1.1 - Smooth Pipes Equation
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Introduction to Fluid Velocity in Pipes
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Welcome everyone! Today, we will dive into the turbulent flow within smooth pipes. Can anyone tell me what the average velocity represents in this context?
Is it the typical speed at which fluid flows through a section of the pipe?
Exactly! The average velocity is crucial for understanding how fluids behave in a pipe. Now, can anyone share what frictional velocity means?
Is it related to the resistance a fluid faces due to the pipe's surface?
Yes, well put! We express the relationship using the equation: \( \frac{u}{u_*} \). This helps characterize the flow. Which velocity do you think is higher, average or frictional?
I think the average velocity would generally be higher since it accounts for more factors?
Correct! The average velocity is indeed often higher.
To summarize: the average velocity is vital for flow analysis, contrasting with the frictional velocity which measures resistance.
Comparing Smooth and Rough Pipes
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Moving on, let's discuss how the flow equations change for rough pipes compared to smooth ones. What do you think is a key similarity?
Maybe the logarithmic form of the equations?
Yes! Both cases maintain a similar structure in their equations. Can anyone recall the expression for the difference in velocity for smooth pipes?
It’s \(\frac{u - V_{avg}}{u_*} = 5.75 \log_{10}\left(\frac{y}{R}\right) + 3.75\) right?
Well done! What does this tell us about flow patterns in different pipe types?
That despite surface roughness, flow behavior can be predicted similarly?
Exactly! Understanding these patterns aids in predicting flow in real-world systems.
Recap: the structural similarities of equations provide insights into fluid behaviors across pipe types.
Power Law Velocity Profile
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Today, we will introduce the power law velocity profile. Who can describe what this entails?
It describes how velocity varies with distance from the centerline of the pipe?
Exactly! The equation \(\frac{u}{u_{max}} = \left(\frac{y}{R}\right)^{\frac{1}{n}}\) represents this. Can anyone guess how 'n' affects the profile?
If 'n' is larger, does it make the profile more gradual?
Yes! A larger 'n' indicates a more gradual velocity increase. It also means that at the center, you won't have zero slope, which can lead to challenges in calculating wall shear stress.
In summary: the power law provides insights into velocity distributions, crucial for practical applications in engineering.
Practical Application: Average Velocity Calculation
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Let’s apply what we’ve learned to a real problem: calculating average velocity from a specified profile. Who can recall how we start?
Start with integrating the velocity profile over the area?
Right! We set the average velocity as \(V_{avg} = \frac{1}{A} \int u(y) A \, dy\). How do we express the area of the pipe?
As \(\pi R^2\) for a circular pipe?
Good! We use this in our calculations. Make sure to simplify correctly when integrating. Let's perform this step-by-step.
So what result should we expect when we simplify and plug values back in?
You should find approximately \(0.816 u_{max}\). Excellent! This approach showcases the practical side of the equations we've derived.
To conclude our discussion, understanding how to calculate average velocities is integral to fluid dynamics.
Introduction & Overview
Read summaries of the section's main ideas at different levels of detail.
Quick Overview
Standard
In this section, we delve into the equations for turbulent flow in pipes, discussing the average velocity and frictional velocity in both smooth and rough pipes. Key equations, observations, and the power law velocity profile are also presented.
Detailed
Smooth Pipes Equation
This section explores the fundamental equations governing the flow of turbulent fluids in pipes. Key elements discussed include the average velocity, frictional velocity, and specific equations pertinent to smooth and rough pipes.
Key Equations and Observations
- The average velocity divided by the frictional velocity is a crucial ratio in turbulent pipe flow.
- The equations derived indicate that the difference in velocity at any point and the average velocity remains consistent for both smooth and rough pipes. This observation is significant, highlighting the similarity in behavior despite the surface texture differences of the pipes.
- For smooth pipes, the equation can be expressed as:
$$\frac{u - V_{avg}}{u_*} = 5.75 \log_{10}\left(\frac{y}{R}\right) + 3.75$$
Where:
- $u$ is local velocity,
- $V_{avg}$ is average velocity,
- $u_*$ is frictional velocity,
- $y$ is distance from the wall,
- $R$ is radius of the pipe.
Similarly, for rough pipes, the equation follows the same logarithmic form with slight adjustments.
Power Law Velocity Profile
The power law velocity profile for smooth pipes can be simplified to:
$$\frac{u}{u_{max}} = \left(\frac{y}{R}\right)^{\frac{1}{n}}$$
where the value of $n$ is dependent on the Reynolds number, and a common choice is \(n = 7\) providing a well-known reference for the average velocity profile. The profile reveals that power law does not account for the wall shear stress adequately.
Problem Solving Example
We also go through an example of calculating the average velocity given a specific velocity profile, illustrating practical application of the discussed theories.
Audio Book
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Overview of Velocity in Smooth Pipes
Chapter 1 of 10
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Chapter Content
So, what is this? This is the average velocity divided by the frictional velocity for the turbulent pipe flow case.
Detailed Explanation
In turbulent pipe flow, we examine the relationship between the average velocity of the fluid and the frictional velocity, which is a measure of the velocity fluctuations due to turbulence. This ratio helps to characterize the flow regime within the pipe.
Examples & Analogies
Think of a river during a flood. The average speed of the water in the river is like the average velocity in a pipe, while pockets of fast and slow-moving water represent the frictional velocities due to turbulence and obstacles in the river.
Difference of Velocity
Chapter 2 of 10
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Now, the difference of the velocity at any point and the average velocity for smooth pipes. For smooth pipes, we have seen that the u by u star we had, we came, we derived this equation, correct.
Detailed Explanation
The focus here is on how the velocity at any point in the pipe (u) relates to the average velocity (V average). The equation derived relates these two velocities in a way that helps us understand the flow behavior within smooth pipes.
Examples & Analogies
Imagine driving on a highway. The average speed of cars is like the average velocity in a pipe, while individual cars may speed up or slow down, reflecting the difference between the velocity at any point (u) and the average velocity (V average).
Deriving the Velocity Equation
Chapter 3 of 10
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And therefore, from the above equation we can simply subtract these two equations and we are able to find u minus V average by u star.
Detailed Explanation
In this step, we manipulate the derived equations to express the difference between point velocity and average velocity as a function of turbulence characteristics, leading to a specific formula involving logarithmic functions.
Examples & Analogies
Think of it as putting together pieces of a puzzle. By understanding how each piece (or in this case, equation) fits together, you can create a complete picture (the overall flow behavior in the pipe).
Key Equation for Smooth Pipes
Chapter 4 of 10
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Chapter Content
So, it will be u star is common, so, it will be u minus V average by u star is equal to 5.75 log to the base 10 u star y by nu u star R by nu.
Detailed Explanation
This equation represents an important relationship in smooth pipe flow, connecting the local velocity, average velocity, and viscosity. By isolating 'u' and 'V average' terms, we can further explore how these velocities interact within smooth pipe conditions.
Examples & Analogies
Consider a smooth escalator. The average speed of movement is constant, but individual movements can vary (like with turbulence). This equation helps us understand how these variations relate to the smooth operation of the escalator.
Comparison with Rough Pipes
Chapter 5 of 10
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Now, we did it for smooth pipes. Now, for rough pipes, we have an equation and we also obtained V average by u star.
Detailed Explanation
This section introduces the concept of rough pipes, indicating that similar equations can be derived for these types of pipes as well, albeit with modified parameters to account for increased friction due to surface roughness.
Examples & Analogies
Imagine a road that's been chipped and cracked versus a newly paved road. The roughness of the surface affects how smoothly vehicles can pass, similar to how rough pipes influence fluid flow.
Observations from Velocity Differences
Chapter 6 of 10
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Is there any observation? If you see for either for smooth or for rough this difference came out to be the same.
Detailed Explanation
An important observation is that the difference between local velocity and average velocity remains consistent regardless of whether the pipe surface is smooth or rough. This consistency is significant for understanding flow behavior.
Examples & Analogies
It's like how the gusts of wind feel similar on both a calm and windy day. The overall effect (difference in weather) can feel the same despite the conditions changing.
Power Law Velocity Profile
Chapter 7 of 10
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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.
Detailed Explanation
This introduces the power law velocity profile, which is an alternative way to express how velocity changes in smooth pipes with respect to the distance from the center. The exponent 'n' relates to the Reynolds number and changes for different flow conditions.
Examples & Analogies
Think of a balloon gradually deflating. The power law describes how the speed of air exiting changes based on how much pressure is left, similar to how fluid velocity changes with distance in a pipe.
Limitations of Power Law Profiles
Chapter 8 of 10
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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.
Detailed Explanation
While power law profiles provide useful information, they have limitations such as not being able to represent a flat profile at the center of the pipe. This poses a challenge in accurately calculating shear stress at the wall, which is critical for understanding fluid behavior.
Examples & Analogies
Think of trying to measure how smooth a surface is with inaccurate tools. If the tools (like power law profiles) can’t give you precise measurements, understanding key aspects like shear stress becomes difficult.
Calculating Average Velocity
Chapter 9 of 10
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Chapter Content
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.
Detailed Explanation
This section introduces a practical problem where we use a specific velocity profile to derive an expression for average velocity in a pipe. This demonstrates how theoretical concepts apply in real-world situations.
Examples & Analogies
It’s like following a recipe while cooking. Each step you take (calculation) must be followed to create the final dish (average velocity) successfully.
Final Average Velocity Expression
Chapter 10 of 10
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Chapter Content
So, V bar is 2 u max into, just copying the same thing from the last line, 7/15 and V bar is going to be 0.816 u max.
Detailed Explanation
After going through a series of calculations, we arrive at a final expression for average velocity (V bar), showing a clear relationship to the maximum velocity. This is a crucial outcome for practical applications in fluid dynamics.
Examples & Analogies
Just like in sports, where you might end up with a final score after many plays, these calculations lead us to a 'score' for average velocity based on our initial conditions.
Key Concepts
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Turbulent Flow: A flow regime characterized by chaotic changes in pressure and velocity.
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Frictional Velocity: A measure of the effect of friction on the flow of fluid.
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Logarithmic Velocity Profile: A common profile used to represent velocity in turbulent flow conditions.
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Power Law Velocity Profile: A mathematical model that relates local velocity to the distance from the center of the pipe.
Examples & Applications
Example: Calculate the average velocity in a smooth pipe if the maximum velocity (u_max) is known and the wall distance (y) is provided.
Example: Use the power law velocity profile to find the average velocity when given the radius of the pipe and n=7.
Memory Aids
Interactive tools to help you remember key concepts
Rhymes
When pipes flow smooth and straight, their speed is sure to elevate; Turbulence will cause a fuss, but average velocity stays with us.
Stories
Imagine a race between two rivers, one smooth and one rocky. The smooth river travels faster, while the rocky one struggles, illustrating how surface texture influences speed.
Memory Tools
To remember the variables, think of the word F.A.R.F: Frictional velocity (u_*), Average velocity (V_avg), Radius (R), and distance from the wall (y).
Acronyms
SPEED
Smooth Pipes Exhibit Easy Dynamics.
Flash Cards
Glossary
- Average Velocity (V_avg)
The mean speed of fluid flowing through a given section of the pipe.
- Frictional Velocity (u_*)
A velocity scale representing the shear stress effect on fluid motion.
- Power Law Velocity Profile
A mathematical representation of velocity distribution across a pipe's cross-section defined by an exponent 'n'.
- Reynolds Number (Re)
A dimensionless number that characterizes the flow regime in a fluid.
- Logarithmic Velocity Profile
A type of velocity distribution commonly used to describe turbulent flow in pipes.
Reference links
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