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Today, we're going to dive into turbulent pipe flow. Can anyone tell me what average velocity is?
Is it the total distance traveled divided by the total time?
Exactly! Now, in turbulent flows, we compare that with frictional velocity. Understand that for turbulent flow, the average velocity divided by the frictional velocity gives important insights into the flow characteristics.
What about smooth and rough pipes? Do they behave differently?
Good question! The equations show that the difference in velocity at any point compared to the average velocity remains the same for both pipe types. Can anyone recall that important equation related to this?
Is it the one that involves the logarithm with 5.75?
Yes! The difference is represented by the equation: u - V average = 5.75 log10(y/R) + 3.75. Great job!
Now let’s shift our focus to the power law velocity profile. Who can tell me the significance of the value n?
Isn't it related to the Reynolds number?
Correct! As the Reynolds number increases, so does n. That's crucial as it shapes our understanding of flow behavior in pipes.
But can we calculate wall shear stress using this profile?
That’s a critical point! Power law profiles can't provide accurate wall shear stress because they imply an infinite velocity gradient at the walls. Remember, it can't give a 0 slope at the center of the pipe either.
That's interesting! How do we find average velocity then?
Great segue! We’ve got the average velocity derived when provided with specific flow profiles.
Let’s work through a problem together. We know that u of r is given with a specific equation. How do we start finding the average velocity?
We can integrate the velocity profile from 0 to R, right?
Exactly, we set up our integral over the entire cross-section of the flow. What’s the structure of that integral?
It's 1/pi R² integral of u max
Right! Simplifying will help find that average velocity. It’s essential to understand the steps and methodology we use in practical scenarios.
And the final solution gives us an expression for average velocity, correct?
Exactly! Our goal is to express average velocity as a fraction of u max, which, through our calculations, gives us 0.816 u max.
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The section elaborates on the difference between average velocity and frictional velocity in turbulent pipe flow, presenting significant equations for both smooth and rough pipes. It emphasizes that the velocity difference behaves similarly for both types, along with introducing the power law velocity profile and its implications in hydraulic engineering.
In this section, we address the average velocity divided by the frictional velocity specifically for turbulent pipe flows. We explore how the velocity at any given point relates to the average velocity for smooth pipes using derived equations. The main takeaway is that the difference between the velocity at any point and the average velocity remains the same for both smooth and rough pipes, firmly establishing the relevance of these equations in practical applications.
Significant velocity profile considerations include the power law, which highlights how the profile behaves differently based on the Reynolds number and specifies that it cannot accurately determine the wall shear stress due to its unique characteristics. Through an example problem, we outline the process of calculating average velocity in a given pipe flow, culminating this exploration with introductory references to future topics in hydraulic engineering.
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Now, about the power law velocity profile, a little bit on that. So, the power law velocity profile for smooth pipes can be expressed as, it is, u by u max can be written as y by R to the power 1 by n. This is the power law velocity that was given or we can always write in terms of R because y is, y is R minus small r and that you substitute here, you will end up in this equation. So, this 1/n depends upon the Reynolds number, putting n is equal to 7 in above equation gives one-seventh power law velocity profile. This is one of the very famous velocity profiles.
This chunk introduces the power law velocity profile, which describes how fluid velocity varies with distance from the wall in a smooth pipe. The relationship is defined by the equation u/u_max = (y/R)^(1/n), where 'u' is the fluid velocity at radial position 'y', 'R' is the pipe's radius, and 'n' is an exponent that is influenced by the flow's Reynolds number. Setting n to 7 gives a specific and commonly used profile, revealing how complex fluid dynamics can be quantified using mathematical models.
Think of the power law velocity profile like a ramp that gradually slopes up. As you move from the bottom to the top of the ramp (representing distance from the pipe wall), you gain height (representing fluid velocity). Different ramps can be steeper or more gradual, much like how different values of 'n' alter the fluid's behavior in the pipe.
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The value of n will increase with increasing Reynolds number. Power law velocity profiles cannot give 0 slope at the pipe center. So, power law of velocity profiles also cannot calculate the wall shear stress. Why? Because the power law profiles gives a velocity gradient of infinity at the walls. That you can try, by substituting r is equal to, small r is equal to capital R.
In this chunk, we learn that as the Reynolds number (a measure of flow turbulence) rises, so does 'n', affecting how the velocity profile behaves. A noteworthy characteristic of power law profiles is that they cannot produce a zero slope at the center of the pipe, which is a theoretical ideal for steady laminar flow. Additionally, power law profiles don't account for wall shear stress accurately since they suggest an infinite velocity gradient at the pipe's walls—meaning that there's an unrealistic change in velocity right at the surface where the fluid touches the pipe.
Imagine swimming in a pool. When you swim close to the edge (pipe wall), you may feel a strong pull from the wall, indicating how the water rushes rapidly against it. However, as you move toward the center of the pool, the water's movement is less influenced by the walls and more influenced by the overall pool current. This analogy reflects how power law profiles struggle to accurately depict this variability in velocity gradient at the walls.
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Now, we are going to solve one of the problems. So, the velocity profile for incompressible turbulent fluid in a pipe of radius R is given by u of r as u max into 1 minus r by R to the power 1 by 7. Obtain an expression for the average velocity in the pipe.
This chunk sets the stage for a practical example where we calculate the average velocity for a turbulent fluid represented by the equation: u(r) = u_max(1 - (r/R)^(1/7)). The next steps would include integration to find the average velocity across the entire cross-section of the pipe using calculus. The detailed steps involve substituting values, integrating within the specified limits, and simplifying the equations, which ultimately leads to a calculated average velocity.
Consider filling a round swimming pool with water that flows out of a hose. While water at the surface flows faster than at the depths, calculating the average speed of water exiting the hose can be a challenge. Just like finding the average speed of water in the pool using the formula we discussed, you'll consider the varying speeds at different depths before finding the overall average.
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So, these are the references, as I have already shown you in the book, I mean, also in the introduction slides. And so, this week’s lecture on the laminar and turbulent flow is finished. I will see you next week with another set of lectures on hydraulic engineering. Thank you so much. Have a nice weekend.
In this concluding chunk, we summarize the key concepts discussed during the lecture on laminar and turbulent flow. The speaker expresses gratitude and informs students about the upcoming topics in the next class, reinforcing the continuity of learning in the field of hydraulic engineering.
Imagine finishing a chapter of a book where each section has built upon the last. The conclusion serves to recap the learning journey and prepare you for the next adventure in the story—much like how engineers build upon principles learned to tackle increasingly complex challenges in fluid dynamics.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Turbulent Flow: Characterized by chaotic fluid movement.
Average Velocity: Calculated as total fluid distance over time.
Frictional Velocity: A key parameter for turbulent flow effects.
Power Law Velocity Profile: A method to model velocity distribution.
Reynolds Number: A dimensionless indicator of flow regime.
See how the concepts apply in real-world scenarios to understand their practical implications.
For a pipe of known radius, use wheel tubes to measure the turbulent flow profile and calculate the average velocity.
Use computational fluid dynamics software to model flow velocity in a rough pipe to validate average velocity calculations.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In turbulent flow, see how it goes, chaotic and wild, that's how it flows.
Imagine a river flowing smoothly and suddenly encountering rocks - that chaos is turbulent flow!
TAP (Turbulent flows Average velocity and Power law profile) helps remember key concepts.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Turbulent Flow
Definition:
A type of fluid flow characterized by chaotic property changes.
Term: Average Velocity
Definition:
The total distance traveled by fluid per unit time across a specific area.
Term: Frictional Velocity
Definition:
A parameter used in turbulent flows to quantify friction effects.
Term: Power Law Velocity Profile
Definition:
A mathematical approach used to describe the velocity distribution in turbulent flows.
Term: Reynolds Number
Definition:
A dimensionless number used to predict flow patterns in different fluid flow situations.