Course syllabus adopted 2023-02-12 by Head of Programme (or corresponding).
Overview
- Swedish nameTurbulensmodellering
- CodeMTF271
- Credits7.5 Credits
- OwnerMPAME
- Education cycleSecond-cycle
- Main field of studyMechanical Engineering
- DepartmentMECHANICS AND MARITIME SCIENCES
- GradingTH - Pass with distinction (5), Pass with credit (4), Pass (3), Fail
Course round 1
- Teaching language English
- Application code 03116
- Block schedule
- Open for exchange studentsYes
Credit distribution
Module | Sp1 | Sp2 | Sp3 | Sp4 | Summer | Not Sp | Examination dates |
---|---|---|---|---|---|---|---|
0120 Written and oral assignments, part A 1.5 c Grading: UG | 1.5 c | ||||||
0220 Written and oral assignments, part B 1.5 c Grading: UG | 1.5 c | ||||||
0320 Examination 4.5 c Grading: TH | 4.5 c |
|
In programmes
- MPAME - APPLIED MECHANICS, MSC PROGR, Year 1 (compulsory elective)
- MPCAS - COMPLEX ADAPTIVE SYSTEMS, MSC PROGR, Year 1 (compulsory elective)
- MPENM - ENGINEERING MATHEMATICS AND COMPUTATIONAL SCIENCE, MSC PROGR, Year 1 (compulsory elective)
Examiner
- Lars Davidson
- Full Professor, Fluid Dynamics, Mechanics and Maritime Sciences
Eligibility
General entry requirements for Master's level (second cycle)Applicants enrolled in a programme at Chalmers where the course is included in the study programme are exempted from fulfilling the requirements above.
Specific entry requirements
English 6 (or by other approved means with the equivalent proficiency level)Applicants enrolled in a programme at Chalmers where the course is included in the study programme are exempted from fulfilling the requirements above.
Course specific prerequisites
MTF072 Computational fluid dynamics (CFD) or Mechanics of Fluids or any corresponding course
Aim
The object of the course is to give the students a thorough knowledge and understanding of modern,
advanced turbulence models for unsteady fluid flow simulations.
Learning outcomes (after completion of the course the student should be able to)
- Describe different RANS turbulence models such as Reyonlds stess models, algebraic Reynolds stress models, k-els, k-omega, V2F, k-omega SST
- Understand and outline the difference between LES, RANS, URANS, DES and hybrid LES-RANS
- Derive the exact transport turbulence equations using tensor notation
- Describe the modeling assumptions, using tensor notation, in turbulence models
- Identify and interpret the different terms in the turbulence models presented in the course.
- Describe the difference between resolved and modeled Reynolds stresses
- Describe different approaches to handle the near-wall problem in LES
- Describe the advantages of second-moment closures compared to eddy-viscosity models
- Derive the V2F model
- Reproduce the different spatial filtering approaches in LES
- Derive the SGS models using tensor notation
- Understand and describe the concept of modeled (for example SGS) dissipation between resolved and modeled scales
- Describe the method how to prescribe unsteady, fluctuating inlet boundary conditions
- Be able to carry out an simulation with a commercial CFD code
Content
The development of computers and Computational Fluid Dynamics (CFD) has made the numerical simulation of complex fluid flow, combustion, aero-acoustics and heat transfer problems possible. Turbulent flow in three-dimensional, complex geometries -- unsteady or steady -- can be dealt with. Presently CFD methods can replace, or complement, many experimental methods; we can use a numerical wind tunnel instead of an experimental one.Today, most CFD simulations are carried out with traditional RANS (Reynolds-Averaged Navier-Stokes). In RANS, we split the flow variables into one time-averaged (mean) part and one turbulent part. The latter is modelled with a turbulence model such as k-eps or Reynolds Stress Model. For many flows it is not appropriate to use RANS, since the turbulent part can be very large and of the same order as the mean. Examples are unsteady flow in general, wake flows or flows with large separation. For this type of flows, it is more appropriate to use Large Eddy Simulation (LES). In order to extend LES to high Reynolds number flows new methods have been developed. These are called DES (Detached Eddy Simulation), URANS (Unsteady RANS) or Hybrid LES-RANS. They are all unsteady methods and they are a mixture of LES and RANS. In aero-acoustics the noise is generated by turbulence. The best way to accurately predict large-scale turbulence is to carry out an unsteady simulation of the flow field (i.e. LES, DES, hybrid LES-RANS or URANS). After that the noise is predicted separately in CAA (Computational Aero-Acoustics).
In LES, DES, URANS and Hybrid LES-RANS the large-scale part of the turbulence is solved for by the discretized equations whereas the small-scale turbulence is modeled. The definition of ''large-scale'' varies in the different methods. Furthermore, the limit between ''large-scale'' and ''small-scale' is often not well defined. Since turbulence is three-dimensional and unsteady, it means that in all the methods the simulations must always be carried out as three-dimensional, unsteady simulations.
We will address questions like:
- How should I make my mesh?
- why should I in LES use a non-dissipative discretization scheme?
- is it necessary to used central differencing in DES and URANS?
- what is the different between LES and unsteady RANS?
- what turbulence models can I use in DES and unsteady RANS?
- to enhance numerical stability, can a turbulence model with high dissipation be used?
- how do I prescribe inlet boundary conditions?
- inlet boundary conditions: can I use steady inlet boundary conditions? which is best, synthesized turbulence or a pre-cursor DNS?
In the first project, we will learn how to interpretat results from
an unsteady simulation. We will also use a commercial CFD package to
evaluate different RANS turbulence models.
When doing LES-URANS/DES, you have to ask yourself similar questions as when doing measurements:
- when is the flow fully developed so that I can start time-averaging?
- for how long time do I need to time-average?
- is it enough if I get accurate mean flow or do I also need accurate resolved turbulent stresses?
- how do I estimate the quality of my LES or hybrid LES-RANS? Spectra? 2-point correlations? SGS dissipation?
The
most important drawback/bottleneck of LES is the requirement to use
very fine grid near walls. The grid must be fine in all directions, not
only the wall-normal direction. Much of the research on LES is today
focused in getting around this bottleneck. One approach is hybrid
LES-RANS. In this method RANS is used near walls and LES is used in the
remaining part of the domain.
.For more information
Organisation
11 pre-recorded lectures are uploaded to Canvas.
There will be five discussion seminars during lectures on Campus.
- The students will register in six groups (approximately five in each).
- Each discussion seminar will last 30 minutes.
The assignments will supervised on Campus.
Students can use
- Python (recommended), (recommended),
- Matlab or
For Assignment 2b, only Python scripts are available.
1. In the first part of Assignment 1, the students will be given data from a numerical simulation (LES or DNS). The data will be two-dimensional, time-averaged velocity (recirculating flow) and pressure fields, the Reynolds stresses and the (SGS) dissipation. The data will be analyzed.
We will start analyzing the transport equations of the turbulent Reynolds stresses, u_iu_j. We identifiy regions of large production terms, which should correspond to regions of large Reynolds stresses. Reynolds stresses will be computed using the
eddy-viscosity assumption, and these will be compared to their exact counter-parts.
In the second part of Assignment 1, the students will use Machine Learning and try to improve turbulence models. The first attempt could be to improve the standard k-eps model my optimizing the C_mu coefficient. Influence parameters may be velocity gradients (coordinate-invariant) and/or the turbulent time-scale, k/ε, both functions of x and y. The output parameter will be C_mu = C_mu (x,y). For more details, see Course Plan
2. In Assignment 2, the students will be given flowfields of channel flow at high Reynolds number and the flow
over a hump. Both flows have been obtained using PANS/DES/IDDES.These flows will be analysed using different modeling assumptions such as DES, DDES, PANS and SAS. For more detail, see Assignment 2a and 2b in the eBook Course home page
Literature
The eBook can be downloaded from the course home pageExamination including compulsory elements
Grades. 20-29: passed; 30-39: grade 4; 40-50: grade 5- Part 1: Two assignments including written presentations. This part is mandatory.
- Part 2: Discussion seminars. This part is not mandatory.
- Part 3: Either Quiz or oral exam is mandatory.
- Part 3a: Quiz. Students who pass this quiz get 20 points (grade 3, passed).
- Part 3b: Oral exam based on the questions in the Discussion seminars and the Assignments.The teachers will also ask follow-up questions.There we try to test if the student has understood the topic or if he/she has memorized it. A good understanding gives grade 4 or 5. Two students at the time. max 40 points.
- To get grade 'passed', you must have 20 points on either the Quiz or the Oral exam and handing in the two assignment reports.
The course examiner may assess individual students in other ways than what is stated above if there are special reasons for doing so, for example if a student has a decision from Chalmers on educational support due to disability.
The course syllabus contains changes
- Changes to examination:
- 2024-06-10: Exam by department Changed to exam by department by Examinator
[2024-08-20 4,5 hec, 0320] Given by dept
- 2024-06-10: Exam by department Changed to exam by department by Examinator