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Today, we're going to start with Large Eddy Simulation, or LES, which is critical for understanding turbulent flows. Can anyone tell me why we might choose LES over Direct Numerical Simulation?
Because LES is less computationally intensive than DNS?
Exactly! LES provides a tradeoff, allowing us to capture the essential characteristics of turbulent flows without the full computational cost of DNS. Remember, LES focuses on the larger eddies while modeling the smaller ones.
What’s the difference in behavior between large and small eddies in this context?
Great question! Large eddies are anisotropic, meaning their behavior is influenced by the flow's geometry and boundary conditions. Smaller eddies, on the other hand, exhibit a more universal behavior. Think of it this way - large eddies extract energy from the mean flow.
So the energy transfers between different scales of eddies in turbulence?
That's correct! This energy transfer follows a cascade process, where smaller eddies draw energy from larger eddies. It's all part of the Kolmogorov hypothesis, which, though complex, illustrates how we approach turbulence modeling.
In summary, LES is vital for capturing flow characteristics while conserving computational resources by focusing on larger eddies.
Now let’s dive into the concept of spatial filtering in LES. Can anyone tell me what spatial filtering does?
Does it help to separate the scales of turbulence?
Exactly! Spatial filtering helps us differentiate between large and small eddies. In LES, we apply a filter function that relates to the size of our mesh.
What is a filter width?
Good question! The filter width is set close to the mesh size. This effectively captures the large scales while modeling the smaller scales with a turbulence model. Remember, there are two types of scales here: Grid Scale (GS) for larger eddies and Subgrid Scale (SGS) for smaller ones.
So the smaller eddies aren't directly solved, but modeled?
Precisely! By using subgrid scale modeling, we account for the influence of smaller eddies through the large eddies we compute. And that’s essential for accurate turbulence predictions.
To summarize, the filter function and width are crucial for distinguishing between eddies in LES. Remembering the GS and SGS is important.
Next, let’s explore the governing equations of LES. What do you think these equations represent?
Are they the equations that describe the flow behavior?
Yes! The filtered momentum equations describe how momentum is distributed and altered through large and small eddies. What’s important here is the introduction of the subgrid scale stress term, tau ij.
How does tau ij differ from the standard Reynolds stress?
Great observation! tau ij is comprised of several components including the Leonard and cross terms. While resolving large scales, we must still acknowledge the influence of small scales through these stress terms.
So, does this make LES more efficient than DNS in some ways?
Yes! By reducing the number of scales we resolve, we improve computational efficiency while still getting reasonable turbulence results.
In summary, the governing equations and the introduction of subgrid scale modeling are central to the success of LES.
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The text discusses Large Eddy Simulation (LES), highlighting its potential as a compromise between Direct Numerical Simulation (DNS) and Reynolds Averaged Navier-Stokes (RANS). It emphasizes the differences in energy dynamics between large and small eddies and introduces concepts such as filtering and subgrid scale modeling.
Large Eddy Simulation (LES) is a pivotal method in computational fluid dynamics (CFD) that focuses on the dynamics of large eddies while modeling the smaller turbulent scales. Unlike Direct Numerical Simulation (DNS), which requires extensive computational resources due to its accuracy in solving for all scales of turbulence, LES serves as a balance between accuracy and reusability of computational time. The large eddies, which are anisotropic and dependent on the geometry of the flow and body forces, extract energy from the mean flow, whereas smaller, isotropic eddies derive their energy from larger eddies in a defined cascade, a concept rooted in the Kolmogorov hypothesis. LES employs spatial filtering to distinguish these scales through governing equations that incorporate both large scales and subgrid scale models for smaller eddies. This method addresses the challenge of developing a universal turbulence model while highlighting the complexities stemming from varying scales of turbulence.
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Another such technique is called Large Eddy simulation. See in the DNS one important thing to note was that we had the best accuracy but lot of computational time is required. LES is sort of a tradeoff between the Reynolds average in Reynolds average we do many approximations so the results are not that accurate compared to DNS, but LES is something which is a tradeoff between DNS and Reynolds average Navier-Stokes equation.
Large Eddy Simulation (LES) is a computational fluid dynamics technique used to simulate turbulent flows. It strikes a balance between the accuracy of Direct Numerical Simulation (DNS) and the simplified models used in Reynolds-averaged Navier-Stokes (RANS) equations. While DNS provides highly accurate results, it requires significant computational resources, which may not always be feasible. On the other hand, RANS, which uses many approximations, may sacrifice accuracy for speed, making LES a practical compromise.
Imagine you are trying to capture the movements of waves in the ocean. A DNS would be like a high-definition video that captures every detail, requiring a lot of time and resources. RANS would be more like a rough sketch that simplifies the waves into basic shapes. LES is like a medium-quality film that captures the essence of the waves without getting lost in every tiny detail or simplifying too much.
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So there is a big difference in the behaviors of large and small eddies in a turbulent flow field.
In a turbulent flow, eddies, which are swirling motions of fluid, can vary significantly in size. Large eddies, often associated with bigger structures in the flow, exhibit anisotropic behavior, meaning their characteristics depend on the geometry of the environment they are in, such as how obstacles affect their movement. On the other hand, smaller eddies tend to behave more uniformly (isotropically), exhibiting consistent characteristics regardless of the flow's geometry.
Think about a crowd at a concert. The large groups of people moving together represent large eddies—they may change paths based on the layout of the venue. In contrast, smaller groups of fans jumping to the music represent smaller eddies; they move and act similarly, regardless of the larger crowd's behavior.
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The important thing to remember is that the large eddies extract energy from the mean flow, whereas small eddies take energy from a little bit larger eddies.
In turbulent flows, there exists a phenomenon known as energy cascade. Large eddies extract energy from the average flow (the mean flow), which fuels their motion. As these large eddies break down into smaller eddies, they pass on their energy to these smaller eddies. This process continues down to the smallest scales, where energy dissipates as heat due to viscous effects. This cascading process is crucial for understanding how energy moves through turbulent flows.
Consider a waterfall—large volumes of water at the top represent large eddies drawing energy from the height of the waterfall. As the water cascades down, smaller streams break off from the main flow, representing smaller eddies that take energy from the larger ones above them until the water hits the bottom pool and dissipates energy.
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In LES, the larger eddies are computed with a time-dependent simulation where the influence of the small eddies is incorporated through a turbulence model.
In the Large Eddy Simulation framework, the simulation focuses on computing large eddies while accounting for small eddies via models. The size of the computational grid (grid scale) is chosen such that it is capable of resolving large eddies appropriately, whereas smaller eddies are not directly simulated but rather modeled based on their influence. The filter width must be close to the grid size so that the simulation captures significant flow dynamics accurately.
Picture a sound recording studio where an engineer chooses to emphasize the bass frequencies (large eddies) while using filters to manage the treble frequencies (small eddies). The engineer’s goal is to capture the richness of the music without getting lost in every note, similar to how LES focuses on large scale dynamics in turbulent flow while modeling smaller scales.
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The filtering operation that we have talked about is defined by a filter function g of x, x dash, delta as it is a very complex but there is a filtering operation that you must know that in LES we use a filtering operation to cut off the smaller eddies and solve in reality for the larger eddies.
In LES, a filter function is applied to separate the larger eddies from the smaller ones. By applying this filter, we can solve the Navier-Stokes equations for the larger eddies while approximating the effects of smaller eddies through models. This allows for a more efficient computation as it simplifies the problem while still capturing the essential features of turbulence.
Imagine using a kitchen sieve to separate fine dust from flour—you're able to keep the flour (larger eddies) while filtering out the dust (smaller eddies). Just as the sieve efficiently sorts through the mixture to give you usable flour, filtering operations in LES help focus on important flow structures without needing to calculate every tiny detail.
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Key Concepts
Tradeoff between LES and DNS: LES provides a more computationally efficient method at the cost of some accuracy.
Energy Cascade: In turbulence, energy transfers between large and small eddies in a hierarchical manner.
Filtering Operation: Used in LES to separate large and small eddies for effective simulation.
See how the concepts apply in real-world scenarios to understand their practical implications.
In weather forecasting, LES is often used to model large-scale atmospheric flows while accounting for smaller turbulent structures indirectly.
In engineering, LES helps in studying the aerodynamic properties around large objects like vehicles or buildings, effectively capturing large vortices.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Large eddies soar high, smaller ones comply; Energy flows down, through the turbulence sky.
In the world of turbulent fluid, the large eddies play the role of powerful wizards, drawing energy from the flow, while smaller ones follow their commands, redistributing energy in their smaller realm.
Remember ‘GREAT’ for LES - Grid size, Reynolds effect, Energy transfer, Anisotropic, Turbulence modeling.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Large Eddy Simulation (LES)
Definition:
A fluid simulation technique that focuses on resolving large turbulent scales while modeling smaller scales.
Term: Direct Numerical Simulation (DNS)
Definition:
A highly detailed simulation that solves the Navier-Stokes equations for all scales without approximations.
Term: Turbulence Model
Definition:
Mathematical representation of turbulence effects to simplify complex fluid flow calculations.
Term: Kolmogorov Hypothesis
Definition:
A principle that states small eddies have a universal behavior and energy cascades through various scales of turbulence.
Term: Grid Scale (GS)
Definition:
The scales of turbulence directly resolved in the LES grid for large eddies.
Term: Subgrid Scale (SGS)
Definition:
The scales of turbulence not directly resolved in the LES grid, modeled through a turbulence model.
Term: Filtered NavierStokes Equations
Definition:
Equations used in LES that account for large eddies while modeling the influence of smaller ones.