Limit Analysis of Stability of Circular Foundation Pit
|
|
- Marylou Henry
- 5 years ago
- Views:
Transcription
1 Limi Anlyi of Sbiliy of Ciul Foundion Pi, Wu Simei Sool of Civil Engineeing Sndong Univeiy Sool of Civil Engineeing, Sou Cmpu of Sndong Univeiy, Jingi Rod 73#, Jinn, 561 Cin p:// Ab: - Ciul foundion pi ofen ppe in ivil engineeing. In ode o obin e iil dep of e non-uppoed iul foundion pi, e uppe-bound meod in pliiy meni w employed. Te umed lip ufe in nlyi w e oionl logpil ufe. Te kinemilly dmiible veloiy field w obined oding o e oied flow ule fo Coulomb meil, nd e opimizion model of e iil dep w eblied nd olved wi SQP opimizion lgoim. Te viion of e iil dep wi e lope ngle, e io of dep o diu of pi nd e inenl fiion ngle of oil wee udied. Te effe of e iul foundion pi mke e iil dep lge n e iil eig of e plne lope; oweve, wen e io of dep o diu of pi ppoe zeo, e uppe-bound oluion of e fome ppoe of e le. If e io of dep o dimee of pi i le n 1, e effe my be ignoed nd e foundion pi n be nlyzed e plne lope wi e meod of lie. Compion beween uppe-bound oluion(ubs), e oluion fom ppoxime lip line eoy(sls) nd finie diffeene oluion(fds) owed UBS i le n SLS nd lge ligly n FDS. Key-Wod: - iul foundion pi; lope; iil dep; limi nlyi; uppe-bound meod; effe 1 Inoduion Limi nlyi eoy i n impon bn of pli meni. I w developed fom e mel pli eoy nd ledy been exended o ok nd oil meni now. Limi nlyi w ued o olve ome engineeing poblem, u lope biliy nd limi lod[1-8]. I onin wo kind of bi meod, i.e. e uppe-bound meod nd e lowe-bound meod. Bed on uppe-bound eoem, e uppe-bound meod need o ebli e kinemilly dmiible filue menim nd veloiy field in dvne. Te veloiy field mu mee moion boundy ondiion nd oied pli flow ule. Bed on lowe-bound eoem, e lowe-bound meod need o e up illy dmiible e field wi mu ify equilibium equion, e boundy ondiion nd no diobey e filue ieion wi i Mo- Coulomb filue ieion fo ok nd oil. Limi nlyi n give e definie bound of ome poblem u e lope iil eig nd e pile being piy[1-8]. Howeve, e oluion fom igid limi equilibium meod, wi i noe nlyi meod ued exenively in geomeni, i diffiul o ell i i n uppebound oluion o lowe-bound oluion. Fo Some filue menim ued in limi equilibium meod, e oeponding kinemilly dmiible veloiy field fo limi nlyi n be obined oding o viul wok piniple. So e limi equilibium oluion fom ee filue menim e uppe-bound oluion, ju e Sm meod wi i n impon meod olving e fey fo of lope. Bu fo Some filue menim ued fequenly in limi equilibium meod, e oeponding kinemilly dmiible veloiy field n be e up, o e limi equilibium oluion en uppebound oluion, ju e veil lie meod nd e iul lide meod ued fo e biliy nlyi of lope. Fo veil lie meod, inelie foe n ify Mo-Coulomb filue ieion. Fo Coulomb meil obeying oied flow ule, e ngle beween veloiy jump veo nd e ngen of e lip ufe ould be equl o e inenl fiion ngle of meil, bu fo e iul igid lide menim, we n e up ny veloiy field ifying i. ISS: Iue 1, olume, Deembe 7
2 In ddiion, e limi equilibium oluion n be ued e lowe-bound oluion beue e e field in igid body i no known. Te uppe-bound meod i pplied moe exenively n e lowe-bound meod beue e eblimen of illy dmiible e field i e diffiul. Wile olving e poblem wi e uppe-bound meod, vlid filue menim i umed fily, nd en e inenl enegy diipion e nd e wok done by exenl lod e luled epeively nd equed wi e oe. Tu eil of uppe-bound oluion oeponding o e peifi menim e obined, nd finlly, e opimum uppe-bound oluion n be goen by employing opimizion enology[8]. Donld I nd Cen Z Y udied e biliie of pln in nd ee-dimenion lope uing igid blok nlionl filue menim[1-]. Muff obined e lel being piy of pile wi ee-dimenionl defoming menim[3]. Howeve, limi nlyi n be ued o olve e xiymeil poblem ye. Axiymeil poblem ppe fequenly in geonil engineeing u e biliie of iul foundion pi nd mo in-iu e u CPT nd SPT. Te im of i ppe i o olve e non-uppoed iil dep of e iul foundion pi o demone e ppliion of uppe-bound meod o xiymeil poblem. Te iul foundion pi i ofen nlyzed e plne in poblem wen e io of dep o diu of pi i lge enoug. Wen e io of dep o diu of pi i mll, oweve, e plne in oluion i no ue beue e effe of oil m lgely enne e biliy of e pi. In i ppe, limi nlyi meod will be employed o olve e iil dep of e iul foundion pi. Bed on e wok of Верезанцев В Г[9], limi equilibium oluion w lo obined nd omped wi uppe-bound oluion. In nlyi, oil i umed omogeneou nd ioopi, nd e filue i xiymeil. liding m nd long e lip ufe i le n e wok e done by e exenl lod. Ω σ * ij ε ij dω + σ Γε ΓdΓ W + T (1) Γ wee σ ij nd σ Γ denoe e of ee wiin e liding m egion Ω nd on poenil lip ufe Γ in pli limi e. ε ij, ε Γ nd denoe e of kinemilly dmiible in e wiin e liding m, on e poenil lip ufe Γ nd e veloiy field of e m, epeively. W nd T e e weig of liding m nd e exenl foe ing on e liding m, epeively. Fig.1 Sliding m of lope. Filue Menim A kind of lope, e ommon filue ufe of iul foundion pi i logpil ufe, ju own in fig.. Te oing ene of filue fe i on e xi of foundion pi. Te funion of logpil ufe i: e ( ) n φ Wee φ i inenl fiion ngle of oil, pol diu of poin b wee. () i Poblem Fomulion.1 Uppe-bound Teoem Wen lope liding m bove poenil lip ufe i in pli limi e (Fig.1), nd wen ny kinemilly dmiible veloiy field i inodued o e liding m, bed on uppebound eoem, e enegy diipion wiin e Fig. Filue menim of iul foundion pi ISS: Iue 1, olume, Deembe 7
3 Te pe of foundion pi n be deibed wi e io of dep o boom diu D / R nd lope ngle α of foundion pi, own in fig.. One ey e known, e dimenion of e wole filue zone n be deemined by wo independen vible: e eii ngle nd e dep of foundion pi D. In Fig., L i e leng of b ; β i defined pli ngle i e ngle beween lip ufe nd pi wll lope oe. Le A D / nd B L /. Ten equion (3)-(5) n be deived fom Fig.1: (3) (4) (5) (6) ( ) n φ A in e in B o o e β ( ) n φ A φ + α π / Te funion of e line in in Te funion of e line b i: i: oα in + nα (o B) in + nα o (7) (8) Te pol ngle of e poin o B o in Aoding o geomeil elionip, n be obined fom e following equion: (9) D R in e ( ) nφ ( ) nφ in e i: o in, nd ψ e dil, ngenil nd iumfeenil veloiy omponen in peil oodine yem (,, ψ ), epeively. Aoding o e oied pli flow ule, ψ on e logpil filue ufe. Hee we ume fue ψ in e wole defoming egion. n be deemined oding o e oied pli flow ule. In peil oodine, eno- in-e e wien : (1) ε 1 ε o εψ 1 γ ( γ ψ γ ψ ) Beue γ ψ γ ψ, ε ψ i pinipl in e. Aoding o e nomliy ofε, ε nd ε ψ, we know ε nd ε e lo pinipl in e. Subequenly we n know: (11) γ 1 ( ) Fo Coulomb meil ming oied flow ule, Cen W F gve e following equion[8]: (1) T ε + ε φ wee T n ( π 4 ), ε nd ε e e ummion of pinipl enionl in e nd e ummion of pinipl ompeive in e, epeively. oe enionl in e e poiive in i ppe. If φ, e following equion n be obined fom Eq.(1): ε + ε (13) `.3 eloiy Field ISS: Iue 1, olume, Deembe 7
4 Eq.(13) efle e inompeibiliy of Te meil nd i uied fo undined e of ued oil m. Beue ε, we know fom equion (1) ee i mximum in e ε mx nd minimum in eε min in ε ndε ψ. In ode o obin veloiy field, we udied e following wo e., ε ε min (1) ε ψ ε mx (1) (13) Fom Eq.(1) nd Eq.(1), we obin: o + T Fom Eq.(11) nd Eq.(1), we obin: T o + Te pil diffeenil equion bove n be olved uing e vible epion meod. Le f ( ) g( ), nd ubiue i ino Eq.(13) nd obin: (14) C 1 f ( ) g ( ) n C f ( ) g( ) T wee i onn. Solving e wo odiny diffeenil equion in Eq.(14), f () nd g ( ) n be obined. Te finl expeion of i: (15) ( ) ( 1 1 ) C in TC f g C wee C i onn. Subiuing Eq.(15) ino Eq.(11) o Eq.(1) led o C 1 1, u Eq.(15) n be wien (16) C in T Beue ε ψ ε mx >, we n know C > fe ubiuing Eq.(16) ino Eq.(1). A e me 1 π ime, < <. So we n know >. Ti indie oil m lide down nd doen diobey e ue pyil e., ε ψ ε min () ε ε mx Uing e me meod, we obin: T C in 1 (17) Beue ε ψ ε min <, C < n be known fe ubiuing Eq.(17) ino Eq.(1). A e me π ime, < <. So we n know <. Ti implie oil m lide up nd diobey e ue pyil ondiion. ow we know e mximum nd minimum pinipl in e e ε ψ ndε, epeively, nd i deemined uniquely by Eq. (16)..4 Inenl Enegy Diipion Re nd Exenl Foe Wok Re Enegy diipion ou on e lip ufe nd in e defoming zone. Hee wok i done by gviy of oil only beue ee e no oe exenl foe..4.1 Enegy Diipion Re Te inenl enegy diipion e inlude oe on filue ufe nd in pliiy defoming zone. Aoding o e lieue [8], e enegy diipion e of uni e on filue ufe i luled wi e following equion: (18) E 1 wee i oeion of oil; i ngenil veloiy jump o e filue ufe. Te ol enegy diipion e D 1 on filue ufe i obined by ineging Eq.(18) long e ufe i goen by oing e logpil line b bou e xe of foundion pi, own in Fig.: wee b D π o / oφe d (19) 1 b 1 i obined by Eq.(). ISS: Iue 1, olume, Deembe 7
5 Lieue [8] lo gve e expeion of e inenl enegy diipion e of uni volume in pliiy defoming zone: () E T One veloiy field i known, in e field n be obined oding o geomei equion. Bu i diffiul o obin e nlyi expeion of pinipl in e nd i limi e ppliion of Eq.(). In oogonl oodine yem { x, y, z}, if { x, y, z } of defoming egion i known, e pli noml in e field { ε x, ε y, ε z } n be obined oding o geomey equion. Fo oogonl oodine yem, ee i: ε ε + ε + ε ε + ε + ε x y z 1 3 ε + ε ε (1) wee ε i ( i 1,,3 ) e pinipl pli in e, ε i e bulk in e, ε nd ε e own in Eq.(1). Fom Eq.(1) nd Eq.(1), ε nd ε n be obined: ε ε () 1 T ε ε (3) 1 1/ T Fom Eq.() nd Eq.(), new expeion of e enegy diipion e pe uni volume n be obined: E oφ ε (4) Eq.(4) implie e enegy diipion e pe uni volume n be expeed wi e funion of pli bulk in e. In Eq.(4), oφ i e oodine of veex of e ig exgonl pymid woe ufe epeen Mo-Coulomb yield ufe in pinipl e pe. Wen φ, Coulomb meil will end o Te meil, o φ nd ε. Fo Te meil, e inenl enegy diipion e pe uni volume i: E ε (5) mx Comping Eq.(4) wi Eq.(5), e following equion n be obined: limoφε ε (6) φ mx Beue e pli bulk in e n be obined diely fom veloiy field nd geomey equion, Eq.(4) povide genel olving meod of e enegy diipion e pe uni volume. Te meod implifie e olving poe of e enegy diipion e. Te enegy diipion e of uni volume in defoming egion of iul pi n be obined fom Eq.(1) nd Eq.(4): E (7) C(1 T )oφ o in Te ol inenl enegy diipion e in defoming egion D n be luled by ineging Eq.(7) in e nnul domin i obined by oing e e b bou e xe of foundion pi, own in Fig.: D + d bd b π π T oe dd oe dd (9) wee b nd e obined by Eq.(6) nd Eq.(7), epeively, bd nd d e obined by Eq.()..4. Exenl Foe Wok Re Fo e foundion pi udied in i ppe, e gviy of oil i e only exenl foe. Te gviy wok e of uni volume oil i expeed: (3) w γ o wee γ i oil bulk deniy. Te ol gviy wok e of oil m W n be obined by ineging Eq.(3) in e nnul ISS: Iue 1, olume, Deembe 7
6 domin i obined by oing e e b bou e xe of foundion pi, own in Fig.: W + bd b d π π ow dd ow dd (31) wee nd e obined by Eq.(6) nd b Eq.(7), epeively, nd e obined by bd Eq.(). Te inegion bove ve no nlyi oluion, o we need o employ numeil meod o olve em..5 Memi Model Aoding o uppe-bound eoem, ee i (3) D D W 1 + d 3 Reul nd Anlyi 3.1 Ciil Heig Wen D / R i equl o.1 nd 1., epeively, e viion of wi φ nd α e owed in Fig.3. inee wi e inemen of φ. Moeove, e bigge φ i, e moe pidly vie. deee wi e inemen of α, fuemoe, e mlle α i, e moe pidly vie. Fig.4 ow viion of wi D / R nd φ wen α 9. inee wi e inemen of D / R. Moeove, wen D / R i vey mll, e viion of i lo mll. Ti ow e effe of oil m lgely enne e biliy of e foundion pi. Te iil dep of foundion pi n be expeed : D/R 1 (33) D γ f ( ) φ / ( ) In ode o obin e minimum uppe-bound oluion of iil dep, we need o olve e minimum of funion f ( ). Le min f ( ), wee i dimenionle vible, independen of nd γ nd only eled o φ, α nd D / R. Te memi model ued o olve e minimum uppe-bound oluion of iil dep of foundion pi i follow: () D/R 1 D/R.1 φ / ( ) (34) min f ( ) B (b) D/R.1 Fig.3 ying uve of wi φ nd α Te onin ondiion in Eq.(34) mke ue poin b i on e ig of poin, own in Fig.. Be on SQP opimizion lgoim, we ued mlb ofwe o olve e minimum uppe-bound of iil dep of iul foundion pi. ISS: Iue 1, olume, Deembe 7
7 α 9 Rigid zone Filue ufe β φ Rigid zone Fig.4 ying uve of wi D/R nd φ Fig.5 ow viion of eii ngle wi φ nd α. inee wi e inemen of φ nd α. One nd e known, oe eii ngle nd nd eii dimenion u, L nd o on n ll be obined. Tu e loion nd pe of e lip ufe n be deided. Wen D / R i vey mll, e iul foundion pi n be nlyzed e plne lope. In limi nlyi of plne lope, wo kind of filue menim e uully ued, i.e. igid blok nlionl nd oionl menim, own in fig.6 nd fig.7, epeively. In ble 1, of veil iul foundion pi wi D / R.1 nd veil plne lope fom diffeen filue menim e given, epeively. Wen D / R i vey mll, i n be found of iul foundion pi ppoxime of pln lope fom igid blok nlionl menim, nd bo of em e ligly gee n fom igid blok oionl menim. /( ) D/R D/R 1 φ /( ) Fig.5 ying uve of wi φ nd α Fig.6 Rigid blok nlionl filue menim Aoding o e eul ompued wi e meod popoed in i ppe, we lo know wen D / R. Ti implie e oionl logpil ufe degenee o e iul uned ufe. A e me ime, e iil lip ngle β oeponding o D i e me e iil vlue of β own in Fig.5 nd bo e equl o ( π / 4 φ / ). Bu i doen imply e pliiy defoming egion degenee o igid egion beue inenl enegy diipion e expeed by Eq.(4) in equl o zeo. Tble 1 obined fom ome filue menim φ α Plne lope wi igid blok nlionl filue menim Rigid zone Plne lope wi igid blok oionl filue menim Ciul foundion pi of D/R.1 wi xiymeil filue menim φ Rigid zone Logpil ufe Fig.7 Rigid blok oionl filue menim ISS: Iue 1, olume, Deembe 7
8 Te biliy of plne lope ofen i nlyzed wi veil lie meod, e.g. Jnbu meod. Fo pln lope, wen φ, fom Jnbu meod i equl o 6.1. I i vey imil o e uppe limi oluion of iul foundion pi woe D / R i.. So e effe of e foundion pi my be ignoed nd i n be egded pln lope nd nlyzed wi e lie meod wen e io of dep o dimee of pi i le n Slip Sufe Knowing nd, e pe nd loion of lip ufe n be obined. Hee, ume d nd e e oizonl nd veil dine of ny poin on lip ufe fom foundion pi wll oe, ju poin own in Fig.. In ode o plo lip ufe fom diffeen e on digm, nomlize d nd wi D nd obin dimenionle vible d / D nd / D, epeively. Fig.8 ow e effe of D / R on lip ufe of ylindil foundion pi wen φ. Wi e inee of D / R, lip ufe ink inwd. 4 Diuion Fig.9 Effe of φ on lip ufe Te oluion fom lip-line eoy (SLS) nd e oluion fom finie diffeene meod (FDS) wee ompued o omped wi e uppe-bound oluion (UBS). 4.1 Compion of UBS wi SLS Uing xiymeil lip-line eoy, Верезанцев В Г obined e ppoxime ive e peue on eining wll of ylindil foundion pi [9], own in e following equion: p T R λ R λ γ R [1 ( ) 1 ] + o φ( ) T ( 35) λ 1 Z Z wee γ i oil bulk deniy, φ nd e inenl fiion ngle nd oeion of oil, epeively, R π φ i diu of ylindil pi, T n ( ), 4 λ nφ / T, Z R + z T nd z i e dep unde gound, own in Fig.1. Fig.8 Effe of D / R on lip ufe Fig.9 ow e effe of φ on lip ufe of ylindil foundion pi wen D / R.8. Wi e inee of φ, lip ufe ink inwd. O x z Fig.1 Cylindil foundion pi ISS: Iue 1, olume, Deembe 7
9 Le R, we n obin: p γ zt T (36) Fom Eq.(36), e expeion of ive e peue i een o be e me Rnkin fomul fo plne poblem wen R i vey lge. In ode o olve e iil dep of ylindil foundion pi, following nion meod of Tezgi nd pek[1], e ive e peue i ineged long e dep nd equing e inegl zeo: D p dz (37) Fom Eq.(35) nd Eq.(37), we n obin: ( A B)( λ )( λ 1) T D [ BT ( λ) + A( λ 1)] R + [ BT ( λ) R + A( λ 1)( R λ ( ) 1 T D + R T D + R)] (38) T wee A γr, B oφ. λ 1 SLS of iil dep of ylindil foundion pi n be obined by olving Eq.(38) wi numeil meod. Compion w mde beween UBS nd SLS, own in Fig.7. Fo ylindil foundion pi, i n be een UBS i ligly gee n SLS wen φ, oweve, in oe e, e fome i lwy le n e le. UBS SLS Auming 1 nd e UBS nd SLS of, epeively, e elion of 1 nd n be eblied. Fo ylindil foundion pi, (39) D f (, γ, R, φ) omlize wo ide of Eq.(39) nd we n obin: (4) (4) Dγ Rγ g(, φ) Fom Eq.(33) nd Eq.(34), we know Rγ 1 D / R Fom Eq.(4) nd Eq.(41), we n obin 1 g(, φ) D / R 1 (41) Eq.(4) give e elion beween nd. Fo D / R.1 ~ 1., e elion beween nd i e D / R φ 1 (43) Fig.1 ow e fiing effeive of Eq.(43). Te elion beween nd n be expeed well wi Eq.(43). 1 φ /( ) Fig.11 Compion beween UBS nd SLS of iil dep Fig.1 Fiing effeive digm ISS: Iue 1, olume, Deembe 7
10 4. Compion of UBS wi FDS FLAC/SLOPE pogm w ued o ompue e numeil oluion of. Ti pogm i miniveion of FLAC(F Lgngin Anlyi of Coninu) i povided by I Conuling Goup, In. FLAC/Slope i deigned peifilly o pefom fo-of-fey lulion fo lope biliy nlyi. Beide wo-dimenionl plnein nlyi, xiymmei nlyi n lo be pefomed wi FLAC/Slope. FLAC/Slope povide n lenive o diionl limi equilibium pogm o deemine fo of fey. Limi equilibium ode ue n ppoxime eme - ypilly bed on e meod of lie -in wi numbe of umpion e mde (e.g., e loion nd ngle of inelie foe). Sevel umed filue ufe e eed, nd e one giving e lowe fo of fey i oen. Equilibium i only ified on n idelized e of ufe. In on, FLAC/Slope povide full oluion of e oupled e/diplemen, equilibium nd oniuive equion, ju FEM[11-13]. Given e of popeie, e yem i deemined o be ble o unble. By uomilly pefoming eie of imulion wile nging e eng popeie (e eng eduion enique), e fo of fey n be found o oepond o e poin of biliy, nd e iil filue ufe n be loed. Aoding o eng eduion enique, eng pmee ued in biliy nlyi n be wien :, F nφ n φ (44) wee F i fey fo, nd φ e mobile oeion nd mobile inenl fiion ngle of oil, epeively. Wen iil filue ppen unde ndφ, F n be obined fom Eq.(44). In ode o obin e iil dep of ylindil pi, nge e dep gdully nd obin e oeponding fey fo. Wen e fey fo i ppoximely 1., e dep i e iil one. Fig.13 illue e ompuing poe in wi fey fo vie wi dep. In Fig.13, γ k/m 3, 1kP, φ 3 nd R.5m. F Fig.13 D-F uve Fom Eq.(33) nd Eq.(34), we obin Dγ (45) Some numeil eul of iil dep of ylindil pi wee lied in ble nd omped wi UBS. I n be een UBS of i lge ligly n FDS. Tble Compion of UBS wi FDS φ 3 1 D/R FDS UBS Filue ufe n be obined long wi D. Fo e e of γ k/m 3, 1kP, φ nd R.5m, e filue of pi i illued in Fig.14. Te filue ufe i een o ppo e oionl logpil ufe umed in limi nlyi in i ppe. ISS: Iue 1, olume, Deembe 7
11 JOB TITLE :. FLAC/SLOPE (eion 5.) 8-Ap-8 14:19 LEGED Fo of Sfey 1.1 Mx. e in-e 5.E-7 1.E-6 1.5E-6.E-6.5E-6 3.E-6 3.5E-6 4.E-6 4.5E-6 Conou inevl 5.E-7 (zeo onou omied) Boundy plo 5E eloiy veo mx veo 1.167E-5 E (*1^1) Fig.14 Filue ufe 5 Conluion Auming oil m i omogeneou nd ioopi nd e filue model of iul foundion pi i xiymeil, kinemilly dmiible filue menim nd veloiy field wee eblied oding o oied pli flow ule. Uing em, e biliy of e iul foundion pi w nlyzed nd e limi uppebound oluion of iil eig w obined. Te following e ome impon onluion: (1) Ciil dep inee wi e deemen of lope ngle of foundion pi nd e inemen of e io of dep o diu nd inenl fiion ngle of oil. () Te effe of iul foundion pi mke i iil dep gee n e iil eig of plne lope. Howeve, e effe i unonpiuou wen e io of dep o dimee of pi i le n 1. (3) Wen e io of dep o diu i vey mll, e uppe-bound oluion of iul foundion pi i vey loe o e one of plne lope obined fom igid blok nlionl filue menim. Moeove, on e xiymeil ufe, e oionl logpil filue line degenee o ig line, nd e iil lip ngle i e me plne lope fom igid blok nlionl menim, oweve, e pliiy defoming zone in igid ye. (4) UPS of e iil dep i le n SLS nd lge ligly n FDS. In i ppe, e iil dep of e nonuppoed iul foundion pi w udied; oweve, fue eee e ugen on e biliy of iul pi einfoed, fo exmple, by oil nil. (*1^1) Aknowledgemen Ti wok w uppoed by Cine ul Siene Foundion(o.57856) nd ul Siene Foundion of Sndong Povine, Cin(o. Q6F). Refeene: [1] Donld I, Cen Z Y. Slope biliy nlyi by e uppe-bound ppo: fundmenl nd meod. Cndin Geoenil Jounl, ol.34, o.6, 1997, pp [] Cen Z Y, Wng X G, Hbefield C, e l. A ee-dimenionl lope biliy nlyi meod uing e uppe-bound eoem P 1: eoy nd meod. Inenionl Jounl of Rok Meni nd Mining Siene, ol.38, o.6, 1, pp [3] Muff J D, Hmilon J M. P-ulime fo undined nlyi of lelly loded pile. Jounl of Geoenil Engineeing, ol.119, o.1, 1993, pp [4] Dee A, Deouny E. Limi lod in nlionl filue menim fo oiive non-oiive meil. Geoenique, ol.43, o.3, 1993, pp [5] Oni J, Oii H nd Ymmoo K. Being piy nlyi of einfoed foundion on oeive oil. Geoexile nd Geomembne, ol.16, 1998, pp [6] Zeng X, Booke J R, Ce J P. Limi nlyi of e being piy of fiued meil. Inenionl Jounl of Solid nd Suue, ol.37,, pp [7] Pob A, Zo A, Kobyi M nd Kiid T. Uppe bound eime of led einfoed oil eining wll. Geoexile nd Geomembne, ol.18,, pp [8] Cen W F. Limi nlyi nd oil pliiy. Amedm, e eelnd: Elevie Publiing Co., 1975 [9] Верезанцев В Г. Axil-ymmeil limi equilibium poblem of looe medi. Beijing: Cin Aieue nd Building Pe, 1981 [1] Tezgi K, Pek R B. Soil Meni in Engineeing Pie[M]. ew Yok: Wiley, 1967 [11] Lin, Suliu, Ann S. Adpive Finie Elemen Anlyi fo Soluion of Complex Engineeing Poblem. We Tnion on Applied nd Teoeil Meni, ol.1, 6, pp [1] Bbiei A, Cei A. Anlyi of mony olumn by 3D FEM omogeniion poedue. We Tnion on Applied nd Teoeil Meni, ol., 6, pp.4-51 ISS: Iue 1, olume, Deembe 7
12 [13] Dubvk M. On dimenionl eduion in mulile, finie elemen nd omii nlyi in olid meni. We Tnion on Applied nd Teoeil Meni, ol.1, 6, pp.16-4 ISS: Iue 1, olume, Deembe 7
ME 141. Engineering Mechanics
ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics
More informationSection P.1 Notes Page 1 Section P.1 Precalculus and Trigonometry Review
Secion P Noe Pge Secion P Preclculu nd Trigonomer Review ALGEBRA AND PRECALCULUS Eponen Lw: Emple: 8 Emple: Emple: Emple: b b Emple: 9 EXAMPLE: Simplif: nd wrie wi poiive eponen Fir I will flip e frcion
More information() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration
Secion 1.4 Moion in Spce: Velociy nd Acceleion We e going o dive lile deepe ino somehing we ve ledy inoduced, nmely () nd (). Discuss wih you neighbo he elionships beween posiion, velociy nd cceleion you
More informationAcceleration and Deceleration Phase Nonlinear Rayleigh-Taylor Growth at Spherical Interfaces
Aeleion nd Deeleion Pse Nonline Ryleig-Tylo Gow Speil Inefes Pesened o: HEDP Summe Sool Dniel S. Clk nd Mx Tbk Lwene Livemoe Nionl Lbooy Augus 5 Tis wok ws pefomed unde e uspies of e U.S. Depmen of Enegy
More informationEquations from The Four Principal Kinetic States of Material Bodies. Copyright 2005 Joseph A. Rybczyk
Equions fom he Fou Pinipl Kinei Ses of Meil Bodies Copyigh 005 Joseph A. Rybzyk Following is omplee lis of ll of he equions used in o deied in he Fou Pinipl Kinei Ses of Meil Bodies. Eh equion is idenified
More informationInvert and multiply. Fractions express a ratio of two quantities. For example, the fraction
Appendi E: Mnipuling Fions Te ules fo mnipuling fions involve lgei epessions e el e sme s e ules fo mnipuling fions involve numes Te fundmenl ules fo omining nd mnipuling fions e lised elow Te uses of
More information10.3 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 informationD zone schemes
Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic
More informationLimit Analysis of Stability of Circular Foundation Pit
5t WSEAS Int. Conf. on ENIRONMENT, ECOSYSTEMS and DEELOPMENT, Teneife, Spain, Decembe 14-16, 27 13 Limit Analyi of Stability of Cicula Foundation Pit CUI XINZHUANG, YAO ZHANYONG, JIN QING, WU SHIMEI Scool
More informationComputer Aided Geometric Design
Copue Aided Geoei Design Geshon Ele, Tehnion sed on ook Cohen, Riesenfeld, & Ele Geshon Ele, Tehnion Definiion 3. The Cile Given poin C in plne nd nue R 0, he ile ih ene C nd dius R is defined s he se
More informationMotion on a Curve and Curvature
Moion on Cue nd Cuue his uni is bsed on Secions 9. & 9.3, Chpe 9. All ssigned edings nd execises e fom he exbook Objecies: Mke cein h you cn define, nd use in conex, he ems, conceps nd fomuls lised below:
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationCircuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.
4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss
More informationf(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2
Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe
More informationLAPLACE TRANSFORMS. 1. Basic transforms
LAPLACE TRANSFORMS. Bic rnform In hi coure, Lplce Trnform will be inroduced nd heir properie exmined; ble of common rnform will be buil up; nd rnform will be ued o olve ome dierenil equion by rnforming
More informationSome algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER
. Soe lgoi o solving syse o line vole inegl eqion o second ind by sing MATLAB 7 ALAN JALAL ABD ALKADER College o Edcion / Al- Msnsiiy Univesiy Depen o Meics تقديم البحث :-//7 قبول النشر:- //. Absc ( /
More informationPrimal and Weakly Primal Sub Semi Modules
Aein Inenionl Jounl of Conepoy eeh Vol 4 No ; Jnuy 204 Pil nd Wekly Pil ub ei odule lik Bineh ub l hei Depen Jodn Univeiy of iene nd Tehnology Ibid 220 Jodn Ab Le be ouive eiing wih ideniy nd n -ei odule
More informationConsider a Binary antipodal system which produces data of δ (t)
Modulaion Polem PSK: (inay Phae-hi keying) Conide a inay anipodal yem whih podue daa o δ ( o + δ ( o inay and epeively. Thi daa i paed o pule haping ile and he oupu o he pule haping ile i muliplied y o(
More informationReinforcement learning
CS 75 Mchine Lening Lecue b einfocemen lening Milos Huskech milos@cs.pi.edu 539 Senno Sque einfocemen lening We wn o len conol policy: : X A We see emples of bu oupus e no given Insed of we ge feedbck
More informationX-Ray Notes, Part III
oll 6 X-y oe 3: Pe X-Ry oe, P III oe Deeo Coe oupu o x-y ye h look lke h: We efe ue of que lhly ffee efo h ue y ovk: Co: C ΔS S Sl o oe Ro: SR S Co o oe Ro: CR ΔS C SR Pevouly, we ee he SR fo ye hv pxel
More informationCSC 373: Algorithm Design and Analysis Lecture 9
CSC 373: Algorihm Deign n Anlyi Leure 9 Alln Boroin Jnury 28, 2013 1 / 16 Leure 9: Announemen n Ouline Announemen Prolem e 1 ue hi Friy. Term Te 1 will e hel nex Mony, Fe in he uoril. Two nnounemen o follow
More informationAddition & Subtraction of Polynomials
Addiion & Sucion of Polynomil Addiion of Polynomil: Adding wo o moe olynomil i imly me of dding like em. The following ocedue hould e ued o dd olynomil 1. Remove enhee if hee e enhee. Add imil em. Wie
More informationCh.4 Motion in 2D. Ch.4 Motion in 2D
Moion in plne, such s in he sceen, is clled 2-dimensionl (2D) moion. 1. Posiion, displcemen nd eloci ecos If he picle s posiion is ( 1, 1 ) 1, nd ( 2, 2 ) 2, he posiions ecos e 1 = 1 1 2 = 2 2 Aege eloci
More informationDetection of a Solitude Senior s Irregular States Based on Learning and Recognizing of Behavioral Patterns
eeion of oliude enio Ieul e ed on Lenin nd Reonizin of eviol en ieki oki onmeme ki nii eme uio Kojim eme Kunio ukun eme Reenly enion i id o monioin yem w evio of oliude eon in ome e oulion of oliude enio
More informationPhysics 232 Exam II Mar. 28, 2005
Phi 3 M. 8, 5 So. Se # Ne. A piee o gl, ide o eio.5, h hi oig o oil o i. The oil h ide o eio.4.d hike o. Fo wh welegh, i he iile egio, do ou ge o eleio? The ol phe dieee i gie δ Tol δ PhDieee δ i,il δ
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationPHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM
PHYS 0 Suen Nme: Suen Numbe: FAUTY OF SIENE Viul Miem EXAMINATION PHYSIS 0 Ino PHYSIS-EETROMAGNETISM Emines: D. Yoichi Miyh INSTRUTIONS: Aemp ll 4 quesions. All quesions hve equl weighs 0 poins ech. Answes
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationClassification of Equations Characteristics
Clssiiion o Eqions Cheisis Consie n elemen o li moing in wo imensionl spe enoe s poin P elow. The ph o P is inie he line. The posiion ile is s so h n inemenl isne long is s. Le he goening eqions e epesene
More informationMEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING
MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens
More informationEECE 260 Electrical Circuits Prof. Mark Fowler
EECE 60 Electicl Cicuits Pof. Mk Fowle Complex Numbe Review /6 Complex Numbes Complex numbes ise s oots of polynomils. Definition of imginy # nd some esulting popeties: ( ( )( ) )( ) Recll tht the solution
More informationcan be viewed as a generalized product, and one for which the product of f and g. That is, does
Boyce/DiPrim 9 h e, Ch 6.6: The Convoluion Inegrl Elemenry Differenil Equion n Bounry Vlue Problem, 9 h eiion, by Willim E. Boyce n Richr C. DiPrim, 9 by John Wiley & Son, Inc. Someime i i poible o wrie
More informationScience Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253
Science Adeisemen Inegoenmenl Pnel on Clime Chnge: The Phsicl Science Bsis hp://www.ipcc.ch/spmfeb7.pdf /3/7 Phsics 53 hp://www.fonews.com/pojecs/pdf/spmfeb7.pdf /3/7 Phsics 53 3 Sus: Uni, Chpe 3 Vecos
More informationgraph of unit step function t
.5 Piecewie coninuou forcing funcion...e.g. urning he forcing on nd off. The following Lplce rnform meril i ueful in yem where we urn forcing funcion on nd off, nd when we hve righ hnd ide "forcing funcion"
More informationON THE EXTENSION OF WEAK ARMENDARIZ RINGS RELATIVE TO A MONOID
wwweo/voue/vo9iue/ijas_9 9f ON THE EXTENSION OF WEAK AENDAIZ INGS ELATIVE TO A ONOID Eye A & Ayou Eoy Dee of e Nowe No Uvey Lzou 77 C Dee of e Uvey of Kou Ou Su E-: eye76@o; you975@yooo ABSTACT Fo oo we
More informationA parallel index for semistructured data
A pllel index fo emiuued d Bin F. Coope Λ Dep. of Compue Siene Snfod Univeiy Snfod, CA 9435 USA oopeb@nfod.edu Nel Smple y Dep. of Compue Siene Snfod Univeiy Snfod, CA 9435 USA nmple@nfod.edu Mohe Shdmon
More informationPhysics 201, Lecture 5
Phsics 1 Lecue 5 Tod s Topics n Moion in D (Chp 4.1-4.3): n D Kinemicl Quniies (sec. 4.1) n D Kinemics wih Consn Acceleion (sec. 4.) n D Pojecile (Sec 4.3) n Epeced fom Peiew: n Displcemen eloci cceleion
More informationHow dark matter, axion walls, and graviton production lead to observable Entropy generation in the Early Universe. Dr.
How dk me, xion wlls, nd gvion poduion led o obsevble Enopy geneion in he Ely Univese D. Andew Bekwih he D Albembein opeion in n equion of moion fo emegen sl fields implying Non-zeo sl field V && Penose
More information(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.
Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)
More informationGraphical Representation of Fuzzy State Space of a Boiler System
EEN DNES in NEU NEWOKS UZZY SYSES & EOUIONY OPUIN il eeenion o uzzy Se Se o oile Syem NOO INY HISH ZIDH ISI 3 HI HD uly o omue nd emil Siene Unieiy enoloi 445 S lm Selno YSI 3 Demen o emi uly o Siene Unieii
More informationCompressive modulus of adhesive bonded rubber block
Songklnkin J. Sci. Tecnol. 0 (, -5, M. - Ap. 008 p://www.sjs.ps.c. Oiginl Aicle Compessive modls of desive bonded bbe block Coeny Decwykl nd Wiiy Tongng * Depmen of Mecnicl Engineeing, Fcly of Engineeing,
More informationBINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =
wwwskshieduciocom BINOMIAL HEOREM OBJEIVE PROBLEMS he coefficies of, i e esio of k e equl he k /7 If e coefficie of, d ems i e i AP, e e vlue of is he coefficies i e,, 7 ems i e esio of e i AP he 7 7 em
More informationDerivation of the Metal-Semiconductor Junction Current
.4.4. Derivio of e Mel-Seiouor uio Curre.4.4.1.Derivio of e iffuio urre We r fro e epreio for e ol urre e iegre i over e wi of e epleio regio: q( µ + D (.4.11 wi be rewrie b uig -/ uliplig bo ie of e equio
More informationMaximum likelihood estimate of phylogeny. BIOL 495S/ CS 490B/ MATH 490B/ STAT 490B Introduction to Bioinformatics April 24, 2002
Mmm lkelhood eme of phylogey BIO 9S/ S 90B/ MH 90B/ S 90B Iodco o Bofomc pl 00 Ovevew of he pobblc ppoch o phylogey o k ee ccodg o he lkelhood d ee whee d e e of eqece d ee by ee wh leve fo he eqece. he
More informationMaximum Flow. Flow Graph
Mximum Flow Chper 26 Flow Grph A ommon enrio i o ue grph o repreen flow nework nd ue i o nwer queion ou meril flow Flow i he re h meril move hrough he nework Eh direed edge i ondui for he meril wih ome
More informationU>, 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 informationENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]
ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual
More informationOptimization. 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 informationSatellite Orbits. Orbital Mechanics. Circular Satellite Orbits
Obitl Mechnic tellite Obit Let u tt by king the quetion, Wht keep tellite in n obit ound eth?. Why doen t tellite go diectly towd th, nd why doen t it ecpe th? The nwe i tht thee e two min foce tht ct
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationProperties 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 informationChapter Introduction. 2. Linear Combinations [4.1]
Chper 4 Inrouion Thi hper i ou generlizing he onep you lerne in hper o pe oher n hn R Mny opi in hi hper re heoreil n MATLAB will no e le o help you ou You will ee where MATLAB i ueful in hper 4 n how
More informationLECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.
LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle
More informatione t dt e t dt = lim e t dt T (1 e T ) = 1
Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie
More informationAfrican Journal of Science and Technology (AJST) Science and Engineering Series Vol. 4, No. 2, pp GENERALISED DELETION DESIGNS
Af Joul of See Tehology (AJST) See Egeeg See Vol. 4, No.,. 7-79 GENERALISED DELETION DESIGNS Mhel Ku Gh Joh Wylff Ohbo Dee of Mhe, Uvey of Nob, P. O. Bo 3097, Nob, Key ABSTRACT:- I h e yel gle ele fol
More information0 for t < 0 1 for t > 0
8.0 Sep nd del funcions Auhor: Jeremy Orloff The uni Sep Funcion We define he uni sep funcion by u() = 0 for < 0 for > 0 I is clled he uni sep funcion becuse i kes uni sep = 0. I is someimes clled he Heviside
More informationCHAPTER 7 Applications of Integration
CHAPTER 7 Applitions of Integtion Setion 7. Ae of Region Between Two Cuves.......... Setion 7. Volume: The Disk Method................. Setion 7. Volume: The Shell Method................ Setion 7. A Length
More informationAQA Maths M2. Topic Questions from Papers. Circular Motion. Answers
AQA Mths M Topic Questions fom Ppes Cicul Motion Answes PhysicsAndMthsTuto.com PhysicsAndMthsTuto.com Totl 6 () T cos30 = 9.8 Resolving veticlly with two tems Coect eqution 9.8 T = cos30 T =.6 N AG 3 Coect
More informationUser s Guide NBC 2005, Structural Commentaries (Part 4 of Division B)
Ue Guide NBC 2005, Stutual Commentaie (Pat 4 of Diviion B) Eata Iued by the Canadian Commiion on Building and Fie Code The table that follow lit eata that apply to the Ue Guide NBC 2005, Stutual Commentaie
More informationPositive and negative solutions of a boundary value problem for a
Invenion Journl of Reerch Technology in Engineering & Mngemen (IJRTEM) ISSN: 2455-3689 www.ijrem.com Volume 2 Iue 9 ǁ Sepemer 28 ǁ PP 73-83 Poiive nd negive oluion of oundry vlue prolem for frcionl, -difference
More information8.1. a) For step response, M input is u ( t) Taking inverse Laplace transform. as α 0. Ideal response, K c. = Kc Mτ D + For ramp response, 8-1
8. a For ep repone, inpu i u, U Y a U α α Y a α α Taking invere Laplae ranform a α e e / α / α A α 0 a δ 0 e / α a δ deal repone, α d Y i Gi U i δ Hene a α 0 a i For ramp repone, inpu i u, U Soluion anual
More informationdefined on a domain can be expanded into the Taylor series around a point a except a singular point. Also, f( z)
08 Tylo eie nd Mcluin eie A holomophic function f( z) defined on domin cn be expnded into the Tylo eie ound point except ingul point. Alo, f( z) cn be expnded into the Mcluin eie in the open dik with diu
More informationFractional Order Thermoelastic Deflection in a Thin Circular Plate
Aville ://vuedu/ Al Al M ISSN: 93-9466 Vol Iue Decee 7 898-99 Alicion nd Alied Meic: An Inenionl Jounl AAM Fcionl Ode eoelic Deflecion in in Cicul Ple J J ii S D We C Deuk 3 nd J Ve 4 Deen of Meic D Aedk
More informationOn Fractional Operational Calculus pertaining to the product of H- functions
nenonl eh ounl of Enneen n ehnolo RE e-ssn: 2395-56 Volume: 2 ue: 3 une-25 wwwene -SSN: 2395-72 On Fonl Oeonl Clulu enn o he ou of - funon D VBL Chu, C A 2 Demen of hem, Unve of Rhn, u-3255, n E-ml : vl@hooom
More informationDevelopment of a Dynamic Model of a Small High-Speed Autonomous Underwater Vehicle
lp i Ml Sll Hi-Sp Uw Vil Hi N., il J. Silwll Bl p Elil p Eii Viii Pli Ii S Uii Bl, V 1 Eil: {, ilwll }@. P : i p, Wii, KS 777 W L. N p p O Eii Viii Pli Ii S Uii Bl, V 1 Eil: @. i l i lp ll, ip w il. il
More informationFaraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf
Objecie F s w Tnsfome Moionl To be ble o fin nsfome. moionl nsfome n moionl. 331 1 331 Mwell s quion: ic Fiel D: Guss lw :KV : Guss lw H: Ampee s w Poin Fom Inegl Fom D D Q sufce loop H sufce H I enclose
More informationTWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA
WO INERFIL OLLINER GRIFFIH RS IN HERMO- ELSI OMOSIE MEDI h m MISHR S DS * Deme o Mheml See I Ie o eholog BHU V-5 I he oee o he le o he e e o eeg o o olle Gh e he ee o he wo ohoo mel e e e emee el. he olem
More information1 The Network Flow Problem
5-5/65: Deign & Anlyi of Algorihm Ooer 5, 05 Leure #0: Nework Flow I l hnged: Ooer 5, 05 In hee nex wo leure we re going o lk ou n imporn lgorihmi prolem lled he Nework Flow Prolem. Nework flow i imporn
More informationv T Pressure Extra Molecular Stresses Constitutive equations for Stress v t Observation: the stress tensor is symmetric
Momenum Blnce (coninued Momenum Blnce (coninued Now, wh o do wih Π? Pessue is p of i. bck o ou quesion, Now, wh o do wih? Π Pessue is p of i. Thee e ohe, nonisoopic sesses Pessue E Molecul Sesses definiion:
More informationEE 410/510: Electromechanical Systems Chapter 3
EE 4/5: Eleomehnl Syem hpe 3 hpe 3. Inoon o Powe Eleon Moelng n Applon of Op. Amp. Powe Amplfe Powe onvee Powe Amp n Anlog onolle Swhng onvee Boo onvee onvee Flyb n Fow onvee eonn n Swhng onvee 5// All
More informationDamper Tuning with the use of a Seven Post Shaker Rig
SAE TECHNICAL PAPER SERIES 00-0-0804 Dme Tuning wih he ue of Seven Po She Rig Heni Kowlzy ARC Indinoli-Reynd Mooo SAE 00 Wold Conge Deoi, Mihign Mh 4-7, 00 400 Commonwelh Dive, Wendle, PA 5096-000 USA
More informationRole of diagonal tension crack in size effect of shear strength of deep beams
Fu M of Co Co Suu - A Fu M of Co - B. H. O,.( Ko Co Iu, Sou, ISBN 978-89-578-8-8 o of o o k z ff of of p m Y. Tk & T. Smomu Nok Uy of Tooy, N, Jp M. W Uym A Co. L., C, Jp ABSTACT: To fy ff of k popo o
More informationMolecular Evolution and Phylogeny. Based on: Durbin et al Chapter 8
Molecula Evoluion and hylogeny Baed on: Dubin e al Chape 8. hylogeneic Tee umpion banch inenal node leaf Topology T : bifucaing Leave - N Inenal node N+ N- Lengh { i } fo each banch hylogeneic ee Topology
More informationANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 2
ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER Seion Eerise -: Coninuiy of he uiliy funion Le λ ( ) be he monooni uiliy funion defined in he proof of eisene of uiliy funion If his funion is oninuous y hen
More information1. Kinematics of Particles
1. Kinemics o Picles 1.1 Inoducion o Dnmics Dnmics - Kinemics: he sud o he geome o moion; ele displcemen, eloci, cceleion, nd ime, wihou eeence o he cuse o he moion. - Kineics: he sud o he elion eising
More informationTMA4329 Intro til vitensk. beregn. V2017
Norges eknisk naurvienskapelige universie Insiu for Maemaiske Fag TMA439 Inro il viensk. beregn. V7 ving 6 [S]=T. Sauer, Numerical Analsis, Second Inernaional Ediion, Pearson, 4 Teorioppgaver Oppgave 6..3,
More informationFinal Exam. Tuesday, December hours, 30 minutes
an Faniso ae Univesi Mihael Ba ECON 30 Fall 04 Final Exam Tuesda, Deembe 6 hous, 30 minues Name: Insuions. This is losed book, losed noes exam.. No alulaos of an kind ae allowed. 3. how all he alulaions.
More informationPreviously. 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 informationEquations from the Millennium Theory of Inertia and Gravity. Copyright 2004 Joseph A. Rybczyk
Equtions fo the illenniu heoy of Ineti nd vity Copyight 004 Joseph A. Rybzyk ollowing is oplete list of ll of the equtions used o deived in the illenniu heoy of Ineti nd vity. o ese of efeene the equtions
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationAns: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes
omewok # P7-3 ecngul loop of widh w nd heigh h is siued ne ve long wie cing cuen i s in Fig 7- ssume i o e ecngul pulse s shown in Fig 7- Find he induced cuen i in he ecngul loop whose self-inducnce is
More informationGlobal alignment in linear space
Globl linmen in liner spe 1 2 Globl linmen in liner spe Gol: Find n opiml linmen of A[1..n] nd B[1..m] in liner spe, i.e. O(n) Exisin lorihm: Globl linmen wih bkrkin O(nm) ime nd spe, bu he opiml os n
More informationOn the Use of Rigging Angle and Canopy Tilt for Control of a Parafoil and Payload System
Digil Common @ Geoge o Univei ul Puliion - Demen of ehnil nd Civil Engineeing Demen of ehnil nd Civil Engineeing 3 On he Ue of Rigging ngle nd Cno il fo Conol of Pfoil nd Plod em Nhn lege Geoge o Univei,
More information_ J.. C C A 551NED. - n R ' ' t i :. t ; . b c c : : I I .., I AS IEC. r '2 5? 9
C C A 55NED n R 5 0 9 b c c \ { s AS EC 2 5? 9 Con 0 \ 0265 o + s ^! 4 y!! {! w Y n < R > s s = ~ C c [ + * c n j R c C / e A / = + j ) d /! Y 6 ] s v * ^ / ) v } > { ± n S = S w c s y c C { ~! > R = n
More informationElectric 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 informationTwo 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 informationControl Volume Derivation
School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass
More informationAdditional Exercises for Chapter What is the slope-intercept form of the equation of the line given by 3x + 5y + 2 = 0?
ddiional Eercises for Caper 5 bou Lines, Slopes, and Tangen Lines 39. Find an equaion for e line roug e wo poins (, 7) and (5, ). 4. Wa is e slope-inercep form of e equaion of e line given by 3 + 5y +
More informationGeneral 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 informationModule 5: Two Dimensional Problems in Cartesian Coordinate System
Moule : Two Dimenionl Problem in Crein Coorine Sem Moule/Leon.. SOLUTIONS OF TWODIMENSIONAL PROBLEMS BY THE USE OF POLYNOMIALS Te equion given b will be iie b ereing Air uncion (, ) olnomil. () Polnomil
More informationFlow Networks Alon Efrat Slides courtesy of Charles Leiserson with small changes by Carola Wenk. Flow networks. Flow networks CS 445
CS 445 Flow Nework lon Efr Slide corey of Chrle Leieron wih mll chnge by Crol Wenk Flow nework Definiion. flow nework i direced grph G = (V, E) wih wo diingihed erice: orce nd ink. Ech edge (, ) E h nonnegie
More informationNEWBERRY FOREST MGT UNIT Stand Level Information Compartment: 10 Entry Year: 2001
iz oy- kg vg. To. 1 M 6 M 10 11 100 60 oh hwoo uvg N o hul 0 Mix bg. woo, moly low quliy. Coif ompo houghou - WP/hmlok/pu/blm/. vy o whi pi o h ouh fig of. iffiul o. Th o hi i o PVT l wh h g o wll big
More informationû s L u t 0 s a ; i.e., û s 0
Te Hille-Yosida Teorem We ave seen a wen e absrac IVP is uniquely solvable en e soluion operaor defines a semigroup of bounded operaors. We ave no ye discussed e condiions under wic e IVP is uniquely solvable.
More informationImportant 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 informationDetermining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek
Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom
More informationRadial 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 informationComparison between the Discrete and Continuous Time Models
Comparison beween e Discree and Coninuous Time Models D. Sulsky June 21, 2012 1 Discree o Coninuous Recall e discree ime model Î = AIS Ŝ = S Î. Tese equaions ell us ow e populaion canges from one day o
More informationTechnical Vibration - text 2 - forced vibration, rotational vibration
Technicl Viion - e - foced viion, oionl viion 4. oced viion, viion unde he consn eenl foce The viion unde he eenl foce. eenl The quesion is if he eenl foce e is consn o vying. If vying, wh is he foce funcion.
More information