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Today, we will explore turbulent flow in smooth pipes. Can anyone remind me what defines turbulent flow?
I think it has to do with the Reynolds number being greater than about 4000?
Exactly! When the Reynolds number exceeds 4000, flow becomes turbulent. Remember, Reynolds number is a dimensionless quantity indicating flow type based on speed, viscosity, and characteristic length.
What happens at a microscopic level during turbulent flow?
Great question! In turbulent flow, fluid particles move chaotically, creating mixing and fluctuations in velocity, which we will dive into now.
As a memory aid, remember the acronym 'RAPID' - Reynolds, Apply, Particles, Irregular motion, Disruptive flow - to encapsulate turbulent flow properties.
That’s helpful! How do we mathematically express this turbulent flow?
We use specific equations! Let's look at Equation 18, which helps depict velocity profiles along a smooth pipe.
Are these equations used in real-world applications?
Yes, they’re critical in engineering design for pipelines, channels, and any flow systems. Now, let's summarize: turbulent flows involve high Reynolds numbers, chaotic particle motions, and specific mathematical expressions.
Now, let’s take a closer look at velocity profiles in smooth pipes. Does anyone remember the significance of distance from the wall in our equations?
Yes, distance influences velocity profiles, right? I think we saw that in Equation 22.
That's right! As we approach the wall of a pipe, the velocity decreases due to viscous effects. At the wall, velocity is zero. This is important for calculations of turbulent hydraulic systems.
How do we calculate the average velocity from these profiles?
Good question! We’ll integrate the velocity equations over the cross-sectional area of the pipe. For smooth pipes, this brings us to results highlighted in Equation 28 and 30 in our material.
Can you recall our previous unit on laminar flow? Do we have similar equations?
Yes, while laminar flow uses simpler linear and parabolic profiles, turbulent flow involves logarithmic distributions, which are more complex but reflect the chaotic nature. Remember, 'TURBULENT' highlights key elements - T for turbulent, U for unpredictable, R for roughness impacts, B for blending of layers.
So, turbulent flow has both velocity layers and roughness factors to consider?
Exactly! Let's summarize: turbulent velocity profiles vary with distance from the wall due to viscous effects and involve logarithmic equations.
Let’s put our knowledge into practice! I’ll present an example; we must determine the roughness height for a specified flow rate. Who wants to give it a try?
I'll give it a shot! What's the diameter of the pipe again?
The diameter is 10 cm, with velocity at various heights given. We need to apply our earlier equations to find the roughness! What's our first step?
We need to convert the diameter and heights into meters first!
Correct! Now, rewrite the velocities based on the given ratios. What can we find next?
We can set up the equations based on observations at different heights and input them to solve for k, the roughness height.
Right! By approaching from experimental data like Nikuradse’s findings, we can ensure our calculations reflect real-world applications. What did we learn here?
It’s crucial to consider both the theory and experimental data when assessing turbulent flows in engineering.
Excellent summary! Of course, these computations have implications across hydraulic systems making them vital in civil engineering.
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The content elaborates on the principles and equations governing turbulent flow in smooth pipes, derived from fundamental theories and experiments. Significant attention is given to the velocity profiles and the role of roughness in turbulent flow.
This section delves into the concepts of laminar and turbulent flow within hydraulic engineering. It specifically addresses turbulent flow in smooth pipes, guided by foundational equations and empirical evidence.
The discourse begins by reiterating the importance of Reynolds number, which categorizes flow types based on velocity and parameters like viscosity. It presents Equation 18, which forms the basis for understanding velocity profiles at various distances from a wall.
Through substitution, Equation 23 illustrates the velocity distribution for turbulent flow in smooth and rough pipes, emphasizing Nikuradse's experiments that relate roughness height to flow behavior. This section also includes practical insights, evidenced by a problem-solving example challenging students to determine roughness based on given velocities at specific distances from the pipe wall.
Furthermore, the section introduces methods for calculating average velocity in both smooth and rough pipes reinforcing the application of theory in real-world scenarios. The equations discussed facilitate a profound understanding of the turbulent velocity distributions crucial for civil engineering applications.
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Welcome back to this last lecture of turbulent flow and laminar flows where we are going to talk about turbulent flow in smooth pipes.
This introduction sets the stage for discussing turbulent flow in smooth pipes. It indicates that the lecture will build upon previous topics and concepts related to fluid dynamics, specifically focusing on turbulent flow, which is characterized by chaotic changes in pressure and flow velocity.
Think of a river; when the water flows smoothly, it resembles laminar flow. But when it hits rocks, creating rapids, it turns into turbulent flow. This lecture helps us understand the physics behind how fluid behaves in both calm and chaotic states.
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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.
This section emphasizes a critical point in fluid mechanics: the velocity of fluid at the very wall of a pipe (where y = 0) is theoretically zero, as consequences from Logarithmic Velocity Profile equations. It shows that as you move closer to a wall, the velocity decreases until it hits zero due to molecular adhesion, known as the 'no-slip condition'.
Imagine two cars driving on a highway; one stops right at the edge of the road (like fluid at the wall), while the other is further back on the road. The closer a car gets to the road's edge, the slower it can go due to congestion at the barrier, similar to how fluid slows at the wall.
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Hence, from equation 18, we say that at distance y prime C will be minus u star by Kappa ln y prime. Therefore, we obtain, if we use this in equation number 18 and substitute Kappa is equal to 0.4.
The derivation discusses how the velocity distribution of turbulent flow can be expressed mathematically. Substituting constants into the logarithmic equations provides a more concrete understanding of how velocity varies within the fluid. The 'C' comes from boundary conditions reflecting the effects of viscosity and distance from the wall on velocity.
Think of this equation as a temperature chart on the road. At the center of the road (far from edges), the temperature might be a constant high, while along the edges, it gradually gets cooler. Similarly, fluid speed is fastest at the center of the flow and slows down as it approaches the boundaries.
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For rough pipes Nikuradse obtained the value of y prime as k/30. This is obtained by Nikuradse.
The discussion shifts focus to turbulent flow in rough pipes, where the roughness affects the velocity distribution. Nikuradse's research gives us a comparative model to analyze how variation in pipe surface influences fluid dynamics. The introduced variables help in deriving equations applicable specifically to rough surfaces.
Imagine riding a bike on a smooth road compared to a gravel path. On the smooth road, you maintain speed easily; however, on the rough path, your speed drops due to increased friction. This analogy shows how rough pipes can impede fluid flow, resembling how rough terrain affects a cyclist.
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Now, it is a good idea to solve one problem here, on this particular concept...
The framed problem engages students to actively apply the learned concepts. Students are asked to calculate the roughness height of a pipe based on given conditions, reinforcing the theoretical knowledge presented in previous sections by transitioning it to practical applications.
Solving this problem can be compared to cooking: following a recipe (analogous to the problem statement) helps you create a dish while understanding the science behind it. Just like precision in measurements can result in the perfect cake, accuracy in applying these formulas will refine our understanding in fluid mechanics.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Turbulent Flow: Flow characterized by chaotic fluctuations in velocity and pressure.
Reynolds Number: Key parameter for determining flow type indicating laminar or turbulent behavior.
Velocity Profile: The distribution of velocity at different distances from the pipe wall, crucial for design calculations.
See how the concepts apply in real-world scenarios to understand their practical implications.
Determining the roughness height of a pipe when given the velocity differences at varying distances from the wall.
Application of turbulent flow equations to predict the behavior of water flowing through a smooth versus a rough pipe.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In flow so wild, chaos does prevail; turbulent motion, a swirling tale.
Imagine a peaceful river flowing smoothly, that's laminar. Then picture a storm with rough waves; that's turbulent flow!
RAPID - Reynolds, Apply, Particles, Irregular motion, Disruptive flow for remembering turbulent flow characteristics.
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Review the Definitions for terms.
Term: Reynolds Number
Definition:
A dimensionless number used to predict flow patterns in different fluid flow situations, calculated as the ratio of inertial forces to viscous forces.
Term: Turbulent Flow
Definition:
A flow regime characterized by chaotic property changes, such as velocity and pressure, occurring at high Reynolds numbers.
Term: Viscous Sublayer
Definition:
The layer of fluid in contact with a surface where the flow is laminar and dominated by viscous forces.
Term: Logarithmic Profile
Definition:
A mathematical description of velocity distribution in turbulent flows, commonly used to describe flows near boundaries.
Term: Nikuradse’s Experiment
Definition:
An experimental assessment of turbulent flow in rough pipes, establishing relationships for roughness height and its impact on velocity profiles.