Heat transfer between shell and rigid body through the thin heat-conducting layer taking into account mechanical contact
|
|
- Augustus Malone
- 5 years ago
- Views:
Transcription
1 Advanced Cmpuainal Meds in Hea Tansfe X 8 Hea ansfe beween sell and igid bdy ug e in ea-cnducing laye aking in accun mecanical cnac V. V. Zzulya Cen de Invesigación Cienífica de Yucaán, Méida, Yucaán, Meic Absac A pblem f ea cnducing and unilaeal cnac f a sell wi a igid bdy ug e ea-cnducing laye is fmulaed. An appac cnsiss in cnsideing a cange f laye ickness in e pcess f e sell defmain. F mdelling emelasic sae f e sell classical Kicff-Lve's mdel is epled. F mdelling ea cnduciviy f e sell epansin in a plynmial Legende seies in ems f e ickness is used. Cnac cndiins a ake in accun pssibiliies f unilaeal mecanical cnac and cange f ea ansfe cndiins beween sell and igid bdy ae fmulaed. Numeical eamples f e unilaeal emelasic cnac f e cylindical sells and igid bdy ug e ea-cnducing laye ae cnsideed. Influence f pysical and gemeical paamees f e sell and ea cnducing laye is invesigaed. Keywds: ea-cnduciviy, cylindical sell, ea-cnducing laye, mecanical cnac. Inducin Cnac ineacin is e ms cmmn way ansfe lad fm ne bdy ane. In e case f cnacing bdies aving diffeen empeaues beween em ea-cnac ineacins ake place. Teefe, n nly e cndiin f e mecanical cnac, bu als cndiins f e emal cnac ave be cnsideed. Usually, pefec emal cnac is assumed, i.e. i is assumed a e empeaue and e emal flu f e cnacing bdies in e cnac aea ae e same []. In numeus publicains [, 4 5] i was swn a in many cases ese cnac cndiins ae n accepable because ey can n ake in WIT Tansacins n Engineeing Sciences, Vl 6, 8 WIT Pess ISSN 74-5 (n-line) di:.495/ht88
2 8 Advanced Cmpuainal Meds in Hea Tansfe X accun pysical pcesses elaed defmain and ea ecange. In ese publicains e pblem f emelasic cnac f plaes and sells ave been cnsideed ug a ea-cnducin laye wi cnsideing cange f e laye ickness duing e plaes and sells defmain. Numeical eamples pesened ee sw a in many impan cases f science and engineeing e esul bained using pefec emelasic cnac cndiins and e cndiins wi cnsideing cange f e laye ickness in e pcess f defmain ae vey diffeen. In sme cases e diffeence is n nly quaniaive bu als qualiaive. Teefe, i is vey impan cnside cnac cndiins wic elae defmains and ea ansfe in e pblems wee in-walled sucues may ave cnac ug e ea-cnducing laye in e inensive empeaue field. Suc kinds f pblems ake place in many impan sucues, equipmen, and devices in cemical, aispace, nuclea indusies, ec. Te develped appac ave been applied e plaes and sells emelasic cnac pblems in [4 7, 5], e laminaed cmpsie maeials wi e pssibiliy f delaminain and emelasic cnac in empeaue field in [8, 9], and e pencil-in nuclea fuel ds mdeling in []. In is pape sme new esuls elaed unilaeal emelasic cnac f e aisymmeical cylindical sell ug e ea-cnducing laye ae fmulaed. Te cnneced equains f emelasiciy and ea cnduciviy ae ceaed. Tese equains ake in accun cange f e cndiins f ea ecange beween e sell and e igid bdy duing is defmain and pssibiliy f clse unilaeal mecanical cnac. Numeical eamples f e ea cnduciviy f e cylindical sells ug e ea-cnducing laye ae cnsideed. Te emmecanical effecs caused by cnac ineacin and ei influence n e emmecanics paamees ae invesigaed. Saemen f e pblem Le us cnside an aisymmeical cylindical sell wi paamees: is a + adius, is a ickness, l is a leng, and Ω ae middle, eenal and inenal sufaces f e sell. We cnside w siuains illusaed in e fig.: a) a igid punc is placed inside f e sell wi gap ( ) b) a cylindical sell placed inside f e cylindical le in e igid bdy wi gap ( ). Te ea is ansfeed fm e bdy suface ψ e sell and invesely ug e ea cnducing laye wic is n esised sell defmain. Te sell can be subjeced eenal mecanical lad p() and empeaue T (). Cnsequenly, e sell is defmed and can cme in mecanical cnac wi e igid bdy. As a ± esul is esablised as unknwn befe clse cnac aea Ωe = Ω ψ and fces f cnac ineacin g (). Tus we ave a siuain wi defmain influence n ea ecange and empeaue influence n defmain. In suc fmulain we ave cnneced e emelasic and ea cnducing pblem. In is case, equains f emelasiciy and ea cnduciviy cann WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
3 Advanced Cmpuainal Meds in Hea Tansfe X 8 be slved sepaaely. Te pssibiliy f unilaeal mecanical cnac ave be als aken in accun. Figue.. Equains f emelasiciy f e sell We will use ee a classical Kicff-Lve's sell ey. Accding is ey aial ε and cicula ε θ defmains f e sell middle suface ae defined by e equains du + dv du d w π ( z + w) π ( z) w w ε = = + z, ε = θ = () d d d π ( z) z and cespnding sesses by = E du d w w σ + z + + T ν α ( ν ), ν = E du d w w σ + z + + T θ ν ν α ( ν ), () ν wee u and w ae displacemens in aial and cicula diecins, E and ν ae mdulus f elasiciy and Pisn ai, T = T + T z is empeaue f e sell. Diffeenial equains f em-elasiciy ave e fm 4 d w 4 d T + 4β w = ( p g) a 4 T + a, () d D d 4 ( ν ) α ( ν ) α ( + ν ) wee β = a =, a = 4. Equains f ea cnduciviy f e sell Fllwing [4] we epesen empeaue f e sell in e fm z = T T, T = T + Tdz, T = Tzdz (4) WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
4 84 Advanced Cmpuainal Meds in Hea Tansfe X Ten diffeenial equains f ea cnduciviy ave e fm d T + + ( Q Q ) Q = d d T + + ( Q + Q ) Q + Q = (5) d Hee T i and Q i ae cefficiens f e plynmial epansin f e empeaue and ea flu. Tey ae elaed by equains = ( ) + Q T T, ( ) + 5 Q = T + T, Q = 5Q T, Q + Q = Q + Q Q + Q = Q (6) + + wee T, T, Q and especively. ( ). Bunday and cnac cndiins +, Q ae ei values n e sufaces Ω + and F finie leng sell we cnside e fllwing mecanical bunday cndiins. d w d w dw =, = - fee end; w L p =, = - fied end; d d d L p L p L p d w w L p =, = - simply supped end. (7) d L p F infinie leng sell we cnside e fllwing cndiins a infiniy dw d w d w w,,, f (8) d d d Bunday cndiins f e equains f ea cnduciviy ae L T L = T - if empeaue is pescibed; Ω dt L λ = q - if ea flu is pescibed; (9) d L Ω T α L + ( T T ) = - f cnvecive ea ansfe λ Ω L wee λ is a cefficien f ea cnduciviy, α is a cefficien ea ecange ug a suface. Mecanical and emal cnac cndiins ae pesened in e fm [4 7] w < g =, Ω + \ Ωe, w = g >, Ωe + λ( w) T + λ* T T = T k, T k = () λ( w) + λ* I is impan menin a emal cnac cndiins include sell deflecin w nnlinealy and eefe equain () elaes e equains f sell emelasiciy () and ea cnduciviy (5). As a esul we ave Ω WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
5 Advanced Cmpuainal Meds in Hea Tansfe X 85 cnneced nnlinea pblems f emelasiciy and ea cnduciviy wi unilaeal cnac cndiins..4 Tansfmain e inegal equain In [4, 6, 7, 5] i was swn a e diffeenial equains f e sell emelasiciy () and ea cnduciviy (5) can be ansfmed in e inegal equains f Hammesein's ype G (, y) F ( y) dy = T G, y F T y dy = wee F, ( ) ( ) l l W (, y) [ p( y) g( y) ] β F ( y) dy = w, () D l =.5ε ( T + Tk ) + ( Tk T ), F.5 ( Tk T ) + ( Tk + T )- T F = β ( F + ε T )- β T = ε, Te kenels in ese inegal equains ae fundamenal sluins f cespnding diffeenial peas. Tey ave e fm G (, y) = ep( ε y )/ ε, G (, y) = ep( ε y )/ ε () W (, y) = ep( β y )[ cs( β y ) + sin( β y )] 8β D wee 5 ( ν ) ατ ( ν ) α ε =, ε =, β =, β = + τ E, D = ν.5 Algim f e pblem sluin ( ) Algims f e pblem s sluin cnsiss in an ieaive pcess f e nnlinea inegal equains f Hammesein's ype sluin and in e case if unilaeal cnac aking place an addiinal ieaive algim is used. Te algim as been elabaed in [4, 6]. In e pblems unde cnsideain e algim is cnvegen and cnvegence is fas enug..6 Sess calculain Sesses in e aisymmeical cylindical sell ae calculaed by fmulas (), wic f cnvenience may be pesened in e fm E d w z σ = z ( + ν ) α T, (4) ν d σ θ = Ew α T E E + ν d w ν z ( + ν ) α T d z WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
6 86 Advanced Cmpuainal Meds in Hea Tansfe X Deiving fm () epessin f e secnd deivaive f e displacemens and subsiuing i in (4) we bain e fllwing inegal epesenains f sess = l d G( ξ, ) σ ( ) b T ( ξ ) dξ + (5) d wee b b l + [ ] d G( ξ, ) G( ξ, ) T ( ξ ) dξ bt ( ) b p( ξ ) q( ξ ) dξ d σ θ l [ ( ) + T ( z] Ew( ) ( ) = νσ ( ) + α E T ) 5 Eα z =, b ( + ν ) 6 z α b =, 6 ( +ν ) Eα z = τ, b 4 ( ) α τ 4 E z =, ( ν ) Ez ν α E z β =, z β =, β =. 8 Mizes sesses ae calculaed by e equains σ i = ( σ ) + ( σ )( σ ) + ( σ ), (6) σ ( q) ( ) ( ) q i = σ + σ σ + σ + Using equains (5) and (6) sesses in e sell can be easy calculaed. Invesigain f e em-mecanical sae f e sell We will cnside ee em-mecanical sae f e sell wi cnsideing influence f e sell defmain n e ea ansfe beween i and a igid bdy. Calculain ave been dne f e daa: maeial 5 5 ppeies: E =.5 MPa, ν =.5.5 α τ = C, λ = V m C and gemeical paamees =. 5m, =. m, l b =, Eample. We cnside an aisymmenical cylindical sell f infinie leng placed in e igid siup wi a mgeneus iniial gap as is swn in fig.. Tempeaue n e siup suface is n mgeneus and equal + T ( ) = Tm + Tb sin π / lb, Tb = 6 C Tm = C. (7) On e sell suface ac mgeneus lad p( ) = MPa, empeaue n e inenal suface f sell is T = C, iniial gap is equal =. 5 and λ = λ *. In fig. ae pesened: Mizes sesses n eenal σ + and inenal σ sufaces f e sell, fce f cnac ineacin g, nmalized bending W = w / and empeaue n cnac suface T k. Te dased lines cespnd a sluin f pefec emal cnac wiu cuning influence f e sell defmain n e ea ecange and e slid lines cespnd e sluin pesened ee. WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
7 Advanced Cmpuainal Meds in Hea Tansfe X 87 Figue. Figue. + Mizes sesses n eenal σ and inenal σ sufaces f e sell, fce f cnac ineacin g, f e same daa and iniial gap =. ae pesened in fig 4 and 5 eenal and inenal punc especively. Figue 4. Figue 5. Analysis f ese daa sws a n mgeneus empeaue disibuin cause significan sell defmains and clse mecanical cnac wi a igid siup. As a esul significan sess ccus in e sell. Calculains assuming pefec emal cnac lead significan inaccuacy, wic is n nly quaniaive bu als qualiaive. Eample. Hee we cnside an aisymmenical cylindical sell f infinie leng placed in e igid siup wi n mgeneus iniial gap, as swn in e Fig.6. Te gap is given by e funcin * ( ) = + sin π / l, =. 5, b = /, l b =. b b Figue 6. Figue 7. WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
8 88 Advanced Cmpuainal Meds in Hea Tansfe X In fig.7 ae pesened: Mizes sesses n eenal σ + and inenal σ sufaces f e sell, nmalized bending W = w / and empeaue n cnac suface T k. Te dased lines cespnd sluin f pefec emal cnac wiu cuning influence f e sell defmain n e ea ecange and e slid lines cespnd e sluin pesened ee. Analysis f ese daa sws, a n mgeneus iniial gap cause significan sell defmains. As a esul, in e sell, n significan mgeneus sess and empeaue disibuin ccus. Calculains assuming pefec emal cnac lead significan inaccuacy. Sme values f emmecanical sae diffe. Eample. We als invesigae influence f diffeen paamees n sell defmain and ea ecange. In fig. 8 ae pesened defmains and empeaue n e cnac suface f fied-end sell in mgeneus + empeaue field T = 5 C, T = C, f λ = 4λ*, =. 5. Figue 8. Figue 9. I is ineesing pin u a in e case wen T > T + accuning influence f e sell defmain n e ea ecange deceases is defmain, sess and empeaue disibuins. In fig. 9 is pesened dependence f e sell deflecin n is adius. Calculains ave been dne f e fllwing daa: λ = 5λ* =. 5, cuve f e eenal punc and Tb = 6 C, cuve f e inenal punc and Tb = C. I is impan menin a f eenal punc wen / > 5 dependence becmes nnlinea and e sell is aaced e punc, slid cuve. All e abve calculains ave been dne f e case wen n e sufaces Ω and ψ is pescibed empeaue. In fig. and fig. dependences w = f ( λ / λ* ) and w = f ( / ) f e eenal punc ae pesened. Cuves cespnd e case wen n e sufaces ψ empeaue and n e suface Ω ea flu ae se. Cuves cespnd e case wen n e sufaces Ω empeaue and ψ n e suface ea flu ae se. In b cases empeaue is disibued in accdance wi equain (7), ea ansfe ae is equal 4 4 q = [ V / m K] and q =.4 [ V / m K] f e fis and secnd cases WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
9 Advanced Cmpuainal Meds in Hea Tansfe X 89 especively. In e fis case sell deflecin is minimal f λ λ and / * = inceases wen / decease. In e secnd case sell deflecin is maimal f λ / λ* = and des n depend muc n /. In b cases sell deflecin des n cange muc f λ λ. / * > Figue. Figue. 4 Cnclusins Te esuls pesened ee sw a in many siuains in-walled sucues subjeced ig empeaue pefec emal cnac cndiins ae n accepable because ey cann ake in accun pysical pcesses elaed defmain and ea ecange. Suc kinds f pblems may ccu in diffeen field f science and engineeing, f eample in nuclea, aespace, cemical indusies, ec. In suc siuains e appac develped ee and in u pevius publicains ave be used. Refeences [] Bley B.A. and Weine J.H. Tey f emal sess, Wiley, New Yk, 96. [] Kan B. Ya., Zzulya V.V. Cnneced pblem n cnac plae wi igid bdy ug e ea-cnducing laye, Dclady Akademii Nauk Uk. SSR, 4, pp., 988. (in Russian) [] Psigac Ya. S, Sves P. N. Yu. M., Temelasiciy f in sells, Kiev, Naukva dumka, 978. (in Russian) [4] Zzulya V.V. Cnac cylindical sell wi a igid bdy ug e eacnducing laye, Dclady Akademii Nauk Uk. SSR, 989,, pp (in Russian) [5] Zzulya V.V. Te cmbined pblem f em- elasic cnac beween w plaes ug a ea cnducing laye, Junal Applied Maemaics and Mecanics, 5(5), pp.7 77, 989. [6] Zzulya V.V. Bending f a plae in empeaue field unde esicins, Izvesiya vuzv. Engineeing,, pp. 4 7, 99. (in Russian) WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
10 9 Advanced Cmpuainal Meds in Hea Tansfe X [7] Zzulya V.V. Cnac cylindical sell wi a igid bdy ug e eacnducing laye in ansiinal empeaue field, Mecanics f Slids, Vl., pp.6 65, 99. [8] Zzulya V. V. Nnpefec cnac f laminaed sells wi cnsideing debnding beween laminas in empeaue field, Teeical and Applied Mecanics, Vl. 4, pp.9 97, 6. [9] Zzulya V.V. Laminaed sells wi debnding beween laminas in empeaue field, Inenainal Applied Mecanics, Vl. 4(7), pp. 5 4, 6. [] Zzulya V.V. Maemaical Mdelling f Pencil-Tin Nuclea Fuel Rds, in Pc. SMIRT9 Cnf. Sucual Mecanics in Reac Tecnlgy, A. Gupa Ed., Tn, 7, pp. C4 C. [] Zzulya V.V. Cnac f a sell and igid bdy ug e ea-cnducing laye empeaue field, Inenainal Junal f Maemaical Mdels and Meds in Applied Sciences, (), pp.8 45, 7. [] Zzulya V.V. Cnac f e in-walled sucues and igid bdy ug e ea-cnducing laye, in Pc. Teeical and Epeimenal aspecs f ea and mass ansfe, Acapulc, Meic, pp. 45 5, 8. [] Zzulya V.V., Aguila M., Tem-elasic cnac and ea ansfe beween plaes ug e ea-cnducing laye, in Hea ansfe, B. Sunden and C.A. Bebbia Eds. Cmpuainal Mecanics Publicains, Suampn, UK and Bsn, USA, pp.,. [4] Zzulya V.V., Bdenk Yu. N. Temelasic cndiin f cylindical sell, wic ineacin wi a igid bdy ug e ea-cnducing laye, Izvesiay vuzv. Engineeing, 8, pp. 47 5, 99. (in Russian) [5] Zzulya V.V., Bdenk Yu. N. Cnnecing pblem n cnac f cylindical sells wi a igid bdy in empeaue ug e eacnducing laye, Dclady Akademii Nauk Uk. SSR, 4, pp.5 4, 99. (in Russian). WIT Tansacins n Engineeing Sciences, Vl 6, ISSN 74-5 (n-line) 8 WIT Pess
MEAN GRAVITY ALONG PLUMBLINE. University of New Brunswick, Department of Geodesy and Geomatics Engineering, Fredericton, N.B.
MEA GRAVITY ALG PLUMBLIE Beh-Anne Main 1, Chis MacPhee, Rbe Tenze 1, Pe Vaníek 1 and Macel Sans 1 1. Inducin 1 Univesiy f ew Bunswick, Depamen f Gedesy and Gemaics Engineeing, Fedeicn,.B., E3B 5A3, Canada
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 informationHeat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating
ISSN(Online): 319-8753 ISSN (Pin): 347-671 Inenaional Jounal of Innovaive Reseac in Science, Engineeing and Tecnology (An ISO 397: 7 Ceified Oganiaion) Vol 4, Issue 1, Decembe 15 Hea Concion Poblem in
More informationOutline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II
Steady Heat ansfe ebuay, 7 Steady Heat ansfe wit Cnductin and Cnvectin ay Caett Mecanical Engineeing 375 Heat ansfe ebuay, 7 Outline eview last lectue Equivalent cicuit analyses eview basic cncept pplicatin
More information2. The units in which the rate of a chemical reaction in solution is measured are (could be); 4rate. sec L.sec
Kineic Pblem Fm Ramnd F. X. Williams. Accding he equain, NO(g + B (g NOB(g In a ceain eacin miue he ae f fmain f NOB(g was fund be 4.50 0-4 ml L - s -. Wha is he ae f cnsumpin f B (g, als in ml L - s -?
More informationMaximum Cross Section Reduction Ratio of Billet in a Single Wire Forming Pass Based on Unified Strength Theory. Xiaowei Li1,2, a
Inenainal Fum n Enegy, Envinmen and Susainable evelpmen (IFEES 06 Maximum Css Sein Reduin Rai f Bille in a Single Wie Fming Pass Based n Unified Sengh They Xiawei Li,, a Shl f Civil Engineeing, Panzhihua
More informationExample
hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a
More informationOn Control Problem Described by Infinite System of First-Order Differential Equations
Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical
More informationSTUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION
Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE
More informationPhysics Courseware Electromagnetism
Pysics Cousewae lectomagnetism lectic field Poblem.- a) Find te electic field at point P poduced by te wie sown in te figue. Conside tat te wie as a unifom linea cage distibution of λ.5µ C / m b) Find
More informationLecture 3. Electrostatics
Lecue lecsics In his lecue yu will len: Thee wys slve pblems in elecsics: ) Applicin f he Supepsiin Pinciple (SP) b) Applicin f Guss Lw in Inegl Fm (GLIF) c) Applicin f Guss Lw in Diffeenil Fm (GLDF) C
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 informationMaxwell Equations. Dr. Ray Kwok sjsu
Maxwell quains. Ray Kwk sjsu eeence: lecmagneic Fields and Waves, Lain & Csn (Feeman) Inducin lecdynamics,.. Giihs (Penice Hall) Fundamenals ngineeing lecmagneics,.k. Cheng (Addisn Wesley) Maxwell quains.
More informationVisco-elastic Layers
Visc-elasic Layers Visc-elasic Sluins Sluins are bained by elasic viscelasic crrespndence principle by applying laplace ransfrm remve he ime variable Tw mehds f characerising viscelasic maerials: Mechanical
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 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 informationApplication of Fractional Calculus in Food Rheology E. Vozáry, Gy. Csima, L. Csapó, F. Mohos
Applicain f Facinal Calculus in F Rhelgy Szen Isán Uniesiy, Depamen f Physics an Cnl Vzay.sze@ek.szie.hu Keyws: facinal calculus, iscelasic, f, ceep, ecey Absac. In facinal calculus he e (β) f iffeeniain
More informationStrees Analysis in Elastic Half Space Due To a Thermoelastic Strain
IOSR Junal f Mathematics (IOSRJM) ISSN: 78-578 Vlume, Issue (July-Aug 0), PP 46-54 Stees Analysis in Elastic Half Space Due T a Themelastic Stain Aya Ahmad Depatment f Mathematics NIT Patna Biha India
More informationa. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with
Aignmen #5 EE7 / Fall 0 / Aignmen Sluin.7 hermal cnducin Cnider bra ally wih an X amic fracin f Zn. Since Zn addiin increae he number f cnducin elecrn, we have cale he final ally reiiviy calculaed frm
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 informationNumerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1
Numerical Analysis MTH60 PREDICTOR CORRECTOR METHOD Te metods presented so far are called single-step metods, were we ave seen tat te computation of y at t n+ tat is y n+ requires te knowledge of y n only.
More informationThe Flatness Problem as A Natural Cosmological Phenomenon
Inenainal Junal f Pue and Applied Physics ISSN 0973-1776 Vlume 4, Numbe (008), pp. 161 169 Reseach India Publicains hp://www.ipublicain.cm/ijpap.hm The Flaness Pblem as A Naual Csmlgical Phenmenn 1 Maumba
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 information( ) ( ) Last Time. 3-D particle in box: summary. Modified Bohr model. 3-dimensional Hydrogen atom. Orbital magnetic dipole moment
Last Time 3-dimensional quantum states and wave functions Couse evaluations Tuesday, Dec. 9 in class Deceasing paticle size Quantum dots paticle in box) Optional exta class: eview of mateial since Exam
More informationUniversity of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering
Univesity f Pisa - ITALY - Depatment f Mechanical, Nuclea and Pductin Engineeing Them-Mechanical Behaviu f Li 4 SO 4 and Li TiO 3 N. Zaccai, D. Aqua Cntents f Pesentatin This pesentatin descibes the them-mechanical
More informationDesign Guideline for Buried Hume Pipe Subject to Coupling Forces
Design Guideline fo Buied Hume Pipe Sujec o Coupling Foces Won Pyo Hong 1), *Seongwon Hong 2), and Thomas Kang 3) 1) Depamen of Civil, nvionmenal and Plan ngineeing, Chang-Ang Univesiy, Seoul 06974, Koea
More information( ) ( ) CHAPTER 8. Lai et al, Introduction to Continuum Mechanics. Copyright 2010, Elsevier Inc 8-1
CHAPER 8 81 Shw ha f an incmpessible Newnian fluid in Cuee flw he pessue a he ue cylinde ( R ) is always lage han ha a he inne cylinde ha is bain R i Ri ρ ω R R d B Ans In Cuee flw v vz and vθ A+ [see
More information( t) Steady Shear Flow Material Functions. Material function definitions. How do we predict material functions?
Rle f aeial Funins in Rhelgial Analysis Rle f aeial Funins in Rhelgial Analysis QUALIY CONROL QUALIAIVE ANALYSIS QUALIY CONROL QUALIAIVE ANALYSIS mpae wih he in-huse daa n qualiaive basis unknwn maeial
More informationOverview. Overview Page 1 of 8
COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSITE BEAM DESIGN AISC-LRD93 Tecnical Noe Compac and Noncompac Requiemens Tis Tecnical Noe descibes o e pogam cecks e AISC-LRD93 specificaion
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 informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
More informationProblem Set 5: Universal Law of Gravitation; Circular Planetary Orbits
Poblem Set 5: Univesal Law of Gavitation; Cicula Planetay Obits Design Engineeing Callenge: Te Big Dig.007 Contest Evaluation of Scoing Concepts: Spinne vs. Plowe PROMBLEM 1: Daw a fee-body-diagam of a
More informationA Numerical Hydration Model of Portland Cement
A Numeical Hydaion Model of Poland Cemen Ippei Mauyama, Tesuo Masushia and Takafumi Noguchi ABSTRACT : A compue-based numeical model is pesened, wih which hydaion and micosucual developmen in Poland cemen-based
More informationDevelopment of a Simplified Theoretical Model for Dynamic Burst Time And Pressure of a Cylindrical Shell
Te Open Ocean Engineeing Jounal 9 6 Open Access Developmen of a Simplified Teoeical Model fo Dynamic Bus Time And essue of a Cylindical Sell Cunjiang Ceng and G E Oo Widea Bjoksen Reseac Lab BIT 7 INC
More informationTotal Deformation and its Role in Heavy Precipitation Events Associated with Deformation-Dominant Flow Patterns
ADVANCES IN ATMOSPHERIC SCIENCES VOL. 25 NO. 1 2008 11 23 Tal Defmain and is Rle in Heavy Pecipiain Evens Assciaed wih Defmain-Dminan Flw Paens GAO Shuing 1 (påë) YANG Shuai 12 (fl R) XUE Ming 3 (Å ) and
More informationPart 2: CM3110 Transport Processes and Unit Operations I. Professor Faith Morrison. CM2110/CM Review. Concerned now with rates of heat transfer
CM30 anspot Pocesses and Unit Opeations I Pat : Pofesso Fait Moison Depatment of Cemical Engineeing Micigan ecnological Uniesity CM30 - Momentum and Heat anspot CM30 Heat and Mass anspot www.cem.mtu.edu/~fmoiso/cm30/cm30.tml
More informationCHAPTER 24 GAUSS LAW
CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and
More informationPressure Vessels Thin and Thick-Walled Stress Analysis
Pessue Vessels Thin and Thick-Walled Sess Analysis y James Doane, PhD, PE Conens 1.0 Couse Oveview... 3.0 Thin-Walled Pessue Vessels... 3.1 Inoducion... 3. Sesses in Cylindical Conaines... 4..1 Hoop Sess...
More informationBrace-Gatarek-Musiela model
Chaper 34 Brace-Gaarek-Musiela mdel 34. Review f HJM under risk-neural IP where f ( T Frward rae a ime fr brrwing a ime T df ( T ( T ( T d + ( T dw ( ( T The ineres rae is r( f (. The bnd prices saisfy
More information= h. Geometrically this quantity represents the slope of the secant line connecting the points
Section 3.7: Rates of Cange in te Natural and Social Sciences Recall: Average rate of cange: y y y ) ) ), ere Geometrically tis quantity represents te slope of te secant line connecting te points, f (
More informationCHAPTER GAUSS'S LAW
lutins--ch 14 (Gauss's Law CHAPTE 14 -- GAU' LAW 141 This pblem is ticky An electic field line that flws int, then ut f the cap (see Figue I pduces a negative flux when enteing and an equal psitive flux
More informationSpecial Vector Calculus Session For Engineering Electromagnetics I. by Professor Robert A. Schill Jr.
pecil Vect Clculus essin Engineeing Electmgnetics I Pfess et. cill J. pecil Vect Clculus essin f Engineeing Electmgnetics I. imple cmputtin f cul diegence nd gdient f ect. [peicl Cdinte stem] Cul Diegence
More informationTransient Radial Flow Toward a Well Aquifer Equation, based on assumptions becomes a 1D PDE for h(r,t) : Transient Radial Flow Toward a Well
ansien Radial Flw wad a Well Aqife Eqain, based n assmpins becmes a D PDE f h(,) : -ansien flw in a hmgenes, ispic aqife -flly peneaing pmping well & infinie, hiznal, cnfined aqife f nifm hickness, hs
More informationGCSE: Volumes and Surface Area
GCSE: Volumes and Suface Aea D J Fost (jfost@tiffin.kingston.sc.uk) www.dfostmats.com GCSE Revision Pack Refeence:, 1, 1, 1, 1i, 1ii, 18 Last modified: 1 st August 01 GCSE Specification. Know and use fomulae
More informationApplication of Net Radiation Transfer Method for Optimization and Calculation of Reduction Heat Transfer, Using Spherical Radiation Shields
Wld Applied Sciences Junal (4: 457-46, 00 ISSN 88-495 IDOSI Publicatins, 00 Applicatin f Net Radiatin Tansfe Methd f Optimizatin and Calculatin f Reductin Heat Tansfe, Using Spheical Radiatin Shields Seyflah
More informationOBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470
Assignment 7 Paallel Resnance OBJECTIVE T investigate the paallel cnnectin f R,, and C. EQUIPMENT REQUIRED Qty Appaatus 1 Electicity & Electnics Cnstuct EEC470 1 Basic Electicity and Electnics Kit EEC471-1
More informationWater Tunnel Experiment MAE 171A/175A. Objective:
Wate Tunnel Expeiment MAE 7A/75A Objective: Measuement of te Dag Coefficient of a Cylinde Measuement Tecniques Pessue Distibution on Cylinde Dag fom Momentum Loss Measued in Wake it lase Dopple Velocimety
More information5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:
5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the
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 informationdm dt = 1 V The number of moles in any volume is M = CV, where C = concentration in M/L V = liters. dcv v
Mg: Pcess Aalyss: Reac ae s defed as whee eac ae elcy lue M les ( ccea) e. dm he ube f les ay lue s M, whee ccea M/L les. he he eac ae beces f a hgeeus eac, ( ) d Usually s csa aqueus eeal pcesses eac,
More information02. MOTION. Questions and Answers
CLASS-09 02. MOTION Quesions and Answers PHYSICAL SCIENCE 1. Se moves a a consan speed in a consan direcion.. Reprase e same senence in fewer words using conceps relaed o moion. Se moves wi uniform velociy.
More informationPart 2 KINEMATICS Motion in One and Two Dimensions Projectile Motion Circular Motion Kinematics Problems
Pa 2 KINEMATICS Min in One and Tw Dimensins Pjecile Min Cicula Min Kinemaics Pblems KINEMATICS The Descipin f Min Physics is much me han jus he descipin f min. Bu being able descibe he min f an bjec mahemaically
More informationLast lecture (#4): J vortex. J tr
Last lecture (#4): We completed te discussion of te B-T pase diagram of type- and type- superconductors. n contrast to type-, te type- state as finite resistance unless vortices are pinned by defects.
More informationThermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850)
emal-fluids I Capte 7 Steady eat conduction D. Pimal Fenando pimal@eng.fsu.edu P: (850 40-633 Steady eat conduction Hee we conside one dimensional steady eat conduction. We conside eat tansfe in a plane
More informationLIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION
LIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION LAURA EVANS.. Introduction Not all differential equations can be explicitly solved for y. Tis can be problematic if we need to know te value of y
More informationβ A Constant-G m Biasing
p 2002 EE 532 Anal IC Des II Pae 73 Cnsan-G Bas ecall ha us a PTAT cuen efeence (see p f p. 66 he nes) bas a bpla anss pes cnsan anscnucance e epeaue (an als epenen f supply lae an pcess). Hw h we achee
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 informationOn orthonormal Bernstein polynomial of order eight
Oen Science Junal f Mathematic and Alicatin 2014; 22): 15-19 Publihed nline Ail 20, 2014 htt://www.enciencenline.cm/junal/jma) On thnmal Bentein lynmial f de eight Suha N. Shihab, Tamaa N. Naif Alied Science
More informationThe Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook
The Gadient and Applicatins This unit is based n Sectins 9.5 and 9.6 Chapte 9. All assigned eadings and eecises ae fm the tetbk Objectives: Make cetain that u can define and use in cntet the tems cncepts
More information158 Calculus and Structures
58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you
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 informationDepartment of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN
D. Keffe - ChE 40: Hea Tansfe and Fluid Flow Deamen of Chemical Enee Uniesi of Tennessee Pof. Daid Keffe Couse Lecue Noes SIXTEEN SECTION.6 DIFFERENTIL EQUTIONS OF CONTINUITY SECTION.7 DIFFERENTIL EQUTIONS
More informationFundamental concept of metal rolling
Fundamental cncept metal rlling Assumptins 1) Te arc cntact between te rlls and te metal is a part a circle. v x x α L p y y R v 2) Te ceicient rictin, µ, is cnstant in tery, but in reality µ varies alng
More informationFundamental Vehicle Loads & Their Estimation
Fundaenal Vehicle Loads & Thei Esiaion The silified loads can only be alied in he eliinay design sage when he absence of es o siulaion daa They should always be qualified and udaed as oe infoaion becoes
More informationImpact Switch Study Modeling & Implications
L-3 Fuzing & Ordnance Sysems Impac Swich Sudy Mdeling & Implicains Dr. Dave Frankman May 13, 010 NDIA 54 h Annual Fuze Cnference This presenain cnsiss f L-3 Crprain general capabiliies infrmain ha des
More informationGEOID-QUASIGEOID CORRECTION IN FORMULATION OF THE FUNDAMENTAL FORMULA OF PHYSICAL GEODESY. Robert Tenzer 1 Petr Vaníček 2
GEID-QUASIGEID CECTI I FMULATI F TE FUDAMETAL FMULA F PYSICAL GEDESY be Tenze 1 Pe Vaníček 1 Depamen f Gedesy and Gemaics Enineein Univesiy f ew Bunswick P Bx 4400 Fedeicn ew Bunswick Canada E3B 5A3; Tel
More informationSection 15.6 Directional Derivatives and the Gradient Vector
Section 15.6 Directional Derivatives and te Gradient Vector Finding rates of cange in different directions Recall tat wen we first started considering derivatives of functions of more tan one variable,
More informationSec. 9.1 Lines and Angles
Sec. 9. Line and Angle Leaning Objective:. Identify line, line egment, ay, and angle.. Claify angel a acute, igt, btue, taigt.. Identify cmplementay and upplementay angle. 4. Find meaue f angle. 5. Key
More informationElastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density
Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially
More informationControl Volume Derivation
School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass
More informationHotelling s Rule. Therefore arbitrage forces P(t) = P o e rt.
Htelling s Rule In what fllws I will use the tem pice t dente unit pfit. hat is, the nminal mney pice minus the aveage cst f pductin. We begin with cmpetitin. Suppse that a fim wns a small pa, a, f the
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 information3 ) = 10(1-3t)e -3t A
haper 6, Sluin. d i ( e 6 e ) 0( - )e - A p i 0(-)e - e - 0( - )e -6 W haper 6, Sluin. w w (40)(80 (40)(0) ) ( ) w w w 0 0 80 60 kw haper 6, Sluin. i d 80 60 40x0 480 ma haper 6, Sluin 4. i (0) 6sin 4-0.7
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationA) N B) 0.0 N C) N D) N E) N
Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce
More informationNSEP EXAMINATION
NSE 00-0 EXAMINATION CAEE OINT INDIAN ASSOCIATION OF HYSICS TEACHES NATIONAL STANDAD EXAMINATION IN HYSICS 00-0 Tal ie : 0 inues (A-, A- & B) AT - A (Tal Maks : 80) SUB-AT A- Q. Displaceen f an scillaing
More informationPropagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface
Applied Mahemaical Sciences Vol. 7 no. 9 49 437 Popagaion of Tosional Sface Waves in Heeogeneos Half-Space wih Iegla Fee Sface M. M. Selim Depamen of Mahemaics Facly of Еdcaion Se Canal Univesiy Se Egyp
More informationJournal of Theoretics
Junal f Theetics Junal Hme Page The Classical Pblem f a Bdy Falling in a Tube Thugh the Cente f the Eath in the Dynamic They f Gavity Iannis Iaklis Haanas Yk Univesity Depatment f Physics and Astnmy A
More informationAutomatic Measuring of English Language Proficiency using MT Evaluation Technology
Aumaic Measuing f English Language Pficiency using MT Evaluain Technlgy Keiji Yasuda ATR Spken Language Tanslain Reseach Labaies Depamen f SLR 2-2-2 Hikaidai, Keihanna Science Ciy Ky 69-0288 Japan keiji.yasuda@a.jp
More informationREVIEW SHEET 1 SOLUTIONS ( ) ( ) ( ) x 2 ( ) t + 2. t x +1. ( x 2 + x +1 + x 2 # x ) 2 +1 x ( 1 +1 x +1 x #1 x ) = 2 2 = 1
REVIEW SHEET SOLUTIONS Limit Concepts and Problems + + + e sin t + t t + + + + + e sin t + t t e cos t + + t + + + + + + + + + + + + + t + + t + t t t + + + + + + + + + + + + + + + + t + + a b c - d DNE
More informationDo not turn over until you are told to do so by the Invigilator.
UNIVERSITY OF EAST ANGLIA School of Mathematics Main Seies UG Examination 2015 16 FLUID DYNAMICS WITH ADVANCED TOPICS MTH-MD59 Time allowed: 3 Hous Attempt QUESTIONS 1 and 2, and THREE othe questions.
More informationChapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1
hapte ONE DIMENSIONAL SEADY SAE ONDUION hapte hee 38 HEA ONDUION HOUGH OMPOSIE EANGULA WALLS empeatue pofile A B X X 3 X 3 4 X 4 Χ A Χ B Χ hapte hee 38 hemal conductivity Fouie s law ( is constant) A A
More informationNUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS
Join Inenaional Confeence on Compuing and Decision Making in Civil and Building Engineeing June 14-16, 26 - Monéal, Canada NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS ABSTRACT
More informationMath 212-Lecture 9. For a single-variable function z = f(x), the derivative is f (x) = lim h 0
3.4: Partial Derivatives Definition Mat 22-Lecture 9 For a single-variable function z = f(x), te derivative is f (x) = lim 0 f(x+) f(x). For a function z = f(x, y) of two variables, to define te derivatives,
More informationCHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from
CHAPTE 7 CHONOPOTENTIOMETY In his echnique he curren flwing in he cell is insananeusly sepped frm zer sme finie value. The sluin is n sirred and a large ecess f suppring elecrlye is presen in he sluin;
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 informationA) (0.46 î ) N B) (0.17 î ) N
Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes
MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.7J Fall 13 Lecure 15 1/3/13 I inegral fr simple prcesses Cnen. 1. Simple prcesses. I ismery. Firs 3 seps in cnsrucing I inegral fr general prcesses 1 I inegral
More informationFinding and Using Derivative The shortcuts
Calculus 1 Lia Vas Finding and Using Derivative Te sortcuts We ave seen tat te formula f f(x+) f(x) (x) = lim 0 is manageable for relatively simple functions like a linear or quadratic. For more complex
More informationSuggested solutions, FYS 500 Classical Mechanics and Field Theory 2015 fall
UNIVERSITETET I STAVANGER Institutt for matematikk og naturvitenskap Suggested solutions, FYS 500 Classical Mecanics and Field Teory 015 fall Set 1 for 16/17. November 015 Problem 68: Te Lagrangian for
More informationMEM202 Engineering Mechanics Statics Course Web site:
0 Engineeing Mechanics - Statics 0 Engineeing Mechanics Statics Cuse Web site: www.pages.dexel.edu/~cac54 COUSE DESCIPTION This cuse cves intemediate static mechanics, an extensin f the fundamental cncepts
More informationACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019
ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS MATH00030 SEMESTER 208/209 DR. ANTHONY BROWN 6. Differential Calculus 6.. Differentiation from First Principles. In tis capter, we will introduce
More informationWYSE Academic Challenge Sectional Mathematics 2006 Solution Set
WYSE Academic Challenge Sectinal 006 Slutin Set. Cect answe: e. mph is 76 feet pe minute, and 4 mph is 35 feet pe minute. The tip up the hill takes 600/76, 3.4 minutes, and the tip dwn takes 600/35,.70
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 informationJournal of Solid Mechanics and Materials Engineering
Junal f Slid Mechanics and Mateials Engineeing Vl. 4, N. 8, 21 Themal Stess and Heat Tansfe Cefficient f Ceamics Stalk Having Ptubeance Dipping int Mlten Metal* Na-ki NOD**, Henda**, Wenbin LI**, Yasushi
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 informationGAMS Handout 2. Utah State University. Ethan Yang
Uah ae Universiy DigialCmmns@UU All ECAIC Maerials ECAIC Repsiry 2017 GAM Handu 2 Ehan Yang yey217@lehigh.edu Fllw his and addiinal wrs a: hps://digialcmmns.usu.edu/ecsaic_all Par f he Civil Engineering
More informationPROBLEM SET 5. SOLUTIONS March 16, 2004
Havad-MIT ivision of Health Sciences and Technology HST.54J: Quantitative Physiology: Ogan Tanspot Systems Instuctos: Roge Mak and Jose Venegas MASSACHUSETTS INSTITUTE OF TECHNOLOGY epatments of Electical
More informationThe Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie
e Quanum eory of Aoms and Molecules: e Scrodinger equaion Hilary erm 008 Dr Gran Ricie An equaion for maer waves? De Broglie posulaed a every paricles as an associaed wave of waveleng: / p Wave naure of
More informationAnnouncements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do
Wed., /11 Thus., /1 Fi., /13 Mn., /16 Tues., /17 Wed., /18 Thus., /19 Fi., / 17.7-9 Magnetic Field F Distibutins Lab 5: Bit-Savat B fields f mving chages (n quiz) 17.1-11 Pemanent Magnets 18.1-3 Mic. View
More information