Lecture 1 Ramiro Neves, 1397

Slides:



Advertisements
Similar presentations
Lecture 2 Properties of Fluids Units and Dimensions 1.
Advertisements

Aula Teórica 1&2 Ramiro Neves, 1397
Lecture 2 Properties of Fluids Units and Dimensions.
Ch 24 pages Lecture 8 – Viscosity of Macromolecular Solutions.
Continuity Equation. Continuity Equation Continuity Equation Net outflow in x direction.
Equations of Continuity
Continuum Mechanics General Principles M. Ali Etaati Eindhoven University of Technology Math. & Computer Science Dept. CASA Apr
Introduction. Outline Fluid Mechanics in Chemical and Petroleum Engineering Normal Stresses (Tensile and Compressive) Shear stress General Concepts of.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 6 FLUID KINETMATICS.
California State University, Chico
Momentum flux across the sea surface
1 MFGT 242: Flow Analysis Chapter 4: Governing Equations for Fluid Flow Professor Joe Greene CSU, CHICO.
1 MFGT 242: Flow Analysis Chapter 3: Stress and Strain in Fluid Mechanics Professor Joe Greene CSU, CHICO.
Fluid Properties and Units CVEN 311 . Continuum ä All materials, solid or fluid, are composed of molecules discretely spread and in continuous motion.
ENG. SAMRA ESSALAIMEH PHILADELPHIA UNIVERSITY 2 ND SEMESTER Thermo-Fluid.
Lecture of : the Reynolds equations of turbulent motions JORDANIAN GERMAN WINTER ACCADMEY Prepared by: Eng. Mohammad Hamasha Jordan University of Science.
Numerical Hydraulics Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa Lecture 1: The equations.
Fluid mechanics 3.1 – key points
Viscosity. Average Speed The Maxwell-Boltzmann distribution is a function of the particle speed. The average speed follows from integration.  Spherical.
Flow and Thermal Considerations
CEE 262A H YDRODYNAMICS Lecture 1* Introduction and properties of fluids *Adapted from notes by Prof. Stephen Monismith 1.
FLUID MECHANICS.
ME 231 Thermofluid Mechanics I Navier-Stokes Equations.
CEE 262A H YDRODYNAMICS Lecture 5 Conservation Laws Part I 1.
Chapter 9: Differential Analysis of Fluid Flow SCHOOL OF BIOPROCESS ENGINEERING, UNIVERSITI MALAYSIA PERLIS.
INTRODUCTION TO CONDUCTION
MAE 3130: Fluid Mechanics Lecture 5: Fluid Kinematics Spring 2003
ME 254. Chapter I Integral Relations for a Control Volume An engineering science like fluid dynamics rests on foundations comprising both theory and experiment.
KINEMATICS Kinematics describes fluid flow without analyzing the forces responsibly for flow generation. Thereby it doesn’t matter what kind of liquid.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Reynolds Transport Theorem We need to relate time derivative of a property of a system to rate of change of that property within a certain region (C.V.)
Pressure distribution in a fluid Pressure and pressure gradient Lecture 4 Mecânica de Fluidos Ambiental 2015/2016.
FLUID PROPERTIES Independent variables SCALARS VECTORS TENSORS.
Fluids. Introduction The 3 most common states of matter are: –Solid: fixed shape and size (fixed volume) –Liquid: takes the shape of the container and.
Mechanics of Fluids I.GNANASEELAN lecturer, department of mechanical Engineering, Parisutham institute of technology and science.
Vectors n v What is the projection of the vector (1, 3, 2) onto the plane described by ? Louisiana Tech University Ruston, LA
Chapter 1 INTRODUCTION AND OVERVIEW
Ch 4 Fluids in Motion.
Ocean Dynamics Previous Lectures So far we have discussed the equations of motion ignoring the role of friction In order to understand ocean circulations.
MAE 5360: Hypersonic Airbreathing Engines
The Meaning of Einstein’s Equation*
Introduction to Fluid Mechanics
Introduction to Fluid Mechanics
CP502 Advanced Fluid Mechanics
Integral budgets: mass and momentum Lecture 7 Mecânica de Fluidos Ambiental 2015/2016.
LECTURE №1 2014/ Introduction to Fluid Mechanics The Fluid mechanics The Fluid mechanics is a part of mechanics, that studies the states of motion.
CP502 Advanced Fluid Mechanics
Basic concepts of heat transfer
Fluid Mechanics-I Spring 2010 Lecture # Course Outline  Introduction to Fluids and Fluid Properties  Fluid Statics  Integral Relations for fluid.
Unit 61: Engineering Thermodynamics Lesson 1: Setting the Scene for the Course.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
05:53 Fluid Mechanics Basic Concepts.
Chapter 1: Basic Concepts
Subject Name: FLUID MECHANICS Subject Code:10ME36B Prepared By: R Punith Department: Aeronautical Engineering Date:
FLUID MECHANICS.
Ramiro Neves Ext 1397, tel Catchment Modelling Ramiro Neves Ext 1397, tel
Chapter 4 Fluid Mechanics Frank White
Continuum Mechanics (MTH487)
Chapter 9: Differential Analysis of Fluid Flow
Today’s Lecture Objectives:
Introduction to Fluid Mechanics
UNIT - 4 HEAT TRANSFER.
Lecture – 1 Ms. Thevasha Sathiyakumar
Advection – Diffusion Equation
Continuum Mechanics for Hillslopes: Part IV
Today’s Lecture Objectives:
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Convective Heat Transfer
Marine Hydrodynamics Lecture – 01
Basic concepts of heat transfer: Heat Conduction
Presentation transcript:

Lecture 1 Ramiro Neves,

Teachers Ramiro Neves, ext. 1397, telem – Lígia Pinto Offices: Pavilhão de Mecânica I, 1º floor

Where to use Fluid Mechanics? About everywhere...

Thessaloniki NATO ARW (19-24 April 2005) Boussinesq Model Douro Estuary mouth: West and SW Waves

Dia mundial da água, Cascais, D Overland flow Precipitation variable in time & space 3D Porous Media 1D Drainage network Integrated Basin Modelling

Integrated Basin Modeling Rain Intensity Flow Production: ●2 Different Soils ●Infiltration ●Overland Flow

Dia mundial da água, Cascais, 2007 Integrated Basin Modeling Rain Intensity Sediment transport: ●2 Catchments ●1 Reservoir

Classical Problems

Reduction of air resistance

Flow in a artery Flow around a leaf

Balloon fish Low mobility high toxicity....

Even the bacteria know the importance of fluids mechanics

Difficulties? The formalism...

Difficulties are apparent because: Fluid Mechanics requires a limited number of physical concepts; Mathematical operators are mostly derivatives, gradients and divergences; This course is an excellent opportunity to consolidate basic concepts of Engineering Sciences

Set of courses downstream MFA Transferência de Energia e Massa Hidráulica Ambiental Hidrologia Ambiental e Recursos Hídricos Física da Atmosfera e do Oceano Ecologia.... Modelação Ambiental Gestão Integrada de Bacias Hidrográficas

Requirements Physics: Forces, Newton law and acceleration, kinetic energy, momentum, fluxes. Mathematics: derivative, integral, divergence, gradient, vector internal and external products.

Knowledge to acquire Understanding of fluid mechanics equations and processes that determine the fluid motion Control of the advection and diffusion concepts and of the evolution equation concept essential for the downstream courses

MFA practical part A computational component is added to the classical exercises with 3 objectives: –To show that Fluid Mechanics goes much beyond simple analytical solutions; –To help students to enhance their programing skills; –To replace the classical laboratory lectures (essential before computational methods were available) This component will be consolidated with a group home work programmed using (preferentially) VBA – VBA is part of the MS Office, is object oriented and useful for a wide range of engineering issues (database, internet...).

Bibliography Fluid Mechanics, Frank White, McGraw-Hill, (or any other Fluid Mechanics Introduction book) Apontamentos de Mecânica dos Fluidos I (Mecânica) Texts about specific subjects Lectures’ PP T

Students Knowledge Assessment Tests/Exam (75%) Computational exercise report (25%) Exams: (14 and 31 January 2015)

What is a fluid? Is formed by molecules... –that move, as in any other type of matter, above 0 kelvin; –the difference between a fluid and a solid is that in the fluid the molecules can change their relative positions allowing them to get the shape of the containers; –fluids can be liquids or gases. In gases molecules have free relative movement In liquids molecules form groups with relative free movement (allowing them to get the shape of the container) which dimension depends on temperature (influencing their viscosity)

Why is Fluid Mechanics distinct from Solid Mechanics? In a fluid each molecule (or group of molecules) have relative movement freedom and in solids not. The consequence is that tangential stress deforms the fluids. Or in other words, if there is tangential stress there is movement. Normal stress compress the fluid, that can remain at rest. Tangential shear moves the fluid in layers creating velocity gradients. Shear is proportional to the rate of deformation

Elementary Volume Is large enough to include a large number of molecules and small enough to have uniform properties. If the Elementary volume is of the order of the size of a molecule, the density value is uncertain due to the number of molecules it contains. If it is too large the density can change from one region to another.

Continuum Hypothesis The elementary volume is much larger than 10 nm Necessary because we cannot assess the movement of individual molecules (too many and the Heisenberg principle) But they move individually.... –The unknown molecule movement will be dealt as diffusion in the equations. When do we have velocity in a fluid? –When there is net mass transport across a surface.

What is the velocity? Velocity is the flux of volume per unit of area. The Velocity is defined at a point and thus is the flow per unit of area, when the area tends to zero: A surface can have 3 orientations in a tridimensional space and thus velocity can have up to 3 components. The velocity component in one direction is the internal product of the velocity vector by the unitary vector along that direction. Using the surface normal one can write :

Discharge / Advective Flux Knowing the 3 velocity components and knowing that the velocity is the discharge per unit of area when the area tends to zero ( the velocity is defined at a point) we can compute the discharge across an area integrating the velocity along the whole area: Defining a specific property as its value per unit of volume (when the volume tends to zero) And the flux of M across a surface is: We can say that the flux of M across an elementary surface is: If c is uniform along the surface then:

Summary We know what is fluid Mechanics and what is for; We know what is a fluid; We know what is velocity and the advective flux; We know that Fluid Mechanics aims to study flows and thus to know the velocity distributions; To compute fluxes we also need to know specific properties distributions….