(Circulation. 1999;100:756-760.)
© 1999 American Heart Association, Inc.
Basic Science Reports |
From Beth IsraelDeaconess Medical Center, Boston, Mass (J.P.C., D.J.C., D.S.B.), and Boston Scientific Corp, Minneapolis, Minn (S.E.H.).
Correspondence to Donald S. Baim, MD, Cardiovascular Division, Beth IsraelDeaconess Medical Center, Boston, MA 02215. E-mail dbaim{at}bidmc.harvard.edu
| Abstract |
|---|
|
|
|---|
Methods and ResultsThirty-two stents (8 Gianturco-Roubin II, 8 Palmaz-Schatz, 8 MultiLink, and 8 NIR) were deployed in nondiseased coronary arteries of 8 Yorkshire pigs. All stents were then expanded according to 1 of 3 balloon strategies: appropriately sized compliant balloons, oversized compliant balloons, or oversized noncompliant balloons. Continuous ultrasound imaging was performed during stepwise balloon inflation and deflation, with an 0.018-in imaging core positioned within the guidewire lumen of the balloon. In these normal arteries, balloon underexpansion relative to the nominal size was not observed. After balloon deflation, however, all stents showed significant recoil from their maximum inflated CSA. Recoil was significantly greater for the coil Gianturco-Roubin II stent (30% CSA) than for the 3 slotted-tube stent designs (15% to 17% CSA).
ConclusionsIn normal, compliant coronary arteries, stent recoil is the predominant mechanism by which stents fail to achieve the nominal CSA of their dilating balloon. The magnitude of this in vivo stent recoil is significantly greater than reported from bench testing and varies with stent design (coil versus slotted tube). Postdilatation strategies that result in controlled stent overexpansion are needed to overcome this recoil phenomenon and result in a final stent CSA that approximates the reference artery CSA.
Key Words: stents arteries balloon ultrasonics
| Introduction |
|---|
|
|
|---|
Although high-pressure dilatation increases the lumen CSA within the stent, final stent CSA still rarely exceeds 60% to 70% of the nominal balloon CSA.7 8 This may result from either failure of the balloon to expand fully to its nominal area or recoil of the stent after balloon deflation. The ability to distinguish between these mechanisms (or a combination thereof) has been limited by difficulties in accurately measuring in vivo balloon CSA as a function of pressure and quantifying the amount of stent area recoil that occurs immediately after balloon deflation.
To overcome these limitations, we used an 0.018-in high-frequency ultrasound imaging core positioned within the guidewire lumen of various balloons (both compliant and noncompliant) during stent dilatation. This allowed ultrasonic measurement of balloon CSA as a function of pressure during inflation and immediate quantification of any loss of stent CSA during balloon deflation for different stent designs.
| Methods |
|---|
|
|
|---|
Stent Procedure
An 0.014-in angioplasty guidewire (Choice PT, Boston
Scientific Corp) was advanced into either the distal right or
circumflex coronary artery. After the administration of 200
µg nitroglycerin IC, standard IVUS was performed with
a 2.9F catheter (UltraCross, CVIS Corp) to assess lumen size. Each
stent design (see below) was then deployed at low pressure (
6 atm)
with a delivery balloon less than or equal to reference vessel size.
Each stent was then assigned randomly to 1 of 3 postdilatation
strategies: appropriate-sized compliant balloon (Cobra-18,
Boston Scientific Corp) with nominal
balloon-to-artery ratio
1.0; oversized compliant balloon (Cobra-18,
Boston Scientific Corp) with nominal
balloon-to-artery ratio
1.2; or oversized noncompliant balloon (NC
Cobra-18, Boston Scientific Corp) with nominal
balloon-to-artery ratio
1.2.
The postdilating balloon was delivered into the stent over the angioplasty guidewire. The guidewire was then removed and its lumen flushed with heparinized saline. An 0.018-in 30-MHz rotating imaging core (Boston Scientific) was inserted into the guidewire lumen of the deflated balloon and positioned just distal to the balloon midmarker. The imaging wire was connected to the rotating motor drive unit, and all images were processed by use of the CVIS ClearView System. The balloon and the inflation device were filled with heparinized normal saline rather than iodinated contrast medium to avoid changes in density, and thus the speed of sound, in the intervening liquid medium during inflation. Continuous ultrasound imaging was performed as the balloon was gradually inflated in 2-atm steps from 2 to 12 atm. Pressure (and thus balloon volume) was allowed to equilibrate for at least 10 seconds at each pressure level. Ultrasound images were also acquired during slow, progressive balloon deflation. In a subset of stents (n=6), conventional IVUS imaging was performed with the CVIS catheter after balloon deflation and core wire imaging to assess correlation between the 2 imaging modalities.
Stents
Four different stent designs were evaluated: the coil
Gianturco-Roubin II stent (Cook Cardiology), the
slotted-tube Palmaz-Schatz coronary stent (Cordis Corp), the
MultiLink stent (Guidant Corp), and the NIR stent (Medinol). To ensure
unbiased distribution of each stent design in a particular location,
each stent was implanted in each animal according to a matrix that
randomly assigned the stent to vessel location and position (proximal,
mid, or distal vessel).
Data Analysis and Statistics
All images were recorded on S-VHS videotape. CSA, minimum
lumen diameter (MLD), and maximum lumen diameters were quantified with
online, integrated measurement software. Elastic recoil was calculated
in the following manner: % area recoil=1-(stent
CSAdeflation/balloon CSA12
atm); % diameter recoil=1-(stent
MLDdeflation/balloon MLD12
atm).
Data are expressed as mean±SEM. Comparisons were made by ANOVA and Student's t test with correction for multiple comparisons by the Bonferroni method. Correlation between continuous variables was assessed by linear regression. Data were analyzed by JMP software (SAS Institute).
| Results |
|---|
|
|
|---|
1.2), however, had measured balloon areas that were smaller at high
pressure than specified in the manufacturers' compliance charts.
|
|
Stent Recoil
In the subset of stents in which conventional IVUS imaging was
performed after balloon deflation and imaging wire assessment, there
was excellent correlation of stent CSA as measured by IVUS and the
imaging core (Figure 2
). The magnitude of
acute stent recoil (from maximum expansion to postdeflation) ranged
from 15% to 30% CSA and differed among the 4 stent types (Figure 3
). Area recoil was significantly greater
for the coil design (Gianturco-Roubin II stent) than for any of the
slotted-tube configurations (Figure 4
).
The corresponding diameter recoil (17.8% versus 10.4%,
P<0.01) was also significantly greater for the
Gianturco-Roubin stent than for the reference Palmaz-Schatz
coronary stent. As a result of these differences in stent
recoil, the ratio of final stent to reference vessel area was
significantly smaller for the coil than for the slotted-tube stents
(0.94±0.06 versus 1.11±0.04; P=0.022) despite similar
ratios of maximum measured balloon size to reference vessel CSA across
all 4 stent designs (Figure 5
). This
greater recoil of the coil stent design is reflected graphically by a
downward shift in the final stentmaximum balloon expansion curve when
normalized by vessel size (Figure 6
). To
overcome this recoil effect in a coil design would require
substantially greater overexpansion (to a balloon-to-artery area ratio
of 1.4 by area [diameter ratio 1.2]) than in a slotted-tube design
(area ratio 1.2 [diameter ratio 1.1]).
|
|
|
|
|
| Discussion |
|---|
|
|
|---|
Nakamura et al7 demonstrated that despite excellent angiographic appearance, the majority of stents deployed at low pressure remain suboptimally expanded by IVUS criteria. Use of high-pressure postdilatation increased stent CSA and improved stent geometry, so that routine high-pressure postdilatation is now a universally accepted practice. Even so, final stent CSA rarely exceeds 60% to 80% of the nominal balloon CSA. Potential explanations for this persistent stent undersizing include balloon underexpansion (despite high inflation pressures), acute stent recoil, or a combination of the 2 mechanisms.
Haude et al12 reported that compared with conventional balloon dilatation, the slotted-tube Palmaz-Schatz coronary stent reduced diameter (3.5%) and area (5.1%) recoil. These findings have been interpreted to mean that stenting largely eliminates acute elastic recoil after coronary intervention. In that study, however, high-pressure dilatation was not performed uniformly, and recoil was calculated by use of geometric assumptions derived from angiographic variables. Lumen CSA was thus calculated from a single, measured diameter assuming a uniform, elliptical geometry. In addition, expansion was assumed to be uniform along the entire length of the balloon. Because the maximum balloon diameter was measured and equivalence was assumed in the diseased noncompliant segment of the artery, balloon size may have been significantly overestimated. More recently, Bermejo and colleagues13 used a combination of quantitative angiography and IVUS to assess the relative contribution of balloon underexpansion and stent recoil to the residual lumen stenosis after high-pressure dilatation. They measured minimum and maximum balloon diameters by quantitative coronary angiography and demonstrated a failure to reach nominal diameter as well as nonuniformity of balloon expansion within the diseased segments. By then performing IVUS in the same stented segments after high-pressure dilatation, they calculated area recoil of 15% for the Palmaz-Schatz stent and 26% for the coil Wiktor stent relative to the inflated balloon area.
In the present study, online IVUS was performed with an 0.018-in imaging core positioned in the guidewire lumen of the balloon to allow accurate assessment of both the balloon expansion during progressively higher-pressure inflation and acute stent recoil during balloon deflation. Balloon diameters and CSAs were thus measured directly, rather than being calculated from geometric assumptions and disparate imaging methodologies. In these normal (nondiseased) porcine arteries, balloon CSA closely matched that expected from the manufacturers' compliance charts. The only exception to this finding was for oversized (balloon-to-artery ratio >1.15) compliant balloons, for which some balloon underexpansion relative to specifications was seen at the highest pressures (12 atm).
The surprising finding, however, was the magnitude of stent recoil during balloon deflations. Acute stent recoil ranged from 15% to 17% area for the slotted-tube stents and 30% area for the coil stents. This corresponds to diameter recoil of 6.9% to 10.4% for slotted-tube stents, versus 17.8% for the coil stent. This 2-fold greater elastic recoil observed for the Gianturco-Roubin coil was similar to what Bermejo et al13 and Werner et al14 observed for the Wiktor coil stent compared with the Palmaz-Schatz slotted-tube design. These recoil data may explain the greater residual stenosis observed clinically after coil stent compared with slotted-tube placement.15 Despite similar maximum balloon-to-artery ratios with all 4 stent designs, the greater magnitude of recoil observed for the Gianturco-Roubin stent led to a significantly lower final ratio of stent to reference artery CSA than in the slotted-tube designs (0.9 versus 1.1, P=0.02). To achieve a final stent-to-artery ratio of 1.0, the coil stents would require overexpansion to a balloon-to-artery area ratio of 1.4 (diameter ratio 1.2), whereas slotted-tube stents would require overexpansion only to an area ratio of 1.2 (diameter ratio 1.1).
With the exception of oversized compliant balloons, balloon
underexpansion was not observed in this study. This is in
contradistinction to the findings of Bermejo et al, which documented up
to a 33% balloon underexpansion in diseased human coronary
arteries. The discrepancy between these studies may be due to different
methodologies (quantitative coronary angiography versus IVUS
balloon sizing) or because balloon underexpansion is more likely in
diseased vessels, which are less compliant and often contain bulky
fibrocalcific plaque (which physically limits balloon expansion), than
in normal arteries as evaluated in the present
study.16 17 It must be noted, however, that the magnitude
of elastic stent recoil (20% to 30% of stent area) seen in this study
is comparable to that seen by Bermejo et al and would alone be
sufficient to explain the degree of final stent undersizing seen
clinically. To compensate for this elastic stent recoil and achieve the
optimal stent result (final stent-to-artery ratio of 1.0), stents must
then be overexpanded by 10% to 20% diameter relative to the reference
vessel diameter. This may be done by use of either an oversized
noncompliant balloon or a correctly sized compliant balloon relative to
the reference lumen that is inflated to high pressure. As long as the
desired degree of balloon oversizing is achieved, however, inflation to
high pressure is not per se a requirement for optimal stent results.
This principle may explain the recent trend toward lower (
12 atm)
inflation pressures with balloons slightly oversized relative to the
desired reference lumen diameter (including balloons sized to approach
the diameter of the external elastic lamina measured by IVUS). In
heavily diseased arteries, however, this calculation may increase the
risk of edge dissection or frank vessel rupture, as was observed in the
early experience of Colombo et al.9
Limitations
This study has several important limitations. First, all stents
were expanded in nondiseased, compliant arteries. The forces resisting
balloon expansion are clearly less in this model than in
atherosclerotic vessels. The contribution of balloon undersizing to
final stent underexpansion may thus have been underestimated
significantly compared with that which occurs in diseased human
arteries. Second, the degree of stent recoil may be even higher in
diseased arteries, which may exert greater recoil force. Even so, the
15% area recoil observed for slotted-tube stents and 30% area recoil
observed for coil stents in this study represent a "best-case
scenario" for these devices and mandate intentional stent
overexpansion to achieve the desired final stent luminal CSA.
| Acknowledgments |
|---|
| Footnotes |
|---|
Received December 7, 1998; revision received April 14, 1999; accepted April 15, 1999.
| References |
|---|
|
|
|---|
This article has been cited by other articles:
![]() |
E. De Benedetti and P. Urban Coronary stenting: why size matters Heart, December 1, 2007; 93(12): 1500 - 1501. [Abstract] [Full Text] [PDF] |
||||
![]() |
R. J Russo, P. D Silva, and M. Yeager Coronary artery overexpansion increases neointimal hyperplasia after stent placement in a porcine model Heart, December 1, 2007; 93(12): 1609 - 1615. [Abstract] [Full Text] [PDF] |
||||
![]() |
J Gunn, N Arnold, K H Chan, L Shepherd, D C Cumberland, and D C Crossman Coronary artery stretch versus deep injury in the development of in-stent neointima Heart, October 1, 2002; 88(4): 401 - 405. [Abstract] [Full Text] [PDF] |
||||
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
|
Circulation Home | Subscriptions | Archives | Feedback | Authors | Help | AHA Journals Home | Search Copyright © 1999 American Heart Association, Inc. All rights reserved. Unauthorized use prohibited. |