STUDY ON EFFECTIVE USE OF AN ICE THERMAL STORAGE SYSTEM WITH SIMULATION. Mingjie Zheng 1. Nagoya, Aichi, , Japan

Size: px
Start display at page:

Download "STUDY ON EFFECTIVE USE OF AN ICE THERMAL STORAGE SYSTEM WITH SIMULATION. Mingjie Zheng 1. Nagoya, Aichi, , Japan"

Transcription

1 Prceedngs f Buldng Smulatn 2011: STUDY O EFFECTIVE USE OF A ICE THERMAL STORAGE SYSTEM WITH SIMULATIO Mngje Zheng 1 1 Technlgy Dvsn, SAKO Ar Cndtnng CO., LTD. agya, Ach, , Japan ABSTRACT It s mprtant t evaluate hether an thermal strage system can perate effectvely as the ay planned at the desgn stage. Whle desgnng an thermal strage system, generally, the thermal strage tme s calculated y usng rated capacty f refrgeratr r the heat exchange capacty f -n-cl, and the heatng capacty tme s calculated y usng the average meltng alty f the thermal strage tank. In ths paper, the authr develps a smulatn prgram fr mult-cnnected cmplete-lendng thermal strage tank and dscusses the effectve usalty f a practcal assemled strage system y usng the prgram. ITRODUCTIO The smulatn mdel f the external meltng Ice-n-cl type f thermal strage system can e dvded nt drect and ndrect smulatn. In drect smulatn, the -n-cl s mdeled as a cmpnent f evapratr. In ndrect smulatn, the thermal strage tank can e mdeled as a cmpnent f a heat exchanger. A drect thermal strage smulatn mdel that cntans a detaled mdel fr heat transfer frm the thermal strage tank t the refrgerant as develped (Jacsn, 1986) y usng a quas-steady thermal resstance netrk heat transfer mdel. Cleman (1990) extended the rk f Jacsn y develpng a mre cmplete mdel usng the thermal resstance netrk technque appled t the entre cl. Slver et al. (1988) develped anther mdel usng the thermal resstance netrk technque. Hever, Slver et al. dvded the cls n a fnte numer f segments. Generally, the refrgeratn capacty and heat exchange amunt f evapratr change dependng n the thckness and the evapratng temperature. In the Jacsn R's mdel, the evapratr capacty s set equal t the rated cmpressr capacty, s t can nt exactly reprduce the dynamc perfrmance f the -n-cl thermal strage system. The prlem th the mdel s n the asence f nfrmatn such as the tue length, s users must estmate the tank specfcatns, hch destrys the accuracy f the detaled mdel. In addtn, the executn tme f the detaled mdel s unfavraly lng fr an annual smulatn, hch means pr applcalty t a real -n-cl thermal strage system. A dynamc -n-cl evapratr mdel as develped as a stand-alne smulatn prgram cnsderng the heat transfer and pressure drp crrelatns avalalty (Mltz, 1987). In ths mdel, ased n the heat alance f the layer n the length f the tue n the steady state, t calculate amunt f the makng and meltng. Calculatn f the evapratn amunt ncludes the effects f the refrgerant superheat, changes f the evapratng pressure and thckness. Jnes and Shddapur (1995) appled and mprved Mltz s drect -n-cl evapratr mdel t an ndrect -n-ppe cmpnents mdel and develped an ndrect thermal strage system smulatn prgram y usng a fnte dfference apprach. The results ndcated that the mdel lacks sme accuracy, manly durng the egnnng f the chargng perd as ell as durng the meltng perd. A smulatn mdel f a temperature stratfcatn thermal strage tank as develped (u, 1984) ased n the expermental results f an ndrect thermal strage tank th a fnte dfference apprach. In ths smulatn mdel, the capacty f the chller as mdfed y the rne temperature that changes due t the change f the ater temperature and the heat alance eteen the amunt f the heat transfer thrugh the cl and chller utput. Mngje et. al (2001) mdfed akahara's mdel, and ncrprated t nt HVACSIM + (J). Mtsh et. al. (1986) develped anther smulatn mdel f ndrect thermal strage tank. In ths mdel, althugh the changes f the external heat transfer ceffcent f the cl alng the tue length drectn as taken nt accunt, the capacty f the chller as nt mdfed. Hever, these smulatn mdel shn ave, except fr u s mdel hen gven certan parameters as nputs, can nt smulate an actually assemled mult-cnnected cmplete-lendng thermal strage tank. Therefre, In ths paper, takng nt accunt the effect f the thckness n the makng and meltng alty, and the chller COP varatn due t the changes f the nlet and utlet rne temperature, the authr develps a smulatn

2 Prceedngs f Buldng Smulatn 2011: prgram fr mult-cnnected cmplete-lendng thermal strage tank and dscusses the effectve usalty f a practcal strage system y usng the prgram. OUTLIES OF BUILDIGS AD ICE THERMAL STORAGE SYSTEM The utlnes f target uldngs and thermal strage system are sh n Tale 1. And the utlne f target heat surce system and the Ice-n-cl placement s sh n Fgure 1. The target thermal strage system cnssts f t rne heat pumps and eleven -n-cls. In addtn, ecause each -n-cl cnssts f 17 parallel clumns f hrzntal tue and each clumn f tue s cnnected t the heat pump chllers va the vertcal headers (See Fgure 2), almst n temperature dfference exsts fr vertcal drectn n each tank durng the makng, s the target thermal strage tanks can e assumed f eng a mult-cnnected cmpletelendng thermal strage tank. Fgure 2 The structure f target -n-cl Tale 1 The utlnes f the target uldngs and thermal strage system Structure Buldn gs Heat surce system Renfrced cncrete made Usage Research faclty Ttal flr area 9,734m2 Brne heat pump 100 Hp 2 chller Strage capacty 440kW Brne temperature -7 C -3 C range Chlled capacty 560kW Chlled ater temperature range 7 C 12 C Dmensn f a tank Maxmum vlume umer f -n-cl Ice thermal strage tanks Avalale ater vlume 208.9m3 Materal and cncentratn Ethylene glycl f rne 60% Materal f rne, ttal Cpper, m length, nsde and utsde 16mm, 19.05mm dameter f tue Water temperature range f 5 C 2 C strage tank Chlled ater fl vlume m3/h Fgure 1 Outlne f heat surce system and -n-cl placement m2 3.5m (H) 30.1m3 4.7m3 9,3.1m3 2

3 Prceedngs f Buldng Smulatn 2011: CALCULATIO OF CAPACITY AD TIME OF THERMAL STORAGE When desgnng an thermal strage system, generally, the thermal strage tme s calculated y the use f rated capacty f refrgeratng machne r the heat exchange capacty f -n-cl, respectvely. Smple Calculatn Methd f Thermal Strage Tme Assumng the alty f heat strage equals t the rated capacty f the chller durng the thermal strage peratn, the sensle and latent heat strage tme can e calculated as fllng. The calculated results are shn n Tale 2. hk M C Tm / HP (1) h M C HP (2) s, max / Where, t as assumed that the rne temperature f utlet and nlet f chller are ther desgn values, and the heat exchanger temperature dfference s the average temperature dfference eteen the rne and ater temperature. Frm Tale 2, t can e understd that the ttal thermal strage tme s 9.2 hurs, less than the 10 hrs f nghttme duty eteen 22:00 and 8:00 f the cheaper electrcty rate schedule set fr the peak shft peratn frm the daytme. Apprxmatn Methd f Thermal Strage Tme On the ther hand, hen the -n-cl strage system s n actual peratn, the thermal strage capacty perates apart frm the rated capacty f the chller, ut s lmted t heat exchange capacty f cl. Mrever, the heat exchange capacty f -n-cl s decreasng th ncrease f thckness. In an apprxmatn methd, th an assumptn that the rate f sensle heat exchange n -n-cl prprtns t the average temperature dfference eteen the rne and ater, and frmatn s n prprtn t the latent heat exchange rate as ell, h s and h k are calculated y usng Equatn (3) and (4) respectvely. The calculatn results are als shn n Tale 2. hk M C Tm / KLT m Tm (3) h M C / KLT 0 (4) s, max m In Equatn (4), t s assumed that the heat exchange rate f -n-cl equals t the ne hen the vlume s a half f the desgned maxmum vlume. Frm Tale 2, t s shn that the ttal thermal strage tme s 15.5 hurs that s 1.7 tmes f the result th a smple calculatn methd, hch shs a g dfference eteen the t methds. Thermal Strage Tme Smulatn th the Present Tl T methds descred ave d nt accurately calculate changes f the ver-all heat transfer amunt f -n-cl due t the change f thckness. Therefre, t calculate the thermal strage tme mre accurately, a smulatn prgram that takes nt accunt the changes f the thckness and the rne chller COP changes due t the changes f the rne temperature that nfluence the makng capacty f the thermal strage system. Assumptns n the thermal strage smulatn (a) The ater temperature n the tank s n a fully mxed state and s 5 degree C n the egnnng f thermal strage. () The ater temperature n the tank s 0 degree C hen the egns t prduce. (c) The ler lmt f the rne temperature n the chller utlet s -10 degree C. (d) The chlled ater temperature n the tank nlet s cnstant. Heat transfer n the nsde and utsde surface f the tue As the nsde surface f the tue s n the frced cnvectn state, the heat transfer ceffcent can e taned y Equatn (5) r Equatn (6) (SHASEJ, 1995) Pr Re Re 2100 (5) 2 r 2r Pr Re l Re 2100 (6) r 2 / 3 2r (Pr ) Re l As the utsde surface f the tue s n the natural cnvectn, heat transfer ceffcent can e taned y Equatn (7) (SHASEJ, 1995) Gr 10 4 Gr Pr 10 8 (7) 2 r Smulatn f thermal strage capacty a) The ver-all heat transfer rate f the cl (Q c ) Q c 2Lc KT g (8) Where, T g s the lgarthmc mean temperature dfference and can e calculated y Equatn (9). T, c T, c Tg (9) ln[( T T, c ) /( T T, c )] K s the ver-all heat transfer ceffcent f tue, and can e calculated y Equatn (10) r 1 ln (10) K r cl r r ) The rne temperature at the cl utlet (T,c ) T, c T, c c Q / C F (11) c) The capacty f the chller s mdfed usng a theretcal COP frmula (akahara, 1984). ' ' ' T 273 T Tcd T T HP HP ' ' (12) T 273 T Tcd T T d) When the capacty f the chller (HP ) s larger than the ver-all heat transfer amunt f the cl (Q c ),

4 Prceedngs f Buldng Smulatn 2011: revse the rne temperature n the chller nlet (T ) t dnard untl the T equals t ts ler lmt value. And hen HP s smaller than Q c, adjust T t upard. e) The ater temperature n the tank s represented th dfferental Equatn (13). 1 dt Lc K Tg dt (13) M C f) When the ater temperature n the tank reaches 0 degree C, frmatn egns. The vlume s represented th dfferental Equatn (14). 2 K T g L c dm dt (14) C Hever, at the mment f the phase change frm ater t at the uter surface f the -n-cl, the heat transfer ceffcent ecmes almst nfnte, s that the calculatn f the thermal transmttance n the -n-cl (K ) ll ecme as Equatn (15). 1 K 1 1 r cl r 1 ln r r D ln r (15) The calculatn f thermal strage tme a) The sensle heat changes f ater n the tank (Q) can e calculated y Equatn (16) Q C M dt (16) ) The sensle heat strage tme As the ver-all sensle heat transfer amunt f the cl equals t the varatn f sensle heat f ater n the tank, lnkng Equatn (8) and (16), and then ntegratng Equatn (17) frm ntal ater temperature n the tank t 0 degree C, the sensle heat strage tme (h k ) can e taned as Equatn (17). 0 C M (17) h k T 2 L c KT g dt c) The Latent heat strage tme When the tank ater temperature ecmng 0 degree C, the latent heat strage amunt equals t the latent heat rate fr makng, and t can e taned y ntegratng Equatn (14) up t desgned maxmze vlume, as shn n equatn (18). Smulatn results f the sensle and latent heat strage tme are als shn n Tale 2. h s M, max 0 C 2 L dm (18) c K T g Smulatn fl Because the capacty f the chller (HP ) depends n the rne temperature n the chller nlet, t s needed (a) t mdfy the capacty f the chller th Start Intalzatn f T, T cd, T Calculate HP Calculate, 0,K h s =h s + t Calculate T,Q c Upard T HP = Q c? Y HP Q c? Y T -10 C? h k = h k + t Y Calculate T, M Dnard T T = 0 C? Y M = M,max? Y Output h k, h s End Fgure 3 A fl chart f the smulatn

5 Prceedngs f Buldng Smulatn 2011: the rne temperature n the chller nlet at frst tme; () t calculate, 0, K, T and M th the average temperature f the rne and t calculate Q c and T y usng them; (c) t mdfy T y cmparng HP th Q c and t repeat calculatns untl HP ecmes equal t Q c ; (d) The smulatn shall e carred ut untl that the desgned maxmum vlume s attaned, and then h k and h s s taned. Fgure 3 shs the fl f smulatn. Cmparng Results f Three Calculatn Methds Fgure 4 and 5 sh the amunt f sensle and latent heat strage n target thermal strage system and the rne temperature f the nlet and utlet n the chller, respectvely. Frm Fgure 4, 5 and Tale 2, the fllng fndngs are taned. a) Fllng the ncrease f the thckness, the amunt f the thermal strage decreases. ) The makng tme smulated s lnger than that calculated y the smple methd, and s less than that calculated y the apprxmatn methd. The dfferences amng three methds can e explaned as flls. (a) Increase f the thermal resstance accrdng the thckness t e cnsdered n smulatn. () The average rne temperature as used n an apprxmatn methd. (c) The rne temperature n the chller utlet as adjusted dnard as the capacty f the chller t maxmze value n smulatn. c) After egnnng t make, the rne temperature n the chller utlet arrved at the lest lmt value, -10 degree C, and ths ndcates that ttal uter surface f cl n ject thermal strage system s t small. d) Accrdng t the smulatn result, the thermal strage tme f ject thermal strage system s 12.9 hurs. If just 10 hurs f nghttme peratn s desred fr strage peratn, nsuffcent cl surface area s the cause f t. Hever, ths ll e allale cnsderng that ths nsuffcency nly ccurs at a fe days f peak clng seasn n summer. Tale 2 Cmparng calculatn results f thermal strage tme (h) f three methds Methd Sensle heat strage tme Latent heat strage tme Ttal tme Smplfy Apprxmate Develped tl Fgure 4 The amunt f sensle and latent nlet f the chller CALCULATIO OF CAPACITY AD TIME REQUIRED FOR HEAT DISSIPATIO Apprxmatn Methd f Clng Capacty Tme The clng capacty s reduced accrdng t reductn f surface area. The apprxmatn methd used y the desgner assumed that there s a lnear relatnshp eteen the clng capacty and the resdual vlume, and calculated the clng capacty tme usng a half f the desgned maxmum vlume. The calculatn methds and results are shn n Tale 3. The meltng tme s 5.23 hurs, and there s suffcent meltng alty n the ject thermal strage system. Hever, ths methd can nt reprduce the effects f nn-lnear changes f the vlume durng the meltng. Fgure 5 The rne temperature f utlet and heat strage Smulatn fr Alty and Tme f the Ice Meltng Assumptns f the meltng smulatn a) The target thermal strage tank cnssts f eleven cl unts and fur tanks, and all -n-cl s nt placed n seres alng the ater fl drectn. Therefre, fur tanks ere changed t nne tanks n the smulatn, as ndcated y thn dashed lnes n Fgure 1. ) The ater temperature n each tank s n a fully mxed state and s 0 degree C hen egnnng t melt. c) The temperature and fl rate f the returnng chlled ater frm the secndary sde equal t the desgn values, 5 degree C and m 3 /h, respectvely. d) The vlume equals t the desgned maxmum vlume, and s evenly dstruted n each cl

6 Prceedngs f Buldng Smulatn 2011: Tale 3 The calculatn frmula and results f apprxmatn methd Sgn Unt Interpretatn Calculatn methds Results M m 3 /m Ice vlume f unt cl length hen the vlume 3.8E-3 M 1/ 2M, max / L s 1/2 f the desgned maxmum vlume d,m m Dameter f uter surface f the hen the d M d 1/ vlume s 1/2 f the desgned maxmum vlume 2, m 4 / A xm m 2 Outer surface area f hen the vlume s 1/2 f the desgned maxmum vlume T gm C Lgarthmc mean temperature dfference A T d xm, m gm L T T Ln( T ) Ln( T ) Q MJ Mean alty f the meltng Q T A ( 180) 1,773 Q s MJ Latent heatng capacty Qs M C 9,274 Q k MJ Sensle heatng capacty Qk M C Tgm 2,868 h h Ice meltng tme h M C / Q 5.23 ater temperature f the last tank, frm hch the The meltng smulatn mdel chlled ater s suppled t the clng crcut, If a large numer f tues are arranged n parallel t gradually rses. Therefre, t s cnsdered that the each cls, the cnvectve heat transfer ceffcent smulated sensle heatng capacty s larger than the f the uter surface f the s calculated y ne th an apprxmatn methd. Equatn (19) (SHASEJ, 1995). Fgure 7 shs the varatn f resdual vlume n hn Pr Re each tank durng the meltng prcess. After fur 0 (19) hurs f clng peratn, n s fund n the tank d 1 and 2; ut the tank 8 and 9 mantan the untl the last mment as shn. The varatn f the sensle, latent and ttal clng capacty durng the meltng are shn n Fgure 8-Fgure 10, respectvely. Frm these fgures, the fllng fndngs are taned: a) The clng capacty f each tank s dfferent ecause the length f the tue f -n-cl n each tank s als dfferent. ) Because the ntal ater temperature n the tank s 0 degree C, there s the sensle clng capacty durng all the meltng perd. c) The meltng tme s 9 hurs, lnger than that calculated y the apprxmatn methd. Heat alance f ttal clng capacty f each thermal strage tank durng the meltng s represented y the dfferental Equatn (20) dt ( 1 IPF) VC FC T n T Ax T 0(20) dt Dfferencng and srt ut Equatn (20), Equatn (21) s taned and temperature f each tank can e calculated. 1 1 T {(1 IPF ) VT FTnt}/ B IPF 0 (21) 1 T { VmT FTnt}/ A IPF 0 Where, 1 A x B (1 IPF ) V ( F ) t, A V F t (22) c IPF s a percentage f the vlume n the tank, and s calculated y Equatn (23). IPF r D r (23) r The amunt f meltng n each tank s represented y the dfferental Equatn (24). dm A x T 0 (24) dt C The meltng tme can e taned y ntegratng Equatn (24) frm the desgned maxmum vlume t 0 as shn n Equatn (25). h 0 M,max C dm A ( T 0) x (25) The meltng smulatn results and dscussn Smulatn n the step respnse f 5 degrees C ater temperature nput as executed and Fgure 6 shs the temperature prfles f the ject thermal strage tanks durng the meltng prcess. The gm xm Fgure 6 Temperature prfle n tanks Fgure 7 Changes f vlume n each tank

7 Prceedngs f Buldng Smulatn 2011: Fgure 8 Changes f latent heatng capacty n each tank Fgure 9 Changes f Sensle heatng capacty n each tank Fgure 10 Changes f ttal heatng capacty Cmparsn eteen the Results f T Calculatn Methds Cmparsn eteen the results f t calculatn methds s shn n Tale 4. The result f ther latent heatng capacty s same; hever, the meltng tme taned y each calculatn methd s dfferent. Ths s ecause the average rates f the meltng eteen the t calculate methds are dfferent. The result f the sensle clng capacty th smulatn s greater than that y the apprxmatn methd. The dfference appeared n the ater temperature n the tank utlet, n hch t rased up t 5 degree C fr the smulatn methd, ut t keeps 2 degree C, the desgned value, fr the apprxmatn methd. When a real thermal strage system perates n a cndtn f the meltng, the altes f the meltng vary alng th changes f the resdual vlume and the ater temperature n tank utlet. Fr ths reasn, t s cnsdered that the smulatn results are mre accurate than the ne y usng an apprxmatn methd. DISCUSSIO In ths paper, takng nt accunt the effect f the thckness n the makng and meltng alty, and the chller COP varatn due t the changes f the nlet and utlet rne temperature, the authr develped a smulatn prgram fr an assemled mult-cnnected cmplete-lendng thermal strage tank and dscussed the effectve usalty f a practcal strage system y usng the prgram. The fllng results ere taned. 1) Because the calculated capacty strage alty f the target thermal strage tank s smaller than the rated capacty f the chller, the smulatn value f the thermal strage tme s lnger than that y a smplfy calculatn, and shrter than that usng the average verall heat transfer ceffcent f the -n-cl. Ths shs that the smulatn prgram reprduces the ncrease f the verall thermal resstance f the cl, due t freezng n the uter surface f the cl, and the actual chller capacty changes and rks n the cndtns dfferent frm the rated. 2) In the smulatn f the clng capacty durng the daytme, the smulatn reprduces the changes f the meltng alty due t changes f the ater temperature and resdual n each thermal strage tank. The smulatn value f the meltng tme s lnger than that calculated y an apprxmatn methd th the average meltng alty f the -n-cl, the frmer f hch taned a value that s clse t the actual ne. Mrever, hen a real thermal strage system perates n a cndtn f the meltng, returned chlled ater temperature frm the secndary sde vares dependng n changes f the clng lad. Hever, accrdng t the smulatn descred n ths paper, 5 degree, the desgned value f the chlled ater, as appled. Therefre, t s cnsdered there s a small dfference eteen the smulatn value f the meltng tme and actual value. Tale 4 Cmparsn f the Results eteen T Calculatn Methds Methds Average altes Latent heatng Sensle Ttal heatng The f the capacty heatng capacty meltng tme meltng [MJ] [MJ] capacty [MJ] [MJ] [h] Apprxmatn 1,773 9,274 2,868 12, Develped tl 1,070 9,274 4,079 13,

8 Prceedngs f Buldng Smulatn 2011: REFERECES Cleman G Smulatn f Ice Strage Systems. M.S. thess, Unversty f Illns at Urana-Champagn, Urana. Jacsn D. I Smulatn and Optmzatn f the Operatn f an Ice Strage System. M.S. thess, Unversty f Illns at Urana- Champagn, Urana. Jnes J.W. and Shddapur G. S Evaluatn f RP-495 Algrthms fr Mdelng External Met, Ice-n-ppe Thermal Strage System Cmpnents, ASHRAE Transactns, Vl. 101(2), pp Mltz, A A umercal Mdel f an Ice Strage Tank Evapratr, M.S. Thess, Department f Mechancal Engneerng, Unversty f Texas at Austn. Mngje Zheng, Techuj Yasutm and u akahara Dynamc Smulatn f HVAC th the Heat Strage System y Usng HVACSIM +, Part 1 A smulatn mdel f the strage tank f the temperature-stratfed type, SHASE Transactns (2001.9), pp , Kyt, (In Japanese). Mtsh Myamae, T. Iamt, T. Sagara, T. Ara,. Takeda and M. Ichn Study n Ar Cndtnng System ased n Ice Energy Strage fr Large Buldngs, Part 10 Mdel valdatn n the meltng and estmatn f varus parameters, SHASE Transactns ( ), pp , (In Japanese). u akahara Study n the Predctn f Characterstcs f Ice Strage Tank, Part 1 - Study n perfrmance evaluatn system, SHASE Transactns ( ), pp , (In Japanese). SHASEJ Ar Cndtnng and Santary Engneerng Handk, The 12 th Edtn, Maruzen, Tky, (In Japanese). Slver S.C., Mltz A., Jnes J.W., Petersn J.L. and Hunn B.D Cmpnent Mdels fr Cmputer Smulatn f Ice Strage Systems, ASHRAE Transactns, Vl. 95(1), pp Zehnder J.W Cmputerzed Mdel f an Ice Thermal Strage System. M.E. thess, Department f Mechancal Engneerng, Unversty f Lusvlle, Lusvlle, KY. menclature A x Outer surface area f [m 2 ] C Specfc heat f rne [kj/kg] C Heat f fusn f [kj/kg] d Dameter [m] D Ice Thckness [m] F Fl rate [m 3 /h] G r Grashf numer h Strage tme [h] h The meltng tme [h] IPF Ice packng factr [%] K Over-all heat transfer ceffcent f tue at nn-freezng [kw/(mk)] K Over-all heat transfer ceffcent f tue at freezng [kw/(mk)] l Tue length f each layer n an cl [m] L Ttal tue length n all tanks [m] L c Ttal tue length f each cl [m] M Vlume [m 3 ] M,max Desgn maxmum amunt f [m 3 ] n Crrectn factr ased n Re and the rat eteen the tue dameter and ptch f adjacency tues HP Refrgeratr capacty [kw] P r Prandtl numer Q Amunt f latent heat strage [kj] Q c Amunt f ver-all heat transfer f tue [kj] r Radus f tue [m] R e Reynlds numer t Tme [h] T Temperature [ C] T m Average rne temperature f strage [ C] T g Lgarthmc mean temperature dfference at heat strage [ C] T n Return chlled ater temperature frm the secndary sde [ C] T m The average temperature dfference f heat exchange at sensle heat strage [ C] T Intal ater temperature n tank [ C] V ater vlume n each tank [m 3 ] V m Ice vlume melted n each tank [m 3 ] Heat transfer ceffcent [W/(m 2 K)] Cl percentage fllng n tank [%] Thermal cnductvty [W/(m/K)] Crrectn factr ased n the tues numer f clumns alng the drectn f ater fl Densty [kg/m 3 ] T Temperature dfference eteen rne utlet temperature and evapratng temperature [ C] T cd Temperature dfference eteen the clng ater utlet temperature and cndensatn temperature [ C] T T +T cd [ C] t Tme step f dfference calculatn [h] Suscrpts : Value fr rne : Value f chller nlet,c: Value f cl nlet : Value f chller utlet,c: Value f cl utlet cd: Value aut clng ater cl: Value fr cl : Value f the cl nter surface : Value fr k: Value fr sensle heat : Value f the cl uter surface s: Value fr Latent heat : Value fr ater : Value f any cndtns

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1 Lecture 2 Heat Exchangers Heat Exchangers Chee 38 Heat Exchangers A heat exchanger s used t exchange heat between tw fluds f dfferent temperatures whch are separated by a sld wall. Heat exchangers are

More information

Comparison of Building Codes and Insulation in China and Iceland

Comparison of Building Codes and Insulation in China and Iceland Prceedngs Wrld Gethermal Cngress 00 Bal, Indnesa, 5-9 prl 00 Cmparsn f Buldng Cdes and Insulatn n Chna and Iceland Hayan Le and Pall Valdmarssn Tanjn Gethermal esearch & Tranng Centre, Tanjn Unversty,

More information

Chapter 3, Solution 1C.

Chapter 3, Solution 1C. COSMOS: Cmplete Onlne Slutns Manual Organzatn System Chapter 3, Slutn C. (a If the lateral surfaces f the rd are nsulated, the heat transfer surface area f the cylndrcal rd s the bttm r the tp surface

More information

Conduction Heat Transfer

Conduction Heat Transfer Cnductn Heat Transfer Practce prblems A steel ppe f cnductvty 5 W/m-K has nsde and utsde surface temperature f C and 6 C respectvely Fnd the heat flw rate per unt ppe length and flux per unt nsde and per

More information

SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES

SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES Mhammadreza Dlatan Alreza Jallan Department f Electrcal Engneerng, Iran Unversty f scence & Technlgy (IUST) e-mal:

More information

A Proposal of Heating Load Calculation considering Stack Effect in High-rise Buildings

A Proposal of Heating Load Calculation considering Stack Effect in High-rise Buildings A Prpsal f Heatng Lad Calculatn cnsderng Stack Effect n Hgh-rse Buldngs *Dsam Sng 1) and Tae-Hyuk Kang 2) 1) Department f Archtectural Engneerng, Sungkyunkwan Unversty, 2066 Sebu-r, Jangan-gu, Suwn, 440-746,

More information

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh Frst CIRCLE YOUR DIVISION: Dv. 1 (9:30 am) Dv. (11:30 am) Dv. 3 (:30 m) Prf. Ruan Prf. Na Mr. Sngh Schl f Mechancal Engneerng Purdue Unversty ME315 Heat and Mass ransfer Eam #3 Wednesday Nvember 17 010

More information

3-42. Chapter 15 Steady Heat Conduction. Heat Conduction in Cylinders and Spheres

3-42. Chapter 15 Steady Heat Conduction. Heat Conduction in Cylinders and Spheres Chapter 5 Steady Heat Cnductn Heat Cnductn n Cylnders and Spheres 3-64C When the dameter f cylnder s very small cmpared t ts length, t can be treated as an ndefntely lng cylnder. Cylndrcal rds can als

More information

Analytical Modeling of Natural Convection in Horizontal Annuli

Analytical Modeling of Natural Convection in Horizontal Annuli Analytcal Mdelng f Natural Cnvectn n Hrzntal Annul Peter Teertstra, M. Mchael Yvanvch, J. Rchard Culham Mcrelectrncs Heat Transfer Labratry Department f Mechancal Engneerng Unversty f Waterl Waterl, Ontar,

More information

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune Chapter 7 Flud Systems and Thermal Systems 7.1 INTODUCTION A. Bazune A flud system uses ne r mre fluds t acheve ts purpse. Dampers and shck absrbers are eamples f flud systems because they depend n the

More information

Transient Conduction: Spatial Effects and the Role of Analytical Solutions

Transient Conduction: Spatial Effects and the Role of Analytical Solutions Transent Cnductn: Spatal Effects and the Rle f Analytcal Slutns Slutn t the Heat Equatn fr a Plane Wall wth Symmetrcal Cnvectn Cndtns If the lumped capactance apprxmatn can nt be made, cnsderatn must be

More information

Advances in Engineering Research (AER), volume 102 Second International Conference on Mechanics, Materials and Structural Engineering (ICMMSE 2017)

Advances in Engineering Research (AER), volume 102 Second International Conference on Mechanics, Materials and Structural Engineering (ICMMSE 2017) Secnd Internatnal Cnference n Mechancs, Materals and Structural Engneerng (ICMMSE 2017) Materal Selectn and Analyss f Ol Flm Pressure fr the Flatng Rng Bearng f Turbcharger Lqang PENG1, 2, a*, Hupng ZHENG2,

More information

Feedback Principle :-

Feedback Principle :- Feedback Prncple : Feedback amplfer s that n whch a part f the utput f the basc amplfer s returned back t the nput termnal and mxed up wth the nternal nput sgnal. The sub netwrks f feedback amplfer are:

More information

Physic 231 Lecture 33

Physic 231 Lecture 33 Physc 231 Lecture 33 Man pnts f tday s lecture: eat and heat capacty: Q cm Phase transtns and latent heat: Q Lm ( ) eat flw Q k 2 1 t L Examples f heat cnductvty, R values fr nsulatrs Cnvectn R L / k Radatn

More information

Bi-level Optimization Method of Air-conditioning System Based on Office Building Energy Storage Characteristics

Bi-level Optimization Method of Air-conditioning System Based on Office Building Energy Storage Characteristics IOP Cnference Seres: Materals Scence and Engneerng PAPER OPEN ACCESS B-level Optmzatn Methd f Ar-cndtnng System Based n Offce Buldng Energy Strage Characterstcs T cte ths artcle: Qngze Wang et al 017 IOP

More information

Department of Civil Engineering & Applied Mechanics McGill University, Montreal, Quebec Canada

Department of Civil Engineering & Applied Mechanics McGill University, Montreal, Quebec Canada Department f Cvl Engneerng & Appled Mechancs McGll Unversty, Mntreal, Quebec Canada CIVE 90 THEMODYNAMICS & HEAT TANSFE Assgnment #6 SOUTIONS. Cnsder a.-m hgh and -m-wde duble-pane wndw cnsstng f tw 3-mmthck

More information

A/2 l,k. Problem 1 STRATEGY. KNOWN Resistance of a complete spherical shell: r rk. Inner and outer radii

A/2 l,k. Problem 1 STRATEGY. KNOWN Resistance of a complete spherical shell: r rk. Inner and outer radii Prblem 1 STRATEGY KNOWN Resstance f a cmplete sphercal shell: R ( r r / (4 π r rk sphere Inner an uter ra r an r, SOLUTION Part 1: Resstance f a hemsphercal shell: T calculate the resstance f the hemsphere,

More information

Water vapour balance in a building moisture exposure for timber structures

Water vapour balance in a building moisture exposure for timber structures Jnt Wrkshp f COST Actns TU1 and E55 September 21-22 9, Ljubljana, Slvena Water vapur balance n a buldng msture expsure fr tmber structures Gerhard Fnk ETH Zurch, Swtzerland Jchen Köhler ETH Zurch, Swtzerland

More information

The Effect Of Type-III Antifreeze Proteins (AFPs) On CO2 Hydrate Slurry Formation

The Effect Of Type-III Antifreeze Proteins (AFPs) On CO2 Hydrate Slurry Formation Purdue Unversty Purdue e-pubs Internatnal Refrgeratn and Ar Cndtnng Cnference Schl f Mechancal Engneerng 2014 The Effect Of Type-III Antfreeze Prtens (AFPs) On CO2 Hydrate Slurry Frmatn Hngxa Zhu Delft

More information

Optimization and Analysis of a Vertical Ground- Coupled Heat Pump

Optimization and Analysis of a Vertical Ground- Coupled Heat Pump INTERNATIONAL JOURNAL f RENEWABLE ENERGY RESEARCH Al Savsh Krd et al., Vl.2, N.1, 2012 Optmzatn and Analyss f a Vertcal Grund- Cupled Heat Pump Al Savsh Krd*, Seyed Al Jazayer* *K.N.Ts Unversty f Technlgy,

More information

Introduction to Electronic circuits.

Introduction to Electronic circuits. Intrductn t Electrnc crcuts. Passve and Actve crcut elements. Capactrs, esstrs and Inductrs n AC crcuts. Vltage and current dvders. Vltage and current surces. Amplfers, and ther transfer characterstc.

More information

CHAPTER 3 ANALYSIS OF KY BOOST CONVERTER

CHAPTER 3 ANALYSIS OF KY BOOST CONVERTER 70 CHAPTER 3 ANALYSIS OF KY BOOST CONERTER 3.1 Intrductn The KY Bst Cnverter s a recent nventn made by K.I.Hwu et. al., (2007), (2009a), (2009b), (2009c), (2010) n the nn-slated DC DC cnverter segment,

More information

ME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function

ME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function Mdellng Physcal Systems The Transer Functn Derental Equatns U Plant Y In the plant shwn, the nput u aects the respnse the utput y. In general, the dynamcs ths respnse can be descrbed by a derental equatn

More information

Dynamic Model-Based Fault Detection and Diagnosis Residual Considerations for Vapor Compression Systems

Dynamic Model-Based Fault Detection and Diagnosis Residual Considerations for Vapor Compression Systems Prceedngs f the 26 Amercan Cntrl Cnference Mnneapls, Mnnesta, USA, June 4-6, 26 FrA7. Dynamc Mdel-Based Fault Detectn and Dagnss Resdual Cnsderatns fr Vapr Cmpressn Systems Mchael C. Ker, Andrew G. Alleyne,

More information

Design of Analog Integrated Circuits

Design of Analog Integrated Circuits Desgn f Analg Integrated Crcuts I. Amplfers Desgn f Analg Integrated Crcuts Fall 2012, Dr. Guxng Wang 1 Oerew Basc MOS amplfer structures Cmmn-Surce Amplfer Surce Fllwer Cmmn-Gate Amplfer Desgn f Analg

More information

Influences of pitch-length louvered strip insert on thermal characteristic in concentric pipe heat exchanger

Influences of pitch-length louvered strip insert on thermal characteristic in concentric pipe heat exchanger MATEC Web f Cnferences 0, 0304 (07) DOI: 0.05/ mateccnf/0700304 Influences f ptch-length luvered strp nsert n thermal characterstc n cncentrc ppe heat exchanger Indr Yanngsh,*, and Agung Tr Wjayanta Mechancal

More information

Circuits Op-Amp. Interaction of Circuit Elements. Quick Check How does closing the switch affect V o and I o?

Circuits Op-Amp. Interaction of Circuit Elements. Quick Check How does closing the switch affect V o and I o? Crcuts Op-Amp ENGG1015 1 st Semester, 01 Interactn f Crcut Elements Crcut desgn s cmplcated by nteractns amng the elements. Addng an element changes vltages & currents thrughut crcut. Example: clsng a

More information

PHYSICS 536 Experiment 12: Applications of the Golden Rules for Negative Feedback

PHYSICS 536 Experiment 12: Applications of the Golden Rules for Negative Feedback PHYSICS 536 Experment : Applcatns f the Glden Rules fr Negatve Feedback The purpse f ths experment s t llustrate the glden rules f negatve feedback fr a varety f crcuts. These cncepts permt yu t create

More information

IGEE 401 Power Electronic Systems. Solution to Midterm Examination Fall 2004

IGEE 401 Power Electronic Systems. Solution to Midterm Examination Fall 2004 Jós, G GEE 401 wer Electrnc Systems Slutn t Mdterm Examnatn Fall 2004 Specal nstructns: - Duratn: 75 mnutes. - Materal allwed: a crb sheet (duble sded 8.5 x 11), calculatr. - Attempt all questns. Make

More information

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California Vlume Change fr a Unaxal Stress Istrpc lastcty n 3D Istrpc = same n all drectns The cmplete stress-stran relatns fr an strpc elastc Stresses actng n a dfferental vlume element sld n 3D: (.e., a generalzed

More information

Natural Convection in a Horizontal Annulus with Oscillating Inner Cylinder Using Lagrangian-Eulerian Kinematics

Natural Convection in a Horizontal Annulus with Oscillating Inner Cylinder Using Lagrangian-Eulerian Kinematics Natural Cnvectn n a Hrzntal Annulus wth Oscllatng Inner Cylnder Usng Lagrangan-Euleran Knematcs Esam M. Alawadh Kuwat Unversty Mechancal Engneerng Department P. O. Bx # 5969, Safat, 3060 KUWAIT Abstract

More information

Pull-Out Strength of a Cast-In-Place Anchor Bolt in Concrete Exposed to High Temperature

Pull-Out Strength of a Cast-In-Place Anchor Bolt in Concrete Exposed to High Temperature Pull-Out Strength f a Cast-In-Place Anchr Blt n Cncrete Expsed t Hgh Temperature Katsuk Takguch, Jun Hashmt Tky Insttute f Technlgy, Japan. ABSTRACT! Many anchr blts are used n nuclear-related facltes

More information

Wp/Lmin. Wn/Lmin 2.5V

Wp/Lmin. Wn/Lmin 2.5V UNIVERITY OF CALIFORNIA Cllege f Engneerng Department f Electrcal Engneerng and Cmputer cences Andre Vladmrescu Hmewrk #7 EEC Due Frday, Aprl 8 th, pm @ 0 Cry Prblem #.5V Wp/Lmn 0.0V Wp/Lmn n ut Wn/Lmn.5V

More information

Drought Modelling based on Artificial Intelligence and Neural Network Algorithms: A case study in Queensland, Australia

Drought Modelling based on Artificial Intelligence and Neural Network Algorithms: A case study in Queensland, Australia Drught Mdellng based n Artfcal Intellgence and Neural Netwrk Algrthms: A case study n Queensland Australa Kavna S Dayal (PhD Canddate) Ravnesh C De Armand A Apan Unversty f Suthern Queensland Australa

More information

EE 204 Lecture 25 More Examples on Power Factor and the Reactive Power

EE 204 Lecture 25 More Examples on Power Factor and the Reactive Power EE 204 Lecture 25 Mre Examples n Pwer Factr and the Reactve Pwer The pwer factr has been defned n the prevus lecture wth an example n pwer factr calculatn. We present tw mre examples n ths lecture. Example

More information

A BESTEST VALIDATION STUDY OF THE DYNAMIC GROUND-COUPLED HEAT TRANSFER MODEL USED IN ACCURATE. Dong Chen 1. PO Box 56, Highett. Vic.

A BESTEST VALIDATION STUDY OF THE DYNAMIC GROUND-COUPLED HEAT TRANSFER MODEL USED IN ACCURATE. Dong Chen 1. PO Box 56, Highett. Vic. A BESTEST VALIDATION STUDY OF THE DYNAMIC GROUND-COUPLED HEAT TRANSFER MODEL USED IN ACCURATE Dng Chen CSIRO Energy Transfrmed Flagshp and CSIRO Ecsystem Scences PO Bx 56, Hghett. Vc. 390, Australa ABSTRACT

More information

CHAPTER 3: FEEDBACK. Dr. Wan Mahani Hafizah binti Wan Mahmud

CHAPTER 3: FEEDBACK. Dr. Wan Mahani Hafizah binti Wan Mahmud CHPTER 3: FEEDBCK Dr. Wan Mahan Hafzah bnt Wan Mahmud Feedback ntrductn Types f Feedback dvantages, Characterstcs and effect f Negatve Feedback mplfers Crcuts wth negatve feedback Pstve feedback and Oscllatr

More information

Big Data Analytics! Special Topics for Computer Science CSE CSE Mar 31

Big Data Analytics! Special Topics for Computer Science CSE CSE Mar 31 Bg Data Analytcs! Specal Tpcs fr Cmputer Scence CSE 4095-001 CSE 5095-005! Mar 31 Fe Wang Asscate Prfessr Department f Cmputer Scence and Engneerng fe_wang@ucnn.edu Intrductn t Deep Learnng Perceptrn In

More information

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas Sectn : Detaled Slutns f Wrd Prblems Unt : Slvng Wrd Prblems by Mdelng wth Frmulas Example : The factry nvce fr a mnvan shws that the dealer pad $,5 fr the vehcle. If the stcker prce f the van s $5,, hw

More information

MODULE 7 HEAT EXCHANGERS

MODULE 7 HEAT EXCHANGERS MODULE 7 HEAT EXCHANGERS 7. What are heat exchangers? Heat exchangers are practcal devces used t transfer energy frm ne flud t anther. Arund the husehld, we are accustmed t seeng the cndensers and evapratrs

More information

Spring 2002 Lecture #17

Spring 2002 Lecture #17 1443-51 Sprng 22 Lecture #17 r. Jaehn Yu 1. Cndtns fr Equlbrum 2. Center f Gravty 3. Elastc Prpertes f Slds Yung s dulus Shear dulus ulk dulus Tday s Hmewrk Assgnment s the Hmewrk #8!!! 2 nd term eam n

More information

Downscaling Geopotential Height Using Lapse Rate

Downscaling Geopotential Height Using Lapse Rate Dwnscalng Geptental Heght Usng Lapse Rate Chrana Surawut and Dusadee Sukawat 2* Earth Sstem Scence, Kng Mngkut s Unverst f Technlg Thnur, Bangkk, Thaland 2* Department f Mathematcs, Kng Mngkut s Unverst

More information

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with Schl f Aerspace Chemcal D: Mtvatn Prevus D Analyss cnsdered systems where cmpstn f flud was frzen fxed chemcal cmpstn Chemcally eactng Flw but there are numerus stuatns n prpulsn systems where chemcal

More information

BME 5742 Biosystems Modeling and Control

BME 5742 Biosystems Modeling and Control BME 5742 Bsystems Mdeln and Cntrl Cell Electrcal Actvty: In Mvement acrss Cell Membrane and Membrane Ptental Dr. Zv Rth (FAU) 1 References Hppensteadt-Peskn, Ch. 3 Dr. Rbert Farley s lecture ntes Inc Equlbra

More information

Shell Stiffness for Diffe ent Modes

Shell Stiffness for Diffe ent Modes Engneerng Mem N 28 February 0 979 SUGGESTONS FOR THE DEFORMABLE SUBREFLECTOR Sebastan vn Herner Observatns wth the present expermental versn (Engneerng Dv nternal Reprt 09 July 978) have shwn that a defrmable

More information

Computer Aided Design (CAD) of a Multi-component Condenser

Computer Aided Design (CAD) of a Multi-component Condenser S. BANDYOPADHYAY et al., Cputer Aded Desgn (CAD) f a Mult-cpnent, Che. Bche. Eng. Q. 21 (2) 97 103 (2007) 97 Cputer Aded Desgn (CAD) f a Mult-cpnent Cndenser S. Bandypadhyay, M. S. Ala, V. K. Agrawal,

More information

State-Space Model Based Generalized Predictive Control for Networked Control Systems

State-Space Model Based Generalized Predictive Control for Networked Control Systems Prceedngs f the 7th Wrld Cngress he Internatnal Federatn f Autmatc Cntrl State-Space Mdel Based Generalzed Predctve Cntrl fr Netwred Cntrl Systems Bn ang* Gu-Png Lu** We-Hua Gu*** and Ya-Ln Wang**** *Schl

More information

A New Method for Solving Integer Linear. Programming Problems with Fuzzy Variables

A New Method for Solving Integer Linear. Programming Problems with Fuzzy Variables Appled Mathematcal Scences, Vl. 4, 00, n. 0, 997-004 A New Methd fr Slvng Integer Lnear Prgrammng Prblems wth Fuzzy Varables P. Pandan and M. Jayalakshm Department f Mathematcs, Schl f Advanced Scences,

More information

Nomenclature: number of electrons e -1. electron charge F constant number, (columbs/moles of e -1 ) atomic number g

Nomenclature: number of electrons e -1. electron charge F constant number, (columbs/moles of e -1 ) atomic number g Quanttatve Analyss f Irreversbltes Causes Vltage Drp n Fuel cell (Smulatn) Hssen Ghadaman*, Dr. Yadlah Sabh** Department f Energy Engneerng, Scence and Research Branch Azad Unversty, Islamc Republc f IRAN

More information

Chem 204A, Fall 2004, Mid-term (II)

Chem 204A, Fall 2004, Mid-term (II) Frst tw letters f yur last name Last ame Frst ame McGll ID Chem 204A, Fall 2004, Md-term (II) Read these nstructns carefully befre yu start tal me: 2 hurs 50 mnutes (6:05 PM 8:55 PM) 1. hs exam has ttal

More information

V. Electrostatics Lecture 27a: Diffuse charge at electrodes

V. Electrostatics Lecture 27a: Diffuse charge at electrodes V. Electrstatcs Lecture 27a: Dffuse charge at electrdes Ntes by MIT tudent We have talked abut the electrc duble structures and crrespndng mdels descrbng the n and ptental dstrbutn n the duble layer. Nw

More information

Where a licence is displayed above, please note the terms and conditions of the licence govern your use of this document.

Where a licence is displayed above, please note the terms and conditions of the licence govern your use of this document. Mdellng the seepage flw durng cassn nstallatn n a natural seabed Faramarz, Asaad; Faz, Khyar; Drar, Samr; Mehravar, Mura; Harreche, Ouahd Dcument Versn Publsher's PDF, als knwn as Versn f recrd Ctatn fr

More information

Learn more at

Learn more at Tensn and Expansn Analyss f Ppe-n-Ppe Rsers: Part A, Theretcal rmulatn Kevn Chuanjan Man, Bn Yue, Adam Szucs, Rcky Theth 2H ffshre nc. Hustn, TX, USA ABSTRACT Ths paper prvdes a mathematcal mdel fr accurate

More information

Sirous Zamanirad 1, Said Mazaheri 2, Mehrdad Ghafourian 1

Sirous Zamanirad 1, Said Mazaheri 2, Mehrdad Ghafourian 1 INERNAIONAL JOURNAL OF COASAL & OFFSHORE ENGINEERING IJCOE Vl.1/N. 2/Summer 2017 (21-26) Avalable nlne at: http://jce.rg/brwse.php?a_cde=a-10-124-1&sd=1&slc_lang=en Intrducng a Methd fr Mre Precse Predctn

More information

Analysis The characteristic length of the junction and the Biot number are

Analysis The characteristic length of the junction and the Biot number are -4 4 The temerature f a gas stream s t be measured by a thermule. The tme t taes t regster 99 erent f the ntal ΔT s t be determned. Assumtns The juntn s sheral n shae wth a dameter f D 0.00 m. The thermal

More information

4.8 Degradation of Elastomers by Heat and/or Radiation

4.8 Degradation of Elastomers by Heat and/or Radiation 4.8 Degradatn f Elastmers by Heat and/r Radatn M.It Japan Atmc Energy Research Insttute, Nuclear Educatn Center 2-28-49, Hnkmagme, Bunkyu-ku Tky, 113, JAPAN Abstract Ths artcle studed sme prblems n the

More information

Study Group Report: Plate-fin Heat Exchangers: AEA Technology

Study Group Report: Plate-fin Heat Exchangers: AEA Technology Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery

More information

2 Analysis of the non-linear aerodynamic loads of hypersonic flow. 1 General Introduction

2 Analysis of the non-linear aerodynamic loads of hypersonic flow. 1 General Introduction 4 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES PRELIMINARY STUDY OF NON-LINEAR AEROELASTIC PHENOMENA IN HYPERSONIC FLOW Zhang Wewe, Ye Zhengyn, Yang Yngnan Cllege f Aernautcs, Nrthwestern Plytechncal

More information

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,

More information

_J _J J J J J J J J _. 7 particles in the blue state; 3 particles in the red state: 720 configurations _J J J _J J J J J J J J _

_J _J J J J J J J J _. 7 particles in the blue state; 3 particles in the red state: 720 configurations _J J J _J J J J J J J J _ Dsrder and Suppse I have 10 partcles that can be n ne f tw states ether the blue state r the red state. Hw many dfferent ways can we arrange thse partcles amng the states? All partcles n the blue state:

More information

Mathematical Model of Gas Exchange for Modified Atmosphere Packaging Containing Pak-choi

Mathematical Model of Gas Exchange for Modified Atmosphere Packaging Containing Pak-choi Prceedngs f the 17th IAPRI Wrld Cnference n Packagng Mathematcal Mdel f Gas Exchange fr Mdfed Atmsphere Packagng Cntanng Pak-ch CAO Fe Dept. f Prntng Engneerng Tanjn Vcatnal Insttute Tanjn, P. R. Chna

More information

The APS Transfer Line from Linac to Injector Synchrotron.

The APS Transfer Line from Linac to Injector Synchrotron. -------------..., The submtted mclnu;..crpt has been authred by a cntractr f the U. S. Gvernment under cntract N. W 31 19-ENG 38. Accrdngly, the U. S. Gvernment retans a nnexclusve, ryalty-free lcense

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient 58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),

More information

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850) hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electrnc Crcuts Feedback & Stablty Sectns f Chapter 2. Kruger Feedback & Stablty Cnfguratn f Feedback mplfer S S S S fb Negate feedback S S S fb S S S S S β s the feedback transfer functn Implct

More information

Outline. Unit Eight Calculations with Entropy. The Second Law. Second Law Notes. Uses of Entropy. Entropy is a Property.

Outline. Unit Eight Calculations with Entropy. The Second Law. Second Law Notes. Uses of Entropy. Entropy is a Property. Unt Eght Calculatons wth Entropy Mechancal Engneerng 370 Thermodynamcs Larry Caretto October 6, 010 Outlne Quz Seven Solutons Second law revew Goals for unt eght Usng entropy to calculate the maxmum work

More information

Common Gate Amplifier

Common Gate Amplifier mmn Gate Ampler Fure (a) shs a cmmn ate ampler th deal current surce lad. Fure (b) shs the deal current surce mplemented by PMOS th cnstant ate t surce vltae. DD DD G M G M G M (a) (b) Fure. mmn ate ampler.

More information

Optimum Design of Heat Exchanger in Diesel Engine Cold EGR for Pollutants Reduction

Optimum Design of Heat Exchanger in Diesel Engine Cold EGR for Pollutants Reduction Wrld Academy f Scence, Engneerng and Technlgy Internatnal Jurnal f Mechancal and Mechatrncs Engneerng Vl:8, N:11, 2014 Optmum Desgn f Heat Exchanger n Desel Engne Cld EGR fr Pllutants Reductn Nasser Ghassembaglu,

More information

element k Using FEM to Solve Truss Problems

element k Using FEM to Solve Truss Problems sng EM t Slve Truss Prblems A truss s an engneerng structure cmpsed straght members, a certan materal, that are tpcall pn-ned at ther ends. Such members are als called tw-rce members snce the can nl transmt

More information

6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS

6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS 6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS Elutratn s the prcess n whch fne partcles are carred ut f a fludzed bed due t the flud flw rate passng thrugh the bed. Typcally, fne partcles are elutrated

More information

Theory of a vertically loaded Suction Pile in SAND

Theory of a vertically loaded Suction Pile in SAND Thery f a vertcally lae Suctn Ple n SAND 1. Cnventn Water t COG Z L Sl z COG D t1 Fgure 1: Overvew f man cmpnents Fgure : Overvew f man parameters Z D L t 1 t W φ φ e c κ p ρ sl γ sl Waterepth Penetratnepth

More information

Dynamic simulation of multi-effect falling-film evaporator: Milk powder production plant

Dynamic simulation of multi-effect falling-film evaporator: Milk powder production plant Dynam smulatn f mult-effet fallng-flm evapratr: Mlk pwder prdutn plant Fateme Medhat Bjnurd, Mhammad Al Fanae *, Had Zhree Department f Chem. Eng., Faulty f Eng., Ferdws Unversty f Mashhad, I. R. Iran

More information

A quote of the week (or camel of the week): There is no expedience to which a man will not go to avoid the labor of thinking. Thomas A.

A quote of the week (or camel of the week): There is no expedience to which a man will not go to avoid the labor of thinking. Thomas A. A quote of the week (or camel of the week): here s no expedence to whch a man wll not go to avod the labor of thnkng. homas A. Edson Hess law. Algorthm S Select a reacton, possbly contanng specfc compounds

More information

Laboratory #2: Introduction to Microstripline Transmission Lines, Reflection and Transmission Coefficients, and S-Parameters

Laboratory #2: Introduction to Microstripline Transmission Lines, Reflection and Transmission Coefficients, and S-Parameters EEE 7 La # Laratry #: Intrductin t Micrstripline Transmissin Lines, Reflectin and Transmissin Cefficients, and -Parameters I. OBJECTIVE A micrstrip transmissin line is designed fr nminally 50Ω. The reflectin

More information

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N Q1. A transverse sinusidal wave travelling n a string is given by: y (x,t) = 0.20 sin (2.5 x 80 t) (SI units). The length f the string is 2.0 m and its mass is 1.5 g. What is the magnitude f the tensin

More information

III. Operational Amplifiers

III. Operational Amplifiers III. Operatnal Amplfers Amplfers are tw-prt netwrks n whch the utput vltage r current s drectly prprtnal t ether nput vltage r current. Fur dfferent knds f amplfers ext: ltage amplfer: Current amplfer:

More information

of Large Helical Device

of Large Helical Device J. Plasma Fusn Res. SRIS, Vl. 5 (22) 25U254 Stran Mntrng System fr Grygenc Structure f Large Helcal Devce NISHIMURA Arata, TAMURA Htstr, IMAGAWA Shnsaku and SATOW Takash Natnal Insttute fr Fusn Scence,

More information

Chapter 4. Unsteady State Conduction

Chapter 4. Unsteady State Conduction Chapter 4 Unsteady State Cnductin Chapter 5 Steady State Cnductin Chee 318 1 4-1 Intrductin ransient Cnductin Many heat transfer prblems are time dependent Changes in perating cnditins in a system cause

More information

1.1. Basic Mechanisms of Heat Transfer

1.1. Basic Mechanisms of Heat Transfer 1.1. Basc Mechansms f Heat Transfer The basc mechansms f heat transfer are generally cnsdered t be cnductn, cnvectn, blng, cndensatn, and radatn. Of these, radatn s usually sgnfcant nly at temperatures

More information

PT326 PROCESS TRAINER

PT326 PROCESS TRAINER PT326 PROCESS TRAINER 1. Descrptn f the Apparatus PT 326 Prcess Traner The PT 326 Prcess Traner mdels cmmn ndustral stuatns n whch temperature cntrl s requred n the presence f transprt delays and transfer

More information

Statistical Speech Analysis and Nonlinear Modeling

Statistical Speech Analysis and Nonlinear Modeling Lmerck, 16th Aprl 23 Statstcal Analyss and Nnlnear Mdelng Nasss Katsamans & Petrs Marags Natnal Techncal Unversty f Athens Schl f Electrcal & Cmputer Engneerng CVSP Grup COST277 Meetng, Intrductn Cntents

More information

Int. J. of Applied Mechanics and Engineering, 2014, vol.19, No.3, pp DOI: /ijame

Int. J. of Applied Mechanics and Engineering, 2014, vol.19, No.3, pp DOI: /ijame Int. J. f Appled Mechancs and Engneerng, 2014, vl.19, N.3, pp.539-548 DOI: 10.2478/jame-2014-0036 APPLICATION OF MULTI-VALUED WEIGHTING LOGICAL FUNCTIONS IN THE ANALYSIS OF A DEGREE OF IMPORTANCE OF CONSTRUCTION

More information

Chapter 6 : Gibbs Free Energy

Chapter 6 : Gibbs Free Energy Wnter 01 Chem 54: ntrductry hermdynamcs Chapter 6 : Gbbs Free Energy... 64 Defntn f G, A... 64 Mawell Relatns... 65 Gbbs Free Energy G(,) (ure substances)... 67 Gbbs Free Energy fr Mtures... 68 ΔG f deal

More information

Effect Of Humidity And Inclination Angle On Microchannel Heat Exchanger Performance

Effect Of Humidity And Inclination Angle On Microchannel Heat Exchanger Performance Purdue Unversty Purdue e-pubs Internatnal Rergeratn and Ar Cndtnng Cnerence Schl Mechancal Engneerng 22 Eect O Humdty And Inclnatn Angle On Mcrchannel Heat Exchanger Perrmance S. M. Sng Unversty Illns

More information

Novel current mode AC/AC converters with high frequency ac link *

Novel current mode AC/AC converters with high frequency ac link * vel current mde AC/AC cnverters wth hgh frequency ac lnk * Dalan Chen, e, Jan u, Shengyang n, Chen Sng Department f Electrcal Engneerng, anjng nversty f Aernautcs & Astrnautcs, anjng, Jangsu, 006 P.R.Chna

More information

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan Wnter 2008 CS567 Stochastc Lnear/Integer Programmng Guest Lecturer: Xu, Huan Class 2: More Modelng Examples 1 Capacty Expanson Capacty expanson models optmal choces of the tmng and levels of nvestments

More information

Out-of-plane orbital maneuvers using swing-bys with the Moon

Out-of-plane orbital maneuvers using swing-bys with the Moon Jurnal f Physcs: Cnference Seres PAPER OPEN ACCESS Out-f-plane rbtal maneuvers usng swng-bys wth the Mn Related cntent - Pwered Swng-By Maneuvers arund the Mn A F Slva, A F B A Prad and O C Wnter cte ths

More information

CHAPTER 3 QUASI-RESONANT BUCK CONVERTER

CHAPTER 3 QUASI-RESONANT BUCK CONVERTER 27 CHAPTER 3 QUASI-RESONANT BUCK CONVERTER Hstrcally, prr t the avalablty f cntrllable swtch wth apprecable vltage and current-handlng capablty, the swtch-mde DC-DC cnverter cnssts f thyrstrs whch pertans

More information

( ) = ( ) + ( 0) ) ( )

( ) = ( ) + ( 0) ) ( ) EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.

More information

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram Adabatc Sorpton of Ammona-Water System and Depctng n p-t-x Dagram J. POSPISIL, Z. SKALA Faculty of Mechancal Engneerng Brno Unversty of Technology Techncka 2, Brno 61669 CZECH REPUBLIC Abstract: - Absorpton

More information

Effect of loading frequency on the settlement of granular layer

Effect of loading frequency on the settlement of granular layer Effect of loadng frequency on the settlement of granular layer Akko KONO Ralway Techncal Research Insttute, Japan Takash Matsushma Tsukuba Unversty, Japan ABSTRACT: Cyclc loadng tests were performed both

More information

Final Exam Spring 2014 SOLUTION

Final Exam Spring 2014 SOLUTION Appled Opts H-464/564 C 594 rtland State nverst A. La Rsa Fnal am Sprng 14 SOLTION Name There are tw questns 1%) plus an ptnal bnus questn 1%) 1. Quarter wave plates and half wave plates The fgures belw

More information

EE 221 Practice Problems for the Final Exam

EE 221 Practice Problems for the Final Exam EE 1 Practce Prblems fr the Fnal Exam 1. The netwrk functn f a crcut s 1.5 H. ω 1+ j 500 Ths table recrds frequency respnse data fr ths crcut. Fll n the blanks n the table:. The netwrk functn f a crcut

More information

A Bidirectional Non-Isolated Multi-Input DC-DC Converter for Hybrid Energy Storage Systems in Electric Vehicles

A Bidirectional Non-Isolated Multi-Input DC-DC Converter for Hybrid Energy Storage Systems in Electric Vehicles Ths artcle has been accepted fr publcatn n a future ssue f ths jurnal, but has nt been fully edted. ntent may change prr t fnal publcatn. tatn nfrmatn: DOI.9/TT.5.5683, IEEE Transactns n ehcular Technlgy

More information

THERMAL TEST LEVELS & DURATIONS

THERMAL TEST LEVELS & DURATIONS PREFERRED RELIABILITY PAGE 1 OF 7 PRACTICES PRACTICE NO. PT-TE-144 Practice: 1 Perfrm thermal dwell test n prtflight hardware ver the temperature range f +75 C/-2 C (applied at the thermal cntrl/munting

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

Mode-Frequency Analysis of Laminated Spherical Shell

Mode-Frequency Analysis of Laminated Spherical Shell Mde-Frequency Analyss f Lamnated Sphercal Shell Umut Tpal Department f Cvl Engneerng Karadenz Techncal Unversty 080, Trabzn, Turkey umut@ktu.edu.tr Sessn ENG P50-00 Abstract Ths paper deals wth mde-frequency

More information

THE CURRENT BALANCE Physics 258/259

THE CURRENT BALANCE Physics 258/259 DSH 1988, 005 THE CURRENT BALANCE Physcs 58/59 The tme average force between two parallel conductors carryng an alternatng current s measured by balancng ths force aganst the gravtatonal force on a set

More information

Improved Bridgeless Interleaved Boost PFC Rectifier with Optimized Magnetic Utilization and Reduced Sensing Noise

Improved Bridgeless Interleaved Boost PFC Rectifier with Optimized Magnetic Utilization and Reduced Sensing Noise Jurnal f Pwer Electrncs, Vl. 14, N. 5, pp. 815-86, September 014 815 JPE 14-5-1 http://dx.d.rg/10.6113/jpe.014.14.5.815 ISSN(Prnt): 1598-09 / ISSN(Onlne): 093-4718 Imprved Brdgeless Interleaved Bst PFC

More information

Module B3. VLoad = = V S V LN

Module B3. VLoad = = V S V LN Mdule B Prblem The -hase lads are cnnected n arallel. One s a urely resste lad cnnected n wye. t cnsumes 00kW. The secnd s a urely nducte 00kR lad cnnected n wye. The thrd s a urely caacte 00kR lad cnnected

More information