Analysis of cable membrane structures using the Dynamic Relaxation Method
|
|
- Brooke Tate
- 6 years ago
- Views:
Transcription
1 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 Poo, Pouga, June - Juy 4 A. Cuna,. Caeano, P. beo, G. üe (eds.) ISSN: -9; ISBN: Anayss of cabe membane sucues usng e Dynamc eaxaon eod. Hüne, J. áca, P. Fajman Dep. of ecancs, Facuy of Cv ng., Czec ec. Unvesy n Pague, Ing. oš Hüne, Pague, Czec ep. Dep. of ecancs, Facuy of Cv ng., Czec ec. Unvesy n Pague, Pof. Jří áca, CSc., Pague, Czec ep. Dep. of ecancs, Facuy of Cv ng., Czec ec. Unvesy n Pague, Doc. Pe Fajman, CSc., Pague, Czec ep. ema: mos.une@fsv.cvu.cz, maca@ fsv.cvu.cz, fajman@ fsv.cvu.cz ABSAC: s pape compaes e effecveness of dffeen scemes of dynamc eaxaon meod (D) fo e anayss of cabe and membane sucues. D s an eave pocess a s used o fnd sac equbum. D s no used fo e dynamc anayss of sucues; a dynamc souon s used fo a fcous damped sucue o aceve a sac souon. e saby of e meod depends on e fcous vaabes (.e. mass a dampng) and e sep. e effec of mass dsbuon aong e sucue s aso suded n e pape. g dffeen scemes D w be used n s pape. Scemes A and B ae based on e eoy of vscous dampng. Scemes C, D and ae based on e eoy of nec dampng (KD) w a pea n e mdde of e e sep and scemes F, G and H ae based on e eoy of KD w paaboc appoxaon. A cabe s appoxaed as a enson ba, a caenay (sevea enson bas) and a pefecy fexbe eemen. Fo membane sucues a angua eemen s consdeed. e cosen meods ae apped o sx consucons. e cabe sucues ae anayzed n xampes o, e membane sucues ae anayzed n xampes 4 o 6. e esus py a a s possbe o deemne e bes sceme. In s conex, may be noced a e meods based on nec dampng appea moe sabe and fase. Fo ba eemen, caenay and cabe eemens e esus confm a s benefca o dvde e same amoun of mass no a nodes of e sucue popoonay o e sffes node of e soved sucue (scemes C and F). Fo membane eemen s pefeed o use e nec dampng meod w e appoxaon of e nec enegy pea n e mdde of e e sep Δ. KY WODS: Dynamc eaxaon, Cabe sucues, embane sucues, Knec dampng. INODUCION e oad anayss of cabe-membane sucues s a geomeca nonnea pobem. Fo numeca modeng of cabe sucues can be used deazaon of e sucue no e eemens and nodes. e suface of membane sucue s dscezed no a sysem of jons and ange membane eemens. e edges of e ange fom e connecon beween e jons and ey ae caed ns. e jons can be dvded no wo goups suppoed o unsuppoed ones. e equbum of poson unsuppoed nodes oaded by e noda oads can be seaced eavey. Lage dspacemens of e sucue and sma defomaon of eemens ae consdeed. Sevea meods exs o sove ese sucues. e dynamc eaxaon meod (D) w be examned n s pape. e saby of e meod depends on e fcous vaabes (.e. mass a dampng) and e sep. s pape compaes e effecveness of dffeen scemes of D fo e anayss of cabe and membane sucues. e effec of mass dsbuon aong e sucue s aso suded n e pape. s pape deveops papes [] and [].. enson ba e ba connecs e endpons and caes ony posve noma foce. e nena foce (noma foce) n one ba eemen can be cacuaed accodng o e we-nown quaon (). A = ( s ), () s wee: s e Young s moduus of eascy, A s e coss-secona aea, s e dsance beween wo end jons n e cod decon (cuen eng), s s e un-eongaed eng of eemen (sac eng). If e foce s negave, en s equa o zeo. e deadweg of su as been assumed o be concenaed equay a s wo end jons. e used ba eemen can be seen n Fgue. LNS A cabe can be appoxaed as a enson ba, a caenay (sevea enson bas) and a pefecy fexbe eemen (wee bendng momens o zeo). Homogeneous maea w a consan coss-secon ougou s eng s assumed n a cases. Fo membane sucues a angua eemen s consdeed. Fgue. Ba eemen. 99
2 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4. Caenay e basc assumpon of s eoy s a e beavou of a cabe can be appoxaed by a few bas. ese bas ae neconneced by jons and susan ony posve noma foce. e beavou of ndvdua bas s descbed n Cape.. As found n [], fve bas ae we enoug o descbe coecy e caacescs of e cabe.. Cabe eemen e basc assumpon of e anayss of a fexbe easc cabe s a e cabe s egaded o be pefecy fexbe and s devod of any fexua gdy. Load on a cabe, wc mus ncude a eas sef-weg, s dsbued unfomy aong e cuve of e cabe wc s assumed o be a paaboa. e deaed anayss can be found n [4] and [5]. I s necessay fo e a of e sudy o use an nena foce, wc s aways posve and e poance of wc s sown n Fgue..4 embane eemen Fo a membane sucues e naua sffness eemen can be used fo cacuaon of nena foces. e ogna fomuaon of e naua sffness eemen s ceded o Agys [6] bu e fomuaon ee foows e wo of Banes [7] and oppng [8]. Fo e fomuaon of e naua sffness eemen a angua eemen s consdeed. s eemen as ony n-pane sffness so e eemen fomuaon s w espec o dspacemens n e oca coodnae decons. Usng equaons of equbum, s possbe o conve e suface sess wn e eemen no foces aong e sdes of e ange. Genea appcaon of s eemen s descbed e.g. n [8]. In s case e deazaon of a ypca eemen s as sown n Fgue wee e oca coodnae sysem s conveneny cosen suc a way a e axs concdes w e fs sde. e sesses n e eemen w espec o x and y decons, w σ z equa o zeo, ae e sandad pane sess fomuaon fo an soopc maea [9]. Fgue. Cabe eemen. Foce can be cacuaed eavey fom quaon (). g(,,, c, s A, ) = n c = c 4 ( a b ) ( a b ) c 8 b = n c s a () wee: s e Young s moduus of eascy, A s e coss-secona aea, s e dsance beween wo end jons n e cod decon (cuen eng), s s e un-eongaed eng of eemen (sac eng). s e ozona dsance beween e wo end jons, c s e veca sepaaon beween jon j and jon (can be negave), s e esuan of e veca unfom oad q acng vecay e ene eng of paaboc cuved cabe, we = qs. Fo easons of cay, quaon () noduces wo moe subsuons: a = 4c 4 4c, () b = 4c 4 4c. (4) In Fgue s: Fgue. embane eemen.,, s e eng of e edge,, s e ncnaon of e edge o e oca x axs, θ θ s e ncnaon of e edge o e oca x axs. e na foces, and of sdes, and ae defned fo membane eemen as: / = Ad and σ x σ = y τ xy wee: / ( ν ) ( ν ) ν ( ν ) ( ν ) ν / ( ν) ac ac c c ac ac a b ab ab ab σ x b σ y b τ xy c b Δ c Δ Δ b (5) (6) 9
3 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 A d ν s e aea of e membane eemen, s e cness of e membane, s e Young s moduus of eascy, s e Posson s ao, s e eng of e edge of e unoaded eemen, s e eng of e edge of e unoaded eemen, s e eng of e edge of e unoaded eemen, Δ, Δ, Δ s e eongaon of e edge, and Fuemoe, ey ae used subsuons (fo =,, ): and c a b = cos θ, (7) = sn θ, (8) = snθ cosθ, (9) = b. () c bc e dec sffness S of sde ( =,, ) s defned fo membane eemen as: S Ad =. () ( ) DYNAIC LAXAION e dynamc eaxaon meod (D) s an eave pocess a s used fo e sac anayss of sucues. D s no used fo e dynamc anayss of sucues; a dynamc souon s used fo a fcous damped sucue o aceve a sac souon. e eoy of s meod was fs descbed by Day []. Dung sevea yeas, e D ave been poved pogessvey. e nec dampng ecnque was suggesed by Cunda []. oppng [8] and Lews [] aso conbued o e nec dampng meod. Pacca exampes of e appcaon can be seen n [,,,,].. Pncpe e basc unnowns ae noda veoces, wc ae cacuaed fom noda dspacemens. e dscezaon fom ene w e sep Δ w be pefomed. Dung e sep Δ a nea cange of veocy s assumed. e acceeaon dung e sep Δ s us consdeed o be consan. By subsung e above assumpons e veocy fo jon n decon m ( x, y and z ) can be expessed n a new e pon ( Δ /) us: v ( Δ / ) = v ( Δ / ) / Δ C / Δ C / / / Δ C /,() wee: s e esdua foce a e noda pon, n e decon m and a e e, s e fcous mass a e noda pon and n e decon m, C s e fcous dampng faco fo e noda pon and n e decon m, ( / ) v Δ s e veocy a e noda pon n e decon m and a e e. e cuen coodnaes of e noda pon a e e nsan ( Δ ) may en be expessed as foows: x = Δ v. () ( Δ ) ( Δ / ) x Say, equaons may be wen fo e y and z coodnae decons. Fom e baance (beween exena and nena foces) n e node, we may cacuae e esdua foces ( m = x, y, o z ) fo e coespondng node a e e. z x y = P z = P x = P y x x j y y j z z j, (4) wee: s e ndex of e n (eemen o edge) eneng e noda pon. j s e second endpon on e n. P x P y P z x, s e exena oad a e noda pon n e decon x, s e exena oad a e noda pon n e decon y, s e exena oad a e noda pon n e decon z, s e esuan of e veca unfom oad fo eac n, y, z ae e cuen coodnaes of e noda pon, s e dsance beween wo end jons fo eac n. e nena foce fo eac n can be cacuaed fom quaon () fo e cabe eemen; fom quaon () fo e ba eemen; and fom quaons (5) fo e edge of membane eemen. If e sum of e foces n e n s ess an zeo so mus be se equa o zeo. In ode o sa cacuaons, e veocy a e e pon Δ / mus be cacuaed. Usng e na condons fo e e = wee v =, we oban: wee v ( Δ / ) Δ = ae esdua foces a e e =., (5) 9
4 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 A eac e nsan, s aso possbe o cacuae e nec enegy U ougou e sucue: U n ( Δ / ) n n p m ( Δ / ) ( v ) =, (6) wee n s e numbe of jons and p s e numbe of densons (D o D).. Scemes g dffeen scemes D w be used n s pape. Scemes A and B ae based on e eoy of vscous dampng []. Scemes C, D and ae based on e eoy of nec dampng (KD) w a pea n e mdde of e e sep [8] and scemes F, G and H ae based on e eoy of KD w paaboc appoxaon []... Sceme A Dscezed mass s cosen n s sceme e same fo eac node and a decons fom foows quaon (7): Δ = ( max S ), (7) wee S s e ages dec sffness of e - jon n e m decon. e sffness S of eac n (eneng no jon ) s fo e eemen (cabe o ba) epesened by wo componens G namey, e geomec sffness S and e easc sffness S. A G S = S S = s. (8) Sffness S D membane eemen soud be deemned fo eac edge of e equaon (). Hence, e foowng quaon (7) appes o e sffness of e node S : S = S, m, (9) wee S, m s e sffness S - fom quaon (8), especvey fom quaon () - dsbued n e m decon. Vscous dampng coeffcen C fo e woe sucue s cacuaed usng e coeffcen of cca dampng []: e eave agom conveges fases wen usng e ccay damped mode. In an undamped mode, e sucue w oscae aound s poson of equbum, and e vscous dampng coeffcen, nown as cca dampng, may be found fom quaon (): 4π C = S =, () NΔ wee N denoes e numbe of eaons equed o compee one cyce of oscaon. I may now be seen a n ode o oban e vaue of e vscous dampng coeffcen, an addona compue un s necessay, w C se o zeo... Sceme B In s sceme, e fcous vaues and C ae cacuaed fo eac jon sepaaey. e dscezed mass fo eac jon s cacuaed fom quaon (): wee Δ =, () S ( S, S S ) S = max,. () e vscous dampng coeffcen C fo e noda pon s cacuaed as foows: C = S = 8 () Δ.. Sceme C s sceme s based on e eoy of KD w a pea n e mdde of e e sep [8]. Wen e ecnque of nec dampng s empoyed, e vscous dampng coeffcen s aen as zeo. e sysem s boug o es by foowng a pocess soppng e eaons, weneve a pea n e nec enegy of e ene sysem s deeced, and en esang e compuaon fom e cuen confguaon, bu w zeo na veocy []. e coodnaes ae se o assumed o ave occued. en x ( Δ / ) x y z ( Δ / ) x wen e pea s Δ ( Δ / ) = x vx. (4) Say, equaons may be wen fo e y and z coodnae decons. e mass fo woe sucue s cacuaed fom quaon (7)...4 Sceme D s sceme s sa o e Sceme C, bu e dscezed mass fo eac jon s cacuaed sepaaey fom quaon ()...5 Sceme s sceme s sa o Sceme D bu masses ecacuaed afe eac esa of e nec enegy. ae..6 Scemes F, G and H ese scemes ae sa o Sceme C (especvey D and ) bu ee s used e eoy of KD w paaboc appoxaon []. e ace of nec enegy nea e pea can be appoxaed by a paaboc cuve. e coodnaes ae se o ( βδ) wen e pea s assumed o ave occued. en x wee x = x βδ v ( βδ ) ( Δ / ) x, (5) 9
5 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 K K K K K β =, (6) ( Δ / ) and wee K = U n s e nec enegy a e e ( Δ / ) ( Δ / ) pon ( Δ / ), K = U, K = U. n 4 XAPLS e cosen meods ae apped o sx sucues. e cabe sucues ae anayzed n xampes o, e membane sucues ae anayzed n xampes 4 o 6. e na geomey (no nena sess) s evden fom ndvdua fgues. e cacuaons wee emnaed wen e nec enegy of e sucue was ess an. -6 J and we e esdua foces of a e degees of feedom wee ess an e vaue (defned ndvduay fo eac exampe). e maxum numbe of eaons s cosen accodng o e eemens max. 5 eaons fo ba eemens max. 5 eaons fo cabe and membane eemens. e e sep s cosen Δ = s n a cacuaons. Sef-ceaed scps n ALAB (a) was used fo a cacuaons. e cacuaons wee caed ou on e compue ASUS pocesso AD -45 APU.65 GHz, memoy 4GB A. e esus of e cacuaons (e numbe of eaons and e CPU e) ae pesened n abes o xampe A suspended cabe ng sown n Fgue 4, wc as been dscussed n [], s anaysed ee o sow e accuacy and speed of e compuaons deveoped n s pape. n acs on e sucue. An unfom oad q =.55 - N/m acs on eac cabe. e coodnaes z of e unsuppoed nodes wee aways se o zeo. e vaue of a esdua foce s accuacy of e cacuaon s appoxaey ± cm. =. N. e abe. e numbe of eaons xampe. sceme/eemen ba caenay cabe vscous A 4-66 dampng B nec C dampng D Δ/ nec dampng βδ F G H abe. e of souon (CPU e n seconds) xampe. sceme/eemen ba caenay cabe vscous A.7-6. dampng B nec C dampng D Δ/ nec dampng βδ F G H xampe Hypa ne e exampe s aen fom Lews []: wo ses of sag ne cabes geneae a mode of a ypeboc paabood suface, sown n Fgue 5. Fgue 4. A pan vew of xampe. e sucue consss of 6 cabes conneced o 6 jons (-8 ae fee, A-H ae fxed) w an nne adus of 5 m and oue adus of 75 m. e sucues ave 8 ada cabes and 8 angena cabes. A cabes ave e same coss-secona aea A = m and e same Young's moduus = 7 GPa. e sac eng s of a ada cabes s 4 m, and a of a ng cabes s m. Any exena node oads Fgue 5. opoogy of Hypa ne. e sucue as 6 degees of feedom. e oad P z of.57 N s apped a a nena nodes, excep fo nodes 7,, and. e coss-secona aea of e cabes s.785 mm and Young s moduus s 4.8 N/mm. e pe-enson foce n a cabes s. N. e pevous anayss and expeena measuemens of e same sucue ae epoed n [4]. e vaue of a esdua foce s =. N. e accuacy of e cacuaon s appoxaey ± mm. 9
6 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 abe. e numbe of eaons xampe. sceme/eemen ba caenay cabe vscous A dampng B nec C dampng D 97-9 Δ/ nec dampng βδ F G 9-65 H abe 4. e of souon (CPU e n seconds) xampe. sceme/eemen ba caenay cabe vscous A dampng B nec C dampng D Δ/ nec dampng βδ F G H e paamees of cabes ae as foows: cabes 7: = 4 GPa, A = mm, q =. N/m cabes 8 : = 4 GPa, A = 8 mm, q =.7 N/m. e foowng cabe engs (seeced cabes) wee consdeed: cabe. m, cabe.68 m, cabe 4.4 m, cabe 4. m, cabe m, cabe 6.8 m. e oad s apped a jons 8 and 9 wee e foces exeed by e canvas ac. ese foces amoun o: P 8 z = N and P 9 = 6 N. e vaue of a esdua foce s =. N. e accuacy of e cacuaon s appoxaey ± 5 cm. 4. xampe am sop Fuemoe, one ea sucue was esed, see Fgue 6. Fgue 7. e pespecve vew of Baandov am sop. Fgue 6. Baandov am sop. I s a cabe-membane sucue w a cena symmey, ony one fou of e sucue was subjeced o modeng. e canvas was epesened by foces exeed by e sucue s own weg and pesess n e mode. e bacgound fo e ceaon of e mode was e geodec suvey of e exsng sucue made n Novembe, see Fgue 7. e measuemen of foces n cabes as been dscussed n [5]. e ancong of e cabes no anco bocs was modeed as a fxed suppo. e pon wee e cabes wee ancoed no anco bocs was modeed as a sdng jon aowng e jon s moon ony n e decon of e x and y axes. e sucua sceme of e sucue consdeed s evden fom Fgue 8. Fgue 8. A pan vew of a am sop. abe 5. e numbe of eaons xampe. sceme/eemen ba caenay cabe vscous A dampng B 5-9 nec C dampng D 5 - Δ/ 9 5 nec dampng βδ F G - 5 H
7 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 abe 6. e of souon (CPU e n seconds) xampe. sceme/eemen ba caenay cabe vscous A dampng B nec C dampng D Δ/ nec dampng βδ 4.4 xampe 4 F G H I s a membane sucue w 6 nodes (of wc ae unsuppoed) neconneced w 4 membane eemens. s sucue s sown n Fgue 9. e oad P z = N acs on bo unsuppoed jons. e paamees of membanes ae aways = 5 Pa, d = mm and ν =.. e vaue of a esdua foce s =. N. e accuacy of e cacuaon s appoxaey ± mm. I s a membane sucue w 5 nodes (of wc ae unsuppoed) neconneced w 6 membane eemens. s sucue s sown n Fgue. e oad P =.75 N. e paamees of membanes ae aways = 5 Pa, d = mm and ν =.. e vaue of a esdua foce s =. N. e accuacy of e cacuaon s appoxaey ± mm. abe 8. e numbe of eaons and e of souon (CPU e n seconds) xampe 5. sceme numbe of eaons e of souon vscous A 4.8 dampng nec dampng Δ/ nec dampng βδ B C.5 D F 49.8 G 4. H xampe 6 I s a membane sucue w 65 nodes (of wc 57 ae unsuppoed) neconneced w 96 membane eemens. e opoogy and na geomey of s sucue s sown n Fgue. Fgue 9. opoogy and na geomey of xampe 4. abe 7. e numbe of eaons and e of souon (CPU e n seconds) xampe 4. sceme numbe of eaons e of souon vscous A 66. dampng B nec C 4.7 dampng D 4.7 Δ/ 4.8 nec dampng βδ 4.5 xampe 5 F 4. G 4. H 6.8 Fgue. opoogy and na geomey of xampe 6. e oad P z = N fo nena jons and P z = 5 N fo a exena jons. e paamees of membanes ae aways = 5 Pa, d = mm and ν =.. e vaue of a esdua foce s = N. e accuacy of e cacuaon s appoxaey ± cm. abe 9. e numbe of eaons and e of souon (CPU e n seconds) xampe 6. sceme numbe of eaons e of souon vscous A 67.9 dampng B nec C dampng D Δ/ 6.8 nec dampng βδ F G H 59. Fgue. opoogy and na geomey of xampe 5. 95
8 Poceedngs of e 9 Inenaona Confeence on Sucua Dynamcs, UODYN 4 5 FINAL CONS e ovea anng of meods soed by e numbe of eos (sum of a exampes), e oa numbe of eaons and e oa CPU e ae sown n abes o. e esus py a a s possbe o deemne ceay e bes sceme. In s conex, may be noced a e meods based on nec dampng appea moe sabe and fase, wc confms e concusons pesened n [,,]. Fo ba eemen, caenay and cabe eemens e esus confm a s benefca o dvde e same amoun of mass no a nodes of e sucue popoonay o e sffes node of e soved sucue (scemes C and F). Fo membane eemen s pefeed o use e nec dampng meod w e appoxaon of e nec enegy pea n e mdde of e e sep Δ. 6 CONCLUSIONS I may be concuded a e Sceme C based on nec dampng w a pea n e mdde of e e sep and e equa mass dvded no a nodes popoonay o e sffes node as poved e mos compeensve esus. abe. e summay of esus ba eemen. sceme numbe of e of eos an eaons souon vscous A dampng B nec C dampng D Δ/. 6 nec dampng βδ F 6.5 G H 9. 5 abe. e summay of esus caenay. sceme numbe of e of eos an eaons souon vscous A dampng B 8 nec C dampng D 8 Δ/ nec dampng βδ F G 8 H abe. e summay of esus cabe eemen. sceme numbe of e of eos an eaons souon vscous A dampng B nec C dampng D 7 9. Δ/ nec dampng βδ F G H abe. e summay of esus membane eemen. sceme numbe of e of eos an eaons souon vscous A dampng B nec C 7. dampng D Δ/ nec dampng βδ F G H ACKNOWLDGNS e esus pesened n s pape ae oupus of e eseac pojec P5//59 - Cabe - membane sucues anayses suppoed by Czec Scence Foundaon and pojec SGS4/9/OHK// - Advanced agoms fo numeca modeng n mecancs of sucues and maeas suppoed by e Czec ecnca Unvesy n Pague. FNCS []. Hüne, J. áca and P. Fajman, Anayss of Cabe Sucues usng e Dynamc eaxaon eod, n B.H.V. oppng, P. Ivány, (dos), Poceedngs of e Foueen Inenaona Confeence on Cv, Sucua and nvonmena ngneeng Compung, Cv- Comp Pess, Sngse, UK, Pape 45,. do:.4/ccp..45 []. Hüne, J. áca, embane sucues - dynamc eaxaon, Poceedngs of e 4 Confeence Nano & aco ecancs. Pague, ČVU,, pp75-8. ISBN []. Hüne, J. áca, Cabe sucues - numeca anayss. Poceedngs of e d confeence: N Nano & aco mecancs. Pague, ČVU,, pp ISBN [4] H. Deng,.F. Jang, A.S.K. Kwan, Sape fndng of ncompee cabesu assembes conanng sac and pesessed eemens, Compues and Sucues, (8), 5, -, pp , ISSN [5] J. Kadčá, Saa nosnýc an vsuýc sřec. Academa, Pague, 99, 6 p. ISBN (n Czec). [6] J.H. Agys, ecen Advances n ax eods of Sucua Anayss, Pogess n Aeonauca Scences. Pegamon Pess, London, 964, 4. ISSN [7].. Banes, Fom and sess engneeng of enson sucues, Sucua ngneeng evew, 994, 6 (-4), pp 75-. ISSN [8] B.H.V. oppng, P. Ivány, Compue Aded Desgn of Cabe embane Sucues. Saxe-Cobug Pubcaons, Kppen, Sngse, Scoand, 7, p, ISBN [9] O. Zenewcz,. ayo, e fne eemen meod voume e bass. Buewo-Henemann, Oxfod, ngand. 5p. ISBN [] A.S. Day, An noducon o dynamc eaxaon. e ngnee. Januay 965, pp8-, ISSN -89. [] P.A. Cunda, xpc fne-dffeence meods n geomecancs, Poceedngs.F. conf. numeca meods n geomecancs. Bacsbug, 976, pp-5. [] W.J. Lews, enson sucues: Fom and beavou, omas efod, London,, p, ISBN []. ezaee-pajand, S.. Saafaz, H. ezaee, ffcency of dynamc eaxaon meods n nonnea anayss of uss and fame sucues, Compues and Sucues., (-), s 95-, ISSN [4] W.J. Lews, e ffcency of Numeca eods fo e Anayss of Pesessed Nes and Pn-joned Fame Sucues, Compues and Sucues,, pp79-8, 989. [5] P. Fajman,. Poá, Dopínání an nosné onsuce zasávy Baandov. Konsuce,, 4, ISSN 8-84 (n Czec). 96
Several Intensive Steel Quenching Models for Rectangular and Spherical Samples
Recen Advances n Fud Mecancs and Hea & Mass ansfe Sevea Inensve See Quencng Modes fo Recangua and Speca Sampes SANDA BLOMKALNA MARGARIA BUIKE ANDRIS BUIKIS Unvesy of Lava Facuy of Pyscs and Maemacs Insue
More information5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )
5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma
More informationModel of the Feeding Process of Anisotropic Warp Knitted Fabrics
Zgnew Mo³ajczy Technca Unvesy of ódÿ Insue of Knng Technoogy and Sucue of Kned oducs u. eomsego 6 90-54 ódÿ oand Mode of he Feedng ocess of Ansooc Wa Kned Facs Asac The mode of he feedng ocess of ansooc
More information793. Instantaneous frequency identification of a time varying structure using wavelet-based state-space method
793. Insananeous fequency denfcaon of a me vayng sucue usng wavee-based sae-space mehod X. Xu 1, Z. Y. Sh, S. L. Long 3 Sae Key Laboaoy of Mechancs and Cono of Mechanca Sucues Nanng Unvesy of Aeonaucs
More informationChapter 6 Plane Motion of Rigid Bodies
Chpe 6 Pne oon of Rd ode 6. Equon of oon fo Rd bod. 6., 6., 6.3 Conde d bod ced upon b ee een foce,, 3,. We cn ume h he bod mde of e numbe n of pce of m Δm (,,, n). Conden f he moon of he m cene of he
More informationName of the Student:
Engneeng Mahemacs 05 SUBJEC NAME : Pobably & Random Pocess SUBJEC CODE : MA645 MAERIAL NAME : Fomula Maeal MAERIAL CODE : JM08AM007 REGULAION : R03 UPDAED ON : Febuay 05 (Scan he above QR code fo he dec
More informations = rθ Chapter 10: Rotation 10.1: What is physics?
Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous
More informationCHAPTER 10: LINEAR DISCRIMINATION
HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g
More information2 shear strain / L for small angle
Sac quaons F F M al Sess omal sess foce coss-seconal aea eage Shea Sess shea sess shea foce coss-seconal aea llowable Sess Faco of Safe F. S San falue Shea San falue san change n lengh ognal lengh Hooke
More informationField due to a collection of N discrete point charges: r is in the direction from
Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc
More informationLecture 5. Plane Wave Reflection and Transmission
Lecue 5 Plane Wave Reflecon and Tansmsson Incden wave: 1z E ( z) xˆ E (0) e 1 H ( z) yˆ E (0) e 1 Nomal Incdence (Revew) z 1 (,, ) E H S y (,, ) 1 1 1 Refleced wave: 1z E ( z) xˆ E E (0) e S H 1 1z H (
More informationChapter 5. Long Waves
ape 5. Lo Waes Wae e s o compaed ae dep: < < L π Fom ea ae eo o s s ; amos ozoa moo z p s ; dosac pesse Dep-aeaed coseao o mass
More informationChapter 3: Vectors and Two-Dimensional Motion
Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon
More informationCourse Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles
Couse Oulne. MATLAB uoal. Moon of syses ha can be dealzed as pacles Descpon of oon, coodnae syses; Newon s laws; Calculang foces equed o nduce pescbed oon; Deng and solng equaons of oon 3. Conseaon laws
More information1 Constant Real Rate C 1
Consan Real Rae. Real Rae of Inees Suppose you ae equally happy wh uns of he consumpon good oday o 5 uns of he consumpon good n peod s me. C 5 Tha means you ll be pepaed o gve up uns oday n eun fo 5 uns
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationLOW ORDER POLYNOMIAL EXPANSION NODAL METHOD FOR A DeCART AXIAL SOLUTION
9 Inenaona Nucea Aanc Confeence - INAC 9 Ro de JaneoRJ az epembe7 o Ocobe 9 AOCIAÇÃO RAILEIRA DE ENERGIA NUCLEAR - AEN IN: 978-85-994--8 LOW ORDER POLYNOMIAL EXPANION NODAL METHOD FOR A DeCART AXIAL OLUTION
More informationFIRMS IN THE TWO-PERIOD FRAMEWORK (CONTINUED)
FIRMS IN THE TWO-ERIO FRAMEWORK (CONTINUE) OCTOBER 26, 2 Model Sucue BASICS Tmelne of evens Sa of economc plannng hozon End of economc plannng hozon Noaon : capal used fo poducon n peod (decded upon n
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Fne Dffeence Mehod fo Odnay Dffeenal Eqaons Afe eadng hs chape, yo shold be able o. Undesand wha he fne dffeence mehod s and how o se o solve poblems. Wha s he fne dffeence mehod? The fne dffeence
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationA VISCOPLASTIC MODEL OF ASYMMETRICAL COLD ROLLING
SISOM 4, BUCHAEST, - May A VISCOPLASTIC MODEL OF ASYMMETICAL COLD OLLING odca IOAN Spu Hae Unvesy Buchaes, odcaoan7@homal.com Absac: In hs pape s gven a soluon of asymmecal sp ollng poblem usng a Bngham
More informationCptS 570 Machine Learning School of EECS Washington State University. CptS Machine Learning 1
ps 57 Machne Leann School of EES Washnon Sae Unves ps 57 - Machne Leann Assume nsances of classes ae lneal sepaable Esmae paamees of lnea dscmnan If ( - -) > hen + Else - ps 57 - Machne Leann lassfcaon
More informationajanuary't I11 F or,'.
',f,". ; q - c. ^. L.+T,..LJ.\ ; - ~,.,.,.,,,E k }."...,'s Y l.+ : '. " = /.. :4.,Y., _.,,. "-.. - '// ' 7< s k," ;< - " fn 07 265.-.-,... - ma/ \/ e 3 p~~f v-acecu ean d a e.eng nee ng sn ~yoo y namcs
More informationI-POLYA PROCESS AND APPLICATIONS Leda D. Minkova
The XIII Inenaonal Confeence Appled Sochasc Models and Daa Analyss (ASMDA-009) Jne 30-Jly 3, 009, Vlns, LITHUANIA ISBN 978-9955-8-463-5 L Sakalaskas, C Skadas and E K Zavadskas (Eds): ASMDA-009 Seleced
More informationTwo-Pion Exchange Currents in Photodisintegration of the Deuteron
Two-Pion Exchange Cuens in Phoodisinegaion of he Deueon Dagaa Rozędzik and Jacek Goak Jagieonian Univesiy Kaków MENU00 3 May 00 Wiiasbug Conen Chia Effecive Fied Theoy ChEFT Eecoagneic cuen oeaos wihin
More informationN 1. Time points are determined by the
upplemena Mehods Geneaon of scan sgnals In hs secon we descbe n deal how scan sgnals fo 3D scannng wee geneaed. can geneaon was done n hee seps: Fs, he dve sgnal fo he peo-focusng elemen was geneaed o
More informationSAVE THESE INSTRUCTIONS
SAVE ESE NSUNS FFEE AE ASSEMY NSUNS SYE #: 53SN2301AS ASSEME N A FA, PEED SUFAE PPS EAD SEWDVE NEEDED F ASSEMY; N NUDED PA S FGUE UANY DESPN AA 1 P P 1 P EF SDE FAME 1 P G SDE FAME D 1 P A PANE E 2 PS
More informationModern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.
Moden Enegy Funconal fo Nucle and Nuclea Mae By: lbeo noosa Teas &M Unvesy REU Cycloon 008 Meno: D. Shalom Shlomo Oulne. Inoducon.. The many-body poblem and he aee-fock mehod. 3. Skyme neacon. 4. aee-fock
More informationGo over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration
Mh Csquee Go oe eco nd eco lgeb Dsplcemen nd poson n -D Aege nd nsnneous eloc n -D Aege nd nsnneous cceleon n -D Poecle moon Unfom ccle moon Rele eloc* The componens e he legs of he gh ngle whose hpoenuse
More informationSCIENCE CHINA Technological Sciences
SIENE HINA Technologcal Scences Acle Apl 4 Vol.57 No.4: 84 8 do:.7/s43-3-5448- The andom walkng mehod fo he seady lnea convecondffuson equaon wh axsymmec dsc bounday HEN Ka, SONG MengXuan & ZHANG Xng *
More informationNanoparticles. Educts. Nucleus formation. Nucleus. Growth. Primary particle. Agglomeration Deagglomeration. Agglomerate
ucs Nucleus Nucleus omaon cal supesauaon Mng o eucs, empeaue, ec. Pmay pacle Gowh Inegaon o uson-lme pacle gowh Nanopacles Agglomeaon eagglomeaon Agglomeae Sablsaon o he nanopacles agans agglomeaon! anspo
More informationPHYS 705: Classical Mechanics. Central Force Problems I
1 PHYS 705: Cassica Mechanics Centa Foce Pobems I Two-Body Centa Foce Pobem Histoica Backgound: Kepe s Laws on ceestia bodies (~1605) - Based his 3 aws on obsevationa data fom Tycho Bahe - Fomuate his
More informationDynamic analysis of hoisting viscous damping string with time-varying length
Journa of Physcs: Conference Seres OPEN ACCESS Dynamc anayss of hosng vscous dampng srng wh me-varyng engh To ce hs arce: P Zhang e a 3 J. Phys.: Conf. Ser. 448 Vew he arce onne for updaes and enhancemens.
More informationRotations.
oons j.lbb@phscs.o.c.uk To s summ Fmes of efeence Invnce une nsfomons oon of wve funcon: -funcons Eule s ngles Emple: e e - - Angul momenum s oon geneo Genec nslons n Noehe s heoem Fmes of efeence Conse
More informationUniversity of California, Davis Date: June xx, PRELIMINARY EXAMINATION FOR THE Ph.D. DEGREE ANSWER KEY
Unvesy of Calfona, Davs Dae: June xx, 009 Depamen of Economcs Tme: 5 hous Mcoeconomcs Readng Tme: 0 mnues PRELIMIARY EXAMIATIO FOR THE Ph.D. DEGREE Pa I ASWER KEY Ia) Thee ae goods. Good s lesue, measued
More informationTwo-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch
Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion
More informationp E p E d ( ) , we have: [ ] [ ] [ ] Using the law of iterated expectations, we have:
Poblem Se #3 Soluons Couse 4.454 Maco IV TA: Todd Gomley, gomley@m.edu sbued: Novembe 23, 2004 Ths poblem se does no need o be uned n Queson #: Sock Pces, vdends and Bubbles Assume you ae n an economy
More information1.050 Engineering Mechanics I. Summary of variables/concepts. Lecture 27-37
.5 Engneeng Mechancs I Summa of vaabes/concepts Lectue 7-37 Vaabe Defnton Notes & ments f secant f tangent f a b a f b f a Convet of a functon a b W v W F v R Etena wok N N δ δ N Fee eneg an pementa fee
More informationExponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.
Eponenial and Logaihmic Equaions and Popeies of Logaihms Popeies Eponenial a a s = a +s a /a s = a -s (a ) s = a s a b = (ab) Logaihmic log s = log + logs log/s = log - logs log s = s log log a b = loga
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More informationFast Calibration for Robot Welding System with Laser Vision
Fas Calbaon fo Robo Weldng Ssem h Lase Vson Lu Su Mechancal & Eleccal Engneeng Nanchang Unves Nanchang, Chna Wang Guoong Mechancal Engneeng Souh Chna Unves of echnolog Guanghou, Chna Absac Camea calbaon
More informationAn axisymmetric incompressible lattice BGK model for simulation of the pulsatile ow in a circular pipe
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS In. J. Nume. Meh. Fluds 005; 49:99 116 Publshed onlne 3 June 005 n Wley IneScence www.nescence.wley.com). DOI: 10.100/d.997 An axsymmec ncompessble
More informationScienceDirect. Behavior of Integral Curves of the Quasilinear Second Order Differential Equations. Alma Omerspahic *
Avalable onlne a wwwscencedeccom ScenceDec oceda Engneeng 69 4 85 86 4h DAAAM Inenaonal Smposum on Inellgen Manufacung and Auomaon Behavo of Inegal Cuves of he uaslnea Second Ode Dffeenal Equaons Alma
More informationNumerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs)
USOD 005 uecal Sudy of Lage-aea An-Reonan Reflecng Opcal Wavegude (ARROW Vecal-Cavy Seconduco Opcal Aplfe (VCSOA anhu Chen Su Fung Yu School of Eleccal and Eleconc Engneeng Conen Inoducon Vecal Cavy Seconduco
More informationDYNAMIC ANALYSIS OF BRIDGES SUBJECTED TO MOVING VEHICLES
Mahmood: Dynamc Anayss Of Brdges Subjeced o Mong Vehces DYNAMIC ANALYSIS OF BRIDGES SUBJECTED TO MOVING VEHICLES Dr. Mohamad Najm Mahmood Ayad Thab Saeed A-Ghabsha Asssan Professor Asssan Lecurer C Engneerng
More informationHandling Fuzzy Constraints in Flow Shop Problem
Handlng Fuzzy Consans n Flow Shop Poblem Xueyan Song and Sanja Peovc School of Compue Scence & IT, Unvesy of Nongham, UK E-mal: {s sp}@cs.no.ac.uk Absac In hs pape, we pesen an appoach o deal wh fuzzy
More informationABOUT THE DESIGN OF PRESTRESSED FRAMES WITH THE INFINITELY RIGID BEAM, SUBJECTED TO HORIZONTAL FORCES
NTERNTONL SCENTFC CONFERENCE CBv 00 November 00, Braşov BOUT THE DESGN OF PRESTRESSED FRES WTH THE NFNTELY RGD BE, SUBJECTED TO HORZONTL FORCES Dan PRECUPNU*, Codrin PRECUPNU** *Prof., Universiy G. saci
More informationChapter 6 Area and Volume
Capte 6 Aea and Volume Execise 6. Q. (i) Aea of paallelogam ( ax)( x) Aea of ectangle ax ( x + ax)( x) x x ( + a) a x a Faction x ( + a) + a (ii) Aea of paallelogam Aea of ectangle 5 ax (( + 5 x)( x ax)
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationCoordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to
Coodinate Geomet Conic sections These ae pane cuves which can be descibed as the intesection of a cone with panes oiented in vaious diections. It can be demonstated that the ocus of a point which moves
More informationIncreasing the Image Quality of Atomic Force Microscope by Using Improved Double Tapered Micro Cantilever
Rece Reseaces Teecocaos foacs Eecocs a Sga Pocessg ceasg e age Qa of oc Foce Mcope Usg pove oe Tapee Mco aeve Saeg epae of Mecaca Egeeg aava Bac sac za Uves aava Tea a a_saeg@aavaa.ac. sac: Te esoa feqec
More informationcalculating electromagnetic
Theoeal mehods fo alulang eleomagne felds fom lghnng dshage ajeev Thoapplll oyal Insue of Tehnology KTH Sweden ajeev.thoapplll@ee.kh.se Oulne Despon of he poblem Thee dffeen mehods fo feld alulaons - Dpole
More information156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2
156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of
More informationPrediction of modal properties of circular disc with pre-stressed fields
MAEC Web of Confeences 157 0034 018 MMS 017 hps://do.og/10.1051/aecconf/0181570034 Pedcon of odal popees of ccula dsc h pe-sessed felds Mlan Naď 1* Rasslav Ďuš 1 bo Nánás 1 1 Slovak Unvesy of echnology
More informationObjectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.
Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae
More informationMidterm Exam. Thursday, April hour, 15 minutes
Economcs of Grow, ECO560 San Francsco Sae Unvers Mcael Bar Sprng 04 Mderm Exam Tursda, prl 0 our, 5 mnues ame: Insrucons. Ts s closed boo, closed noes exam.. o calculaors of an nd are allowed. 3. Sow all
More informationMEI Structured Mathematics. Module Summary Sheets. Numerical Methods (Version B reference to new book)
MEI Matematics in Education and Industy MEI Stuctued Matematics Module Summay Seets (Vesion B efeence to new book) Topic : Appoximations Topic : Te solution of equations Topic : Numeical integation Topic
More informationFI 2201 Electromagnetism
F Eectomagnetism exane. skana, Ph.D. Physics of Magnetism an Photonics Reseach Goup Magnetostatics MGNET VETOR POTENTL, MULTPOLE EXPNSON Vecto Potentia Just as E pemitte us to intouce a scaa potentia V
More informationMechanics Physics 151
Mechanics Physics 151 Lectue 6 Kepe Pobem (Chapte 3) What We Did Last Time Discussed enegy consevation Defined enegy function h Conseved if Conditions fo h = E Stated discussing Centa Foce Pobems Reduced
More informationMolecular dynamics modeling of thermal and mechanical properties
Molecula dynamcs modelng of hemal and mechancal popees Alejando Sachan School of Maeals Engneeng Pudue Unvesy sachan@pudue.edu Maeals a molecula scales Molecula maeals Ceamcs Meals Maeals popees chas Maeals
More information1. A body will remain in a state of rest, or of uniform motion in a straight line unless it
Pncples of Dnamcs: Newton's Laws of moton. : Foce Analss 1. A bod wll eman n a state of est, o of unfom moton n a staght lne unless t s acted b etenal foces to change ts state.. The ate of change of momentum
More informationCHAPTER 7: CLUSTERING
CHAPTER 7: CLUSTERING Semparamerc Densy Esmaon 3 Paramerc: Assume a snge mode for p ( C ) (Chapers 4 and 5) Semparamerc: p ( C ) s a mure of denses Mupe possbe epanaons/prooypes: Dfferen handwrng syes,
More informationCOMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS
ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant
More informationChapter Fifiteen. Surfaces Revisited
Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)
More informationTHIS PAGE DECLASSIFIED IAW E
THS PAGE DECLASSFED AW E0 2958 BL K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW E0 2958 B L K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW EO 2958 THS PAGE DECLASSFED AW EO 2958 THS
More informationA hybrid method to find cumulative distribution function of completion time of GERT networks
Jounal of Indusal Engneeng Inenaonal Sepembe 2005, Vol., No., - 9 Islamc Azad Uvesy, Tehan Souh Banch A hybd mehod o fnd cumulave dsbuon funcon of compleon me of GERT newos S. S. Hashemn * Depamen of Indusal
More informationL4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3
elave moon L4:1 To appl Newon's laws we need measuemens made fom a 'fed,' neal efeence fame (unacceleaed, non-oang) n man applcaons, measuemens ae made moe smpl fom movng efeence fames We hen need a wa
More informationRotor profile design in a hypogerotor pump
Jounal of Mechancal Scence and Technology (009 459~470 Jounal of Mechancal Scence and Technology www.spngelnk.com/conen/78-494x DOI 0.007/s06-009-007-y oo pofle desgn n a hypogeoo pump Soon-Man Kwon *,
More informationProbabilistic Models. CS 188: Artificial Intelligence Fall Independence. Example: Independence. Example: Independence? Conditional Independence
C 188: Aificial Inelligence Fall 2007 obabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Lecue 15: Bayes Nes 10/18/2007 Given a join disibuion, we can eason abou unobseved vaiables
More informationMCTDH Approach to Strong Field Dynamics
MCTDH ppoach o Song Feld Dynamcs Suen Sukasyan Thomas Babec and Msha Ivanov Unvesy o Oawa Canada Impeal College ondon UK KITP Sana Babaa. May 8 009 Movaon Song eld dynamcs Role o elecon coelaon Tunnel
More informationPoS(ICRC2017)088. Forward to automatic forecasting and estimation of expected radiation hazards level. Speaker. Dorman Lev 1. Pustil nik Lev.
Fowad o auomac foecasng and esmaon of epeced adaon hazads eve Doman Lev Isae Cosmc ay and Space Weahe Cene (ICSWC) affaed o e Avv Unvesy Sham eseach Insue and Isae Space Agency P.O. Bo 900 e Avv ISAEL
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationINDOOR CHANNEL MODELING AT 60 GHZ FOR WIRELESS LAN APPLICATIONS
IDOOR CHAEL MODELIG AT 60 GHZ FOR WIRELESS LA APPLICATIOS ekaos Moas, Plp Consannou aonal Tecncal Unesy of Aens, Moble RadoCommuncons Laboaoy 9 Heoon Polyecnou 15773 Zogafou, Aens, Geece, moa@moble.nua.g
More informationA multiple-relaxation-time lattice Boltzmann model for simulating. incompressible axisymmetric thermal flows in porous media
A mulple-elaxaon-me lace Bolmann model fo smulang ncompessble axsymmec hemal flows n poous meda Qng Lu a, Ya-Lng He a, Qng L b a Key Laboaoy of Themo-Flud Scence and Engneeng of Mnsy of Educaon, School
More informationHomework 1 Solutions CSE 101 Summer 2017
Homewok 1 Soutions CSE 101 Summe 2017 1 Waming Up 1.1 Pobem and Pobem Instance Find the smaest numbe in an aay of n integes a 1, a 2,..., a n. What is the input? What is the output? Is this a pobem o a
More informationAlgebra-based Physics II
lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of
More informationECON 3710/4710 Demography of developing countries STABLE AND STATIONARY POPULATIONS. Lecture note. Nico Keilman
ECON 37/47 Demogaphy of deveoping counies STAE AND STATIONARY POPUATIONS ecue noe Nico Keiman Requied eading: Sabe and saionay modes Chape 9 in D Rowand Demogaphic Mehods and Conceps Ofod Univesiy Pess
More informationTelematics 2 & Performance Evaluation
Teeacs & Pefoance Evauaon Chae Modeng and Anayss Teeacs / Pefoance Evauaon WS /8: Modeng & Anayss Goas of hs chae Gves an ovevew on he hases & es used n heoeca efoance evauaon Dscusson on basc odeng echnues
More informationEN221 - Fall HW # 7 Solutions
EN221 - Fall2008 - HW # 7 Soluions Pof. Vivek Shenoy 1.) Show ha he fomulae φ v ( φ + φ L)v (1) u v ( u + u L)v (2) can be pu ino he alenaive foms φ φ v v + φv na (3) u u v v + u(v n)a (4) (a) Using v
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationMathematical Modeling and Nonlinear Dynamic Analysis of Flexible Manipulators using Finite Element Method
Unvesa Jouna of Non-nea Mechancs (), 56-6 www.papescences.com Mathematca Modeng and Nonnea Dynamc Anayss of Fexbe Manpuatos usng Fnte Eement Method J. Jafa, M. Mzae, M. Zandbaf Depatment of Mechancs, Damavand
More informationControl Volume Derivation
School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More information24-2: Electric Potential Energy. 24-1: What is physics
D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a
More informationPHYS 1443 Section 001 Lecture #4
PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law
More informationDesign of an electromagnetic-transducer energy harvester
Journa of Physcs: Conference Seres PAPE OPEN ACCESS Desgn of an eecromagnec-ransducer energy harveser To ce hs arce: L Smeone e a 06 J. Phys.: Conf. Ser. 744 0084 eaed conen - A non-near 3D prned eecromagnec
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationPHYS PRACTICE EXAM 2
PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,
More informationEXISTING PROPERTY INFORMATION: A A V LAND UNITS 1-4 O BOARD OF EDUCATION. L f. 135 R-55 NORTHWESTERN HIGH SCHOOL PARCEL 1 PROPOSED
K Q : : : : () : Z / / Z: - Z Q: sqf -: : / o ac -: : : : / f - : / : : K Z J K X X -- ea f / f : - K - X (-): (-): -- : // : -- : ( ) / : : : : - & - : X : K X J / f f & f Z K Z Q abe cefes ha hs pan
More informationA DISCRETE PARAMETRIC MARKOV-CHAIN MODEL OF A TWO NON-IDENTICAL UNIT COLD STANDBY SYSTEM WITH PREVENTIVE-MAINTENANCE
IJRRA 7 (3) Decembe 3 www.aaess.com/volumes/vol7issue3/ijrra_7_3_6.df A DICRETE PARAMETRIC MARKOV-CHAIN MODEL OF A TWO NON-IDENTICAL UNIT COLD TANDBY YTEM WITH PREVENTIVE-MAINTENANCE Rakes Gua¹ * & Paul
More informationOverview. Overview Page 1 of 8
COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSITE BEAM DESIGN AISC-LRD93 Tecnical Noe Compac and Noncompac Requiemens Tis Tecnical Noe descibes o e pogam cecks e AISC-LRD93 specificaion
More information( ) ( )) ' j, k. These restrictions in turn imply a corresponding set of sample moment conditions:
esng he Random Walk Hypohess If changes n a sees P ae uncoelaed, hen he followng escons hold: va + va ( cov, 0 k 0 whee P P. k hese escons n un mply a coespondng se of sample momen condons: g µ + µ (,,
More informationAnswers to Odd Problems in Intermediate Dynamics
Answes to Odd Pobems in Intemediate Dynamics Patick Hami San Jose State Univesity San Jose, Caifonia Januay, 9 Capte. 75.7 cm/sec at.8 above te oizonta. (a) 44ft= sec (b) mp..5 v = k b e bt (bt + ) x =
More informationdm dt = 1 V The number of moles in any volume is M = CV, where C = concentration in M/L V = liters. dcv v
Mg: Pcess Aalyss: Reac ae s defed as whee eac ae elcy lue M les ( ccea) e. dm he ube f les ay lue s M, whee ccea M/L les. he he eac ae beces f a hgeeus eac, ( ) d Usually s csa aqueus eeal pcesses eac,
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More informationStochastic State Estimation and Control for Stochastic Descriptor Systems
Sochasc Sae smaon and Conro for Sochasc Descrpor Sysems hwe Gao and aoyan Sh Schoo of ecrc and ecronc ngneerng ann Unversy ann 372, Chna e-ma: zhwegac@pubc.p..cn bsrac In hs paper, a sochasc observer s
More informationFORMULAE. 8. a 2 + b 2 + c 2 ab bc ca = 1 2 [(a b)2 + (b c) 2 + (c a) 2 ] 10. (a b) 3 = a 3 b 3 3ab (a b) = a 3 3a 2 b + 3ab 2 b 3
FORMULAE Algeba 1. (a + b) = a + b + ab = (a b) + 4ab. (a b) = a + b ab = (a + b) 4ab 3. a b = (a b) (a + b) 4. a + b = (a + b) ab = (a b) + ab 5. (a + b) + (a b) = (a + b ) 6. (a + b) (a b) = 4ab 7. (a
More informationSolution of Non-homogeneous bulk arrival Two-node Tandem Queuing Model using Intervention Poisson distribution
Volume-03 Issue-09 Sepembe-08 ISSN: 455-3085 (Onlne) RESEARCH REVIEW Inenaonal Jounal of Muldscplnay www.jounals.com [UGC Lsed Jounal] Soluon of Non-homogeneous bulk aval Two-node Tandem Queung Model usng
More information