Multi-zone buildings thermo-hygrometric analysis: a novel dynamic simulation code based on adaptive control

Size: px
Start display at page:

Download "Multi-zone buildings thermo-hygrometric analysis: a novel dynamic simulation code based on adaptive control"

Transcription

1 Muli-zon buildings hrmo-hygromric analysis: a novl dynamic simulaion cod basd on adapiv conrol Annamaria Buonomano Dparmn of Indusrial Enginring, Univrsiy of Napls Fdrico II, Ialy annamaria.buonomano@unina.i Umbro Monanaro Dparmn of Indusrial Enginring, Univrsiy of Napls Fdrico II, Ialy umbro.monanaro@unina.i Adolfo Palombo Dparmn of Indusrial Enginring, Univrsiy of Napls Fdrico II, Ialy adolfo.palombo@unina.i Sfania Sanini Dparmn of Elcrical Enginring and Informaion chnology, Univrsiy of Napls Fdrico II, Ialy sfania.sanini@unina.i Absrac his papr prsns a novl dynamic simulaion modl for h analysis of muli-zon buildings hrmal rspons and h assssmn of building nrgy prformanc and indoor comfor. In his nw rlas of h cod, calld DEEC.3, wo imporan innovaions ar implmnd. hy rgard h simulaion modl of muli-zon buildings, consising of hrmal zons oally nclosd in ohrs, and h dsign of a novl mpraur-humidiy conrol algorihm. h dvlopd innovaiv conrol sragy is basd on a rfrnc adapiv conrol schm for h onlin adapaion of h conrol gains, wih h aim of ovrcoming h wllknown problms of classical fixd gain conrol algorihms. his faur will b a ky ool for h nx gnraion of building prformanc simulaion cods (also oward NZEB analyss). Boh h innovaions mbddd in h cod can b xploid o simula spcial indoor nvironmns of hospials / laboraoris, rooms or musum halls. Wih h aim of showing h faurs and h ponialiis of h simulaion cod coupld wih h nw conrol schm, a suiabl cas sudy rlad o an xpo indoor spac of a musum building, including a display cas wih an accura clima conrol, was dvlopd. Dails abou haing and cooling dmands and loads ar providd. Good racking prformanc for boh h mpraur and humidiy conrol ar obaind hrough h prsnd conrol schm. 1. Inroducion A crucial challng for h nx gnraion of buildings is h capabiliy o ovrcom h radoff bwn low nrgy dmands and high hrmal and hygromric comfor lvls. h growing anion o hs issus has ld h rsarch inrs oward h us of building managmn sragis wih h aim of improving boh building nrgy fficincy and occupans comfor. In his rgard, Building Enrgy Prformanc Simulaion (BEPS) ools play a ky rol. In h las yars, rcn advancs in h numrical analysis basd on compuaional mhods, as wll as compur calculaion powr, providd significan opporuniis for dvloping and/or improving a nw gnraion of BEPS cods. Hr, paricular anion was paid o: i) invsigaing nw building nvlop chnologis and innovaiv HVAC sysms, ofn suppord by rnwabl nrgis; ii) implmning advancd conrol algorihms and sysms (Shaikh P. H. al. 14). h prsnd papr focuss on his spcific framwork. In paricular, h aricl dscribs h nw faurs includd in DEEC.3, which updas a prvious rlas (DEEC. (Buonomano A. and Palombo A. 14)) validad by mans of h BESES procdur. Spcifically, DEEC.3 nabls h simulaion of mulihrmal zons (in paricular of zons oally nclosd in ohrs). Furhrmor, i implmns advancd hrmo-hygromric conrol acions abl 19

2 Annamaria Buonomano, Umbro Monanaro, Adolfo Palombo, Sfania Sanini o auomaically adap o h variaions of h simulad sysm and is surrounding nvironmn. h cod, purposly dvlopd by h auhors for rsarch aims, is concivd as a rliabl hrmo-hygromric calculaion ool for building nrgy dsign and prformanc analysis. DEEC allows on o dynamically calcula haing and cooling dmands of muli-zon buildings and o assss h bnfis of diffrn and advancd building nvlop chniqus (PCM, BIPV, BIPV/, sunspac, c.). hus, dsigns of high-prformanc buildings can b obaind. I is worh noing ha ofn svral rsarch opics canno b analysd by commrcial BEPS cods (.g. rcn prooypal chnologis, non-sandard opraing iions, paricular sysm schduling, c.). Such inninc can b xcdd by dvloping in-hous cods such as DEEC. Hr, updaing and modificaions of h includd modls can b carrid ou by auhors for all h occurring rsarch nds. h aim of his papr is o show h ffcivnss of h cod in prdicing h bhaviour of building hrmal zons wih rigid hrmo-hygromric consrains. Such a goal is achivd by xploiing h faurs of h adapiv conrol schm mbddd ino in DEEC.3, basd on a nw opimal modl rfrnc schm (namd L- EMAC, Linar uadraic Exndd Modl frnc Adapiv Conrol). h major advanag of his conrol chniqu is h conrol of h hrmo-hygromric variabls for indoor spacs in uncrain iions, wihou rquiring an a priori knowldg of h building dynamics. o his aim, diffrn from sandard fixd gains chniqus such as, for xampl, h PI approach implmnd in h prvious DEEC. rlas, h implmnd conrol algorihm is abl on-lin o auomaically vary is gains valus o conrac abrup and unknown changs in h building bhaviour and/or is faurs and xrnal iions. h ida bhind his approach is o achiv gra conrol flxibiliy and robusnss in ordr o guaran, a h sam im, opimaliy wih rspc o a crain cos funcion subjc o som consrains. h L-EMAC approach xnds and fuss h classical Modl frnc Adapiv Conrol (MAC) schm ha has bn provd o b ffciv in conrolling uncrain plans (Di Brnardo M. al. 8), wih an L algorihm, ypical in h opimal conrol hory. A suiabl cas sudy is hr dvlopd in ordr o show h ffcivnss of h adopd approach. In paricular, i rfrs o an indoor hall of a musum building wih an includd glass display cas. Hr, an accura clima conrol (rigid consrains of mpraur and humidiy of h cas indoor air) is rquird. As is wll known, such an occurrnc is mandaory in cas of paricular xhibid ims conaind in musum glass cass (.g. archival arifacs, papr-basd objcs, c.). Hr, prsrvaion chniqus mus b mphasizd in ordr o avoid any irrvrsibl damag. h cas sudy building is locad in h Mdirranan wahr zon of Napls, souhrn Ialy. o h bs of h auhors knowldg, his is h firs amp in liraur o modl in BEPS cods: i) conrol by mans of advancd schms (abl o guaran rigorous consrains of mpraurs and humidiy, simulanously); ii) hrmal zons oally includd ino ohrs.. hrmodynamic modl In his papr, a suiabl rsisiv-capaciiv (C) hrmal nwork simulaion modl (assuming 1D ransin ha ransfr) for h hrmo hygromric analysis of wo hrmal zons (on opionally complly nclosd in h ohr on) is dscribd. I is mbddd in h nw rlas of DEEC (Buonomano A. and Palombo A. 14). hrough such a modl, h assssmn of h dynamics of mpraurs and humidiy, as wll as of haing and cooling loads and dmands, can b carrid ou. A skch of h modlld C hrmal nwork is shown in Fig. 3. h calculaion procdur concrns h ha flows bwn: i) h oudoor nvironmn and h main modlld hrmal zon (zon 1 in Fig. 3); ii) h zon 1 and h rlad includd hrmal zon (Fig. 3). h following modl simplificaions ar considrd: i) h indoor air of ach hrmal zon is uniform and modlld as a singl indoor air mpraur nod; ii) h building nvlop of zon 1 is subdividd ino M muli-layr lmns (adoping a high ordr C hrmal nwork); iii) h 11

3 Muli-zon buildings hrmo-hygromric analysis: a novl dynamic simulaion cod basd on adapiv conrol consrucion nvlop of zon is lumpd in a singl nod; iv) ach m-h muli-layr building lmn of zon 1 is subdividd in N sub-layrs (of diffrn hicknsss), whr hrmal masss and uciviis ar uniformly discrisd; v) N+ capaciiv and surfac nods ar accound for ach m-h nvlop componn of zon 1, whil 1 nod is rfrrd o is indoor air; vi) nods ar modlld for zon, ach on for h lumpd nvlop and h indoor air. For zon 1, in ach -h im sp and for ach n-h capaciiv nod (j = 1,..., N) of h m-h lmn (m = 1,..., M), h diffrnial quaion dscribing h nrgy ra of chang of ach mpraur nod of h building nvlop is: n+1 dmn,, m, j - m,n Cmn d q j=n-1 m, j (1) whr C and ar h hrmal capacianc and mpraur of h nod, rspcivly. mj, is h sum of h halvs sub-layrs hrmal rsisancs mj, (ha links h n-h nod o hir nighbours, Fig. 3). For non-capaciiv our (n = ) and innr (n = N+1) surfac boundary nods, h algbraic quaion dscribing h ha ransfr is: 1,, n m j m n, cv mn jn1 mj, cv m, j is ihr a civ (xrnal inrnal m,n+1 q () m, or m,n ) or a uciv rsisanc ( ), dpnding on h sid layr of h considrd nod (Fig. 3). m, and nods o hos rlad o h m,n+1 connc non capaciiv oudoor air mpraur (ou) and o h indoor air on (in,1), rspcivly. In cas of floor lmns, ou and cv m, j ar rplacd wih h ground mpraur (gr) and an quivaln hrmal uciv rsisanc ( ). h modlld forcing funcion mn, includs h incidn solar and h long-wav radiaion xchang acing on our and innr surfacs of zon 1 (Buonomano A. and Palombo A. 14). A simplifid approach is adopd for zon. Hr, h diffrnial quaion dscribing h nrgy ra of chang of h mpraur nod of h zon nvlop (w,) is calculad as: k gr dw,, in j w, Cw, d j=1 j (3) whr Cw, is h nvlop lumpd hrmal capacianc, whos indoor air mpraur is in,; j is a al hrmal rsisanc ha aks ino accoun all h ha ransfr ffcs. For zon 1, 1 is calculad by adding h half sub-layr uciv hrmal rsisanc of h zon nvlop nod o h quivaln civ and radiaiv hrmal rsisanc (modlld by a combind linarizd civ-radiaiv hrmal rsisanc). A simplifid approach is considrd for zon. Hr, h radiaiv xchang only aks ino accoun h long-wav fracion vs. h zon 1. hus, for zon, h quivaln al hrmal rsisanc ( and cion phnomna only. ) includs combind ucion h diffrnial quaions on h hrmal nwork nods rlad o h indoor air of zon 1 and zon mus b solvd simulanously wih h sysm of qs. (1), () and (3). h snsibl nrgy ra of chang of zon 1 and zon indoor air masss (a in,1 and in,, rspcivly) can b calculad as: d - -, M in,1 m,n in,1 w, in,1 ou in,1 in, in,1 C in 1 + g, 1 AC,1 d m=1 m,in 1 v v, zns din, w, in, in,1 in, Cin, g, AC, d v, zns (4) (5) whr h hrmal rsisancs v and v,zns dscrib h air vnilaion and infilraion hrmal loads: v links h indoor air nod of zon 1 o h xrnal on (oudoor air a ou), v,zns links h indoor air nod of zon o h on rlad o zon

4 Annamaria Buonomano, Umbro Monanaro, Adolfo Palombo, Sfania Sanini ou sky rad sky x I m m, m, m,1 m,1 C m,1 m,1 m,1 m-h building lmn (xrnal wall, roof, ciling, floor, inrior wall, window) Zoom of ZONE includd in ZONE 1 mn, mn, C m,n Linkd o air nod of ZONE 1 mn, mn, 1 w, C W, Zon in I m rad mm, Fig. 3 Skch of h C hrmal nwork rad m,1 rad m, m,n+1 gr C in, M, N+1 rad m,m -1 Zon 1 in, m,n +1 AC, Zon 1 g, in,1 v, C in,1 M-1,N+1 1,N+1 AC,1 Excp for h hrmal load du o h solar radiaion ransmid hrough h windows and incidn on h indoor surfacs, includd in mn,, in ( I m, Fig. 3), all h rmaining snsibl ha gains ar considrd as civ lumpd ha sourc rms, nworkd o h indoor air nods only. hy includ: i) h hrmal zon inrnal gains du o occupans, lighs and quipmn, g,1 and g, ; ii) h snsibl ha o b supplid o (or rmovd from) h building spac by an idal HVAC sysm, aiming a mainaining h indoor air a h dsird s poin mpraur, AC, 1 and AC,. hrfor, h whol sysm including zon 1 and zon is modlld hrough a hrmal nwork of (M x N) + 5 nods. h diffrnial and algbraic quaions dscribing h sysm hrmal bhaviour ar: (1), (), (3), (4) and (5). h assssmn of h lan nrgy o b addd o (or subracd from) boh h hrmal zons 1 and (for mainaining h slcd rlaiv humidiy spoin of h indoor air) is carrid ou by adoping a dcoupld approach (Ghiaus C. 14). For ach indoor spac h moisur balanc is calculad by nglcing h moisur xchang bwn h air nod and h surrounding building surfacs. In ach τ-h simulaion im sp and for ach hrmal zon (z = 1, ), h adopd moisur balanc is: g,1 v,1,n+1 1 w, Zon, la din z AC,, *,,,, z in z mv z ou z in z mwg z d hvs whr Ωin in is h indoor dry air mass; air vnilaion mass flow ra; (6) m v is h m wg is h inl war vapour mass flow ra o h hrmal zon (du o occupans); ωou* and ωin ar h xrnal and indoor air spcific humidiy, rspcivly (no ha h xrnal air spcific humidiy is rfrrd o h: i) oudoor air for zon 1; ii) zon 1 air for zon ); hvs is h war lan vaporaion ha a C..1 ducd ordr modl For conrol aims, a linar simplifid modl was drivd. Such a modl sms from h abov prsnd high ordr on (of (M x N) + nods (qs. (1) and ()) rlad o zon 1) which has bn simplifid ino a linar and s-ordr modl, xploid for h rfrnc modl dsign, whr: i) h hrmal capaciy of h whol building nvlop of zon 1 is lumpd in a singl nod; ii) h inpu signals acing on h hrmal nwork nods ar: ou, x I, gr and g,1 ; iii) an quivaln hrmal rsisanc of h building nvlop for inrnal and xrnal surfacs is adopd; iv) wighd avrag hrmal propris ar assumd. hus, qs. (1) and () bcom: d x -1 w,1 ou -w,1 I hou in,1 -w,1 gr -w,1 C w,1 = d q q q q x x in gr As a consqunc, quaion (4) bcoms: d - - ou -in,1 in, -in,1 in,1 w,1 in,1 w, in,1 C in,1 = q g,1 ± AC,1 d in 1 v v,zns (7) (8) As an xampl, for h snsibl load calculaion, h following vcors and marics ar considrd: i) mpraurs vcor of h lumpd nvlop and indoor air hrmal capaciancs of boh h zons, x = w,1 in,1 w, in, ; ii) vcor of snsibl ha o b supplid or rmovd from h building spac, u = AC,1 AC, ; iii) h upl (A, B, C) of dynamic marix A, inpu and h oupu vcors B -1-1 and C (.g. B = Cin,1 C in, and C= 1 1 for h snsibl load calculaion), s Scion 3. 11

5 Muli-zon buildings hrmo-hygromric analysis: a novl dynamic simulaion cod basd on adapiv conrol 3. h nhancd opimal L-MAC algorihm In ordr o conrol h hrmo-hygromric bhaviour, a nw conrol schm ha nhancs h classical Modl frnc Adapiv Conrol (MAC) sragy proposd by Landau (Landau I. D. (1979)) is adopd. h novl conrol algorihm (namd Linr-uadraic Enhancd Modl frnc Adapiv Conrol, L-EMAC) includs addiional conrol acions o improv h closdloop prformanc wih rspc o hos providd by h mor classical MAC approach. Furhrmor, i mbds as a rfrnc modl a rough plan modl conrolld via an L sragy (Andrson B.D.O. and Moor J.B. 1971). his implis ha closd-loop dynamics, opimal wih rspc o a givn prformanc indx, ar imposd o h plan undr invsigaion via h adapiv acion. Mor prcisly, h rfrnc modl is a rough simaion of plan dynamics: x = A x + B u, y = C x (9) (whr x n is h plan sa, uy, ar h conrol inpu and h sysm oupu, rspcivly, A n n is h dynamic marix, and B n, C 1 n ar h inpu and h oupu marics, rspcivly, wih n bing h sa spac dimnsion) drivn by a full sa opimal fdback conrol acion as: op op uop K x K r bing (1) op 1n op K, K som fixd conrol paramrs. From Opimal Conrol hory, i follows ha h conrol signal in (1) minimizs a quadraic funcional of h form: + J = y()- r y()- r +u ()u() d (11) (whr r is h s-poin o impos o h plan oupu, is h iniial im insan, and ar som posiiv marics). As a rsul, h closd-loop opimal dynamics o b imposd o h plan ar h soluions, xm, of h following opimally-conrolld im-invarian sysm: x A x B r (1) m m m m bing op Am A B K and B BK op m. Dails on h conrol algorihm and h conrol gains adapaion mchanism can b found in h following Appndix. 4. Cas sudy and dsign of h L- EMAC algorihm h prsnd cas sudy rfrs o a musum indoor spac in which wo hrmal zons ar modlld. In paricular, h firs zon rfrs o a musum hall whil h s on (oally includd in h firs zon) o a glass display cas wih an accura clima conrol (rigid consrains of mpraur and humidiy of h cas indoor air) ncssary o prsrv collcd xhibis such as: pains, woods, paprs and lahrs (which rquir suiabl iions of indoor air mpraur and rlaiv humidiy, simulanously). h skch of h wo-zon building is shown in Fig. 3. h simulaion, carrid ou by DEEC.3, rfrs o h wahr zon of Napls (souhrn Ialy), by using a Monorm hourly daa fil. For zon 1, a ypical Ialian building nvlop is akn ino accoun, wih lngh, widh and high qual o, 1 and 3.5 m, rspcivly. h building s longiudinal axis is as ws orind and a souh-facing windows (4-6-4 air filld doubl-glazd sysm) of 3 m is akn ino accoun. h hicknss of h building s walls and floor/ciling ar 5 and 3 cm, rspcivly. hir sraigraphy is dsignd by concr bricks (λ =.51 W/mK, ρ = 14 kg/m 3, c = 1 J/kgK) and hrmal insulaion (λ =.4 W/mK, ρ = 15. kg/m 3, c = 14 J/kgK). No ha ach building lmn is subdividd in 1 sub layrs of qual hicknss. h dirc solar radiaion ransfrrd hrough h windows o h insid zon is assumd o b absorbd by h floor wih an absorpion facor of.3. h absorpion and mission facors of inrior surfacs ar assumd o b qual o.15 and.9, rspcivly. For such a zon, a vnilaion ra qual o 1 Vol/h and a crowding indx of.1 prson/m ar akn ino accoun. A cubic shapd zon wih a 1 m lngh sid is considrd. In paricular, a glass nvlop of 3 cm hicknss, wih an occurring air infilraion of l/h is modlld. h simulaion sars on : of January 1 s and nds a 4: of Dcmbr 31 s. h haing/cooling sysm of h hrmal zon 1 is swichd on from 7: o 18:, from Novmbr 1 s o March 31 s (haing mod) and from Jun 1 s o Spmbr 3 h (cooling mod). h haing and cooling s poins 113

6 Annamaria Buonomano, Umbro Monanaro, Adolfo Palombo, Sfania Sanini indoor air mpraur ar s a 19 and 5 C, rspcivly. h rlaiv humidiy of h zon 1 indoor air is conrolld a 5%. h haing/cooling sysm of h hrmal zon is swichd on 4/7 o accuraly consrv h cas xhibid ims. Hr, h indoor air mpraur and rlaiv humidiy ar conrolld hroughou h yar a C and 65%, rspcivly. h L-EMAC has bn implmnd o conrol h air mpraur and humidiy, simulanously, of boh h modlld hrmal zons. In paricular, following a dcnralizd conrol approach (ach conrol variabl is usd o impos h dynamic bhaviour of only on variabl o b conrolld, s Pdro A. and Sala A. (4)), four diffrn and indpndn adapiv conrollrs ar synhsizd. In ordr o dsign h L-EMAC conrol, h simplifid modls (s Scion.1) wr adopd as nominal modls o b opimizd via h L approach, by sing o zro h disurbanc acing on h plan dynamics. No ha h choic of hs simplifid modls rducs h complxiy of h conrol dsign, wihou jopardizing h closd-loop prformanc. No ha h opimaliy and robusnss of h closd-loop conrol is guarand by h adapiv acions, whos gains volv o compnsa any paramr mismach and/or prsnc of unmodlld dynamics (s Appndix), and o assur h minimizaion of a quadraic cos funcion, for indoor air mpraur and humidiy racking rrors and snsibl and lan loads. hus, h minimizaion of haing and cooling dmands can b also achivd. In so doing, diffrn from classical fixd gains algorihms lik PI (implmnd in h prvious DEEC rlas), h proposd approach allows on o impos, on h sysm undr conrol, a dynamic bhaviour ha can also b opimal from h nrgy dmand poin of viw. h wigh marics ( and, which dfin h cos funcion in q. (11)) wr s in ordr o impos: i) a sling im of 5 minus for zon 1 and 1 minus for zon ; ii) absnc of ovrshoos for any sp variaion of h rfrnc signal. h choic of h rlaxaion im of zon 1 is don according o (Ghiaus C. and Hazyuk I. 1), wih h aim o nsur a smooh daily ransiion during h ransin opraion oward h rgim s-poin (conrol sysm is swichd on from 7: o 18:). Conrarily, a fasr ransin rquirmn is imposd on h sling im of zon bcaus of is rigorous hrmo hygromric rquirmns. Finally, h rfrnc inpu signals (r in Scion 3) dpnds on h slcd mpraur and humidiy s poins. No ha h humidiy conrol is obaind hrough h inpu rfrnc s poin of indoor air spcific humidiy (ωsp), in ordr o achiv h slcd rlaiv humidiy s-poin (φsp). 5. suls and discussion In h following, h rsuls rlad o h ffcivnss assssmn of h novl DEEC conrol approach, in imposing rfrnc indoor air mpraur and humidiy dynamics, ar shown. h analysis rfrs o boh h invsigad hrmal zons 1 and. As mniond abov, mpraur and humidiy ar conrolld daily from 7: o 18: in zon 1 and 4/7 in zon (for prsrvaion purposs of h xhibid ims). Fig. 4 shows h dynamic rnd of zon 1 indoor air mpraur, for wo sampl winr days (January 13 h and 14 h, i.. h 13 h and 14 h days of h yar) and for wo sampl summr days (July 5 h and 6 h, i.. h 6 h and 7 h days of h yar). Hr, a saisfacory prformanc of h dvlopd closdloop conrol schm can b obsrvd (coincidn rfrnc and obaind mpraur profils). No ha h s poin mpraur shifs from 19 C (for h winr sason) o 5 C (for h cooling sason). In Fig. 5 h im hisory of h indoor air mpraur during h ransin HVAC sysm rgim (sling im from 7: o 8:3) is shown for January 13 h. Also hr h obaind mpraur profil ovrlaps h dsird rfrnc on. ( C) Fig. 4 Zon 1 - Conrolld indoor air mpraur (rd solid lin for January 13 h and 14 h and blu dashd lin for July 5 h and 6 h ) and rfrnc mpraurs (grn dashd lin). 114

7 Muli-zon buildings hrmo-hygromric analysis: a novl dynamic simulaion cod basd on adapiv conrol ( C) 17 (kw) im (h) Fig. 5 Swichd on HVAC sysm in zon 1 in January 13h - im hisory of h indoor air mpraur (rd solid lin), rfrnc mpraur (grn dashd lin), s poin mpraur (black dashd lin). Fig. 6 shows h dynamic rnd of zon 1 indoor air humidiy for July 5 h and 6 h (Fig. 6a) and h lan load (dhumidificaion) rsuling from h conrol acion (Fig. 6b). Hr, h spcific humidiy s poin is 1 g/kg, corrsponding o a rlaiv humidiy of 5%. As in Fig. 5, Fig. 6c shows h im hisory of h indoor air humidiy during h sling im, for July 6 h. No ha h obaind humidiy profils ovrlap h dsird rfrnc ons. In Fig. 7, h snsibl hrmal load ( AC, 1), calculad according o h mpraur conrol of Fig. 4, is rpord. A similar bhaviour is obaind la for AC, 1 (no shown for sak of brviy). (g/kg) a) c) im (h) (W) (g/kg) - b) Fig. 6 Zon 1: a) conrolld indoor air humidiy (grn solid lin), b) lan hrmal load (grn dashd lin), c) humidiy im hisory during h sling im (grn solid lin) - frnc humidiy (rd dashd lin) Fig. 7 im hisory of zon 1 snsibl hrmal load (rd lin haing mod - January 13 h and 14 h, blu lin for cooling mod - July 5 h and 6 h ) - AC,1. Wih h hlp of hs simulaion rsuls, som conclusions can b highlighd, such as: i) mpraur and humidiy s poins (conrol aim) ar always saisfacorily achivd for any iniial indoor air mpraur and humidiy and vry disurbanc; ii) ypical xponnial bhaviours of asympoically sabl linr-im-invarian sysms (wih uni gain, ral ignvalus and a sling im of abou on hour) occur for boh h mpraur and humidiy conrols during h ransin HVAC rgims; iii) smooh dynamic rnds of h conrolld variabls and corrsponding haing and cooling dmands (conrol acions) ar obaind. I is noworhy o rmark ha a good racking prformanc of h closd-loop conrols is achivd. Vry low roo man squard rrors ar obaind (.4 C and g/kg for h air mpraur and humidiy conrol, rspcivly). In Fig. 8, for zon (whr a coninuous conrol of boh h mpraur and humidiy is rquird), h obaind rgulaion rror for h indoor air mpraur is shown (from April 9 h o May nd ). Such conrol rror is boundd wihin.1 C, dspi h significan oscillaion of h yarly indoor air mpraur of zon 1 (which rang from h minimum winr mpraur of 1 C and h maximum summr on of 3 C). In all hs figurs, h gry shadd rgions rfr o unoccupid hours, during which h HVAC sysm is swichd off and fr floaing hrmohygromric iions and null conrol acions occur. 115

8 Annamaria Buonomano, Umbro Monanaro, Adolfo Palombo, Sfania Sanini.1 Zon mpraur rror ( C) Zon 1 indoor air mpraur (W) Fig. 8 gulaion mpraur rror wihin zon and indoor air mpraur of zon 1 (up-righ cornr). Corrspondingly, h humidiy conrol rror vs. h slcd s poin in zon is lowr han 1-8 for h nir simulad yar, dspi a significan zon 1 humidiy variaion (from 4o 15g/kg), as clarly dpicd in FFig. 9. (-) 1 x x 1-8 Zon humidiy rror Zon 1 humidiy Fig. 9 gulaion humidiy rror wihin zon and indoor air mpraur of zon 1 (up-righ cornr). Obviously, boundd conrol acions ar h rsul of boundd conrol gains, as clarly shown in Fig. 1. Hr, as an xampl, h dynamic rnd of h snsibl hrmal load of zon ( AC, ), rsuling from h conrol of h indoor air mpraur from April 9 h o May nd (s also Fig. 8) is rpord. As xpcd, h zon hrmal loads ar much smallr han hos in zon 1. No ha, in Fig. 1, haing and cooling loads (as wll as humidificaion and dhumidificaion dmands) ar dcd, bcaus of h coninuous hrmo-hygromric conrol (i.. no gry shadd rgions occur in figur). F Fig. 1 im hisory of zon snsibl hrmal load - AC,. Finally, in Fig. 11 for boh h invsigad hrmal zons, h calculad haing and cooling (snsibl and lan) yarly uniary dmands, ar shown. Hr, i can b obsrvd ha h cooling dmands ar rmarkably highr han h haing ons (according o h high inrnal gains assumd for zon 1 and o h simulad wahr iions). In addiion, i is worh noing ha for zon h humidificaion and dhumidificaion dmands vs. h snsibl ons ar proporionally highr han hos occurring in zon 1. [kwh/m y] - -4 Zon 1 Zon Snsibl Haing Humidificaion Snsibl Cooling Dhumidificaion Fig. 11 Haing and cooling snsibl and lan dmands. his rsul is du o h coninuous humidiy conrol of zon and o h considrd indoor air mpraur and rlaiv humidiy s poins (in, = C, φsp = 65%). Noic ha, during h haing and cooling priods slcd for h hrmal zon 1, h humidificaion and dhumidificaion rquirmns of zon ar abou 78 and 89% of h rlad yarly calculad dmands, rspcivly. 6. Conclusion In his papr, nw faurs of h in-hous dvlopd compur cod (calld DEEC.3) for h building dynamic nrgy prformanc simulaion ar prsnd. h cod, dvlopd for 116

9 Muli-zon buildings hrmo-hygromric analysis: a novl dynamic simulaion cod basd on adapiv conrol rsarch purposs, nabls h auhors o modl and analys nw prooypal chnologis, nonsandard opraing iions, paricular sysm schduling, c., which canno b dal wih (or simulanously akn ino accoun) hrough commrcial BEPS cods. From his poin of viw, anohr advanag of DEEC is h possibiliy o upda and modify all h includd modls for ach occurring rsarch nd. Wih h hlp of h prsnd cod rlas, muli-zon buildings, consising of hrmal zons oally nclosd ino ohrs, can b modlld. In addiion, all h simulad zons can b govrnd by rigid assignd hrmo-hygromric consrains. his is accomplishd hrough an innovaiv adapiv conrol sragy (calld L-EMAC). Hr, h onlin adapaion of h conrol gains is achivd in ordr o assur h minimizaion of a quadraic cos funcion, which wighs boh h mpraur / humidiy racking rror and h snsibl / lan nrgy dmand. h conrol algorihm was dsignd on a simplifid fourh ordr modl. hn, i was sd and applid on h original and daild DEEC on, basd on mor han 7 diffrnial quaions. In his papr, h ffcivnss of h proposd novl building simulaion ool was vrifid hrough a suiabl cas sudy in which wo hrmal zons of a musum building ar modlld. Hr, a glass display cas wih a rigid mpraur / humidiy micro-clima conrol (for prsrving aims) is nclosd in a larg indoor spac. Simulaion rsuls show vry good racking prformanc of air mpraur and humidiy, simulanously, in boh h simulad hrmal zons. Boundd conrol gains and haing and cooling loads (during h ransin rgim) ar obaind. suls also confirm h robusnss of h dvlopd conrol approach for unmodlld dynamics. Appndix h L-EMAC conrol acion is: u( ) umac ( ) ui ( ) ue( ) (13) wih umac K( ) x( ) K( ) r( ), ue KE sgn y, and xi x() d. h im-varying u K x I I I conrol gains (adapiv gains) ar compud as: K( ) y ( ) x ( ) d y ( ) x ( ) K ( ) y ( ) r( ) d y ( ) r( ) I I d I K ( ) y ( ) x ( ) y ( ) x ( ) K () y d E whr,,, n, wih (14) n bing h nn subspac of diagonal marics in and,, ar som adapiv wighs wih h op sam sign of K assumd o b known (Ioannou P. and Fidan B. 6). h oupu rror y is compud as y C x, bing x ( ) x ( ) x( ) and C B P wih P soluion of h Lyapunov m quaion (Andrson B.D.O. and Moor J.B. (1971), PA A P M, M >. m m Nomnclaur Symbols C hrmal capacianc (J/K) h civ ha ransfr coff. (W/m K) hvs war lan vaporaion ha (J/g) I irradianc (W/m ) m flow ra (g/s) hrmal load (W) ω Ω hrmal rsisanc (K/W) mpraur (K) im (s) air spcific humidiy (g/g) dry air mass (g) Subscrips/Suprscrips AC q x g gr in in la ou rfrrd o h HVCAC sysm ucion cion quivaln xrnal inrnal gain al ground indoor air inrnal lan oudoor air m 117

10 Annamaria Buonomano, Umbro Monanaro, Adolfo Palombo, Sfania Sanini v vnilaion w nclosd zon nvlop wg war vapour frncs Andrson B.D.O. and Moor J.B. (1971). Linar Opimal Conrol, Englwood Cliff NJ, Prnic Hall. Buonomano A. and Palombo A. (14). "Building nrgy prformanc analysis by an in-hous dvlopd dynamic simulaion cod: An invsigaion for diffrn cas sudis." Applid Enrgy 113(): Di Brnardo M. al. (8). "Novl hybrid MAC- L conrol schms: synhsis, analysis and applicaions." Inrnaional Journal of Conrol 81(6): Ghiaus C. (14). "Linar algbra soluion o psychomric analysis of air-iioning sysms." Enrgy 74(): Ghiaus C. and Hazyuk I. (1). "Calculaion of opimal hrmal load of inrminly had buildings." Enrgy and Buildings 4(8): Ioannou P. and Fidan B. (6). Adapiv Conrol uorial: Advancs in Dsign and Conrol, SIAM. Landau I. D. (1979). Adapiv Conrol, h modl rfrnc approach, Springr-Varlag. Pdro A. and Sala A. (4). Mulivariabl Conrol Sysms: An Enginring Approach, Springr. Shaikh P. H. al. (14). "A rviw on opimizd conrol sysms for building nrgy and comfor managmn of smar susainabl buildings." nwabl and Susainabl Enrgy viws 34():

UNSTEADY FLOW OF A FLUID PARTICLE SUSPENSION BETWEEN TWO PARALLEL PLATES SUDDENLY SET IN MOTION WITH SAME SPEED

UNSTEADY FLOW OF A FLUID PARTICLE SUSPENSION BETWEEN TWO PARALLEL PLATES SUDDENLY SET IN MOTION WITH SAME SPEED 006-0 Asian Rsarch Publishing work (ARP). All righs rsrvd. USTEADY FLOW OF A FLUID PARTICLE SUSPESIO BETWEE TWO PARALLEL PLATES SUDDELY SET I MOTIO WITH SAME SPEED M. suniha, B. Shankr and G. Shanha 3

More information

MEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control

MEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ

More information

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract Applicaion of Diffrnial... Gnral Aricl Applicaion of diffrnial uaion in - and C- circui analysis by classical mhod. ajndra Prasad gmi curr, Dparmn of Mahmaics, P.N. Campus, Pokhara Email: rajndraprasadrgmi@yahoo.com

More information

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn

More information

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review Spring 6 Procss Dynamics, Opraions, and Conrol.45 Lsson : Mahmaics Rviw. conx and dircion Imagin a sysm ha varis in im; w migh plo is oupu vs. im. A plo migh imply an quaion, and h quaion is usually an

More information

Transfer function and the Laplace transformation

Transfer function and the Laplace transformation Lab No PH-35 Porland Sa Univriy A. La Roa Tranfr funcion and h Laplac ranformaion. INTRODUTION. THE LAPLAE TRANSFORMATION L 3. TRANSFER FUNTIONS 4. ELETRIAL SYSTEMS Analyi of h hr baic paiv lmn R, and

More information

Modelling of three dimensional liquid steel flow in continuous casting process

Modelling of three dimensional liquid steel flow in continuous casting process AMME 2003 12h Modlling of hr dimnsional liquid sl flow in coninuous casing procss M. Jani, H. Dyja, G. Banasz, S. Brsi Insiu of Modlling and Auomaion of Plasic Woring Procsss, Faculy of Marial procssing

More information

A MATHEMATICAL MODEL FOR NATURAL COOLING OF A CUP OF TEA

A MATHEMATICAL MODEL FOR NATURAL COOLING OF A CUP OF TEA MTHEMTICL MODEL FOR NTURL COOLING OF CUP OF TE 1 Mrs.D.Kalpana, 2 Mr.S.Dhvarajan 1 Snior Lcurr, Dparmn of Chmisry, PSB Polychnic Collg, Chnnai, India. 2 ssisan Profssor, Dparmn of Mahmaics, Dr.M.G.R Educaional

More information

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER A THREE COPARTENT ATHEATICAL ODEL OF LIVER V. An N. Ch. Paabhi Ramacharyulu Faculy of ahmaics, R D collgs, Hanamonda, Warangal, India Dparmn of ahmaics, Naional Insiu of Tchnology, Warangal, India E-ail:

More information

CSE 245: Computer Aided Circuit Simulation and Verification

CSE 245: Computer Aided Circuit Simulation and Verification CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy

More information

CPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees

CPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees CPSC 211 Daa Srucurs & Implmnaions (c) Txas A&M Univrsiy [ 259] B-Trs Th AVL r and rd-black r allowd som variaion in h lnghs of h diffrn roo-o-laf pahs. An alrnaiv ida is o mak sur ha all roo-o-laf pahs

More information

Lecture 2: Current in RC circuit D.K.Pandey

Lecture 2: Current in RC circuit D.K.Pandey Lcur 2: urrn in circui harging of apacior hrough Rsisr L us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R and a ky K in sris. Whn h ky K is swichd on, h charging

More information

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS Answr Ky Nam: Da: UNIT # EXPONENTIAL AND LOGARITHMIC FUNCTIONS Par I Qusions. Th prssion is quivaln o () () 6 6 6. Th ponnial funcion y 6 could rwrin as y () y y 6 () y y (). Th prssion a is quivaln o

More information

Midterm exam 2, April 7, 2009 (solutions)

Midterm exam 2, April 7, 2009 (solutions) Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions

More information

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -

More information

The transition:transversion rate ratio vs. the T-ratio.

The transition:transversion rate ratio vs. the T-ratio. PhyloMah Lcur 8 by Dan Vandrpool March, 00 opics of Discussion ransiion:ransvrsion ra raio Kappa vs. ransiion:ransvrsion raio raio alculaing h xpcd numbr of subsiuions using marix algbra Why h nral im

More information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

More information

Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors

Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar

More information

Wave Equation (2 Week)

Wave Equation (2 Week) Rfrnc Wav quaion ( Wk 6.5 Tim-armonic filds 7. Ovrviw 7. Plan Wavs in Losslss Mdia 7.3 Plan Wavs in Loss Mdia 7.5 Flow of lcromagnic Powr and h Poning Vcor 7.6 Normal Incidnc of Plan Wavs a Plan Boundaris

More information

C From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction.

C From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction. Inducors and Inducanc C For inducors, v() is proporional o h ra of chang of i(). Inducanc (con d) C Th proporionaliy consan is h inducanc, L, wih unis of Hnris. 1 Hnry = 1 Wb / A or 1 V sc / A. C L dpnds

More information

1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to:

1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to: Rfrncs Brnank, B. and I. Mihov (1998). Masuring monary policy, Quarrly Journal of Economics CXIII, 315-34. Blanchard, O. R. Proi (00). An mpirical characrizaion of h dynamic ffcs of changs in govrnmn spnding

More information

Section. Problem Representation. Substation. Protection Device. protection equipments. Substation. Client. EPDS divided in blocks connected by

Section. Problem Representation. Substation. Protection Device. protection equipments. Substation. Client. EPDS divided in blocks connected by HIERARCHICAL MULTIPLE CRITERIA OPTIMIZATION OF MAINTENANCE ACTIVITIES ON POWER DISTRIBUTION NETWORKS Problm Rprsaion EPDS comprising: Subsaions, primary nworks, scondary, nworks; Fdrs (cabls, lins, pols,

More information

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 ) AR() Procss Th firs-ordr auorgrssiv procss, AR() is whr is WN(0, σ ) Condiional Man and Varianc of AR() Condiional man: Condiional varianc: ) ( ) ( Ω Ω E E ) var( ) ) ( var( ) var( σ Ω Ω Ω Ω E Auocovarianc

More information

4.3 Design of Sections for Flexure (Part II)

4.3 Design of Sections for Flexure (Part II) Prsrssd Concr Srucurs Dr. Amlan K Sngupa and Prof. Dvdas Mnon 4. Dsign of Scions for Flxur (Par II) This scion covrs h following opics Final Dsign for Typ Mmrs Th sps for Typ 1 mmrs ar xplaind in Scion

More information

Charging of capacitor through inductor and resistor

Charging of capacitor through inductor and resistor cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.

More information

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields! Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr

More information

A Backstepping Simple Adaptive Control Application to Flexible Space Structures

A Backstepping Simple Adaptive Control Application to Flexible Space Structures Chins Journal of Aronauics 5 (01) 446-45 Conns liss availabl a cincdirc Chins Journal of Aronauics journal hompag: www.lsvir.com/loca/cja A Backspping impl Adapiv Conrol Applicaion o Flxibl pac rucurs

More information

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT [Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI

More information

I) Title: Rational Expectations and Adaptive Learning. II) Contents: Introduction to Adaptive Learning

I) Title: Rational Expectations and Adaptive Learning. II) Contents: Introduction to Adaptive Learning I) Til: Raional Expcaions and Adapiv Larning II) Conns: Inroducion o Adapiv Larning III) Documnaion: - Basdvan, Olivir. (2003). Larning procss and raional xpcaions: an analysis using a small macroconomic

More information

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form:

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form: Th Ingraing Facor Mhod In h prvious xampls of simpl firs ordr ODEs, w found h soluions by algbraically spara h dpndn variabl- and h indpndn variabl- rms, and wri h wo sids of a givn quaion as drivaivs,

More information

Lecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey

Lecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey cur : Growh and dcay of currn in circui Growh of currn in Circui us considr an inducor of slf inducanc is conncd o a DC sourc of.m.f. E hrough a rsisr of rsisanc and a ky K in sris. Whn h ky K is swichd

More information

Applied Statistics and Probability for Engineers, 6 th edition October 17, 2016

Applied Statistics and Probability for Engineers, 6 th edition October 17, 2016 Applid Saisics and robabiliy for Enginrs, 6 h diion Ocobr 7, 6 CHATER Scion - -. a d. 679.. b. d. 88 c d d d. 987 d. 98 f d.. Thn, = ln. =. g d.. Thn, = ln.9 =.. -7. a., by symmry. b.. d...6. 7.. c...

More information

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018 DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Aoc. Prof. Dr. Burak Kllci Spring 08 OUTLINE Th Laplac Tranform Rgion of convrgnc for Laplac ranform Invr Laplac ranform Gomric valuaion

More information

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35 MATH 5 PS # Summr 00.. Diffrnial Equaions and Soluions PS.# Show ha ()C #, 4, 7, 0, 4, 5 ( / ) is a gnral soluion of h diffrnial quaion. Us a compur or calculaor o skch h soluions for h givn valus of h

More information

7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS *

7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS * Andri Tokmakoff, MIT Dparmn of Chmisry, 5/19/5 7-11 7.4 QUANTUM MECANICAL TREATMENT OF FLUCTUATIONS * Inroducion and Prviw Now h origin of frquncy flucuaions is inracions of our molcul (or mor approprialy

More information

4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b

4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b 4. Th Uniform Disribuion Df n: A c.r.v. has a coninuous uniform disribuion on [a, b] whn is pdf is f x a x b b a Also, b + a b a µ E and V Ex4. Suppos, h lvl of unblivabiliy a any poin in a Transformrs

More information

Microscopic Flow Characteristics Time Headway - Distribution

Microscopic Flow Characteristics Time Headway - Distribution CE57: Traffic Flow Thory Spring 20 Wk 2 Modling Hadway Disribuion Microscopic Flow Characrisics Tim Hadway - Disribuion Tim Hadway Dfiniion Tim Hadway vrsus Gap Ahmd Abdl-Rahim Civil Enginring Dparmn,

More information

symmetric/hermitian matrices, and similarity transformations

symmetric/hermitian matrices, and similarity transformations Linar lgbra for Wirlss Communicaions Lcur: 6 Diffrnial quaions, Grschgorin's s circl horm, symmric/hrmiian marics, and similariy ransformaions Ov Edfors Dparmn of Elcrical and Informaion Tchnology Lund

More information

Poisson process Markov process

Poisson process Markov process E2200 Quuing hory and lraffic 2nd lcur oion proc Markov proc Vikoria Fodor KTH Laboraory for Communicaion nwork, School of Elcrical Enginring 1 Cour oulin Sochaic proc bhind quuing hory L2-L3 oion proc

More information

CHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano

CHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano Expcaions: Th Basic Prpard by: Frnando Quijano and Yvonn Quijano CHAPTER CHAPTER14 2006 Prnic Hall Businss Publishing Macroconomics, 4/ Olivir Blanchard 14-1 Today s Lcur Chapr 14:Expcaions: Th Basic Th

More information

H is equal to the surface current J S

H is equal to the surface current J S Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion

More information

EE 434 Lecture 22. Bipolar Device Models

EE 434 Lecture 22. Bipolar Device Models EE 434 Lcur 22 Bipolar Dvic Modls Quiz 14 Th collcor currn of a BJT was masurd o b 20mA and h bas currn masurd o b 0.1mA. Wha is h fficincy of injcion of lcrons coming from h mir o h collcor? 1 And h numbr

More information

Complex Dynamic Models of Star and Delta Connected Multi-phase Asynchronous Motors

Complex Dynamic Models of Star and Delta Connected Multi-phase Asynchronous Motors Complx Dynamic Modls of Sar and Dla Conncd Muli-pas Asyncronous Moors Robro Zanasi Informaion Enginring Dparmn Univrsiy of Modna Rggio Emilia Via Vignols 95 4 Modna Ialy Email: robrozanasi@unimori Giovanni

More information

Lecture 4: Laplace Transforms

Lecture 4: Laplace Transforms Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions

More information

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas Third In-Class Exam Soluions Mah 6, Profssor David Lvrmor Tusday, 5 April 07 [0] Th vrical displacmn of an unforcd mass on a spring is givn by h 5 3 cos 3 sin a [] Is his sysm undampd, undr dampd, criically

More information

Power communication network traffic prediction based on two dimensional prediction algorithms Lei Xiao Xue Yang Min Zhu Lipeng Zhu

Power communication network traffic prediction based on two dimensional prediction algorithms Lei Xiao Xue Yang Min Zhu Lipeng Zhu 4h Inrnaional Confrnc on Elcrical & Elcronics Enginring and Compur Scinc (ICEEECS 216 Powr communicaion nwork raffic prdicion basd on wo dimnsional prdicion algorihms Li Xiao Xu Yang Min Zhu Lipng Zhu

More information

On the Speed of Heat Wave. Mihály Makai

On the Speed of Heat Wave. Mihály Makai On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.

More information

Physics 160 Lecture 3. R. Johnson April 6, 2015

Physics 160 Lecture 3. R. Johnson April 6, 2015 Physics 6 Lcur 3 R. Johnson April 6, 5 RC Circui (Low-Pass Filr This is h sam RC circui w lookd a arlir h im doma, bu hr w ar rsd h frquncy rspons. So w pu a s wav sad of a sp funcion. whr R C RC Complx

More information

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is 39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h

More information

Real time estimation of traffic flow and travel time Based on time series analysis

Real time estimation of traffic flow and travel time Based on time series analysis TNK084 Traffic Thory sris Vol.4, numbr.1 May 008 Ral im simaion of raffic flow and ravl im Basd on im sris analysis Wi Bao Absrac In his papr, h auhor sudy h raffic parn and im sris. Afr ha, a im sris

More information

Logistic equation of Human population growth (generalization to the case of reactive environment).

Logistic equation of Human population growth (generalization to the case of reactive environment). Logisic quaion of Human populaion growh gnralizaion o h cas of raciv nvironmn. Srg V. Ershkov Insiu for Tim aur Exploraions M.V. Lomonosov's Moscow Sa Univrsi Lninski gor - Moscow 999 ussia -mail: srgj-rshkov@andx.ru

More information

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15] S.Y. B.Sc. (IT) : Sm. III Applid Mahmaics Tim : ½ Hrs.] Prlim Qusion Papr Soluion [Marks : 75 Q. Amp h following (an THREE) 3 6 Q.(a) Rduc h mari o normal form and find is rank whr A 3 3 5 3 3 3 6 Ans.:

More information

14.02 Principles of Macroeconomics Problem Set 5 Fall 2005

14.02 Principles of Macroeconomics Problem Set 5 Fall 2005 40 Principls of Macroconomics Problm S 5 Fall 005 Posd: Wdnsday, Novmbr 6, 005 Du: Wdnsday, Novmbr 3, 005 Plas wri your nam AND your TA s nam on your problm s Thanks! Exrcis I Tru/Fals? Explain Dpnding

More information

Transient Performance Analysis of Serial Production Lines

Transient Performance Analysis of Serial Production Lines Univrsiy of Wisconsin Milwauk UWM Digial Commons Thss and Dissraions Augus 25 Transin Prformanc Analysis of Srial Producion Lins Yang Sun Univrsiy of Wisconsin-Milwauk Follow his and addiional works a:

More information

Economics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 4/25/2011. UW Madison

Economics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 4/25/2011. UW Madison conomics 302 (Sc. 001) Inrmdia Macroconomic Thory and Policy (Spring 2011) 4/25/2011 Insrucor: Prof. Mnzi Chinn Insrucor: Prof. Mnzi Chinn UW Madison 21 1 Th Mdium Run ε = P * P Thr ar wo ways in which

More information

S-Z AC ANALYSIS OF SWITCHED CIRCUITS IN PSPICE

S-Z AC ANALYSIS OF SWITCHED CIRCUITS IN PSPICE S-Z AC ANALYSIS OF SWITCHED CIRCUITS IN PSPICE PROF. ING. DALIBOR BIOLEK, CSC. ING. IERA BIOLKOÁ DOC. DR. ING. ZDENĚK KOLKA Absrac: Th papr xplains basic idas how o modl and analyz h AC bhavior of circuis

More information

Routing in Delay Tolerant Networks

Routing in Delay Tolerant Networks Rouing in Dlay Tolran Nworks Primary Rfrnc: S. Jain K. Fall and R. Para Rouing in a Dlay Tolran Nwork SIGCOMM 04 Aug. 30-Sp. 3 2004 Porland Orgon USA Sudn lcur by: Soshan Bali (748214) mail : sbali@ic.ku.du

More information

Integrity Control in Nested Certificates

Integrity Control in Nested Certificates Ingriy onrol in Nsd s $OEHUW/HYLDQG08IXNdD OD\DQ %R D]LoL8QLYHUVLW\'HSDUWPHQWRI&RPSXWHU(QJLQHHULQJ Bbk, Isanbul 80815, Turky lvi@boun.du.r caglayan@boun.du.r Absrac Nsd crificas [3,4] ar proposd as crificas

More information

Control System Engineering (EE301T) Assignment: 2

Control System Engineering (EE301T) Assignment: 2 Conrol Sysm Enginring (EE0T) Assignmn: PART-A (Tim Domain Analysis: Transin Rspons Analysis). Oain h rspons of a uniy fdack sysm whos opn-loop ransfr funcion is (s) s ( s 4) for a uni sp inpu and also

More information

Arturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/

Arturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/ Comparison of RPA-lik modls in Nurino-Nuclus Nuclus Procsss Aruro R. Samana* in collaboraion wih Carlos Brulani* & FranjoKrmpoicUNLP-Argnina *Dparmn of Physics Txas A&M Univrsiy -Commrc 07/ 0/008 Aomic

More information

RESONANT CAVITY. Supplementary Instructions

RESONANT CAVITY. Supplementary Instructions UNIEITY OF TOONTO Dparmn of Elcrical and ompur Enginring Filds and Wavs aboraory ourss EE 3F and EE 357 III Yar EONANT AITY upplmnary Insrucions EONANE Pag of 3 Pag 3 of 3. Inroducion, gnral rsonanc A

More information

where: u: input y: output x: state vector A, B, C, D are const matrices

where: u: input y: output x: state vector A, B, C, D are const matrices Sa pac modl: linar: y or in om : Sa q : f, u Oupu q : y h, u u Du F Gu y H Ju whr: u: inpu y: oupu : a vcor,,, D ar con maric Eampl " $ & ' " $ & 'u y " & * * * * [ ],, D H D I " $ " & $ ' " & $ ' " &

More information

The Science of Monetary Policy

The Science of Monetary Policy Th Scinc of Monary Policy. Inroducion o Topics of Sminar. Rviw: IS-LM, AD-AS wih an applicaion o currn monary policy in Japan 3. Monary Policy Sragy: Inrs Ra Ruls and Inflaion Targing (Svnsson EER) 4.

More information

Institute of Actuaries of India

Institute of Actuaries of India Insiu of Acuaris of India ubjc CT3 Probabiliy and Mahmaical aisics Novmbr Examinaions INDICATIVE OLUTION Pag of IAI CT3 Novmbr ol. a sampl man = 35 sampl sandard dviaion = 36.6 b for = uppr bound = 35+*36.6

More information

Impulsive Differential Equations. by using the Euler Method

Impulsive Differential Equations. by using the Euler Method Applid Mahmaical Scincs Vol. 4 1 no. 65 19 - Impulsiv Diffrnial Equaions by using h Eulr Mhod Nor Shamsidah B Amir Hamzah 1 Musafa bin Mama J. Kaviumar L Siaw Chong 4 and Noor ani B Ahmad 5 1 5 Dparmn

More information

A HAMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS

A HAMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS Europan Scinific Journal Ocobr 13 diion vol9, No3 ISSN: 1857 7881 (Prin) - ISSN 1857-7431 A AMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS Ola A Jarab'ah Tafila Tchnical Univrsiy, Tafila, Jordan Khald

More information

Single Electron Devices for Logic Applications

Single Electron Devices for Logic Applications Sinl Elcron Dvics for Loic Applicaions Rza M. Rad UMB Basd on pas 45-441 441 of Nanolcronics and Informaion Tchnoloy,, Rainr Wasr Inroducion Scalin down MOSFETs has bn fundamnal in improvin h prformanc

More information

A Condition for Stability in an SIR Age Structured Disease Model with Decreasing Survival Rate

A Condition for Stability in an SIR Age Structured Disease Model with Decreasing Survival Rate A Condiion for abiliy in an I Ag rucurd Disas Modl wih Dcrasing urvival a A.K. upriana, Edy owono Dparmn of Mahmaics, Univrsias Padjadjaran, km Bandung-umng 45363, Indonsia fax: 6--7794696, mail: asupria@yahoo.com.au;

More information

Asymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct

Asymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct Qus Journals Journal of Rsarch in Applid Mahmaics Volum ~ Issu (5 pp: -5 ISSN(Onlin : 94-74 ISSN (Prin:94-75 www.usjournals.org Rsarch Papr Asympoic Soluions of Fifh Ordr Criically Dampd Nonlinar Sysms

More information

Review Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( )

Review Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( ) Rviw Lcur 5 Firs-ordr circui Th sourc-fr R-C/R-L circui Sp rspons of an RC/RL circui v( ) v( ) [ v( 0) v( )] 0 Th i consan = RC Th final capacior volag v() Th iniial capacior volag v( 0 ) Volag/currn-division

More information

Theoretical modeling of airways pressure waveform for dual-controlled ventilation with physiological pattern and linear respiratory mechanics

Theoretical modeling of airways pressure waveform for dual-controlled ventilation with physiological pattern and linear respiratory mechanics J. Biomdical Scinc and Enginring,, 4, 3-34 doi:.436/jbis..444 ublishd Onlin April (hp://www.sci.org/journal/jbis/). Thorical modling of airways prssur wavform for dual-conrolld vnilaion wih physiological

More information

Advances in automation design for fast vessels propulsion

Advances in automation design for fast vessels propulsion Advancs in auomaion dsign for fas vssls propulsion M. Alosol, G. Bnvnuo & M. Marlli Dparmn of Naval Archicur and Elcrical Enginring, Gnova, Ialy M. Galli Sasma S.p.A., Gnova, Ialy ABSTRACT: Suprior prformanc,

More information

SRF OPTIMIZATION OF THE END CELLS IN SRF CAVITIES

SRF OPTIMIZATION OF THE END CELLS IN SRF CAVITIES SRF588-7 OPTIMIZATION OF THE END CELLS IN SRF CAVITIES Jonahan W. Luk Univrsiy of California, San Digo, La Jolla, CA 9293 Valry Shmlin Laboraory for Elmnary-Paricl Physics, Cornll Univrsiy, Ihaca, NY 14853

More information

Reliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach.

Reliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach. Inrnaional Journal of Compuaional Sin and Mahmais. ISSN 97-3189 Volum 3, Numr 3 11, pp. 351-3 Inrnaional Rsarh Puliaion Hous hp://www.irphous.om Rliailiy Analysis of a Bridg and Paralll Sris Nworks wih

More information

Chemistry 988 Part 1

Chemistry 988 Part 1 Chmisry 988 Par 1 Radiaion Dcion & Masurmn Dp. of Chmisry --- Michigan Sa Univ. aional Suprconducing Cycloron Lab DJMorrissy Spring/2oo9 Cours informaion can b found on h wbsi: hp://www.chmisry.msu.du/courss/cm988uclar/indx.hml

More information

3(8 ) (8 x x ) 3x x (8 )

3(8 ) (8 x x ) 3x x (8 ) Scion - CHATER -. a d.. b. d.86 c d 8 d d.9997 f g 6. d. d. Thn, = ln. =. =.. d Thn, = ln.9 =.7 8 -. a d.6 6 6 6 6 8 8 8 b 9 d 6 6 6 8 c d.8 6 6 6 6 8 8 7 7 d 6 d.6 6 6 6 6 6 6 8 u u u u du.9 6 6 6 6 6

More information

Part I: Short Answer [50 points] For each of the following, give a short answer (2-3 sentences, or a formula). [5 points each]

Part I: Short Answer [50 points] For each of the following, give a short answer (2-3 sentences, or a formula). [5 points each] Soluions o Midrm Exam Nam: Paricl Physics Fall 0 Ocobr 6 0 Par I: Shor Answr [50 poins] For ach of h following giv a shor answr (- snncs or a formula) [5 poins ach] Explain qualiaivly (a) how w acclra

More information

5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t

5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t AP CALCULUS FINAL UNIT WORKSHEETS ACCELERATION, VELOCTIY AND POSITION In problms -, drmin h posiion funcion, (), from h givn informaion.. v (), () = 5. v ()5, () = b g. a (), v() =, () = -. a (), v() =

More information

Modelling and optimization of multi-energy source building systems in the design concept phase

Modelling and optimization of multi-energy source building systems in the design concept phase rocdgs of Clima 2007 WllBg Indoors Modllg and opimizaion of muli-nrgy sourc buildg sysms h dsign concp phas Vcnzo Corrado, Enrico Fabrizio and Marco Filippi Diparimno di Enrgica (DENER), olicnico di Toro,

More information

Chapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System

Chapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System EE 422G No: Chapr 5 Inrucor: Chung Chapr 5 Th Laplac Tranform 5- Inroducion () Sym analyi inpu oupu Dynamic Sym Linar Dynamic ym: A procor which proc h inpu ignal o produc h oupu dy ( n) ( n dy ( n) +

More information

Estimation of Metal Recovery Using Exponential Distribution

Estimation of Metal Recovery Using Exponential Distribution Inrnaional rd Journal o Sinii sarh in Enginring (IJSE).irjsr.om Volum 1 Issu 1 ǁ D. 216 ǁ PP. 7-11 Esimaion o Mal ovry Using Exponnial Disribuion Hüsyin Ankara Dparmn o Mining Enginring, Eskishir Osmangazi

More information

Lagrangian for RLC circuits using analogy with the classical mechanics concepts

Lagrangian for RLC circuits using analogy with the classical mechanics concepts Lagrangian for RLC circuis using analogy wih h classical mchanics concps Albrus Hariwangsa Panuluh and Asan Damanik Dparmn of Physics Educaion, Sanaa Dharma Univrsiy Kampus III USD Paingan, Maguwoharjo,

More information

Study on the Lightweight checkpoint based rollback recovery mechanism

Study on the Lightweight checkpoint based rollback recovery mechanism 9 Inrnaional Confrnc on Compur Enginring and Applicaions II vol. IAI rss, Singapor Sudy on h ighwigh chcpoin basd rollbac rcovry mchanism Zhang i,3, ang Rui Dai Hao 3, Ma Mingai 3 and i Xianghong 4 Insiu

More information

FWM in One-dimensional Nonlinear Photonic Crystal and Theoretical Investigation of Parametric Down Conversion Efficiency (Steady State Analysis)

FWM in One-dimensional Nonlinear Photonic Crystal and Theoretical Investigation of Parametric Down Conversion Efficiency (Steady State Analysis) Procdings of h Inrnaional MuliConfrnc of nginrs and Compur Sciniss 9 Vol II IMCS 9 March 8-9 Hong Kong FWM in On-dimnsional Nonlinar Phoonic Crysal and Thorical Invsigaion of Paramric Down Convrsion fficincy

More information

Double Slits in Space and Time

Double Slits in Space and Time Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an

More information

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu Chapr 3: Fourir Rprsnaion of Signals and LTI Sysms Chih-Wi Liu Oulin Inroducion Complx Sinusoids and Frquncy Rspons Fourir Rprsnaions for Four Classs of Signals Discr-im Priodic Signals Fourir Sris Coninuous-im

More information

FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Introduction and Linear Systems

FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Introduction and Linear Systems FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Inroducion and Linar Sysms David Lvrmor Dparmn of Mahmaics Univrsiy of Maryland 9 Dcmbr 0 Bcaus h prsnaion of his marial in lcur will diffr from

More information

A Simple Procedure to Calculate the Control Limit of Z Chart

A Simple Procedure to Calculate the Control Limit of Z Chart Inrnaional Journal of Saisics and Applicaions 214, 4(6): 276-282 DOI: 1.5923/j.saisics.21446.4 A Simpl Procdur o Calcula h Conrol Limi of Z Char R. C. Loni 1, N. A. S. Sampaio 2, J. W. J. Silva 2,3,*,

More information

14.02 Principles of Macroeconomics Fall 2005 Quiz 3 Solutions

14.02 Principles of Macroeconomics Fall 2005 Quiz 3 Solutions 4.0 rincipl of Macroconomic Fall 005 Quiz 3 Soluion Shor Quion (30/00 poin la a whhr h following amn ar TRUE or FALSE wih a hor xplanaion (3 or 4 lin. Each quion coun 5/00 poin.. An incra in ax oday alway

More information

A new cast-resin transformer thermal model based on recurrent neural networks

A new cast-resin transformer thermal model based on recurrent neural networks AHIVES OF ELETIAL ENGINEEING VOL. 66(), pp. 7-28 (207) DOI 0.55/a-207-0002 A n cas-rsin ransformr hrmal modl basd on rcurrn nural nors DAVOOD AZIZIAN, MEHDI BIGDELI 2 Dparmn of Elcrical Enginring, Abhar

More information

Final Exam : Solutions

Final Exam : Solutions Comp : Algorihm and Daa Srucur Final Exam : Soluion. Rcuriv Algorihm. (a) To bgin ind h mdian o {x, x,... x n }. Sinc vry numbr xcp on in h inrval [0, n] appar xacly onc in h li, w hav ha h mdian mu b

More information

ERROR ANALYSIS A.J. Pintar and D. Caspary Department of Chemical Engineering Michigan Technological University Houghton, MI September, 2012

ERROR ANALYSIS A.J. Pintar and D. Caspary Department of Chemical Engineering Michigan Technological University Houghton, MI September, 2012 ERROR AALYSIS AJ Pinar and D Caspary Dparmn of Chmical Enginring Michigan Tchnological Univrsiy Houghon, MI 4993 Spmbr, 0 OVERVIEW Exprimnaion involvs h masurmn of raw daa in h laboraory or fild I is assumd

More information

Coherence and interactions in diffusive systems. Cours 4. Diffusion + e-e interations

Coherence and interactions in diffusive systems. Cours 4. Diffusion + e-e interations Cohrnc and inracions in diffusiv sysms G. Monambaux Cours 4 iffusion + - inraions nsiy of sas anomaly phasing du o lcron-lcron inracions Why ar h flucuaions univrsal and wak localizaion is no? ΔG G cl

More information

Fixed-Relative-Deadline Scheduling of Hard Real-Time Tasks with Self-Suspensions

Fixed-Relative-Deadline Scheduling of Hard Real-Time Tasks with Self-Suspensions Fixd-Rlaiv-Dadlin Schduling of Hard Ral-Tim Tasks wih Slf-Suspnsions Jian-Jia Chn Dparmn of Informaics TU Dormund Univrsiy, Grmany jia.chn@u-dormund.d Absrac In many ral-im sysms, asks may xprinc slf-suspnsion

More information

The Optimal Timing of Transition to New Environmental Technology in Economic Growth

The Optimal Timing of Transition to New Environmental Technology in Economic Growth h Opimal iming of ransiion o Nw Environmnal chnology in Economic Growh h IAEE Europan Confrnc 7- Spmbr, 29 Vinna, Ausria Akira AEDA and akiko NAGAYA yoo Univrsiy Background: Growh and h Environmn Naural

More information

ARTHUR STANLEY HOUSE WELCOME AND INTRODUCTION. The Site Today. Existing: G o o d g e P l a c e V i e w

ARTHUR STANLEY HOUSE WELCOME AND INTRODUCTION. The Site Today. Existing: G o o d g e P l a c e V i e w WELCOME AND INTRODUCTION W s b ro o k P a r n r s w l c o m s y o u o i s d ro p - i n s s s i o n o v i w i s p ro p o s a l s f o r a r v i s d m i x d u s d v l o p m n f o r A r h u r S a n l y H o

More information

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline. Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.

More information

( ) C R. υ in RC 1. cos. ,sin. ω ω υ + +

( ) C R. υ in RC 1. cos. ,sin. ω ω υ + + Oscillaors. Thory of Oscillaions. Th lad circui, h lag circui and h lad-lag circui. Th Win Bridg oscillaor. Ohr usful oscillaors. Th 555 Timr. Basic Dscripion. Th S flip flop. Monosabl opraion of h 555

More information

Title. Author(s)ANG, K. K.; THI, T. M.; HAI, L. V. Issue Date Doc URL. Type. Note. File Information.

Title. Author(s)ANG, K. K.; THI, T. M.; HAI, L. V. Issue Date Doc URL. Type. Note. File Information. il RACK VIBRAIONS DURING ACCEERAING AND DECEERAIN Auhor(s)ANG, K. K.; HI,. M.; HAI,. V. Issu Da 01-09-1 Doc UR hp://hdl.handl.n/115/54479 yp procdings No h hirnh Eas Asia-Pacific Confrnc on Sruc 1, 01,

More information

EXERCISE - 01 CHECK YOUR GRASP

EXERCISE - 01 CHECK YOUR GRASP DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc

More information