Journal of Simulation & Analysis of Novel Technologies in Mechanical Engineering 10 (4) (2017) 0049~0064

Size: px
Start display at page:

Download "Journal of Simulation & Analysis of Novel Technologies in Mechanical Engineering 10 (4) (2017) 0049~0064"

Transcription

1 Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (4 (7 49~64 ISSN: Theo-elstic Anlysis of Functionlly Ge Thick- Wlle Cyline with Novel Tepetue Depenent Mteil Popeties using Petution Technique Hi Mohi Hooyeh, Aliez Nfoskouie Deptent of Soli Mechnics, Fculty of Mechnicl Engineeing, Univesity of Eyvnekey, Gs, In Astct (Mnuscipt Receive M. 8; Revise --- My 8; Accepte July 8 In this wok, theo elstic nlysis fo functionlly ge thick wlle cyline with tepetue - epenent teil popeties t stey conition is cie out. The length of cyline is infinite n loing is consist of intenl hyosttic pessue n tepetue gient. All of physicl n echnicl popeties expect the Poisson's tio e consiee s ultiplie n exponentil function of tepetue n powe function of ius. With these ssuptions, the nonline iffeentil equtions fo tepetue istiution t cylinicl coointe is otine. Tepetue istiution is chieve y solving this eqution using clssicl petution etho. With consieing stin isplceent, stess stin n equiliiu eltions n tepetue istiution tht poucte pevious, the constitutive iffeentil eqution fo cyline is otine. By eploying echnicl ouny conition the il isplceent is yiel. With hving il isplceent, stesses istiution long the thickness e chieve. The esults of this wok show tht y incesing the oe of tepetue petution seies the convegence t cuves is occue n lso iensionless il stess ecese n othe stesses with iensionless il isplceent incese. Keywos: Infinite thick wlle cyline, nonline het tnsfe, clssicl petution etho, tepetue-epenent popeties, functionlly ge teil. - Intouction Functionlly ge teils (FGMs e icoscopiclly inhoogeneous in which the echnicl popeties vy soothly n continuously fo one sufce to the othe [-]. FGMs e ege s one of the ost poising cnites fo futue vnce coposites in ny engineeing sectos such s the eospce, icft, utooile, n efense inusties, n ost ecently the electonics n ioeicl sectos [4-6]. All of these inusties use piping systes n thickwlle cylines. Mny stuies fo thel stesses of functionlly ge cylines e ville in the litetue. Ji et l. [7] epesente genel nlysis fo one-iensionl stey-stte thel stesses in hollow thick wlle FGM cyline. They consiee tht the teil popeties, except Poisson s tio, e ssue to epen on vile the ius n they e expesse s powe function. Thei esults evele tht the gnitue of the il stess is incese s the teil pete ( is incese. Sho n M [8] stuie theoechnicl nlysis of functionlly ge hollow cicul cylines sujecte to echnicl los n linely incesing ouny tepetue. They ssue tht the theo-echnicl popeties of FGM to e tepetue inepenent n vy

2 5 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 continuously in the il iection of cyline. They otine tie-epenent tepetue n unstey theoechnicl stesses y Lplce tnsfo techniques n seies solving etho. Di n Fu [9] pesente exct solutions fo stesses n petutions of the gnetic fiel vecto in FGM hollow cylines using the infinitesil theoy of gnetotheoelsticity. Thei esults illustte tht the inhoogeneity constnt hs jo effect on the gnetotheoelstic stesses, negtive vlues yiels copessive il n cicufeentil stesses in the whole FGM hollow cyline, while positive vlues gives conty esult. Axisyetic isplceents n stesses in functionllyge hollow cylines sujecte to unifo intenl pessue using plne elsticity theoy n Copleenty Functions etho escie y Tutuncu n Teel []. Sho n Wng [] investigte nlyticl solutions of the thee-iensionl tepetue n theoelstic stess fiels in the FGM cylinicl pnel with finite length. They consiee tht the thel n echnicl popeties of the FGM to e tepetue inepenent. Thei esults showe tht the xil stess is lge thn the il stess n is slle thn the cicufeentil stess. Tutuncu [] lso otine powe seies solutions fo stesses n isplceents in FG cylinicl vessels sujecte to intenl pessue lone using infinitesil theoy of elsticity. It is conclue fo his esults tht negtive inhoogeneity constnt woul cete stess plifiction effect. His stuy y e useful fo specific pplictions to contol the stess istiution. Moh n Mhooeh Azi [] cie out nonline tnsient het tnsfe n theoelstic stess nlyses of thick-wlle FGM cyline with tepetue - epenent teils using the Heitin tnsfinite eleent etho. The tepetue istiution n the il n cicufeentil stesses e investigte vesus tie, geoeticl petes n inex of powe lw in thei esech. Thei esech epesente tht y incesing of thickness, stesses ecese ue to ecesing of tepetue gient. A novel etho fo theoelstic nlysis of cylinicl vessel of FGMs pesente y Peng n Li [4].The thel n theoelstic petes ssue to itily vy long the il iection of the hollow cyline in thei wok. They coine the ouny vlue pole with theoelstic pole n then convete to Fehol integl eqution. Accoingly, y nueiclly solving the esulting eqution, the istiution of the thel stesses n il isplceent ws otine. They tht ppopite gient cn ke the istiution of thel stesses oe gentle in foun the whole stuctue. Exct n ppoxite solutions of theoelstic stesses in FG cylines with powe lw n exponentilly vitions of teil popeties eive y Seifi [5]. He conclue tht effects of high tepetue on the stesses e oe ipotnt thn the high intenl pessue. Exct theoelstic nlysis of FG nisotopic hollow cylines with ity teil gtion povie y Vel [6]. He solve the iffeentil equtions of het conuction n theoelsticity using powe seies solution technique. He foun tht the tepetue, isplceents n stesses e sensitive to the teil gtion. Loghn n Ps [7] nlyze the gneto-theo-elstic esponse fo thick oule-wlle cyline e fo FGM intelye n hoogeneous oute lye. They showe tht tht une theogneto-echnicl loing iniu effective stess istiution n the iniu il isplceent cn e chieve y selecting n ppopite teil pete in the FGM lye. Ghonpou Ani n his esech goup [8] escie electo-theo-echnicl ehvio of illy polize otting functionlly ge piezoelectic cyline. They consiee tht the teil

3 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 5 popeties except Poisson s tio n thel conuction coefficient to e exponentilly istiute long ius. It is conclue fo thei esults tht the inhoogeneity exponent plys sustntil ole in il n cicufeentil stess istiutions. Theo-electoechnicl ehvio of FG piezoelectic hollow cyline une nonxisyetic los stuie y Atin et l. [9] Aefi n Rhii [] investigte the effect of nonhoogeneity n en suppots on the theo elstic ehvio of clpe-clpe FG cyline une echnicl n thel los. They eploye Hilton pinciple n fist oe she efotion theoy (FSDT fo eivtion of the pinciple iffeentil equtions. Thei esults showe tht the solute vlue of xil isplceent of the cyline eceses with incesing the non hoogenous inex. Thel stesses nlysis of FG cylinicl shell une thel shock se on iffeentil qutue etho chieve y Zhng et l. [] They illustte tht the thel stesses coul e llevite y ens of chnging the volue fctions of the constituents. Theo-elstic nlysis of clpe-clpe thick FGM cylines y using thi-oe she efotion theoy inicte y Ghooni et l. [] They solve the set of nonhoogenous line iffeentil equtions fo the cyline with clpe-clpe ens. It is oseve fo thei esults tht using negtive inhoogeneities in the cyline cuses sll eceses une thel lo n consiele incese une echnicl lo in il isplceents. Two iensionl theoelstic nlysis of FG cyline fo iffeent functionlities y using the highe oe she efotion theoy pesente y Aefi []. His esults showe tht the il isplceent eceses with incesing powe low inex ue to n incese in the cyline stiffness with incesing powe low inex. Aefi n his esech goup [4] epesente two-iensionl theoelstic nlysis of FG cylinicl shell esting on the Pstenk fountion sujecte to echnicl n thel los se on FSDT foultion. They use enegy etho n Eule equtions fo govening iffeentil equtions of syste. They showe tht y incesing the nonhoogeneity inex oth, il n xil isplceent eceses. In ll of pevious stuies tht conucte on the FGM, siply oeling fo echnicl n physicl chnges popeties ws selecte. These oels wee exponentilly istiute o expesse y powe function long the ius. In cuent wok, we ie to consie chnges ll physicl n echnicl popeties (except fo Poisson's tio s powe function vesus ius n function of exponentilly vesus tepetue. This ction le to nonline iffeentil eqution fo het tnsfe tht y solving of it using petution technique we cn use the tepetue istiution t theoelstic nlysis. - Geoety, loing conition n ssuptions An infinitely long, functionlly ge thick wlle hollow cyline with inne ius n oute ius is consiee. This cyline is sujecte to n intenl hyosttic pessue P n unifo tepetue fiel with inne sufce tepetue T n oute tepetue of T. One iensionl n stey stte het conuction e selecte fo tepetue istiution. Cente cylinicl coointes is on the cente of the cyline n xil syety in geoety n loing will e consiee. Figue shows the schetic view of the cyline n its loing.

4 5 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 Figue. Schetic of FG cyline une echnicl n thel los - Het conuction pole The het conuction eqution with eg to the ove-entione ssuptions n without ny het souce is witten in cylinicl coointe s follow: T k ( In which, k n T e ius, noinl het conuctivity coefficient n tepetue istiution espectively. It is ssue tht the theophysicl n echnicl popeties expect the Poisson's tio e consiee s pouct of n exponentil function of tepetue n powe function of ius. Futheoe, the noinl het conuctivity coefficient is ssue to epen on tepetue s follow [5]: k, T k ( k ( T ( The exponentil function of tepetue is ssue s follow fo: 6 k( T kexp( ( T T ( The powe function istiution in the il iection consiee s [5], [6]: k ( k 4( Accoingly, fo noinl het conuctivity coefficient cn e witten s follow: 6 k, T k exp( ( T T k k k 5( Whee k,, e the physicl constnts chcteizing the teil ehvio. By sustituting Eq. ( in to Eq. ( we hve: T T ( k (, T k (,T k (, T T T k (, T 6( k (, T In which is clculte using the pouct ule s follow: k (,T 6 ( k exp( ( T T 6 (exp( ( T T k 7( 6 k exp( ( T T 6 6 T k exp( ( T T Sustituting Eq. (7 in to Eq. (6 n then siplify, the following nonline iffeentil eqution of the secon oe is otine: T 6 T T 8( - - Petution technique Petution technique is one of the ost efficient ppoch to solving vious ouny issues in elstic stuctues. This etho s ens of ppoxite - nlyticlly useful is eploye to solve lge pt of the nonline poles. Accoing to the petution etho, coplex nonline iffeentil eqution is ivie to unliite nue of eltively siple equtions (Petution eqution. Accoingly, the solution of oiginl eqution is the sution of solving ech Petution equtions with the ising powe of sll petution pete s coefficient is expesse. Theefoe, the fist few tes, epesent the view of solving the pole. It is ipotnt t petution technique tht the sll petution pete, select the ppopite. In using this etho it is necessy tht the sll petution

5 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 5 pete to e consiee slle thn one. This etho is use in continue. By iviing Eq. (8 on pete we hve: 6 T T T 9( 6 The sll tio of is to ppe in the nonline iffeentil eqution (9 tht we cn now efine this tio equl to sll pete. Theefoe the Eq. (9 cn e ewitten s follow: T T T ( Petution theoy les to n expession fo the esie solution in tes of fol powe seies in soe sll pete, known s petution seies, tht quntifies the evition fo the exctly solvle pole. The leing te in this powe seies is the solution of the exctly solvle pole, while futhe tes escie the evition in the solution, ue to the evition fo the initil pole. Folly, we hve fo the ppoxition to the full solutiont, seies in the sll pete, like the following [7-]: T T T T... In Eq. (, T woul e the known solution to the exctly solvle initil pole nt, T,... epesent the higheoe tes which y e foun itetively y soe systetic poceue. Fo sll these highe-oe tes in the seies ecoe successively slle. An ppoxite petution solution is otine y tuncting the seies, usully y keeping only the fist thee tes, the secon-oe petution coection cn e witten s []: T T T T By sustituting Eq. ( into Eq. ( n gouping ll tes with the se powe of gives: T T ( T T ( T T T ( T T ( With setting zeo coefficient of vious powes of (the coefficient of will e ignoe set of iffeentil eqution cn e otine s follow: T T O ( : ( T T T O ( : ( 4 T T T O ( : ( Fist, the O ( pole is to e solve n then it esults in highe-oe ppoxition is use. The nswe of O ( pole cn e chieve s: c T ( c 5 c n c e the integtion constnts which cn e eteine y the following thel ouny conitions: T( T T( T 6 Iposition of these ouny conitions onto the Eq. (5 gives the following eltions fo the integtion constnts c n c :

6 54 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 c T T T c T, 7 By sustituting Eq. ( into the O ( t Eq. (, the iffeentil eqution fo O ( pole will e otine s follow: T T c 8 This is n inhoogeneous Cuchy Eule oiny iffeentil eqution whose genel n pticul solutions cn e foun s: c c T( c4 9 The integtion constnts c n c 4 cn e chieve y pplying thel ouny conitions (6 to the solution (9 s: c ( ( T T c ( c 4 ( c T ( ( c T ( As efoe, we sustituting Eq. (9 into the O ( t Eq. ( n the O ( iffeentil eqution will e epesente s follow: T T c c ( Eq. ( is gin n inhoogeneous Cuchy-Eule iffeentil eqution whose genel solution is pesente s the su of the hoogeneous solution n pticul solution s follow: c5 4 4 T ( c6 c cc c Appliction of ouny conitions (6 to the genel solution ( yiels the integtion constnts c5 nc 6 s follow: c 5 6 c ( ( 4 c c ( ( 6 c ( ( T T c ( c ( 4 c c 4 4 ( (6c T c 4 ( 4 4 c cc ( (6c T ( ( 4 Theefoe, the tepetue istiutions t iffeent oes of ppoxition cn e otine s follow: c T ( ( c O ( T ( ( c c c ( c c O ( 4 c T ( ( c c c ( c4 c ( c c c c c O ( Theoelstic nlysis 4- - Stess stin eltions The stess stin eltions t cylinicl coointes syste t genel fo cn e witten s follow []: 4

7 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 55 ( ( z T ( E ( ( z T ( E ( z ( z z T ( E,, G G G z z z z 5 In which, n z enotes il, cicufeentil n xil iections, espectively. i n i ( i,, z e the stess n stin, n E e the Poisson's tio n oulus elsticity, espectively. G is the young oulus n i ( i,, z is the coefficient of thel expnsion tht consiee to e se t ll coointes. Accoing to the ssuptions, ll she stins n cicufeentil eivtives e zeo n fo plne stin conitions the xil stess is consiee s follow: E T ( z z 6 With sustituting Eq. (6 into Eq. (5 n siplify, the stess stin eltions fo functionlly ge thick wlle cyline t one iensionl het conuction e foun s follow: T ( 7 T ( The coefficients in Eq. (6 e in the powe n exponentil functions fo n e efine s elow: T T E ( ( ( 6 exp( ( 6 exp( ( T T E ( ( ( T T 6 exp( ( ( z Stin isplceent eltions The stess isplceent eltions t cylinicl coointes syste t genel fo cn e otine s follow []: u u u, uz u u u, z u u z u u z z, z z z 9 Whee ui ( i,, z is the isplceent vecto. These eltions with consieing ssuptions ewitten s elow: u u, 4- - Stess isplceent eltions Sustituting Eq. ( into Eq. (7, the stess isplceent eltions yiels s follow: u u T ( u u T ( 4-4- Equiliiu eltions The equiliiu equtions of the hollow cyline t genel fo e s follow [], []: z z F t z z u F t z z z u z z Fz t u

8 56 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 Whee Fi ( i,, z e the oy foces n is the teil ensity. The equiliiu eqution of the FGM hollow cyline, with consieing pevious ssuptions n stey conitions in the sence of oy foces, is expesse s: 4-5- Theoeltic constitutive eqution By sustituting the esulting tepetue istiution fo Eq. (4 into Eq. ( n then into Eq. ( the theoelstic constitutive eqution fo FG thick wlle hollow cyline with tepetue epenent teil popety is eive s follow: u u ( u ( c c c c c4 c c c5 c6 4 4 cc ( c c c 4 4 c 4 cc c c5 4 The oots of the chcteistic eqution e: So, the genel solution of the inhoogeneous eqution (4 cn e expesse s su of pticul solution n the genel solution of the hoogeneous one s elow: u ( u ( u ( C C g g 4 4 g g g In which: p c c4 c6 g ( c c g ( ( ( 4 4 c g 4 ( 4 ( ( 4 cc g 4 ( ( ( 7 8 Cn C e the integtion constnts which will e foun s follow Integtion constnts By sustituting il isplceent Eq. (7 into Eq. ( the il stess cn e ewitten s: This eqution is the fili Cuchy-Eule iffeentil eqution fo il isplceent tht chcteistic eqution fo it is s follow: 5

9 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 57 exp( ( T T ( C C g g g g exp( ( T T ( C C g g g g 4 exp( ( T T ( c c 6 c c c c c c c c 5 c6 The theoelstic pole is sujecte to the following echnicl ouny conitions. The cyline is loe with intenl hyosttic pessue: 9 P( P P( 4 Appliction of these ouny conitions to the il stess (9 yiels the following eltions fo the integtion constnts: C (( ( ( c c 4(( g ( ( c c 4( ( g 4 ( c 48 g (( 4 4 ( cc 9g 4( ( ( exp( ( T T P 5 ( c c c ( c 48 g (( 4 4 ( cc 9 g 4(( ( ( c c c ( ( c c c g ( ( 4 4

10 58 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 C (6( ( c c 6 4 c 4(( 4(( g ( g 48 g (( ( cc 9 g 4(( ( ( ( c c 5 ( c c c 4 exp( ( T T P 4 4 ( c 48 g (( ( ( c5 c c 6 4 ( ( ( cc 9 g 4(( ( ( c c c g 4 With fining unknown constnts the ll stesses n il isplceent cn e clculte. Also the Von Mises stess cn e otine s follow: eff ( z ( z 5- Nueicl esults n iscussion 4 In the following nueicl clcultions, the echnicl n geoetic popeties fo FGM cyline e consiee s [- 5]: E (G P..e 6( C P (MP 4 It shoul e note tht tepetue vlues t inne n oute sufces n othe pete is escie fte thn ny figue. Fo ette nlysis of esults the iensionless pete e pesente s follows: i i i,, z, eff P 44 u u A istiute tepetue fiel ue to stey-stte het conuction fo thickwlle FGM cyline vesus iensionless ius with iffeent oes of ppoxition illustte in figue. It is shown fo this figue tht y incesing the oes of ppoxition fo zeothoe (i.e., line pole until the secon- oe solution the convegence of petution seies is occus. Also, it is oseve esily tht the thel ouny conitions hve een stisfie. Figues n 4 inicte the influence of physicl constnts chcteizing the teil ehvio (, on the tepetue istiution (secon oe. It is cle fo figues n 4 tht y incesing the vlue of n the tepetue istiution inceses long the thickness of FGM cyline. Figue 5 epesents the iensionless il stess istiution vesus iensionless ius with iffeent oes of ppoxition. It is conclue tht iensionless il stesses eceses with incesing oes of ppoxition. Fo this figue lso convegence of petution seies is otine. Futheoe, it is copessive t the inne pt of the cyline which hs to stisfy the intenl pessue ouny conition. Diensionless cicufeentil n xil stesses long the thickness of cyline with incesing the oes of ppoxition e eonstte y Figues 6 n 7, espectively. It cn e conclue fo these figues tht y

11 T( o C T( o C T( o C H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 59 incesing iensionless ius the iensionless cicufeentil n xil stesses inceses. It cn e seen tht xiu n iniu stesses hppens t inne n oute sufces, espectively. Figues 8 n 9 epicts the effects of incesing the oes of ppoxition on the iensionless effective stesses n istiution of iensionless il isplceent long the thickness of cyline, espectively. It is shown tht y incesing oes of ppoxition the iensionless effective stess n iensionless il isplceent inceses. Also it is oseve tht xiu effective stess n il isplceent e t inne sufce n it ens tht xiu ge occus t in this sufce. The influence the influence of physicl constnts chcteizing the teil ehvio (, on the iensionless effective stess e epesente in figues n. It is conclue fo figue tht fo constnt vlue of, y incesing the vlue of the vlues of iensionless effective stess t the inne lye to the ile lye of the cyline hs een euce n the iensionless effective stess vlues of the oute lye is e. Figue show tht y incesing the vlue of, t constnt vlue of, the iensionless effective stess eceses T +T +T Figue. Tepetue istiution stess long the thickness of FGM cyline with iffeent oes of ppoxition T ( C, T ( C, 4, = - = - = - = = = Figue. Tepetue istiution stess long the thickness of FGM cyline with iffeent vlue of T ( C, T ( C, =.6 =.7 =.8 = Figue4. Tepetue istiution stess long the thickness of FGM cyline with iffeent vlue of T ( C, T ( C, +T +T +T Figue5. Diensionless il stess long the thickness of FGM cyline with iffeent oes of ppoxition T 5( C, T 5( C,,.

12 6 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~ T +T +T u Figue6. Diensionless cicufeentil stess long the thickness of FGM cyline with iffeent oes of ppoxition T 5( C, T 5( C,, z T +T +T Figue7. Diensionless xil stess long the thickness of FGM cyline with iffeent oes of ppoxition T 5( C, T 5( C,, eff 9 x T +T +T Figue9. Diensionless il stess long the thickness of FGM cyline with iffeent oes of ppoxition eff T 5( C, T 5( C,,. = = = = Figue. Diensionless effective stess long the thickness of FGM cyline with iffeent vlue of.5 T 5( C, T 5( C,. =. =.5 =. =.5 +T +T +T eff Figue. Diensionless effective stess long the thickness of FGM cyline with iffeent vlue of T 5( C, T 5( C, Figue8. Diensionless effective stess long the thickness of FGM cyline with iffeent oes of ppoxition 5- Conclusion T 5( C, T 5( C,,. In this ppe theoelstic nlysis of functionlly ge thick wlle cyline

13 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 6 with tepetue epenent teil popety is investigte. This ticle epesente suitle ppoch fo nlysis teil tht thei theophysicl n echnicl popeties expect the Poisson's tio e consiee s pouct of n exponentil function of tepetue n powe function of ius. Fo this pupose, petution technique is use to solving nonline iffeentil eqution fo tepetue istiution. This tepetue istiution is eploye t giving ehvio of thel stesses. The esults of this ticle cn e liste s follows: - By incesing the oes of ppoxition fo zeoth-oe (i.e., line pole until the secon- oe solution the convegence of petution seies t ll figues is occus. - By incesing the vlue of n the tepetue istiution inceses long the thickness of FGM cyline. - The iensionless il stesses eceses n iensionless cicufeentil, xil n effective stesses n il isplceent inceses with incesing oes of tepetue ppoxition. 4- Mxiu effective stess n il isplceent e locte t inne sufce. It ens tht xiu ge occus t in this sufce. The otine esults fo this esult cn e use to esign of cylinicl stuctues. 5- By incesing the vlue of the iensionless effective stess t the inne lye to the ile lye of the cyline hs een euce n the iensionless effective stess t the oute lye inceses. Also y incesing the vlue of the iensionless effective stess eceses. Refeences: [] S. Suesh, n A. Motensen, Funentls of functionlly ge teils, Bnes n Nole Pulictions, 998. [] M.Ynouchi, n M. Koizui, Functionlly gient teils. Poceeing of the fist intentionl syposiu on functionlly ge teils, Seni, Jpn, 99. [] M.M. Njfizeh, n H.R. Heyi, An exct solution fo uckling of functionlly ge cicul pltes se on highe oe she efotion plte theoy une unifo il copession, Int. J. Mech. Sci., vol. 5, pp. 6 6, 8. [4] H.J. Xing, n J. Yng, Fee n foce vition of linte FGM Tioshenko e of vile thickness une het conuction, Copos. Pt B (Eng, vol. 9, pp. 9, 8. [5] R. Ansi, n M. Dvizeh, Peiction of ynic ehviou of FGM shells une ity ouny conitions, Copos. Stuct., vol. 85, pp. 84 9, 8. [6] A. Allhveizeh, M.H. Nei, n M. Nikkhh Bhi, Vition plitue n thel effects on the nonline ehvio of thin cicul functionlly ge pltes, Int. J. Mech. Sci., vol. 5, pp , 8. [8] M. Ji, S. Sohpou, n M.R. Eslic, Mechnicl n thel stesses in functionlly ge hollow cyline ue to illy syetic los, Int. J. Pessue Vessels Piping, vol. 79, pp ,. [9] Z.S. Sho, n G.W. M, Theoechnicl stesses in functionlly ge cicul hollow cyline with linely incesing ouny tepetue, Copos. Stuct., vol.8 pp , 8. [] H.L. Di, n Y.M. Fu, Mgnetotheoelstic intections in hollow stuctues of functionlly ge teil sujecte to echnicl los, Int. J. Pessue Vessels Piping vol. 84 pp. 8, 7.

14 6 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 [] N.Tutuncu, n B. Teel, A novel ppoch to stess nlysis of pessuize FGM cylines, isks n sphees, Copos. Stuct., vol. 9, pp. 85 9, 9. [] Z. Sho, T.J. Wng, Theeiensionl solutions fo the stess fiels in functionlly ge cylinicl pnel with finite length n sujecte to thel/echnicl los, Int. J. Solis. Stuct., vol.4, pp , 6. [] N. Tutuncu, Stesses in thick-wlle FGM cylines with exponentilly-vying popeties, Eng. Stuct., vol.9, pp.- 5, 7. [4] M. Azi, n M. Azi, Nonline tnsient het tnsfe n theoelstic nlysis of thick-wlle FGM cyline with tepetue-epenent teil popeties using Heitin tnsfinite eleent, J. Mech. Sci Tech., vol., pp , 9. [5] X.L. Peng, n X.F. Li, Theoelstic nlysis of cylinicl vessel of functionlly ge teils, Int. J. Pessue Vessels Piping, vol. 87 pp. -,. [6] R. Seifi, Exct n ppoxite solutions of theoelstic stesses in functionlly ge cylines, J. Thel Stesses, vol. 8, pp. 6 8, 5. [7] S.S.Vel, Exct theoelstic nlysis of functionlly ge nisotopic hollow cylines with ity teil gtion, Mech. Av. Mte. Stuct., vol. 8, pp.4,. [8] A. Loghn, n H. Ps, Exct solution fo gneto-theo-elstic ehviou of oule-wlle cyline e of n inne FGM n n oute hoogeneous lye, Int. J. Mech. Sci., vol. 88, pp. 9-99, 4. [9] A. Ghonpou Ani, A. Loghn, A. Aollhithei, n V. Atkhshin, Electotheoechnicl ehvio of illy polize otting functionlly ge piezoelectic cyline, J. Mech. Mte. Stuct., vol.6, pp ,. [9] A. Atin, J. Jfi Feshki, n S. H. Noukhsh, Theo-electoechnicl ehvio of functionlly ge piezoelectic hollow cyline une nonxisyetic los, Appl. Mth. Mech. Engl. E., vol. 5, pp , 5. [] M. Aefi, n G.H. Rhii, The effect of nonhoogeneity n en suppots on the theo elstic ehvio of clpeclpe FG cyline une echnicl n thel los, Int. J. Pess Vessels Piping, vol. 96, pp. -7,. [] J.H. Zhng, G.Z. Li, S.R. Li, n Y.B. M, DQM-se thel stesses nlysis of functionlly ge cylinicl shell une thel shock, J. Thel Stesses, vol. 8, pp , 5. [] H. Ghooni, M. Ghnn, n M.Z.Nej, Theo-elstic nlysis of clpe-clpe thick FGM cylines y using thi-oe she efotion theoy, Ltin Aeicn Jounl of Solis n Stuctues, vol., pp , 6. [] M. Aefi, Two iensionl theoelstic nlysis of FG cyline fo iffeent functionlities y using the highe oe she efotion theoy, J. Appl. Mech. Tech. Phys, vol. 56, pp , 5. [4] M. Aefi, A.R. Asi, n M.R.Vzii Seeshk, Two-iensionl theoelstic nlysis of FG cylinicl shell esting on the Pstenk fountion sujecte to echnicl n thel los se on FSDT foultion, J. Thel stesses, vol. 9, pp , 6. [5] M. Aefi, Nonline thel nlysis of functionlly ge hollow cyline with tepetue vile teil popeties, J. Appl. Mech. Tech. Phys., vol. 56, pp. 67-7, 5. [6] A. loghn, n M. Moi, The nlysis of tie-epenent ceep in FGPM thick wlle sphee une electo-gnetotheo-echnicl loings, Mech. Tie- Depenent Mteils, vol. 7, pp. 5 9,. [7] A.M. Wzwz, Ptil iffeentil equtions n solity Wves theoy, Nonline Physicl Science, Spinge, 9.

15 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64 6 [8] A. Sighi, n D.D. Gnji, Exct solutions of Lplce eqution y hootopy-petution n Aoin ecoposition ethos, Phys. Lett. A., vol. 67, pp. 8-87, 7. [9] R. Vtnkhh, M.H. Khoiyn, A. Alsty, n M.T. Ahin, Nonline foce vition of stin gient icoes, Appl. Mth. Moel., vol. 7, pp ,. [] A. Moosie, Axisyetic stey tepetue fiel in FGM cylinicl shells with tepetue-epenent het conuctivity n ity line ouny conitions, Ach. Mech., vol. 67, pp. 5, 5. [] A.C., Ugul, n S.K., Fenste, Avnce stength n pplie elsticity, New Jesey Institute of Thechnology,. [] A. Alieigloo, A.M. Kni, n M.H. Pshei, Elsticity solution fo the fee vition nlysis of functionlly ge cylinicl shell one to thin piezoelectic lyes, Int. J. Pessue Vessels Piping, vol. 89, pp. 98-,. [] A. Loghn, S.M.A. Aleyou, n M. Hsni Si, Tie-epenent gnetotheoelstic ceep oeling of FGM sphees using etho of successive elstic solution, Appl. Mth. Moel., vol. 6, pp ,. [] J. Jfi Feshki, A. Loghn, M. Yzipoo, n S. Goli, Sei-nlyticl solution of tie-epenent theoechnicl ceep ehvio of FGM hollow sphees, Mech. Tie-Depenent Mteils, vol. 8, pp. 4 5, 4. [4] A. Loghn, A. Ghonpou Ani, S. Ai, n A. Vjei, Mgnetotheoelstic ceep nlysis of functionlly ge cylines, Int. J. Pessue Vessels Piping, vol. 87, pp ,.

16 64 H.Mohi et l./ Jounl of Siultion & Anlysis of Novel Technologies in Mechnicl Engineeing (7 49~64

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

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

More information

Effect of Heat Generation on Quasi- Static Thermal Stresses in a Solid Sphere

Effect of Heat Generation on Quasi- Static Thermal Stresses in a Solid Sphere IOS Jounl of Mthetics (IOS-JM) e-issn: 78-578,p-ISSN: 39-765X, Volue 7, Issue 5 (Jul. - Aug. 3), PP -9 www.iosjounls.og Effect of Het Genetion on Qusi- Sttic Thel Stesses in Solid Sphee S.P. Pw, K.C. Deshukh,

More information

Ch 26 - Capacitance! What s Next! Review! Lab this week!

Ch 26 - Capacitance! What s Next! Review! Lab this week! Ch 26 - Cpcitnce! Wht s Next! Cpcitnce" One week unit tht hs oth theoeticl n pcticl pplictions! Cuent & Resistnce" Moving chges, finlly!! Diect Cuent Cicuits! Pcticl pplictions of ll the stuff tht we ve

More information

Fourier-Bessel Expansions with Arbitrary Radial Boundaries

Fourier-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 information

Chapter 25 Electric Potential

Chapter 25 Electric Potential Chpte 5 lectic Potentil consevtive foces -> potentil enegy - Wht is consevtive foce? lectic potentil = U / : the potentil enegy U pe unit chge is function of the position in spce Gol:. estblish the eltionship

More information

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations Adv. Theo. Appl. Mech., Vol. 7, 2014, no. 1, 1-7 HIKARI Ltd, www.m-hiki.com http://dx.doi.og/10.12988/tm.2014.458 Qulittive Anlysis fo Solutions of Clss of Nonline Odiny Diffeentil Equtions Juxin Li *,

More information

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

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

More information

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

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

More information

FI 2201 Electromagnetism

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

More information

U>, and is negative. Electric Potential Energy

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

More information

Electric Potential. and Equipotentials

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

More information

Lecture 4. Electric Potential

Lecture 4. Electric Potential Lectue 4 Electic Ptentil In this lectue yu will len: Electic Scl Ptentil Lplce s n Pissn s Eutin Ptentil f Sme Simple Chge Distibutins ECE 0 Fll 006 Fhn Rn Cnell Univesity Cnsevtive Ittinl Fiels Ittinl

More information

Using Potential Energy

Using Potential Energy Using Potentil Enegy You ve job poviing te engineeing elp o n citect in Coloo. You e cuently esigning cble tow to pull sies up ill so tey cn si own. e custoe woul lie te cble tow to pull sie upill t constnt

More information

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

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

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 20

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 20 .615, MHD Theoy of Fusion Systes Pof. Feideg Lectue Resistive Wll Mode 1. We hve seen tht pefectly conducting wll, plced in close poxiity to the pls cn hve stong stilizing effect on extenl kink odes..

More information

4.2 Boussinesq s Theory. Contents

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

More information

Chapter 6 Thermoelasticity

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

More information

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

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

More information

Classical Electrodynamics

Classical Electrodynamics Fist Look t Quntu hysics Cssic Eectoynics Chpte gnetosttics Fy s Lw Qusi-Sttic Fies Cssic Eectoynics of. Y. F. Chen Contents Fist Look t Quntu hysics. The etionship between eectic fie n gnetic fie. iot

More information

(1) It increases the break down potential of the surrounding medium so that more potential can be applied and hence more charge can be stored.

(1) It increases the break down potential of the surrounding medium so that more potential can be applied and hence more charge can be stored. Cpcito Cpcito: Cpcito ( o conense ) is evice fo stoing chge. It essentilly consists of two conucting sufces such s two pltes o two spheicl shell o two cylines etc. kept exctly pllel to ech othe septe y

More information

Elastic limit angular speed of solid and annular disks under thermomechanical

Elastic limit angular speed of solid and annular disks under thermomechanical MultiCft Intentionl Jounl of Engineeing, Science nd Technology Vol. 8, No., 016, pp. 30-45 INTERNATIONAL JOURNAL OF ENGINEERING, SCIENCE AND TECHNOLOGY www.ijest-ng.com www.jol.info/index.php/ijest 016

More information

A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS ABSTRACT

A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS ABSTRACT A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS S. W. Chung* School of Achitectue Univesity of Uth Slt Lke City, Uth, USA S.G. Hong Deptment of Achitectue Seoul Ntionl Univesity

More information

Influence of the Magnetic Field in the Solar Interior on the Differential Rotation

Influence of the Magnetic Field in the Solar Interior on the Differential Rotation Influene of the gneti Fiel in the Sol Inteio on the Diffeentil ottion Lin-Sen Li * Deptment of Physis Nothest Noml Univesity Chnghun Chin * Coesponing utho: Lin-Sen Li Deptment of Physis Nothest Noml Univesity

More information

Discrete Model Parametrization

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

More information

CHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES

CHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES HPTER ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy So,. foce between chges 4 So, foce between chges.6 weight of

More information

CHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton

CHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton Downloe fo HPTER? ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy.5 So, foce between chges 4 So, foce between chges

More information

3.1 Magnetic Fields. Oersted and Ampere

3.1 Magnetic Fields. Oersted and Ampere 3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,

More information

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

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

More information

9.4 The response of equilibrium to temperature (continued)

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

More information

Answers to test yourself questions

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

More information

About Some Inequalities for Isotonic Linear Functionals and Applications

About Some Inequalities for Isotonic Linear Functionals and Applications Applied Mthemticl Sciences Vol. 8 04 no. 79 8909-899 HIKARI Ltd www.m-hiki.com http://dx.doi.og/0.988/ms.04.40858 Aout Some Inequlities fo Isotonic Line Functionls nd Applictions Loedn Ciudiu Deptment

More information

Fluids & Bernoulli s Equation. Group Problems 9

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

More information

A Parametric Study on the Centrifugal Force-Induced Stress and Displacements in Power-Law Graded Hyperbolic Discs

A Parametric Study on the Centrifugal Force-Induced Stress and Displacements in Power-Law Graded Hyperbolic Discs Oiginl Aticle A Pmetic Study on the Centifugl Foce-Induced Stess nd Displcements in Powe-Lw Gded Hypebolic Discs Abstct An extensive pmetic study on the vition of the centifugl-foce-induced stess nd displcements

More information

10 Statistical Distributions Solutions

10 Statistical Distributions Solutions Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques

More information

Supplementary material for " Coherent and Tunable Terahertz Radiation from Graphene Surface Plasmon Polarirons Excited by Cyclotron Electron Beam "

Supplementary material for  Coherent and Tunable Terahertz Radiation from Graphene Surface Plasmon Polarirons Excited by Cyclotron Electron Beam Suppleenty teil fo " Coheent nd Tunble Tehet Rdition fo Gphene Sufce Plson Polions Excited by Cycloton Electon Be " To Zho,, Sen Gong,, Min Hu,, Renbin Zhong,,Diwei Liu,,Xioxing Chen,, Ping hng,, Xinn

More information

Equilibria of a cylindrical plasma

Equilibria of a cylindrical plasma // Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the

More information

Electronic Supplementary Material

Electronic Supplementary Material Electonic Supplementy Mteil On the coevolution of socil esponsiveness nd behvioul consistency Mx Wolf, G Snde vn Doon & Fnz J Weissing Poc R Soc B 78, 440-448; 0 Bsic set-up of the model Conside the model

More information

AXIAL GAP ELECTROSTATIC WOBBLE MICROMOTOR

AXIAL GAP ELECTROSTATIC WOBBLE MICROMOTOR XIL GP ELETOSTTI WOLE MIOMOTO nc TOMESU Soin NTONIU F.M.G. TOMESU Electicl Engineeing Dept. POLITEHNI Univesity uchest ãzvn MOEI ING OMNI uchest The toque vesus ngle mechnicl chcteistic of n xil gp electosttic

More information

Consolidation Solutions of a Saturated Porothermoelastic Hollow Cylinder with Infinite Length

Consolidation Solutions of a Saturated Porothermoelastic Hollow Cylinder with Infinite Length ngineeing,,, **-** oi:.36/eng..5 Pulishe Online Jnuy http://www.scip.og/jounl/eng/). Consolition Solutions of Stute Poothemoelstic Hollow Cyline with nfinite Length Astct Consolition Solutions of Poothemoelstic

More information

Exact Solution for Electro- Thermo- Mechanical Behavior of Composite Cylinder Reinforced by BNNTs under Non- Axisymmetric Thermo- Mechanical Loads

Exact Solution for Electro- Thermo- Mechanical Behavior of Composite Cylinder Reinforced by BNNTs under Non- Axisymmetric Thermo- Mechanical Loads mikabi Univesity of Technology (Tehan Polytechnic) Vol, No, Sping 3, pp - mikabi Intenational Jounal of Science & Reseach (Moeling, Ientification, Simulation & Contol) (IJ - MISC) Exact Solution fo Electo-

More information

6. Numbers. The line of numbers: Important subsets of IR:

6. Numbers. The line of numbers: Important subsets of IR: 6. Nubes We do not give n xiotic definition of the el nubes hee. Intuitive ening: Ech point on the (infinite) line of nubes coesponds to el nube, i.e., n eleent of IR. The line of nubes: Ipotnt subsets

More information

Two dimensional polar coordinate system in airy stress functions

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

More information

Chapter 28 Sources of Magnetic Field

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

More information

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

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

More information

Investigations of Boundary Treatments in Incompressible Smoothed Particle Hydrodynamics for Fluid-Structural Interactions

Investigations of Boundary Treatments in Incompressible Smoothed Particle Hydrodynamics for Fluid-Structural Interactions Recent Reseches in Mechnics Investigtions of Boundy Tetments in Incompessile Smoothed Pticle Hydodynmics fo Fluid-Stuctul Intections Fnfn Sun, Mingyi Tn, nd Jing T Xing Astct Two oundy tetment methods

More information

Week 8. Topic 2 Properties of Logarithms

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

More information

Michael Rotkowitz 1,2

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

More information

Jerk and Hyperjerk in a Rotating Frame of Reference

Jerk and Hyperjerk in a Rotating Frame of Reference Jek an Hypejek in a Rotating Fame of Refeence Amelia Caolina Spaavigna Depatment of Applie Science an Technology, Politecnico i Toino, Italy. Abstact: Jek is the eivative of acceleation with espect to

More information

SHAPE OPTIMIZATION USING BOUNDARY ELEMENTS

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

More information

Micro-scale adhesive contact of a spherical rigid punch on a. piezoelectric half-space

Micro-scale adhesive contact of a spherical rigid punch on a. piezoelectric half-space http://www.ppe.edu.cn Mico-scle dhesive contct of spheicl igid punch on piezoelectic hlf-spce Z.R. Chen, S.W. Yu * Deptment of Engineeing Mechnics, Tsinghu Univesity, Beijing 84, P.R. Chin Abstct The mico-scle

More information

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

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

More information

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)

More information

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

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

More information

Physics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems.

Physics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems. Physics 55 Fll 5 Midtem Solutions This midtem is two hou open ook, open notes exm. Do ll thee polems. [35 pts] 1. A ectngul ox hs sides of lengths, nd c z x c [1] ) Fo the Diichlet polem in the inteio

More information

Radial geodesics in Schwarzschild spacetime

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

More information

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1 Week : DTMC Alictions Rnking Web ges & Slotted ALOHA etwok efonce - Outline Aly the theoy of discete tie Mkov chins: Google s nking of web-ges Wht ge is the use ost likely seching fo? Foulte web-gh s Mkov

More information

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s: Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,

More information

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

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

More information

Research Article Modeling of Thermal Distributions around a Barrier at the Interface of Coating and Substrate

Research Article Modeling of Thermal Distributions around a Barrier at the Interface of Coating and Substrate Abstct nd Applied Anlysis Volume 23, Aticle ID 968464, 8 pges http://dx.doi.og/.55/23/968464 Resech Aticle Modeling of Theml Distibutions ound Bie t the Intefce of Coting nd Substte Ali Shin Deptment of

More information

PH126 Exam I Solutions

PH126 Exam I Solutions PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium

More information

Lecture 10. Solution of Nonlinear Equations - II

Lecture 10. Solution of Nonlinear Equations - II Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution

More information

Integrals and Polygamma Representations for Binomial Sums

Integrals and Polygamma Representations for Binomial Sums 3 47 6 3 Jounl of Intege Sequences, Vol. 3 (, Aticle..8 Integls nd Polygmm Repesenttions fo Binomil Sums Anthony Sofo School of Engineeing nd Science Victoi Univesity PO Box 448 Melboune City, VIC 8 Austli

More information

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

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

More information

Electric Potential. chapter

Electric Potential. chapter chpte 25 Electic Potentil 25.1 Electic Potentil n Potentil Diffeence 25.2 Potentil Diffeence in Unifom Electic Fiel 25.3 Electic Potentil n Potentil Enegy Due to Point Chges 25.4 Otining the Vlue of the

More information

On Some Hadamard-Type Inequalıtıes for Convex Functıons

On Some Hadamard-Type Inequalıtıes for Convex Functıons Aville t htt://vuedu/ Al Al Mth ISSN: 93-9466 Vol 9, Issue June 4, 388-4 Alictions nd Alied Mthetics: An Intentionl Jounl AAM On Soe Hdd-Tye Inequlıtıes o, Convex Functıons M Ein Özdei Detent o Mthetics

More information

Review of Mathematical Concepts

Review of Mathematical Concepts ENEE 322: Signls nd Systems view of Mthemticl Concepts This hndout contins ief eview of mthemticl concepts which e vitlly impotnt to ENEE 322: Signls nd Systems. Since this mteil is coveed in vious couses

More information

Solutions to Midterm Physics 201

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

More information

EXPANSION OF LIQUIDS

EXPANSION OF LIQUIDS EXPNSION OF LIQUIDS. block of woo is flotin on wte t C with cetin volume V bove wte level. The tempetue of wte is slowly ise fom C to C. How the volume V chne with the ise of tempetue ) V will emin unchne

More information

Electric Potential Energy

Electric Potential Energy Electic Ptentil Enegy Ty Cnsevtive Fces n Enegy Cnsevtin Ttl enegy is cnstnt n is sum f kinetic n ptentil Electic Ptentil Enegy Electic Ptentil Cnsevtin f Enegy f pticle fm Phys 7 Kinetic Enegy (K) nn-eltivistic

More information

igid nd non-leky two-comptment building. Yu et l [8] developed non-line govening equtions by consideing the effect of bckgound lekge. Howeve, thee e n

igid nd non-leky two-comptment building. Yu et l [8] developed non-line govening equtions by consideing the effect of bckgound lekge. Howeve, thee e n The Seventh Intentionl Colloquium on Bluff Body Aeodynmics nd Applictions (BBAA7) Shnghi, Chin; Septembe -, Coupled vibtion between wind-induced intenl pessues nd lge spn oof fo two-comptment building

More information

A, Electromagnetic Fields Final Exam December 14, 2001 Solution

A, Electromagnetic Fields Final Exam December 14, 2001 Solution 304-351, Electrognetic Fiels Finl Ex Deceer 14, 2001 Solution 1. e9.8. In chpter9.proles.extr.two loops, e of thin wire crry equl n opposite currents s shown in the figure elow. The rius of ech loop is

More information

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

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

More information

15. SIMPLE MHD EQUILIBRIA

15. SIMPLE MHD EQUILIBRIA 15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

More information

Scientific Computing & Modelling NV, Vrije Universiteit, Theoretical Chemistry, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands c

Scientific Computing & Modelling NV, Vrije Universiteit, Theoretical Chemistry, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands c Electonic Supplementy Mteil (ESI) fo Physicl Chemisty Chemicl Physics. This jounl is The Royl Society of Chemisty 2014 Suppoting Infomtion fo: Pedicting phosphoescent lifetimes nd zeo-field splitting of

More information

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

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

More information

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton. PHY 8 Test Pactice Solutions Sping Q: [] A poton an an electon attact each othe electically so, when elease fom est, they will acceleate towa each othe. Which paticle will have a lage acceleation? (Neglect

More information

Friedmannien equations

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

More information

Introductions to ArithmeticGeometricMean

Introductions to ArithmeticGeometricMean Intoductions to AitheticGeoeticMen Intoduction to the Aithetic-Geoetic Men Genel The ithetic-geoetic en eed in the woks of J Lnden (77, 775) nd J-L Lgnge (784-785) who defined it though the following quite-ntul

More information

Electricity & Magnetism Lecture 6: Electric Potential

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

More information

Physics 1502: Lecture 2 Today s Agenda

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

More information

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates,

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates, MAE B Homewok Solution #6 Winte Quate, 7 Poblem a Expecting a elocity change of oe oe a aial istance, the conition necessay fo the ow to be ominate by iscous foces oe inetial foces is O( y ) O( ) = =

More information

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

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

More information

N igerian Journal of M athematics and Applications V olume 24, (2015),

N igerian Journal of M athematics and Applications V olume 24, (2015), N igeian Jounal of M athematics an Applications V olume 24, 205), 228 236 c N ig. J. M ath. Appl. http : //www.kwsman.com Flow of an Incompessible MHD Thi Gae Flui Though a Cylinical Pipe with Isothemal

More information

Chapter 21: Electric Charge and Electric Field

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

More information

On the Eötvös effect

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

More information

Angular Contac t Ball Bearings

Angular Contac t Ball Bearings High Pecision Angul Contct ll eings Stn Seies 1 Angul Contct ll eings Ult High-Spee Angul Contct ll eings Angul Contct ll eings Pt 4 1. ANGULAR CONTACT ALL EARINGS High Pecision Angul Contct ll eings (Stn

More information

Chapter 1. Model Theory

Chapter 1. Model Theory Chte odel heo.. Intoduction Phsicl siultion of hdulic henoenon, such s the flow ove sillw, in the lboto is clled hsicl odel o onl odel. Potote is the hdulic henoen in the ntue like the sillw ove d. odels

More information

Energy Dissipation Gravitational Potential Energy Power

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

More information

Multi-Electron Atoms-Helium

Multi-Electron Atoms-Helium Multi-lecto Atos-Heliu He - se s H but with Z He - electos. No exct solutio of.. but c use H wve fuctios d eegy levels s sttig poit ucleus sceeed d so Zeffective is < sceeig is ~se s e-e epulsio fo He,

More information

4. Compare the electric force holding the electron in orbit ( r = 0.53

4. Compare the electric force holding the electron in orbit ( r = 0.53 Electostatics WS Electic Foce an Fiel. Calculate the magnitue of the foce between two 3.60-µ C point chages 9.3 cm apat.. How many electons make up a chage of 30.0 µ C? 3. Two chage ust paticles exet a

More information

Quantum Mechanics I - Session 5

Quantum Mechanics I - Session 5 Quantum Mechanics I - Session 5 Apil 7, 015 1 Commuting opeatos - an example Remine: You saw in class that Â, ˆB ae commuting opeatos iff they have a complete set of commuting obsevables. In aition you

More information

PX3008 Problem Sheet 1

PX3008 Problem Sheet 1 PX38 Poblem Sheet 1 1) A sphee of dius (m) contins chge of unifom density ρ (Cm -3 ). Using Guss' theoem, obtin expessions fo the mgnitude of the electic field (t distnce fom the cente of the sphee) in

More information

Creep modeling in functionally graded rotating disc of variable thickness

Creep modeling in functionally graded rotating disc of variable thickness Jounl of Mechnicl Science nd Technology 4 () () ~3 www.spingelink.com/content/738-494x DOI.7/s6--87- Ceep modeling in functionlly gded otting disc of vile thickness D. Deepk, V. K. Gupt,* nd A. K. Dhm

More information

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

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

More information

Newton s Shell Theorem via Archimedes s Hat Box and Single-Variable Calculus

Newton s Shell Theorem via Archimedes s Hat Box and Single-Variable Calculus Newton s Shell Theoem vi Achimees s Ht Box n Single-Vible Clculus Pete McGth Pete McGth (pjmcgt@upenn.eu, MRID955520) eceive his Ph.D. fom Bown Univesity n is cuently Hns Remche Instucto t the Univesity

More information

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

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

More information

Mark Scheme (Results) January 2008

Mark Scheme (Results) January 2008 Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question

More information

CRYSTALLOGRAPHY OF COAXIAL AND SCROLL NANOTUBES OF ARBITRARY COMPOSITION

CRYSTALLOGRAPHY OF COAXIAL AND SCROLL NANOTUBES OF ARBITRARY COMPOSITION CHEMISTRY & CHEMICAL TECHNOLOGY Vol. 9, No. 1, 15 Cheisty Oleg Figovsky 1, Dity Pshin, Zuf Khlitov n Din Vleev CRYSTALLOGRAPHY OF COAXIAL AND SCROLL NANOTUBES OF ARBITRARY COMPOSITION 1 Intentionl Nnotechnology

More information

Simple analytical solutions for underground circular and elliptical openings

Simple analytical solutions for underground circular and elliptical openings Simple nlyticl solutions fo undegound cicul nd ellipticl openings Autho: Pof. D. hbil. Heinz Konietzky, (TU Begkdemie Feibeg, Geotechnicl Institute) 1 Intoduction... Anlyticl solutions in D... 3.1 Intenl

More information