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Today, we're focusing on the shear stress in turbulent flow. Unlike laminar flow, which only accounts for viscous shear stress, turbulent flow introduces an additional component due to turbulence itself. Can anyone tell me what this additional component is called?
Is it the eddy viscosity, sir?
Exactly! The eddy viscosity (η) signifies the added complexity in turbulent flow. It's essential because it helps us quantify the shear stress. Now, can anyone explain why we can't just rely on dynamic viscosity here?
I think it’s because eddy viscosity depends on flow conditions and isn’t a property of the fluid itself.
Correct! Eddy viscosity changes depending on how turbulent the flow is. Great job, everyone! Let's summarize the key points: turbulent flow has additional shear stress from eddy viscosity, while laminar flow's shear stress is purely from dynamic viscosity.
Next, let’s explore Reynolds shear stress. Who can tell me what it is in simple terms?
It’s the shear stress caused by turbulence between fluid layers separated by a small distance, right?
Absolutely! Reynolds proposed a way to express this with the equation: minus ρ u' v' bar. What do u' and v' represent?
They are the fluctuating velocity components in the x and y directions.
Exactly! Since these fluctuate, it’s tough to calculate accurately. But understanding Reynolds shear stress is crucial for analyzing turbulent flow dynamics efficiently.
Remember, mixing length helps us determine the interactions in turbulent shear stress. Any questions before we move on?
Now, let's dive into Prandtl's mixing length theory, which provides a practical approach to estimating turbulent shear stress. Can anyone explain what mixing length refers to?
It's the distance between fluid layers that allows for effective mixing of momentum between them?
Excellent! And Prandtl suggested that this distance is related to the average velocity gradient. How do you think this relationship works?
Is it because the mixing length helps transfer the velocity gradient’s influence across layers?
Yes, the mixing length enhances momentum transfer between fluid layers. Prandtl derived an important equation where u' relates to mixing length and the velocity gradient. Let’s summarize: the mixing length helps quantify turbulent shear stress and connects effectively with velocity gradients.
Finally, let's consider how we can apply this theory in real-world engineering. Why is it important to understand turbulent flow in pipe systems?
Because it affects how we design pipes for efficient fluid transport, right?
Exactly! The majority of flow in pipes is turbulent. If we can define shear stress accurately using mixing length and understand that it varies with distance from the wall, we’ll make better design choices. How does this relate back to what we've discussed about viscosity?
It shows that turbulence has a much bigger influence in most of the flow zones than the viscosity does!
Right! And that’s crucial for engineers when considering flow efficiency and system design. Let's recap: the mixing length helps simplify complex flows by directly relating to shear stress and velocity gradients.
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The mixing length is introduced as a crucial factor in determining shear stress in turbulent flow, with Prandtl's theory explaining its relationship with velocity gradients. The section further distinguishes between turbulent and laminar flow, highlighting the unique properties of eddy viscosity.
In this section, we delve into the concept of mixing length (lm) as a critical component of shear stress in turbulent flow. Prandtl's mixing length theory describes how the momentum exchange occurs between fluid layers, facilitated by the mixing length, which is defined as the vertical distance needed for fluid particles to effectively mix and equate their momentum. Turbulent flow exhibits additional shear stress due to turbulence, requiring a different approach to determine its effects compared to laminar flow, which relies solely on viscosity. The theory introduces important parameters like eddy viscosity (η) and Reynolds shear stress, paving the way for understanding turbulent flow behaviors in hydraulic systems. Key equations illustrate how these parameters relate to velocity gradients and distance from boundaries, marking significant steps in fluid dynamics and hydraulic engineering.
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In 1925, Prandtl introduced the concept of mixing length, which can be utilized to express the shear stress in turbulent flow in terms of some measurable quantity.
In 1925, the engineer Prandtl proposed the mixing length concept to understand turbulent flow better. He aimed to find a way to express turbulent shear stress in measurable terms. This approach emerged because calculating turbulent shear stress directly is complex and difficult.
Think of mixing in a kitchen. Just as you might mix ingredients like flour and water to make dough, fluid particles in turbulent flow mix together. Mixing length is like measuring how far these ingredients have blended — it helps us understand how energy or momentum is transferred in the flow.
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Mixing length, lm, is the distance between two fluid layers in the vertical direction, so that the bundles of fluid particles from one layer could reach the other layer and mix in the new layer.
The mixing length (lm) is defined as the vertical distance that allows fluid particles from one layer to reach and mix into an adjacent layer. Prandtl illustrated this by assuming there's a specific distance where the mixing happens, crucial for calculating momentum transfer in turbulent flows.
Imagine two layers of ingredients in a salad bowl, one above the other. Mixing length represents how far you need to stir the salad to ensure the dressing reaches and blends all the ingredients below — similar principles apply to fluid layers in turbulent flow!
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Prandtl related u' to mixing length lm, stating that u' can be expressed as mixing length lm multiplied by the gradient of the average velocity du/dy.
Prandtl established a mathematical relationship connecting the fluctuating velocity (u') to mixing length (lm) and the velocity gradient (du/dy). This equation helps us quantify the turbulent flow's characteristics in relation to mixing length, making theoretical predictions possible.
Consider a busy street where cars have to merge. The speed of merging cars (u') can be thought of as a reflection of how well the two lanes are mixing. The mixing length (how far back the first lane extends) would influence how quickly cars can enter and mix with the faster-moving lanes.
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Substituting findings into Reynolds’ turbulence model yields tau turbulent = rho lm² (du bar/dy).
By substituting the relationships developed into Reynolds' turbulence model, we derive a new equation for turbulent shear stress. This equation expresses the shear stress in terms of known quantities, such as density (rho) and average velocity gradient (du/dy), incorporating mixing length (lm) as an essential factor.
Imagine you are trying to gauge how much force is needed to mix paint. The paint thickness and the distance you can stir before it becomes homogeneous (mixing length) are crucial. This derived equation helps engineers predict the force needed to mix fluids effectively in engineering processes.
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Prandtl assumed that the mixing length lm is a linear function of distance y from the wall, where lm can be written as lm = kappa * y.
To simplify the calculation further, Prandtl assumed that mixing length varies linearly with the distance from a boundary. This assumption means that as you move away from a wall, the mixing length increases proportionately, represented mathematically by lm = kappa * y, where kappa is a constant.
Think of how deep water gets stirred in a swimming pool. Near the pool walls, it mixes less than in the middle. The distance from the wall (y) might give us a way to estimate how much energy needs to be applied to achieve good mixing across varying depths.
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In turbulent flow, viscous shear stresses exist only near the boundary, while the region is dominated by turbulence, allowing us to approximate total shear stress using derived equations.
In turbulent flow, majority shear stress comes from turbulence rather than viscosity, especially away from the boundary. This means engineers can primarily rely on the derived equations related to turbulent shear stress for most flow conditions, simplifying their analyses.
It's like cooking pasta. When the water is bubbling with turbulence, it's easy for moving water to mix the pasta uniformly. In this case, most of the stirring happens in the middle far away from the pot's edges, allowing us to focus on how the pasta is moving rather than the subtle effects near the edges of the pot.
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Key Concepts
Mixing Length (lm): The distance between two fluid layers allowing momentum mixing.
Eddy Viscosity (η): Represents extra shear stresses in turbulent flow.
Reynolds Shear Stress: A formula to express turbulent shear stress between fluid layers.
See how the concepts apply in real-world scenarios to understand their practical implications.
In a turbulent river flow, the mixing length can help predict the energy loss due to friction against the riverbed and banks.
In pipe flow analysis, using mixing length theory allows for better designs that minimize energy losses in fluid transport.
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Turbulent flow can swirl and twist, mixing layers you cannot resist.
Imagine a river where currents collide; the mixing length is the distance they ride, ensuring momentum flows side by side.
M.E.R.C. - Mixing length, Eddy viscosity, Reynolds shear stress, and it’s Critical for turbulent flow understanding.
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Review the Definitions for terms.
Term: Eddy Viscosity
Definition:
The apparent viscosity in a turbulent flow, which accounts for the additional shear stresses due to the turbulent motion.
Term: Reynolds Shear Stress
Definition:
The shear stress resulting from turbulent fluctuations in velocity between fluid layers.
Term: Mixing Length (lm)
Definition:
The vertical distance between fluid layers required for effective momentum mixing between them.
Term: Dynamic Viscosity (µ)
Definition:
A measure of a fluid's resistance to shear or flow, an intrinsic property of the fluid.
Term: Kinematic Viscosity (ν)
Definition:
Ratio of dynamic viscosity to fluid density; an important characteristic in fluid flow.