Problem Solving for Parallel Plates - 3.6 | 17. Laminar and Turbulent Flow (Contnd.) | Hydraulic Engineering - Vol 1
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Introduction to Laminar Flow between Parallel Plates

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0:00
Teacher
Teacher

Welcome, everyone! Today, we’re diving into laminar flow between parallel plates. Can anyone tell me what laminar flow is?

Student 1
Student 1

Isn't it when the fluid flows in parallel layers without disruption?

Teacher
Teacher

Exactly! In laminar flow, each layer of fluid moves smoothly past adjacent layers. Now, when we have two fixed plates, what happens to the fluid between them?

Student 2
Student 2

The flow becomes more predictable and we can describe it with specific equations?

Teacher
Teacher

Right! We often describe this flow with a parabolic velocity profile. Remember, for laminar flow, the Reynolds number is less than 2000, which ensures smooth flow. Let’s move forward!

Deriving the Velocity Profile

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Teacher
Teacher

Now, let’s derive the equation for velocity in laminar flow. What do we consider in our equation?

Student 3
Student 3

We need the pressure gradient and viscosity, right?

Teacher
Teacher

Yes! The relationship we derive shows the velocity distribution is parabolic, expressed as u = -1/(2*mu)*(dP/dx)*(t^2 - y^2). Can anyone explain why it's parabolic?

Student 4
Student 4

Because the fluid's velocity decreases towards the plate due to viscosity, creating a smooth curve.

Teacher
Teacher

Precisely! This parabolic equation is crucial for understanding how fluids behave between plates. Let's practice applying this to a problem!

Solving Problems with Parallel Plates

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Teacher
Teacher

Let’s tackle a problem. If we have a maximum velocity of 2 m/s and a plate distance of 0.1 m, with a viscosity of 2.45 Pascal seconds, what would we do first?

Student 1
Student 1

First, we would find the average velocity using the equation you provided.

Teacher
Teacher

Correct! And what does that lead us to find next?

Student 2
Student 2

We calculate the pressure gradient using the average velocity relationship.

Teacher
Teacher

Exactly! This systematic approach allows us to determine key parameters in fluid dynamics. How do we fix our boundary conditions?

Student 3
Student 3

We set the velocities at both plates to zero due to the no-slip condition!

Teacher
Teacher

Well done! With this, we can now calculate shear stress as well. Practice this with the example homework!

Introduction & Overview

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Quick Overview

This section delves into the dynamics of laminar flow between parallel plates, discussing key equations, principles, and practical problem-solving techniques.

Standard

In this section, we investigate laminar flow between fixed parallel plates, deriving critical equations and relationships, such as pressure gradients and shear stresses. Practical examples illustrate their application, showing how to determine relevant fluid parameters in engineering contexts.

Detailed

Problem Solving for Parallel Plates

In this section, we explore the intricacies of laminar flow between two fixed parallel plates, a simple yet critical setup in hydraulic engineering. The section begins with a review of fundamental concepts like shear stress and pressure gradients. Through a systematic breakdown of the underlying physics, we derive relevant equations, including the average flow velocity, discharge per unit width, and the relationship between shear stress and pressure gradient.

The section illustrates how boundary conditions influence fluid dynamics, showcasing a parabolic velocity profile characteristic of laminar flow. To solidify understanding, we present practical problems that involve calculating parameters such as pressure gradient and shear stress, allowing students to engage directly with the principles at play. By the end of this section, students will be equipped with both the theoretical knowledge and problem-solving skills necessary for dealing with laminar flow systems in real-world applications.

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Introduction to Laminar Flow Between Parallel Plates

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Now we have done the laminar flow through the circular pipe. Now we are going to see the laminar flow between the parallel plates. So, this is a parallel plate. So, whatever assumptions that we have made for laminar flowing pipes are valid here also. In this case both the plates are fixed plate and this is also fixed plate. As you can observe, this is x direction and this is y direction.

Detailed Explanation

In this chunk, we shift our focus from laminar flow in pipes to laminar flow between parallel plates. Similar principles apply; however, the arrangement of the system is different. The fixed parallel plates establish a controlled environment allowing students to explore how fluids behave under shear between stationary boundaries.

Examples & Analogies

Imagine squeezing a tube of toothpaste. If you hold the bottom of the tube still and push down on the top, the toothpaste flows out in a way that resembles how fluid moves between fixed plates. The toothpaste in the middle is similar to the fluid moving slower where it is closest to the surface.

Concept of Pressure and Forces in the System

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The thick the distance between the plate is given by t, the flow is in this direction positive x axis and what we have assumed is an element having the thickness this length is delta x and this is delta y this is the direction. And as we have written all the forces in a similar fashion as we did it for the pipe flow.

Detailed Explanation

This segment introduces how we visualize the spacing, referred to as 't', between the plates, and establishes the flow direction. By dissecting the system into infinitesimally small elements (delta x and delta y), we can analyze the forces acting due to pressure and shear stresses. The balance of these forces will be critical in deriving meaningful equations for flow between the plates.

Examples & Analogies

Picture two flat surfaces, like a sandwich, being pressed together. The pressure between the slices creates a scenario similar to the way forces act across the plates, showing how the 'thickness' influences movement and pressure distribution between them.

Force Balance Analysis

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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.

Detailed Explanation

In this chunk, we perform a force balance analysis by identifying all acting forces. The pressure force acts in one direction while the shear force acts in the opposite direction. This balance of forces is fundamental to finding the relationship governing the flow characteristics, particularly the pressure gradient.

Examples & Analogies

Think of a game of tug-of-war where one side pulls with force derived from pressure and the other side exerts a resisting force via friction (shear). The equilibrium between these forces will determine who wins – in this case, the 'winner' tells us how the fluid will flow!

Deriving the Relationship for Flow

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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. So, this is one important equation that we are going to get.

Detailed Explanation

Upon performing the mathematical manipulations, we arrive at a simplified equation that relates the pressure gradient (dP/dx) and the rate of change of shear stress (dτ/dy). This equation forms the basis for predicting how changes in pressure affect flow rates within the confines of the parallel plates.

Examples & Analogies

Imagine a flow of cars (fluid) on a road (the plate space). If there is a speed limit enforced (pressure gradient) and traffic flow (shear), understanding how one influences the other can help city planners optimize traffic flow – much like how we optimize fluid flow using dP/dx and dτ/dy.

Boundary Conditions and Final Velocity Profile

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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. So, this is the equation we get. 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.

Detailed Explanation

This part discusses the application of boundary conditions, specifically the no-slip condition (fluids in contact with a solid surface don't move relative to that surface). By integrating the relationship we previously derived and applying these conditions, we can arrive at the velocity profile of the fluid between the plates, which, notably, takes on a parabolic shape.

Examples & Analogies

Think of icing on a cake. The frosting spreads out more in the middle and less at the edges (the plates), representing how fluid velocity behaves where it reaches a maximum at the center and diminishes near the surfaces due to the no-slip condition.

Average Velocity and Discharge Calculations

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Now, repeating the same procedure of average velocity, maximum velocity and discharge. The average velocity is again given by integral 0 to t u dy / t... This means the maximum velocity again is at the center line, which is y is equal to t / 2.

Detailed Explanation

In this segment, we calculate the average velocity and maximum velocity of fluid flow between parallel plates. The average is derived through integration of the velocity profile, and it distinctly shows that the maximum velocity occurs at the midpoint of the gap between the plates. This discussion also leads to how we determine the overall discharge.

Examples & Analogies

If you've ever watched a fountain, the water shoots highest at the center but slows as it splashes around. This animation is akin to how velocities vary in fluid flow between the two plates, showcasing a peak in the midsection.

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Pressure Gradient: The rate of pressure change in the fluid, affecting flow movement.

  • Shear Stress: Defines the force applied per unit area, critical in fluid dynamics.

  • Velocity Profile: The shape of the velocity distribution across the fluid layer.

Examples & Real-Life Applications

See how the concepts apply in real-world scenarios to understand their practical implications.

Examples

  • For a fluid with a maximum velocity of 3 m/s between two plates 0.2 m apart and viscosity of 1.5 Pa·s, calculate the average velocity and pressure gradient using derived equations.

  • If the shear stress at the wall of a parallel plate flow is found to be 50 N/m², what does this suggest about the flow characteristics?

Memory Aids

Use mnemonics, acronyms, or visual cues to help remember key information more easily.

🎵 Rhymes Time

  • In smooth layers they flow, laminar will show, no turbulence to sow.

📖 Fascinating Stories

  • Imagine a calm river with two parallel banks, fluid slips by silently, no waves to rank.

🧠 Other Memory Gems

  • LAMP: Laminar flow, Average velocity, Maximum velocity, Pressure gradient.

🎯 Super Acronyms

PALS - Plates And Layered Shear, a reminder of parallel plate flow dynamics.

Flash Cards

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Glossary of Terms

Review the Definitions for terms.

  • Term: Laminar Flow

    Definition:

    A type of fluid flow characterized by smooth, parallel layers of fluid.

  • Term: Reynolds Number

    Definition:

    A dimensionless number used to predict flow patterns in different fluid flow situations.

  • Term: Shear Stress

    Definition:

    The force per unit area acting parallel to the fluid layers, significant in laminar flows.

  • Term: Pressure Gradient

    Definition:

    The rate of pressure change in a fluid and is crucial for determining fluid movement.

  • Term: Velocity Profile

    Definition:

    A representation of the variation of fluid velocity across a cross-section of flow.