Lecture 2 Single Phase Flow Concepts

Slides:



Advertisements
Similar presentations
FLOW IN PIPES, PIPE NETWORKS
Advertisements

Chapter Four Fluid Dynamic
Chapter Four Fluid Dynamic
Lecture 15: Capillary motion
Chapter 2 Introduction to Heat Transfer
Physics Part 1 MECHANICS
Chapter 4 Mass and Energy Analysis of Control Volumes (Open Systems)
The Bernoulli Equation - Work and Energy
Momentum Conservation
Two Phase Flow Modeling Prepared by: Tan Nguyen Two Phase Flow Modeling – PE 571 Chapter 3: Slug Flow Modeling Dukler and Hubbard – Horizontal Pipes.
PETE 203 DRILLING ENGINEERING
Chapter 9 Solids and Fluids (c).
Flow of Liquids Through Pipes
California State University, Chico
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 9: FLOWS IN PIPE
1 Lec 26: Frictionless flow with work, pipe flow.
Fluid mechanics 3.1 – key points
CBE 150A – Transport Spring Semester 2014 Friction Losses Flow through Conduits Incompressible Flow.
Unit 3 - FLUID MECHANICS.
Flow Sensors.
Lesson 10 Drilling Hydraulics (cont’d)
Core Ag Engineering Principles – Session 1
PFR design. Accounting for pressure drop Chemical Reaction Engineering I Aug Dec 2011 Dept. Chem. Engg., IIT-Madras.
Hydraulic Routing in Rivers
SURVIVAL MODE Quiz 3 –
PHAROS UNIVERSITY ME 259 FLUID MECHANICS FOR ELECTRICAL STUDENTS Basic Equations for a Control Volume.
Fluid Mechanics and Applications MECN 3110
Chapter 4 – Source Models
Drilling Engineering – PE 311 Turbulent Flow in Pipes and Annuli
Fluid Properties: Liquid or Gas
Measurement of flowing fluids
Pressure drop during fluid flow
Unit: IV-Fluid Dynamic
Chapter Six Non-Newtonian Liquid.
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
Lesson 22 BERNOULLI’S EQUATION
CP502 Advanced Fluid Mechanics
CBE 150A – Transport Spring Semester 2014 Macroscopic Mechanical Energy Balance.
Lesson 23 HEAD LOSS DEFINE the terms head loss, frictional loss, and minor losses. DETERMINE friction factors for various flow situations using the Moody.
Hydraulic Routing in Rivers Reference: HEC-RAS Hydraulic Reference Manual, Version 4.1, Chapters 1 and 2 Reading: HEC-RAS Manual pp. 2-1 to 2-12 Applied.
PIPELINE DESIGN ‘ THE ENGINEERING APPROACH’ SESSION OBJECTIVES THE ENGINEERING EQUATIONS TRANSMISSION LINE GAS FLOW LIQUID SYSTEM.
© Pritchard Introduction to Fluid Mechanics Chapter 8 Internal Incompressible Viscous Flow.
Dr. Jason Roney Mechanical and Aerospace Engineering
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.
ME 101: Fluids Engineering Chapter 6 ME Two Areas for Mechanical Engineers Fluid Statics –Deals with stationary objects Ships, Tanks, Dams –Common.
OC FLOW: ENERGY CONCEPTS, CHANNEL ANALYSIS
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.
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
Friction Losses Flow through Conduits Incompressible Flow.

Pipe flow analysis.
Elementary Mechanics of Fluids CE 319 F Daene McKinney Energy Equation.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
Fundamental (First) Principles of Fluid Mechanics
Major loss in Ducts, Tubes and Pipes
Open Channel Hydraulic
8.2 OBJECTIVES  Describe the appearance of laminar flow and turbulent flow  State the relationship used to compute the Reynolds number  Identify the.
1 Dept. of Agricultural & Biological Engineering University of Illinois TSM 363 Fluid Power Systems TSM 363 Fluid Power Systems Bernoulli’s Law and Applications.
First Law of Thermodynamics applied to Flow processes
Energy Loss in Valves Function of valve type and valve position
ABE 223 ABE Principles – Machine systems Bernoulli’s Law Tony Grift
FRICTION FACTOR A common parameter used in LAMINAR and especially in TURBULENT flow is the Fanning friction factor, f ‘f ’is as the ratio defined of wall.
TEM – Lecture 2 Basic concepts of heat transfer:
Review of ChE Fluid Mechanics
FLUID MECHANICS REVIEW
FLUIDS IN MOTION The equations that follow are applied when a moving fluid exhibits streamline flow. Streamline flow assumes that as each particle in the.
Asst. Prof. Dr. Hayder Mohammad Jaffal
FLUID MECHANICS - Review
8. FLUID FLOW: mechanical energy equation
9. FLUID FLOW: Working Problems
Presentation transcript:

Lecture 2 Single Phase Flow Concepts

Wellbore Performance Wellbore performance analysis involves establishing a relationship between tubular size wellhead and bottom-hole pressure fluid properties fluid production rate

Single-Phase Liquid Flow Single-phase liquid flow exists in an oil well only when the wellhead pressure is above the bubble-point pressure of the oil, which is usually not a reality. This is just a start point. Multiphase flow usually dominates.

Conservation of Momentum The rate of momentum out, minus the rate of momentum in, plus the rate of momentum accumulation in a given pipe segment must equal the sum of all forces on the fluids.

Conservation of Momentum Conservation of mass

Flow to the Surface - Liquids Taken as a macroscopic balance the changes at two selected points can be examined

Conservation of Momentum

Flow to the Surface - Liquids Flow of slightly compressible liquids is described by the steady state mechanical energy balance Steady state means that no properties are changing with time.

Kinetic Energy Term (KE) (acc) The change in kinetic energy is the energy change brought about by a change in velocity between points 1 & 2. For turbulent flow this is expressed as Velocity is related to volumetric throughput or flux by

Potential Energy Term (PE) (el) The change in potential energy is the change brought about by elevation change between point 1 & 2. The flow may be inclined at an angle, or be horizontal.

Friction Frictional energy loss is a function of velocity, viscosity, density, pipe size, & condition. Correlations developed by Moody are widely used to obtain a Fanning friction factor based on Reynolds Number Fanning friction factor Moody friction factor

Moody Friction Factor

Moody Friction Factor

Pipe Roughness

Fanning Friction Factor Many correlations exist. A good one is presented by Chen Fanning friction factor = (1/4) Moody friction factor

Friction in Fittings Friction loss in fittings is negligible in flow though long lines. However it may be important in short distance applications. If so it is added to the friction term as

Friction in Fittings

Mechanical Energy Balance for Liquids Note the condition of no flow. Calc an example.

Example 1 Calculate the pressure change in a water injection well. The following data are known.

Example 2 Suppose that 1,000 bbl/day of 40 API, 1.2 cp oil is being produced through 2 7⁄8-in., 8.6 lbm/ft tubing in a well that is 15 degrees from vertical. If the tubing wall relative roughness is 0.001, calculate the pressure drop over 1,000 ft of tubing.

Liquid Pressure Traverse A pressure traverse is a plot of the flowing pressure versus position in the pipe. For the case of a slightly compressible liquid the plot is a straight line from P1 to P2 across L1 to L2. You can verify this result by breaking the flow length into increments and computing and plotting the end point of each increment.

Production Well Example

Single-Phase Gas Flow The first law of thermodynamics (conservation of energy) governs gas flow in tubing. The effect of kinetic energy change is negligible because the variation in tubing diameter is insignificant in most gas wells. With no shaft work device installed along the tubing string, the first law of thermodynamics yields the following mechanical balance equation:

Single-Phase Gas Flow Since dz is Sin(θ).dL The gas density from the gas law can be expressed as The velocity can be written in terms of volumetric flow rate at the standard condition as

Main Equation for Gas Flow in Wellbores

Solution This equation contains Three variables that are functions of position Z (compressibility factor) Temperature Pressure A simple approach is to use average values of temperature and Z over a segment of the pipe. There are two options for temperature in a segment between points 1 and 2

Method to Calculate P in a Segment T_average can be obtained from T1 and T2 Z_average is calculated from T_average and P1 In the segment, we can calculate P2 Z_average can be updated with new P in the segment which is (P1+P2)/2 We repeat the calculate until convergence. P1, T1 P2, T2

Solution For the special case of horizontal well

Oil Field Unit P1 P2

Example 3