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Today, we will delve into velocity distribution for turbulent flow, particularly in smooth and rough pipes. Can anyone tell me what they think might affect the velocity in these scenarios?
I think surface roughness might play a role in how fast the fluid moves.
Exactly! Surface roughness impacts the flow, and we use equations derived from experiments to quantify this. For smooth pipes, we derive a logarithmic velocity profile. Remember the word **laminar**? It refers to a smooth flow.
What does logarithmic mean in this context?
Great question! The logarithmic profile shows the relationship between velocity and the distance from the wall. Think of it as how the velocity changes in layers of fluid near the pipe wall.
So does this mean there are equations we can use to calculate this?
Absolutely! For smooth pipes, we can utilize Equation 22, and for rough pipes, we’ll have a different set of coefficients. Let's remember that with the acronym **SURF**: Surface roughness affects the flow.
How do we apply these equations practically?
We’ll solve real problems to see how these equations help us predict flow rates. Let’s summarize: understanding velocity distribution is key, and roughness will alter our equations.
Now that we’ve discussed the impact of roughness, let’s explore specific equations. Can anyone recall what we learned about Equation 22?
I remember it relates to velocity at a distance from the wall.
Correct! It gives us a way to calculate the velocity in smooth pipes. When we adapt this for rough pipes, we use Nikuradse's findings for our coefficients. Why do you think these adaptations are necessary?
Because rough pipes create more turbulence, right?
Precisely! The roughness increases energy losses, requiring different calculations. Remember to memorize **NIKU**: Nikuradse helps us adapt the equations for roughness effects.
Can we see these equations in action?
Sure! We’ll solve a problem based on the variations in velocity at specific heights in the rough pipe.
Let’s tackle a problem! We have a rough pipe 10 cm in diameter, and the velocity at 4 cm from the wall is 40% more than at 1 cm. What information do we need to start?
We need the equations related to rough pipes, right?
Exactly! We use the coefficients derived from Nikuradse's experiments. Let’s denote our known values: diameter D and velocities at specified heights. What’s a good first step?
Insert the values into the equation for velocity?
Good thought! For rough surfaces, our equations differ, and we need to equate the two velocities we’re comparing. Now, let’s solve to find the average height of roughness k. Remember our mnemonic **Vary K**: Varying K for varying surface conditions!
So finding k will help us understand how the roughness affects our calculations?
Correct! Let’s work through the math to find that k value.
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The section elaborates on the concepts of velocity distribution for turbulent flow in smooth and rough pipes, emphasizing equations derived from laboratory experiments, particularly by Nikuradse, to define the characteristics of flow in these systems. It highlights the importance of understanding the impact of surface roughness on flow velocity and provides examples and problem-solving techniques.
In hydraulic engineering, understanding the velocity distribution in turbulent flow is crucial for efficient design and operation of piping systems. This section focuses on turbulent flow in both smooth and rough pipes, utilizing key equations derived from empirical research, notably that of Nikuradse.
The theoretical model begins with the velocity profile equation, where the wall velocity is defined, leading to discussions of the natural logarithmic profiles for both smooth and rough surfaces. The approximation involved in determining velocity at specific distances from the wall is crucial, particularly the concept of the laminar sublayer. The section presents equation 22 for smooth pipes, illustrating how it transitions into equations applicable for rough pipes, adjusting key coefficients that account for surface roughness.
A practical exercise is included to compute the average height of roughness for a rough pipe with a provided diameter and velocity differences at specified distances from the wall, reinforcing the analytical skills applied in real-world scenarios. Furthermore, it transitions into discussing turbulent velocity distribution concerning average velocity, integrating over a defined area to assess overall flow characteristics.
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Now, what about the turbulent flow? So, it is better to note down this equation. Now, we have to see equation 23. So, actually this is valid for rough surface as well because all the approximation that we did was on this y dash.
In this part, the focus is on discussing the behavior of turbulent flow specific to rough pipes. The speaker indicates that the previous equations, particularly equation 23, are applicable even for rough surfaces. It's essential to understand that while smooth pipes and rough pipes may have different characteristics, the fundamental principles derived for smooth pipes can still aid in analyzing rough pipes.
Consider a smooth road versus a rough road. The same car can drive on both but the behavior of the car (like speed and handling) will change based on the road conditions. Similarly, the principles for predicting flow can still be applied to both types of pipes but the results will vary due to different surface roughness.
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For rough pipes Nikuradse obtained the value of y prime as k/30. This is obtained by Nikuradse and if you substitute this y prime in equation number 23 this one, we can obtain, or if you take this 30 out, it is.
Nikuradse's work is pivotal in understanding the flow characteristics in rough pipes. He discovered that the distance above the bed where the velocity is close to zero for rough pipes (y prime) can be represented as k/30, where k is a roughness parameter. This finding allows for substituting values into established equations to yield velocity distributions specific to rough surfaces.
Think of the way water flows over different terrains. When it flows over smooth pebbles, it moves differently compared to when it flows over rough rocks. Nikuradse's finding is akin to measuring how high the water must rise over a rough surface before it behaves like it's not influenced by that roughness.
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Now you see, this is the velocity distribution of turbulent flow in rough pipes. These coefficients are little different this k is different, more importantly, it also has some sort of logarithmic form, both smooth and the rough.
The speaker emphasizes that the velocity distribution in rough pipes follows a logarithmic pattern, similar to smooth pipes, but with adjustments to accommodate the surface roughness. The coefficients involved differ, highlighting the distinct characteristics of turbulent flow in various pipe types. This mathematical formulation allows engineers to predict how fluid behaves in different conditions.
Imagine trying to ride a bike on both a smooth track and a bumpy track. Your speed and experience on these tracks will differ due to the surface. Similarly, the equations account for differences in flow caused by surface roughness.
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Now, we are going to talk about turbulent velocity distribution in terms of average velocity. So, there is a flow and there is an elementary circular ring here, as you can see, this is of radius R.
This section transitions to discussing how to calculate the average velocity from turbulent flow in pipes. The concept of an elementary circular ring is introduced, with radius R being crucial to understanding how the velocity is assessed at various points within the fluid flow. This sets the groundwork for deriving important hydrological equations.
Imagine observing waves in a pool. If you want to measure the average height of the waves, you wouldn’t just look at one spot; you would look around at several points in the pool. Similarly, average velocity takes into account various layers within a pipe to provide an overall picture.
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If we integrate this equation number 28 and using the results in equation 29, that is, dividing by pi R square for obtaining V average, we can get.
The focus here is on the mathematical integration of the velocity equations to find the average flow velocity in turbines. By dividing the total flow by the area, represented by pi R squared, the average velocity can be computed, making abstract calculations more tangible.
Think of filling a container with water at different speeds at various holes. To find out how fast the container fills on average, you look at the total volume filled over time rather than just at one hole. This averaging is the same as what we're doing mathematically with the flow in the pipes.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Velocity Distribution: The pattern of how fluid speed varies at different distances from the pipe wall.
Surface Roughness: Characteristics of a pipe's inner surface that significantly affect flow behavior.
Nikuradse's Contribution: His experiments provide crucial data and equations for adapting flow calculations in rough pipes.
See how the concepts apply in real-world scenarios to understand their practical implications.
If a rough pipe has a diameter of 10 cm, the average height of roughness can be calculated through provided velocity variations at specified distances from the wall.
Considering values for smooth pipes, the logarithmic velocity profile can help determine flow rates effectively.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In the pipe, the flow does twist, turbulence is what we can't resist.
Imagine a smooth pipe - water flows gently. Now picture a rough pipe - the water fights and churns.
Remember SURF: Surface, Uniform, Roughness, Flow - key aspects in understanding turbulent behavior.
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Review the Definitions for terms.
Term: Turbulent Flow
Definition:
A type of fluid flow characterized by chaotic and irregular fluid motion.
Term: Velocity Distribution
Definition:
The variation of flow velocity at different points in a fluid, especially near a surface.
Term: Rough Pipes
Definition:
Pipes with uneven surfaces that increase turbulence and friction.
Term: Nikuradse's Experiment
Definition:
Research conducted by Nikuradse to determine the impact of surface roughness on flow.
Term: Laminar Sublayer
Definition:
The layer of fluid near a boundary where flow is laminar despite overall turbulence.