STATIC SIMULATION PROGRAM OF COPPER SOLVENT EXTRACTION CONFIGURATIONS USING MICROSOFT EXCEL SOLVER

Size: px
Start display at page:

Download "STATIC SIMULATION PROGRAM OF COPPER SOLVENT EXTRACTION CONFIGURATIONS USING MICROSOFT EXCEL SOLVER"

Transcription

1 STATIC SIMULATION PROGRAM OF COPPER SOLVENT EXTRACTION CONFIGURATIONS USING MICROSOFT EXCEL SOLVER Joseph Kafumbila This textbook provides the proedure for design stati simulation programs using Exel Solver for optimization on an Exel worksheet. This proedure will allow the design of a stati simulation program for all opper solvent extration onfigurations. The stati simulation program will be designed to size a new plant or trak performane of an old plant. K afumbila K asonta Joseph P r o e s s d e s i g n e r

2 Design of simulation program of opper solvent extration onfiguration using Mirosoft Exel Solver 06 Joseph Kafumbila

3 Contents. INTRODUCTION EQUILIBRIUM LINE SIMULATION MODELS EXTRACTION STEP STRIPPING STEP EQUILIBRIUM LINE AND MACCABE THIELE DIAGRAM EQUILIBRIUM LINE MACCABE THIELE DIAGRAM CONSTRAINTS OF COPPER SX-EW PLANT EQUILIBRIUM CONSTRAINTS BETWEEN EXTRACTION AND STRIPPING STEPS MAXIMUM VALUE OF EXTRACTANT VOLUME PERCENTAGE FREE ACID CONCENTRATION IN PLS MAXIMUM FREE ACID CONCENTRATION IN SPENT ELECTROLYTE MINIMUM COPPER CONCENTRATION IN SPENT ELECTROLYTE MAXIMUM COPPER CONCENTRATION IN ADVANCE ELECTROLYTE OPTIMUM VALUE OF RATIO OF ORGANIC TO AQUEOUS OF EXTRACTION STEP SATURATION RATIO SR SIMULATION PROGRAM USING EXCEL SOLVER PROGRAM DESCRIPTION STATIC SIMULATION PROGRAM DESIGN BIBLIOGRAPHY... 74

4 . Introdution Copper prodution tehnology hanges drastially in the last 5 years with introdution of solvent extration-eletrowinning iruit as a opper prodution method. The tehnology of opper solvent extration produes the most eonomial opper from low-grade opper ore. Copper solvent extration tehnology onsists of two iruits onneted by a ommon organi phase. In the first step, alled extration step, metal is extrated from aqueous phase by organi phase. In the seond step, alled stripping step, metal is reovered from organi phase. The seond aqueous phase is more pure and onentrated. At the beginning, opper solvent extration onfiguration operating on dilute aqueous phases were onstituted with two stages respetively to extration and stripping steps. Design of this ExS onfiguration was simple and based on the value of opper transfer per extratant volume perentage of 0. (g/l/% v/v). This value gives opper extration effiieny greater than 98% and opper stripping effiieny of 60%. Afterwards, understanding that opper extration effiieny was not the most important parameter than the ost of opper prodution plant, one stage of stripping step was removed and the value of opper transfer was inreased to 0.6 (g/l/%v/v). Design of this ExS onfiguration was based on the expeted value of opper extration effiieny of 90%. MaCabe Thiele method was introdued in design of opper solvent extration onfiguration when opper solvent extration tehnology started to be used for high-grade opper ore. A large number of laboratory tests were required before obtaining the optimal onfiguration by using MaCabe Thiele method. It was at this level that a simulation model of equilibrium line of extration and stripping steps was introdued. Several simulation models of equilibrium line of opper solvent extration using helating reagents were made. These simulation models were based either on equilibrium onstant of opper solvent extration hemial reation [] or on extrapolation urves of equilibrium lines of extration and stripping steps []. Simulation model based on hemial reation equilibrium onstant was required knowledge of phenomenology of hemial reation. Currently, most of stati simulation programs of opper solvent extration onfiguration use equilibrium line simulation models based on hemial reation equilibrium onstants beause it is easy to simulate impat of iron o-extration to extration step and temperature to stripping step. Design of this stati simulation program requires a ertain level of knowledge in omputer programming. This bloks innovation in design of new reagent or omplex opper solvent extration onfigurations beause stati simulation programs are developed by extratant suppliers far from plant designers. Equilibrium line simulation model based on hemial reation equilibrium onstant requires knowledge of all intermediate hemial reations. Example of intermediate hemial reations ourring during opper solvent extration with MOC- 45 is the following []: Cu + + HR CuR + H + (a) 3

5 Cu + + (HR) CuR + H + (b) HR (HR) () HR and (HR) are the moleular forms of MOC- 45 extratant in organi phase. (3). Equilibrium onditions of eah hemial reation are given by mathematial expressions (), (), and K a = [CuR ]x[h+ ] [Cu + ]x[hr] () K b = [CuR ]x[h+ ] [Cu + ]x[(hr) ] () K = [(HR) ] [HR] (3) where K a, K b, and K are respetively hemial reation equilibrium onstants of hemial reations (a), (b), and (). Stati simulation model will be defined by finding the equilibrium onstants values using experimental data of equilibrium lines. It must involve the following mathematial expressions giving mass balanes. - Copper mass Balane: [Cu + ] i = [Cu + ] f + V o V a x [CuR ] (5) - Oxime radial R mass balane: [HR] t = [HR] + x [(HR) ] + x [CuR ] (6) - Hydrogen ion mass balane: [H + ] f = [H + ] i + x V o V a x [CuR ] (7) Where the indies i, f and t respetively mean initial, final and total. V o and V a respetively mean volume of organi and aqueous phases. 4

6 One the values of hemial reation equilibrium onstants are obtained, the equilibrium line simulation model will use these mathematial expressions from () to (7) to predit the value of opper onentration in organi phase from the value of opper and free aid onentrations in aqueous and the values of V a and V o. This design method of equilibrium line simulation model is used by reagent suppliers and its design is omplex. For dynami modeling used in industrial opper solvent extration plant, plant metallurgists use extrapolation urves of equilibrium lines []. In most ases, the onditions for using these extrapolation equations are limited to this opper solvent extration plant. The goal of this textbook is to give a simple proedure for designing a stati simulation program of opper solvent extration onfiguration. This simple proedure will allow designers to quikly have a stati simulation program for omplex onfiguration or new produt that have not yet simulation program developed by supplier. It will also allow plant metallurgists to have a stati simulation program for heking plant performanes. This stati simulation program uses Exel solver program for optimization. Exel Solver is the Mirosoft add-in program used for what-if analysis. Exel solver program allows finding the optimum value for a formula in one ell. Knowledge of the use of Exel Solver is not suffiient. The textbook also gives advie that prevents stati simulation programs to rash when initial data hange. In the seond hapter, the textbook offers equilibrium line simulation models of extration and stripping steps not requiring knowledge of intermediate hemial reations. Equilibrium ondition of global hemial reation is resulted on the assumption that ioni strength varies very little only in aqueous phase. On the other hand, the ioni strength varies in organi phase. The textbook gives results of experimental tests. Extration and stripping equilibrium lines were generated by ontating a series of different volumes of aqueous phase and stripped organi phase by mehanial stirring. Following attainment of equilibrium after 5 min, phases were allowed to separate. After phase disengagement, opper was analyzed in raffinate by AAS, whereas free aid was determined by titration. After more than 0 years of researh, the new theory of equilibrium ondition of opper solvent extration hemial reation begins to be lear. In the third and fourth hapters, the textbook also gives theoretial onepts of opper solvent extration and industrial onstraints whih allow, together with equilibrium line simulation models, to design a stati simulation program of simple or omplex opper solvent extration onfiguration. In the fifth hapter, the textbook gives the design proedure of the stati simulation program of opper solvent extration onfiguration from an example. The proedure involves two options. The first onerns the designers and the seond onerns the plant metallurgists. The simulation program alled SimSXCu Full version.0 gives stati simulation programs of eighteen opper solvent extration onfigurations. 5

7 . Equilibrium line simulation models.. Extration step... Equilibrium ondition Extration step is guided by thermodynami disequilibrium between aqueous and organi phases. Copper mass transfer is stopped when thermodynami property reahes equilibrium ondition in both phases. Global opper solvent extration hemial reation with Lix984N extratant is followed hemial reation (d) [3]. LIX 984N reagent, a : volume blend of LIX 860N-I and LIX 84N-I, is a mixture of 5- nonylsaliylaldoxime and -hydroxy-5-nonylaetophenone oxime. Cu + + HR CuR + H + (d) where Cu + and H + are opper and hydrogen ioni speies in aqueous phase, HR is aid form of Lix984N extratant, and CuR is opper omplex form in organi phase expression (8) [4]. Thermodynami equilibrium ondition of global hemial reation (a) is given by the mathematial μ CuR + μ H + - μ Cu + - μ HR = 0 (8) where μ ρ is hemial potential of speies ρ Chemial potential of speies ρ is given by the mathematial expression (9). μ ρ = RTln(β ρ x γ ρ x C ρ C ρ 0) (9) where β ρ is standard-state ativity of speies ρ and is a funtion of solvent nature and temperature, 0 γ ρ is hemial ativity oeffiient of speie ρ, C ρ is molar onentration of speies ρ, C ρ is referene molar onentration whih by onvention is molar onentration, R is the perfet gas onstant, and T is the temperature The substitution of the mathematial expression (9) for all speies in the mathematial expression (8) gives the mathematial expression (0) whih is the thermodynami equilibrium ondition. 6

8 [Cu e or ] x [H e aq ] [Cu e aq ] x [HR or β CuR x β H x γ Cu x γ HR e ] = β Cu x β HR γ CuR x γ H = K e (0)... Value of K e from molar onentration... Definition The value of thermodynami equilibrium ondition K e from molar onentrations alled K e is given by the mathematial expression (). K e = [Cu or e ]x[h e aq ] () e e ] [Cu aq ]x[hr or... Copper molar onentrations in organi and aqueous phases The values of opper molar onentrations at the steady-state in organi and aqueous phases are respetively given by the mathematial expressions () and (3). [Cu e or ] = Cu e or () [Cu e aq ] = Cu aq e (3) e e where Cu aq and Cu or are respetively opper onentrations (g/l) in aqueous and organi phases The mathematial expression (4) gives opper mass balane at the steady-state. e i i e Cu or = Cu or + (Cu aq - Cu aq ) x V aq (4) V or i i where Cu aq and Cu or are respetively initial opper onentrations (g/l) in aqueous and organi phases. V aq and V or are respetively volumes of aqueous and organi phases Free extratant molar onentration in organi phase expression (5). The value of free extratant molar onentration in organi phase is given by the mathematial [HR e V% x 0.9 x 000 or ] = 00 x 70 - x Cuor e (5) 7

9 where v% is extratant volume perentage (v/v) in organi phase. 0.9 is the density of Lix984N extratant. 70 is the mass molar of Lix984N extratant Hydrogen ion molar onentration in aqueous phase The value of hydrogen ion molar onentration in aqueous phase omes from sulfuri aid dissoiation reation. Sulfuri aid dissoiation reation has followed hemial reations (e) and (f). H SO 4 HSO 4 + H + K a = 0 4 (e) HSO 4 SO 4 + H + K a =.5 0 (f) If C is free sulfuri aid molar onentration in aqueous phase and C is molar onentration of anion SO 4 assoiated with opper and buffers in aqueous phase. Sulfuri aid dissoiation reation (e) is omplete a beause the value of hemial reation equilibrium onstant K is big. Following mass balane omes from sulfuri dissoiation reation (e). H SO 4 HSO 4 H + Initial state C 0 0 Final state -C C C Mass balane 0 C C Sulfuri aid dissoiation reation (f) is not omplete beause the value of hemial reation equilibrium onstant K a is not big enough. Following mass balane omes from sulfuri aid dissoiation reation (f). Y is molar onentration of anion HSO 4 whih goes into dissoiation. HSO 4 SO 4 H + Initial state C C C Final state -Y Y Y Mass balane C -Y C +Y C +Y Thermodynami equilibrium ondition of sulfuri aid dissoiation reation (f) is given by the mathematial expression (6). Resolution of the mathematial expression (6) gives seond-degree equation. Hydrogen ion molar onentration in aqueous phase is given by the mathematial expression (7). The value of molar onentration Y is given by the mathematial expression (8) and the values of onstants A and B are given by the mathematial expressions (9) and (0). K a = (C +Y)(C +Y) (C Y) (6) 8

10 [H e aq ] = C + Y (7) Y = ( A+ A 4 x B) (8) A = C + C + K a (9) B = C x (C - K a ) (0) From the mathematial expression (8), the value of molar onentration Y beomes zero when the value of molar onentration C is equal to the value of hemial reation equilibrium onstant K a. When the value of molar onentration C is greater than the value of hemial reation equilibrium onstant K a, the value of molar onentration Y is lower than zero. In this ondition, the value of molar onentration Y in the mathematial expression (7) is zero. When the value of molar onentration C is lower than the value of hemial reation equilibrium onstant k a, the value of molar onentration Y is greater than zero...3. Value of K e from hemial ativity oeffiients..3.. Definition The value of thermodynami equilibrium ondition K e from hemial ativity oeffiients of speies alled K e is given by the mathematial expression (). β CuR x β H x γ Cu x γ HR K e = β Cu x β HR γ CuR x γ H () The value of K e is multipliation of two ratios. First ratio is the ratio of standard state ativities of speies whih is a onstant and seond ratio is the ratio of hemial ativity oeffiients of speies. The seond ratio of hemial ativity oeffiients also is multipliation of ratios of hemial ativity oeffiients in organi and aqueous phases respetively Ratio of hemial ativity oeffiients in aqueous phase Depending on molar onentrations of speies in aqueous phase, three ases are possible [5]: - Aqueous phase very diluted. In this ondition, the values of hemial ativity oeffiients tend to. - Ioni strength in aqueous phase varies very little. In the ondition, the value of ratio of hemial ativity oeffiients is a onstant. - Ioni strength in aqueous phase varies. In this ondition, the value of ratio of hemial ativity oeffiients is a variable. 9

11 The assumption is that ioni strength varies very little. So, ratio of hemial ativity oeffiients is a onstant in aqueous phase Ratio of hemial ativity oeffiients in organi phase In organi phase, the study done on the extratant Kelex 00, whih is helating opper solvent extration reagent, shows that ratio of hemial ativity oeffiients of speies in organi phase is a funtion of opper onentration in organi phase [4]. The assumption is that this thermodynami property is also true for helating opper extratant...4. Observations Conlusion from preeding observations is that the value of thermodynami equilibrium ondition K e is a funtion of opper onentration in organi phase...5. Mathematial relationship between the values of thermodynami equilibrium ondition and opper onentration in organi phase..5.. Pure opper sulfate aqueous phase Test onditions of lab test done with pure opper sulfate aqueous phase are the following: - Initial opper onentration in aqueous phase: 8 g/l. - Initial free aid onentration in aqueous phase: 5 g/l. - Extratant: Lix984N. - Extratant volume perentage in organi: 0%. Table gives equilibrium line data of lab test from whih the values of thermodynami equilibrium ondition K e of eah steady-state position are alulated. Data of steady-state position having the value of opper onentration in aqueous of 0.79 g/l are derived from ondition that the value of molar onentration C is equal to the value of hemial reation equilibrium onstant K a. Corresponding opper onentration in organi phase is obtained by extrapolation on equilibrium line. Figure gives the values of thermodynami equilibrium ondition K e versus the values of opper onentration in organi phase. Results show that: - The values of thermodynami equilibrium ondition K e are not the same for steady-state positions of equilibrium line. - The value of thermodynami equilibrium ondition K e is a linear funtion of the value of opper onentration in organi phase. 0

12 - The values of line slope are not the same in the ranges (0.8 to 5.75 g/l Cu) and (5.75 to 0.8 g/l Cu) where molar onentration Y is greater or lower than zero respetively. Table : Value of K e from equilibrium line data of lab test Lab test Organi Aqueous Aq Org Cu Cu Cu Free Lix984N Cu Y C C H K e g/l g/l moles/l moles/l moles/l moles/l moles/l moles/l moles/l Figure : Values of K e versus values of opper onentrations in organi phase of lab test..5.. Industrial opper sulfate aqueous phase Test onditions of lab test done with industrial opper sulfate aqueous phase are the following: - Elements grade of industrial opper sulfate aqueous phase is given in Table. - Extratant: Lix984N. - Extratant volume perentage in the organi: 8%. Table 3 gives equilibrium line data from whih the values of thermodynami equilibrium ondition K e of eah steady-state position are alulated. Figure gives the values of thermodynami equilibrium ondition K e versus the value of opper onentration in organi phase.

13 Table : Element grades of industrial opper sulfate aqueous phase of lab test Cu Co Al Fe Mg Mn Zn Ni Aid g/l g/l g/l g/l g/l g/l g/l g/l g/l Table 3: Value of K e from equilibrium line data of lab test Lab test Organi Aqueous Aq Org Cu Cu Cu Free Lix984N Cu Y C C H K e g/l g/l moles/l moles/l moles/l moles/l moles/l moles/l moles/l Figure : Values of K e versus values of opper onentration in organi phase of lab test Results show that: - In the industrial aqueous phase ontaining various sulfate buffers, molar onentration C is greater than the value of hemial reation equilibrium onstant K a. So, molar onentration Y is lower than zero.

14 - The value of thermodynami equilibrium ondition K e also is a linear funtion of the value of opper onentration in organi phase Observations In order to get loser to industrial onditions, only the range where molar onentrations Y are lower than zero will be taken in simulation model. Hydrogen ion onentration in aqueous phase is given now by the mathematial expression (). The mathematial expression (3) gives sulfuri aid onentrations in aqueous phase after opper solvent extration. [H or e ] = AC aq e 98 () e i i A aq = A aq + (Cu aq - Cu e aq ) x,54 (3) e i where A aq is sulfuri aid onentration (g/l) in aqueous phase at the steady-state and A aq is initial sulfuri aid onentration (g/l) in aqueous phase...6. Equilibrium line simulation model of extration step The substitution of the mathematial expressions (), (3), (5) and () in the mathematial expression () gives the mathematial expression (4) whih gives the value of thermodynami equilibrium ondition K e as a funtion of extratant volume perentage in organi phase, free aid onentration in aqueous phase and opper onentrations in organi and aqueous phases. K e = Cu e org [A Cue x e aq ] aq [ x V% x Cu org e ] (4) The value of thermodynami equilibrium ondition K e obtained from the mathematial expression (4) is plotted versus the values of opper onentration in organi phase in the range where the value of molar onentration Y is lower than zero using pure opper sulfate aqueous phase. Table 4 gives equilibrium line data of lab test, 3, 4 and 5. Figure 3 gives the value of thermodynami equilibrium ondition K e versus the values of opper onentration in organi phase. Results show that: - Initial free aid onentration does not affet the value of line slope. - The value of line slope is a funtion only of extratant volume perentage in organi phase. Line mathematial expression of thermodynami equilibrium ondition obtained from equilibrium line data has a shape given by the mathematial expression (5). 3

15 K e =D x Cu e or + E (5) Table 4: Equilibrium line data of lab tests, 3, 4 and 5 of extration step Lab test Lab test 3 Lab test 4 Lab test 5 i Cu aq 8 g/l i Cu aq 8 g/l i Cu aq 8 g/l i Cu aq 8 g/l i A aq 5 g/l i A aq 5 g/l i A aq 0 g/l i A aq 0 g/l V% 0 % V% 0 % V% 5 % V% 5 % e e Cu aq Cu or e e Cu aq Cu or e e Cu aq Cu or e e Cu aq Cu or Figure 3: Values of K versus the values of opper onentrations in organi phase from equilibrium line data of lab tests, 3, 4, and 5 The values of onstants D and E are funtions of extratant volume perentage. Mathematial expressions giving the values of onstants D and C are extrapolation urves of the value of onstants D and C obtained at different values of extratant volume perentage in the range of 8-3%. Equilibrium line simulation model of extration step is given by the mathematial expression (6). Thermodynami equilibrium onditions of K e and K e given by the mathematial expressions (6) and (4) are equals for eah steady-state position of equilibrium line. K =(-8.5 x v% (.746) ) x Cu e or +.7 x v% ( 0.646) (6) 4

16 .. Stripping step... Equilibrium ondition Stripping step is guided by thermodynami disequilibrium between aqueous and organi phases. Copper mass transfer is stopped when thermodynami property reahes equilibrium ondition in both phases. Copper stripping hemial reation with Lix984N extratant is followed hemial reation (g) whih is the reverse reation of opper extration hemial reation. CuR + H + Cu + + HR (g) The mathematial expression (7) gives the thermodynami equilibrium ondition. [Cu e or ] x [H e aq ] [Cu e aq ] x [HR or β CuR x β H x γ Cu x γ HR e ] = β Cu x β HR γ CuR x γ H = K s (7)... Simulation with equilibrium line model of extration step Thermodynami equilibrium ondition of extration and stripping steps are similar. Equilibrium line simulation model of extration step is used to simulate equilibrium line of stripping step. Test onditions of lab test 6 of stripping step are the following: - Initial opper onentration in aqueous phase: 35 g/l - Initial free aid onentration in aqueous phase: 80 g/l. - Copper onentration in loaded organi: 5.98 g/l. - Extratant: Lix984N. - Extratant volume perentage in organi: 3%. Table 5 gives equilibrium line data and the values of opper onentration in organi phase from equilibrium line simulation model of extration step. Figure 4 gives the values of opper onentration in aqueous phase from equilibrium line data and Extration step simulation model versus the values of opper onentration in organi phase Results show that there is a gap between the values of opper onentration from experimental data and equilibrium line simulation model of extration step. The gap is due probably to the differene of ioni strength between extration and stripping aqueous phases. 5

17 Table 5: Copper onentration in organi simulated with extration step simulation model Equilibrium line data Model Aqueous Organi Aqueous Cu (g/l) Cu (g/l) Cu (g/l) Figure 4: Copper onentration from equilibrium line data and Extration step simulation model in aqueous phase versus opper onentration in organi phase of lab test Equilibrium line simulation model of stripping step Table 6 gives equilibrium line data and the values of thermodynami equilibrium ondition K s of lab test 6. Figure 5 gives the value of thermodynami equilibrium ondition K s versus the values of opper onentration in organi phase. Results show that: - The value of thermodynami equilibrium ondition K s is a linear funtion of the values of opper onentration in organi phase. 6

18 - Auray of the value of thermodynami equilibrium ondition K s depends on auray in hemial analysis of opper onentration in aqueous phase. - The value of molar onentration Y is lower than zero. So, line slope is a funtion of extratant volume perentage only. The values of K s is given by the mathematial expression (8). K s = Cu e org [A Cue x e aq ] aq [ x V% x Cu org e ] (8) Table 6: Value of K s from equilibrium line data of lab test 6 Lab test Organi Aqueous Aq Org Cu Cu Cu Free Lix984N Cu Y C C H K s g/l g/l moles/l moles/l moles/l moles/l moles/l moles/l moles/l Figure 5: Values of K s versus the values of opper onentration in organi phase of lab test 6 Line mathematial expression of thermodynami equilibrium ondition obtained from equilibrium line data has a shape given by the mathematial expression (9). K s =F x Cu e or + G (9) 7

19 The values of onstants D and E are funtions of extratant volume perentage. Mathematial expressions giving the values of onstants D and C are extrapolation urves of the value of onstants D and C obtained at different values of extratant volume perentage in the range 8-3%. Equilibrium line simulation model of stripping step is given by the mathematial expression (30). Thermodynami equilibrium onditions of K s and K s given by the mathematial expressions (30) and (8) are equals for eah steady-state position of equilibrium line. K s =( x 0 3 e x v% ) x Cu or x v% ( 0.85) (30) 8

20 3. Equilibrium line and MaCabe Thiele diagram 3.. Equilibrium line 3... Desription Equilibrium line gives the distribution of dissolved omponent, between two phases. In the ase of opper solvent extration, it shows how opper distributes between aqueous and organi phases under the different onditions experiened in the proess. Equilibrium line data are obtained from lab test or by omputer modeling Computer modeling of equilibrium line Thermodynami equilibrium onditions given by the mathematial expressions (4) and (6) for extration step and by the mathematial expression (8) and (30) for stripping step are used for omputer modeling of extration and stripping equilibrium lines respetively. Copper and free aid onentrations in initial aqueous phase and also extratant volume perentage in organi phase are data whih must be known for omputer modeling of equilibrium lines. Thermodynami equilibrium onditions K e and K e for extration step and K s and K s for stripping step are rearranged to have opper onentration in aqueous phase on one side and opper onentration in organi phase on the other side. It appears two news equilibrium orretions α and α for extration step and π and π for stripping step. The mathematial expressions of news equilibrium orretions are given by the mathematial expressions (3) and (3) for extration step and (33) and (34) for stripping step. At the steadystate, the equilibrium orretions α and α are equals for extration step and π and π are equals for stripping step. α = [A aq i +(Cui aq Cu e aq ) x.54] Cue aq α = [ 8.5 x v%(.746) x Cu e or +.7 x v% ( 0.646) ] x (3.303 x V% x Cu e or ) Cue or π = [A aq i +(Cui aq Cu e aq ) x.54] Cue aq (3) (3) (33) π = [( x 0 3 x v% 0.983) x Cu e or x v% ( 0.85) ]x(3.303 x V% x Cu e or ) Cue or (34) 9

21 There are two ways for omputer modeling of equilibrium line. The first way is started from the known value of opper onentration in aqueous phase from whih opper onentration in organi phase is alulated. Grouping of equilibrium orretions α and α of extration step or π and π of stripping step gives a ubi equation as a funtion of opper onentration in organi phase. The seond way is started from the known value of opper onentration in organi phase from whih opper onentration in aqueous phase is alulated. Grouping of equilibrium orretions α and α of extration step or π and π of stripping step gives a seond-degree equation as a funtion of opper onentration in aqueous phase. For extration step, the value of opper onentration in aqueous phase is given by the mathematial expression (35) where the values of onstants H and J are given by the mathematial expression (36) and (37). e Cu aq = H H 4 x J (35) i i H = -.99 x A aq x Cu aq 0.4 x α (36) i J = (0.644 x A aq i + Cu aq ) (37) For stripping step, the value of opper onentration in aqueous phase is given by the mathematial expression (38) where the values of onstants L and M are given by the mathematial expressions (39) and (40). e Cu aq = L L 4 x M (38) i i L = -.99 x A aq x Cu aq 0.4 x π (39) i M = (0.644 x A aq i + Cu aq ) (40) Maximum loading Maximum loading (ML) is the value of opper onentration in organi phase orresponding to the value of initial opper onentration in aqueous phase on equilibrium line at the steady-state. Maximum loading is a funtion of the values of opper and free aid onentrations in aqueous phase and also extratant volume perentage in organi phase. The value of maximum loading is given by the first away method for omputer modeling of equilibrium line in whih the value of opper onentration in aqueous i phase at steady-state is the value of initial opper onentration Cu aq. The value of equilibrium orrelation α is hanged to α ML. The value of equilibrium orrelation α ML is given by the mathematial expression (4). 0

22 ML α = [A aq i ] Cui aq (4) Absolute maximum loading Absolute maximum loading is the value of maximum loading when the value of initial free aid onentration in aqueous phase is zero. Therefore, the values of equilibrium orrelations α and α are also zeros. The value of absolute maximum loading (AML) omes from equilibrium orrelation α and is given by the mathematial expression (4). The value of absolute maximum loading is not a linear funtion of extratant volume perentage. AML = x (V%). (4) 3.. MaCabe Thiele diagram 3... Stage sheme of extration and stripping steps Extration and stripping steps of opper solvent extration are frequently arried out at industrial sale with mixer-settlers. This equipment inludes a mixer in one stage or two stages in series to disperse one phase into other to provide interfaial ontat for mass transfer, followed by a settler to allow phases to oalese and separate Extration step Figure 6 gives sheme of stage of rank n of extration step in asade onfiguration. Stage of rank n of extration step reeives aqueous phase E n aq from stage of rank n- and organi phase E n+ or from stage of n rank n+. Stage of rank n produes aqueous phase E aq and organi phase E n or. Figure 6: Sheme of stage of rank n of extration step

23 For asade onfiguration ontaining m stages, stage of rank reeives PLS (E o aq ) and produes Loaded organi LO e (E or ). Stage of rank m reeives stripped organi SO e (E m+ or ) and produes raffinate Raf (E m aq ) Stripping step Figure 7 gives sheme of stage of rank n of stripping steps in asade onfiguration. Stage of rank n of stripping step reeives aqueous phase S n+ aq from stage of rank n+ and organi phase S n or from stage of n rank n-. Stage of rank n produes aqueous phase S aq and organi phase S n or. For asade onfiguration ontaining p stages, stage of rank reeives loaded organi LO s (S 0 or ) and produes advane eletrolyte AD (S aq ). Stage of rank p reeives spent eletrolyte SP (S p+ aq ) and produes stripped organi SO s (S p or ). Figure 7: Sheme of stage of rank n of stripping step 3... Parameters and designation 3... Stage of rank n Eah aqueous phase leaving stage of rank n of extration or stripping step is haraterized by the following independent parameters: n - V aq n - Cu aq : Flowrate (m 3 /h). : Copper onentration (g/l). n - A aq - : Free aid onentration (g/l). Eah organi phase leaving stage of rank n of extration or stripping step is haraterized by the following independent parameters:

24 n - V or n - Cu or : Flowrate (m 3 /h). : Copper onentration (g/l). - v% n : Extratant volume perentage in organi phase (%). The important parameters of stage of rank n of extration and stripping are: - Ratios R e n and R s n are ratios of organi to aqueous flowrates of extration and stripping stage of rank n respetively. - Parameters Mef e n and Mef s n are respetively mixer effiieny of stage of rank n of extration and stripping steps Casade The important parameters of asade onfiguration are: - Ratios R e and R s are respetively ratios of organi to aqueous flowrates of extration and stripping asade. - Parameter v% is extratant volume perentage in organi phase (%) of asade. - Parameters Eff e and Eff s are respetively extration and stripping effiieny of asade. - Parameter Cu t is net opper transfer from organi phase to opper eletrolyte per % of extratant volume perentage of stripping asade Mass balane Extration step Stage of rank n Conservation of opper mass flowrate at stage of rank n is given by the mathematial expression (43). The value of ratio R e n of stage of rank n is given by the mathematial expression (44). The value of free aid onentration in outlet aqueous phase of stage of rank n is given the mathematial expression (45). n n n n+ n n V aq x Cu aq + V or x Cu or = V aq x Cu aq + V n n or x Cu or (43) R n e = V n or V aq n = Cu aq n Cun aq Cu n+ or Cu or n (44) n n n A aq = A aq + (Cu aq - Cu n aq ) x.54 (45) 3

25 Casade Conservation of opper mass flowrate of asade is given by the mathematial expression (46). The value of ratio of R e of asade is given by the mathematial expression (47). The value of free aid onentration in outlet aqueous phase of asade is given by the mathematial expression (48). Copper extration effiieny of asade is given by the mathematial expression (49). V aq x PLS + V or x SO e = V aq x Raf + V or x LO e (46) R e = V or V = PLS Raf aq LO e SO e (47) m 0 A aq = A aq + (PLS-Raf) x.54 (48) Eff e = (PLS Raf) PLS x 00 (49) Stripping step Stage of rank n Conservation of opper mass flowrate of stage of rank n is given by the mathematial expression (50). The value of ratio R s n is given by the mathematial expression (5). The value of free aid onentration in outlet aqueous phase of stage of rank n is given by the mathematial expression (5). n n n n+ n n n n V or x Cu or + V aq x Cu aq = V or x Cu or + V aq x Cu aq (50) n R s = V n or V aq = Cuaq n Cun+ aq n Cu n or Cu or n (5) n n+ n+ A aq = A aq + (Cu aq - Cu n aq ) x.54 (5) Casade Conservation of opper mass flowrate of asade is given by the mathematial expression (53). The value of ratio R s is given by the mathematial expression (54). The value of free aid onentration in outlet aqueous phase of asade is given by the mathematial expression (55). Copper stripping effiieny of asade is given by the mathematial expression (56). Net opper transfer from organi phase to aqueous phase is given by the mathematial expression (57). 4

26 V or x LO s + V aq x SP = V or x SO s + V aq x AD (53) R s = V or V = AD SP aq LO s SO s (54) A aq = A p+ aq + (Cu p+ aq - Cu aq ) x.54 (55) Eff s = (LO s SO s ) LO s x 00 (56) Cu t = (LO s SO s ) V% = AD SP V% x R s (g/l/v%) (57) MaCabe Thiele diagram Extration step MaCabe Thiele diagram of stage of rank n of extration step is shown in Figure 8. The Point A n gives feed oordinates, the Point B n gives outlet oordinates and the Point C n gives outlet equilibrium oordinates. Triangle E n B n B n D n D n E n gives MaCabe Thiele diagram of stage of rank n of extration step. Slope of line E n D n is given by the mathematial expression (58). Slope of line A n B n is given by the mathematial expression (59). Slope E n D n = Cu or n Cun+ or n = Rn (58) e Cu n aq Cu aq Slope A n B n = Cu or n Cun+ or n = - Rn (59) e Cu n aq Cu aq Copper onentrations in aqueous and organi phases, leaving stage of rank n are given by the mathematial expressions (60) and (6). Cu n n aq = Cu (aq/e) x Mef e n + Cu 00 aq n x (- Mef e n ) (60) 00 Cu or n n = Cu (or/e) x Mef e n 00 + Cu or n+ x (- Mef e n 00 ) (6) 5

27 Figure 8: MaCabe Thiele diagram of stage of rank n of extration step Stripping step MaCabe Thiele diagram of stage of rank n of stripping step is shown in Figure 9. The Point A n gives feed oordinates, the Point B n gives outlet oordinates and the Point C n gives outlet equilibrium oordinates. Triangle D n B n B n E n E n D n gives MaCabe Thiele diagram of stage of rank n of stripping step. Slope of line E n D n is given by the mathematial expression (6). Slope of line A n B n is given by the mathematial expression (63). Slope E n D n = Cu or n Cun or n+ = Rn (6) s Cu n aq Cu aq Slope A n B n = Cu or n Cun or n = - Rn (63) s Cu n+ aq Cu aq Copper onentrations in aqueous and organi phases, leaving stage of rank n are given by the mathematial expressions (64) and (65). Cu n n aq = Cu (aq/e) x Mef s n + Cu 00 aq n+ x (- Mef s n ) (64) 00 Cu or n = Cu (or/e) n x Mef s n 00 + Cu or n x (- Mef s n 00 ) (65) 6

28 Figure 9: MaCabe diagram of stage of rank n of stripping step 7

29 4. Constraints of opper SX-EW plant 4.. Equilibrium onstraints between extration and stripping steps In opper solvent extration plant having extration step ontaining one or more asades and stripping step ontaining one or more asades, equilibrium onstraints between extration and stripping steps are given by the mathematial expressions (66) and (67). LO e = LO s (66) SO e = SO s (67) 4.. Maximum value of extratant volume perentage Organi phase is onstituted with extratant and diluent. Extratant is organi ompound whih extrats metal from aqueous phase. Diluent is organi liquid in whih extratant is dissolved. In the industrial praties, the maximum value of extratant volume perentage in organi phase in opper solvent extration is between 30 33% [6]. Organi phase visosity inreases with inreasing of extratant volume perentage in organi phase Free aid onentration in PLS from 0.5 to 80 g/l. Free aid onentration in PLS depends on leahing tehnique. Free aid onentration in PLS an go 4.4. Maximum free aid onentration in spent eletrolyte The value of maximum free aid onentration in spent eletrolyte is 80 g/l. This value of maximum free aid onentration is fixed by anode orrosion rate in EW iruit. It has been observed that inreasing of free aid onentration in opper eletrolyte inreases disonnetion of PbO to Pb metalli. Therefore, it inreases anode orrosion rate [7] Minimum opper onentration in spent eletrolyte In opper EW iruit, limiting urrent density is urrent density beyond whih opper powder is produed. The value of limiting urrent density inreases with inreasing opper onentration in opper 8

30 eletrolyte. Critial urrent density is urrent density beyond whih opper athode struture starts to be granular. It has been observed that the value of ritial urrent density is 35% of limiting urrent density [8]. The maximum value of urrent density in opper EW iruit is fixed by anode orrosion rate due to oxygen evolution on anode. Evolution of oxygen gas on anode inreases with inreasing urrent density. Inreasing of oxygen evolution on anode also inreases unhooking of PbO on anode. The maximum value of urrent density, whih allows to anodes to have a life of 5 years is 30 A/m. In the presene of obalt in opper eletrolyte at the level of 00 mg/l (obalt stabilizes PbO on anode), the maximum value of urrent density an reah 370 A/m. The value of maximum urrent density must be lower than ritial urrent density of opper onentration in spent eletrolyte. It has been observed that the minimum value of opper onentration in spent eletrolyte whih respets this onstraint is 30 g/l. In the industrial pratie, the value of opper onentration in spent eletrolyte is varied between 30 and 35 g/l Maximum opper onentration in advane eletrolyte In the past time, ratio R s /R e was fixed. This ratio is the enrihment fator of opper onentration from leah solution to opper eletrolyte. Under this ondition, opper onentration in advane eletrolyte inreases with inreasing amount of opper transferred. The value of maximum opper onentration in advane eletrolyte is reahed when opper onentration in loaded organi reahes the value of maximum loading (ML). Copper onentration in advane eletrolyte is given by the mathematial expression (68) AD = SP + R s R e x (PLS Raf) (68) Currently, opper tankhouse onsists of two parts; the first, alled savenger ells, is treating advane eletrolyte to oxidize soluble organi phase oming with advane eletrolyte. The seond, alled ommerial ells, is treating mixture of outlet eletrolyte from savenger ells and reyled eletrolyte from ommerial ells. Design of opper tankhouse is done suh as flowrate of opper eletrolyte to ommerial ells is 4 times greater than advane eletrolyte flowrate to savenger ells. This means that 0% of ells in opper tankhouse work as savenger ells. Maximum opper onentration drop aross ell is fixed at 3 g/l beause opper eletrolyte flowrate in onventional ell is fixed by athode fae veloity for a better quality of opper athode surfae. In the industrial pratie, athode fae veloity is 0.0 m 3 /hrs. per m of total athode area in the ell [9]. Copper onentration in spent eletrolyte is fixed at 35 g/l. In this ondition, opper onentration drop between spent and advane eletrolytes is 5 g/l and maximum opper onentration in advane eletrolyte is 50 g/l. These onditions give smallest size of opper tankhouse. The value of ratio R s is given by the mathematial expression (69). R s = R e x (AD SP) (PLS Raf) (69) 9

31 4.7. Optimum value of ratio of organi to aqueous of extration step Ratios R e and R s are external ratios. Internal ratio is ratio of volume flowrates inside of mixer. When the value of internal ratio (O/A) is greater than., aqueous phase is dispersed in organi phase. Mixer works in organi ontinuity regime. On the other side, when ratio (A/O) is greater than., organi phase is dispersed in aqueous phase. Mixer works in aqueous ontinuity regime. It has been observed that rud formation dereases when mixer works in organi ontinuity regime [0]. Therefore, all mixers of extration and stripping steps work in organi ontinuity regime and the optimum value of ratio R e is now. whih gives smallest size of mixer and settler without any organi or aqueous stage reyle Saturation ratio SR Currently, saturation of organi phase with opper (high value of (LO/ML) is important parameter in design of opper solvent extration plant. This parameter takes into aount good use of organi phase (high value of Net opper transfer) and also rejetion of iron from organi phase. In opper solvent extration, iron is transferred to opper eletrowinning iruit by physial entrainment. In addition, Ferri is transferred by hemial entrainment. Studies on iron transfer show that the average of iron hemial entrainment is between 35 to 60% of total entrainment []. Iron presene in opper eletrolyte auses redution of urrent effiieny. Maximum iron onentration in opper eletrolyte is.5g/l whih will give urrent effiieny greater than 90%. Copper eletrolyte bleed is used to maintain this iron level in eletrolyte. Inreasing of flowrate of opper eletrolyte bleed inreases ost of obalt reagent whih is added to opper EW iruit. In all opper solvent extration plants having asade onfiguration with two stages to extration step, it has been observed that iron onentration in loaded organi out of stage of rank is lower than iron onentration in partially loaded organi out of stage of rank. This effet is alled rowding []. The value of ratio ( LO ) is a new onstraint alled saturation ratio SR. This onstraint is appliable to ML all opper solvent extration onfigurations (ExS, ExS, 3ExS, series-parallel, interlaed, double seriesparallel and others). The mathematial expression (70) gives the value of saturation ratio. SR = LO x 00 (%) (70) ML 30

32 5. Simulation program using Exel solver program 5.. Desription Simulation program is done on Exel spreadsheet in format of Exel solver program. Exel solver is the Mirosoft add-in program used for what-if analysis. Exel solver program allows finding the optimum value for a formula in ell alled the objetive ell. First step of stati simulation program design is reation of simulation program table on Exel spreadsheet. Simulation program table is made with three small tables whih are table of extration step, table of stripping step, and table of simulation program onstraint. In simulation program table, data have red olor, solver onstraints have blue olor and solver onstraints have green olor. There are two stati simulation program options for eah opper solvent extration onfiguration. For eah option of eah opper solvent extration onfiguration, there is a stati simulation program table. Two options are: - Option : Unknown parameter in opper solvent extration simulation program is extratant volume perentage in organi phase. This stati simulation program is for designer of opper solvent extration onfiguration. - Option : Unknown parameters in opper solvent extration simulation program are extratant volume perentage, saturation ratio, and mixer effiienies of extration and stripping steps for existing plant. This simulation program is for plant metallurgist. 5.. Stati simulation program design 5... General In this book for good understanding, stati simulation program design will be done step by step using a onventional onfiguration ontaining two stages in asade to extration step and two stages in asade to stripping step as an example. 3

33 5... Option. In this option, unknown parameter is extratant volume perentage. Table 7 gives data of hosen example for explanation of simulation program oneption. Table7: Data of hosen example of opper solvent extration onfiguration Desription Symbol Unity Value Extration step PLS Flow PLS Flow m 3 /h 400 Copper onentration in PLS PLS Cu g/l 7 Aid onentration in PLS PLS A g/l.96 Ratio O/A R e. Saturation ratio SR % 80 Number of extration stage Stage of rank mixer effiieny Mef e % 9 Stage of rank mixer effiieny Mef e % 95 Stripping step Copper onentration in spent eletrolyte SP Cu g/l 35 Aid onentration in spent eletrolyte SP A g/l 80 Copper onentration in advane eletrolyte AD Cu g/l 50 Number of stripping stage Stage of rank mixer effiieny Mef s % 98 Stage of rank mixer effiieny Mef s % 85 Stati simulation program table of option of ExS onfiguration is given in Table 8 as it appears on Exel Mirosoft spreadsheet. Data from Table 7 have red olor. In extration table, designation α n, H n and J n are respetively the values of equilibrium orrelation α and onstants H and J of stage of rank n for alulating the value of opper onentration in aqueous phase from the value of opper onentration in organi phase. Designation A n, C n, D n and E n are the Points A, B, C, and D from extration step MaCabe Thiele diagram of stage of rank n. In stripping table, designation π n, L n and M n are respetively the values of equilibrium orrelation π and onstants L and M of stage of rank n for alulating the value of opper onentration in aqueous phase from the value of opper onentration in organi phase. Designation A n, C n, D n and E n are the Points A, B, C, and D from stripping step MaCabe Thiele diagram of stage of rank n Extration step Data Simulation program design is started with solver variables of data. These solver variables will be data of all mathematial expressions of extration step. 3

34 - In the ell F6 of solver variable of PLS flowrate (PLS flow), enter the number giving the value of PLS flowrate data that is in the ell C6. - In the ell F7 of solver variable of PLS opper onentration (PLS Cu), enter the number giving the value of PLS opper onentration data that is in the ell C7. - In the ell F8 of solver variable of PLS free aid onentration (PLS A), enter the number giving the value of PLS aid onentration data that is in the ell C8. - In the ell F9 of solver variable of saturation ratio (SR), enter the number giving the value of saturation ratio data that is in the ell C9. - In the ell F0 of solver variable of ratio (R e ), enter the number giving the value of ratio (R e ) data that is in the ell C0. - In the ell F of solver variable of mixer effiieny ( Mef e ), enter the number giving the value of mixer effiieny ( Mef e ) that is in the ell C. - In the ell F of solver variable of mixer effiieny (Mef e ), enter the number giving the value of mixer effiieny (Mef e ) that is in the ell C. Solver onstraints of solver variables of extration step data are the following: - In the ell I6, enter formula: =F6-C6. - In the ell I7, enter formula: =F7-C7. - In the ell I8, enter formula: =F8-C8. - In the ell I9, enter formula: =F9-C9. - In the ell I0, enter formula: =F0-C0. - In the ell I, enter formula: =F-C. - In the ell I, enter formula: =F-C. Starting value The starting value of extratant volume perentage of simulation program is random number between and 3%. The starting value of extratant volume perentage is used in all mathematial expression of extration step as extration volume perentage data. The optimum value of extratant volume perentage is known at the end of simulation program by running Exel Solver program. The starting value of extratant volume perentage is the expeted value of extratant volume perentage for those who have experiene. For this ase, hosen starting value is 5%. - In the ell F5, enter the number 5. General The value of organi flowrate is in the ell C8. This value is given by the mathematial expression (47) where the values of ratio (R e ) is in the ell F0 and PLS flowrate is in the ell F6. 33

General Equilibrium. What happens to cause a reaction to come to equilibrium?

General Equilibrium. What happens to cause a reaction to come to equilibrium? General Equilibrium Chemial Equilibrium Most hemial reations that are enountered are reversible. In other words, they go fairly easily in either the forward or reverse diretions. The thing to remember

More information

KINETICS OF IRON OXIDE DIRECT REDUCTION BY COAL E.R. ABRIL 1

KINETICS OF IRON OXIDE DIRECT REDUCTION BY COAL E.R. ABRIL 1 KINETICS OF IRON OXIDE DIRECT REDUCTION BY COAL E.R. ABRIL 1 CIMM- Av.Velez Sarsfield 1561 C.P.5000 Córdoba, Argentina. aabril@intiemor.gov.ar Abstrat - A new interpretation to the kinetis of iron oxide

More information

JF Physical Chemistry JF CH 1101: Introduction to Physical Chemistry.

JF Physical Chemistry JF CH 1101: Introduction to Physical Chemistry. JF Physial Chemistry 010-011. JF CH 1101: Introdution to Physial Chemistry. Dr Mike Lyons. Shool of Chemistry Trinity College Dublin. melyons@td.ie A ompendium of past examination questions set on Physial

More information

Fig Review of Granta-gravel

Fig Review of Granta-gravel 0 Conlusion 0. Sope We have introdued the new ritial state onept among older onepts of lassial soil mehanis, but it would be wrong to leave any impression at the end of this book that the new onept merely

More information

A simple expression for radial distribution functions of pure fluids and mixtures

A simple expression for radial distribution functions of pure fluids and mixtures A simple expression for radial distribution funtions of pure fluids and mixtures Enrio Matteoli a) Istituto di Chimia Quantistia ed Energetia Moleolare, CNR, Via Risorgimento, 35, 56126 Pisa, Italy G.

More information

Lab.6. Extraction. Upper phase. water. Bottom phase. chloroform

Lab.6. Extraction. Upper phase. water. Bottom phase. chloroform Lab.6. Extration Key words: Solubility, immisible solvent, partition solutes in two phase system, distribution onstant, partition neutral ompound, partition aids and basis, fators (ph, temperature), partition

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

BINARY RANKINE CYCLE OPTIMIZATION Golub, M., Koscak-Kolin, S., Kurevija, T.

BINARY RANKINE CYCLE OPTIMIZATION Golub, M., Koscak-Kolin, S., Kurevija, T. BINARY RANKINE CYCLE OPTIMIZATION Golub, M., Kosak-Kolin, S., Kurevija, T. Faulty of Mining, Geology and Petroleum Engineering Department of Petroleum Engineering Pierottijeva 6, Zagreb 0 000, Croatia

More information

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 2/3/2014

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 2/3/2014 Amount of reatant/produt //01 quilibrium in Chemial Reations Lets look bak at our hypothetial reation from the kinetis hapter. A + B C Chapter 15 quilibrium [A] Why doesn t the onentration of A ever go

More information

Chapter 14. The Concept of Equilibrium and the Equilibrium Constant. We have for the most part depicted reactions as going one way.

Chapter 14. The Concept of Equilibrium and the Equilibrium Constant. We have for the most part depicted reactions as going one way. Chapter 14 The Conept of Equilibrium and the Equilibrium Constant In hapter 1 we dealt with Physial Equilibrium Physial Changes HO 2 (l) HO 2 (g) In hapter 14 we will learn about Chemial Equilibrium. We

More information

Chapter 8 Thermodynamic Relations

Chapter 8 Thermodynamic Relations Chapter 8 Thermodynami Relations 8.1 Types of Thermodynami roperties The thermodynami state of a system an be haraterized by its properties that an be lassified as measured, fundamental, or deried properties.

More information

13.4 REDOX STOICHIOMETRY

13.4 REDOX STOICHIOMETRY (d) In a double-blind study, randomly seleted ontrol and experimental groups of 500 volunteers are studied for hanges whih affet their irulatory system. The ontrol group gets an ordinary braelet (plaebo)

More information

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Determination of the reaction order

Determination of the reaction order 5/7/07 A quote of the wee (or amel of the wee): Apply yourself. Get all the eduation you an, but then... do something. Don't just stand there, mae it happen. Lee Iaoa Physial Chemistry GTM/5 reation order

More information

2 How far? Equilibrium Answers

2 How far? Equilibrium Answers How far? Equilibrium Answers ratie: pages 37 39 1 Answer is D. Only a hange in temperature harges the value of the equilibrium onstant. Answer is D. [B] /[A] so [B] [A] or [B] [A] 1/ 3 Answer is B. Amounts

More information

23.1 Tuning controllers, in the large view Quoting from Section 16.7:

23.1 Tuning controllers, in the large view Quoting from Section 16.7: Lesson 23. Tuning a real ontroller - modeling, proess identifiation, fine tuning 23.0 Context We have learned to view proesses as dynami systems, taking are to identify their input, intermediate, and output

More information

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 5/27/2014

Chapter 15 Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium. Reversible Reactions & Equilibrium 5/27/2014 Amount of reatant/produt 5/7/01 quilibrium in Chemial Reations Lets look bak at our hypothetial reation from the kinetis hapter. A + B C Chapter 15 quilibrium [A] Why doesn t the onentration of A ever

More information

Mean Activity Coefficients of Peroxodisulfates in Saturated Solutions of the Conversion System 2NH 4. H 2 O at 20 C and 30 C

Mean Activity Coefficients of Peroxodisulfates in Saturated Solutions of the Conversion System 2NH 4. H 2 O at 20 C and 30 C Mean Ativity Coeffiients of Peroxodisulfates in Saturated Solutions of the Conversion System NH 4 Na S O 8 H O at 0 C and 0 C Jan Balej Heřmanova 5, 170 00 Prague 7, Czeh Republi balejan@seznam.z Abstrat:

More information

A Spatiotemporal Approach to Passive Sound Source Localization

A Spatiotemporal Approach to Passive Sound Source Localization A Spatiotemporal Approah Passive Sound Soure Loalization Pasi Pertilä, Mikko Parviainen, Teemu Korhonen and Ari Visa Institute of Signal Proessing Tampere University of Tehnology, P.O.Box 553, FIN-330,

More information

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that

More information

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Speed-feedbak Diret-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Y. Yamamoto, T. Nakamura 2, Y. Takada, T. Koseki, Y. Aoyama 3, and Y. Iwaji 3

More information

Answer: Easiest way to determine equilibrium concentrations is to set up a table as follows: 2 SO 2 + O 2 2 SO 3 initial conc change

Answer: Easiest way to determine equilibrium concentrations is to set up a table as follows: 2 SO 2 + O 2 2 SO 3 initial conc change Problem #1 6 mol of SO and 4 mol of O are plaed into a 1 L flask at temperature, T. The equilibrium onentration of SO is found to be 4 mol/l. Determine K. SO (g) + O (g) SO (g) K = [SO ] / [SO ] [O ] Answer:

More information

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential

More information

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 4, 2012

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 4, 2012 INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume, No 4, 01 Copyright 010 All rights reserved Integrated Publishing servies Researh artile ISSN 0976 4399 Strutural Modelling of Stability

More information

3 Tidal systems modelling: ASMITA model

3 Tidal systems modelling: ASMITA model 3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level

More information

Gluing Potential Energy Surfaces with Rare Event Simulations

Gluing Potential Energy Surfaces with Rare Event Simulations This is an open aess artile published under an ACS AuthorChoie Liense, whih permits opying and redistribution of the artile or any adaptations for non-ommerial purposes. pubs.as.org/jctc Gluing Potential

More information

Mass Transfer 2. Diffusion in Dilute Solutions

Mass Transfer 2. Diffusion in Dilute Solutions Mass Transfer. iffusion in ilute Solutions. iffusion aross thin films and membranes. iffusion into a semi-infinite slab (strength of weld, tooth deay).3 Eamples.4 ilute diffusion and onvetion Graham (85)

More information

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION 09-1289 Citation: Brilon, W. (2009): Impedane Effets of Left Turners from the Major Street at A TWSC Intersetion. Transportation Researh Reord Nr. 2130, pp. 2-8 IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE

More information

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines DOI.56/sensoren6/P3. QLAS Sensor for Purity Monitoring in Medial Gas Supply Lines Henrik Zimmermann, Mathias Wiese, Alessandro Ragnoni neoplas ontrol GmbH, Walther-Rathenau-Str. 49a, 7489 Greifswald, Germany

More information

Directional Coupler. 4-port Network

Directional Coupler. 4-port Network Diretional Coupler 4-port Network 3 4 A diretional oupler is a 4-port network exhibiting: All ports mathed on the referene load (i.e. S =S =S 33 =S 44 =0) Two pair of ports unoupled (i.e. the orresponding

More information

A Stochastic Analysis of Liquid Mixing in Bubble Column

A Stochastic Analysis of Liquid Mixing in Bubble Column Amerian Journal of Fluid Dynamis 013, 3(3): 75-79 DOI: 193/j.ajfd.0130303.04 A Stohasti Analysis of Liquid Mixing in Bubble Column Rajeev Parmar, Subrata Kumar Majumder * Department of Chemial Engineering,

More information

An excess of concentrated hydrochloric acid is added to separate aqueous solutions containing [Cu(H 2 O) 6 ] 2 and [Co(H 2 O) 6 ] 2.

An excess of concentrated hydrochloric acid is added to separate aqueous solutions containing [Cu(H 2 O) 6 ] 2 and [Co(H 2 O) 6 ] 2. 1 An exess of a given reagent is added to eah of the following pairs of aqueous metal ions. For eah metal ion, state the initial olour of the solution and the final oservation that you would make. In eah

More information

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO Evaluation of effet of blade internal modes on sensitivity of Advaned LIGO T0074-00-R Norna A Robertson 5 th Otober 00. Introdution The urrent model used to estimate the isolation ahieved by the quadruple

More information

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach Amerian Journal of heoretial and Applied tatistis 6; 5(-): -8 Published online January 7, 6 (http://www.sienepublishinggroup.om/j/ajtas) doi:.648/j.ajtas.s.65.4 IN: 36-8999 (Print); IN: 36-96 (Online)

More information

Numerical simulation of a one-dimensional shock tube problem at supercritical fluid conditions

Numerical simulation of a one-dimensional shock tube problem at supercritical fluid conditions International Journal of Physial Sienes Vol. 3 (1), pp. 314-30, Deember, 008 Available online at http://www.aademijournals.org/ijps ISSN 199-1950 008 Aademi Journals Full ength esearh Paper Numerial simulation

More information

Chapter 15 Chemical Equilibrium

Chapter 15 Chemical Equilibrium Chapter 5 Chemial Equilibrium 5. The Conept of Equilibrium Figure: 3. from Chemistry by MMurray & Fey Figure 3.(a) NO 4( g) NO( g) olorless brown we start with reatant, N O 4, so the solution is olorless

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

Part G-4: Sample Exams

Part G-4: Sample Exams Part G-4: Sample Exams 1 Cairo University M.S.: Eletronis Cooling Faulty of Engineering Final Exam (Sample 1) Mehanial Power Engineering Dept. Time allowed 2 Hours Solve as muh as you an. 1. A heat sink

More information

Chapter 2 Linear Elastic Fracture Mechanics

Chapter 2 Linear Elastic Fracture Mechanics Chapter 2 Linear Elasti Frature Mehanis 2.1 Introdution Beginning with the fabriation of stone-age axes, instint and experiene about the strength of various materials (as well as appearane, ost, availability

More information

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker. UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable

More information

Part II SECTION I : One or more options correct Type

Part II SECTION I : One or more options correct Type [1] JEE Advaned 2013/ Paper -2 Part II SECTION I : One or more options orret Type This setion ontains 8 multiple hoie questions. Eah question has four hoies (A), (B), (C) and (D), out of whih ONE or MORE

More information

An Improved Model for Calculating Heats of Dilution and Equilibrium Constants for High Temperature Aqueous Electrolyte Solutions

An Improved Model for Calculating Heats of Dilution and Equilibrium Constants for High Temperature Aqueous Electrolyte Solutions Brigham Young University BYU SholarsArhive All Theses and Dissertations 2007-01-08 An Improved Model for Calulating Heats of Dilution and Equilibrium Constants for High Temperature Aqueous Eletrolyte Solutions

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

2. Mass transfer takes place in the two contacting phases as in extraction and absorption.

2. Mass transfer takes place in the two contacting phases as in extraction and absorption. PRT 11- CONVECTIVE MSS TRNSFER 2.1 Introdution 2.2 Convetive Mass Transfer oeffiient 2.3 Signifiant parameters in onvetive mass transfer 2.4 The appliation of dimensional analysis to Mass Transfer 2.4.1

More information

The gravitational phenomena without the curved spacetime

The gravitational phenomena without the curved spacetime The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,

More information

Taste for variety and optimum product diversity in an open economy

Taste for variety and optimum product diversity in an open economy Taste for variety and optimum produt diversity in an open eonomy Javier Coto-Martínez City University Paul Levine University of Surrey Otober 0, 005 María D.C. Garía-Alonso University of Kent Abstrat We

More information

Chapter 15: Chemical Equilibrium

Chapter 15: Chemical Equilibrium Chapter 5: Chemial Equilibrium ahoot!. At eq, the rate of the forward reation is the rate of the reverse reation. equal to, slower than, faster than, the reverse of. Selet the statement that BEST desribes

More information

ES 247 Fracture Mechanics Zhigang Suo

ES 247 Fracture Mechanics Zhigang Suo ES 47 Frature Mehanis Zhigang Suo The Griffith Paper Readings. A.A. Griffith, The phenomena of rupture and flow in solids. Philosophial Transations of the Royal Soiety of London, Series A, Volume 1 (191)

More information

Determination of the Aerodynamic Characteristics of Flying Vehicles Using Method Large Eddy Simulation with Software ANSYS

Determination of the Aerodynamic Characteristics of Flying Vehicles Using Method Large Eddy Simulation with Software ANSYS Automation, Control and Intelligent Systems 15; 3(6): 118-13 Published online Deember, 15 (http://www.sienepublishinggroup.om//ais) doi: 1.11648/.ais.1536.14 ISSN: 38-5583 (Print); ISSN: 38-5591 (Online)

More information

POROUS CARBON PARTICLE COMBUSTION IN AIR

POROUS CARBON PARTICLE COMBUSTION IN AIR MCS 7 Chia Laguna, Cagliari, Sardinia, taly, 11-15, 11 POOUS CABON PATCLE COMBUSTON N A V. M. Gremyahkin grema@ipmnet.ru nstitute for Problems in Mehanis, AS, Mosow, ussia Abstrat Theoretial investigation

More information

Modeling real gas equations of state in high density combustion

Modeling real gas equations of state in high density combustion 26 th ICDERS July 3 th August 4 th, 217 Boston, MA, USA Modeling real gas equations of state in high density ombustion Chenwei Zheng, Deshawn Coombs, Ben Akih-Kumgeh Department of Mehanial and Aerospae

More information

Mechanistic Model for Reactive Transport of Radionuclides on Iron-(Oxy)Hydroxide Colloids at the Yucca Mountain Repository

Mechanistic Model for Reactive Transport of Radionuclides on Iron-(Oxy)Hydroxide Colloids at the Yucca Mountain Repository U.S. Department of Energy Offie of Civilian Radioative Waste Management Mehanisti Model for Reative Transport of Radionulides on Iron-(Oxy)Hydroxide Colloids at the Yua Mountain Repository Presented to:

More information

RESEARCH ON RANDOM FOURIER WAVE-NUMBER SPECTRUM OF FLUCTUATING WIND SPEED

RESEARCH ON RANDOM FOURIER WAVE-NUMBER SPECTRUM OF FLUCTUATING WIND SPEED The Seventh Asia-Paifi Conferene on Wind Engineering, November 8-1, 9, Taipei, Taiwan RESEARCH ON RANDOM FORIER WAVE-NMBER SPECTRM OF FLCTATING WIND SPEED Qi Yan 1, Jie Li 1 Ph D. andidate, Department

More information

Optimal control of solar energy systems

Optimal control of solar energy systems Optimal ontrol of solar energy systems Viorel Badesu Candida Oanea Institute Polytehni University of Buharest Contents. Optimal operation - systems with water storage tanks 2. Sizing solar olletors 3.

More information

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field Four-dimensional equation of motion for visous ompressible substane with regard to the aeleration field, pressure field and dissipation field Sergey G. Fedosin PO box 6488, Sviazeva str. -79, Perm, Russia

More information

Analysis of discretization in the direct simulation Monte Carlo

Analysis of discretization in the direct simulation Monte Carlo PHYSICS OF FLUIDS VOLUME 1, UMBER 1 OCTOBER Analysis of disretization in the diret simulation Monte Carlo iolas G. Hadjionstantinou a) Department of Mehanial Engineering, Massahusetts Institute of Tehnology,

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

FINITE WORD LENGTH EFFECTS IN DSP

FINITE WORD LENGTH EFFECTS IN DSP FINITE WORD LENGTH EFFECTS IN DSP PREPARED BY GUIDED BY Snehal Gor Dr. Srianth T. ABSTRACT We now that omputers store numbers not with infinite preision but rather in some approximation that an be paed

More information

Sample Teaching Sequence (Hong Kong Secondary 4 6 Chemistry)

Sample Teaching Sequence (Hong Kong Secondary 4 6 Chemistry) Revised (1 Sept 009 Sample Teahing Suene (Hong Kong Seondary 4 6 Chemistry Topi: Chemial Equilibrium Teahing Suene Content 1.1 Reversible reations Examples of reversible reation; forward reation; reverse

More information

Notation 2, 8, 1 2, 8, 2 2, 8

Notation 2, 8, 1 2, 8, 2 2, 8 Page 90 Atomi struture 2 1 a Contains 3 protons (1); and 4 neutrons (1) Page 90 Eletroni struture 2 a 2, 8 Type of reation Ionisation Nulear fission Nulear fusion Change in mass of nuleus Stays the same

More information

Modeling of Threading Dislocation Density Reduction in Heteroepitaxial Layers

Modeling of Threading Dislocation Density Reduction in Heteroepitaxial Layers A. E. Romanov et al.: Threading Disloation Density Redution in Layers (II) 33 phys. stat. sol. (b) 99, 33 (997) Subjet lassifiation: 6.72.C; 68.55.Ln; S5.; S5.2; S7.; S7.2 Modeling of Threading Disloation

More information

Replacement of gas phase with liquid, for hexamine production

Replacement of gas phase with liquid, for hexamine production Proeedings of the International Conferene on Ciruits, Systems, Signals Replaement of gas phase with liquid, for hexamine prodution Anita Kovač Kralj¹ Davorin Kralj² Faulty of Chemistry and Chemial Engineering,

More information

Computer simulation and verification of deliming process mathematical model

Computer simulation and verification of deliming process mathematical model Computer simulation and verifiation of deliming proess mathematial model Hana Charvátová, Dagmar Janáčová, ladimír ašek, Pavel Mokrejš, Karel Kolomazník Abstrat The paper deals with hemial deliming proess

More information

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state:

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state: CE304, Spring 2004 Leture 6 Volumetri roperties of ure Fluids, part 4 The generi ubi equation of state: There are many possible equations of state (and many have been proposed) that have the same general

More information

Multicomponent analysis on polluted waters by means of an electronic tongue

Multicomponent analysis on polluted waters by means of an electronic tongue Sensors and Atuators B 44 (1997) 423 428 Multiomponent analysis on polluted waters by means of an eletroni tongue C. Di Natale a, *, A. Maagnano a, F. Davide a, A. D Amio a, A. Legin b, Y. Vlasov b, A.

More information

Introduction to Exergoeconomic and Exergoenvironmental Analyses

Introduction to Exergoeconomic and Exergoenvironmental Analyses Tehnishe Universität Berlin Introdution to Exergoeonomi and Exergoenvironmental Analyses George Tsatsaronis The Summer Course on Exergy and its Appliation for Better Environment Oshawa, Canada April, 30

More information

THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE?

THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE? THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE? The stars are spheres of hot gas. Most of them shine beause they are fusing hydrogen into helium in their entral parts. In this problem we use onepts of

More information

The universal model of error of active power measuring channel

The universal model of error of active power measuring channel 7 th Symposium EKO TC 4 3 rd Symposium EKO TC 9 and 5 th WADC Workshop nstrumentation for the CT Era Sept. 8-2 Kosie Slovakia The universal model of error of ative power measuring hannel Boris Stogny Evgeny

More information

Study on the leak test technology of spacecraft using ultrasonic

Study on the leak test technology of spacecraft using ultrasonic SINCE2013 Singapore International NDT Conferene & Exhibition 2013, 19-20 July 2013 Study on the test tehnology of spaeraft using ultrasoni Yan Rongxin, Li Weidan Beijing Institute of Spaeraft Environment

More information

Chemistry (Physical chemistry) Lecture 10.

Chemistry (Physical chemistry) Lecture 10. Chemistry (Physial hemistry) Leture 0. EPM, semester II by Wojieh Chrzanowsi, PhD, DS Wyłady współfinansowane ze środów Unii Europejsiej w ramah EFS, UDA-POKL 04.0.02.-00-37/-00 Absolwent Wydziału Chemiznego

More information

III. SURFACE PROPERTIES III.A. SURFACE TENSION SURFACE PROPERTIES

III. SURFACE PROPERTIES III.A. SURFACE TENSION SURFACE PROPERTIES III. SURFACE PROPERTIES III.A. SURFACE TENSION GOAL: To investigate the influene of the solution onentration and/or the kind of the solute on the surfae tension INTRODUCTION Liquids tend to adopt shapes

More information

An Integrated Architecture of Adaptive Neural Network Control for Dynamic Systems

An Integrated Architecture of Adaptive Neural Network Control for Dynamic Systems An Integrated Arhiteture of Adaptive Neural Network Control for Dynami Systems Robert L. Tokar 2 Brian D.MVey2 'Center for Nonlinear Studies, 2Applied Theoretial Physis Division Los Alamos National Laboratory,

More information

Optimization of an ejector refrigeration cycle

Optimization of an ejector refrigeration cycle DOTTORATO DI RICERCA IN "Energetia a Tenologie industriali innovative" CICLO XXV COORDINATORE Prof. Maurizio De Luia Optimization of an ejetor refrigeration yle Settore Sientifio Disiplinare ING/IND10

More information

A model for measurement of the states in a coupled-dot qubit

A model for measurement of the states in a coupled-dot qubit A model for measurement of the states in a oupled-dot qubit H B Sun and H M Wiseman Centre for Quantum Computer Tehnology Centre for Quantum Dynamis Griffith University Brisbane 4 QLD Australia E-mail:

More information

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION VIII International Conferene on Frature Mehanis of Conrete and Conrete Strutures FraMCoS-8 J.G.M. Van Mier, G. Ruiz, C. Andrade, R.C. Yu and X.X. Zhang Eds) MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP

More information

CALCULATION OF THE HEAT TRANSFER AND TEMPERATURE ON THE AIRCRAFT ANTI-ICING SURFACE

CALCULATION OF THE HEAT TRANSFER AND TEMPERATURE ON THE AIRCRAFT ANTI-ICING SURFACE 7 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES CALCULATION OF THE HEAT TRANSFER AND TEMPERATURE ON THE AIRCRAFT ANTI-ICING SURFACE W. Dong, J. J. Zhu, X. H. Min Shool of Mehanial Engineering,

More information

Journal of Chemical and Pharmaceutical Research, 2014, 6(10): Research Article

Journal of Chemical and Pharmaceutical Research, 2014, 6(10): Research Article Available online www.jopr.om Journal of Chemial and Pharmaeutial Researh, 014, 6(10:441-449 Researh Artile ISSN : 0975-7384 CODEN(USA : JCPRC5 Modeling and simulation of a wetted-wall olumn for SO absorption

More information

Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene

Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene Exerpt from the Proeedings of the OMSOL onferene 010 Paris Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene M. Bekmann-Kluge 1 *,. errero 1, V. Shröder 1, A. Aikalin and J. Steinbah

More information

Process engineers are often faced with the task of

Process engineers are often faced with the task of Fluids and Solids Handling Eliminate Iteration from Flow Problems John D. Barry Middough, In. This artile introdues a novel approah to solving flow and pipe-sizing problems based on two new dimensionless

More information

ONLINE APPENDICES for Cost-Effective Quality Assurance in Crowd Labeling

ONLINE APPENDICES for Cost-Effective Quality Assurance in Crowd Labeling ONLINE APPENDICES for Cost-Effetive Quality Assurane in Crowd Labeling Jing Wang Shool of Business and Management Hong Kong University of Siene and Tehnology Clear Water Bay Kowloon Hong Kong jwang@usthk

More information

NUMERICAL SIMULATION OF ATOMIZATION WITH ADAPTIVE JET REFINEMENT

NUMERICAL SIMULATION OF ATOMIZATION WITH ADAPTIVE JET REFINEMENT Paper ID ILASS8--7 ILASS 28 Sep. 8-, 28, Como Lake, Italy A44 NUMERICAL SIMULATION OF ATOMIZATION WITH ADAPTIVE JET REFINEMENT Anne Bagué, Daniel Fuster, Stéphane Popinet + & Stéphane Zaleski Université

More information

Cavity flow with surface tension past a flat plate

Cavity flow with surface tension past a flat plate Proeedings of the 7 th International Symposium on Cavitation CAV9 Paper No. ## August 7-, 9, Ann Arbor, Mihigan, USA Cavity flow with surfae tension past a flat plate Yuriy Savhenko Institute of Hydromehanis

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

A Longitudinal Aerodynamic Data Repeatability Study for a Commercial Transport Model Test in the National Transonic Facility

A Longitudinal Aerodynamic Data Repeatability Study for a Commercial Transport Model Test in the National Transonic Facility NASA Tehnial Paper 3522 A Longitudinal Aerodynami Data Repeatability Study for a Commerial Transport Model Test in the National Transoni Faility R. A. Wahls and J. B. Adok Langley Researh Center Hampton,

More information

"Research Note" ANALYSIS AND OPTIMIZATION OF A FISSION CHAMBER DETECTOR USING MCNP4C AND SRIM MONTE CARLO CODES *

Research Note ANALYSIS AND OPTIMIZATION OF A FISSION CHAMBER DETECTOR USING MCNP4C AND SRIM MONTE CARLO CODES * Iranian Journal of Siene & Tehnology, Transation A, Vol. 33, o. A3 Printed in the Islami Republi of Iran, 9 Shiraz University "Researh ote" AALYSIS AD OPTIMIZATIO OF A FISSIO CHAMBER DETECTOR USIG MCP4C

More information

Lightpath routing for maximum reliability in optical mesh networks

Lightpath routing for maximum reliability in optical mesh networks Vol. 7, No. 5 / May 2008 / JOURNAL OF OPTICAL NETWORKING 449 Lightpath routing for maximum reliability in optial mesh networks Shengli Yuan, 1, * Saket Varma, 2 and Jason P. Jue 2 1 Department of Computer

More information

Homework Set 4. gas B open end

Homework Set 4. gas B open end Homework Set 4 (1). A steady-state Arnold ell is used to determine the diffusivity of toluene (speies A) in air (speies B) at 298 K and 1 atm. If the diffusivity is DAB = 0.0844 m 2 /s = 8.44 x 10-6 m

More information

EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS

EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS -Tehnial Note- EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS H.-M. Chu * W.-L. Li ** Department of Mehanial Engineering Yung-Ta Institute of Tehnology & Commere Ping-Tung,

More information

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics IOSR Journal of ehanial and Civil Engineering (IOSR-JCE) e-issn: 78-1684,p-ISSN: 30-334X, Volume 11, Issue 6 Ver. IV (Nov- De. 014), PP 1-6 Stress triaxiality to evaluate the effetive distane in the volumetri

More information

ELECTROCHEMISTRY Lecture/Lession Plan -1

ELECTROCHEMISTRY Lecture/Lession Plan -1 Chapter 4 ELECTROCHEMISTRY Leture/Lession Plan -1 ELECTROCHEMISTRY 4.1 Conept of eletrohemistry Eletrohemistry is a branh of hemistry where we will study how hemial energy an be transformed into eletrial

More information

The simulation analysis of the bridge rectifier continuous operation in AC circuit

The simulation analysis of the bridge rectifier continuous operation in AC circuit Computer Appliations in Eletrial Engineering Vol. 4 6 DOI 8/j.8-448.6. The simulation analysis of the bridge retifier ontinuous operation in AC iruit Mirosław Wiślik, Paweł Strząbała Kiele University of

More information

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip 27-750, A.D. Rollett Due: 20 th Ot., 2011. Homework 5, Volume Frations, Single and Multiple Slip Crystal Plastiity Note the 2 extra redit questions (at the end). Q1. [40 points] Single Slip: Calulating

More information

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013 Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it

More information

Supplementary Materials

Supplementary Materials Supplementary Materials Neural population partitioning and a onurrent brain-mahine interfae for sequential motor funtion Maryam M. Shanehi, Rollin C. Hu, Marissa Powers, Gregory W. Wornell, Emery N. Brown

More information

Temperature Control of Batch Suspension Polyvinyl Chloride Reactors

Temperature Control of Batch Suspension Polyvinyl Chloride Reactors 1285 A publiation of CHEMICAL ENGINEERING TRANSACTIONS VOL. 39, 2014 Guest Editors: Petar Sabev Varbanov, Jiří Jaromír Klemeš, Peng Yen Liew, Jun Yow Yong Copyright 2014, AIDIC Servizi S.r.l., ISBN 978-88-95608-30-3;

More information

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II Journal of Applied Mathematis and Computational Mehanis 2014, 13(2), 141-147 MATHEMATICA AND NUMERICA BAI OF BINARY AOY OIDIFICATION MODE WITH UBTITUTE THERMA CAPACITY. PART II Ewa Węgrzyn-krzypzak 1,

More information

What s New in ChemSep TM 6.8

What s New in ChemSep TM 6.8 What s New in ChemSep TM 6.8 January 2011 (Updated Marh 2011) Harry Kooijman and Ross Taylor In this doument we identify and desribe the most important new features in ChemSep. 1. New: GUI an diretly load

More information

STUDY OF INTERFACIAL BEHAVIOR OF CNT/POLYMER COMPOSITE BY CFE METHOD

STUDY OF INTERFACIAL BEHAVIOR OF CNT/POLYMER COMPOSITE BY CFE METHOD THE 19TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS STUDY OF INTERFACIAL BEHAVIOR OF CNT/POLYMER COMPOSITE BY CFE METHOD Q. S. Yang*, X. Liu, L. D. Su Department of Engineering Mehanis, Beijing University

More information

EE 321 Project Spring 2018

EE 321 Project Spring 2018 EE 21 Projet Spring 2018 This ourse projet is intended to be an individual effort projet. The student is required to omplete the work individually, without help from anyone else. (The student may, however,

More information