Vascular Biology |
From the Laboratoire de Pharmacologie Cardiovasculaire (V.M., P.K., I.L.-I., J.A.), Faculté de Pharmacie, Université Henri Poincaré-Nancy, Nancy, France, and the Brookdale Center in the Department of Biochemistry and Molecular Biology (B.G., F.R.), Mount Sinai School of Medicine, New York, NY.
Correspondence to Jeffrey Atkinson, Laboratoire de Pharmacologie Cardiovasculaire, EA 3116, Faculté de Pharmacie de lUniversité Henri Poincaré, Nancy I, 5 rue Albert Lebrun, 54 000 Nancy, France. E-mail atkinson{at}pharma.u-nancy.fr
| Abstract |
|---|
|
|
|---|
Key Words: fibrillin-1 elastic modulus aneurysm desmosines elastic fibers
| Introduction |
|---|
|
|
|---|
Early ideas were based on the regulatory role played by microfibrils in the organized deposition of tropoelastin molecules during elastogenesis.3 It was suggested that FBN1 mutations prevented normal cross-linking (formation of desmosine cross-bridges), leading to disorganized microfibrillar assembly, and that this weakened the mechanical strength of the media. This hypothesis was recently challenged by homologous gene-targeting experiments in the mouse,4 which indicated that FBN1 microfibrils were predominantly engaged in global tissue homeostasis rather than in elastic matrix assembly. Studies performed on mgR/mgR mice, which are characterized by a hypomorphic mutation of FBN1,5 suggested that aortic dilatation was due to the failure by the microfibrillar array of the adventitia to sustain wall integrity in the face of hemodynamic stress. The resulting increase in wall stress is associated with localized calcium deposition, macrophage infiltration, and metalloproteinase release in the media, leading to fragmentation of the medial elastic network and aortic dilatation.
The present study is an attempt to distinguish between these 2 mechanisms: a defect in early elastogenesis or later fragmentation of elastic fibers, in mgR/mgR mice underexpressing FBN1.5 The content of desmosine plus isodesmosine, cross-linking amino acids specific to elastin, was used as an index of early elastogenesis, and fragmentation of elastic fibers was analyzed by histomorphometry.
It has also been suggested that pulse pressure is a major determinant of dilatation in patients with Marfan syndrome.6 Were fragmentation of the medial elastic network to occur in this Marfan model, then the aortic wall would stiffen, as previously reported in studies evaluating the impact of elastases7 or elastocalcinosis.8 A loss of aortic wall elasticity would lead to increased cyclic stress and pulse pressure, thereby amplifying aortic dilatation.
In the present work, we simultaneously evaluated changes in aortic mechanics and geometry. Elasticity of the aortic wall was estimated from the thoracoabdominal pulse wave velocity at baseline (a pressure-dependent index of wall elasticity) and at steady-state levels of mean arterial pressure after controlled hypotension (the slope of the pulse wave velocitypressure curve being used as a pressure-independent index of elasticity). Baseline elastic modulustowall stress ratio was used as a pressure- and geometry-independent index of elasticity.
| Methods |
|---|
|
|
|---|
Aortic Pulse Wave Velocity in
Nonanesthetized Mice
Polyethylene cannulas (intravascular portion
0.61 mm/0.32 mm, outer diameter/inner diameter; extravascular
portion 0.96 mm/0.58 mm) were chronically implanted in the
mice under pentobarbital anesthesia (80 mg/kg IP) into the
descending aorta (1 mm below the carotid ostium), the abdominal
aorta (3 mm above the iliac bifurcation), and the abdominal vena
cava (3 mm above the iliac bifurcation). Twenty-four hours later,
the aortic cannulas of the nonanesthetized, freely moving mice
were filled with heparinized (5 UI/mL), gas-free, 0.15 mol/L NaCl and
connected to low-volume pressure transducers
(Baxter, Bentley Laboratories Europe) with 15 cm
of polyethylene cannula.
Signal analysis has been described in detail previously.7 9 After a 30-minute habituation period, baseline parameters were determined beat-to-beat and averaged over periods of 4 seconds every 30 seconds for 30 minutes, at a sampling rate of 256 Hz. An algorithm detected the maximal and minimal values of each pressure signal and calculated central mean aortic blood pressure (CMABP; mm Hg) from the waveform area, pulse pressure as the diastolic-systolic difference, and heart rate (beats per minute) by counting the number of cycles over the 4-second period.
Pulse wave velocity (cm/s) was calculated as the distance between the 2 cannula tips (measured in situ after postmortem fixation by sticking a damp cotton thread onto the aorta: 4.6±0.2 cm in mgR/mgR and 4.3±0.2 cm in wild-type mice; P=0.3180) divided by transit time. Transit times (ms) were measured online for each 4-second period (38 heart beats, 3 to 4 respiratory cycles) by an algorithm that systematically shifted in time the peripheral pressure waveform with respect to the central pressure waveform and then determined the value of the time shift giving the highest correlation.7 This approach is based on a least-squares analysis of the differences in amplitudes of the central and peripheral pressure signals at a given point in time; the analysis was repeated following increments in the peripheral sampling points and creating intermediate points by linear interpolation. The calculated resolution of the transit time measurement was ±0.39 ms, ie, ±7% error for a wave traveling at 835 cm/s in mgR/mgR mice and ±4% error for a wave traveling at 440 cm/s in wild-type mice. The ratio of pulse wave velocity to the CMABP ratio was used as a pressure-independent index of elasticity.
Pulse Wave VelocityPressure Curves During
Pharmacological Hypotension in Nonanesthetized Mice
After baseline hemodynamic
measurements were made, CMABP was reduced in a stepwise fashion
(10 mm Hg per step) to half its initial value by progressively
increasing the infusion rate of a sodium nitroprusside solution
(2.3 mmol/L in 10 mmol/L phosphate buffer, pH 7.4 at 25°C;
Sigma Chemical
Co).9 At each
stabilized step, 15 measurements of aortic blood pressure and transit
time were performed and averaged. By the end of infusion, animals had
received a volume <8% of their total blood volume; the mean dose of
sodium nitroprusside in mgR/mgR and wild-type mice was 979±167 and
442±117 nmol · kg-1 ·
min-1, respectively
(P for the group, 0.0223 by
1-way ANOVA). For each mouse, pulse wave velocity
(y) was expressed as a function
of CMABP (x) by using an exponential model:
y=b · eax.9
Slopes (a) and intercepts
(b) of the pulse wave
velocitypressure curves were treated as independent,
parametric variables and averaged. Slopes were used as a
pressure-independent index of elasticity.
Descending Thoracic Aorta Geometry, Wall
Stress, Elastic Modulus, and Elastic Fiber Network
Fragmentation
At the end of the hypotension protocol, the sodium
nitroprusside infusion was stopped; the mice were humanely killed with
a sodium pentobarbital overdose and perfused for 15 minutes at their
baseline CMABP with 10% formol containing phosphate-buffered saline. A
0.5-cm-long sample of the proximal descending thoracic aorta
(downstream from the aortic arch) was excised, immersed in 10% formol,
dehydrated in graded ethanol solutions, and embedded in paraffin.
Sections (10 µm thick) stained with Weigerts solution were used for
measurement of internal diameter and medial thickness and for
determination of the degree of elastic network fragmentation (see
below). Morphometric analysis was performed using the
Saisam® algorithm (Microvision Instruments);
each section was examined twice in a blinded fashion. Medial
cross-sectional area (mm2) was calculated as
/4 ·
(Do2-Di2),
where Do
and Di
are the outer and inner diameters (mm), with
Di
delimited by the internal elastic lamina, such that
Do=Di+2h,
where h is media thickness
defined as the distance between internal and external elastic laminae
(mm).
Elastic modulus and circumferential wall stress
(106 dyn/cm2)
were calculated from the Moens-Korteweg or Lamé equations, which
correct pulse wave velocity (PWV; elastic modulus) or CMABP (wall
stress) by internal diameter
(Di) and
medial thickness (h): elastic
modulus=([PWV]2 ·
Di ·
)/h and wall stress=(CMABP
·
Di)/2h,
where PWV was measured in nonanesthetized mice (cm/s),
Di=internal
diameter (as above; cm),
h=medial thickness (cm),
=blood density (1.05 g/mL), and
CMABP=(dyn/cm2).
The elastic modulustowall stress ratio was used as an index of wall elasticity, which is independent of intravascular pressure and aortic morphology. Elastic network fragmentation was evaluated by measuring the number of medial elastic segments per square millimeter and the percentage of medial surface occupied by elastic fibers (excluding the external and internal laminae).
Calcium, Elastin Cross-Linking, and Collagen
Contents of the Aorta
A second 1-cm-long sample of the thoracic aorta was
excised and the wall calcium content determined by atomic absorption
spectrophotometry (AA10, Varian Ltd) after
mineralization and HNO3
digestion.10 The remaining
abdominal end of the aorta was removed, weighed, and hydrolyzed in HCl
(6 mol/L, 24 hours at 105°C). Protein content (mg/g wet weight) was
determined by the dinitrofluorobenzene reaction by using a value of 92
for the molecular weight of an amino
acid.11 Collagen content
(mg/g wet weight) was determined by the chloramine T and
paradimethylaminobenzaldehyde reaction as hydroxyproline content
multiplied by 7.46.11
Desmosine and isodesmosine contents were determined by capillary zone
electrophoresis.12
Statistics
Values are given as mean±SEM. Because 2-way ANOVA
(sex, age) gave probability levels >0.05 for age, sex, and agexsex,
we pooled the results from different age groups and both sexes.
Differences between groups were evaluated by 1-way ANOVA plus the
Bonferroni test. A value of
P<0.05 was chosen as being
indicative of statistical
significance.
| Results |
|---|
|
|
|---|
|
|
|
Descending Thoracic Aorta Geometry, Wall
Stress, Elastic Modulus, Elastic Network Fragmentation, and Wall
Composition
Internal diameter (+27%,
P<0.05) and medial
cross-sectional area (+36%,
P<0.05) were greater in
mgR/mgR mice (outward hypertrophic remodeling). Wall stress was not
significantly different in mgR/mgR mice, but there were substantial
increases in elastic modulus (4-fold,
P<0.05) and the elastic
modulustowall stress ratio (4-fold,
P<0.05)
(Table 3
). The elastic network was highly fragmented in
mgR/mgR mice
(Figure 2
), as revealed by a substantial increase in the
number of medial elastic segments (+75%) and a decrease in the
percentage of medial surface occupied by elastic fibers (-40%,
Table 3
).
|
|
There were significant, negative linear relations between
dilatation (ie, internal diameter, a dependent variable) and the
percentage of medial surface occupied by elastic fibers (an independent
variable; slope=-2.7±0.2 mm,
r2=0.982,
P=0.0010;
intercept=1.3±0.1 mm,
P<0.0001) as well as between
wall stiffness (ie, elastic modulus, a dependent variable) and the
percentage of medial surface occupied by elastic fibers (an independent
variable; slope=-161±33 106
dyn/cm2,
r2=0.887,
P=0.0167; intercept=49±6
106 dyn/cm2,
P=0.0047) in mgR/mgR but not in
wild-type mice. Desmosine content was similar in mgR/mgR and wild-type
mice
(Table 3
), as were protein, collagen, and calcium contents.
There was no significant correlation between aortic dilatation and wall
desmosine content (P>0.05;
results not shown).
| Discussion |
|---|
|
|
|---|
Defects in Early Elastogenesis or Later
Fragmentation of the Medial Elastic Network?
Early hypotheses explaining why an FBN1 deficiency
leads to aneurysm in Marfan patients were based on the
regulatory role played by microfibrils in the organized deposition of
tropoelastin molecules during
elastogenesis.3 It was
suggested that FBN1 mutations
prevented the normal formation of desmosine cross-bridges and that this
weakened the mechanical strength of the media. Elastin expression and
its organization into insoluble polymers after formation of desmosine
cross-bridges are largely confined to the perinatal period. In mice
hemizygous for the elastin gene (ELN+/-), a
transgenic model for alterations of this early period of elastic fiber
formation, there is a paradoxical increase in the number of elastic
lamellae, and therefore, arterial compliance at
physiological pressures remains
normal.13 The authors
suggested that reduced elastin mRNA expression, together with thinning
and reduced extensibility of elastic lamella during gestation,
stimulated the synthesis of new elastic lamellae. Were this early
period of elastogenesis to be affected in our mgR/mgR model (by means
of a defect in desmosine cross-linking?), then a similar compensatory
increase in elastic lamellae synthesis might also occur, thereby
maintaining aortic wall elastic properties. This is not the case,
suggesting that in the mgR/mgR mouse, fragmentation of the elastic
fibers occurs later in life when lamellar structure is already
established.
This conclusion (later fragmentation of elastic fibers leading to functional abnormalities of the aorta, dilatation, and stiffening) is based on histological analysis and on the lack of difference in desmosine content between mgR/mgR and wild-type mice. Because the sensitivity and reproducibility of the method used to measure desmosine content (capillary zone electrophoresis) are very high (1 ng and <5%, respectively12 ), the possibility cannot be excluded that the small differences observed in desmosine content between groups (432±31 vs 492±42 ng/mg, or -14%) would reach statistical significance with larger numbers of animals; however, the difference will probably remain tenuous. In another model of stiffening of the aortic wall (the VDN rat model) with the same degree of wall stiffening as that observed in the mgR/mgR mouse, fragmentation of elastic fibers (induced by elastocalcinosis8 14 ) is associated with a severe and statistically significant fall in desmosine content (-50%). Overall, these observations suggest that changes in absolute amounts of desmosine (even if they were statistically significant) are not highly involved in the functional abnormalities of the aorta in mgR/mgR mice.
Medial Elastic Network Fragmentation and
Aortic Stiffening
The increase in pulse wave velocity and the slope of
the relation between pulse wave velocity and distending intraluminal
pressure or wall stress suggest that elastic fiber fragmentation leads
to increased wall stiffness in mgR/mgR mice. This hypothesis depends on
the veracity of pulse wave velocity as an index of wall stiffness.
Although the method that we used for the measurement of aortic pulse
wave transit time has been extensively verified in the
rat,7 9 use of this
technique in the mouse could be complicated by several
factors.
First, the frequency response of the cannula plus transducer system is lower in the mouse than in the rat. Although this characteristic will modify the harmonic composition of the waveform, it will presumably be of less importance because our algorithm compares whole waveforms rather than in other systems, which compare specific points on the waveform (wavefront or the "foot" of the initial diastolic-systolic pulse). Furthermore, because identical cannulas were used at the central and peripheral sites, distortion of the 2 signals will be the same. In a separate experiment performed on anesthetized adult OF1 mice, differences in transit time measured with polyethylene cannulas (n=3) or Millar Mikro-Tip pressure transducers (1.4+f, SPR-671, Millar Instruments; n=3) were not significantly different (Mikro-tip transducers: 0.084±0.002 ms/mm Hg, n=78 observations; cannulas: 0.086±0.001 ms/mm Hg, n=75 observations; P=0.4086).
A second factor that may be of concern is the higher heart rate of the mouse compared with that of the rat. Here again, this difference will change the harmonics of the waveform and could theoretically modify wave transmission. However, because baseline heart rate and reflex tachycardia after hypotension (results not shown) were not statistically different in the 2 groups, this factor should not be important.
A third factor is the smaller aortic length in the mouse than in the rat, which may increase the error of measurement of pulse wave transit time and require a compensatory increase in sample rate. However, our algorithm creates intermediate points by linear interpolation, thus allowing sample resolution to be increased 10-fold. In the present experiment at 256 Hz, the percent error for measurement of transit time was 4% to 7%. In a separate experiment, transit times measured at 256 or 1024 Hz were not different (anesthetized adult OF1 mice, n=5, polyethylene cannulas, 100 to 110 mm Hg: 12.6±1.2 ms at 256 Hz and 11.7±0.3 ms at 1024 Hz, P>0.05; at 130 to 140 mm Hg: 5.8±0.8 ms at 256 Hz and 4.6±0.3 ms at 1024 Hz, P>0.05). On the basis of these methodological experiments, we conclude that the 4-fold increase in wall stiffness in mgR/mgR mice is not artifactual.
Although aortic stiffening in mgR/mgR mice is probably primarily related to medial elastic network fragmentation, other factors have to be considered. Fibrillin is involved in calcium fixation,15 and it is known that diffuse calcification of the arterial wall makes it stiffer.14 In our experiment, the total calcium content of the descending aorta was not increased in mgR/mgR mice, thus excluding diffuse calcification as an important determinant of aortic stiffening in this model. However, this does not exclude a role for focal aortic wall calcification in the inflammation process observed in the early stages of aortic aneurysmal dissection.5 Collagen content did not change in the aortic wall of mgR/mgR mice, thus excluding fibrosis as a mechanism of aortic stiffening. Aortic smooth muscle tone, which may modify wall stiffness,16 cannot be entirely ruled out, because the induced hypotension in mgR/mgR mice required a vasodilator dose twice as high as that required in wild-type mice. In the rat, however, we have previously shown that aortic vasomotion is of minor importance in the determination of aortic wall mechanics.17
Whether aortic stiffening per se participates in aortic dilatation remains to be elucidated, and several aspects need to be investigated and discussed. First, the method for determining aortic dimensions by fixation and dehydration may induce tissue shrinkage. However, because fixation was performed in situ and before the aorta was isolated and dissected free from the surrounding tissue, shrinkage was probably minimal and uniform within samples and likely did not dramatically influence the calculated values for mechanical parameters. Second, some authors have concluded that aortic dilatation and wall stiffness evolve independently,18 19 whereas others have shown that the increase in central pulse pressure (resulting from stiffening of the aortic wall) is a major determinant of aortic diameter6 in Marfan syndrome. Central pulse pressure increased in mgR/mgR mice; although all of the determinants of pulse pressure were not measured in the present studyand it would be appropriate to normalize the measured pulse pressures for differences in stroke volumethis increase in pulse pressure is more dependent on the 4-fold increase in aortic wall stiffness than on any increase in stroke volume. This suggests that, as in Marfan syndrome,6 the fatiguing effect of cyclic wall stress is more important than that of steady stress for elastic fiber fragmentation and aortic dilatation in mgR/mgR mice. In Marfan patients, elastic fiber degradation is most prominent in the cardiac valves and thoracic aorta, where elastic fibers may be subjected to the most severe mechanical stresses.20 Finally, the latter authors showed that elastic fiber fragmentation occurred in association with an upregulation of the synthesis of metalloproteinases and probably with an increased susceptibility to metalloproteinase activity of the elastin formed in the presence of the defect in FBN1.20 Therefore, after inflammation and macrophage infiltration of the aortic wall, as has been shown in mgR/mgR mice,5 a stress-dependent and/or stress-independent activation of metalloproteinases may also participate in elastolysis.
In conclusion, underexpression of FBN1 in mice leads to severe elastic network fragmentation, with no change in elastin cross-linking. Subsequently, the aorta dilates and the wall stiffens. These results suggest that medial elastic fiber fragmentation and not defects in early elastogenesis is the major determinant of aortic dilatation and stiffening in Marfan syndrome.
When attempting to extrapolate the above data to humans, it must be borne in mind that there are dramatic differences in aortic geometry, heart rate, pressures, and time course. We observed marked dilatation in the mgR/mgR mouse with no decrease in medial thickness or wall collagen content. Because vascular wall integrity depends on collagen,7 which is mainly located in the adventitia, it has been suggested that aneurysm occurs in humans once destruction of adventitial collagen occurs (after medial necrosis). Further studies on the evolution in time of the relative roles of the media and adventitia are required.
| Acknowledgments |
|---|
Received January 3, 2001; accepted April 13, 2001.
| References |
|---|
|
|
|---|
This article has been cited by other articles:
![]() |
H Senzaki, Y Iwamoto, H Ishido, T Matsunaga, M Taketazu, T Kobayashi, H Asano, T Katogi, and S Kyo Arterial haemodynamics in patients after repair of tetralogy of Fallot: influence on left ventricular after load and aortic dilatation Heart, January 1, 2008; 94(1): 70 - 74. [Abstract] [Full Text] [PDF] |
||||
![]() |
R. Jesudason, L. Black, A. Majumdar, P. Stone, and B. Suki Differential effects of static and cyclic stretching during elastase digestion on the mechanical properties of extracellular matrices J Appl Physiol, September 1, 2007; 103(3): 803 - 811. [Abstract] [Full Text] [PDF] |
||||
![]() |
A. W.Y. Chung, K. Au Yeung, G. G.S. Sandor, D. P. Judge, H. C. Dietz, and C. van Breemen Loss of Elastic Fiber Integrity and Reduction of Vascular Smooth Muscle Contraction Resulting From the Upregulated Activities of Matrix Metalloproteinase-2 and -9 in the Thoracic Aortic Aneurysm in Marfan Syndrome Circ. Res., August 31, 2007; 101(5): 512 - 522. [Abstract] [Full Text] [PDF] |
||||
![]() |
H. I. Ha, J. B. Seo, S. H. Lee, J.-W. Kang, H. W. Goo, T.-H. Lim, and M. J. Shin Imaging of Marfan Syndrome: Multisystemic Manifestations RadioGraphics, July 1, 2007; 27(4): 989 - 1004. [Abstract] [Full Text] [PDF] |
||||
![]() |
V. Gaillard, D. Casellas, C. Seguin-Devaux, H. Schohn, M. Dauca, J. Atkinson, and I. Lartaud Pioglitazone Improves Aortic Wall Elasticity in a Rat Model of Elastocalcinotic Arteriosclerosis Hypertension, August 1, 2005; 46(2): 372 - 379. [Abstract] [Full Text] [PDF] |
||||
![]() |
S. Laurent, P. Boutouyrie, and P. Lacolley Structural and Genetic Bases of Arterial Stiffness Hypertension, June 1, 2005; 45(6): 1050 - 1055. [Abstract] [Full Text] [PDF] |
||||
![]() |
L. D. Black, K. K. Brewer, S. M. Morris, B. M. Schreiber, P. Toselli, M. A. Nugent, B. Suki, and P. J. Stone Effects of elastase on the mechanical and failure properties of engineered elastin-rich matrices J Appl Physiol, April 1, 2005; 98(4): 1434 - 1441. [Abstract] [Full Text] [PDF] |
||||
![]() |
S. Chai, Q. Chai, C. C. Danielsen, P. Hjorth, J. R. Nyengaard, T. Ledet, Y. Yamaguchi, L. M. Rasmussen, and L. Wogensen Overexpression of Hyaluronan in the Tunica Media Promotes the Development of Atherosclerosis Circ. Res., March 18, 2005; 96(5): 583 - 591. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. Del Campo Aortic insufficiency in patients with Marfan syndrome: A surgical dilemma J. Thorac. Cardiovasc. Surg., January 1, 2004; 127(1): 303 - 304. [Full Text] [PDF] |
||||
![]() |
R. A. Bleasdale, K. H. Parker, and C. J. H. Jones Chasing the wave. Unfashionable but important new concepts in arterial wave travel Am J Physiol Heart Circ Physiol, June 1, 2003; 284(6): H1879 - H1885. [Full Text] [PDF] |
||||
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
|
ATVB Home | Subscriptions | Archives | Feedback | Authors | Help | AHA Journals Home | Search Copyright © 2001 American Heart Association, Inc. All rights reserved. Unauthorized use prohibited. |