Evaluation of Virtual Refrigerant Mass Flow Sensors

Size: px
Start display at page:

Download "Evaluation of Virtual Refrigerant Mass Flow Sensors"

Transcription

1 Purdu Univrsity Purdu -Pubs Intrnational Rfrigration and Air Conditioning Confrnc School of Mchanical Enginring 01 Evaluation of Virtual Rfrigrant Mass Flow Snsors Woohyun Kim Jams E. Braun Follow this and additional works at: Kim, Woohyun and Braun, Jams E., "Evaluation of Virtual Rfrigrant Mass Flow Snsors" (01). Intrnational Rfrigration and Air Conditioning Confrnc. Papr This documnt has bn mad availabl through Purdu -Pubs, a srvic of th Purdu Univrsity Libraris. Plas contact pubs@purdu.du for additional information. Complt procdings may b acquird in print and on CD-ROM dirctly from th Ray W. Hrrick Laboratoris at Hrrick/Evnts/ordrlit.html

2 99, Pag 1 Evaluation of Virtual Rfrigrant Mass Flow Snsors Woohyun Kim, Jams E. Braun* Hrrick Laboratory, Purdu Univrsity, Mchanical Enginring, Wst Lafaytt, IN, 7906, USA * Corronding Author: jbraun@purdu.du ABSTRACT Rfrigrant mass flow rat is an important masurmnt for monitoring quipmnt prformanc and nabling fault dtction and diagnostics. Howvr, a traditional mass flow mtr is xpnsiv to purchas and install. A virtual rfrigrant mass flow snsor (VRMF) uss a mathmatical modl to stimat flow rat using low-cost masurmnts and can potntially b implmntd at low cost. This study valuats thr VRMFs for stimating rfrigrant mass flow rat. Th first modl uss a comprssor map that rlats rfrigrant flow rat to masurmnts of inlt and outlt prssur, and inlt tmpratur masurmnts. Th scond modl uss an nrgy-balanc mthod on th comprssor that uss a comprssor map for powr consumption, which is rlativly indpndnt of comprssor faults that influnc mass flow rat. Th third modl is dvlopd using an mpirical corrlation for an lctronic xpansion valv (EEV) basd on an orific quation. Th thr VRMFs ar shown to work wll in stimating rfrigrant mass flow rat for various systms undr fault-fr conditions with lss than 5% RMS rror. Each of th thr mass flow rat stimats can b utilizd to diagnos and track th following faults: 1) loss of comprssor prformanc, ) fould condnsr or vaporator filtr, 3) faulty xpansion dvic, rctivly. For xampl, a comprssor rfrigrant flow map modl only provids an accurat stimation whn th comprssor oprats normally. Whn a comprssor suction or discharg valv is laking and th comprssor is not dlivring th xpctd flow, th nrgy-balanc or EEV modl can provid accurat flow stimats. In this cas, th flow diffrncs provid an indication of loss of comprssor prformanc and can b usd for fault dtction and diagnostics, as will b dmonstratd in this papr. 1. Introduction Spac hating, vntilation and air conditioning (HVAC) account for 0% of rsidntial primary nrgy us, and for 30% of primary nrgy us in commrcial buildings (DOE,010). Ovr half of all conditiond floor ac in th U.S. incorporats packagd HVAC quipmnt in thir systm dsign (Brodrick, 000). Th study conductd by Mssngr (008) indicats unitary air conditionrs typically do not achiv ratd fficincy bcaus of impropr installation or lack of srvicing in th fild. This papr suggstd that srvic and rplacmnt programs can yild nrgy savings on th ordr of 30 to 50%. Th othr study from ADM (009) valuatd 109 units in th fild and found that 89 had fault conditions, with 31having two or mor faults. Th avrag EER for th units incrasd from 6.6 bfor srvicing to 7.0 aftr srvicing, an avrag incras of 6.1%. Anothr invstigation (Katipamula, 005) suggstd that faults or non-optimal control can caus th malfunction of quipmnt or prformanc dgradation from 15 to 50%. Automatd diagnostics has th potntial to addrss ths fild prformanc problms and produc significant nrgy savings. Rfrigrant mass flow rat is an important masurmnt for monitoring HVAC systms and nabling Automatd Fault Dtction and Diagnostics (AFDD) to sav nrgy and xtnd quipmnt lif. Thr diffrnt virtual rfrigrant mass flow (VRMF) snsors wr dvlopd and valuatd in this study that us mathmatical modls to stimat flow rat using low cost masurmnts. Th thr approachs us: 1) a comprssor map for rfrigrant mass flow rat that uss inlt prssur and tmpratur and outlt prssur as inputs; ) an nrgy-balanc mthod mploys a virtual snsor for powr consumption basd on a comprssor map; 3) smi-mpirical corrlations for EEV and thrmostatic xpansion valvs (TXV) that ar basd on an orific quation. Th modls wr traind and tstd using data obtaind from arlir laboratory studis. Th application of th virtual snsors for diagnosing comprssor valv faults and insnsitivity to othr faults ar also dmonstratd using th availabl data. Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

3 99, Pag. Systm dscriptions and tst conditions Laboratory tst data from a varity of sourcs wr usd to dvlop and valuat VRMF snsors. Tabl 1 givs cifications for quipmnt whr data wr obtaind through laboratory tsting. Th systms includ a watr-towatr hat pump with a variabl-d comprssor, a rsidntial air lit systm, and light commrcial packagd systms with fixd and variabl-d comprssors. Th systms usd ithr a TXV or EEV as an xpansion dvic and R- or R-10A as a rfrigrant. Som of th units includd low-sid accumulators. Tabl prsnts th rang of oprating tst conditions for ach unit, including th rang of rfrigrant flow rats ncountrd. Th laboratory tst data wr obtaind with variations in both indoor and ambint tmpratur. Thr of four systms wr tstd with diffrnt condnsr and vaporator airflow rats, which could rprsnt faults associatd with a dirty air filtr or coil fouling. All of th systms xcpt for systm II wr tstd at diffrnt rfrigrant charg lvls to simulat impropr charg srvic and rfrigrant lakag. Systms I and III includd simulatd comprssor valv lakag faults whr a portion of th discharg flow from th comprssor was bypassd to th comprssor suction. Systm II was a laboratory stup for tsting lctronic xpansion valvs ovr a vry wid rang of rfrigrant flows. Two diffrnt valvs (B0B and B1F in th Tabl 1) wr tstd with two diffrnt rfrigrants (R-10A and R-0A in Tabl ). Th B1F valv has a ratd rfrigrant flow (also cooling capacity and associatd air/watr flow) that is thr tims highr than that for th B0B valv with a 10 bar prssur diffrnc across th imum valv opning, basd on th cification in th manufacturr s catalog. During th cours of tsting for systm II, it was discovrd that th comprssor was not oprating normally and was dlivring significantly lss than th ratd flow. Thus, this data st could also b usd to rprsnt faulty comprssor bhavior. Systm III also includd fault tsting for a liquid lin rstriction (additional prssur drop incras through liquid lin) and th prsnc of non-condnsabl gas (injction of nitrogn gas into th systm). In gnral, only normal oprating (i.., no-fault) data wr usd to larn paramtrs of th VRMF snsors, whras all of th data wr usd for assssing VRMF snsor prformanc. Tabl 1 Systm dscriptions for laboratory tst data Systm Siz (kw) Rfrigrant Comprssor Expansion Dvic Accumulator Systm Typ Variabl-d I (Kim,005) 3 R- EEV No comprssor Watr to Watr R-10A EEV II (Bach, 010) 7.0 Fixd-d Ys R-0A (B0B/B1F) comprssors III (Payn, 008) 8.8 R-10A TXV Ys Air Split Typ Systm Indoor Tmpratur Dry Wt Tabl Tst conditions for laboratory tsting data Prcntag of Ambint Indoor air/ rat rfrigrant tmpratur watr flow rat mass flow rat Outdoor air/ watr flow rat Rfrigrant charg ( C ) ( C) ( F ) [ % ] [ % ] [%] [ % ] I //3/0 65~100 35~100 5~100 60~100 II / 8 0~100 (R10A) 10~100 (R0A) III 6.7 / 1 19 / 15/ Dry 3.1 Dvlopmnt of VRMF snsor I 8/ 35/ 39 60~100 70~ VRMF snsor I basd on a comprssor flow map 50~100 (Coil Block) 70~130 A comprssor map is usd to stimat rfrigrant mass flow rat using input masurmnts of inlt and outlt prssur. Basd on ARI Standard 50, rfrigrant mass flow rat for a fixd d comprssor can b rprsntd using a 10-cofficint polynomial quation for a cifid amount of suprhat. Th map at th cifid suprhat is typically corrctd using th ratio of th comprssor suction dnsity at th actual suprhat to th dnsity at th Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

4 99, Pag 3 tstd suprhat. Basd on th ARI modl form, th VRMF Snsor I for a fixd-d comprssor is dtrmind using quation 1. m a a T a T a T a T 3 a T T a T 3 6 a T 3 7 a T T a T T map suc 0 1 c c 5 c c c (1) whr m map is th stimatd rfrigrant mass flow rat, th a s ar mpirical cofficints, T is vaporating saturation tmpratur, T c is condnsing saturation tmpratur, and ρ suc is th dnsity at th suction (inlt) of th comprssor. Th dvlopmnt of VRMF snsor I for a variabl-d comprssor is xplaind in Kim and Braun (01). Equation 1 is usd to map th mass flow rat for a ratd frquncy and this is corrctd for othr frquncis using a scond-ordr polynomial as givn in quation. Th c and b cofficints ar stimatd using rgrssion analysis applid to xprimntal data. map suc 8 9 c c 1 f fratd c f fratd c3 b 0 bt 1 c bt c b3t bt b5t c Tc ratd, frquncy m () whr th b s and c s ar mpirical cofficints, f is comprssor frquncy, and f ratd is th ratd comprssor frquncy. 3. Prformanc of VRMF snsor I Figurs 1 and show th prformanc of VRMF Snsor I that is basd on a comprssor map. Th trms Normal, Comp Fault, Cond Fault, Evap Fault, Liquid Fault, Charg Fault, and NonCond Fault stand for no fault, comprssor lakag fault, condnsr fouling fault, vaporator fouling fault, liquid-lin rstriction fault, rfrigrant lakag fault, and non-condnsabl gas fault, rctivly To valuat prformanc of th VRMF snsor, th prdictd ratio of rfrigrant mass flow rat to ratd flow is compard to th valu dtrmind using masurmnts. Th VRMF modls wr dvlopd using only th normal data but usd to prdict flow rats for all of th fault tsts. Figur 1: Prformanc of VRMF snsor basd on fixd-d comprssor map for systm III undr no fault and fault conditions (RMS of snsor rrors shown for ach fault typ) Figur : Prformanc of VRMF snsor basd on variabl d comprssor map for systm I undr no fault and fault conditions (RMS of snsor rrors shown for ach fault typ) Figur 1 shows th prformanc of VRMF snsor I for systm III with a fixd-d comprssor undr no fault and various faulty conditions. Th RMS rror is gnrally lss than % for normal opration and with a varity of faults xcpt for comprssor valv lakag. For th rang of comprssor lakag conditions considrd, th RMS rror for th VRMF snsor I was 19%. In gnral, th rror incrass with th svrity of th comprssor lakag fault. As a rsult, diffrncs btwn rfrigrant flow dtrmind using VRMF snsor I and othr VRMF snsors can b usd to diagnos a fault associatd with th comprssor not dlivring th propr rfrigrant flow. Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

5 99, Pag Figur shows th prformanc of VRMF snsor I for systm I with a variabl-d comprssor undr no fault and various fault conditions. Although th VRMF snsor I was traind using only no-fault data, it accuratly stimats mass flow rat for faulty conditions ovr th rang of oprating frquncis, xcpt for th comprssor valv lakag fault. Th RMS rrors for VRMF snsor I wr lss than 3% for condnsr fouling, rfrigrant charg, and vaporator fouling conditions, rctivly. Howvr, VRMF snsor I prdictions wr about 16% highr than masurmnts for th rang of comprssor fault conditions considrd, with th rrors incrasing with fault lvl..1 Dvlopmnt of VRMF snsor II. VRMF snsor II basd on a comprssor nrgy balanc In ordr to diagnos comprssor flow problms, it is ncssary to hav an altrnativ VRMF snsor. On altrnativ approach is to us an nrgy balanc on th comprssor to stimat flow rat as shown in quation 3. Li (006) dmonstratd that this mthod provids accurat flow prdictions whn using a virtual comprssor snsor for powr consumption, vn in th prsnc of a comprssor valv lakag fault or othr faults. Compard to th map-basd mthod, th nrgy balanc modl is much simplr and can b usd for both fixd-d and variabl-d comprssors. m nrgy h ( T, P W 1 ) h dis dis dis suc suc suc (3) whr α loss is comprssor hat loss ratio, W is comprssor powr consumption, and h dis (T dis,p dis ) and h suc (T suc,p suc ) ar th discharg lin and suction lin rfrigrant nthalpy. Th comprssor powr consumption, discharg prssur (P dis ) and suction prssur (P suc ) can b stimatd using othr virtual snsors. α loss is gnrally vry small (undr 5%) for quipmnt having a fixd-d comprssor oprating normally. Howvr, it can b mor significant at low comprssor ds for variabl-d quipmnt or with faults for fixdd quipmnt. For xampl, dcrasing th comprssor frquncy from 60Hz to 30Hz almost doubls th hat loss as a fraction of th powr input. To provid mor accurat mass flow rats prdictions undr various faulty conditions and/or ds, an mpirical modl for α loss was dvlopd that is traind using rgrssion applid to data. Th modl for fixd-d quipmnt is givn in quation, whil a function for variabl-d quipmnt is shown in quation 5. loss ( T, P loss, prd c0 c1pdis cpsuc c3tdis ctsuc loss, prd c0 c1p dis cpsuc c3t dis ct suc c5 ) () f (5) whr th c s ar mpirical cofficints, P suc is suction prssur, P dis is discharg prssur, T amb is comprssor ambint tmpratur, T suc is suction tmpratur, and f is d of th comprssor motor.. Prformanc of VRMF snsor II Figur 3 shows th prformanc of VRMF snsor II for systm III with a fixd-d comprssor. Th mass flow rat prdiction was dtrmind using hat loss stimats and prdictions of othr virtual snsors. Th hat loss modl was dtrmind using data for normal opration whr th hat loss was dtrmind from an nrgy balanc on th comprssor with th flow masurd. Th powr consumption was dtrmind using a map in trms of suction prssur and tmpratur and discharg prssur as outlind in Kim and Braun (01). Th RMS rror for th VRMF snsor was lss than 3% for all of th data, including both normal and faulty conditions. Th largr rrors for th vaporator fouling occurrd whn th suprhat at th comprssor inlt was blow 1.5F. Th incorrct comprssor suction nthalpy du to a two-phas rfrigrant inlt stat ld to th inaccurat stimat of mass flow rat. Th VRMF snsor II is rlativly indpndnt of comprssor faults compard to th VRMF snsor I. Figur shows th prformanc of VRMF snsor II for systm II with a variabl-d comprssor. Th mass flow rat stimats wr compard to masurmnts for a rang of diffrnt faults at diffrnt fault lvls. Th RMS rror for th VRMF snsor II is lss than 5%. Excpt for svral low comprssor d conditions, th VRMF works wll rgardlss of th fault conditions. Howvr, thr wr som significant rrors (10%) at low frquncis. Additional Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

6 99, Pag 5 work is ncssary to accuratly dtrmin hat loss for variabl-d comprssors whn oprating at low frquncis. Figur 3: Prformanc of VRMF snsor II basd on nrgy balanc for systm III undr no fault and fault conditions (RMS of rrors shown for ach fault typ) Figur : Prformanc of VRMF snsor II basd on nrgy balanc for systm I undr no fault and fault conditions (RMS of rrors shown for ach fault typ) 5. VRMF snsor III basd on an xpansion valv modl Expansion dvics ar usd to drop th prssur of th rfrigrant and to rgulat th rfrigrant mass flow rat in rons to a variabl load. Thr ar thr typs of xpansion dvics usd in air conditionrs: fixd-orific (FXO), thrmostatic xpansion valv (TXV), and lctronic xpansion valv (EEV). Evn though an FXO has advantags of simplicity and low cost, it is not appropriat for a systm that rquirs prcis flow control for a wid rang of flow rat rquirmnts. TXV and EEV dvics ar adjustabl throat-ara xpansion valvs. Th TXV adopts a mchanical control mthod to obtain rlativly constant suprhat at th vaporator outlt. Th EEV provids a mor prcis control of suprhat and fast flow control for a wid rang of mass flow rats bcaus it uss lctronic actuation and snsor information along with a digital fdback controllr. Most of th prvious litratur on modling of xpansion dvics has focusd on constant-ara xpansion dvics, such as FXO. Modls for prdicting th mass flow charactristics of TXVs and EEVs ar limitd. Li (008) dvlopd gnralizd xprssions for TXV mass flow as a function of suprhat and valv. Shanwi t al. (005) and Park t al. (007) dvlopd mpirical corrlations for mass flow rat through an EEV by prforming th dimnsionlss analysis basd on a powr law form. Howvr, ths xisting modls rquir ithr dtaild gomtric paramtrs or many masurmnts to rprsnt prformanc. This papr prsnts VRMF snsors for TXV and EEV dvics basd on a smi-mpirical modl that can b traind using a rlativly small amount of data and thn can stimat rfrigrant mass flow rat as part of an automatd diagnostic systm. 5.1 Dvlopmnt of VRMF snsor III for TXV Th valv opning for a TXV is dtrmind by a forc balanc on a diaphragm, as dpictd in Figur 5. Th bulb and suction-lin prssur act on opposit sids of th diaphragm and coupld with th ring forc, control th ffctiv orific ara. Th vaporator inlt and condnsr prssur influnc th flow rat through th orific for a givn opning. Th bulb typically contains a two-phas mixtur of th sam rfrigrant that is mployd within th systm. Thrfor, whn a positiv suprhat xists at th vaporator outlt thn thr is a positiv diffrnc btwn th bulb and vaporator outlt prssurs acting th diaphragm. Th ring is usd to nsur a positiv suprhat at th vaporator xit sinc th bulb prssur must b gratr than th vaporator xit prssur in ordr to ovrcom th forc of th ring. Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

7 99, Pag 6 As dpictd in Figur 5, a conical pin movs up and down to chang th opn ara for rfrigrant flow in rons to th valv control. Th mass flow rat through th TXV is assumd to b linar function of th opn ara as givn in quation 6. Aorific Apin mtxv m (6) A orific whr A orific = ((D orific ) π)/ is th ara at th full opning, A pin = ((D pin ) π)/ is closd ara associatd with th pin, and m is th rfrigrant mass flow rat associatd with a full opn condition. Figur 5: Diagram of TXV Th imum flow rat for a givn valv is a function of th prssur drop across th valv and th siz of th orific. Th imum flow rat for a givn orific is calculatd using th mpirical corrlation givn in quations 7 and 8, as dvlopd by Hmjak (1989). P P K C P P K m C A (7) 0 orific f c 1 3 SC C Pcri P K C C C5 (8) TCri Pcri whr th C s ar mpirical cofficints, ( P c -P ) is th diffrnc btwn th valv inlt prssur and th vaporating prssur, ρ f is th dnsity of th rfrigrant at th valv inlt, SC is th subcooling of th rfrigrant at th valv inlt, T cri and P cri ar th critical tmpratur and prssur. Th ring dflction, δ nds to known in ordr to find th ffctiv orific ara. Th dflction of th ring can b found using quation 9. F F, cl (9) k whr F is th ring forc, F,cl is th ring forc whn th valv is closd and k is th ring constant. Both F,cl and k ar fixd for a givn xpansion valv. F is calculatd from a quasi-static forc balanc on th diaphragm, as shown in quation 10. F diaph P P A P P A (10) b suc whr ( P b -P suc ) is th prssur diffrnc btwn bulb and suction lin, and A diaph is th ara of diaphragm. F,cl, A diaph and k ar constants basd on th valv dsign and initial stting. Sinc th ring forc is a linar function of th dflction, th ring dflction can b xprssd using mpirical cofficints a s, as shown in quation 11. diaph suc f c Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

8 99, Pag 7 Adiaph P Psuc F, cl a1p Psuc a (11) k If th pin dflction is zro, no rfrigrant flows through th orific, and if th pin dflction is at som imum valu, th pin will not obstruct th flow and th valv will oprat at th imum flow rat. Th ffctiv orific ara is calculatd by subtracting th obstructing ara of th pin from th ara of th valv orific. Th VRMF snsor for a TXV is dvlopd by substituting δ from quation 11 into quation 6 and xprssing th rsult in trms of nw mpirical cofficints that ar dtrmind through rgrssion. m TXV A orific A A orific pin m m C m a 3P Psuc a P Psuc a5 m (1) 5. Prformanc of VRMF snsor III for TXV Th mpirical cofficints C 1, C, C 3, C and C 5 within orific quations 7 and 8 wr stimatd by minimizing mass flow rat prdiction rrors using fully opn TXV tst data and non-linar rgrssion. Fully opn TXV tst data wr collctd from th conditions whr suprhat of th comprssor inlt was highr than th ratd suprhat. Th mpirical cofficints a 3, a, and a 5 within th TXV modl quation 1 wr stimatd basd on th availabl normal tst data with suprhat undr control using linar rgrssion. Th data includs variations in ambint tmpratur, and indoor dry bulb tmpratur with positiv subcooling ntring th valv. Sinc quation 8 uss subcooling as an input, zro subcooling data wr disrgardd for training and tsting. Th paramtr stimation mthods minimizd th rrors btwn prdictd and known mass flow rats. Th rsulting modl with mpirical cofficints dtrmind from normal data was applid to prdict rfrigrant mass flow rat for all of th availabl data including various fault conditions. Figur 6: Prformanc of VRMF snsor III basd on TXV for systm III undr no fault and fault conditions (RMS of snsor rrors shown for ach fault typ) Figur 7: Prformanc of VRMF snsor III basd on EEV for systm I undr no fault and fault conditions (RMS of snsor rrors shown for ach fault typ) Figur 6 shows rfrigrant mass flow rat stimatd from th VRMF snsor III for TXV applid to systm III with six diffrnt kinds of faults individually implmntd. Th ovrall RMS rrors wr about 1% for no fault conditions and 3% of actual mass flow rat for all fault conditions. Th prformanc of th VRMF snsor is vry good ovr a wid rang of rfrigrant mass flow rats and oprating conditions rgardlss of th fault. Thr wr som significant rrors of about 10% for low rfrigrant charg lvls whn th ntring subcooling was almost zro. With zro subcooling and two-phas conditions ntring th TXV, th VRMF snsor III may not b rliabl. Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

9 99, Pag Dvlopmnt of VRMF snsor III for EEV Elctronic xpansion valvs (EEV) wr dvlopd in th 1980s to provid tightr and mor stabl control of suprhat with fastr rons. Th applications of EEV for high fficincy air conditionr and multi-vaporator hat pump systms hav incrasd in rcnt yars. Howvr, mass flow modls of EEV for fault dtction and diagnosis ar vry limitd. In this study, th VRMF snsor basd on an mpirical corrlation can prdict rfrigrant mass flow rats through EEV. Th mpirical mass flow corrlation was dvlopd by incorporating a dimnsionlss cofficint in trms of EEV gomtris and oprating conditions into th orific quations 6 and 7 bcaus th only diffrnc btwn th EEV and TXV modl is how th ara opns and closs. Th mpirical corrlation for VRMF snsor is givn in quation 13. Th variation of th actual orific diamtr controls th rfrigrant flow ara for flow rstriction. Th mass flow rat proportionally incrass with th ris of th flow ara. C3 D acutal Pcri P SC meev Aactual m C1 f Pc P C C C 5 (13) TCri P cri whr th C s ar mpirical cofficints, D actual is actual orific diamtr (s Figur 8), ρ f is th dnsity of rfrigrant at th valv inlt, P c and P ar th inlt prssur and vaporator prssur. Figur 8 shows th flow passag structur and gomtric rprsntation for an EEV. A ndl valv movs up and down to chang th flow ara, typically using a stppr motor to maintain prcis control of th rfrigrant suprhat at th vaporator xit. At a crtain pin tip position h, th rfrigrant flow ara A actual can b calculatd by subtracting th obstructing ara of th ndl from th ara of th valv orific as dvlopd by Li (008) and givn in quation 1. A actual D actual D D D tan H h orific pin orific (1) whr D pin =( tanθ (H-h)) is th currnt ndl diamtr that is within th plan of th flow orific, and D orific = H tanθ is th orific diamtr. Th currnt ndl diamtr can thn b xprssd in trms of th orific diamtr and ndl position as shown in quation 15. D Dorific h H h Dorific (15) H H pin 1 Equations 1 and 15 can b combind to xprss th rfrigrant flow ara for any ndl position, A actual, as h h h h Aactual Dorific Dorific 1 Dorific (16) H H H H Th rfrigrant mass flow rat through th EEV can b obtaind by substituting th rfrigrant flow ara, quation 16, into th gnral modl quation 13. D orific h h m EEV C 1 f Pc P K (17) H H Th flow ara of th EEV varis with th up-and-down movmnt of th ndl valv that is drivn by a stp motor. Th ndl position (h) is linarly proportional to th motor stp of EEV, as givn in quation 18. EEVSTEP h EEVSTEP currnt H (18) Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

10 99, Pag 9 Figur 8: Flow passag structur and gomtric modls for EEV In this study, th VRMF snsor for an EEV was dvlopd by substituting th ratio of motor stp, quation 18, into th EEV rfrigrant mass flow rat quation 17. Th corrction cofficint in 19 can b dtrmind using linar rgrssion basd on normal tst data. EEVSTEP EEVSTEP D currnt currnt orific m EEV C C f Pc P K EEVSTEP 3 EEVSTEP (19) 5. Prformanc of th VRMF snsor III for EEV Th mpirical cofficints within orific quation 8 wr dtrmind using non-linar rgrssion applid to fully opn EEV data. Fully opn EEV data wr collctd from th conditions whr th motor stp was at a imum. Lik th TXV, quation 8 uss subcooling as in input, and thus zro subcooling data wr disrgardd for training and tsting. Onc th mpirical cofficints of orific quation ar obtaind, th EEV quation 19 was thn fit to normal oprating (i.., no-fault) data using linar rgrssion. Th bst fit quation was thn usd to prdict th rfrigrant mass flow rat through th EEV for all availabl tst data including various fault conditions. Figur 7 shows prformanc of th VRMF snsor III for EEV approach applid to systm I. Th modl provids rsults that ar gnrally within 6% ovr a wid rang of mass flow rats and oprating conditions. Largr rrors for low rfrigrant charg and condnsr fouling occurrd whn th subcooling at th condnsr outlt was blow F. Figurs 9 and 10 show prformanc of th VRMF snsor III for EEV applid to systm II with R-10A and R-0A as rfrigrant. Rsults ar prsntd for two diffrnt EEVs that wr tstd in this systm. Ovrall, th RMS rrors of th VRMF snsor III wr 6% and 5% for R-10A and R-0A, rctivly. Som of th largr rrors may b associatd with two-phas rfrigrant conditions at th EEV inlt with nar-zro subcooling. 6. Application of VRMF snsors for fault dtction and diagnosis Outputs from th thr VRMF snsors can b compard in ordr to dtct a fault and localiz faults within a systm, including: 1) loss of comprssor prformanc, ) faulty comprssor motor, and 3) faulty xpansion dvic. Figurs 11 to 1 dmonstrat th us of th VRMF snsors for isolating a fault condition whr th comprssor is not providing xpctd flow. Figur 11 shows comparisons of th thr VRMF snsors with mass flow masurmnts for systm III oprating at fixd d with a simulatd comprssor valv lakag fault. With this fault, th rfrigrant mass flow rat is rducd compard to normal opration. As a rsult, th comprssor map ovr-prdicts rfrigrant mass flow rat whras th othr VRMF snsors provid accurat flow stimats. Th RMS rrors for comprssor nrgy balanc Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

11 99, Pag 10 modl and TXV modls wr about %, whras th RMS rror for th fixd-d comprssor modl was 19 %. Thus, a comprssor flow fault could b isolatd through comparison of th VRMF snsors for this cas. Figur 1 similar rsults for systm I having a variabl-d comprssor and EEV. Th RMS rrors for th VRMF snsors wr about 5 % basd on a comprssor nrgy balanc and 3 % basd on th EEV modl, but wr approximatly 16 % for th variabl-d comprssor map. Figurs 13 and 1 show rsults for systm II with B1F and B0B as xpansion dvics and th two diffrnt rfrigrant typs, R-10A and R-0a. Th data did not includ information that could b usd to valuat th nrgy balanc mthod. Th tsts covrd a wid rang of comprssor fault lvls from 10 to 100%. For ithr st of tst data, a comprssor fault could b radily idntifid by comparing prdictions of th comprssor map with thos from th EEV modl. Figur 9: Prformanc of VRMF snsor III basd on EEV with R10a as rfrigrant for systm II Figur 10: Prformanc of VRMF snsor III basd on EEV with R10a as rfrigrant for systm II Figur 11: Comparison of VRMF snsor outputs for systm III with comprssor flow fault Figur 1: Comparison of VRMF snsor outputs for systm I with comprssor flow fault 7. CONCLUSIONS Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

12 99, Pag 11 Figur 13: Comparison of VRMF snsor outputs for systm II (R10A) with comprssor flow fault Figur 1: Comparison of VRMF snsor outputs for systm II (R0A) with comprssor flow fault Rfrigrant mass flow rat is an important masurmnt for quipmnt prformanc monitoring, fault dtction, and diagnostics. Howvr, a typical rfrigrant mass flow mtr is xpnsiv and installation for xisting fild quipmnt is complicatd bcaus it rquirs an quipmnt modification that can lad to rfrigrant lakag. To nabl low-cost implmntations for on-lin prformanc monitoring and automatd diagnostics, thr diffrnt virtual rfrigrant mass flow (VRMF) snsors wr dvlopd for stimating rfrigrant mass flow rat from lowcost masurmnts that ar basd on: 1) a comprssor map, ) a comprssor nrgy balanc, and 3) a smimpirical corrlation for th xpansion dvic (TXV or EEV). Th VRMF snsors prsntd in this papr wr validatd for systms having fixd and variabl-d comprssors, diffrnt rfrigrants, and diffrnt xpansion dvics (TXV/EXV) oprating ovr a wid rang of oprating conditions both with and without faults. Th thr VRMFs work wll in stimating th rfrigrant mass flow rat for th various systms undr fault-fr conditions with lss than a 5% RMS rror. Prdictions from th VRMF snsor basd on a comprssor map dviat from th othr VRMF snsors in th prsnc of a comprssor fault with th dviations growing with th magnitud of th fault. Ths diffrncs can b usd within a diagnostic systm to isolat this particular fault sinc th accuracy of th nrgy balanc modl and xpansion dvic modls ar indpndnt of comprssor flow faults. NOMENCLATURE A ara m Subscripts a, b, c Empirical constants actual Actual C d,v Corrction cofficint for EEV modl b Bulb C d,v,pi Corrction cofficint for PI thorm c Condnsr D Diamtr m cri Critical d Currnt ndl diamtr m diaph Diagram EEV Elctronic xpansion valv dis Discharg EEVSTEP Opning of EEV Stp Evaporator F Forc N dis Discharg f Comprssor d Hz f Liquid FDD Fault Dtction and Diagnostics g Gas H Maximum ndl position m Maximum Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

13 99, Pag 1 h Crtain ndl position m orific Orific h Enthalpy kj/kg Ratd Ratd condition k Spring constant N/m Spring m map m nrgy m TXV m EEV Rfrigrant mass flow rat basd on comprssor map Rfrigrant mass flow rat basd on comprssor nrgy balanc Rfrigrant mass flow rat basd on TXV modl Rfrigrant mass flow rat basd on EEV modl kg/s,cl Closd ring kg/s suc Suction kg/s TXV Thrmostatic valv xpansion P Prssur Pa Grk kg/s W Comprssor input Powr W ρ Dsnsity SC Subcooling C α loss Comprssor hat loss ratio TXV Thrmostatic valv xpansion δ Spring dflction T Tmpratur C Viscosity VRMF Virtual rfrigrant mass flow snsor θ Angl of pin REFERENCES ADM Associats, 009, Markt assssmnt and fild M&V study for comprhnsiv packagd A/C systms program, SCE086, July, 009. Amrican Rfrigration Institut (ARI), 1999, Positiv dilacmnt rfrigrant comprssors and comprssor units. Bach, C. 010, Prsonal communication, Ray W. Hrrick Laboratoris, Purdu Univrsity. Brodrick, J., 000, Ar fans blowing your nrgy budgt?, HPAC Hating/Piping/Air Conditioning Enginring, p Hrnjak, P.S., Lngr, M.J., and Jacobi, A.M., 1998, Suprhat stability of an vaporator and thrmostatic xpansion valv, air conditioning and rfrigration cntr., Univrsity of Illinois at Urbana-Champaign Katipamula, S. and Brambly, M.R., 005. Mthods for fault dtction, diagnostics, and prognostics for vapor comprssion quipmnt Systms, A Rviw, Part I, HVAR&R Rsarch, Vol. 11(1), p Kim, M. and Kim, M.S., 003, Prformanc invstigation of a variabl d vapor comprssion systm for fault dtction and diagnosis, Intrnational Journal of Rfrigrant, Vol. 8, p Kim, W.H and Braun, J.E., 01, Virtual rfrigrant mass flow and powr snsors for variabl-d comprssors, Intrnational Rfrigrant and Air conditioning Confrnc, No. 99. Li, H. and Braun, J.E., 008, A mthod for modling adjustabl throat-ara xpansion valvs using manufacturrs' rating data, HVAC&R Rsarch, Vol. 1(), p Mssngr, M., Stratgic Plan to Rduc th Enrgy Impact of Air Conditionrs, CEC , Jun, 008. Payn, W. V., Kim, M. S., Yoon, S. H., and Domanski, P. A., 008, Cooling mod fault dtction and diagnosis mthod for a rsidntial Hat Pump., NIST SP 1087; NIST Spcial Publication p.1087; 98 Park, C., Cho, H. and Kim, Y., 007, Mass flow charactristics and mpirical modling of R AND R10A flowing through lctronic xpansion valvs, Intrnational Journal of Rfrigration, Vol. 03, p Shanwi, M., Chuan, Z., Jiangping, C., and Zhiujiu, C., 005, Exprimntal rsarch on rfrigrant mass flow cofficint of lctronic xpansion valv, Applid Thrmal Eng., Vol. 5, p U.S. Dpartmnt of Enrgy, 010, Enrgy fficincy trnds in rsidntial and commrcial buildings, August, 010. ACKNOWLEDGEMENT This work was supportd by th Dpartmnt of Enrgy through th Enrgy Efficint Buildings Hub. Intrnational Rfrigration and Air Conditioning Confrnc at Purdu, July 16-19, 01

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

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

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

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot 5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg

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

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

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

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

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

Extraction of Doping Density Distributions from C-V Curves

Extraction of Doping Density Distributions from C-V Curves Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =

More information

Studies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO*

Studies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO* Studis of Turbulnc and Transport in Ohmic Plasmas with Phas Contrast Imaging and Comparisons with GYRO* L. Lin 1, M. Porkolab 1, E.M. Edlund 1, J.C. Rost 1, M. Grnwald 1, D.R. Mikklsn 2, N. Tsujii 1 1

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

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

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

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

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

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

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

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

CE 530 Molecular Simulation

CE 530 Molecular Simulation CE 53 Molcular Simulation Lctur 8 Fr-nrgy calculations David A. Kofk Dpartmnt of Chmical Enginring SUNY Buffalo kofk@ng.buffalo.du 2 Fr-Enrgy Calculations Uss of fr nrgy Phas quilibria Raction quilibria

More information

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt

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

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

Overcoming the shrink-and-swell effect in water level control strategy on industrial boiler-drum

Overcoming the shrink-and-swell effect in water level control strategy on industrial boiler-drum Standard Scintific Rsarch and Essays Vol1 (1): 019-024, Fbruary 2013 http://www.standrsjournals.org/journals/ssre Rsarch Articl Ovrcoming th shrink-and-swll ffct in watr lvl control stratgy on industrial

More information

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005.

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005. Intrnational Linar Collidr Machin Dtctor Intrfac Workshop: ILCSLAC, January 68, 2005. Prsntd by Brtt Parkr, BNLSMD Mssag: Tools ar now availabl to optimiz IR layout with compact suprconducting quadrupols

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

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

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

EFFECT OF BALL PROPERTIES ON THE BALL-BAT COEFFICIENT OF RESTITUTION

EFFECT OF BALL PROPERTIES ON THE BALL-BAT COEFFICIENT OF RESTITUTION EFFECT OF BALL PROPERTIES ON THE BALL-BAT COEFFICIENT OF RESTITUTION A. M. NATHAN 1 AND L. V. SMITH 2 1 Univrsity of Illinois, 1110 W. Grn Strt, Urbana, IL 61801, USA, E-mail: a-nathan@illinois.du 2 Washington

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

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

Observer Bias and Reliability By Xunchi Pu

Observer Bias and Reliability By Xunchi Pu Obsrvr Bias and Rliability By Xunchi Pu Introduction Clarly all masurmnts or obsrvations nd to b mad as accuratly as possibl and invstigators nd to pay carful attntion to chcking th rliability of thir

More information

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-interaction mass formula that relates all leptons and quarks to the electron Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris

More information

Aalborg Universitet. Non-linear and adaptive control of a refrigeration system Rasmussen, Henrik; Larsen, Lars F. S.

Aalborg Universitet. Non-linear and adaptive control of a refrigeration system Rasmussen, Henrik; Larsen, Lars F. S. Aalborg Univrsitt Non-linar and adaptiv control of a rfrigration systm Rasmussn, Hnrik; Larsn, Lars F. S. Publishd in: IET Control Thory & Applications DOI (link to publication from Publishr):.9/it-cta.9.56

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

MODELING OF COMPONENTS IN ABSORPTION REFRIGERATION SYSTEMS DURING TRANSIENT OPERATION

MODELING OF COMPONENTS IN ABSORPTION REFRIGERATION SYSTEMS DURING TRANSIENT OPERATION MODELING OF COMPONENTS IN ABSORPTION REFRIGERATION SYSTEMS DURING TRANSIENT OPERATION A. Nouri-Borujrdi, A. Mirzai Islamic Azad Univrsity, South Thran Branch Jamal-Zadh Strt, Thrah, Iran Tl: +98 1 66165547,

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

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

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Differentiation of Exponential Functions

Differentiation of Exponential Functions Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of

More information

Statistical Thermodynamics: Sublimation of Solid Iodine

Statistical Thermodynamics: Sublimation of Solid Iodine c:374-7-ivap-statmch.docx mar7 Statistical Thrmodynamics: Sublimation of Solid Iodin Chm 374 For March 3, 7 Prof. Patrik Callis Purpos:. To rviw basic fundamntals idas of Statistical Mchanics as applid

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

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

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

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

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

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

Learning Spherical Convolution for Fast Features from 360 Imagery

Learning Spherical Convolution for Fast Features from 360 Imagery Larning Sphrical Convolution for Fast Faturs from 36 Imagry Anonymous Author(s) 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 3 3 33 34 35 In this fil w provid additional dtails to supplmnt th main papr

More information

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

More information

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes Articl Intrnational Journal of Modrn Mathmatical Scincs 014 11(1): 40-48 Intrnational Journal of Modrn Mathmatical Scincs Journal hompag:www.modrnscintificprss.com/journals/ijmms.aspx ISSN:166-86X Florida

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

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

Characteristics of Gliding Arc Discharge Plasma

Characteristics of Gliding Arc Discharge Plasma Caractristics of Gliding Arc Discarg Plasma Lin Li( ), Wu Bin(, Yang Ci(, Wu Cngkang ( Institut of Mcanics, Cins Acadmy of Scincs, Bijing 8, Cina E-mail: linli@imc.ac.cn Abstract A gliding arc discarg

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

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

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

0 +1e Radionuclides - can spontaneously emit particles and radiation which can be expressed by a nuclear equation.

0 +1e Radionuclides - can spontaneously emit particles and radiation which can be expressed by a nuclear equation. Radioactivity Radionuclids - can spontanously mit particls and radiation which can b xprssd by a nuclar quation. Spontanous Emission: Mass and charg ar consrvd. 4 2α -β Alpha mission Bta mission 238 92U

More information

Applied Statistics II - Categorical Data Analysis Data analysis using Genstat - Exercise 2 Logistic regression

Applied Statistics II - Categorical Data Analysis Data analysis using Genstat - Exercise 2 Logistic regression Applid Statistics II - Catgorical Data Analysis Data analysis using Gnstat - Exrcis 2 Logistic rgrssion Analysis 2. Logistic rgrssion for a 2 x k tabl. Th tabl blow shows th numbr of aphids aliv and dad

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

Computational Hydrodynamics and Control Modeling for Autonomous Underwater Vehicles

Computational Hydrodynamics and Control Modeling for Autonomous Underwater Vehicles Computational Hydrodynamics and Control Modling for Autonomous Undratr Vhicls David L. Bradly Th Pnnsylvania Stat Univrsity Applid Rsarch Laboratory P.O. Box 30, Stat Collg, PA 16804-0030 Phon: 814-863-9916

More information

EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS

EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS Octobr 12-17, 28, Bijing, China EFFECT OF CONSOLIDATION RATIOS ON MAXIMUM DYNAMIC SHEAR MODULUS OF SANDS Xiaoming YUAN 1 Jing SUN 2 and Rui SUN 3 1 Profssor, Dpt. of otchnical Enginring, Institut of Enginring

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

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

INVESTIGATION OF UPSTREAM LENGTH REQUIREMENTS FOR VENTURI TUBE INSTALLATION USING CFD 1 A.Tukimin, 2 M.Zuber, 2 K.A.Ahmad, 2 S.

INVESTIGATION OF UPSTREAM LENGTH REQUIREMENTS FOR VENTURI TUBE INSTALLATION USING CFD 1 A.Tukimin, 2 M.Zuber, 2 K.A.Ahmad, 2 S. Sci.Int.(Lahor),9(5),5-,07 ISSN 0-56;CODEN: SINTE 8 5 INVESTIGATION OF UPSTREAM LENGTH REQUIREMENTS FOR VENTURI TUBE INSTALLATION USING CFD A.Tukimin, M.Zubr, K.A.Ahmad, S.Saadon Dpartmnt of Mchanical

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

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

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

4037 ADDITIONAL MATHEMATICS

4037 ADDITIONAL MATHEMATICS CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Ordinary Lvl MARK SCHEME for th Octobr/Novmbr 0 sris 40 ADDITIONAL MATHEMATICS 40/ Papr, maimum raw mark 80 This mark schm is publishd as an aid to tachrs and candidats,

More information

Inference Methods for Stochastic Volatility Models

Inference Methods for Stochastic Volatility Models Intrnational Mathmatical Forum, Vol 8, 03, no 8, 369-375 Infrnc Mthods for Stochastic Volatility Modls Maddalna Cavicchioli Cá Foscari Univrsity of Vnic Advancd School of Economics Cannargio 3, Vnic, Italy

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-Classical States of the Simple Harmonic Oscillator Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats

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

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems Daling with quantitati data and problm soling lif is a story problm! A larg portion of scinc inols quantitati data that has both alu and units. Units can sa your butt! Nd handl on mtric prfixs Dimnsional

More information

Robust surface-consistent residual statics and phase correction part 2

Robust surface-consistent residual statics and phase correction part 2 Robust surfac-consistnt rsidual statics and phas corrction part 2 Ptr Cary*, Nirupama Nagarajappa Arcis Sismic Solutions, A TGS Company, Calgary, Albrta, Canada. Summary In land AVO procssing, nar-surfac

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

SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS

SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS Hirokazu Tahara, Takashi Fujioka, Atsushi Shirasakiand Takao Yoshikawa Graduat School of Enginring Scinc, Osaka Univrsity 1-3, Machikanyama,

More information

Solution of Assignment #2

Solution of Assignment #2 olution of Assignmnt #2 Instructor: Alirza imchi Qustion #: For simplicity, assum that th distribution function of T is continuous. Th distribution function of R is: F R ( r = P( R r = P( log ( T r = P(log

More information

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a

More information

Atomic and Laser Spectroscopy

Atomic and Laser Spectroscopy L-E B, OL, MOV 83 Atomic and Lasr Spctroscopy Th aim of this xrcis is to giv an ovrviw of th fild of lasr spctroscopy and to show modrn spctroscopic mthods usd in atomic, molcular and chmical physics.

More information

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker Evaluating Rliability Systms by Using Wibull & Nw Wibull Extnsion Distributions Mushtak A.K. Shikr مشتاق عبذ الغني شخير Univrsity of Babylon, Collg of Education (Ibn Hayan), Dpt. of Mathmatics Abstract

More information

CHAPTER 16 HW: CONJUGATED SYSTEMS

CHAPTER 16 HW: CONJUGATED SYSTEMS APTER 6 W: JUGATED SYSTEMS NAMING PLYENES. Giv th IUPA nam for ach compound, including cis/trans or E/Z dsignations whr ndd. ompound no E/Z trans or E 2 3 4 3 Nam trans-2-mthyl-2,4-hxadin 2-mthoxy-,3-cyclohptadin

More information

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case wwwnvisol-canadaca Sara Godoy dl Olmo Calculation of contaminatd soil volums : Gostatistics applid to a hydrocarbons spill Lac Mgantic Cas Gostatistics: study of a PH contamination CONTEXT OF THE STUDY

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

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

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

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

Sundials and Linear Algebra

Sundials and Linear Algebra Sundials and Linar Algbra M. Scot Swan July 2, 25 Most txts on crating sundials ar dirctd towards thos who ar solly intrstd in making and using sundials and usually assums minimal mathmatical background.

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

Review Statistics review 14: Logistic regression Viv Bewick 1, Liz Cheek 1 and Jonathan Ball 2

Review Statistics review 14: Logistic regression Viv Bewick 1, Liz Cheek 1 and Jonathan Ball 2 Critical Car Fbruary 2005 Vol 9 No 1 Bwick t al. Rviw Statistics rviw 14: Logistic rgrssion Viv Bwick 1, Liz Chk 1 and Jonathan Ball 2 1 Snior Lcturr, School of Computing, Mathmatical and Information Scincs,

More information

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by: Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any

More information

4 x 4, and. where x is Town Square

4 x 4, and. where x is Town Square Accumulation and Population Dnsity E. A city locatd along a straight highway has a population whos dnsity can b approimatd by th function p 5 4 th distanc from th town squar, masurd in mils, whr 4 4, and

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

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

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

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

3-2-1 ANN Architecture

3-2-1 ANN Architecture ARTIFICIAL NEURAL NETWORKS (ANNs) Profssor Tom Fomby Dpartmnt of Economics Soutrn Mtodist Univrsity Marc 008 Artificial Nural Ntworks (raftr ANNs) can b usd for itr prdiction or classification problms.

More information

Massachusetts Institute of Technology Department of Mechanical Engineering

Massachusetts Institute of Technology Department of Mechanical Engineering Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our

More information

AS 5850 Finite Element Analysis

AS 5850 Finite Element Analysis AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form

More information