Minimally invasive therapeutic techniques


A. Hepatic embolisation by glue injection

Glue embolization is a therapeutic treatment technique used to block the blood flow to specific targeted sites by injecting surgical glues that polymerize in contact
with blood. One application concerns patients suffering from malignant liver tumors, who need to undergo partial liver ablation (figure 1). When the volume of the remnant liver
part is not sufficient, preoperative portal vein embolization is used to arrest blood flow in the liver part to be resected. This induces the hypertrophy of the remnant
liver and enables the ablation procedure after a couple of weeks.

Figure 1: Glue is injected percutaneously to embolize the part of the liver to be resected.


From a fluid mechanics point of view, embolization is governed by the dynamics of two co-flowing immiscible fluids, which is coupled with the kinetics of glue
polymerization. Experimental investigations on drop formation in liquid-liquid systems have shown the existence of two regimes, dripping and jetting. Most studies have focused on dripping in unconfined environment. We aim at characterizing the flow topology during portal vein embolization by studying experimentally the confined liquid-in-liquid injection, neglecting glue polymerization as a first approach.

An experimental setup has been designed to create and visualize the co-flow of two immiscible fluids. The dispersed phase is injected through a capillary tube into the continuous phase, which flows steadily in a straight cylindrical tube. The experiment is conducted in similarity with the physiological case.

We find that both regimes may occur during hepatic embolization (figure 2). Large drops form periodically during the dripping regime. During jetting, a jet forms instead at the tip of the catheter and destabilizes after a short distance, leading to the formation of small drops. The dripping-to-jetting transition is governed by the ratio of the inertial forces of the injected phase to the interfacial forces with the external phase (Weber number).
During dripping, the drop size is only dependent upon the ratio of the viscous forces of the external face to the interfacial forces (capillary number). An analytical model has been develop to predict the drop size evolution; good agreement is found with experimental data. During jetting, the drop size tends towards a constand value, which is a function of the jet diameter.

a.            b.

Figure 2 : In vitro experiment simulating the injection of a non-miscible fluid in a co-flow. (a) Dripping regime. (b) Jetting regime.


Collaborators

Dr. Olivier Balédent, Service de Biophysique et Traitement de l’Image, CHU Amiens
Dr. Roger Bouzerar, Service de Biophysique et Traitement de l’Image, CHU Amiens
Prof. Marc-Etienne Meyer, Service de Biophysique et Traitement de l’Image, CHU Amiens
Dr. Thierry Yzet, Département de Gastroentérologie, CHU Amiens
Prof. Hervé Deramond, Département de Neuroradiologie, CHU Amiens
Dominique Haye, Plate Forme Mécatronique, Saint Quentin


Mihai-Cristinel Sandulache, Caractérisation in vitro de la technique endovasculaire d’embolisation par colle chirurgicale, PhD thesis, UTC, October 2011.
Bilal Merei, Etude de l’embolisation hépatique par colle. Simulation numérique de l’injection dans une veine hépatique, Master Thesis, UTC, September 2010.
Océane Lançon, Etude in vitro de l’injection d’une colle chirurgicale pour l’embolisation hépatique, Master Thesis, UTC, September 2012.

B. Stenting of arterio-venous fistula

An arteriovenous fistula (AVF) is a surgical vessel connection between an artery and a vein. It is created in end stage renal disease to provide adequate blood access for hemodialysis. In the present study, the local hemodynamics is investigated in a patient-specific AVF using a computational fluid structure interaction (FSI) simulation. The fluid and solid governing equations are solved using ANSYS (ANSYS, Inc.).

We focus on an end-to-side AVF between the end of the ce-phalic vein and the brachial artery. The geometry of the vessel lumen is obtained from CT-scan angiography. The vessel wall is modeled as a monolayer of shell elements of uniform thick-ness, since the actual wall thickness cannot be obtained from medical images.

We investigate the effect of the presence of a severe stenosis upstream of the anastomosis by comparing two different geometries: model 1 consists of the complete patient-specific AVF, presenting a stenosis inside the proximal brachial artery and an enlargement at the cephalic vein; model 2 is obtained from model 1 by substituting the stenosed artery with a straight cylinder.

For both models, a physiological time-dependent velocity in-let profile and flow-dependent resistive pressure outlets are imposed as boundary conditions. The hyperelastic, 3rd-order Yeoh model is used as constitutive law to model the vessel wall.

The presence of the stenosis increases the mass flow through the vein by 9.6%. But even if the flow rate increases slightly, the WSS in the cephalic vein remains lower than the physiological range during the entire cardiac cycle. The stenosed case is therefore more likely to suffer from the formation of atherosclerotic plaques in this region. Stent placement in the case of stenosed AVFs would be beneficial as it would greatly reduce the vein area subjected to pathological flow conditions.



a.   b.

Figure 3: (a) Forearm anatomy in a patient with an arterio-venous fistula. (b) Patient-specific geometry used in the fluid-structure interaction numerical simulation.


Collaborators

Dr. Zaher Kharboutly, BMBI, UTC
Dr. Cécile Legallais, BMBI, UTC

Dr. Vanessa Diaz, University College London (UK)
Prof. Gabriele Dubini, Politecnico di Milano (Italy)
Dr. Justin Penrose, ANSYS UK (UK)

Iolanda Decorato (PhD student), Simulation numérique des interactions fluides structure dans une fistule artério-veineuse : effet de la pose d’un stent sur l’hémodynamique, UTC.
Tommaso Vassallo, Etude in vitro de l’hémodynamique dans une fistule artério-veineuse, Master Thesis, UTC, September 2012.