Module 3 : Analysis of Strain
|
|
- Gloria Miles
- 6 years ago
- Views:
Transcription
1 Mod/Lsso Mod : Aasis of trai.. INTROUCTION T o dfi ora strai rfr to th fooi Fir. hr i AB of a aia oadd br has sffrd dforatio to bco A B. Fir. Aia oadd bar Th th of AB is. As sho i Fir.(b) poits A ad B ha ach b dispacd i.. at poit A a aot ad at poit B a aot. Poit B has b dispacd b a aot i additio to dispact of poit A ad th th has b icrasd b. No ora strai a b dfid as i d d (.) I i of th iiti procss th abo rprsts th strai at a poit. Thrfor "trai is a asr of rati cha i th or cha i shap". Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
2 Mod/Lsso.. TYPE OF TRAIN trai a b cassifid ito dirct ad shar strai. (a) (b) (c) (d) Fir. Tps of strais Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
3 Mod/Lsso Fir.(a).(b).(c).(d) rprst odisioa todisioa thrdisioa ad shar strais rspcti. I cas of todisioa strai to ora or oitdia strais ar i b si appis to oatio; si to cotractio. (.) No cosidr th cha pricd b riht a AB i th Fir. (d). Th tota aar cha of a AB bt is i th ad dirctios is dfid as th shari strai ad dotd b. \ a a (.) Th shar strai is positi h th riht a bt to positi as dcrass othris th shar strai is ati. I cas of a thrdisioa t a pris ith sids d d d as sho i Fir.(c) th fooi ar th ora ad shari strais: (.) Th raii copots of shari strai ar siiar ratd: (.4) Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
4 Mod/Lsso.. EFORMATION OF AN INFINITEIMAL LINE ELEMENT Fir. Li t i dford ad dford bod Fir. Li t i dford ad dford bod Cosidr a ifiitsia i t i th dford otr of a di as sho i th Fir.. Wh th bod dros dforatio th i t passs ito th i t P Q. I ra both th th ad th dirctio of ar chad. Lt th coordiats of P ad Q bfor dforatio b ( )( ) rspcti ad th dispact ctor at poit P ha copots ( ). Th coordiats of P P ad Q ar ( ) P : ( ) P : Appid Easticit for Eirs 4 T.G.ithara & L.GoidaRaj
5 Mod/Lsso 5 Appid Easticit for Eirs T.G.ithara & L.GoidaRaj Q : Th dispact copots at Q diffr siht fro thos at poit P sic Q is aa fro P b ad. \ Th dispacts at Q ar ad No if Q is r cos to P th to th first ordr approiatio (a) iiar (b) Ad (c) Th coordiats of Q ar thrfor Q Bfor dforatio th st had copots ad ao th thr as. Aftr dforatio th st Q P has copots ad ao th thr as. Hr th trs ik ad tc. ar iportat i th aasis of strai. Ths ar th radits of th dispact copots i ad dirctios. Ths ca b rprstd i th for of a atri cad th dispactradit atri sch as j i
6 Mod/Lsso 6 Appid Easticit for Eirs T.G.ithara & L.GoidaRaj..4 CHANGE IN LENGTH OF A LINEAR ELEMENT Wh th bod dros dforatio it cass a poit P( ) i th bod dr cosidratio to b dispacd to a positio P ith coordiats hr ad ar th dispact copots. Aso a ihbori poit Q ith coordiats ts dispacd to Q ith coordiats. No t b th th of th i t ith its copots. \ iiar b th th Q P ith its copots P Q \ Fro qatios (a) (b) ad (c) Taki th diffrc bt ad t Q P { } (.5) hr (.5a)
7 Mod/Lsso 7 Appid Easticit for Eirs T.G.ithara & L.GoidaRaj (.5b) (.5c) (.5d) (.5) (.5f) No itrodci th otatio hich is cad th rati tsio of poit P i th dirctio of poit Q o Fro Eqatio (.5) sbstitti for t If ad ar th dirctio cosis of th bstitti ths qatitis i th abo prssio Th abo qatio is th a of th rati dispact at poit P i th dirctio ith dirctio cosis ad.
8 Mod/Lsso..5 CHANGE IN LENGTH OF A LINEAR ELEMENTLINEAR COMPONENT It ca b obsrd fro th Eqatio (.5a) (.5b) ad (.5c) that th cotai iar trs ik tc. as as oiar trs ik. tc. If th dforatio iposd o th bod is sa th trs ik tc ar tr sa so that thir sqars ad prodcts ca b ctd. Hc rtaii o iar trs th iar strai at poit P i th dirctio ca b obtaid as bo. (.6) (.6a) (.6b) If hor th i t is para to ais th ad th iar strai is iiar for t para to ais th ad th iar strai is ad for t para to ais th ad th iar strai is Th ratios prssd b qatios (.6) ad (.6a) ar ko as th strai dispact ratios of Cach...6 TRAIN TENOR Jst as th stat of strss at a poit is dscribd b a itr arra th strai ca b rprstd tsoria as bo: Appid Easticit for Eirs 8 T.G.ithara & L.GoidaRaj
9 ij i j j i Mod/Lsso (i j ) (.7) Th factor / i th abo Eqatio (.7) faciitats th rprstatio of th strai trasforatio qatios i idicia otatio. Th oitdia strais ar obtaid h i j; th shari strais ar obtaid h i ¹ j ad. It is car fro th Eqatios (.) ad (.) that (.8) ij ji Thrfor th strai tsor ( ij ji ) is i b ij (.9)..7 TRAIN TRANFORMATION If th dispact copots ad at a poit ar rprstd i trs of ko fctios of ad rspcti i cartsia coordiats th th si strai copots ca b dtrid b si th straidispact ratios i bo. ad If at th sa poit th strai copots ith rfrc to aothr st of coordiats as ad ar dsird th th ca b cacatd si th cocpts of ais trasforatio ad th corrspodi dirctio cosis. It is to b otd that th abo qatios ar aid for a sst of orthooa coordiat as irrspcti of thir oritatios. Hc Appid Easticit for Eirs 9 T.G.ithara & L.GoidaRaj
10 Mod/Lsso Appid Easticit for Eirs T.G.ithara & L.GoidaRaj Ths th trasforatio of strais fro o coordiat sst to aothr ca b ritt i atri for as bo: I ra [ ] [ ][ ][ ] T a a..8 PHERICAL AN EVIATORIAL TRAIN TENOR Lik th strss tsor th strai tsor is aso diidd ito to parts th sphrica ad th diatoria as E E E hr E sphrica strai (.) E ) ( ) ( ) ( diatoria strai (.) ad It is otd that th sphrica copot E prodcs o o chas ithot a cha of shap hi th diatoria copot E prodcs distortio or cha of shap. Ths copots ar tsi sd i thoris of fair ad ar sotis ko as "diatatio" ad "distortio" copots.
11 ..9 PRINCIPAL TRAIN TRAIN INVARIANT Mod/Lsso ri th discssio of th stat of strss at a poit it as statd that at a poit i a coti thr ists thr ta orthooa pas ko as Pricipa pas o hich thr ar o shar strsss. iiar to that pas ist o hich thr ar o shar strais ad o ora strais occr. Ths pas ar trd as pricipa pas ad th corrspodi strais ar ko as Pricipa strais. Th Pricipa strais ca b obtaid b first dtrii th thr ta prpdicar dirctios ao hich th ora strais ha statioar as. Hc for this prpos th ora strais i b Eqatio (.6b) ca b sd. i.. As th as of ad cha o ca t diffrt as for th strai. Thrfor to fid th ai or ii as of strai ar rqird to qat to ro if ad r a idpdt. Bt o of th dirctio cosis is ot idpdt sic th ar ratd b th ratio. No taki ad as idpdt ad diffrtiati ith rspct to ad t No diffrtiati ith rspct to ad for a tr t ( ) ( ) bstitti for ad fro Eqatio. t (.) Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
12 Mod/Lsso oti th riht had prssio i th abo to qatios b ad (.a) Usi qatio (.a) ca obtai th as of ad hich dtri th dirctio ao hich th rati tsio is a tr. No tipi th first Eqatio b th scod b ad th third b ad addi th W t ( ) ( ) (.b) Hr Hc Eqatio (.b) ca b ritt as hich as that i Eqatio (.a) th as of ad dtri th dirctio ao hich th rati tsio is a tr ad aso th a of is qa to this tr. Hc Eqatio (.a) ca b ritt as ( ) ( ) oti ( ) Eqatio (.c) ca b ritt as th (.c) Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
13 Mod/Lsso ( ) ( ) ( ) (.d) Th abo st of qatios is hooos i ad. I ordr to obtai a otriia sotio of th dirctios ad fro Eqatio (.d) th dtriat of th cofficits shod b ro. i.. ( ) ( ) ( ) Epadi th dtriat of th cofficits t J J J (.) hr J J J W ca aso rit as J J J 4 4 Hc th thr roots ( ) ( ) ad of th cbic Eqatio (.) ar ko as th pricipa strais ad J J ad J ar trd as first iariat scod iariat ad third iariat of strais rspcti. Iariats of trai Tsor Ths ar asi fod ot b tiii th prfct corrspodc of th copots of strai tsor ij ith thos of th strss tsor t ij. Th thr iariats of th strai ar: Appid Easticit for Eirs T.G.ithara & L.GoidaRaj
14 J J 4 ( ) J 4 ( ) Mod/Lsso (.) (.4) (.5).. OCTAHERAL TRAIN Th strais acti o a pa hich is qa icid to th thr coordiat as ar ko as octahdra strais. Th dirctio cosis of th ora to th octahdra pa ar. Th ora octahdra strai is: ( ) oct \ ( ) oct ( ) (.6) Rstat octahdra strai ( R ) oct Octahdra shar strai oct ( ) (.7) ( (.8) ) ( ) ( ) Appid Easticit for Eirs 4 T.G.ithara & L.GoidaRaj
dy ds dz ds dx ds ds ds ds ds ds 4-1 DEFORMATION OF A BODY Let there be a line segment PQ in the body with coordinates as:
5:44 (58:54 ENERGY PRNCPLES N SRUCURAL MECHANCS 4- DEFORMAON OF A BODY Q Q Let there be a ie seget PQ i the bo with cooriates as: P(,,, Q(,, Legth of the ifferetia eeet: P P Uit taget vector aog PQ: e
More informationECEN 5005 Crystals, Nanocrystals and Device Applications Class 14 Group Theory For Crystals
ECEN 5005 Cryta Naocryta ad Dvic Appicatio Ca 14 Group Thory For Cryta Spi Aguar Motu Quatu Stat of Hydrog-ik Ato Sig Ectro Cryta Fid Thory Fu Rotatio Group 1 Spi Aguar Motu Spi itriic aguar otu of ctro
More informationTime : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120
Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,
More informationDigital Signal Processing, Fall 2006
Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti
More information1985 AP Calculus BC: Section I
985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b
More information10. Joint Moments and Joint Characteristic Functions
0 Joit Momts ad Joit Charactristic Fctios Followig sctio 6 i this sctio w shall itrodc varios paramtrs to compactly rprst th iformatio cotaid i th joit pdf of two rvs Giv two rvs ad ad a fctio g x y dfi
More informationThe Asymptotic Form of Eigenvalues for a Class of Sturm-Liouville Problem with One Simple Turning Point. A. Jodayree Akbarfam * and H.
Joral of Scic Ilaic Rpblic of Ira 5(: -9 ( Uirity of Thra ISSN 6- Th Ayptotic For of Eigal for a Cla of Str-Lioill Probl with O Sipl Trig Poit A. Jodayr Abarfa * ad H. Khiri Faclty of Mathatical Scic Tabriz
More informationThomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple
5/24/5 A PROOF OF THE CONTINUED FRACTION EXPANSION OF / Thomas J Oslr INTRODUCTION This ar givs aothr roof for th rmarkabl siml cotiud fractio = 3 5 / Hr is ay ositiv umbr W us th otatio x= [ a; a, a2,
More informationDiscrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform. Discrete Fourier Transform
Discrt Fourir Trasform Dfiitio - T simplst rlatio btw a lt- squc x dfid for ω ad its DTFT X ( ) is ω obtaid by uiformly sampli X ( ) o t ω-axis btw ω < at ω From t dfiitio of t DTFT w tus av X X( ω ) ω
More informationNational Quali cations
PRINT COPY OF BRAILLE Ntiol Quli ctios AH08 X747/77/ Mthmtics THURSDAY, MAY INSTRUCTIONS TO CANDIDATES Cdidts should tr thir surm, form(s), dt of birth, Scottish cdidt umbr d th m d Lvl of th subjct t
More informationChapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series
Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris
More informationz 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z
Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist
More informationChapter Taylor Theorem Revisited
Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o
More informationNEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES
Digst Joural of Naomatrials ad Biostructurs Vol 4, No, March 009, p 67-76 NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES A IRANMANESH a*, O KHORMALI b, I NAJAFI KHALILSARAEE c, B SOLEIMANI
More informationPURE MATHEMATICS A-LEVEL PAPER 1
-AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio
More informationUNIT 2: MATHEMATICAL ENVIRONMENT
UNIT : MATHEMATICAL ENVIRONMENT. Itroductio This uit itroducs som basic mathmatical cocpts ad rlats thm to th otatio usd i th cours. Wh ou hav workd through this uit ou should: apprciat that a mathmatical
More information7. Differentiation of Trigonometric Function
7. Diffrtiatio of Trigootric Fctio RADIAN MEASURE. Lt s ot th lgth of arc AB itrcpt y th ctral agl AOB o a circl of rais r a lt S ot th ara of th sctor AOB. (If s is /60 of th circfrc, AOB = 0 ; if s =
More informationPower Spectrum Estimation of Stochastic Stationary Signals
ag of 6 or Spctru stato of Stochastc Statoary Sgas Lt s cosr a obsrvato of a stochastc procss (). Ay obsrvato s a ft rcor of th ra procss. Thrfor, ca say:
More informationVtusolution.in FOURIER SERIES. Dr.A.T.Eswara Professor and Head Department of Mathematics P.E.S.College of Engineering Mandya
LECTURE NOTES OF ENGINEERING MATHEMATICS III Su Cod: MAT) Vtusoutio.i COURSE CONTENT ) Numric Aysis ) Fourir Sris ) Fourir Trsforms & Z-trsforms ) Prti Diffrti Equtios 5) Lir Agr 6) Ccuus of Vritios Tt
More informationDTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1
DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT
More informationDEPARTMENT OF MATHEMATICS BIT, MESRA, RANCHI MA2201 Advanced Engg. Mathematics Session: SP/ 2017
DEARMEN OF MAEMAICS BI, MESRA, RANCI MA Advad Egg. Mathatis Sssio: S/ 7 MODULE I. Cosidr th two futios f utorial Sht No. -- ad g o th itrval [,] a Show that thir Wroskia W f, g vaishs idtially. b Show
More informationH2 Mathematics Arithmetic & Geometric Series ( )
H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic
More informationMONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx
MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of
More informationDiscrete Fourier Transform. Nuno Vasconcelos UCSD
Discrt Fourir Trasform uo Vascoclos UCSD Liar Shift Ivariat (LSI) systms o of th most importat cocpts i liar systms thory is that of a LSI systm Dfiitio: a systm T that maps [ ito y[ is LSI if ad oly if
More informationChapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1
Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida
More informationLINEARIZATION OF NONLINEAR EQUATIONS By Dominick Andrisani. dg x. ( ) ( ) dx
LINEAIZATION OF NONLINEA EQUATIONS By Domiick Adrisai A. Liearizatio of Noliear Fctios A. Scalar fctios of oe variable. We are ive the oliear fctio (). We assme that () ca be represeted si a Taylor series
More informationThey must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.
37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam
More informationA Simple Proof that e is Irrational
Two of th most bautiful ad sigificat umbrs i mathmatics ar π ad. π (approximatly qual to 3.459) rprsts th ratio of th circumfrc of a circl to its diamtr. (approximatly qual to.788) is th bas of th atural
More informationSection 10.3 The Complex Plane; De Moivre's Theorem. abi
Sectio 03 The Complex Plae; De Moivre's Theorem REVIEW OF COMPLEX NUMBERS FROM COLLEGE ALGEBRA You leared about complex umbers of the form a + bi i your college algebra class You should remember that "i"
More informationMotivation. We talk today for a more flexible approach for modeling the conditional probabilities.
Baysia Ntworks Motivatio Th coditioal idpdc assuptio ad by aïv Bays classifirs ay s too rigid spcially for classificatio probls i which th attributs ar sowhat corrlatd. W talk today for a or flibl approach
More informationProbability & Statistics,
Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said
More informationMagnetic Moment of the Proton
SB/F/35.3-2 Magtic Mot of th Proto G. Gozálz-Martí*, I.Taboada Dpartato d Física, Uivrsidad Sió Bolívar, Apartado 89, Caracas 18-A, Vzula. ad J. Gozálz Physics Dpartt, Northatr Uivrsity, Bosto, U.S.A.
More informationLU FACTORIZATION. ELM1222 Numerical Analysis. ELM1222 Numerical Analysis Dr Muharrem Mercimek
EM Nmeric Asis Dr Mhrrem Mercimek FACTORIZATION EM Nmeric Asis Some of the cotets re dopted from ree V. Fsett, Appied Nmeric Asis sig MATAB. Pretice H Ic., 999 EM Nmeric Asis Dr Mhrrem Mercimek Cotets
More informationChapter At each point (x, y) on the curve, y satisfies the condition
Chaptr 6. At ach poit (, y) o th curv, y satisfis th coditio d y 6; th li y = 5 is tagt to th curv at th poit whr =. I Erciss -6, valuat th itgral ivolvig si ad cosi.. cos si. si 5 cos 5. si cos 5. cos
More informationFooling Newton s Method a) Find a formula for the Newton sequence, and verify that it converges to a nonzero of f. A Stirling-like Inequality
Foolig Nwto s Mthod a Fid a formla for th Nwto sqc, ad vrify that it covrgs to a ozro of f. ( si si + cos 4 4 3 4 8 8 bt f. b Fid a formla for f ( ad dtrmi its bhavior as. f ( cos si + as A Stirlig-li
More informationChapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering
haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of
More informationNarayana IIT Academy
INDIA Sc: LT-IIT-SPARK Dat: 9--8 6_P Max.Mars: 86 KEY SHEET PHYSIS A 5 D 6 7 A,B 8 B,D 9 A,B A,,D A,B, A,B B, A,B 5 A 6 D 7 8 A HEMISTRY 9 A B D B B 5 A,B,,D 6 A,,D 7 B,,D 8 A,B,,D 9 A,B, A,B, A,B,,D A,B,
More informationOrdinary Differential Equations
Ordiary Diffrtial Equatio Aftr radig thi chaptr, you hould b abl to:. dfi a ordiary diffrtial quatio,. diffrtiat btw a ordiary ad partial diffrtial quatio, ad. Solv liar ordiary diffrtial quatio with fid
More informationLinear Algebra Existence of the determinant. Expansion according to a row.
Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit
More informationDerivation of a Predictor of Combination #1 and the MSE for a Predictor of a Position in Two Stage Sampling with Response Error.
Drivatio of a Prdictor of Cobiatio # ad th SE for a Prdictor of a Positio i Two Stag Saplig with Rspos Error troductio Ed Stak W driv th prdictor ad its SE of a prdictor for a rado fuctio corrspodig to
More informationEE 570: Location and Navigation: Theory & Practice
EE 570: Locatio ad Naigatio: Thory & Practic Naigatio Ssors ad INS Mchaizatio NMT EE 570: Locatio ad Naigatio: Thory & Practic Slid 1 of 13 Naigatio Ssors ad INS Mchaizatio Naigatio Equatios Cas 3: Na
More informationZero Point Energy: Thermodynamic Equilibrium and Planck Radiation Law
Gaug Institut Journa Vo. No 4, Novmbr 005, Zro Point Enrgy: Thrmodynamic Equiibrium and Panck Radiation Law Novmbr, 005 vick@adnc.com Abstract: In a rcnt papr, w provd that Panck s radiation aw with zro
More informationDiscrete Fourier Series and Transforms
Lctur 4 Outi: Discrt Fourir Sris ad Trasforms Aoucmts: H 4 postd, du Tus May 8 at 4:3pm. o at Hs as soutios wi b avaiab immdiaty. Midtrm dtais o t pag H 5 wi b postd Fri May, du foowig Fri (as usua) Rviw
More informationFourier Transforms. Convolutions. Capturing what s important. Last Time. Linear Image Transformation. Invertible Transforms.
orr Trasors Rq rad: Captr 7 92 &P Adso Soc ad ra (adot o) Opt rad: Hor 7 & 8 P 8 Last T Cooto trs: a/box tr Gassa tr t drc tr Lapaca o Gassa tr Ed Dtcto Cootos Cooto s coptatoay costy ad a copx oprato
More informationFurther Results on Pair Sum Graphs
Applid Mathmatis, 0,, 67-75 http://dx.doi.org/0.46/am.0.04 Publishd Oli Marh 0 (http://www.sirp.org/joural/am) Furthr Rsults o Pair Sum Graphs Raja Poraj, Jyaraj Vijaya Xavir Parthipa, Rukhmoi Kala Dpartmt
More informationChemistry 342 Spring, The Hydrogen Atom.
Th Hyrogn Ato. Th quation. Th first quation w want to sov is φ This quation is of faiiar for; rca that for th fr partic, w ha ψ x for which th soution is Sinc k ψ ψ(x) a cos kx a / k sin kx ± ix cos x
More informationSolution to 1223 The Evil Warden.
Solutio to 1 Th Evil Ward. This is o of thos vry rar PoWs (I caot thik of aothr cas) that o o solvd. About 10 of you submittd th basic approach, which givs a probability of 47%. I was shockd wh I foud
More informationHWA CHONG INSTITUTION JC1 PROMOTIONAL EXAMINATION Wednesday 1 October hours. List of Formula (MF15)
HWA CHONG INSTITUTION JC PROMOTIONAL EXAMINATION 4 MATHEMATICS Higher 974/ Paper Wedesda October 4 hors Additioal materials: Aswer paper List of Formla (MF5) READ THESE INSTRUCTIONS FIRST Write or ame
More informationDETERMINATION OF THERMAL STRESSES OF A THREE DIMENSIONAL TRANSIENT THERMOELASTIC PROBLEM OF A SQUARE PLATE
DRMINAION OF HRMAL SRSSS OF A HR DIMNSIONAL RANSIN HRMOLASIC PROBLM OF A SQUAR PLA Wrs K. D Dpr o Mics Sr Sivji Co Rjr Mrsr Idi *Aor or Corrspodc ABSRAC prs ppr ds wi driio o prr disribio ow prr poi o
More informationResearch of an Adaptive Cubature Kalman Filter for GPS/SINS Tightly Integrated Navigation System
tratioa Jora of Eiri ad Appid Scics (JEAS) SSN: 394-366 Vo-4 ss-5 Ma 7 Rsarch of a Adaptiv atr Kaa Fitr for PS/SNS iht tratd Naviatio Sst h Zhao Shai h Yipi Wa Astract viw of th charactrtics of Batic si
More informationGaussian Processes, Multivariate Probability Density Function, Transforms
Gassia Processes, Mltivariate Probabilit Desit Fctio, rasfors A realvaled rado process Xt is called a Gassia process, if all of its thorder joit probabilit desit fctios are variate Gassia pdfs. he thorder
More informationln x = n e = 20 (nearest integer)
H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77
More informationDifferential 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 informationAn Introduction to Asymptotic Expansions
A Itroductio to Asmptotic Expasios R. Shaar Subramaia Asmptotic xpasios ar usd i aalsis to dscrib th bhavior of a fuctio i a limitig situatio. Wh a fuctio ( x, dpds o a small paramtr, ad th solutio of
More informationFrequency Response & Digital Filters
Frquy Rspos & Digital Filtrs S Wogsa Dpt. of Cotrol Systms ad Istrumtatio Egirig, KUTT Today s goals Frquy rspos aalysis of digital filtrs LTI Digital Filtrs Digital filtr rprstatios ad struturs Idal filtrs
More informationNational Quali cations
Ntiol Quli ctios AH07 X77/77/ Mthmtics FRIDAY, 5 MAY 9:00 AM :00 NOON Totl mrks 00 Attmpt ALL qustios. You my us clcultor. Full crdit will b giv oly to solutios which coti pproprit workig. Stt th uits
More informationOrdinary Differential Equations
Basi Nomlatur MAE 0 all 005 Egirig Aalsis Ltur Nots o: Ordiar Diffrtial Equatios Author: Profssor Albrt Y. Tog Tpist: Sakurako Takahashi Cosidr a gral O. D. E. with t as th idpdt variabl, ad th dpdt variabl.
More informationWorksheet: Taylor Series, Lagrange Error Bound ilearnmath.net
Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.
More informationDiscrete Fourier Transform (DFT)
Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial
More informationThat is, we start with a general matrix: And end with a simpler matrix:
DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss
More informationElementary Linear Algebra
Elemetary Liear Algebra Ato & Rorres th Editio Lectre Set Chapter : Eclidea Vector Spaces Chapter Cotet Vectors i -Space -Space ad -Space Norm Distace i R ad Dot Prodct Orthogoality Geometry of Liear Systems
More informationCDS 101: Lecture 5.1 Reachability and State Space Feedback
CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray ad Hido Mabuchi 5 Octobr 4 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls
More informationFrequency Measurement in Noise
Frqucy Masurmt i ois Porat Sctio 6.5 /4 Frqucy Mas. i ois Problm Wat to o look at th ct o ois o usig th DFT to masur th rqucy o a siusoid. Cosidr sigl complx siusoid cas: j y +, ssum Complx Whit ois Gaussia,
More informationP.L. Chebyshev. The Theory of Probability
P.L. Chbyshv Th Thory of Probability Traslatd by Oscar Shyi Lcturs dlivrd i 879 88 as tak dow by A.M. Liapuov Brli, 4 Oscar Shyi www.shyi.d.., 879 88.....!" 936 Cotts Itroductio by th Traslator Forword
More informationامتحانات الشهادة الثانوية العامة فرع: العلوم العامة
وزارة التربية والتعليم العالي المديرية العامة للتربية دائرة االمتحانات امتحانات الشهادة الثانوية العامة فرع: العلوم العامة االسم: الرقم: مسابقة في مادة الرياضيات المدة أربع ساعات عدد المسائل: ست مالحظة:
More informationDIOPHANTINE APPROXIMATION WITH FOUR SQUARES AND ONE K-TH POWER OF PRIMES
oural of atatical Scics: Advacs ad Alicatios Volu 6 Nubr 00 Pas -6 DOPHANNE APPROAON WH FOUR SQUARES AND ONE -H POWER OF PRES Dartt of atatics ad foratio Scic Ha Uivrsit of Ecooics ad Law Zzou 000 P. R.
More informationIranian Journal of Mathematical Chemistry, Vol. 2, No. 2, December 2011, pp (Received September 10, 2011) ABSTRACT
Iraa Joral of Mathatcal Chstry Vol No Dcbr 0 09 7 IJMC Two Tys of Gotrc Arthtc dx of V hylc Naotb S MORADI S BABARAHIM AND M GHORBANI Dartt of Mathatcs Faclty of Scc Arak Ursty Arak 856-8-89 I R Ira Dartt
More informationCHAPTER 5d. SIMULTANEOUS LINEAR EQUATIONS
CHAPTE 5. SIUTANEOUS INEA EQUATIONS A. J. Crk Schoo of Egirig Dprtmt of Civi Eviromt Egirig by Dr. Ibrhim A. Asskkf Sprig ENCE - Compttio thos i Civi Egirig II Dprtmt of Civi Eviromt Egirig Uivrsity of
More informationME311 Machine Design
ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform
More informationPayroll Direct Deposit
Payroll Dirct Dposit Dirct Dposit for mploy paychcks allows cntrs to avoi printing an physically istributing papr chcks to mploys. Dirct posits ar ma through a systm known as Automat Claring Hous (ACH),
More informationChapter 3 Fourier Series Representation of Periodic Signals
Chptr Fourir Sris Rprsttio of Priodic Sigls If ritrry sigl x(t or x[] is xprssd s lir comitio of som sic sigls th rspos of LI systm coms th sum of th idividul rsposs of thos sic sigls Such sic sigl must:
More informationFractal diffusion retrospective problems
Iraoa ora o App Mahac croc a Copr Avac Tchoo a Scc ISSN: 47-8847-6799 wwwaccor/iamc Ora Rarch Papr Fraca o rropcv prob O Yaro Rcv 6 h Ocobr 3 Accp 4 h aar 4 Abrac: I h arc w h rropcv vr prob Th rropcv
More informationWashington State University
he 3 Ktics ad Ractor Dsig Sprg, 00 Washgto Stat Uivrsity Dpartmt of hmical Egrg Richard L. Zollars Exam # You will hav o hour (60 muts) to complt this xam which cosists of four (4) problms. You may us
More information8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions
Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for
More informationGRADED QUESTIONS ON COMPLEX NUMBER
E /Math-I/ GQ/Comple umer GRADED QUESTINS N CMPEX NUMBER. The umer of the form + i y where ad y are real umers ad i = - i. e.( i ) is called a comple umer ad it is deoted y z i.e. z = + i y.the comple
More informationChapter 9 Infinite Series
Sctio 9. 77. Cotiud d + d + C Ar lim b lim b b b + b b lim + b b lim + b b 6. () d (b) lim b b d (c) Not tht d c b foud by prts: d ( ) ( ) d + C. b Ar b b lim d lim b b b b lim ( b + ). b dy 7. () π dy
More informationOn the approximation of the constant of Napier
Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of
More informationDFT: Discrete Fourier Transform
: Discrt Fourir Trasform Cogruc (Itgr modulo m) I this sctio, all lttrs stad for itgrs. gcd m, = th gratst commo divisor of ad m Lt d = gcd(,m) All th liar combiatios r s m of ad m ar multils of d. a b
More informationCalculus Revision A2 Level
alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ
More informationFigure 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 informationy = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b)
4. y = y = + 5. Find th quation of th tangnt lin for th function y = ( + ) 3 whn = 0. solution: First not that whn = 0, y = (1 + 1) 3 = 8, so th lin gos through (0, 8) and thrfor its y-intrcpt is 8. y
More informationA Review of Complex Arithmetic
/0/005 Rviw of omplx Arithmti.do /9 A Rviw of omplx Arithmti A omplx valu has both a ral ad imagiary ompot: { } ad Im{ } a R b so that w a xprss this omplx valu as: whr. a + b Just as a ral valu a b xprssd
More informationSOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3
SOLVED EXAMPLES E. If f() E.,,, th f() f() h h LHL RHL, so / / Lim f() quls - (D) Dos ot ist [( h)+] [(+h) + ] f(). LHL E. RHL h h h / h / h / h / h / h / h As.[C] (D) Dos ot ist LHL RHL, so giv it dos
More information5.1 The Nuclear Atom
Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 5.1 Th Nuclar tom Qustio Papr Lvl IGSE Subjct Physics (0625) Exam oard Topic Sub Topic ooklt ambridg Itratioal
More informationIntroduction. Question: Why do we need new forms of parametric curves? Answer: Those parametric curves discussed are not very geometric.
Itrodctio Qestio: Why do we eed ew forms of parametric crves? Aswer: Those parametric crves discssed are ot very geometric. Itrodctio Give sch a parametric form, it is difficlt to kow the derlyig geometry
More informationphysicsandmathstutor.com
physicsadmathstutor.com 5. Solve, for 0 x 180, the equatio 3 (a) si( x + 10 ) =, 2 (b) cos 2x = 0.9, givig your aswers to 1 decimal place. (4) (4) 10 *N23492B01028* 8. (a) Fid all the values of, to 1 decimal
More informationGeometric Camera Calibration Chapter 2
Geoetric Caera Calibratio Chapter 2 Gido Gerig CS 6643 Sprig 27 Slides odified fro Marc ollefeys, UNC Chapel Hill, Cop256, Other slides ad illstratios fro J. oce, added to corse book, ad reor Darrell,
More informationQuantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points)
Chm 5 Problm St # ANSWER KEY 5 qustios, poits Qutum Mchics & Spctroscopy Prof. Jso Goodpstr Du ridy, b. 6 S th lst pgs for possibly usful costts, qutios d itgrls. Ths will lso b icludd o our futur ms..
More informationTwo-Dimensional Quantum Harmonic Oscillator
D Qa Haroc Oscllaor Two-Dsoal Qa Haroc Oscllaor 6 Qa Mchacs Prof. Y. F. Ch D Qa Haroc Oscllaor D Qa Haroc Oscllaor ch5 Schrödgr cosrcd h cohr sa of h D H.O. o dscrb a classcal arcl wh a wav ack whos cr
More informationINTEGRATION BY PARTS
Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd
More informationDiagonalization of Quadratic Forms. Recall in days past when you were given an equation which looked like
Diagoalizatio of Qadratic Forms Recall i das past whe o were gie a eqatio which looked like ad o were asked to sketch the set of poits which satisf this eqatio. It was ecessar to complete the sqare so
More informationIntroduction to logistic regression
Itroducto to logstc rgrsso Gv: datast D { 2 2... } whr s a k-dmsoal vctor of ral-valud faturs or attrbuts ad s a bar class labl or targt. hus w ca sa that R k ad {0 }. For ampl f k 4 a datast of 3 data
More informationBlackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?
All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody
More informationQuasi-Supercontinuum Interband Lasing Characteristics of Quantum Dot Nanostructures
USOD 008 ottiha UK Quasi-Suprcotiuu Itrbad Lasi Charactristics of Quatu Dot aostructurs C. L. a Y. Wa H. S. Di B. S. Ooi Ctr for Optica choois ad Dpartt of ctrica ad Coputr iri Lhih Uivrsity Bthh Psyvaia
More informationPH4210 Statistical Mechanics
PH4 Statistical Mchaics Probl Sht Aswrs Dostrat that tropy, as giv by th Boltza xprssio S = l Ω, is a xtsiv proprty Th bst way to do this is to argu clarly that Ω is ultiplicativ W ust prov that if o syst
More informationEconomics 201b Spring 2010 Solutions to Problem Set 3 John Zhu
Economics 20b Spring 200 Solutions to Problm St 3 John Zhu. Not in th 200 vrsion of Profssor Andrson s ctur 4 Nots, th charactrization of th firm in a Robinson Cruso conomy is that it maximizs profit ovr
More information3.4 Properties of the Stress Tensor
cto.4.4 Proprts of th trss sor.4. trss rasformato Lt th compots of th Cauchy strss tsor a coordat systm wth bas vctors b. h compots a scod coordat systm wth bas vctors j,, ar gv by th tsor trasformato
More informationHadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms
Math Sci Ltt Vol No 8-87 (0) adamard Exotial al Matrix, Its Eigvalus ad Som Norms İ ad M bula Mathmatical Scics Lttrs Itratioal Joural @ 0 NSP Natural Scics Publishig Cor Dartmt of Mathmatics, aculty of
More information[ ] Review. For a discrete-time periodic signal xn with period N, the Fourier series representation is
Discrt-tim ourir Trsform Rviw or discrt-tim priodic sigl x with priod, th ourir sris rprsttio is x + < > < > x, Rviw or discrt-tim LTI systm with priodic iput sigl, y H ( ) < > < > x H r rfrrd to s th
More informationME 501A Seminar in Engineering Analysis Page 1
St Ssts o Ordar Drtal Equatos Novbr 7 St Ssts o Ordar Drtal Equatos Larr Cartto Mcacal Er 5A Sar Er Aalss Novbr 7 Outl Mr Rsults Rvw last class Stablt o urcal solutos Stp sz varato or rror cotrol Multstp
More information