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Today, we're going to explore laminar flow in pipes. Can anyone tell me what laminar flow means?
Isn't it when the fluid flows in smooth layers or 'laminas'?
Exactly! In laminar flow, the fluid's motion is orderly and layers do not mix. Now, if we have oil flowing through a circular pipe, how would we calculate the pressure difference?
We need to know the viscosity and the flow rate, right?
Correct. We calculate the flow rate and then use the pressure gradient formula. Remember, for laminar flow, the Reynolds number should be less than 2000. Let's derive it using our earlier example.
What’s the formula for flow in a pipe again?
It's Q = -π/8μ * (dP/dx) * R^4. Where R is the radius of the pipe. Can anyone derive the pressure difference using this formula?
Sure, after substituting the values, we get a pressure difference of around -5599 pascals.
Let’s discuss shear stress in laminar flow. How is shear stress calculated in the context of laminar flow?
Isn't it related to the velocity gradient and viscosity?
Yes! The shear stress τ is given by τ = μ * (du/dy). What do we think is du/dy?
It's the change in velocity with respect to distance!
Exactly. When analyzing flow between plates, the velocity distribution is parabolic. Can someone derive the equation for the maximum velocity?
Using the relationship, it would be um = 1.5 * V_avg.
Great! And the average velocity would be one-twelfth of the shear stress and the pressure gradient. Let's remember this relation!
Moving on to the force balance analysis in parallel plates. Can anyone tell me how we start our calculations?
We begin by analyzing the forces acting on a fluid element.
Exactly! We have pressure forces and shear forces. If we want the equilibrium, what do we equate?
We set the sum of forces equal to zero.
Right! Following this process, we can derive dP/dx = -12μV_avg/t². What do we achieve from this?
We can express how changes in pressure affect flow rates!
Correct, excellent job everyone! Let’s summarize. Today's key concepts were the calculations for flow in pipes, shear stress analysis, and the force balance in parallel plate flow.
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The focus of this section is on analyzing the force balance in laminar flow through both pipes and parallel plates. It discusses the influence of pressure gradients, shear stresses, and the derivation of relevant equations to calculate flow characteristics.
In this section, we delve into force balance analysis in hydraulic engineering, specifically for laminar flow. It starts by addressing laminar flow in circular pipes, providing an example calculation to derive the pressure difference between the two ends of the pipe based on fluid properties like viscosity and specific gravity. The section then shifts to parallel plate flow, highlighting the equilibrium of forces acting on a fluid element between two fixed plates. We derive key equations governing the pressure gradient and shear stress in this scenario. This analysis is crucial in hydraulic engineering for predicting fluid behavior under various conditions, integral to designing efficient systems.
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So, with this in background, we start to write the force or we do the force balance analysis along the flow direction. So, for your convenience I have made the free body diagram that is there, I have just reproduced it in the top corner. You see, P delta y, that is, force per unit length minus this one here and this again is in the negative direction tau delta x.
In this initial part, we begin our force balance analysis by laying out the forces acting on a fluid element in laminar flow. A free body diagram helps visualize these forces: the pressure force acting in the positive direction and the shear stress acting in the opposite direction. The pressure force per unit length is represented as P delta y, while the force due to shear stress is represented as tau delta x. This setup is crucial for deriving further relationships in fluid mechanics.
Think of a thick book resting on a smooth table. If you push the book (applying a force), the frictional force (which acts in the opposite direction) resists your push. Similarly, in fluid flow, the pressure inside a fluid pushes it forward, while shear stress (like the friction from the table) opposes the motion.
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Now, if we divide both sides by delta x into delta y, that is, area, what we are going to get is, so, this becomes P delta x delta y and this also become P delta x into delta y whole square. So, this will get cancelled here, here. So, if you do these cancellations what we are actually left with is dP dx here and d tau dy, rest of the things will get cancelled.
By dividing both sides of the force balance equation by the area (delta x times delta y), we simplify the equation. This helps us isolate the differentials – the change in pressure (dP) with respect to x and the change in shear stress (d tau) with respect to y. This mathematical manipulation is crucial as it leads us to understand how these forces interact within a fluid element as it flows.
Imagine you have a stretched rubber band. The tension in the rubber band would represent pressure, while the stretching forces along the length symbolize shear stress. If you cut the rubber band into small segments, examining tension over each segment helps us understand how the entire band behaves under stretching, similar to analyzing forces in fluid flow.
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Now, this is again a laminar flow assumption and also we will also assume that the mu the viscosity is constant. So, this is the equation that we get after we put in this, this is equation 8.
Under the assumption that flow is laminar and viscosity remains constant, we can express the relationship obtained into an equation (Equation 8). This equation relates the pressure gradient to shear stress and, crucially, outlines that the behavior of fluid flow can be described mathematically. This is fundamental in fluid mechanics as it provides a direct connection between forces acting on a fluid and the resulting motion.
Consider a slow-moving stream of honey. It's thick and flows smoothly. The constant thickness (viscosity) helps us predict how the honey will flow in different conditions. Similarly, the equivalent equation in our analysis helps predict fluid behavior under varying pressures.
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Now, because here it is double integral, so we will integrate it twice. So, we will get, because we have assumed y, you see, y is in this direction.
The equation derived from our force balance needs to be integrated to consider the cumulative effect of pressure and shear stress along the flow direction (y). By performing double integration, we account for variations in both pressure and shear stress across the height of the fluid element. This integration will yield velocity profiles and help in understanding the flow behavior more completely.
Think of filling a two-dimensional container with water. As you pour the water in (the primary force), the water distributes itself throughout the container bottom, creating a varied depth profile. Similarly, double integration in our analysis allows us to capture the varying effects of forces in the flow across a depth.
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Now the boundary conditions are u at y equal to 0 if the plate is fixed. So, due to no slip condition the velocity will be 0 also at the thickness at the other end after the distance t.
When setting up our equations, we must apply boundary conditions to account for real-world scenarios. The no-slip condition dictates that the fluid at the boundary (in contact with a fixed plate) has zero velocity. Similarly, at the opposing boundary (thickness t), the velocity remains zero. These conditions are crucial for ensuring that the equations reflect actual behavior of fluids in confined spaces.
Imagine a car that comes to a stop at a red light. The tires touching the asphalt (fixed plate) aren't moving. This situation affects the whole car's behavior (similar to fluid behavior), where the velocity gradient starts to form as you go away from the stopping point towards the fast-moving center of the road.
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This is also something that you can try to remember because it is quite simple. Here, also the velocity distribution is parabolic, you see, ty - y square, parabolic in nature.
The resulting equation for fluid velocity profile shows a parabolic distribution, which is typical for laminar flow between parallel plates. This implies that fluid flows fastest at the centerline and slowest at the boundaries due to viscous effects. Understanding this profile is key in applications where laminar flow is critical, such as in designing certain types of piping systems.
Think of a slide in a water park. The water flows faster in the middle (the centerline), mimicking the parabolic shape of the velocity profile, while the edges (where it contacts the slide) slow down due to friction. Recognizing this helps in predicting where water moves fastest and planning better for flow systems.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Laminar flow: Fluid motion characterized by orderly layers.
Pressure difference: Variation in pressure that can be calculated via fluid properties.
Force balance: The equilibrium of forces acting on a fluid element in motion.
See how the concepts apply in real-world scenarios to understand their practical implications.
Calculating pressure drop in a horizontal pipe due to oil flow.
Determining shear stress between fixed parallel plates under laminar flow conditions.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Flow in layers, calm and tight, Laminar’s the order, pure delight.
Imagine a calm river with layers of leaves floating smoothly. Each leaf represents a lamina, gliding effortlessly without disturbance.
To remember the sequence for force balances - 'PEST' - Pressure, Equilibrium, Shear, Transition.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Laminar Flow
Definition:
A type of fluid flow characterized by smooth, orderly layers of fluid.
Term: Viscosity
Definition:
A measure of a fluid's resistance to deformation or flow.
Term: Reynolds Number
Definition:
A dimensionless number that helps predict flow patterns in different fluid flow situations.
Term: Pressure Gradient
Definition:
The rate of change of pressure in a fluid flow per unit distance.
Term: Shear Stress
Definition:
The stress component that acts parallel to the surface of a material.