CRITICAL COMPARISON OF MASS TRANSFER MODELS FOR INTERNALLY CONTROLLED SCF EXTRACTION OF SOLID SUBSTRATES

Size: px
Start display at page:

Download "CRITICAL COMPARISON OF MASS TRANSFER MODELS FOR INTERNALLY CONTROLLED SCF EXTRACTION OF SOLID SUBSTRATES"

Transcription

1 CRITICAL COMPARISON OF MASS TRANSFER MODELS FOR INTERNALLY CONTROLLED SCF EXTRACTION OF SOLID SUBSTRATES Joé Manul dl Vall,* & Edgar Uquich Pont. Univ. Católica d Chil, Avda. Vicuña Macknna 486, Macul, Santiago, Chil. Univ. d La Frontra, Avda. Francico Salazar 45, Tmuco, Chil. * Fax: ( dlvall@ing.uc.cl. Thr modl or th urcritical luid (SCF xtraction o olid with dirnt intrnal ma tranr mchanim wr critically comard in thi work. Intrnal ma tranr hyothi includd: tranint diuion; linar driving orc (LDF; and dortiondiolution-diuion (DDD. A nitivity analyi wa rormd on th bai o Biot numbr (Bi ratio btwn intrnal and xtrnal ma tranr ritanc and charactritic xtrnal xtraction tim (τ ratio btwn th xtrnal ma tranr ritanc and ridnc tim o th SCF in th xtractor. Th ngativ ct o a -ordr o magnitud incra in Bi ( in dcraing xtraction rat wa quivalnt to that o a on-ordr o magnitud incra in τ (.. Th LDF aroximation could b ud or th two othr modl undr analyi i th total comoundd oroity o th bd (ε and articl (ε wa conidrd, a modl-dndnt dinition o Bi wa utilizd (Bik R/D K or Fickan and LDF modl, Bi k R/D or DDD modl, and th valu o Bi wr <. Th LDF modl wa alid to litratur data on ntial oil xtraction rom lavndr lowr and nnyroyal lav with urcritical carbon dioxid (SC-CO at bar and 5 C. Analyi o intrtitial olvnt vlocity ct uggtd that th convctiv ma tranr coicint in th SCF i mallr than rdictd by dimnionl corrlation or ackd bd orating with SCF. INTRODUCTION Ma tranr aramtr drivd rom data gnratd in a laboratory or ilot lant unit can aid in th caling-u and dign o indutrial SCF xtraction roc or olid ubtrat []. Paramtr valuation, in turn, dnd on th imlmntation o aroriat ma tranr modl or ackd bd. Unortunatly, inc modl with dirnt hyothi about th limiting ma tranr mchanim can dcrib tyical cumulativ xtraction lot (rcovrd olut vru xtraction tim or botanical ubtrat tratd with SCF, it i diicult to dicriminat btwn modl bad on thir itting caabiliti or xrimntal data []. In thi work, w xandd a rviou contribution by conidring altrnativ intrnal ma tranr mchanim rood in cializd litratur. Hyoth includd Fickan [] or arabolic concntration roil o ridual olut in th olid matrix [], and a dortiondiolution-diuion mchanim [3]. MATHEMATICAL MODELS Fickan modl. Thi corrond to th gnral modl o dl Vall t al. []. A dirntial ma balanc quation wa writtn or th SCF urrounding hrical articl o olid ubtrat in a ackd bd (qn.. Th lux o olut tranrrd rom th olid to th SCF (J wa timatd uing quation, which aum a contant artition coicint o udo-olut (KC / C btwn th olid matrix and SCF. Equation 3 rrnt olut *

2 diuion within th olid articl, and inally, quation 4a- rrnt th initial and boundary condition o th ytm. ε + u J z ε ( 3 k C r R, J C R K ( C D + r (3 C (4a C z, t (4b C r, Co (4c r, D r R, k C r R, K C LDF modl. Ma balanc quation ali in thi ca alo. Howvr, whn th concntration roil o ridual olut in th olid matrix i aumd to b arabolic, dinition and dirntial quation 3 can b rlacd by quation 5 and 6, rctivly []. In thi ca only avrag olut concntration in th olid matrix ( C ar o intrt. Initial condition 4a and boundary condition 4b wr maintaind in thi ca, and initial/boundary condition 4c- wr rlacd by quation 7. 5 k DK C J C k R + 5DKR K (5 J (6 C Co (7 DDD modl. Thi modl wa dcribd by in dtail by Goto t al. [3]. Ma balanc quation ali, but a ditinction i mad in thi ca btwn th olut bound to th olid matrix (C and in it or (C, which ar rlatd by dortion kintic. Howvr, it wa aumd that quilibrium i tablihd intantanouly in th or du to rlativly at * dortion, which can b charactrizd by a contant artition coicint o olut (KC / C btwn th olid matrix and luid ha within th or. Undr th aumtion, dinition and dirntial quation 3 wr rlacd by quation 8 and 9, rctivly. Initial condition 4a and boundary condition 4b wr alo maintaind in thi ca, but initial/boundary condition 4c- wr rlacd by quation a-c. 3 k J ( C C (8 r R, R (4d (4

3 ε r, C C D r, D + K( ε o r R, k C + r ( C C r R, (9 (a (b (c SENSITIVITY ANALYSIS Th Fickan and LDF modl wr r-writtn in trm o a dimnionl tim [ (t u/h ], axial oition [ ξ (z/h ], radial oition [ δ (r/r ], and olut concntration in th SCF [ Y (K C /C o ] and olid ha [ X (C /C o ; X ( C /C o ]. On th on othr hand, dimnionl concntration or th DDD modl wr r-dind a: YC /C o, or th SCF ha; Y C /C o, or th luid ha within th or; and XC /C o, or th olid ha, whr C o K C o /K and K ε +K(-ε. Tabl ummariz th dimnionl dirntial ma balanc quation, initial condition, and boundary condition or th two ha and th thr modl. Clo xamination uggt that th olution o th dirntial quation in Tabl dnd on th artition o olut btwn th ha (K, K, bd and articl oroity (ε, ε and two dimnionl aramtr, namly: i Biot numbr (Bik R/D K or Fickan and LDF Bi k R/D or DDD modl, which rrnt th ratio btwn intrnal and xtrnal modl, ma tranr ritanc; and, ii charactritic xtrnal xtraction tim (τ u/k a H, whr a 3/R, which rrnt th ratio btwn th xtrnal ritanc to ma tranr and th ridnc tim o th SCF in th xtractor. A nitivity analyi wa rormd on th bai o Bi and τ, which i ummarizd in Figur or th LDF modl (th ba ca wa: K, ε.6, Bi, and τ.. Extraction rat incrad a a rult o a dcra in ithr Bi or τ, but th ct o a on-ordr o magnitud chang in τ (.- wa imilar to that o a -ordr o magnitud chang in Bi (-. dl Vall t al. [] tudid th ct o variation in K and ε by man o anothr dimnionl aramtr (Γε/(-εK that i rlatd to th artition o olut btwn th SCF and olid ha undr quilibrium condition, and concludd that a Γ incra (and th olut i mor tightly hld by th olid matrix, th amount o olut carrid out by th SCF dcra, thu incraing xtraction tim.

4 Tabl. Dimnionl dirntial ma balanc quation, initial condition, and boundary condition or th SCF ha and olid matrix ha or th Fickan, LDF and DDD modl. Modl SCF ha Solid ha / Por within olid ha ξ ε ε τ Fickan + ( X Y Y, ξ Y, ξ X + 3 K τbi δ δ δ X δ, ξ, δ δ δ, ξ, δ, ξ, Bi ( X Y δ, ξ, ξ, ξ ε 5 ε τ Bi + 5 LDF + ( X Y Y, ξ Y, ξ ε DDD + ( Y Y ξ Y, ξ Y, ξ ε τ τ X, ξ 5 Bi + 5 ( X Y Y τ 3 K Bi δ K X δ, ξ, K Y δ, ξ, K δ δ, ξ, Bi + δ δ ( Y Y δ, ξ, ξ, Figur comar rdiction o th Fickan, LDF and DDD modl or two combination o Bi and τ. Solut artition btwn th ha (K and total oroity (ε T ε+ε (-ε.6 wr kt contant in all ca. Two valu o articl oroity wr alo comard or th DDD modl (ε. and.375 that rultd in dirnt valu o bd oroity (ε.5 and.375, rctivly. Prdictd cumulativ xtraction lot wr virtually th am or th thr modl undr analyi or at xtraction (Fig. A, and mall dirnc wr obrvd or low xtraction (Fig. B. Th LDF aroximation wa inaroriat or <6. Thi i in agrmnt with Do & Ric [4], who howd that ridual radial olut concntration roil can b aumd to b arabolic in ha only whn /Biτ 3 (/Biτ 6 in Fig. B. On th othr hand, Goto t al. [3] uggtd that th LDF i aroriat only whn Bi<. Figur B alo uggt that xtraction rat imrov lightly a a rult o an incra in ε or long xtraction tim. It can b concludd that th LDF aroximation can b alid or th two othr modl undr analyi rovidd that th total oroity o th bd and articl (ε T i conidrd, that a modl-dndnt

5 ud, and that valu o Bi ar not too larg. To illutrat th ct o th dinition o Bi, an additional imulatd xtraction lot i includd in Figur A or th DDD modl and K, ε., ε.5, τ., and Bi (corronding to Bik R/D K. FITTING OF LITERATURE DATA Th u o th LDF modl or itting xrimntal cumulativ xtraction lot i illutratd in Figur 3 or lctd litratur data on ntial oil xtraction with SC-CO. Data corrond to tudi on th ct o olvnt ratio or th xtraction o camhor and nchon rom lavndr (Lavandula tocha ubci C. Boi lowr [5], and o ntial oil rom nnyroyal (Mntha ulgium L. lav [6]. Both t o xrimnt wr rormd with SC-CO at bar and 5 ºC. Partition aramtr (K wr timatd by lotting th ntial oil yild vru ciic olvnt conumtion or ach on o th two xrimntal t, and calculating th lo o th initial traight ortion [7]. Valu o K wr 7.6 or lavndr, and 6.6 or nnyroyal. W rocdd to timat bt-it valu o k, 5k D K/(k R+5D K, or ach condition. Dimnionl corrlation or th convctiv ma tranr coicint in th SCF ha (k hav th gnral orm: n.33 N a (N (N ( Sh R Sc whr N Sh (k R/D i th dimnionl Shrwood numbr, N R (ρur/µ, th dimnionl Rynold numbr, and N Sc (µ/ρd, th dimnionl Schmidt numbr. Th hyical rorti o th loadd SCF ha (ρ, µ, D wr timatd uing th rocdur rood by dl Vall t al. [8] uing PM885.4 g/mol and V c 3 cm 3 /mol or a tyical olut in lant ntial oil [7]. Whn th olvnt condition rmain unchangd, quation rduc to: n n- k a U R ( In a cond tag, bt-it valu o k or ach xrimnt wr ud to dtrmin bt it valu o a (.89, n (.8, and ubtrat-dndnt D (.5x -9 m / or lavndr, 3x -9 m / or nnyroyal. Valu o n in dimnionl corrlation or ma tranr coicint in ackd bd rang rom.6 [9] and.83 []. Bt-it valu o k timatd uing th aormntiond rocdur rangd x 6 m/, which ar about tim mallr than rdictd uing th corrlation o Tan t al. [], which ha bn uggtd or

6 th xtraction o vgtabl ubtrat with SC-CO in a ackd bd [8]. Modl itting wa obviouly wort or th data o Akgün t al. [5] than that o Ri-Vaco t al. [6] (c. Fig. 3. Th valu o Bi rangd rom.3 to. or lavndr lowr and rom.7 to.5 or nnyroyal lav, or which th LDF aroximation i adquat rgardl o th intrnal ma tranr mchanim. Acknowldgmnt Funding by Fondcyt (rojct rom Chil i gratly acknowldgd. REFERENCES [] DEL VALLE, J.M., NAPOLITANO, P., FUENTES, N., Ind. Eng. Chm. R., 39,,. 47 [] PEKER, H., SRINIVASAN, M.P., SMITH, J.M., McCOY, B.J., AIChE J., 38, 99,. 76 [3] GOTO, M., ROY, B.C., KODAMA, A., HIROSE, T., J. Chm. Eng. Jaan, 3, 998,. 7 [4] DO, D.D., RICE, R.G., AIChE J., 3, 986,. 49 [5] AKGÜN, M., AKGÜN, N.A., DINÇER, S., Ind. Eng. Chm. R. 39,,. 473 [6] REIS-VASCO, E.M.C., COELHO, J.A.P., PALAVRA, A.M.F., MARRONE, C., REVERCHON, E., Chm. Eng. Sci. 55,,. 97 [7] REVERCHON, E., MARRONE, C., Chm. Eng. Sci. 5, 997,. 34 [8] DEL VALLE, J.M., RIVERA, O., MATTEA, M., RUETSCH, L., DAGHERO, J., FLORES, A., J. Surcrit. Fluid (ubmittd [9] WAKAO, N., KAGUEI, S., Hat and Ma Tranr in Packd Bd, Gordon and Brach: Nw York, 98 [] TAN, C.-S., LIANG, S.-K., LIOU, D.-C., Chm. Eng. J. 38, 988,. 7

WEEK 3 Effective Stress and Pore Water Pressure Changes

WEEK 3 Effective Stress and Pore Water Pressure Changes WEEK 3 Effctiv Str and Por Watr Prur Chang 5. Effctiv tr ath undr undraind condition 5-1. Dfinition of ffctiv tr: A rvi A you mut hav larnt that th ffctiv tr, σ, in oil i dfind a σ σ u Whr σ i th total

More information

5.2 Plasticity I: Hypoelastic-Plastic Models

5.2 Plasticity I: Hypoelastic-Plastic Models 5. Platicity Hyolatic-Platic Modl h two main ty o claical laticity modl or larg train ar th hyolaticlatic modl and th hyrlatic-latic modl. h irt o th i dicud in thi ction. 5.. Hyolaticity n th hyolatic-latic

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

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

More information

MAE 110A. Homework 4: Solutions 10/27/2017

MAE 110A. Homework 4: Solutions 10/27/2017 MAE 0A Homwork 4: Solution 0/27/207 MS 4.20: Th figur blow provid tady-tat data for watr vapor flowing through a piping configuration. At ach xit, th volumtric flow rat, prur, and tmpratur ar qual. Dtrmin

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Engineering Differential Equations Practice Final Exam Solutions Fall 2011 9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.

More information

An Inventory Model with Change in Demand Distribution

An Inventory Model with Change in Demand Distribution Autralian Journal of Baic and Applid cinc, 5(8): 478-488, IN 99-878 An Invntory Modl with Chang in Dmand Ditribution P.. hik Uduman,. rinivaan, 3 Dowlath Fathima and 4 athyamoorthy, R. Aociat Profor, H.O.D

More information

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here,

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here, Numrical Eampl In thi final chaptr, w tart b illutrating om known rult in th thor and thn procd to giv a fw novl ampl. All ampl conidr th quation F(u) = u f(u) = g, (-) with Dirichlt boundar condition

More information

Influence of polarization of conduction electrons in semiconductor on their light absorption

Influence of polarization of conduction electrons in semiconductor on their light absorption Smiconductor Phyic, Quantum Elctronic & Otolctronic, V 4, N 4 P 445-45 PACS 77Ch, Ej; 78Bh, Ci, - Influnc of olariation of conduction lctron in miconductor on thir light abortion VS Svrin National Aviation

More information

Job No. Sheet 1 of 6 Rev A. Made by JG/AO Date Feb Checked by GZ Date March 2006

Job No. Sheet 1 of 6 Rev A. Made by JG/AO Date Feb Checked by GZ Date March 2006 Jo No. Sht 1 of 6 Rv A Jo Titl Sujct Clint Stainl Stl Valoriation Projct Dign xaml 11 Dign of a two-an trazoidal roof hting ad y JG/AO Dat F 006 Chckd y GZ Dat arch 006 DSIGN XAPL 11 DSIGN OF A TO-SPAN

More information

The Frequency Response of a Quarter-Wave Matching Network

The Frequency Response of a Quarter-Wave Matching Network 4/1/29 Th Frquncy Rsons o a Quartr 1/9 Th Frquncy Rsons o a Quartr-Wav Matchg Ntwork Q: You hav onc aga rovidd us with conusg and rhas uslss ormation. Th quartr-wav matchg ntwork has an xact SFG o: a Τ

More information

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level 5.76 Lctur #6 //94 Pag of 8 pag Lctur #6: Polyatomic Vibration III: -Vctor and H O Lat tim: I got tuck on L G L mut b L L L G F-matrix: too many F ij vn at quadratic-only lvl It obviou! Intrnal coordinat:

More information

Principles of Humidity Dalton s law

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

More information

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

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

More information

Adsorption of Congo Red Dye from Aqueous Solutions using Neem Leaves as Adsorbent

Adsorption of Congo Red Dye from Aqueous Solutions using Neem Leaves as Adsorbent Aian Journal of Chmitry Vol. 2, No. 7 (28), 4994-5 Adortion of Congo Rd Dy from Aquou Solution uing Nm Lav a Adorbnt SHIV PRATAP RAGHUVANSHI*, RENU SINGH and C.P. KAUSHIK Cntr for Enrgy Studi, Indian Intitut

More information

TO THE MODEL OBJECT WITH INERTIA SECOND TO THE MODEL OBJECT WITH INERTIA SECOND ORDER AND TIME DELAY

TO THE MODEL OBJECT WITH INERTIA SECOND TO THE MODEL OBJECT WITH INERTIA SECOND ORDER AND TIME DELAY THE TUNING OF THE PID AND PIDD ALGORITHMS TO THE MODEL OBECT WITH INERTIA SECOND ORDER AND TIME DELAY THE TUNING OF THE PID AND PIDD ALGORITHMS TO THE MODEL OBECT WITH INERTIA SECOND ORDER AND TIME DELAY

More information

Chapter 10 Time-Domain Analysis and Design of Control Systems

Chapter 10 Time-Domain Analysis and Design of Control Systems ME 43 Sytm Dynamic & Control Sction 0-5: Stady Stat Error and Sytm Typ Chaptr 0 Tim-Domain Analyi and Dign of Control Sytm 0.5 STEADY STATE ERRORS AND SYSTEM TYPES A. Bazoun Stady-tat rror contitut an

More information

Random Process Part 1

Random Process Part 1 Random Procss Part A random procss t (, ζ is a signal or wavform in tim. t : tim ζ : outcom in th sampl spac Each tim w rapat th xprimnt, a nw wavform is gnratd. ( W will adopt t for short. Tim sampls

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Search sequence databases 3 10/25/2016

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

More information

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC

More information

Analytical Model of an Eddy Current Retarder with Consideration of Nonlinear Magnetization Characteristics of its Ferromagnetic Material

Analytical Model of an Eddy Current Retarder with Consideration of Nonlinear Magnetization Characteristics of its Ferromagnetic Material ICONS 04 : Th Ninth Intrnational Confrnc on Sytm Analytical Modl of an Eddy Currnt Rtardr with Conidration of Nonlinar Magntiation Charactritic of it Frromagntic Matrial Songyun Park Kyihwan Park School

More information

Unit 6: Solving Exponential Equations and More

Unit 6: Solving Exponential Equations and More Habrman MTH 111 Sction II: Eonntial and Logarithmic Functions Unit 6: Solving Eonntial Equations and Mor EXAMPLE: Solv th quation 10 100 for. Obtain an act solution. This quation is so asy to solv that

More information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C Tchniqus of Intgration c Donald Kridr and Dwight Lahr In this sction w ar going to introduc th first approachs to valuating an indfinit intgral whos intgrand dos not hav an immdiat antidrivativ. W bgin

More information

Need to understand interaction of macroscopic measures

Need to understand interaction of macroscopic measures CE 322 Transportation Enginring Dr. Ahmd Abdl-Rahim, h. D.,.E. Nd to undrstand intraction o macroscopic masurs Spd vs Dnsity Flow vs Dnsity Spd vs Flow Equation 5.14 hlps gnraliz Thr ar svral dirnt orms

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

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

More information

Constrained Single Period Stochastic Uniform Inventory Model With Continuous Distributions of Demand and Varying Holding Cost

Constrained Single Period Stochastic Uniform Inventory Model With Continuous Distributions of Demand and Varying Holding Cost Journal of Matmati Statiti (): 334-338, 6 ISSN 549-3644 6 Sin Publiation Contraind Singl Priod Stoati Uniform Invntory Modl Wit Continuou Ditribution of Dm Varying Holding Cot Hala, A. Frgany M. E. El-Saadani

More information

Lecture 4: Parsing. Administrivia

Lecture 4: Parsing. Administrivia Adminitrivia Lctur 4: Paring If you do not hav a group, pla pot a rqut on Piazzza ( th Form projct tam... itm. B ur to updat your pot if you find on. W will aign orphan to group randomly in a fw day. Programming

More information

Convective energy transport

Convective energy transport PH217: Aug-Dc 2003 1 Convctiv nrgy tranpt In tllar intri, onc th tmpratur gradint bcom larg, it may bcom m favourabl to tranpt nrgy via convction rathr than radiativ diffuion and conduction. Th critrion

More information

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,

More information

Asymptotic Behaviour of the Solutions. of the Falkner-Skan Equations. Governing the Swirling Flow

Asymptotic Behaviour of the Solutions. of the Falkner-Skan Equations. Governing the Swirling Flow Adv. Thor. Appl. Mch., Vol. 3,, no. 4, 5-58 Aymptotic Bhaviour o th Solution o th Falknr-Skan Equation Govrning th Sirling Flo J. Singh Dpartmnt o Civil Enginring, ntitut o Tchnology, Banara Hindu Univrity,

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

Final Exam : Solutions

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

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

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

More information

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

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

More information

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

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

More information

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

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

More information

Byeong-Joo Lee

Byeong-Joo Lee OSECH - MSE calphad@postch.ac.kr Equipartition horm h avrag nrgy o a particl pr indpndnt componnt o motion is ε ε ' ε '' ε ''' U ln Z Z ε < ε > U ln Z β ( ε ' ε '' ε ''' / Z' Z translational kintic nrgy

More information

Prod.C [A] t. rate = = =

Prod.C [A] t. rate = = = Concntration Concntration Practic Problms: Kintics KEY CHEM 1B 1. Basd on th data and graph blow: Ract. A Prod. B Prod.C..25.. 5..149.11.5 1..16.144.72 15..83.167.84 2..68.182.91 25..57.193.96 3..5.2.1

More information

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

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

More information

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

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

More information

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

More information

CEE 772: Instrumental Methods in Environmental Analysis

CEE 772: Instrumental Methods in Environmental Analysis Updatd: 23 Octobr 2005 Print vrion CEE 772: Intrumntal Mthod in Environmntal Analyi Lctur #0 Sampl Prparation: : Baic and Phyical Mthod (Skoog,, nothing) (Harri, Chapt.. 23 & 28) (64-646 646 & 87-839)

More information

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity Ch. 8 Inlation, Intrst Rats & FX Rats Topics Purchasing Powr Parity Intrnational Fishr Ect Purchasing Powr Parity Purchasing Powr Parity (PPP: Th purchasing powr o a consumr will b similar whn purchasing

More information

Source code. where each α ij is a terminal or nonterminal symbol. We say that. α 1 α m 1 Bα m+1 α n α 1 α m 1 β 1 β p α m+1 α n

Source code. where each α ij is a terminal or nonterminal symbol. We say that. α 1 α m 1 Bα m+1 α n α 1 α m 1 β 1 β p α m+1 α n Adminitrivia Lctur : Paring If you do not hav a group, pla pot a rqut on Piazzza ( th Form projct tam... itm. B ur to updat your pot if you find on. W will aign orphan to group randomly in a fw day. Programming

More information

Elements of Statistical Thermodynamics

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

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

More information

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

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

More information

THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS

THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS ABSTRACT Th mchanical rotator mut b corrctly alignd and th prob placd in th propr location whn prforming phrical nar-fild maurmnt.

More information

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables.

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables. Chaptr Functions o Two Variabls Applid Calculus 61 Sction : Calculus o Functions o Two Variabls Now that ou hav som amiliarit with unctions o two variabls it s tim to start appling calculus to hlp us solv

More information

A constitutive model for unsaturated cemented soils under cyclic loading

A constitutive model for unsaturated cemented soils under cyclic loading A contitutiv modl for unaturatd cmntd oil undr cyclic loading C. Yang 1, Y.J. Cui 2,3, J.M. Prira 2,3, M.S. Huang 1 1. Dartmnt of Gotchnical Enginring, Tongji Univrity, Shanghai, China 2. Ecol National

More information

Multiple Short Term Infusion Homework # 5 PHA 5127

Multiple Short Term Infusion Homework # 5 PHA 5127 Multipl Short rm Infusion Homwork # 5 PHA 527 A rug is aministr as a short trm infusion. h avrag pharmacokintic paramtrs for this rug ar: k 0.40 hr - V 28 L his rug follows a on-compartmnt boy mol. A 300

More information

Nonlinear Poroelastoplastic Behavior of Geothermal Rocks

Nonlinear Poroelastoplastic Behavior of Geothermal Rocks Procding World Gothrmal Congr 15 Mlbourn, Autralia, 19-5 April 15 Nonlinar Porolatoplatic havior o Gothrmal Rock Mario-Céar Suárz A., Frnando Samanigo V., Joé-Eduardo Ramírz L.M., Omar A. Vicncio F. and

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

Math 34A. Final Review

Math 34A. Final Review Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right

More information

STUDY OF EFFECT OF LEAD ANGLE OF SHANKS ON PERFORMANCE OF DUCKFOOT SWEEP CULTIVATOR

STUDY OF EFFECT OF LEAD ANGLE OF SHANKS ON PERFORMANCE OF DUCKFOOT SWEEP CULTIVATOR STUDY OF EFFECT OF LEAD ANGLE OF SHANKS ON PERFORMANCE OF DUCKFOOT SWEEP CULTIVATOR Muhammad Danih mohddanih_huain@yahoo.com All Saint Collg Tchnology, Bhopal Abul Kalam danihaint@gmail.com ABSTRACT Tractor

More information

6. Negative Feedback in Single- Transistor Circuits

6. Negative Feedback in Single- Transistor Circuits Lctur 8: Intrductin t lctrnic analg circuit 36--366 6. Ngativ Fdback in Singl- Tranitr ircuit ugn Paprn, 2008 Our aim i t tudy t ffct f ngativ fdback n t mall-ignal gain and t mall-ignal input and utput

More information

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas

More information

EE 119 Homework 6 Solution

EE 119 Homework 6 Solution EE 9 Hmwrk 6 Slutin Prr: J Bkr TA: Xi Lu Slutin: (a) Th angular magniicatin a tlcp i m / th cal lngth th bjctiv ln i m 4 45 80cm (b) Th clar aprtur th xit pupil i 35 mm Th ditanc btwn th bjctiv ln and

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

Platform Pricing with Strategic Buyers

Platform Pricing with Strategic Buyers 0 45th Hawaii Intrnational Confrnc on ytm cinc Platform Pricing with tratgic uyr Yifan Dou Tinghua Univrity douyf03@mtinghuaducn D J Wu Gorgia Intitut of Tchnology djwu@mgtgatchdu Jian Chn Tinghua Univrity

More information

Schematic of a mixed flow reactor (both advection and dispersion must be accounted for)

Schematic of a mixed flow reactor (both advection and dispersion must be accounted for) Cas stuy 6.1, R: Chapra an Canal, p. 769. Th quation scribin th concntration o any tracr in an lonat ractor is known as th avction-isprsion quation an may b writtn as: Schmatic o a mi low ractor (both

More information

The basic elements of the magnetotail of the magnetosphere (Figure 9.1) are

The basic elements of the magnetotail of the magnetosphere (Figure 9.1) are Chaptr 9 Quit Magntotail Th baic lmnt of th magntotail of th magntophr (Figur 9.1) ar Mantl (currnt): Rgion of opn fild with high dnity magntohath plama. Lob: Low dnity, trong magntic fild rgion. Enrgy

More information

Analysis of spontaneous emission and its self-amplification in free-electron laser

Analysis of spontaneous emission and its self-amplification in free-electron laser FLS006 DESY Analyi of pontanou miion and it lf-amplification in fr-lctron lar Jia Qika ( 贾启卡 ) 18 May 006 National Synchrotron Radiation laboratory Univrity of Scinc and Tchnology of China Hfi, Anhui,

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6 ECE 6345 Spring 2015 Prof. David R. Jackon ECE Dpt. Not 6 1 Ovrviw In thi t of not w look at two diffrnt modl for calculating th radiation pattrn of a microtrip antnna: Elctric currnt modl Magntic currnt

More information

VSMN30 FINITA ELEMENTMETODEN - DUGGA

VSMN30 FINITA ELEMENTMETODEN - DUGGA VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional

More information

Adaptive Hysteresis Band Control for Constant Switching Frequency in Direct Torque Control of Induction Machine Drives

Adaptive Hysteresis Band Control for Constant Switching Frequency in Direct Torque Control of Induction Machine Drives Adaptiv Hytri Band Control for Contant Switching Frquncy in Dirct Torqu Control of Induction Machin Driv Mutafa AKTAŞ H. İbrahim OKUMUŞ -mail: makta@ktu.du.tr -mail: okumu@ktu.du.tr Karadniz Tchnical Univrity,

More information

5.80 Small-Molecule Spectroscopy and Dynamics

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

More information

Southern Taiwan University

Southern Taiwan University Chaptr Ordinar Diffrntial Equations of th First Ordr and First Dgr Gnral form:., d +, d 0.a. f,.b I. Sparabl Diffrntial quations Form: d + d 0 C d d E 9 + 4 0 Solution: 9d + 4d 0 9 + 4 C E + d Solution:

More information

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

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

More information

ATMO 551a Homework 6 solutions Fall 08

ATMO 551a Homework 6 solutions Fall 08 . A rising air parcl in th cor of a thundrstorm achivs a vrtical vlocity of 8 m/s similar to th midtrm whn it rachs a nutral buoyancy altitud at approximatly 2 km and 2 mb. Assum th background atmosphr

More information

. This is made to keep the kinetic energy at outlet a minimum.

. This is made to keep the kinetic energy at outlet a minimum. Runnr Francis Turbin Th shap th blads a Francis runnr is cmplx. Th xact shap dpnds n its spciic spd. It is bvius rm th quatin spciic spd (Eq.5.8) that highr spciic spd mans lwr had. This rquirs that th

More information

Exponential Functions

Exponential Functions Eponntial Functions Dinition: An Eponntial Function is an unction tat as t orm a, wr a > 0. T numbr a is calld t bas. Eampl: Lt i.. at intgrs. It is clar wat t unction mans or som valus o. 0 0,,, 8,,.,.

More information

Diploma Macro Paper 2

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

More information

Electrochemistry L E O

Electrochemistry L E O Rmmbr from CHM151 A rdox raction in on in which lctrons ar transfrrd lctrochmistry L O Rduction os lctrons xidation G R ain lctrons duction W can dtrmin which lmnt is oxidizd or rducd by assigning oxidation

More information

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D

More information

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

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

More information

Labor Productivity by Country and Good United States Shirts 10 shirts/day 6 shirts/day Food 30 bushels/day 2 bushels/day. 2bushels.

Labor Productivity by Country and Good United States Shirts 10 shirts/day 6 shirts/day Food 30 bushels/day 2 bushels/day. 2bushels. Fall 010 Econ 455 Anwr to Problm St Harvy Lapan 1. Conidr a Ricardian modl o comparativ advantag. Thr ar two countri, th U.S. and. Each country can produc two good, hirt (S and ood (F. Aum th US ha 1000

More information

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

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

More information

ACOUSTIC CHARACTERISTICS OF INTERNAL SOUND FIELD IN CYLINDRICAL STRUCTURE WITH AN EXCITED END PLATE

ACOUSTIC CHARACTERISTICS OF INTERNAL SOUND FIELD IN CYLINDRICAL STRUCTURE WITH AN EXCITED END PLATE ACOUSTC CHARACTERSTCS OF NTERNAL SOUND FELD N CYLNDRCAL STRUCTURE WTH AN ECTED END LATE.Eng. Kojima A. rof. D.Eng. oriyama H. and rof. D.Eng. Ohinoya Y. Cour of Scinc and Tchnology Graduat School of Tokai

More information

SIMPLE MODELS FOR SUPERCRITICAL EXTRACTION OF NATURAL MATTER

SIMPLE MODELS FOR SUPERCRITICAL EXTRACTION OF NATURAL MATTER SIMPLE MODELS FOR SUPERCRITICAL EXTRACTION OF NATURAL MATTER Camilo Pardo Manuel Velásquez and Gustavo Bolaños* Applied Thermodynamics and Supercritical Fluids Group School of Chemical Engineering Universidad

More information

are given in the table below. t (hours)

are given in the table below. t (hours) CALCULUS WORKSHEET ON INTEGRATION WITH DATA Work th following on notbook papr. Giv dcimal answrs corrct to thr dcimal placs.. A tank contains gallons of oil at tim t = hours. Oil is bing pumpd into th

More information

Constants and Conversions:

Constants and Conversions: EXAM INFORMATION Radial Distribution Function: P 2 ( r) RDF( r) Br R( r ) 2, B is th normalization constant. Ordr of Orbital Enrgis: Homonuclar Diatomic Molculs * * * * g1s u1s g 2s u 2s u 2 p g 2 p g

More information

y = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b)

y = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b) 4. y = y = + 5. Find th quation of th tangnt lin for th function y = ( + ) 3 whn = 0. solution: First not that whn = 0, y = (1 + 1) 3 = 8, so th lin gos through (0, 8) and thrfor its y-intrcpt is 8. y

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information

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

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

More information

Introduction to Condensed Matter Physics

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

More information

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

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

More information

Characteristic Equations and Boundary Conditions

Characteristic Equations and Boundary Conditions Charatriti Equation and Boundary Condition Øytin Li-Svndn, Viggo H. Hantn, & Andrw MMurry Novmbr 4, Introdution On of th mot diffiult problm on i onfrontd with In numrial modlling oftn li in tting th boundary

More information

Alpha and beta decay equation practice

Alpha and beta decay equation practice Alpha and bta dcay quation practic Introduction Alpha and bta particls may b rprsntd in quations in svral diffrnt ways. Diffrnt xam boards hav thir own prfrnc. For xampl: Alpha Bta α β alpha bta Dspit

More information

DESIGN OF TWO-CHANNEL FIR FILTERBANKS WITH RATIONAL SAMPLING FACTORS BY USING THE FREQUENCY- RESPONSE MASKING TECHNIQUE

DESIGN OF TWO-CHANNEL FIR FILTERBANKS WITH RATIONAL SAMPLING FACTORS BY USING THE FREQUENCY- RESPONSE MASKING TECHNIQUE R. Brgović and T. Saramäki, Dign of two-channl FIR filtrbank with rational amling factor by uing th fruncy-ron making tchniu, Proc. 4 th Int. orkho on Sctral Mthod and Multirat Signal Procing, Vinna, Autria,

More information

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

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

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

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

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

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

NUMERICAL SIMULATION OF HEAT TRANSFER OF NANOFLUIDS IN AN ENCLOSURE. 1,2 Mathematics Group

NUMERICAL SIMULATION OF HEAT TRANSFER OF NANOFLUIDS IN AN ENCLOSURE. 1,2 Mathematics Group Svnth Intrnational Conrnc on CFD in th Minral an Proc Inutri CSIRO Mlbourn Autralia 9- Dcmbr 9 NUMERICAL SIMULAION OF HEA RANSFER OF NANOFLUIDS IN AN ENCLOSURE Sana SHARMA * Arvin Kumar GUPA Mathmatic

More information