Design of a Spherical Wrist with Parallel Architecture: Application to Vertebrae of an Eel Robot

Size: px
Start display at page:

Download "Design of a Spherical Wrist with Parallel Architecture: Application to Vertebrae of an Eel Robot"

Transcription

1 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot Daen Chablat and Phlppe Wenge Insttut de echeche en Councatons et Cbenétque de Nantes, ue de la Noë, BP 9, 44 Nantes Cedex Fance Daen.Chablat@ccn.ec-nantes.f Abstact - he desgn of a sphecal wst wth paallel achtectue s the object of ths atcle. hs stud s pat of a lage poject, whch as to desgn and to buld an eel obot fo nspecton of esed ppng. he kneatc analss of the echans s pesented fst to chaactee the sngula confguatons as well as the sotopc confguatons. We add the desgn constants elated to the applcaton, such as () the copactness of the echans, () the set of the eleents n ode to ensue statc and dnac balance and () the possblt of the echans to fll the ellptc fo of the ell sectons. Kewods - Sphecal wst, paallel obots, sotopc desgn. Caangdae as jacks, hose ackeel o popano [8]) d on oscllatons of the bod and () the angullfo swng (of snake tpe, eel, lape, etc.) d on undulatons of the bod. An angullfo swe popels tself fowad b popagatng waves of cuvatue backwad along ts bod []. I. INDUCIN ve llons of eas, fsh have evolved swng capact fa supeo n an was to what has been b nautcal scence and technolog. he use the stealned bodes to explot flud-echancal pncples. hs wa, the can acheve extaodna populson effcences, acceleaton and aneuveablt not feasble b the best naval achtects []. Paallel kneatc achtectues ae coonl claed to offe seveal advantages ove the seal countepats, lke hgh stuctual gdt, hgh dnac capactes and hgh accuac []. hus, the ae nteestng fo applcatons whee these popetes ae needed, such as flght sulatos [] and hghspeed achnes. ecentl, new applcatons have used such echanss to buld huanod obots [4], o snake obots [5]. he pupose of ths atcle s to desgn vetebae of an eel obot b usng the advantages of the paallel achtectues whle appoachng eel opholog. he next secton pesents the objectves of the boetc as well as sutable sphecal achtectues. he desgn paaetes and the kneatcs of the echans to be opted ae epoted n Secton. Fg. : Change n bod shape n swng and a subdvson of ts bod o ca out angullfo swng, the bod of the eel s ade of a successon of vetebae whose undulaton poduces oton, as depcted n Fg.. In natue, thee s onl one degee of feedo between each veteba because the oton contol of the vetebae s coupled wth the oton of the dosal and vental fn. hese two fns beng not easl epoducble, we wll gve to each veteba, oe oblt to account pobles of ollng, fo exaple. he assebl of these vetebae, coupled to a head havng two fns ust allow the epoducton of the eel swng. Fo the obsevaton of Euopean eel, Angulla angulla, we have data concenng hs kneatc swng such as wave speed, ccle fequenc, apltude o local bendng [9]. he aw s gven fo fowad and backwad swng on total bod length, as depcted n Fg.. he othe angles ae obtaned usng Nave-Stokes equatons on chaactestc tajectoes []. Fo ou pototpe, we took as constants of desgn, ± degees n aw fo fowad swng, ±5 degees n ptchng fo dvng and ±4 degees n ollng to copensate fo toson n dvng. II. PELIMINAIES A. Boetc obotcs he object of the boetc obotcs s to c lfe, to tate bologcal sstes o to conceve new technologes dawn fo the lesson of the stud [6]. Fo the last twent eas o so, an eseaches have been ade n the undewate feld n Aeca and n Japan [7]. Aong those, a good nube attepted to epoduce fsh. In ths context, two odes of locooton anl attact the attenton of eseaches () the caangd swng (fal Ptchng Yaw ollng Fg. : ollng, ptchng and aw angles of vetebae he objectve of ou stud s to buld an eel obot wth vetebae and an oveall length of 5 (wth the head and

2 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. the tal ncluded). Each veteba wll have an ellptc secton of 5 and focal dstance espectvel and wll be a thck. B. Mechancal achtectues he desgn of the vetebae of an eel s equvalent to the desgn of sphecal wsts. Indeed, an eel beng able to be copaable wth a bea, two theoes can goven ts oves, () the theo of essne [], whch poses a 6 DF kneatc echans (ealable b the stackng of Gough-Steewat's platfos) and () the theo of Kchoff of the nextensble beas, whch poses the kneatcs of the ball jont tpe []. Sphecal wsts wth seal achtectue ase seveal pobles, whch lead us to stud paallel achtectues. he fst poble s elated to the copactness of the wst because the dstance between the successve vetebae ust be ned n ode to ceate a contnuous defoaton of the eel bod. he second poble s elated to the sngulat of seal wst (fst and last axs algned) and, f we use such achtectue, onl the second evolute jont s anl used to poduce the oscllaton of the bod, whch elds pobles of denson. Convesel, sphecal wsts wth paallel achtectue ae nueous [-]. If we want to c the dsplaceents ceated b the uscles, the coespondng jont s a psatc actuato. Most exstng actuatos ae d on the use of a ota oto, a educe and a ball scew. Such devces ae used, fo exaple, n the flght sulatos usng Gough-Stewat's platfos. In the next secton, we wll pesent an achtectue that uses evoluton jonts to poduce equvalent otons. III. KINEMAIC SUDY F HE SELECED ACHIECUE A. Descpton Sphecal paallel echanss can be classfed nto two an goups, setcal o asetcal echanss, whch can be oveconstant o non-oveconstant [4]. Fo the fst goup, we have the agle ee [5] whch uses evolute jonts fxed on the (Fg. ). It s fstl developed fo the apd oentaton of a caea but t s also used fo cang a tool [6]. Fg. : he agle ee [5] Fo exaple, the natue caea attached to the endeffecto can be ponted n a cone of vson of 4 wth ± n toson [7]. Such popetes ae not asked fo ou pototpe because onl the aw angle ust be hghe and t s dffcult to place the actuated jonts on an ellptc bass. hus, we wll stud a sphecal wst, whch can poduce hgh aw and whee engne toques can be added b usng the pncple of the dffeental echans. he selected achtectue s a non-oveconstaned asetcal achtectue that s epoted n [4] as an (, 6, 6) achtectue. he and the oble platfo ae connected b thee kneatc chans, as depcted n Fg. 4. C B x θ C A θ A θ x B Fg. 4: Stuctue of the studed sphecal wst hs achtectue esults fo the eseach aound the Le Goup of Eucldan dsplaceents []. hee ae () two kneatc chans, noted legs and, to poduce a geneal gd bod dsplaceent fo the subgoup {D} (6 DF) and () a kneatc chan, noted leg, fo the sphecal subgoup {S} and ade b thee coaxal evolute jonts ( DF). hee s onl one actuated jont on each leg ( θ, θ, θ ). If the ealaton of leg s eas (thee coaxal evolute jont), t s dffcult to enueate all the legs wth 6-DF. he ost cuent geneato of {D} s of the UPS tpe (Gough- Stewat's platfo, wth P psatc actuated jont, U fo unvesal jont and S fo sphecal jont), whch has the dsadvantage of usng a psatc actuato that s not fxed on the bass. In the lteatue, an equvalent echans exsts but the geneato of {D} s of PUS tpe (wth P psatc actuated jont). Fo legs and, the psatc actuated jonts ae n paallel to the vetebal colun whch s haful fo the copactness of the echans. he oentaton can be changed but the effcenc deceases consdeabl. Fo leg, the fst evolute jont (located on the ) s actuated. hus, we have changed the tpe of legs and, b a US tpe (wth evolute actuated jont) as depcted n Fg. 4. n the next secton, we wll justf the placeents and the densons b the stud of the Jacoban atx. B. Kneatcs A fxed efeence fae, noted fxed ( x,,, ) s located on the and s oented n such a wa that () plane x s planed b ponts C and, () the -axs s vetcal, () x-axs s dected fo A to A. he coodnates of ponts A n ae wtten as fxed [ A ] = [ a b c] and [ A ] [ ] a b c fxed fxed = () he lengths a, b, and c wll be chosen b the stud of the Jacoban atx n the next subsecton.

3 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. he oble platfo wll be otatng aound pont that s the ogn of the oble fae, noted oble. he oentaton of oble ( x,,, ) s defned so that () plane x s the plane defned b ponts C and, () x -axs s dected fo to C and () -axs s dected fo to C. Let θ be the vecto of jont coodnates assocated wth the actuated evolute jonts. he oentaton of the oble platfo wth espect to fxed fae s defned b the "ollng Ptchng Yaw" paaetes (PY) whee the fst paaete s the oentaton angle θ of the fst evolute jont of leg ). fxed θ= [ θ θ θ ] (, θ ) ( ', φ) ( '', ψ) oble = x he angles θ, φ and ψ ae assocated wth the followng cascaded otatons () a otaton of angle θ aound -axs, () a otaton of angle φ aound the '-axs (obtaned fo the pevous otaton and whose axs s the axs of the second evolute jont of leg ), () a otaton of ψ aound the x''-axs (obtaned fo the second otaton and whose axs s the axs of the thd evolute jont of leg ). C. Jacoban atces o chaactee the sngula confguatons, we wll use an nvaant fo, whch allows ou esults to be applcable to an achtectue studed hee. hus, thee s no poble of sngulat of tansfoaton n the otaton atx between fxed and oble. c b to have We wte the Chasles's elaton on ( ) ( ) = ( ) + ( ) ( ) c b c o o a b a () In ths equaton, all the vectos ae expessed n fxed. o splf calculatons, we set ( ), ( ), ( ) et ( ) = c b p = c o b = o a l = b a B dffeentatng Eq. () wth espect to te, we obtan, & = p& & l () wth fxed [ ] = [ ] p p (4) oble fxed oble Dffeentatng wth espect to te, we fnd fxed [ p ] = Q& [ p ] & oble (5) fxed oble snce vecto [ p ] s a constant vecto when expessed oble n fae oble. Moeove, the te devaton of the otaton atx can be wtten as Q& = Ω Q (6) whee Ω s the angula veloct tenso. Fnall, fo Eqs. () and (6), we get p& = Ω p = ω p whee denotes the coss poduct of the two vectos and ω s the angula veloct vecto. We note and, the unt vectos passng though the axs of the fst evolute jont of legs and, espectvel. Moeove, we can wte vecto l& as functon of angula veloctes & θ and & θ & l = l (& θ. ) and & l = l (& θ. ) hus, Eq. () can be wtten n the fo & = ω p l (& θ. ) We ultpl the pecedng equaton b because. & =. hus, we have.( ω p) =.( l ( & θ. )) ( p ). ω = ( l ).(& θ. ) hese two equatons can be cast n vecto fo wth Aω + Bq& = (7) ( p ) ( ) A = p (8) ( l ). B = ( l ). (9) and q & = & θ & θ & θ hen, when B s not sngula, the nvese Jacoban atx s wtten, ( ) p ( l ). ( ) J = p ( l ). D. Sngula confguatons he paallel sngulates occu when the detenant of the atx A vanshes,.e. when det( A ) =. In such confguatons, t s possble to ove locall the oble platfo wheeas the actuated jonts ae locked. hese sngulates ae patculal undesable because the stuctue cannot esst an foce o toque. Fo Eq. (7), we have ( p ) ( p ) o ( p ) = o ( p ) = It s equvalent to have B, B and coplana o

4 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. to have ( B, ) o ( B, ) algned, as depcted n Fg. 5. B A l p p l B A l C A C p p C C A densons of each veteba to elnate the sngula confguatons fo the wokspace and to axe the kneatc popetes aound ts sotopc confguatons. he atx A s sotopc when p and p and ( p ) ( p ) and = p = = p = Moeove, A s equal to the dentt atx, as depcted n Fg. (7). he coss poduct ( p ) and ( p ) and the - axs fo an othogonal fae. l Fg. 5: Paallel sngulat when B, B and ae coplana and B and ae algned C p p C Seal sngulates occu when the detenant of the atx B vanshes,.e. when det( B ) =. At a seal sngulat, an oentaton exsts along whch an angula veloct cannot be poduced. Fo Eq. (8), we have ( ). l = o ( ). = l ( l ). = o l o ( ). = It s equvalent to have () l and algned, o () l and algned, o () and algned, o (v) and algned, as depcted n Fg.6. B B Fg. 7: Isotopc confguaton of atx A he atx B s sotopc and equal to the dentt atx when l and l and l and l and = l = he esult of the sotopc constants on A and B ae shown n Fg. 4 as an exaple. In fact, thee s an nfnt of soluton because no constant gves us the oentaton of copaed to. Fgue 4 shows and paallel but the can be dffeent. p p C C B B l l C p p A C l A F. Boetc constants and odel splfcatons Fo the pecedng esult, we wll pesent thee sutable solutons of ou pototpe. he fst soluton s the echans depcted n Fg. 4 that we could call "paallel axes". Equaton gves the locaton of ponts A n fo a unt echans, A A B B Fg. 6: Seal sngulat when l and ae algned and l and ae algned E. Condton nube and sotopc confguatons he Jacoban atx s sad to be sotopc when ts condton nube attans ts nu value of one [8]. he condton nube of the Jacoban atx s an nteestng pefoance ndex, whch chaacteses the dstoton of a unt ball unde the tansfoaton epesented b the Jacoban atx. he Jacoban atx of a anpulato s used to elate () the jont ates and the Catesan veloctes, () the statc load on the output lnk and the jont toques o foces. hus, the condton nube of the Jacoban atx can be used to easue the unfot of the dstbuton of the tool veloctes and foces n the Catesan wokspace. he a of ths secton s to defne the placeent and a =, b =, c = If ths soluton adts an sotopc confguaton, the behavou n fowad swng leads to use legs and sultaneous. When we appl as nput veloct θ & = [ ], the angula veloct obtaned s ω= [ ]. hs eans that we aplf the otatonal oton just afte havng used a educton gea on the ota oto to ncease the avalable toque. hus, the length of the otos s constaned b the shape of the coss secton of the eel, as depcted n Fg. 9. he second soluton, called "othogonal axes", s to place and othogonall as depcted n Fg. 8. he locaton of ponts A n concdes wth pont.

5 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. C x θ C Concenng the ntegaton nto the coss-secton of the eel, the placeent s less constaned, as shown n Fg.. A A Motos B C B C B θ θ x A A Fg. 8: Sphecal wst wth othogonal actuatos In ths case, the dect and nvese kneatc odels ae sple but t s oe dffcult to place the otos of legs and, as shown n Fg. 9. Moeove, thee also exsts an angula aplfcaton facto n the fowad swng. Motos A Motos A A A B C B C B B C B C Fg. 9: Placeent of the otos and the legs fo the "paallel axes" and the "othogonal axes" he last soluton has paallel actuatos and the axes ntesect the -axs, as depcted n Fg.. When the eel obot s swng, the angula veloct of the actuated jonts of legs and s equal to aw veloct. C B A θ x x θ C B A Fg. : Sphecal wst wth paallel actuatos hs eans that fo the fowad o backwad swng, the kneatc odels ae sple and the toque needed fo the oton s dstbuted. Howeve, onl A can be sotopc because we have ( l ). = fo =, Equaton gves the locaton of ponts A n fo a unt echans, a =, b =, c = θ Fg. : Placeent of the otos and the legs fo sphecal wst wth paallel actuatos G. Dect and nvese kneatc odels he dect kneatc odel can be wtten when we know the poston of B and C. hus, we have, C S B = + and n oble, o n fxed C S B = + C = [ ] C = [ ] CC φ C = SCφ S φ wth C = cos( θ ), S sn ( θ ) S φ CSS φ ψ SC ψ C = SSφSψ + CCψ CS φ ψ = fo =,, φ = cos( φ), = sn( φ) ψ = cos( ψ ) and S ψ = sn( ψ ). We add the constant that BC = CC φ + SC φ C + Sφ + S = () CSS φ ψ SC ψ + + SSS φ ψ + CC ψ C + S C S = φ ψ () o solve the dect kneatc, we know θ = [ θ θ θ ] and we use the followng substtutons Q Q sn( φ ) = cos( φ) = + Q + Q hus, we can eak that Eq. depends onl on φ and s a quadatc equaton of Q ( SQ QC QCS Q + CS C S) ( Q ) = ne soluton s Q =,.e. φ = π /+ kπ that does not depend on the actuated jonts. Fgue depcts the fou dect kneatc soluton fo θ =., θ =., θ = π / 4. Solutons and ae found when Q = and can be easl solated. Fo solutons (c) and (d), onl the second one s sutable that

6 Chablat D. et Wenge P., Desgn of a Sphecal Wst wth Paallel Achtectue: Applcaton to Vetebae of an Eel obot, Poc. IEEE Int. Conf. ob. utoaton, Bacelone, -6 Avl 5. can be solated b the dot poduct of b p. A A C C A B A C B C B A B A (c) (d) C A B A C B C Fg. : he fou dect kneatc solutons fo θ =., θ =., θ = π / 4 o solve the nvese kneatc, we use two substtutons, = tan( θ / ) and S = tan( θ / ) that pet us to have two quadatc and ndependent equatons as functon of and S espectvel. Fgue shows the fou nvese kneatc solutons fo θ = π /4, φ = π /, ψ = π / that we can solate b calculatng l. and l. fo legs and, espectvel. B A A B A B A B C C C C B A A A A B C C Fg. : he fou nvese kneatc solutons fo θ = π /4, φ = π /, ψ = π / o conclude, we have fou solutons fo the dect kneatc and fou solutons fo the nvese kneatc (two fo legs and, espectvel). B C B C B C B IV. CNCLUSINS he desgn of sphecal wsts takng nto account the constants on the boetc of the eel was ade n ths pape. A new achtectue s nvestgated and sotopc constants ae appled to poduce thee sutable solutons. he setcal constants lead us to choose the one whee the placeent of the actuated jonts s optal because the ae located on a edan plane whee the focal dstance s axa. ACKNWLEDGMENS hs eseach was patall suppoted b the CNS ("Angulle" Poject). EFEENCES [] antafllou, M. S. and antafllou G. S., An Effcent Swng Machne, Scentf Aecan, pp. 65-7, Mach 995 [ eb,. and Zn,., Slat laws of seal and paallel anpulatos fo achne tools, Poc. Int. Sena on Ipovng Machne ool Pefoances, pp. 5-, Vol., 998. [] Melet J-P, Paallel obots, Kluwe Acadec Publshes,. [4] Lenacc J., Stansc, M. M. and Paent-Castell, Kneatc Desgn of a Huanod obotc Shoulde Coplex, poceedngs of IEEE Intenatonal Confeence on obotcs utoaton, Apl 4-8,. [5] Lee K-M. et Ajunan S,. A thee-degees-of feedo cooton npaallel actuated anpulato, IEEE ans. on obotcs utoaton, ctobe 99. [6] Cha J.G., Bale S.A.lak J.E., Full.J.utkosk M.., Fast and obust: Hexapedal obots va Shape Deposton Manufactung, he Int. Jounal of obotcs eseach, vol., no., pp (4), ctobe. [7] Hose, S., Bologcall nsped obots: Snake-lke loconotos and anpulatos, xfod Unv. Pess, xfod, 99. [8] McIsaac, K.A., stowsk, J.P., A geoetc appoach to angullfo locooton odellng of an undewate eel obot, IEEE Int. Conf. obot. uto., ICA 999, pp [9] D'Août K., Ats P., A Kneatc Copaason of Fowad and Backwad Swng n the Eeel Angulla Angulla, Jounal of Expeental Bolog, pp. 5-5, 999. [] Calng J., Wllas. L., Bowtell G., Self-Popelled Angullfo Swng: Sultaneous Soluton of the wo-densonal Nave-Stokes Equatons and Newton's Laws of Moton, 998. [] So J.C. and Vu-Quoc L., n the dnacs n space of ods undegong lage otons - A geoetcall exact appoach, Cop. Meth. Appl. Mech. Eng., 66, 988, pp [] Boe, F., Pault, D., Fnte eleent of slende beas n fnte tansfoatons: a geoetcall exact appoach, Intenatonal Jounal fo Nuecal Methods n Engneeng, 4: 59, pp [] Hevé J. M., Analse stuctuale des écanses pa goupe des déplaceents, Mech. Mach. heo, Vol., No.4, pp.47-45, 978. [4] Kaoua, M., Concepton stuctuale de ecanses paalleles spheques, hèse de doctoat, I -6, École Centale de Pas,. [5] Gosseln C., Hael J.F., he agle ee: a hgh pefoance thee-degeeof-feedo caea-oentng devce, IEEE Int. confeence on obotcs utoaton, pp San Dego, 8- Ma 994. [6] Bdault, F., eng. P. ngeles, J., Stuctual optaton of a sphecal paallel anpulato usng a two-level appoach, Poc. ASME Desgn Engneeng echncal Confeences, Pttsbugh, PA, Sept. 9- D-M DEC /DAC-,. [7] Gosseln C., St-Pee E. and Gagné M., n the developent of the agle ee: echancal desgn, contol ssues and expeentaton, IEEE obotcs utoaton Socet Magane, Vol., No. 4, pp. 9-7, 996. [8] Golub, G. H. and Van Loan. F., Matx Coputatons, he John Hopkns Unvest Pess, Baltoe, 989.

Fundamental principles

Fundamental principles JU 07/HL Dnacs and contol of echancal sstes Date Da (0/08) Da (03/08) Da 3 (05/08) Da 4 (07/08) Da 5 (09/08) Da 6 (/08) Content Reve of the bascs of echancs. Kneatcs of gd bodes coodnate tansfoaton, angula

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

Scalars and Vectors Scalar

Scalars and Vectors Scalar Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg

More information

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41. Chapte I Matces, Vectos, & Vecto Calculus -, -9, -0, -, -7, -8, -5, -7, -36, -37, -4. . Concept of a Scala Consde the aa of patcles shown n the fgue. he mass of the patcle at (,) can be epessed as. M (,

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

1. 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 information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

Physics 1501 Lecture 19

Physics 1501 Lecture 19 Physcs 1501 ectue 19 Physcs 1501: ectue 19 Today s Agenda Announceents HW#7: due Oct. 1 Mdte 1: aveage 45 % Topcs otatonal Kneatcs otatonal Enegy Moents of Ineta Physcs 1501: ectue 19, Pg 1 Suay (wth copason

More information

Kinematic Analysis of the vertebra of an eel like robot

Kinematic Analysis of the vertebra of an eel like robot Kneatc Analss of the vertebra of an eel lke robot Daen Chablat o cte ths verson: Daen Chablat. Kneatc Analss of the vertebra of an eel lke robot. 3nd Annual Mechanss and obotcs Conference (M), Aug 8, New-York,

More information

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER Edton CAPTER 8 VECTOR MECANCS FOR ENGNEERS: DYNAMCS Fednand P. Bee E. Russell Johnston, J. Lectue Notes: J. Walt Ole Teas Tech Unvest Knematcs of Rgd Bodes n Thee Dmensons 003 The McGaw-ll Companes, nc.

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

gravity r2,1 r2 r1 by m 2,1

gravity r2,1 r2 r1 by m 2,1 Gavtaton Many of the foundatons of classcal echancs wee fst dscoveed when phlosophes (ealy scentsts and atheatcans) ted to explan the oton of planets and stas. Newton s ost faous fo unfyng the oton of

More information

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

COMPLEMENTARY 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 information

THE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n

THE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n HE EQUIVAENCE OF GRA-SCHID AND QR FACORIZAION (page 7 Ga-Schdt podes anothe way to copute a QR decoposton: n gen ectos,, K, R, Ga-Schdt detenes scalas j such that o + + + [ ] [ ] hs s a QR factozaton of

More information

Physics 207 Lecture 16

Physics 207 Lecture 16 Physcs 07 Lectue 6 Goals: Lectue 6 Chapte Extend the patcle odel to gd-bodes Undestand the equlbu of an extended object. Analyze ollng oton Undestand otaton about a fxed axs. Eploy consevaton of angula

More information

24-2: Electric Potential Energy. 24-1: What is physics

24-2: 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 information

Review of Vector Algebra and Vector Calculus Operations

Review of Vector Algebra and Vector Calculus Operations Revew of Vecto Algeba and Vecto Calculus Opeatons Tpes of vaables n Flud Mechancs Repesentaton of vectos Dffeent coodnate sstems Base vecto elatons Scala and vecto poducts Stess Newton s law of vscost

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle 1 PHYS 705: Classcal Mechancs Devaton of Lagange Equatons fom D Alembet s Pncple 2 D Alembet s Pncple Followng a smla agument fo the vtual dsplacement to be consstent wth constants,.e, (no vtual wok fo

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution oden Appled Scence The Fomn Theoy and the NC achnn fo The Rotay us wth the Spectal Ede Dstbuton Huan Lu Depatment of echancal Enneen, Zhejan Unvesty of Scence and Technoloy Hanzhou, c.y. chan, 310023,

More information

Rotary motion

Rotary motion ectue 8 RTARY TN F THE RGD BDY Notes: ectue 8 - Rgd bod Rgd bod: j const numbe of degees of feedom 6 3 tanslatonal + 3 ota motons m j m j Constants educe numbe of degees of feedom non-fee object: 6-p

More information

The Finite Strip Method (FSM) 1. Introduction

The Finite Strip Method (FSM) 1. Introduction The Fnte Stp ethod (FS). ntoducton Ths s the ethod of se-nuecal and se-analtcal natue. t s sutale fo the analss of ectangula plates and plane-stess eleents o stuctues eng the conaton of oth. Theefoe, the

More information

BALANCING OF ROTATING MASSES

BALANCING OF ROTATING MASSES www.getyun.co YIS OF HIES IG OF ROTTIG SSES www.getyun.co Rotatng centelne: The otatng centelne beng defned as the axs about whch the oto would otate f not constaned by ts beangs. (lso called the Pncple

More information

7/1/2008. Adhi Harmoko S. a c = v 2 /r. F c = m x a c = m x v 2 /r. Ontang Anting Moment of Inertia. Energy

7/1/2008. Adhi Harmoko S. a c = v 2 /r. F c = m x a c = m x v 2 /r. Ontang Anting Moment of Inertia. Energy 7//008 Adh Haoko S Ontang Antng Moent of neta Enegy Passenge undego unfo ccula oton (ccula path at constant speed) Theefoe, thee ust be a: centpetal acceleaton, a c. Theefoe thee ust be a centpetal foce,

More information

Thermoelastic Problem of a Long Annular Multilayered Cylinder

Thermoelastic Problem of a Long Annular Multilayered Cylinder Wold Jounal of Mechancs, 3, 3, 6- http://dx.do.og/.436/w.3.35a Publshed Onlne August 3 (http://www.scp.og/ounal/w) Theoelastc Poble of a Long Annula Multlayeed Cylnde Y Hsen Wu *, Kuo-Chang Jane Depatent

More information

Chapter Fifiteen. Surfaces Revisited

Chapter 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 information

UNIT10 PLANE OF REGRESSION

UNIT10 PLANE OF REGRESSION UIT0 PLAE OF REGRESSIO Plane of Regesson Stuctue 0. Intoducton Ojectves 0. Yule s otaton 0. Plane of Regesson fo thee Vaales 0.4 Popetes of Resduals 0.5 Vaance of the Resduals 0.6 Summay 0.7 Solutons /

More information

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4 CSJM Unvesty Class: B.Sc.-II Sub:Physcs Pape-II Ttle: Electomagnetcs Unt-: Electostatcs Lectue: to 4 Electostatcs: It deals the study of behavo of statc o statonay Chages. Electc Chage: It s popety by

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part V: Velocity and Acceleration Analysis of Mechanisms Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.

More information

GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS

GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS #A39 INTEGERS 9 (009), 497-513 GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS Mohaad Faokh D. G. Depatent of Matheatcs, Fedows Unvesty of Mashhad, Mashhad,

More information

3.1 Electrostatic Potential Energy and Potential Difference

3.1 Electrostatic Potential Energy and Potential Difference 3. lectostatc Potental negy and Potental Dffeence RMMR fom mechancs: - The potental enegy can be defned fo a system only f consevatve foces act between ts consttuents. - Consevatve foces may depend only

More information

10/15/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101

10/15/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101 10/15/01 PHY 11 C Geneal Physcs I 11 AM-1:15 PM MWF Oln 101 Plan fo Lectue 14: Chapte 1 Statc equlbu 1. Balancng foces and toques; stablty. Cente of gavty. Wll dscuss elastcty n Lectue 15 (Chapte 15) 10/14/01

More information

INVERSE DYNAMICS OF THE CINCINNATI-MILACRON WRIST ROBOT

INVERSE DYNAMICS OF THE CINCINNATI-MILACRON WRIST ROBOT INVERSE DYNMIS OF THE ININNTI-MILRON WRIST ROOT ŞTEFN STIU * Recusve matx elatons n dynamcs of the ncnnat-mlacon wst obot ae establshed n ths pape. The pototype of ths mechansm s a thee-degees-offeedom

More information

Complex atoms and the Periodic System of the elements

Complex atoms and the Periodic System of the elements Complex atoms and the Peodc System of the elements Non-cental foces due to electon epulson Cental feld appoxmaton electonc obtals lft degeneacy of l E n l = R( hc) ( n δ ) l Aufbau pncple Lectue Notes

More information

SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes

SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes Факултет по математика и информатика, том ХVІ С, 014 SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15 NIKOLAY I. YANKOV ABSTRACT: A new method fo constuctng bnay self-dual codes wth

More information

BALANCING OF ROTATING MASSES

BALANCING OF ROTATING MASSES VTU EUST PROGRE - 7 YIS OF HIES Subject ode - E 54 IG OF ROTTIG SSES otes opled by: VIJYVITH OGE SSOITE PROFESSOR EPRTET OF EHI EGIEERIG OEGE OF EGIEERIG HSS -57. KRTK oble:94488954 E-al:vvb@cehassan.ac.n

More information

Design and Analysis of a Three Degrees of Freedom Parallel Kinematic Machine

Design and Analysis of a Three Degrees of Freedom Parallel Kinematic Machine Desgn and Analyss of a Thee Degees of Feedom Paallel Knematc Machne by Xaoln Hu A Thess Submtted n Patal Fulfllment of the Requements fo the Degee of Maste of Appled Scence n The Faculty of Engneeng and

More information

Dynamics of Rigid Bodies

Dynamics of Rigid Bodies Dynamcs of Rgd Bodes A gd body s one n whch the dstances between consttuent patcles s constant thoughout the moton of the body,.e. t keeps ts shape. Thee ae two knds of gd body moton: 1. Tanslatonal Rectlnea

More information

PHY126 Summer Session I, 2008

PHY126 Summer Session I, 2008 PHY6 Summe Sesson I, 8 Most of nfomaton s avalable at: http://nngoup.phscs.sunsb.edu/~chak/phy6-8 ncludng the sllabus and lectue sldes. Read sllabus and watch fo mpotant announcements. Homewok assgnment

More information

Rotating Disk Electrode -a hydrodynamic method

Rotating Disk Electrode -a hydrodynamic method Rotatng Dsk Electode -a hdodnamc method Fe Lu Ma 3, 0 ente fo Electochemcal Engneeng Reseach Depatment of hemcal and Bomolecula Engneeng Rotatng Dsk Electode A otatng dsk electode RDE s a hdodnamc wokng

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o? Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What

More information

A. Thicknesses and Densities

A. Thicknesses and Densities 10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe

More information

EFFICIENT COMPUTATION OF THE GENERALIZED INERTIAL TENSOR OF ROBOTS BY USING THE GIBBS- APPELL EQUATIONS

EFFICIENT COMPUTATION OF THE GENERALIZED INERTIAL TENSOR OF ROBOTS BY USING THE GIBBS- APPELL EQUATIONS EFFICIEN CMPUAIN F HE ENERALIZED INERIAL ENSR F RBS BY USIN HE IBBS- APPELL EQUAINS Povenzano S. (*) Mata V.(**) Ceccaell M.(***) and Suñe J.L. (**) (*) Escuela de Ingeneía Mecánca Unvesdad de Los Andes

More information

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin Some Appoxmate Analytcal Steady-State Solutons fo Cylndcal Fn ANITA BRUVERE ANDRIS BUIIS Insttute of Mathematcs and Compute Scence Unvesty of Latva Rana ulv 9 Rga LV459 LATVIA Astact: - In ths pape we

More information

A New Approach for Deriving the Instability Potential for Plates Based on Rigid Body and Force Equilibrium Considerations

A New Approach for Deriving the Instability Potential for Plates Based on Rigid Body and Force Equilibrium Considerations Avalable onlne at www.scencedect.com Poceda Engneeng 4 (20) 4 22 The Twelfth East Asa-Pacfc Confeence on Stuctual Engneeng and Constucton A New Appoach fo Devng the Instablty Potental fo Plates Based on

More information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

1. Starting with the local version of the first law of thermodynamics q. derive the statement of the first law of thermodynamics for a control volume

1. Starting with the local version of the first law of thermodynamics q. derive the statement of the first law of thermodynamics for a control volume EN10: Contnuum Mechancs Homewok 5: Alcaton of contnuum mechancs to fluds Due 1:00 noon Fda Febua 4th chool of Engneeng Bown Unvest 1. tatng wth the local veson of the fst law of themodnamcs q jdj q t and

More information

Chapter 23: Electric Potential

Chapter 23: Electric Potential Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done

More information

A. Proofs for learning guarantees

A. Proofs for learning guarantees Leanng Theoy and Algoths fo Revenue Optzaton n Second-Pce Auctons wth Reseve A. Poofs fo leanng guaantees A.. Revenue foula The sple expesson of the expected evenue (2) can be obtaned as follows: E b Revenue(,

More information

Chapter 13 - Universal Gravitation

Chapter 13 - Universal Gravitation Chapte 3 - Unesal Gataton In Chapte 5 we studed Newton s thee laws of moton. In addton to these laws, Newton fomulated the law of unesal gataton. Ths law states that two masses ae attacted by a foce gen

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

Contact, information, consultations

Contact, information, consultations ontact, nfomaton, consultatons hemsty A Bldg; oom 07 phone: 058-347-769 cellula: 664 66 97 E-mal: wojtek_c@pg.gda.pl Offce hous: Fday, 9-0 a.m. A quote of the week (o camel of the week): hee s no expedence

More information

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondence Analyss & Related Methods Ineta contbutons n weghted PCA PCA s a method of data vsualzaton whch epesents the tue postons of ponts n a map whch comes closest to all the ponts, closest n sense

More information

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. Flux: = da i. Force: = -Â g a ik k = X i. Â J i X i (7. Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum

More information

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage Median Ranked Set Sampling for Estimating the Population Median Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm

More information

Dynamic Performance, System Identification and Sensitivity Analysis of the Ladder Tracks. Ontario, Canada

Dynamic Performance, System Identification and Sensitivity Analysis of the Ladder Tracks. Ontario, Canada Dynamc Pefomance, System Identfcaton and Senstvty Analyss of the adde Tacks D. Younesan 1, S. Mohammadzadeh 1, E. Esmalzadeh 1 School of Ralway Engneeng, Ian Unvesty of Scence and Technology, Tehan, Ian,

More information

8 Baire Category Theorem and Uniform Boundedness

8 Baire Category Theorem and Uniform Boundedness 8 Bae Categoy Theoem and Unfom Boundedness Pncple 8.1 Bae s Categoy Theoem Valdty of many esults n analyss depends on the completeness popety. Ths popety addesses the nadequacy of the system of atonal

More information

CHAPTER 15 SPECIAL PERTURBATIONS

CHAPTER 15 SPECIAL PERTURBATIONS CHAPTER 5 SPECIAL PERTURBATIONS [Ths chapte s unde developent and t a be a athe long te befoe t s coplete. It s the ntenton that t a deal wth specal petubatons, dffeental coectons, and the coputaton of

More information

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017 COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER 1 016/017 PROGRAMME SUBJECT CODE : Foundaton n Engneeng : PHYF115 SUBJECT : Phscs 1 DATE : Septembe 016 DURATION :

More information

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GNRAL PHYSICS PH -3A (D. S. Mov) Test (/3/) key STUDNT NAM: STUDNT d #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

MULTIPOLE FIELDS. Multipoles, 2 l poles. Monopoles, dipoles, quadrupoles, octupoles... Electric Dipole R 1 R 2. P(r,θ,φ) e r

MULTIPOLE FIELDS. Multipoles, 2 l poles. Monopoles, dipoles, quadrupoles, octupoles... Electric Dipole R 1 R 2. P(r,θ,φ) e r MULTIPOLE FIELDS Mutpoes poes. Monopoes dpoes quadupoes octupoes... 4 8 6 Eectc Dpoe +q O θ e R R P(θφ) -q e The potenta at the fed pont P(θφ) s ( θϕ )= q R R Bo E. Seneus : Now R = ( e) = + cosθ R = (

More information

A Study of C-Reducible Finsler Space. With Special Cases

A Study of C-Reducible Finsler Space. With Special Cases Matheatcs Today Vol.27(June-2011)( Poc. of Maths Meet 2011) 47-54 ISSN 0976-3228 A Study of C-Reducble Fnsle Space Wth Specal Cases D. Pooja S. Saxena, D. Puneet Swaoop, E. Swat Swaoop Abstact The noton

More information

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t Indeternate Analyss Force Method The force (flexblty) ethod expresses the relatonshps between dsplaceents and forces that exst n a structure. Prary objectve of the force ethod s to deterne the chosen set

More information

arxiv: v2 [cs.it] 11 Jul 2014

arxiv: v2 [cs.it] 11 Jul 2014 A faly of optal locally ecoveable codes Itzhak Tao, Mebe, IEEE, and Alexande Bag, Fellow, IEEE axv:1311.3284v2 [cs.it] 11 Jul 2014 Abstact A code ove a fnte alphabet s called locally ecoveable (LRC) f

More information

Balancing of Stephenson s Mechanisms

Balancing of Stephenson s Mechanisms Intenatona Jouna of uent Engneeng and Technoogy E-ISSN 77 0, P-ISSN 37 0INPRESSO, Rghts Reseved vaabe at http://npessco.co/categoy/jcet Reseach tce aancng of Stephenson s Mechanss P. Neheah epatent of

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

Please initial the statement below to show that you have read it

Please initial the statement below to show that you have read it EN40: Dynacs and Vbatons Fnal Exanaton Wednesday May 18 011 School of Engneeng own Unvesty NAME: Geneal Instuctons No collaboaton of any knd s petted on ths exanaton. You ay use double sded pages of efeence

More information

UNIVERSITÀ DI PISA. Math thbackground

UNIVERSITÀ DI PISA. Math thbackground UNIVERSITÀ DI ISA Electomagnetc Radatons and Bologcal l Inteactons Lauea Magstale n Bomedcal Engneeng Fst semeste (6 cedts), academc ea 2011/12 of. aolo Nepa p.nepa@et.unp.t Math thbackgound Edted b D.

More information

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner.

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner. (C) 998 Gerald B Sheblé, all rghts reserved Lnear Prograng Introducton Contents I. What s LP? II. LP Theor III. The Splex Method IV. Refneents to the Splex Method What s LP? LP s an optzaton technque that

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-Type Inequalities and Their Applications in Optimization Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009

More information

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time Intenatonal Jounal of ompute Applcatons (5 ) Volume 44 No, Apl Optmal System fo Wam Standby omponents n the esence of Standby Swtchng Falues, Two Types of Falues and Geneal Repa Tme Mohamed Salah EL-Shebeny

More information

Machine Learning 4771

Machine Learning 4771 Machne Leanng 4771 Instucto: Tony Jebaa Topc 6 Revew: Suppot Vecto Machnes Pmal & Dual Soluton Non-sepaable SVMs Kenels SVM Demo Revew: SVM Suppot vecto machnes ae (n the smplest case) lnea classfes that

More information

Design and Simulation of a Three-Phase Electrostatic Cylindrical Rotary Micromotor

Design and Simulation of a Three-Phase Electrostatic Cylindrical Rotary Micromotor Intenatonal Jounal of Advanced Botechnology and Reseach (IJBR) ISSN 0976-61, Onlne ISSN 78 599X, Vol-7, Specal Issue-Numbe5-July, 016, pp917-91 http://www.bpublcaton.com Reseach Atcle Desgn and Smulaton

More information

Potential Theory. Copyright 2004

Potential Theory. Copyright 2004 Copyght 004 4 Potental Theoy We have seen how the soluton of any classcal echancs poble s fst one of detenng the equatons of oton. These then ust be solved n ode to fnd the oton of the patcles that copse

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

PHYS 1443 Section 003 Lecture #21

PHYS 1443 Section 003 Lecture #21 PHYS 443 Secton 003 Lectue # Wednesday, Nov. 7, 00 D. Jaehoon Yu. Gavtatonal eld. negy n Planetay and Satellte Motons 3. scape Speed 4. lud and Pessue 5. Vaaton of Pessue and Depth 6. Absolute and Relatve

More information

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c nd Intenatonal Confeence on Electcal Compute Engneeng and Electoncs (ICECEE 15) Dstnct 8-QAM+ Pefect Aays Fanxn Zeng 1 a Zhenyu Zhang 1 b Lnje Qan 1 c 1 Chongqng Key Laboatoy of Emegency Communcaton Chongqng

More information

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today? Clce Quz I egsteed my quz tansmtte va the couse webste (not on the clce.com webste. I ealze that untl I do so, my quz scoes wll not be ecoded. a Tue b False Theoetcal hyscs: the etenal quest fo a mssng

More information

Orbital Angular Momentum

Orbital Angular Momentum Obta Anua Moentu In cassca echancs consevaton o anua oentu s soetes teated b an eectve epusve potenta Soon we w sove the 3D Sch. Eqn. The R equaton w have an anua oentu te whch ases o the Theta equaton

More information

Chapter I Vector Analysis

Chapter I Vector Analysis . Chpte I Vecto nlss . Vecto lgeb j It s well-nown tht n vecto cn be wtten s Vectos obe the followng lgebc ules: scl s ) ( j v v cos ) ( e Commuttv ) ( ssoctve C C ) ( ) ( v j ) ( ) ( ) ( ) ( (v) he lw

More information

Groupoid and Topological Quotient Group

Groupoid and Topological Quotient Group lobal Jounal of Pue and Appled Mathematcs SSN 0973-768 Volume 3 Numbe 7 07 pp 373-39 Reseach nda Publcatons http://wwwpublcatoncom oupod and Topolocal Quotent oup Mohammad Qasm Manna Depatment of Mathematcs

More information

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3. 3 Eath s Rotaton 3.1 Rotatng Famewok Othe eadng: Valls 2.1, 2.2; Mashall and Plumb Ch. 6; Holton Ch. 2; Schubet Ch. 3 Consde the poston vecto (the same as C n the fgue above) otatng at angula velocty.

More information

Physics 1: Mechanics

Physics 1: Mechanics Physcs : Mechancs Đào Ngọc Hạnh Tâm Offce: A.503, Emal: dnhtam@hcmu.edu.vn HCMIU, Vetnam Natonal Unvesty Acknowledgment: Sldes ae suppoted by Pof. Phan Bao Ngoc Contents of Physcs Pat A: Dynamcs of Mass

More information

Chapter 31 Faraday s Law

Chapter 31 Faraday s Law Chapte 31 Faaday s Law Change oving --> cuent --> agnetic field (static cuent --> static agnetic field) The souce of agnetic fields is cuent. The souce of electic fields is chage (electic onopole). Altenating

More information

CHAPTER 3 SYSTEMS OF PARTICLES

CHAPTER 3 SYSTEMS OF PARTICLES HAPTER 3 SYSTEMS O PARTILES 3. Intoducton By systes of patcles I ean such thngs as a swa of bees, a sta cluste, a cloud of gas, an ato, a bck. A bck s ndeed coposed of a syste of patcles atos whch ae constaned

More information

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor Mcoelectoncs Ccut Analyss and Desgn Donald A. Neamen Chapte 5 The pola Juncton Tanssto In ths chapte, we wll: Dscuss the physcal stuctue and opeaton of the bpola juncton tanssto. Undestand the dc analyss

More information

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation By Rudy A. Gdeon The Unvesty of Montana The Geatest Devaton Coelaton Coeffcent and ts Geometcal Intepetaton The Geatest Devaton Coelaton Coeffcent (GDCC) was ntoduced by Gdeon and Hollste (987). The GDCC

More information

Mechanical design of IM. Torque Control of. Induction Machines... Slip ring rotor. Mathematical model. r r. Stator same as PMSM Rotor:

Mechanical design of IM. Torque Control of. Induction Machines... Slip ring rotor. Mathematical model. r r. Stator same as PMSM Rotor: Toqe ontol of Incton Machne... a copae to PMSM Intal Electcal Engneeng an Atoaton Mechancal egn of IM Stato ae a PMSM oto: at aln Won coppe /Slp ng Intal Electcal Engneeng an Atoaton n Unvety, Sween Nan

More information

One-dimensional kinematics

One-dimensional kinematics Phscs 45 Fomula Sheet Eam 3 One-dmensonal knematcs Vectos dsplacement: Δ total dstance taveled aveage speed total tme Δ aveage veloct: vav t t Δ nstantaneous veloct: v lm Δ t v aveage acceleaton: aav t

More information

ISSN: [Ramalakshmi* et al., 6(1): January, 2017] Impact Factor: 4.116

ISSN: [Ramalakshmi* et al., 6(1): January, 2017] Impact Factor: 4.116 IJESRT ITERATIOAL JOURAL OF EGIEERIG SCIECES & RESEARCH TECHOLOGY AALYSE THE OPTIMAL ERROR AD SMOOTHESS VALUE OF CHEBYSHEV WAVELET V.Raalaksh, B.Raesh Kua, T.Balasubaanan (Depatent o Matheatcs, atonal

More information

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork Joned Physcs Analyss Cente Summe Wokshop on the Reacton Theoy Execse sheet 8 Vncent Matheu Contact: http://www.ndana.edu/~sst/ndex.html June June To be dscussed on Tuesday of Week-II. Classwok. Deve all

More information

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs

More information

Minimising Energy Consumption for Robot Arm Movement

Minimising Energy Consumption for Robot Arm Movement Mnmsng Enegy Consumpton fo obot Am Movement Abdullah Mohammed, Benad Schmdt, Lhu Wang, Lang Gao KH oyal Insttute of echnology, Bnellvägen 8, Stockholm, SE- Sweden, E-Mal: abdullah.mohammed@tm.kth.se, lhu.wang@p.kth.se

More information

ScienceDirect. Dynamic model of a mobile robot

ScienceDirect. Dynamic model of a mobile robot Avalable onlne at www.scencedect.com ScenceDect Poceda Engneeng 96 (014 ) 03 08 Modellng of Mechancal and Mechatonc Systems MMaMS 014 Dynamc model of a moble obot Ján Kadoš* Faculty of Electcal Engneeng

More information