Key Engineering Materials ISSN: 1662-9795, Vols. 270-273, pp 2061-2066 doi:10.4028/www.scientific.net/KEM.270-273.2061 © 2004 Trans Tech Publications, Switzerland Citation & Copyright (to be inserted by the publisher) Online: 2004-08-15 A Nondestructive Diagnostic Modeling for Muscular Dysfunction of Human Pharynx using Finite Element Method Sung Min Kim1, Sung Jae Kim1, Ha Suk Bae2, Byeong Chul Choi3, Joung Hwan Mun4 1 2 Dept. of Biomedical Eng., College of Medicine, Konkuk University, Chungbuk, Korea. Dept. of Rehabilitation Medicine, College of Medicine, Yonsei University, Seoul, Korea 3 4 Dept. of Biomedical Eng., Choonhae College, Ulsan, Korea Dept. of Bio-Mechatronics, Sungkyunkwan University, Suwon, Korea Keywords: Nondestructive Diagnosis, Biomechanical Modeling Abstract. Pharynx is a organ which transports food into the esophagus through peristaltic motion (repeat of contraction and expansion movement) and functions as an air passage. In this study, a structural change of human pharynx caused by muscular dysfunction is analyzed by a biomechanical model using CT and FEM(finite element method). For the biomechanical model, a loading condition is assumed so that equal internal pressure loaded sequentially to the inside of pharyngeal tissue. In order to analyze the pharyngeal muscular dysfunction by the biomechanical model, the pharyngeal dysfunctions are classified into 3 cases in the clinical complication by neuromuscular symptoms such as pharyngeal dysfunction after stroke. Those cases frequently show a change of material property and we investigated muscular tissue stiffness, deformation of cross sectional area of the pharynx by increasing the stiffness to 25%, 50%, 75% on the basis of stress-strain relationship of the pharyngeal tissue in each case. With three-dimensional reconstruction of pharyngeal structure using FEM and the optimization process by using inverse dynamic approach, the biomechanical model of the human pharynx is implemented and the muscular dysfunction is simulated. Introduction Dysfunction of Pharynx may cause various kinds of complication called dysphagia and the weakening of pharyngeal function accompanied especially by aging and other diseases. However, this case is not to be found at the early stage of various complications. Therefore, the synthetic analysis of pharyngeal dysfunction is essential to this case. In general, previous investigations has put the key point in a visible phenomenal description of a pharyngeal swallowing and one of the research [1] has tried to measure actual degree of the muscle activity and pressure of the pharyngeal cavity through electromyography of main pharyngeal muscle. This type of study shows various important aspects. Considering physiological variables, however, it cannot provide reliable methodology. It has been reported that 45% of acute aproplexy (By Gorden et al. [4]) and 51% of serious brain damaged patients have dysphagia(by Elliott[3]). In diagnosis of dysphagia, a case history or a physical examination of the patient is a basic methodology, which is insufficient for clinical judgment. A video fluoroscopy test is one of the standard methods used in most cases. Ultrasonic endoscope, ECG, manometry[5] test has also been used , but many problems remain unsolved yet. The results of those methods may be integrated into the objective diagnostic index. Fixed quantity measurement is compared with the video fluoroscopy. The result is that it has an advantage which estimation of the pharyngeal cavity pass time can be measured[6][7]. Even though a biomechanical pharyngeal model by finite element analysis is used as an approximate method, the evaluation of dysphagia through a biomechanical model of pharyngeal dysfunction can be effective for noninvasive diagnosis of dysphagia. A biomechanical esophageal model based on fluid mechanics describing esophageal motion by bolus transport is proposed by All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of Trans Tech Publications, www.ttp.net. (#69805896, Pennsylvania State University, University Park, USA-18/09/16,00:30:40) 2062 Advances in Nondestructive Evaluation Title of Publication (to be inserted by the publisher) Brasseur et al [8]. The investigations on the changes of cross-sectional area caused by bolus volume were reported by Kahrilas et al[12, 13, 14]. In this study, we present a new approach for the diagnosis of the pharyngeal muscular dysfunction through a biomechanical model by utilizing FEA(Finite Element Analysis) in a structural analysis in which we simulate a functional disorder of pharynx. Methods Material properties. To express a viscoelastic material behavior of pharyngeal tissue, we test several human pharyngeal tissues in order to obtain several important material properties such as stress relaxation test data and elastic response. The characteristic of the material of pharyngeal tissue used for biomechanical model is assumed to be isometric. Poisson’s ratio is given as v=0.45. Several material variables of viscoelastic behavior are obtained by stress relaxation test and uniaxial tensile test. Finite element analysis of pharyngeal structure. A pharyngeal 3-D model for FEA(finite element analysis) using 8 level pharyngeal 2-D CT image data is implemented by taking 7mm interval CT from the base of tongue to cricopharyngeus of a normal subject’s pharynx with no clinical history(Fig. 1-(a)). The subject swallowed 10ml radio-opaque bolus and we obtained the total CT image to reach from the oral cavity to the cricopharyngeus. The structure of the pharynx was implemented with time in the image information and deformation of cross-sectional area variation on the course of the section of the 5 step were observed in an each level to a 0.1 seconds interval. (a) (b) (c) Fig. 1. (a) Schematic image of pharynx and adjacent structures. (b) Schematic posterior view of the musculature of hypopharynx and adjacent esophagus (c) Finite element model of pharynx. Key Engineering Materials Vols. 270-273 2063 Title of Publication (to be inserted by the publisher) Fig. 2. Finite element model of pharyngeal muscular dysfunction The 3-D 8-node elements are used in each level (Fig. 1-(c)). As for loading condition, it is assumed that equal pressure is loaded sequentially to the inside of pharyngeal structure. The origin of the coordinate is located at the center of superior pharynx; medial-lateral and anterior-posterior directions are defined as x-axis and y-axis. The thickness of the pharyngeal tissue is assumed to be uniform in the model. The structure of the model is showed at Fig.2-(a). Pressure values are increased with each 6mmHg in the pressure range from 3mmHg to 36mmHg, The nodes on the uppermost level (base of tongue) are fixed and served as fixed boundary conditions. We assume that the central portion of the posterior pharyngeal geometry is constrained by the cervical spine, and this is also considered as a fixed boundary condition. In this study, pharyngeal muscular dysfunctions are classified into 3 cases as follows.(Fig 2-b),(c),(d)) Case1 : dysfunction of half in the medial-lateral direction in the model Case2 : dysfunction of 2, 3, 4 level in the model(mainly cricopharyngeal muscle) Case3 : dysfunction of 7, 8 level in the model(connection part of esophagus and pharynx) Bolus driving force in pharyngeal cavity can be expressed as pressure gradient. However, since the measurement of the pressure gradient is practically difficult, the value of the pressure in pharyngeal cavity is estimated by calculating the deformation of pharyngeal structure due to the change of pressure (3mmHg~36mmHg, in this study) by FEM, and comparing the value with the one obtained from CT image data. Taking into account the clinical complication by neuromuscular symptom such as pharyngeal dysfunction by stroke, may result in muscular tissue stiffness caused by the change of material property. Changes of cross section area of the pharynx are observed by increasing the stiffness by 25%, 50%, 75% on the basis of stress-strain relationship. Results Finite Element Analysis of Pharynx Subjected to Assumed Forcess. All input and output variables are presented with respect to the coordinate system fixed in the most superior level. The output 2064 Advances in Nondestructive Evaluation Title of Publication (to be inserted by the publisher) variables of the model are the resultant displacements of the internal lumen of the pharynx, and the pressure necessary to counterbalance the external load on pharyngeal wall. Each solution is obtained from an optimization procedure. The resultant counterbalance pressure magnitude is then equivalent to the intraluminal “swallowing” pressure. In general finite element analysis, geometry, the material properties, and loading conditions on the structure are known, and the nodal displacements (the deformations) are directly solved. However, in the present study, pharyngeal geometry of the “deformed” structure, which comes from cine CT image, is known, and the loading condition (in this case, pressure) remains as unknown variable (inverse to dynamic approach). A finite element method is used to determine geometry of pharynx during swallowing, corresponding to an assumed force history. The nodes on the uppermost level (base of tongue) are fixed and served as fixed boundary conditions. The central portion of the posterior pharyngeal geometry is assumed to be constrained by the cervical spine, which is also considered as a fixed boundary condition. The analysis is completed with a series of different assumed pressure patterns acting on the inner surface of the pharynx with spatial, as well as temporal, variation. A computer-predicted geometry of the pharynx is compared with the geometry of the pharynx as depicted by the cine CT scan images at corresponding instances. The difference between the observed geometry and the computer-predicted geometry is defined as a percent error and is to be minimized via multiple modeling iterations. When the percent error approximates zero, a good kinematic match occurs, and hence, the corresponding pressures are expected to be reliable estimates of the intraluminal pressure gradients of pharyngeal swallowing. Similarity between the result of the simulation of the change of cross section area due to the arbitrary pressure and that of measuring the pressure gradient by means of CT is obtained. The pharyngeal muscular dysfunction simulation by the model, i.e., pharyngeal tissue stiffness increases by 25%, 50%, and 75% each, is performed. From the result, the tendency of change of cross section area due to the stiffness of pharyngeal muscular tissue shows the maximum decrement when the pressure is at 30mmHg on the first level in half model. The cross-sectional area decrement ratio shows a trend to increase by 30 mmHg in all cases whereas it decreases after 30mmHg. The FEA results of pharyngeal muscular dysfunction show that, in the Case 1 model, when pressure increases by 9mmHg, the cross-sections of all levels show the decreasing ratio of 1%-8% when the stiffness increases by 25 %. When it is compared with the normal one, the upper part of the model on the basis of UES(Upper Esophageal Sphincter) shows 8-10 % decreasing ratio at 30 mmHg , 1) When the stiffness increases by 50%, the model shows the decreasing ratio of 15-21% , 2) When the stiffness increases by 75%, the model shows the decreasing ratio of 20-30% . And lower part (level 5,6,7,8) in Case 1 shows the decreasing ratio of 3-5 % at 36 mmHg when the stiffness increases by 25%, 1) When the stiffness increases by 50 %, the model shows the decreasing ratio of 5-12% . 2) When the stiffness increases by 75% , the model shows the decreasing ratio of 7-15% . In the Case 2 model (dysfunction of 2, 3, 4 level in the model), when pressure increases until 9mmHg, the cross-sections of all levels show the decreasing ratio of 1%- 7% when the stiffness increases by 25 %. When it is compared with the normal one, the upper part on the basis of UES (Upper Esophageal Sphincter) shows the decreasing ratio of 7-9 % at 30 mmHg, In the Case 3 model (dysfunction of 7, 8 level in the model), the level 7,8 (lower part ) shows the decreasing ratio of 2-5% at 36 mmHg when the stiffness increases by 25 %, Table .1 represents the results of all 3 case models simulation results. Key Engineering Materials Vols. 270-273 2065 Title of Publication (to be inserted by the publisher) Table 1. Estimated cress-sectional area decreasing ratio of pharynegeal muscular dysfunction Stiffness Increase Ratio(%) Range of decrease ratio (each level) Case1 Case2 Case3 125% 150% 175% L1234 L5678 8-10% 3-5% 15-21% 5-12% 20-30% 7-15% at 30mmHg at 36mmHg L123 L45 L678 L123456 L78 7-9% 5-6% Under 5% Under 7% 2-5% 15-18% 9-11% Under 5% Under 7% 4-9% 20-27% 12-15% under 5% Under 7% 6-12% at 30mmHg at 36mmHg at 36mmHg Discussion In this study, mathematical model of viscoelasticity of pharynx is implemented based on viscoelastic theory proposed by Y. C. Fung and the parameters of the model are obtained from experimental test. By way of three-dimensional reconstruction of pharyngeal structure by using optimization process based on inverse dynamic approach method and directly applying the results to the model, we may estimate consecutive pressure gradient of the pressure created internally when the pharynx functions. The change of the various pressure gradients in the pharyngeal structure was estimated by quasi-static method and the simulation results shows that the pressure gradient of the pharynx is changed in all levels from proximal to distal part. Also, maximal change of the pharyngeal deformation is observed at the anterior portions rather than at the posterior ones and localized stress concentration is assumed to be at the posterior region. From the model simulations, the trajectory of the pressure gradient in the pharynx by given deformation of each level’s pharyngeal cross section area is compared with previous investigations and shows similar patterns with those. Conclusions In this study we estimates pressure gradient of the pharynx in various pharyngeal muscular dysfunction cases caused by stiffness of tissue resulted in the tendency of cross sectional deformation change, applying the results as the clinical index to diagnosing the degree of abnormality of pharyngeal tissue. To make this method effective for the early diagnosis of pharyngeal dysfunction, the model should include various biomechanical parameters. Also, it is necessary to characterize the active mechanism of pharyngeal tissue by EMG measurement, The results can be applied as a useful diagnosis model which is able to discover pharyngeal disorder at an early stage and the mechanism of pharyngeal function. Such a biomechanical model can simulate the structural or pathological variation by the pharyngeal paralysis, cancer, tumor resection and pharyngo-esophageal stenosis. References [1] FMS. McConnel : Analysis of pressure generation and bolus transit during pharyngeal swallowing. Laryngoscope, Vol. 98, pp. 71-78, 1988. [2] 1Finestone HM, Greene-Finestone LS, Wilson ES, Teasell RW, Malnutrition in stroke patients on the rehabilitation service and at follow-up:prevalence and predictors . Arch Phys Med Rehabil Vol. 76, pp. 310-316, 1995. [3] Gordon C, Hewer RL, Wade DT, dysphagia in acute stroke , Br Med J vol. 295, pp. 411-414. [4] J.L.Elliott, "Swallowing disorders in the elderly", Geriatrics, vol. 43, pp. 95-113, 1988. 2066 Advances in Nondestructive Evaluation Title of Publication (to be inserted by the publisher) [5] DJ. Curtis, DF. Cruess and AH. Dachman, "Normal erect swallowing. Normal function and incidence of variations.", Invest Radiol, Vol. 20, pp. 717-726, 1985. [6] EM. Sokol, P. Heitmann, BS. Wolf and BR. Cohen, "Simultaneous cineradiographic and manometric study of the pharynx.", hypopharynx and cervical esophagus. Gastroenterology, Vol. 51, pp. 960-974, 1966. [7] P. Pouderoux, P. J. Kahrilas, "Deglutive tongue force modulation by volition, volume, and viscosity in humans.", Gastroenterology, Vol. 108 pp. 1418-1426, 1995. [8] Brasseur JG and Dodds WJ, "Interpretation of intraluminal manometric measurements in terms of swallowing mechanics", Dysphagia, Vol. 6, pp. 100-119, 1991. [9] Kim SM, McCulloch TM and Lim K., "Pharyngeal pressure analysis by the finite element method during liquid bolus swallow", Ann Otol Rhinol Laryngol, Vol. 109, No. 6, pp. 585-589, 2000. [10] Kim SM, McCllouch and TM, Rim K., "Evaluation of the Viscoelastic Properties of Pharyngeal Tissue", Tissue Eng, Vol. 4, No. 4, pp. 393-398, 1998. [11] Kahrilas, P. J., Logemann, J. A. and Gibbons, P., Food intake by maneuver; an extreme compensation for impaired swallowing, Dysphagia, Vol. 5,, pp. 155-160, 1992. [12] P. J. Kahrilas, J. Chen and J. A. Logemann, "Oropharyngeal Accommodation to swallow volume.", Gastroenterology, 1996. [13] P. J. Kahrilas, J. Chen and J. A. Logemann, "Three-dimensional modeling of the Oropharynx during swallowing.", Radiology, Vol. 194, pp. 575-579, 1995. [14] P. Pouderoux, P. J. Kahrilas, "Deglutive tongue force modulation by volition, volume, and viscosity in humans.", Gastroenterology, Vol. 108 pp. 1418-1426, 1995.
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