Derivation of Annular Plate Sector Element for General Bending Analysis
|
|
- Bethany Hamilton
- 5 years ago
- Views:
Transcription
1 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 Divtion of Annul Plt Scto Elmnt fo Gnl Bnding Anlysis Lctu D. Hyd Abdulm Mhdi Civil ngining dptmnt, Engining collg, Al_ Mustnsiiyh Univsity Abstct A nw mthmticl finit lmnt modl suitbl fo th gnl bnding nlysis of nnul plt stuctu is dvlopd in pol coodints systm dpnding on th stin bsd ppoch hs bn divd. Th lmnt is simpl nd contins only th ssntil dgs of fdom. Th lmnt hs 5 dgs of fdom, th t ch nod nd stisfis th ct psnttion of th igid body mods of displcmnt. Th sults obtind by using th poposd lmnt in svl numicl poblms hv shown tht pid convgnc to ct solution cn b obtind with ccptbl dg of ccucy whn only fw lmnt usd. Th lmnt hs th dvntg ov th oth vilbl nnul plt lmnts. Th impovmnt obtind is du to th fct tht ll th displcmnt filds of th psnt lmnt stisfy th ct psnttion of igid body mods of displcmnts thn th shp function o du to igid body mods bcoms zo. Also, th psnt lmnt stisfis th full gomty of th nnul plt du to this point disctiztion o bcoms zo. Finlly th o du to stin mod bcoms vy smll bcus th psnt lmnt stisfis th comptibility qutions of stins nd th th cofficints of stin mod divd ctly fom ptil diffntil qutions of stins. Th numicl solution of svl poblms by using th psnt lmnt povd to b powful in th stuctul bnding nlysis of cicul nnul plts. Its sults btt thn th solution of oth lmnts nd pckgs with spct to nlyticl. Kywods: nnul scto plt, Stin bsd ppoch lmnt 4
2 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 الخلاصة: اشتقاق عنصر محدد لتحلیل الانحناء العام للصفاي ح الداي ریة بالا حداثیات القطبیة قسم الھندسة المدنیة م. د. حیدر عبدالا میر مھدي / كلیة الھندسة / الجامعة المستنصریة تم في ھذه الدراسة تطویر عنصر جدید للتحلیل الا نحناي ي للص فاي ح الحلقی ة با س تخدام نظ ام الا ح داثیات القطبی ة یعتمد على طریقة الا نفعال حیث یظم درجات الطلاقة الري یسیة. العنصر یحقق مواصفات الحركة للجسم الصلب بش كل ت ام full gomty of ) كم ا یحق ق كام ل الخ واص للش كل الھندس ي للص فاي ح الحلقی ة (ct igid body mod) comptibility qution ) إضافة إلى ذلك فا ن العنصر یحقق شروط التواف ق لمع ادلات الا نفع ال (nnul plt.(of stin یمتلك ھذا العنصر خمسة عشر درج ة طلاقة حرة fdom) (dg of ثلاث ة ف ي ك ل عق دة ركنی ة وثلاث ة ف ي عق دة الوس ط یعتب ر ھ ذا العنص ر م لاءم للتحلی ل الا نحن اي ي الع ام للص فاي ح الحلقی ة وھ و أفض ل م ن العناص ر الس ابقة لتحلی ل المنشاءات الا نفة الذكر حیث أن الا خطاء التي تظھر في العناصر المحددة السابقة مثل أخط اء التقس یم ) discitiztion (o أخطاء الدوال الشكلیة o) (shp function تختفي في ھذا العنصر نتیج ة للمواص فات الت ي یتمت ع بھ ا. تم استخدام العنصر الحالي في التحلیل العددي لعدد من المساءل المختلفة إذ أنھ ا تب ین وتب رھن أن العنص ر الح الي ممت از وكفو في تحلیل عدة أنواع من التحمیل بش كل أفض ل م ن العناص ر المح ددة لب احثین آخ رین حی ث اظھ رت النت اي ج امكانی ة الاقتراب السریع الى نتاي ج الحل الدقیق solution) (ct وبدرج ة دق ة عالی ة وبا س تخدام ع دد قلی ل م ن العناص ر عن د تمثیل المنشاء. Nottion:, Ɵ Pol coodints D E M, M Ɵ M Ɵ, M Ɵ P q Q Q Ɵ w w w s Bnding igidity. Modulus of lsticity. Th bnding momnts in th dictions of nd Ɵ s, spctivly. Th twisting momnts. Point lod Th unifomly distibutd lod cting on th plt. Th out of pln shing stss sultnt in th -diction of gnl plt thoy Th out of pln shing stss sultnt in th Ɵ-diction of gnl plt thoy Out of pln displcmnt in Z-diction fo ctsin coodint, nd in noml diction fo pol coodints. Th middl sufc noml displcmnts of th nnul plt lmnt du to th igid body pt. Th middl sufc noml displcmnts of th nnul plt lmnt du to th stin pt. 5
3 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 { } is th vcto of constnt tms of th displcmnt function { δ } [A] [B] [D] [f] Th tnsfomtion mti. Th stin mti. Th igidity mti. is th mti contining th coodint vibls [K ] Th stiffnss mti of th finit lmnt. P Th vcto contining th nodl lods cting on th finit lmnt. δ ε σ ϕ ϕ Ɵ Th vcto contining th dgs of fdom of th finit lmnt. Th vcto contining th stin (nd cuvtus) of th finit lmnt. Th vcto contining th stsss in th finit lmnt. Rottion in th -diction of gnl plt thoy Rottion in th Ɵ-diction of gnl plt thoy. Intoduction Fo th gnl bnding nlysis of nnul plts bsd on th clssicl thoy of thin plts. In gnl, th following th numicl mthods hv bn usd fo th nlysis of nnul plts [] :. Th finit diffnc mthod (FDM).. Th finit stip mthod (FSM).. Th finit lmnt mthod (FEM). Th pimntl wok bout this subjct w tmly limitd fo simpl css such s point lods nd simpl suppot []. Th finit lmnt mthod of stuctul nlysis is now fimly stblishd s powful tchniqu fo hndling diffnt poblms in solid mchnics []. Th simplst lmnt shps fo nnul plt poblms obviously tingl lmnt with th nods s in wok of Chung t l [4], nd ctngul lmnt with fou nods s in th wok of Ro [5]. Olson nd Lindbg [], dvlopd n nnul sgmnt plt bnding lmnt with fou con nods ch hving th tnl nodl dgs of fdom. Howv, using ths lmnts fo cuvd boundy poblms mns, tht th cuvd boundy is bing ppoimtd by sis of stight lin sgmnts. Hnc, th pps to nd to dvlop nw lmnt by using th pol coodints systm to gt btt psnttion of th cuvd boundis. Th psnt lmnt hv n dvntgous ov th vilbl nnul plt lmnts. Th finl poptis of th psnt lmnt s follows: Th lmnt stisfis th full gomty of nnul plt sgmnt, nd du to this point th discitiztion os tht pp in th cuvd boundy bcoms zo. Th lmnt stisfis th ct igid body mods of nnul plt sgmnt, nd du to this point th shp function o of igid body mod pt bcoms zo. 6
4 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 Th stin mod of lmnt is obtind fom intgting of ssumd stin functions stisfying th comptibility qution of nnul plt sgmnt; du to this point th shp function o of stin mod pt bcoms vy smll. Th plicit intgtion is usd to div this lmnt; du to this point th o in numicl intgtion bcoms zo. Accoding to th cntl nod of lmnt th l vlu of stsss in th cnt of lmnt found, not ppoimt stsss du to th mn of fou con nods s in th oth vilbl nnul plt lmnts.. Divtion of Annul Plt Elmnt Using Stin Bsd Appoch. Thoticl Considtion Figu () shows n nnul plt scto. To idliz this nnul plt scto, n lmnt is chosn s shown in Figu (). Fo th gnl bnding nlysis of nnul plt scto und bity loding, th stins (dict stins nd chngs in cuvtu) of th middl sufc divd fom svl thois of nnul plt scto [] : Th ltl dflction (w) is function of () nd (Ө), thn th lplcin opto bcoms [] : w w w w. () Thn th dflction sufc of ltlly lodd plt tnsfoms is bcoms: w w w w q D.....() Du to lod is symmticlly distibutd with spct to th cnt of th plt, th ltl dflction (w) is indpndnt of () nd th bov qution bcoms [] : w w w q D. () Wh q is th pplid lod nd it is givn s function of () nd (), D is th flul igidity, nd quls Et D ( ν ) 7
5 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 Th out of pln componnts of th stins cuvtus follows: w χ. (4) w w χ.... (4b) w χ w... (4c) wh: () is th dil coodint msud fom th p of th nnul plt scto, nd ( ) is th ngul coodint msud ound th cicumfnc. Th qution of dil, ngul nd twisting momnts, M, M Ѳ, nd M Ѳ spctivly bcoms: { } M D χ υχ.. (5) { υχ } M D χ... (5b) M ( ν ) D{ χ }... (5c) nd th vticl shing focs Q, nd Q Ѳ spctivly bcoms: Q D [ w]... (6) Q D [ w]... (6b) Th bov th componnts of stins cnnot b considd indpndnt s thy in tms of th ltl displcmnt (w) nd hnc, th stins must stisfy dditionl qutions clld th comptibility qutions. Ths qutions obtind by liminting th ltl displcmnt (w) fom qutions (4). Th finl sults of comptibility qutions s follows: ( χ ) χ 0. (7) ( χ ) ( χ ) χ 0.. (7b) 8
6 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Displcmnt Functions: Th poposd lmnt is llowd to hv only th ssntil tnl dgs of fdom (w, φ, nd φ ) t ch nod. Pocding s with th usul stin-bsd ppoch, th fist mjo componnt of th displcmnt function is du to (stin-f) igid body mods of displcmnt nd cn b obtind by quting ll th componnts of stins [8], qutions (4), to zo nd intgting th sulting ptil diffntil qutions bcoms: w R cos sin... (8) In this qution w R th igid body componnt of th displcmnt fild w, nd is pssd in tms of th th indpndnt constnts (, ),. Th scond mjo componnt of th displcmnt function is du to stining of th lmnt. If th lmnt is to hv fiftn dgs of fdom (th t ch nod) thn th stins of th lmnt must b ssocitd with twlv dditionl constnts ( 4,, 5 ) of ( ) constnts Assuming stin polynomil functions χ w A 4 A5 A6 A7 A8... (9) χ w w A 9 A0 A A A... (9b) w w 4 A A... (9c) χ 5 Chcking th bov polynomils of stin fo comptibility qutions of nnul plt scto (7, nd 7b). Finlly, th ssumd stin functions of nnul plt scto lmnt which stisfy th quimnt of comptibility qutions th sm of qutions 9, nd 9b cpt qution 9c bcom: χ S 9 4 A A ( A A ) ( A A ) ( A A ) ( A A ) (0) Th bov th qutions 9, 9b, nd 0 intgtd in th sm pocdu tht ws usd to div th igid body mods of nnul plt scto lmnt, thn th finl polynomil function of stin mod bcoms: w S () 9
7 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Th complt displcmnt fild functions fo th poposd lmnt is bcoms. w w w s sin cos w... () Th ottion φ, nd φ lso givn blow: sin cos φ w... () cos sin φ w... (4). Th Elmnt Stiffnss Mti Figu () shows tht th oigin of th dil coodint of th lmnt () is loctd t th p of th nnul plt scto. Consquntly, th oigin of th ngul coodint () is loctd t th cnt of th lmnt. Sinc, th clcultion of th stiffnss mti is cid out plicitly; this choic of th oigin will simplify th tsk of intgtion, thus: [ ] [ ] ] [ ] ][ [ ] [ A B dd D B A k T T β β... (5) wh [A], [B] nd [D] th tnsfomtion, stin nd igidity mtics of th lmnt, spctivly. Th (5X5) lmnt stiffnss mti [k ], cn now b clcultd using th displcmnt functions () nd th stin displcmnt ltionships (4). On th oth hnd, to kp th stog mmoy smll th stiffnss mti is condnstd fom (55) to () by moving th influnc of th cntl point (nod 5) to th fou con points (nods,,, nd 4) s follows: [ ]{ } { } n n n P K δ... (6) wh: [ ] [ ] [ ][ ] [ ] n K K K K K { } { } n δ δ { } { } [ ][ ] { } ( ) n P K K P P
8 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Consistnt Lod Vcto Th tnl pplid nodl lods considd in th psnt finit lmnt nlysis clcultd by using consistnt lod vcto. Th consistnt lod vcto is obtind by quting th wok don by th nodl lods on th nodl displcmnts to th wok don by th tnl pplid lod on th ssumd displcmnt function of th lmnt. Th nnul plt lmnt shown in Figu () is considd. If th lmnt is subjctd to svl loding typs such s, distibutd noml pssu (q), concnttd lod (P i ), unifom distibutd momnt (M), nd concnttd momnt (M i ) th lod vcto bcoms [] : β β q { P 5} [ A] [ f ] dd [ A] [ f ] β m β t nod ( i) Pi dd Mi... (7) Fo th lmnt stiffnss mti ft condnstion, th lod vcto is tkn s follows: ( ) n { P } { P } [ K 5][ K ] { P }... (8) φ 4 φ 4 R Z φ w 4 φ 5 φ w5 φ 5 φ β β w w φ φ φ w Y Fig.() An nnul sgmnt lmnt with th coodints systm fo plt bnding poblms.
9 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 M4 φ 4 w4 φ 4 M 4 R Z β β w φ M M φ w5 φ M 5 φ M φ 5 φ 5 M5 w φ M M φ w M Y Fig.() Displcmnt nd thi cosponding focs fo nnul plt lmnt.. An nnul plt und point lod Th poblm considd is tht of n nnul plt dfoming unsymmticlly s shown in Figu (). Th plt is clmpd long th inn dg ( b), nd lodd by concnttd lod t th out dg ( ). An ct solution fo this poblm is givn in Timoshnko nd Woinowsky-Kig [6] fo b/ /.5 nd μ0.. Olson nd Lindbg [], Tuki [7] nd Alkhfji nd Mhdi [8] psntd n nnul finit lmnt, to nlyz this poblm. Symmty bout th dimt contining th lod ws usd, so tht, only on hlf of th plt ws to b modld. Th sults fo th ltl displcmnt (w) und th lod fo diffnt msh sizs givn in Tbl (). Whn this poblm is nlyzd with (54) msh using both lmnts, th o is bout 0.45% fo Olson nd Lindbg [], Tuki [7], nd 0.% fo Al-khfji nd Mhdi [8], but th o is bout 0.% fo th psnt lmnt nd with (84) gid fo both lmnts th o is bout 0.7% fo Olson nd Lindbg [], Tuki [7], nd 0.089% fo Alkhfji nd Mhdi [8], but th o is bout 0.06% fo th psnt lmnt. It is cl in Figu () tht th ltl dflctions long th inn dg convg pidly to th ct solution whn th msh siz is find. Olson nd Lindbg [] confind th sults in thi publishd wok to dflctions only (no sults w givn fo th momnts). Figu () shows th distibution of dil bnding momnt in non-dimnsionl fom of (M /P) long th inn dg fo (4) msh. It is
10 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 vidnt fom this figu tht th poposd lmnt givs stisfctoy sults fo momnts whn compd with th ct solution givn by Timoshnko nd Woinowsky-Kig [6]. Tbl () shows th convgnc o of fou lmnts, th sult pps tht convgnc of th psnt lmnt is stbl s whn lmnt msh is incsing th o of solution is dcsing continuously, but in th oth lmnts th convgnc of solution is unstbl with incsing msh siz s pping in Tbl (). In gnl, th two typs of convgnc shown in Figu (4). Th son of two typs of os concludd by th igid body mod nd stin mod os, th psnt lmnt stisfis th igid body nd stin mods s this lmnt s sult is stbl, th o is dcsing whn msh siz is incsing, but oth lmnts do not stisfy th bov conditions. Tbl.() Convgnc of th ltl dflction und th pplid point lod Msh siz Olson s nd Lindbg Elmnt Dflction * P/D Tuki s Elmnt Mhdi's Elmnt Psnt Elmnt Ect (Timoshnko nd Woinowsky-Kig 98) Tbl.() Convgnc o of svl mshs of th ltl dflction und th pplid point lod. Msh siz Dflction * P/D Olson s Elmnt Tuki s Elmnt Mhdi's Elmnt Psnt Elmnt 6 0.5% 0.0%.900% 0.% 8.0%.0%.500% 0.95% 0.6% 0.6%.060% 0.5% 44 0.% 0.% 0.40% 0.4% % 0.45% 0.00% 0.% % 0.57% 0.00% % % 0.66% 0.089% 0.06% 4 0.6% 0.54% 0.048% %
11 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 C.L Msh (4) Ect Solution of (Ms) F.E.S. Solution of (Ms) b Unit Point Lod t 8.05 mm b mm t 7.6 mm µ 0. E 7.89Gp Rdil Momnt Rdil momnt (M) Angls (dgs) Fig.() An nnul plt und point lod in poblm. Fig.(4) Distibution of dil bnding momnt (Ms) long th inn dg in poblm. () Al-khfji nd Mhdi, nd Psnt lmnt bhvio. (b) Olson s nd Lindbg lmnt nd Tuki s lmnt bhvio. Fig.(5) Gnl typs of convgnc os of finit lmnt solution. 4. An nnul plt und unifomly distibutd lod As n isymmtic poblm, cicul plt with cntl cicul hol is nlyzd. Fou css considd s shown in Figu (6), nd in ch cs, on lmnt in th ngul diction is usd with n includd ngl of 4.5 o. Insting zo vlu th noml 4
12 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 ottion φ t ll nods long both th dil dgs, thus stisfying th cicul symmty cition. Tbl () shows th mimum dflctions nd momnts which, obtind by using th poposd lmnt togth with thos obtind by th ct solution givn by Timoshnko nd Woinowsky-Kig (6) nd Swko,s lmnt [9]. Tbl (4) shows th convgnc of mimum dflctions nd momnts. Rfing to this tbl, it is concludd tht th diffnc in th sults is vy smll nd in most css tnds to b stbl, spcilly, fo dflctions. Gnlly, stisfctoy sults cn b obtind with lss thn 0.% diffnc by using 4 dgs of fdom fo dflctions nd 60 dgs of fdom fo momnts, in ll considd css. Th ccucy of this ppoimtion is illusttd in Figus (7) fo vious loding nd boundy conditions. This tbl lso shows th convgnc of th mimum dflction fo ll considd css. Cs q d Cs q Cs q 406.6mm b0.mm 4.5 dg µ0. t7.6mm E7.89 Gp Cs 4 q b Fig.(6) Unifomly distibutd lod nnul plts scto. 5
13 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 Tbl.() Mimum dflctions of poblm in Figu (6) Cs No. W m *q 4 /D*0 - Ect Swko's Elmnt Tuki s Elmnt Psnt Elmnt Cs Cs Cs Cs Tbl.(4) Mimum momnts of poblm in Figu (6) Cs No. M m *q /D*0 - Ect Swko's Elmnt Tuki s Elmnt Psnt Elmnt Cs Cs Cs Cs Fig.(7) Msh study fo convgnc of fou css poblm in Figu (6) to ct solution fo (W m *q 4 /D*0 - ) 6
14 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Unifomly lodd nnul plt scto with ll dgs clmpd. Th finl poblm considd is tht of unifomly lodd nnul plt scto with ll dgs clmpd. Th sktch of this nnul plt nd its poptis givn in th following figu. This poblm ws fist nlysd by Chung nd Chn [0], using th finit stip mthod. Hik [] dvlopd n nlyticl solution to psnt this poblm. Th mimum dflction nd th mimum positiv momnts (dil nd ngul momnts) long th cntl dil lin clcultd by th poposd lmnt fo (9*9) msh, nd fo diffnt vlus of th (b/) tio. Th sults givn in Tbls (5, B, And C), togth with thos of th oth mthods. Convgnc tsts w cid out using th poposd lmnt fo th dflctions nd momnts whn th nnul plt is dividd into mshs nging fom (44) to (66). Tbl (6) shows th convgnc of mimum dflctions nd mimum positiv momnts long th cntl dil lin nd whn th (b/) tio quls (0.75). Clmpd dgs d d8.6 mm 60 υ0. t7.6 mm E68.95Gp. b Fig.(8) Unifomly lodd nnul plt scto with ll dg clmpd nd its poptis. 7
15 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN 8-78 b/ Tbl.(5) Mimum dflctions of poblm in Figu (8) W m *q 4 /D*0-4 Chung nd Chn (9) Hik () Psnt Elmnt Tbl.(5b) Mimum momnts of poblm in Figu (8) b/ M m *q /D*0 - Chung nd Chn (9) Hik () Psnt Elmnt Tbl.(5c) Mimum momnts of poblm in Figu (8) b/ Mq m *q /D*0 - Chung nd Chn (9) Hik () Psnt Elmnt Tbl.(6) Convgnc of th mimum dflctions nd positiv momnts long th cntl dil lin in poblm in Figu (8) fo b/ msh W m *q 4 /D*0-4 M m *q /D*0 - Mq m *q /D*
16 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Conclusion: Annul plt finit lmnt suitbl fo th gnl bnding nlysis of nnul plt scto hs bn dvlopd. Th lmnt is simpl nd contins only th ssntil dgs of fdom. Th lmnt hs th dvntg ov th oth vilbl nnul plt lmnt. Th impovmnt obtind is du to th fct tht ll th displcmnt filds of th psnt lmnt stisfy th ct psnttion of igid body mods of displcmnts. Also, th displcmnt filds du to stining of th lmnt bsd on indpndnt stins nd stisfy th ct comptibility qutions of stin mods. Th psnt lmnt is usd to nlyz svl typs of poblm. Th numicl sults of th psnt lmnt compd with th nlyticl, nd numicl sults of oth schs. Th sults of th psnt lmnt showd good nd pid convgnc of displcmnts nd stsss with th us fw lmnts. Th os of output sults is lss thn 0.5% of msh siz (6) nd lss thn 0.0% of msh siz (84) fo sttic nlysis of plt poblms. 7. Rfncs. Hik, I. E. "Anlyticl solution to othotopic sctos", J. Eng. Mch., ASCE, Vol. 0, No. 4, Apil 984, pp Coull, A. nd Ds, P. C., "Anlysis of cuvd bidg dsks", Poc. Inst. Civ. Eng., Vol. 7, My, 967, pp Olson, M. D. nd Lindbg, G. M., Annul nd cicul scto finit lmnt of bnding nlysis, Int. J. Mch. Sci., Vol., 970, pp Chung, Y. K., King, I. P., nd Zinkiwiz, O. C, "Slb Bidgs with bity shp nd suppot conditions: A gnl mthod of nlysis bsd on finit lmnts" Poc. Inst. Civ. Engs., Vol. 40, My, 968., pp Ro, S. S., "Th finit lmnt mthod in ngining", nd Ed., Pgmn Pss, Timoshnko, S. P. nd Kig, S. W., Thoy of plts nd shlls, copyight, 98, intntionl dition McGw-Hill book co, Nw Yok. 7. Tuki B., A finit lmnt modl fo bnding nlysis of othogonlly stiffnd nnul plt sctos, MSc. Thsis submittd to Dptmnt of Civil Engining, Collg of Engining, Al-Mustnsiiyh Univsity Al-Khfji, J. M., nd Mhdi, H. A., " Stin Bsd Finit Elmnt Modl fo Conicl Shlls", Intntionl jounl fo ngining nd tchnology, Indi, 0, pp Swko, F., nd Mimn, P. A., "An nnul sgmnt finit lmnt fo plt bnding", Int. J. Num. Mth. In Eng., Vol., 97, pp
17 Jounl of Engining nd Dvlopmnt, Vol. 9, No., Jnuy 05, ISSN Chung, M. S., nd Chn, M. Y. T., "Sttic nd dynmic nlysis of thin nd thick stuctul plts by th finit stip mthod", Comp. nd Stuc., Vol. 4, No., 988, pp El_Eis, H. F., Finit lmnt nlysis of shll stuctus, Ph.D Thsis, 989, submittd to Cdiff Univsity, U. K.. Szild, R., "Thoy nd nlysis of plt", Pintic-Hll, Inc. Englwood Cliffc, N. J., Zinkiwics, O. C., nd Tylo, R. L., "Finit lmnt mthod fo solid nd stuctul mchnics", Sith dition, 005, Elsvi Inc, Ofod, London, U.K. 0
E. Computation of Permanent Magnetic Fields
E. Computtion of Pmnnt Mgntic Filds Th following pssgs should giv n impssion, how pmnnt mgnts cn b clcultd in spct of thi fild distibution. This ovviw ctinl cnnot cov ll subjcts. It will ml intoduc th
More informationTheory of Spatial Problems
Chpt 7 ho of Sptil Polms 7. Diffntil tions of iliim (-D) Z Y X Inol si nknon stss componnts:. 7- 7. Stt of Stss t Point t n sfc ith otd noml N th sfc componnts ltd to (dtmind ) th 6 stss componnts X N
More informationC-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)
An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...
More informationPAVEMENT DESIGN AND EVALUATION
THE REQUIRED MATHEMATICS AND ITS APPLICATIONS F. Vn Cuwlt Edito: Mc Stt Fdtion of th Blgin Cmnt Industy B-7 Bussls, Ru Volt 9. i ii INTRODUCTION Pvmnt Dsign nd Evlution: Th Rquid Mthmtics nd Its Applictions
More informationPath (space curve) Osculating plane
Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions
More informationELEC 351 Notes Set #18
Assignmnt #8 Poblm 9. Poblm 9.7 Poblm 9. Poblm 9.3 Poblm 9.4 LC 35 Nots St #8 Antnns gin nd fficincy Antnns dipol ntnn Hlf wv dipol Fiis tnsmission qution Fiis tnsmission qution Do this ssignmnt by Novmb
More informationCIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7
CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr
More informationInternational Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN
Intntinl Junl f Scintific & Engining Rsch, Vlum, Issu 9, Sptmb- bstct: Jcbin intgl nd Stbility f th quilibium psitin f th cnt f mss f n xtnsibl cbl cnnctd stllits systm in th lliptic bit. Vijy Kum ssistnt
More information40th AIAA Aerospace Sciences Meeting and Exhibit January 14 17, 2002/Reno, NV
AIAA 2002 0788 Rsistnc Appoc fo Annul Fins wit Contct Conductnc nd End Cooling Susnt K. Mit nd M. Micl Yovnovic Dptmnt of Mcnicl Engining, Univsity of Wtloo, Wtloo, Cnd, N2 3G 40t AIAA Aospc Scincs Mting
More informationدراسة عددیة لاستقراریة سدود الانضاب الخلویة باستخدام برنامج ANSYS
FINITE ELEMENT ANALYSIS OF CELLULAR CIRCLE COFFERDAM FOR WET SOIL Assist.Prof. Dr. Kareem R. Al-Murshidi Civil engineering department University of Kufa, Iraq Kareem_radhi@yahoo.com Assist. Prof. Kadhim
More informationE F. and H v. or A r and F r are dual of each other.
A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π
More informationTHE CARTAN GEOMETRY OF THE PLANE POLAR COORDINATES: ROTATIONAL DYNAMICS IN TERMS OF THE CARTAN SPIN CONNECTION
Jounl of Foundtions of Physics nd Chmisty 3 HE CARAN GEOMERY OF HE PLANE POLAR COORDINAES: ROAIONAL DYNAMICS IN ERMS OF HE CARAN SPIN CONNECION M. W. Evns nd H. Eck Alph Institut fo Advncd Studis (www.wbchiv.og.uk,
More information8 - GRAVITATION Page 1
8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving
More informationElastic Analysis of Pavement Structure with Application of Vertical and Centripetal Surface Forces
Elstic nlysis of Pvmnt Stct with ppliction of Vticl nd ntiptl Sfc Focs Min. W. SIR ilt Envionmnt Ptoi Soth fic Fjinmi K. & Mtsi K. ptmnt of ivil nd Envionmntl Engining Tokyo nki Univsity Sitm pn Tkmi Ino
More informationInstructions for Section 1
Instructions for Sction 1 Choos th rspons tht is corrct for th qustion. A corrct nswr scors 1, n incorrct nswr scors 0. Mrks will not b dductd for incorrct nswrs. You should ttmpt vry qustion. No mrks
More informationStudy Material with Classroom Practice solutions. To Electromagnetic Theory CONTENTS. 01 Static Fields Maxwell Equations & EM Waves 06 11
Pg No. Stud Mtil with lssoom Pctic solutions To lctomgntic Tho ONTNTS hpt No. Nm of th hpt Pg No. Sttic Filds 5 Mwll qutions & M Wvs 6 Tnsmission ins Wvguids 5 6 5 lmnts of ntnns 7 hpt. ns: V cos cos î
More informationPhysics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM
Physics 0, Lctu 5 Today s Topics nnouncmnts: Homwok #3 on Wbssign by tonight Du (with Homwok #) on 9/4, 10 PM Rviw: (Ch. 5Pat I) Elctic Potntial Engy, Elctic Potntial Elctic Potntial (Ch. 5Pat II) Elctic
More informationPart II, Measures Other Than Conversion I. Apr/ Spring 1
Pt II, Msus Oth hn onvsion I p/7 11 Sping 1 Pt II, Msus Oth hn onvsion II p/7 11 Sping . pplictions/exmpls of th RE lgoithm I Gs Phs Elmnty Rction dditionl Infomtion Only fd P = 8. tm = 5 K =. mol/dm 3
More informationA Study of Generalized Thermoelastic Interaction in an Infinite Fibre-Reinforced Anisotropic Plate Containing a Circular Hole
Vol. 9 0 ACTA PHYSICA POLONICA A No. 6 A Study of Gnalizd Thmolastic Intaction in an Infinit Fib-Rinfocd Anisotopic Plat Containing a Cicula Hol Ibahim A. Abbas a,b, and Abo-l-nou N. Abd-alla a,b a Dpatmnt
More informationLecture 35. Diffraction and Aperture Antennas
ctu 35 Dictin nd ptu ntnns In this lctu u will ln: Dictin f lctmgntic ditin Gin nd ditin pttn f ptu ntnns C 303 Fll 005 Fhn Rn Cnll Univsit Dictin nd ptu ntnns ptu ntnn usull fs t (mtllic) sht with hl
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationMechanism Analysis of Dynamic Compaction based on Large Deformation
Th Opn Civil Engining Jounal,,, - Opn Accss Mchanism Analysis of Dynamic Compaction basd on Lag Dfomation Xi Nnggang *, Chn Yun, Y Y and Wang Lu Anhui Univsity of Tchnology, Maanshan, Anhui Povinc, China,
More information1 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 informationGAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL
GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL Ioannis Iaklis Haanas * and Michal Hany# * Dpatmnt of Physics and Astonomy, Yok Univsity 34 A Pti Scinc Building Noth Yok, Ontaio, M3J-P3,
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 informationEstimating effective damping introduced by a Pendulum Tuned Mass Damper using the Extended Kalman Filter
Pocdings of th 9th Intntionl Confnc on Stuctul Dynmics, EURODYN 4 Poto, Potugl, 3 Jun - July 4 A. Cunh, E. Ctno, P. Ribio, G. Müll (ds. ISSN: 3-9; ISBN: 978-97-75-65-4 Estimting ffctiv dmping intoducd
More informationHydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals
Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas
More informationCurrent Status of Orbit Determination methods in PMO
unt ttus of Obit Dtintion thods in PMO Dong Wi, hngyin ZHO, Xin Wng Pu Mountin Obsvtoy, HINEE DEMY OF IENE bstct tit obit dtintion OD thods hv vovd ot ov th st 5 ys in Pu Mountin Obsvtoy. This tic ovids
More informationCONTINUITY AND DIFFERENTIABILITY
MCD CONTINUITY AND DIFFERENTIABILITY NCERT Solvd mpls upto th sction 5 (Introduction) nd 5 (Continuity) : Empl : Chck th continuity of th function f givn by f() = + t = Empl : Emin whthr th function f
More informationCHAPTER TWO MULTIPLE INTEGRAL
CHAPTE TWO MULTIPLE INTEGAL Aft complting ths tutoils, stunts shoul b bl to: vlut th oubl intgl ov th givn ctngul gion fin th volum of th soli boun b th plns fin th of th gion boun b th cuvs ug oubl intgl
More informationSolid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch
Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag
More informationMiscellaneous open problems in the Regular Boundary Collocation approach
Miscllnous opn problms in th Rgulr Boundry Colloction pproch A. P. Zilińsi Crcow Univrsity of chnology Institut of Mchin Dsign pz@mch.p.du.pl rfftz / MFS Confrnc ohsiung iwn 5-8 Mrch 0 Bsic formultions
More informationGRAVITATION 4) R. max. 2 ..(1) ...(2)
GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body
More informationPH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.
PH67 WINTER 5 Poblm St # Mad, hapt, poblm # 6 Hint: Th tight-binding band function fo an fcc cstal is ( U t cos( a / cos( a / cos( a / cos( a / cos( a / cos( a / ε [ ] (a Th tight-binding Hamiltonian (85
More informationCONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections
Conic Sctions 16 MODULE-IV Co-ordint CONIC SECTIONS Whil cutting crrot ou might hv noticd diffrnt shps shown th dgs of th cut. Anlticll ou m cut it in thr diffrnt ws, nml (i) (ii) (iii) Cut is prlll to
More information, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x,
Clculus for Businss nd Socil Scincs - Prof D Yun Finl Em Rviw vrsion 5/9/7 Chck wbsit for ny postd typos nd updts Pls rport ny typos This rviw sht contins summris of nw topics only (This rviw sht dos hv
More informationInvestigation into Deformation Monitoring of Mosul Dam
Dr. Rasheed Saleem Abed Remote Sensing Center, University of Mosul/Mosul Email: rasheed@uomosul.edu.iq Received on: 10/2/2013 & Accepted on: 5/12/2013 ABSTRACT It is crucial to monitor the deformation
More informationME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören
ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(
More informationIFYFM002 Further Maths Appendix C Formula Booklet
Ittol Foudto Y (IFY) IFYFM00 Futh Mths Appd C Fomul Booklt Rltd Documts: IFY Futh Mthmtcs Syllbus 07/8 Cotts Mthmtcs Fomul L Equtos d Mtcs... Qudtc Equtos d Rmd Thom... Boml Epsos, Squcs d Ss... Idcs,
More informationUnsteady Casson Fluid Flow through Parallel Plates with Hall Current, Joule Heating and Viscous Dissipation
AMSE JOURNALS 015-Sis: Modlling B; Vol. 84; N 1; pp 1- Submittd Aug. 014; Rvisd Fb. 015; Aptd Fb. 8 015 Unstdy Csson Fluid Flow though Plll Plts with Hll Cunt Joul Hting nd Visous issiption *Md. Fisl Kbi
More informationGRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6
GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is
More informationbe two non-empty sets. Then S is called a semigroup if it satisfies the conditions
UZZY SOT GMM EGU SEMIGOUPS V. Chinndi* & K. lmozhi** * ssocit Pofsso Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd ** Dtmnt of Mthmtics nnmli Univsity nnmling Tmilnd bstct: In this w hv discssd bot th
More informationLoss factor for a clamped edge circular plate subjected to an eccentric loading
ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut
More informationTheoretical Study on the While Drilling Electromagnetic Signal Transmission of Horizontal Well
7 nd ntrntionl Confrnc on Softwr, Multimdi nd Communiction Enginring (SMCE 7) SBN: 978--6595-458-5 Thorticl Study on th Whil Drilling Elctromgntic Signl Trnsmission of Horizontl Wll Y-huo FAN,,*, Zi-ping
More information4.2 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 informationChapter 7 Electrodynamics
Cpt 7 Elctonics 7. Elctootiv Foc 7.. O s Lw Cunt Dnsity: ( n ) q ( n l) Q q qnv Fo lcton: n( )v nd d qnv Fo ost sustncs, t cunt dnsity is popotionl to t foc p unit cg: F ( E + v B) q. : conductivity, pfct
More informationBehavior of Steel Plate Girders with Web Openings Loaded in Shear
Openings Loaded in Shear Dr. May J. Hamoodi Building and Construction Engineering Department, University of Technology/Baghdad Marwa S. Abdul Gabar Building and Construction Engineering Department, University
More informationNew Advanced Higher Mathematics: Formulae
Advcd High Mthmtics Nw Advcd High Mthmtics: Fomul G (G): Fomul you must mmois i od to pss Advcd High mths s thy ot o th fomul sht. Am (A): Ths fomul giv o th fomul sht. ut it will still usful fo you to
More informationChapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures
Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.
More informationStudy on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model
Jounal of Emging Tnds in Economics and Managmnt Scincs (JETEMS 3 (1: 116-1 Scholalink sach Institut Jounals, 1 (ISS: 141-74 Jounal jtms.scholalinksach.og of Emging Tnds Economics and Managmnt Scincs (JETEMS
More informationSTATISTICAL MECHANICS OF DIATOMIC GASES
Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific
More informationThe polarization property of nanotubes with taking into account
Th poliztion popty of nnotubs with ting into ccount th dil otion of vlnc lctons V.A. Alsndov A.V. Stpnov b nd G.M. ilippov b Chuvsh Stt Univsity Russi Chuvsh Rpublic ChbosyMosovsiy pospct 5 b Chbosy Politchnic
More informationSUPPLEMENTARY INFORMATION
SUPPLMNTARY INFORMATION. Dtmin th gat inducd bgap cai concntation. Th fild inducd bgap cai concntation in bilay gaphn a indpndntly vaid by contolling th both th top bottom displacmnt lctical filds D t
More informationChapter 4 Circular and Curvilinear Motions
Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion
More information۲۷۹۶ 0 "' ی " #! ۴۳ و م د ; < : ی"98! ی"#"!
*+, " ان ی" ت/ ر ل. د& ر/ ی/ ر 3 ی" ی" ق: یb نi ی: ی: ی: ره 0 ی/? ی 3 ۲۷۹۶ +* - د' #"! 6 آ (۱)4, 3 2 ا. -, & + ک& ) & ( % $ # ی ا 6 آ 4, / ) $ 2 & ) ر د آ ر د $ 2 ر د : 9-8 د > E < D 2 ا C د: B? > = A
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
More informationEE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.
Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading:
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS
VSRT MEMO #05 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 Fbrury 3, 009 Tlphon: 781-981-507 Fx: 781-981-0590 To: VSRT Group From: Aln E.E. Rogrs Subjct: Simplifid
More informationOPTIMAL SHIFTING OF EIGENVALUES FOR LOAD FREQUENCY CONTROL SYSTEMS
857 OPTIMAL SHIFTING OF EIGENVALUES FOR LOAD FREQUENCY CONTROL SYSTEMS Corresponding author E-mail address: drali_yousef@yahoocom Ali M Yousef Department of Electrical Eng, Faculty of Engineering, Assiut
More informationThe Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton
Journl of Modrn hysics, 014, 5, 154-157 ublishd Onlin August 014 in SciRs. htt://www.scir.org/journl/jm htt://dx.doi.org/.436/jm.014.51415 Th Angulr Momnt Diol Momnts nd Gyromgntic Rtios of th Elctron
More informationDeformation Characteristics of Base and Subbase Layers under Monotonic & Cyclic Loading
Eng. &Tech. Journal, Vol.31, Part (A), No.16, 2013 Deformation Characteristics of Base and Subbase Layers under Monotonic Omar Abbas AL-Azzawi Building & Construction Engineering Department, University
More informationPEP 332: Mathematical Methods for Physicists. Math Methods (Hassani 2009) Ch 15 Applied Vector Analysis. (1) E = ρ ϵ 0 ; (2) B =0; (3) E = B (1) ; (2)
PEP 33: Mmticl Mthods fo Phsicts Mth Mthods (Hsni 9 Ch 5 pplid c nls doul dl options mgntic multipols plcin s ( E d Q ϵ ; ( d ; (3 C E d dφ m dt ; (4 C d µ I ( E ρ ϵ ; ( ; (3 E ; (4 µ J µ ϵ E Φ( (53 ov
More informationNoon Sakinah and Tanween. Chapter 5
Noon Sakinah and Tanween Chapter 5 Outline Definition of Noon Sakinah Definition of Tanween Al Idhar Al Idgham Al Qalb Al Ikhfa Definition of Noon Sakinah The ن does not have one of the three diacritical
More informationOn Calculation of Lattice Energy in Spatially Confined Domains
Advncs in Mtis Scinc nd Appictions Dc., Vo. Iss. 4,. 7-7 On Ccution of Lttic Engy in Sptiy Confind Domins Yvgn Biotsky Dptmnt of Mti Scinc nd Engining, Ato nivsity Foundtion Schoo of Chmic Tchnoogy,.O.
More informationANALYSIS OF DYNAMIC CHARACTERISTICS OF FLEXIBLE ROBOT ARM USING SYMBOLIC MANIPULATION
Al-Qadisiya Journal For Engineering Sciences Vol. No. ٢ Year 009 ANALYSIS OF DYNAMIC CHARACERISICS OF FLEXIBLE ROBO ARM USING SYMBOLIC MANIPULAION Mustafa. Hussein Department of mechanical Engineering
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 informationNew Correlation To Calculate Absolute Permeability From Gas Permeameter
Number 6 Volume 18 June 2012 Journal of Engineering New Correlation To Calculate Absolute Permeability From Gas Permeameter Ass. Lecture Dhorgham S. Ibrahim Ass. Lecture Hussein H. Hussein University of
More informationGeometrical Analysis of the Worm-Spiral Wheel Frontal Gear
Gomtical Analysis of th Wom-Spial Whl Fontal Ga SOFIA TOTOLICI, ICOLAE OACEA, VIRGIL TEODOR, GABRIEL FRUMUSAU Manufactuing Scinc and Engining Dpatmnt, Dunaa d Jos Univsity of Galati, Domnasca st., 8000,
More informationData Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.
Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i
More informationDaham: Analytical Study of Reinforced Concrete Two Way Slabs With and Without
ANALYTICAL STUDY OF REINFORCED CONCRETE TWO- WAY SLABS WITH AND WITHOUT OPENING HAVING DIFFERENT BOUNDARY CONDITIONS Hosam A. Daham Assistant Lecturer Civil Engineering Department University of Tikrit
More informationSTAFF SELECTION COMMISSION COMPLETE EXAM DETAILS
STAFF SELECTION COMMISSION COMPLETE EXAM DETAILS SSC MTS Pp-1 Exm Pttn Pp-1 i n onlin pp hving multipl choic qution in ction: Roning, Englih Lngug, Numicl Aptitud nd Gnl Awn Th nti pp i of totl 1 m nd
More informationFourier-Bessel Expansions with Arbitrary Radial Boundaries
Applied Mthemtics,,, - doi:./m.. Pulished Online My (http://www.scirp.og/jounl/m) Astct Fouie-Bessel Expnsions with Aity Rdil Boundies Muhmmd A. Mushef P. O. Box, Jeddh, Sudi Ai E-mil: mmushef@yhoo.co.uk
More informationSchool of Electrical Engineering. Lecture 2: Wire Antennas
School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/
More informationPhysics 240: Worksheet 15 Name
Physics 40: Woksht 15 Nam Each of ths poblms inol physics in an acclatd fam of fnc Althouh you mind wants to ty to foc you to wok ths poblms insid th acclatd fnc fam (i.. th so-calld "won way" by som popl),
More informationADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction
ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS Ghiocl Goza*, S. M. Ali Khan** Abstact Th additiv intgal functions with th cofficints in a comlt non-achimdan algbaically closd fild of chaactistic 0 a studid.
More informationErrata for Second Edition, First Printing
Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1 G( x)] = θp( R) + ( θ R)[1 G( R)] pg 15, problm 6: dmnd of
More informationIntegration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals
Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion
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 informationAn Elementary Approach to a Model Problem of Lagerstrom
An Elmntay Appoach to a Modl Poblm of Lagstom S. P. Hastings and J. B. McLod Mach 7, 8 Abstact Th quation studid is u + n u + u u = ; with bounday conditions u () = ; u () =. This modl quation has bn studid
More information1. 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 informationLecture 4. Conic section
Lctur 4 Conic sction Conic sctions r locus of points whr distncs from fixd point nd fixd lin r in constnt rtio. Conic sctions in D r curvs which r locus of points whor position vctor r stisfis r r. whr
More information1. 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 informationsin sin 1 d r d Ae r 2
Diffction k f c f Th Huygn-Fnl Pincil tt: Evy unobtuct oint of vfont, t givn intnt, v ouc of hicl cony vlt (ith th m funcy tht of th imy v. Th mlitu of th oticl fil t ny oint byon i th uoition of ll th
More informationModelling of Fission Chambers in Current Mode Analytical Approach
Modlling of Fission Chmbs in Cunt Mod Anlyticl Appoch Sébstin Chbod,, Gbil Fioni, Alin Ltounu, Fédéic Mi DSM/DAPNIA/SPhN, CA-Scly, 99 Gif-Su-Yvtt, Fnc DSM, CA-Scly, 99 Gif-Su-Yvtt, Fnc Abstct A comphnsiv
More informationPhysics 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 informationAbstract. The study reached some important recommendations, such as:
./Master-GE/GO -GRH /2016 قس ع و التسيير أ Abstract This study aimed at identifying the perception of workers in the waters company, about the level of organizational communication, and to identify the
More informationLecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationA STUDY OF PROPERTIES OF SOFT SET AND ITS APPLICATIONS
Intnational sach Jounal of Engining and Tchnology IJET -ISSN: 2395-0056 Volum: 05 Issu: 01 Jan-2018 wwwijtnt p-issn: 2395-0072 STDY O POPETIES O SOT SET ND ITS PPLITIONS Shamshad usain 1 Km Shivani 2 1MPhil
More informationINTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)
Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..
More informationMathematics. Mathematics 3. hsn.uk.net. Higher HSN23000
Highr Mthmtics UNIT Mthmtics HSN000 This documnt ws producd spcilly for th HSN.uk.nt wbsit, nd w rquir tht ny copis or drivtiv works ttribut th work to Highr Still Nots. For mor dtils bout th copyright
More informationSimulation of Boiler Drum Wall Temperature Differential and its Estimation 1 تمثیل و تخمین فرق درجات الحرارة لجدار وعاء المرجل البخاري
Differential and its Estimation 1 Prof Dr. Waladin K. Said 2 Bashra Kadhim Oleiwi 2 Abstract This paper is concerned with the problem of boiler drum wall temperature estimation to limit thermal stresses.
More informationElliptical motion, gravity, etc
FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs
More informationWalk Like a Mathematician Learning Task:
Gori Dprtmnt of Euction Wlk Lik Mthmticin Lrnin Tsk: Mtrics llow us to prform mny usful mthmticl tsks which orinrily rquir lr numbr of computtions. Som typs of problms which cn b on fficintly with mtrics
More informationUNIT # 08 (PART - I)
. r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'
More informationElasticity 1. 10th April c 2003, Michael Marder
Elasticity 0th Apil 003 c 003, Michal Mad Gnal Thoy of Lina Elasticity Bfo dfomation Aft dfomation Many ways to div lasticity. Cold div fom thoy of atoms and thi intactions. Howv, this appoach is not histoically
More informationA Simple Method for Determining the Manoeuvring Indices K and T from Zigzag Trial Data
Rind 8-- Wbsi: wwwshimoionsnl Ro 67, Jun 97, Dlf Univsiy of chnoloy, Shi Hydomchnics Lbooy, Mklw, 68 CD Dlf, h Nhlnds A Siml Mhod fo Dminin h Mnouvin Indics K nd fom Ziz il D JMJ Jouné Dlf Univsiy of chnoloy
More informationMEDIUM EFFECT ON ACTIVATION PARAMETERS FOR THE KINETICS OF REACTION BETWEEN β - BROMOPROPIONATE AND THIOSULFATE IONS
MEDIUM EFFECT ON ACTIVATION PARAMETERS FOR THE KINETICS OF REACTION BETWEEN β - BROMOPROPIONATE AND THIOSULFATE IONS Zahida Khalid Rehana Saeed and Fahim Uddin * Department of Chemistry, University of
More informationKeywords: Soil-structure interaction, Across wind, Chimney, Annular raft
Th Eighth Asi-Pifi Confn on Wind Engining, Dm 0, 03, Chnni, Indi EVALUATION OF TE EFFECT OF SOIL-STRUCTURE INTERACTION ON TE RAFT OF TALL REINFORCED CONCRETE CINEYS UNDER ACROSS WIND LOAD Jish S.V, Jylkshmi
More informationThe Z transform techniques
h Z trnfor tchniqu h Z trnfor h th rol in dicrt yt tht th Lplc trnfor h in nlyi of continuou yt. h Z trnfor i th principl nlyticl tool for ingl-loop dicrt-ti yt. h Z trnfor h Z trnfor i to dicrt-ti yt
More informationExtinction Ratio and Power Penalty
Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application
More information