Tom BLASINGAME Texas A&M U. Slide 1

Size: px
Start display at page:

Download "Tom BLASINGAME Texas A&M U. Slide 1"

Transcription

1 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Slide 1

2 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Slide

3 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow Relations fo a Radial System fom Deatment of Petoleum Engineeing Couse Notes (1997) Slide 3

4 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 4

5 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 5

6 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 6

7 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 7

8 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 8

9 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 9

10 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 10

11 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi (Deivation of the Pseudosteady-State Flow Relations fo a Radial System) Slide 11

12 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Illustations of Pseudosteady-State Pefomance in Radial Flow Systems fom Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986) Slide 1

13 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 13

14 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 14

15 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 15

16 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 16

17 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pessue Tends fom Deatment of Petoleum Engineeing Couse Notes (01) Slide 17

18 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pessue Distibutions: Solutions Steady-State Solution: w e All elations given in FIELD units. q 141. scb ln( / w ) kh q 141. scb ln( e / ) kh [ wf fom] [ e fom] Radius of Investigation: Full Solution: (q sc =constant) D E 1 kh ( qb 4t D D i 1 E 1 ) 4t ed D t D ed ex 4t ed D inv -.434x10 D ed k c 1 ex 4 4t ed D t t Slide 18

19 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pessue Distibutions: Tansient Flow Pessue, sia Radial Pessue Distibution (Lee text Fig. 1.7) Pessue Dawdown and Buildu Cases E1(x) Solution t = 1000 h i = 000 sia 0.1 h 1 h 10 h 100 h 1000 h t = 100 h t = 10 h t = 1 h t = 0.1 h t = 0.1 h 1 h 10 h 100 h 1000 h e = 3000 ft Legend: D_DD(, t_ 1Em1 h) D_DD(, t_ 1E0 h) D_DD(, t_ 1E1 h) D_DD(, t_ 1E h) D_DD(, t_ 1E3 h) D_BU(,t_+_ Dt_ 1Em1 h) D_BU(,t_+_ Dt_ 1E0 h) D_BU(,t_+_ Dt_ 1E1 h) D_BU(,t_+_ Dt_ 1E h) D_BU(,t_+_ Dt_ 1E3 h) E-01 1.E+00 1.E+01 1.E+0 1.E+03 1.E+04 Pessue Distibutions fo Tansient Radial Flow Note the effect of the dawdown. Note that the buildu essue tends etace last dawdown tend. Recall that all measuements ae at the wellboe, we cannot "see" in the esevoi ou analyses ae infeed fom wellboe measuements. Radial Distance, ft Slide 19

20 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pessue Distibutions: Pseudosteady-State The hysical concet of the PSEUDOSTEADY-STATE FLOW condition is defined as the condition whee the essue at all oints in the esevoi changes at the same ate. Mathematically, this condition is given by: d [ (, t)] constant dt Slide 0

21 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pessue Distibutions: Pseudosteady-State Concet: (essue changes at the same ate at all oints in the esevoi) d d Resevoi Pessue Schematic: constant Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 1

22 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow: Summay of Relations ( - wf ) Flow Relations: (Cicula Resevoi) ( - wf ) Flow Relations: ( = Eule's constant) Time-Deendent Pseudosteady-State Flow Relations: ) ( ) ( 1 ln ) ( 141. s kh qb w e w w w e e wf Fomulatio n) (Geneal 1 4 ln Resevoi) (Cicula 4 3 ln 141. s C A e kh qb s kh qb A w wf w e wf t c V qb s kh qb t c V qb kh qb t w e i wf t w e w e i ln ) ( ) ( 1 ln 141. Slide

23 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow: Illustative Behavio inv -.434x10 k ct t Figue : Resevoi Pessue Distibution Constant Rate Tansient Flow Dawdown. Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 3

24 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow: Illustative Behavio k ct Figue 7: Resevoi Pessue Distibution Constant Wellboe Pessue Tansient Flow Dawdown. inv.434x10 - t Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 4

25 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow: Illustative Behavio k ct Figue 5: Resevoi Pessue Distibution Constant Rate Post- Tansient Flow Dawdown, Homogeneous Resevois. inv -.434x10 t Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 5

26 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Pseudosteady-State Flow: Illustative Behavio Figue 57: Resevoi Pessue Distibution Constant Wellboe Pessue Post-Tansient Flow Dawdown, Homogeneous Resevois. inv -.434x10 k ct t Fom: Blasingame, T.A.: Vaiable-Rate Analysis: Tansient and Pseudosteady-State Methods of Inteetation and Alication, M.S. Thesis, Texas A&M Univesity (1986). Slide 6

27 Petoleum Engineeing 60 Fluid Flow in Petoleum Resevois Fundamental Flow Lectue 4 Pseudosteady-State Flow in a Cicula Resevoi Resevoi Pessue Tends: Questions to Conside Q1. Why study "esevoi essue tends?" A1. We can not measue essue in the esevoi only at the wellboe (o sandface). In ode to estimate the behavio in the esevoi, we must use "model-based" essue distibutions. Q. Isn't the use of a simle model too limiting? A. Actually, no. Simle models ae extemely consistent, and as such, even when "wong," the "tend" behavio is tyically quite eesentative. Q3. What is the "adius of investigation?" A3. Fo the infinite-acting adial flow case, the adius of investigation is the oint in the esevoi whee the logaithm of adius equation (staight line) intesects the initial esevoi essue. It is a fictitious oint, but it eesents the "theoetical" location of the font of the essue distibution font. inv.434 x 10 k c t t Slide 7

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997) Pseudoseady-Sae Flow Relaions fo a Radial Sysem fom Deamen of Peoleum Engineeing Couse Noes (1997) (Deivaion of he Pseudoseady-Sae Flow Relaions fo a Radial Sysem) (Deivaion of he Pseudoseady-Sae Flow

More information

Solution and Type Curve Analysis of Fluid Flow Model for Fractal Reservoir

Solution and Type Curve Analysis of Fluid Flow Model for Fractal Reservoir Wold Jounal of Mechanics, 0,, 09-6 doi:0.436/wjm.0.507 Published Online Octobe 0 (htt://www.scirp.og/jounal/wjm) Solution and Tye Cuve Analysis of Fluid Flow Model fo Factal Resevoi Yulong Zhao, Liehui

More information

PRESSURE DRAWDOWN EQUATIONS FOR MULTIPLE-WELL SYSTEMS IN CIRCULAR-CYLINDRICAL RESERVOIRS

PRESSURE DRAWDOWN EQUATIONS FOR MULTIPLE-WELL SYSTEMS IN CIRCULAR-CYLINDRICAL RESERVOIRS VOL. 8, NO. 7, JULY 013 ISSN 1819-6608 ARPN Jounal of Engineeing and Applied Sciences 006-013 Asian Reseac Publising Netwok (ARPN). All igts eseved. www.apnjounals.com PRESSURE RAWOWN EQUATIONS FOR MULTIPLE-WELL

More information

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website: Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula

More information

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1 Physics 1501 Fall 2008 Mechanics, Themodynamics, Waves, Fluids Lectue 6: motion in two and thee dimensions III Slide 6-1 Recap: elative motion An object moves with velocity v elative to one fame of efeence.

More information

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface . CONICAL PROJECTIONS In elementay texts on map pojections, the pojection sufaces ae often descibed as developable sufaces, such as the cylinde (cylindical pojections) and the cone (conical pojections),

More information

8 Separation of Variables in Other Coordinate Systems

8 Separation of Variables in Other Coordinate Systems 8 Sepaation of Vaiables in Othe Coodinate Systems Fo the method of sepaation of vaiables to succeed you need to be able to expess the poblem at hand in a coodinate system in which the physical boundaies

More information

H5 Gas meter calibration

H5 Gas meter calibration H5 Gas mete calibation Calibation: detemination of the elation between the hysical aamete to be detemined and the signal of a measuement device. Duing the calibation ocess the measuement equiment is comaed

More information

Petroleum Engineering 324 Well Performance Daily Summary Sheet Spring 2009 Blasingame/Ilk. Date: Materials Covered in Class Today: Comment(s):

Petroleum Engineering 324 Well Performance Daily Summary Sheet Spring 2009 Blasingame/Ilk. Date: Materials Covered in Class Today: Comment(s): Petroleum Engineering 324 Well Performance Daily Summary Sheet Sring 2009 Blasingame/Ilk Date: Materials Covered in Class Today: Comment(s): Pressure Transient Analysis Pressure Buildu Test Analysis Lee

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small. Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak Designing a Sine-Coil fo Measuement of Plasma Displacements in IR-T Tokamak Pejman Khoshid, M. Razavi, M. Ghoanneviss, M. Molaii, A. TalebiTahe, R. Avin, S. Mohammadi and A. NikMohammadi Dept. of Physics,

More information

7.2.1 Basic relations for Torsion of Circular Members

7.2.1 Basic relations for Torsion of Circular Members Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,

More information

ANALYSIS OF PRESSURE VARIATION OF FLUID IN AN INFINITE ACTING RESERVOIR

ANALYSIS OF PRESSURE VARIATION OF FLUID IN AN INFINITE ACTING RESERVOIR Nigeian Jounal of Technology (NIJOTECH) Vol. 36, No. 1, Januay 2017, pp. 80 86 Copyight Faculty of Engineeing, Univesity of Nigeia, Nsukka, Pint ISSN: 0331-8443, Electonic ISSN: 2467-8821 www.nijotech.com

More information

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2 THE LAPLACE EQUATION The Laplace (o potential) equation is the equation whee is the Laplace opeato = 2 x 2 u = 0. in R = 2 x 2 + 2 y 2 in R 2 = 2 x 2 + 2 y 2 + 2 z 2 in R 3 The solutions u of the Laplace

More information

From Gravitational Collapse to Black Holes

From Gravitational Collapse to Black Holes Fom Gavitational Collapse to Black Holes T. Nguyen PHY 391 Independent Study Tem Pape Pof. S.G. Rajeev Univesity of Rocheste Decembe 0, 018 1 Intoduction The pupose of this independent study is to familiaize

More information

Lecture 5. Torsion. Module 1. Deformation Pattern in Pure Torsion In Circular Cylinder. IDeALab. Prof. Y.Y.KIM. Solid Mechanics

Lecture 5. Torsion. Module 1. Deformation Pattern in Pure Torsion In Circular Cylinder. IDeALab. Prof. Y.Y.KIM. Solid Mechanics Lectue 5. Tosion Module 1. Defomation Patten in Pue Tosion In Cicula Cylinde Defomation Patten Shafts unde tosion ae eveywhee. Candall, An Intoduction to the Mechanics of solid, Mc Gaw-Hill, 1999 1 Defomation

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

Kinematics in 2-D (II)

Kinematics in 2-D (II) Kinematics in 2-D (II) Unifom cicula motion Tangential and adial components of Relative velocity and acceleation a Seway and Jewett 4.4 to 4.6 Pactice Poblems: Chapte 4, Objective Questions 5, 11 Chapte

More information

Petroleum Engineering 613 Natural Gas Engineering. Texas A&M University. Lecture 07: Wellbore Phenomena

Petroleum Engineering 613 Natural Gas Engineering. Texas A&M University. Lecture 07: Wellbore Phenomena Petroleum Engineering 613 Natural Gas Engineering Texas A&M University Lecture 07: T.A. Blasingame, Texas A&M U. Department of Petroleum Engineering Texas A&M University College Station, TX 77843-3116

More information

Galactic Contraction and the Collinearity Principle

Galactic Contraction and the Collinearity Principle TECHNISCHE MECHANIK, Band 23, Heft 1, (2003), 21-28 Manuskipteingang: 12. August 2002 Galactic Contaction and the Collineaity Pinciple F.P.J. Rimott, FA. Salusti In a spial galaxy thee is not only a Keplefoce

More information

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei Intenational Confeence on Intelligent Systems Reseach and Mechatonics Engineeing (ISRME 0) Analysis of high speed machining cente spindle dynamic unit stuctue pefomance Yuan guowei Liaoning jidian polytechnic,dan

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

Psychometric Methods: Theory into Practice Larry R. Price

Psychometric Methods: Theory into Practice Larry R. Price ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include

More information

Exam 1. Exam 1 is on Tuesday, February 14, from 5:00-6:00 PM.

Exam 1. Exam 1 is on Tuesday, February 14, from 5:00-6:00 PM. Exam 1 Exam 1 is on Tuesday, Febuay 14, fom 5:00-6:00 PM. Testing Cente povides accommodations fo students with special needs I must set up appointments one week befoe exam Deadline fo submitting accommodation

More information

Physics 1502: Lecture 4 Today s Agenda

Physics 1502: Lecture 4 Today s Agenda 1 Physics 1502: Today s genda nnouncements: Lectues posted on: www.phys.uconn.edu/~cote/ HW assignments, solutions etc. Homewok #1: On Mastephysics today: due next Fiday Go to masteingphysics.com and egiste

More information

6.4 Period and Frequency for Uniform Circular Motion

6.4 Period and Frequency for Uniform Circular Motion 6.4 Peiod and Fequency fo Unifom Cicula Motion If the object is constained to move in a cicle and the total tangential foce acting on the total object is zeo, F θ = 0, then (Newton s Second Law), the tangential

More information

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation One-Dimensional, Steady-State State Conduction with Themal Enegy Geneation Implications of Enegy Geneation Involves a local (volumetic) souce of themal enegy due to convesion fom anothe fom of enegy in

More information

APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE GEOTHERMAL RESERVOIRS

APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE GEOTHERMAL RESERVOIRS PROCEEDINGS, Twenty-Eighth Wokshop on Geothemal Resevoi Engineeing Stanfod Univesity, Stanfod, Califonia, Januay 27-29, 23 SGP-TR-173 APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE

More information

where a = x 10-3 for units of kcal/mol

where a = x 10-3 for units of kcal/mol Detemining the Enegy of Activation Paametes fom Dynamic MR Expeiments: -D. Rich Shoemake (Souce: Dynamic MR Spectoscopy by J. Sandstöm, and me) he esults contained in this document have been published:

More information

Effect of no-flow boundaries on interference testing. in fractured reservoirs

Effect of no-flow boundaries on interference testing. in fractured reservoirs Effect of no-flo boundaies on intefeence testing in factued esevois T.Aa. Jelmet 1 1 epatement of petoleum engineeing and applied geophysics,, Noegian Univesity of Science and Tecnology, NTNU. Tondheim,

More information

Lecture 2 - Thermodynamics Overview

Lecture 2 - Thermodynamics Overview 2.625 - Electochemical Systems Fall 2013 Lectue 2 - Themodynamics Oveview D.Yang Shao-Hon Reading: Chapte 1 & 2 of Newman, Chapte 1 & 2 of Bad & Faulkne, Chaptes 9 & 10 of Physical Chemisty I. Lectue Topics:

More information

ME 425: Aerodynamics

ME 425: Aerodynamics ME 5: Aeodynamics D ABM Toufique Hasan Pofesso Depatment of Mechanical Engineeing, BUET Lectue- 8 Apil 7 teachebuetacbd/toufiquehasan/ toufiquehasan@mebuetacbd ME5: Aeodynamics (Jan 7) Flow ove a stationay

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

3.012 Fund of Mat Sci: Bonding Lecture 5/6. Comic strip removed for copyright reasons.

3.012 Fund of Mat Sci: Bonding Lecture 5/6. Comic strip removed for copyright reasons. 3.12 Fund of Mat Sci: Bonding Lectue 5/6 THE HYDROGEN ATOM Comic stip emoved fo copyight easons. Last Time Metal sufaces and STM Diac notation Opeatos, commutatos, some postulates Homewok fo Mon Oct 3

More information

Stellar Structure and Evolution

Stellar Structure and Evolution Stella Stuctue and Evolution Theoetical Stella odels Conside each spheically symmetic shell of adius and thickness d. Basic equations of stella stuctue ae: 1 Hydostatic equilibium π dp dp d G π = G =.

More information

Mechanics Physics 151

Mechanics Physics 151 Mechanics Physics 151 Lectue 5 Cental Foce Poblem (Chapte 3) What We Did Last Time Intoduced Hamilton s Pinciple Action integal is stationay fo the actual path Deived Lagange s Equations Used calculus

More information

CBE Transport Phenomena I Final Exam. December 19, 2013

CBE Transport Phenomena I Final Exam. December 19, 2013 CBE 30355 Tanspot Phenomena I Final Exam Decembe 9, 203 Closed Books and Notes Poblem. (20 points) Scaling analysis of bounday laye flows. A popula method fo measuing instantaneous wall shea stesses in

More information

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Dynamics (Stömningsläa), 2013-05-31, kl 9.00-15.00 jälpmedel: Students may use any book including the textbook Lectues on Fluid Dynamics.

More information

, the tangent line is an approximation of the curve (and easier to deal with than the curve).

, the tangent line is an approximation of the curve (and easier to deal with than the curve). 114 Tangent Planes and Linea Appoimations Back in-dimensions, what was the equation of the tangent line of f ( ) at point (, ) f ( )? (, ) ( )( ) = f Linea Appoimation (Tangent Line Appoimation) of f at

More information

5.111 Lecture Summary #6 Monday, September 15, 2014

5.111 Lecture Summary #6 Monday, September 15, 2014 5.111 Lectue Summay #6 Monday, Septembe 15, 014 Readings fo today: Section 1.9 Atomic Obitals. Section 1.10 Electon Spin, Section 1.11 The Electonic Stuctue of Hydogen. (Same sections in 4 th ed.) Read

More information

π(x, y) = u x + v y = V (x cos + y sin ) κ(x, y) = u y v x = V (y cos x sin ) v u x y

π(x, y) = u x + v y = V (x cos + y sin ) κ(x, y) = u y v x = V (y cos x sin ) v u x y F17 Lectue Notes 1. Unifom flow, Souces, Sinks, Doublets Reading: Andeson 3.9 3.12 Unifom Flow Definition A unifom flow consists of a velocit field whee V φ = uî + vθˆ is a constant. In 2-D, this velocit

More information

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas C:\Dallas\0_Couses\0_OpSci_330\0 Lectue Notes\04 HfkPopagation.doc: Page of 9 Lectue 04: HFK Popagation Physical Optics II (Optical Sciences 330) (Updated: Fiday, Apil 9, 005, 8:05 PM) W.J. Dallas The

More information

Fri Angular Momentum Quiz 10 RE 11.a; HW10: 13*, 21, 30, 39 Mon , (.12) Rotational + Translational RE 11.b Tues.

Fri Angular Momentum Quiz 10 RE 11.a; HW10: 13*, 21, 30, 39 Mon , (.12) Rotational + Translational RE 11.b Tues. Fi. 11.1 Angula Momentum Quiz 10 R 11.a; HW10: 13*, 1, 30, 39 Mon. 11.-.3, (.1) Rotational + Tanslational R 11.b Tues. P10 Mon. 11.4-.6, (.13) Angula Momentum & Toque Tues. Wed. 11.7 -.9, (.11) Toque R

More information

Particle Systems. University of Texas at Austin CS384G - Computer Graphics Fall 2010 Don Fussell

Particle Systems. University of Texas at Austin CS384G - Computer Graphics Fall 2010 Don Fussell Paticle Systems Univesity of Texas at Austin CS384G - Compute Gaphics Fall 2010 Don Fussell Reading Requied: Witkin, Paticle System Dynamics, SIGGRAPH 97 couse notes on Physically Based Modeling. Witkin

More information

6.1: Angles and Their Measure

6.1: Angles and Their Measure 6.1: Angles and Thei Measue Radian Measue Def: An angle that has its vetex at the cente of a cicle and intecepts an ac on the cicle equal in length to the adius of the cicle has a measue of one adian.

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Depatment Physics 8.033 Decembe 5, 003 Poblem Set 10 Solutions Poblem 1 M s y x test paticle The figue above depicts the geomety of the poblem. The position

More information

PROBLEM SET 5. SOLUTIONS March 16, 2004

PROBLEM SET 5. SOLUTIONS March 16, 2004 Havad-MIT ivision of Health Sciences and Technology HST.54J: Quantitative Physiology: Ogan Tanspot Systems Instuctos: Roge Mak and Jose Venegas MASSACHUSETTS INSTITUTE OF TECHNOLOGY epatments of Electical

More information

Chapters 5-8. Dynamics: Applying Newton s Laws

Chapters 5-8. Dynamics: Applying Newton s Laws Chaptes 5-8 Dynamics: Applying Newton s Laws Systems of Inteacting Objects The Fee Body Diagam Technique Examples: Masses Inteacting ia Nomal Foces Masses Inteacting ia Tensions in Ropes. Ideal Pulleys

More information

Cross section dependence on ski pole sti ness

Cross section dependence on ski pole sti ness Coss section deendence on ski ole sti ness Johan Bystöm and Leonid Kuzmin Abstact Ski equiment oduce SWIX has ecently esented a new ai of ski oles, called SWIX Tiac, which di es fom conventional (ound)

More information

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

More information

THERMAL PROPERTIES OF FRACTAL STRUCTURE MATERIALS

THERMAL PROPERTIES OF FRACTAL STRUCTURE MATERIALS HERMAL PROPERIES OF FRACAL SRUCURE MAERIALS Oldřich Zmeškal, Mioslav Buchníček, Matin Nežádal Pavla Štefková, Radek Capoušek Institute of Physical and Applied Chemisty, Faculty of Chemisty, Bno Univesity

More information

LINEAR PLATE BENDING

LINEAR PLATE BENDING LINEAR PLATE BENDING 1 Linea plate bending A plate is a body of which the mateial is located in a small egion aound a suface in the thee-dimensional space. A special suface is the mid-plane. Measued fom

More information

Physics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!!

Physics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!! Physics 161 Fall 011 Exta Cedit Investigating Black Holes - olutions The Following is Woth 50 Points!!! This exta cedit assignment will investigate vaious popeties of black holes that we didn t have time

More information

11.2. Area of a Circle. Lesson Objective. Derive the formula for the area of a circle.

11.2. Area of a Circle. Lesson Objective. Derive the formula for the area of a circle. 11.2 Aea of a Cicle Lesson Objective Use fomulas to calculate the aeas of cicles, semicicles, and quadants. Lean Deive the fomula fo the aea of a cicle. A diamete divides a cicle of adius into 2 semicicles.

More information

Nuclear Medicine Physics 02 Oct. 2007

Nuclear Medicine Physics 02 Oct. 2007 Nuclea Medicine Physics Oct. 7 Counting Statistics and Eo Popagation Nuclea Medicine Physics Lectues Imaging Reseach Laboatoy, Radiology Dept. Lay MacDonald 1//7 Statistics (Summaized in One Slide) Type

More information

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6 MOTION IN A PLANE 1. Scala Quantities Physical quantities that have only magnitude and no diection ae called scala quantities o scalas. e.g. Mass, time, speed etc. 2. Vecto Quantities Physical quantities

More information

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the

More information

INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS. Abstract

INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS. Abstract INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS Mohammad Mohammadi, National Cente fo Physical Acoustics, Univesity of Mississippi, MS Caig J. Hicey, National Cente fo Physical Acoustics,

More information

Applied Aerodynamics

Applied Aerodynamics Applied Aeodynamics Def: Mach Numbe (M), M a atio of flow velocity to the speed of sound Compessibility Effects Def: eynolds Numbe (e), e ρ c µ atio of inetial foces to viscous foces iscous Effects If

More information

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Lawence Bekeley National Laboatoy Lawence Bekeley National Laboatoy Title Numeical simulation o single-phase and multiphase non-acy low in poous and actued esevois Pemalink https://escholaship.og/uc/item/5jd465xg

More information

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased PHYS 0B - HW #7 Sping 2004, Solutions by David Pace Any efeenced euations ae fom Giffiths Poblem statements ae paaphased. Poblem 0.3 fom Giffiths A point chage,, moves in a loop of adius a. At time t 0

More information

A 1. EN2210: Continuum Mechanics. Homework 7: Fluid Mechanics Solutions

A 1. EN2210: Continuum Mechanics. Homework 7: Fluid Mechanics Solutions EN10: Continuum Mechanics Homewok 7: Fluid Mechanics Solutions School of Engineeing Bown Univesity 1. An ideal fluid with mass density ρ flows with velocity v 0 though a cylindical tube with cosssectional

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

4.4 Buoyant plume from a steady heat source

4.4 Buoyant plume from a steady heat source 1 Notes on 1.63 Advanced Envionmental Fluid Mechanics Instucto: C. C. Mei, 22 ccmei@mit.edu, 1 617 253 2994 Octobe 25, 22 4-4 buoyplum.tex 4.4 Buoyant plume fom a steady heat souce [Refeence]: Gebhat,

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

STRESS ANALYSIS OF THE MULTI-LAYERED THICK CYLINDERS

STRESS ANALYSIS OF THE MULTI-LAYERED THICK CYLINDERS Yea STRESS ANALYSIS OF THE MULTI-LAYERED THICK CYLINDERS Assist Lectue Abdul Munium Razoki Majeed Algboy Institute of Medical Technology (Baghdad) Foundation of Technical Education ABSTRACT In this study,

More information

Contact impedance of grounded and capacitive electrodes

Contact impedance of grounded and capacitive electrodes Abstact Contact impedance of gounded and capacitive electodes Andeas Hödt Institut fü Geophysik und extateestische Physik, TU Baunschweig The contact impedance of electodes detemines how much cuent can

More information

But for simplicity, we ll define significant as the time it takes a star to lose all memory of its original trajectory, i.e.,

But for simplicity, we ll define significant as the time it takes a star to lose all memory of its original trajectory, i.e., Stella elaxation Time [Chandasekha 1960, Pinciples of Stella Dynamics, Chap II] [Ostike & Davidson 1968, Ap.J., 151, 679] Do stas eve collide? Ae inteactions between stas (as opposed to the geneal system

More information

MATH section 2.7 Related Rates Page 1 of 7

MATH section 2.7 Related Rates Page 1 of 7 MATH 0100 section.7 Related Rates Page 1 of 7 Unfotunatel, thee isn t much I can infom befoe ou encounte difficulties in this section. Remembe that this section is all wod poblems. You must be able to

More information

3.23 Electrical, Optical, and Magnetic Properties of Materials

3.23 Electrical, Optical, and Magnetic Properties of Materials MIT OpenCouseWae http://ocw.mit.edu 3.23 Electical, Optical, and Magnetic Popeties of Mateials Fall 27 Fo infomation about citing these mateials o ou Tems of Use, visit: http://ocw.mit.edu/tems. 3.23 Fall

More information

PHYSICS 220. Lecture 08. Textbook Sections Lecture 8 Purdue University, Physics 220 1

PHYSICS 220. Lecture 08. Textbook Sections Lecture 8 Purdue University, Physics 220 1 PHYSICS 0 Lectue 08 Cicula Motion Textbook Sections 5.3 5.5 Lectue 8 Pudue Univesity, Physics 0 1 Oveview Last Lectue Cicula Motion θ angula position adians ω angula velocity adians/second α angula acceleation

More information

Short Term Production Well: Estimation of the Shut-in Temperature

Short Term Production Well: Estimation of the Shut-in Temperature PROCEEINGS 43d Woksho on Geothemal Resevoi Engineeing Stanod Univesity Stanod Calionia Febuay 1-14 018 SGP-R-13 Shot em Podution Well: Estimation o the Shut-in emeatue L.V. Eelbaum 1 and I.M. Kutasov 1

More information

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables). II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent

More information

A Stochastic EOQ Policy of Cold-Drink-For a Retailer

A Stochastic EOQ Policy of Cold-Drink-For a Retailer Vietnam Jounal of Mathematics 33:4 005) 437 44 9LHWQDP -RXUQDO RI 0$7+0$7,&6 9$67 A Stochastic EOQ Policy of Cold-Dink-Fo a Retaile Shib Sanka Sana 1 Kipasindhu Chaudhui 1 Depatment of Math., Bhanga Mahavidyalaya

More information

12th WSEAS Int. Conf. on APPLIED MATHEMATICS, Cairo, Egypt, December 29-31,

12th WSEAS Int. Conf. on APPLIED MATHEMATICS, Cairo, Egypt, December 29-31, th WSEAS Int. Conf. on APPLIED MATHEMATICS, Caio, Egypt, Decembe 9-3, 7 5 Magnetostatic Field calculations associated with thick Solenoids in the Pesence of Ion using a Powe Seies expansion and the Complete

More information

Velocimetry Techniques and Instrumentation

Velocimetry Techniques and Instrumentation AeE 344 Lectue Notes Lectue # 05: elocimety Techniques and Instumentation D. Hui Hu Depatment of Aeospace Engineeing Iowa State Univesity Ames, Iowa 500, U.S.A Methods to Measue Local Flow elocity - Mechanical

More information

x 1 b 1 Consider the midpoint x 0 = 1 2

x 1 b 1 Consider the midpoint x 0 = 1 2 1 chapte 2 : oot-finding def : Given a function f(), a oot is a numbe satisfying f() = 0. e : f() = 2 3 = ± 3 question : How can we find the oots of a geneal function f()? 2.1 bisection method idea : Find

More information

Single Particle State AB AB

Single Particle State AB AB LECTURE 3 Maxwell Boltzmann, Femi, and Bose Statistics Suppose we have a gas of N identical point paticles in a box of volume V. When we say gas, we mean that the paticles ae not inteacting with one anothe.

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

More information

Fluid flow in curved geometries: Mathematical Modeling and Applications

Fluid flow in curved geometries: Mathematical Modeling and Applications Fluid flow in cuved geometies: Mathematical Modeling and Applications D. Muhammad Sajid Theoetical Plasma Physics Division PINSTECH, P.O. Niloe, PAEC, Islamabad Mach 01-06, 010 Islamabad, Paistan Pesentation

More information

PROBLEM SET #3A. A = Ω 2r 2 2 Ω 1r 2 1 r2 2 r2 1

PROBLEM SET #3A. A = Ω 2r 2 2 Ω 1r 2 1 r2 2 r2 1 PROBLEM SET #3A AST242 Figue 1. Two concentic co-axial cylindes each otating at a diffeent angula otation ate. A viscous fluid lies between the two cylindes. 1. Couette Flow A viscous fluid lies in the

More information

Flux Shape in Various Reactor Geometries in One Energy Group

Flux Shape in Various Reactor Geometries in One Energy Group Flux Shape in Vaious eacto Geometies in One Enegy Goup. ouben McMaste Univesity Couse EP 4D03/6D03 Nuclea eacto Analysis (eacto Physics) 015 Sept.-Dec. 015 Septembe 1 Contents We deive the 1-goup lux shape

More information

PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS. G. Michael Shook

PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS. G. Michael Shook PROCEEDINGS, Tenty-Fouth Wokshop on Geothemal Resevoi Engineeing Stanfod Univesity, Stanfod, Califonia, Januay 25-27, 1999 SGP-TR-162 PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS G. Michael Shook

More information

Force between two parallel current wires and Newton s. third law

Force between two parallel current wires and Newton s. third law Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel

More information

3. Electromagnetic Waves II

3. Electromagnetic Waves II Lectue 3 - Electomagnetic Waves II 9 3. Electomagnetic Waves II Last time, we discussed the following. 1. The popagation of an EM wave though a macoscopic media: We discussed how the wave inteacts with

More information

PHYS 301 HOMEWORK #10 (Optional HW)

PHYS 301 HOMEWORK #10 (Optional HW) PHYS 301 HOMEWORK #10 (Optional HW) 1. Conside the Legende diffeential equation : 1 - x 2 y'' - 2xy' + m m + 1 y = 0 Make the substitution x = cos q and show the Legende equation tansfoms into d 2 y 2

More information

Physics 201, Lecture 6

Physics 201, Lecture 6 Physics 201, Lectue 6 Today s Topics q Unifom Cicula Motion (Section 4.4, 4.5) n Cicula Motion n Centipetal Acceleation n Tangential and Centipetal Acceleation q Relatie Motion and Refeence Fame (Sec.

More information

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

Edulearn 11. Barcelona, Spain. June An Experiment in flow of fluids in unsteady state, with control

Edulearn 11. Barcelona, Spain. June An Experiment in flow of fluids in unsteady state, with control Edulean. Bacelona, Spain. June n Expeiment in flow of fluids in unsteady state, with contol Lucila Méndez Chávez, ntonio Valiente Badeas Facultad de Química, UNM. C.U. México.F. bstact he authos ae pofessos

More information

PHYS 1114, Lecture 21, March 6 Contents:

PHYS 1114, Lecture 21, March 6 Contents: PHYS 1114, Lectue 21, Mach 6 Contents: 1 This class is o cially cancelled, being eplaced by the common exam Tuesday, Mach 7, 5:30 PM. A eview and Q&A session is scheduled instead duing class time. 2 Exam

More information

Lab 10: Newton s Second Law in Rotation

Lab 10: Newton s Second Law in Rotation Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have

More information

On the exact transient solution of fluid queue driven by a birth death process with specific rational rates and absorption

On the exact transient solution of fluid queue driven by a birth death process with specific rational rates and absorption OPSEARCH Oct Dec 25 524:746 755 DOI.7/s2597-5-99-4 THEORETICAL ARTICLE On the exact tansient solution of fluid queue diven by a bith death pocess with specific ational ates and absoption Shuti Kapoo Dhamaaja

More information

Physics 161: Black Holes: Lecture 5: 22 Jan 2013

Physics 161: Black Holes: Lecture 5: 22 Jan 2013 Physics 161: Black Holes: Lectue 5: 22 Jan 2013 Pofesso: Kim Giest 5 Equivalence Pinciple, Gavitational Redshift and Geodesics of the Schwazschild Metic 5.1 Gavitational Redshift fom the Schwazschild metic

More information

Physics 411 Lecture 34. Sourced Radiation. Lecture 34. Physics 411 Classical Mechanics II

Physics 411 Lecture 34. Sourced Radiation. Lecture 34. Physics 411 Classical Mechanics II Physics 411 Lectue 34 Souced Radiation Lectue 34 Physics 411 Classical Mechanics II Novembe 21st, 2007 We ae eady to move on to the souce side of lineaized waves. The point of this whole section has been

More information

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden Applied Mathematical Sciences, Vol. 7, 13, no. 7, 335-348 Mathematical Model of Magnetometic Resistivity Sounding fo a Conductive Host with a Bulge Ovebuden Teeasak Chaladgan Depatment of Mathematics Faculty

More information

Handout: IS/LM Model

Handout: IS/LM Model Econ 32 - IS/L odel Notes Handout: IS/L odel IS Cuve Deivation Figue 4-4 in the textbook explains one deivation of the IS cuve. This deivation uses the Induced Savings Function fom Chapte 3. Hee, I descibe

More information