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SIMULATION ON AIRFLOW INSIDE THE NASAL CAVITY WITH AND WITHOUT UNCINATE PROCESS MUHAMMAD BIN NOR SHAKIIMAN Report submitted in partial fulfilment of the requirements for the award of the degree of Bachelor of Mechanical with Manufacturing Engineering Faculty of Mechanical Engineering UNIVERSITY MALAYSIA PAHANG DECEMBER 2010

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Page 1: SIMULATION ON AIRFLOW INSIDE THE NASAL CAVITY WITH …

SIMULATION ON AIRFLOW INSIDE THE NASAL CAVITY WITH AND WITHOUT UNCINATE PROCESS

MUHAMMAD BIN NOR SHAKIIMAN

Report submitted in partial fulfilment of the requirements for the award of the degree of

Bachelor of Mechanical with Manufacturing Engineering

Faculty of Mechanical Engineering UNIVERSITY MALAYSIA PAHANG

DECEMBER 2010

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vi

ABSTRACT

Functional Endoscopic Sinus Surgery (FESS) is proposed for people with chronic sinus problems who do not respond to medical therapy. During (FESS) procedure, removal of uncinectomy is necessary. Excision of the uncinate process (UP) is to open the maxillary sinus orifice. The UP is a small structure bone in nasal cavity and it's located under the middle turbinate membranes. However, some patients have claimed that the (FESS) process has reduces their smelling capabilities and voice impairment. Due to this, this study is focusing the effect of changes airflow pattern after remove the UP. The main objective of this study is to simulate, compare and analyze the flow properties inside the nasal cavity with and without UP. This simulation has been done with 3 different models of nasal cavity. The parameter for this simulation is 0.0075 m3 s 1 and 0.015m3s air flow rate at the inlet nostril and ambient pressure at the outlet throat. These simulation show positive result and this indicates that the removal of the UP will result smelling capabilities decrease and voice impairment.

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VII

ABSTRAK

Functional Endoscopic Sinus Surgery (FESS) dicadangkan untuk orang yang mempunyai masalah sinus yang kronik yang tidak mempunyai respon terhadap perubatan terapi. Semasa prosedur, penghapusan uncinectomy adalah sangat diperlukan. Penghapusan uncinate process (UP) adalah untuk membuka lubang sinus maksilaris. UP adalah tulang struktur kecil di dalam rongga hidung dan ia terletak di bawah selaput turbinate tengah. Namun, beberapa pesakit telah mendakwa bahawa pembedahan mi telah mengurangkan deria bau dan perubahan suara. Oleh hal yang demikian, tumpuan kajian mi adalah tertumpu kepada perubahan pola aliran udara selepas membuang UP. Tujuan utama dari penelitian mi adalah untuk mensimulasikan, membandingkan dan menganalisis sifat aliran dalam rongga hidung dengan dan tanpa UP. Simulasi mi telah dilakukan dengan 3 model rongga hidung yang berbeza. Parameter untuk simulasi mi adalah 0.0075 m3 s 1 dan 0.015 M3 s-1 dan lubang hidung inlet dan tekanan ambien tekak outlet. Simulasi mi menunjukkan hasil yang positif dan mi menunjukkan bahawa penghapusan UP akan mengakibatkan penurunan terhadap deria bau dan perubahan suara.

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Viii

TABLE OF CONTENTS

Page

SUPERVISOR'S DECLARATION 11

STUDENT'S DECLARATION

ACKNOWLEDGEMENTS V

ABSTRACT vi

ABSTRAK vii

TABLE OF CONTENTS viii

LIST OF TABLES Xl

LIST OF FIGURES Xli

LIST OF ABBREVIATIONS X1V

CHAPTER 1 INTRODUCTION

1.1 Project Background 1

1.2 Problem Statement 2

1.3 Objective 3

1.4 Scope of the Study 3

CHAPTER 2 LITERATURE REVIEW

2.1 Introduction 4

2.2 Anatomy 4

2.2.1 Nasal Cavity 4

2.2.2 Uncinate Process 5

2.2.3 Middle Meatus 5

2.2.4 Olfactory Mucous Membrane 7

2.2.5 Olfactory Nerves 7

2.3 Nasal Cavity Geometry 8

2.4 Standardized Geometry of The Human Nasal Cavity 10

2.5 Nasal Airway Boundary 12

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2.5.1 Steady state Boundary Condition 12 2.5.2 Unsteady Boundary Conditions 13

2.6 Changes of Nasal Airflow 13

2.6.1 Middle Turbinectomy 14 2.6.2 Inferior Turbinectomy 14

2.7 Unsteadiness of The Flow 15

2.7.1 Laminar and Turbulent Flow 15 2.7.2 Airflow Pattern 16

2.8 Airflow Studies In Nose 17

2.8.1 Digital Particle Image Velocimetry 18 2.8.2 CFD Simulation 20 2.8.3 Acoustic Rhinometry 21

CHAPTER 3 METHODOLOGY

3.1 Introduction 23

3.2 Methodology of Flow Chart 23

3.3 Computational Methods 25

3.4 Constructing Model of Nasal cavity 25

3.5 Solidwork Design 28

2.5.1 Drawing 28

3.6 Analysis with Cosmos (CFD) 32

3.6.1 Parameter Selection 32

3.7 Conclusion 33

CHAPTER 4 RESULT AND DISCUSSIONS

4.1 Introduction 34

4.2 Data Aquasition

4.2.1 Parameter Selection of Flow Analysis 34 4.2.2 Data Air Density with 0%, 50%, and 100% UP at

Flow Rate 0.0075 m3s' 35 4.2.3 Data Air Density with 0%, 50%, and 100% UP at

Flow Rate 0.0 15 m3 s' 37

4.3 Comparison Data Between Model of Nasal Cavity

with 0% and 100% UP

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4.3.1 Path Streamline 4

4.4 Percentage of Reducing Air Density 43

4.4.1 For Flow rate of 0.0075 m3 s 1 43 4.4.1 For Flow rate of 0.015 m 3 s 1 44

4.5 Ratio of Density 44

4.5.1 For Flow rate of 0.0075 m3s' 44 4.5.1 For Flow rate of 0.015 m 3 s 1 44

4.6 Discussion 45

CHAPTER 5 CONCLUSION AND RECOMMENDATIONS

5.1 Introduction 48

5.2 Conclusions 48

5.3 Limitation and Recommendation 48

REFERENCES

50

APPENDICES

A Gantt chart Final Year Project 1

52

B Gantt chart Final Year Project 2

53

C Flow Streamlines Nasal Cavity With 0%, 50% And 100% Up,

0.0075 m3s1

54

D Flow Streamlines Nasal Cavity With 0%, 50% And 100% Up,

0.015 m3s1

56

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LIST OF TABLES

Table No. Title Page

2.1 Subject and CT scan information for 30 individuals in current 11 study

3.1 Measurements of frontal/nostril regions from 7 sets of CT scans 25

3.2 Averaged dimensions of the nostril inlet plane compared with 26 final values for the Carleton-Civic Standardized Model

3.3 Dimension of nasal cavity 28

3.4 Boundary condition 32

4.1 Maximum density at upper turbinate 35

4.2 Average air velocity in nasal cavity with 0% and 100% UP 36

4.3 Maximum density at upper turbinate t 37

4.4 Average air velocity in nasal cavity with 0% and 100% UP 38

xi

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LIST OF FIGURES

Figure No. Title Page

2.1 Structure of lateral wall of nose. 6

2.2 Lateral wall of nose with middle turbinate removed 6

2.3 Lateral nose with olfactory nerves 8

2.4 3D model of the real nasal cavity 9

2.5 Simplified of 3D nasal cavity model with coronal section 10

2.6 Flow streamlines in the nasal cavity at different rate 17

2.7 Experimental model of nasal cavity 20

2.8 Rhinomanometer used to measure nasal inspiratory flow and 22

pressure

3.1 Flowchart of the Overall Methodology 24

3.2 Scale at top of image of nasal cavity in cm 27

3.3 Coronal plane images of nasal cavity 27

3.4 Sketching dimension of nasal cavity in solid work 29

3.5 Nasal cavity with 100% UP drawing 29

3.6 Nasal cavity with 50% UP drawing 30

3.7 Nasal cavity with 0% UP drawing 30

3.8 Front view of the constructed nasal cavity model 31

3.9 Drawing sketch view of nasal cavity 31

4.1 The comparison of density of air in \lpper turbinate against its 35 distance

4.2 Graph velocity of air in nasal cavity against iteration. 37

4.3 The comparison of density of air in upper turbinate against its 38 distance

xli

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All!

4.4 Graph velocity of air in nasal cavity against iteration 39

4.5 Air density for nasal cavity with 100% UP 40

4.6 Air density for Nasal cavity with 0% UP. 40

4.7 Flow streamline nasal cavity with 0% UP, 0.0075 m 3 s 1 41

4.8Flow streamline nasal cavity with 100% UP, 0.0075 m3s' 42

4.9 Flow Streamlines nasal cavity with 0% UP, 0.015 m3s-1 42

4.10 Flow streamline nasal cavity with 100% UP, 0.015 m3s-1 43

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LIST OF ABBREVIATIONS

UP Uncinate Process

CFD Computational Fluids Design

FESS Functional Endoscopic Sinus Surgery

OMCs Ostiomeatel complexes

CT Computed tomography

3D three-dimensional

RMS Root Mean square

DPIV Digital particle image of velucimetry

OW

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CHAPTER 1

INTRODUCTION

1.1 PROJECT BACKGROUND

Nowadays, we are facing with a various modern diseases. This is because, we

are exposed to a variety of ways such as disease spreads through dietary imbalance, air

pollution, viruses that spread and so forth. A disease that is quite popular among human

diseases associated with nose. Among them is sinusitis, sinus disease, paranasal sinus

cancer and so on. All of these diseases are very dangerous and complicated because it

has occurred in the nose and head. The surgery will have a hard decision and

complicated to finish it. A long time ago, nasal surgery has to operate through the nose

to remove the cancer. However today, new modern medical surgery have developed

new machine that can remove cancer in nose without operate through the face. They

called Functional Endoscopic Sinus Surgery (FESS).

Endoscopic sinus surgery is performed for those people who sinuses have

chronic or acute sinusitis that persists for greater than six weeks after maximum medical

therapy. Functional endoscopic sinus surgery (FESS) differs somewhat from the

conventional surgical approach to this problem in that it stresses a careful diagnostic

workup to try to identify the underlying cause of the problem, frequently in the anterior

ethmoid area, the area of the openings of the maxillary and frontal sinus. Sometimes,

with endoscopic sinus surgery examined may reveal a problem that can't be found with

another method. . The first step of (FE55) is excision of the uncinate process (UP) to

open the maxillary sinus orifice (Eitan Yaniv, 1997). This is because; the UP is located

at the beginning of nasal passage

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and removal of UP is necessary for entry into the interior of the nasal cavity. The UP is

a small structure bone in nasal cavity and it's located under the middle turbinate

membranes. In case, most patients claim that immediately after removal of UP, nasal

airflow significantly improves. This sensation last as long as the maxillary sinus orifice

remains patent.

The advantage of this procedure is that, in general, the surgery is less extensive,

there is often less removal of normal tissues, and the surgery can frequently be

performed on an outpatient basis without the necessity for nasal packing. In general, the

techniques are similar to those utilized for an intranasal ethmoidectomy, however, better

visualization is obtained during surgery by the use of endoscopes. The endoscopes also

allow problems in other sinuses to be viewed directly and, in many cases, for diseased

tissue to be removed.

1.2 PROBLEM STATEMENT

Until now, there is no strong evident whether the removal of UP will lead to post

operative complications or not. Some patients however, have claimed that the process

has decreased their smelling capabilities. Early postulation stated that the flow profile

during respiration will be different for the nasal cavity with and without the UP. In

addition, removal of the UP may influence the performance of smelling receptors in the

nose as result of flow profile alterations.

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1.3 OBJECTIVE

This research will focus on the two aims as follows:

i. To study the characteristic of airflow phenomenon inside the nasal cavity

with and without uncinate process.

ii. To simulate, compare and analyze the flow profiles inside the nasal

cavity with and without uncinate process.

iii. To relate the medical effect by removing the uncinate process.

1.4 SCOPE

The main scopes of this research are:

i. The percentage of uncinate process removal will be studied to see the

effect on the flow profile inside the nasal cavity.

ii. The airflow phenomenon from the throat until the nostril will be obtained

iii. The inferior and middle turbinate must be considered impact in nasal

cavity.

iv. Medical effect will be neglected. Only the difference of density, velocity

and flow profile will be considered in this experiment.

V. The range of age patient is between 20 to 30 years old.

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CHAPTER 2

LITERATURE REVIEW

2.1 INTRODUCTION

The purpose of this chapter is to provide a review past research related to the

geometry in nasal cavity, mechanics of airflow, airflow profile and airflow

characteristic in the human nasal airways.

2.2 ANATOMY

Understanding the anatomy of nasal cavity is important and its anomalies are

important because it leads of imaging anatomy, which is needed to plan of constructing

the model.

2.2.1 NASAL CAVITY

Nasal cavity is a large fluid filled space above and behind the nose in the middle

of the face plays an important role in breathing. The nasal cavity is divided into a right

and left passageway by a vertical fin called nasal septum. This cavity runs along the top

of the palate (the roof of the mouth, the shelf that separates your nose from your mouth)

and turns downward to join the passage from the mouth to the throat. Sinuses are

cavities or small tunnels. They are called paranasal because they are around or near the

nose. The nasal cavity and paranasal sinuses help filter, warm, and humidify the air you

breathe. They also give your voice resonance, lighten the weight of the skull, and

provide a bony framework

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for the face and eyes. According to Mygind and Dahl in its entirety consists of a 5cm

high and 10 cm chamber long chamber (D.J. Doorly et al., 2008). The internal walls

opposite the nasal septum have ridges formed bone called conchae (turbinate) bones.

Under and lateral to each turbinate are passages called the inferior, middle and superior.

These turbinates disrupt the airflow, directing air toward the olfactory epithelium on the

surface of the turbinates and the septum. Below of middle turbinate have a bone called

uncinate process. This UP is a one of the structure bone in nasal cavity.

2.2.2 UNCINATE PROCESS

The Uncinate Process (UP) which form part of the anterior ostiomeatel

complexes (OMCs), is one of the most important bony structure. The UP is acts as an

air vent shield which is preventing direct inspiration of air into the maxillary sinus and

protecting the egress of the mucociliary clearance. The UP is the first structure to be

identified and surgically removed because it is located at central to Functional

Endoscopic Sinus Surgery (FESS). The UP arises from the lateral wall and occasionally

from the inferior turbinate and projects into the airway of nasal cavity.

2.2.3 MIDDLE MEATUS

Middle meatus located in posterior half of the lateral wall. In the middle meatus

is rounded bulge call bulla ethmoidalis which is due to the middle ethmoidal air cell

which is open or above it. The UP is formed on the floor and medial wall of the ethmoid

(PL Dhingra, 1998). Figure 2.1 and figure 2.2 show the structure of lateral wall in

human nose.

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Frontal sinu

Superior nasal conchs (turbina

Superior nasal meatus

Middle nasal concha (turbinate).

Agger nasI....

Atrium of middle nasal meatus

Middle nasal meatus

Inferior nasal concha

Inferior nasal meatus —

Palatine process of maxi

Incisive canal,

Tongue

Opening of nasofi

Semilunar hi

LJncinaie proces

Opening of maxillary sinus

Inferior nasal

Eihmoidal cells

Opening of sphenoidal sinus

Sphenoidal sinu

Middle nasal concha (cu( away)

Sphenoethmoidal recess

_ Opening of sphenoidal sinus

_- I-Iypophysis (pituitary gland) In sella turcica

Sphenoidal sinus

Pharyngeal tonsil (adenoid if enlarged)

Basilar part of occipital bone Pharyngobasilar fascia

Nasopharyngeal opening

Torus tuharius Openingof auditory (Eustachian) tube Pharyngeal recess

Horizontal plate of palatine bone

Soft palate

Figure 2.1: Structure of lateral wall of nose

Source: Dr. Wan Islah, (2010)

Figure 2.2: Lateral wall of nose with middle turbinate removed

Source: Dr. Wan Islah, (2010)

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2.2.4 OLFACTORY MUCOUS MEMBRANE

Smell receptors is chemeoreceptors that are stimulated by molecules in solution

mucus in the nose. The smell receptors are distance receptors and there is no neocortical

projection area for olfaction. The olfactory receptors are located in a specialized portion

of the nasal mucosa. The olfactory mucous membrane is constantly covered by mucus.

The axons of the olfactory receptors neurons pierce the cribriform pate of the ethmoid

bone and enter the olfactory bulbs. The olfactory neurons, like the taste receptors

(William F. Ganong, 1999).

2.2.5 OLFACTORY NERVES

One of a pair of nerves associated with the sense of smell. They are composed of

numerous fine filaments that ramify in the mucous membrane of the olfactory area. The

fibers of the olfactory nerve are nonmedullated and unite into fasciculi that form a

plexus under the mucous membrane and rise in grooves or canals in the ethmoid bone.

The fibers pass into the skull and form synapses with the dendrites of the mitral cells.

The area in which the olfactory nerves arise is situated in the most superior part of the

mucous membrane that covers the superior nasal concha. The olfactory sensory endings

are modified epithelial cells and the least specialized of the special senses. The olfactory

nerves connect with the olfactory bulb and the olfactory tract, which are components of

the part of the brain associated with the sense of smell. Figure 2.3 shows the located of

the olfactory bulb in human nose.

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Oftc1ry bu Qliac trac crbraJ Crn

1&ct

bonj

Fbers or o1facory nors

Figure 2.3: Lateral nose with olfactory nerves

Source: Mosby's Medical Dictionary, 8th edition, {2009)

2.3 NASAL CAVITY GEOMETRY

A nasal cavity was obtained with computer tomography (CT) scan. CT scan

will capture outlined slices in the X-Y pane at the different position along the Z axis

from the entrance of nasal cavity to anterior of the larynx at interval 1-5mm. The image

sectioned scans were imported with modeling program software called GAMBIT into a

3D image. This software will created a smooth curve that connected point on the other

coronal section (S.M Wang et al., 2009). Image from CT scan also can be process with

MIMICS software. Mimics is an image processing software package for 3D design and

modeling. Mimics generates and modifies surface 3D models from stacked medical

images such as CT scan, Confocal Microscopy, Micro CT, and Magnetic Resonance

Imaging (MRI) through image segmentation done in the STL format. From the

segmented image, data captured by CT scan, a surface triangular mesh that modeled the

surface of the nasal cavity. The mesh was use as input to the volume grid generator and

to comply with a set of constraints and quality measures dictated by the grid generator

and the CFD software (M. Kieven et,al., 2005).

An anatomically correct replica model with inferior and middle turbinate is

constructed. The superior turbinate is neglected where it is always vestigial in the

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average human nasal passage. The anatomical middle turbinate will be denoted as upper

turbinate and the inferior turbinate as lower turbinate. The geometry of the nasal cavity

includes besides lower and upper turbinate also cartilage spurs. These are illustrated

together with a coronal cross section. The real nasal geometry has been extracted from a

CT scan data set. A centered cube, enclosing the complete geometry, generates an initial

grid. The grid is repeatedly refined and newly generated grid cells, which do not occur

inside the geometry. An alternating digital tree algorithm (ADT) does the refinement (I.

Hörschler et al., 2009). Figure 2.4 and figure 2.5 show the constructed of real and

simplified 3D nasal cavity model.

( -

Figure 2.4: 3D model of the real nasal cavity

Source: I. Hörschler et al., (2009)

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lEl]

C

Figure 2.5: Simplified of 3D nasal cavity model with coronal section

Source: I. Hörschler et al., (2009)

2.4 STANDARDIZED GEOMETRY OF THE HUMAN NASAL CAVITY

A standardized geometry of human nasal cavity was created by aligning and

processing 30 sets of computed tomography (CT) scans of nasal airways. The 3D

geometries of the single 60 single human nasal cavities were generated from the CT

scans. The measurements of physical parameters of each single nasal cavity were

performed. A methodology was developed to scale, orient and align the nasal

geometries, after which 2D digital coronal cross sectional slices were generated. (Y.

Liu, M. R. Johnson, E. A. Matida, S. Kherani, and J. Marsan, 2009). Table 2.1 show

the data collection of CT scan from various person.

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Table 2.1 Subject and CT scan information for 30 individuals in current study

Subject Distance Between Resolution in x-y Number of No. Sex Age Slices, mm Plane, mmlpixel Scan Planes

1 F 45 2.5 0.325 38

2 M 59 2.5 0.325 40

3 F 63 2.0 0.24 39

4 F 36 2.5 0.325 38

5 F 20 2.5 0.325 40

6 F 49 2.0 0.325 36

7 F 30 2.5 0.325 32

8 M 74 2.5 0.325 43

9 M 60 2.5 0.325 42

10 F 17 2.5 0.325 39

11 M 56 2.5 0.325 40

12 M 52 2.5 0.325 44

13 M 39 2.5 0.325 40

14 F 37 2.5 0.325 38

15 M 52 2.5 0.3 43

16 M 41 2.5 0.293 39

17 F 78 2.5 0.339 43

18 F 26 2.5 0.245 41

19 M 52 2.5 0.283 42

20 F 23 2.5 0.313 44

21 M 52 2.5 0.325 39

22 F 45 2.5 0.325 34

23 F 52 2.5 0.325 38

24 F 30 2.5 0.325 45

25 F 34 2.5 0.325 41

I

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26 F 66 1.0 0.348 80

27 F 49 2.5 0.325 42

28 M 36 2.5 0.325 40

29 M 42 2.5 0.293 47

30 M 45 2.5 0.293 40

Average 45.3 2.42 0.315 41.6

Median 45 2.5 0.325 40

Max 78 2.5 0.348 80

Min 17 1 0.24 32

M, male; F, female.

Source: Y. Liu, M. R. Johnson, E. A. Matida, S. Kherani, and J. Marsan, (2009)

2.5 NASAL AIRWAY BOUNDARY

In reality, model of nasal cavity are very complicated. The airways boundary is

time varying, possibly compliant at elevated flow and covered for the most part by a

thin film of mucus (M. Kleven et.al., 2005). The structures outside of the nasal cavity

itself affect the flow dynamic during respiratory where the shape of the external nose

influence flow entering the nares. During the expiration, the exhaled now will

impressed the airways geometry below the nasopharynx. Until today, no model has yet

completed with all these features. The flow is considered as a laminar flow through a

confined geometry that is representing a nasal cavity. Boundary conditions are therefore

required along the cavity walls and at the inflow and outflow boundaries as well. These

are the assumptions of the physiological conditions. These conditions are in principle

periodically in time with changing main flow direction for inspiration and expiration.

The flow can be assumed quasi-stationary according to the breathing frequency is

Sufficiently small (M. Finck et al., 2007).

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2.5.1 STEADY STATE BOUNDARY CONDITION

A no-slip isothermal condition with Twa ii = T. and a zero pressure gradient

normal to the wall are imposed on the wall. The 1-Dimensional energy equation for

compressible, isentropic flow can be used in a modified form at the inflow boundary to

interactively compute the static pressure from the given value of the velocity

distribution. The quantity of velocity distribution is an integral value for the inflow

cross section such that the actual velocity distribution has to be prescribed as an

additional condition by assuming a fully developed flow. On the outflow boundary, the

static pressure level is imposed (I. Hörschler et al., 2009).

2.5.2 UNSTEADY BOUNDARY CONDITIONS

The conditions on the wall are no slip, isothermal and zero normal pressure

gradient, still hold in time-dependent flows. To mimics the unsteady flow of the human

respiration cycle respiration is understood as an isentropic expansion from a steady

ambient state with stagnation pressure for the inflow boundary at the nostril. At

expiration, the outflow and inflow boundaries are exchange. That is, expiration the

throat boundary is the inflow boundary. As isentropic expansion from a steady state is

generated through a time dependent stagnation pressure in the throat, where as a

constant pressure at the nostril (I. Hörschler et al., 2009).

2.6 CHANGES OF NASAL AIRFLOW

Changes in the nasal air were studied for pathologic conditions such as the

presence of polyps, swelling, atrophy or resection of tubinates, and for enlarged

adenoids (Tonndorf, 1939). The presence of polyps in the superior meatus, and

generalized swelling of the turbinates seem to have the most effect on airflow pattern.

The effect of various kind of turbinectomy on nasal airflow of great interest to

rhinologists who must consider such aspects of surgical treatment prior to treating nasal

obstruction (Seung-Kyu Chung, 2008).

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2.6.1 MIDDLE TURBINECTOMY

The middle turbinate is located in the anterior portion of the middle nasal airway

and its shape is thought to have an important influence in nasal airflow. The exact shape

and size of the middle turbinate not indentified yet but it may be reshaped partially

during endoscopic sinus surgery. By using DPIV methods, it can be measures the

changes of nasal cavity by using three different models of turbinectomy. There are

partial, anterior partial and total middle turbinectomy (Kim and Chung, 2004). The

airflow through the upper airway including the middle meatus was increased in that

threeturbiflectOmiZed model. The airflow was identified in term of RMS velocity.

However, there are different results showing that the middle turbinate did not influence

the overall flow pattern during expiration and inspiration with numerical and DPIV

studied using schematic nasal cavity models (Hörschler et al., 2006; Kim and Chung,

2008). The RMS velocity is consistently increase after the turbinectomy with the

occurrence of eddies following atrophy or for a resected middle turbinate in nasal cavity

(Torndorf, 1939; Kim and Chung, 2008).

2.6.2 INFERIOR TURBINECTOMY

Many turbinate procedures are done worldwide to enlarge the valve area and the

inferior airway because of the enlargement of the inferior turbinate is considered as a

major cause of nasal obstruction. The DPIV method was used to investigate the effect of

three kind of inferior turbinectomy - partial, anterior partial and total inferior

turbinectomy on nasal cavity, the main airflow through the middle airway, including the

middle meatus, was not overly different between the two partial turbinectomy models.

The main pathway of airflow in the totally resected model was altered in the middle and

inferior airways and the lateral portion of the enlarged airways was filled with very low

flow that was indicative of eddies. The RIvLS velocity was increase in the two partially

operated models, in the total inferior turbinectomy model, the lowest airway was not

used as effective air tract. The inferior turbinate and spurs seemed to serve a guide vane

to ensure a homogeneous velocity distribution in the nasal cavity channel. In the total

resection of the inferior turbinate, the airflow was characterized by massive vortices that

impacted ion flow distribution in the nasal cavity (Hörschler et al., 2006; Kim and