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A short class with Sarah and her students. The other ways are under More.
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Let's start by deriving the momentum thickness using the definition. It’s defined as the integral of the product of the velocity profile and the velocity deficit. Can someone remind me what the velocity profile is?
Isn't it given by u/U = 2y/δ - (y/δ)²?
Correct! Based on this, we substitute into the momentum thickness formula. Can anyone tell me what the integral looks like?
The integral will be from 0 to δ of (2y/δ - (y/δ)²)(1 - (2y/δ - (y/δ)²) dy, right?
Exactly! Now, what do we get when we evaluate this integral?
After substituting the limits, I think we end up with 2δ/15 for the momentum thickness θ.
Excellent! So, θ = 2δ/15 is our result. This thickness characterizes the flow. Let’s summarize!
Next, let's find the wall shear stress τ0. How do we start with this?
We can use the von-Karman momentum integral equation: τ0 = ρU² dθ/dx.
That's right. Now let's find dθ/dx based on our derived formula for θ.
Since θ = 2δ/15, we differentiate this with respect to x, right?
Exactly! This gives us the relationship: τ0 = 2/15 ρU² (dδ/dx). Now, how can we express τ0 using viscosity?
Using Newton's law of viscosity, possibly τ0 = μ (du/dy) at y = 0?
Right again! This dual relationship leads us to a final form. Let's wrap this session.
Now let’s calculate the boundary layer thickness after we establish the relationship that δ²/2 = 15 μx/ρU. How do we proceed with this?
We can integrate this from 0 to δ on the left and from 0 to x on the right.
Correct! After integration, we’ll solve for δ. What is δ in terms of the Reynolds number?
δ = 5.48x/√Re_x, right? Because Re_x is Ux/ν.
Absolutely! This is crucial for predicting turbulent flow as well. Let’s summarize everything we've learned!
A measure of the thickness of the boundary layer concerning fluid momentum.
The frictional force per unit area exerted by the fluid at the boundary surface.
A dimensionless number that helps predict flow patterns based on inertial and viscous forces.
In the layer thin and tight, flow starts from zero to take flight.
Imagine a smooth river flowing past a rocky bank. The rocks slow the water directly at their surface, creating a calm layer—a thin boundary layer.
For momentum, remember: 'Always (A) Integrate (I) Velocity (V) Negatively (N)' → AIVN.
B.L. - Boundary layer important for predicting flow behavior.
Term
What is the boundary layer?
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Term
How is momentum thickness defined?
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A thin region adjacent to the boundary of an object where flow velocity changes from zero at the surface to free stream velocity.
A measure of the thickness of the boundary layer based on momentum loss and is defined through an integral involving the velocity profile.
The tangential stress exerted by the fluid on the boundary surface.
A dimensionless quantity used to predict flow patterns in different fluid flow situations.
A type of flow where the fluid moves in smooth paths or layers, characterized by low Reynolds numbers.
This section focuses on the analysis of the given velocity profile for a laminar boundary layer, deriving expressions for boundary layer thickness and wall shear stress.
The section provides a detailed derivation of boundary layer thickness and wall shear stress using the given velocity profile for a laminar boundary layer. It explores the formulation of momentum thickness and applies von-Karman momentum integral equations to arrive at key results.
This section investigates the behavior of laminar boundary layers using the velocity profile given by:
.
Momentum Thickness Calculation:
The momentum thickness is defined as:
Substituting the velocity profile into the equation leads to an integral that can be solved to find the momentum thickness...
Boundary Layer Thickness Derivation: Further analysis using the von-Karman momentum equation provides: and recognizing that gives a relationship between the shear stress, viscosity, and boundary layer thickness.
Final Results: The expressions for boundary layer thickness and shear stress are derived:
These results are significant for understanding fluid flow behavior in laminar scenarios over flat plates.