Chapter 5: 8, 16, 25, 27, 28, 35, 36, 49, 52, 57, 72, 82 and 87.
|
|
- Rose Gibson
- 5 years ago
- Views:
Transcription
1 aper : 8,,, 7, 8,,, 9,, 7, 7, 8 and e fne dfference frulan f sead w-densnal ea cnducn n a edu w ea eneran and cnsan eral cnducv s ven b, n n,, n n, n, n, n, n recanular crdnaes. s relan can be dfed fr e ree-densnal case b spl addn aner nde j e eperaure n e z drecn, and aner dfference er fr e z drecn as, n, j, n, j, n, j, n, j, n, j, n, j, n, j, n, j, n, z, n, j j - A plane wall w n ea eneran s subjeced specfed eperaure a e lef nde and ea flu a e r bundar nde 8. e fne dfference frulan f e bundar ndes and e fne dfference frulan fr e rae f ea ransfer a e lef bundar are be deerned. Assupns Hea ransfer ru e wall s ven be sead, and e eral cnducv be cnsan. Hea ransfer s ne-densnal snce e plae s lare relave s cness. ere s n ea eneran n e edu. Analss Usn e ener balance apprac and an e drecn f all ea ransfers be wards e nde under cnsderan, e fne dfference frulans bece Lef bundar nde: R bundar nde: A q A r 8 Hea ransfer a lef surface: Q lef surface A
2 - A ln ranular fn aaced a surface s cnsdered. e ndal eperaures, e rae f ea ransfer, and e fn effcenc are be deerned nuercall usn equall spaced ndes. Assupns Hea ransfer aln e fn s ven be sead, and e eperaure aln e fn var n e drecn nl s a. eral cnducv s cnsan. Prperes e eral cnducv s ven be 8 W/. e essv f e fn surface s.9. Analss e fn len s ven be L c, and e nuber f ndes s specfed be M. erefre, e ndal spacn s L M.. - e eperaure a nde s ven be, and e eperaures a e reann ndes are be deerned. erefre, we need ave equans deerne e unquel. Ndes,,, and are nerr ndes, and e fne dfference frulan fr a eneral nerr nde s baned b appln an ener balance n e vlue eleen f s nde. Nn a ea ransfer s sead and ere s n ea eneran n e fn and assun ea ransfer be n e edu fr all sdes, e ener balance can be epressed as Q Alef Ar Acnv εσasurface[ surr 7 } all sdes Ne a ea ransfer areas are dfferen fr eac nde n s case, and usn eercal relans, e can be epressed as A A lef r He wd He / w L [ / ] [ / ] w L w / csθ { εσ[ anθ anθ Asurface Len wd w / csθ Subsun, w[ L. ] anθ w[ L. ] anθ Dvdn eac er b wl anθ / ves surr 7 ]} εσ L L Lsnθ Lsnθ surr Subsun, : εσ.. [ surr 7 ] L L Lsnθ Lsnθ : εσ.. [ surr 7 ] L L Lsnθ Lsnθ : εσ.. [ surr 7 ] L L Lsnθ Lsnθ : εσ.. [ surr 7 ] L L Lsnθ Lsnθ / / [ 7 ] An ener balance n e nde ves e equan, : / / an θ εσ [ surr 7 ] csθ csθ
3 Prb. - cnnued Slvn e equans abve sulaneusl fr e unnwn ndal eperaures ves 77., 7., 7., 8., and. b e al rae f ea ransfer fr e fn s spl e su f e ea ransfer fr eac vlue eleen e aben, and fr w s deerned fr Q fn Q eleen, Asurface, εσa surface, [ 7 Nn a e ea ransfer surface area s w /csθ fr e bundar ndes and, and wce as lare fr e nerr ndes,,, and, we ave w Q fn [ ] csθ w εσ {[ 7 surr ] [ 7 surr ] [ 7 surr ] [ 7 surr ] csθ [ W 7 surr ] [ 7 surr ]} surr ]
4 -7 A plae s subjeced specfed ea flu n ne sde and specfed eperaure n e er. e fne dfference frulan f s prble s be baned, and e unnwn surface eperaure under sead cndns s be deerned. Assupns Hea ransfer ru e base plae s ven be sead. Hea ransfer s nedensnal snce e plae s lare relave s cness. ere s n ea eneran n e plae. Radan ea ransfer s nelble. e enre ea eneraed b e ressance eaers s ransferred ru e plae. Prperes e eral cnducv s ven be W/. Analss e ndal spacn s ven be. c. en e nuber f ndes M beces L. c M. c e r surface eperaure s ven be 8. s prble nvlves unnwn ndal eperaures, and us we need ave equans deerne e unquel. Ndes,, and are nerr ndes, and us fr e we can use e eneral fne dfference relan epressed as snce, fr and e fne dfference equan fr nde n e lef surface subjeced unfr ea flu s baned b appln an ener balance n e alf vlue eleen abu nde and an e drecn f all ea ransfers be wards e nde under cnsderan: Nde r surface - cnvecn : Ndenerr : Nde nerr : q were. c, W/, 8, and q Q / A 8W /., W/. e sse f equans w unnwn eperaures cnsue e fne dfference frulan f e prble. b e ndal eperaures under sead cndns are deerned b slvn e equans abve sulaneusl w an equan slver be, 9, and 9 Dscussn s prble can be slved analcall b slvn e dfferenal equan as descrbed n ap., and e analcal eac slun can be used cec e accurac f e nuercal slun abve.
5 -8 A plae s subjeced specfed ea flu and specfed eperaure n ne sde, and n cndns n e er. e fne dfference frulan f s prble s be baned, and e eperaure f e er sde under sead cndns s be deerned. Assupns Hea ransfer ru e plae s ven be sead and ne-densnal. ere s n ea eneran n e plae. Prperes e eral cnducv s ven be. W/. Analss e ndal spacn s ven be.. en e nuber f ndes M beces L. M. Ndes,,, and are nerr ndes, and us fr e we can use e eneral fne dfference relan epressed as snce, fr,,, and e fne dfference equan fr nde n e lef surface s baned b appln an ener balance n e alf vlue eleen abu nde and an e drecn f all ea ransfers be wards e nde under cnsderan, 8 q 7 W/. W/.. Oer ndal eperaures are deerned fr e eneral nerr nde relan as fllws: : : : : erefre, e eperaure f e er surface wll be. Dscussn s prble can be slved analcall b slvn e dfferenal equan as descrbed n ap., and e analcal eac slun can be used cec e accurac f e nuercal slun abve.
6 - One sde f a vercal plae s be cled b aacn cpper pn fns. e fne dfference frulan f e prble fr all ndes s be baned, and e ndal eperaures, e rae f ea ransfer fr a snle fn and fr e enre surface f e plae are be deerned. Assupns Hea ransfer aln e fn s ven be sead and ne-densnal. e eral cnducv s cnsan. bned cnvecn and radan ea ransfer ceffcen s cnsan and unfr. Prperes e eral cnducv s ven be 8 W/. Analss e ndal spacn s ven be. c. en e nuber f ndes M beces L c M 7. c e base eperaure a nde s ven be. s prble nvlves unnwn ndal eperaures, and us we need ave equans deerne e unquel. Ndes,,,, and are nerr ndes, and us fr e we can use e eneral fne dfference relan epressed as A A p p / A e fne dfference equan fr nde a e fn p s baned b appln an ener balance n e alf vlue eleen abu a nde. en, : p / A : p / A : p / A : p / A : p / A Nde : A p / A were., 7 W/,,, W/ A πd / π. c /.9c.9 and p πd π..78 b e ndal eperaures under sead cndns are deerned b slvn e equans abve sulaneusl w an equan slver be 98., - 97., 9.7, 9., 9.7, 9. c e rae f ea ransfer fr a snle fn s spl e su f e ea ransfer fr e ndal eleens, Q fn Q eleen, p / A surface, p p / A. W d e nuber f fns n e surface s N.f fns 7,778 fns.. en e rae f ea ranfer fr e fns, e unfnned prn, and e enre fnned surface bece Q Q Q fn, al `unfnned al N. f fns Q A Q fn, al Q unfnned fn unfnned 7,778. W,7 W W/,7 7,78 W - 7, W
7 - w cas rn sea ppes are cnneced eac er ru w -c c flanes, and ea s ls fr e flanes b cnvecn and radan. e fne dfference frulan f e prble fr all ndes s be baned, and e eperaure f e p f e flane as well as e rae f ea ransfer fr e epsed surfaces f e flane are be deerned. Assupns Hea ransfer ru e flane s saed be sead and ne-densnal. e eral cnducv and essv are cnsans. nvecn ea ransfer ceffcen s cnsan and unfr. Prperes e eral cnducv and essv are ven be W/ and ε.8. Analss e dsance beween ndes and s e cness f e ppe,. c.. e ndal spacn aln e flane s ven be c.. en e nuber f ndes M beces L c M 7 c s prble nvlves 7 unnwn ndal eperaures, and us we need ave 7 equans deerne e unquel. Nn a e al cness f e flane s., e ea cnducn area a an lcan aln e flane s Acnd πr were e values f rad a e ndes and beween e ndes e d pns are r., r., r., r.7, r.8, r.9, r. r.8, r., r., r.7, r.8, r.9 en e fne dfference equans fr eac nde are baned fr e ener balance be as fllws: Nde : π r πr Nde : π r πr [π r r / ] / { εσ[ surr 7 ]} Nde : π r πr πr { εσ[ surr 7 ]} Nde : π r πr πr { εσ[ surr 7 ]} Nde : π r πr πr { εσ[ surr 7 ]} Nde : π r πr πr { εσ[ surr 7 ]} Prb. - cnnued Nde : π r [π / r r / πr ]{ εσ[ surr 7 ]} were.,., W/, ε.8, 8, n, 9 K and surr -8, 8 W/,.7 W/ K. W/ σ e sse f 7 equans w 7 unnwns cnsues e fne dfference frulan f e prble. b e ndal eperaures under sead cndns are deerned b slvn e 7 equans abve sulaneusl w an equan slver be.,., 9., 8.9, 8.7, 8., and 8.,
8 c Knwn e nner surface eperaure, e rae f ea ransfer fr e flane under sead cndns s spl e rae f ea ransfer fr e sea e ppe a flane secn Q fn Q eleen, Asurface, εσa were A surface, are as ven abve fr dfferen ndes. surface, [ 7 surr ]. W
9 -9 A ln sld bd s subjeced sead w-densnal ea ransfer. e unnwn ndal eperaures are be deerned. Assupns Hea ransfer ru e bd s ven be sead and w-densnal. ere s n ea eneran n e bd. Prperes e eral cnducv s ven be W/. Analss e ndal spacn s ven be l., and e eneral fne dfference fr f an nerr nde fr sead w-densnal ea cnducn fr e case f n ea eneran s epressed as ndel lef p r b nde nde lef p r b / a ere s ser abu e nsulaed surfaces as well as abu e danal lne. erefre, and,, and are e nl unnwn ndal eperaures. us we need nl equans deerne e unquel. Als, we can replace e ser lnes b nsulan and ulze e rrr-ae cncep wen wrn e fne dfference equans fr e nerr ndes. Ndenerr : Nde nerr : Nde nerr : 8 8 / / Slvn e equans abve sulaneusl ves 8 9 / b ere s ser abu e nsulaed surface as well as e danal lne. Replacn e ser lnes b nsulan, and ulzn e rrr-ae cncep, e fne dfference equans fr e nerr ndes can be wren as Ndenerr : Nde nerr : Nde nerr : Nde nerr : / / / Slvn e equans abve sulaneusl ves.9 8. / Dscussn Ne a an advanae f ser splfed e prble real.
10 - A ln sld bd s subjeced sead w-densnal ea ransfer. e unnwn ndal eperaures are be deerned. Assupns Hea ransfer ru e bd s ven be sead and w-densnal. ere s n ea eneran n e bd. Prperes e eral cnducv s ven be W/. Analss e ndal spacn s ven be l., and e eneral fne dfference fr f an nerr nde fr sead w-densnal ea cnducn fr e case f n ea eneran s epressed as ndel lef p r b nde lef p r b nde a ere s ser abu a vercal lne passn ru e ndes and. erefre,,, and,,, and are e nl unnwn ndal eperaures, and us we need nl equans deerne e unquel. Als, we can replace e ser lnes b nsulan and ulze e rrr-ae cncep wen wrn e fne dfference equans fr e nerr ndes. Nde nerr : Nde nerr : Nde nerr : Nde nerr : Slvn e equans abve sulaneusl ves 7 b ere s ser abu a vercal lne passn ru e ddle. erefre, and. Replacn e ser lnes b nsulan and ulzn e rrr-ae cncep, e fne dfference equans fr e nerr ndes and are deerned be Ndenerr : Nde nerr : Slvn e equans abve sulaneusl ves Dscussn Ne a an advanae f ser splfed e prble real.
11 -7 e epsed surface f a ln cncree dan f ranular crss-secn s subjeced slar ea flu and cnvecn and radan ea ransfer. e vercal secn f e dan s subjeced cnvecn w waer. e eperaures a e p, ddle, and b f e epsed surface f e dan are be deerned. Assupns Hea ransfer ru e dan s ven be sead and w-densnal. ere s n ea eneran wn e dan. Hea ransfer ru e base s nelble. eral prperes and ea ransfer ceffcens are cnsan. Prperes e eral cnducv and slar absrpv are ven be. W/ and α s.7. Analss e ndal spacn s ven be l, and all ndes are bundar ndes. Nde n e nsulaed bundar can be reaed as an nerr nde fr wc lef p r b nde. Usn e ener balance apprac and an e drecn f all ea ransfer be wards e nde, e fne dfference equans fr e ndes are baned be as fllws: l l l / l sn s s Nde : l l l l l l l l l l s qs l l sn Nde : l l l l l Nde : Nde : l l / [ sqs ] l sn Nde : [ α q ] Nde : [ ] were l,. W/, W/,, W/,, α s.7, and q s 8 W/. e sse f equans w unnwns cnsues e fne dfference frulan f e prble. e ndal eperaures under sead cndns are deerned b slvn e equans abve sulaneusl w an equan slver be p.,., ddle.,.,., b. Dscussn Ne a e es eperaure ccurs a a lcan fures awa fr e waer, as epeced.
12 -7 A plane wall w varable ea eneran and cnsan eral cnducv s subjeced unfr ea flu q a e lef nde and cnvecn a e r bundar nde. e eplc ransen fne dfference frulan f e bundar ndes s be deerned. Assupns Hea ransfer ru e wall s ven be ransen, and e eral cnducv be cnsan. Hea ransfer s ne-densnal snce e plae s lare relave s cness. Radan ea ransfer s nelble. Analss Usn e ener balance apprac and an e drecn f all ea ransfers be wards e nde under cnsderan, e eplc fne dfference frulans bece Lef bundar nde: A A A q A / R bundar nde: A A A A /
13 -8 A uranu plae nall a a unfr eperaure s subjeced nsulan n ne sde and cnvecn n e er. e ransen fne dfference frulan f s prble s be baned, and e ndal eperaures afer n and under sead cndns are be deerned. Assupns Hea ransfer s ne-densnal snce e plae s lare relave s cness. eral cnducv s cnsan. Radan ea ransfer s nelble. Prperes e cnducv and dffusv are ven be 8 W/ and α. /s. Analss e ndal spacn s ven be.. en e nuber f ndes beces / L M.8/.. s prble nvlves unnwn ndal eperaures, and us we need ave equans. Nde s n nsulaed bundar, and us we can rea as an nerr ne b usn e rrr ae cncep. Ndes,, and are nerr ndes, and us fr e we can use e eneral eplc fne dfference relan epressed as e fne dfference equan fr nde n e r surface subjeced cnvecn s baned b appln an ener balance n e alf vlue eleen abu nde and an e drecn f all ea ransfers be wards e nde under cnsderan: : Nde cnvecn Nde nerr : Nde nerr : Ndenerr : : Nde nsulaed r were, W/, 8 W/, W/.,, and. α /s. e upper l f e e sep s deerned fr e sabl crera a requres all prar ceffcens be reaer an r equal zer. e ceffcen f s saller n s case, and us e sabl crera fr s prble can be epressed as α / / snce α /. Subsun e ven quanes, e au allwable e e sep beces. s ] /8 W/... W/ /s[.. erefre, an e sep less an. s can be used slve s prble. Fr cnvenence, le us cse e e sep be s. en e es Furer nuber beces α / s s Subsun s value f and er ven quanes, e ndal eperaures afer / e seps n are deerned be Afer n: 8.9, 8.,.8,., and 9.9
14 b e e needed fr ransen peran be esablsed s deerned b ncreasn e nuber f e seps unl e ndal eperaures n lner cane. In s case sead peran s esablsed n ---- n, and e ndal eperaures under sead cndns are deerned be,, 9,, and Dscussn e sead slun can be ceced ndependenl b bann e sead fne dfference frulan, and slvn e resuln equans sulaneusl.
15 -87 e fran f f n e lass surfaces f a car s be prevened b aacn elecrc ressance eaers e nner surfaces. e eperaure dsrbun ruu e lass n afer e srp eaers are urned n and als wen sead cndns are reaced are be deerned usn e eplc ed. Assupns Hea ransfer ru e lass s ven be ransen and w-densnal. eral cnducv s cnsan. ere s ea eneran nl a e nner surface, wc wll be reaed as prescrbed ea flu. Prperes e cnducv and dffusv are ven be.8 W/ and α 9. /s. Analss e ndal spacn s ven be. c and c. e eplc fne dfference equans are deerned n e bass f e ener balance fr e ransen case epressed as Q G V All sdes eleen eleen We cnsder nl 9 ndes because f ser. Ne a we d n ave a square es n s case, and us we wll ave rel n ener balances ban e fne dfference equans. Usn ener balances, e fne dfference equans fr eac f e 9 ndes are baned as fllws: Nde : Nde : Nde : Nde : 7 Nde : 8 Nde : 9 Nde 7: W Nde 8: Nde 9: were.8 W/., α /. 9 /s, - W/., W/.,., and.. e upper l f e e sep s deerned fr e sabl crera a requres e ceffcen f n e epressn e prar ceffcen be reaer an r equal zer fr all ndes. e salles prar ceffcen n e 9 equans abve s e ceffcen f 9 n e epressn snce s epsed s cnvecn per un vlue s can be verfed. e equan fr nde can be rearraned as 9 α α erefre, e sabl crera fr s prble can be epressed as
16 α α Subsun e ven quanes, e au allwable value f e e sep s deerned be r, s W/ W/ /.9 s erefre, an e sep less an.8 s can be used slve s prble. Fr cnvenence, we cse e e sep be s. en e eperaure dsrbun ruu e lass n afer e srp eaers are urned n and wen sead cndns are reaced are deerned be fr e EES sluns ds n: -., -., -., -.8, -., -.7, 7., 8.7, 9 9. Sead-sae: -., -., -., -.8, -., -.7, 7., 8.7, 9 9. Dscussn Sead peran cndns are reaced n abu 8 n.
. Analysis The nodal spacing is given to be x = 0.02 m. Then the number of nodes becomes 1. i m. i m. i m
aper Nuerca Meds n Hea nducn - - A uranu pae na a a unfr eperaure s subjeced nsuan n ne sde and cnvecn n e er. e ransen fne dfference fruan f s prbe s be baned, and e nda eperaures afer n and under sead
More informationPROBLEM-Chapter 1-5 (Heat Transfer, Yanus A. Cengel)
POBEM-hape -5 Hea ansfe Yanus. ene - he nne and ue sufaces f a bc wa ae ananed a specfed epeaues. he ae f hea ansfe huh he wa s be deened. ssupns Seady pean cndns es snce he suface epeaues f he wa ean
More information2015 Sectional Physics Exam Solution Set
. Crrec answer: D Ne: [quan] denes: uns quan WYSE cadec Challenge 05 Secnal Phscs Ea SOLUTION SET / / / / rce lengh lengh rce enu ass lengh e a) / ass ass b) energ c) wrk lengh e pwer energ e d) (crrec
More informationR th is the Thevenin equivalent at the capacitor terminals.
Chaper 7, Slun. Applyng KV Fg. 7.. d 0 C - Takng he derae f each erm, d 0 C d d d r C Inegrang, () ln I 0 - () I 0 e - C C () () r - I 0 e - () V 0 e C C Chaper 7, Slun. h C where h s he Theenn equalen
More informationMass Linear Momentum Moment of Momentum Energy Putting it all together!
inie Cnrl lue nalsis vin fr a Sse a inie Cnrl lue a Linear enu en f enu Ener Puin i all eer! D Cnservain f a B = Tal aun f a in e e b = a er uni a = DB ˆ b b n ˆ n ˆ equain Bu D / =! Cninui Equain a leavin
More informationNormal Random Variable and its discriminant functions
Noral Rando Varable and s dscrnan funcons Oulne Noral Rando Varable Properes Dscrnan funcons Why Noral Rando Varables? Analycally racable Works well when observaon coes for a corruped snle prooype 3 The
More informationAnalysis with boundary elements of heat conductivity in steady state regime
Recen Advances n Fud Mechancs, Hea & Mass Transfer and Bgy Anayss wh bundary eeens f hea cnducvy n seady sae rege Prf. dr. eng. IOA SÂRBU Deparen f Budng Servces Pehnca Unversy f Tsara Paa Bserc, n. 4A,
More informationConvection and conduction and lumped models
MIT Hea ranfer Dynamc mdel 4.3./SG nvecn and cndcn and lmped mdel. Hea cnvecn If we have a rface wh he emperare and a rrndng fld wh he emperare a where a hgher han we have a hea flw a Φ h [W] () where
More informationChapter 3 Dynamics of Earthquake Analysis
Chaper 3 Dynamcs f Earhquake Analyss 3. Inrucn Earhquake r sesmc analyss s a subse f srucural analyss whch nvlves he calculan f he respnse f a srucure subjece earhquake excan. Ths s requre fr carryn u
More informationRheological Models. In this section, a number of one-dimensional linear viscoelastic models are discussed.
helgcal Mdels In hs secn, a number f ne-dmensnal lnear vscelasc mdels are dscussed..3. Mechancal (rhelgcal) mdels The wrd vscelasc s derved frm he wrds "vscus" + "elasc"; a vscelasc maeral exhbs bh vscus
More informationSharif University of Technology,
-,,,, A FINITE DIFFERENE SHEME TO AATE THE OPTION PRIES IN STOHASTI VOATIITY MODES S. Zaman & B. Zargar Sarf nvers f Tecnlg, zaman@sarf.ed Absrac: In scasc vlal mdels, Erpean pn prces are slns parablc
More informationEnergy Storage Devices
Energy Srage Deces Objece f ecure Descrbe The cnsrucn f an nducr Hw energy s sred n an nducr The elecrcal prperes f an nducr Relanshp beween lage, curren, and nducance; pwer; and energy Equalen nducance
More informationStructural and Thermal Analysis of Heat Exchanger with Tubes of Elliptical Shape انتحهيم انتركيبي و انحراري نمبادل حراري ذو أنابيب بيضوية انشكم
Srucural and Thermal Analyss f Hea Exchanger wh Tubes f Ellpcal Shape Nawras H. Msafa By Qusay R. Al-Hagag Absrac: An apprach selec he ube wall hckness dsrbun f sreamlned ubes nended fr use n hea exchangers
More informationTransient Conduction: Spatial Effects and the Role of Analytical Solutions
Transent Cnductn: Spatal Effects and the Rle f Analytcal Slutns Slutn t the Heat Equatn fr a Plane Wall wth Symmetrcal Cnvectn Cndtns If the lumped capactance apprxmatn can nt be made, cnsderatn must be
More informationelement k Using FEM to Solve Truss Problems
sng EM t Slve Truss Prblems A truss s an engneerng structure cmpsed straght members, a certan materal, that are tpcall pn-ned at ther ends. Such members are als called tw-rce members snce the can nl transmt
More informationMidterm Exam. Thursday, April hour, 15 minutes
Economcs of Grow, ECO560 San Francsco Sae Unvers Mcael Bar Sprng 04 Mderm Exam Tursda, prl 0 our, 5 mnues ame: Insrucons. Ts s closed boo, closed noes exam.. o calculaors of an nd are allowed. 3. Sow all
More informationEstimation of condensate mass flow rate during purging time in heat recovery steam generator of combined cycle power plant Ehyaei,M.
Esman f cndensae mass flw rae durn purn me n hea recvery seam enerar f cmbned cycle pwer plan Ehyae,M. () () sssan Prfessr f Islamc zad Unversy, Pards Branch, P.O. Bx 6555/35, Pards New Cy, ehran,iran,
More informationDiscontiuum mechanics of isotropic multilayered soils beneath a uniform vertical load
scnuum mechancs f srpc mullaered sls beneah a unfrm vercal lad alr Yanqu eparmen f vl Enneern San usn Nanal Unvers f requpa, requpa, Peru SR hs paper deals wh he basc prncples f he deermnsc dscnnuum mechancs
More informationPopulation Balance Model for C 3 S Hydration
Ppulan Balance Mdel fr C S Hydran Jseph J. Bernack and Tanan e Deparmen f Chemcal Engneerng Tennessee Technlgcal Unversy Inernanal Summ n Cemen Hydran Knecs and Mdelng July v. 7 6 9 Oulnes Inrducn Sme
More informationLecture 12: HEMT AC Properties
Lecure : HEMT A Proeres Quas-sac oeraon Transcaacances -araeers Non-quas ac effecs Parasc ressances / caacancs f f ax ean ue for aer 6: 7-86 95-407 {407-46 sk MEFET ars} 47-44. (.e. sk an MEFET ars brefl
More informationPhys 331: Ch 9,.6-.7 Noninertial Frames: Centrifugal and Corriolis forces 1
Phs : Ch 9 6-7 Nnneral Frames: Cenrfugal and Crrls frces Wed /8 Thurs /9 Fr /0 Mn / Tues /4 Wed /5 Thurs /6 Fr /7 98-9 Free Fall & Crls Fucaul Pendulum 0- Cener f Mass & Ran abu a Fed As 0-4 Ran abu an
More informationPhysics 20 Lesson 9H Rotational Kinematics
Phyc 0 Len 9H Ranal Knemac In Len 1 9 we learned abu lnear mn knemac and he relanhp beween dplacemen, velcy, acceleran and me. In h len we wll learn abu ranal knemac. The man derence beween he w ype mn
More information2010 Sectional Physics Solution Set
. Crrec nwer: D WYSE CDEMIC CHLLENGE Secnl hyc E 00 Slun Se y 0 y 4.0 / 9.8 /.45 y. Crrec nwer: y 8 0 / 8 /. Crrec nwer: E y y 0 ( 4 / ) ( 4.9 / ) 5.6 y y 4. Crrec nwer: E 5. Crrec nwer: The e rce c n
More informationChapter 2 Linear Mo on
Chper Lner M n .1 Aerge Velcy The erge elcy prcle s dened s The erge elcy depends nly n he nl nd he nl psns he prcle. Ths mens h prcle srs rm pn nd reurn bck he sme pn, s dsplcemen, nd s s erge elcy s
More informationCIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh
Frst CIRCLE YOUR DIVISION: Dv. 1 (9:30 am) Dv. (11:30 am) Dv. 3 (:30 m) Prf. Ruan Prf. Na Mr. Sngh Schl f Mechancal Engneerng Purdue Unversty ME315 Heat and Mass ransfer Eam #3 Wednesday Nvember 17 010
More informationCHAPTER II AC POWER CALCULATIONS
CHAE AC OWE CACUAON Conens nroducon nsananeous and Aerage ower Effece or M alue Apparen ower Coplex ower Conseraon of AC ower ower Facor and ower Facor Correcon Maxu Aerage ower ransfer Applcaons 3 nroducon
More informationDISCRETE SLIDING MODE CONTROL OF PERMANENT MAGNET STEPPER MOTOR USING FLATNESS PROPERTY.
DSCRETE SLDNG MODE CONTROL OF ERMANENT MAGNET STEER MOTOR USNG FLATNESS ROERTY. V. Thaar, B. Bpadha nerdscplnar rramme n Ssems Cnrl Enneern, T Bmba, Mumba 6, nda Emal: v@ee.b.ac.n ; bjnan@ee.b.ac.n hne:
More informationResponse of MDOF systems
Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss
More informationOur main purpose in this section is to undertake an examination of the stock
3. Caial gains ax and e sock rice volailiy Our main urose in is secion is o underake an examinaion of e sock rice volailiy by considering ow e raional seculaor s olding canges afer e ax rae on caial gains
More informationOutline. Energy-Efficient Target Coverage in Wireless Sensor Networks. Sensor Node. Introduction. Characteristics of WSN
Ener-Effcen Tare Coverae n Wreless Sensor Newors Presened b M Trà Tá -4-4 Inroducon Bacround Relaed Wor Our Proosal Oulne Maxmum Se Covers (MSC) Problem MSC Problem s NP-Comlee MSC Heursc Concluson Sensor
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationLecture 12. Heat Exchangers. Heat Exchangers Chee 318 1
Lecture 2 Heat Exchangers Heat Exchangers Chee 38 Heat Exchangers A heat exchanger s used t exchange heat between tw fluds f dfferent temperatures whch are separated by a sld wall. Heat exchangers are
More information[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5
TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres
More informationInfluence of Incident Illumination Angle on Capacitance of a Silicon Solar Cell under Frequency Modulation
Research Jurnal f Appled Scences Engneerng and Technlgy 5(4): -8 0 ISSN: 040-7459; e-issn: 040-7467 Mawell Scenfc Organzan 0 Sumed: May 06 0 Acceped: June 08 0 Pulshed: Feruary 0 0 Influence f Incden Illumnan
More informationD Solute mass diffusivity ( m ) D Mass diffusivity ( m s ) Gc Pr. Sc Sr Re g. q Radiative heat flux. U Reference velocity ( m s )
ISSN (e): 5 35 Vlme 7 Isse 6 Jne 7 Inernanal Jrnal f mpanal Engneerng Research (IJER) Nare f assn Fld n ransen Free nvecn Fl Pas ards an Implsvel Sared Vercall Inclned Plae: hermal Dffsn and agnec Feld
More information( ) () we define the interaction representation by the unitary transformation () = ()
Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger
More informationLearning Objectives. Self Organization Map. Hamming Distance(1/5) Introduction. Hamming Distance(3/5) Hamming Distance(2/5) 15/04/2015
/4/ Learnng Objecves Self Organzaon Map Learnng whou Exaples. Inroducon. MAXNET 3. Cluserng 4. Feaure Map. Self-organzng Feaure Map 6. Concluson 38 Inroducon. Learnng whou exaples. Daa are npu o he syse
More informationConduction Heat Transfer
Cnductn Heat Transfer Practce prblems A steel ppe f cnductvty 5 W/m-K has nsde and utsde surface temperature f C and 6 C respectvely Fnd the heat flw rate per unt ppe length and flux per unt nsde and per
More informationP a g e 3 6 of R e p o r t P B 4 / 0 9
P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J
More informationKinematics Review Outline
Kinemaics Review Ouline 1.1.0 Vecrs and Scalars 1.1 One Dimensinal Kinemaics Vecrs have magniude and direcin lacemen; velciy; accelerain sign indicaes direcin + is nrh; eas; up; he righ - is suh; wes;
More informationAP Physics 1 MC Practice Kinematics 1D
AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec
More informationEffectiveness of a Vertical Barrier against Intrusion of Flood Plain Infiltrated Water into an Aquifer
Hydrlgy Days 007 Effecveness f a Vercal Barrer agans Inrusn f Fld Plan Inflraed Waer n an Aqufer Cnza Mracapll Unversy f Appled Scences Nrhwesern Swzerland, Insue f Cvl Engneerng cnza.mracapll@fhnw.ch
More informationIn the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!
ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal
More informationHigher Order Difference Schemes for Heat Equation
Available a p://pvau.edu/aa Appl. Appl. Ma. ISSN: 9-966 Vol., Issue (Deceber 009), pp. 6 7 (Previously, Vol., No. ) Applicaions and Applied Maeaics: An Inernaional Journal (AAM) Higer Order Difference
More informationGraduate Macroeconomics 2 Problem set 5. - Solutions
Graduae Macroeconomcs 2 Problem se. - Soluons Queson 1 To answer hs queson we need he frms frs order condons and he equaon ha deermnes he number of frms n equlbrum. The frms frs order condons are: F K
More informationA progressive failure model for mesh-size-independent FE analysis of composite laminates subject to low-velocity impact damage
A prgressve alure del r esh-sze-ndependen F analss cpse lanaes subjec lw-velc pac daage L Rand a,1, L Iannucc a, P Rbnsn a, and PT Curs b a Iperal Cllege Lndn, Deparen Aernaucs, Suh Kensngn Capus, SW7
More informationTHEORETICAL AUTOCORRELATIONS. ) if often denoted by γ. Note that
THEORETICAL AUTOCORRELATIONS Cov( y, y ) E( y E( y))( y E( y)) ρ = = Var( y) E( y E( y)) =,, L ρ = and Cov( y, y ) s ofen denoed by whle Var( y ) f ofen denoed by γ. Noe ha γ = γ and ρ = ρ and because
More informationJ i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.
umercal negraon of he dffuson equaon (I) Fne dfference mehod. Spaal screaon. Inernal nodes. R L V For hermal conducon le s dscree he spaal doman no small fne spans, =,,: Balance of parcles for an nernal
More informationwhere v means the change in velocity, and t is the
1 PHYS:100 LECTURE 4 MECHANICS (3) Ths lecture covers the eneral case of moton wth constant acceleraton and free fall (whch s one of the more mportant examples of moton wth constant acceleraton) n a more
More informationCONTRIBUTION TO THE DISCUSSION ON ABSOLUTE INTEGRATION OF DIFFERENTIAL EQUATIONS OF GEODESICS IN NON-EUCLIDEAN SPACE UDC :514.13:
FACTA UNIVERSITATIS Seres: Mechancs, Aumac Cnrl and Rbcs Vl3, N, 00, pp 55-70 CONTRIBUTION TO THE DISCUSSION ON ABSOLUTE INTEGRATION OF DIFFERENTIAL EQUATIONS OF GEODESICS IN NON-EUCLIDEAN SACE UDC 5793:543:583(045)
More information( 1) β function for the Higgs quartic coupling λ in the standard model (SM) h h. h h. vertex correction ( h 1PI. Σ y. counter term Λ Λ.
funon for e Hs uar oun n e sanar moe (SM verex >< sef-ener ( PI Π ( - ouner erm ( m, ( Π m s fne Π s fne verex orreon ( PI Σ (,, ouner erm, ( reen funon ({ } Σ s fne Λ Λ Bn A n ( Caan-Smanz euaon n n (
More informationScattering at an Interface: Oblique Incidence
Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may
More informationThe automatic optimal control process for the operation changeover of heat exchangers
Te aua pal rl pre fr e pera agever f ea exager K. L. Lu B. eeyer 4 & M. L very f e Feeral Are Fre Haburg Geray very f Saga fr See & Telgy P. R. Ca Tg J very P. R. Ca 4 GKSS Reear Cere Geray Abra Crl prble
More informationDr. Kasra Etemadi February 20, 2007
Dr. Kasra Eeadi February, 7 Seady-Sae Sinusidal Analysis Sinusidal Surces: Elecric pwer disribued fr residences and businesses Radi cunicain All signal f pracical ineres are cpsed f sinusidal cpnens Furier
More informationDishonest casino as an HMM
Dshnes casn as an HMM N = 2, ={F,L} M=2, O = {h,} A = F B= [. F L F L 0.95 0.0 0] h 0.5 0. L 0.05 0.90 0.5 0.9 c Deva ubramanan, 2009 63 A generave mdel fr CpG slands There are w hdden saes: CpG and nn-cpg.
More information10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :
. A. IUITS Synopss : GOWTH OF UNT IN IUIT : d. When swch S s closed a =; = d. A me, curren = e 3. The consan / has dmensons of me and s called he nducve me consan ( τ ) of he crcu. 4. = τ; =.63, n one
More informationENGI 4421 Probability and Statistics Faculty of Engineering and Applied Science Problem Set 10 Solutions Chi-Square Tests; Simple Linear Regression
ENGI 441 Prbbly nd Sscs Fculy f Engneerng nd Appled Scence Prblem Se 10 Sluns Ch-Squre Tess; Smple Lner Regressn 1. Is he fllwng se f bservns f bjecs n egh dfferen drecns cnssen wh unfrm dsrbun? Drecn
More informationChapter 3, Solution 1C.
COSMOS: Cmplete Onlne Slutns Manual Organzatn System Chapter 3, Slutn C. (a If the lateral surfaces f the rd are nsulated, the heat transfer surface area f the cylndrcal rd s the bttm r the tp surface
More informationIs current gain generally significant in FET amplifiers? Why or why not? Substitute each capacitor with a
FET Sall Snal Mdband Mdel Ntatn: C arables and quanttes are enerally desnated wth an uppercase subscrpt. AC arables and quanttes are enerally desnated wth a lwercase subscrpt. Phasr ntatn wll be used when
More informationPHYS 1443 Section 001 Lecture #4
PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law
More informationPhysics 231 Ch 10 Day
Physcs 3 Ch Day 3 r., /5.6-.8 Scaerng R.b Mn., /8 Tues. /9 Wed.,/ Lab r., /.9-. Cllsn Clcans: Inelasc, Relasc, & Quanzed.5,. Deren Reerence raes L Cllsns (ballsc endulu?). Translanal Angular Menu Quz R.c
More informationRequired: Solution: 1.4)
CHAER.) ) 000 000 000 00 k b) 000, 000W 000,000 W 000,000 W 00, 000 W W ) d) k 8.... s 4... s.) 8 r nn n s 9 s p p p.) Gen:.4) n 9 r re r re / dy / r re n n / s dy ) 8 b) nn dy 4 0 0se nds dy 8400s r re
More informationTHE BOOST CONVERTER REVISITED
TH BOOST CONVT VSTD B. W. Wllams, T. C. m Deparmen f lecrnc and lecrcal ngneerng, Unersy f Srahclyde, Glasgw G XW, UK Absrac - The dc--dc bs cnerer s a sngleswch, sngle-nducr, swchng crcu used effcenly
More informationActive Load. Reading S&S (5ed): Sec. 7.2 S&S (6ed): Sec. 8.2
cte La ean S&S (5e: Sec. 7. S&S (6e: Sec. 8. In nteate ccuts, t s ffcult t fabcate essts. Instea, aplfe cnfuatns typcally use acte las (.e. las ae w acte eces. Ths can be ne usn a cuent suce cnfuatn,.e.
More informationAnalysis The characteristic length of the junction and the Biot number are
-4 4 The temerature f a gas stream s t be measured by a thermule. The tme t taes t regster 99 erent f the ntal ΔT s t be determned. Assumtns The juntn s sheral n shae wth a dameter f D 0.00 m. The thermal
More informationLecture 3: Resistive forces, and Energy
Lecure 3: Resisive frces, and Energy Las ie we fund he velciy f a prjecile ving wih air resisance: g g vx ( ) = vx, e vy ( ) = + v + e One re inegrain gives us he psiin as a funcin f ie: dx dy g g = vx,
More informationElectrostatic/magnetostatic forces
Eecsc/gnesc ces spes ppc: eneg e ec eneg ce (vec) ve (vec) en ( eneg ) ( snce) ne s cn gve e O ce (n pessue) u cn en snge sp cne s pe e ce spe epe: pe pes eecsc: ppe vge gnesc: cuen I Den. Nekk 00, s upe
More informationThe Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components
Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due
More informationLet s treat the problem of the response of a system to an applied external force. Again,
Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem
More informationComparison between the Discrete and Continuous Time Models
Comparison beween e Discree and Coninuous Time Models D. Sulsky June 21, 2012 1 Discree o Coninuous Recall e discree ime model Î = AIS Ŝ = S Î. Tese equaions ell us ow e populaion canges from one day o
More informationAdvanced time-series analysis (University of Lund, Economic History Department)
Advanced me-seres analss (Unvers of Lund, Economc Hsor Dearmen) 3 Jan-3 Februar and 6-3 March Lecure 4 Economerc echnues for saonar seres : Unvarae sochasc models wh Box- Jenns mehodolog, smle forecasng
More informationVibrations and Waves
Chaper 3 3 Vbraons and Waes PROBEM SOUIONS 3. (a) ang o he rgh as pose, he sprng orce acng on he bloc a he nsan o release s F s 30 N 0.3 7 N or 7 N o he le A hs nsan, he acceleraon s a F s 7 N 0.60 g 8
More informationNotes on the stability of dynamic systems and the use of Eigen Values.
Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon
More informationComparing Possibly Misspeci ed Forecasts
Supplemenl Appendx : Cmprng Pssbly Msspec ed Frecss Andrew J. Pn Duke Unversy 4 Augus Ts supplemenl ppendx cnns w prs. Appendx SA. cnns dervns used n e nlycl resuls presened n e pper. Appendx SA. cnns
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationA New Structure of Buck-Boost Z-Source Converter Based on Z-H Converter
Jurnal f Operan and Auman n wer Engneerng l. 4, N., ec., ages: 7-3 hp://jape.uma.ac.r A New rucure f Buck-Bs Z-urce nverer Based n Z-H nverer E. Babae*,. Ahmadzadeh Faculy f Elecrcal and mpuer Engneerng,
More informationOutline. Review Numerical Approach. Schedule for April and May. Review Simple Methods. Review Notation and Order
Sstes of Ordnar Dfferental Equatons Aprl, Solvng Sstes of Ordnar Dfferental Equatons Larr Caretto Mecancal Engneerng 9 Nuercal Analss of Engneerng Sstes Aprl, Outlne Revew bascs of nuercal solutons of
More informationI N A C O M P L E X W O R L D
IS L A M I C E C O N O M I C S I N A C O M P L E X W O R L D E x p l o r a t i o n s i n A g-b eanste d S i m u l a t i o n S a m i A l-s u w a i l e m 1 4 2 9 H 2 0 0 8 I s l a m i c D e v e l o p m e
More informationConservation of Energy
Chapter 8 Conseraton o Ener 8.3 U + K = U + K mh + = m ( ) + m ( 3.5 ) = ( ) + F= m = 3. n+ m= m 3. n = m = m =.m 3 n =. 5. 9.8 m s =.98 N downward FIG. 8.3 (5. 3.) Δ A B 8.4 (a) K = W = W = m Δ h = m
More informationrcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.
hapter 1 c) When the average bld velcity in the capillary is reduced by a factr f 10, the delivery f the slute t the capillary is liited s that the slute cncentratin after crit 0.018 c is equal t er at
More information3-42. Chapter 15 Steady Heat Conduction. Heat Conduction in Cylinders and Spheres
Chapter 5 Steady Heat Cnductn Heat Cnductn n Cylnders and Spheres 3-64C When the dameter f cylnder s very small cmpared t ts length, t can be treated as an ndefntely lng cylnder. Cylndrcal rds can als
More informationTHE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS
THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he
More informationBag for Sophia by Leonie Bateman and Deirdre Bond-Abel
Bag for Sopha 2012 by Leone Baeman and Derdre Bond-Abel Ths bag was desgned o go wh he beauful feled wool scarf of our book Elegan Quls, Counry Charm. Make boh and you ll have he perfec ensemble o wear
More informationModule 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur
Mdle Analysis f Saically Indeerminae Srcres by he Direc Siffness Mehd Versin CE IIT, Kharagr Lessn The Direc Siffness Mehd: Temerare Changes and Fabricain Errrs in Trss Analysis Versin CE IIT, Kharagr
More informationWater Hammer in Pipes
Waer Haer Hydraulcs and Hydraulc Machnes Waer Haer n Pes H Pressure wave A B If waer s flowng along a long e and s suddenly brough o res by he closng of a valve, or by any slar cause, here wll be a sudden
More informationû s L u t 0 s a ; i.e., û s 0
Te Hille-Yosida Teorem We ave seen a wen e absrac IVP is uniquely solvable en e soluion operaor defines a semigroup of bounded operaors. We ave no ye discussed e condiions under wic e IVP is uniquely solvable.
More informationFMPE: Discriminatively Trained Features for Speech Recogntion
F: Dcnavl Tand Fau f Spc Rcnn Danl Pv Ban Knbu Lda anu G San Han Slau Gff Zw IB T.J. an Rac Cn NY ICASSP 005 Pn: Fan-Hu Cu Ouln / Inducn f H-dnnal fau nan Acuc cnx xpann Fau pcn Tann ax Sn f upda Calculan
More informationLecture 17. Dielectric Materials
Lecture 17 Dielectric Materials 3/ 3 3 3/ 3/ 4 4 exp = = = e R R B B e B v c B g v c e k k k k E π π π Dielectric aterials play a large rle in electrnics. One exaple was te xide in te MOS structures. Als
More information( )a = "t = 1 E =" B E = 5016 V. E = BHv # 3. 2 %r. c.) direction of induced current in the loop for : i.) "t < 1
99 3 c dr b a µ r.? d b µ d d cdr a r & b d & µ c µ c b dr µ c µ c b & ' ln' a +*+* b ln r ln a a r a ' µ c b 'b* µ c ln' * & ln, &a a+ ncreang no he page o nduced curren wll creae a - feldou of he page
More information11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work
MÜHENDİSLİK MEKNİĞİ. HFT İş-Eneji Pwe f a fce: Pwe in he abiliy f a fce d wk F: The fce applied n paicle Q P = F v = Fv cs( θ ) F Q v θ Pah f Q v: The velciy f Q ÖRNEK: İŞ-ENERJİ ω µ k v Calculae he pwe
More informationIX Mechanics of Rigid Bodies: Planar Motion
X Mechancs of Rd Bodes: Panar Moton Center of Mass of a Rd Bod Rotaton of a Rd Bod About a Fed As Moent of nerta Penduu, A Genera heore Concernn Anuar Moentu puse and Coson nvovn Rd Bodes. Rd bod: dea
More informationCORRELATION EQUATIONS: FORCED AND FREE CONVECTION
CHAPER 0 0. Inroducion CORREAION EQUAIONS: FORCED AND FREE CONECION A ey facor in convecion is e ea e ea ransfer coefficien. Insead of deermining we deermine e ssel number, wic a dimensionless ea ransfer
More informationChapter 6 DETECTION AND ESTIMATION: Model of digital communication system. Fundamental issues in digital communications are
Chaper 6 DCIO AD IMAIO: Fndaenal sses n dgal concaons are. Deecon and. saon Deecon heory: I deals wh he desgn and evalaon of decson ang processor ha observes he receved sgnal and gesses whch parclar sybol
More informationPhysics 140. Assignment 4 (Mechanics & Heat)
Physis 14 Assignen 4 (Mehanis & Hea) This assignen us be handed in by 1 nn n Thursday 11h May. Yu an hand i in a he beginning f he leure n ha day r yu ay hand i yur labrary densrar befrehand if yu ish.
More informationPHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #10 Solutions November 19/20
PHY 40Y FOUNDTIONS OF PHYSICS 00-00 Tutrial Questins #0 Slutins Nveer 9/0 Dape an Driven Harnic Mtin, Resnance. ass f 0 g is cnnecte t a light spring having frce cnstant 5.4 N/. It is free t scillate n
More informationANALOG ELECTRONICS DR NORLAILI MOHD NOH
24 ANALOG LTRONIS lass 5&6&7&8&9 DR NORLAILI MOHD NOH 3.3.3 n-ase cnfguatn V V Rc I π π g g R V /p sgnal appled t. O/p taken f. ted t ac gnd. The hybd-π del pdes an accuate epesentatn f the sall-sgnal
More informationSection 14 Forces in Circular Motion
Secion 14 orces in Circular Moion Ouline 1 Unifor Circular Moion Non-unifor Circular Moion Phsics 04A Class Noes Wh do objecs do wha he do? The answer we have been invesigaing is forces If forces can eplain
More informationElectromagnetic energy, momentum and forces in a dielectric medium with losses
leroane ener, oenu and fores n a deler edu wh losses Yur A. Srhev he Sae Ao ner Cororaon ROSAO, "Researh and esn Insue of Rado-leron nneern" - branh of Federal Senf-Produon Cener "Produon Assoaon "Sar"
More informationOn Line Supplement to Strategic Customers in a Transportation Station When is it Optimal to Wait? A. Manou, A. Economou, and F.
On Line Spplemen o Sraegic Comer in a Tranporaion Saion When i i Opimal o Wai? A. Mano, A. Economo, and F. Karaemen 11. Appendix In hi Appendix, we provide ome echnical analic proof for he main rel of
More informationPHY2053 Summer 2012 Exam 2 Solutions N F o f k
HY0 Suer 0 Ea Slutns. he ree-bdy dagra r the blck s N F 7 k F g Usng Newtn s secnd law r the -cnents F a F F cs7 k 0 k F F cs7 (0 N ( Ncs7 N he wrk dne by knetc rctn k r csθ ( N(6 cs80 0 N. Mechancal energy
More information