Dimensional Analysis and Similitude . Dimensional Analysis ä Dimensions and Units   Theorem ä Assemblage of Dimensionless Parameters ä Dimensionless.

Slides:



Advertisements
Similar presentations
Fluid Mechanics EIT Review.
Advertisements

FLUID MECHANICS AND MACHINERY U3MEA03 Prepared by Mr. Kannan, Assistant Professor, Mechanical Department VelTech Dr.RR & Dr.SR Technical University.
VELTECH Dr RR & Dr SR TECHNICAL UNIVERSITY DEPARTMENT OF MECHANICAL ENGINEERING DEPARTMENT OF AUTOMOBILE ENGINEERING U3MEA03 FLUID MECHANICS AND MACHINERY.
Convection.
HYDRAULIC 1 CVE 303.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 7.
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Closed Conduit Flow CEE 332.
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Closed Conduit Flow CEE 332.
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 9: FLOWS IN PIPE
Pertemuan CLOSED CONDUIT FLOW 2
Dimensional Analysis and Similitude CEE 331 Summer 2000 CEE 331 Summer 2000 
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Dimensional Analysis and Similitude CEE 331 June 22, 2015 
FINAL LECTURE of NEW MATERIAL!!! (1) How to build a better model (2) Lift, Drag, Pressure forces considered together.
Fluid Mechanics Wrap Up CEE 331 June 27, 2015 CEE 331 June 27, 2015 
CEE 331 Fluid Mechanics April 17, 2017
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Dimensional Analysis and Similitude CEE 331 June 28, 2015 CEE 331 June 28, 2015 
California State University, Chico
Pertemuan CLOSED CONDUIT FLOW 1
CEE 331 Fluid Mechanics April 17, 2017
Resistance and Powering of Ships
Fluid mechanics 3.1 – key points
FE Hydraulics/Fluid Mechanics Review
Convection Prepared by: Nimesh Gajjar. CONVECTIVE HEAT TRANSFER Convection heat transfer involves fluid motion heat conduction The fluid motion enhances.
Similitude and Dimensional Analysis
Pharos University ME 259 Fluid Mechanics Lecture # 9 Dimensional Analysis and Similitude.
Fluid Properties: Liquid or Gas
CEE 331 Fluid Mechanics April 22, 2017
Buckingham Pi Theorem This example is the same as example 7.2 in the textbook except that we assume the pipe is a smooth pipe. Using Buckingham Pi theorem,
Aula Teórica 18 & 19 Adimensionalização. Nº de Reynolds e Nº de Froude. Teorema dos PI’s, Diagrama de Moody, Equação de Bernoulli Generalizada e Coeficientes.
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
Chapter 7: DIMENSIONAL ANALYSIS AND MODELING
Lesson 21 Laminar and Turbulent Flow
Turbomachinery Lecture 4a Pi Theorem Pipe Flow Similarity

QUESTIONS ON DIMENSIONAL ANALYSIS
Reynolds ( ) Ernst Mach (1838 – 1916).
Chapter 4 DIMENSIONAL ANALYSIS AND DYNAMIC SIMILITUDE
Dimensional Analysis A tool to help one to get maximum information from a minimum number of experiments facilitates a correlation of data with minimum.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 6: DIMENTIONAL ANALYSIS Instructor: Professor C. T. HSU.
© Fox, Pritchard, & McDonald Introduction to Fluid Mechanics Chapter 7 Dimensional Analysis and Similitude.
Unit 1: Fluid Dynamics An Introduction to Mechanical Engineering: Part Two Fluid dynamics Learning summary By the end of this chapter you should have learnt.
30 th June 20111Enrico Da Riva, V. Rao Parametric study using Empirical Results June 30 th 2011 Bdg 298 Enrico Da Riva,Vinod Singh Rao CFD GTK.
 Most of the problems encountered in engineering are of unsteady type.  Two main types of problems under unsteady conditions  The first is where the.
Flow In Circular Pipes Objective ä To measure the pressure drop in the straight section of smooth, rough, and packed pipes as a function of flow rate.
Dimensional Analysis.
DIMENSIONAL ANALYSIS SECTION 5.
VISCOUS FLOW IN CONDUITS  When we consider viscosity in conduit flows, we must be able to quantify the losses in the flow Fluid Mechanics [ physical.
Chapter 7: Dimensional Analysis and Modeling SCHOOL OF BIOPROCESS ENGINEERING, UNIVERSITI MALAYSIA PERLIS.
Elementary Mechanics of Fluids CE 319 F Daene McKinney Dimensional Analysis.
Viscous Flow in Pipes: Overview
Dimensional Analysis. Experimentation and modeling are widely used techniques in fluid mechanics.
Flow Similarity and Model Testing Geometrical similarity: similar geometry. Kinematic similarity: flow pattern around the model should be similar to...
Basic Hydraulics: Energy and Momentum concepts. Energy of flow Three kinds of energy gradients cause flow Elevation (called potential energy) Pressure.
Prepared by: Samera Samsuddin Sah Biosystems Engineering Programme School of Bioprocess Engineering, Universiti Malaysia Perlis (UniMAP)
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
SUGGESTED MINIMUM KNOWLEDGE OF FLUID MECHANICS AND FOR FE EXAM
4.4 DISCUSSION OF DIMENSIONLESS PARAMETERS
Chapter 11 DIMENSIONAL ANALYSIS. 2 Fundamental theory preliminary expt. Dimensional analysis: ( 因次分析 ) Experiments Practical Problems analytical soln.
IIT-Madras, Momentum Transfer: July 2004-Dec 2004 Dimensional Analysis & Similarity Uses: Verify if eqn is always usable Predict nature of relationship.
8.2 OBJECTIVES  Describe the appearance of laminar flow and turbulent flow  State the relationship used to compute the Reynolds number  Identify the.
Turbomachinery Lecture 4a Pi Theorem Pipe Flow Similarity
Part II. Dimensional Analysis and Experimentation
Chapter 4. Analysis of Flows in Pipes
Fluid Mechanics Chapter 8 Dimensional Analysis and Similitude Dr
Similitude and Dimensional Analysis
Chapter 7 : Dimensional Analysis Modeling, and Similitude
Subject Name: FLUID MECHANICS
DIMENSIONAL ANALYSIS.
Introduction to Fluid Mechanics
Lecture 4 Dr. Dhafer A .Hamzah
Presentation transcript:

Dimensional Analysis and Similitude 

Dimensional Analysis ä Dimensions and Units   Theorem ä Assemblage of Dimensionless Parameters ä Dimensionless Parameters in Fluids ä Model Studies and Similitude ä Dimensions and Units   Theorem ä Assemblage of Dimensionless Parameters ä Dimensionless Parameters in Fluids ä Model Studies and Similitude

Frictional Losses in Pipes circa 1900 ä Water distribution systems were being built and enlarged as cities grew rapidly ä Design of the distribution systems required knowledge of the head loss in the pipes (The head loss would determine the maximum capacity of the system) ä It was a simple observation that head loss in a straight pipe increased as the velocity increased (but head loss wasn’t proportional to velocity). ä Water distribution systems were being built and enlarged as cities grew rapidly ä Design of the distribution systems required knowledge of the head loss in the pipes (The head loss would determine the maximum capacity of the system) ä It was a simple observation that head loss in a straight pipe increased as the velocity increased (but head loss wasn’t proportional to velocity).

The Buckingham  Theorem ä “in a physical problem including n quantities in which there are m dimensions, the quantities can be arranged into n-m independent dimensionless parameters” ä We reduce the number of parameters we need to vary to characterize the problem! ä “in a physical problem including n quantities in which there are m dimensions, the quantities can be arranged into n-m independent dimensionless parameters” ä We reduce the number of parameters we need to vary to characterize the problem!

Assemblage of Dimensionless Parameters ä Several forces potentially act on a fluid ä Sum of the forces = ma (the inertial force) ä Inertial force is always present in fluids problems (all fluids have mass) ä Nondimensionalize by creating a ratio with the inertial force ä The magnitudes of the force ratios for a given problem indicate which forces govern ä Several forces potentially act on a fluid ä Sum of the forces = ma (the inertial force) ä Inertial force is always present in fluids problems (all fluids have mass) ä Nondimensionalize by creating a ratio with the inertial force ä The magnitudes of the force ratios for a given problem indicate which forces govern

ä Forceparameterdimensionless ä Mass (inertia)______ ä Viscosity____________ ä Gravitational____________ ä Pressure____________ ä Surface Tension____________ ä Elastic____________ ä Forceparameterdimensionless ä Mass (inertia)______ ä Viscosity____________ ä Gravitational____________ ä Pressure____________ ä Surface Tension____________ ä Elastic____________ Forces on Fluids   R  F pp CpCp  W K M Dependent variable

Inertia as our Reference Force ä F=ma  Fluids problems always (except for statics) include a velocity (V), a dimension of flow (l), and a density (  ) ä F=ma  Fluids problems always (except for statics) include a velocity (V), a dimension of flow (l), and a density (  )

Viscous Force ä What do I need to multiply viscosity by to obtain dimensions of force/volume? Reynolds number

Gravitational Force Froude number

Pressure Force Pressure Coefficient

Dimensionless parameters ä Reynolds Number ä Froude Number ä Weber Number ä Mach Number ä Pressure Coefficient ä (the dependent variable that we measure experimentally) ä Reynolds Number ä Froude Number ä Weber Number ä Mach Number ä Pressure Coefficient ä (the dependent variable that we measure experimentally)

Application of Dimensionless Parameters ä Pipe Flow ä Pump characterization ä Model Studies and Similitude ä dams: spillways, turbines, tunnels ä harbors ä rivers ä ships ä... ä Pipe Flow ä Pump characterization ä Model Studies and Similitude ä dams: spillways, turbines, tunnels ä harbors ä rivers ä ships ä...

Example: Pipe Flow Inertial diameter, length, roughness height Reynolds l/D viscous  /D ä What are the important forces? ______, ______. Therefore _________ number. ä What are the important geometric parameters? _________________________ ä Create dimensionless geometric groups ______, ______ ä Write the functional relationship ä What are the important forces? ______, ______. Therefore _________ number. ä What are the important geometric parameters? _________________________ ä Create dimensionless geometric groups ______, ______ ä Write the functional relationship

Example: Pipe Flow C p proportional to l f is friction factor ä How will the results of dimensional analysis guide our experiments to determine the relationships that govern pipe flow? ä If we hold the other two dimensionless parameters constant and increase the length to diameter ratio, how will C p change? ä How will the results of dimensional analysis guide our experiments to determine the relationships that govern pipe flow? ä If we hold the other two dimensionless parameters constant and increase the length to diameter ratio, how will C p change?

E+031E+041E+051E+061E+071E+08 R friction factor laminar smooth Each curve one geometryCapillary tube or 24 ft diameter tunnelWhere is temperature?Compare with real data!Where is “critical velocity”?Where do you specify the fluid? At high Reynolds number curves are flat. Frictional Losses in Straight Pipes

What did we gain by using Dimensional Analysis? ä Any consistent set of units will work ä We don’t have to conduct an experiment on every single size and type of pipe at every velocity ä Our results will even work for different fluids ä Our results are universally applicable ä We understand the influence of temperature ä Any consistent set of units will work ä We don’t have to conduct an experiment on every single size and type of pipe at every velocity ä Our results will even work for different fluids ä Our results are universally applicable ä We understand the influence of temperature

Model Studies and Similitude: Scaling Requirements MachReynoldsFroudeWeber ä dynamic similitude ä geometric similitude ä all linear dimensions must be scaled identically ä roughness must scale ä kinematic similitude ä constant ratio of dynamic pressures at corresponding points ä streamlines must be geometrically similar ä _______, __________, _________, and _________ numbers must be the same ä dynamic similitude ä geometric similitude ä all linear dimensions must be scaled identically ä roughness must scale ä kinematic similitude ä constant ratio of dynamic pressures at corresponding points ä streamlines must be geometrically similar ä _______, __________, _________, and _________ numbers must be the same

Relaxed Similitude Requirements same size ä Impossible to have all force ratios the same unless the model is the _____ ____ as the prototype ä Need to determine which forces are important and attempt to keep those force ratios the same ä Impossible to have all force ratios the same unless the model is the _____ ____ as the prototype ä Need to determine which forces are important and attempt to keep those force ratios the same

Similitude Examples ä Open hydraulic structures ä Ship’s resistance ä Closed conduit ä Hydraulic machinery ä Open hydraulic structures ä Ship’s resistance ä Closed conduit ä Hydraulic machinery

Scaling in Open Hydraulic Structures ä Examples ä spillways ä channel transitions ä weirs ä Important Forces ä inertial forces ä gravity: from changes in water surface elevation ä viscous forces (often small relative to gravity forces) ä Minimum similitude requirements ä geometric ä Froude number ä Examples ä spillways ä channel transitions ä weirs ä Important Forces ä inertial forces ä gravity: from changes in water surface elevation ä viscous forces (often small relative to gravity forces) ä Minimum similitude requirements ä geometric ä Froude number NCHRP Request For Proposal on “Effects of Debris on Bridge-Pier Scour “

Froude similarity difficult to change g ä Froude number the same in model and prototype ä ________________________ ä define length ratio (usually larger than 1) ä velocity ratio ä time ratio ä discharge ratio ä force ratio ä Froude number the same in model and prototype ä ________________________ ä define length ratio (usually larger than 1) ä velocity ratio ä time ratio ä discharge ratio ä force ratio

Example: Spillway Model ä A 50 cm tall scale model of a proposed 50 m spillway is used to predict prototype flow conditions. If the design flood discharge over the spillway is 20,000 m 3 /s, what water flow rate should be tested in the model?

Ship’s Resistance Viscosity, roughness gravity Reynolds Froude ä Skin friction ______________ ä Wave drag (free surface effect) ________ ä Therefore we need ________ and ______ similarity ä Skin friction ______________ ä Wave drag (free surface effect) ________ ä Therefore we need ________ and ______ similarity

Water is the only practical fluid Reynolds and Froude Similarity? ReynoldsFroude L r = 1

Ship’s Resistance ä Can’t have both Reynolds and Froude similarity ä Froude hypothesis: the two forms of drag are independent ä Measure total drag on Ship ä Use analytical methods to calculate the skin friction ä Remainder is wave drag ä Can’t have both Reynolds and Froude similarity ä Froude hypothesis: the two forms of drag are independent ä Measure total drag on Ship ä Use analytical methods to calculate the skin friction ä Remainder is wave drag empirical analytical

Closed Conduit Incompressible Flow viscosity inertia velocity ä Forces ä __________ ä If same fluid is used for model and prototype ä VD must be the same ä Results in high _________ in the model ä High Reynolds number (R) ä Often results are independent of R for very high R ä Forces ä __________ ä If same fluid is used for model and prototype ä VD must be the same ä Results in high _________ in the model ä High Reynolds number (R) ä Often results are independent of R for very high R

Example: Valve Coefficient ä The pressure coefficient,, for a 600-mm-diameter valve is to be determined for 5 ºC water at a maximum velocity of 2.5 m/s. The model is a 60-mm-diameter valve operating with water at 5 ºC. What water velocity is needed?

Example: Valve Coefficient ä Note: roughness height should scale! ä Reynolds similarity ä Note: roughness height should scale! ä Reynolds similarity ν = 1.52 x m 2 /s V m = 25 m/s

Use water at a higher temperature Example: Valve Coefficient (Reduce V m ?) ä What could we do to reduce the velocity in the model and still get the same high Reynolds number? Decrease kinematic viscosity Use a different fluid

Example: Valve Coefficient ä Change model fluid to water at 80 ºC ν m = ______________ ν p = ______________ V m = 6 m/s x m 2 /s 1.52 x m 2 /s

Approximate Similitude at High Reynolds Numbers ä High Reynolds number means ______ forces are much greater than _______ forces ä Pressure coefficient becomes independent of R for high R ä High Reynolds number means ______ forces are much greater than _______ forces ä Pressure coefficient becomes independent of R for high R inertial viscous

Pressure Coefficient for a Venturi Meter E+001E+011E+021E+031E+041E+051E+06 R CpCp Similar to rough pipes in Moody diagram!

Hydraulic Machinery: Pumps streamlines must be geometrically similar ä Rotational speed of pump or turbine is an additional parameter ä additional dimensionless parameter is the ratio of the rotational speed to the velocity of the water _________________________________ ä homologous units: velocity vectors scale _____ ä Now we can’t get same Reynolds Number! ä Reynolds similarity requires ä Scale effects ä Rotational speed of pump or turbine is an additional parameter ä additional dimensionless parameter is the ratio of the rotational speed to the velocity of the water _________________________________ ä homologous units: velocity vectors scale _____ ä Now we can’t get same Reynolds Number! ä Reynolds similarity requires ä Scale effects

Dimensional Analysis Summary ä enables us to identify the important parameters in a problem ä simplifies our experimental protocol (remember Saph and Schoder!) ä does not tell us the coefficients or powers of the dimensionless groups (need to be determined from theory or experiments) ä guides experimental work using small models to study large prototypes ä enables us to identify the important parameters in a problem ä simplifies our experimental protocol (remember Saph and Schoder!) ä does not tell us the coefficients or powers of the dimensionless groups (need to be determined from theory or experiments) ä guides experimental work using small models to study large prototypes Dimensional analysis: end

Ship’s Resistance: We aren’t done learning yet! FASTSHIPS may well ferry cargo between the U.S. and Europe as soon as the year Thanks to an innovative hull design and high-powered propulsion system, FastShips can sail twice as fast as traditional freighters. As a result, valuable cargo should be able to cross the Atlantic Ocean in 4 days.

Port Model ä A working scale model was used to eliminated danger to boaters from the "keeper roller" downstream from the diversion structure

Hoover Dam Spillway A 1:60 scale hydraulic model of the tunnel spillway at Hoover Dam for investigation of cavitation damage preventing air slots.

Irrigation Canal Controls

Spillways Frenchman Dam and spillway (in use). Lahontan Region (6)

Dams Dec 01, 1974 Cedar Springs Dam, spillway & Reservoir Santa Ana Region (8)

Spillway Mar 01, 1971 Cedar Springs Spillway construction. Santa Ana Region (8)

Kinematic Viscosity 1.00E E E E E-03 mercury carbon tetrachloride water ethyl alcohol kerosene air sae 10W SAE 10W-30 SAE 30 glycerine kinematic viscosity 20C (m 2 /s)

Kinematic Viscosity of Water 0.0E E E E E Temperature (C) Kinematic Viscosity (m 2 /s)