COMBINING SPATIAL COMPONENTS IN SEISMIC DESIGN

Size: px
Start display at page:

Download "COMBINING SPATIAL COMPONENTS IN SEISMIC DESIGN"

Transcription

1 Transactons, SMRT- COMBINING SPATIAL COMPONENTS IN SEISMIC DESIGN Mchae O Leary, PhD, PE and Kevn Huberty, PE, SE Nucear Power Technooges Dvson, Sargent & Lundy, Chcago, IL 6060 ABSTRACT Accordng to Reguatory Gude.9 [], the square root of the sum of the squares (SRSS) method and the rue are acceptabe means of combnng spata components n sesmc desgn. The two methods are compared n order to carfy ther proper mpementaton and to dentfy the advantages of each approach wth respect to the fnte eement-based desgn process common throughout the nucear ndustry. The excess conservatsm and the manpuaton of the sgns of mutpe response parameters requred for the adequate mpementaton of the SRSS method mae the rue a better approach for desgn. INTRODUCTION The two-step method s a common ndustry approach to ncorporate the effects of so-structure nteracton (SSI) anayss nto the desgn of new concrete nucear structures. The frst step s to perform the SSI anayss and the second step s to mae an equvaent statc sesmc fnte eement mode based on the SSI anayss resuts. Typcay the noda zero perod acceeratons (ZPA) from the SSI anayss resuts are mutped by ther trbutary mass to determne equvaent statc sesmc forces assocated wth a horzonta or vertca nput moton. These forces are apped to a three-dmensona equvaent statc sesmc fnte eement mode and combned usng the SRSS method or the percent combnaton rue n accordance wth Reguatory Gude.9 []. The two-step method offers a fexbe and practca approach to new desgn. If a coarser mesh s requred n the SSI anayss mode due to computatona mtatons, for exampe, the two-step method can accommodate a more refned mesh n the desgn mode. Snce a of the equvaent statc forces assocated wth the noda acceeratons act n phase, t s generay accepted that the two-step approach s conservatve []. The fowchart n Fgure summarzes ths concrete desgn process. Two acceptabe methods for combnng spata components n sesmc desgn (SRSS and rue) n Reguatory Gude.9 [] are compared n order to carfy ther proper mpementaton and to dentfy the advantages of each approach wthn the context of the desgn process common throughout the nucear ndustry. COMBINATION OF THREE-DIMENSIONAL EARTHQUAKE EFFECTS AND MULITPLE RESPONSE PARAMETERS In accordance wth Reguatory Gude.9 [], the SRSS combnaton of three-dmensona earthquae effects s R= RI, () I = where R s any response of nterest and R I s the combned response for the I th component of sesmc nput moton (e.g., x, y, or z component). ASCE 4-98 [4] adds that the SRSS method shoud ncude postve and negatve permutatons of the response.

2 SSI anayss Extract maxmum noda ZPAs and mutpy by the trbutary mass n an equvaent statc sesmc FE mode Post-process oad combnatons Determne requred renforcement that satsfes statc and dynamc demand for a structura members Fgure : Sesmc anayss and desgn process for concrete nucear structures. The rue s defned n Reguatory Gude.9 [] as ( ) R = R + R + R () where R, R, and R are the maxmum responses of the structure caused by each of the three earthquae components such that R R R. In ASCE 4-98 [4], a possbe twenty-four permutatons of the rue are made expct by the foowng expresson: [ ] or [ ] or [ ] R =± R ± R ± R ± R ± R ± R ± R ± R ± R. () The prncpe advantage of equaton () over () s that the drectona nature of the oad s made expct n the expresson. Moreover, the response R from equaton () w aways be equa to or greater than the response R from equaton (). Therefore, when the rue s nvoed throughout the remander of ths paper, the twenty-four responses contaned n equaton () are mped. As ndcated n On the Correct Appcaton of the Rue [], f the methodoogy prescrbed n ASCE 4-98 [4] for determnng the maxmum sesmc desgn forces s foowed, the rue s neary aways conservatve reatve to the SRSS method. Secton..7.. of ASCE 4-98 [4] states that when there s more than one response parameter, such as coumn axa force and moment, to be used n the desgn cacuaton, the combned vaue sha be cacuated. In other words, whether the rue or SRSS method s used to determne the co-drectona response from three earthquae components, the maxmum axa force sha be combned wth the maxmum moment for desgn. By contrast, secton C4.. of ASCE 4- (draft verson) [5] recommends n cases nvovng mutpe nteractng desgn parameters the maxmum vaue of each desgn parameter [s consdered] together wth the vaues of the other parameters that correspond to the same drectona combnaton. Indeed, the purpose of a sesmc mode s to conservatvey represent maxmum oadng condtons. A bref revew of tme hstory anayss resuts reveas that the maxmum forces from mutpe parameters rarey, f ever, occur at the same tme step. Snce the maxmum axa force amost never occurs at the same tme as the

3 maxmum bendng moment, the revsed ASCE 4- (draft verson) [5] approach resuts n more reasonabe renforcement whe mantanng the conservatsm requred n sesmc desgn. Under the ASCE 4- (draft verson) [5] approach, however, the SRSS method s amost aways more conservatve than the rue, as can be seen n the foowng exampe. COLUMN EXAMPLE Consder a smpe 0 ft coumn wth a ft by ft cross secton. The sesmc responses due to the x, y, and z drecton exctatons are each equa to 0 ps apped at the top of the coumn: R x = R y = R z = 0 ps. As can be seen n Tabe, the rue yeds the maxmum snge response parameter hghghted n red, but these parameters nteract wth ower correspondng response parameters. Subsequenty, M x and M y ponts from rue may fa wthn the baxa nteracton surface where the SRRS ponts do not due to the hgher correspondng axa oad as shown schematcay n Fgure. Furthermore, f there s a torsona component to the sesmc response, the maxmum torson does not tend occur n the same oad combnaton as the maxmum shear force under the rue. Agan, whe the maxmum torson due to the SRSS method may be ower than the rue, the correspondng shear force s typcay hgher and subsequenty more crtca. P M x x M y Pane of P = P y P M x Pane of P = 0 Pane of P = 9. Pane of P = 4 M y Pane of P = 9. SRSS P M x M y M x M y Fgure : Schematc baxa nteracton curve. Pane of P =

4 Tabe : Mutpe response parameters (absoute vaues) for a 0 ft coumn where R x = R y = R z = 0 ps. Combnaton P M x (p-ft) M y (p-ft) V x V y SRSS SHEAR WALL FINITE ELEMENT MODEL The test mode shown n Fgures 4 s three stores hgh wth three bays n both drectons. There s a twenty foot span between each of the three bays. The three foors are spaced at 8 feet and the sabs are 0 nches thc. The three openngs shown n Fgure 4 are ony found on the second foor. A was, ncudng the two nteror shear was are two feet thc. For ths study, the fxed base mode s frst subected to the three orthogona tme hstores shown n Fgure 5. The maxmum absoute acceeratons from a three tme hstory anayses are extracted and combned by the SRSS method. These three orthogona acceeratons are mutped by ther trbutary masses to determne an x, y, and z drecton equvaent statc force. These three forces are then combned by means of the SRSS method and the rue. Athough the fxed-base acceeratons are not dentca to SSI anayss, the process of determnng equvaent statc sesmc forces s the same. y z x Fgure : Fnte eement test mode.

5 Fgure 4: Mode foor pan and eevaton. Acceeraton (g) Tme (sec) a.) X drecton exctaton. Acceeraton (g) Tme (sec) b.) Y drecton exctaton.

6 Acceeraton (g) Tme (sec) c.) Z drecton exctaton. Fgure 5: Tme hstores used n the fxed base tme hstory anayses. RESULTS The maxmum anaytca resuts for vertca axa forces n the nteror wa dentfed n Fgure are shown n Fgure 6. In order to compare the accuracy of the oad path, the maxmum tme hstory anayss resuts are shown aong wth the rue and the SRSS method resuts. Snce the three tme hstory cases are anayzed separatey, ony the resuts from the domnant drectona oad are shown. The maxmum anaytca resuts for vertca axa forces n the exteror wa dentfed n Fgure are shown n Fgure 7. Tabes and provde the sum of the eement forces aong the bottom of the nteror and exteror shear was hghghted n Fgure, respectvey for the oad combnatons where the n-pane shear forces are greatest n magntude. The n-pane moment s cacuated by summng the moment of the vertca eement forces of the bottom row of eements about the geometrc center of the wa: n w M n pane = F x = (4) where F represents the force assocated wth the bottom face of the n th eement, w s the entre wa ength, and x s the force ocaton reatve to the center ne of the wa. Athough the sgn of the SRSS axa forces are postve across the entre ength of the shear wa, t s assumed that a the forces on one sde of the geometrc center of the wa are postve and a the forces on the other sde are negatve n determnng the n-pane moment. None of the resuts ncude the effect of the dead oad on the structure. Ony the anaytca resuts of the equvaent statc nerta oads are shown.

7 SRSS Y drecton tme hstory Fgure 6: Maxmum vertca axa eement forces (ps/ft) n the nteror wa for the rue, the SRSS method, and the y drecton tme hstory anayss at tme step seconds SRSS X drecton tme hstory Fgure 7: Maxmum vertca axa eement forces (ps/ft) n the exteror wa for the rue, the SRSS method, and the x drecton tme hstory anayss at tme step.45 seconds.

8 Tabe : Maxmum eement forces summed up aong the bottom of the nteror shear wa Load combnaton Equvaent statc (-)40-00-(-)40 Equvaent statc SRSS Tme hstory at t = sec ( ) Tme hstory at t = sec (SRSS) Out-ofpane shear In-pane shear Axa force Out-of-pane moment (p-ft) In-pane moment (p-ft) Tabe : Maxmum eement forces summed up aong the bottom of the exteror shear wa Load combnaton Equvaent statc (-)00-40-(-)40 Equvaent statc SRSS Tme hstory at t =.45 sec ( ) Tme hstory at t =.45 sec (SRSS) Out-ofpane shear In-pane shear Axa force Out-of-pane moment (p-ft) In-pane moment (p-ft) DISCUSSION The axa eement force pots of the , SRSS, and tme hstory oad cases shown n Fgures 6 and 7 are smar n terms of magntude and oad dstrbuton. The maxmum mutpe response parameters reported n Tabes and echo the nteracton shown n Tabe for the coumn exampe. Whe the maxmum snge response occurs n one of the twenty-four permutatons of the rue, t nteracts wth ower correspondng response parameters than the SRSS oad. Moreover, the crtca response parameters n the drecton of the earthquae oad, ncudng the n-pane shear, and n-pane moment forces, are smar for both the rue and the SRSS method. The correspondng SRSS axa forces n both the nteror and exteror was are we over twce the magntude of the rue axa forces, however. As a resut, the SRSS method s more an to usng a combnaton rue for desgnng a shear wa for axa force and moment. Asde from the excess conservatsm of the SRSS method, the eement force pots shown n Fgures 6 and 7 ndcate a potenta probem n ts mpementaton. As expaned above, the ony way to obtan the n-pane moment from the eement resuts s to manuay reverse the sgn of the axa force on ether sde of the geometrc center of the shear wa. Wth more compcated structures typca n nucear concrete desgn n whch mutpe was and sabs frame nto shear was wth openngs, ths approach

9 cannot be easy mpemented, however. The actua drectona oad path s requred to determne the npane moment. Fnay, a resuts combned by the SRSS method are postve or negatve. But as secton cut force Tabes and revea, mutpe response parameters from drectona oads do not necessary have the same sgn. Therefore, uness the anayst manpuates the sgn of response parameters as part of a postprocessng routne, the SRSS method potentay msses oad combnatons n whch the sesmc response parameter nteracts constructvey wth dead or ve oad response parameters, for exampe. Fgure 8 ustrates the sgn conventon for she eements. Tabes 4 and 5 st the permutatons of the sesmc response for she eements and frame eements that are mssed by the postve and negatve mpementaton of equaton (). Athough the number of requred permutatons for frame eements n Tabe 5 s greater than the number of she permutatons, the permutatons requred to account for n-pane moment when the SRSS method s used are not ncuded Tabe 5. (-)N (-)N (-)N Tenson Compresson Tenson Compresson (compresson) (-)N (compresson) (-)M Compresson Tenson (+)M (-)M Compresson (+)M Tenson (+)N (+)N (tenson) (+)N (+)N (tenson) (+)M (-)M Fgure 8: She eement sgn conventon. Tabe 4: Requred she eement permutatons for SRSS. Permutaton N M N M M F V V +SRSS SRSS Not captured Not captured

10 Tabe 5: Requred frame eement permutatons for SRSS. Permutaton P M x M y +SRSS SRSS Not captured Not captured Not captured Not captured Not captured Not captured CONCLUSION Ths study has confrmed the conservatsm of the rue reatve to the SRSS method for a snge response parameter as we the conservatsm of the SRSS method when mutpe response parameters are consdered. Both methods of combnng spata components of earthquaes n determnng equvaent statc oads are acceptabe accordng to Reguatory Gude.9 [] and both methods adequatey enveop the crtca forces from tme hstory anayss. In ths respect, the rue s preferred for desgn snce the fna renforcement w be ess congested than a desgn based on the SRSS method. Both methods aso requre permutatons of sgns to adequatey capture the most crtca oad combnatons. The advantage of the rue s that the permutatons of the oads are requred before anayss, whch s a reatvey smpe tas. The SRSS method, on the other hand, requres manpuaton of the sgn of ndvdua response parameters outsde of the fnte eement anayss. And for a more compcated structure usng the SRSS method, there may be no cear way of evauatng n-pane moment. In concuson, the drectona nature of the oads and the reatve smpcty of ts mpementaton mae t preferabe to the SRSS method. ACKNOWLEDGMENTS The authors gratefuy acnowedge Andrew Bomqust and Wam Godfrey of Sargent & Lundy for ther assstance n preparng the fnte eement modes and certan fgures. REFERENCES [] U.S. Nucear Reguatory Commsson. (0). Reguatory Gude.9, Combnng Moda Responses and Spata Components n Sesmc Response Anayss, Revson. [] Watns, D., Gürbüz, O., and Ma, T. (006). Two-step method of sesmc anayss, Proc., Frst European Conference on Earthquae Engneerng and Sesmoogy, Geneva, Swtzerand. [] Ne, J., Morante, R., Mranda, M., and Braverman, J. (00). On the correct appcaton of the rue for combnng responses due to three drectons of earthquae oadng, Proc., ASME 00 Pressure Vesses and Ppng Dvson, Beevue, WA. [4] Amercan Socety of Cv Engneers. (000). ASCE 4-98: Sesmc Anayss of Safety-Reated Nucear Structures, Revson. [5] Amercan Socety of Cv Engneers. (0). ASCE 4-: Sesmc Anayss of Safety-Reated Nucear Structures, Draft.

Strain Energy in Linear Elastic Solids

Strain Energy in Linear Elastic Solids Duke Unverst Department of Cv and Envronmenta Engneerng CEE 41L. Matr Structura Anass Fa, Henr P. Gavn Stran Energ n Lnear Eastc Sods Consder a force, F, apped gradua to a structure. Let D be the resutng

More information

LECTURE 21 Mohr s Method for Calculation of General Displacements. 1 The Reciprocal Theorem

LECTURE 21 Mohr s Method for Calculation of General Displacements. 1 The Reciprocal Theorem V. DEMENKO MECHANICS OF MATERIALS 05 LECTURE Mohr s Method for Cacuaton of Genera Dspacements The Recproca Theorem The recproca theorem s one of the genera theorems of strength of materas. It foows drect

More information

Neural network-based athletics performance prediction optimization model applied research

Neural network-based athletics performance prediction optimization model applied research Avaabe onne www.jocpr.com Journa of Chemca and Pharmaceutca Research, 04, 6(6):8-5 Research Artce ISSN : 0975-784 CODEN(USA) : JCPRC5 Neura networ-based athetcs performance predcton optmzaton mode apped

More information

Chapter 6. Rotations and Tensors

Chapter 6. Rotations and Tensors Vector Spaces n Physcs 8/6/5 Chapter 6. Rotatons and ensors here s a speca knd of near transformaton whch s used to transforms coordnates from one set of axes to another set of axes (wth the same orgn).

More information

REAL-TIME IMPACT FORCE IDENTIFICATION OF CFRP LAMINATED PLATES USING SOUND WAVES

REAL-TIME IMPACT FORCE IDENTIFICATION OF CFRP LAMINATED PLATES USING SOUND WAVES 8 TH INTERNATIONAL CONERENCE ON COMPOSITE MATERIALS REAL-TIME IMPACT ORCE IDENTIICATION O CRP LAMINATED PLATES USING SOUND WAVES S. Atobe *, H. Kobayash, N. Hu 3 and H. ukunaga Department of Aerospace

More information

Research on Complex Networks Control Based on Fuzzy Integral Sliding Theory

Research on Complex Networks Control Based on Fuzzy Integral Sliding Theory Advanced Scence and Technoogy Letters Vo.83 (ISA 205), pp.60-65 http://dx.do.org/0.4257/ast.205.83.2 Research on Compex etworks Contro Based on Fuzzy Integra Sdng Theory Dongsheng Yang, Bngqng L, 2, He

More information

Note 2. Ling fong Li. 1 Klein Gordon Equation Probablity interpretation Solutions to Klein-Gordon Equation... 2

Note 2. Ling fong Li. 1 Klein Gordon Equation Probablity interpretation Solutions to Klein-Gordon Equation... 2 Note 2 Lng fong L Contents Ken Gordon Equaton. Probabty nterpretaton......................................2 Soutons to Ken-Gordon Equaton............................... 2 2 Drac Equaton 3 2. Probabty nterpretaton.....................................

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: Instructor s Name and Secton: (Crcle Your Secton) Sectons:

More information

3. Stress-strain relationships of a composite layer

3. Stress-strain relationships of a composite layer OM PO I O U P U N I V I Y O F W N ompostes ourse 8-9 Unversty of wente ng. &ech... tress-stran reatonshps of a composte ayer - Laurent Warnet & emo Aerman.. tress-stran reatonshps of a composte ayer Introducton

More information

A finite difference method for heat equation in the unbounded domain

A finite difference method for heat equation in the unbounded domain Internatona Conerence on Advanced ectronc Scence and Technoogy (AST 6) A nte derence method or heat equaton n the unbounded doman a Quan Zheng and Xn Zhao Coege o Scence North Chna nversty o Technoogy

More information

[WAVES] 1. Waves and wave forces. Definition of waves

[WAVES] 1. Waves and wave forces. Definition of waves 1. Waves and forces Defnton of s In the smuatons on ong-crested s are consdered. The drecton of these s (μ) s defned as sketched beow n the goba co-ordnate sstem: North West East South The eevaton can

More information

Cyclic Codes BCH Codes

Cyclic Codes BCH Codes Cycc Codes BCH Codes Gaos Feds GF m A Gaos fed of m eements can be obtaned usng the symbos 0,, á, and the eements beng 0,, á, á, á 3 m,... so that fed F* s cosed under mutpcaton wth m eements. The operator

More information

Associative Memories

Associative Memories Assocatve Memores We consder now modes for unsupervsed earnng probems, caed auto-assocaton probems. Assocaton s the task of mappng patterns to patterns. In an assocatve memory the stmuus of an ncompete

More information

SPATIAL KINEMATICS OF GEARS IN ABSOLUTE COORDINATES

SPATIAL KINEMATICS OF GEARS IN ABSOLUTE COORDINATES SATIAL KINEMATICS OF GEARS IN ABSOLUTE COORDINATES Dmtry Vasenko and Roand Kasper Insttute of Mobe Systems (IMS) Otto-von-Guercke-Unversty Magdeburg D-39016, Magdeburg, Germany E-ma: Dmtr.Vasenko@ovgu.de

More information

Drift Design Method for High-rise Buildings using Dynamic Resizing Algorithm

Drift Design Method for High-rise Buildings using Dynamic Resizing Algorithm ctbuh.org/papers Tte: Authors: Subject: Keywords: Drft Desgn Method for Hgh-rse Budngs usng Dynac Reszng Agorth Hyo Seon Park, Ph.D Canddate, Yonse Unversty Seo J Hyun, Assocate Professor, Yonse Unversty

More information

Development of whole CORe Thermal Hydraulic analysis code CORTH Pan JunJie, Tang QiFen, Chai XiaoMing, Lu Wei, Liu Dong

Development of whole CORe Thermal Hydraulic analysis code CORTH Pan JunJie, Tang QiFen, Chai XiaoMing, Lu Wei, Liu Dong Deveopment of whoe CORe Therma Hydrauc anayss code CORTH Pan JunJe, Tang QFen, Cha XaoMng, Lu We, Lu Dong cence and technoogy on reactor system desgn technoogy, Nucear Power Insttute of Chna, Chengdu,

More information

On the general evaluation of the maximum allowable drift at the top of shear walls (constant and variable stiffness)

On the general evaluation of the maximum allowable drift at the top of shear walls (constant and variable stiffness) Internatona Journa of Cv Engneerng and Constructon Scence 4; (): 8-5 Pubshed onne June, 4 (http://www.aasct.org/ourna/cecs) On the genera evauaton of the maxmum aowabe drft at the top of shear was (constant

More information

EXPERIMENT AND THEORISATION: AN APPLICATION OF THE HYDROSTATIC EQUATION AND ARCHIMEDES THEOREM

EXPERIMENT AND THEORISATION: AN APPLICATION OF THE HYDROSTATIC EQUATION AND ARCHIMEDES THEOREM EXPERIMENT AND THEORISATION: AN APPLICATION OF THE HYDROSTATIC EQUATION AND ARCHIMEDES THEOREM Santos Lucía, Taaa Máro, Departamento de Físca, Unversdade de Avero, Avero, Portuga 1. Introducton Today s

More information

Image Classification Using EM And JE algorithms

Image Classification Using EM And JE algorithms Machne earnng project report Fa, 2 Xaojn Sh, jennfer@soe Image Cassfcaton Usng EM And JE agorthms Xaojn Sh Department of Computer Engneerng, Unversty of Caforna, Santa Cruz, CA, 9564 jennfer@soe.ucsc.edu

More information

Structural analysis - displacement method for planar frames and gridworks

Structural analysis - displacement method for planar frames and gridworks Structura anayss - dspacement method for panar frames and grdworks Petr Řeřcha October, 6 Contents Summary of the sope defecton method notaton and formuas Dspacement method for panar frames. End forces

More information

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. ME 270 Fall 2012 Fnal Exam Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: INSTRUCTIONS Begn each problem

More information

Optimum Selection Combining for M-QAM on Fading Channels

Optimum Selection Combining for M-QAM on Fading Channels Optmum Seecton Combnng for M-QAM on Fadng Channes M. Surendra Raju, Ramesh Annavajjaa and A. Chockangam Insca Semconductors Inda Pvt. Ltd, Bangaore-56000, Inda Department of ECE, Unversty of Caforna, San

More information

ON AUTOMATIC CONTINUITY OF DERIVATIONS FOR BANACH ALGEBRAS WITH INVOLUTION

ON AUTOMATIC CONTINUITY OF DERIVATIONS FOR BANACH ALGEBRAS WITH INVOLUTION European Journa of Mathematcs and Computer Scence Vo. No. 1, 2017 ON AUTOMATC CONTNUTY OF DERVATONS FOR BANACH ALGEBRAS WTH NVOLUTON Mohamed BELAM & Youssef T DL MATC Laboratory Hassan Unversty MORO CCO

More information

GROUND LATERAL SPREAD EFFECTS ON SINGLE PILE USING UNCOUPLED ANALYSIS METHOD

GROUND LATERAL SPREAD EFFECTS ON SINGLE PILE USING UNCOUPLED ANALYSIS METHOD Journa of GeoEngneerng, Vo., No. San-Shyan, pp. 5-, Ln, December et a.: Ground Latera Spread Effects on Snge Pe Usng Uncouped Anayss Method 5 GROUND LATERAL SPREAD EFFECTS ON SINGLE PILE USING UNCOUPLED

More information

Numerical Investigation of Power Tunability in Two-Section QD Superluminescent Diodes

Numerical Investigation of Power Tunability in Two-Section QD Superluminescent Diodes Numerca Investgaton of Power Tunabty n Two-Secton QD Superumnescent Dodes Matta Rossett Paoo Bardea Ivo Montrosset POLITECNICO DI TORINO DELEN Summary 1. A smpfed mode for QD Super Lumnescent Dodes (SLD)

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. ME 270 Summer 2014 Fnal Exam NAME (Last, Frst): Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: INSTRUCTIONS

More information

9.2 Seismic Loads Using ASCE Standard 7-93

9.2 Seismic Loads Using ASCE Standard 7-93 CHAPER 9: Wnd and Sesmc Loads on Buldngs 9.2 Sesmc Loads Usng ASCE Standard 7-93 Descrpton A major porton of the Unted States s beleved to be subject to sesmc actvty suffcent to cause sgnfcant structural

More information

Predicting Model of Traffic Volume Based on Grey-Markov

Predicting Model of Traffic Volume Based on Grey-Markov Vo. No. Modern Apped Scence Predctng Mode of Traffc Voume Based on Grey-Marov Ynpeng Zhang Zhengzhou Muncpa Engneerng Desgn & Research Insttute Zhengzhou 5005 Chna Abstract Grey-marov forecastng mode of

More information

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project SE 8 Fnal Project Story Shear Frame u m Gven: u m L L m L L EI ω ω Solve for m Story Bendng Beam u u m L m L Gven: m L L EI ω ω Solve for m 3 3 Story Shear Frame u 3 m 3 Gven: L 3 m m L L L 3 EI ω ω ω

More information

Uncertainty Specification and Propagation for Loss Estimation Using FOSM Methods

Uncertainty Specification and Propagation for Loss Estimation Using FOSM Methods Uncertanty Specfcaton and Propagaton for Loss Estmaton Usng FOSM Methods J.W. Baer and C.A. Corne Dept. of Cv and Envronmenta Engneerng, Stanford Unversty, Stanford, CA 94305-400 Keywords: Sesmc, oss estmaton,

More information

Lower bounds for the Crossing Number of the Cartesian Product of a Vertex-transitive Graph with a Cycle

Lower bounds for the Crossing Number of the Cartesian Product of a Vertex-transitive Graph with a Cycle Lower bounds for the Crossng Number of the Cartesan Product of a Vertex-transtve Graph wth a Cyce Junho Won MIT-PRIMES December 4, 013 Abstract. The mnmum number of crossngs for a drawngs of a gven graph

More information

DUE: WEDS FEB 21ST 2018

DUE: WEDS FEB 21ST 2018 HOMEWORK # 1: FINITE DIFFERENCES IN ONE DIMENSION DUE: WEDS FEB 21ST 2018 1. Theory Beam bendng s a classcal engneerng analyss. The tradtonal soluton technque makes smplfyng assumptons such as a constant

More information

The work described by this report was supported by NSF under contract

The work described by this report was supported by NSF under contract BINAR ULTIPLICATION UING PARTIALL REDUNDANT ULTIPLE Gary Bewck chae J. Fynn Technca Report No. CL-TR-92-528 June 992 The work descrbed by ths report was supported by NF under contract IP88-2296 BINAR ULTIPLICATION

More information

THRUST NETWORK ANALYSIS: A NEW METHODOLOGY FOR THREE-DIMENSIONAL EQUILIBRIUM

THRUST NETWORK ANALYSIS: A NEW METHODOLOGY FOR THREE-DIMENSIONAL EQUILIBRIUM TRUST NETWORK ANALYSIS: A NEW METODOLOGY FOR TREE-DIMENSIONAL EQUILIBRIUM Phppe BLOCK Research Assstant Budng Technoogy, MIT Cambrdge, MA, USA John OCSENDORF Assocate Professor Budng Technoogy, MIT Cambrdge,

More information

A DIMENSION-REDUCTION METHOD FOR STOCHASTIC ANALYSIS SECOND-MOMENT ANALYSIS

A DIMENSION-REDUCTION METHOD FOR STOCHASTIC ANALYSIS SECOND-MOMENT ANALYSIS A DIMESIO-REDUCTIO METHOD FOR STOCHASTIC AALYSIS SECOD-MOMET AALYSIS S. Rahman Department of Mechanca Engneerng and Center for Computer-Aded Desgn The Unversty of Iowa Iowa Cty, IA 52245 June 2003 OUTLIE

More information

A Mechanics-Based Approach for Determining Deflections of Stacked Multi-Storey Wood-Based Shear Walls

A Mechanics-Based Approach for Determining Deflections of Stacked Multi-Storey Wood-Based Shear Walls A Mechancs-Based Approach for Determnng Deflectons of Stacked Mult-Storey Wood-Based Shear Walls FPINNOVATIONS Acknowledgements Ths publcaton was developed by FPInnovatons and the Canadan Wood Councl based

More information

COXREG. Estimation (1)

COXREG. Estimation (1) COXREG Cox (972) frst suggested the modes n whch factors reated to fetme have a mutpcatve effect on the hazard functon. These modes are caed proportona hazards (PH) modes. Under the proportona hazards

More information

we have E Y x t ( ( xl)) 1 ( xl), e a in I( Λ ) are as follows:

we have E Y x t ( ( xl)) 1 ( xl), e a in I( Λ ) are as follows: APPENDICES Aendx : the roof of Equaton (6 For j m n we have Smary from Equaton ( note that j '( ( ( j E Y x t ( ( x ( x a V ( ( x a ( ( x ( x b V ( ( x b V x e d ( abx ( ( x e a a bx ( x xe b a bx By usng

More information

SCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.

SCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors. SCALARS AND ECTORS All phscal uanttes n engneerng mechancs are measured usng ether scalars or vectors. Scalar. A scalar s an postve or negatve phscal uantt that can be completel specfed b ts magntude.

More information

Multispectral Remote Sensing Image Classification Algorithm Based on Rough Set Theory

Multispectral Remote Sensing Image Classification Algorithm Based on Rough Set Theory Proceedngs of the 2009 IEEE Internatona Conference on Systems Man and Cybernetcs San Antono TX USA - October 2009 Mutspectra Remote Sensng Image Cassfcaton Agorthm Based on Rough Set Theory Yng Wang Xaoyun

More information

QUARTERLY OF APPLIED MATHEMATICS

QUARTERLY OF APPLIED MATHEMATICS QUARTERLY OF APPLIED MATHEMATICS Voume XLI October 983 Number 3 DIAKOPTICS OR TEARING-A MATHEMATICAL APPROACH* By P. W. AITCHISON Unversty of Mantoba Abstract. The method of dakoptcs or tearng was ntroduced

More information

The line method combined with spectral chebyshev for space-time fractional diffusion equation

The line method combined with spectral chebyshev for space-time fractional diffusion equation Apped and Computatona Mathematcs 014; 3(6): 330-336 Pubshed onne December 31, 014 (http://www.scencepubshnggroup.com/j/acm) do: 10.1164/j.acm.0140306.17 ISS: 3-5605 (Prnt); ISS: 3-5613 (Onne) The ne method

More information

Decentralized Adaptive Control for a Class of Large-Scale Nonlinear Systems with Unknown Interactions

Decentralized Adaptive Control for a Class of Large-Scale Nonlinear Systems with Unknown Interactions Decentrazed Adaptve Contro for a Cass of Large-Scae onnear Systems wth Unknown Interactons Bahram Karm 1, Fatemeh Jahangr, Mohammad B. Menhaj 3, Iman Saboor 4 1. Center of Advanced Computatona Integence,

More information

Lower Bounding Procedures for the Single Allocation Hub Location Problem

Lower Bounding Procedures for the Single Allocation Hub Location Problem Lower Boundng Procedures for the Snge Aocaton Hub Locaton Probem Borzou Rostam 1,2 Chrstoph Buchhem 1,4 Fautät für Mathemat, TU Dortmund, Germany J. Faban Meer 1,3 Uwe Causen 1 Insttute of Transport Logstcs,

More information

D hh ν. Four-body charm semileptonic decay. Jim Wiss University of Illinois

D hh ν. Four-body charm semileptonic decay. Jim Wiss University of Illinois Four-body charm semeptonc decay Jm Wss Unversty of Inos D hh ν 1 1. ector domnance. Expected decay ntensty 3. SU(3) apped to D s φν 4. Anaytc forms for form factors 5. Non-parametrc form factors 6. Future

More information

Xin Li Department of Information Systems, College of Business, City University of Hong Kong, Hong Kong, CHINA

Xin Li Department of Information Systems, College of Business, City University of Hong Kong, Hong Kong, CHINA RESEARCH ARTICLE MOELING FIXE OS BETTING FOR FUTURE EVENT PREICTION Weyun Chen eartment of Educatona Informaton Technoogy, Facuty of Educaton, East Chna Norma Unversty, Shangha, CHINA {weyun.chen@qq.com}

More information

Inthem-machine flow shop problem, a set of jobs, each

Inthem-machine flow shop problem, a set of jobs, each THE ASYMPTOTIC OPTIMALITY OF THE SPT RULE FOR THE FLOW SHOP MEAN COMPLETION TIME PROBLEM PHILIP KAMINSKY Industra Engneerng and Operatons Research, Unversty of Caforna, Bereey, Caforna 9470, amnsy@eor.bereey.edu

More information

Structural Dynamics and Earthquake Engineering

Structural Dynamics and Earthquake Engineering Structural Dynamcs and Earthuake Engneerng Course 9 Sesmc-resstant desgn of structures (1) Sesmc acton Methods of elastc analyss Course notes are avalable for download at http://www.ct.upt.ro/users/aurelstratan/

More information

Second Order Analysis

Second Order Analysis Second Order Analyss In the prevous classes we looked at a method that determnes the load correspondng to a state of bfurcaton equlbrum of a perfect frame by egenvalye analyss The system was assumed to

More information

CHAPTER 4. Vector Spaces

CHAPTER 4. Vector Spaces man 2007/2/16 page 234 CHAPTER 4 Vector Spaces To crtcze mathematcs for ts abstracton s to mss the pont entrel. Abstracton s what makes mathematcs work. Ian Stewart The man am of ths tet s to stud lnear

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. NME (Last, Frst): Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: INSTRUCTIONS Begn each problem n the space

More information

Application of Particle Swarm Optimization to Economic Dispatch Problem: Advantages and Disadvantages

Application of Particle Swarm Optimization to Economic Dispatch Problem: Advantages and Disadvantages Appcaton of Partce Swarm Optmzaton to Economc Dspatch Probem: Advantages and Dsadvantages Kwang Y. Lee, Feow, IEEE, and Jong-Bae Par, Member, IEEE Abstract--Ths paper summarzes the state-of-art partce

More information

Remark: Positive work is done on an object when the point of application of the force moves in the direction of the force.

Remark: Positive work is done on an object when the point of application of the force moves in the direction of the force. Unt 5 Work and Energy 5. Work and knetc energy 5. Work - energy theore 5.3 Potenta energy 5.4 Tota energy 5.5 Energy dagra o a ass-sprng syste 5.6 A genera study o the potenta energy curve 5. Work and

More information

Module 11 Design of Joints for Special Loading. Version 2 ME, IIT Kharagpur

Module 11 Design of Joints for Special Loading. Version 2 ME, IIT Kharagpur Module 11 Desgn o Jonts or Specal Loadng Verson ME, IIT Kharagpur Lesson 1 Desgn o Eccentrcally Loaded Bolted/Rveted Jonts Verson ME, IIT Kharagpur Instructonal Objectves: At the end o ths lesson, the

More information

Buckling of laminated glass columns

Buckling of laminated glass columns Buckng of amnated gass coumns Johan Baauwendraad Facuty of Cv Engneerng and Geoscences, Deft Unversty of Technoogy, Deft, the Netherands The buckng force of a amnated gass coumn s hghy dependent on the

More information

Dynamic Analysis Of An Off-Road Vehicle Frame

Dynamic Analysis Of An Off-Road Vehicle Frame Proceedngs of the 8th WSEAS Int. Conf. on NON-LINEAR ANALYSIS, NON-LINEAR SYSTEMS AND CHAOS Dnamc Anass Of An Off-Road Vehce Frame ŞTEFAN TABACU, NICOLAE DORU STĂNESCU, ION TABACU Automotve Department,

More information

Distributed Moving Horizon State Estimation of Nonlinear Systems. Jing Zhang

Distributed Moving Horizon State Estimation of Nonlinear Systems. Jing Zhang Dstrbuted Movng Horzon State Estmaton of Nonnear Systems by Jng Zhang A thess submtted n parta fufment of the requrements for the degree of Master of Scence n Chemca Engneerng Department of Chemca and

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

I have not received unauthorized aid in the completion of this exam.

I have not received unauthorized aid in the completion of this exam. ME 270 Sprng 2013 Fnal Examnaton Please read and respond to the followng statement, I have not receved unauthorzed ad n the completon of ths exam. Agree Dsagree Sgnature INSTRUCTIONS Begn each problem

More information

Simulations and Trajectory Tracking of Two Manipulators Manipulating a Flexible Payload

Simulations and Trajectory Tracking of Two Manipulators Manipulating a Flexible Payload Smuatons and rajectory racng of wo Manpuators Manpuatng a Fexbe Payoad Peng Zhang Coege of Communcaton Engneerng Jn Unversty Changchun, Chna Yuan-chuan L Coege of Communcaton Engneerng Jn Unversty Changchun,

More information

MARKOV CHAIN AND HIDDEN MARKOV MODEL

MARKOV CHAIN AND HIDDEN MARKOV MODEL MARKOV CHAIN AND HIDDEN MARKOV MODEL JIAN ZHANG JIANZHAN@STAT.PURDUE.EDU Markov chan and hdden Markov mode are probaby the smpest modes whch can be used to mode sequenta data,.e. data sampes whch are not

More information

Approximate merging of a pair of BeÂzier curves

Approximate merging of a pair of BeÂzier curves COMPUTER-AIDED DESIGN Computer-Aded Desgn 33 (1) 15±136 www.esever.com/ocate/cad Approxmate mergng of a par of BeÂzer curves Sh-Mn Hu a,b, *, Rou-Feng Tong c, Tao Ju a,b, Ja-Guang Sun a,b a Natona CAD

More information

Nested case-control and case-cohort studies

Nested case-control and case-cohort studies Outne: Nested case-contro and case-cohort studes Ørnuf Borgan Department of Mathematcs Unversty of Oso NORBIS course Unversty of Oso 4-8 December 217 1 Radaton and breast cancer data Nested case contro

More information

Workshop on Geophysical Data Analysis and Assimilation

Workshop on Geophysical Data Analysis and Assimilation 373-9 Workshop on Geophysca Data Anayss and Assmaton 9 October - 3 November, 1 Determnaton of sesmc source parameters and anayss of uncertantes. Appcaton to studes of strong recent earthquakes. B. Bukchn

More information

Assessment of Site Amplification Effect from Input Energy Spectra of Strong Ground Motion

Assessment of Site Amplification Effect from Input Energy Spectra of Strong Ground Motion Assessment of Ste Amplfcaton Effect from Input Energy Spectra of Strong Ground Moton M.S. Gong & L.L Xe Key Laboratory of Earthquake Engneerng and Engneerng Vbraton,Insttute of Engneerng Mechancs, CEA,

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,

More information

arxiv: v1 [physics.comp-ph] 17 Dec 2018

arxiv: v1 [physics.comp-ph] 17 Dec 2018 Pressures nsde a nano-porous medum. The case of a snge phase fud arxv:1812.06656v1 [physcs.comp-ph] 17 Dec 2018 Oav Gateand, Dck Bedeaux, and Sgne Kjestrup PoreLab, Department of Chemstry, Norwegan Unversty

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: Instructor s Name and Secton: (Crcle Your Secton) Sectons:

More information

On the Power Function of the Likelihood Ratio Test for MANOVA

On the Power Function of the Likelihood Ratio Test for MANOVA Journa of Mutvarate Anayss 8, 416 41 (00) do:10.1006/jmva.001.036 On the Power Functon of the Lkehood Rato Test for MANOVA Dua Kumar Bhaumk Unversty of South Aabama and Unversty of Inos at Chcago and Sanat

More information

A MIN-MAX REGRET ROBUST OPTIMIZATION APPROACH FOR LARGE SCALE FULL FACTORIAL SCENARIO DESIGN OF DATA UNCERTAINTY

A MIN-MAX REGRET ROBUST OPTIMIZATION APPROACH FOR LARGE SCALE FULL FACTORIAL SCENARIO DESIGN OF DATA UNCERTAINTY A MIN-MAX REGRET ROBST OPTIMIZATION APPROACH FOR ARGE SCAE F FACTORIA SCENARIO DESIGN OF DATA NCERTAINTY Travat Assavapokee Department of Industra Engneerng, nversty of Houston, Houston, Texas 7704-4008,

More information

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp.

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp. Clck to Vew Mathcad Document 2011 Knovel Corp. Buldng Structural Desgn. homas P. Magner, P.E. 2011 Parametrc echnology Corp. Chapter 3: Renforced Concrete Slabs and Beams 3.2 Renforced Concrete Beams -

More information

Counting Crosswords. April 19, 2006 Draft 2.5

Counting Crosswords. April 19, 2006 Draft 2.5 ountng rosswords avd J.. ackay Jeremy horpe pr 19, 2006 raft 2.5 bstract hannon s cacuaton of the number of crosswords assumed that the rows and coumns of crosswords contan typca strngs from the anguage.

More information

Analysis of Block OMP using Block RIP

Analysis of Block OMP using Block RIP Anayss of ock OMP usng ock RIP Jun Wang, Gang L, Hao Zhang, Xqn Wang Department of Eectronc Engneerng, snghua Unversty, eng 00084, Chna Emas: un-wang05@mas.tsnghua.eu.cn, {gang, haozhang, wangq_ee}@tsnghua.eu.cn

More information

ACCURATE COMPUTATION OF CRITICAL RESPONSE QUANTITES FOR LAMINATED COMPOSITE STRUCTURES

ACCURATE COMPUTATION OF CRITICAL RESPONSE QUANTITES FOR LAMINATED COMPOSITE STRUCTURES ACCURATE COMPUTATION OF CRITICAL RESPONSE QUANTITES FOR LAMINATED COMPOSITE STRUCTURES C.S. UPADHYAY, P.M. MOHITE and A. K. ONKAR Department of Aerospace Engneerng Indan Insttute of Technoogy Kanpur Kanpur

More information

Unified spin-wave theory for quantum spin systems with single-ion anisotropies

Unified spin-wave theory for quantum spin systems with single-ion anisotropies J. Phys. A: Math. Gen. 3 (999) 6687 674. Prnted n the UK PII: S35-447(99)67-8 Unfed spn-wave theory for quantum spn systems wth snge-on ansotropes Le Zhou and Yoshyuk Kawazoe Insttute for Materas Research,

More information

Interference Alignment and Degrees of Freedom Region of Cellular Sigma Channel

Interference Alignment and Degrees of Freedom Region of Cellular Sigma Channel 2011 IEEE Internatona Symposum on Informaton Theory Proceedngs Interference Agnment and Degrees of Freedom Regon of Ceuar Sgma Channe Huaru Yn 1 Le Ke 2 Zhengdao Wang 2 1 WINLAB Dept of EEIS Unv. of Sc.

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. ME 270 Sprng 2017 Exam 1 NAME (Last, Frst): Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: Instructor s Name

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. ME 270 Sprng 2014 Fnal Exam NME (Last, Frst): Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: INSTRUCTIONS

More information

G : Statistical Mechanics

G : Statistical Mechanics G25.2651: Statstca Mechancs Notes for Lecture 11 I. PRINCIPLES OF QUANTUM STATISTICAL MECHANICS The probem of quantum statstca mechancs s the quantum mechanca treatment of an N-partce system. Suppose the

More information

CABLE STRUCTURE WITH LOAD-ADAPTING GEOMETRY

CABLE STRUCTURE WITH LOAD-ADAPTING GEOMETRY Compostes n Constructon Thrd Internatona Conerence Lon, France, Ju 3, CABLE STRUCTURE WITH LOAD-ADAPTING GEOMETRY A.S. Jüch, J.F. Caron and O. Bavere Insttut Naver - Lam, ENPC-LCPC 6 et, avenue Base Pasca

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1 P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal

More information

Correspondence. Performance Evaluation for MAP State Estimate Fusion I. INTRODUCTION

Correspondence. Performance Evaluation for MAP State Estimate Fusion I. INTRODUCTION Correspondence Performance Evauaton for MAP State Estmate Fuson Ths paper presents a quanttatve performance evauaton method for the maxmum a posteror (MAP) state estmate fuson agorthm. Under dea condtons

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

ERROR MODELING FOR STRUCTURAL DEFORMATIONS OF MULTI-AXIS SYSTEM BASED ON SVR

ERROR MODELING FOR STRUCTURAL DEFORMATIONS OF MULTI-AXIS SYSTEM BASED ON SVR Journa of Theoretca and Apped Informaton Technoogy 3 st January 03. Vo. 47 No.3 005-03 JATIT & LLS. A rghts reserved. ISSN: 99-8645 www.jatt.org E-ISSN: 87-395 ERROR MODELING FOR STRUCTURAL DEFORMATIONS

More information

Coincidences of Hypercubic Lattices in 4 dimensions

Coincidences of Hypercubic Lattices in 4 dimensions Concdences of Hypercubc Lattces n 4 dmensons P. Zener Insttute for Theoretca Physcs & CMS, TU Wen, Wedner Hauptsraße 8 0, 040 Venna, Austra May 7, 006 Abstract We consder the CSLs of 4 dmensona hypercubc

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

corresponding to those of Heegaard diagrams by the band moves

corresponding to those of Heegaard diagrams by the band moves Agebra transformatons of the fundamenta groups correspondng to those of Heegaard dagrams by the band moves By Shun HORIGUCHI Abstract. Ths paper gves the basc resut of [1](1997),.e., a hande sdng and a

More information

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15 NGN 40 ynamcs and Vbratons Homework # 7 ue: Frday, Aprl 15 1. Consder a concal hostng drum used n the mnng ndustry to host a mass up/down. A cable of dameter d has the mass connected at one end and s wound/unwound

More information

Algebraic expression of system configurations and performance metrics for mixed-model assembly systems

Algebraic expression of system configurations and performance metrics for mixed-model assembly systems IIE Transactons 204 46, 230 248 Copyrght C IIE ISSN: 0740-87X prnt / 545-8830 onne DOI: 0080/074087X20383093 Agebrac expresson of system confguratons and performance metrcs for mxed-mode assemby systems

More information

Supplementary Material: Learning Structured Weight Uncertainty in Bayesian Neural Networks

Supplementary Material: Learning Structured Weight Uncertainty in Bayesian Neural Networks Shengyang Sun, Changyou Chen, Lawrence Carn Suppementary Matera: Learnng Structured Weght Uncertanty n Bayesan Neura Networks Shengyang Sun Changyou Chen Lawrence Carn Tsnghua Unversty Duke Unversty Duke

More information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS

More information

( ) = ( ) + ( 0) ) ( )

( ) = ( ) + ( 0) ) ( ) EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.

More information

P.H.G. l-leseab.ci-l LABORATORIES - LABORATORY 1WTE. Di vision a r.e ed arose for decade pulse counters possessing certain

P.H.G. l-leseab.ci-l LABORATORIES - LABORATORY 1WTE. Di vision a r.e ed arose for decade pulse counters possessing certain .E. Y. 3/22.... P.H.G. -ESEAB.- LABORATORES - LABORATORY 1WTE,... ;;' ~ Decadc Puse ounter Empoyng a ove Seque9ce of States 1, ntrouctc~: n t r,e ccu r se of deveopment of eq_upment n the Frequency Standards

More information

MULTIVARIABLE FUZZY CONTROL WITH ITS APPLICATIONS IN MULTI EVAPORATOR REFRIGERATION SYSTEMS

MULTIVARIABLE FUZZY CONTROL WITH ITS APPLICATIONS IN MULTI EVAPORATOR REFRIGERATION SYSTEMS MULTIVARIABLE FUZZY CONTROL WITH I APPLICATIONS IN MULTI EVAPORATOR REFRIGERATION SYSTEMS LIAO QIANFANG Schoo of Eectrca and Eectronc Engneerng A thess submtted to the Nanyang Technoogca Unversty n parta

More information

The Application of BP Neural Network principal component analysis in the Forecasting the Road Traffic Accident

The Application of BP Neural Network principal component analysis in the Forecasting the Road Traffic Accident ICTCT Extra Workshop, Bejng Proceedngs The Appcaton of BP Neura Network prncpa component anayss n Forecastng Road Traffc Accdent He Mng, GuoXucheng &LuGuangmng Transportaton Coege of Souast Unversty 07

More information

Chapter # A SYSTEM FOR SIMULATION OF 2D PLANT TISSUE GROWTH AND DEVELOPMENT

Chapter # A SYSTEM FOR SIMULATION OF 2D PLANT TISSUE GROWTH AND DEVELOPMENT 218 Part 3.3 Chapter # A SYSTEM FOR SIMULATION OF 2D PLANT TISSUE GROWTH AND DEVELOPMENT Noaev S.V. *1, Peneno A.V. 2, Beavsaya V.V. 1, Mjosness E. 3, Kochanov N.A. 1 1 Insttute of Cytoogy and Genetcs,

More information

The Principle of Virtual Displacements in Structural Dynamics

The Principle of Virtual Displacements in Structural Dynamics The Prncpe of Vrtua Dspacements n Structura Dynamcs 1 Stran Energy n Eastc Sods CEE 541. Structura Dynamcs Department of Cv and Envronmenta Engneerng Due Unversty Henr P. Gavn Fa 18 Consder an eastc object

More information

Quantitative Evaluation Method of Each Generation Margin for Power System Planning

Quantitative Evaluation Method of Each Generation Margin for Power System Planning 1 Quanttatve Evauaton Method of Each Generaton Margn for Poer System Pannng SU Su Department of Eectrca Engneerng, Tohoku Unversty, Japan moden25@ececetohokuacjp Abstract Increasng effcency of poer pants

More information

Short-Term Load Forecasting for Electric Power Systems Using the PSO-SVR and FCM Clustering Techniques

Short-Term Load Forecasting for Electric Power Systems Using the PSO-SVR and FCM Clustering Techniques Energes 20, 4, 73-84; do:0.3390/en40073 Artce OPEN ACCESS energes ISSN 996-073 www.mdp.com/journa/energes Short-Term Load Forecastng for Eectrc Power Systems Usng the PSO-SVR and FCM Custerng Technques

More information

Stability Problems of Pyramidal von Mises Planar Trusses with Geometrical Imperfection

Stability Problems of Pyramidal von Mises Planar Trusses with Geometrical Imperfection Stabty Probems of Pyramda von Mses Panar Trusses wth Geometrca Imperfecton MARTIN KALINA 1a 1 Insttute of Structura Mechancs 1 Brno Unversty of Technoogy 1 Facuty of Cv Engneerng, Veveří Str. 95, 60 00,

More information