4 research outputs found
νλ¦μ΄ μ±κ² μμ μ λ―ΈμΉλ μν₯
νμλ
Όλ¬Έ(μμ¬)--μμΈλνκ΅ λνμ :곡과λν 건μ€ν경곡νλΆ,2019. 8. ν©μ§ν.Complex hydrodynamic structures inside the benthic boundary layer influence various biological process of marine ethology. The external fertilization of sea urchins is one of the biological mechanism which highly depend on flow conditions of boundary layer. To explain fertilization process from perspective of mechanics, the analysis of fluid structure near sea urchins should be preceded. In general, turbulent boundary layers are developed near rough walls and behind streamline objects, and variations of flow structure generate complex hydrodynamic structures. Gametes released from sea urchins are transported via surrounding flow to reach collision and fertilization with different sex through complex interaction with hydrodynamic structures.
The main objective of corresponding study is to analyze the flow effects on sea urchin fertilization. Fertilization rate is explored for uni-directional flow with free stream velocity ranging from 0.025 to 0.2 m/s to analyze the effect of velocity on fertilization and relative contribution of different locations (aboral, wake, substrate, and water column). As velocity increases, fertilization decreases and wake had most influence on total fertilization in general. Corresponding study is progressed in three steps. First, hydrodynamic characteristics near sea urchin and trajectory of gametes are simulated through Lagrangian Particle Tracking. Second, actual eggs being fertilized are computed based on relative distance between gametes of different sex and nearby sperm concentration. Last, contribution of each location on fertilization is computed and fertilization process is explained by hydrodynamic structures around sea urchin.
Corresponding study suggest mechanical perspective to understand biological process and Computational Fluid Dynamics (CFD) as possible tool to simulate fertilization process of sea urchins. The methods applied to this study can help analyze various engineering or scientific problems that are driven by turbulent mixing and reaction between particles. It suggests wider perspective and possibilities to study complex processes which requires analysis of both particles and background flow.ν΄μ κ²½κ³μΈ΅ λ΄λΆμ 볡μ‘ν μ 체μνμ ꡬ쑰λ ν΄μ μνκ³μ λ€μν μλ¬Όνμ νμμ μ§λ°°νλ μ£Όμ μΈμμ΄λ€. μ±κ²μ λ²μ κ³Όμ μ 체μΈμμ μ ν΅ν΄ μ΄λ£¨μ΄μ§λ©° κ²½κ³μΈ΅ λ΄μ νλ¦ μ‘°κ±΄μ μμ‘΄νλ€. λ°λΌμ μ±κ²μ μμ κ³Όμ μ μνμ μΌλ‘ μ€λͺ
νκΈ° μν΄μλ μ£Όλ³ μ 체μ λν μ΄ν΄κ° μ νλμ΄μΌ νλ€. μΌλ°μ μΌλ‘ κ±°μΉ λ°λ₯κ³Ό μ μ ν 물체 λ€μμλ λλ₯ κ²½κ³μΈ΅μ΄ νμ±λλ©°, κ²½κ³μΈ΅ λ΄λΆμ κΈκ²©ν μ 체 ꡬ쑰 λ³νλ λλ₯ νΌν©μ λ°μμν¨λ€. μ±κ²μ λͺΈμ²΄μμ λ°©λ₯λ μμ μΈν¬λ μ΄λ¬ν λλ₯ νΌν©μ μν΄ μλ‘ λ§λκ³ μμ λλ€.
λ³Έ μ°κ΅¬μ λͺ©μ μ μ±κ² μμ μ μμΉκ° λ―ΈμΉλ μν₯μ νλ¦ μ‘°κ±΄μ λ°λΌ νμ
νλ κ²μ΄λ€. λ¨μΌ λ°©ν₯ νλ¦ μ‘°κ±΄μμ μ μ λ²μκ° 0.025 β 0.05 m/s μΌ λ, μμ λ₯ μ κ³μ°νμμΌλ©° μ μμλ³λ‘ (Aboral, Wake, Substrate, Water Column) μ 체 μμ λ₯ μ λ―ΈμΉλ μλμ μν₯λ ₯μ νμ
νμλ€. μλκ° μ¦κ°ν μλ‘, μμ λ₯ μ κ°μνλ νμμ 보μμΌλ©°, μ λ°μ μΌλ‘ Wakeμ§μμμ κ°μ₯ λ§μ μμ μ΄ μΌμ΄λ¬λ€. μ°κ΅¬λ 3λ¨κ³λ‘ μ§νλλ©° μμλ λ€μκ³Ό κ°λ€. 첫 λ²μ§Έ, μμΉ λͺ¨μλ₯Ό ν΅ν΄ ꡬ쑰물 νλ₯μ ꡬ쑰λ₯Ό νμ
νκ³ μ
μ νμ° κΆ€μ μ Lagrangian Particle Tracking (LPT)μ ν΅ν΄ ꡬννλ€. λ λ²μ§Έ, λμμ μ μ μ¬μ΄μ 거리μ μ μμ λ°λλ₯Ό λ°νμΌλ‘ μμ λ μμμΈν¬λ₯Ό νμ
νλ€. λ§μ§λ§ λ¨κ³λ μ 체 ꡬ쑰λ₯Ό λ°νμΌλ‘ μ΄ 4κ°λ‘ λλ μ μμμ΄ μ 체 μμ μ λ―ΈμΉλ μλμ μν₯λ ₯μ λΆμνλ€.
λ³Έ μ°κ΅¬λ μ νμ°κ΅¬μμ μ€νμΌλ‘ λͺ¨μν μ±κ²μ μμ κ³Όμ μ μμΉ λͺ¨λΈλ§μ ν΅ν΄ ꡬννκ³ μνμ κ΄μ μΌλ‘ νμ₯νμ¬ λΆμνλλ° μμκ° μλ€. λ³Έ μ°κ΅¬μ μ μ©λ λ°©λ²λ‘ μ ν΅ν΄ λλ₯ νμ°κ³Ό μ
μ μ¬μ΄μ λ°μ μμ©μ μν΄ λ°μνλ λ€μν 곡νμ μμ°κ³Όνμ νμμ μ°κ΅¬ ν μ μμΌλ©° μ
μμ κΆ€μ κ³Ό μ μ μ₯μ λμμ κ³μ°ν΄μΌνλ 볡μ‘ν λ¬Έμ μ λν ν΄κ²°μ±
μ μ μνλ€.ABSTRACT i
TABLE OF CONTENTS iii
List of Figures v
List of Tables vii
List of Symbol viii
CHAPTER 1. INTRODUCTION 1
1.1 General introduction 1
1.2 Objectives 4
CHAPTER 2. THEORETICAL BACKGROUNDS 6
2.1 Fertilization process of sea urchin 6
2.1.1 External fertilization of sea urchin 6
2.2.2 Analytical models to explain external fertilization 7
2.2.3 Precedent and present research 8
2.2 Flow structure in the benthic boundary layer 11
2.2.1 Boundary boundary layer 11
2.2.2 Flow structures behind a sea urchin 12
2.2.3 Turbulent motions 13
2.3 Particle-laden flow 16
2.3.1 Introduction to particle-laden flown 16
2.3.2 Quantification of particle distribution 20
CHAPTER 3. METHODOLOGY 23
3.1 Numerical model description 23
3.1.1 Governing equations for fluid motion 24
3.1.2 Lagrangian particle tracking 25
3.1.3 Contact and fertilization detection algorithm 27
3.2 Simulation setup 31
3.3 Model validation 34
3.3.1 Model convergence 34
3.3.2 Comparison with laboratory experiment 38
CHAPTER 4. Results and discussion 43
4.1 Collision and fertilization 43
4.2 Flow structure analysis 49
4.3 Analysis of sea urchin fertilization process 57
4.3.1 Distribution of sea urchin gametes 57
4.3.2 Sperm density 67
4.3.3 Analysis of contact rate and fertilization rate 71
4.4 Relative contribution of different locations on fertilization 72
CHAPTER 5. Conclusion 77
5.1 Summary 77
5.2 Recommendation and future works 79
REFERENCES 80
κ΅λ¬Έμ΄λ‘ 85Maste
Quantifying the Response of Grass Carp Larvae to Acoustic Stimuli Using Particle-Tracking Velocimetry
Acoustic deterrents are recognized as a promising method to prevent the spread of invasive grass carp, Ctenopharyngodon idella (Valenciennes, 1844) and the negative ecological impacts caused by them. As the efficacy of sound barriers depends on the hearing capabilities of carp, it is important to identify whether carps can recognize acoustic signals and alter their swimming behavior. Our study focuses on quantifying the response of grass carp larvae when exposed to out-of-water acoustic signals within the range of 100β1000 Hz, by capturing their movement using particle-tracking velocimetry (PTV), a quantitative imaging tool often used for hydrodynamic studies. The number of responsive larvae is counted to compute response ratio at each frequency, to quantify the influence of sound on larval behavior. While the highest response occurred at 700 Hz, we did not observe any clear functional relation between frequency of sound and response ratio. Overall, 20β30% of larvae were consistently reacting to sound stimuli regardless of the frequency. In this study, we emphasize that larval behaviors when exposed to acoustic signals vary by individual, and thus a sufficient number of larvae should be surveyed at the same time under identical conditions, to better quantify their sensitivity to sound rather than repeating the experiment with individual specimens. Since bulk quantification, such as mean or quantile velocities of multiple specimens, can misrepresent larval behavior, our study finds that including the response ratio can more effectively reflect the larval response