4.2.1 - Equation 18
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Introduction to Turbulent Flow
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Welcome everyone! Today, we’re going to explore turbulent flow in smooth pipes. Before we dive into Equation 18, can anyone explain what distinguishes turbulent flow from laminar flow?
Turbulent flow is when the fluid moves in erratic paths, while laminar flow is smooth and orderly.
Exactly! So, how does this relate to the Reynolds number?
The Reynolds number helps determine whether the flow will be laminar or turbulent based on the speed and viscosity of the fluid.
Great point! Remember, a Reynolds number above 4000 typically indicates turbulent flow, and that’s important as we look at our equations today.
Understanding Equation 18
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Let’s analyze Equation 18 together. Who can tell me what happens to the velocity at the wall when the distance approaches zero?
The velocity becomes negatively infinite because of the logarithm of zero.
Right. This leads us to conclude that the flow velocity is zero at a specific finite distance from the wall, denoted as y'. Can anyone recall how we express this relationship mathematically?
It’s represented as u at distance y' equals −u star divided by Kappa times ln of y prime.
Exactly! This is essential in understanding how we move from chaotic turbulence to stable velocity profiles.
Practical Application and Problem Solving
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Now that we understand Equation 18, let's apply our knowledge to a problem. What is the average height of roughness for a rough pipe of diameter 10 cm, given the velocity characteristics?
We need to recall the equations relating velocities at y = 1 cm and y = 4 cm to find the height of roughness.
Correct! And how do we ensure we account for the roughness in our logarithmic formula?
We apply the rough pipe equation that incorporates surface roughness factors.
Good thinking! Let’s solve the problem step by step and see what we obtain.
Velocity Distribution in Rough Pipes
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As we extend our discussion to rough pipes, can anyone summarize how their velocity profile differs from smooth pipes?
A rough pipe’s velocity profile will have more irregularities and takes into account surface roughness.
Absolutely! Furthermore, what effect does Nikuradse’s findings have on our equations?
They provide empirical data to find how y' (the distance for no velocity) behaves in rough pipes compared to smooth ones.
Correct again! This interplay of theory and empirical data is what strengthens our grasp of hydraulic engineering.
Introduction & Overview
Read summaries of the section's main ideas at different levels of detail.
Quick Overview
Standard
In this section, we analyze turbulent flow in smooth pipes, emphasizing Equation 18's role in determining velocity distribution. The implications of velocity profiles, both for smooth and rough pipes, are explored in depth, along with relevant derivations and practical examples.
Detailed
Detailed Summary
This section delves into the dynamics of turbulent flow within smooth pipes, centering around equations derived during the analysis of velocity distribution. Equation 18 reveals that the velocity at the wall becomes infinitely negative at a zero distance from the wall, suggesting that there is a specific distance from the wall where the velocity equals zero. This particular relationship establishes a logarithmic profile that underpins the understanding of fluid dynamics within smooth and rough pipes.
Additionally, differences in turbulent flow regimes between smooth and rough surfaces are discussed, with key results from Nikuradse's experiments providing foundational insight into rough pipe behavior. Examples are given to clarify the effects of surface roughness on velocity profiles, aiding in the practical application of these theoretical findings. Alongside the mathematical findings, practical problems are solved to enhance comprehension of turbulent flow characteristics.
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Understanding Velocity at the Wall
Chapter 1 of 5
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Chapter Content
From the above equation, the velocity at the wall u at y is equal to 0 will be minus infinity, correct. If we put y is equal to 0. So, if we put ln 0, it will be minus infinity. u is positive at some distance far away from the wall.
Detailed Explanation
This chunk explains that when we try to calculate the velocity (u) at the wall (y = 0), we encounter a mathematical issue. The natural logarithm of zero (ln(0)) approaches negative infinity. This means that directly at the wall, our velocity calculation is not defined. However, as we move away from the wall to some distance, the velocity becomes a positive value, which indicates fluid movement at a distance from the wall.
Examples & Analogies
Think of a water faucet. When it's off (similar to y=0), no water flows (u = minus infinity in our analogy), but as you slowly open it (moving away from the wall), water starts to flow at increasing speeds. Hence, we need to consider some distance away from the wall for realistic calculations.
Logarithmic Profile Assumption
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Hence, u is 0 at some finite distance y prime from the wall, that is, y at y prime is equal to 0. Hence, from equation 18, we can say that at distance y prime C will be minus u star by Kappa ln y prime.
Detailed Explanation
At some finite distance from the wall (referred to as y prime), we assume the velocity (u) becomes zero. We can derive a constant (C) in equation 18 that relates to the parameters of the flow. Here, C is determined to be negative u star divided by Kappa multiplied by the natural logarithm of y prime. This equation helps us understand how the velocity profile changes as we move away from the wall.
Examples & Analogies
Imagine standing at a beach where the waves gradually dissipate near the shore (y=0). Farther out in the water (at y prime), you feel the water starting to push against your legs, resembling how velocity approaches zero at a point closer to the wall. This gradual change is modeled in this logarithmic equation.
Velocity Distribution for Turbulent Flow
Chapter 3 of 5
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Chapter Content
Now, this as you see, the velocity distribution for turbulent flow in smooth pipe. This is the velocity distribution for turbulent flow in a smooth pipe, where there is no irregularity.
Detailed Explanation
In this part, we acknowledge that the derived equation represents the velocity distribution of turbulent flow in smooth pipes. This is important because it lays out how turbulent flow behaves without any surface roughness, giving us a mathematical understanding of flow characteristics in ideal conditions.
Examples & Analogies
Think of a well-maintained, smooth road that allows a car to drive quickly without any bumps or obstacles. Here, the smooth surface helps maintain a steady speed, akin to how turbulent flow behaves in a smooth pipe.
Incorporating Surface Roughness
Chapter 4 of 5
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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.
Detailed Explanation
This piece indicates that the earlier derived equations are also applicable when considering rough surfaces, not just smooth ones. Surface roughness significantly influences fluid flow, and the equations allow us to approximate flow behavior by adjusting for surface characteristics.
Examples & Analogies
Consider riding a bike on a sidewalk versus a gravel path. While you can ride smoothly on the sidewalk, the rough gravel path makes it harder to maintain speed. Similarly, our equations account for these changes in surface conditions when predicting turbulent flow.
Practical Problem Solving
Chapter 5 of 5
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Chapter Content
Now, it is a good idea to solve one problem here, on this particular concept, and the solving the problem will give more understanding now.
Detailed Explanation
In this section, the lecture introduces a practical problem related to turbulent flow. Solving such problems helps reinforce the concepts learned theoretically by applying them to real-world scenarios. The problem relates to measuring fluid velocities at different distances from the wall in a rough pipe.
Examples & Analogies
Imagine you are trying to measure how fast a river flows at different points, like near the bank versus further in the middle. By solving similar problems mathematically, we understand flow behavior better and how different factors influence that flow.
Key Concepts
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Turbulent Flow: Characterized by chaotic and fluctuating fluid motion, usually occurring at high velocities.
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Logarithmic Profile: A mathematical representation of the velocity distribution relative to distance from a surface in turbulent flow.
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Reynolds Number: A coefficient that helps predict whether flow will be laminar or turbulent based on various factors.
Examples & Applications
In practical engineering scenarios—like water flowing through pipes—understanding the transition from laminar to turbulent flow helps optimize design.
Nikuradse's experiments provide a framework for calculating flow rates based on surface roughness, showcasing how different textures influence flow behavior.
Memory Aids
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Rhymes
In pipes we flow, smooth or rough, Understanding their ways can save us from tough!
Stories
Imagine a river flowing smoothly on a calm day - that's laminar flow. Now imagine a storm stirring it up, creating waves and chaos - that's turbulent flow!
Memory Tools
Reynolds' Ruler: 'R1' for Re < 2000 (Laminar), 'R2' for Re > 4000 (Turbulent) – remember the flow types!
Acronyms
TURB
Turbulent flow
Unpredictable
Reynolds number > 4000
Backward motion near walls.
Flash Cards
Glossary
- Turbulent Flow
A type of fluid flow where the velocity of the fluid undergoes irregular fluctuations.
- Laminar Flow
A type of fluid flow characterized by smooth and orderly motion, with layers of fluid sliding past one another.
- Reynolds Number
A dimensionless number used to predict flow patterns in different fluid flow situations.
- Logarithmic Profile
A representation of how velocity varies with distance from a surface in turbulent flow.
- Nikuradse’s Experiment
Experiments conducted to study flow characteristics in pipes with various surface roughness.
- Surface Roughness (k)
A measure of the texture of a surface, which impacts fluid flow patterns.
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