Industry-relevant training in Business, Technology, and Design to help professionals and graduates upskill for real-world careers.
Fun, engaging games to boost memory, math fluency, typing speed, and English skills—perfect for learners of all ages.
Enroll to start learning
You’ve not yet enrolled in this course. Please enroll for free to listen to audio lessons, classroom podcasts and take practice test.
Listen to a student-teacher conversation explaining the topic in a relatable way.
Today, we'll begin our exploration of the discharge Q, which is crucial in understanding fluid flow in pipes. Discharge represents the volume of fluid flowing through a pipe per unit time.
Is discharge measured in specific units?
Yes, discharge is usually measured in cubic meters per second (m³/s). It’s essential for hydraulic engineering to quantify how much fluid can be transported.
Turbulent flow occurs when fluid moves chaotically, influenced by the Reynolds number. This transition influences how fluid personifies within a pipe.
What exactly influences the Reynolds number?
Great question! The Reynolds number is influenced by fluid velocity, fluid density, fluid viscosity, and the pipe diameter. As it surpasses a critical value, flow becomes turbulent.
Let’s analyze the velocity profile in smooth pipes. As we use the logarithmic profile, it's important to note how the velocity nears zero at certain points from the wall.
How does that relate to our equations?
Excellent! The behavior we observe leads us to express relationships through our equations, specifically transforming log relationships between velocity and distance.
Now, let’s explore how rough pipes differ from smooth ones. The characteristics of roughness must be accounted for in our equations.
How do we quantify the roughness in our calculations?
We typically characterize roughness using the height of roughness k, as derived from experiments by Nikuradse. The impact of roughness can change our velocity profile expressions markedly.
Lastly, let’s apply our knowledge to a real-world problem to solidify your understanding. Given certain parameters, we will determine the roughness of a pipe.
What are the fundamental steps we’ll take?
We’ll start with the known diameters and velocities, applying our derived equations to find the height of roughness. Let’s get started!
Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.
In this section, we delve into the fundamental concepts of discharge Q and the equations that describe turbulent flow in pipes. We highlight the differences between smooth and rough pipe surfaces, introduce key equations, and provide practical examples to facilitate understanding.
This section examines the derivation of the discharge equation Q and discusses the unique characteristics of turbulent flow in both smooth and rough pipes. Starting with a reference to equation 18, we analyze the implications of smooth pipe behavior in the context of velocity profiles and logarithmic function applications. Notably, the derivations showcase how the velocity approaches zero at some finite distance from the pipe wall and incorporate experimental findings from Nikuradse. The conversion from natural logarithm to common logarithm is also discussed, alongside the significance of roughness in turbulent flows through additional equations for rough pipes.
We conclude this section by solving practical problems that illustrate how to determine the roughness of a pipe based on velocity measurements at different distances from the wall, paving the way for a better understanding of discharge calculations and their applications in hydraulic engineering.
Dive deep into the subject with an immersive audiobook experience.
Signup and Enroll to the course for listening the Audio Book
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. Because if we put y is equal to 0 it is going to be infinity. So, this logarithmic profile does not fit this. Therefore, we assume that u is 0 at some finite distance y dash y prime from the wall.
In fluid mechanics, particularly when studying flow near a boundary (like a pipe wall), we find that the speed of fluid (velocity) is not uniform. At the wall, the velocity is 0 due to the no-slip condition, where the fluid 'sticks' to the surface. As we move away from the wall (to a distance y prime), the velocity increases. The equation indicates that this pattern resembles a logarithmic curve, showing that at a specific point, the velocity becomes a function of the distance from the wall and a constant that scales with velocity, known as the von Kármán constant (Kappa). However, at an infinitely close distance to the wall (y=0), the logarithm function approaches negative infinity, indicating we cannot just plug in 0 into our equations.
Think of a thick blanket lying on a table. At the point where it touches the table (the wall), it doesn’t move; this represents the no-slip condition (velocity is zero). However, if you lift the blanket just a little off the table, it begins to ripple and creates motion. The distance at which it starts to ripple (the velocity begins to increase) is similar to our y prime, showing how the velocity changes with distance from the boundary.
Signup and Enroll to the course for listening the Audio Book
Now, this equation number 22, can be expressed in terms of common logarithm as, so, what we have done? We have done, converted ln into log, because the previous equation was in terms of natural log.
In fluid dynamics, equations can be expressed using different types of logarithms depending on the context. Here, the natural logarithm (ln) used in earlier equations has been converted into a base-10 logarithm. This is often done for ease of calculation or to conform to standardized equations that some engineers may prefer to use. This step ensures that our turbulence equations will be widely applicable and easier to handle in calculations.
Imagine you are trying to explain how tall a tree is, but you have a ruler that measures in inches and your friend uses a meter stick. To make your communication clearer, you convert your measurements into meters, which your friend understands better. Similarly, converting from natural log to common logarithm makes our calculations and communication about fluid flow much more straightforward and collaborative.
Signup and Enroll to the course for listening the Audio Book
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.
The roughness of a pipe surface affects how the fluid flows through it. Nikuradse's work established that the distance at which the velocity profile behaves in a specific manner (y prime) for rough surfaces can be approximated as k divided by 30. Here, 'k' represents the roughness height of the pipe surface. This finding implies that the velocity profile will vary depending on the texture of the pipe surface, emphasizing the importance of accounting for surface roughness in calculations related to turbulent flow.
Consider sliding down a slide at a playground. A smooth slide allows you to go down quickly, while a slide made of rough material will slow you down significantly. The roughness of the slide is akin to the roughness of a pipe; it impacts how smoothly and quickly the fluid flows through.
Signup and Enroll to the course for listening the Audio Book
Given is, D is equal to 10 centimeters or 10 into 10 to the power minus 2 meters or 0.1 meter. It is given, u at y is equal to 4 centimeters or 4 is equal to 1.4 times u at y is equal to 1 and the surface is rough.
In this example, we are provided with specific values, such as the diameter of the pipe and the velocity of fluid at various points from the wall. The concept here is to determine the average height of surface roughness through calculations based on fluid velocities at specific distances from the wall. This example walks through the necessary steps and substitute values into established equations to get to the result, showcasing the practicality of the previously derived equations in real-world scenarios.
Imagine you're trying to assess how steep a hill is by measuring the slope at different points with a protractor. Here, each measurement you take at a different distance is like measuring the fluid's velocity at those specified distances in the pipe. By comparing these measurements through calculations, you can understand the overall steepness (or roughness) of the hill (or pipe).
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Discharge Q: Measurement of fluid flow in pipes.
Turbulent Flow: Chaotic fluid movement characterized by high Reynolds numbers.
Height of Roughness (k): Significant in understanding flow in rough pipes.
See how the concepts apply in real-world scenarios to understand their practical implications.
An example of calculating discharge with a known flow rate and pipe diameter.
Using velocity measurements at different heights in a rough pipe to determine its roughness.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In pipes so round, fluid does abound; Discharge flows smooth, whereas turbulence is profound.
Imagine a river. As it flows swiftly, it turns tumultuous with eddies and waves, like the chaos in turbulent flow, while calm lakes reflect tranquility, representing laminar flow.
R.E.T. - Remember Energy Tied, where R is Reynolds, E for Efficiency, T for Turbulent flow.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Discharge (Q)
Definition:
The volume of fluid flowing through a pipe per unit time, typically measured in cubic meters per second.
Term: Turbulent Flow
Definition:
A type of fluid flow characterized by chaotic changes in pressure and flow velocity.
Term: Reynolds Number (Re)
Definition:
A dimensionless number that helps predict flow patterns in different fluid flow situations.
Term: Logarithmic Profile
Definition:
An expression used to relate fluid velocity to distance from the wall in turbulent flow.
Term: Height of Roughness (k)
Definition:
A parameter representing the average roughness of a pipe's surface, affecting flow characteristics.