Theory of Spatial Problems

Size: px
Start display at page:

Download "Theory of Spatial Problems"

Transcription

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

2 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-

3 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-

4 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

5 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

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

7 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

8 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

9 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

10 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-

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

12 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-

13 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-

14 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

15 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

16 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

17 θ 7-7

18 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

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

Path (space curve) Osculating plane

Path (space curve) Osculating plane Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions

More information

E. Computation of Permanent Magnetic Fields

E. Computation of Permanent Magnetic Fields E. Computtion of Pmnnt Mgntic Filds Th following pssgs should giv n impssion, how pmnnt mgnts cn b clcultd in spct of thi fild distibution. This ovviw ctinl cnnot cov ll subjcts. It will ml intoduc th

More information

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

Elastic Analysis of Pavement Structure with Application of Vertical and Centripetal Surface Forces Elstic nlysis of Pvmnt Stct with ppliction of Vticl nd ntiptl Sfc Focs Min. W. SIR ilt Envionmnt Ptoi Soth fic Fjinmi K. & Mtsi K. ptmnt of ivil nd Envionmntl Engining Tokyo nki Univsity Sitm pn Tkmi Ino

More information

Self-Adjusting Top Trees

Self-Adjusting Top Trees Th Polm Sl-jsting Top Ts ynmi ts: ol: mintin n n-tx ost tht hngs o tim. link(,w): ts n g twn tis n w. t(,w): lts g (,w). pplition-spii t ssoit with gs n/o tis. ont xmpls: in minimm-wight g in th pth twn

More information

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

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8. PH67 WINTER 5 Poblm St # Mad, hapt, poblm # 6 Hint: Th tight-binding band function fo an fcc cstal is ( U t cos( a / cos( a / cos( a / cos( a / cos( a / cos( a / ε [ ] (a Th tight-binding Hamiltonian (85

More information

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

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(

More information

Lecture 35. Diffraction and Aperture Antennas

Lecture 35. Diffraction and Aperture Antennas ctu 35 Dictin nd ptu ntnns In this lctu u will ln: Dictin f lctmgntic ditin Gin nd ditin pttn f ptu ntnns C 303 Fll 005 Fhn Rn Cnll Univsit Dictin nd ptu ntnns ptu ntnn usull fs t (mtllic) sht with hl

More information

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

Accretion disks around rotating black holes. (c)2017 van Putten 1 Acction disks ond otting blck hols (c)07 vn Pttn Contnts Bod X-spctm of ion-lins fom n inn cction disk Spcil Rltivity: Doppl shifts nd ltivistic bming Gnl Rltivity: Rdshift nd fm-dgging Inn ost Stbl Cicl

More information

Chapter 4 Circular and Curvilinear Motions

Chapter 4 Circular and Curvilinear Motions Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion

More information

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)

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) An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...

More information

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

be two non-empty sets. Then S is called a semigroup if it satisfies the conditions UZZY SOT GMM EGU SEMIGOUPS V. Chinndi* & K. lmozhi** * ssocit Pofsso Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd ** Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd bstct: In this w hv discssd bot th

More information

Acoustics and electroacoustics

Acoustics and electroacoustics coustics and lctoacoustics Chapt : Sound soucs and adiation ELEN78 - Chapt - 3 Quantitis units and smbols: f Hz : fqunc of an acoustical wav pu ton T s : piod = /f m : wavlngth= c/f Sound pssu a : pzt

More information

PAVEMENT DESIGN AND EVALUATION

PAVEMENT DESIGN AND EVALUATION THE REQUIRED MATHEMATICS AND ITS APPLICATIONS F. Vn Cuwlt Edito: Mc Stt Fdtion of th Blgin Cmnt Industy B-7 Bussls, Ru Volt 9. i ii INTRODUCTION Pvmnt Dsign nd Evlution: Th Rquid Mthmtics nd Its Applictions

More information

spring from 1 cm to 2 cm is given by

spring from 1 cm to 2 cm is given by Problem [8 pts] Tre or Flse. Give brief explntion or exmple to jstify yor nswer. ) [ pts] Given solid generted by revolving region bot the line x, if we re sing the shell method to compte its volme, then

More information

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

Part II, Measures Other Than Conversion I. Apr/ Spring 1 Pt II, Msus Oth hn onvsion I p/7 11 Sping 1 Pt II, Msus Oth hn onvsion II p/7 11 Sping . pplictions/exmpls of th RE lgoithm I Gs Phs Elmnty Rction dditionl Infomtion Only fd P = 8. tm = 5 K =. mol/dm 3

More information

ELEC 351 Notes Set #18

ELEC 351 Notes Set #18 Assignmnt #8 Poblm 9. Poblm 9.7 Poblm 9. Poblm 9.3 Poblm 9.4 LC 35 Nots St #8 Antnns gin nd fficincy Antnns dipol ntnn Hlf wv dipol Fiis tnsmission qution Fiis tnsmission qution Do this ssignmnt by Novmb

More information

1 Using Integration to Find Arc Lengths and Surface Areas

1 Using Integration to Find Arc Lengths and Surface Areas Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s

More information

AP Calculus AB Exam Review Sheet B - Session 1

AP Calculus AB Exam Review Sheet B - Session 1 AP Clcls AB Em Review Sheet B - Session Nme: AP 998 # Let e the nction given y e.. Find lim nd lim.. Find the solte minimm vle o. Jstiy tht yo nswe is n solte minimm. c. Wht is the nge o? d. Conside the

More information

Instructions for Section 1

Instructions for Section 1 Instructions for Sction 1 Choos th rspons tht is corrct for th qustion. A corrct nswr scors 1, n incorrct nswr scors 0. Mrks will not b dductd for incorrct nswrs. You should ttmpt vry qustion. No mrks

More information

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

CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7 CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr

More information

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

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

More information

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

Study Material with Classroom Practice solutions. To Electromagnetic Theory CONTENTS. 01 Static Fields Maxwell Equations & EM Waves 06 11 Pg No. Stud Mtil with lssoom Pctic solutions To lctomgntic Tho ONTNTS hpt No. Nm of th hpt Pg No. Sttic Filds 5 Mwll qutions & M Wvs 6 Tnsmission ins Wvguids 5 6 5 lmnts of ntnns 7 hpt. ns: V cos cos î

More information

Electric Potential. and Equipotentials

Electric Potential. and Equipotentials Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil

More information

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

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque

More information

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

CONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections Conic Sctions 16 MODULE-IV Co-ordint CONIC SECTIONS Whil cutting crrot ou might hv noticd diffrnt shps shown th dgs of th cut. Anlticll ou m cut it in thr diffrnt ws, nml (i) (ii) (iii) Cut is prlll to

More information

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

1. Given the longitudinal equations of motion of an aircraft in the following format, Cht 4. Gin th lnitdinl tins f tin f n icft in th fllin ft, U cs W (4. n th in dinlss f fd t ind s. Discss th lti its f th tins f tin in dinl, dinlss nd cncis fs. Ans f it is ssd tht th icft is in ll fliht,

More information

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

, MATHS H.O.D.: SUHAG R.KARIYA, BHOPAL, CONIC SECTION PART 8 OF DOWNLOAD FREE FROM www.tekoclsses.com, PH.: 0 903 903 7779, 98930 5888 Some questions (Assertion Reson tpe) re given elow. Ech question contins Sttement (Assertion) nd Sttement (Reson). Ech question hs

More information

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 604 Problem Set 1 Due Sept 16, 2010 Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside

More information

Electric Potential ANSWERS TO QUESTIONS

Electric Potential ANSWERS TO QUESTIONS 5 Elctic Potntil CHAPTE UTNE 5 Potntil Dinc nd Elctic Potntil 5 Potntil Dinc in Uniom Elctic ild 5 Elctic Potntil nd Potntil Eny Du to Point Chs 5 tinin th lu o th Elctic ild om th Elctic Potntil 55 Elctic

More information

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)

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) PEP 33: Mmticl Mthods fo Phsicts Mth Mthods (Hsni 9 Ch 5 pplid c nls doul dl options mgntic multipols plcin s ( E d Q ϵ ; ( d ; (3 C E d dφ m dt ; (4 C d µ I ( E ρ ϵ ; ( ; (3 E ; (4 µ J µ ϵ E Φ( (53 ov

More information

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:

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: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

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

We are looking for ways to compute the integral of a function f(x), f(x)dx. INTEGRATION TECHNIQUES Introdction We re looking for wys to compte the integrl of fnction f(x), f(x)dx. To pt it simply, wht we need to do is find fnction F (x) sch tht F (x) = f(x). Then if the integrl

More information

Physics 1502: Lecture 2 Today s Agenda

Physics 1502: Lecture 2 Today s Agenda 1 Lectue 1 Phsics 1502: Lectue 2 Tod s Agend Announcements: Lectues posted on: www.phs.uconn.edu/~cote/ HW ssignments, solutions etc. Homewok #1: On Mstephsics this Fid Homewoks posted on Msteingphsics

More information

Section 35 SHM and Circular Motion

Section 35 SHM and Circular Motion Section 35 SHM nd Cicul Motion Phsics 204A Clss Notes Wht do objects do? nd Wh do the do it? Objects sometimes oscillte in simple hmonic motion. In the lst section we looed t mss ibting t the end of sping.

More information

8 - GRAVITATION Page 1

8 - GRAVITATION Page 1 8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving

More information

Modern Channel Coding

Modern Channel Coding Modrn Chnnl Coding Ingmr Lnd & Joss Sir Lctr 4: EXIT Chrts ACoRN Smmr School 27 Itrti Dcoding How dos th mtl informtion ol in n itrti dcoding lgorithm? W h lrnd tht it is possibl to optimiz LDPC cods so

More information

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

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

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

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9 Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:

More information

CHAPTER TWO MULTIPLE INTEGRAL

CHAPTER TWO MULTIPLE INTEGRAL CHAPTE TWO MULTIPLE INTEGAL Aft complting ths tutoils, stunts shoul b bl to: vlut th oubl intgl ov th givn ctngul gion fin th volum of th soli boun b th plns fin th of th gion boun b th cuvs ug oubl intgl

More information

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

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

4.2 Boussinesq s Theory. Contents

4.2 Boussinesq s Theory. Contents 00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte

More information

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

FSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, * CmSc 365 Thory of Computtion Finit Stt Automt nd Rgulr Exprssions (Chptr 2, Sction 2.3) ALPHABET oprtions: U, conctntion, * otin otin Strings Form Rgulr xprssions dscri Closd undr U, conctntion nd * (if

More information

TOPIC 5: INTEGRATION

TOPIC 5: INTEGRATION TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function

More information

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

Solution Set 2. y z. + j. u + j Soltion Set 2. Review of Div, Grd nd Crl. Prove:. () ( A) =, where A is ny three dimensionl vector field. i j k ( Az A = y z = i A A y A z y A ) ( y A + j z z A ) ( z Ay + k A ) y ( A) = ( Az y A ) y +

More information

Estimation of a Random Variable

Estimation of a Random Variable Estimation of a andom Vaiabl Obsv and stimat. ˆ is an stimat of. ζ : outcom Estimation ul ˆ Sampl Spac Eampl: : Pson s Hight, : Wight. : Ailin Company s Stock Pic, : Cud Oil Pic. Cost of Estimation Eo

More information

Lecture 4. Conic section

Lecture 4. Conic section Lctur 4 Conic sction Conic sctions r locus of points whr distncs from fixd point nd fixd lin r in constnt rtio. Conic sctions in D r curvs which r locus of points whor position vctor r stisfis r r. whr

More information

ChE 548 Final Exam Spring, 2004

ChE 548 Final Exam Spring, 2004 . Keffer, eprtment of Chemil Engineering, University of ennessee ChE 58 Finl Em Spring, Problem. Consider single-omponent, inompressible flid moving down n ninslted fnnel. erive the energy blne for this

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

Physics 240: Worksheet 15 Name

Physics 240: Worksheet 15 Name Physics 40: Woksht 15 Nam Each of ths poblms inol physics in an acclatd fam of fnc Althouh you mind wants to ty to foc you to wok ths poblms insid th acclatd fnc fam (i.. th so-calld "won way" by som popl),

More information

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

Figure 1: Schematic of a fluid element used for deriving the energy equation. Driation of th Enrg Eation ME 7710 Enironmntal Flid Dnamics Spring 01 This driation follos closl from Bird, Start and Lightfoot (1960) bt has bn tndd to incld radiation and phas chang. W can rit th 1 st

More information

Elementary Linear Algebra

Elementary Linear Algebra Elementry Liner Algebr Anton & Rorres, 9 th Edition Lectre Set Chpter : Vectors in -Spce nd -Spce Chpter Content Introdction to Vectors (Geometric Norm of Vector; Vector Arithmetic Dot Prodct; Projections

More information

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

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture: Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin

More information

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

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept

More information

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

Suggested t-z and q-z functions for load-movement responsef 40 Rtio (Exponent = 0.5 80 % Fnction (.5 times 0 Hypeolic ( = 0 % SHAFT SHEAR (% of lt 00 80 60 ULT Zhng = 0.0083 / = 50 % Exponentil (e = 0.45 80 % (stin-softening 40 0 0 0 5 0 5 0 5 RELATIVE MOVEMENT

More information

Physics 11b Lecture #11

Physics 11b Lecture #11 Physics 11b Lectue #11 Mgnetic Fields Souces of the Mgnetic Field S&J Chpte 9, 3 Wht We Did Lst Time Mgnetic fields e simil to electic fields Only diffeence: no single mgnetic pole Loentz foce Moving chge

More information

Ch 1.2: Solutions of Some Differential Equations

Ch 1.2: Solutions of Some Differential Equations Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of

More information

, 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,

, 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, Clculus for Businss nd Socil Scincs - Prof D Yun Finl Em Rviw vrsion 5/9/7 Chck wbsit for ny postd typos nd updts Pls rport ny typos This rviw sht contins summris of nw topics only (This rviw sht dos hv

More information

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

TMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont. Lctr 8; ntrodctor 2-dimnsional lastostatics; cont. (modifid 23--3) ntrodctor 2-dimnsional lastostatics; cont. W will now contin or std of 2-dim. lastostatics, and focs on a somwhat mor adancd lmnt thn

More information

Elliptical motion, gravity, etc

Elliptical motion, gravity, etc FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs

More information

Chapter 3 Higher Order Linear ODEs

Chapter 3 Higher Order Linear ODEs ht High Od i ODEs. Hoogous i ODEs A li qutio: is lld ohoogous. is lld hoogous. Tho. Sus d ostt ultils of solutios of o so o itvl I gi solutios of o I. Dfiitio. futios lld lil iddt o so itvl I if th qutio

More information

Chapter 7 Electrodynamics

Chapter 7 Electrodynamics Cpt 7 Elctonics 7. Elctootiv Foc 7.. O s Lw Cunt Dnsity: ( n ) q ( n l) Q q qnv Fo lcton: n( )v nd d qnv Fo ost sustncs, t cunt dnsity is popotionl to t foc p unit cg: F ( E + v B) q. : conductivity, pfct

More information

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

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4 MATHEMATICS IV MARKS. If + + 6 + c epesents cicle with dius 6, find the vlue of c. R 9 f c ; g, f 6 9 c 6 c c. Find the eccenticit of the hpeol Eqution of the hpeol Hee, nd + e + e 5 e 5 e. Find the distnce

More information

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

θ θ φ EN2210: Continuum Mechanics Homework 2: Polar and Curvilinear Coordinates, Kinematics Solutions 1. The for the vector i , calculate: EN0: Continm Mchanics Homwok : Pola and Cvilina Coodinats, Kinmatics Soltions School of Engining Bown Univsity x δ. Th fo th vcto i ij xx i j vi = and tnso S ij = + 5 = xk xk, calclat: a. Thi componnts

More information

ROTATION IN 3D WORLD RIGID BODY MOTION

ROTATION IN 3D WORLD RIGID BODY MOTION OTATION IN 3D WOLD IGID BODY MOTION igid Bod Motion Simultion igid bod motion Eqution of motion ff mmvv NN ddiiωω/dddd Angulr velocit Integrtion of rottion nd it s eression is necessr. Simultion nd Eression

More information

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

Lecture 5. Differential Analysis of Fluid Flow Navier-Stockes equation Lectre 5 Differential Analsis of Flid Flo Naier-Stockes eqation Differential analsis of Flid Flo The aim: to rodce differential eqation describing the motion of flid in detail Flid Element Kinematics An

More information

Concept of Stress at a Point

Concept of Stress at a Point Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS

More information

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

Problem set 5: Solutions Math 207B, Winter r(x)u(x)v(x) dx. Problem set 5: Soltions Mth 7B, Winter 6. Sppose tht p : [, b] R is continosly differentible fnction sch tht p >, nd q, r : [, b] R re continos fnctions sch tht r >, q. Define weighted inner prodct on

More information

3.4 Repeated Roots; Reduction of Order

3.4 Repeated Roots; Reduction of Order 3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &

More information

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

Mathematical Reflections, Issue 5, INEQUALITIES ON RATIOS OF RADII OF TANGENT CIRCLES. Y.N. Aliyev themtil efletions, Issue 5, 015 INEQULITIES ON TIOS OF DII OF TNGENT ILES YN liev stt Some inequlities involving tios of dii of intenll tngent iles whih inteset the given line in fied points e studied

More information

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

This immediately suggests an inverse-square law for a piece of current along the line. Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line

More information

Lecture 11: Potential Gradient and Capacitor Review:

Lecture 11: Potential Gradient and Capacitor Review: Lectue 11: Potentil Gdient nd Cpcito Review: Two wys to find t ny point in spce: Sum o Integte ove chges: q 1 1 q 2 2 3 P i 1 q i i dq q 3 P 1 dq xmple of integting ove distiution: line of chge ing of

More information

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

CSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata CSE303 - Introduction to th Thory of Computing Smpl Solutions for Exrciss on Finit Automt Exrcis 2.1.1 A dtrministic finit utomton M ccpts th mpty string (i.., L(M)) if nd only if its initil stt is finl

More information

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

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

More information

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

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions Mid Ya Eamination 3 F. Matmatics Modul (Calculus & Statistics) Suggstd Solutions Ma pp-: 3 maks - Ma pp- fo ac qustion: mak. - Sam typ of pp- would not b countd twic fom wol pap. - In any cas, no pp maks

More information

( ) ( ) (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

( ) ( ) (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 Hrk Sltis. Th fllig ipttpt rltis dscri ssts ith ipt d tpt. Which ssts r lir? Which r spc-irit? [6 pts.] i. tst lirit tstig lir sprpsiti lt thr t ipt sigls d tpt s th s f th tpts fr ch sigl idiidll ' tpt

More information

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

The Derivative of the Natural Logarithmic Function. Derivative of the Natural Exponential Function. Let u be a differentiable function of x. Th Ntrl Logrithmic n Eponntil Fnctions: : Diffrntition n Intgrtion Objctiv: Fin rivtivs of fnctions involving th ntrl logrithmic fnction. Th Drivtiv of th Ntrl Logrithmic Fnction Lt b iffrntibl fnction

More information

Free vibration of a magneto-electro-elastic toroidal shell

Free vibration of a magneto-electro-elastic toroidal shell icccb Nottingha Unisity Pss Pocdings of th Intnational onfnc on opting in iil and ilding ngining W izani (dito) F ibation of a agnto-lcto-lastic tooidal shll. Rdkop patnt of Mchanical ngining, Unisity

More information

Section - 2 MORE PROPERTIES

Section - 2 MORE PROPERTIES LOCUS Section - MORE PROPERTES n section -, we delt with some sic properties tht definite integrls stisf. This section continues with the development of some more properties tht re not so trivil, nd, when

More information

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

Winter 2016 COMP-250: Introduction to Computer Science. Lecture 23, April 5, 2016 Wintr 2016 COMP-250: Introduction to Computr Scinc Lctur 23, April 5, 2016 Commnt out input siz 2) Writ ny lgorithm tht runs in tim Θ(n 2 log 2 n) in wors cs. Explin why this is its running tim. I don

More information

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

INFLUENCE OF ANTICLIMBING DEVICE ON THE VARIATION OF LOADS ON WHEELS IN DIESEL ELECTRIC 4000 HP U..B. Si. Bull., Si D, Vol.,., SS 454-5 UEE O AMBG DEVE O HE VARAO O OADS O WHEES DESE EER 4 H onl ătălin OESU Dipozitiul nt intodu ini uplimnt p oţil oiilo loomotilo. n lu pzint iti to ini, unţi d dtl

More information

U>, and is negative. Electric Potential Energy

U>, and is negative. Electric Potential Energy Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When

More information

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

Equations from Relativistic Transverse Doppler Effect. The Complete Correlation of the Lorentz Effect to the Doppler Effect in Relativistic Physics Equtins m Rltiisti Tnss ppl Et Th Cmplt Cltin th Lntz Et t th ppl Et in Rltiisti Physis Cpyight 005 Jsph A. Rybzyk Cpyight Risd 006 Jsph A. Rybzyk Fllwing is mplt list ll th qutins usd in did in th Rltiisti

More information

Electricity and Magnetism Electric Dipole Continuous Distribution of Charge

Electricity and Magnetism Electric Dipole Continuous Distribution of Charge Electricit nd Mgnetism Electric Dipole Continos Distribtion of Chrge Ln heridn De Anz College Jn 16, 2018 Lst time electric field lines electric field from point chrge net electric field from mn chrges

More information

GUC (Dr. Hany Hammad)

GUC (Dr. Hany Hammad) Lct # Pl s. Li bdsid s with ifm mplitd distibtis. Gl Csidtis Uifm Bimil Optimm (Dlph-Tchbshff) Cicl s. Pl s ssmig ifm mplitd citti m F m d cs z F d d M COMM Lct # Pl s ssmig ifm mplitd citti F m m m T

More information

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

Department of Mathematics. Birla Institute of Technology, Mesra, Ranchi MA 2201(Advanced Engg. Mathematics) Session: Tutorial Sheet No. Dpm o Mhmics Bi Isi o Tchoog Ms Rchi MA Advcd gg. Mhmics Sssio: 7---- MODUL IV Toi Sh No. --. Rdc h oowig i homogos dii qios io h Sm Liovi om: i. ii. iii. iv. Fid h ig-vs d ig-cios o h oowig Sm Liovi bod

More information

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

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 ics Announcements dy, embe 28, 2004 Ch 6: Cicul Motion - centipetl cceletion Fiction Tension - the mssless sting Help this week: Wednesdy, 8-9 pm in NSC 128/119 Sundy, 6:30-8 pm in CCLIR 468 Announcements

More information

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

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

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

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion

More information

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

:9 :9. Public Water Crossings - DE NORTHERN PASS PROJECT. Ashland. Bridgewater Lgnd ol/ Loction Nothn ss Nothn ss nsission Lins Nub - - - kv Lin Evsouc Lins 5 kv Hight (in ft oss Sction 75-4 -4 5-4 Evsouc 5 kv Lin E5-8 E5- E5- E5-. Rf to Nothn ss nsission LL ublic Wt ossings SE ockt

More information

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 = =

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 = = Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon

More information

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

Dynamically Equivalent Systems. Dynamically Equivalent Systems. Dynamically Equivalent Systems. ME 201 Mechanics of Machines ME 0 Mechnics of Mchines 8//006 Dynmicy Equivent Systems Ex: Connecting od G Dynmicy Equivent Systems. If the mss of the connecting od m G m m B m m m. Moment out cente of gvity shoud e zeo m G m B Theefoe;

More information

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

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA Innionl Jonl of Phoonis n Oil Thnolo Vol. 3 Iss. : 36-4 Jn 7 Rliisi Dnis n lonis in Unifol l n in Unifol Roin s-th Gnl ssions fo h loni 4-Vo Ponil in Sfi Unisi of Clifoni 387 So Hll UC Bkl Clifoni US s@ll.n

More information

Two dimensional polar coordinate system in airy stress functions

Two dimensional polar coordinate system in airy stress functions I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in

More information

Section 3: Antiderivatives of Formulas

Section 3: Antiderivatives of Formulas Chptr Th Intgrl Appli Clculus 96 Sction : Antirivtivs of Formuls Now w cn put th is of rs n ntirivtivs togthr to gt wy of vluting finit intgrls tht is ct n oftn sy. To vlut finit intgrl f(t) t, w cn fin

More information

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

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium .65, MHD Thory of usion Systms Prof. ridrg Lctur 8: Effct of Vrticl ild on Tokmk Equilirium Toroidl orc lnc y Mns of Vrticl ild. Lt us riw why th rticl fild is imortnt. 3. or ry short tims, th cuum chmr

More information

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

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:

More information

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

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97 Univesity of Bhin Physics 10 Finl Exm Key Fll 004 Deptment of Physics 13/1/005 8:30 10:30 e =1.610 19 C, m e =9.1110 31 Kg, m p =1.6710 7 Kg k=910 9 Nm /C, ε 0 =8.8410 1 C /Nm, µ 0 =4π10 7 T.m/A Pt : 10

More information

Solutions to Midterm Physics 201

Solutions to Midterm Physics 201 Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of

More information

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

CDS 101/110: Lecture 7.1 Loop Analysis of Feedback Systems CDS 11/11: Lctu 7.1 Loop Analysis of Fdback Systms Novmb 7 216 Goals: Intoduc concpt of loop analysis Show how to comput closd loop stability fom opn loop poptis Dscib th Nyquist stability cition fo stability

More information

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

Compact Guide Cylinder with One-way Lock Series MLGP ø40, ø50, ø63. Prevents dropping when air supply pressure falls or residual pressure is exhausted Compct uid Cylindr with On-wy ock ris MP ø, ø, ø Prvnts dropping whn ir supply prssur flls or rsidul prssur is xhustd Cn lockd t ny position h locking position cn chngd to ccommodt n xtrnl stoppr position

More information