and the distal region least compliant. This is a functional adaptation, because the aorta’s elasticity must convert the heart’s pulsatile flow to steady flow in peripheral vessels. This is, of course, the well-known windkessel model.

Similarly, our data on circumferential Cauchy stress show uniformity along the aorta during the first postpartum period, which is consistent with previous studies (18); the stress imposed on the proximal aorta is higher than the distal abdominal aorta thereafter. Hence, the Cauchy stress becomes heterogeneous along the length of the aorta during postnatal growth and development.

Tendency for strain homeostasis. The present data, in conjunction with a recent study by Guo and Kassab (11) on mice 10 wk of age, can be used to explore the issue of mechanical homeostasis. Our data show a rapid (3- to 4-fold) increase of the circumferential Cauchy stress in the first 30 days of age (Fig. 6B). The change in stress at 10 wk compared with 30 days appears significant (mean of 302 ± 70.4 and 198 ± 41.4 kPa, respectively). Hence, the circumferential stress continues to increase. The circumferential elastic modulus of the mouse aorta increases gradually from the time of birth and reaches a relatively constant value after 2 wk of age. These results suggest that the aorta becomes stiffer with development, with stiffness of abdominal > thoracic aorta. This is consistent with the structural remodeling observed in the microstructure described earlier. The modulus also continues to increase from 30 days to 10 wk, although the change is not statistically significant (mean of 44.9 ± 5.4 and 82.9 ± 22.9 kPa, respectively). The strain, however, is unchanged at 10 wk relative to that at 30 days (mean of 1.3 ± 0.26 and 1.2 ± 0.11, respectively). Indeed, the circumferential Green strain of the mouse aorta reached the adult value at the age of 2 wk. The tendency to reach a uniform strain is remarkable.

The WSS is at birth significantly higher than physiological values (10–20 dyn/cm2) and decreases linearly during development. This is certainly a strong stimulus for the remodeling of the lumen of the aorta. Interestingly, the WSS is essentially normalized at 30 days (mean of 23 vs. 20 dyn/cm2). In conclusion, it appears that the circumferential strain and WSS normalize faster than the circumferential stress. Hence, the WSS and strain appear to attain their homeostatic values early in life.

The finding that strain may be a homeostatic mechanical parameter is in agreement with the findings of Guo and Kassab (12). They recently determined the distribution of circumferential stress and strain along the porcine aorta and throughout the coronary arterial tree. They showed that the stretch ratio (circumference of the artery at physiological loading relative to the zero-stress state) and stress varied from 1.2–1.6 and 10–150 kPa, respectively, along the aorta and the entire LAD arterial tree (more than 3 orders of magnitude difference in vessel diameters). The relative uniformity of strain (50% variation) from the proximal aorta to a 10-µm arteriole implies that the vascular system closely regulates the degree of deformation. Additional studies have shown that the circumferential strain (computed in reference to the zero-stress state) responds faster and recovers more quickly than the circumferential stress in pressure overload and flow overload models (23, 29). The homeostasis of strain has important implications for mechanotransduction and for vascular growth and remodeling.

Implications. The aorta grows and remodels in the circumferential, axial, and radial directions during normal development. Although the aorta is a relatively uniform organ geometrically and mechanically at birth, it becomes transformed into a tapering organ with varying mechanical properties along its length within the first 30 days of birth in the mouse model. The structural and mechanical remodeling is consistent with the functional adaptation of the aorta during development. Furthermore, it appears that strain attains its homeostatic values earlier than other mechanical parameters. In addition to the foregoing implications, the present data will serve as a physiological reference state for understanding pathological change in this transgenic model.


    GRANTS
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 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 
This research was supported in part by National Science Foundation Grant 9978199 and by National Heart, Lung, and Blood Institute Grant 2 R01 HL-055554-06.


    FOOTNOTES
 

Address for reprint requests and other correspondence: G. S. Kassab, Dept. of Biomedical Engineering, Univ. of California, Irvine, 204 Rockwell Engineering Center, Irvine, CA 92697-2715 (e-mail: gkassab{at}uci.edu)

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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 ABSTRACT
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 REFERENCES
 

  1. Berry CL, Greenwald SE, and Rivett JF. Static mechanical properties of the developing and mature rat aorta. Cardiovasc Res 9: 669–678, 1975.[Web of Science][Medline]
  2. Cox RH, Jones AW, and Fischer GM. Carotid artery mechanics, connective tissue, and electrolyte changes in puppies. Am J Physiol 227: 563–568, 1974.[Free Full Text]
  3. Davis EC. Elastic lamina growth in the developing mouse aorta. J Histochem Cytochem 43: 1115–1123, 1995.[Abstract]
  4. Dobrin P, Canfield T, and Sinha S. Development of longitudinal retraction of carotid arteries in neonatal dogs. Experientia 31: 1295–1296, 1975.[CrossRef][Web of Science][Medline]
  5. Duch BU, Andersen HL, Smith J, Kassab GS, and Gregersen H. Structural and mechanical remodeling of the common bile duct during experimental obstruction. Neurogastroenterol Motil 14: 111–122, 2002.[CrossRef][Web of Science][Medline]
  6. Dunn T. Spontaneous lesions of mice. In: The Pathology of Laboratory Animals, edited by Rilein WE and McCoy JR. Springfield, IL: Thomas, 1965, p. 303–329.
  7. Fischer GM and Llaurado JG. Collagen and elastin content in canine arteries selected from functionally different vascular beds. Circ Res 19: 394–399, 1966.[Abstract/Free Full Text]
  8. Fung YC and Liu SQ. Change of residual strains in arteries due to hypertrophy caused by aortic constriction. Circ Res 65: 1340–1349, 1989.[Abstract/Free Full Text]
  9. Fung YC and Liu SQ. Change of zero-stress state of rat pulmonary arteries in hypoxic hypertension. J Appl Physiol 262: 2455–2470, 1992.
  10. Fung YC. Biomechanics: Motion, Flow, Stress, and Growth. New York: Springer Verlag, 1990, p. 384–394.
  11. Guo X and Kassab GS. Variation of mechanical properties along the length of the aorta in C57bl/6 mice. Am J Physiol Heart Circ Physiol 285: H2614–H2622, 2003.[Abstract/Free Full Text]
  12. Guo X and Kassab GS. Distribution of stress and strain along the porcine aorta and coronary arterial tree. Am J Physiol Heart Circ Physiol 286: H2361–H2368, 2004.[Abstract/Free Full Text]
  13. Heymann MA, Iwamoto HS, and Rudolph AM. Factors affecting changes in the neonatal systemic circulation. Annu Rev Physiol 43: 371–383, 1981.[CrossRef][Web of Science][Medline]
  14. Kassab GS, Gregersen H, Nielsen SL, Liu X, Tanko L, and Falk E. Remodeling of the coronary arteries in supra-valvular aortic stenosis. J Hypertens 20: 2429–2437, 2002.[CrossRef][Web of Science][Medline]
  15. Katsuda S, Waki H, Yamasaki M, Nagayama T, O-Ishi H, Katahira K, Machida N, Hasegawa M, and Shimizu T. Postnatal changes in the rheological properties of the aorta in Sprague-Dawley rats. Exp Anim 51: 83–93. 2002.[CrossRef][Web of Science][Medline]
  16. Langille BL. Remodeling of developing and mature arteries: endothelium, smooth muscle and matrix. J Cardiovasc Pharmacol 21: S11–S17, 1993.[Web of Science][Medline]
  17. Langille BL. Blood flow-induced remodeling of the artery wall. In: Flow-Dependent Regulation of Vascular Function, edited by Bevan JA, Kaley G, and Rubanyi G. New York: Oxford University Press, 1995, p. 277–299.
  18. Langille BL, Brownlee RD, and Adamson SL. Perinatal aortic growth in lambs-relation to blood-flow change at birth. Am J Physiol Heart Circ Physiol 259: H1247–H1253, 1990.[Abstract/Free Full Text]
  19. Laurent S. Arterial wall hypertrophy and stiffness in essential hypertensive patients. Hypertension 26: 355–362, 1995.[Abstract/Free Full Text]
  20. Leuenberger HG and Kunstyr I. Gerontological data of C57BL/6J mice. I. Sex differences in survival curves. J Gerontol 2: 157–162, 1975.
  21. Liu SQ and Fung YC. Relationship between hypertension, hypertrophy, and opening angle of zero-stress state of arteries following aortic constriction. J Biomech Eng 111: 325–335, 1989.[Medline]
  22. Lu X, Yang J, Zhao JB, Gregersen H, and Kassab GS. Shear modulus of coronary arteries: Contribution of media and adventitia. Am J Physiol Heart Circ Physiol 285: H1966–H1975, 2003.
  23. Lu X, Zhao JB, Wang GR, Gregersen H, and Kassab GS. Remodeling of the zero-stress state of the femoral artery in response to flow-overload. Am J Physiol Heart Circ Physiol 280: H1547–H1559, 2001.[Abstract/Free Full Text]
  24. Marchii M and Becker AE. Morphologic features of the normal aortic arch in neonates, infants, and children pertinent to growth. Ann Thorac Surg 64: 511–515, 1997.[Abstract/Free Full Text]
  25. Matsumoto T and Hayashi K. Mechanical and dimensional adaptation of rat aorta to hypertension. J Biomech Eng 116: 278–283, 1994.
  26. Mattson DL. Comparison of arterial blood pressure in different stains of mice. Am J Hypertens 14: 405–408, 2001.[CrossRef][Web of Science][Medline]
  27. Olivetti G, Anversa P, Melissari M, and Loud AV. Morphometric study of early postnatal development of the thoracic aorta in the rat. Circ Res 47: 417–424, 1980.[Abstract/Free Full Text]
  28. Ping L, Sur SH, Mistlberger RE, and Morris M. Circadian blood pressure and heart rate rhythms in mice. Am J Physiol Regul Integr Comp Physiol 276: R500–R504, 1999.[Abstract/Free Full Text]
  29. Quang D, Gregersen H, Duch B, and Kassab GS. Indicial response of growth and remodeling of common bile duct post obstruction. Am J Physiol Gastrointest Liver Physiol 286: G420–G427, 2004.
  30. Russell ES and Meier H. Constitutional diseases. In: The Biology of the Laboratory Mouse (2nd ed.), edited by Green EL. New York: Dover, 1966, p. 571–587.
  31. Saini A, Berry C, and Greenwald S. Effect of age and sex on residual stress in the aorta. J Vasc Res 32: 398–405, 1995.
  32. Silver FH, Christiansen DL, and Buntin CM. Mechanical properties of the aorta: a review. Crit Rev Biomed Eng 17: 323–358, 1989.[Web of Science][Medline]
  33. Wells SM, Langille BL, and Adamson SL. In vivo and in vitro mechanical properties of the sheep thoracic aorta in the perinatal period and adulthood. Am J Physiol Heart Circ Physiol 274: H1749–H1760, 1998.[Abstract/Free Full Text]
  34. Wells SM, Langille BL, Lee JM, and Adamson SL. Determinants of mechanical properties in the developing ovine thoracic aorta. Am J Physiol Heart Circ Physiol 277: H1385–H1391, 1999.[Abstract/Free Full Text]
  35. Wiesmann F, Ruff J, Hiller KH, Rommel E, Haase A, and Neubauer S. Developmental changes of cardiac function and mass assessed with MRI in neonatal, juvenile, and adult mice. Am J Physiol Heart Circ Physiol 278: H652–H657, 2000.[Abstract/Free Full Text]
  36. Wong LC and Langille BL. Developmental remodeling of the internal elastic lamina of rabbit arteries: effect of blood flow. Circ Res 78: 799–805, 1996.[Abstract/Free Full Text]
  37. Zhang W, Herrera C, Atluri SN, and Kassab GS. The effect of longitudinal pre-stretch and radial constraint on the stress distribution in the vessel wall: a new hypothesis. Mech Chem Biosystems 2: 41–52, 2005.



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