Difference between revisions of "Izzuddin Al Qossam"
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The lid-driven cavity flow problem is a classical benchmark problem in fluid dynamics used to study the behavior of incompressible fluid flow inside a square or rectangular cavity. The cavity is typically closed on all sides, but the flow is induced by moving one of the cavity walls (the "lid") at a constant velocity, while the other walls remain stationary. The problem is a simplified model of fluid motion, and it helps test numerical methods for solving the Navier-Stokes equations, which describe fluid flow. The lid-driven cavity flow problem is often solved using numerical methods such as finite difference, finite element, or spectral methods to discretize and solve the Navier-Stokes equations. | The lid-driven cavity flow problem is a classical benchmark problem in fluid dynamics used to study the behavior of incompressible fluid flow inside a square or rectangular cavity. The cavity is typically closed on all sides, but the flow is induced by moving one of the cavity walls (the "lid") at a constant velocity, while the other walls remain stationary. The problem is a simplified model of fluid motion, and it helps test numerical methods for solving the Navier-Stokes equations, which describe fluid flow. The lid-driven cavity flow problem is often solved using numerical methods such as finite difference, finite element, or spectral methods to discretize and solve the Navier-Stokes equations. | ||
− | Recent research on the use of the k-epsilon turbulence model in lid-driven cavity flows, especially combined with heat transfer analysis, has shown interesting developments. The k-epsilon model remains widely used due to its balance between computational efficiency and accuracy when dealing with turbulent flows, including cavity-driven setups. It helps in understanding the turbulence production and dissipation within the cavity, which significantly affects the heat transfer characteristics. In some research, the heat transfer characteristics are influenced by aspect ratio and shape of cavity, artificial roughness, and boundary conditions[[https://www.academia.edu/67765943/Effect_of_cavity_aspect_ratio_on_flow_and_heat_transfer_characteristics_in_pipes_a_numerical_study]][[https://pubs.aip.org/aip/pof/article-abstract/30/2/025103/363479/Mixed-convection-heat-transfer-enhancement-in-a?redirectedFrom=fulltext]][[https://doiserbia.nb.rs/Article.aspx?ID=0354-98362400056M]]. | + | Recent research on the use of the k-epsilon turbulence model in lid-driven cavity flows, especially combined with heat transfer analysis, has shown interesting developments. The k-epsilon model remains widely used due to its balance between computational efficiency and accuracy when dealing with turbulent flows, including cavity-driven setups. It helps in understanding the turbulence production and dissipation within the cavity, which significantly affects the heat transfer characteristics. In some research, the heat transfer characteristics are influenced by aspect ratio and shape of cavity, artificial roughness, and boundary conditions [[https://www.academia.edu/67765943/Effect_of_cavity_aspect_ratio_on_flow_and_heat_transfer_characteristics_in_pipes_a_numerical_study]][[https://pubs.aip.org/aip/pof/article-abstract/30/2/025103/363479/Mixed-convection-heat-transfer-enhancement-in-a?redirectedFrom=fulltext]][[https://doiserbia.nb.rs/Article.aspx?ID=0354-98362400056M]]. |
• Aspect Ratio and Shape: The aspect ratio and shape of the cavity influence the flow and heat transfer. Aspect ratio (AR) is cavity width divided by cavity depth. Higher aspect ratios generally enhance heat transfer, while different shapes (rectangular, triangular, circular) show varying efficiencies [[https://pubs.aip.org/aip/pof/article-abstract/35/3/033114/2881958/Effect-of-cavity-aspect-ratio-on-mixed-convective?redirectedFrom=fulltext]][[https://www.researchgate.net/publication/235897506_Numerical_study_of_flow_and_thermal_behaviour_of_lid-driven_flows_in_cavities_of_small_aspect_ratios]][[https://www.jstage.jst.go.jp/article/jtst/11/1/11_2016jtst0012/_article]]. | • Aspect Ratio and Shape: The aspect ratio and shape of the cavity influence the flow and heat transfer. Aspect ratio (AR) is cavity width divided by cavity depth. Higher aspect ratios generally enhance heat transfer, while different shapes (rectangular, triangular, circular) show varying efficiencies [[https://pubs.aip.org/aip/pof/article-abstract/35/3/033114/2881958/Effect-of-cavity-aspect-ratio-on-mixed-convective?redirectedFrom=fulltext]][[https://www.researchgate.net/publication/235897506_Numerical_study_of_flow_and_thermal_behaviour_of_lid-driven_flows_in_cavities_of_small_aspect_ratios]][[https://www.jstage.jst.go.jp/article/jtst/11/1/11_2016jtst0012/_article]]. | ||
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Khalid N. Alammar (2006) [[https://www.academia.edu/67765943/Effect_of_cavity_aspect_ratio_on_flow_and_heat_transfer_characteristics_in_pipes_a_numerical_study]] found that the primary mechanism of heat transfer enhancement is turbulence generated by cavities. In a two-dimensional simulation using the standard k-ε turbulence model, cavities with higher aspect ratios showed enhanced heat transfer more than those with lower aspect ratios. Higher aspect ratios generated more complex vortex structures, contributing to both increased Nusselt numbers and higher pressure drops. The artificial roughness introduced on the heated bottom wall of a cavity containing a rotating cylinder was investigated by Ali Khaleel Kareem and Shian Gao (2018) [[https://pubs.aip.org/aip/pof/article-abstract/30/2/025103/363479/Mixed-convection-heat-transfer-enhancement-in-a?redirectedFrom=fulltext]]. The presence of additional roughness with a rotating cylinder significantly | Khalid N. Alammar (2006) [[https://www.academia.edu/67765943/Effect_of_cavity_aspect_ratio_on_flow_and_heat_transfer_characteristics_in_pipes_a_numerical_study]] found that the primary mechanism of heat transfer enhancement is turbulence generated by cavities. In a two-dimensional simulation using the standard k-ε turbulence model, cavities with higher aspect ratios showed enhanced heat transfer more than those with lower aspect ratios. Higher aspect ratios generated more complex vortex structures, contributing to both increased Nusselt numbers and higher pressure drops. The artificial roughness introduced on the heated bottom wall of a cavity containing a rotating cylinder was investigated by Ali Khaleel Kareem and Shian Gao (2018) [[https://pubs.aip.org/aip/pof/article-abstract/30/2/025103/363479/Mixed-convection-heat-transfer-enhancement-in-a?redirectedFrom=fulltext]]. The presence of additional roughness with a rotating cylinder significantly | ||
+ | [[File:izaq1.jpg]] | ||
+ | Fig 1. a. Circulation inside a cavity; AR = 3, b. Circulation inside a cavity; AR = 6 (Khalid, 2006) | ||
+ | [[File:izaq2.jpg]] | ||
− | increased the turbulent kinetic energy, contributing to better heat transfer. Employing the Unsteady Reynolds-Averaged Navier-Stokes (URANS) equations with a standard k-ε turbulence model, the simulation results can be inferred that the advanced heat transfer was more prominent at higher Reynolds numbers. Gnanasekaran Manogaran and Satheesh Anbalagan (2024) [[https://doiserbia.nb.rs/Article.aspx?ID=0354-98362400056M]] also confirmed that higher intensity of turbulence kinetic energy results in enhanced heat transfer. Using the k-ε turbulence model and the FVM (Finite Volume Method)-based SIMPLE algorithm, the study figured that as the speed ratio (S=U_bottom/U_top) increased, secondary vortices were formed, and the primary vortex shrank. The primary vortex was larger at lower speed ratios and got displaced as the speed ratio and Reynolds numbers increased. Lower aspect ratios (K = 0.5) resulted in higher intensity of turbulence kinetic energy and dissipation rates near the top of the cavity. Increasing the aspect ratio decreased the concentration of turbulence but distributed it more uniformly across the cavity. | + | Fig 2. a. Turbulence kinetic energy distribution, and b. Nusselt numbers distribution near cavities (Khalid, 2006) |
+ | |||
+ | |||
+ | increased the turbulent kinetic energy, contributing to better heat transfer. Employing the Unsteady Reynolds-Averaged Navier-Stokes (URANS) equations with a standard k-ε turbulence model, the simulation results can be inferred that the advanced heat transfer was more prominent at higher Reynolds numbers. Gnanasekaran Manogaran and Satheesh Anbalagan (2024) [[https://doiserbia.nb.rs/Article.aspx?ID=0354-98362400056M]] also confirmed | ||
+ | |||
+ | [[File:izaq3.jpg]] | ||
+ | |||
+ | Fig 3. The schematic diagrams of the lid-driven cavity containing a rotating cylinder in the cases of a. square (S), b. square ribs (R-s), and c. half-circle ribs (R-c) (Ali & Shian, 2018) | ||
+ | |||
+ | |||
+ | that higher intensity of turbulence kinetic energy results in enhanced heat transfer. Using the k-ε turbulence model and the FVM (Finite Volume Method)-based SIMPLE algorithm, the study figured that as the speed ratio (S=U_bottom/U_top) increased, secondary vortices were formed, and the primary vortex shrank. The primary vortex was larger at lower speed ratios and got displaced as the speed ratio and Reynolds numbers increased. Lower aspect ratios (K = 0.5) resulted in higher intensity of turbulence kinetic energy and dissipation rates near the top of the cavity. Increasing the aspect ratio decreased the concentration of turbulence but distributed it more uniformly across the cavity. | ||
+ | |||
+ | [[File:izaq4.jpg]] | ||
+ | |||
+ | Fig 4. a. The isotherm, b. the streamline and velocity magnitude contours for different Reynolds numbers, 5000 and 10 000, and bottom wall conditions (S, R-s) at -5 ≤ Ω ≤ 5 (Ali & Shian, 2018) | ||
+ | |||
+ | |||
+ | [[File:izaq5.jpg]] | ||
+ | |||
+ | Fig 5. Effect of speed ratio (S) and Reynolds numbers on streamline contours at aspect ratio (K) = 1.0 (Gnanasekaran & Satheesh, 2024) |
Revision as of 14:20, 31 October 2024
Background
Penelitian saya terkait steam combustion pada incinerator MSW. Kegiatan ini merupakan kolaborasi antara Laboratorium Gasifikasi dan PT Bumiresik Nusantara Raya. Permasalahan yang ingin diselesaikan adalah bagaimana asap pembakaran sampah pada incinerator menjadi lebih bersih dan tidak terjadi overheated. Salah satu inovasi yang coba dikembangkan adalah intermittent furnace dengang dual chamber. Primary chamber menggunakan sistem superheated steam untuk meningkatkan suhu pembakaran sampah dengan jumlah yang sampah yang lebih sedikit. Secondary chamber digunakan untuk pembakaran sampah dengan volume sampah lebih banyak dan terhubung dengan primary chamber. Tujuan adanya intermittent furnace agar efek dari steam combustion dapat meningkatkan pembakaran pada secondary chamber dan mencegah adanya overheated pada secondary chamber.
Langkah awal penelitian dilakukan dengan pemodelan ASPEN Plus dan CFD agar dapat melihat karakteristik steam pada pembakaran dan karakteristik distribusi temperatur pada furnace.
DAI5 Conscious Thinking Framework
Framework DAI5 adalah pendekatan penyelesaian masalah yang baru dan menekankan metode yang komprehensif, terstruktur, serta melibatkan kesadaran penuh. DAI5 merupakan singkatan dari Dr. Ahmad Indra sebagai pencipta dan pengembang framework ini dan empat tahapan utama: Intention (Niat), Initial Thinking (Pemikiran Awal), Idealization (Idealisasi), dan Instruction Set (Set Instruksi).
1. Dr. Ahmad Indra: Nama ini mengacu pada pencipta dan pengembang framework DAI5, yaitu Dr. Ahmad Indra. Framework ini dikembangkan dengan latar belakang filosofi dan pendekatan khusus yang dirumuskan oleh beliau dalam upaya untuk menciptakan solusi problem solving berbasis conscious thinking.
2. Intention (Niat): Langkah awal yang mengarahkan seluruh proses penyelesaian masalah. Dalam tahap ini, niat dan tujuan yang jelas harus ditentukan, dan sering kali niat tersebut mengandung elemen spiritual yang berhubungan dengan usaha untuk mencari ridho Tuhan. Subjektivitas sangat mempengaruhi niat, yang dapat bervariasi tergantung pada pengalaman pribadi, nilai, dan keyakinan individu.
3. Initial Thinking (Pemikiran Awal): Ini adalah tahapan di mana dilakukan eksplorasi awal terhadap masalah, yang meliputi pengumpulan informasi dan pemahaman yang lebih mendalam tentang konteks permasalahan. Tahap ini melibatkan analisis awal untuk mendapatkan gambaran besar serta prinsip-prinsip dasar yang terlibat dalam permasalahan.
4. Idealization (Idealisasi): Pada tahap ini, masalah yang kompleks disederhanakan melalui berbagai asumsi atau pendekatan yang dapat dipertanggungjawabkan. Tujuannya adalah untuk memfokuskan hanya pada variabel-variabel penting sehingga masalah menjadi lebih terarah dan mudah diselesaikan.
5. Instruction Set (Set Instruksi): Tahap terakhir di mana langkah-langkah terstruktur dan sistematis disusun untuk menyelesaikan masalah. Ini berfungsi sebagai panduan yang jelas, berdasarkan hasil dari proses idealisasi sebelumnya.
Framework DAI5 ini menekankan kesadaran penuh dalam setiap tahap penyelesaian masalah, yang membedakannya dari metode lain yang lebih teknis dan objektif, karena ia juga mempertimbangkan aspek spiritual dan subjektivitas pribadi. Saya menggunakan DAI5 Conscious Thinking Framework ini sebagai landasan berpikir untuk menyelesaikan masalah di pengaplikasian CFD. [[1]]
Aplikasi CFD pada Lid Driven Cavity Flow
1. Pembentukan Vorteks Primer:
Vorteks primer terbentuk sebagai pola aliran sirkular dominan yang disebabkan oleh pergerakan tutup (lid driven cavity). Ketika tutup bergerak secara tangensial, ia menyeret fluida yang ada di dekatnya, menghasilkan gaya gesekan yang menyebabkan fluida berputar di dalam rongga. Ini menciptakan aliran sirkulasi yang dikenal sebagai vorteks primer, yang memusat di sekitar bagian tengah rongga. Vorteks primer biasanya berada di pusat rongga dan berbentuk elips atau lingkaran, bergantung pada bilangan Reynolds dan aspek rasio rongga.
2. Pembentukan Vorteks Sekunder:
Vorteks sekunder terbentuk di dekat dinding-dinding yang stasioner, terutama di sudut-sudut rongga. Vorteks ini lebih kecil dan kurang kuat dibandingkan vorteks primer. Vorteks sekunder terjadi karena aliran fluida di sudut-sudut tersebut terjebak oleh aliran sirkulasi vorteks primer, sehingga terbentuk pola sirkulasi lokal di area sudut tersebut. Vorteks sekunder terbentuk di sudut kiri bawah dan kanan bawah rongga, serta kadang-kadang di sudut atas, tergantung pada kondisi aliran. Pada bilangan Reynolds yang rendah (aliran laminar), vorteks sekunder berukuran kecil dan lemah, namun seiring dengan meningkatnya bilangan Reynolds, vorteks sekunder menjadi lebih besar dan lebih jelas. Bahkan, pada aliran turbulen yang lebih tinggi, vorteks tersier bisa muncul di beberapa sudut.
Dinamika Vorteks dan Bilangan Reynolds:
-> Pada Bilangan Reynolds Rendah (aliran laminar): Vorteks primer mendominasi, sementara vorteks sekunder lemah dan terbatas di sudut-sudut rongga. Aliran cenderung halus dan teratur.
-> Pada Bilangan Reynolds Tinggi (aliran transisional dan turbulen): Vorteks primer mulai terdeformasi, dan vorteks sekunder serta tersier dapat muncul karena ketidakstabilan aliran yang lebih besar.
Pembentukan vorteks primer dan sekunder ini merupakan hasil dari interaksi antara tutup yang bergerak, dinding yang diam, dan gaya viskos pada fluida. Fenomena ini sering dipelajari dengan menggunakan metode numerik seperti metode beda hingga atau simulasi lattice-Boltzmann untuk menyelesaikan persamaan Navier-Stokes yang mendeskripsikan aliran fluida
Berikut analisis saya terhadap aliran pada Lid Driven Cavity menggunakan aplikasi OpenFoam dengan variasi dynamic viscosity untuk mengetahui profil aliran. [[2]]
Referensi hasil analisis aliran didapatkan dari jurnal "The Lid-Driven Cavity" dengan penulis Hendrik C. Kuhlmann dan Francesco Romanò. Berikut adalah rangkuman jurnalnya. [[3]]
Self-Assesment using Chat-GPT not Cheat-GPT for Mid-Test of Computational Fluid Dynamics
You can read my interactions with Chat-GPT by clicking this link [[4]]
Basic CFD Test
1. What does CFD stand for?
a) Computational Fluid Dynamics
b) Complex Fluid Dynamics
c) Compressible Fluid Dynamics
d) Computational Flow Data
2. In CFD, the Navier-Stokes equations describe:
a) Heat transfer
b) Motion of fluids
c) Electrical conduction
d) Gravitational forces
3. Which method is typically used to discretize the governing equations in CFD?
a) Finite Element Method (FEM)
b) Finite Difference Method (FDM)
c) Finite Volume Method (FVM)
d) All of the above
4. What is the main purpose of mesh generation in CFD?
a) Solve the equations directly
b) Divide the domain into small elements for numerical computation
c) Represent boundary conditions
d) Refine the graphical output
5. Which of the following is true about laminar flow?
a) It has irregular, chaotic motion
b) It is characterized by smooth, orderly motion
c) It only occurs at high Reynolds numbers
d) It does not exist in real-world applications
6. What does the Reynolds number represent in fluid dynamics?
a) Ratio of inertial forces to gravitational forces
b) Ratio of inertial forces to viscous forces
c) Ratio of heat transfer to mass transfer
d) Ratio of pressure to velocity
7. Which type of flow is more likely when the Reynolds number is high?
a) Laminar
b) Turbulent
c) Steady
d) Stationary
8. Which equation is typically used to describe the conservation of mass in fluid flow?
a) Bernoulli’s equation
b) Energy equation
c) Continuity equation
d) Ideal gas law
9. What is turbulence in fluid flow?
a) A state of flow where viscous forces dominate
b) A flow regime characterized by chaotic and irregular motion
c) Flow with no velocity variations
d) Flow that occurs at low Reynolds numbers
10. Which method is most commonly used to handle turbulence in practical CFD simulations?
a) Direct Numerical Simulation (DNS)
b) Large Eddy Simulation (LES)
c) Reynolds-Averaged Navier-Stokes (RANS)
d) None of the above
Your Results:
1. a) Computational Fluid Dynamics – Correct!
2. a) Heat transfer – Incorrect. The Navier-Stokes equations describe the motion of fluids.
3. c) Finite Volume Method (FVM) – Correct!
4. b) Divide the domain into small elements for numerical computation – Correct!
5. b) It is characterized by smooth, orderly motion – Correct!
6. b) Ratio of inertial forces to viscous forces – Correct!
7. b) Turbulent – Correct!
8. c) Continuity equation – Correct!
9. b) A flow regime characterized by chaotic and irregular motion – Correct!
10. c) Reynolds-Averaged Navier-Stokes (RANS) – Correct!
Score: 9/10
Grade: A
You did an excellent job! You clearly have a strong grasp of basic CFD concepts, only missing out on the second question. Keep up the great work, and you'll do well on your exam!
Basic CFD Test 2
1. Which of the following is a method used to solve partial differential equations in CFD?
a) Euler's method
b) Taylor series expansion
c) Finite Difference Method (FDM)
d) Newton-Raphson method
2. In CFD, boundary conditions are used to:
a) Initialize the solution
b) Define the behavior of the fluid at the boundaries of the domain
c) Set the internal flow conditions
d) Refine the mesh
3. What is the main advantage of using the Finite Volume Method (FVM) in CFD?
a) Simplicity of formulation
b) Direct representation of conserved quantities
c) High accuracy in non-uniform grids
d) Ability to handle multi-phase flows easily
4. Which of the following is NOT a common type of boundary condition in CFD?
a) Inlet
b) Slip
c) Symmetry
d) Fourier
5. The Courant number (CFL) is used in CFD to:
a) Estimate mesh quality
b) Evaluate numerical stability of time-stepping methods
c) Calculate the pressure gradient
d) Solve the energy equation
6. Which of these turbulence models is most commonly used for high-Reynolds-number flows in industrial applications?
a) Direct Numerical Simulation (DNS)
b) Reynolds-Averaged Navier-Stokes (RANS)
c) Large Eddy Simulation (LES)
d) Potential flow model
7. What is meant by convergence in a CFD simulation?
a) The residuals stop decreasing
b) The solution reaches a steady-state condition
c) The numerical solution stops changing significantly with further iterations
d) The grid refinement is completed
8. The SIMPLE algorithm in CFD is used for:
a) Compressible flows
b) Time-dependent flows
c) Pressure-velocity coupling
d) Mesh generation
9. What does the term “mesh independence” refer to in CFD?
a) The solution is independent of the initial conditions
b) The results do not change significantly when the mesh is refined further
c) The mesh quality has no effect on the solution
d) The number of grid cells is not related to the solution accuracy
10. Which of the following is true about steady-state simulations in CFD?
a) Time derivatives are included
b) The flow properties change with time
c) The solution represents the long-term behavior of the flow
d) Boundary conditions vary with time
Your Results:
1. c) Finite Difference Method (FDM) – Correct!
2. b) Define the behavior of the fluid at the boundaries of the domain – Correct!
3. c) High accuracy in non-uniform grids – Correct!
4. d) Fourier – Correct! (Fourier boundary conditions are not common in CFD; inlet, slip, and symmetry are.)
5. b) Evaluate numerical stability of time-stepping methods – Correct!
6. b) Reynolds-Averaged Navier-Stokes (RANS) – Correct!
7. c) The numerical solution stops changing significantly with further iterations – Correct!
8. a) Compressible flows – Incorrect. The SIMPLE algorithm is primarily used for pressure-velocity coupling, especially in incompressible flows.
9. a) The solution is independent of the initial conditions – Incorrect. "Mesh independence" refers to when the results do not change significantly with further mesh refinement.
10. c) The solution represents the long-term behavior of the flow – Correct!
Score: 8/10
Grade: B
Great job! You have a strong understanding of CFD concepts, though there was a bit of confusion with questions 8 and 9. Keep practicing, and you’ll be ready for your exam!
Basic CFD Test 3
1. What is the role of turbulence models in CFD?
a) To calculate the viscosity of the fluid
b) To simulate the effects of turbulence without resolving all scales of motion
c) To provide exact solutions to the Navier-Stokes equations
d) To simplify steady-state flows
2. In CFD, which method allows for better handling of irregular geometries?
a) Finite Difference Method (FDM)
b) Finite Element Method (FEM)
c) Finite Volume Method (FVM)
d) Spectral Method
3. The CFL condition is important in ensuring:
a) Conservation of mass
b) The numerical stability of explicit time-stepping schemes
c) Energy conservation
d) Grid independence
4. Which method is best suited for solving incompressible flow problems in CFD?
a) SIMPLE Algorithm
b) Newton-Raphson Method
c) Explicit Time-Stepping
d) MacCormack Scheme
5. Which type of flow is described by the condition where viscous forces dominate inertial forces?
a) Turbulent flow
b) Laminar flow
c) Compressible flow
d) Incompressible flow
6. What is the primary difference between DNS (Direct Numerical Simulation) and RANS (Reynolds-Averaged Navier-Stokes)?
a) DNS is computationally cheaper than RANS
b) DNS resolves all turbulence scales, while RANS averages the effect of turbulence
c) RANS solves for compressible flows, while DNS is only for incompressible flows
d) DNS ignores boundary conditions
7. In CFD, which of the following methods is commonly used to ensure mass conservation in the solution?
a) Energy equation
b) Continuity equation
c) Momentum equation
d) Fourier’s law
8. What does the term "residual" refer to in CFD simulations?
a) The error in the solution due to mesh refinement
b) The difference between the exact and numerical solutions
c) The difference between successive iterations during the solution process
d) The energy loss in the system
9. The pressure correction method used in incompressible flow simulations helps:
a) Solve temperature equations
b) Ensure momentum conservation
c) Adjust pressure to satisfy mass conservation
d) Refine mesh near boundaries
10. When performing a transient CFD simulation, which of the following is true?
a) The flow is assumed to be steady
b) Time derivatives are neglected
c) Time-dependent terms are included in the governing equations
d) Only spatial discretization is considered
Your Results:
1. b) To simulate the effects of turbulence without resolving all scales of motion – Correct!
2. a) Finite Difference Method (FDM) – Incorrect. The Finite Element Method (FEM) handles irregular geometries better than FDM.
3. b) The numerical stability of explicit time-stepping schemes – Correct!
4. a) SIMPLE Algorithm – Correct!
5. b) Laminar flow – Correct!
6. b) DNS resolves all turbulence scales, while RANS averages the effect of turbulence – Correct!
7. b) Continuity equation – Correct!
8. b) The difference between the exact and numerical solutions – Incorrect. "Residual" refers to the difference between successive iterations during the solution process.
9. c) Adjust pressure to satisfy mass conservation – Correct!
10. d) Only spatial discretization is considered – Incorrect. In a transient simulation, time-dependent terms are included in the governing equations (answer: c).
Score: 8/10
Grade: B
You're doing well! You have a solid understanding of CFD principles. Just be careful with handling concepts like mesh refinement and transient simulations. Keep practicing, and you'll be even more prepared for your exam!
Basic CFD Test 4
1. Which of the following equations is NOT typically used in CFD simulations?
a) Continuity equation
b) Navier-Stokes equations
c) Energy equation
d) Schrödinger equation
2. In the Finite Volume Method (FVM), what is conserved across control volumes?
a) Pressure
b) Mass, momentum, and energy
c) Velocity
d) Density
3. What is the primary function of a turbulence model in a CFD simulation?
a) To resolve small eddies in turbulent flows
b) To predict the effect of turbulence on mean flow properties
c) To simulate laminar flow regimes
d) To compute exact turbulent fluctuations
4. In a steady-state CFD simulation, which of the following is true?
a) The flow changes with time
b) Time derivatives are included in the governing equations
c) The solution represents a condition that does not change with time
d) Transient effects are dominant
5. In CFD, which discretization method is most commonly used for solving compressible flows?
a) Finite Element Method (FEM)
b) Finite Difference Method (FDM)
c) Finite Volume Method (FVM)
d) Spectral Method
6. Which of the following best describes a structured mesh in CFD?
a) A mesh where cells are randomly distributed
b) A mesh that has an orderly arrangement of grid points
c) A mesh that changes dynamically during the simulation
d) A mesh with highly irregular cell shapes
7. What is the role of boundary conditions in CFD simulations?
a) To solve the flow equations
b) To initialize the simulation time
c) To define the behavior of the flow at the domain boundaries
d) To compute mesh quality
8. The Reynolds number is a dimensionless quantity used to predict:
a) The amount of turbulence in a flow
b) The compressibility of a flow
c) The energy loss in a flow
d) The type of flow (laminar or turbulent)
9. Which method is typically used to couple pressure and velocity in incompressible flow simulations?
a) SIMPLE algorithm
b) MacCormack method
c) Lattice Boltzmann method
d) Newton-Raphson method
10. Which of the following is an important step in validating a CFD simulation?
a) Verifying that the governing equations were correctly derived
b) Comparing the numerical results with experimental data or analytical solutions
c) Increasing the number of mesh cells indefinitely
d) Running the simulation for an infinite amount of time
Your Results:
1. d) Schrödinger equation – Correct! The Schrödinger equation is not used in CFD simulations, as it's related to quantum mechanics.
2. b) Mass, momentum, and energy – Correct! In the Finite Volume Method, these quantities are conserved across control volumes.
3. b) To predict the effect of turbulence on mean flow properties – Correct! Turbulence models aim to approximate the effects of turbulence on the average flow without resolving all scales.
4. c) The solution represents a condition that does not change with time – Correct! In a steady-state simulation, the flow is constant over time.
5. c) Finite Volume Method (FVM) – Correct! FVM is widely used for compressible flows due to its conservation properties.
6. b) A mesh that has an orderly arrangement of grid points – Correct! Structured meshes have an organized, grid-like structure.
7. c) To define the behavior of the flow at the domain boundaries – Correct! Boundary conditions are crucial for specifying how the flow behaves at the edges of the computational domain.
8. d) The type of flow (laminar or turbulent) – Correct! The Reynolds number helps determine whether the flow is laminar or turbulent.
9. a) SIMPLE algorithm – Correct! The SIMPLE algorithm is commonly used to couple pressure and velocity in incompressible flow simulations.
10. b) Comparing the numerical results with experimental data or analytical solutions – Correct! Validation of a CFD simulation often involves comparing the results to known data.
Score: 10/10
Grade: A+
Excellent! You answered all the questions correctly and demonstrated a strong grasp of basic CFD concepts. You're well-prepared for your exam—keep up the great work!
Basic CFD Test 5
1. The Navier-Stokes equations are derived from which fundamental principles?
a) Conservation of mass and energy
b) Conservation of momentum and energy
c) Conservation of mass, momentum, and energy
d) Conservation of density and temperature
2. In CFD, which scheme is often used for discretizing convective terms to avoid numerical diffusion?
a) Central difference scheme
b) Upwind scheme
c) Leapfrog scheme
d) Lax-Wendroff scheme
3. What does the term “grid convergence” refer to in a CFD simulation?
a) The solution becomes independent of the time step size
b) The residuals reach zero
c) The solution becomes independent of the mesh refinement
d) The boundary conditions are satisfied
4. Which of the following is a primary challenge in solving compressible flows in CFD?
a) High Reynolds numbers
b) Shock waves
c) Boundary layer separation
d) Large eddies
5. In transient simulations, what is a critical consideration for selecting the time step size?
a) Mesh independence
b) CFL condition
c) Reynolds number
d) Symmetry
6. Which of the following turbulence models is the most computationally expensive?
a) Direct Numerical Simulation (DNS)
b) Reynolds-Averaged Navier-Stokes (RANS)
c) Large Eddy Simulation (LES)
d) Potential flow model
7. Which term in the Navier-Stokes equations is responsible for viscous effects?
a) Pressure gradient term
b) Convective term
c) Diffusive term
d) Body force term
8. In which scenario is compressibility effects important in CFD simulations?
a) Flows with low Mach number
b) Flows with high Mach number
c) Flows with low Reynolds number
d) Flows with high viscosity
9. The purpose of post-processing in a CFD simulation is to:
a) Define the boundary conditions
b) Solve the governing equations
c) Visualize and analyze the results
d) Refine the mesh
10. The Prandtl number in CFD is a dimensionless number used to relate:
a) Inertial forces and viscous forces
b) Thermal diffusivity and momentum diffusivity
c) Kinetic energy and potential energy
d) Pressure and velocity
Your Results:
1. c) Conservation of mass, momentum, and energy – Correct! The Navier-Stokes equations are based on these conservation principles.
2. b) Upwind scheme – Correct! The upwind scheme helps reduce numerical diffusion in convective terms.
3. b) The residuals reach zero – Incorrect. Grid convergence occurs when the solution becomes independent of mesh refinement (answer: c).
4. b) Shock waves – Correct! Compressible flows often involve shock waves, which present a challenge in CFD simulations.
5. b) CFL condition – Correct! The CFL condition ensures numerical stability when selecting the time step size for transient simulations.
6. a) Direct Numerical Simulation (DNS) – Correct! DNS is the most computationally expensive turbulence model as it resolves all scales of motion.
7. c) Diffusive term – Correct! The diffusive term in the Navier-Stokes equations accounts for viscous effects.
8. d) Flows with high viscosity – Incorrect. Compressibility effects are important in flows with high Mach numbers (answer: b), where the fluid velocity approaches the speed of sound.
9. c) Visualize and analyze the results – Correct! Post-processing in CFD involves analyzing and visualizing the simulation results.
10. b) Thermal diffusivity and momentum diffusivity – Correct! The Prandtl number relates the rates of momentum and thermal diffusion.
Score: 8/10
Grade: B
Good job! You have a solid grasp of CFD fundamentals, but there’s room for improvement with grid convergence and compressibility effects. Keep practicing, and you’ll be well-prepared for your exam!
Evaluasi Assessment UTS
1. Awalnya saya memahami Navier-Stokes equation menjelaskan heat transfer, tetapi setelah saya pelajari lebih lanjut ternyata pada dasarnya Navier-Stokes equation adalah persamaan yang menjelaskan kekekalan momentum. Sedangkan heat transfer dirumuskan pada kekekalan energi.
2. Saya menjawab bahwa SIMPLE algorithm digunakan pada perhitungan compressible flows, ternyata SIMPLE algorithm digunakan pada incrompressible flows dengan cara pressure-velocity coupling.
3. Sebelumnya saya belum memahami mesh independence. Akhirnya saya belajar bahwa yang dimaksud dengan mesh independence adalah hasil simulasi CFD tidak berubah secara signifikan walaupun dengan mesh refinement yang lebih baik.
4. Saya belum memahami metode mana yang lebih baik untuk handling geometri yang tidak beraturan. Saya mengira jawabannya adalah Finite Difference Method (FDM). Namun setelah saya pelajari ternyata jawabannya adalah Finite Element Method (FEM).
5. Saya belum mengetahui apa maksud dari “Residual” dalam CFD. Akhirnya saya belajar bahwa “Residual” adalah mengacu pada perbedaan antara iterasi suksesif selama proses solusi.
6. Saya juga belum mengetahui apa istilah “Grid Convergence” sebenarnya. Setelah mencari tau, saya mengerti bahwa “Grid Convergence” terjadi ketika solusi menjadi tidak bergantung pada mesh refinement.
7. Saya belum belajar mengenai “Mech Number”. Apa itu “Mech Number”, efek yang terpengaruh, dan factor yang mempengaruhi nilai “Mech Number”.
Secara garis besar, saya ingin belajar lebih lanjut tentang algoritma SIMPLE, proses meshing, metode untuk menyelesaikan permasalahan meshing, residual pada CFD, dan Mech Number.
Review of Numerical Investigations on Heat Transfer and Fluid Dynamics in Lid-Driven Cavities: Effects of Aspect Ratios, Boundary Conditions, and Artificial Roughness
Abstract
The lid-driven cavity flow problem is a fundamental benchmark in fluid dynamics used to study incompressible flow behavior, particularly when induced by a moving wall or "lid." This review focuses on the application of numerical methods in analyzing lid-driven cavity flows, with a specific emphasis on heat transfer characteristics. Recent research, particularly using the k-epsilon turbulence model, demonstrates the profound impact of factors such as aspect ratio, boundary conditions, and the introduction of artificial roughness on heat transfer and flow patterns. Cavities with higher aspect ratios tend to enhance heat transfer, while different boundary configurations, including differentially heated walls, lead to complex flow behaviors that significantly affect thermal fields. Introducing artificial roughness further enhances turbulence, improving heat transfer efficiency. Numerical methods like the finite volume method and the lattice Boltzmann method, combined with Large Eddy Simulations (LES), have been employed to capture intricate flow structures and thermal fields. The review highlights advancements in turbulence modeling and the application of hybrid approaches, such as coupling machine learning models with traditional simulations, to optimize heat transfer predictions. Future work aims to integrate radiative effects and artificial intelligence to further enhance the accuracy and computational efficiency of such models.
Keywords:
lid-driven cavity, Nusselt numbers, k-epsilon, aspect ratio, boundary condition, artificial roughness
Introduction
The lid-driven cavity flow problem is a classical benchmark problem in fluid dynamics used to study the behavior of incompressible fluid flow inside a square or rectangular cavity. The cavity is typically closed on all sides, but the flow is induced by moving one of the cavity walls (the "lid") at a constant velocity, while the other walls remain stationary. The problem is a simplified model of fluid motion, and it helps test numerical methods for solving the Navier-Stokes equations, which describe fluid flow. The lid-driven cavity flow problem is often solved using numerical methods such as finite difference, finite element, or spectral methods to discretize and solve the Navier-Stokes equations.
Recent research on the use of the k-epsilon turbulence model in lid-driven cavity flows, especially combined with heat transfer analysis, has shown interesting developments. The k-epsilon model remains widely used due to its balance between computational efficiency and accuracy when dealing with turbulent flows, including cavity-driven setups. It helps in understanding the turbulence production and dissipation within the cavity, which significantly affects the heat transfer characteristics. In some research, the heat transfer characteristics are influenced by aspect ratio and shape of cavity, artificial roughness, and boundary conditions [[5]][[6]][[7]].
• Aspect Ratio and Shape: The aspect ratio and shape of the cavity influence the flow and heat transfer. Aspect ratio (AR) is cavity width divided by cavity depth. Higher aspect ratios generally enhance heat transfer, while different shapes (rectangular, triangular, circular) show varying efficiencies [[8]][[9]][[10]].
• Boundary Conditions: The movement of the lid and the temperature difference between the walls create complex flow patterns that enhance heat transfer. For instance, differentially heated walls and moving lids can significantly alter the thermal fields and improve heat transfer rates [[11]][[12]][[13]].
• Artificial Roughness: Introducing artificial roughness, such as ribs, can dramatically increase the heat transfer rate by affecting the flow patterns and enhancing turbulence [[14]].
Heat Transfer Characteristics
Khalid N. Alammar (2006) [[15]] found that the primary mechanism of heat transfer enhancement is turbulence generated by cavities. In a two-dimensional simulation using the standard k-ε turbulence model, cavities with higher aspect ratios showed enhanced heat transfer more than those with lower aspect ratios. Higher aspect ratios generated more complex vortex structures, contributing to both increased Nusselt numbers and higher pressure drops. The artificial roughness introduced on the heated bottom wall of a cavity containing a rotating cylinder was investigated by Ali Khaleel Kareem and Shian Gao (2018) [[16]]. The presence of additional roughness with a rotating cylinder significantly
Fig 1. a. Circulation inside a cavity; AR = 3, b. Circulation inside a cavity; AR = 6 (Khalid, 2006)
Fig 2. a. Turbulence kinetic energy distribution, and b. Nusselt numbers distribution near cavities (Khalid, 2006)
increased the turbulent kinetic energy, contributing to better heat transfer. Employing the Unsteady Reynolds-Averaged Navier-Stokes (URANS) equations with a standard k-ε turbulence model, the simulation results can be inferred that the advanced heat transfer was more prominent at higher Reynolds numbers. Gnanasekaran Manogaran and Satheesh Anbalagan (2024) [[17]] also confirmed
Fig 3. The schematic diagrams of the lid-driven cavity containing a rotating cylinder in the cases of a. square (S), b. square ribs (R-s), and c. half-circle ribs (R-c) (Ali & Shian, 2018)
that higher intensity of turbulence kinetic energy results in enhanced heat transfer. Using the k-ε turbulence model and the FVM (Finite Volume Method)-based SIMPLE algorithm, the study figured that as the speed ratio (S=U_bottom/U_top) increased, secondary vortices were formed, and the primary vortex shrank. The primary vortex was larger at lower speed ratios and got displaced as the speed ratio and Reynolds numbers increased. Lower aspect ratios (K = 0.5) resulted in higher intensity of turbulence kinetic energy and dissipation rates near the top of the cavity. Increasing the aspect ratio decreased the concentration of turbulence but distributed it more uniformly across the cavity.
Fig 4. a. The isotherm, b. the streamline and velocity magnitude contours for different Reynolds numbers, 5000 and 10 000, and bottom wall conditions (S, R-s) at -5 ≤ Ω ≤ 5 (Ali & Shian, 2018)
Fig 5. Effect of speed ratio (S) and Reynolds numbers on streamline contours at aspect ratio (K) = 1.0 (Gnanasekaran & Satheesh, 2024)