Korean Circ J.  2011 Feb;41(2):91-96. 10.4070/kcj.2011.41.2.91.

Evaluation of Local Flow Conditions in Jailed Side Branch Lesions Using Computational Fluid Dynamics

Affiliations
  • 1Department of Internal Medicine, Seoul National University College of Medicine, Seoul, Korea. bkkoo@snu.ac.kr
  • 2Cardiovascular Center, Seoul National University Hospital, Seoul, Korea.
  • 3Department of Emergency Medicine, Seoul National University College of Medicine, Seoul, Korea.
  • 4Institute of Medical and Biological Engineering, Medical Research Center, Seoul National University, Seoul, Korea.

Abstract

BACKGROUND AND OBJECTIVES
Lesions of vascular bifurcation and their treatment outcomes have been evaluated by anatomical and physiological methods, such as intravascular ultrasound and fractional flow reserve (FFR). However, local changes in flow dynamics in lesions of bifurcation have not been well evaluated. This study aimed at evaluating changes in the local flow patterns of bifurcation lesions.
MATERIALS AND METHODS
Eight (n=8) representative simulation-models were constructed: 1 normal bifurcation, 5 main-branch (MB) stenting models with various side-branch (SB) stenoses (ostial or non-ostial 75% diameter stenosis with 1- or 2-cm lesion lengths, ostial 75% diameter stenosis caused by carina shift), and 2 post-kissing models (no or 50% SB residual stenosis). Pressure, velocity, and wall shear stress (WSS) profiles around the bifurcation sites were investigated using computational fluid dynamics.
RESULTS
Post-stenting models revealed significant pressure drop in the SB (FFR<0.75), excluding the carina shift model (FFR=0.89). In the post-kissing models, there was no significant pressure drop. All post-stenting models revealed eccentric low velocity flow patterns and areas of low WSS, primarily in the lateral wall on distal MB. Post-kissing angioplasty improved pressure drop in the SB but resulted in alteration of flow distribution in the MB. In the carina shift model, kissing ballooning resulted in deteriorated local flow conditions due to increased area of low velocity and WSS.
CONCLUSION
This study suggests that the most commonly used bifurcation intervention strategy may cause local flow disturbances, which may partially explain high restenosis and event rates in patients with bifurcation lesions.

Keyword

Fluid dynamics; Pressure; Blood flow velocity; Shear strength; Fractional flow reserve, myocardial

MeSH Terms

Angioplasty
Blood Flow Velocity
Constriction, Pathologic
Fractional Flow Reserve, Myocardial
Humans
Hydrodynamics
Shear Strength
Stents

Figure

  • Fig. 1 Bifurcation lesion modeling with computational fluid dynamics. A normal bifurcation model was created using Finet's law and a typical bifurcation angle. As the boundary condition, inlet pressure of the main branche was defined as 110 mmHg, and venous pressure of 10 mmHg was applied to the outlet of the micro-vessels. To consider the physiology of the myocardium, micro-vessels were assumed as porous media that mimicked the pressure drop from arterial pressure to venous pressure (10 mmHg). The rheological property of blood was assumed as Newtonian fluid with a density of 1,060 kg/m3 and viscosity of 0.004 Pa·s.

  • Fig. 2 Representative computational fluid dynamics models. A: normal bifurcation. B and C: post-MB stenting models with various SB stenoses. F: post-MB stenting model with carina shift. G and H: post-kissing balloon angioplasty models with or without SB residual stenosis. MB: main branch, SB: side branch.

  • Fig. 3 Static pressure profiles in the 8-computational bifurcation models. There was no significant pressure drop in the normal bifurcation model (A). The post-MB stenting models are shown in (B) to (E). Post-MB stenting models with native ostial (B and C) and, non-ostial (D and E) SB stenosis revealed significant pressure drops in the SB. Regarding the carina shift model (F), the pressure drop was lower than those in the native SB stenosis models (B-E). After the kissing ballooning in the SB lesion, the pressure of SB was restored to the level of the distal MB pressure (G). Regarding residual stenosis after kissing ballooning (H), the pressure of SB was higher than that in the models with post-stenting SB lesions (B-E). *FFR is defined as the ratio of PSB/PMB. FFR: fractional flow reserve, MB: main branch, SB: side branch.

  • Fig. 4 Velocity profiles in computational bifurcation models. Velocity patterns in the bifurcation site were typical in the normal bifurcation model (A). Velocity profiles were skewed toward the carina, resulting in high velocity along the medial walls (yellow and red) and low velocity along the outer lateral walls (green and blue). In post-MB stenting models with significant SB stenosis, high velocity jet flows were observed at the site of stenosis, and low velocity areas were located in the lateral MB walls and medial SB walls (B-F). In post-kissing models (G and H), the low velocity area in SB was smaller than that in post-MB stenting models, but a larger low velocity area in the MB lateral wall was still observed relative to the area in the normal bifurcation model. MB: main branch, SB: side branch.

  • Fig. 5 Wall shear stresses in the 8-computational bifurcation models. In the normal bifurcation model (A), a small low WSS area was observed along the lateral side walls (green and blue). In post-MB stenting models with significant SB stenosis (B-E), low WSS areas were observed in the SB and lateral side MB wall. Low WSS areas in the lateral side MB were also more exaggerated in the post-kissing balloon angioplasty models (G and H) and carina shift model (F). MB: main branch, SB: side branch, WSS: wall shear stress.


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