Design optimal of refrigeration insulations

Size: px
Start display at page:

Download "Design optimal of refrigeration insulations"

Transcription

1 Issu 5, Volum 7, Dsign optimal of rfrigration insulations Ioan Sarbu, Emilian Stfan Vala, and Gabril Ostaf Abstract Economic opration with minimal nrgy consumption and low costs of a coold room or a rfrigrant piping systm dpnds largly on th quality and thicknss of thir insulation. h classical mthod of insulation rating for rfrigration systms is basd on rspct of th condition to prvnt condnsation of watr vapours in th air on th surfac of insulation or on limiting hat gain, but rarly lads to optimum in trms of a tchnical and conomic critrion. In this papr ar dscribd som typs of insulation for rfrigration applications and is dvlopd a rating optimation modl of ths insulations with a high lvl of gnrality. It uss multipl dynamic optimation critria simpl or compound, which bttr rflcts th conomic and nrgy complx aspcts, prsnt and futur. Basd on this modl wr laboratd two computr programs implmntd on PC microsystms. Numrical xampls will b prsntd to dmonstrat th accuracy and fficincy of th proposd optimation modl. hs show th good prformanc of th nw modl. Kywords Coold rooms, Rfrigrant piping, Insulation rating, Optimation modl, Comparativ analysis. I. INRODUCION HE rol of rfrigration systm insulation is to rduc hat flow to coold spacs or to cold dvics and pips in which th rfrigrant tmpratur blow ambint tmpratur (fr air, soil or nighbouring rooms). hrfor, rfrigration insulation is commonly usd to rduc nrgy consumption of rfrigrating systms and quipmnt. Economic opration of a coold room or a cold pip dpnds largly on th quality and thicknss of thir insulation. Hnc th propr slction importanc of th insu-lation matrial and rating of thir rfrigration insulations, lading to judicious us of invstmnt funds, to normal opration with minimal nrgy consumption and low costs. Cllular glass, flxibl lastomric, minral wool, polyisocyanurat, and xpandd or xtrudd polystyrn ar insulation matrials commonly usd in rfrigrant applications. h classical mthod of insulation rating for rfrigration systms is basd on rspct of th condition to prvnt condnsation of watr vapours in th air on th surfac of insulation, but rarly lads to optimum in trms of a tchnical and conomic rason. In cas of flat surfacs is usd hat Ioan Sarbu is currntly a Profssor and Dpartmnt Had at th Building Srvics Enginring Dpartmnt, Polithnica Univrsity of imisoara, ROMANIA, -mail addrss: ioan.sarbu@ct.upt.ro Emilian Stfan Vala is currntly a Lcturr at th Building Srvics Enginring Dpartmnt, Polithnica Univrsity of imisoara, ROMANIA, -mail addrss: milian.vala@ct.upt.ro Gabril Ostaf is currntly a Assistant Profssor at th Building Srvics Enginring Dpartmnt, Polithnica Univrsity of imisoara, ROMANIA, -mail addrss: gabril.ostaf@ct.upt.ro transfr quation which admits a hat gain so that nithr rsults too thick xpnsiv insulation, nor vry high cool consumption. In spcialty litratur [2], [11] ar rcommndd thicknsss for rfrigration insulation basd on condnsation control or for limiting hat gain. h most conomical insulation thicknss can b dtrmind by considring both initial costs and long-trm nrgy savings. Optimal computation of th insulations applid to coold rooms and to cold pips basd on conomic critria of minimum total lif-cycl cost lads to insulation thicknss that applid in practic bcom incorrct at som point aftr th xcution, bcaus pric volution in tim. h nrgy costs ar volatil, and a ful cost inflation factor may incras mor quickly than gnral inflation. In this papr is dvlopd a computational modl of th optimal thicknss of ths insulations, with a high lvl of gnrality. his modl uss multipl dynamic optimation critria simpl or compound, which bttr rflcts th conomic and nrgy complx aspcts, prsnt and futur. Basd on this optimation modl ar laboratd two computr programs implmntd on PC microsystms. II. YPES OF INSULAION FOR REFRIGERAION APPLICAIONS Rfrigration systms covr a broad spctrum of application tmpraturs and nvironmnts. But thy all fac th sam issus rlating to both condnsation control and moistur. Sinc moistur is a good thrmal conductor, its prsnc in an insulation systm is highly dtrimntal. Unlik hot systms, whr marginal insulation may rsult in incrasd nrgy us (and addd cost), rfrigration systms fac condnsation, which oftn lads to complt systm failur. Evn with today s high nrgy costs, th dsign thicknss in most rfrigration applications is dictatd by what is ndd to prvnt condnsation, rathr than by conomic payback. Rfrigration systms typically oprat in th rang of 5 C (for Fron systms) to as low as 45 C (for ammonia systms). hy can us a varity of rfrigrants and fluids in addition to Fron and ammonia, including glycol, brin, and othr spcialty fluids. Coppr, iron, stainlss stl, or othr piping matrials may b usd to carry th cooling mdium. ypical applications includ thos in suprmarkts, bvrag dispnsing lins, chillrs, and food procssing, frzing, and storag facilitis. Othr applications includ thos at ic rinks and various uniqu applications. All of ths applications shar common concrns rgarding condnsation control and long-trm rliability, but thy also hav particular issus with installation, rquird thicknss, and th nvironmntal conditions in which thy oprat.

2 Issu 5, Volum 7, Rliability should b th primary concrn whn considring th dsign and installation for any application. Dsign must considr factors including th application tmpratur, nvironmntal considrations, consquncs if a failur occurs, and xpctations of th job by th ownrs (longvity of th systm, asthtics, tc.). h following ar som important faturs of th insulation in various rfrigration applications: thrmal conductivity; watr vapor transmission (WV) proprtis; watr absorption proprtis; cofficint of thrmal xpansion; moistur wicking. hr ar rcommndd th following insulation matrials for rfrigration applications [2]: cllular glass, closd-cll phnolic, flxibl lastomric, polyisocyurant, and polystyrn. All of ths matrials ar closd-cll foam matrials, which mans thy will hav good WV and low watr absorption charactristics. In all cass, th ntir systm (sams, butt joints, and trmination points) must b compltly sald with adhsivs to protct against air intrusion into th systm, which would carry moistur and rsult in condnsation btwn th cold pip and th insulation. Rlying on a singl, concntratd vapor rtardr is not rcommndd. Gnrally, closd-cll foam insulations ar usd for ths applications. Sams should b minimd. On multilayr systms, th sams should b staggrd. apd sams ar only allowd as a complimntary closur systm. Suprmarkts ar on of th biggst and most noticabl applications for rfrigration systms. hy fac svral issus, including changs in rfrigrant, coldr lin tmpraturs, highr tmpratur hot gas dfrost cycls, changing stor dsigns, and prssurs to rduc installation tim to dcras stor build tim. In [2] ar dtaild many of th issus rlatd to this markt sgmnt. Using prinsulatd pip hangrs is a concpt that is gaining accptanc in suprmarkts bcaus it savs tim and improvs rliability by rducing condnsation at hangr locations. h majority of piping on a suprmarkt is indoors, but for th outdoor and rooftop sctions, th us of flxibl jacktingpolyvinyl chlorid (PVC), AL laminats, tc., is bing valuatd, ithr installd at th job sit or factory applid to improv th longvity and apparanc of th job. Us of protctiv coatings that nd priodic maintnanc is bcoming lss spcifid. Rfrigration piping on most suprmarkts is found insid, but som stors ar dsignd with 90% of th piping on th roof. Som lastomric insulation products ar bing promotd as ultraviolt (UV) rsistant and accptabl for us outdoors without th additional protction of coatings, jackts, or cladding matrials. But UV protction is not th only issu whn it coms to outdoor applications. Mchanical abus (by birds, cats, popl, tc.) and nvironmntal abus (by hail, sand, dirt, wind, rain, tc.) play a rol in th rliability and longvity of th insulation systm. For optimum prformanc, coatings, jackting, or cladding should b usd for outdoor applications. h insulation systm installd on a suprmarkt rfrigration systm must b highly rliabl, as it will oprat 24 hours a day for up to 10 yars. Closd-cll lastomric matrials hav bn usd in this application for many yars bcaus thy ar xtrmly rliabl and cost-ffctiv. It is a primary product usd for suprmarkt rfrigration applications bcaus of its low WV, allowabl us tmpratur rang, and as of installation. Using a coating or flxibl jackting can improv th apparanc, durability, wathr rsistanc, and longvity of th insulation on a unit. Flxibl, closd-cll lastomric insulation is th prdominat product usd in this application. A 2.0 cm thicknss is commonly usd. Food procssing, frzing, storag, and distribution applications oftn us ammonia rfrigration bcaus of its lowr oprating costs. As ammonia systms ar dsignd for smallr applications at an conomical up-front cost, thy ar gtting mor considration than mor xpnsiv oprating systms. Whil most aras do not xcd high tmpraturs abov 70 C, som sctions may cycl from 40 C to 120 C. Lowr tmpraturs (down to 20 C) man gratr insulation thicknss (5 8 cm) is usually rquird to prvnt condnsation. ypically, 8 cm of insulation is usd to prvnt condnsation, as many of ths applications ar in highhumidity aras. h majority of th insulation is installd outdoors, so jackting slction is critical. As a rsult of th cost and thicknss rquird, polystyrn and polyisocyurant with a stainlss stl jackt ar th most common matrials usd. Of ky concrn is corrosion of iron pip. Propr insulation installation (with no opn or through sams) is a major concrn, and us of scondary vapor-rtardr systms is th norm. h rfrigration markt covrs a broad spctrum of applications, ach with uniqu rquirmnts but all with a common goal: prvntion of moistur intrusion and condnsation to maintain long-trm systm rliability. Installation tchniqus ar just as critical as matrial slction. h consquncs of systm failur can includ dgradd thrmal prformanc of th insulation, highr systm oprating cost, inadquat cooling capacity, mold and mildw, ic formation, ruind cilings, slippry floors, quipmnt downtim, and corrodd pips. In blow-ambint systms lik rfrigration applications (including chilld watr and cryognic systms) closd-cll insulation products ar prfrrd bcaus of thir low WV and inhrnt moistur rsistanc. It s important to slct th right insulation product for th application. Customr xpctations must b matchd to product prformanc and cost. Rfrigration applications ar dmanding and rquir carful considration in matrial slction and installation to obtain optimum prformanc for th nd usr. III. OPIMIZAION MODEL h optimation mthod minims th analytical xprssion of various simpl or compound optimation critria. h computational modl involvs som known data as: gnral data, nrgy-conomic paramtrs, rfrring data to

3 Issu 5, Volum 7, rooms or piping and to construction lmnts or rfrigrant utild in rfrigration systm. In Figurs 1 and 2 ar prsntd calculation schma of rfrigration insulation for a flat and rspctivly cylindrical surfac. Fig. 1 Diagram of rfrigration insulation to a flat surfac Fig. 2 Diagram of rfrigration insulation to a cylindrical surfac h thrmal conductivity λ of insulation is xprssd as an analytical dpndnc: = b 0 + bt m λ (1) in which b 0, b ar constants dpnding on insulation matrial [11]; t m man tmpratur of insulator layr. otal rsistanc to hat transfr R is calculatd with quations: for flat surfacs of coold rooms: NS δ 1 δ j 1 R = λ α i λ j= j α 1 for cylindrical surfacs of cold pips: d R = + + ( ln πα d πα d 2π λ d whr: i i p 1 d 1 d p + ln + ) (3) λ d λ d p c i + (2) d = d + δ ; d = d + 2δ ; d p = d + 2δ p (4) i 2 c in which: δ is insulation thicknss; δ j, λ j thicknss and thrmal conductivity of layr j of componnt matrial of a flat surfac; δ c wall thicknss of a pip; δ p protctiv layr thicknss of pip insulation; d i, d insid and outsid diamtr of th pip; α i, α intrnal and xtrnal hat transfr cofficints of componnt lmnt of coold nvironmnt; NS matrial layrs numbr of a lmnt. Analytic optimation critria ar minimd and is fulfilld th condition of air condnsation prvnt on insulation surfac: flat surfacs: t ti = α i ( t p ti ) (5) R cylindrical surfacs: d d 2λ t ti ln 1 (6) d d α d t t pr in which: t i is coold nvironmnt tmpratur (indoor air or rfrigrant from pip); t outdoor air tmpratur; t p intrnal surfac tmpratur of a flat wall; t pr air dw-point tmpratur. It is assumd that th rfrigration systm is on with vapour mchanical comprssion and lctric driv. h optimal insulation thicknss can b dtrmind by considring as optimation critria: th insulation achivmnt cost, th oprating costs, th nrgy mbddd in insulation or th nrgy consumd to maintain low tmpratur [14]. A. Economic Critrion Economic critrion adoptd for optiming rfrigration insulation thicknss is th minimum updatd total cost (capital cost and nrgy cost). aking into account th spcific invstmnt cost for insulation I, th annual cost for maintnanc and rpair of insulation C ir, th annual cost of nrgy losss by insulatd surfac C f and th xprssion of updatd rat r for annual costs during normal rcovry tim: 1 ( 1+ r0 ) 1 r = =, (7) t 1+ r r r ( ) ( ) t = this critrion implis th miniming of following objctiv function: Cir + C f FC = I + (8) t= ( + ) t 1 1 r0 in which r 0 =1/ is dprciation rat for rcovry priod (10 15 yars). h optimal insulation thicknss is obtaind by solving th quation: F C / δ =0. For flat surfacs that finally lad to th rlation: ( ) NS rστ c f t ti λ = 1 δ j 1 δ + + λ rp + c (9) 1000( 1) αi j= 1 λ j α For cylindrical surfacs is applid th mthod of succssiv approximations aftr xplicating th objctiv function (8):

4 Issu 5, Volum 7, F C ( t t ) rσ τc f i = ( rp + 1) cδ ( d + δ ) + (10) 1000 R in which: c is th spcific invstmnt cost of a m 3 of insulation; p th dprciation, rpairs and maintnanc rat for an insulation ( ); σ additional cold loss cofficint through pip fittings or du to non-stady stat ( ); τ th numbr of hours ndd to provid cool during a yar ( hours/yar); c f cooling nrgy cost pric B. Enrgy Critrion h nrgy optimal insulation thicknss is dtrmind miniming th sum of nrgy mbddd in insulation E and oprating nrgy E rquird to maintain low tmpratur in coold nvironmnt. Enrgy critrion is xprssd analytically by th function: F E = E + E (11) For cylindrical surfacs this function rcivs particular form: F E ( t t ) σ τ i = δ ( d + δ ) + (12) 1000 R and could b minimd applying succssiv approximations mthod. Explicating th quation (11) for flat surfacs and introducing minimum condition ( F E / δ =0), aftr a sris of algbraic transformations, is obtaind th trm nrgy optimum insulation thicknss for coold rooms: δ ( )( ) NS t ( ) c t0 t ti στ λ 1 δ j 1 λ η + η f t0 273 α i λ j= 1 j α = (13) in which: is spcific nrgy mbddd in on m 3 of insulation; t c, t 0 th condnsation and vaporation tmpraturs of th rfrigrant; η avrag fficincy of obtaining lctricity from primary nrgy ( ); η f fficincy of ral rfrigration cycl vrsus rfrntial rvrsd Carnot cycl ( ). C. Enrgy-Economical Critrion Enrgy-conomical optimation critrion considrs th two abov critria combind. hus rflcts in a mor objctiv way th wight of tchnical and nrgy aspcts during lif-cycl of th insulatd construction or pip. So, if ar illustratd curvs F C =f(δ ) and F E =f(δ ) in two prpndicular plans (Fig. 3), thr is absolutly optimal point M (F C,min and F E,min ). his point rprsntd in a third plan formd by axs F C and F E is a fictional point, bcaus, in gnral, is not in th xistnc fild of functional rlationship F E =f(f C ). It is lookd for anothr point N so that MN distanc is minimd. It is dfind a complx critrion that includs th two abov mntiond in th form of miniming th Euclidan distanc in th plan (F C, F E ): F Fig. 3 3D-Rprsntation of bicritrial optimation function CE 2 ( F F ) + (1 ψ ( F F ) 2 = ψ (14) C C, min ) E E,min whr ψ is a critrial wight cofficint by which can b giv prfrnc to on or anothr of th componnt critria in diffrnt prics circumstancs, rspctivly in nrgy pnury. For flat surfacs, is obtaind th gnral xprssion of optimum insulation thicknss: δ = ψrc f (1 ψ) + η η ψ( rp + 1) c f ( tc t ) ( t + 273) 0 ( t t ) i στ (1 ψ) 0 λ NS λ 1 δ j α i j= 1 λ j α (15) By ψ = 1 and ψ = 0 in (14) or (15) ar found particular cass of optimation on conomic and nrgy critrion, xprssd by rlations (9) and (13) for flat surfacs and th rlations (10) and (12) for cylindrical surfacs. Basd on th prviously dvlopd optimation modl, two computr programs DEFRIZOP for coold rooms and COFRIZOP for cold pips hav laboratd in FORRAN programming languag, for PC microsystms. hs programs oprat squntially and hav flow charts in Figurs 4 and 5. IV. NUMERICAL APPLICAIONS It is xmplifid th application of th proposd computational modl for optimal sing of insulation on a plastrd xtrnal wall of a coold room to t i = 10 C tmpratur, which oprat all yar round and on a stl prssur pip carrying liquid ammonia at tmpratur t i = 10 C.

5 Issu 5, Volum 7, Fig. 4 Flow chart of DEFRIZOP program

6 Issu 5, Volum 7, Fig. 5 Flow chart of COFRIZOP program

7 Issu 5, Volum 7, h xtrnal wall is north orintd, has dimnsions 6 4 m, and ar known gnral data: δ 1 = 0.02 m; λ 1 = 0.93 W/(m K), δ 2 = 0.30 m, λ 2 = 0.80 W/(m K), t = 30 o C, w = 4 m/s, w i = 0 m/s, p = 0.05, = 10 yars, β o = 0.1, σ = 1.1, η = 0.3, η f = 0.6. h cold pip has diamtrs d /d i = 219/203 mm, lngth L = 15 m, flow rat G = m 3 /s and ar known gnral data: t = 30 o C, w = 0 m/s, δ p = 0.02 m, λ p = 0.29 W/(m K), p = 0.05, = 10 yars, σ = 1.1. abl 1. Insulation thicknss for xtrnal wall Using computr programs DEFRIZOP and COFRIZOP is prformd a rating comparativ study of ths insulations both with optimation modl and classical mthod. Considr svral cofficints ψ and as insulation xpandd polystyrn (EP) and minral wool (MW). Ar also allowd mor valus c f to highlight thir variation on insulation thicknss. h numrical rsults obtaind ar summard in abls 1 and 2. δ [mm] Optimation modl c f Classical Enrgy crit. Enrgy-conomical critrion c Econ. crit. [ /kwh] mthod ψ = 0 ψ = 0.25 ψ = 0.50 ψ = 0.75 ψ = 1.00 EP MW EP MW EP MW EP MW EP MW EP MW abl 2. Insulation thicknss for rfrigrant pip δ [mm] Optimation modl c f Classical Enrgy crit. Enrgy-conomical critrion c Econ. crit. [ /kwh] mthod ψ = 0 ψ = 0.25 ψ = 0.50 ψ = 0.75 ψ = 1.00 EP MW EP MW EP MW EP MW EP MW EP MW V. CONCLUSIONS From th prformd study rsults th following: h insulation thicknss dtrmind basd on conomic critrion, and also spcially nrgy critrion, is gratr than th thicknss usually practicd. Vry high insulation thicknss valus obtaind using xclusivly nrgy optimation critrion, is du to th larg wight of nrgy ndd to maintain th low tmpratur in pip compard with nrgy mbddd. hr is a slow variation of th optimal insulation thicknss with th cooling nrgy cost. Applying complx optimation critrion for a highr wight of nrgy critrion and for qual wights of both componnt critria, insulation thicknss valus ar high; this situation is normald admitting a dcrasd wight for nrgy critrion compard to th conomic critrion. h proposd optimation modl is complx and mor fficint. Dvlopd computr programs ar applicabl to any significant changs in conomic and nrgy policy. hy can hlp achiv savings in capital and nrgy, particularly important in th currnt conomic junctur. REFERENCES [1] ASHRAE, Fundamntals Handbook, Amrican Socity of Hating, Rfrigrating and Air-Conditioning Enginrs, Atlanta, [2] ASHRAE, Rfrigration Handbook, Amrican Socity of Hating, Rfrigrating and Air-Conditioning Enginrs, Atlanta, [3] J.P. Curtis, Optimation of multipl thin thrmal insulation layrs, Procdings of th 3 th IASME/ WSEAS Int. Confrnc on Hat ransfr, hrmal Enginring and Environmnt, Corfu, Grc, August 20-22, 2005, pp [4] N. Gorgscu, Mthodology to stablish th total mbddd nrgy in building matrials, Civil Enginring Journal, Bucharst, no. 9, [5] C.P. Hdlin, Moistur gains by foam plastic roof insulations undr controlld tmpratur gradints, Journal of Cllular Plastics, no 3, 1977, pp [6] V. Korsgaard, Innovativ concpt to prvnt moistur formation and icing of cold pip insulation, ASHRAE ransactions, vol. 99, no. 1, 1993, pp [7] M.K. Kumaran, Vapour transport charactristics of minral fibbr insulation from hat flow mtr masurmnts, In: ASM SP 1039, Watr vapour transmission through building matrials and systms: Mchanisms and masurmnt, Amrican Socity for sting and Matrials, 1989, pp [8] R.S. Lnox, P.A. Hough, Miniming corrosion of coopr tubing usd in rfrigration systms, ASHRAE Journal, vol. 37, 1995, pp. 11. [9] J.F. Malloy, hrmal insulation, Van Nostrand Rinhold, Nw York, 1969.

8 Issu 5, Volum 7, [10] I. Sarbu, I. Numrical modlling and optimations in building srvics, Polytchnic Publishing Hous, imisoara, 2010 (in Romanian). [11] I. Sarbu, Rfrigration systms, Mirton Publishing Hous, imisoara, 1998 (in Romanian). [12] I. Sarbu, C. Sbarchivici, hrmal rhabilitation of buildings, NAUN Intrnational Journal of Enrgy, vol.5, no.2, 2011, pp [13] I. Sarbu, I. C. Sbarchivici, Effcts analysis of additional thrmal protction for rtrofittd buildings, Journal of Enginring and Applid Scincs, vol. 6, no. 6, 2011, pp [14] I. Sarbu, E. Vala, G. Ostaf, Insulation rating optimation for rfrigrating systms, In: Rcnt Advancs in Environmntal Scinc, Procdings of th 9 th WSEAS Int. Confrnc on Enrgy, Environmnt, Ecosystms and Sustainabl Dvlopmnt, Lmsos, Cyprus, March 21-23, 2013, pp [15] M. Storkmann, Insulating against th low tmpraturs by flxibl insulation matrials, chnical Building Equipmnts, vol. 22, no. 5, g. Murs, Romania, 2004, pp [16] W.C. urnr, J.F. Malloy, hrmal insulation handbook, McGraw Hill Book Company, Nw York, 1981.

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

COMPUTATIONAL NUCLEAR THERMAL HYDRAULICS

COMPUTATIONAL NUCLEAR THERMAL HYDRAULICS COMPUTTIONL NUCLER THERML HYDRULICS Cho, Hyoung Kyu Dpartmnt of Nuclar Enginring Soul National Univrsity CHPTER4. THE FINITE VOLUME METHOD FOR DIFFUSION PROBLEMS 2 Tabl of Contnts Chaptr 1 Chaptr 2 Chaptr

More information

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which

More information

Topology Optimization of Suction Muffler for Noise Attenuation

Topology Optimization of Suction Muffler for Noise Attenuation Purdu Univrsity Purdu -Pubs Intrnational Comprssor Enginring Confrnc School of Mchanical Enginring 2012 Topology Optimization of Suction Mufflr for Nois Attnuation Jin Woo L jinwool@ajou.ac.kr Dong Wook

More information

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect Advancd Matrials sarch Onlin: -8-6 ISS: 66-8985, Vols. 34-36, pp 389-39 doi:.48/www.scintific.nt/am.34-36.389 rans ch Publications, Switzrland Instantanous Cutting Forc Modl in High-Spd Milling Procss

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

More information

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

WASTE HEAT RECOVERY USING DIRECT THERMODYNAMIC CYCLE

WASTE HEAT RECOVERY USING DIRECT THERMODYNAMIC CYCLE Bulltin of th Transilvania Univrsity of Braşov Vol. 8 (57) No. 2-2015 Sris I: Enginring Scincs WASTE HEAT RECOVERY USING DIRECT THERMODYNAMIC CYCLE I. COSTIUC 1 L. COSTIUC 2 S. RADU 3 Abstract: For wast

More information

Estimation of apparent fraction defective: A mathematical approach

Estimation of apparent fraction defective: A mathematical approach Availabl onlin at www.plagiarsarchlibrary.com Plagia Rsarch Library Advancs in Applid Scinc Rsarch, 011, (): 84-89 ISSN: 0976-8610 CODEN (USA): AASRFC Estimation of apparnt fraction dfctiv: A mathmatical

More information

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

Chapter 13 Aggregate Supply

Chapter 13 Aggregate Supply Chaptr 13 Aggrgat Supply 0 1 Larning Objctivs thr modls of aggrgat supply in which output dpnds positivly on th pric lvl in th short run th short-run tradoff btwn inflation and unmploymnt known as th Phillips

More information

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS Journal of Optolctronics and Advancd Matrials Vol. 6 No. March 4 p. 63-69 STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS N. N. Puscas * Physics Dpartmnt

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB MEASURING HEAT FLUX FROM A COMPONENT ON A PCB INTRODUCTION Elctronic circuit boards consist of componnts which gnrats substantial amounts of hat during thir opration. A clar knowldg of th lvl of hat dissipation

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

dr Bartłomiej Rokicki Chair of Macroeconomics and International Trade Theory Faculty of Economic Sciences, University of Warsaw

dr Bartłomiej Rokicki Chair of Macroeconomics and International Trade Theory Faculty of Economic Sciences, University of Warsaw dr Bartłomij Rokicki Chair of Macroconomics and Intrnational Trad Thory Faculty of Economic Scincs, Univrsity of Warsaw dr Bartłomij Rokicki Opn Economy Macroconomics Small opn conomy. Main assumptions

More information

The Open Economy in the Short Run

The Open Economy in the Short Run Economics 442 Mnzi D. Chinn Spring 208 Social Scincs 748 Univrsity of Wisconsin-Madison Th Opn Economy in th Short Run This st of nots outlins th IS-LM modl of th opn conomy. First, it covrs an accounting

More information

Unfired pressure vessels- Part 3: Design

Unfired pressure vessels- Part 3: Design Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This

More information

Principles of LEV Design. Duct friction losses Friction losses increase linearly with duct length increasing air density, typical form: L

Principles of LEV Design. Duct friction losses Friction losses increase linearly with duct length increasing air density, typical form: L Typs of losss Entry losss, ducts and hoods Friction Losss: Fluid in motion ncountrs drag along th surfac Enrgy is ndd to ovrcom th drag forc Th drag forc is du to th fluid viscosity Dynamic losss Turbulnc

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE 13 th World Confrnc on Earthquak Enginring Vancouvr, B.C., Canada August 1-6, 2004 Papr No. 2165 INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA * 17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

Where k is either given or determined from the data and c is an arbitrary constant.

Where k is either given or determined from the data and c is an arbitrary constant. Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is

More information

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.) Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of

More information

AerE 344: Undergraduate Aerodynamics and Propulsion Laboratory. Lab Instructions

AerE 344: Undergraduate Aerodynamics and Propulsion Laboratory. Lab Instructions ArE 344: Undrgraduat Arodynamics and ropulsion Laboratory Lab Instructions Lab #08: Visualization of th Shock Wavs in a Suprsonic Jt by using Schlirn tchniqu Instructor: Dr. Hui Hu Dpartmnt of Arospac

More information

Part 7: Capacitance And Capacitors

Part 7: Capacitance And Capacitors Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

COMPARATIVE ANALYSIS OF AN ORGANIC RANKINE CYCLE FOR WASTE COGENERATION PLANTS

COMPARATIVE ANALYSIS OF AN ORGANIC RANKINE CYCLE FOR WASTE COGENERATION PLANTS Bulltin of th Transilvania Univrsity of Braşov Vol. 10 (59) No. 2-2017 Sris I: Enginring Scincs COMPARATIVE ANALYSIS OF AN ORGANIC RANKINE CYCLE FOR WASTE COGENERATION PLANTS L. COSTIUC 1 I. COSTIUC 2

More information

Finite Element Model of a Ferroelectric

Finite Element Model of a Ferroelectric Excrpt from th Procdings of th COMSOL Confrnc 200 Paris Finit Elmnt Modl of a Frrolctric A. Lópz, A. D Andrés and P. Ramos * GRIFO. Dpartamnto d Elctrónica, Univrsidad d Alcalá. Alcalá d Hnars. Madrid,

More information

Finite element discretization of Laplace and Poisson equations

Finite element discretization of Laplace and Poisson equations Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization

More information

Flow Switch Diaphragm Type Flow Switch IFW5 10 N Diaphragm type flow switch. Thread type. Model Body size Set flow rate

Flow Switch Diaphragm Type Flow Switch IFW5 10 N Diaphragm type flow switch. Thread type. Model Body size Set flow rate Flo Sitch Diaphragm Typ Flo Sitch IFW5 Sris [Option] Th flo sitch, IFW sris is usd for dtction and confirmation of th flo as a rlaying dvic for th gnral atr applications in som various uipmnt such as cooling

More information

15. Stress-Strain behavior of soils

15. Stress-Strain behavior of soils 15. Strss-Strain bhavior of soils Sand bhavior Usually shard undr draind conditions (rlativly high prmability mans xcss por prssurs ar not gnratd). Paramtrs govrning sand bhaviour is: Rlativ dnsity Effctiv

More information

A New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG *

A New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG * 2017 2nd Intrnational Conrnc on Applid Mchanics, Elctronics and Mchatronics Enginring (AMEME 2017) ISBN: 978-1-60595-497-4 A Nw Approach to th Fatigu Li Prdiction or Notchd Componnts Undr Multiaxial Cyclic

More information

Design of a Test Rig for the Study of Methane Drying by Cooling Effect

Design of a Test Rig for the Study of Methane Drying by Cooling Effect Availabl onlin at http://journals.usamvcluj.ro/indx.php/promdiu ProEnvironmnt ProEnvironmnt 7 (204) 23-3 Original Articl Dsign of a Tst Rig for th Study of Mthan Drying by Cooling Effct SAFIRESCU Călin

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Serge 10% COLLECTION REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 10%

Serge 10% COLLECTION REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 10% Srg 10% COLLECTION 2018-2021 REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 10% Scrns that rflct & absorb solar nrgy outsid th hous. Mt OUT. Srg 10% GLASSFIBRE OF = 10% Tchnical spcifications Srg 600 010010

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

Ecrano COLLECTION REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 2%

Ecrano COLLECTION REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 2% Ecrano COLLECTION 2018-2021 REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 2% Scrns that rflct & absorb solar nrgy outsid th hous. Mt OUT. Ecrano GLASSFIBRE OF = 2% Tchnical spcifications Ecrano 002010 whit

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing INCAS BULLETIN, Volum, Numbr 1/ 1 Numrical considrations rgarding th simulation of an aircraft in th approaching phas for landing Ionl Cristinl IORGA ionliorga@yahoo.com Univrsity of Craiova, Alxandru

More information

Thermodynamical insight on the role of additives in shifting the equilibrium between white and grey tin

Thermodynamical insight on the role of additives in shifting the equilibrium between white and grey tin hrmodynamical insight on th rol of additivs in shifting th quilibrium btwn whit and gry tin Nikolay Dmntv Dpartmnt of Chmistry, mpl Univrsity, Philadlphia, PA 19122 Abstract In this study mthods of statistical

More information

Thermodynamic Modeling of an Ammonia-Water Absorption System Associated with a Microturbine

Thermodynamic Modeling of an Ammonia-Water Absorption System Associated with a Microturbine Int. J. of Thrmodynamics Vol. 12 (No. 1), pp. 38-43, March 29 ISSN 131-9724 www.icatwb.org/journal.htm Abstract Thrmodynamic Modling of an Ammonia-Watr Absorption Systm Associatd with a Microturbin Janilson

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h For t BWR oprating paramtrs givn blow, comput and plot: a) T clad surfac tmpratur assuming t Jns-Lotts Corrlation b) T clad surfac tmpratur assuming t Tom Corrlation c) T clad surfac tmpratur assuming

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Ultimate lateral load resistance of laterally loaded pile

Ultimate lateral load resistance of laterally loaded pile Ultimat latral load rsistanc of latrally loadd pil Md. M. Rahman Assistant Profssor, Dpartmnt of Civil Enginring, RUET, Rajshahi, Bangladsh Md. R. arim, A. L. Baki & D.. Paul Lctr, Dpartmnt of Civil Enginring,

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Blockout Serge 600 Solar COLLECTION REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3%

Blockout Serge 600 Solar COLLECTION REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3% Blockout Srg 600 Solar COLLECTION 2018-2021 REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3% Scrns that rflct & absorb solar nrgy outsid th hous. Mt OUT. Srg 600 BO Solar GLASSFIBRE OF = 3% Tchnical spcifications

More information

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach Intrnational Journal of Application or Innovation in Enginring & Managmnt (IJAIEM) Wb Sit: www.ijaim.org Email: ditor@ijaim.org Volum 6, Issu 7, July 07 ISSN 39-4847 Full Ordr Obsrvr Controllr Dsign for

More information

Recursive Estimation of Dynamic Time-Varying Demand Models

Recursive Estimation of Dynamic Time-Varying Demand Models Intrnational Confrnc on Computr Systms and chnologis - CompSysch 06 Rcursiv Estimation of Dynamic im-varying Dmand Modls Alxandr Efrmov Abstract: h papr prsnts an implmntation of a st of rcursiv algorithms

More information

MA 262, Spring 2018, Final exam Version 01 (Green)

MA 262, Spring 2018, Final exam Version 01 (Green) MA 262, Spring 218, Final xam Vrsion 1 (Grn) INSTRUCTIONS 1. Switch off your phon upon ntring th xam room. 2. Do not opn th xam booklt until you ar instructd to do so. 3. Bfor you opn th booklt, fill in

More information

Electromagnetism Physics 15b

Electromagnetism Physics 15b lctromagntism Physics 15b Lctur #8 lctric Currnts Purcll 4.1 4.3 Today s Goals Dfin lctric currnt I Rat of lctric charg flow Also dfin lctric currnt dnsity J Charg consrvation in a formula Ohm s Law vryon

More information

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

ME311 Machine Design

ME311 Machine Design ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform

More information

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles Lct-30 Lct-30 In this lctur... Subsonic and suprsonic nozzls Working of ths nozzls rformanc paramtrs for nozzls rof. Bhaskar Roy, rof. A M radp, Dpartmnt of Arospac, II Bombay Lct-30 Variation of fluid

More information

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real. Midtrm #, Physics 37A, Spring 07. Writ your rsponss blow or on xtra pags. Show your work, and tak car to xplain what you ar doing; partial crdit will b givn for incomplt answrs that dmonstrat som concptual

More information

A Control Strategy for Photovoltaic-Solid Polymer Electrolysis System Based on Surface Temperature of PV Panel

A Control Strategy for Photovoltaic-Solid Polymer Electrolysis System Based on Surface Temperature of PV Panel Amrican Journal of Applid Scincs 5 (7): 5-, ISSN 1546-939 Scinc Publications Corrsponding Author: A Control Stratgy for Photovoltaic-Solid Polymr Elctrolysis Systm Basd on Surfac Tmpratur of PV Panl 1

More information

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea 2017 Watr Ractor Ful Prformanc Mting Sptmbr 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jju Jju Island, Kora Study of Ful Rod Bhavior with Missing Pllt Surfac Dfct Zhnhai Liu 1, Yi Zhou 1, Ping Chn 1, Yuanming

More information

Blockout Serge 600 Solar COLLECTION REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3%

Blockout Serge 600 Solar COLLECTION REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3% Blockout Srg 600 Solar COLLECTION 2018-2021 REFLECTS SUNLIGHT OUTDOORS BLOCKOUT OF = 3% Scrns that rflct & absorb solar nrgy outsid th hous. Mt OUT. GLASSFIBRE OF = 3% Tchnical spcifications 010010 charcoal

More information

2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line

2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line //03 Ovrviw -owr Transmission Txt: 4.6-4.0 ECEGR 45 owr ystms Consrvation of Complx owr hort in owr Transmission owr Transmission isualization Radial in Mdium and ong in owr Transmission oltag Collaps

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME Introduction to Finit Elmnt Analysis Chaptr 5 Two-Dimnsional Formulation Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e 8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain

More information

Electric (Rocket) Propulsion. EP Overview

Electric (Rocket) Propulsion. EP Overview Elctric (Rockt) Propulsion EP Ovrviw Elctric Propulsion-1 Basics Rockt Propulsion Elmnts Propllant Enrgy Sourc Storag Fd Systm sam in chmical rockts Storag Convrsion Acclrator Elctric Propulsion- 1 Elctric

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

A General Thermal Equilibrium Discharge Flow Model

A General Thermal Equilibrium Discharge Flow Model Journal of Enrgy and Powr Enginring 1 (216) 392-399 doi: 1.17265/1934-8975/216.7.2 D DAVID PUBLISHING A Gnral Thrmal Equilibrium Discharg Flow Modl Minfu Zhao, Dongxu Zhang and Yufng Lv Dpartmnt of Ractor

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna 1 Journal of Microwavs, Optolctronics and Elctromagntic Applications, Vol. 6, No. 2, Dcmbr 2007 406 Koch Fractal Boundary Singl fd Circularly Polarizd Microstrip Antnna P. Nagswara Rao and N. V. S.N Sarma

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions. Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

Chapter 14 Aggregate Supply and the Short-run Tradeoff Between Inflation and Unemployment

Chapter 14 Aggregate Supply and the Short-run Tradeoff Between Inflation and Unemployment Chaptr 14 Aggrgat Supply and th Short-run Tradoff Btwn Inflation and Unmploymnt Modifid by Yun Wang Eco 3203 Intrmdiat Macroconomics Florida Intrnational Univrsity Summr 2017 2016 Worth Publishrs, all

More information

4.4 Design of Sections for Flexure (Part III)

4.4 Design of Sections for Flexure (Part III) 4.4 Dsign of Sctions for Flxur (Part ) This sction covrs th following topics. Choic of Sctions Dtrmination of Limiting Zon Post-tnsioning in Stags 4.4.1 Choic of Sctions Th typ of sction is slctd asd on

More information

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,

More information

Discrete Hilbert Transform. Numeric Algorithms

Discrete Hilbert Transform. Numeric Algorithms Volum 49, umbr 4, 8 485 Discrt Hilbrt Transform. umric Algorithms Ghorgh TODORA, Rodica HOLOEC and Ciprian IAKAB Abstract - Th Hilbrt and Fourir transforms ar tools usd for signal analysis in th tim/frquncy

More information

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Diploma Macro Paper 2

Diploma Macro Paper 2 Diploma Macro Papr 2 Montary Macroconomics Lctur 6 Aggrgat supply and putting AD and AS togthr Mark Hays 1 Exognous: M, G, T, i*, π Goods markt KX and IS (Y, C, I) Mony markt (LM) (i, Y) Labour markt (P,

More information

A nonequilibrium molecular dynamics simulation of evaporation

A nonequilibrium molecular dynamics simulation of evaporation Intrnational Confrnc Passiv and Low Enrgy Cooling 543 A nonquilibrium molcular dynamics simulation of vaporation Z.-J. Wang, M. Chn and Z.-Y. Guo Dpartmnt of Enginring Mchanics, Tsinghua Univrsity, Bijing

More information

Classical Magnetic Dipole

Classical Magnetic Dipole Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt

More information

1. In the given figure PQRS is a parallelogram. Find the coordinates of R.

1. In the given figure PQRS is a parallelogram. Find the coordinates of R. Tst Assss Achiv Class : 9 CLASS : 9 Mathmatics 1. In th givn figur PQRS is a paralllogram. Find th coordinats of R. Y S(2, 3) R O P(1, 0) Q(5, 0) X (5, 2) (5, 3) (6, 2) (6, 3) 2. Th prpndicular distanc

More information

INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor

INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor INC 693, 48 Dynamics Systm and Modlling: Th Languag o Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Prossor Dpartmnt o Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity o Tchnology

More information

Module 8 Non equilibrium Thermodynamics

Module 8 Non equilibrium Thermodynamics Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information