bio mechanics of human common carotid artery and design
TRANSCRIPT
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
1/9
Biomechanics of human common carotid artery and designof novel hybrid textile compliant vascular grafts
B. S. Gupta1,* and V. A. Kasyanov1,2
1College of Textiles, Department of Textile Engineering, Chemistry, and Science, North Carolina State University,
Raleigh, N orth Carolina 27695-8301; 2 Laboratory of Biomechanics, Riga Technical University, Riga, LV-1658, Latvia
The mechanical properties and structure of a human com-mon carotid artery were stud ied in order to d evelop criteriafor designing and manu facturing comp liant textile vasculargrafts. The arterial w all comprised a comp osite of elastinand collagen fibers w ith the collagen fibers crimp ed. Thisstructure led to a unique pressurecircumferential stretchratio curve, the slope of which increased with an increase instrain. The increase in slope was particularly rapid at a
stretch ratio above 1.4 or pressure above 120 mmHg. Basedon the knowledge gained, a criteria for the design of biome-chanically compliant arterial grafts was developed. An elas-tomeric prestretched p olyurethane monofilament yarn witha low modulus of elasticity and a bulked polyester multi-
filament yarn with a high modulus of elasticity were com-bined and used as threads in the manufacture of grafts. Tu-bular structures of diameters in the range 46 mm weremad e by weaving. Transverse compliance and morphologi-cal and permeability properties of these grafts were deter-mined and compared with those of a currently availablewoven commercial grafts and hum an carotid arteries. Re-sults indicated that the compliance values of the hybrid
grafts were comparable with those of the human carotidartery. Preliminary in vivo studies in dogs showed promis-ing results: a thin, stable neointima developed within 6months of implantation on the flow surface. 1997 JohnWiley & Sons, Inc.
INTRODUCTION
The design and fabrication of synthetic vascular
grafts has been a challenging area in vascular surgicalresearch during the past 30 years. Large diameter
grafts (diameter 6 m m) u sed for bypassing arteries in
high flow regions such as the thoracic and abdom inal
aorta have generally performed well. However, the
replacement with grafts of small diameter arteries,
such as the coronary, renal, and carotid, has not yet
been successful and continues to be a problem in re-
constructive surgery. Efforts to develop vascular
grafts of diameters less than 6 mm with potential for
long-term patency have not yet met with success. A
major cause for poor performance of such grafts has
been shown to be the lack of comp liance.14
Replacement of small arteries by rigid woven or
knitted prostheses, which have little or no compliance
in the circum ferential direction, causes th e dam pen ing
out of the higher harmonic in the pulse wave5 that
leads to an increase in the pulse wave velocity and
therefore to an increase in wave reflection and energy
loss. The extent to which the pulse amplitude is damp-
ened depends upon the length of the rigid part. For
examp le, in a stud y by Womersly,5 a 15-cm long rigid
section inserted in the femoral artery of a dog showed
a redu ction of the amp litud e by about 13% in the first
and 42% in the fourth harmonic. This problem was
also noted and discussed by How and Clarke6 (1984).
Baird and Abbott7 and Rittgers et al.8 showed that
hemodynamic forces play an important role in the for-
mation of thrombus and hyperp lastic intima. Doo and
colleagues9 determined theoretically and experimen-
tally the differences in the behaviors of an elastic and
rigid tube used as a model for an aortic arch. The
resulting flow distributions examined showed a dif-
ference in the flow behaviors of the rigid and the elas-
tic mod els of the arterial system. The arterial w all elas-ticity had an effect on the blood flow distribution; a
lack of elasticity led to high turbulence. The work by
Stein et al.10 showed that for a given Reynolds nu mber
the intensity of turbulence was significantly lower in
compliant tubes than in rigid ones. In the latter, unfa-
vorable flow conditions led to the formation of anas-
tomotic aneurysm, development of hyperplastic neo-
intima, and failure of sutures or tearing of the host
artery.*To whom correspondence should be addressed.
Journal of Biomedical Materials Research, Vol. 34, 341349 (1997) 1997 John Wiley & Sons, Inc. CCC 0021-9304/ 97/ 030341-09
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
2/9
Clearly, successful d evelopm ent of a small diameter
vascular graft will depend not only on the use of new
biocomp atible m aterials but also on ideas of n ew con-
structions. Special attention has been devoted in re-
cent years to the use of polyurethanes, which have
good biocomp atibility11,12 and deform ational andstrength p roperties.6,1316 However, problems have
been encountered with the u se of sm all diam eter
grafts made exclusively of this material. The polymer
is found to creep, which leads to the development of
aneurysm. Thus, in spite of the availability of conve-
nient spray technology for manufacturing grafts with
such elastomers, interest in woven and knitted textile
grafts continues because the latter have been success-
ful in m edium and large caliber app lications, and su b-
stantial experience has been gained in th eir design and
construction du ring the past four decades.
1721
The literature makes it clear that mechanical char-
acteristics of vascular grafts play an important role in
governing long-term patency. Specifically, the most
important consideration to be given in d esigning a
graft is to match the m echanical prop erties of the pr os-
thesis with th ose of the host artery. Information exists
in the literature on the mechanical properties of the
arteries of animals, especially the dog.2226 The work
of Hayashi et al. and that of one of the present auth ors
(V.A.K.) and his associates2830 shed some light on the
properties of human blood vessels; however, more in-
sight is needed on the structure and properties of ar-teries before small diameter grafts with maximum po-
tential success can be engineered.
The objectives in the p resent work w ere to study the
structure and mechanical behavior of a human com-
mon carotid artery (CCA), and to use the information
in designing and constructing a compliant textile vas-
cular graft. The gr aft so constructed was composite in
structure an d characterized by nonlinear elasticity and
large transverse deformation. Animal studies con-
ducted with the grafts showed highly promising re-
sults.
MATERIALS AND METHODS
Mechanical properties and structure ofhuman CCA
Seven hu man CCAs, retrieved at the autopsies of
persons aged 2135 years, were used as experimental
materials. The vessels were marked with gentian vio-
let stain before resetting to identify the in situ axialextension ratio. After resection, the specimens were
stored in physiological salt solution until the mechani-
cal tests, conducted within 2 h, were performed. The
device used for these tests is shown in Figure 1. An
artery was cannulated at both ends. The sample was
placed in the chamber with the physiological salt so-
lution maintained at the temperature of 37 1C. One
end of the tube was clamped to a support to which a
pressure transdu cer (Micron Inst. M-15) and a spe-
cially designed inductive force transducer were con-
nected. The other end was clamped to a support to
which a pressure bottle containing fluid was con-
nected. The force transd ucer recorded the force neces-
sary to maintain the vessel at its in situ length. Axial
stretch w as introdu ced by a slide m echanism to w hich
the balance arm s w ere fixed. The axial deformation of
the artery was measured with a specially designed
inductive strain transdu cer connected to one of the
arms of the balance. Diameter changes in the specimen
were sensed optically with a video-dimensional ana-
lyzer coupled with a suitable lighting system for high
contrast. The changes in diameter with pressure were
tracked and recorded continuously.
An arterial samp le was gradu ally loaded by internal
pressure from 0 to 200 mmHg while maintaining thelength of the sample constant at L0, the length in situ.
The pressure was elevated in 20-mmHg steps with
pressure held constant in each step for 1 m in. The
initial external diameter a t inner p ressure p = 0 mmH g
a n d a t in situ axial length L0 was noted as D0. The
diameter D was recorded at each pressure level. The
value of wall thickness h was calculated as follows:
h = h0 3, (1)
where
3 =1
1 2, (2)
2 = (D/D0), (3)
an d
Figure 1. The schematic of the experimental device. 1,sample in chamber with a physiological solution; 2, force
transd ucer; 3, pressure tr ansd ucer; 4, TV camera; 5, displace-ment transd ucer; 6, stepper motor; 7, system for liquid feed-ing.
342 GUPTA AN D KASYAN OV
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
3/9
1 = (L/L0) = 1.0. (4)
In these equations, h0 is the initial thickness of the
specimen wall and 1, 2, and 3 are, respectively, the
stretch ratios in the axial, circumferential, and radial
directions. Because the length of the artery was main-tained constant at L0, the value of1 (=L/L0) was 1.
The initial wall thickness h0 was measured with a
cathetometer to 0.001 mm accuracy. The artery was
preconditioned before the tests by subjecting it to cy-
clic loading to bring it to a stable state, which would
give a more reproducible mechanical response. Dur-
ing this process the vessel was p ressurized from 0 to
200 mmH g in 20 mm Hg steps five times with pr essure
held constant for 1 m in at each step. The initial curves
were m arkedly hysteretic, but the th ird or fourth cycle
gave reproducible curves with minimal hysteresis.
The structure of the inner layers was studied after
sectioning under a JEM-100C scanning electron micro-
scope (SEM). For this the p rep ared section w as fixed in
3% glutaraldehyde for 8 h, postfixed in 1% osmium
tetroxide for 5 h, dehydrated in ethanol of increasing
concentration, and dried in a Japanese Eiko-Dh-I criti-
cal point apparatus. The dried section was coated in a
vacuum chamber with 5060 nm of gold and exam-
ined under an SEM with a ASJD-4D scanning attach-
ment at 40-kV accelerating voltage and 80030,000
magnification. Light microscopy (LM) w as used to
gain preliminary information about the constitutiveelements of the connective tissue. For the latter, the
samples were fixed in 10% formaldehyde (pH 7.0) and
then embedd ed in p araffin wax, sectioned in various
directions, and stained using hematoxylin-eosin. The
co ll ag e n fi be r s w e r e d y e d u s in g t h e v a n G is on
method, and the elastin fibers were dyed using the
Weigert method.
Manufacturing, mechanical properties, and
structure of composite textile grafts
The performances of textile comp osite vascular
grafts designed and constructed in this work and of
available commercial w oven grafts (CVG)1 (6-mm di-
ameter, woven structure m ade of 7 tex linear d ensity
polyester, North, St. Petersburg, Russia) were evalu-
ated. In ma nufacturing the former, textile threads w ith
two widely different deformative characteristics, one
nearly matching those of the elastin and the other of
the collagen fibers, were selected. The m aterials u sed
were a polyurethane monofilament yarn (VolgogradChemical Thread Plant, Volgograd, Russia) with a low
modulus of elasticity (0.8 MPa) and a bulked polyester
multifilament yarn (Mogilev Chemical Thread Plant,
Mogilev, Russia) with a high modulus of elasticity (1.4
102 MPa). Tubular grafts of diameters 46 mm were
made by a weaving process utilizing a foil ribbon
loom.
Two types of grafts were made. In the first type
(HVG-1), polyester threads of 9 tex linear density were
used as the warp (Fig. 2), and the same polyester and
a prestretched polyurethane (7.8 tex linear density)were used as the w eft. The stretch in the elastic thread
caused the crim p to d evelop in the weft threads,
which made the graft stretchable in the transverse di-
rection. In the second variant (HVG-2), prestretched
polyurethane thread combined with p olyester w as
used as both the warp and the weft. This combination
in the warp threads is novel in that the crimp, usually
introdu ced in the longitud inal direction by the tedious
process of crimping and heat setting in commercial
grafts, developed autom atically in this gra ft by d iffer-
ential shrinkage. The gr afts obtained were stretchableand thus compliant in both the transverse and the lon-
gitudinal directions.
The mechanical prop erties of the grafts so prod uced
were determined at pressures ranging from 0 to 200
mmHg by following the procedure described for the
carotid arteries. Five specimens of each type were
tested. A thin latex tube of diameter larger than those
of the grafts was inserted into the sp ecimen before the
fluid was passed and the graft pressurized. For deter-
mining hydraulic permeability, the procedure of Gui-
doin et al.31 was used. In this method, the volume of
water passing through the wall under a fixed hydro-static pressure of 120 mmHg was collected for 5 min
and expressed as milliliters per minute p er square cen-
timeter of water. The grafts were also examined u nd er
an SEM for their surface and pore characteristics.
Eight HVG-1 hybrid grafts were also implanted in
the carotid and femoral regions of mongrel dogs1 for
periods of up to 1 year. (In performing the in vivo
studies, the guidelines of the Scientific Councils of the
Latvian Academy of Sciences and Academy of Medi-
cine w ere followed.) The form of the pulse w ave
found in the graft, the healing characteristics of the
Figure 2. The structure of the hybr id textile vascular grafts:(a) the p olyester yarn and (b) the p olyurethane yarn.
343CAROTID ARTERY/ BIOMECHANICS AND NOVEL VASCULAR GRAFTS
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
4/9
surface, and the changes in the mechanical properties
as a result of implantation were examined.
Compliance and stiffness parameter
The flexibility and stiffness of arteries or grafts have
been frequently characterized by the values of com-
pliance,32 Cv, pressurestrain elastic modu lus,33 Ep ,
and stiffness parameter,27 . These parameters are de-
fined as follows:
Cv = (2/ De) (De/P); (5)
Ep = De (P/De); (6)
ln (P/Ps) = (D/Ds 1). (7)
In these De is the external diameter at 80 mm Hg, P
is the pressure difference (12080 mm Hg) over wh ich
measurements are made, Ps is the mean systemic pres-
sure (100 mmHg), and Ds is the corresponding exter-
nal diameter. Compliance Cv is thus the fractional
change in external d iameter, De, w ith change in
physiological pressure, P, from 80 to 120 mmHg (orfrom 10.67 to 16 kPa), and the coefficient is the slope
of the natural logarithm (ln) pressurediameter curve
and thus represents the stiffness of the vascular wall.
Because the pressurediameter relation of an arte-
rial wall is generally nonlinear, even within the ph ysi-ological pressure range, the parameters Cv an d Ep ar e
not usually material constants but change with the
internal pr essure. The stiffness param eter , however,
is independent of the pressure and has been used to
characterize the elastic properties of polyurethane
grafts.6,13
RESULTS
A typical pressure p to circumferential stretch ratio
2 relationship for hum an CCA, which differs fromthe relationship generally found on traditional p oly-
mer materials, is shown in Figure 3. The p2 curves
for the arteries are concave upward as expected.27,30
The slope gradually increases with stretch ratio and
becomes exceptionally high when 2 reaches a value
of about 1.42 0.12 (or when pressure exceeds 120
mmH g). The u nderlying structure of the arterial wall
must be responsible for the noted mechanical behav-
ior. Studies by Wolinsky and Glagov34 and Lange-
wou ters et al.35
show tha t the wall tissue is mad e up ofat least two major fibrous materials, an elastin fiber
with a low modulus of elasticity (25 105 Pa) and a
collagen fiber w ith a high mod ulus of elasticity (510
107 Pa). In the relaxed state, the collagen fibers are
slack. At low strain or pressure, most of the load is
borne by the elastin fibers, and therefore, the artery is
highly distensible. However, as the pressure is raised
a n d t h e s t r ai n i s i n c r ea s ed , t h e c ol la g e n f ib e r s
straighten out and start to bear load. This process
causes an increase in the slope.
Results from LM and the SEM show that carotid
arteries have a sp ecific wavy structure an d the tissue is
a biocomposite (Figs. 4 and 5). The wavy membranes
consist of the elastic fibers plaited w ith collagen fibers.
With an increase of internal pressure the diameter of
the artery increases and the degree of waviness de-
creases [Figs. 4(b) and 5(b)]. At a pressure of 120
mmH g and the longitudinal stretch ratio correspond-
ing to the in situ length, the waviness of the wall ele-
ments practically disappears. With a further increase
in pressure, the collagen fibers begin to resist the cir-
cumferential strain in the artery and thus give rise to
the behavior noted in Figure 3.
The behavior of grafts H VG-1 and HVG-2, also
shown in Figure 3, is similar in character to that of the
c ar o t id a r t er y . T h e p o l yu r e t h a n e a n d p o l ye s te r
threads in the former seem to play about the sameroles as the elastin and the collagen fibers, respec-
tively, in the latter. Some differences are noted in the
values and the shapes of the curves. A pressure of 160
mmHg or greater is needed in the grafts to straighten
out the higher modulus fibers; in arteries the corre-
Figure 3. Pressure p to circumferential stretch ratio 2 re -lationship. 1, commercial vascular graft (CVG); 2, h ybridtextile vascular graft (HVG-1, after 3 months of imp lanta-tion); 3, hybrid textile vascular graft (HVG-2); 4, hybrid tex-tile vascular graft (HVG-1); and 5, human common carotidartery.
344 GUPTA AN D KASYAN OV
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
5/9
sponding pressure was lower. For the pressure range
80120 mm Hg, the increase in circumferential stretch
ratio w as 7.14% for the carotid arteries, 9.02% for the
HVG-1 graft, 6.06% for the HVG-2 graft, and only
0.32% for the commercial graft. These results show
that the commercial grafts used are the least disten-
sible of all materials examined and are n ot biocomp li-
ant. Comp liance values of the hybrid textile grafts
compare favorably with those of the carotid arteries
(Table I).
Comparison of the Cv an d Ep values shows that the
deformability of the HVG-1 graft is greater than that of
the carotid ar tery. Based on the valu es of the stiffness
parameter , one can conclude that graft HVG-1 is
more compliant than graft HVG-2, the stiffness coef-
ficients being 4.87 1.56 and 7.81 1.62, respectively.
Clearly, the differences in the values of the two graftsarise from the differences in their structures, indicat-
ing that a graft with the d esired m echanical properties
could be constructed if the structure was carefully
controlled.
The results of the water perm eability obtained show
that HVG-1 grafts are less w ater p erm eable than
HVG-2 grafts, the values being 2.06 0.16 and 2.42
0.18 mL/ m in/ cm 2. These values are about the same as
obtained by others on grafts.17,31
HVG-1 grafts of 4-mm internal diameter were im-
planted in eight mongrel dogs for periods of 1 monthto 1 year. Four were implanted in the carotid and the
other four in the femoral regions. Six grafts functioned
satisfactorily, but the remaining two (femoral) devel-
oped a stenose of d istal anastomoses. Six months a fter
implantation, the circumferential stretch ratio (for the
ran ge 80120 mm Hg ) d ecreased from 9.02 to 2.62 (Fig.
3), due obviously to some inward growth of the sur-
rounding tissues.
The structure of the grafts was examined with LM
and an SEM before implantation and after retrieval
following implantation. Figure 6 shows the structureof the outer and inner walls of HVG-1 before implan-
tation. The loops noted are those of the bulked poly-
e st e r y a r n s f or m e d b y t h e r e c ov e ry o f t h e p o ly -
urethan e yarns. Figures 7 and 8 show typical morp hol-
ogy found in the six p atent grafts after implantation.
These figures indicate that the healing process pro-
Figure 5. SEM of the circumferential slice of the carotidartery wall: (a) at zero internal p ressure and (b) at internalpressur e of 120 mmH g (sample 9, man 34 years old; originalma gnification 5000).
Figure 4. Circumferential histological slice of the carotidarterial wall: (a) at zero internal pressure and (b) at internalpressure of 120 mmHg (sample 9, man 34 years old; originalmagnification 50).
345CAROTID ARTERY/ BIOMECHANICS AND NOVEL VASCULAR GRAFTS
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
6/9
gressed norm ally. At retrieval, none of the grafts
showed any aneurysm formation, p erigraft h emato-
mas, or rupture. All anastomoses were intact, and ex-
ternal tissue reaction was minimal. The inner surface
was lined with a smooth, thin layer of transparent
glistening tissue, with occasional small foci of yellow-
tan staining, but there was no evidence of adherent
thrombus (Fig. 7). SEM examination showed that the
endothelial-like cells app eared flattened with elon-
gated nuclei (Fig. 8). The results of the pulse wave
measured on the dogs showed that the pulse wave
obtained with compliant grafts was practically of the
same form as found with the carotid artery (Fig. 9).
DISCUSSION
Although many factors affect the success of a vas-
cular graft in surgery, the two most important are the
mechanical characteristics of the graft and the ability
of the graft to heal. The hope for achieving long-term
patency in 6-mm grafts lies in matching the compli-
ance of a vascular graft with that of the artery and
developing a thromboresistant surface at the luminal
wall.
Numerous studies have shown that a positive cor-
relation exists between the matching of compliance
and the p atency of the graft.1,2,12,14,36,37 Preliminary
studies show15 that compliance is a particularly im-
portant factor during the first six or so weeks of the
operation; long-term compliance may be a negligible
factor in determining the overall patency of small
grafts. In an ideal graft, the velocity of flow is high
while the stresses at the suture lines and the reflected
energy losses are small. For achieving minimum stress
concentration and energy losses in the existing com-
mercial grafts, the diameter of the graft chosen has to
be 1.41.5 times the diameter of the host artery.38
An impedance mismatch between the host and thegraft leads to development of eddy currents and wave
reflections. These contribute to structural fatigue, false
aneurysm, thrombus formation, hyperplastic tissue
growth, an d atherosclerotic changes in th e host artery,
which can lead to early occlusion of the graft.14,39 The
amount of reflected energy can be reduced to zero if a
perfect match exists between the fluid impedances of
the host artery and the graft. In a study by Scott and
Wilson40 in wh ich blood flow behavior in the hu man
leg was sim ulated with a com puter m odel, it was
shown that a m atch of both the diam eters and the
compliances of the prosthesis and the host vessel were
needed to maximize flow velocity while minimizing
reflected energy losses and stresses at th e sutu re lines.
The present work shows that in the human CCA,
the slope of the pressure (p)circumferential stretch
Figure 6. SEM of th e h ybrid textile vascular gr afts: (a) out-side structure an d (b) inside structure.
TABLE IMean Value SD of Human Common Carotid Artery (CCA), Textile H ybrid Vascular Grafts (HVG-1 and HVG-2),
and Commercial Graft (CVG)
Artery or
Graft
Specimen
Wall
Thickness
(mm)
Diameter
(mm)
Compliance, Cv
(kPa1
)
Elastic
Modulus,
Ep (kPa)
Stiffness
Parameter,
CCA 1.54 0.12 5.92 0.47 0.0238 0.0132 83.86 22.38 5.18 1.94
H VG-1 0.42 0.04 4.02 0.04 0.0324 0.0083 61.81 16.92 4.87 1.56
H VG-2 1.23 0.06 4.05 0.06 0.0227 0.0078 87.78 19.04 7.81 1.62
CVG 0.27 0.02 6.01 0.04 0.00186 0.0005 1074.64 136.18 102.91 16.84
346 GUPTA AN D KASYAN OV
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
7/9
ratio (2) curve increases w ith pressure and becomes
exponential at pressures greater than 120 mmHg (Fig.
3). The LM and SEM analyses show that the arterial
wall is a biocomposite of elastin and collagen fibers
and has a specific crimped character. This structure, as
explained earlier, leads to the unu sual m echanical be-
havior noted above, which differs from that of the
traditional polymer materials. The value of compli-
ance measured on hum an carotid arteries coincides
with the values obtained by Hayashi et al.27 w ho
found that the stiffness param eter had a value of 5.25 for the hum an CCA and 19.84 for the femoral
artery. Our r esults show a v alue of 5.18 for the h um an
carotid artery (see Table I).
The novel hybrid textile vascular grafts prod uced in
this work have elastic properties that match those of
the hu man carotid artery. The materials used in their
construction were polyurethane and polyester yarns
that allowed the hybrid textile grafts to have a com-
pliance value in the circumferential direction 10 or
more times those of the currently available commer-
cial grafts. The w ater p ermeability value of the h ybrid
grafts is at the same level as found in the commercial
prostheses. All commercial grafts are crimped by one
or two heat-setting processes. These grafts rapidly lose
crimp and longitud inal compliance up on implanta-
tion.17 The procedure used in manufacturing the hy-
brid textile prostheses, on the other hand, renders the
heat setting process for crimping unnecessary. The
combination of prestretched polyurethane yarns with
polyester in the warp threads led to the d evelopment
of a stable crimp in the longitudinal direction. More-
over, by varying the sizes and properties of the indi-
vidual yarns, the structure and properties of vasculargrafts could be effectively and conveniently engi-
neered to suit the application.
However, the mechanical compliance alone does
not guarantee success in vivo. Kambic et al.41 showed
that no one material satisfies the requirements for by-
pass of all small caliber arteries. Future research mu st
additionally focus on development of improved inner
surface coatings, which may minimize tissue reaction
and undesirable cellular events at the anastomoses. A
g e la t in co a tin g w a s u s e d t o p r o v id e a b lo od -
compatible graft with a smooth nonpseudoneointimagenerating surface that does not prom ote cell in-
growth at the anastomoses.15
A difficult problem faced in matching compliance is
a change in the mechanical properties of the graft that
is induced by tissue ingrowth. The in vivo test results
on the grafts of this study are encouraging. Examina-
tion of the HVG-1 grafts after 6 months of implanta-
tion indicated th at the h ealing p rocess progressed n or-
mally. Some loss of compliance was noted due to tis-
sue ingrowth into the wall. Hasegava and Azuma,42
working with woven Dacron or Teflon grafts, foundthat 3 weeks postimplantation, the longitudinal stiff-
ness h ad increased but the circumferential stiffness
had not changed. On the other hand, the w ork of Lee
and Wilson37 showed a marked increase in circumfer-
ential stiffness after 3 months of implantation, indicat-
ing that at 3 months the connective tissue ingrowth
was orga nized an d played a significant role in increas-
ing wall stiffness.
It was also found43 that although both neointima
and adventitia cells were closely attached to the poly-
urethane fibers near the surface, there was no trans-
mural or through growth of the tissues. After 9months of implantation in m ini-pigs, the grafts w ere
still fairly compliant. Studies on spandex prostheses in
dogs indicated 18 that while these grafts lost some cir-
cumferential stretchability after becoming infiltrated
with unyielding collagenous tissue, they remained
compliant d uring the first w eek after insertion and
adapted their diameter to the flow conditions of the
arteries that were bypassed. The spandex grafts usu-
ally adjust their diameter in response to changing flow
Figure 7. Hybrid vascular graft HVG-1 after 6 months ofimplantation. The interior is lined with a thin layer of trans-parent glistening tissue w ithout thrombu s.
Figure 8. Endothelium cells on the flowing surface of theHVG-1 graft.
347CAROTID ARTERY/ BIOMECHANICS AND NOVEL VASCULAR GRAFTS
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
8/9
and pressure conditions, particularly the former, and
develop a thin, almost transparent, neointima on the
flow surface.
Another important parameter that determines the
success of a graft in bypass application is porosity.Tissue incorporation and healing of synthetic grafts
are related to this property.44 The pore size affects the
type of tissue grown through the wall.4 Working with
polyurethane grafts, White4 showed that if the pore
size was less than 15 m, minimal tissue ingrowth
took place; if it was greater than 15 m but less than
about 45 m, fibrohistiocytic tissues grew; and if the
size w as greater than about 50 m, the structure was
infiltrated with organized fibrous tissue.
The above results thus indicate that by choosing
appropriate materials and controlling the structure, atextile graft can be engineered that h as the desired
compliance and the potential for attaining the needed
tissue ingrowth. An important question still remains;
however: Should th e properties of the host be matched
by those of the virgin prostheses or those of the pros-
theses after they have been at the site for some length
of time?45 To address this question, it is necessary to
know what changes take place in the properties of a
graft with time in situ and how these affect the func-
tion of the product. Clearly, this knowledge is needed
before an optimally useful graft can be designed.
The benefits accruing to the au thors from a commercial or
industrial party will be applied to a research fund, nonprofit
institution, or other organization with which the authors are
associated.
References
1. I. G. Kidson and W. M. Abbot, Low compliance andarterial graft occlusion, Trans. Am. Soc. Artif. Intern.Organs, 58, 1.11.4 (1978).
2. R. Walden, G. J. ILtalien, J. Megerman, and W. M. Ab-
bott, Matching elastic properties and successful arte-rial grafting, Arch. Surg., 115, 11661169 (1980).
3. J. G. Slad en and T. M. Maxwall, Experience in vivo 130polytetrafluoethylene grafts,Am . J. Su rg., 141, 545548(1981).
4. R. A. White, The effect of porosity and biomaterial onthe healing and long-term mechanical properties ofvascular prostheses, Trans. Am. Soc. Artif. Intern. Or-gans, 34, 94100 (1988).
5. J. R. Wom ersly, Oscillatory flow in arteries. II: Thereflection of the pu lse wave at junction and rigid insertsin the arterial system, Phys. Med. Biol., 2, 313323(1958).
6. T. V. H ow and R. M. Clarke, The elastic prop erties of
a p olyurethan e arterial prosth esis, J. Biomech., 17, 597608 (1984).
7. R. N. Baird and W. M. Abbott, Pulsatile blood flow inarterial grafts, Lancet, 2, 948950 (1976).
8. S. E. Rittgers, P. E. Karayannacos, J. F. Guy, R. M.Nerem, G. H. Shaw, J. R. H ostetler, and J. S. Vasko,Velocity distribution and initial proliferation in autog-enous vein grafts in dogs, Circ. R es., 42, 792801(1978).
9. I. Doo, W. Jedruch, J. Kennedy, P. Adams, and C. M.Rodkiewicz, Wall distensibility effect on arterial flowdistribution, J. Biomech., 17, 643 (1984).
10. P. D. Stein, F. J. Walburn, and E. F. Blick, Damp ingeffect of distensible tubes on turbulent flow: implica-tion in cardiovascular system, Biorheology, 17, 275281(1980).
11. P. Beahan and D. Hull, A study of the interface be-tween a fibrous polyurethane arterial prosthesis andnatural tissue, J. Biomed. M ater. Res., 16, 827838(1982).
12. K. Hayashi, Keynote lecture. Biomechanical approachto the design of vascular prostheses, Tissue Eng., 14,510 (1989).
13. K. Hayashi, K. Takamizaw a, T. Saito, K. Kira, K. Hira-matsu, and K. Kondo, Elastic properties and strengthof a novel small-diam eter, comp liant polyurethan e vas-cular graft, J. Biomed. Mater. Res. Appl. Biomater., 23,229244 (1989).
14. B. van der Lei and Ch. R. H. Wildevuur, From a syn-thetic, microporous, compliant, biodegradable small-caliber vascular graft to a new artery, Thorac. Cardio-vasc. Surg., 37, 337347 (1989).
15. H. E. Kambic, Polyurethane small artery substitutes,Trans. A m. Soc. Artif. Intern. O rgans, 34, 10471050(1989).
16. G. Soldani, G. Pan ol, H. F. Sasken, M. B. Godd ard, andP . M . G a ll et t i , Sm a l l d i a m e t e r p o l y u r e t h a n e -polydimethylsiloxane vascular prostheses made by aspraying, ph ase-inversion process,J. Mater. Sci. Mater.
Med., 3, 106, 113 (1992).
17. M. W. King, R. G. Guidoin, K. R. Gunasekera, and C.
Gosselin, Designing polyester vascular prostheses forthe future, Med. Progr. Technol., 9, 217226 (1983).
18. N. Rosenberg, A. N. Simpson, and R. E. Brown, A cir-cumferential elastic prostheses: three-year studies of adacron-spandex graft in the dog, J. Surg. Res., 34, 716(1983).
19. C. C. Chu a nd L. E. Lecaroz, Design an d in vivo testing
Figure 9. Shape of the pulse waves: (a) dog carotid artery,(b) commercial graft, and (c) hybrid vascular graft HVG-1.
348 GUPTA AN D KASYAN OV
-
8/6/2019 Bio Mechanics of Human Common Carotid Artery and Design
9/9
of newly made biocomponent knitted fabric for vascu-lar surgery, A dv. Biomed. Polym. Proc. Sy mp., Chicago,Sept. 815, 1987.
20. L. ShuTung, A collagen-dacron composite vasculargraft for arterial reconstructions, Adv. Biomed. Polym.Proc. S ymp., Chicago, Sept. 815, 1987.
21. V. Kasyanov and B. Pur inya, Elastic properties of thecomposite vascular grafts, presented at the 3rd Inter-national ITV Conference on Biomechanics, Medical Textiles
for Implantation, Stuttgart, Germany, 1989, p . 39.
22. R. H. Cox, Anisotropic properties of the canine carotidartery in vitro, J. Biomech., 8, 293300 (1975).
23. D. J. Patel and D. L. Fry, The elastic symmetry of ar-terial segments in dogs, Circ. Res., 24, 18 (1969).
24. D. J. Patel an d J. S. Janicki, Statical elastic p rop erties ofthe left coronary circumflex artery and common carotidartery in dogs, Circ. Res., 27, 149158 (1970).
25. R. N. Vaishn av, J. T. You ng, J. S. Janicki, an d D. J. Patel,Nonlinear anisotropic elastic properties of the canine
aorta, Biophys. J., 12, 10081027 (1972).26. P. B. Dobrin, Biaxial anisotropy of carotid artery: es-timation of circumferential elastic mod ulus,J. Biomech.,19, 351358 (1986).
27. K. Hayashi, H. H anda, S. Nagasawa, A. Okumu ra, andK. Moritake, Stiffness and elastic behavior of humanintracranial and extracranial arteries, J. Biomech., 13,175184 (1980).
28. V. Kasyanov and A. Kregers, Differences in the defor-mation and strength properties of human large bloodvessels as a function of location, loading direction andage, Polym. Mech., 4, 606611 (1975).
29. B. Purinya and V. Kasyanov, Changes in the m echani-cal properties of human coronary arteries with age,
Polym. Mech., 2, 251255 (1977).30. V. Kasyanov, B. Purinya, and E. Ceders, Determina-
tion of the shear modu lus of hum an blood v essel wall,Polym. Mech., 5, 753755 (1978).
31. R. Guidon, M. King, D. Marceau, A. Cardou, D. Faye,J.-M. Legendre, and P. Blais, Textile arterial prosthe-ses: Is water permeability equivalent to porosity, J.
Biomed. Mater. Res., 21, 6567 (1987).
32. B. S. Gow and M. G. Taylor, Measuremen t of v isco-elastic properties of arteries in the living dog, Circ.
Res., 23, 111122 (1968).
33. L. H. Peterson, R. E. Jensen, and R. Parnell, Mechani-cal properties of arteries in vivo, Circ. Res., 8, 622639(1960).
34. H. Wolinsky and S. Glagov, Structural basis for thestatic mechanical properties of the aortic media, Circ.
Res., 14, 400413 (1964).
35. G. J. Langewouters, K. H. Wesseling, and W. J. Goed-hard , The pressur e dep enden t d ynam ic elasticity of 35thoracic and 16 abdominal human aortas in vivo d e-scribed by a five component model, J. Biomech., 18,613620 (1985).
36. D. J. Lyman, D. Albo, Jr., R. Jackson, and K. Knutson,Development of small d iameter v ascular p rostheses,Trans. Am. Soc. Artif. Intern. Organs, 23, 253261 (1977).
37. J. M. Lee and G. J. Wilson, Anisotropic tensile visco-elastic p roperties of vascular graft materials tested atlow strain rates, Biomaterials, 7, 423431 (1986).
38. P. E. Paasche, C. E. Kinley, F. G. Dolan, E. R. Gonza,and A. E. Marble, Consideration of suture line stressesin th e selection of synthetic grafts for implantation, J.
Biomech., 6, 253259 (1973).
39. R. R. Kowligi, W. W. von Maltzahn, and R. Eberhart,Fabrication and characterization of small-diametervascular-prostheses, J. Biomed. Mater. Res., 22, 245256(1988).
40. S. M. Scott an d B. S. Wilson, The m echanical d esign ofvascular p rostheses, presented at The Sy mposium on
Hemodynamics of the Limbs, Toulouse, France, May 1719, 1979, pp. 251259.
41. H. Kam bic, S. Mur abay ashi, an d Y. Nose, Biomater ialsin artificial organs, Chem. Eng. News, 64, 3048 (1986).
42. M. Hasegava and T. Azuma, Mechanical pr operties ofsynthetic arterial grafts, Biomechanics, 12, 509517(1979).
43. D. Annis, A. Bornat, R. Edw ard s, A. Higham , B. Love-
day, and J. Wilson, An elastomeric vascular prosthe-sis, Trans. Am. Soc. Artif. Intern. Organs, 24, 209214(1978).
44. S. A. Wesolowski, C. C. Fries, R. T. Domingo, W. I.Liebig, and P. N. Sawyer, The compou nd prostheticvascular graft: a path ologic surv ey, Surgery, 53, 1944(1963).
45. T. V. How, Mechanical properties of arteries and ar-terial grafts, in Cardiovascular Biomaterials, G. W. Hast-ings (ed.), SpringerVerlag, New York, 1992, pp. 135.
Received February 6, 1995Accepted March 8, 1996
349CAROTID ARTERY/ BIOMECHANICS AND NOVEL VASCULAR GRAFTS