Near Time-Optimal Feedback Instantaneous Impact Point (IIP)

Size: px
Start display at page:

Download "Near Time-Optimal Feedback Instantaneous Impact Point (IIP)"

Transcription

1 1 Ne Time-Otiml Feedbck Instntneous Imct Point (IIP) Guidnce Lw fo Rocket Byeong-Un Jo 1 nd Jemyung An Koe Advnced Institute of Science nd Tecnology (KAIST) 91 Dek-Ro Dejeon Reublic of Koe Abstct Tis e ooses feedbck guidnce lw to move te instntneous imct oint (IIP) of ocket to desied loction. Anlytic exessions elting te time deivtives of n IIP wit te extenl cceletion of te ocket e intoduced. A ne time-otiml feedbck-fom guidnce lw to detemine te diection of te cceletion fo guiding te IIP is develoed using te deivtive exessions. Te effectiveness of te oosed guidnce lw in comison wit te esults of oen-loo tjectoy otimiztion ws demonstted toug IIP ointing cse studies. Keywods Instntneous Imct Point (IIP) Guidnce Ne Time-Otiml Rocket I. Intoduction Te instntneous imct oint (IIP) of ocket given its osition nd velocity is defined s its toucdown oint ssuming fee-fll fligt (witout oulsion) [1]. Te IIP is consideed s vey imotnt infomtion fo sfe lunc oetion of ocket nd it sould be clculted nd monitoed in el-time on te gound fcility o on-bod of te ocket. Te tesssing of IIP tjectoy coss destuction line (DL) is one imotnt citeion fo nge sfety decision ctivtion of te fligt temintion 1 Gdute Resec Assistnt Detment of Aeosce ngineeing 91 Dek-Ro. Associte Pofesso of Aeosce ngineeing 91 Dek-Ro; jemyung.n@kist.c.k. (Coesonding Auto).

2 system (FTS) fo fligt sfety oetion. A numbe of studies on ediction of te IIP nd tei lictions fo fligt sfety oetion could be found in te litetue. Tese studies include te tecniques fo comuting te IIP in vious coodinte systems [-5] metods on comenstion fo te effects of gvity etubtion nd tmoseic dg [6] exessions fo te time deivtives of IIP [7] nd intoduction of new fligt sfety citeion [8]. In ddition to fligt sfety oetions te IIP cn be used fo e-fligt nlysis nd oen-loo otimiztion of ocket ticully to obtin nd secify te imct oint of seted stges. Yoon nd An oosed tjectoy otimiztion ocedue consideing te IIPs of te fist-stge nd ylod fiing segments of lunc veicle s exlicit constints [9]. Using te disesion nlysis Mndic intoduced guidnce nd contol lgoitm tt cn stee ocket so tt its imct oint eces tget loction [10]. Te IIP cnge is imotnt fo ecent lnding guidnce of seted stge of eusble lunc veicle. Fo exmle it is known tt te lnding guidnce fo te seted fist stge of Flcon 9 involves te boostbck bun using tee out of nine engines wic cnge te IIP of stge towd te lnding site (bge si o lunc site) [11]. Tis e ooses new ne time-otiml feedbck guidnce lw tt moves te IIP of ocket to tget oint wose scemtic digm is sown in Fig. 1. Te nlytic fomultion tt descibes te time deivtives of n IIP fo given extenl cceletion vecto (imily oduced by te oulsion system) ws estblised. An otimiztion oblem tt detemines te comonents of te extenl cceletion vecto to lign te IIP deivtive vecto wit te desied diection nd mximize its mgnitude ws fomulted nd it cn be solved nlyticlly by intoducing te Lgnge multilies. Te oosed guidnce lw ws vlidted toug cse study nd comed wit te esults of n oen-loo tjectoy otimiztion to minimize te finl time. Tee key contibutions of tis study e summized s follows. Fist te oosed guidnce lw is feedbck fom tt cn exlicitly secify te IIP t te finl time. Since te guidnce lw is feedbck fom it is obust to te eo coming fom vious souces (e.g. te osition nd velocity eos t te beginning of te guidnce). Second its efomnce is ne time-otiml nd ne fuel-

3 3 otiml ssuming te cceletion ofile of te ocket is given. Lstly te oosed lw does not involve ny itetive ocedue wic is vey ttctive oety fo its otentil on-bod imlementtion. Tis eminde of tis e is ognized s follows. Section II intoduces te metodology to clculte te Kelein IIP nd its time deivtives. Section III ooses feedbck guidnce lw to move te IIP of ocket to desied oint in ne time-otiml mnne wic is obtinble by solving constined otimiztion oblem estblised bsed on te esults of Section II. Cse studies fo vlidting te guidnce lw e esented in Section IV. Finlly Section V discusses te comeensive conclusions of tis study nd otentil ootunities fo futue wok. Figue 1. Scemtic digm exlining IIP guidnce

4 4 II. Clcultion of IIP nd Its Time Deivtives Tis section intoduces te ocedues to clculte te IIP nd its time deivtives in n inetil (t centeed inetil CI) nd otting (t centeed t fixed CF) fmes wic ovides te fundmentls of te feedbck IIP guidnce lw discussed in tis e. Note tt Subsections II-A nd II- B e witten by summizing te esults of io studies conducted by An nd Ro [5 7]. Te metes nd geomety used to comute te IIP nd its time deivtives e sown in Fig.. Figue. Pmetes nd geomety fo comuting IIP nd its deivtives A. Clcultion of Kelein IIP [5] Conside te tnsltionl motion of ocket subject to gvity ( g ) nd n extenl cceletion ( ) s follows:

5 5 v (1) v g g i i i () () In te dynmic equtions nd v e osition nd velocity of te ocket esectively; nd e te comonents of cceletion vecto in osition tngentil nd line momentum diections esectively. In ddition te unit vectos i i nd i e defined s i (3) i v v v v i i i (4) (5) If te Kelein two-body motion is ssumed te gvittionl cceletion is exessed s g() (6) 3 Given cuent osition ( v 0 ) of te ocket its IIP in te CI coodinte fme is exessed s follows: 0 ) nd velocity ( cos( ) sin i i i (7) cos 0 cos v 0 In tis eqution 0 nd e esectively te fligt t ngle nd te ngle of fligt of te ocket exessed s 0 sin v v v v sin ( ) sin ( 0 0 ) c1c 3 c1 c3 ( c1 c )( c3 c ) c1 c (8) (9) wee c 1 c nd c 3 e exessed s c ( ) c 1 c 1 v (10)

6 6 Te time of fligt of te lunc veicle between te cuent time nd te imct time is exessed s follows [1] t F 1 tn (1 cos ) (1 ) sin cos tn v cos 1 cos cos( ) ( ) 1 cos cot sin cos cos 0 0 (11) wee ( ( v / v ) v / ) is defined s te sque of te tio between te cuent velocity nd 0 c 0 0 te cicul obit velocity wit given dius ( vc / 0 ). Te IIP ltitude nd longitude in te CI coodinte system cn be exessed using te comonents of te IIP unit vecto in q. (7) s 1 Lt sin ( iz ) (1) 1 Lon tn ( iy ix) (13) Te IIP longitude in te CF coodinte system is obtined by eflecting te t s ottion duing te time of fligt s Lon Lon ( t t t ) Lon t (14) e ef F e wee e indictes te ottionl te of te t t is te cuent time nd t ef is te time wen te CI nd CF coodintes coincide. Fo detils on te ocedue to comute te fligt time efe to efeences [5 13]. B. Time Deivtives of Kelein IIP [7] Cnge in te IIP of ocket occus wen te extenl cceletion is not zeo ( 0). Te time deivtive of te IIP unit vecto ( d( i ) / dt ) is exessed s line combintion of comonents of te extenl cceletion vecto s follows: T d dix diy diz i d d d (15) dt dt dt dt

7 7 In tis eqution d d nd d e te diections of te IIP deivtive ssocited wit tee comonents of extenl cceletion ( nd ) defined s follows: D d ( sin ( 0 v0)cos ) i0 ( 0 v0 cos ) i v0 (16) D d [ sin ( 0 v0)cos i0 ( 0 v0 cos ) i v0] (17) 1 d 0 sin i (18) In qs. (16)-(18) D nd D eesent te influence of nd on nd e exessed s D sin D ( c sin c cos ) 1 v 0 / e cos 0 0 sin ( c sin c cos ) 1 (19) (0) Note tt owing to te oety tt IIP moves long te sufce of te t te time deivtive comonents d d nd d e ll tngentil to i. In ddition qs. (16) nd (17) indicte tt d nd d wic e te in-lne cceletion comonents ssocited wit nd e llel. On te ote nd genetes te lne cnge motion of te ocket wose contibution in te IIP deivtive is diected to d. Te time deivtive of te time of fligt ( t F ) is exessed s follows e T e tf tf tf tf tf tf t 1 D D 1 D D D D D D D D 1 t (1) F e e F wee F D D F t t e D D e D nd e D in q. (1) e given s D 1 cos 1 cos t 3t 1 e e tf F F e 0 0 en sin sin 0 ()

8 8 t 1 cos 1 ecos cos 1 ecos tf F 0 0 De sin sin 0 e n esin esin 0 (3) D v0 sin0 e v0 sin0 D e (4) D v0cos 0 0 v0 cos e 0 D (5) e In qs. (4) nd (5) e nd n e te semimjo xis eccenticity semimete nd men motion of te obit esectively nd 0 nd e te eccentic nomly vlues of te ocket t te cuent nd imct oints exessed s follows 1 1/ v / 0 0 (6) (7) n 3 (8) / e 1 / (9) 0 cos e 1 0 (30) 1 cos e (31) Note tt t F is comosed of two ts: te t cused by gvity (-1) nd te deivtive ceted by extenl cceletion ( t F ). Te second t ( t otting (CF) fme wic is discussed in te next subsection. F ) is used to define te time deivtive of IIP in

9 9 C. Time Deivtives of Kelein IIP in CF Fme Te time deivtive of te Kelein IIP in te CF coodinte fme is exessed s follows d R d i TI ( i ) tf ( e i ) (3) dt dt wee i is te IIP unit vecto exessed in te CF fme T I is te tnsfom mtix fom te CI to CF coodinte system nd s e is te vecto eesenting te ottion of te t exessed i [ i i i ] T [cos(lt ) cos(lon ) cos(lt )sin(lon ) sin(lt )] T (33) x y z cos( et) sin( et) 0 T I sin( et) cos( et) 0 (34) [0 0 ] T (35) e Combining qs. (15) (1) nd (3) one cn obtin te following exession fo time deivtive of IIP in CF fme. d i d d d (36) dt wee i y t F d ed i x TI d (37) 0 i y t F d ed ix I T d (38) 0 I e d T d (39)

10 10 III. Feedbck Lw fo Ne Time-Otiml IIP Guidnce Tis section ooses ne time-otiml feedbck guidnce lw fo cnging te cuent IIP to te desied loction. Te guidnce lw ensues tt te IIP te vecto is ligned wit te diection of cicul c deting fom te cuent IIP nd iving t te tget osition wit its mximum mgnitude ossible. As eesented in Fig. 3 te sotest t between te cuent nd desied IIP long te sufce of te t is te c connecting te two oints. Let i denote te tget IIP vecto in CF coodi- t nte system. Ten q is defined s vecto noml to te lne secified by i nd t t ( i i) nd i q is defined s its unit vecto s follows: q i i i (40) t ( ) i q / q (41) q Figue 3: Definitions of unit vectos used fo IIP guidnce commnd genetion

11 11 Te unit vecto in te diection of te c (sotest t) between te cuent nd te tget IIPs ( defined s follows. i u ) is i i i (4) u q Te oblem detemines te cceletion vecto [ ] T wose mgnitude is given s m. Te IIP deivtive owing to (= d( i ) / dt d d d ) sould be llel to i u nd its mgnitude sould be mximized. Tt is we wnt to mximize [ d( i ) / dt] i subject to two u constints: 1) [ d( i ) / dt] i 0 nd ) q m 0. Tis oblem (P) cn be fomulted s constined otimiztion oblem descibed s follows. [P CG: IIP guidnce cceletion genetion] subject to T mx J( x) ( c x ) c x c x c x (43) x T xx m x1 x x3 m 0 (44) T f x f1x1 fx f3x3 0 (45) wee x is te decision vecto nd c T nd f T e te oblem metes defining te objective function nd constint esectively defined s x [ ] T (46) T c [ iu d iu d iu d ] [ c c c ] (47) 1 3 T f [ iq d iq d iq d ] [ f f f ] (48) 1 3 Te constined otimiztion oblem defined by qs. (43)-(48) cn be solved by intoducing L- T gnge multilies ssocited wit qs (44) nd (45) λ ( [ 1 ] ). Te ugmented cost function J ( ) x λ cn be defined s J ( x λ) c x ( x x ) ( f x) T T T 1 m ( c x c x c x ) ( x x x ) ( f x f x f x ) m (49) By lying J / x 0 (fo i = 1 3) te following equtions e obtined. i

12 1 J ( f c ) c x f 0 x x J ( f c ) c x f 0 x x 1 J ( f c ) c x f 0 x x (50) (51) (5) Putting qs. (50)-(5) into q. (45) nd solving fo te Lgnge multilie yields cf ( c f c f c f ) T T f f f1 f f3 (53) In ddition by combining qs. (50)-(5) wit q. (44) 1 is detemined s ( f1 c1 ) ( f c) ( f3 c3) T ( if c ( f c) 0) m 1 ( f1 c1 ) ( f c) ( f3 c3) T ( if ( ) 0) c f c m (54) Te cceletion comonents e given s f c 1 1 x1 (55) 1 f c x (56) 1 f c 3 3 x3 (57) 1 Te inuts to te oosed guidnce lw e te cuent osition ( 0) nd velocity (v 0) wic e used to clculte te cuent IIP nd diections fo IIP deivtives nd te oututs of te guidnce lw e te comonents of te guidnce cceletion vecto ( ). In ddition it sould be noted tt te ocedue does not involve ny itetion loos wic is n imotnt oety fo in-fligt imlementtion. Te ovell stuctue of te feedbck IIP guidnce lw esented in tis section is sown s block digm (wit elted eqution numbes) in Fig. 4. Te oosed guidnce is feedbck fom

13 13 tt uses te osition () nd velocity (v) s te inuts comutes te IIP ( i ) nd its diection vectos ( d d d ) s intemedite metes nd genetes te cceletion commnd () s te outut. In ddition ll te ocedues e sequentil witout ny involvement of itetions; even te otiml commnd genetion oblem (P CG) is solved nlyticlly. Figue 4. Block digm descibing te oosed feedbck IIP guidnce ocedue

14 14 IV. Cse Study Te vlidity of te oosed IIP guidnce lgoitm esented in Section III is demonstted toug cse study. Te IIP cnge mneuve of te seted fist stge of eusble lunc veicle (Flcon 9 of Sce X) ws selected s te scenio fo te cse study. Tble 1 summizes te configution of te ocket (seted stge) nd te initil condition used fo te cse study. Tble 1. Rocket configution nd initil condition fo cse study Rocket Configution Pmete Vlue Dy mss ton. Poellnt mss ton 57 Tust tonf 79.6 Secific imulse s 311 Fligt Condition Vlue Initil ltitude km 15.5 Initil seed inetil ( Initil fligtt ngle ( v 0 0 ) km/s ) deg 3.9 Initil osition ( 0) [km km km] [ ] Initil velocity (v 0) [m/s m/s m/s] [ ] Refeence time (t ef) s -40 Fig. 5 sows te cuent loction te oiginl IIP nd te desied imct loction fo te cse study. Te fist nd second cses decese te IIP distnce long te downnge diection by 100 km / 00 km. Te tid nd fout cses incese te nges by 100 km / 00 km. Te fift cse cnges te IIP to te cossnge diection by 150 km. To demonstte te qulity of te solution te esults of te feedbck IIP guidnce simultion wee comed wit te oen-loo tjectoy otimiztion. Te Genel Pseudosectl Otiml Contol Softwe (GPOPS) develoed by Ro et l. [14] ws used to cete te oen-loo otiml solutions fo cses. Te objective of te oen-loo tjectoy otimiztion ws cosen s minimiztion of te finl time (t f) te diection of te cceletion wee used nd te contol vibles nd te IIP t t f ws t imosed s constint ( i i ( t )). Bot te IIP guidnce simultion nd oen-loo otimiztion f

15 15 wee imlemented using MATLAB R015b nd un on mcine wit 3.5 GHz Intel Coe i7 CPU 16 GB RAM nd Windows 7 oeting system. Figue 5: Cuent nd imct loctions fo cse study Tble summizes te esults of te cse study obtined by using te oosed IIP guidnce lw nd te oen-loo tjectoy otimiztion. It cn be seen tt te diffeences in te objective function (finl time) between te esults obtined by two metods e vey smll less tn 1 % fo tee cses nd less tn 5 % even fo te wost cse (Cse ). Wen te esults e inteeted s te vlues of te velocity incements duing te mneuve te efomnce diffeence ws just 6.1 % t te wost cse. Bsed on tis comison esults we cn conclude tt te oosed IIP guidnce lw is ne time-otiml wit eltively smll mount of otimlity g. It is obseved tt te efomnce g (between te IIP guidnce nd te otiml esults) is eltively lge wen te cnge in IIP is not ligned wit te downnge diection. Cse equies tt te IIP cnge to te oosite of te downnge diection nd Cse 5 cnges te IIP in diection eendicul to te downnge diection.

16 16 Tble. Cse study esults (comison wit oen-loo otimiztion) Cse Finl Time (tf) s Poellnt Consumtion ton Otimiztion IIP Guidnce Diffeence % Otimiztion IIP Guidnce Otimiztion IIP Guidnce Diffeence % V m/s Figs. 6-8 sow te gound tjectoies of te ocket osition nd IIP obtined by te two metods fo Cses 4 nd 5 wee te IIPs e moving towd te desied loctions successfully. Tee is little noticeble diffeence between te two tjectoies. Figue 6. Tjectoies of ocket nd its IIP obtined by two metods (Cse )

17 17 Figue 7. Tjectoies of ocket nd its IIP obtined by two metods (Cse 4) Figue 8. Tjectoies of ocket nd its IIP obtined by two metods (Cse 5)

18 18 Te tjectoies using te two metods lmost efectly mtc. Howeve te cceletion ofiles ve meningful diffeences ticully in Cses nd 5. Figs come te istoies of cceletion comonents ( ) obtined by te IIP guidnce nd te oen-loo otimiztion fo Cses 4 nd 5. Te diffeences in cceletion comonents fo Cse 4 esented in Fig. 10 wic moves te IIP in te downnge diection wee eltively low. On te conty te ofiles of cceletion comonents fo te cses wee te diection of IIP cnge is significntly diffeent fom te downnge diection (Cse : te oosite diection Cse 5: 90 degee diffeence). It ws obseved tt te diffeences in comonents ssocited wit in-lne mneuve ( ) e eltively lge comed wit te diffeence in wic govens te lne cnge mneuve. Figue 9: Histoies of cceletion comonents obtined by two metods (Cse )

19 19 Figue 10. Histoies of cceletion comonents obtined by two metods (Cse 4) Figue 11: Histoies of cceletion comonents obtined by two metods (Cse 5)

20 0 Wile te esults of te cse study esented in tis section demonstte te ne time-otiml efomnce of te oosed feedbck IIP guidnce lw (oximtely 5 % diffeence in finl time fo IIP cnge of 00 km) some dditionl nlyses on te lgoitm e equied to justify its cticbility. Additionl test cses wit vious initil conditions nd IIP cnge tsks sould be conducted to undestnd te efomnce ccteistics nd obustness of te oosed lgoitm. In-det nlysis on te comuttionl lod of te ocedue is otentil subject fo futue wok. Studies on te detemintion of time to stt te oosed guidnce lw nd te imlementtion of te lgoitm witout cutoff cbility would be inteesting subjects fo otentil futue esec to imove its licbility. V. Conclusion A ne otiml feedbck guidnce lw to cnge te IIP of ocket to desied osition ws oosed in tis e. Te oosed lw is develoed by incooting te nlytic exessions fo te IIP nd its time deivtives nd solving constined otimiztion oblem wic ovides te cceletion commnd tt ligns te IIP deivtive vecto wit te desied diection nd mximizes its mgnitude. Cse studies on simultion of te IIP guidnce lw fo ocket (seted stge of lunc veicle) wit vious tget oints nd tei comisons wit numeiclly obtined oen-loo tjectoy otimiztion esults wee conducted. Te esults of te cse study demonstted te ne time-otiml efomnce of te oosed guidnce lw. Futemoe it cn be otentilly used s n on-bod lgoitm fo moving te IIP of ocket fte dditionl veifiction/vlidtion nd studies fo efomnce imovement. Acknowledgements Tis wok ws eed t te Koe Advnced Institute of Science nd Tecnology Detment of Aeosce ngineeing unde esec gnt fom te Ntionl Resec Foundtion of Koe (NRF- 013M1A3A3A004461). Autos tnk te Ntionl Resec Foundtion of Koe fo te suot of tis wok.

21 1 Refeences [1] Licensing nd Sfety Requiements fo Oetion of Lunc Site FAA Code of Fedel Regultions 14 Wsington D.C. Oct. 000 [] J. An W. Ro J. Pk G. Co Instntneous imct oint clcultion lgoitm of sounding ockets nd its liction to nge sfety system Jounl of te Koen Society fo Aeonuticl & Sce Sciences 8(6) (000) [3] O. Montenbuck M. Mkgf W. Jung B. Bull W. ngle GPS bsed ediction of te instntneous imct oint fo sounding ockets Aeosce Science nd Tecnology 6 (00) [4] O. Montenbuck M. Mkgf Globl ositioning system senso wit instntneous-imctoint ediction fo sounding ockets Jounl of Scecft nd Rockets 41 (004) [5] J. An W. Ro Nonitetive instntneous imct oint ediction lgoitm fo lunc oetions Jounl of Guidnce Contol nd Dynmics 35() (01) [6] J. An J. Seo Instntneous imct oint ediction using te esonse sufce metod Jounl of Guidnce Contol nd Dynmics 35() (01) [7] J. An W. Ro Anlytic time deivtives of instntneous imct oint Jounl of Guidnce Contol nd Dynmics 37() (014) [8] Y. Nm J. An T. Seong Adjusted instntneous imct oint nd new fligt sfety decision ule Jounl of Scecft nd Rockets 53(4) (016) [9] N. Yoon J. An Tjectoy otimiztion of lunc veicle wit exlicit instntneous imct oint constints fo vious nge sfety equiements Jounl of Aeosce ngineeing 9(3) (016) [10] S. Mndic Guidnce of gound to gound ockets using fligt t steeing metod Scientific Tecnicl Review 59(3-4) (009) [11] Te wy nd ow of lnding ockets SceX News June 015 URL: tt:// (Accessed on Nov ).

22 [1] A. D. Weelon. Fee fligt of bllistic missile ARS Jounl 9(1) (1959) [13] P. Zcn Tcticl nd Sttegic Missile Guidnce sixt edition Pogess in Aeonutics nd Astonutics AIAA Wsington D. C [14] A. V. Ro D. Benson C. Dby M. A. Ptteson C. Fncolin I. Sndes G. T. Huntington Algoitm 90: GPOPS MATLAB softwe fo solving multile-se otiml contol oblems using te Guss seudosectl metod ACM Tnsctions on Mtemticl Softwe 37() (010) 9-36.

On the Eötvös effect

On the Eötvös effect On the Eötvös effect Mugu B. Răuţ The im of this ppe is to popose new theoy bout the Eötvös effect. We develop mthemticl model which loud us bette undestnding of this effect. Fom the eqution of motion

More information

4.2 Boussinesq s Theory. Contents

4.2 Boussinesq s Theory. Contents 00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte

More information

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1 RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the

More information

mslumped-parameter (zero-dimensions!) groundwater model of Bangladesh

mslumped-parameter (zero-dimensions!) groundwater model of Bangladesh mslumed-pmete (zeo-dimensions!) goundwte model of Bngldesh You gol in this oblem set is to develo bucket model fo the hydology of ou study site in Bngldesh. Using this model, you will investigte how the

More information

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016 Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw

More information

1. The sphere P travels in a straight line with speed

1. The sphere P travels in a straight line with speed 1. The sphee P tels in stight line with speed = 10 m/s. Fo the instnt depicted, detemine the coesponding lues of,,,,, s mesued eltie to the fixed Oxy coodinte system. (/134) + 38.66 1.34 51.34 10sin 3.639

More information

Spring-Pendulum Dynamic System

Spring-Pendulum Dynamic System Sping-endulum Dynmic System echtonics Sping-endulum Dynmic System 1 esuements, Clcultions, nufctue's Specifictions odel mete ID Which metes to Identify? Wht Tests to efom? hysicl System hysicl odel th

More information

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess Motition Gien elocit field o ppoimted elocit field, we wnt to be ble to estimte

More information

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = = Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon

More information

Solutions to Midterm Physics 201

Solutions to Midterm Physics 201 Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of

More information

Answers to test yourself questions

Answers to test yourself questions Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E

More information

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy: LCTROSTATICS. Quntiztion of Chge: Any chged body, big o smll, hs totl chge which is n integl multile of e, i.e. = ± ne, whee n is n intege hving vlues,, etc, e is the chge of electon which is eul to.6

More information

7.5-Determinants in Two Variables

7.5-Determinants in Two Variables 7.-eteminnts in Two Vibles efinition of eteminnt The deteminnt of sque mti is el numbe ssocited with the mti. Eve sque mti hs deteminnt. The deteminnt of mti is the single ent of the mti. The deteminnt

More information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque

More information

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME Qulity contol Finl exm: // (Thu), 9:-: Q Q Q3 Q4 Q5 YOUR NAME NOTE: Plese wite down the deivtion of you nswe vey clely fo ll questions. The scoe will be educed when you only wite nswe. Also, the scoe will

More information

Design optimization of a damped hybrid vibration absorber

Design optimization of a damped hybrid vibration absorber This is the Pe-Published Vesion. Design otimiztion of dmed hybid vibtion bsobe Y. L. CHEUNG, W. O. WONG, L. CHENG Detment of Mechnicl Engineeing, The Hong Kong Polytechnic Univesity, Hung Hom, Hong Kong

More information

A CYLINDRICAL CONTACT MODEL FOR TWO DIMENSIONAL MULTIASPERITY PROFILES

A CYLINDRICAL CONTACT MODEL FOR TWO DIMENSIONAL MULTIASPERITY PROFILES Poceedings of 003 STLE/ASME Intentionl Joint Tibology Confeence Ponte Ved Bech, loid USA, Octobe 6 9, 003 003TIB-69 A CYLINDICAL CONTACT MODEL O TWO DIMENSIONAL MULTIASPEITY POILES John J. Jgodnik nd Sinn

More information

Michael Rotkowitz 1,2

Michael Rotkowitz 1,2 Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted

More information

Radial geodesics in Schwarzschild spacetime

Radial geodesics in Schwarzschild spacetime Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using

More information

APPROXIMATION OF STRONG ELECTRIC FIELD

APPROXIMATION OF STRONG ELECTRIC FIELD APPROXIMATION OF STRONG ELECTRIC FIELD PROF. RNDR. ING. MILOSLAV KOŠEK, CSC. ING. JIŘÍ PRIMAS ING. MICHAL MALÍK PROF. ING. ALEŠ RICHTER, CSC. Abstct: Since stong electic field is used now in mny es, simle

More information

Physics 1502: Lecture 2 Today s Agenda

Physics 1502: Lecture 2 Today s Agenda 1 Lectue 1 Phsics 1502: Lectue 2 Tod s Agend Announcements: Lectues posted on: www.phs.uconn.edu/~cote/ HW ssignments, solutions etc. Homewok #1: On Mstephsics this Fid Homewoks posted on Msteingphsics

More information

6. Gravitation. 6.1 Newton's law of Gravitation

6. Gravitation. 6.1 Newton's law of Gravitation Gvittion / 1 6.1 Newton's lw of Gvittion 6. Gvittion Newton's lw of gvittion sttes tht evey body in this univese ttcts evey othe body with foce, which is diectly popotionl to the poduct of thei msses nd

More information

Chapter 21: Electric Charge and Electric Field

Chapter 21: Electric Charge and Electric Field Chpte 1: Electic Chge nd Electic Field Electic Chge Ancient Gees ~ 600 BC Sttic electicit: electic chge vi fiction (see lso fig 1.1) (Attempted) pith bll demonsttion: inds of popeties objects with sme

More information

U>, and is negative. Electric Potential Energy

U>, and is negative. Electric Potential Energy Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When

More information

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system 436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique

More information

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons

More information

Friedmannien equations

Friedmannien equations ..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions

More information

10.3 The Quadratic Formula

10.3 The Quadratic Formula . Te Qudti Fomul We mentioned in te lst setion tt ompleting te sque n e used to solve ny qudti eqution. So we n use it to solve 0. We poeed s follows 0 0 Te lst line of tis we ll te qudti fomul. Te Qudti

More information

r a + r b a + ( r b + r c)

r a + r b a + ( r b + r c) AP Phsics C Unit 2 2.1 Nme Vectos Vectos e used to epesent quntities tht e chcteized b mgnitude ( numeicl vlue with ppopite units) nd diection. The usul emple is the displcement vecto. A quntit with onl

More information

This immediately suggests an inverse-square law for a "piece" of current along the line.

This immediately suggests an inverse-square law for a piece of current along the line. Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line

More information

Open Access SAR Image Enhancement Based On Fractional Fourier Transform

Open Access SAR Image Enhancement Based On Fractional Fourier Transform Send Odes fo Reints to eints@benthmscience.e The Oen Automtion nd Contol Systems Jounl, 14, 6, 53-58 53 Oen Access SAR Imge Enhncement Bsed On Fctionl Fouie Tnsfom Tn Gewei *, Pn Gungwu nd Lin Wei School

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology Int. J. Pue l. Sci. Technol. () (0). -6 Intentionl Jounl of Pue nd lied Sciences nd Technology ISSN 9-607 vilble online t www.ijost.in Resech Pe Rdil Vibtions in Mico-Isotoic Mico-Elstic Hollow Shee R.

More information

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468 ics Announcements dy, embe 28, 2004 Ch 6: Cicul Motion - centipetl cceletion Fiction Tension - the mssless sting Help this week: Wednesdy, 8-9 pm in NSC 128/119 Sundy, 6:30-8 pm in CCLIR 468 Announcements

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

Fluids & Bernoulli s Equation. Group Problems 9

Fluids & Bernoulli s Equation. Group Problems 9 Goup Poblems 9 Fluids & Benoulli s Eqution Nme This is moe tutoil-like thn poblem nd leds you though conceptul development of Benoulli s eqution using the ides of Newton s 2 nd lw nd enegy. You e going

More information

Numerical solution of the first order linear fuzzy differential equations using He0s variational iteration method

Numerical solution of the first order linear fuzzy differential equations using He0s variational iteration method Malaya Jounal of Matematik, Vol. 6, No. 1, 80-84, 2018 htts://doi.og/16637/mjm0601/0012 Numeical solution of the fist ode linea fuzzy diffeential equations using He0s vaiational iteation method M. Ramachandan1

More information

Optimization. x = 22 corresponds to local maximum by second derivative test

Optimization. x = 22 corresponds to local maximum by second derivative test Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible

More information

Chapter 4 Kinematics in Two Dimensions

Chapter 4 Kinematics in Two Dimensions D Kinemtic Quntities Position nd Velocit Acceletion Applictions Pojectile Motion Motion in Cicle Unifom Cicul Motion Chpte 4 Kinemtics in Two Dimensions D Motion Pemble In this chpte, we ll tnsplnt the

More information

NETWORK ANALYSIS OF ANTENNA BASED ON SCATTERING PARAMETERS

NETWORK ANALYSIS OF ANTENNA BASED ON SCATTERING PARAMETERS Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: 347-698 Volume-3, Issue-, Fe.-5 NETWORK ANALYI OF ANTENNA BAED ON CATTERING ARAMETER RENU INGH, KUMARI MAMTA Resech chol Associte ofesso

More information

Electric Potential. and Equipotentials

Electric Potential. and Equipotentials Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil

More information

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept

More information

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model Relace 85.8.3.2 with the following: 85.8.3.2 Tansmitted outut wavefom The 40GBASE-CR4 and 100GBASE-CR10 tansmit function includes ogammable equalization to comensate fo the fequency-deendent loss of the

More information

CELESTIAL MECHANICS. Advisor: Steve Surace Assistant: Margaret Senese

CELESTIAL MECHANICS. Advisor: Steve Surace Assistant: Margaret Senese CELESTIAL MECHANICS Andew Dvis, My Gemino, Etn Govemn, Semmie Kim, Dniel Mogn, Kte Sfin, Jke Snell, Alexnde Stepn, Denys Voytenko, Roslie Yn, Dniel Yoo, Eileen Zung Adviso: Steve Suce Assistnt: Mget Senese

More information

CHAPTER 2 ELECTROSTATIC POTENTIAL

CHAPTER 2 ELECTROSTATIC POTENTIAL 1 CHAPTER ELECTROSTATIC POTENTIAL 1 Intoduction Imgine tht some egion of spce, such s the oom you e sitting in, is pemeted by n electic field (Pehps thee e ll sots of electiclly chged bodies outside the

More information

1 Using Integration to Find Arc Lengths and Surface Areas

1 Using Integration to Find Arc Lengths and Surface Areas Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s

More information

Chapter 4 Two-Dimensional Motion

Chapter 4 Two-Dimensional Motion D Kinemtic Quntities Position nd Velocit Acceletion Applictions Pojectile Motion Motion in Cicle Unifom Cicul Motion Chpte 4 Two-Dimensionl Motion D Motion Pemble In this chpte, we ll tnsplnt the conceptul

More information

Analysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic

Analysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic In the fixed-oint imlementation of a digital filte only the esult of the multilication oeation is quantied The eesentation of a actical multilie with the quantie at its outut is shown below u v Q ^v The

More information

Energy Dissipation Gravitational Potential Energy Power

Energy Dissipation Gravitational Potential Energy Power Lectue 4 Chpte 8 Physics I 0.8.03 negy Dissiption Gvittionl Potentil negy Powe Couse wesite: http://fculty.uml.edu/andiy_dnylov/teching/physicsi Lectue Cptue: http://echo360.uml.edu/dnylov03/physicsfll.html

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

Study on Heat and Mass Transfer During Urea Prilling Process

Study on Heat and Mass Transfer During Urea Prilling Process Intentionl Jounl of Chemicl Engineeing nd Alictions, Vol., No. 5, Octobe 01 Study on Het nd Mss Tnsfe Duing Ue Pilling Pocess Ali Mehez, Ahmed Hmz H. Ali, W. K. Zh, S. Ookw, nd M. Suzuki Abstct Ue ills

More information

Comparative Studies of Law of Gravity and General Relativity. No.1 of Comparative Physics Series Papers

Comparative Studies of Law of Gravity and General Relativity. No.1 of Comparative Physics Series Papers Comptive Studies of Lw of Gvity nd Genel Reltivity No. of Comptive hysics Seies pes Fu Yuhu (CNOOC Resech Institute, E-mil:fuyh945@sin.com) Abstct: As No. of comptive physics seies ppes, this ppe discusses

More information

PROPER CURVATURE COLLINEATIONS IN SPECIAL NON STATIC AXIALLY SYMMETRIC SPACE-TIMES

PROPER CURVATURE COLLINEATIONS IN SPECIAL NON STATIC AXIALLY SYMMETRIC SPACE-TIMES POPE CUVATUE COLLINEATIONS IN SPECIAL NON STATIC AXIALLY SYMMETIC SPACE-TIMES GHULAM SHABBI, M. AMZAN Fculty of Engineeing Sciences, GIK Institute of Engineeing Sciences nd Technology, Toi, Swbi, NWFP,

More information

Assistant Professor: Zhou Yufeng. N , ,

Assistant Professor: Zhou Yufeng. N , , Aitnt Pofeo: Zhou Yufeng N3.-0-5, 6790-448, yfzhou@ntu.edu.g http://www3.ntu.edu.g/home/yfzhou/coue.html . A pojectile i fied t flling tget hown. The pojectile lee the gun t the me intnt tht the tget dopped

More information

π,π is the angle FROM a! TO b

π,π is the angle FROM a! TO b Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two

More information

Electronic Companion for Optimal Design of Co-Productive Services: Interaction and Work Allocation

Electronic Companion for Optimal Design of Co-Productive Services: Interaction and Work Allocation Submitted to Mnufctuing & Sevice Oetions Mngement mnuscit Electonic Comnion fo Otiml Design of Co-Poductive Sevices: Intection nd Wok Alloction Guillume Roels UCLA Andeson School of Mngement, 110 Westwood

More information

SHAPE OPTIMIZATION USING BOUNDARY ELEMENTS

SHAPE OPTIMIZATION USING BOUNDARY ELEMENTS SHAPE OPIMIZAION USING BOUNDARY ELEMENS Vlimi Kobelev Institute fo Poblems in Mechnics, Acemy of Sciences USSR Av. Venskogo. 101, Moscow, SU-117528, USSR 1. INRODUCION. he metho of eivtion of she sensitivity

More information

Important design issues and engineering applications of SDOF system Frequency response Functions

Important design issues and engineering applications of SDOF system Frequency response Functions Impotnt design issues nd engineeing pplictions of SDOF system Fequency esponse Functions The following desciptions show typicl questions elted to the design nd dynmic pefomnce of second-ode mechnicl system

More information

Two dimensional polar coordinate system in airy stress functions

Two dimensional polar coordinate system in airy stress functions I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in

More information

The Formulas of Vector Calculus John Cullinan

The Formulas of Vector Calculus John Cullinan The Fomuls of Vecto lculus John ullinn Anlytic Geomety A vecto v is n n-tuple of el numbes: v = (v 1,..., v n ). Given two vectos v, w n, ddition nd multipliction with scl t e defined by Hee is bief list

More information

Chapter 28 Sources of Magnetic Field

Chapter 28 Sources of Magnetic Field Chpte 8 Souces of Mgnetic Field - Mgnetic Field of Moving Chge - Mgnetic Field of Cuent Element - Mgnetic Field of Stight Cuent-Cying Conducto - Foce Between Pllel Conductos - Mgnetic Field of Cicul Cuent

More information

Electricity & Magnetism Lecture 6: Electric Potential

Electricity & Magnetism Lecture 6: Electric Potential Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why

More information

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

1.4 Using Newton s laws, show that r satisfies the differential equation 2 2

1.4 Using Newton s laws, show that r satisfies the differential equation 2 2 EN40: Dnmics nd Vibtions Homewok 3: Solving equtions of motion fo pticles School of Engineeing Bown Univesit. The figue shows smll mss m on igid od. The sstem stts t est with 0 nd =0, nd then the od begins

More information

cos kd kd 2 cosθ = π 2 ± nπ d λ cosθ = 1 2 ± n N db

cos kd kd 2 cosθ = π 2 ± nπ d λ cosθ = 1 2 ± n N db . (Balanis 6.43) You can confim tat AF = e j kd cosθ + e j kd cosθ N = cos kd cosθ gives te same esult as (6-59) and (6-6), fo a binomial aay wit te coefficients cosen as in section 6.8.. Tis single expession

More information

s c s (b) Hence, show that the entropy for rubber-like materials must have the separable form

s c s (b) Hence, show that the entropy for rubber-like materials must have the separable form EN: Continuum Mechnics Homewok 6: Aliction of continuum mechnics to elstic solids Due Decembe th, School of Engineeing Bown Univesity. Exeiments show tht ubbe-like mteils hve secific intenl enegy ( ) nd

More information

9.4 The response of equilibrium to temperature (continued)

9.4 The response of equilibrium to temperature (continued) 9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d

More information

LA0011_11GB. Formulas and Units. Rotation 2 W. W = work in Ws = J = Nm. = ang. velocity in rad./sec. f = frequency in rev./sec.

LA0011_11GB. Formulas and Units. Rotation 2 W. W = work in Ws = J = Nm. = ang. velocity in rad./sec. f = frequency in rev./sec. Tnsmission technicl clcultions Min Fomuls Size designtions nd units ccoding to the SI-units Line moement: s m/s t s t m s 1 m t m/s t P F W F m N Rottion ω π f d/s ω π f m/s M F P M ω W M J ω J ω W Ws

More information

Chapter 2: Electric Field

Chapter 2: Electric Field P 6 Genel Phsics II Lectue Outline. The Definition of lectic ield. lectic ield Lines 3. The lectic ield Due to Point Chges 4. The lectic ield Due to Continuous Chge Distibutions 5. The oce on Chges in

More information

This is a repository copy of Modeling soil behaviors under principal stress rotations.

This is a repository copy of Modeling soil behaviors under principal stress rotations. This is eositoy coy of Modeling soil behvios unde incil stess ottions. White Rose Resech Online URL fo this e: htt://eints.whiteose.c.uk/15185/ Vesion: Acceted Vesion Poceedings Pe: Yng, Y, Wng, Z nd Yu,

More information

Electromagnetic circulatory forces and rotordynamic instability in electric machines

Electromagnetic circulatory forces and rotordynamic instability in electric machines In: Hhn, E. J. & Rndll, R. B. (eds.). Poceedings of the 6th Intentionl Confeence on Roto Dynmics. Sydney, Austli, 3.9 4... Vol.. Sydney: Univesity of New South Wles Pinting Sevices,. P. 446 463. ISBN -7344-963-

More information

Nonlinear Feedback Control of VTOL UAVs

Nonlinear Feedback Control of VTOL UAVs Nonline Feedbck Contol of VTOL UAVs Dniele Pucci, Minh-Duc Hu, Pscl Moin, Tek Hmel, Clude Smson To cite this vesion: Dniele Pucci, Minh-Duc Hu, Pscl Moin, Tek Hmel, Clude Smson. Nonline Feedbck Contol

More information

NS-IBTS indices calculation procedure

NS-IBTS indices calculation procedure ICES Dt Cente DATRAS 1.1 NS-IBTS indices 2013 DATRAS Pocedue Document NS-IBTS indices clcultion pocedue Contents Genel... 2 I Rw ge dt CA -> Age-length key by RFA fo defined ge nge ALK... 4 II Rw length

More information

13.5. Torsion of a curve Tangential and Normal Components of Acceleration

13.5. Torsion of a curve Tangential and Normal Components of Acceleration 13.5 osion of cuve ngentil nd oml Components of Acceletion Recll: Length of cuve '( t) Ac length function s( t) b t u du '( t) Ac length pmetiztion ( s) with '( s) 1 '( t) Unit tngent vecto '( t) Cuvtue:

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.

More information

Physics 11b Lecture #11

Physics 11b Lecture #11 Physics 11b Lectue #11 Mgnetic Fields Souces of the Mgnetic Field S&J Chpte 9, 3 Wht We Did Lst Time Mgnetic fields e simil to electic fields Only diffeence: no single mgnetic pole Loentz foce Moving chge

More information

A Cornucopia of Pythagorean triangles

A Cornucopia of Pythagorean triangles A onucopi of Pytgoen tingles onstntine Zelto Deptment of temtics 0 ckey Hll 9 Univesity Plce Univesity of Pittsbug Pittsbug PA 60 USA Also: onstntine Zelto PO Bo 80 Pittsbug PA 0 USA e-mil ddesses: ) onstntine_zelto@yoocom

More information

Winter 2004 OSU Sources of Magnetic Fields 1 Chapter 32

Winter 2004 OSU Sources of Magnetic Fields 1 Chapter 32 Winte 4 OSU 1 Souces Of Mgnetic Fields We lened two wys to clculte Electic Field Coulomb's Foce de 4 E da 1 dq Q enc ˆ ute Foce Clcultion High symmety Wht e the nlogous equtions fo the Mgnetic Field? Winte

More information

Section 35 SHM and Circular Motion

Section 35 SHM and Circular Motion Section 35 SHM nd Cicul Motion Phsics 204A Clss Notes Wht do objects do? nd Wh do the do it? Objects sometimes oscillte in simple hmonic motion. In the lst section we looed t mss ibting t the end of sping.

More information

AUTOMATIC WHITE BALANCE FOR DIGITAL STILL CAMERA

AUTOMATIC WHITE BALANCE FOR DIGITAL STILL CAMERA AUTOMATI WHITE ALANE FOR DIGITAL STILL AMERA Tzn-Sheng hiou ( 邱贊生 ), hiou-shnn Fuh ( 傅楸善 ), nd Vsh hikne Detment of omute Science nd Infomtion Engineeing, Ntionl Tiwn Univesity, Tiei, Tiwn. E-mil: fuh@csie.ntu.edu.tw

More information

Phase Velocities of Three-Dimensional and Axis-Symmetrical Elastic Waves in Isotropic Cylindrical Shell

Phase Velocities of Three-Dimensional and Axis-Symmetrical Elastic Waves in Isotropic Cylindrical Shell Intentionl ounl of Teoeticl nd Mteticl Pysics, (6): 96- DOI:.593/j.ijtp.6.4 Pse Velocities of Tee-Diensionl nd Axis-Syeticl Elstic Wves in Isotopic Cylindicl Sell S. L. Ile nov *, A. A. Klescev Sint-Petesug

More information

St Andrew s Academy Mathematics Department Higher Mathematics VECTORS

St Andrew s Academy Mathematics Department Higher Mathematics VECTORS St ndew s cdemy Mthemtics etment Highe Mthemtics VETORS St ndew's cdemy Mths et 0117 1 Vectos sics 1. = nd = () Sketch the vectos nd. () Sketch the vectos nd. (c) Given u = +, sketch the vecto u. (d) Given

More information

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue 9 Top of tin foi Cyst pne () Bottom of tin foi B Lw d sinθ n Equtions connectin te Cyst metes (,, ) nd d-spcin wit bem pmetes () ( ) ne B Lw d (nm)

More information

Problem Set 3 SOLUTIONS

Problem Set 3 SOLUTIONS Univesity of Albm Deptment of Physics nd Astonomy PH 10- / LeCli Sping 008 Poblem Set 3 SOLUTIONS 1. 10 points. Remembe #7 on lst week s homewok? Clculte the potentil enegy of tht system of thee chges,

More information

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 604 Problem Set 1 Due Sept 16, 2010 Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside

More information

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin 1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic

More information

Available online at ScienceDirect. Procedia Engineering 91 (2014 ) 32 36

Available online at   ScienceDirect. Procedia Engineering 91 (2014 ) 32 36 Aville online t wwwsciencediectcom ScienceDiect Pocedi Engineeing 91 (014 ) 3 36 XXIII R-S-P semin Theoeticl Foundtion of Civil Engineeing (3RSP) (TFoCE 014) Stess Stte of Rdil Inhomogeneous Semi Sphee

More information

MAGNETIC EFFECT OF CURRENT & MAGNETISM

MAGNETIC EFFECT OF CURRENT & MAGNETISM TODUCTO MAGETC EFFECT OF CUET & MAGETM The molecul theo of mgnetism ws given b Webe nd modified lte b Ewing. Oested, in 18 obseved tht mgnetic field is ssocited with n electic cuent. ince, cuent is due

More information

Chapter 6 Thermoelasticity

Chapter 6 Thermoelasticity Chpte 6 Themoelsticity Intoduction When theml enegy is dded to n elstic mteil it expnds. Fo the simple unidimensionl cse of b of length L, initilly t unifom tempetue T 0 which is then heted to nonunifom

More information

Week 8. Topic 2 Properties of Logarithms

Week 8. Topic 2 Properties of Logarithms Week 8 Topic 2 Popeties of Logithms 1 Week 8 Topic 2 Popeties of Logithms Intoduction Since the esult of ithm is n eponent, we hve mny popeties of ithms tht e elted to the popeties of eponents. They e

More information

A Two-Dimensional Analytical Modeling of the Current-Voltage Characteristics for Submicron Gate-Length Ga As MESFET s

A Two-Dimensional Analytical Modeling of the Current-Voltage Characteristics for Submicron Gate-Length Ga As MESFET s Intentionl Jounl of ngineeing & Tecnolog IJT-IJN Vol: No:4 7 Two-imensionl nlticl Modeling of te Cuent-Voltge Ccteistics fo ubmicon Gte-Lengt G s MFT s deddine Kemissi, nd Ceif zizi bstct two-dimensionl

More information

NARAYANA I I T / P M T A C A D E M Y. C o m m o n Pr a c t i c e T e s t 0 9 XI-IC SPARK Date: PHYSICS CHEMISTRY MATHEMATICS

NARAYANA I I T / P M T A C A D E M Y. C o m m o n Pr a c t i c e T e s t 0 9 XI-IC SPARK Date: PHYSICS CHEMISTRY MATHEMATICS . (D). (B). (). (). (D). (A) 7. () 8. (B) 9. (B). (). (A). (D). (B). (). (B) NAAYANA I I T / T A A D E Y XIS-I-IIT-SA (..7) o m m o n c t i c e T e s t 9 XI-I SA Dte:..7 ANSWE YSIS EISTY ATEATIS. (B).

More information

Discrete Model Parametrization

Discrete Model Parametrization Poceedings of Intentionl cientific Confeence of FME ession 4: Automtion Contol nd Applied Infomtics Ppe 9 Discete Model Pmetition NOKIEVIČ, Pet Doc,Ing,Cc Deptment of Contol ystems nd Instumenttion, Fculty

More information

Mathematical formulation of the F 0 motor model

Mathematical formulation of the F 0 motor model negy Tnsduction in TP Synthse: Supplement Mthemticl fomultion of the F 0 moto model. Mkov chin model fo the evolution of the oto stte The fou possible potontion sttes of the two oto sp61 sites t the otostto

More information

Topics for Review for Final Exam in Calculus 16A

Topics for Review for Final Exam in Calculus 16A Topics fo Review fo Finl Em in Clculus 16A Instucto: Zvezdelin Stnkov Contents 1. Definitions 1. Theoems nd Poblem Solving Techniques 1 3. Eecises to Review 5 4. Chet Sheet 5 1. Definitions Undestnd the

More information

Collection of Formulas

Collection of Formulas Collection of Fomuls Electomgnetic Fields EITF8 Deptment of Electicl nd Infomtion Technology Lund Univesity, Sweden August 8 / ELECTOSTATICS field point '' ' Oigin ' Souce point Coulomb s Lw The foce F

More information

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018. SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl

More information

Properties and Formulas

Properties and Formulas Popeties nd Fomuls Cpte 1 Ode of Opetions 1. Pefom ny opetion(s) inside gouping symols. 2. Simplify powes. 3. Multiply nd divide in ode fom left to igt. 4. Add nd sutt in ode fom left to igt. Identity

More information

+ r Position Velocity

+ r Position Velocity 1. The phee P tel in tight line with contnt peed of =100 m/. Fo the intnt hown, detemine the coeponding lue of,,,,, eltie to the fixed Ox coodinte tem. meued + + Poition Velocit e 80 e 45 o 113. 137 d

More information

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts Chpte 5: Cuent, esistnce nd Electomotive Foce Chge cie motion in conducto in two pts Constnt Acceletion F m qe ndomizing Collisions (momentum, enegy) =>esulting Motion Avege motion = Dift elocity = v d

More information