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FLUID MECHANICS By Farhan Ahmad [email protected] Department of Chemical Engineering, University of Engineering & Technology Lahore

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Page 1: Fluid Mechanics - Chemical Engineering documents 2012chemicalengineeringdocuments.weebly.com/uploads/1/4/2/7/14278644/... · Behavior of a flowing fluid - solid boundaries. ... REYNOLDS

FLUID MECHANICS

By

Farhan Ahmad

[email protected]

Department of Chemical Engineering,

University of Engineering & Technology Lahore

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Behavior of a flowing fluid - solid boundaries.

Influence of the wall is small

the shear stress may be negligible

one that is incompressible and has zero viscosity

potential flow is also called irrotational flow.

No dissipation of mechanical energy into heat.

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Potential Flow

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A streamline is a curve that is everywhere tangent to the

instantaneous local velocity vector.

The flow pattern provided by the streamlines is an instantaneous

visualization of the flow field.

Streamline

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A pathline is the actual path traveled by an individual fluid particle over

some time period.

Pathline

Streakline

A streakline is the locus of fluid particles that have passed sequentially

through a prescribed point in the flow.

Timeline

A timeline is a set of adjacent fluid particles that were marked at the

same (earlier) instant in time.

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REYNOLDS EXPERIMENT

Laminar vs Turbulent Flow

The distinction between the laminar and turbulent flow was first demonstrated in a classic experiment by Osborne Reynolds, reported in 1883.

He used a tank with a pipe taking water from the center into which he injected a dye through a needle.

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Reynolds found that, at low flow rates, the jet of colored water

flowed intact along with the mainstream and no cross mixing

occurred.

The behavior of the color band showed clearly that the water was

flowing in parallel straight lines and that the flow was laminar.

Reynolds Experiment Observations

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When the flow rate was increased, a velocity, called the critical

velocity, was reached at which the thread of color became wavy and

gradually disappeared, as the dye spread uniformly throughout the

entire cross section of the stream of water.

This behavior of the colored water showed that the water no longer

flowed in laminar motion but moved erratically in the form of

crosscurrents and eddies.

This type of motion is turbulent flow.

Reynolds Experiment Observations

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Reynolds Experiment Observations

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Laminar flow Re < 2000

'low' velocity

Dye does not mix with water

Fluid particles move in straight lines

Simple mathematical analysis possible

Rare in practice in water systems.

Transitional flow 2000 < Re < 4000

'medium' velocity

Dye stream wavers in water - mixes slightly.

Reynolds Experiment: Summary

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Reynolds Experiment: Summary

Turbulent flow Re > 4000

'high' velocity

Dye mixes rapidly and completely

Particle paths completely irregular

Average motion is in the direction of the flow

Cannot be seen by the naked eye

Changes/fluctuations are very difficult to detect. Must use laser.

Mathematical analysis very difficult - so experimental measures are used

Most common type of flow.

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Concepts

In a pipe, when

NRe < 2100 (Laminar Flow)

2100 < NRe < 4000 (Transition Flow)

NRe > 4000 (Turbulent Flow)

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Reynolds No. for Non-Newtonian fluids

For Power Law Fluids;

Critical Reynolds number at which transition to turbulent

flow begins;

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Concept of Boundary Layer

Boundary Layer

A boundary layer is defined as that part of a moving fluid in which

the fluid motion is influenced by the presence of a solid boundary.

Effect of Boundary

Velocity gradient and shear stress

Onset of turbulence

Formation and growth of boundary layer

Separation of boundary layer

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Nature of Turbulence

Wall Turbulence

Free Turbulence

Eddy formation

Viscous dissipation

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Deviating velocities in turbulent flow

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Deviating velocities in turbulent flow

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Deviating velocities in turbulent flow

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Deviating velocities in turbulent flow

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Statistical Nature of Turbulence

Three deviating velocity components at single point as a

function of time

Deviating velocity at different positions over same time period

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Statistical Nature of Turbulence

Correlation of deviating velocity between eddies at two

different points

Correlation of deviating velocity of eddies at same point

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Intensity of Turbulence

Intensity of turbulent field refers to the speed of rotation of

the eddies and the energy contained in an eddy of a specific size.

Intensity is measured by the root-mean square of a velocity component.

Intensity is usually expressed as a percentage of the mean velocity or as

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Scale of Turbulence

Scale of turbulence measures the size of the eddies.

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Isotropic Turbulence

When the root-mean-square components of velocities are equal for all directions at a given point, the turbulence is said to be ISOTROPIC.

Nearly isotropic turbulence exists when there is no velocity gradient, as at the centerline of a pipe or beyond the outer edge of a boundary layer.

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Reynolds Stress

Shear forces much larger than those occurring in laminar flow exist in turbulent flow

The mechanism of turbulent shear depends upon the deviating velocities in anisotropic turbulence.

Turbulent shear stresses are called Reynolds Stresses.

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Reynolds Stress

The momentum flux, after time averaging for all eddies, is a turbulent shear stress or Reynolds Stress.

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Eddy Viscosity

The relationship between shear stress and velocity gradient in a turbulent stream is used to define an eddy viscosity Ev .

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Eddy Viscosity

The total shear stress in a turbulent fluid is the sum of the viscous stress and the turbulent stress

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Flow in Boundary Layers

Boundary Layer

A boundary layer is defined as that part of a moving fluid in which

the fluid motion is influenced by the presence of a solid boundary.

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Laminar and Turbulent Flow in Boundary Layers

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Laminar and Turbulent Flow in Boundary Layers

Turbulent boundary layer consists of 3 zones:

Viscous sublayer

Buffer layer

Turbulent zone

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Laminar and Turbulent Flow in Boundary Layers

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Transition from Laminar and Turbulent Flow: Reynolds No

With parallel flow along a plate, turbulent flow first appears at a critical Reynolds number between about 105 and 3 E6

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Boundary Layer formation in straight tube

When the velocity distribution in the tube reaches its final form and remains unchanged during the remaining length of the tube, such flow with an unchanging velocity distribution is called fully developed flow.

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Boundary Layer formation in straight tube

Transition Length for Laminar and Turbulent flow:

The length of the entrance region of the tube necessary for the boundary layer to reach the center of the tube and for fully developed flow to be established is called the transition length.

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Boundary Layer Separation and Wake formation