DESIGN SPECTRA REDUCTION COEFFICIENTS FOR SYSTEMS WITH SEISMIC ENERGY DISSIPATING DEVICES LOCATED ON FIRM GROUND

Size: px
Start display at page:

Download "DESIGN SPECTRA REDUCTION COEFFICIENTS FOR SYSTEMS WITH SEISMIC ENERGY DISSIPATING DEVICES LOCATED ON FIRM GROUND"

Transcription

1 Th 14 th Worl Confrn on Earthquak Enginring DESIGN SPECTRA REDUCTION COEFFICIENTS FOR SYSTEMS WITH SEISMIC ENERGY DISSIPATING DEVICES LOCATED ON FIRM GROUND S. E. Ruiz 1, J. P. H. Toxqui 2 an J. L. Rivra 3 1 Profssor, Instituto Ingniría, Univrsia Naional Autónoma Méxio, Méxio City 2 Grauat Stunt, Instituto Ingniría, Univrsia Naional Autónoma Méxio, Méxio City 3 Ph.D., formrly at Instituto Ingniría, Univrsia Naional Autónoma Méxio, Méxio City sruizg@iingn.unam.mx, jhialgot@iingn.unam.mx ABSTRACT: A probabilisti man sismi analysis is prform to alulat amping offiints that tak into aount th fft of nrgy issipation on th sign sptral orinats. Two typs of EDDs ar stui: a) linar visous vis, an b) yiling amping systms. Th systms analyz ar loat on firm groun. KEYWORDS: Damping fators, rution offiints, sptral orinats, nrgy issipating vis 1. INTRODUCTION Svral simplifi sign approahs hav bn propos for th sismi sign of struturs with nrgy issipating vis (Collins t al 1995, Ramirz t al 2000, Hanson an Soong 2001, FEMA-450, Whittakr t al 2003 Thos approahs ar ommonly bas on th rution of th alration sign sptrum by mans of amping offiints that tak into aount th fft prou by th nrgy issipating vis (EDDs Th rution fators hav bn obtain, in gnral, from trministi non-linar rspons-history analysis of singl-gr-of-from (SDOF) systms with EDDs, subjt to ror or simulat groun motions. Th iffrn btwn th prsnt stuy an thos foun in th litratur is that hr w tak into aount th fft of all th possibl groun motion intnsitis xpt at th sit, by mans of th orrsponing sismi hazar urvs (Cornll 1968, Estva OBJECTIVE Th objtiv of this stuy is to prsnt a prour for alulating amping fators n to ru th sign psuo-alration sptral orinats, u to th prsn of nrgy issipating vis (EDDs) on th strutural systm. In orr to rah this objtiv a probabilisti man sismi analysis (PDSA) is prform to singl-gr-of-from (SDOF) systms with EDDS, loat on firm groun. Two typs of EDDs ar onsir: a) linar visous systms an b) yiling amping vis. 3. METHODOLOGY First, th uniform annual failur rat (UAFR) sptra of th systm without EDDs (onvntional systm) an, altrnativly, with EDDs (ombin systm) ar alulat using th algorithm prsnt in th nxt stion. Bas on this information, th ratio btwn th sptrum for th onvntional systm an that orrsponing to a systm

2 Th 14 th Worl Confrn on Earthquak Enginring with linar visous EDDs is obtain. Thos ratios ( Q ) ar th rution offiints of th sptrum assoiat with th onvntional strutur. Th visous EDDs onsir in this stuy ar suppos to hav amping offiints qual to 5, 10, 15, 20 an 25% of th ritial. Nxt, w obtain th UAFR sptra for iffrnt valus of SDOF systms with hystrti amprs. Th mhanial haratristis of th EDDs ar givn by mans of th paramtrs α an γ, fin as follows: α = K / K an γ = F y / Fy, whr K is th stiffnss of th, K is th stiffnss of th main SDOF systm, Fy is th yil for of th EDDs, an illustrat in Figur 1. Fy is th yil for of th main SDOF systm. Ths paramtrs ar Figur 1. Main strutural systm with hystrti EDDs Nxt, w plott on th sam graph th UAFR sptra orrsponing to systms with hystrti amprs an th UAFR sptra assoiat with systms with visous amprs. In this mannr w foun th intrstion points btwn both sptra an, bas on th oinins, w stablish quivalns btwn th two typs of ombin systms. Partiularly, w foun th visous amping valu of a onvntional systm with an annual probability of failur qual to that orrsponing to a systm having hystrti EDDs with α an γ paramtrs. 4. UNIFORM ANNUAL FAILURE RATE SPECTRA In orr to obtain th amping fators it is first nssary to onstrut th uniform annual failur rat (UAFR) sptra orrsponing to th SDOF systms with EDDs. In th following w rprou th algorithm propos by th authors (Rivra an Ruiz 2007) for systms with hystrti vis. 1. As a first stp, valus of th following paramtrs orrsponing to th ombin systm ar propos: sismi offiint (C y ), nominal strutural vibration prio T an mass M, as wll as valus of th ratios α = K / K an γ = F y / Fy Nxt, th nominal valu of th latral stiffnss of th ombin systm is alulat ( K T = 4π M / T ). Th nominal stiffnss valus ( K, K ) assoiat rsptivly with th onvntional an with th issipating systms ar obtain ( K = K T /( 1+ α) an K = αk 3. Th yil isplamnt valu of th ombin systm ( yt ) is alulat: yt = CyW /( K + K

3 Th 14 th Worl Confrn on Earthquak Enginring 4. Using th rlations mntion abov, th yil isplamnt valus of th onvntional an of th issipating systms ar alulat ( y = C yw /( K + γk ) an y = γ y 5. Th valus of th stiffnss an of th yil isplamnts of th onvntional systm ( K an y, rsptivly) ar us to alulat th paramtrs Γ 4 an Γ 5 (that orrspon to Babr an Wn 1981 mol In th as of a onvntional rinfor onrt strutur, ths paramtrs ar givn by Γ6 1 K Γ 5 = 2Γ 4 =, whr F υ F y = K y. y 6. In a similar way, th valus of th stiffnss an of th yil isplamnts orrsponing to th issipating systm ( K an, rsptivly) ar us to alulat th valus of th paramtrs Γ an Γ. For stl y Γ6 1 K ma issipating lmnts: Γ5 = Γ 4 =. 2υ F y 7. Eah ombin SDOF systm is subjt to a iffrnt alrogram. Hr w gnrat artifiial groun motions. Eah of ths is sal so that th sptral alration assoiat with th funamntal prio of th systm unr stuy has th sam rturn intrval ( T R ) (Shom an Cornll 1999 Th ratio btwn th sptral alration valu an th invrs of th rturn intrval is givn by th sit sismi hazar urv, whih is assum to b known. 8. Th pak systm isplamnt is obtain stp by stp in tim. Thn, th pak strutural utility man ( μ i ) orrsponing to th i-th simulat ror is alulat. 9. A nominal valu of th utility apaity of th ombin systm is propos ( μ a 10. Th strutural failur of th SDOF systm ours whn th utility man is gratr than th availabl utility (apaity); that is, whn μ i / μ a = Q i 1. Th annual strutural failur rat is valuat by mans of (Estva an Ruiz 1989): ν ν F = P( Q 1Sa ) Sa (1) S a whr ν / y it is th absolut valu of th rivativ of th sit sismi hazar urv (whih is assum to b known), an P( Q 1 y) is th onitional probability that th strutural failur ours, givn a sismi intnsity S a. 11. Th intgral is valuat numrially for iffrnt valus of C y, α, γ an μ a. With th rsults, th man hazar urvs assoiat with SDOF ombin systms with iffrnt vibration prios ar onstrut. In this stuy th strutural man is takn as th lasti for offiint ( S a / g ), so th man hazar urv is a S a / g - vrsus -ν F graph, whr g = gravity. 12. Th UAFR sptra ar rawn on th basis of th man hazar urvs assoiat with iffrnt strutural vibration prios. Th sam algorithm was appli to systms with linar visous vis, xpt that in this as th algorithm boms simplr than that srib abov. 4 5

4 Th 14 th Worl Confrn on Earthquak Enginring 5. GROUND MOTION AND SEISMIC HAZARD CURVES Th SDOF ombin systms analyz ar loat on firm soil. On hunr simulat groun motions wr us as xitations (s stp 7 of th abov algorithm Th simulations wr bas on th ror obtain in Filo Caballo station uring th Sptmbr 19, 1985 arthquak. Th ror is shown in Figur 2a, an its fitt sptral nsity, S (ω), is prsnt in Figur 2b. Th fftiv uration was takn qual to 25s. Figur 2a Bas ror Figur 2b Ajust sptral nsity of th bas ror Th orrsponing sit sismi hazar urvs, for iffrnt strutural prios, ar shown in Figur 3. Figur 3. Sismi hazar urvs orrsponing to th SCT sit

5 Th 14 th Worl Confrn on Earthquak Enginring 6. UAFR SPECTRA FOR STRUCTURES WITH LINEAR VISCOUS DEVICES Th UAFR sptrum was alulat (with th algorithm mntion abov) for iffrnt valus of linar visous amping a to th main systm. In this stuy, a man failur strutural rat qual to was us. Th UAFR ' sptra orrsponing to six iffrnt ratios of ritial amping ( ς = 5, 10, 15, 20, 25 an 30%) ar shown in Figur 4a. From ths sptra, th ratio btwn ah of thm an that orrsponing to ς = 5% was obtain. That ratio ( Q ), prsnt in figur 4b, is th rution offiint of th strngth sptrum that taks into aount th prsn of th visous amprs. Figur 4b orrspon to valus of Q for iffrnt strutural prios an for ' rlations of ritial amping ratios qual to ς ς = 5/30, 5/25, 5/20, 5/15 an 5%/10%. / Figur 4a. UAFR sptra for iffrnt prntags of visous amping Figur 4b. Rution fators. Visous amping Bas on Figur 4b it is possibl to stablish ruls for th onstrution of sign sptra that onsir th fft of xtra amping a to th main strutural systm. For xampl, th authors hav propos to th thnial ommitt in harg of formulating th Sismi Dsign Comision Fral Eltriia (CFE) Manual (now unr rvision) to inorporat th following amping fator xprssion: β ( T ) 1 Q 0.05 ς = = ' λ Whr β is th amping fator that multiplis th sign alration sptrum for 0.05 amping, in orr to tak into aount th prsn of th xtra amping of th strutur is th strutural prio of intrst T ' ς is th fration of ritial amping of th strutur plus EDDs

6 Th 14 th Worl Confrn on Earthquak Enginring 0.45 ; if T < T (2a) λ = T 0.45 T 0.6 ; if T T (2b) T is th prio whr th form of th sptrum hangs 7. UAFR SPECTRA FOR STRUCTURES WITH HYSTERETIC DEVICES Following th algorithm list in stion 4, w onstrut a numbr of UAFR sptra for SDOF systms with hystrti vis. Thos sptra orrspon to SDOF systms having EDDs with iffrnt valus of th paramtrs α an γ (thos wr fin in stion 3, figur 1 Eah of th UAFR sptra of SDOF with hystrti issipating vis was plott on th sam Figur 4a (whih orrspon to sptra for systms with visous amprs) in orr to fin oinin points btwn thir orinats an, in this way, to fin th quivalnt visous amping for ah as. In th following w will try to xplain this prour by mans of an xampl. Figur 5 shows (with isontinuous lins) th sptra that appar in Figur 4a (thy orrspon to SDOF with visous amprs) as wll as th sptrum (with blak full lin) that orrspons to SDOF with hystrti amprs. For this xampl w hav slt th following paramtrs: α = 1 an γ = In Figur 5 w also iniat svral full r irls that orrspon to six points whr th isontinuous urvs (visous amping as) intrst th blak ontinuous urv (hystrti amping as Th orrsponing quivalnt visous amping for th strutural prios ( ) iniat in Figur 5 ar prsnt in th thir olumn of Tabl 1, whr th first olumn rprsnts th strutural prio an th son is th sismi offiint (vrtial axis of Figur 5 Th pairs of valus of th first an th thir olumn in Tabl 1 ar prsnt graphially in Figur 6. This shows that th quivalnt fftiv ritial amping ratio ς pns on th strutural prio, an prsnts its maximum valu los to th ominant prio of th sptrum (in this as, qual to 0.15s Th form of th fitt urv in Figur 6 (for prios longr than th ominant prio) oul b, for xampl, th following xprssion: T = 6 ς ( T + A) + B (3) whr A an B ar onstants that pn on th α an γ valus.

7 Th 14 th Worl Confrn on Earthquak Enginring Figur 5. Intrstion of th sptrum orrsponing to th systms with hystrti EDDs (blak ontinuous lin) with th sptra orrsponing to th systms with visous amprs (isontinuous lins) Tabl 1 Equivalnt visous amping for iffrnt prios Prio (s) T C y ς Figur 6. Efftiv ritial amping ratios orrsponing to a systm with α = 1, γ = 0.3 an ritial amping ratio qual to 5%.

8 Th 14 th Worl Confrn on Earthquak Enginring 6. CONCLUSIONS W hav shown a gnral prour for th alulation of rution fators bas on th ratio btwn th UAFR sptrum orrsponing to th onvntional fram an that of th systms with EDDs, both assoiat with th sam annual failur rat. This approah is bing follow at th National Univrsity of Mxio for th alulation of amping fators. Thos will b submitt for thir possibl inlusion in th CFE Sismi Dsign Manual. ACKNOWLEDEGEMENTS Thanks ar givn to L. Estva for his valuabl ommnts. This rsarh was sponsor by Instituto Invstigaions Elétrias (IIE), by Comisión Fral Eltriia (CFE), an by DGAPA-UNAM-IN REFERENCES Babr T.T. an Wn Y.K. (1981 Ranom vibration of hystrti graing systms. Journal of th Enginring Mhanis Division 107:EM6, Collins, K.R., Wn, Y.K. an Fouth, D.A. (1995), Invstigation of Altrnativ Sismi Dsign Prours for Stanar Builing, Rport No. UILU-ENG , Univrsity of Illinois at Urbana-Champaign, Illinois, USA Cornll, C.A. (1968 Enginring sismi risk analysis. Bulltin of Sismologial Soity of Amria 58:5, Estva, L. (1968), Bass para la Formulaión Disions Disño Sísmio, UNAM, DF, Méxio Estva, L. an Ruiz, S.E. (1989 Sismi failur rats of multistory frams. Journal of Strutural Enginring 115:2, FEMA450 (2003), NEHRP Rommn Provisions for Sismi Rgulations for Nw Builings an Othr Struturs, Builing Sismi Safty Counil National Institut of Builing Sins, Washington D.C., USA Hanson, R.D. an Soong, T.T. (2001), Sismi Dsign with Supplmntal Enrgy Dissipation Dvis, Earthquak Enginring Rsarh Institut, California, USA Ramirz, O., Constantinou, M., Kirhr, C., Whittakr, A., Johnson, M. an Gomz, J. (2000), Dvlopmnt an Evaluation of Simplifi Prours of Analysis an Dsign of Builings with Passiv Enrgy Dissipation Systms, Multiisiplinary Cntr for Earthquak Enginring Rsarh, NY, USA Rivra, J.L. an Ruiz S.E. (2007 Dsign approah bas on UAFR sptra for struturs with isplamnt- pnnt issipating lmnts. Earthquak Sptra 23:2, Shom, N. an Cornll, C. A. (1999), Probabilisti Sismi Dman Analysis of Nonlinar Struturs, Rport No. RMS-35, Dpartmnt of Civil Enginring of th Stanfor Univrsity, California, USA Whittakr, A., Constantinou, M., Ramirz, O., Johnson, M. an Chrysostomou, C. (2003 Equivalnt latral for an moal analysis prours of th 2000 NEHRP provisions for builings with amping systms. Earthquak Sptra 19:4,

A Simple Method of Tuning PI Controllers for Interval Plant of Cold Rolling Mill

A Simple Method of Tuning PI Controllers for Interval Plant of Cold Rolling Mill ntrnational Journal of Rnt Trns in Enginring, Vol. 1, No. 4, May 009 A Simpl Mtho of Tuning P Controllrs for ntrval Plant of Col Rolling Mill S.Umamahswari 1, V.Palanisamy, M.Chiambaram 3, 1 Dpartmnt of

More information

Acoustic Analysis with Consideration of Damping Effects of Air Viscosity in Sound Pathway

Acoustic Analysis with Consideration of Damping Effects of Air Viscosity in Sound Pathway Aousti Analysis with Consiration of Damping Effts of Air Visosity in Soun Pathway M. Sasajima, M. Watana, T. Yamaguhi, Y. Kurosawa, an Y. Koi Astrat Soun pathways in th nlosurs of small arphons ar vry

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c.

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c. MA56 utorial Solutions Qustion a Intgrating fator is ln p p in gnral, multipl b p So b ln p p sin his kin is all a Brnoulli quation -- st Sin w fin Y, Y Y, Y Y p Qustion Dfin v / hn our quation is v μ

More information

First order differential equation Linear equation; Method of integrating factors

First order differential equation Linear equation; Method of integrating factors First orr iffrntial quation Linar quation; Mtho of intgrating factors Exampl 1: Rwrit th lft han si as th rivativ of th prouct of y an som function by prouct rul irctly. Solving th first orr iffrntial

More information

Numerical methods, Mixed exercise 10

Numerical methods, Mixed exercise 10 Numrial mthos, Mi ris a f ( ) 6 f ( ) 6 6 6 a = 6, b = f ( ) So. 6 b n a n 6 7.67... 6.99....67... 6.68....99... 6.667....68... To.p., th valus ar =.68, =.99, =.68, =.67. f (.6).6 6.6... f (.6).6 6.6.7...

More information

Designing of Acceptance Sampling Plan for life tests based on Percentiles of Exponentiated Rayleigh Distribution

Designing of Acceptance Sampling Plan for life tests based on Percentiles of Exponentiated Rayleigh Distribution Intrnational Journal of Currnt Enginring an Thnology E-ISSN 77 46, P-ISSN 347 56 6 INPRESSCO, All Rights Rsrv Availabl at http://inprssoom/atgory/ijt Rsarh Artil Dsigning of Aptan Sampling Plan for lif

More information

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Signal Prossing, Fall 006 Ltur 7: Filtr Dsign Zhng-ua an Dpartmnt of Eltroni Systms Aalborg Univrsity, Dnmar t@om.aau. Cours at a glan MM Disrt-tim signals an systms Systm MM Fourir-omain rprsntation

More information

N1.1 Homework Answers

N1.1 Homework Answers Camrig Essntials Mathmatis Cor 8 N. Homwork Answrs N. Homwork Answrs a i 6 ii i 0 ii 3 2 Any pairs of numrs whih satisfy th alulation. For xampl a 4 = 3 3 6 3 = 3 4 6 2 2 8 2 3 3 2 8 5 5 20 30 4 a 5 a

More information

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice. Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl

More information

The second condition says that a node α of the tree has exactly n children if the arity of its label is n.

The second condition says that a node α of the tree has exactly n children if the arity of its label is n. CS 6110 S14 Hanout 2 Proof of Conflunc 27 January 2014 In this supplmntary lctur w prov that th λ-calculus is conflunt. This is rsult is u to lonzo Church (1903 1995) an J. arkly Rossr (1907 1989) an is

More information

Thomas Whitham Sixth Form

Thomas Whitham Sixth Form Thomas Whitham Sith Form Pur Mathmatics Unit C Algbra Trigonomtr Gomtr Calculus Vctor gomtr Pag Algbra Molus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

Nonlinear Thomson Scattering

Nonlinear Thomson Scattering Nonlinar Thomson Sattring. Many of th th nwr Thomson Sours ar bas on a PULSED Lasr (.g. all of th high-nrgy lasrs ar puls by thir vry natur. Hav vlop a gnral thory to ovr raiation alulations in th gnral

More information

y = 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)

y = 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 information

( ) Differential Equations. Unit-7. Exact Differential Equations: M d x + N d y = 0. Verify the condition

( ) Differential Equations. Unit-7. Exact Differential Equations: M d x + N d y = 0. Verify the condition Diffrntial Equations Unit-7 Eat Diffrntial Equations: M d N d 0 Vrif th ondition M N Thn intgrat M d with rspt to as if wr onstants, thn intgrat th trms in N d whih do not ontain trms in and quat sum of

More information

VTU NOTES QUESTION PAPERS NEWS RESULTS FORUMS

VTU NOTES QUESTION PAPERS NEWS RESULTS FORUMS Diffrntial Equations Unit-7 Eat Diffrntial Equations: M d N d 0 Vrif th ondition M N Thn intgrat M d with rspt to as if wr onstants, thn intgrat th trms in N d whih do not ontain trms in and quat sum of

More information

Multiple Short Term Infusion Homework # 5 PHA 5127

Multiple Short Term Infusion Homework # 5 PHA 5127 Multipl Short rm Infusion Homwork # 5 PHA 527 A rug is aministr as a short trm infusion. h avrag pharmacokintic paramtrs for this rug ar: k 0.40 hr - V 28 L his rug follows a on-compartmnt boy mol. A 300

More information

Uncertainty in non-linear long-term behavior and buckling of. shallow concrete-filled steel tubular arches

Uncertainty in non-linear long-term behavior and buckling of. shallow concrete-filled steel tubular arches CCM14 8-3 th July, Cambridg, England Unrtainty in non-linar long-trm bhavior and bukling of shallow onrt-filld stl tubular arhs *X. Shi¹, W. Gao¹, Y.L. Pi¹ 1 Shool of Civil and Environmnt Enginring, Th

More information

a 1and x is any real number.

a 1and x is any real number. Calcls Nots Eponnts an Logarithms Eponntial Fnction: Has th form y a, whr a 0, a an is any ral nmbr. Graph y, Graph y ln y y Th Natral Bas (Elr s nmbr): An irrational nmbr, symboliz by th lttr, appars

More information

Problem 22: Journey to the Center of the Earth

Problem 22: Journey to the Center of the Earth Problm : Journy to th Cntr of th Earth Imagin that on drilld a hol with smooth sids straight through th ntr of th arth If th air is rmod from this tub (and it dosn t fill up with watr, liquid rok, or iron

More information

Carriers Concentration in Semiconductors - VI. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Carriers Concentration in Semiconductors - VI. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Carrirs Conntration in Smionutors - VI 1 Prof.P. Ravinran, Dpartmnt of Pysis, Cntral Univrsity of Tamil au, Inia ttp://folk.uio.no/ravi/smi01 P.Ravinran, PHY0 Smionutor Pysis, 17 January 014 : Carrirs

More information

MSLC Math 151 WI09 Exam 2 Review Solutions

MSLC Math 151 WI09 Exam 2 Review Solutions Eam Rviw Solutions. Comput th following rivativs using th iffrntiation ruls: a.) cot cot cot csc cot cos 5 cos 5 cos 5 cos 5 sin 5 5 b.) c.) sin( ) sin( ) y sin( ) ln( y) ln( ) ln( y) sin( ) ln( ) y y

More information

EE Power System Analysis

EE Power System Analysis EE650 - owr Syst Analysis UNIT V STABILITYANALYSIS ART A. Dfin Dynai stability of a powr syst. Dynai stability is th stability givn to an inhrntly unstabl syst by autoati ontrol vis an this ynai stability

More information

Case Study Vancomycin Answers Provided by Jeffrey Stark, Graduate Student

Case Study Vancomycin Answers Provided by Jeffrey Stark, Graduate Student Cas Stuy Vancomycin Answrs Provi by Jffry Stark, Grauat Stunt h antibiotic Vancomycin is liminat almost ntirly by glomrular filtration. For a patint with normal rnal function, th half-lif is about 6 hours.

More information

DIFFERENTIAL EQUATION

DIFFERENTIAL EQUATION MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous

More information

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J. Probability and Stochastic Procsss: A Frindly Introduction for Elctrical and Computr Enginrs Roy D. Yats and David J. Goodman Problm Solutions : Yats and Goodman,4.3. 4.3.4 4.3. 4.4. 4.4.4 4.4.6 4.. 4..7

More information

Thomas Whitham Sixth Form

Thomas Whitham Sixth Form Thomas Whitham Sith Form Pur Mathmatics Cor rvision gui Pag Algbra Moulus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv blow th ais in th ais. f () f () f

More information

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Problem Set #2 Due: Friday April 20, 2018 at 5 PM. 1 EE102B Spring 2018 Signal Procssing and Linar Systms II Goldsmith Problm St #2 Du: Friday April 20, 2018 at 5 PM. 1. Non-idal sampling and rcovry of idal sampls by discrt-tim filtring 30 pts) Considr

More information

Junction Tree Algorithm 1. David Barber

Junction Tree Algorithm 1. David Barber Juntion Tr Algorithm 1 David Barbr Univrsity Collg London 1 Ths slids aompany th book Baysian Rasoning and Mahin Larning. Th book and dmos an b downloadd from www.s.ul.a.uk/staff/d.barbr/brml. Fdbak and

More information

Handout 28. Ballistic Quantum Transport in Semiconductor Nanostructures

Handout 28. Ballistic Quantum Transport in Semiconductor Nanostructures Hanout 8 Ballisti Quantum Transport in Smionutor Nanostruturs In this ltur you will larn: ltron transport without sattring (ballisti transport) Th quantum o onutan an th quantum o rsistan Quanti onutan

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Analysis of Algorithms - Elementary graphs algorithms -

Analysis of Algorithms - Elementary graphs algorithms - Analysis of Algorithms - Elmntary graphs algorithms - Anras Ermahl MRTC (Mälaralns Ral-Tim Rsarch Cntr) anras.rmahl@mh.s Autumn 004 Graphs Graphs ar important mathmatical ntitis in computr scinc an nginring

More information

1 Random graphs with specified degrees

1 Random graphs with specified degrees 1 Ranom graphs with spii grs Rall that a vrtx s gr unr th ranom graph mol G(n, p) ollows a Poisson istribution in th spars rgim, whil most ral-worl graphs xhibit havy-tail gr istributions. This irn is

More information

Analysis of Algorithms - Elementary graphs algorithms -

Analysis of Algorithms - Elementary graphs algorithms - Analysis of Algorithms - Elmntary graphs algorithms - Anras Ermahl MRTC (Mälaralns Ral-Tim Rsach Cntr) anras.rmahl@mh.s Autumn 00 Graphs Graphs ar important mathmatical ntitis in computr scinc an nginring

More information

Y 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall

Y 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)

More information

That is, we start with a general matrix: And end with a simpler matrix:

That 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 information

Solutions to Homework 5

Solutions to Homework 5 Solutions to Homwork 5 Pro. Silvia Frnánz Disrt Mathmatis Math 53A, Fall 2008. [3.4 #] (a) Thr ar x olor hois or vrtx an x or ah o th othr thr vrtis. So th hromati polynomial is P (G, x) =x (x ) 3. ()

More information

2. Finite Impulse Response Filters (FIR)

2. Finite Impulse Response Filters (FIR) .. Mthos for FIR filtrs implmntation. Finit Impuls Rspons Filtrs (FIR. Th winow mtho.. Frquncy charactristic uniform sampling. 3. Maximum rror minimizing. 4. Last-squars rror minimizing.. Mthos for FIR

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

On-Line PI Controller Tuning Using Closed-Loop Setpoint Responses for Stable and Integrating Processes*

On-Line PI Controller Tuning Using Closed-Loop Setpoint Responses for Stable and Integrating Processes* On-Lin PI Controllr Tuning Using Closd-Loop Stpoint Rsponss for Stabl and Intgrating Prosss* Mohammad Shamsuzzoha a, Sigurd Skogstad a, Ivar J. Halvorsn b a Norwgian Univrsity of Sin and Thnology (NTNU),

More information

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology Bluchr Mchanical Enginring Procdings May 2014, vol. 1, num. 1 www.procdings.bluchr.com.br/vnto/10wccm TOPOLOGY DESIG OF STRUCTURE LOADED BY EARTHQUAKE P. Rosko 1 1 Cntr of Mchanics and Structural Dynamics,

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Application of Uncertain Temporal Relations Algebra to Diagnostic Problems

Application of Uncertain Temporal Relations Algebra to Diagnostic Problems Appliation of Unrtain Tmporal Rlations Algbra to iagnosti Problms VLAIMIR RYAOV, VAGAN TERZIYAN partmnt of Computr Sin an Information Systms, partmnt of Mathmatial Information Thnology, Univrsity of Jyväskylä,

More information

AN IMPROVED CAPACITY SPECTRUM METHOD BASED ON INELASTIC DEMAND SPECTRA

AN IMPROVED CAPACITY SPECTRUM METHOD BASED ON INELASTIC DEMAND SPECTRA 4th Intrnational Confrnc on Earthquak Enginring Taipi, Taiwan Octobr 1-13, 006 Papr No. 30 AN IMPROVED CAPACITY SPECTRUM METHOD BASED ON INELASTIC DEMAND SPECTRA Xiao Mingkui 1, Dong Yinfng, Liu Gang 3,

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

More information

Development of Shear-key Consisted of Steel Disk and Anchor Bolt for Seismic Retrofitting

Development of Shear-key Consisted of Steel Disk and Anchor Bolt for Seismic Retrofitting Dvlopmnt of Shar-ky Consist of Stl Disk an Anchor olt for Sismic Rtrofitting. Takas & T. Ika Rsrch Institut of Tchnology, TOISHIMA Corporation, Japan. agisawa, T. Satoh & K. Imai Tchnological vlopmnt,

More information

ENGR 323 BHW 15 Van Bonn 1/7

ENGR 323 BHW 15 Van Bonn 1/7 ENGR 33 BHW 5 Van Bonn /7 4.4 In Eriss and 3 as wll as man othr situations on has th PDF o X and wishs th PDF o Yh. Assum that h is an invrtibl untion so that h an b solvd or to ild. Thn it an b shown

More information

Hybrid Inversion technique for predicting geometrical parameters of Porous Materials

Hybrid Inversion technique for predicting geometrical parameters of Porous Materials Aoustis 8 Paris Hybri Invrsion thniqu for priting gomtrial paramtrs of Porous Matrials P. hravag, P. Bonfiglio F. Pompoli Dipartimnto i Inggnria - Univrsity of Frrara, Via aragat 1, 441 Frrara, Italy franso.pompoli@unif.it

More information

Steinberg s Conjecture is false

Steinberg s Conjecture is false Stinrg s Conjtur is als arxiv:1604.05108v2 [math.co] 19 Apr 2016 Vinnt Cohn-Aa Mihal Hig Danil Král Zhntao Li Estan Salgao Astrat Stinrg onjtur in 1976 that vry planar graph with no yls o lngth our or

More information

CONFINEMENT REINFORCEMENT DESIGN FOR REINFORCED CONCRETE COLUMNS

CONFINEMENT REINFORCEMENT DESIGN FOR REINFORCED CONCRETE COLUMNS onfrnsi Nasional Tknik Sipil 3 (ontks 3) Jakarta, 6 7 Mi 2009 CONFINEMENT REINFORCEMENT DESIGN FOR REINFORCED CONCRETE COLUMNS Tavio 1 and Bnn usuma 2 1 Dpartmnt of Civil Enginring, Spuluh Nopmbr Institut

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-Classical States of the Simple Harmonic Oscillator Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats

More information

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit

More information

Online Supplement: Advance Selling in a Supply Chain under Uncertain Supply and Demand

Online Supplement: Advance Selling in a Supply Chain under Uncertain Supply and Demand Onlin Supplmnt Avanc Slling in a Supply Cain unr Uncrtain Supply an Dman. Proos o Analytical sults Proo o Lmma. Using a = minl 0 ; x g; w can rwrit () as ollows (x ; w ; x ; w ) = a +(m0 w )a +( +" x w

More information

SPH4U Electric Charges and Electric Fields Mr. LoRusso

SPH4U Electric Charges and Electric Fields Mr. LoRusso SPH4U lctric Chargs an lctric Fils Mr. LoRusso lctricity is th flow of lctric charg. Th Grks first obsrv lctrical forcs whn arly scintists rubb ambr with fur. Th notic thy coul attract small bits of straw

More information

Abstract Interpretation: concrete and abstract semantics

Abstract Interpretation: concrete and abstract semantics Abstract Intrprtation: concrt and abstract smantics Concrt smantics W considr a vry tiny languag that manags arithmtic oprations on intgrs valus. Th (concrt) smantics of th languags cab b dfind by th funzcion

More information

Logarithms. Secondary Mathematics 3 Page 164 Jordan School District

Logarithms. Secondary Mathematics 3 Page 164 Jordan School District Logarithms Sondary Mathmatis Pag 6 Jordan Shool Distrit Unit Clustr 6 (F.LE. and F.BF.): Logarithms Clustr 6: Logarithms.6 For ponntial modls, prss as a arithm th solution to a and d ar numrs and th as

More information

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

More information

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by: Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

Math 34A. Final Review

Math 34A. Final Review Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right

More information

INC 693, 481 Dynamics System and Modelling: Linear Graph Modeling II Dr.-Ing. Sudchai Boonto Assistant Professor

INC 693, 481 Dynamics System and Modelling: Linear Graph Modeling II Dr.-Ing. Sudchai Boonto Assistant Professor INC 69, 48 Dynamics Systm and Modlling: Linar Graph Modling II Dr.-Ing. Sudchai Boonto Assistant Profssor Dpartmnt of Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity of Tchnology Thonuri

More information

UNTYPED LAMBDA CALCULUS (II)

UNTYPED LAMBDA CALCULUS (II) 1 UNTYPED LAMBDA CALCULUS (II) RECALL: CALL-BY-VALUE O.S. Basic rul Sarch ruls: (\x.) v [v/x] 1 1 1 1 v v CALL-BY-VALUE EVALUATION EXAMPLE (\x. x x) (\y. y) x x [\y. y / x] = (\y. y) (\y. y) y [\y. y /

More information

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE 13 th World Confrnc on Earthquak Enginring Vancouvr, B.C., Canada August 1-6, 2004 Papr No. 2165 INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

More information

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS

NARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS . (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS

More information

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd 1. First you chck th domain of g x. For this function, x cannot qual zro. Thn w find th D domain of f g x D 3; D 3 0; x Q x x 1 3, x 0 2. Any cosin graph is going to b symmtric with th y-axis as long as

More information

Observer Bias and Reliability By Xunchi Pu

Observer Bias and Reliability By Xunchi Pu Obsrvr Bias and Rliability By Xunchi Pu Introduction Clarly all masurmnts or obsrvations nd to b mad as accuratly as possibl and invstigators nd to pay carful attntion to chcking th rliability of thir

More information

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1 F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.

More information

AP Calculus BC Problem Drill 16: Indeterminate Forms, L Hopital s Rule, & Improper Intergals

AP Calculus BC Problem Drill 16: Indeterminate Forms, L Hopital s Rule, & Improper Intergals AP Calulus BC Problm Drill 6: Indtrminat Forms, L Hopital s Rul, & Impropr Intrgals Qustion No. of Instrutions: () Rad th problm and answr hois arfully () Work th problms on papr as ndd () Pik th answr

More information

Integral Calculus What is integral calculus?

Integral Calculus What is integral calculus? Intgral Calulus What is intgral alulus? In diffrntial alulus w diffrntiat a funtion to obtain anothr funtion alld drivativ. Intgral alulus is onrnd with th opposit pross. Rvrsing th pross of diffrntiation

More information

Assignment 4 Biophys 4322/5322

Assignment 4 Biophys 4322/5322 Assignmnt 4 Biophys 4322/5322 Tylr Shndruk Fbruary 28, 202 Problm Phillips 7.3. Part a R-onsidr dimoglobin utilizing th anonial nsmbl maning rdriv Eq. 3 from Phillips Chaptr 7. For a anonial nsmbl p E

More information

ICCAD /96 $ IEEE

ICCAD /96 $ IEEE SIGMA: A Simulator or Sgmnt Dlay Faults Krthi Hragu Vishwani D. Agrawal Janak H. Patl Bll Labs, Lunt Thnologis Cntr or Rliabl an High-Prorman Computing 700 Mountain Avnu Univrsity o Illinois at Urbana-Champaign,

More information

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

Present state Next state Q + M N

Present state Next state Q + M N Qustion 1. An M-N lip-lop works s ollows: I MN=00, th nxt stt o th lip lop is 0. I MN=01, th nxt stt o th lip-lop is th sm s th prsnt stt I MN=10, th nxt stt o th lip-lop is th omplmnt o th prsnt stt I

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved.

6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved. 6.1 Intgration by Parts and Prsnt Valu Copyright Cngag Larning. All rights rsrvd. Warm-Up: Find f () 1. F() = ln(+1). F() = 3 3. F() =. F() = ln ( 1) 5. F() = 6. F() = - Objctivs, Day #1 Studnts will b

More information

NR3A-containing NMDA receptors promote neurotransmitter release and spike timing-dependent plasticity

NR3A-containing NMDA receptors promote neurotransmitter release and spike timing-dependent plasticity NR3A-ontaining NMDA rptors promot nurotransmittr rlas an spik timing-pnnt plastiity Rylan S. Larsn, Rkah J. Corlw, Mail A. Hnson, Aam C. Rorts, Masayoshi Mishina, Masahiko Watana, Stuart A. Lipton, Nouki

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

Network Congestion Games

Network Congestion Games Ntwork Congstion Gams Assistant Profssor Tas A&M Univrsity Collg Station, TX TX Dallas Collg Station Austin Houston Bst rout dpnds on othrs Ntwork Congstion Gams Travl tim incrass with congstion Highway

More information

Department of Mechanical Engineering, Imperial College, London SW7 2AZ, UK

Department of Mechanical Engineering, Imperial College, London SW7 2AZ, UK 1 ST Intrnational Confrn on Composit Matrials Xi an, 0 5 th August 017 THE MECHANICS OF INTERFACE FRACTURE IN LAYERED COMPOSITE MATERIALS: (7) ADHESION TOUHNESS OF MULTILAYER RAPHENE MEMRANES NANOSCALE

More information

MATH 1080 Test 2-SOLUTIONS Spring

MATH 1080 Test 2-SOLUTIONS Spring MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =

More information

Differentiation of Exponential Functions

Differentiation of Exponential Functions Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of

More information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

3 Finite Element Parametric Geometry

3 Finite Element Parametric Geometry 3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,

More information

SEISMIC RESPONSE OF SINGLE DEGREE OF FREEDOM STRUCTURAL FUSE SYSTEMS

SEISMIC RESPONSE OF SINGLE DEGREE OF FREEDOM STRUCTURAL FUSE SYSTEMS 3 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 4 Paper No. 377 SEISMIC RESPONSE OF SINGLE DEGREE OF FREEDOM STRUCTURAL FUSE SYSTEMS Ramiro VARGAS and Michel BRUNEAU

More information

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l h 4D, 4th Rank, Antisytric nsor and th 4D Equivalnt to th Cross Product or Mor Fun with nsors!!! Richard R Shiffan Digital Graphics Assoc 8 Dunkirk Av LA, Ca 95 rrs@isidu his docunt dscribs th four dinsional

More information

Three Concepts: Probability Henry Tirri, Petri Myllymäki

Three Concepts: Probability Henry Tirri, Petri Myllymäki 6..6 robability as a masur o bli Thr Conpts: robability Hnry Tirri, tri Myllymäki 998-6 56 robabilitis ar to b intrprtd Ditionary dinition: probability han liklihood probability? Thr Conpts: robability

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Notes on Vibration Design for Piezoelectric Cooling Fan

Notes on Vibration Design for Piezoelectric Cooling Fan World Aadmy of Sin, Enginring and Thnology Intrnational Journal of Mhanial and Mhatronis Enginring Vol:7, No:, 3 Nots on Vibration Dsign for Pizoltri Cooling Fan Thomas Jin-Ch Liu, Yu-Shn Chn, Hsi-Yang

More information