PETE 411 Well Drilling Lesson 9 Drilling Hydraulics - Hydrostatics.

Slides:



Advertisements
Similar presentations
Fluid mechanics. Pressure at depth In a cylindrical column of water, as in any cylinder the volume is the height x cross sectional area The density of.
Advertisements

PETE 411 Well Drilling Lesson 17 Casing Design.
Archimedes’ Principle An object immersed in a liquid has an upward buoyant force equal to the weight of the liquid displaced by the object. An object will.
PETE 411 Well Drilling Lesson 13 Pressure Drop Calculations
Liquids and Gasses Matter that “Flows”
Chapter 15 Fluids. Pressure The same force applied over a smaller area results in greater pressure – think of poking a balloon with your finger and.
Lesson 20 Abnormal Pressure
DRILLING ENGINEERING Well Control.
Lesson 14 Jet Bit Nozzle Size Selection
Static Fluids Fluids are substances, such as liquids and gases, that have no rigidity. A fluid lacks a fixed shape and assumes the shape of its container.
Fluids & Elasticity (Buoyancy & Fluid Dynamics)
PETE 411 Well Drilling Lesson 5 Hole Problems.
Lesson 22 Prediction of Fracture Gradients
PETE 203 DRILLING ENGINEERING
Petroleum Engineering 411 Well Drilling
Lesson 36 Torque and Drag Calculations
Lec 4: Fluid statics, buoyancy and stability, pressure
Physics 11 Scale Up Fall 2014 Chapter 13.
Fluid mechanics 3.1 – key points
The tendency or ability of an object to float.
Sect. 14.4: Buoyant Forces Archimedes’ Principle
Unit 3 - FLUID MECHANICS.
PETE 411 Well Drilling Lesson 23 Gas Cut Mud.
Lesson 3 The Rig - Drilling Equipment
Lesson 4 Drilling Cost & Drilling Rate
Lesson 10 Drilling Hydraulics (cont’d)
Lesson 25 Well Control, cont’d
Drilling String Design
Hydrostatic Pressure distribution in a static fluid and its effects on solid surfaces and on floating and submerged bodies. Fluid Statics M. Bahrami ENSC.
Fluid Statics.
Lesson 15 Surge and Swab Pressures
Petroleum Engineering 406 Lesson 6 Well Control Unusual Operations.
Lesson 12 Laminar Flow - Slot Flow
Lesson 18 Casing Design Example
Well Design PE 413.
Advanced Physics Chapter 10 Fluids. Chapter 10 Fluids 10.1 Phases of Matter 10.2 Density and Specific Gravity 10.3 Pressure in Fluids 10.4 Atmospheric.
Warm-up Pick up the free response at the door and begin working on it.
Lesson 26 * Well Control * * Variable Geometry *
Drilling Engineering Prepared by: Tan Nguyen Drilling Engineering - PE 311 Laminar Flow in Pipes and Annuli Non-Newtonian Fluids.
Casing Design.
PHYSICS 103: Lecture 17 Fluids  Gases (Air)  Liquids  Archimedes Principle Agenda for Today: Note: The next several lectures will not follow textbook.
CHAPTER 2 Fluid Statics and Its Applications Nature of fluids
CE 1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
Chapter 10 Fluids. Units of Chapter 10 Phases of Matter Density Pressure in Fluids Atmospheric Pressure and Gauge Pressure Pascal’s Principle Measurement.
Fluid Mechanics - Hydrostatics AP Physics 2. States of Matter Before we begin to understand the nature of a Fluid we must understand the nature of all.
Introduction to Fluid Mechanics Engineering 1h Prof Bill Easson.
Introduction To Fluids. Density  = m/V  = m/V   : density (kg/m 3 )  m: mass (kg)  V: volume (m 3 )
Chapter 19 Liquids.
Chapter 12 Outline Fluid Mechanics Density Pressure Gauge pressure Pascal’s law Buoyancy Archimedes’ principle.
Hydrostatics Lesson 6 © nitatravels. Fluids are Everywhere  Liquids or Gasses  Air is a fluid!!!  Typically take the shape of their container.
Liquids Definite volume but no definite shape!. Liquids Pressure Buoyancy Archimedes’ Principle Density Effects Pascal’s Principle.
Density. (a) define the term density What is density? Density is defined as mass per unit volume.mass Density is defined as mass per unit volume.mass.
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.
Dr. Kamel Mohamed Guedri Umm Al-Qura University, Room H1091
Chapter 10.4 Learning Goals
Kick Submited to :- Submitted by:- Er Akash Rana Devahish Yadav B.Tech IIIrd Year Petroleum Technology 1.
Reports Lab Reports for first lab session are due.
Introduction To Fluids. Density ρ = m/V ρ = m/V  ρ: density (kg/m 3 )  m: mass (kg)  V: volume (m 3 )
AKM 205 AKIŞKANLAR MEKANİĞİ Yrd.Doç.Dr. Onur Tunçer İstanbul Teknik Üniversitesi “AKIŞKAN STATİĞİ”
States of Matter. Fluid States In science, gases and liquids are fluids Fluid pressure is the force exerted by the fluid on an area of a surface. p =
Physics 141Mechanics Lecture 20 Fluid Dynamics Yongli Gao A fluid is a substance that can flow. In contrast to a solid, a fluid has no shape, and it takes.
Chapter 2: Casing Design Casing Selection
Design Factors Collapse Corrected
Casing Design Workshop
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
3.2 Pressure and the Buoyant Force
Chapter 2: Casing Design Calculations of Loads on a Casing
Casing Design Workshop
Fluid Mechanics – Buoyancy
Design Calculations Combination Strings
Presentation transcript:

PETE 411 Well Drilling Lesson 9 Drilling Hydraulics - Hydrostatics

Drilling Hydraulics - Hydrostatics Hydrostatic Pressure in Liquid Columns Hydrostatic Pressure in Gas Columns Hydrostatic Pressure in Complex Columns Forces on Submerged Body Effective (buoyed) Weight of Submerged Body Axial Tension in Drill String sA = FA/A

HW #4 ADE #1.18, 1.19, 1.24 Due Monday, Sept 23, 2002 Read: Applied Drilling Engineering, Ch.4 (Drilling Hydraulics) to p. 125 HW #4 ADE #1.18, 1.19, 1.24 Due Monday, Sept 23, 2002

Drilling Hydraulics Applications WHY? Drilling Hydraulics Applications Calculation of subsurface hydrostatic pressures that may tend to burst or collapse well tubulars or fracture exposed formations Several aspects of blowout prevention Displacement of cement slurries and resulting stresses in the drillstring

Drilling Hydraulics Applications cont’d Bit nozzle size selection for optimum hydraulics Surge or swab pressures due to vertical pipe movement Carrying capacity of drilling fluids

Fig. 4-2. The Well Fluid System ppore < pmud < pfrac Well Control Fig. 4-2. The Well Fluid System

Forces Acting on a Fluid Element FWV = specific wt. of the fluid

Pressures in a fluid column At equilibrium, S F = 0 0 = F1 + F2 + F3 (p = rgh)

Incompressible Fluids Integrating,

Incompressible Fluids In field units, 1’ x 1’ x 1’ cube

Incompressible fluids If p0 = 0 (usually the case except during well control or cementing procedures) then,

Compressible Fluids …………… (1) …………… (2) …… (3) But, …… (4) from (3) p = pressure of gas, psia V = gas volume, gal Z = gas deviation factor n = moles of gas R = universal gas constant = 80.3 T = temperature, R r = density, lbm/gal M = gas molecular wt. m = mass of gas …………… (1) …………… (2) …… (3) But, …… (4) from (3)

Compressible Fluids r = density, lbm/gal p = pressure of gas, psia V = gas volume, gal Z = gas deviation factor n = moles of gas R = universal gas constant, = 80.3 T = temperature, oR r = density, lbm/gal M = gas molecular wt. m = mass of gas, lbm

Compressible Fluids From Eqs. (2) and (4): Integrating, Assumptions?

Example Column of Methane (M = 16) Pressure at surface = 1,000 psia Z=1, T=140 F (i) What is pressure at 10,000 ft? (ii) What is density at surface? (iii) What is density at 10,000 ft? (iv) What is psurf if p10,000 = 8,000 psia?

(i) What is pressure at 10,000 ft? Example (i) (i) What is pressure at 10,000 ft?

Example cont’d (ii) What is density at surface? (iii) What is density at 10,000 ft?

(iv) What is psurf if p10,000 = 8,000 psia? Example (iv) What is psurf if p10,000 = 8,000 psia?

Fig. 4-3. A Complex Liquid Column

Fig. 4-4. Viewing the Well as a Manometer Pa = ? Fig. 4-4. Viewing the Well as a Manometer

Figure 4.4

Buoyancy Force = weight of fluid displaced (Archimedes, 250 BC) Figure 4-9. Hydraulic forces acting on a foreign body

Effective (buoyed) Weight Buoyancy Factor Valid for a solid body or an open-ended pipe!

For steel, immersed in mud, the buoyancy factor is: Example For steel, immersed in mud, the buoyancy factor is: A drillstring weighs 100,000 lbs in air. Buoyed weight = 100,000 * 0.771 = 77,100 lbs

Axial Forces in Drillstring Fb = bit weight

Simple Example - Empty Wellbore Drillpipe weight = 19.5 lbf/ft 10,000 ft 0 lbf 195,000 lbf OD = 5.000 in ID = 4.276 in DEPTH, ft A = 5.265 in2 AXIAL TENSION, lbf W = 19.5 lbf/ft * 10,000 ft = 195,000 lbf

Example - 15 lb/gal Mud in Wellbore Drillpipe weight = 19.5 lbf/ft 10,000 ft - 41,100 153,900 195,000 lbf OD = 5.000 in ID = 4.276 in DEPTH, ft A = 5.265 in2 AXIAL TENSION, lbf F = P * A = 7,800 * 5.265 = 41,100 lbf Pressure at bottom = 0.052 * 15 * 10,000 = 7,800 psi W = 195,000 - 41,100 = 153,900 lbf

Anywhere in the Drill Collars: Axial Tension = Wt Anywhere in the Drill Collars: Axial Tension = Wt. - Pressure Force - Bit Wt.

Anywhere in the Drill Pipe: Axial Tension = Wts Anywhere in the Drill Pipe: Axial Tension = Wts. - Pressure Forces - Bit Wt. FT

Axial Tension in Drill String Example A drill string consists of 10,000 ft of 19.5 #/ft drillpipe and 600 ft of 147 #/ft drill collars suspended off bottom in 15#/gal mud (Fb = bit weight = 0). What is the axial tension in the drillstring as a function of depth?

Example A1 Pressure at top of collars = 0.052 (15) 10,000 = 7,800 psi Pressure at bottom of collars = 0.052 (15) 10,600 = 8,268 psi Cross-sectional area of pipe, 10,000’ 10,600’

Cross-sectional area of collars, Example Cross-sectional area of collars, A2

Example 1. At 10,600 ft. (bottom of drill collars) 4 1. At 10,600 ft. (bottom of drill collars) Compressive force = pA = 357,200 lbf [ axial tension = - 357,200 lbf ] 3 2 1

Example 2. At 10,000 ft+ (top of collars) FT = W2 - F2 - Fb 4 2. At 10,000 ft+ (top of collars) FT = W2 - F2 - Fb = 147 lbm/ft * 600 ft - 357,200 = 88,200 - 357,200 = -269,000 lbf Fb = FBIT = 0 3 2 1

Example 3. At 10,000 ft - (bottom of drillpipe) FT = W1+W2+F1-F2-Fb 4 3. At 10,000 ft - (bottom of drillpipe) FT = W1+W2+F1-F2-Fb = 88,200 + 7800 lbf/in2 * 37.5in2 - 357,200 = 88,200 + 292,500 - 357,200 = + 23,500 lbf 3 2 1

Example 4. At Surface FT = W1 + W2 + F1 - F2 - Fb = 19.5 * 10,000 + 23,500 = 218,500 lbf Also: FT = WAIR * BF = 283,200 * 0.7710 = 218,345 lbf 3 2 1

Fig. 4-11. Axial tensions as a function of depth for Example 4.9

Example - Summary 1. At 10,600 ft FT = -357,200 lbf [compression] 3. At 10,000 - ft FT = +23,500 lbf [tension] 4. At Surface FT = +218,500 lbf [tension]