Theory of Spatial Problems

Similar documents
Path (space curve) Osculating plane

E. Computation of Permanent Magnetic Fields

Elastic Analysis of Pavement Structure with Application of Vertical and Centripetal Surface Forces

Self-Adjusting Top Trees

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören

Lecture 35. Diffraction and Aperture Antennas

Accretion disks around rotating black holes. (c)2017 van Putten 1

Chapter 4 Circular and Curvilinear Motions

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

be two non-empty sets. Then S is called a semigroup if it satisfies the conditions

Acoustics and electroacoustics

PAVEMENT DESIGN AND EVALUATION

spring from 1 cm to 2 cm is given by

Part II, Measures Other Than Conversion I. Apr/ Spring 1

ELEC 351 Notes Set #18

1 Using Integration to Find Arc Lengths and Surface Areas

AP Calculus AB Exam Review Sheet B - Session 1

Instructions for Section 1

CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7

E F. and H v. or A r and F r are dual of each other.

Study Material with Classroom Practice solutions. To Electromagnetic Theory CONTENTS. 01 Static Fields Maxwell Equations & EM Waves 06 11

Electric Potential. and Equipotentials

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

CONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections

1. Given the longitudinal equations of motion of an aircraft in the following format,

, MATHS H.O.D.: SUHAG R.KARIYA, BHOPAL, CONIC SECTION PART 8 OF

Physics 604 Problem Set 1 Due Sept 16, 2010

Electric Potential ANSWERS TO QUESTIONS

PEP 332: Mathematical Methods for Physicists. Math Methods (Hassani 2009) Ch 15 Applied Vector Analysis. (1) E = ρ ϵ 0 ; (2) B =0; (3) E = B (1) ; (2)

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

We are looking for ways to compute the integral of a function f(x), f(x)dx.

Physics 1502: Lecture 2 Today s Agenda

Section 35 SHM and Circular Motion

8 - GRAVITATION Page 1

Modern Channel Coding

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9

CHAPTER TWO MULTIPLE INTEGRAL

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

4.2 Boussinesq s Theory. Contents

FSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, *

TOPIC 5: INTEGRATION

Solution Set 2. y z. + j. u + j

Estimation of a Random Variable

Lecture 4. Conic section

ChE 548 Final Exam Spring, 2004

Differential Equations

Physics 240: Worksheet 15 Name

Figure 1: Schematic of a fluid element used for deriving the energy equation.

Elementary Linear Algebra

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

Suggested t-z and q-z functions for load-movement responsef

Physics 11b Lecture #11

Ch 1.2: Solutions of Some Differential Equations

, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x,

TMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont.

Elliptical motion, gravity, etc

Chapter 3 Higher Order Linear ODEs

Chapter 7 Electrodynamics

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4

θ θ φ EN2210: Continuum Mechanics Homework 2: Polar and Curvilinear Coordinates, Kinematics Solutions 1. The for the vector i , calculate:

ROTATION IN 3D WORLD RIGID BODY MOTION

Lecture 5. Differential Analysis of Fluid Flow Navier-Stockes equation

Concept of Stress at a Point

Problem set 5: Solutions Math 207B, Winter r(x)u(x)v(x) dx.

3.4 Repeated Roots; Reduction of Order

Mathematical Reflections, Issue 5, INEQUALITIES ON RATIOS OF RADII OF TANGENT CIRCLES. Y.N. Aliyev

This immediately suggests an inverse-square law for a "piece" of current along the line.

Lecture 11: Potential Gradient and Capacitor Review:

CSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions

( ) ( ) (a) w(x) = a v(x) + b. (b) w(x) = a v(x + b) w = the system IS linear. (1) output as the sum of the outputs from each signal individually

The Derivative of the Natural Logarithmic Function. Derivative of the Natural Exponential Function. Let u be a differentiable function of x.

Free vibration of a magneto-electro-elastic toroidal shell

Section - 2 MORE PROPERTIES

Winter 2016 COMP-250: Introduction to Computer Science. Lecture 23, April 5, 2016

INFLUENCE OF ANTICLIMBING DEVICE ON THE VARIATION OF LOADS ON WHEELS IN DIESEL ELECTRIC 4000 HP

U>, and is negative. Electric Potential Energy

Equations from Relativistic Transverse Doppler Effect. The Complete Correlation of the Lorentz Effect to the Doppler Effect in Relativistic Physics

Electricity and Magnetism Electric Dipole Continuous Distribution of Charge

GUC (Dr. Hany Hammad)

Department of Mathematics. Birla Institute of Technology, Mesra, Ranchi MA 2201(Advanced Engg. Mathematics) Session: Tutorial Sheet No.

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468

GRAVITATION 4) R. max. 2 ..(1) ...(2)

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals

:9 :9. Public Water Crossings - DE NORTHERN PASS PROJECT. Ashland. Bridgewater

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

Dynamically Equivalent Systems. Dynamically Equivalent Systems. Dynamically Equivalent Systems. ME 201 Mechanics of Machines

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA

Two dimensional polar coordinate system in airy stress functions

Section 3: Antiderivatives of Formulas

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

Solutions to Midterm Physics 201

CDS 101/110: Lecture 7.1 Loop Analysis of Feedback Systems

Compact Guide Cylinder with One-way Lock Series MLGP ø40, ø50, ø63. Prevents dropping when air supply pressure falls or residual pressure is exhausted

Transcription:

Chpt 7 ho of Sptil Polms 7. Diffntil tions of iliim (-D) Z Y X Inol si nknon stss componnts:. 7-

7. Stt of Stss t Point t n sfc ith otd noml N th sfc componnts ltd to (dtmind ) th 6 stss componnts X N l m n Y N m n l > Z N n l m Bond condition: X N Y N Z N plcd th cosponding ond sfc foc componnts X Y Z h 6 stss componnts compltl dfin th stss stt t point. Pincipl Stsss nd Pincipl Diction Whn Mimm nd Minimm Stsss 7-

7. omticl tions displcmnt fo o stin igid-od displcmnts lt s tk h cosponding displcmnt componnts cn pssd s ω ω ω ω ω ω o o o th igid-od tnsltions nd ω ω ω th igid-od ottions ot th coodint s. Volm stin chng of olm p nit of th oiginl olm 7-

i.. V V ( )( )( ) 7.5 Phsicl tions fo n isotopic nd pfctl lstic od Hook s l [ ( )] ( ) [ ( )] [ ( )] ( ) ( ) if thn h i.. th coincidnc of Pincipl dictions of stss ith Pincipl dictions of stin (thml stss o thml stin contition). m m ( ) ( ) ( ) ( ) K m K lk modls (lts olm stin nd olm stss) o sm p th 5 nknon fnctions in sptil polm: stss(6) stin(6) displcmnt(). h shold stisf 5 tions: iliim() gomticl(6) phsicl(6). 7-4

displcmnt ond conditions on th sfc: 7.6 il smmt nd sphicl smmt. il smmt: if th gomticl shp of th od concnd th condition of constint nd th tnl lods ll smmticl ith spct to n pln pssing thogh ctin is thn th stss stin nd displcmnt componnts ill h th sm condition of smmt il smmt polm in spc. clindicl coodints th stss stin nd displcmnt componnts ill fnctions of onl to coodints: nd. <> stss componnts: θ. <> od focs K nd Z in nd dictions <> stin componnts: θ nd <4> displcmnts: θ. 7-5

iliim tions: Z K θ omticl tions θ Phsicl tions [ ] [ ] [ ]. θ θ θ θ Bond conditions <> displcmnt <> stss 7-6

Sphicl smmt (o point smmt): shp of th od th condition of constint nd tnl lod ll smmticl ith spct to n pln pssing thogh ctin point. h stss stin nd displcmnts ill fnctions of singl il th distnc fom th point of smmt. idntl sch condition ists onl in solid o hollo sphs. d <> tion of iliim: ( ) K d <> gomticl tions: d d <> phsicl tions: [ ( )] ( ) [ ( )] [( ) ] h cosponding stss componnts ( ) d d d. d 7-7

7.7 Soltion in tms of displcmnts In tms of displcmnt th diffntil tions nd to sol :. Z Y X h Bond conditions: Fo th spcil cs of ismmtic polms. Z K h. Fo th spcil cs of sphicl smmt onl on nknon fnction K d d d d 7-8

7.8 Infinit lstic L Und it nd Unifom Pss Consid n lstic l of infinit tnt nd nifom thicknss hich is fid t its lo sfc nd sjctd to nifom pss of intnsit on its pp sfc ith pln in th pp sfc. h od foc componnts X Y Zρg ρ is th dnsit of th l. W s th smi-ins mthod nd ssm tht: cs of smmt th displcmnt t n point in th l is ticl nd dpnds on onl: () hs h d d d d h diffntil tions fo displcmnts coms: ( ) d d d ρg d Fom hich h d d ( )( ) ( ) ρg 7-9

intgtion h B g g d d ρ ρ B it constnts. g g ρ ρ Stss ond condition: (- ) /(ρg) Displcmnt ond condition: h g h g B ρ ρ So finll h:. h g h g g ρ ρ ρ W cn s: m nd ls h th ltion - cofficint of ltl pss 7-

ht is th slts in pln stss condition? Pln stin? 7-

7.9 Hollo Sph Sjctd to Unifom Pss Consid hollo sph ith inn dis nd ot dis sjctd to nifom pss of intnsit nd on th inn nd ot sfcs spctil h od focs not considd th iliim tion coms d d d d fom hich h B stss componnts: B B ond conditions B hs:. 7-

If nd (onl ot pss ll) If (onl intnl pss) ht is th mimm tnsil stss? If th ond condition is gin inn nd ot displcmnt dtmin th stss fild. 7. Displcmnt Fnctions nd Displcmnt Potntil Intodc displcmnt fnctions to pss th displcmnt componnts Whn od focs nglctd th sic iliim tions in tms of displcmnts com No ssm tht th displcmnt might h potntil i.. th displcmnt componnt in n diction is popotionl to th diti of ctin potntil fnction ( ) ths fth h Sstitting nd o into iliim tions cn s tht mst stisf: 7-

his is tht C. C is n it constnt. hs n fnction stisfing o tion m tkn s displcmnt potntil fom hich displcmnt componnts otind. Whn tk C h thn coms hmonic fnction. In this cs h nd th stss componnts in tms of :. h displcmnt componnts nd stss componnts shold stisf ll th ond conditions. In th spcil cs of il smmt hn od focs nglctd th iliim tions com h Simill tk [ ] thn h 7-4

mst stisf: hich ild C gin. h cosponding stss componnts :. θ W not tht is constnt thoghot th od concnd so th ppliction is limitd sinc constnt l occ. Lo s Displcmnt Fnction Fo th soltion of ismmtic sptil polms.. H. Lo intodcd displcmnt fnction ζ nd pssd th displcmnt componnts s: ζ ζ h nd olm stin is ζ ith nd th fist tion of iliim is idnticll stisfid nd th scond tion is tht 4 ζi.. ζ mst ihmonic fnction. h cosponding stss componnts. ζ ζ ζ ζ θ 7-5

hs n ismmtic polm cn sold if sccd in finding pop ihmonic fnction ζ so tht th otind displcmnt componnts nd stss componnts stisf th ond condition. Concnttd Noml Lod on Bond of Smi-infinit Bod. Consid concnttd noml lod P on th ond pln. idntl this is n ismmtic polm. h ond conditions :. t n hoiontl pln sction t distnc fom th ond pln h dditionll ( πd) P. nd const. W t to s Lo s displcmnt fnction. ccoding to dimnsionl nlsis th pssion fo stss mst P diidd dtic tms of th lin ntitis nd. h displcmnt fnction ζ mst P mltiplid lin tms of nd. No W ssm ζ to podct of constnt (ith th dimnsion of foc) nd th ihmonic fnction : ζ ths h 7-6

. 4 5 5 5 θ 7-7

h ond condition of is stisfid t tht of is not sinc ( ) dos not nish fo ll ls of. hs t to find noth hmonic fnction s displcmnt potntil (not th Lo s fnction) hich ill gi nd cncl ot th o non-o sh stss on th ond. ft sl tils find tht th hmonic fnction ln( ) flfills th imnt tk ln( ) h ln() is non-dimnsionl fnction is n it constnt (ith dimnsion of foc) th cosponding displcmnt nd stss componnts : ( Z) θ ( ) ( ). ft spposition ith th fist soltion cn s tht is stisfid nd th condition coms: ( ) i.. ( ). (*) h condition ( πd) P coms: Fom (*) nd (**) otin 4π(-) π P (**) P ( ) P π π 7-8

h finl soltions ( J. Bonssins (878)) :. P ) ( ) ( ) ( ) ( 5 5 P P P P P π π π π π π θ 7-9