K. K. Dagde * and Y. T. Puyate **

Size: px
Start display at page:

Download "K. K. Dagde * and Y. T. Puyate **"

Transcription

1 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp Sx-lump netc mdellng f adabatc plug-flw rserreactr n an ndustral F unt K. K. Dagde * and Y. T. Puyate ** *( Department f hemcal/ Petrchemcal Engneerng, vers State Unversty f Scence and Technlgy, Prt Harcurt, Ngera,) **( Department f hemcal/ Petrchemcal Engneerng, vers State Unversty f Scence and Technlgy, Prt Harcurt, Ngera,) Abstract A sx-lump netc mdel s presented that descrbes the catalytc cracng reactns tang place n an ndustral rser-reactr. In ths scheme, s (prpane and prpylene gases) and s (butane and butylenes gases) cmpnents f lquefed petrleum gas are predcted ndependently, as well as gaslne, dry gas, and ce. The rser-reactr s mdelled as a plug-flw reactr peratng adabatcally. del-predcted yelds f gaslne, s, s, fuel gas, ce, and rser-reactr utlet-temperature, agree reasnably well wth plant data btaned frm an peratng ndustral rser-reactr. Senstvty analyss carred ut n the rser-reactr ndcates that nlet-temperature f gas-l (feed), catalystt-gas l rat, and ma flwrate f gas-l, are mprtant prce varables that affect the peratn f the rser-reactr. It s shwn that the mnmum catalyst-t-gas l rat requred fr maxmum cnversn f gas-l s. Smulatn results usng catalyst-t-gas l rat f 6.5, nlettemperature f gas-l f 55K, and ma flwrate f gas-l f 67.8 g/s, gve yelds f 5.8% gaslne, 6.% s,.68% s, 5.% fuel gas, 5.% ce, and 6.66% f uncnverted gas-l. Keywrds: ser-reactr; mdellng; catalytc cracng; lump; netcs. Intrductn rude l cntans hydrcarbns rangng frm lght gases and lquefed petrleum gas (LPG) t resdues blng abve 66K []. These prducts f varus blng pnts can be separated usng a dstllatn clumn. Hwever, dstllatn alne cannt prduce suffcent amunt f lghter fractns such as gaslne t meet publc demand. Thus, subsequent refnng prce nwn as flud catalytc cracng (F) s used and frms the heart f a mdern refnery rented twards maxmum gaslne prductn. Flud catalytc cracng, whch taes place n the presence f a catalyst, s a prce whereby heaver dstllates f crude l such as vacuum gas-l (VGO) and ther related heavy stcs are cnverted nt lghter prducts such as hgh ctane gaslne, lght cycle l, and gaseus prducts (LPG, fuel gas, etc.), as well as ce. The F prce cmprses manly tw reactrs: () a rser-reactr, where hgh mlecular weght hydrcarbns cme n cntact wth a catalyst and are craced nt lwer mlecular weght prducts wth smultaneus depstn f ce n the catalyst, and () a regeneratr-reactr, where the ce depsts n the catalyst are burnt-ff usng ar and the regenerated catalyst s returned t the rser-reactr t partly supply the heat requred fr the endthermc cracng reactns. The rser-reactr s prbably the mst mprtant equpment n a F plant because all cracng reactns and fuel frmatn ccur n ths reactr. A mathematcal mdel descrbng the peratns n a rser-reactr can be a valuable tl fr ptmzng the perfrmance f the rser-reactr n rder t btan hgher yeld f prducts. The frst prblem n the mdellng f F rser-reactr s selectn f the netcs scheme. One apprach that deals wth mult-cmpnent mxtures le gas-l whch cntans mre than, dfferent speces s the frmulatn f lumped netc schemes [,, ]. In a three-lump netc mdel, gas-l (.e. the feed, and taen as ne lump) s cnverted nt lght gases plus ce lump, and gaslne [5]. Subsequent studes n the lterature [6, 7, 8, 9] cnsdered the need t present ce and lght gases as separate lumps creatng a fur-lump netc mdel n whch gas-l s cnverted nt lght gases (-), ce, and gaslne; and a fve-lump netc mdel n whch gas-l s cnverted nt ce, gaslne, LPG (- ), and fuel gases (dry gases,.e. -). A majr ue that s cmmn wth the analyses presented n the lterature fr each f these netc mdels s that nly the netc parameters are determned but nt appled t smulate a functnal rser-reactr n an ndustral F unt. Obh et al. [] smulated an ndustral fludzedbed F rser-reactr usng a three-lump netc mdel, but the ce generated durng the cracng reactns culd nt be determned ndependently n the analyss. Snce the heat requred fr the cracng reactns s btaned partly by burnng-ff the ce depsted n the catalyst n the regeneratr, 557 P a g e

2 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. adequate predctn f the amunt f ce n the catalyst s mperatve durng netc mdellng f a rser-reactr. In rder t accunt fr ce frmatn n the catalyst, Obh et al. [] and Obh and Apa [] presented a fur-lump netc mdel t accunt fr the ce frmatn n the catalyst. But the weane f the fur-lump mdel s that the LPG and fuel gases are lumped tgether as lght gases, whch maes t mpble t cnsder ndvdual effects f LPG and fuel gases n the netc scheme. Ths dsadvantage f the fur-lump mdel was taen care f n a fve-lump netc mdel presented by Dagde et al. [], where gas-l s cnverted nt gaslne, LPG, dry gas, and ce. Hwever, the fve-lump scheme culd nt determne separately the s (prpane and prpylene gases) as well as s (butane and butylene gases) whch are lumped n the LPG. In ths wr, a sx-lump netc scheme fr an adabatc plug-flw rser-reactr s presented n whch gas-l s cnverted nt dry gas, ce, gaslne, s, and s. Such a netc scheme allws ndependent predctn f s and s whch have valuable dmestc and labratry applcatns, used as feedstc n the petrchemcal ndustry, and n cmprer and ar blwer desgn [].. The sx-lump netc mdel The sx-lmp netc mdel shwn n Fg. and prpsed by Ancheyta and Stel [] s used n ths study. The mdel aumes that gas-l () s cnverted t () gaslne (5+), () s (butane, I- butane and butene), () s (prpane and prpylene), (5) dry gas ( ), and (6) ce, as well as uncnverted VGO (decanted and lght cycle ls). The netcs f VGO cracng has been fund expermentally t fllw clsely a secnd-rder chemcal reactn [5], whle the cracng f gaslne and LPG ( s and s) fllw a frst-rder chemcal reactn [,, ]. Fg.. Schematc dagram f sx-lump netc scheme The fllwng rate equatns are frmulated fr the varus cmpnents f the sx-lump netc mdel shwn n Fg. : ( r ) ( y () 5 6) ( r ) [( ) y y ] () 5 6 ( r ) [( ) y y y ] () 5 ( r ) [ y y y y ] () 5 ( r ) [ y y y y ] (5) ( r ) ( y y ) (6) where j lumps t respect t lumps y Gas l () / are the rate cnstants fr the cracng f T lumps, wth j ; r ) (, are the reactn rates wth, wth,,, 5, 6; are the ma fractns f the varus dfferent lumps, and as the ma denstes f the T s the ttal ma densty f all the sx lumps; s the effectvene factr; and s the catalyst deactvatn functn. The deactvatn netc mdel f Weeman and Nace [5] s chsen n ths study because f ts smplcty and ppularty n F mdellng, where the decay f catalyst actvty due t ce depstn s represented by the catalyst deactvatn functn expreed n the frm exp d e (6) d t c (7) where s the catalyst decay ceffcent whch s related t the rser-temperature n the Arrhenus equatn exp E T (8) d d / Ga sl ne (5) s () s () 558 P a g e

3 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. t and c [5] t c s the catalyst resdence tme expreed as A L cat F (TO) d (9) where s the catalyst decay pre-expnental F netc factr, s the ma flwrate f gas-l, cat (TO) s the catalyst-t-gas l rat,. s the A ma densty f catalyst, s the cr-sectnal L area f the rser-reactr, s the heght f the rser-reactr, s the unversal gas cnstant, and T s the abslute temperature. Substtutng eq. (9) nt eq. (7) gves d A L exp cat F ( TO) () η The effectvene factr ( ) fr the catalytc cracng f vacuum gas-l s evaluated as [6]: tanh h h () h where s a mdfed Thele mdulus gven as h a ext ( n ) cat D eff n () α where n s the rder f reactn (equal t fr gasl cracng); ext s the catalyst-specfc external surface area; are the netc rate cnstants f the Deff respectve lumps; s the effectve dffusvty f gas-l thrugh the catalyst, and s the mlar cncentratn f the varus lumps. It s mprtant t nte that ext n eq. () can be L, defned usng the characterstc dmensn, Z f the Zelte crystallte (.e. catalyst partcle sze) snce all the cracng reactns tae place n the Zelte crystallte wth lttle nfluence frm the matrx f the catalyst [7]. Therefre, apprxmatng the crystallte gemetry t be a sphere, gves the catalyst-specfc external surface area as [] 6 ext LZ () α whch when substtuted nt eq. () yelds the fllwng expren fr gas-l: h LZ 6 cat ( 5 D 6 ) eff ( 5) where the subscrpt ndcates gas-l. It s expected that dffusn f gas-l taes place n a USY Zelte, and the effectve dffusn ceffcent D eff f gas-l ( ) s gven by the Eryng equatn [8]. Deff Dp exp ED / T (6) Dp where s the pre-expnental factr fr E dffusn, and D s the actvatn energy fr dffusn. A value f D m p 9.58* s and E j D ml were used []... The rser-reactr mdel In the dervatn f the mathematcal mdel fr the rser-reactr, the fllwng aumptns are made: Axal dspersn n the rser-reactr s neglected. atalyst partcles have a unfrm sze n a gven dfferental element, and bth gas-l and gaslne have dentcal catalyst deactvatn functn, []. The rser wall s adabatc Feed vscsty and specfc heat capactes f all cmpnents are cnstant. Adsrptn and dspersn nsde the catalysts partcles are neglgble. Preure changes thrughut the rser heght are due t statc head f catalyst n the rser. e depstn n the catalyst des nt affect the flud flw. In each sectn f the rser-reactr, the catalyst and gas have the same temperature. The ce has the same specfc heat as the catalyst. The rser dynamcs s fast enugh t justfy plugflw characterstcs and a quas-steady state mdel. Instantaneus vaprzatn ccurs at the entrance f the rser-reactr [9]. racng reactns are cmpleted n the rserreactr,ce hence n reactn taes place n the strppng sectn. Applyng the cnservatn prncple t a cntrl A dl vlume ( ) f a plug-flw rser-reactr based n the abve aumptns, where dl s the dfferental heght f the reactr s cntrl vlume, gves the ma and energy balances as 559 P a g e

4 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. dy dy U ( r dt dl ) y L : y =,,, 5, 6 () ( 5 6) y (7) T Tref dy dy U ( r) dt dl We defne the fllwng dmensnle varables [( 5 6) y y ] (8) L Z (5) dy dy L U ( r) dt dl T (6) [( ) y y y ] (9) Tref 5 dy dy U ( r) dt dl [ y y y y ] () 5 dy5 dy5 U ( r5 ) dt dl [ y y y y ] () dy dy6 6 U ( r6) dt dl ( 6y 6y ) () dt A dl ( Fcat pcat F p) ( H) ( H) ( H ) y 5( H5) 6( H6) ( H ) ( H ) 5( H 5 y 6( H 6) y where ( H ) ( H ) y ( H ) y s the ma fractn f lump, 5 ) () s the average vd fractn n the rser-reactr, U s the rser superfcal velcty, cat s the ma flwrate f catalyst, pcat and p are the specfc heat capactes f catalyst and gas-l respectvely, and H j are the heat f reactn fr cracng lumps t j, and t s tme. Snce gas-l s the feed that s craced nt the varus prducts, the ma fractn f gas-l at the nlet ( L ) f the rser-reactr s unty, whle the ma fractns f the prducts at the nlet are equal t zer because n prduct s frmed at the nlet f the rser-reactr. Als, at the nlet f the rserreactr, the feed temperature s taen t be a T reference temperature ( ref ) equal t 8K []. These bundary cndtns at the nlet f the rserreactr are defned mathematcally as F where Z s the dmensnle heght f the rser-reactr, L s the varable heght f the rser-reactr, θ s the dmensnle rser temperature, and T s the rser temperature. Usng eqs. (5) and (6) n eqs. (7) (), and ntng that U F = A A gves dy A L dz F (7) ( ) y (8) 5 6 dy A L dz F y y ] [ (9) 5 6 dy A L dz F y y y ] [ () 5 dy A L dz F [ y y y y ] () 5 dy5 A L dz F [ y y y y ] () dy6 A L dz F d dz ( F cat L A pcat F ( y y ) () 6 6 p ) T ( ) ( ) H 5 H5 y ( H) ( H) 6( H6 ( ) 5( 5) H H y () ( H ) 6( H 6) y ( H) 5( H5) 5( 5) y H and the bundary cndtns () becme ref 56 P a g e

5 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. y LPG t Z : y y y y5 y6 (5) Dry gas ( 5 ) LPG t Dry gas where s the vlumetrc flw rate f gas-l. ( 5 ) atalyst Equatn (8) () were slved numercally decay ( usng a furth-rder unge-kutta algrthm d ) (Lee et al., usng the bundary cndtns (5). 989). Estmatn f netc parameters The rser-reactr mdel equatns cntan unnwn netc parameters such as the reactn rate cnstants ( ) fr the varus reactn paths, j and the catalyst deactvatn functn ( ). These cnstants have t be determned befre equatns (8)-() can be ntegrated. The netc parameters fr the cracng reactns based n the sx-lump netc mdel are presented n Table. Table. Estmated netc parameters fr cracng reactns n the rser-reactr [5] eactn path Gas-l t gaslne ( ) Gas-l t LPG ( ) Gas-l t LPG ( ) Gas-l t dry gas ( 5 ) Gas l t ce ( 6 ) Gaslne t LPG ( ) Gaslne t LPG ( ) Gaslne t Dry gas ( 5 ) Gaslne t ce ( 6 ) LPG t LPG ( ) Preexpnen tal cnstant (s ) Actvat n energy (J/m l) Hea t f reac tn (J/ g) Stch metr c ceffc ent V j The reactn rate cnstants are functns f temperature generally gven by the Arrhenus relatn (Levenspel, 999) E j exp T where the prme ndcates values f (6) j predcted by eq. (6), K are the pre-expnental netc cnstants fr the respectve lumps, and E are the actvatn energes f the dfferent lumps. The rate cnstants ( ), and the stchmetrc ceffcents j ( V j ) f the varus lumps are expreed as (Dagde, 9) Vg V V,, Vg (7) g V (8) V (9) 5 Vd 5, Vd d () 6 Vc 6, Vc () c g Vg, Vg () V g V 5 gd 5 V 6 gc 6 V 5 V d 5,,, g Vg () g Vgd () d g Vgc (5) c, V (6), V d (7) d 56 P a g e

6 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. 5 V the physcal prpertes f the reactng speces, d 5 Vd (8) and catalyst are presented n Table 6. s the mlecular weght f gasl, g where d s the mlecular weght f gaslne, s the mlecular weght f LPG ( ), the mlecular weght f LPG ( ), c s the mlecular weght f ce, d s the mlecular weght f dry gas, V g s the stchmetrc rat f gas-l t gaslne, V s the stchmetrc rat f gas-l t, V s the stchmetrc rat f gas-l t, V d s the stchmetrc rat f gas-l t dry gas, V c s the stchmetrc rat f gas-l t ce, V s the stchmetrc rat f gaslne t, g V g s the stchmetrc rat f gaslne t, V gd s the stchmetrc rat f gaslne t dry gas, V gc s the stchmetrc rat f gaslne t ce, V s the stchmetrc rat f t, s the stchmetrc V d rat f t dry gas, and V d s s the stchmetrc rat f t dry gas. Table shws the average mlecular weghts f the sx lumps used n the study. Table. Average mlecular weghts f the sx lumps [, ] Lump Average mlecular weght (g/ml) Gas l 86 * Gaslne g 7.8** LPG ( ) LPG ( ) 9.** 7.** Dry gas d 8. ** e c **. Prpertes f feed and prducts, and dmensns f sme cmpnents f F unt The prpertes f feed and prducts f the sx-lump catalytc cracng prce, and the dmensns f sme cmpnents f F unt, are presented n Tables and respectvely. The feedstc cmpstn s gven n Table 5, whle Table. Prpertes f feed and prducts f F [] mpnent API mpst Flw rate (g/s) Gravty n, (wt. %) Gas-l feed Fuel gas LPG LPG Gaslne Lght cycle l Bttms e Table. Dmensns f sme cmpnents f F unt [] Parameter Value (m) eactr heght.9 eactr dameter.9 yclne heght. yclne dameter.5 Dsengager heght.9 Table 5. Feedstc cmpstn [] Hydrcarbn % a Paraffns 5. Naphthenes 6. Armatcs 8.5 Table 6. Physcal prpertes f reactng speces and catalyst [] Parameter Value Vapur densty, g/m 9.5 Lqud densty, g/m 9.8 Specfc heat f gas, J/g K. Specfc heat f lqud, J/g.67 K Heat f vapurzatn, J/g 56 Bul densty f catalyst, 975 g/m Partcle sze f catalyst, m 6 75 Specfc heat capacty f. catalyst, J/g K a flwrate f catalyst 7975 frm the rser t regeneratr, g/hr 56 P a g e

7 a Fractn f Gas-l, Gaslne, and e a Fractn f LPG, LPG and Fuel Gases Fractnal yeld f Gaslne and e Fractnal yeld f LPG, LPG and Fuel Gases K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. 5. esults and Dscun Table 7 shws the cmparsn between plant data and mdel-predctns f the catalytc cracng f gas-l based n the sx-lump netc scheme, ndcatng that the mdel-predctns cmpare reasnably well wth the plant data. Table 7. mparsn between mdelpredctns and plant data f F rser-reactr Parameter Plant data delpredctn Ga-l (wt.%) Gaslne (wt.%) LPG (wt.%).7.68 LPG (wt.%) Fuel Gases (wt.%) e (wt.%) ser utlettemperature, K Fgure shws the varatns f ma fractn f gas-l and the varus prducts f the catalytc cracng prce wth the dmensnle heght f the rser-reactr, ndcatng that the ma fractn f gas-l decreases as the heght f the rser-reactr ncreases, whle the ma fractns f gaslne, LPG, fuel gas, and ce, ncrease as the rser-heght ncreases. As gas-l enters the rserreactr, t s craced nt the varus prducts as t s cnveyed up the reactr n cntact wth the catalyst. LPG Fractn LPG Fractn Fuel Gases Gas-Ol Gaslne e Dmensnle Heght f ser - eactr Fg.. Varatns f ma fractn f gas-l and prducts f catalytc cracng wth dmensnle heght f rser-reactr The rate f cracng f gas-l and the cntact tme f gas-l and catalyst, ncrease as the heght f the rser-reactr ncreases. Hence, the ma fractn f gas-l decreases frm an ntal value f unty ( = ) at the nlet f the rser-reactr t a mnmum value at the utlet f the reactr, whle the ma fractn f ndvdual prduct ncreases frm an ntal value f zer frm the nlet f the rser-reactr t a maxmum value at the utlet f the reactr. The dependence f the yeld f the varus prducts f the catalytc cracng prce n the fractnal cnversn f gas-l s shwn n Fg., ndcatng that the fractnal yeld f each prduct ncreases as the fractnal cnversn f gas-l ncreases Gaslne e LPG Fractn L P G F ractn F uel G ases Fractnal nversn f Gas-l Fg.. Dependence f yeld f prducts f catalytc cracng n fractnal cnversn f gasl Ths s a result f the cracng f gas-l t frm the varus prducts whse yelds ncrease as the cnversn f gas-l ncreases. Fgure shws the temperature prgren alng the rser-reactr, where the temperature nsde the reactr decreases frm an nlet value f abut 8K t abut 66K at the ext f the reactr. Snce the endthermc cracng reactns tae place alng the rser-reactr, and the rate f cracng ncreases wth the heght f the reactr, the heat absrbed by the cracng reactns als ncreases wth the heght f the rser-reactr whle the temperature n the rser-reactr decreases as the heght f the reactr ncreases as btaned n Fg P a g e

8 ser - eactr Temperature (K) a Fractn K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp Gas-Ol Gaslne LPG Fractn LPG Fractn Fuel Gases e Dmensnle Heght f ser - eactr Fg.. Steady-state temperature prfle alng the rser-reactr Hwever, the temperature at any pnt alng the rser-reactr des nt change wth tme whch means that the rser-reactr perates at steady-state. 5.. Senstvty Analyss A smulatn mdel can be used t ptmze plant perfrmance by chsng the ptmal set f peratng cndtns such as temperature, preure, flwrate, etc. In ths wr, the effects f nlet-temperature f gas-l, catalyst-t-gas l rat, and ma flwrate f gas-l, n the yeld f prducts and utlet-temperature f the rser-reactr are nvestgated. Fgure 5 shws the effect f nlettemperature f gas-l n the ma fractns f gasl and prducts f the catalytc cracng prce, ndcatng that the ma fractns f gas-l and prducts f the catalytc cracng prce are practcally ndependent f the nlet-temperature f gas-l untl 9K, beynd whch, the ma fractns f the prducts decrease sharply whle the ma fractn f gas-l ncreases tremendusly. Inspectn f Fgs.,, and 5 reveals that the lnear sectn f the prfle fr gas-l n Fg. 5 crrespnds t the mnmum ma fractn f gasl, whle the lnear part f the prfles (Fg. 5) fr the varus prducts f the cracng prce crrespnds t the maxmum ma fractn f the respectve prducts. Ths suggests that ne r mre f the smulated peratng cndtns f the rserreactr (e.g. catalyst-t-gas l rat f 6.5, gas-l ma flwrate f 67.8 g/s; nlet-temperature f gasl f 55K) gve(s) maxmum cnversn f gas-l wth crrespndng maxmum yeld f prducts Inlet Temperature f Gas-l (K) Fg. 5. Varatns f ma fractn f gas-l and prducts f catalytc cracng wth nlet-temperature When the cnversn f gas-l s maxmum, the rate f cracng f gas-l and the quantty f heat absrbed by the endthermc cracng reactns are als maxmum, s that any ncrease n the nlet-temperature f gas-l up t 9K des affect the maxmum cnversn f gasl. Beynd gas-l nlet-temperature f 9K, the catalyst becmes deactvated and the rate f cracng decreases greatly, s that the quantty (and ma fractn) f uncraced gas-l n the rserreactr ncreases whle the yeld (and ma fractn) f the prducts decreases accrdngly as btaned n Fg. 5. Thus, hgh nlet-temperature f gas-l up t 9K and abve d nt favur the catalytc cracng prce as t can cause permanent catalyst deactvatn and cnsequent reductn n the cnversn f gas-l and yeld f prducts. Fgure 6 shws the effect f nlettemperature f gas-l n the utlet-temperature f the rser-reactr, ndcatng that the utlettemperature f the rser-reactr ncreases nearly prprtnately as the nlet-temperature f gas-l ncreases up t 9K; thereafter, the utlettemperature f the rser-reactr rses sharply as the nlet-temperature f gas-l ncreases. The nearly prprtnate ncrease n the rser utlet-temperature as the nlet-temperature f gas-l ncreases up t 9K s cnsstent wth Fg. 5. Snce the rate f cracng f gas-l s maxmum at the smulated peratng cndtns as explaned n the precedng sectn fr Fg. 5, t means the quantty f heat absrbed by the endthermc cracng reactns s als maxmum and mre heat cannt be absrbed by the cracng reactns. 56 P a g e

9 a Fractn ser - eactr Outlet Temperature (K) ser - eactr Outlet Temperature (K) K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. Fg. 7. Varatns f ma fractn f gas-l and prducts f catalytc cracng wth catalyst-t-gas l rat Inlet Temperature f Gas-l (K) Fg. 6. Varatn f rser-reactr utlettemperature wth nlet-temperature f gas-l Therefre, any ncrease n the nlettemperature f gas-l results n a crrespndng ncrease n the rser-temperature whch s manfested n the utlet-temperature f the rserreactr as shwn n Fg. 6 up t gas-l nlettemperature f 9K. Beynd nlet-temperature f gas-l f 9K, the catalyst becmes deactvated and the rate f cracng f gas-l decreases s that the quantty f uncraced gas-l n the rser-reactr ncreases as explaned abve. It s the extra heat n the ncreased quantty f uncraced gas-l caused by the reduced rate f the cracng reactns that shts up the rser-temperature and/r utlettemperature f the rser-reactr fr nlet-temperature f gas-l greater than 9K as btaned n Fg. 6. Fgure 7 shws the effect f catalyst-t-gas l rat (TO) n the ma fractns f gas-l and the prducts f the catalytc cracng prce. The ma fractn f gas-l decreases slghtly t a mnmum value as the TO ncreases frm t, and then remans apprxmately cnstant at the mnmum value fr TO. The slght decrease n the ma fractn f gas-l fr TO s a result f ts cnversn t prducts, wth the rate f cnversn f gas-l ncreasng as TO ncreases frm t Gas-Ol LPG Fractn Fuel Gases Gaslne LPG Fractn e 5 5 atalyst-t-gas l at (TO) Accrdngly, the ma fractn f all the prducts ncreases slghtly t a maxmum value as the TO ncreases frm t ; thereafter, the ma fractn f each prduct remans cnstant at the maxmum value fr TO. Increasng the TO means ncreasng the ma flwrate f catalyst enterng the reactr wth respect t the ma flwrate f gas-l. Wth mre catalyst avalable n the rser-reactr, the number f actve stes f catalyst fr the cracng reactns als ncreases resultng n ncreased cnversn f gas-l t prducts, but the catalyst spends le tme n the rser-reactr at hgh TO than at lw TO. Thus, a mnmum value f TO s recmmended fr maxmum cnversn f gas-l, and the value f TO = 6.5 used n the present smulatns s cnsstent wth Fg. 7 whch als cnfrms the results n Fg. 5. Fgure 8 shws the effect f catalyst-t-gas l rat n the utlet-temperature f the rserreactr, ndcatng that the utlet-temperature f the rser-reactr decreases slghtly frm abut 668K t a mnmum value f 66K as the TO ncreases frm t ; thereafter, the rser-reactr utlettemperature remans practcally cnstant at the mnmum value fr TO atalyst-t-gas l at (TO) Fg. 8. Varatn f rser-reactr utlettemperature wth catalyst-t-gas l rat The slght decrease n rser-reactr utlettemperature fr TO s due t the heat absrbed by the endthermc cracng reactns f gas-l and s cnsstent wth Fg. 7 fr the same range f TO. Fr TO, the rate f cracng f gas-l s maxmum and remans cnstant at the maxmum value. Wth maxmum rate f cracng f gas-l, the quantty f heat absrbed by the 565 P a g e

10 ser - eactr Outlet Temperature (K) a Fractn K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. endthermc cracng reactns s als maxmum, resultng n a cnstant utlet temperature f the rser-reactr fr TO as btaned n Fg. 8. Fgure 9 shws the effect f ma flwrate f gas-l n ts ma fractn and ma fractn f prducts f the catalytc cracng prce., ndcatng that the ma fractn f gaslne ncreases t a maxmum value f abut.6 crrespndng t ma flwrate f gas-l f abut 5 g/s; thereafter, the ma fractn f gaslne decreases as the ma flwrate f gas-l ncreases Gas-Ol Gaslne LPG Fractn LPG Fractn Fuel Gases e gaslne and ther prducts) as the ma flwrate f gas-l ncreases, ndcates that the verall rate f the endthermc catalytc cracng reactns decreases as the ma flwrate f gas-l ncreases s that the quantty (and ma fractn) f uncraced gas-l n the rser-reactr ncreases as the ma flwrate f gas-l ncreases as btaned n Fg. 9. (It s wrthy f nte frm Fg. 9 that althugh the rate f cracng f gas-l t gaslne ncreases t sme extent as the ma flwrate f gas-l ncreases, the rates f all the ther cracng reactns n the sx-lump netc mdel (Fg. ) decrease as the ma flwrate f gas-l ncreases; ths justfes the decrease n the verall rate f the endthermc cracng reactns as the ma flwrate f gas-l ncreases). Fgure shws the effect f ma flwrate f gas-l n the rser-reactr utlettemperature, ndcatng that the rser-reactr utlettemperature ncreases as the ma flwrate f gasl ncreases a Flwrate f Gas-l (Kg/s) Fg. 9. Varatn f ma fractn f gas-l and prducts f catalytc cracng wth ma flwrate f gas-l The ma fractn f gas-l ncreases nearly lnearly as ts ma flwrate ncreases, whle the ma fractns f the ther prducts (except gaslne) decrease as the ma flwrate f gas-l ncreases. We nte that TO = 6.5 was used n Fgs. ; therefre, ncreasng the ma flwrate f nly gas-l whle that f the catalyst remans cnstant, means decreasng the TO wth the effect that the cntact tme f gas-l and catalyst decreases. Thus, as the ma flwrate f gas-l ncreases, the cntact tme f gas-l and catalyst decreases, and the rate f the endthermc cracng reactns and yeld f prducts als decrease, whch s nt fully satsfed by nly gaslne (see Fg. 9). The ntal ncrease n the ma fractn f gaslne as the ma flwrate f gas-l ncreases may partly be attrbuted t () a balance between the reduced cntact tme f catalyst and gas-l, and the ncreased quantty f gas-l enterng the rserreactr per unt tme, s that the rate f cracng f gas-l ncreases, and () the effect f zelte catalyst mst ften used n F whch exhbts the unque prperty f selectvely enhancng the yeld f gaslne. Beynd ma flwrate f gas-l f 5 g/s, the cntact tme f gas-l and catalyst becmes t shrt t sustan effcent cracng f gas-l, s the ma fractn f gaslne decreases. On the ther hand, the cntnuus ncrease n the ma fractn f gas-l (despte ts cnversn t a Flwrate f Gas-l (Kg/s) Fg.. Varatn f rser-reactr utlettemperature wth ma flwrate f gas-l It may be neceary t ndcate that the ttal quantty f heat n the rser-reactr s suppled partly by the regenerated catalyst frm the regeneratr and partly by the gas-l enterng the rser-reactr. Snce gas-l enters the rser-reactr at a cnstant temperature, bth the quantty f heat generated by nly gas-l n the rser-reactr and the ttal quantty f heat n the reactr ncrease as the ma flwrate f gas-l ncreases. Gven that the verall rate f the endthermc cracng reactns tang place n the rser-reactr decreases as the ma flwrate f gas-l ncreases, the ttal quantty f heat absrbed by catalytc cracng reactns als decreases as the ma flwrate f gas-l ncreases, such that the rser-temperature and/r utlettemperature f the rser-reactr ncreases as the ma flwrate f gas-l ncreases as btaned n Fg P a g e

11 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. 6. nclusn A sx-lump netc scheme whch descrbes the catalytc cracng reactns tang place n an adabatc plug-flw rserreactr has been presented. The advantage f the sx-lump netc mdel s that t allws ndependent predctns f s and s. It s shwn that catalyst-t-gas l rat, nlettemperature f gas-l, and ma flwrate f gas-l, have sgnfcant effects n the peratn f the rserreactr, and a mnmum catalyst-t-gas l rat f s requred fr maxmum cnversn f gas-l. Smulatn results presented n the study usng catalyst-t-gas l rat f 6.5, nlet-temperature f gas-l f 55K, and ma flwrate f gas-l f 67.8 g/s, gve yelds f 5.8% gaslne, 6.% s,.68% s, 5.% fuel gas, 5.% ce, and 6.66% f uncnverted gas-l. L z characterstc dmensn f Zelte crystallte used n eq. (), m mlecular weght f lump used n eqs. (7)-(8), g/ml r - rate f cracng speces, s unversal gas cnstant, J/ml K t tme, s T abslute temperature, K T reference temperature, K T V ref temperature f rser-reactr, K j defned n eqs. (7)-(8). y ma fractn f cmpnent dmensnle heght f rser-reactr. Z stchmetrc rat f lump t lump j Nmenclature A cr-sectnal area f the rser-reactr, m mlar cncentratn f lump, ml/m p specfc heat capacty f the catalyst n the cat rser-reactr, J/g K p specfc heat capacty f gas-l n the rser-reactr, J/g K TO catalyst-t-gas l rat D eff effectve dffusvty f gas-l thrugh the catalyst, m /s D p pre-expnental factr fr dffusn used n eq. (6), m /s E D actvatn energy fr dffusn used n eq. (6), J/ml F ma flwrate f gas-l, g/s F cat ma flwrate f catalyst, g/s h mdfed Thele mdulus used n eq. (). h mdfed Thele mdulus fr gas-l used n eq. (5). d catalysts decay ceffcent used n eq. (8), - s catalyst decay pre-expnental netc d - factr used n eq. (8), s ntrnsc rate cnstants f speces, m /g j ml s r m 6 /g ml s pre-expnental (r Arrhenus) factr ml s L used n eq. (6), m /g ml s r m 6 /g heght f rser-reactr, m Gree Letters ext catalyst-specfc external surface area used n eq. (), m - average vd fractn n the rser-reactr ma densty f gas-l, g/m ma densty f catalyst, g/m cat ma densty f lump, g/m T ttal ma densty f all lumps defned after eq. (6), g/m H j heat f reactn fr cracng lump t j, J/ml catalyst deactvatn functn. dmensnle temperature f rser-reactr vlumetrc flwrate f gas-l used n eq. (7), m /s effectvene factr eferences [] Wlsn, J. W. Flud atalytc racng Technlgy and Operatn, Penn Well Bs, Lndn (997). [] Ahar J. S., A. Farsh and K. Frsat, A athematcal delng f the ser eactr n Industral F Unt. Petrleum and al, 5(), 5 (8). [] Xu, O, S. U. Hng Ye,. U. Sheng Jng and. H. U. Jan, 7-Lump Knetc del fr esdual Ol atalytc racng. J. Zhejang Unv. Sc. A, 7(), 9 9 (6). [] Al-Sabaw,., J. A. Atas, and H. I. de Lasa, Knetc delng f atalytc racng f Gas-Ol Feedstcs: eactn 567 P a g e

12 K. K. Dagde, Y. T. Puyate / Internatnal Jurnal f Engneerng esearch and Applcatns (IJEA) ISSN: Vl., Iue 6, Nvember- December, pp. and Dffusn Phenmena. Ind. Eng. hem. es., 5, (6). [5] Weeman, V. W. and D.. Nace, Knetcs f atalytc racng Selectvty n Fxed, vng, and Flud Bed eactrs. AIhE J., 6(), 97- (97). [6] Lee, L. S., V. W. hen and T. N. Huang, Fur-Lump Knetc del fr atalytc racng Prce. anad. J. hem. Eng., 67, 65 6 (989). [7] Wang, L. Y., B. L. Yang and Z. W. Wang, Lumps and Knetcs fr Secndary eactns n atalytcally raced Gaslne. hem. Eng. J., 9( ), 9 (5). [8] Ancheyta-Juarez, J., L. F. Isunza, E. A. drguez and J... ayrga, A Strategy fr Knetc Parameter Estmatn n the Flud atalytc racng Prce. Amer. hem. Sc., 6(), (997). [9] Hagelberg, P., I. Els, J. Hltunen, K. Lpanene, V.. Nem, J. Attama and A.O.I. Krause, Knetc f atalytc racng wth Shrt ntact Tmes. Appl. atalyss A,, 7-8(). [] Obh, E. O., J. G. Apa and K. K. Dagde, Applcatn f the Three-Lump Knetc del fr the atalytc racng f Gas- Ol n a Fludzed Bed eactr. Inter. J. Sc. & Technl., (&), 9-5 (5). [] Obh, E. O., J. G. Apa, K. K. Dagde and D. O. Njbuenwu, Applcatn f the Fur-Lump Knetc del fr the Smulatn f a Fludzed Bed eactr fr atalytc racng f Gas-Ol. J. Eng., 6(), 7 (6). [] Obh, E. O. and J. G. Apa, dellng f a Flud atalytc (F) ser eactr: The Fur-Lump del. J. delng, Desgn and gt. Eng. Sys., (), 9 5 (). [] Dagde, K. K., J. G. Apa, Y. T. Puyate and E. O. Obh, Fve-Lump Knetc del fr Flud atalytc racng f Gas-Ol n a Fludzed Bed eactr. J. Ngeran Sc. hem. Engrs., (&), 9 (8). [] Ancheyta, J. and. Stel, Knetc dellng f Vacuum Gas-Ol atalytc racng. J. excan hem. Sc., 6(), 8 (). [5] Dagde, K. K. Develpment f del Equatns fr the Smulatn f Flud atalytc racng eactrs, Ph.D. Thess, Department f hemcal/petrchemcal Engneerng, vers State Unversty f Scence and Technlgy, Prt Harcurt (9). [6] Levenspel, O. hemcal eactn Engneerng, rd Ed., Jhn Wley and Sns, New Yr (999), pp [7] Tnett, G., J. A., Atas and H. I. de Lasa, F atalysts wth Dfferent Zelte rytallte Szes: Actvty, Structural Prpertes, and eactvty. Appl. atalyss A,, 9-5 (). [8] uthven, D.. Prncples f Adsrptn and Adsrptn Prcees, Jhn Wlley, New Yr (98). [9] Al, H., S. han and J. P. rru, delng and ntrl f a ser Type Flud atalytc racng (F) Unt. Trans. Inst. hem. Engrs., 75, (997). [] NPH. New Prt Harcurt efnery mpany: Tranng Prject Specfc fr Senr Staff, Area, Prce Descrptn, mernt (987). [] en, J., H. X. Weng and F. Y. Lu, Study n mpstn and Structure f Heavy Ol. Petrleum Prceng, (9), 56 6 (99). [] Pext, F.. and J. L. eders, eactn n ult-ndexed ntnuus xtures: atalytc racng f Petrleum Fractns. AIhE J., 7(), (). 568 P a g e

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

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

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

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

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

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

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

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

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

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

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

_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

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

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

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

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

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products modelng of equlbrum and dynamc mult-component adsorpton n a two-layered fxed bed for purfcaton of hydrogen from methane reformng products Mohammad A. Ebrahm, Mahmood R. G. Arsalan, Shohreh Fatem * Laboratory

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

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

Thermodynamics of Materials

Thermodynamics of Materials Thermdynamcs f Materals 14th Lecture 007. 4. 8 (Mnday) FUGACITY dg = Vd SdT dg = Vd at cnstant T Fr an deal gas dg = (RT/)d = RT dln Ths s true fr deal gases nly, but t wuld be nce t have a smlar frm fr

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

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

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

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

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

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

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

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

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

SELECTION OF MODEL PARAMETERS OF BIOGAS IC ENGINE. Karol Cupiał, Grzegorz Katolik

SELECTION OF MODEL PARAMETERS OF BIOGAS IC ENGINE. Karol Cupiał, Grzegorz Katolik TEKA Km. Mt. Energ. Rln., 2006, 6A, 32 38 SELECTION OF MODEL PARAMETERS OF BIOGAS IC ENGINE Karl Cupał, Grzegrz Katlk Insttute f Internal Cmbustn Engnes and Cntrl Engneerng Techncal Unversty f Częstchwa

More information

Linear Plus Linear Fractional Capacitated Transportation Problem with Restricted Flow

Linear Plus Linear Fractional Capacitated Transportation Problem with Restricted Flow Amercan urnal f Operatns Research,,, 58-588 Publshed Onlne Nvember (http://www.scrp.rg/urnal/ar) http://dx.d.rg/.46/ar..655 Lnear Plus Lnear Fractnal Capactated Transprtatn Prblem wth Restrcted Flw Kavta

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

15-69C Under the conditions of complete combustion with stoichiometric amount of air.

15-69C Under the conditions of complete combustion with stoichiometric amount of air. 15-43 Adabatc Flame emperature 15-68C Fr the case f stchmetrc amunt f pure xy snce we have the same amunt f chemcal energy released but a smaller amunt f mass t absrb t. 15-69C Under the cndtns f cmplete

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

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

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

Journal of Separation Science and Engineering Vol. 2, No. 2,, pp Wang-Henke MESH

Journal of Separation Science and Engineering Vol. 2, No. 2,, pp Wang-Henke MESH Jurnal f Separatn Scence and ngneerng l. 2, N. 2,, pp.2-3 s_asad@pnu.ac.r Wang-Henke MSH Pntnen mundsn Henke Wang Hlland SR uca Srdhar perena uca Srdhar Wang- Henke P Wang-Henke 6 Mdfed theta-methd 7 Sum

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

Tubular Flow with Laminar Flow (CHE 512) M.P. Dudukovic Chemical Reaction Engineering Laboratory (CREL), Washington University, St.

Tubular Flow with Laminar Flow (CHE 512) M.P. Dudukovic Chemical Reaction Engineering Laboratory (CREL), Washington University, St. Tubular Flw wth Lamnar Flw (CHE 5) M.P. Dudukvc Chemcal Reactn Engneerng Labratry (CREL), Washngtn Unversty, St. Lus, MO 4. TUBULAR REACTORS WITH LAMINAR FLOW Tubular reactrs n whch hmgeneus reactns are

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

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

C. Ozgur Colpan Ibrahim Dincer Feridun Hamdullahpur

C. Ozgur Colpan Ibrahim Dincer Feridun Hamdullahpur THERMODYNAMIC MODELING O DIRECT INTERNAL REORMING PLANAR SOLID OXIDE UEL CELLS WITH ANODE RECIRCULATION C. Ozgur Clpan Ibrahm Dncer erdun Hamdullahpur OUTLINE INTRODUCTION TO SOCs Advantages, dsadvantages

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

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

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

Exploiting vector space properties for the global optimization of process networks

Exploiting vector space properties for the global optimization of process networks Exptng vectr space prpertes fr the gbal ptmzatn f prcess netwrks Juan ab Ruz Ignac Grssmann Enterprse Wde Optmzatn Meetng March 00 Mtvatn - The ptmzatn f prcess netwrks s ne f the mst frequent prblems

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

Conservation of Energy

Conservation of Energy Cnservatn f Energy Equpment DataStud, ruler 2 meters lng, 6 n ruler, heavy duty bench clamp at crner f lab bench, 90 cm rd clamped vertcally t bench clamp, 2 duble clamps, 40 cm rd clamped hrzntally t

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

ChE 471: LECTURE 4 Fall 2003

ChE 471: LECTURE 4 Fall 2003 ChE 47: LECTURE 4 Fall 003 IDEL RECTORS One f the key gals f chemical reactin engineering is t quantify the relatinship between prductin rate, reactr size, reactin kinetics and selected perating cnditins.

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

A method of constructing rock-analysis diagrams a statistical basks.

A method of constructing rock-analysis diagrams a statistical basks. 130 A methd f cnstructng rck-analyss dagrams a statstcal basks. 0T~ By W. ALF~.D ll~ch).ra)so.~, ~.Se., B.Se. (Eng.), F.G.S. Lecturer n Petrlgy, Unversty Cllege, Nttngham. [Read January 18, 1921.] D R.

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

More information

4DVAR, according to the name, is a four-dimensional variational method.

4DVAR, according to the name, is a four-dimensional variational method. 4D-Varatnal Data Assmlatn (4D-Var) 4DVAR, accrdng t the name, s a fur-dmensnal varatnal methd. 4D-Var s actually a smple generalzatn f 3D-Var fr bservatns that are dstrbuted n tme. he equatns are the same,

More information

A Note on the Linear Programming Sensitivity. Analysis of Specification Constraints. in Blending Problems

A Note on the Linear Programming Sensitivity. Analysis of Specification Constraints. in Blending Problems Aled Mathematcal Scences, Vl. 2, 2008, n. 5, 241-248 A Nte n the Lnear Prgrammng Senstvty Analyss f Secfcatn Cnstrants n Blendng Prblems Umt Anc Callway Schl f Busness and Accuntancy Wae Frest Unversty,

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

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

Module 7: Solved Problems

Module 7: Solved Problems Mdule 7: Slved Prblems 1 A tn-walled nentr tube eat exanger f 019-m lengt s t be used t eat denzed water frm 40 t 60 at a flw rate f 5 kg/s te denzed water flws trug te nner tube f 30-mm dameter wle t

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

An Extended Regular Solution Model with Local Volume Fraction

An Extended Regular Solution Model with Local Volume Fraction () An Etended Regular Slutn Mdel wth cal Vlume Fractn Shgetsh KOBUCHI, Ken ISHIGE (Department f Enrnmental Scence and Engneerng, Graduate Schl f Scence and Engneerng, Yamaguch Unersty) Setsuk YONEZAWA

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

Ph.D. Qualifying Examination in Kinetics and Reactor Design

Ph.D. Qualifying Examination in Kinetics and Reactor Design Knetcs and Reactor Desgn Ph.D.Qualfyng Examnaton January 2006 Instructons Ph.D. Qualfyng Examnaton n Knetcs and Reactor Desgn January 2006 Unversty of Texas at Austn Department of Chemcal Engneerng 1.

More information

Faculty of Engineering

Faculty of Engineering Faculty f Engneerng DEPARTMENT f ELECTRICAL AND ELECTRONIC ENGINEERING EEE 223 Crcut Thery I Instructrs: M. K. Uygurğlu E. Erdl Fnal EXAMINATION June 20, 2003 Duratn : 120 mnutes Number f Prblems: 6 Gd

More information

Phys 344 Ch 5 Lect 4 Feb 28 th,

Phys 344 Ch 5 Lect 4 Feb 28 th, hys 44 Ch 5 Lect 4 Feb 8 th, 009 1 Wed /4 Fr /6 Mn /9 Wed /11 Fr / 1 55 Dlute Slutn 56 Chemcal Equlbrum Revew Exam (C 107 S 60, 61 Bltzmann Statstcs Bnus: hys Sr hess resentatns @ 4pm HW17: 7,76,8 HW18:8,84,86,88,89,91

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

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

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

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

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS

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

Mathematical Modeling of an Industrial Naphtha Reformer with Three Adiabatic Reactors in Series

Mathematical Modeling of an Industrial Naphtha Reformer with Three Adiabatic Reactors in Series Iran. J. Chem. Chem. Eng. Research Note Vol. 28, No. 3, 2009 Mathematcal Modelng of an Industral Naphtha Reformer wth Three Adabatc Reactors n Seres Fazel, Al; Fatem, Shohreh* + ; Mahdavan, Mohammad; Ghaee,

More information

Prediction of Thermal Conductivity of Aligned Short Fibre Composites with Different Fibre Aspect Ratios

Prediction of Thermal Conductivity of Aligned Short Fibre Composites with Different Fibre Aspect Ratios Predctn f Theral Cnductvty f Algned Shrt Fbre Cpstes wth Dfferent Fbre Aspect Rats Predctn f Theral Cnductvty f Algned Shrt Fbre Cpstes wth Dfferent Fbre Aspect Rats Jae-Kn Lee Schl f Mechancal and Auttve

More information

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review) CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal

More information

Problem Set 5 Solutions - McQuarrie Problems 3.20 MIT Dr. Anton Van Der Ven

Problem Set 5 Solutions - McQuarrie Problems 3.20 MIT Dr. Anton Van Der Ven Prblem Set 5 Slutns - McQuarre Prblems 3.0 MIT Dr. Antn Van Der Ven Fall Fall 003 001 Prblem 3-4 We have t derve the thermdynamc prpertes f an deal mnatmc gas frm the fllwng: = e q 3 m = e and q = V s

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

Design Equations. ν ij r i V R. ν ij r i. Q n components. = Q f c jf Qc j + Continuous Stirred Tank Reactor (steady-state and constant phase)

Design Equations. ν ij r i V R. ν ij r i. Q n components. = Q f c jf Qc j + Continuous Stirred Tank Reactor (steady-state and constant phase) Desgn Equatons Batch Reactor d(v R c j ) dt = ν j r V R n dt dt = UA(T a T) r H R V R ncomponents V R c j C pj j Plug Flow Reactor d(qc j ) dv = ν j r 2 dt dv = R U(T a T) n r H R Q n components j c j

More information

Lucas Imperfect Information Model

Lucas Imperfect Information Model Lucas Imerfect Infrmatn Mdel 93 Lucas Imerfect Infrmatn Mdel The Lucas mdel was the frst f the mdern, mcrfundatns mdels f aggregate suly and macrecnmcs It bult drectly n the Fredman-Phels analyss f the

More information

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics Chapters 9 and 35 Thermchemistry and Chemical Thermdynamics 1 Cpyright (c) 011 by Michael A. Janusa, PhD. All rights reserved. Thermchemistry Thermchemistry is the study f the energy effects that accmpany

More information

Thermodynamics Partial Outline of Topics

Thermodynamics Partial Outline of Topics Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)

More information

lecture 5: Nucleophilic Substitution Reactions

lecture 5: Nucleophilic Substitution Reactions lecture 5: Nuclephilic Substitutin Reactins Substitutin unimlecular (SN1): substitutin nuclephilic, unimlecular. It is first rder. The rate is dependent upn ne mlecule, that is the substrate, t frm the

More information

(element) But, we do NOT know G!!! Correct, but not applicable! Free Energy Problems: o r. products. reactants. o f. reactants.

(element) But, we do NOT know G!!! Correct, but not applicable! Free Energy Problems: o r. products. reactants. o f. reactants. SANDARD fr hemcal Rxns prducts G p G reactants r But, we d NO knw G!!! rrect, but nt applcable! prducts G f G reactants f f (element) 0 f standard Gbbs free energy f frmatn Free Energy Prblems: 5. Prf.

More information

Electrical double layer: revisit based on boundary conditions

Electrical double layer: revisit based on boundary conditions Electrcal double layer: revst based on boundary condtons Jong U. Km Department of Electrcal and Computer Engneerng, Texas A&M Unversty College Staton, TX 77843-318, USA Abstract The electrcal double layer

More information

CHEMICAL ENGINEERING

CHEMICAL ENGINEERING Postal Correspondence GATE & PSUs -MT To Buy Postal Correspondence Packages call at 0-9990657855 1 TABLE OF CONTENT S. No. Ttle Page no. 1. Introducton 3 2. Dffuson 10 3. Dryng and Humdfcaton 24 4. Absorpton

More information

Physics 107 HOMEWORK ASSIGNMENT #20

Physics 107 HOMEWORK ASSIGNMENT #20 Physcs 107 HOMEWORK ASSIGNMENT #0 Cutnell & Jhnsn, 7 th etn Chapter 6: Prblems 5, 7, 74, 104, 114 *5 Cncept Smulatn 6.4 prves the ptn f explrng the ray agram that apples t ths prblem. The stance between

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

A brief overview of the principles of thermobarometry Cin-Ty Lee (2009)

A brief overview of the principles of thermobarometry Cin-Ty Lee (2009) A bref vervew f the prncples f thermbarmetry Cn-y Lee (2009) Hmgeneus tem Fr a ne phase tem (hmgeneus tem) characterzed by a fxed cmpstn, the state varable knwn as Gbbs Free energy G s defned as fllws:

More information

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st EN40: Dynamcs and bratons Homework 4: Work, Energy and Lnear Momentum Due Frday March 1 st School of Engneerng Brown Unversty 1. The fgure (from ths publcaton) shows the energy per unt area requred to

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

Monin Obukhov Similarity and Local-Free-Convection Scaling in the Atmospheric Boundary Layer Using Matched Asymptotic Expansions

Monin Obukhov Similarity and Local-Free-Convection Scaling in the Atmospheric Boundary Layer Using Matched Asymptotic Expansions OCTOBER 08 T O N G A N D D I N G 369 Mnn Obukhv Smlarty cal-free-cnvectn Scalng n the Atmspherc Bundary ayer Usng Matched Asympttc Expansns CHENNING TONG AND MENGJIE DING Department f Mechancal Engneerng

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

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,

More information

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review Review Accrding t the nd law f Thermdynamics, a prcess is spntaneus if S universe = S system + S surrundings > 0 Even thugh S system

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

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

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

Modelling of Two Stage Gasification of Waste Biomass

Modelling of Two Stage Gasification of Waste Biomass 1465 A publcatn f VOL. 61, 217 CHEMICAL ENGINEERING TRANSACTIONS Guest Edtrs: Petar S Varbanv, Rngxn Su, Hn Lng Lam, Xa Lu, Jří J Klemeš Cpyrght 217, AIDIC Servz S.r.l. ISBN 978-88-9568-51-8; ISSN 2283-9216

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

SPH3U1 Lesson 06 Kinematics

SPH3U1 Lesson 06 Kinematics PROJECTILE MOTION LEARNING GOALS Students will: Describe the mtin f an bject thrwn at arbitrary angles thrugh the air. Describe the hrizntal and vertical mtins f a prjectile. Slve prjectile mtin prblems.

More information

Electric Current and Resistance

Electric Current and Resistance Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current

More information

Fall 2010 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. (n.b. for now, we do not require that k. vectors as a k 1 matrix: ( )

Fall 2010 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. (n.b. for now, we do not require that k. vectors as a k 1 matrix: ( ) Fall 00 Analyss f Epermental Measrements B. Esensten/rev. S. Errede Let s nvestgate the effect f a change f varables n the real & symmetrc cvarance matr aa the varance matr aa the errr matr V [ ] ( )(

More information