MULTI SCALE POROUS AND COLLOIDAL MATERIALS TEXTURE AND TRANSPORT PROPERTIES P. E. LEVITZ. Transport and invasion properties:

Numerical solution of diffusion mass transfer model in adsorption systems. Prof. Nina Paula Gonçalves Salau, D.Sc.

Numeical solution of diffusion mass tansfe model in adsoption systems Pof., D.Sc. Agenda Mass Tansfe Mechanisms Diffusion Mass Tansfe Models Solving Diffusion Mass Tansfe Models Paamete Estimation 2 Mass

Structure of glasses and melts

Stuctue of glasses and melts Matin Wilding Institute of Mathematical and Physical Sciences, Univesity of Wales, Abeystwyth, Ceedigion, SY3 3BZ Chis Benmoe, Intense Pulsed Neuton Souce and the Advanced

Diffusion and Transport. 10. Friction and the Langevin Equation. Langevin Equation. f d. f ext. f () t f () t. Then Newton s second law is ma f f f t.

Diffusion and Tanspot 10. Fiction and the Langevin Equation Now let s elate the phenomena of ownian motion and diffusion to the concept of fiction, i.e., the esistance to movement that the paticle in the

Mobility of atoms and diffusion. Einstein relation.

Mobility of atoms and diffusion. Einstein elation. In M simulation we can descibe the mobility of atoms though the mean squae displacement that can be calculated as N 1 MS ( t ( i ( t i ( 0 N The MS contains

Current, Resistance and

Cuent, Resistance and Electomotive Foce Chapte 25 Octobe 2, 2012 Octobe 2, 2012 Physics 208 1 Leaning Goals The meaning of electic cuent, and how chages move in a conducto. What is meant by esistivity

What molecular weight polymer is necessary to provide steric stabilization? = [1]

1/7 What molecula weight polyme is necessay to povide steic stabilization? The fist step is to estimate the thickness of adsobed polyme laye necessay fo steic stabilization. An appoximation is: 1 t A d

FLOW IN POROUS MEDIA WITH SLIP BOUNDARY CONDITION

SCA2007-13 1/12 FLOW IN POROUS MEDIA WITH SLIP BOUNDARY CONDITION S. Beg A. W. Cense J. P. Hofman R. M. M. Smits Shell Intenational Exploation and Poduction B.V. Kesslepak 1 2288 GS Rijswijk (Zh) The Nethelands

Final Review of AerE 243 Class

Final Review of AeE 4 Class Content of Aeodynamics I I Chapte : Review of Multivaiable Calculus Chapte : Review of Vectos Chapte : Review of Fluid Mechanics Chapte 4: Consevation Equations Chapte 5: Simplifications

Roger Pynn. Basic Introduction to Small Angle Scattering

by Roge Pynn Basic Intoduction to Small Angle Scatteing We Measue Neutons Scatteed fom a Sample Φ = numbe of incident neutons pe cm pe second σ = total numbe of neutons scatteed pe second / Φ dσ numbe

Introduction to Dielectric Properties and Magnetism

Intoduction to Dielectic opeties and Magnetism At the end of the last lectue we looked at some of the electical popeties of matte and intoduces the notions of electic field and electical conductivity.

Magnetohydrodynamics (MHD) I

Magnetohydodynamics (MHD) I Yong-Su Na National Fusion Reseach Cente POSTECH, Koea, 8-10 May, 006 Contents 1. Review Confinement & Single Paticle Motion. Plasmas as Fluids Fluid Equations 3. MHD Equations

Seepage Characteristics Of Bingham Fluid In Pores Medium

IJREA Intenational Jounal o Reseach in Engineeing & Advanced echnology, Volume, Issue 1, Feb-Ma, 215 ISSN: 22 791 (Impact Facto: 1479 wwwijeatog Seepage Chaacteistics O Bingham Fluid In Poes Medium Zheng

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects

Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the

Do not turn over until you are told to do so by the Invigilator.

UNIVERSITY OF EAST ANGLIA School of Mathematics Main Seies UG Examination 2015 16 FLUID DYNAMICS WITH ADVANCED TOPICS MTH-MD59 Time allowed: 3 Hous Attempt QUESTIONS 1 and 2, and THREE othe questions.

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M.

Magnetic Foces Biot-Savat Law Gauss s Law fo Magnetism Ampee s Law Magnetic Popeties of Mateials nductance F m qu d B d R 4 R B B µ 0 J Magnetostatics M. Magnetic Foces The electic field E at a point in

Multiphase electrokinetic coupling: Insights into the impact of fluid and charge distribution at the pore scale from a bundle of capillary tubes model

Click Hee fo Full Aticle JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 115,, doi:10.1029/2009jb007092, 2010 Multiphase electokinetic coupling: Insights into the impact of fluid and chage distibution at the poe

SIMULATION OF AUTOGENOUS AND DRYING SHRINKAGE BASED ON MICRO-PORE STRUCTURE AND INTERNAL MOISTURE STATE

SIMULATION OF AUTOGENOUS AND DRYING SHRINKAGE BASED ON MICRO-PORE STRUCTURE AND INTERNAL MOISTURE STATE Y. Luan (1), T. Ishida (1) (1) Depatment of Civil Engineeing, the Univesity of Tokyo, Japan Abstact

II. MRI Technology. B. Localized Information. Lorenz Mitschang Physikalisch-Technische Bundesanstalt, 29 th June 2009

Magnetic Resonance Imaging II. MRI Technology A. Limitations to patial Infomation B. Localized Infomation Loenz Mitschang Physikalisch-Technische Bundesanstalt, www.ptb.de 9 th June 009 A. Limitations

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

/6/4 5 Stuctue-Induced Sediment Scou ef: Eosion and Sedimentation, P.Y. Julien, 998 The Mechanics of Scou in the Maine Envionment, B.M. Sume and J. Fedsoe, Evaluating Scou at Bidges (HEC-8), E.. ichadson

Review: Electrostatics and Magnetostatics

Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion

2 Governing Equations

2 Govening Equations This chapte develops the govening equations of motion fo a homogeneous isotopic elastic solid, using the linea thee-dimensional theoy of elasticity in cylindical coodinates. At fist,

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

c 2003, Michael Marder

Expeimental Detemination of Cystal Stuctues 1 8th Januay 003 c 003, Michael Made Histoy Expeiments and theoy in 191 finally evealed locations of atoms in cystalline solids. Essential ingedients: Theoy

Basic properties of X- rays and neutrons

Basic popeties of X- ays and neutons Based on lectue notes of Sunil K. Sinha, UC San Diego, LANL J. Teixiea LLB Saclay G. Knelle, CBM Oléans/SOLEIL The photon also has wave and paticle popeties E=h! =hc/l=

Three dimensional flow analysis in Axial Flow Compressors

1 Thee dimensional flow analysis in Axial Flow Compessos 2 The ealie assumption on blade flow theoies that the flow inside the axial flow compesso annulus is two dimensional means that adial movement of

Collision Frequency of Adsorbed Particles

Bulg. J. Phys. 40 (2013) 214 218 Collision Fequency of Adsobed Paticles N.S. Peev Geogi Nadjakov Institute of Solid State Physics, Bulgaian Academy of Sciences, 72 Tzaigadsko Chaussee Blvd., 1784 Sofia,

Quantum Mechanics II

Quantum Mechanics II Pof. Bois Altshule Apil 25, 2 Lectue 25 We have been dicussing the analytic popeties of the S-matix element. Remembe the adial wave function was u kl () = R kl () e ik iπl/2 S l (k)e

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance

.615, MHD Theoy of Fusion Systems Pof. Feidbeg Lectue 4: Tooidal Equilibium and Radial Pessue Balance Basic Poblem of Tooidal Equilibium 1. Radial pessue balance. Tooidal foce balance Radial Pessue Balance

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

M.M.A HIGHER SECONDARY SCHOOL - PAPPANADU 12 TH PHYSICS - HALF YEARLY EXAM ANSWER KEY

http://www.tbtnpsc.com/07//plus-two-th-half-yealy-exam-questions-pape-answe-key-download-07.html M.M.A HIGHER SEONDARY SHOOL - PAPPANADU TH PHYSIS - HALF YEARLY EXAM ANSWER KEY 07-08 STD : XII - EM PART

Conventional Paper-I (a) Explain the concept of gradient. Determine the gradient of the given field: ( )

EE-Conventional Pape-I IES-013 www.gatefoum.com Conventional Pape-I-013 1. (a) Eplain the concept of gadient. Detemine the gadient of the given field: V ρzsin φ+ z cos φ+ρ What is polaization? In a dielectic

Advanced Subsidiary GCE (H157) Advanced GCE (H557) Physics B (Advancing Physics) Data, Formulae and Relationships Booklet

Advanced Subsidiay GCE (H57) Advanced GCE (H557) Physics B (Advancing Physics) Data, Fomulae and Relationships Booklet The infomation in this booklet is fo the use of candidates following the Advanced

Appendix B The Relativistic Transformation of Forces

Appendix B The Relativistic Tansfomation of oces B. The ou-foce We intoduced the idea of foces in Chapte 3 whee we saw that the change in the fou-momentum pe unit time is given by the expession d d w x

Characterization of Gas Flow Ability and Contribution of Diffusion to Total Mass Flux in the Shale

Reseach Jounal of Applied Sciences, Engineeing and Technology 6(9): 1663-1668, 13 ISSN: 4-7459; e-issn: 4-7467 Maxwell Scientific Oganization, 13 Submitted: Januay 19, 13 Accepted: Febuay, 13 Published:

Fields. Coulomb s Law

Coulomb s Law q t -q q 2 Electic Field Vecto valued function ligned with foce F = q E -q q 2 Supeposition of Electic Field q t -q q 2 Potential Enegy U = U() U() = q du = F d = qe d U = F = qe E d E =

1 Fundamental Solutions to the Wave Equation

1 Fundamental Solutions to the Wave Equation Physical insight in the sound geneation mechanism can be gained by consideing simple analytical solutions to the wave equation. One example is to conside acoustic

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

Eddy Currents and Magnetic Calibrations in LDX using a Copper Plasma. D.P. Boyle, PPPL M.E. Mauel, D.T. Garnier, Columbia J.

Eddy Cuents and Magneti Calibations in LDX using a Coppe Plasma D.P. Boyle PPPL M.E. Mauel D.T. Ganie Columbia J. Kesne MIT PSFC Coppe Plasma Oveview LDX Magnetis Goals Calibate magneti diagnostis positions

Adiabatic evolution of the constants of motion in resonance (I)

Adiabatic evolution of the constants of motion in esonance (I) BH Gavitational 重 力力波 waves Takahio Tanaka (YITP, Kyoto univesity) R. Fujita, S. Isoyama, H. Nakano, N. Sago PTEP 013 (013) 6, 063E01 e-pint:

10. Groundwater in geotechnical problems

. Goundwate in geotechnical poblems Goundwate plays a key ole in many geotechnical poblems. We will look at; - land subsidence - dewateing open pits - Consolidation of sediments Remembe the stoage of wate

X-ray Diffraction beyond the Kinematical Approximation

X-ay Diffaction beyond the Kinematical Appoximation Dynamical theoy of diffaction Inteaction of wave fields X-ays neutons electons with a egula lattice atomic cystal stuctues nanomete scaled multi-layes

PARTICLE TRANSPORT AND DEPOSITION IN POROUS STRUCTURES: EFFECTS OF PARTICLE PROPERTIES, POROSITY AND REYNOLDS NUMBER

ISTP-16, 2005, PRAGUE 16 TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA PARTICLE TRANSPORT AND DEPOSITION IN POROUS STRUCTURES: EFFECTS OF PARTICLE PROPERTIES, POROSITY AND REYNOLDS NUMBER S. Kuz*,

(r) = 1. Example: Electric Potential Energy. Summary. Potential due to a Group of Point Charges 9/10/12 1 R V(r) + + V(r) kq. Chapter 23.

Eample: Electic Potential Enegy What is the change in electical potential enegy of a eleased electon in the atmosphee when the electostatic foce fom the nea Eath s electic field (diected downwad) causes

Observation of Coherent OTR at LCLS. Unexpected Physics in Standard Beam Diagnostics

Obsevation of Coheent OTR at LCLS Unexpected Physics in Standad Beam Diagnostics 16 Novembe 7 Theoy Goup Meeting Henik Loos loos@slac.stanfod.edu Outline Intoduction into LCLS Injecto Coheent OTR Obsevations

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons

Electostatics IB 12 1) electic chage: 2 types of electic chage: positive and negative 2) chaging by fiction: tansfe of electons fom one object to anothe 3) positive object: lack of electons negative object:

Math 209 Assignment 9 Solutions

Math 9 Assignment 9 olutions 1. Evaluate 4y + 1 d whee is the fist octant pat of y x cut out by x + y + z 1. olution We need a paametic epesentation of the suface. (x, z). Now detemine the nomal vecto:

The geometric construction of Ewald sphere and Bragg condition:

The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in

Introduction to Accelerator Physics

Intoduction to Acceleato Physics Pat 3 Pedo Casto / Acceleato Physics Goup (MPY) Intoduction to Acceleato Physics DSY, 5th July 017 acceleating devices vacuum chambe injecto acceleating device staight

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Electomagnetic scatteing Gaduate Couse Electical Engineeing (Communications) 1 st Semeste, 1390-1391 Shaif Univesity of Technology Geneal infomation Infomation about the instucto: Instucto: Behzad Rejaei

1 Spherical multipole moments

Jackson notes 9 Spheical multipole moments Suppose we have a chage distibution ρ (x) wheeallofthechageiscontained within a spheical egion of adius R, as shown in the diagam. Then thee is no chage in the

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum

2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known

Mutual impedance between linear elements: The induced EMF method. Persa Kyritsi September 29th, 2005 FRB7, A1-104

Mutual impedance between linea elements: The induced EMF method Septembe 9th, 5 FRB7, A-4 Outline Septembe 9, 5 Reminde: self impedance nduced EMF method Nea-field of a dipole Self impedance vs. Mutual

EXAM NMR (8N090) November , am

EXA NR (8N9) Novembe 5 9, 9. 1. am Remaks: 1. The exam consists of 8 questions, each with 3 pats.. Each question yields the same amount of points. 3. You ae allowed to use the fomula sheet which has been

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

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

ANTNNAS Vecto and Scala Potentials Maxwell's quations jωb J + jωd D ρ B (M) (M) (M3) (M4) D ε B Fo a linea, homogeneous, isotopic medium and ε ae contant. Since B, thee exists a vecto A such that B A and

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

06 - ROTATIONAL MOTION Page ) A body A of mass M while falling vetically downwads unde gavity beaks into two pats, a body B of mass ( / ) M and a body C of mass ( / ) M. The cente of mass of bodies B and

Dynamic Simulation of Electromagnets. European COMSOL Conference. 5 November 2008

Pesented at the COMSOL Confeence 28 Hannove Dynamic Simulation of Electomagnets Euopean COMSOL Confeence 5 Novembe 28 1 / D. Haald Bille / pinted 21 Octobe 28 Continental AG Contents 1. Electonic bake

V7: Diffusional association of proteins and Brownian dynamics simulations

V7: Diffusional association of poteins and Bownian dynamics simulations Bownian motion The paticle movement was discoveed by Robet Bown in 1827 and was intepeted coectly fist by W. Ramsay in 1876. Exact

Today in Astronomy 142: the Milky Way s disk

Today in Astonomy 14: the Milky Way s disk Moe on stas as a gas: stella elaxation time, equilibium Diffeential otation of the stas in the disk The local standad of est Rotation cuves and the distibution

Physics 235 Chapter 5. Chapter 5 Gravitation

Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus

Pulse Neutron Neutron (PNN) tool logging for porosity

Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Hotwell Handelsges.m.b.H Oedenbuge Stasse 6 7013 Klingenbach, AUSTRIA Tel.: +43 (0) 687-48058 Fax: +43 (0) 687 48059 office@hotwell.at

Pore pressure coefficient for soil and rock and its relation to compressional wave velocity

Title Poe pessue coefficient fo soil and ock and its elation to compessional wave velocity Autho(s) Yang, J Citation Geotechnique, 25, v. 55 n. 3, p. 25-256 Issued Date 25 URL http://hdl.handle.net/722/739

Curvature singularity

Cuvatue singulaity We wish to show that thee is a cuvatue singulaity at 0 of the Schwazschild solution. We cannot use eithe of the invaiantsr o R ab R ab since both the Ricci tenso and the Ricci scala

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006

1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and

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

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

Roger Pynn. Lectures 8: Magnetic Scattering of Neutrons

by oge Pynn Lectues 8: agnetic Scatteing of Neutons This Lectue agnetic scatteing of neutons agnetic popeties of the neuton agnetic scatteing of neutons Scatteing by unpaied electons Effect of magnetic

Enabling Erosion and Dishing Measurements with Electrical Test in Copper Damascene Process

Enabling Eosion and Dishing Measuements with Electical Test in Coppe Damascene Pocess SFR okshop & Review ovembe 4th, 00 Runzi Chang and Costas Spanos Bekele, CA 00 GOAL: to demonstate the feasibilit of

Repetition: Structure Zone Models

Repetition: Stuctue Zone Models Repetition: Film Gowth Mechanisms Zone Mechanism Cha. eatue : T/T M

Micro-bunching: Longitudinal Bunch Profile Measurements at TTF

Shot Pulses in Rings Mico-bunching: Longitudinal Bunch Pofile Measuements at TTF ) The time vaying fields in a tansvese mode cavity kick the font of a bunch up, and the back of the bunch don. ) A betaton

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM

Honou School of Mathematical and Theoetical Physics Pat C Maste of Science in Mathematical and Theoetical Physics COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM HILARY TERM 18 TUESDAY, 13TH MARCH 18, 1noon

Optics for Soft X-ray Seeding of LCLS-II - Grating and Mirrors

FLS ICFA Beam Dynamic Wokshop SLAC National Acceleato Laboatoy Menlo Pak, CA Optics fo Soft X-ay Seeding of LCLS-II - Gating and Mios Y. Feng, J. Wu, M. owen, P. Heimann, J. Kywinski, J. Hastings, et al.

A thermodynamic degree of freedom solution to the galaxy cluster problem of MOND. Abstract

A themodynamic degee of feedom solution to the galaxy cluste poblem of MOND E.P.J. de Haas (Paul) Nijmegen, The Nethelands (Dated: Octobe 23, 2015) Abstact In this pape I discus the degee of feedom paamete

TUTORIAL 9. Static magnetic field

TUTOIAL 9 Static magnetic field Vecto magnetic potential Null Identity % & %$ A # Fist postulation # " B such that: Vecto magnetic potential Vecto Poisson s equation The solution is: " Substitute it into

Lecture 8: The El Niño Phenomenon (continued)

Lectue 8: The El Niño Phenomenon (continued) Henk A. Dijksta; notes by Floence Macotte & Cesa Rocha June 24, 2015 1 Deteministic Chaos So fa we have seen that the oscillatoy behavio of El Nino Southen

Foundations of Chemical Kinetics. Lecture 9: Generalizing collision theory

Foundations of Chemical Kinetics Lectue 9: Genealizing collision theoy Mac R. Roussel Depatment of Chemisty and Biochemisty Spheical pola coodinates z θ φ y x Angles and solid angles θ a A Ω θ=a/ unit:

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

Introduction to Nuclear Forces

Intoduction to Nuclea Foces One of the main poblems of nuclea physics is to find out the natue of nuclea foces. Nuclea foces diffe fom all othe known types of foces. They cannot be of electical oigin since

Electric Charge and Field

lectic Chage and ield Chapte 6 (Giancoli) All sections ecept 6.0 (Gauss s law) Compaison between the lectic and the Gavitational foces Both have long ange, The electic chage of an object plas the same

General Railgun Function

Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

Skin Effect and Formation Damage

Well Stimulation and Sand Poduction Management (PGE 489 ) Sin Effect and Fomation Damage By D. Moammed A. Kami 02-02-2016 Sin Facto A fomation damage model i a dynamic elationip expeing te fluid tanpot

Chapter 4. Newton s Laws of Motion

Chapte 4 Newton s Laws of Motion 4.1 Foces and Inteactions A foce is a push o a pull. It is that which causes an object to acceleate. The unit of foce in the metic system is the Newton. Foce is a vecto

Experiment I Voltage Variation and Control

ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly

A MICRODISCHARGE BASED PRESURE SENSOR*

A MICRODISCHARGE BASED PRESURE SENSOR* Jun-Chieh Wang a), Zhongmin Xiong a), Chistine Eun a), Xin Luo a), Yogesh Gianchandani a) and Mak J. Kushne a) a), Ann Abo, MI 48109 USA unchwan@umich.edu, zxiong@umich.edu,

Lecture 24 Stability of Molecular Clouds

Lectue 4 Stability of Molecula Clouds 1. Stability of Cloud Coes. Collapse and Fagmentation of Clouds 3. Applying the iial Theoem Refeences Oigins of Stas & Planetay Systems eds. Lada & Kylafis http://cfa-www.havad.edu/cete

18.1 Origin of Electricity 18.2 Charged Objects and Electric Force

1 18.1 Oigin of lecticity 18. Chaged Objects and lectic Foce Thee ae two kinds of electic chage: positive and negative. The SI unit of electic chage is the coulomb (C). The magnitude of the chage on an

Analytical calculation of the power dissipated in the LHC liner. Stefano De Santis - LBNL and Andrea Mostacci - CERN

Analytical calculation of the powe dissipated in the LHC line Stefano De Santis - LBNL and Andea Mostacci - CERN Contents What is the Modified Bethe s Diffaction Theoy? Some inteesting consequences of

From Atoms to Materials: Predictive Theory and Simulations. Materials are everywhere

Fom Atoms to Mateials: Pedictive Theoy and Simulations Intoduction Ale Stachan stachan@pudue.edu School of Mateials Engineeing & Bick Nanotechnology Cente Pudue Univesity West Lafayette, Indiana USA Mateials

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics

AE301 Aeodynamics I UNIT B: Theoy of Aeodynamics ROAD MAP... B-1: Mathematics fo Aeodynamics B-2: Flow Field Repesentations B-3: Potential Flow Analysis B-4: Applications of Potential Flow Analysis AE301

seventeen steel construction: columns & tension members ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2014 lecture

ARCHITECTURAL STRUCTURES: ORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS Co-Ten Steel Sculptue By Richad Sea Museum of Moden At ot Woth, TX (AISC - Steel Stuctues of the Eveyday) SUMMER 2014 lectue seventeen

Circular Motion. Mr. Velazquez AP/Honors Physics

Cicula Motion M. Velazquez AP/Honos Physics Objects in Cicula Motion Accoding to Newton s Laws, if no foce acts on an object, it will move with constant speed in a constant diection. Theefoe, if an object

University of Illinois at Chicago Department of Physics. Electricity & Magnetism Qualifying Examination

E&M poblems Univesity of Illinois at Chicago Depatment of Physics Electicity & Magnetism Qualifying Examination Januay 3, 6 9. am : pm Full cedit can be achieved fom completely coect answes to 4 questions.

Look over Chapter 22 sections 1-8 Examples 2, 4, 5, Look over Chapter 16 sections 7-9 examples 6, 7, 8, 9. Things To Know 1/22/2008 PHYS 2212

PHYS 1 Look ove Chapte sections 1-8 xamples, 4, 5, PHYS 111 Look ove Chapte 16 sections 7-9 examples 6, 7, 8, 9 Things To Know 1) What is an lectic field. ) How to calculate the electic field fo a point

Newton s Laws, Kepler s Laws, and Planetary Orbits

Newton s Laws, Keple s Laws, and Planetay Obits PROBLEM SET 4 DUE TUESDAY AT START OF LECTURE 28 Septembe 2017 ASTRONOMY 111 FALL 2017 1 Newton s & Keple s laws and planetay obits Unifom cicula motion

Section 11. Timescales Radiation transport in stars

Section 11 Timescales 11.1 Radiation tanspot in stas Deep inside stas the adiation eld is vey close to black body. Fo a black-body distibution the photon numbe density at tempeatue T is given by n = 2

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

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy

Fascati Physics Seies Vol. X (998), pp. 47-54 4 th Advanced ICFA Beam Dynamics Wokshop, Fascati, Oct. -5, 997 EFFECTS OF FRININ FIELDS ON SINLE PARTICLE DYNAMICS M. Bassetti and C. Biscai INFN-LNF, CP

Thermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850)

emal-fluids I Capte 7 Steady eat conduction D. Pimal Fenando pimal@eng.fsu.edu P: (850 40-633 Steady eat conduction Hee we conside one dimensional steady eat conduction. We conside eat tansfe in a plane

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq