Prediction of Oil-Water Two Phase Flow Pressure Drop by Using Homogeneous Model

Size: px
Start display at page:

Download "Prediction of Oil-Water Two Phase Flow Pressure Drop by Using Homogeneous Model"

Transcription

1 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 Prediction of Oil-Water Two Pase Flow Pressure Drop by Using Nay Zar Aung a, Triyogi Yuwono b a Department of Mecanical Engineering, Institute Tecnology Sepulu Nopember b Department of Mecanical Engineering, Institute Tecnology Sepulu Nopember Abstract Pressure drop in oil-water two-pase flow in a 8 mm diameter steel pipe were predicted by using omogeneous model. Predictions of friction pressure drop and total pressure drop were made at upward inclinations +5, +0, downward inclinations -5. Te mixture velocity was varied from 0.7 m/s to.5 m/s and oil volumetric concentration was between 0% and 90%. Te data resulted form predictions were compared wit experimental data of Angeli (006). Te results sowed tat omogeneous model gives acceptable predictions for total pressure drop at low oil concentration (< 0.4). Homogeneous model gives overestimates for frictional pressure drop. Keyword: Pressure drop, Oil-water two pase flow, Homogeneous model. Introduction Two-pase liquid-liquid flows are very common in te oil and cemical process industries. In te oil industry, in particular, oil and water are often produced and transported togeter in pipelines tat ave various degrees of inclination from te orizontal or vertical. Te knowledge of pressure drop in a twopase flow system is very important for piping design. It enables te designer to size te pump required for te operation of te flow system. Many of empirical correlations ave been proposed for prediction for gas liquid flows some of wic ave been adapted to predict gas water flow or gas-oil flow. In te area of oil industries, liquid-liquid (oil-water) flows are also encountered and many of researc ave been done on oilwater flow and gas-oil-water tree pase flow. However, sometimes problems of test facilities difficulties are still encountered and it takes a long time to get te results. Moreover, modern CFD softwares are also comparatively as expensive as experiments. For two liquids flow wit nearly te same densities, te assumption of combined liquid pases as a single entity (omogeneous fluids) is very reasonable and te assumption makes teory become simple to predict te ydrodynamic penomena and gives acceptable prediction. Spedding (006) tried to use Lockart Martinelli correlation, Dukler Wicks Cleveland correlation, Beggs Brill correlation, etc., to predict te pressure drop in gas oil two-pase flow and gaswater-oil tree-pase flow. Te objective of tis present work is to predict te pressure drop in oil-water two pase by using omogeneous model and to validate wit experimental data of oil-water flow Angeli (006).. In te omogeneous model, te fluids are caracterized by an effective fluid tat as suitably averaged properties of te two pases in te pipe. It is also known as No-Slip Model. It is assumed tat tere is no velocity difference between te pases and te two fluids flow at te same velocity. By assuming no eat and mass transfer, for omogeneous model te pressure gradient can be written as te sum of tree pressure gradient components due to friction, gravity, and acceleration, dp dx total = f ρ U m d US USL + ρgsin( θ) + ρ + ρl D dx α α L () ρ = α ρ + α LρL () μ = α μ + α μ () L L

2 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 f 9.5 = 4log (k / D + ) (4) Re f Re Dρ U μ = m (5) U S α = β = (6) U m U m =U S +U SL (7) Normally, contribution of momentum pressure drop is very small. To simplify te teory in analytical predictions, momentum pressure drop in Equation () will be neglected.. Metodology of Prediction Prediction of pressure drop wit omogeneous model was implemented by using a MATLAB UI (called HOMO). Te UI (rapical User Interface) was created in MATLAB 7. based on te equations of omogeneous model mentioned above. It is sown in Figure. Tere are nine input data for prediction of pressure drop. Te results data will be produced in te results box and also simulated as a grapic. Te required input data are sown in Table. Table. Te required input data for prediction of pressure drop Input Data Pipe Diameter (m) 6 Density of water (kg/m ) Mixture velocity (m/s) 7 Density of oil (kg/m ) Oil concentration 8 Pipe inclination (Degree) 4 Absolute viscosity of water (N-s/m ) 9 Pipe surface rougness (m) 5 Absolute viscosity of oil (N-s/m ) rapic Result box Input data Figure. A MATLAB UI for predicting oil water flow pressure drop

3 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008. Properties of Liquids in Prediction of Pressure Drop In prediction of pressure drop, te liquids used are Oil Exxsol D40 (Exxon Cemicals) and water. Te properties of fluids used in Angeli s experiments are also used for prediction and summarized in Table. Pipe ydraulic surface rougness for steel pipe was mm. Table. Properties of liquids at 5 C Liquid Oil Exxsol D40 (Exxon Cemicals) Water Density (kg/m ) Viscosity (Ns/m ) Surface Tension (N/m) Results and Discussion Te predicted frictional and total pressure drops from omogeneous model are sown in te following tables by comparing wit Angeli s experimental data. Predicted total pressure gradient sowed a good agreement wit experimental data, owever frictional pressure gradients over estimation. At low oil concentration, omogeneous model gives nearly exact solution because at low concentration, oil bubble dispersed in te water as omogeneous flow. Figure. Example of UI for prediction of pressure gradient wit omogeneous model Inclination At +0 inclination, total pressure gradient from omogeneous model as a good agreement wit experimental data. At low mixture velocities (0.7 m/s, m/s,.5 m/s), omogeneous model sowed acceptable accuracy in prediction for total pressure drop. Frictional pressure drop from experiments sowed tat tere is flow pattern affect at medium range of oil concentration. At upward inclination frictional pressure drop are decreasing at medium range of oil concentration and increased again at iger oil concentration.

4 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 Table.Total and frictional pressure gradient at +0 pipe inclination [Prediction Data] Oil Mixture Velocity (m/s) volume Input (%) Total and frictional pressure gradient (kpa/m) ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f Table 4.Total and frictional pressure gradient at +0 pipe inclination [] Inclination Results at -5 inclination are sown in Table 5 and 6 for frictional and total pressure gradient. From experimental data, it can be seen tat downward and upward as te same trend in frictional pressure drop. For downward inclination omogeneous model give overestimations. At mixture velocity.5 m/s, omogenous models started to give positive values for total pressure drop at oil concentration 0.6. But experimental data sowed negative values of total pressure drop at all te range of oil concentration. 4

5 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 Table 5. Total and frictional pressure gradient at -5 pipe inclination [Prediction Data] Oil Mixture Velocity (m/s) volume Input (%) Total and frictional pressure gradient (kpa/m) ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f Table 6. Total and frictional pressure gradient at -5 pipe inclination [] 5

6 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November Inclination For +5 inclination comparison of predicted frictional pressure drop and experimental data at mixture velocities of m/s and m/s are sown in Figure and 4. At m/s te predicted frictional pressure drop approaced to experimental data. But for m/s te experimental frictional pressure drop is decreasing wit oil concentration and predicted frictional pressure drop is sligtly increasing wit oil concentration. Table 7. Total and frictional pressure gradient at +5 pipe inclination [Prediction Data] Oil Mixture Velocity (m/s) volume Input (%) Total and frictional pressure gradient (kpa/m) ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f ΔP t ΔP f Frictional Pressure Drop (kpa/m) Oil Volume Fraction Figure. Comparison of predicted frictional pressure gradient and experimental data, U mix = m/s, + 5 6

7 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November Frictional Pressure Drop (kpa/m) Oil Volume Fraction Figure 4. Comparison of predicted frictional pressure gradient and experimental data, U mix = m/s, Comparison of Pressure Drop at Low Oil Concentration At +0 pipe inclination, total pressure gradient from omogenous model and experimental data were compared for low oil concentration range of 0.~0.4. It can be seen tat omogeneous give an accurate predictions at low mixture velocity (0.7 m/s and m/s). It is obvious pressure drop start to be affected by flow pattern at iger mixture velocities. However predictions wit omogeneous model are still acceptable for low concentration (< 40 %) as sown in following Figures.5~9..5 Total Pressure radient Vs Total Pressure radient kpa/m Figure 5. Comparison of predicted total pressure gradient wit experimental data ( U mix =0.7 m/s), +0 inclination 7

8 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November Total Pressure radient Vs.5 Total Pressure radient Vs Total Pressure radient kpa/m.5 Total Pressure radient kpa/m Figure 6. Comparison of predicted total pressure gradient wit experimental data ( U mix = m/s) Figure 7. Comparison of predicted total pressure gradient wit experimental data ( U mix =.5 m/s) 4.5 Total Pressure radient Vs Total Pressure radient Vs Total Pressure radient kpa/m.5 Total Pressure radient kpa/m Figure 8. Comparison of predicted total pressure gradient wit experimental data ( U mix = m/s) 5. Conclusion Figure 9. Comparison of predicted total pressure gradient wit experimental data ( U mix =.5 m/s) Frictional and total pressure drop in oil-water flow were predicted by using omogeneous model at upward and downward inclination. At bot upward and downward inclination, omogeneous model gives acceptable prediction for total pressure drop for low oil concentration (<0.4). For frictional pressure drop, omogeneous model gives overestimated values. However omogeneous model is recommend for bubbly flow or dispersed pase fraction < 0.4.Homogeneous model will gives a good prediction if density ρ ratio, L < 0 or total mass flux () > 000 kg/m s. ρ 8

9 FUNDAMENTAL DAN APLIKASI TEKNIK KIMIA 008 Surabaya, 5 November 008 Nomenclature D Pipe Diameter (m) f Fanning friction factor k Hydraulic pipe rougness (m) P Pressure (N/m ) Mass flux (kg/m s) U Velocity (m/s) reek letters Subscripts α Pase oldup β Liquid content ρ Density (kg/m ) σ Surface Tension (N/m) μ Viscosity (Ns/m) θ Inclination angle (degree) f L S t friction gas omogeneous liquid superficial total 6. References. Angeli. P, 006, Upward and downward inclination oil water flows, International Journal of Multipase Flow (006) Crowe C.T, 006, Hand Book of Multipase flow, Wasington State University. Jassim. E.W, 005, Prediction of two-pase pressure drop and void fraction in microcannels using probabilistic flow regime mapping, International Journal of Heat and Mass Transfer 49 (006) , Multipase Flow Production Model (Teory and User s Manual), Maurer Engineering Inc, 96 West T.C. Jester Houston, Texas 5. Rodriguez. O.M.H., 005, Experimental study on oil water flow in orizontal a. and sligtly inclined pipes, International Journal of Multipase Flow (006) 4 6. Spedding, P.L., 006, Prediction of pressure drop in multipase orizontal pipe flow, International Communications in Heat and Mass Transfer (006) 05 06, 9

Prediction of Coating Thickness

Prediction of Coating Thickness Prediction of Coating Tickness Jon D. Wind Surface Penomena CE 385M 4 May 1 Introduction Tis project involves te modeling of te coating of metal plates wit a viscous liquid by pulling te plate vertically

More information

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION INTRODUCTION DEFINITION OF FLUID plate solid F at t = 0 t > 0 = F/A plate U p F fluid t 0 t 1 t 2 t 3 FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY O SASKATCHEWAN Department of Pysics and Engineering Pysics Pysics 117.3 MIDTERM EXAM Regular Sitting NAME: (Last) Please Print (Given) Time: 90 minutes STUDENT NO.: LECTURE SECTION (please ceck):

More information

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E.

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E. CFD calculation of convective eat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E. Publised in: IEA Annex 41 working meeting, Kyoto, Japan Publised:

More information

Study of Convective Heat Transfer through Micro Channels with Different Configurations

Study of Convective Heat Transfer through Micro Channels with Different Configurations International Journal of Current Engineering and Tecnology E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rigts Reserved Available at ttp://inpressco.com/category/ijcet Researc Article Study of

More information

Theoretical Analysis of Flow Characteristics and Bearing Load for Mass-produced External Gear Pump

Theoretical Analysis of Flow Characteristics and Bearing Load for Mass-produced External Gear Pump TECHNICAL PAPE Teoretical Analysis of Flow Caracteristics and Bearing Load for Mass-produced External Gear Pump N. YOSHIDA Tis paper presents teoretical equations for calculating pump flow rate and bearing

More information

Part 2: Introduction to Open-Channel Flow SPRING 2005

Part 2: Introduction to Open-Channel Flow SPRING 2005 Part : Introduction to Open-Cannel Flow SPRING 005. Te Froude number. Total ead and specific energy 3. Hydraulic jump. Te Froude Number Te main caracteristics of flows in open cannels are tat: tere is

More information

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow. Annex 41 Kyoto, April 3 rd to 5 th, 2006

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow. Annex 41 Kyoto, April 3 rd to 5 th, 2006 CFD calculation of convective eat transfer coefficients and validation Part I: Laminar flow Annex 41 Kyoto, April 3 rd to 5 t, 2006 Adam Neale 1, Dominique Derome 1, Bert Blocken 2 and Jan Carmeliet 2,3

More information

Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Exchanger using Tangential Entry of Fluid

Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Exchanger using Tangential Entry of Fluid ISR Journal of Mecanical & Civil Engineering (ISRJMCE) e-issn: 2278-1684,p-ISSN: 2320-334X PP 29-34 www.iosrjournals.org Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Excanger

More information

Investigation of slug flow characteristics in inclined pipelines

Investigation of slug flow characteristics in inclined pipelines Computational Methods in Multiphase Flow IV 185 Investigation of slug flow characteristics in inclined pipelines J. N. E. Carneiro & A. O. Nieckele Department of Mechanical Engineering Pontifícia Universidade

More information

WORKBOOK FOR CHEMICAL REACTOR RELIEF SYSTEM SIZING ANNEX 10 NOMENCLATURE A cross-sectional flow area of relief system (m 2 ) A actual actual cross-sectional area of safety valve nozzle (m 2 ) A approx

More information

DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC) SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN

DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC) SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN DYNAMIC MODELING OF ORGANIC RANKINE CYCLE (ORC SYSTEM FOR FAULT DIAGNOSIS AND CONTROL SYSTEM DESIGN Sungjin Coi and Susan Krumdieck University of Canterbury, Private Bag 48, Cristcurc 84 New Zealand sungjin.coi@pg.canterbury.ac.nz

More information

The Basics of Vacuum Technology

The Basics of Vacuum Technology Te Basics of Vacuum Tecnology Grolik Benno, Kopp Joacim January 2, 2003 Basics Many scientific and industrial processes are so sensitive tat is is necessary to omit te disturbing influence of air. For

More information

Two-Phase Flow Regimes Identification using Artificial Neural Network with Nonlinear Normalization

Two-Phase Flow Regimes Identification using Artificial Neural Network with Nonlinear Normalization Proceedings of the nd International Conference on Fluid Flow, Heat and Mass Transfer Ottawa, Ontario, Canada, April 3 May, 5 Paper No. 33 Two-Phase Flow Regimes Identification using Artificial Neural Network

More information

Distribution of reynolds shear stress in steady and unsteady flows

Distribution of reynolds shear stress in steady and unsteady flows University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 13 Distribution of reynolds sear stress in steady

More information

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator Simulation and verification of a plate eat excanger wit a built-in tap water accumulator Anders Eriksson Abstract In order to test and verify a compact brazed eat excanger (CBE wit a built-in accumulation

More information

Hydraulic validation of the LHC cold mass heat exchanger tube.

Hydraulic validation of the LHC cold mass heat exchanger tube. Hydraulic validation o te LHC cold mass eat excanger tube. LHC Project Note 155 1998-07-22 (pilippe.provenaz@cern.c) Pilippe PROVENAZ / LHC-ACR Division Summary Te knowledge o te elium mass low vs. te

More information

Grade: 11 International Physics Olympiad Qualifier Set: 2

Grade: 11 International Physics Olympiad Qualifier Set: 2 Grade: 11 International Pysics Olympiad Qualifier Set: 2 --------------------------------------------------------------------------------------------------------------- Max Marks: 60 Test ID: 12111 Time

More information

7.8 Transient motion in a two-layered sea

7.8 Transient motion in a two-layered sea 1 Lecture Notes on Fluid Dynamics (1.63J/2.21J by Ciang C. Mei, 2002 7-8-2layer.tex Refs: Csandy: Circulation in te Coastal Ocean Cusman-Rosin, Intro to Geopysical Fluid Dynamics 7.8 Transient motion in

More information

Large eddy simulation of turbulent flow downstream of a backward-facing step

Large eddy simulation of turbulent flow downstream of a backward-facing step Available online at www.sciencedirect.com Procedia Engineering 31 (01) 16 International Conference on Advances in Computational Modeling and Simulation Large eddy simulation of turbulent flow downstream

More information

Comment on Experimental observations of saltwater up-coning

Comment on Experimental observations of saltwater up-coning 1 Comment on Experimental observations of saltwater up-coning H. Zang 1,, D.A. Barry 2 and G.C. Hocking 3 1 Griffit Scool of Engineering, Griffit University, Gold Coast Campus, QLD 4222, Australia. Tel.:

More information

Mechanical Engineering Programme of Study

Mechanical Engineering Programme of Study Mechanical Engineering Programme of Study Fluid Mechanics Instructor: Marios M. Fyrillas Email: eng.fm@fit.ac.cy SOLVED EXAMPLES ON VISCOUS FLOW 1. Consider steady, laminar flow between two fixed parallel

More information

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine?

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine? 1 1 Power is transferred troug a macine as sown. power input P I macine power output P O power loss P L Wat is te efficiency of te macine? P I P L P P P O + P L I O P L P O P I 2 ir in a bicycle pump is

More information

Phase space in classical physics

Phase space in classical physics Pase space in classical pysics Quantum mecanically, we can actually COU te number of microstates consistent wit a given macrostate, specified (for example) by te total energy. In general, eac microstate

More information

A = h w (1) Error Analysis Physics 141

A = h w (1) Error Analysis Physics 141 Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.

More information

Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates with Ramped Wall Temperature

Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates with Ramped Wall Temperature Volume 39 No. February 01 Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates wit Ramped Wall Temperature S. Das Department of Matematics University of Gour Banga Malda 73

More information

A Modified Distributed Lagrange Multiplier/Fictitious Domain Method for Particulate Flows with Collisions

A Modified Distributed Lagrange Multiplier/Fictitious Domain Method for Particulate Flows with Collisions A Modified Distributed Lagrange Multiplier/Fictitious Domain Metod for Particulate Flows wit Collisions P. Sing Department of Mecanical Engineering New Jersey Institute of Tecnology University Heigts Newark,

More information

Seepage Analysis through Earth Dam Based on Finite Difference Method

Seepage Analysis through Earth Dam Based on Finite Difference Method J. Basic. Appl. Sci. Res., (11)111-1, 1 1, TetRoad Publication ISSN -44 Journal of Basic and Applied Scientific Researc www.tetroad.com Seepage Analysis troug Eart Dam Based on Finite Difference Metod

More information

Order of Accuracy. ũ h u Ch p, (1)

Order of Accuracy. ũ h u Ch p, (1) Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical

More information

Piping Systems and Flow Analysis (Chapter 3)

Piping Systems and Flow Analysis (Chapter 3) Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution

More information

Wind Turbine Micrositing: Comparison of Finite Difference Method and Computational Fluid Dynamics

Wind Turbine Micrositing: Comparison of Finite Difference Method and Computational Fluid Dynamics IJCSI International Journal of Computer Science Issues, Vol. 9, Issue 1, No 1, January 01 ISSN (Online): 169-081 www.ijcsi.org 7 Wind Turbine Micrositing: Comparison of Finite Difference Metod and Computational

More information

INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW

INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW Daniel Merino Gabriel S. Bassani, Luiz Eduardo A. P. Duarte Deibi E. Garcia Angela O. Nieckele Two-phase Flow

More information

HT TURBULENT NATURAL CONVECTION IN A DIFFERENTIALLY HEATED VERTICAL CHANNEL. Proceedings of 2008 ASME Summer Heat Transfer Conference HT2008

HT TURBULENT NATURAL CONVECTION IN A DIFFERENTIALLY HEATED VERTICAL CHANNEL. Proceedings of 2008 ASME Summer Heat Transfer Conference HT2008 Proceedings of 2008 ASME Summer Heat Transfer Conference HT2008 August 10-14, 2008, Jacksonville, Florida USA Proceedings of HT2008 2008 ASME Summer Heat Transfer Conference August 10-14, 2008, Jacksonville,

More information

10.1 VIBRATIONAL RELAXATION *

10.1 VIBRATIONAL RELAXATION * Andrei Tokmakoff, MIT Department of Cemistry, 3//009 p. 0-0. VIRATIONAL RELAXATION * Here we want to address ow a quantum mecanical vibration undergoes irreversible energy dissipation as a result of interactions

More information

Work and Energy. Introduction. Work. PHY energy - J. Hedberg

Work and Energy. Introduction. Work. PHY energy - J. Hedberg Work and Energy PHY 207 - energy - J. Hedberg - 2017 1. Introduction 2. Work 3. Kinetic Energy 4. Potential Energy 5. Conservation of Mecanical Energy 6. Ex: Te Loop te Loop 7. Conservative and Non-conservative

More information

Development and experimental verification of a numerical model for optimizing the cleaning performance of the doctor blade press roll tribosystem

Development and experimental verification of a numerical model for optimizing the cleaning performance of the doctor blade press roll tribosystem Development and experimental verification of a numerical model for optimizing te cleaning performance of te doctor blade press roll tribosystem M. Rodríguez Ripoll, B. Sceicl,, D. Bianci, B. Jakab, F.

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

2. Temperature, Pressure, Wind, and Minor Constituents.

2. Temperature, Pressure, Wind, and Minor Constituents. 2. Temperature, Pressure, Wind, and Minor Constituents. 2. Distributions of temperature, pressure and wind. Close examination of Figs..7-.0 of MS reveals te following features tat cry out for explanation:

More information

Homework Assignment on Fluid Statics

Homework Assignment on Fluid Statics AMEE 0 Introduction to Fluid Mecanics Instructor: Marios M. Fyrillas Email: m.fyrillas@fit.ac.cy Homework Assignment on Fluid Statics --------------------------------------------------------------------------------------------------------------

More information

Velocity distribution in non-uniform/unsteady flows and the validity of log law

Velocity distribution in non-uniform/unsteady flows and the validity of log law University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 3 Velocity distribution in non-uniform/unsteady

More information

Mechanistic Modeling of Upward Gas-Liquid Flow in Deviated Wells

Mechanistic Modeling of Upward Gas-Liquid Flow in Deviated Wells Advances in Petroleum Exploration and Development Vol. 9, No., 015, pp. 53-57 DOI:10.3968/6659 ISSN 195-54X [Print] ISSN 195-5438 [Online] www.cscanada.net www.cscanada.org SUN Shihui [a],* ; YAN Tie [a]

More information

Conference paper: Analytical Investigation by Using the Two-fluid-model to Study the Interfacial Behavior of Air-water Horizontal Stratified Flow

Conference paper: Analytical Investigation by Using the Two-fluid-model to Study the Interfacial Behavior of Air-water Horizontal Stratified Flow Conference paper: Analytical Investigation by Using the Two-fluid-model to Study the Interfacial Behavior of Air-water Horizontal Stratified Flow Authors: Hadiyan Yusuf Kuntoro; Deendarlianto; Indarto

More information

Fundamentals of Heat Transfer Muhammad Rashid Usman

Fundamentals of Heat Transfer Muhammad Rashid Usman Fundamentals of Heat Transfer Muammad Rasid Usman Institute of Cemical Engineering and Tecnology University of te Punjab, Laore. Figure taken from: ttp://eatexcanger-design.com/20/0/06/eat-excangers-6/

More information

PIPE FLOWS: LECTURE /04/2017. Yesterday, for the example problem Δp = f(v, ρ, μ, L, D) We came up with the non dimensional relation

PIPE FLOWS: LECTURE /04/2017. Yesterday, for the example problem Δp = f(v, ρ, μ, L, D) We came up with the non dimensional relation /04/07 ECTURE 4 PIPE FOWS: Yesterday, for the example problem Δp = f(v, ρ, μ,, ) We came up with the non dimensional relation f (, ) 3 V or, p f(, ) You can plot π versus π with π 3 as a parameter. Or,

More information

The Verlet Algorithm for Molecular Dynamics Simulations

The Verlet Algorithm for Molecular Dynamics Simulations Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical

More information

Analysis of Static and Dynamic Load on Hydrostatic Bearing with Variable Viscosity and Pressure

Analysis of Static and Dynamic Load on Hydrostatic Bearing with Variable Viscosity and Pressure Indian Journal of Science and Tecnology Supplementary Article Analysis of Static and Dynamic Load on Hydrostatic Bearing wit Variable Viscosity and Pressure V. Srinivasan* Professor, Scool of Mecanical

More information

Desalination by vacuum membrane distillation: sensitivity analysis

Desalination by vacuum membrane distillation: sensitivity analysis Separation and Purification Tecnology 33 (2003) 75/87 www.elsevier.com/locate/seppur Desalination by vacuum membrane distillation: sensitivity analysis Fawzi Banat *, Fami Abu Al-Rub, Kalid Bani-Melem

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information

Continuous formulation for bottom friction in free surface flows modelling

Continuous formulation for bottom friction in free surface flows modelling River Basin Management V 81 Continuous formulation for bottom friction in free surface flows modelling O. Maciels 1, S. Erpicum 1, B. J. Dewals 1, 2, P. Arcambeau 1 & M. Pirotton 1 1 HACH Unit, Department

More information

Figure 3: Problem 7. (a) 0.9 m (b) 1.8 m (c) 2.7 m (d) 3.6 m

Figure 3: Problem 7. (a) 0.9 m (b) 1.8 m (c) 2.7 m (d) 3.6 m 1. For the manometer shown in figure 1, if the absolute pressure at point A is 1.013 10 5 Pa, the absolute pressure at point B is (ρ water =10 3 kg/m 3, ρ Hg =13.56 10 3 kg/m 3, ρ oil = 800kg/m 3 ): (a)

More information

ch-01.qxd 8/4/04 2:33 PM Page 1 Part 1 Basic Principles of Open Channel Flows

ch-01.qxd 8/4/04 2:33 PM Page 1 Part 1 Basic Principles of Open Channel Flows ch-01.qxd 8/4/04 2:33 PM Page 1 Part 1 Basic Principles of Open Channel Flows ch-01.qxd 8/4/04 2:33 PM Page 3 Introduction 1 Summary The introduction chapter reviews briefly the basic fluid properties

More information

3. Gradually-Varied Flow

3. Gradually-Varied Flow 5/6/18 3. Gradually-aried Flow Normal Flow vs Gradually-aried Flow Normal Flow /g EGL (energy grade line) iction slope Geometric slope S Normal flow: Downslope component of weigt balances bed friction

More information

COMPARISON OF FUZZY LOGIC CONTROLLERS FOR A MULTIVARIABLE PROCESS

COMPARISON OF FUZZY LOGIC CONTROLLERS FOR A MULTIVARIABLE PROCESS COMPARISON OF FUZZY LOGIC CONTROLLERS FOR A MULTIVARIABLE PROCESS KARTHICK S, LAKSHMI P, DEEPA T 3 PG Student, DEEE, College of Engineering, Guindy, Anna University, Cennai Associate Professor, DEEE, College

More information

Stability of stratified two-phase channel flows of Newtonian/non-Newtonian shear-thinning fluids

Stability of stratified two-phase channel flows of Newtonian/non-Newtonian shear-thinning fluids Stability of stratified two-pase cannel flows of Newtonian/non-Newtonian sear-tinning fluids D. Picci a), I. Barmak b), A. Ullmann, and N. Brauner Scool of Mecanical Engineering, Tel Aviv University, Tel

More information

The marching velocity of the capillary meniscus in a microchannel

The marching velocity of the capillary meniscus in a microchannel INSTITUTE OFPHYSICS PUBLISHING JOURNAL OFMICROMECHANICS ANDMICROENGINEERING J. Micromec. Microeng. 14 (2004) 220 225 PII: S0960-1317(04)61080-1 Te marcing velocity of te capillary meniscus in a microcannel

More information

A general articulation angle stability model for non-slewing articulated mobile cranes on slopes *

A general articulation angle stability model for non-slewing articulated mobile cranes on slopes * tecnical note 3 general articulation angle stability model for non-slewing articulated mobile cranes on slopes * J Wu, L uzzomi and M Hodkiewicz Scool of Mecanical and Cemical Engineering, University of

More information

Section 3.1: Derivatives of Polynomials and Exponential Functions

Section 3.1: Derivatives of Polynomials and Exponential Functions Section 3.1: Derivatives of Polynomials and Exponential Functions In previous sections we developed te concept of te derivative and derivative function. Te only issue wit our definition owever is tat it

More information

Development of new and validation of existing convection correlations for rooms with displacement ventilation systems

Development of new and validation of existing convection correlations for rooms with displacement ventilation systems Energy and Buildings 38 (2006) 163 173 www.elsevier.com/locate/enbuild Development of new and validation of existing convection correlations for rooms wit displacement ventilation systems Atila Novoselac

More information

Optimization of flat tubular molten salt receivers

Optimization of flat tubular molten salt receivers Optimization of flat tubular molten salt receivers Meige Zeng, Jon Pye Researc Scool of Engineering, Australian National University, Canberra, Australia Abstract E-mail: meige.zeng@anu.edu.au, jon.pye@anu.edu.au

More information

Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline

Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline Journal of Scientific & Industrial Research Vol. 74, March 2015, pp. 180-184 Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline K R Naidu 1, T K Mandal 2 and S K Majumder

More information

Measurement of cement s particle size distribution by the buoyancy weighing-bar method

Measurement of cement s particle size distribution by the buoyancy weighing-bar method Measurement of cement s particle size distribution by te buoyancy weiging-bar metod *Rondang Tambun, Nofriko ratama, Ely, and Farida Hanum Department of Cemical Engineering, Faculty of Engineering, University

More information

S.E. (Mech.) (First Sem.) EXAMINATION, (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum Marks : 100

S.E. (Mech.) (First Sem.) EXAMINATION, (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum Marks : 100 Total No. of Questions 12] [Total No. of Printed Pages 8 Seat No. [4262]-113 S.E. (Mech.) (First Sem.) EXAMINATION, 2012 (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum

More information

AN ANALYSIS OF AMPLITUDE AND PERIOD OF ALTERNATING ICE LOADS ON CONICAL STRUCTURES

AN ANALYSIS OF AMPLITUDE AND PERIOD OF ALTERNATING ICE LOADS ON CONICAL STRUCTURES Ice in te Environment: Proceedings of te 1t IAHR International Symposium on Ice Dunedin, New Zealand, nd t December International Association of Hydraulic Engineering and Researc AN ANALYSIS OF AMPLITUDE

More information

Introduction to Derivatives

Introduction to Derivatives Introduction to Derivatives 5-Minute Review: Instantaneous Rates and Tangent Slope Recall te analogy tat we developed earlier First we saw tat te secant slope of te line troug te two points (a, f (a))

More information

Lecture 10: Carnot theorem

Lecture 10: Carnot theorem ecture 0: Carnot teorem Feb 7, 005 Equivalence of Kelvin and Clausius formulations ast time we learned tat te Second aw can be formulated in two ways. e Kelvin formulation: No process is possible wose

More information

THIN FILM FLOW SIMULATION ON A ROTATING DISC

THIN FILM FLOW SIMULATION ON A ROTATING DISC European Congress on Computational Metods in Applied Sciences and Engineering (ECCOMAS 2012) J. Eberardsteiner et.al. (eds.) Vienna, Austria, September 10-14, 2012 THIN FILM FLOW SIMULATION ON A ROTATING

More information

AN EFFICIENT AND ROBUST METHOD FOR SIMULATING TWO-PHASE GEL DYNAMICS

AN EFFICIENT AND ROBUST METHOD FOR SIMULATING TWO-PHASE GEL DYNAMICS AN EFFICIENT AND ROBUST METHOD FOR SIMULATING TWO-PHASE GEL DYNAMICS GRADY B. WRIGHT, ROBERT D. GUY, AND AARON L. FOGELSON Abstract. We develop a computational metod for simulating models of gel dynamics

More information

Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes

Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes Computational Methods in Multiphase Flow VIII 335 Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes B. Moradi, M. Hossain & G. Oluyemi School of Engineering, Robert

More information

VOLUME AVERAGING OF MULTIPHASE FLOWS WITH HYDRATE FORMATION IN SUBSEA PIPELINES

VOLUME AVERAGING OF MULTIPHASE FLOWS WITH HYDRATE FORMATION IN SUBSEA PIPELINES VOLUME AVERAGING OF MULTIPHASE FLOWS WITH HYDRATE FORMATION IN SUBSEA PIPELINES BY Reza Zeinali Torbati A Thesis submitted to the School of Graduate Studies In partial fulfillment of the requirements for

More information

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln 0. (a) Sol: Section A A refrigerator macine uses R- as te working fluid. Te temperature of R- in te evaporator coil is 5C, and te gas leaves te compressor as dry saturated at a temperature of 40C. Te mean

More information

Determination of heat transfer intensity between free streaming water film and rigid surface using thermography

Determination of heat transfer intensity between free streaming water film and rigid surface using thermography IV Conferencia Panamericana de END Buenos Aires Octubre 2007 Determination of eat transfer intensity between free ing water film and rigid surface using termograpy Ivanka Boras and Srecko Svaic Faculty

More information

Lesson 6 Review of fundamentals: Fluid flow

Lesson 6 Review of fundamentals: Fluid flow Lesson 6 Review of fundamentals: Fluid flow The specific objective of this lesson is to conduct a brief review of the fundamentals of fluid flow and present: A general equation for conservation of mass

More information

De-Coupler Design for an Interacting Tanks System

De-Coupler Design for an Interacting Tanks System IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 7, Issue 3 (Sep. - Oct. 2013), PP 77-81 De-Coupler Design for an Interacting Tanks System

More information

Chapter 6 Pneumatic Transport

Chapter 6 Pneumatic Transport Chapter 6 Pneumatic Transport 6.1 Pneumatic Transport Use of a gas to transport a particulate solid through pipeline Powder Rotary valve Blower Three major variables for pneumatic conveying - solid mass

More information

Proceedings of the ASME nd Micro/Nanoscale Heat & Mass Transfer International Conference MNHMT2009 December 18-21, 2009, Shanghai, China

Proceedings of the ASME nd Micro/Nanoscale Heat & Mass Transfer International Conference MNHMT2009 December 18-21, 2009, Shanghai, China Proceedings of te ASME 009 nd Micro/Nanoscale Heat & Mass Transfer International Conference MNHMT009 December 18-1, 009, Sangai, Cina Superydropobic Friction Reduction Microtextured Surfaces Tae Jin KIM,

More information

Department of Mechanical Engineering, Azarbaijan Shahid Madani University, Tabriz, Iran b

Department of Mechanical Engineering, Azarbaijan Shahid Madani University, Tabriz, Iran b THERMAL SCIENCE, Year 2016, Vol. 20, No. 2, pp. 505-516 505 EXPERIMENTAL INVESTIGATION ON FLOW AND HEAT TRANSFER FOR COOLING FLUSH-MOUNTED RIBBONS IN A CHANNEL Application of an Electroydrodinamics Active

More information

PARTICLE IMAGE VELOCIMETRY MEASUREMENTS OF STRATIFIED GAS-LIQUID FLOW IN HORIZONTAL AND INCLINED PIPES

PARTICLE IMAGE VELOCIMETRY MEASUREMENTS OF STRATIFIED GAS-LIQUID FLOW IN HORIZONTAL AND INCLINED PIPES S. Vestøl, et al., Int. J. Comp. Meth. and Exp. Meas., Vol. 6, No. 2 (2018) 411 422 PARTICLE IMAGE VELOCIMETRY MEASUREMENTS OF STRATIFIED GAS-LIQUID FLOW IN HORIZONTAL AND INCLINED PIPES S. VESTØL, W.A.S.

More information

FINITE ELEMENT STOCHASTIC ANALYSIS

FINITE ELEMENT STOCHASTIC ANALYSIS FINITE ELEMENT STOCHASTIC ANALYSIS Murray Fredlund, P.D., P.Eng., SoilVision Systems Ltd., Saskatoon, SK ABSTRACT Numerical models can be valuable tools in te prediction of seepage. Te results can often

More information

3.1 Extreme Values of a Function

3.1 Extreme Values of a Function .1 Etreme Values of a Function Section.1 Notes Page 1 One application of te derivative is finding minimum and maimum values off a grap. In precalculus we were only able to do tis wit quadratics by find

More information

Carnot Factor of a Vapour Power Cycle with Regenerative Extraction

Carnot Factor of a Vapour Power Cycle with Regenerative Extraction Journal of Modern Pysics, 2017, 8, 1795-1808 ttp://www.scirp.org/journal/jmp ISSN Online: 2153-120X ISSN Print: 2153-1196 arnot Factor of a Vapour Power ycle wit Regenerative Extraction Duparquet Alain

More information

The entransy dissipation minimization principle under given heat duty and heat transfer area conditions

The entransy dissipation minimization principle under given heat duty and heat transfer area conditions Article Engineering Termopysics July 2011 Vol.56 No.19: 2071 2076 doi: 10.1007/s11434-010-4189-x SPECIAL TOPICS: Te entransy dissipation minimization principle under given eat duty and eat transfer area

More information

Fluids and Buoyancy. 1. What will happen to the scale reading as the mass is lowered?

Fluids and Buoyancy. 1. What will happen to the scale reading as the mass is lowered? Fluids and Buoyancy. Wat will appen to te scale reading as te mass is lowered? M Using rcimedes Principle: any body fully or partially submerged in a fluid is buoyed up by a force equal to te weigt of

More information

(4.2) -Richardson Extrapolation

(4.2) -Richardson Extrapolation (.) -Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Suppose tat lim G 0 and lim F L. Te function F is said to converge to L as

More information

Problem Solving. Problem Solving Process

Problem Solving. Problem Solving Process Problem Solving One of te primary tasks for engineers is often solving problems. It is wat tey are, or sould be, good at. Solving engineering problems requires more tan just learning new terms, ideas and

More information

ESTIMATING PRODUCTION AND BOOSTER PUMP LOCATION FOR LONG DISTANCE PUMPING

ESTIMATING PRODUCTION AND BOOSTER PUMP LOCATION FOR LONG DISTANCE PUMPING ESTIMATING PRODUCTION AND BOOSTER PUMP LOCATION FOR LONG DISTANCE PUMPING R.E. Randall, Director Center for Dredging Studies Texas A&M University 1WEDA33/TAMU44 Acknowledgements Co author Po hung Yeh Graduate

More information

Multiphase Flow and Heat Transfer

Multiphase Flow and Heat Transfer Multiphase Flow and Heat Transfer ME546 -Sudheer Siddapureddy sudheer@iitp.ac.in Two Phase Flow Reference: S. Mostafa Ghiaasiaan, Two-Phase Flow, Boiling and Condensation, Cambridge University Press. http://dx.doi.org/10.1017/cbo9780511619410

More information

Teaching Differentiation: A Rare Case for the Problem of the Slope of the Tangent Line

Teaching Differentiation: A Rare Case for the Problem of the Slope of the Tangent Line Teacing Differentiation: A Rare Case for te Problem of te Slope of te Tangent Line arxiv:1805.00343v1 [mat.ho] 29 Apr 2018 Roman Kvasov Department of Matematics University of Puerto Rico at Aguadilla Aguadilla,

More information

FLOW PATTERN AND PRESSURE DROP IN HORIZONTAL VISCOUS OIL-WATER FLOWS

FLOW PATTERN AND PRESSURE DROP IN HORIZONTAL VISCOUS OIL-WATER FLOWS HEFAT2014 10 th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics 14 16 July 2014 Orlando, Florida FLOW PATTERN AND PRESSURE DROP IN HORIZONTAL VISCOUS OIL-WATER FLOWS Castro

More information

ICES REPORT Isogeometric Phase-field Simulation of Boiling

ICES REPORT Isogeometric Phase-field Simulation of Boiling ICES REPORT 15-16 June 015 Isogeometric Pase-field Simulation of Boiling by Ju Liu, Tomas J.R. Huges Te Institute for Computational Engineering and Sciences Te University of Texas at Austin Austin, Texas

More information

CFD Analysis and Optimization of Heat Transfer in Double Pipe Heat Exchanger with Helical-Tap Inserts at Annulus of Inner Pipe

CFD Analysis and Optimization of Heat Transfer in Double Pipe Heat Exchanger with Helical-Tap Inserts at Annulus of Inner Pipe IOR Journal Mecanical and Civil Engineering (IOR-JMCE) e-in: 2278-1684,p-IN: 2320-334X, Volume 13, Issue 3 Ver. VII (May- Jun. 2016), PP 17-22 www.iosrjournals.org CFD Analysis and Optimization Heat Transfer

More information

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2 Pysics 121, April 1, 2008. Pysics 121. April 1, 2008. Course Information Discussion of Exam # 2 Topics to be discussed today: Requirements for Equilibrium Gravitational Equilibrium Sample problems Pysics

More information

Numerical analysis of a free piston problem

Numerical analysis of a free piston problem MATHEMATICAL COMMUNICATIONS 573 Mat. Commun., Vol. 15, No. 2, pp. 573-585 (2010) Numerical analysis of a free piston problem Boris Mua 1 and Zvonimir Tutek 1, 1 Department of Matematics, University of

More information

The Foundations of Chemistry 1

The Foundations of Chemistry 1 Te Foundations of Cemistry 1 1-1 (a) Biocemistry is te study of te cemistry of living tings. (b) Analytical cemistry studies te quantitative and qualitative composition analysis of substances. (c) Geocemistry

More information

Graviton Induced Nuclear Fission through Electromagnetic Wave Flux Phil Russell, * Jerry Montgomery

Graviton Induced Nuclear Fission through Electromagnetic Wave Flux Phil Russell, * Jerry Montgomery Graviton Induced Nuclear Fission troug Electromagnetic Wave Flux Pil Russell, * Jerry Montgomery Nort Carolina Central University, Duram, NC 27707 Willowstick Tecnologies LLC, Draper, UT 84020 (Dated:

More information

Evaluation and Accurate Estimation from Petrophysical Parameters of a Reservoir

Evaluation and Accurate Estimation from Petrophysical Parameters of a Reservoir American Journal of Environmental Engineering and Science 2016; 3(2): 68-74 ttp://www.aascit.org/journal/ajees ISSN: 2381-1153 (Print); ISSN: 2381-1161 (Online) Evaluation and Accurate Estimation from

More information

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 12.

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 12. Capter 6. Fluid Mecanics Notes: Most of te material in tis capter is taken from Young and Freedman, Cap. 12. 6.1 Fluid Statics Fluids, i.e., substances tat can flow, are te subjects of tis capter. But

More information

Falling liquid films: wave patterns and thermocapillary effects

Falling liquid films: wave patterns and thermocapillary effects Falling liquid films: wave patterns and termocapillary effects Benoit Sceid Cimie-Pysique E.P., Université Libre de Bruxelles C.P. 65/6 Avenue F.D. Roosevelt, 50-50 Bruxelles - BELGIUM E-mail: bsceid@ulb.ac.be

More information

Quantum Theory of the Atomic Nucleus

Quantum Theory of the Atomic Nucleus G. Gamow, ZP, 51, 204 1928 Quantum Teory of te tomic Nucleus G. Gamow (Received 1928) It as often been suggested tat non Coulomb attractive forces play a very important role inside atomic nuclei. We can

More information

2.8 The Derivative as a Function

2.8 The Derivative as a Function .8 Te Derivative as a Function Typically, we can find te derivative of a function f at many points of its domain: Definition. Suppose tat f is a function wic is differentiable at every point of an open

More information

Section 15.6 Directional Derivatives and the Gradient Vector

Section 15.6 Directional Derivatives and the Gradient Vector Section 15.6 Directional Derivatives and te Gradient Vector Finding rates of cange in different directions Recall tat wen we first started considering derivatives of functions of more tan one variable,

More information