Analysis of Stress in PD Front End Solenoids I. Terechkine
|
|
- Janis Griffin
- 5 years ago
- Views:
Transcription
1 TD Sepembe 0, 005 I. Ioducio. Aalysis of Sess i PD Fo Ed Soleoids I. Teechkie Thee ae fou diffee ypes of supecoducig soleoids used fo beam focusig i he Fod Ed of he Poo Dive. Table 1 gives a idea abou equiemes fo ceai paamees of he soleoids (some quesio maks i he able eflec lack of udesadig of he siuaio ih he available space a he mome. Table 1 DTL MEBT SSR DSR Paamee Boe diamee 5 mm 5 mm 30 mm 30 mm Boe ype am am cold cold Field Iegal FI B dl (T cm Recommeded Bm (T Leff Bm Available eio gap (cm 5 (18? (18? 39 (18? 30 (3? The ceal mageic field is i he age (5 6 T he logiudial field pofile is quasi-ecagula. I eal siuaio, his is fa fom beig ue, ad o each equied Field Iegal (FI ihi available space ad ih sufficie magi fo sable ok, mageic field segh i he coil i some cases mus be as high as ~8.5 T. Wih his field level, sess developed i he sysem leads o defomaio ha ca esul i coil bouday sepaaio ad subseque coil quechig. Tadiioal mehod of solvig his poblem is applyig o he poblem some of ko echiques of sess maageme. Mehods of he sess maageme mus be aalyzed i cojucio ih he soleoid assembly echique befoe pooypes of he devices ae buil. A coveie mea of sess aalysis duig his developme sage ould be vey useful o acceleae he pocess of maeial ad geomey choice. Afe his choice is made, adiioal meas of sess aalysis, like usig ANSIS code, ca be used fo veificaio of sess maageme soluio ad adjusme of desig feaues. Because of elaively simple geomey of he soleoids, hich ae axially symmeical, i is possible o employ geeal mehods of aalysis based o diec soluio of diffeeial equaios ha descibe mechaical behavio of he sysem. I spie of is axial symmey, i he adial diecio sucue of he soleoids ca be quie complex ad usually icludes beam pipe, bobbi, epoxy-impegaed coil (maybe seveal layes, sepaaed by addiioal poecio shells, a colla, ad a seel yoke. Besides, duig idig sage, ieviable ie esioig povides addiioal pe-sess, ha mus be ake io he accou. As a esul, sysem of equaios descibig he sysem becomes quie lage, ad difficul fo diec aalysis. Neveheless, ih some simplificaios, his sysem of equaios ca be solved usig MahCad eviome, visualized, ad aalyzed. This oe povides a descipio of he appoach o he aalysis of sess maageme soluio fo supecoducig soleoids. Examples i his oe do o eflec eal desig of ay of meioed soleoid; hey ahe help o illusae ceai aspecs of he appoach. 1
2 TD Sepembe 0, 005 II. Basic Equaios Descipio of mechaical behavio of ay solid media is based o equaios of equilibium ad elasiciy. Equilibium codiio i a cylidical sysem ih volume foce of ay aue ca be ie as: d ( σ σ F(, /1/ d hee σ is omal sess, σ is ageial sess, ad F( is a exeal foce applied o a ui of volume (e.g. 1.0 m 3 of he maeial. Elasiciy equaios descibe defomaio of maeial subjec o omal ad ageial sess: u σ µσ, E, // du σ µσ d E hee µ is Poisso s aio. Combiig /1/ ad //, geeal equaio of defomaio ca be obaied: d u 1 du u µ + F( /3/ d d E Geeal soluio of he homogeeous pa of his diffeeial equaio (volumeic foce is zeo is ell ko [1]: C u h C1 +, /4/ hee C1 ad C ae cosas ha ca be foud by aalyzig bouday codiios. To fid a paicula soluio of he o-homogeeous equaio /3/, e eed o ko ha he volumeic foce F( looks like. I he case of mageic foce, F( j B( /5/ hee j (A/m is cue desiy i he coil idig. Radial pofile of mageic field ide he body of he coil i soleoids is close o liea, ad i he media plae oly z-compoe exiss, so e ill appoximae i usig he ex fom: (1 αβ (1 β Ro B ( Bi /6/ α hee α R i /R o is he aio of ie ad oue adii R i ad R o, ad β B o /B i is a aio of mageic field levels o he ouside ad ide bode of a paicula laye. As i is easy o check, B(R i B i, ad B(R o β B i. Value of B i mus be foud fo each laye by solvig coespodig mageosaic poblem aalyically (e.g. see [] o by usig a appopiae solve. I ou case, i is coveie o epese his value of mageic field o he ide bode of laye by iig: Bi, K I, /7/
3 TD Sepembe 0, 005 hee I is ie cue. This cue is usually kep cosa eve if ie diamee is diffee fo diffee layes. Ioducig ie coss-secio aea S ad coil compacio faco k S /S c, e ca ie do expessio fo he volumeic foce (fo each cue-cayig laye: kk αβ β F ( I S α R o α /8/ The, o o-homogeeous equaio /3/ looks like d u 1 du u + C01 + C0 d d /9/ µ kki αβ µ kki β ih C 01, ad C 0. E S α E S α Paial soluio of equaio /9/ ca be foud as: u p C01 + C0 /10/ 3 8Ro The he geeal soluio of his equaio is: C u C1 + C01 + C0 /11/ 3 8Ro So, fo each laye of he soleoid (ih o ihou cue, equaio /11/ gives a aalyical soluio fo defomaio. All he coefficies i equaios /9/ /11/ ae uique fo each laye. C0 1 ad C0 become ko he coil dimesios ae posulaed; C1 ad C mus be foud fo each laye by applyig coespodig bouday codiios, hich usually meas koig sess o sess elaioship o boudaies. Koig u, omal ad ageial (hoop sess ca be deived fom //: E du u σ + µ /1/ µ d ad E u du σ + µ /13/ µ d By combiig /11/, /1/, ad /13/, e ge quie geeal aalyical expessios fo omal ad ageial sess i ay laye of he soleoid: E C C0 1 C0 σ ( C1 (1 + µ (1 µ ( + µ + (3 + µ /14/ µ 3 8Ro E C C0 1 C0 σ ( C1 (1 + µ + (1 µ (1 + µ + (1 + 3µ /15/ µ 3 8Ro No e ca use /14 ad /15/ o fid uko C1 ad C fo each laye by solvig a sysem of algebaic equaios ha defie bouday codiios. This sysem is made by combiig coiuiy equaios fo omal sess a he boudaies beee layes m ad m+1 : σ σ /16/ m _ m+1 _ ad iefeece equaios a he same boudaies: R o 3
4 TD Sepembe 0, 005 u m u m +1 δ /17/ Hee δ has sese of a gap beee he o layes, so fo ovelappig layes i mus be egaive: δ < 0. I ohe ods, expessio /17/ meas ha afe assembly, he ie adius of he oue laye is equal o he oue adius of he ie laye: R m+1 + u m+1 R m + u m o R m+1 R m + δ. /18/ Fo ay umbe of layes, e have sufficie amou of algebaic equaios o fid coefficies C1 ad C fo each laye. Oe impoa pacical aspec is ha hile assemblig a mulilaye soleoid, ovelap ca oly be measued elaively o aleady assembled sub-sucue. So, o eadily available ifomaio exiss abou he fee sae ovelap ad meas mus be foud o obai his ifomaio. This evaluaio ill be a muli-sep pocess epeaed as may imes as he umbe of layes is. Defomaio u fo ay laye is defied elaive o he fee o udisubed posiio if he laye, hich ofe ca o be measued diecly. A algoihm o fid he fee sae ovelap is descibed belo. Sep 1: Addig laye # o he laye #1 R1o_0 is he oue adius of he laye #1 befoe addig he laye #. Fo he laye #1 i is he same as he fee sae posiio. Iiial ie adius of he laye # Ri_0 R1o_0 + δ1. /19/ Afe he o layes ae assembled, Ri_1 R1o_1. A his sep, Ri_1 Ri_0 + u(ri R1o_0 + δ1 + u(ri /0/ ad R1o_1 R1o_0 + u1(r1o. /1/ Combiig he las o equaios, e come o ha /17/ equies a he bouday beee he o layes. Afe solvig he sysem of equaios /14/ - /17/, e ca fid Ro_1 Ro_0 + u(ro. // Ro_1 becomes a efeece adius fo deemiig he ovelap beee he layes # ad #3. I he case of oud layes (see belo, koig u(ro allos ecalculaio of a fee sae posiio of he laye s bouday. Sep : Addig laye #3 o he assembly (#1+# Iiial ie adius of he laye 3 R3i_0 Ro_1 + δ3. /3/ Hee ovelap δ3 is measued elaively o he posiio of he oue bouday of he laye # afe i is added o #1. Fo sess evaluaio, oe eed o ko a fee sae ovelap, ha is he ovelap beee he udisubed machig boudaies of he layes: δ3_fee R3i_0 - Ro_0 δ3 + u(ro /4/ No e have hee layes ih o uko coefficies defiig defoma io i eac h of hem. So, e eed six equaios o fid a soluio. Fou equaios ill be made by defiig omal sess a he boudaies (equaios /16/, ad o equaios /17/ ill sae ha boudaies of he iefeig layes ae fused ogehe: Ri_ R1o_ ad R3i_ Ro_. Whe he sysem of equaios is solved e ko defomaios i each layes, icludig he las oe. This allos o fid a efeece adius fo deemiig he ovelap beee he layes #3 ad #4: R3o_ R3o_0 + u3(r3o /5/ 4
5 TD Sepembe 0, 005 The pocedue ca be epeaed as may imes as he umbe of layes is. Alhough mahemaically e ca fid a soluio, i ca be oo vague if e do o exa cly ko popey of all maeials e ae usig o build a soleoid. Some of hem ae composie maeials ih aisoopic popeies depedig o a echique used fo soleoid assembly, so i is ecessay be vey caeful i usig available daa. Hee e ll y o make pelimiay esimae of ha hese popeies ca look like, bu oly pope pooypig ca give us coec umbes. This is also ue fo hemal coacio coefficies of all maeials. This kid of daa is scace ad ofe ueliable fo composie maeials, so ou o judgme is eeded. Oce maeial popeies ae ko, oe ca use he model developed above o make seveal ieaios appoachig a soluio by chagig maeials ad geomeical paamees of a soleoid. III. Composie maeials i soleoid Some aeas of he assembled soleoid have aisoopic popeies ha deped o fabicaio echique. These aeas ae a coil, hich is oud usig NbTi ie ih some esio ad afe idig is impegaed ih epoxy, ad a sepaaio/poecio laye ha is oud usig fibeglass ape above he coil ad also impegaed ih epoxy. I boh cases, oud layes of he coil ae ude esio ad cued epoxy is o sessed. Duig coolig do o he pe-sess is applied, boh oud base ad cued epoxy ok simulaeously o fom a uified composie objec. I his pa, eleva popeies of composie sucue ill be evaluaed based o ko popeies of used maeials. Ho he coil is oud has a big impac of ha popeies o expec. We ill sa ih a egula layeed idig pae sho i Figue 1 belo. Figue 1: Sucue of oud ad impegaed coil. Pae 1 Hee, o ceae a base fo idig each ex laye, a elaively hick film mus be used fo laye sepaaio. This sucue suggess diffee mechaical popeies alog ie ad acoss he layes of idig. Alog he legh of ie (ageial diecio all pas of he coil coss secio ae acig i paallel, so effecive elogaio modulus of he sucue i his diecio is defied by elaive aea of NbTi ie ad ulaig maeial. If (fo simplificaio o accep ha he hee ulaig maeials used i he assembly have simila mechaical popeies (ha of cued epoxy, effecive elogaio modulus ca be foud as 5
6 TD Sepembe 0, 005 E E S + E S /6/ S + S Usig E 100 GPa, E 15 GPa, ad akig ie ad ulaio dimesios fom Figue 1, e ge effecive elogaio modulus i GPa: E E π D 4 bae + E [ D ( D + π Dbae ] D ( D + Hee D bae ad D ae diamees of bae ad ulaed sad. Compacio faco of his coil is 0.57, so epoxy fillig adds abou 10% o ha idig ihou fillig ould sho he seched. Pesece of epoxy is cucially impoa he coil is ude compessio: epoxy fillig ad bodig ues ha he sucue behaves like a solid body. Acoss he layes of idig (i omal diecio hee is moe complicaed combiaio of ieacio paes. The aio of he compoe coss-secios chages coiuously i he omal diecio (coodiae h. We ill evaluae popeies of his composie by aalyzig seial coecio of may hi layes ih coss secio shaed by ie ad ulaio (see Figue. I each laye, effecive elogaio modulus, as befoe, is defied by elaive aea of he o compoes of he sucue ha ac i paallel (simplificaio agai, so his effecive modulus vaies i he omal diecio. /7/ Figue : Illusaio o evaluaio of mechaical popeies of coil sucue i asvese diecio Takig io he accou /6/, ad all vaiable desigaios fom Figue, e ca ie do: h E R h E R + R + (1 R Eeff ( h if h R /8-a/ R + ad E ( h if h > R /8-b/ eff E Global elasiciy modulus ca be foud by akig iegal: R+ + d / 1 1 dh E R + + d / E ( h eσ 0 eff /9/ 6
7 TD Sepembe 0, 005 Evaluaio usig ko popeies of ie ad epoxy ih 46 µm ad d 100 µm gives E eσ 39 GPa. Aohe mode of coil idig is possible he hi ad flexible ulaio is used beee he layes of idig ha ca o peve ies fom fidig hee posiio i oches beee ies of he peviously oud laye (see Figue 3. The oly fucio of his ulaio is o povide addiioal poecio aga shos i he coil duig coolig do: Figue 3: Sucue of oud ad impegaed coil. Pae This ay highe desiy of idig ca be obaied, ha esuls i highe aveage elasiciy modulus. This modulus ca be evaluaed as i as doe fo he pae 1, bu ead of usig +d/ i Figue ad iegal expessio, oe mus use d (see Fig. 4, ha ca be foud geomeically ad depeds o he ulaio hickess, hich is sho as beig 50 µm i Figue 3. Wih his ulaio hickess, d 14.3 µm if he es of he paamees coespod o ha as used fo he pevious case of Pae 1 idig. Figue 4: Pae cell used fo aveage elasiciy modulus evaluaio. Calculaios usig /8/ ad /9/ give i his case elasiciy modulus i asvese diecio of ~58 GPa. I he azimuhal diecio, alog ies, oe mus apply /6/ o fid i GPa: E π R + E [( R + ( R + d π ] 4 bae R 4 bae E 7.6 /30/ ( R + d ( R + Compacio faco i his case is ~ Resuls of his aalysis ca be compaed ih es esuls i [3] o epoxy impegaed coils made of Nb 3 S ad NbTi usig ie ih ecagula coss-secio. Elogaio module as measued i he age GPa. Ohe ok of he same auhos fom NHMFL, [4], also povides some daa elaed o mechaical behavio of oud coils. Wih packig faco of 0.8 (compae ih 0.56 ad 0.68 i ou case, aveage modulus fo coil sechig as ~ 95 GPa. Fo coil compessio i adial diecio, aveage modulus as oly ~ 50 GPa. 7
8 TD Sepembe 0, 005 Resuls of his simple aalysis ad exisig daa sho ha aeio mus be paid o ho coil is fabicaed. Aohe oe: If idig ih glass ape ad subseque impegaio ih epoxy is used above he coil, simila cosideaios ca be used o fid popeies of he compoud maeial. Reliable glass ape (sad segh ad desiy ifomaio is eeded o make his ok havig sese. As a fis appoach, G-10 i he ad diecio daa ca be used. IV. Effecs of coolig do A oom empeaue, dimesios of all pas i he soleoid ca be ell coolled befoe hey ae added o he assembly. Afe seveal coceic pas ae assembled ogehe ih some ovelap, oe does o have immediae cool o he dimesio of pas because of defomaio (alhough dimesios sill ca be calculaed. We ill assume ha he oue suface of each pa is machied afe i is added o he assembly; so ha he as assembled oue diamee is ko evey ime. The he equied ie adius of he ex pa ca be foud usig /18/ if he ovelap δ beee he o layes is posulaed. The equaios /16 ad /17/, ha model he assembly ad ae descibed above, ae based o he diffeeial equaio fo defomaio /3/. As a esul, hee is o eed o calculae exac values of adii; sligh chage of he adius of each bouday adds a coecio o he esul popoioal o u/r. The value of ovelap δ is impoa hough because i defies he iiial defomaio. So, he goal is o fid e values of ovelap fo each couple of laye afe coolig do. Oe of ays of doig i is o use esuls of he sess aalysis a oom empeaue ha povides us ih koledge of he fee dimesios of each laye afe e fid coespodig values of defomaio. Koig he fee o udisubed posiios, e ca apply o hem he ko hemal coacio popeies o fid udisubed dimesios a 4 K. I is saighfoad he o fid ovelap a each bouday ad poceed o solvig he sysem of equaios /14/ - /17/ ih (maybe modified sucual popeies of used maeials. Aohe ay is o eevaluae ovelap ifomaio based o he fee ovelap daa ko fom he oom empeaue case. Fo he iefeece beee he layes m ad, oe ca ie, simila o /17/: (300K (300K δ R R R (1 χ R (1 χ m i mo i _ fee mo _ fee (300K o δ m δ m Rmo ( χ χ m /31/ hee χ m ad χ ae iegaed coacio coefficies of he layes i he empeaue age fom 300 K o 4 K, R mo is he oue adius of he ie pa, ad idexes mo ad i efe o he machig oue ad ie adii of he layes m ad. So, agai, he oly hig ha is eeded hee is daa of fee ovelap a oom empeaue ha ca be foud as as descibed above. Afe e ko ovelap daa, he sysem of equaios /14/ - /17/ mus be solved oly oce o give all he ifomaio e eed. m 8
9 TD Sepembe 0, 005 V. Effec of ie esioig duig idig. Wie esioig is immie duig idig. Quesio aises o ha impac his esioig has o he soleoid mechaical behavio ad hehe his esioig ca be useful hile solvig he sess maageme poblem. Le s coside a laye of ie oud ih esio foce F above he bobbi o peviously oud laye. We ca ea his idig pocess as addig a solid cylidical laye o he exisig sucue ih he ovelap δ a oom empeaue ha coespods o he esio foce: F δ E S, /3/ Whee E is Youg s modulus ad S is coss-secio aea of he sad (ie. Each ex laye ill have diffee iefeece because of diffee adius R ad (maybe esio foce F. Fo each oud laye, he same basic equaio /3/ ill ok ih simila se of bouday codiios. Maeial popeies mus be used caefully hile solvig hese equaios. A his sage, liquid epoxy o o epoxy is used, so oly ie ad ielaye ulaio mus be ake io he accou hile evaluaig sucual popeies of oud layes. Afe epoxy is cued, e values of maeial popeies ad modified hemal coacio coefficie (see belo mus be used o aalyze sess afe coolig do. The appoach o sess calculaio a oom empeaue developed i he pevious chapes is fully applicable because a each idig sep e ko he oue adius of he las oud laye ad he ie adius of he ex laye. Duig coolig do, because hemal popeies of he layes of idig ae ideical, ovelap ill chage oly because of defomaio chage due o sess edisibuio, so agai he same algoihm ca be used. VI. Mechaical behavio of oud ad epoxy impegaed coil Themal coacio of coil sucue is he issue o pay aeio o. If coil s ie is oud ih esio ad he impegaed ih epoxy ad cued, a oom empeaue cued epoxy is usessed hile he coil ie is seched. So, e equilibium ie adius a oom empeaue mus be foud ha coespods o he case he his laye of coil assembly is emoved fom a bobbi (o pevious laye i as assemble o. Koig his adius allos oe o fid iefeece eeded o calculae displacemes ad sess. Aveage popeies of he maeial ca be foud i a ay simila o ha as used i he chape 3 above, so fo each maeial e ill use aveaged value of elasiciy modulus. Afe idig a laye of ie ih esio F, icease of adius is defied by /3/: F F EW SW Whe oud ad cued laye is emoved fom he bobbi, i coacs eleasig he esio uil foce equilibium is eached beee compessed epoxy fillig ad seched ie. Ne equilibium posiio ca be foud fom equaio: eq F eq EW SW ES /33/ 9
10 TD Sepembe 0, 005 Hee eq shos icease of ie adius of he oud coil ih cued epoxy afe i is emoved fom he bobbi i as oud o elaive o ha ihou epoxy; S is ulaio coss-secio pe oe u f he idig. Fom /33/: eq F /34/ EW SW EW SW (1 + ES A his posiio, emaiig ie sechig foce pe ie is F F /35/ EW SW 1+ ES ad adjused ovelap F δ eq F /36/ E S + E S Mechaical behavio of he composie sucue, amely displaceme elaive he e equilibium posiio, ca be deived based o he ko popeies of he compoes makig he sucue ad he e equilibium posiio. If displaceme elaive o his posiio is x, coespodig foce ca be calculaed as: x x + eq F ( x + eq S Eeff EW S Σ W ES /37/ Usig /31/, e ca simplify his expessio o ie: S Σ Eeff EW SW + ES /38/ ha oe could expec jus lookig a /36/. W W VII. Themal coacio of epoxy impegaed sucues Fo supecoducig soleoids, i is also impoa o ko hemal coacio popeies of composie maeials o calculae ovelap a 4K. We ca make a esimae usig he appoach simila o ha as used above. Duig coolig do, due o diffee coefficies of coacio of coil ie ad epoxy, oe ca expec edisibuio of ieal sess ad chage of he equilibium posiio of ie ad oue adii. A oom empeaue, ie adius of he coil i fee codiio is defied by he adius of he bobbi b, ovelap δ, hich is a fucio of ie esio ( b + δ, ad he sechig foce of compessed fillig maeial (epoxy ih he ie adius of b (hich is he oue adius of he bobbi. Afe coolig do, fee sae dimesios of he idig ad of he epoxy fillig chage: 4K (1 χ ( b + δ (1 χ /39/ ad 4K (1 χ, /40/ epo Ne equilibium posiio of he ie adius is commo boh fo idig ad fo epoxy fillig. Also ieal foce mus be compesaed, so b epo 10
11 TD Sepembe 0, 005 eq ep ep eq N i S E W W N i S E hee N is he ieal foce of ieacio beee ie ad epoxy fillig. Usig /39/, /40/, ad /41/, ad akig io he accou /3/, e ge he ex expessio fo he e equilibium adius a 4 K: SW EW χ + S E χ + F eq b 1 /4/ SW EW + S E The secod em i he paeheses above is he effecive iegaed hemal coacio coefficie of a composie maeial. As befoe, S icludes o oly epoxy, bu also ielaye ulaio. Youg s modulus E W of he sad mus be ake fo he logiudial diecio because e deal hee ih laye elogaio ha aslaes io coespodig adius chage. Usig ypical daa oe ca ge: S E N, χ 1.9 * 10-3 S E N, χ 4.3 * 10-3 S E χ + S E χ 10 N, hich is compaable ih he esio foce usually used duig idig. So, ie esio ca modify maeial shikage i he case he epoxy is used as a fille maeial. Fo sue, coil idig pae (compacio faco ill modify umbes sho above. Takig io he accou compacio faco, expessio fo he effecive shikage coefficie ca be ie i he fom: k E F χ + χ + k E E S χ eff /43/ k E 1+ k E Fo k 0.63, ih F 50 N, effecive shikage χ eff Wih F 0, effecive shikage χ eff If he coil spool is made of sailess seel (χ , i ould be a good idea o apply some esio o ie o o lose sess duig coolig do. VIII. Coclusio This oe foms a base fo sess aalysis of supecoducig soleoids: 1. Basic equaios ee deived o aalyze sess ad defomaios;. Expessios ee foud o esimae mechaical popeies of composie maeials like oud ad epoxy impegaed Nb-Ti coil; 3. Algoihm of sess aalysis a LHe empeaue as suggesed; 4. Mehod of sess aalysis he ie esio is used duig idig as suggesed 5. Themal shikage of epoxy impegaed coil as aalyzed o sho ha i depeds o coils idig paes. /41/ 11
12 TD Sepembe 0, 005 This se of algoihms ill be applied ad deived expessios ill be used o make a choice of maeials ad assembly echiques of supecoducig focusig coils i he PD fo ed. IX. Refeeces [1] J.P. De Haog, Segh of maeials, Dove Publicaios, Ic, N-Y, [] D. Buce Mogomey, Soleoid mage desig. The mageic ad mechaical aspecs of esisive ad supecoducig sysems. Wiley-Iesciece, NY, [3] I. Dixo, e al. Axial Mechaical Popeies of Epoxy Impegaed Supecoducig Soleoids a 4. K, IEEE Tas. o Applied Supecoduciviy, v. 10, No. 1, Mach 000 [4] I. Dixo, e al, Mechaical Popeies of Epoxy Impegaed Supecoducig Soleoids, IEEE Tas. o Mageics, v. 3, No. 4, July
Supplementary Information
Supplemeay Ifomaio No-ivasive, asie deemiaio of he coe empeaue of a hea-geeaig solid body Dea Ahoy, Daipaya Saka, Aku Jai * Mechaical ad Aeospace Egieeig Depame Uivesiy of Texas a Aligo, Aligo, TX, USA.
More informationCapítulo. of Particles: Energy and Momentum Methods
Capíulo 5 Kieics of Paicles: Eegy ad Momeum Mehods Mecáica II Coes Ioducio Wok of a Foce Piciple of Wok & Eegy pplicaios of he Piciple of Wok & Eegy Powe ad Efficiecy Sample Poblem 3. Sample Poblem 3.
More informationTransistor configurations: There are three main ways to place a FET/BJT in an architecture:
F3 Mo 0. Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils o povide biasig so ha he asiso has he coec
More informationComparing Different Estimators for Parameters of Kumaraswamy Distribution
Compaig Diffee Esimaos fo Paamees of Kumaaswamy Disibuio ا.م.د نذير عباس ابراهيم الشمري جامعة النهرين/بغداد-العراق أ.م.د نشات جاسم محمد الجامعة التقنية الوسطى/بغداد- العراق Absac: This pape deals wih compaig
More informationECSE Partial fraction expansion (m<n) 3 types of poles Simple Real poles Real Equal poles
ECSE- Lecue. Paial facio expasio (m
More informationINF 5460 Electronic noise Estimates and countermeasures. Lecture 13 (Mot 10) Amplifier Architectures
NF 5460 lecoic oise simaes ad couemeasues Lecue 3 (Mo 0) Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils
More informationThe Central Limit Theorems for Sums of Powers of Function of Independent Random Variables
ScieceAsia 8 () : 55-6 The Ceal Limi Theoems fo Sums of Poes of Fucio of Idepede Radom Vaiables K Laipapo a ad K Neammaee b a Depame of Mahemaics Walailak Uivesiy Nakho Si Thammaa 86 Thailad b Depame of
More information6.2 Improving Our 3-D Graphics Pipeline
6.2. IMPROVING OUR 3-D GRAPHICS PIPELINE 8 6.2 Impovig Ou 3-D Gaphics Pipelie We iish ou basic 3D gaphics pipelie wih he implemeaio o pespecive. beoe we do his, we eview homogeeous coodiaes. 6.2. Homogeeous
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationCalculation of maximum ground movement and deformation caused by mining
Tas. Nofeous Me. Soc. Chia 1(011) s5-s59 Calculaio of maximum goud moveme ad defomaio caused by miig LI Pei xia 1,, TAN Zhi xiag 1,, DENG Ka zhog 1, 1. Key Laboaoy fo Lad Eviome ad Disase Moioig of Sae
More informationOn imploding cylindrical and spherical shock waves in a perfect gas
J. Fluid Mech. (2006), vol. 560, pp. 103 122. c 2006 Cambidge Uivesiy Pess doi:10.1017/s0022112006000590 Pied i he Uied Kigdom 103 O implodig cylidical ad spheical shock waves i a pefec gas By N. F. PONCHAUT,
More informationFresnel Dragging Explained
Fresel Draggig Explaied 07/05/008 Decla Traill Decla@espace.e.au The Fresel Draggig Coefficie required o explai he resul of he Fizeau experime ca be easily explaied by usig he priciples of Eergy Field
More informationOutline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem
adial diffsio eqaio Febay 4 9 Diffsio Eqaios i ylidical oodiaes ay aeo Mechaical Egieeig 5B Seia i Egieeig Aalysis Febay 4, 9 Olie eview las class Gadie ad covecio boday codiio Diffsio eqaio i adial coodiaes
More informationCOST OPTIMIZATION OF SLAB MILLING OPERATION USING GENETIC ALGORITHMS
COST OPTIMIZATIO OF SLAB MILLIG OPERATIO USIG GEETIC ALGORITHMS Bhavsa, S.. ad Saghvi, R.C. G H Pael College of Egieeig ad Techology, Vallah Vidyaaga 388 20, Aad, Gujaa E-mail:sake976@yahoo.co.i; ajeshsaghvi@gce.ac.i
More informationODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003
ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous
More informationBy the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences
Chapte : Theoy of Modula Aithmetic 8 Sectio D Chiese Remaide Theoem By the ed of this sectio you will be able to pove the Chiese Remaide Theoem apply this theoem to solve simultaeous liea cogueces The
More informationRepresenting Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example
C 188: Aificial Inelligence Fall 2007 epesening Knowledge ecue 17: ayes Nes III 10/25/2007 an Klein UC ekeley Popeies of Ns Independence? ayes nes: pecify complex join disibuions using simple local condiional
More informationBig O Notation for Time Complexity of Algorithms
BRONX COMMUNITY COLLEGE of he Ciy Uiversiy of New York DEPARTMENT OF MATHEMATICS AND COMPUTER SCIENCE CSI 33 Secio E01 Hadou 1 Fall 2014 Sepember 3, 2014 Big O Noaio for Time Complexiy of Algorihms Time
More informationThe sudden release of a large amount of energy E into a background fluid of density
10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy
More informationCameras and World Geometry
Caeas ad Wold Geoe How all is his woa? How high is he caea? Wha is he caea oaio w. wold? Which ball is close? Jaes Has Thigs o eebe Has Pihole caea odel ad caea (pojecio) ai Hoogeeous coodiaes allow pojecio
More informationThe Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues
Alied Maheaical Sciece Vol. 8 o. 5 747-75 The No-Tucaed Bul Aival Queue M x /M/ wih Reei Bali Sae-Deede ad a Addiioal Seve fo Loe Queue A. A. EL Shebiy aculy of Sciece Meofia Uiveiy Ey elhebiy@yahoo.co
More informationSpectrum of The Direct Sum of Operators. 1. Introduction
Specu of The Diec Su of Opeaos by E.OTKUN ÇEVİK ad Z.I.ISMILOV Kaadeiz Techical Uivesiy, Faculy of Scieces, Depae of Maheaics 6080 Tabzo, TURKEY e-ail adess : zaeddi@yahoo.co bsac: I his wok, a coecio
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationIdeal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory
Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationComparison between Fourier and Corrected Fourier Series Methods
Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1
More informationAvailable online at J. Math. Comput. Sci. 2 (2012), No. 4, ISSN:
Available olie a h://scik.og J. Mah. Comu. Sci. 2 (22), No. 4, 83-835 ISSN: 927-537 UNBIASED ESTIMATION IN BURR DISTRIBUTION YASHBIR SINGH * Deame of Saisics, School of Mahemaics, Saisics ad Comuaioal
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More information= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n!
0 Combiatoial Aalysis Copyight by Deiz Kalı 4 Combiatios Questio 4 What is the diffeece betwee the followig questio i How may 3-lette wods ca you wite usig the lettes A, B, C, D, E ii How may 3-elemet
More informationClass 36. Thin-film interference. Thin Film Interference. Thin Film Interference. Thin-film interference
Thi Film Ierferece Thi- ierferece Ierferece ewee ligh waves is he reaso ha hi s, such as soap ules, show colorful paers. Phoo credi: Mila Zikova, via Wikipedia Thi- ierferece This is kow as hi- ierferece
More informationS, we call the base curve and the director curve. The straight lines
Developable Ruled Sufaces wih Daboux Fame i iowsi -Space Sezai KIZILTUĞ, Ali ÇAKAK ahemaics Depame, Faculy of As ad Sciece, Ezica Uivesiy, Ezica, Tuey ahemaics Depame, Faculy of Sciece, Aau Uivesiy, Ezuum,
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance
.615, MHD Theoy of Fusion Systems Pof. Feidbeg Lectue 4: Tooidal Equilibium and Radial Pessue Balance Basic Poblem of Tooidal Equilibium 1. Radial pessue balance. Tooidal foce balance Radial Pessue Balance
More informationSUMMATION OF INFINITE SERIES REVISITED
SUMMATION OF INFINITE SERIES REVISITED I several aricles over he las decade o his web page we have show how o sum cerai iiie series icludig he geomeric series. We wa here o eed his discussio o he geeral
More informationStatistical Optics and Free Electron Lasers
Saisical Opics ad Fee leco Lases ialuca eloi uopea XFL Los Ageles UCLA Jauay 5 h 07 Saisical Opics ad Fee leco Lases Theoy ialuca eloi UCLA Los Ageles Jauay 5 h 07 is difficul if o impossible o coceive
More informationOne of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of
Oe of he commo descipios of cuilie moio uses ph ibles, which e mesuemes mde log he ge d oml o he ph of he picles. d e wo ohogol xes cosideed sepely fo eey is of moio. These coodies poide ul descipio fo
More informationEconomics 8723 Macroeconomic Theory Problem Set 2 Professor Sanjay Chugh Spring 2017
Deparme of Ecoomics The Ohio Sae Uiversiy Ecoomics 8723 Macroecoomic Theory Problem Se 2 Professor Sajay Chugh Sprig 207 Labor Icome Taxes, Nash-Bargaied Wages, ad Proporioally-Bargaied Wages. I a ecoomy
More informationF D D D D F. smoothed value of the data including Y t the most recent data.
Module 2 Forecasig 1. Wha is forecasig? Forecasig is defied as esimaig he fuure value ha a parameer will ake. Mos scieific forecasig mehods forecas he fuure value usig pas daa. I Operaios Maageme forecasig
More informationPRESSURE AND PRESSURE DERIVATIVE ANALYSIS FOR PSEUDOPLASTIC FLUIDS IN VERTICAL FRACTURED WELLS
VOL. 7, NO. 8, AUGUST 0 ISSN 89-6608 ARN Joual of Egieeig ad Applied Scieces 006-0 Asia Reseach ublishig Neo (ARN). All ighs eseved..apjouals.com RESSURE AN RESSURE ERIVATIVE ANALYSIS FOR SEUOLASTIC FLUIS
More informationTHE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN
THE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN Musafa KUTANIS Ad Muzaffe ELMAS 2 SUMMARY I is pape, a vaiaio of e FEM wic is so-called geeal subsucue meod is caied
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More information1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)
7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic
More informationF.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mathematics
F.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mahemaics Prelim Quesio Paper Soluio Q. Aemp ay FIVE of he followig : [0] Q.(a) Defie Eve ad odd fucios. [] As.: A fucio f() is said o be eve fucio if
More informationCS 188: Artificial Intelligence Fall Probabilistic Models
CS 188: Aificial Inelligence Fall 2007 Lecue 15: Bayes Nes 10/18/2007 Dan Klein UC Bekeley Pobabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Given a join disibuion, we can
More informationLESSON 15: COMPOUND INTEREST
High School: Expoeial Fuctios LESSON 15: COMPOUND INTEREST 1. You have see this fomula fo compoud ieest. Paamete P is the picipal amou (the moey you stat with). Paamete is the ieest ate pe yea expessed
More informationINVESTMENT PROJECT EFFICIENCY EVALUATION
368 Miljeko Crjac Domiika Crjac INVESTMENT PROJECT EFFICIENCY EVALUATION Miljeko Crjac Professor Faculy of Ecoomics Drsc Domiika Crjac Faculy of Elecrical Egieerig Osijek Summary Fiacial efficiecy of ivesme
More informationProblems and Solutions for Section 3.2 (3.15 through 3.25)
3-7 Problems ad Soluios for Secio 3 35 hrough 35 35 Calculae he respose of a overdamped sigle-degree-of-freedom sysem o a arbirary o-periodic exciaio Soluio: From Equaio 3: x = # F! h "! d! For a overdamped
More informationConsider the time-varying system, (14.1)
Leue 4 // Oulie Moivaio Equivale Defiiios fo Lyapuov Sabiliy Uifomly Sabiliy ad Uifomly Asympoial Sabiliy 4 Covese Lyapuov Theoem 5 Ivaiae- lie Theoem 6 Summay Moivaio Taig poblem i ool, Suppose ha x (
More informationMATH Midterm Solutions
MATH 2113 - Midtem Solutios Febuay 18 1. A bag of mables cotais 4 which ae ed, 4 which ae blue ad 4 which ae gee. a How may mables must be chose fom the bag to guaatee that thee ae the same colou? We ca
More informationElectrical Engineering Department Network Lab.
Par:- Elecrical Egieerig Deparme Nework Lab. Deermiaio of differe parameers of -por eworks ad verificaio of heir ierrelaio ships. Objecive: - To deermie Y, ad ABD parameers of sigle ad cascaded wo Por
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationSection 8 Convolution and Deconvolution
APPLICATIONS IN SIGNAL PROCESSING Secio 8 Covoluio ad Decovoluio This docume illusraes several echiques for carryig ou covoluio ad decovoluio i Mahcad. There are several operaors available for hese fucios:
More informationOLS bias for econometric models with errors-in-variables. The Lucas-critique Supplementary note to Lecture 17
OLS bias for ecoomeric models wih errors-i-variables. The Lucas-criique Supplemeary oe o Lecure 7 RNy May 6, 03 Properies of OLS i RE models I Lecure 7 we discussed he followig example of a raioal expecaios
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationEDEXCEL NATIONAL CERTIFICATE UNIT 28 FURTHER MATHEMATICS FOR TECHNICIANS OUTCOME 2- ALGEBRAIC TECHNIQUES TUTORIAL 1 - PROGRESSIONS
EDEXCEL NATIONAL CERTIFICATE UNIT 8 FURTHER MATHEMATICS FOR TECHNICIANS OUTCOME - ALGEBRAIC TECHNIQUES TUTORIAL - PROGRESSIONS CONTENTS Be able to apply algebaic techiques Aithmetic pogessio (AP): fist
More informationN! AND THE GAMMA FUNCTION
N! AND THE GAMMA FUNCTION Cosider he produc of he firs posiive iegers- 3 4 5 6 (-) =! Oe calls his produc he facorial ad has ha produc of he firs five iegers equals 5!=0. Direcly relaed o he discree! fucio
More informationGeneral Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security
1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,
More informationCalculus BC 2015 Scoring Guidelines
AP Calculus BC 5 Scorig Guidelies 5 The College Board. College Board, Advaced Placeme Program, AP, AP Ceral, ad he acor logo are regisered rademarks of he College Board. AP Ceral is he official olie home
More informationTwo-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch
Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion
More information2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)
Mah PracTes Be sure o review Lab (ad all labs) There are los of good quesios o i a) Sae he Mea Value Theorem ad draw a graph ha illusraes b) Name a impora heorem where he Mea Value Theorem was used i he
More informationBINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =
wwwskshieduciocom BINOMIAL HEOREM OBJEIVE PROBLEMS he coefficies of, i e esio of k e equl he k /7 If e coefficie of, d ems i e i AP, e e vlue of is he coefficies i e,, 7 ems i e esio of e i AP he 7 7 em
More informationSTIFFNESS EVALUATION OF SOME QUASI-ISOTROPIC FIBRE- REINFORCED COMPOSITE LAMINATES
The d Ieaioal Cofeee o Compuaioal Mehais ad Viual gieeig COMC 009 9 0 OCTOBR 009 Basov Romaia STIFFSS VALUATIO OF SOM QUASI-ISOTROPIC FIBR- RIFORCD COMPOSIT LAMIATS H. Teodoesu-Daghiesu S. Vlase A. Chiu
More informationSupplementary materials. Suzuki reaction: mechanistic multiplicity versus exclusive homogeneous or exclusive heterogeneous catalysis
Geeal Pape ARKIVOC 009 (xi 85-03 Supplemetay mateials Suzui eactio: mechaistic multiplicity vesus exclusive homogeeous o exclusive heteogeeous catalysis Aa A. Kuohtia, Alexade F. Schmidt* Depatmet of Chemisty
More informationLecture 22 Electromagnetic Waves
Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More informationNeutron Slowing Down Distances and Times in Hydrogenous Materials. Erin Boyd May 10, 2005
Neu Slwig Dw Disaces ad Times i Hydgeus Maeials i Byd May 0 005 Oulie Backgud / Lecue Maeial Neu Slwig Dw quai Flux behavi i hydgeus medium Femi eame f calculaig slwig dw disaces ad imes. Bief deivai f
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 4 9/16/2013. Applications of the large deviation technique
MASSACHUSETTS ISTITUTE OF TECHOLOGY 6.265/5.070J Fall 203 Lecure 4 9/6/203 Applicaios of he large deviaio echique Coe.. Isurace problem 2. Queueig problem 3. Buffer overflow probabiliy Safey capial for
More informationPhysics 2001/2051 Moments of Inertia Experiment 1
Physics 001/051 Momens o Ineia Expeimen 1 Pelab 1 Read he ollowing backgound/seup and ensue you ae amilia wih he heoy equied o he expeimen. Please also ill in he missing equaions 5, 7 and 9. Backgound/Seup
More informationr P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,
Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:
More informationChemical Engineering 374
Chemical Egieerig 374 Fluid Mechaics NoNeoia Fluids Oulie 2 Types ad properies of o-neoia Fluids Pipe flos for o-neoia fluids Velociy profile / flo rae Pressure op Fricio facor Pump poer Rheological Parameers
More information1 Notes on Little s Law (l = λw)
Copyrigh c 26 by Karl Sigma Noes o Lile s Law (l λw) We cosider here a famous ad very useful law i queueig heory called Lile s Law, also kow as l λw, which assers ha he ime average umber of cusomers i
More informationPure Math 30: Explained!
ure Mah : Explaied! www.puremah.com 6 Logarihms Lesso ar Basic Expoeial Applicaios Expoeial Growh & Decay: Siuaios followig his ype of chage ca be modeled usig he formula: (b) A = Fuure Amou A o = iial
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationMECHANICS OF MATERIALS Poisson s Ratio
Fouh diion MCHANICS OF MATRIALS Poisson s Raio Bee Johnson DeWolf Fo a slende ba subjeced o aial loading: 0 The elongaion in he -diecion is accompanied b a conacion in he ohe diecions. Assuming ha he maeial
More informationClock Skew and Signal Representation
Clock Skew ad Sigal Represeaio Ch. 7 IBM Power 4 Chip 0/7/004 08 frequecy domai Program Iroducio ad moivaio Sequeial circuis, clock imig, Basic ools for frequecy domai aalysis Fourier series sigal represeaio
More informationPhysics of Elastic Magnetic Filaments
Ieaioa Scieific Cooquium Modeig fo Maeia Pocessig iga, Jue 8-9, 6 Physics of Easic Mageic Fiames I. Javaiis Absac The mode of a easic mageic fiame is deveoped. Mode of easic mageic fiame aows ivesigaig
More informationCS623: Introduction to Computing with Neural Nets (lecture-10) Pushpak Bhattacharyya Computer Science and Engineering Department IIT Bombay
CS6: Iroducio o Compuig ih Neural Nes lecure- Pushpak Bhaacharyya Compuer Sciece ad Egieerig Deparme IIT Bombay Tilig Algorihm repea A kid of divide ad coquer sraegy Give he classes i he daa, ru he percepro
More informationStochastic Design of Enhanced Network Management Architecture and Algorithmic Implementations
Ameica Joual of Opeaios Reseach 23 3 87-93 hp://dx.doi.og/.4236/ajo.23.3a8 Published Olie Jauay 23 (hp://.scip.og/joual/ajo) Sochasic Desig of Ehaced Neo Maageme Achiecue ad Algoihmic Implemeaios Sog-Kyoo
More informationA Weighted Moving Average Process for Forcasting
Joual of Mode Applied aisical Mehods Volume 6 Issue Aicle 6 --007 A Weighed Movig Aveage Pocess fo Focasig hou Hsig hih Uivesiy of ouh Floida, sshih@mailusfedu Chis P Tsokos Uivesiy of ouh Floida, pofcp@casusfedu
More informationExistence and Smoothness of Solution of Navier-Stokes Equation on R 3
Ieaioal Joual of Mode Noliea Theoy ad Applicaio, 5, 4, 7-6 Published Olie Jue 5 i SciRes. hp://www.scip.og/joual/ijma hp://dx.doi.og/.436/ijma.5.48 Exisece ad Smoohess of Soluio of Navie-Sokes Equaio o
More informationMATH 507a ASSIGNMENT 4 SOLUTIONS FALL 2018 Prof. Alexander. g (x) dx = g(b) g(0) = g(b),
MATH 57a ASSIGNMENT 4 SOLUTIONS FALL 28 Prof. Alexader (2.3.8)(a) Le g(x) = x/( + x) for x. The g (x) = /( + x) 2 is decreasig, so for a, b, g(a + b) g(a) = a+b a g (x) dx b so g(a + b) g(a) + g(b). Sice
More informationComplementi di Fisica Lecture 6
Comlemei di Fisica Lecure 6 Livio Laceri Uiversià di Triese Triese, 15/17-10-2006 Course Oulie - Remider The hysics of semicoducor devices: a iroducio Basic roeries; eergy bads, desiy of saes Equilibrium
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence
More informationLecture 15: Three-tank Mixing and Lead Poisoning
Lecure 15: Three-ak Miig ad Lead Poisoig Eigevalues ad eigevecors will be used o fid he soluio of a sysem for ukow fucios ha saisfy differeial equaios The ukow fucios will be wrie as a 1 colum vecor [
More informationMultivector Functions
I: J. Math. Aal. ad Appl., ol. 24, No. 3, c Academic Pess (968) 467 473. Multivecto Fuctios David Hestees I a pevious pape [], the fudametals of diffeetial ad itegal calculus o Euclidea -space wee expessed
More informationProgression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P.
Pogessio Sequece & Seies A set of umbes whose domai is a eal umbe is called a SEQUENCE ad sum of the sequece is called a SERIES. If a, a, a, a 4,., a, is a sequece, the the expessio a + a + a + a 4 + a
More informationCHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method
CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3
More informationCalculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.
Limi of a fucio.. Oe-Sided..... Ifiie limis Verical Asympoes... Calculaig Usig he Limi Laws.5 The Squeeze Theorem.6 The Precise Defiiio of a Limi......7 Coiuiy.8 Iermediae Value Theorem..9 Refereces..
More informationPHYS PRACTICE EXAM 2
PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,
More informationActuarial Society of India
Acuarial Sociey of Idia EXAMINAIONS Jue 5 C4 (3) Models oal Marks - 5 Idicaive Soluio Q. (i) a) Le U deoe he process described by 3 ad V deoe he process described by 4. he 5 e 5 PU [ ] PV [ ] ( e ).538!
More informationSamuel Sindayigaya 1, Nyongesa L. Kennedy 2, Adu A.M. Wasike 3
Ieraioal Joural of Saisics ad Aalysis. ISSN 48-9959 Volume 6, Number (6, pp. -8 Research Idia Publicaios hp://www.ripublicaio.com The Populaio Mea ad is Variace i he Presece of Geocide for a Simple Birh-Deah-
More informationGeneralized Fibonacci-Type Sequence and its Properties
Geelized Fibocci-Type Sequece d is Popeies Ompsh Sihwl shw Vys Devshi Tuoil Keshv Kuj Mdsu (MP Idi Resech Schol Fculy of Sciece Pcific Acdemy of Highe Educio d Resech Uivesiy Udipu (Rj Absc: The Fibocci
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationEMA5001 Lecture 3 Steady State & Nonsteady State Diffusion - Fick s 2 nd Law & Solutions
EMA5 Lecue 3 Seady Sae & Noseady Sae ffuso - Fck s d Law & Soluos EMA 5 Physcal Popees of Maeals Zhe heg (6) 3 Noseady Sae ff Fck s d Law Seady-Sae ffuso Seady Sae Seady Sae = Equlbum? No! Smlay: Sae fuco
More informationHighly connected coloured subgraphs via the Regularity Lemma
Highly coeced coloued subgaphs via he Regulaiy Lemma Hey Liu 1 Depame of Mahemaics, Uivesiy College Lodo, Gowe See, Lodo WC1E 6BT, Uied Kigdom Yuy Peso 2 Isiu fü Ifomaik, Humbold-Uivesiä zu Beli, Ue de
More informationReinforcement learning
Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback
More informationOptimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis
Joural of aerials Sciece ad Egieerig B 5 (7-8 (5 - doi: 765/6-6/57-8 D DAVID PUBLISHING Opimizaio of Roaig achies Vibraios Limis by he Sprig - ass Sysem Aalysis BENDJAIA Belacem sila, Algéria Absrac: The
More informationELECTROOSMOTIC FLOW IN A MICROCHANNEL PACKED WITH MICROSPHERES
ELECTROOSMOTIC FLOW IN A MICROCHANNEL PACKED WITH MICROSPHERES KANG YUEJUN SCHOOL OF MECHANICAL & AEROSPACE ENGINEERING NANYANG TECHNOLOGICAL UNIVERSITY 5 Elecoosmoic Flow i a Micochael Packed wih Micosphees
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid
More information