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Today, we're going to focus on how pressure and shear stress behave as fluid flows through a pipe. Can anyone tell me what happens when water first enters the pipe?
Is there a drop in pressure at the entrance?
Exactly! This drop is called the 'entrance pressure drop.' It's influenced by the Reynolds number in laminar and turbulent flow. Can anyone tell me the Reynolds number's influence?
For laminar flow, it's around 0.06 times Re, and for turbulent flow, it's Re to the power of 1/6.
Great job! And once the flow becomes fully developed, how does the pressure drop change?
In fully developed flow, the pressure drop per unit length becomes constant.
Correct! A crucial distinction is that in the entrance region, there's acceleration, while in fully developed flow, there isn't. This affects how viscous forces and pressure forces balance out.
So, pressure helps to overcome viscosity in both regions?
Precisely! Now let's summarize: there's an entrance pressure drop that varies with Reynolds number, while fully developed flow sees a constant pressure drop per unit length.
Moving on, let's talk about the role of viscous forces. Can anyone explain what happens with respect to these forces in laminar and turbulent flows?
In laminar flow, the flow is smooth and orderly while turbulent flow is chaotic.
Right! But did you know that in practical applications, most flows are turbulent? How does this affect our calculations?
We often can't use theoretical models because full development isn't typically reached in short pipes.
Exactly! So how do we derive characteristics for fully developed laminar flow?
We can use Newton’s Second Law to analyze fluid elements.
That's correct! Newton's laws help establish relationships between shear stress and flow profiles. Can anyone summarize what we derive from the shear stress?
It varies linearly with the radius and can help in calculating the pressure drop.
Well done! Remember, the relationship between shear stress and radius is critical in understanding flow dynamics.
Lastly, let's focus on deriving the flow rate in a pipe using Newton's Second Law. What is our goal here?
We want to establish Poiseuille’s Law!
That's it! Can someone point out what parameters we rely on for this equation?
We consider pressure drop, viscosity, length of the pipe, and diameter.
Excellent! When deriving, how do we set up our equations?
We conduct an integral of the flow profile over the cross-sectional area.
Correct! This leads us to derive the equation for the volumetric flow rate. Can you recall the final form of Poiseuille’s Law?
It's Q = (π * D^4 * Δp) / (128 * μ * l)!
Well summarized! This law is fundamental for analyzing laminar flow and provides us with invaluable insights for practical applications in hydraulic engineering.
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In this section, we delve into the application of Newton's Second Law in hydraulic engineering, specifically in understanding flow regime transitions in pipes. Key discussions include the differences between entrance pressure drop and fully developed flow conditions, the derivation of fluid velocity profiles, and the implications of viscous forces on flow behavior, ultimately leading to insights on Poiseuille's Law.
This section focuses on the practical application of Newton's Second Law within the context of fluid flow in pipes. It begins by explaining the pressure drop experienced when fluid enters a pipe, known as the entrance pressure drop, and contrasts this with conditions in the fully developed flow region where the pressure drop per unit length remains constant. The section also highlights the critical role of viscous forces in balancing pressure forces, emphasizing the unique characteristics of laminar versus turbulent flow.
Through a detailed derivation, we explore how Newton’s Second Law can help define the velocity profile of a fluid in a pipe, leading to the formulation of important equations. The discussion culminates with the introduction of Poiseuille's Law, which describes the volumetric flow rate of a fluid through a cylindrical pipe based on parameters such as pressure gradient, viscosity, and pipe dimensions. This information provides a theoretical underpinning for complex flow analyses in hydraulic systems and guides practical applications.
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This is the snapshot of a fluid element at time t, this one here. And in the fully developed laminar flow this is the velocity profile, as we have seen in our laminar and turbulent flow analysis.
In this chunk, we focus on a fluid element inside a pipe at a specific moment in time. The velocity profile of this fluid is determined by the radius (r) from the center of the pipe. As the fluid flows through the pipe, its behavior is influenced by both the viscosity of the fluid and the pipe's diameter.
Imagine you have a garden hose. When water flows through it, the speed of the water will vary depending on its distance from the center of the hose. The center has the highest velocity, while the edges move slower due to friction. This is similar to what happens in laminar flow inside a pipe.
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The assumptions is that the local acceleration is 0 since the flow is steady. We also assume that the convective acceleration is 0 since the flow is fully developed.
In analyzing the flow, certain assumptions are made: the local acceleration (the change of velocity at a point) is zero because the flow is steady; this means that at any point in time, the fluid's velocity does not change. Similarly, convective acceleration, which relates to changes in flow velocity due to movement through the fluid, is assumed to be zero since we are considering a fully developed flow where the velocity profile remains unchanged.
Think of a train traveling on a straight track at a constant speed. There is no acceleration because the speed is constant. Similarly, in our fluid element within the pipe, the conditions are stable, leading to the assumption of no local or convective acceleration.
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The force acting from this side, if there is a pressure p1, on the left side at section 1 and this is section 2 and if we assume the delta p is the pressure drop.
When analyzing the forces on the fluid element, we account for two types of forces: pressure forces and viscous forces. Pressure on one side of the fluid element creates a force that pushes it forward, while the pressure drop (delta p) represents the difference in pressure between two sections of the pipe, causing resistance due to viscosity. By balancing the forces, we can derive important relationships about flow behavior in the pipe.
Imagine trying to push a car. The pressure you apply can move the car forward, but if there are strong brakes (representing viscosity), it will resist your push. The balance of your push (pressure force) against the brakes (viscous forces) determines how fast the car moves, much like how fluid moves in a pipe.
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So, we can write, delta p/l can be written as 2tau/r.
This equation signifies a relationship between the pressure drop (delta p) per unit length of the pipe (l) and the shear stress (tau) acting on the fluid. It indicates that the pressure drop is dependent on the shear stress and the radius of the pipe. Shear stress is a measure of how much force per unit area is required to make the fluid flow, and as we examine longer pipes, even small shear stresses can lead to significant pressure drops.
Think of stirring a thick mixture with a spoon. The effort (shear stress) you apply to stir can result in a greater 'pressure' in terms of how hard it is to keep the spoon moving through the mixture. In a long pipe, even a small resistance can lead to a big difference in how easy or difficult it is to move the fluid.
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We have used Newton’s second law to derive the discharge rate through a pipe as a function of pressure gradient delta p and this is Poiseuille’s law.
Newton's second law, which connects force, mass, and acceleration, is key in finding out how much fluid flows through a pipe. By applying this law to a fluid element, we establish equations that link the pressure drop to the rate of flow (discharge rate) in the pipe. This relationship we derive is known as Poiseuille’s law, a fundamental principle in fluid mechanics for laminar flow.
Consider a water fountain. The height of water (pressure) influences how fast the water flows out. Poiseuille’s law helps us understand how pressure differences directly affect the flow rate. Just like how a taller fountain will shoot water higher and faster, a higher pressure can push more fluid through a pipe.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Entrance Flow: Characterized by a pressure drop as fluid starts flowing into a pipe.
Fully Developed Flow: A flow state where pressure drop per unit length is constant.
Viscous Force: The resistance within the fluid that impacts flow dynamics.
Poiseuille's Law: Formula for calculating flow rate of a viscous fluid through a pipe.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example of calculating the pressure drop in a pipe using a known Reynolds number.
Practical application of Poiseuille's Law in biomedical engineering for blood flow in capillaries.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
When fluid enters, pressure does drop, in turbulence, watch the flow swap.
Imagine a painter flowing paint smoothly into a tube, each stroke needing just the right pressure to overcome sticky viscosity.
P - Pressure drop, R - Reynolds number, D - Developed flow - Remember PRD for understanding flow dynamics!
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Review the Definitions for terms.
Term: Entrance Pressure Drop
Definition:
The decrease in pressure that occurs as a fluid flows into a pipe, influenced by flow type, such as laminar or turbulent.
Term: Fully Developed Flow
Definition:
A flow regime characterized by steady conditions where the velocity profile and pressure drop remain consistent along a pipe.
Term: Viscous Forces
Definition:
The resistance forces within a fluid due to viscosity that affect flow behavior and pressure drop.
Term: Poiseuille's Law
Definition:
An equation that describes the volumetric flow rate of a viscous fluid through a cylindrical pipe in relation to pressure difference, viscosity, and pipe dimensions.
Term: Reynolds Number
Definition:
A dimensionless number used to predict flow patterns in different fluid flow situations, indicating the transition between laminar and turbulent flow.