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Hydrometallurgy A general shrinkingparticle model for the chemical dissolution of all types of cylinders and discs
A general shrinkingparticle model for the chemical dissolution of all types of cylinders and discs
C. Núñez, M. Cruells, L. GarcíaSotoآپ کو یہ کتاب کتنی پسند ہے؟
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جلد:
36
سال:
1994
زبان:
english
صفحات:
10
DOI:
10.1016/0304386x(94)900272
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PDF, 398 KB
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hydrometallurgy ELSEVIER Hydrometallurgy 36 (1994) 285294 A general shrinkingparticle model for the chemical dissolution of all types of cylinders and discs C. N f f i e z a'*, M. Cruells b' 1, L. GarciaSoto a aE. T.S. de Ingenieros Industriales, Mendizabal s/n (Esteiro), 15403 Ferrol, La Coruga, Spain bFacultad de Quimica, Departemento de Ingenieria Quimica y Metalurgia, Avda. Diagonal 64 7, 7° Piso, 08028 Barcelona, Spain Received October 12, 1993; revised version accepted January 14, 1994 Abstract There is a manifest lack of models with exact solutions for describing the kinetic behaviour of cylindrical solids in reactions under chemical control and for determining the kinetic constants of the reaction system. This paper deduces two models that offer exact solutions: one for any type of cylinder with a diameter less than the height and another for any type of disc with a diameter greater than the height. It is demonstrated that the approximate kinetic model proposed in the literature for cylinders is actually the exact model for a regular toroid. Finally, we propose a single model for any type of cylinder or disc, making use of the socalled kinetic sphere radius. I. Introduction Deducing simple kinetic models for the chemical dissolution of bodies of various geometric shapes is one of the most primary and elementary of tasks in heterogeneous kinetics and has become part of the body of doctrine in the field. In spite of the large number of models proposed, very little attention has been paid to the deduction of a kinetic model for dissolving cylinders. At present we have no exact model for the dissolution of cylinders or discs and only approximate solutions are available [ 13 ]. For the purpose of modelling the behaviour of a cylindrical solid when it is dissolved in a reagent under chemical control, it has been assumed that, for a cylinder of sufficient length, such as a wire, the input of the bases to the amount tAuthor for correspondence. 0304386X/94/$07.00 © 1994 Elsevier Science B.V. All; rights reserved SSDI 0304386X ( 94 )000060 C. Nft~ez et aL / Hydrometallurgy 36 (1994) 285294 286 [_ "1% Io j " Fig. 1. The dimensions of interest in modelling a cylinder of/o> 2ro. of solid dissolved is negligible, which allows the solid to dissolve only according to the area of the cylindrical surface. This means that the length of the cylinder (l) can be taken as constant and only the radius of the cylinder base (r) diminishes during the reaction. Under these conditions, the following model can be deduced for a reaction like the one described in Eq. (2) below: 1  (1  x ) ½=flkqC~'t paro (1) where: x = fraction reacted; fl= stoichiometric coefficient; kq = chemical constant (varies only with temperature); C~, = activity of the reagent in the fluid phase, raised to its order, a; PB = molar density of cylindrical solid; t = time; ro and lo are the initial radius of the base and the initial length of the cylinder, respectively (Fig. 1). As shown below we will see that this approximate model for sufficiently long cylinders, as presented in the literature, is actually the exact kinetic model for the dissolution of a toroid under chemical control. The model in Eq. (1) begins to show considerable errors when the cylinder length approaches the value of its diameter. It becomes unacceptablenot because of larger errors but because it is not applicablewhen the cylinder has a size of 2ro > 10. Those cases in which the cylinder diameter is greater than its height are perhaps the most interesting for industry and, as yet, are lacking an adequate kinetic model as simple as other accepted models currently in use. This paper presents two models: one for cylinders and another for discs, but they are the same and are exact and valid for any cylinder or disc. 2. A general kinetic model for cylinders This model will be applied, in principle, only to cylinders of diameter 2ro and height lo, such that: 2ro < lo. Let us consider a solid (B), compact, kinetically isotropic and homogeneous, which is dissolved under chemical control in a reagent (A), present in the fluid phase to give certain products, according to the following stoichiometry: C. N~fiez et al. /Hydrometallurgy 36 (1994) 285294 Ali q ~ flBso I ~. Products 287 (2 ) From a batch mass balance, let v be the reaction rate, defined by: V= 1 dN A k C '~ S ~ ~ q A (3) where: S = t h e solid surface area and NA= number of moles of reagent A; other symbols as in Eq. ( 1 ). Since: fldNA =dNB (4) dNs =pBdV (5) where: NB = number of moles of reagent B; V= volume of solid B. From this point on, any magnitude bearing the subscript o refers to its value at the initial moment, t=0. Combining Eqs. (4) and ( 5 ) with Eq. ( 3 ) and solving, we get [ 4 ]: v f dV y=L[flkqC~'] jt=v,t (6) Vo To integrate the first member of this equation, let us assume a cylinder like the one in Fig. l, where h is the uniform thickness reduced by a certain time of chemical reaction [ 5 ], so that: r=ro  h (7) l=lo2h (8) With these equations, the value of l in terms of r will be: l=(lo2ro)+2r (9) The expressions for the volume and surface area of the cylinder, respectively, are: V=rcr2l (10) S= 2~rl + 2rcr2 ( 11 ) Substituting the value of l, as given by Eq. (9), in these two equations we get: V= ~(10 2ro)r2+2~r 3 (12) S= 2~( lo  2ro )r + 6gr 2 (13) Differentiating Eq. ( 12 ) with respect to r and dividing it by Eq. ( 13 ), we get: d~=dr=dh (14) C. Nt~gezet aL / Hydrometallurgy36 (1994)285294 288 Substituting this value of d V/S in Eq. (6) and solving, the result is: lr=FflkqC~q~Vlt ro l PB Aroro (15) This is the valid kinetic model for the dissolution of all /o>2ro cylinders. Nevertheless, to follow up the reaction by chemical analysis, the relation between the cylinder radius and the fraction reacted is as follows: r21=ro2(1x) lo (16) Substituting the value of I as given in Eq. (9), and ordering, we get: r3k ( / o  2 r o ) 2 ro2lo,, 2 r ~t,x) =0 (17) Eq. ( 17 ) enables us to calculate the value of r that satisfies Eq. ( 15 ) for each experimental value of x. By obtaining a sufficient number of values for r we can plot r o  r against t and, adjusting the points to a straight line, we can find the slope (v 1 )the brackets in Eq. ( 15 ). We can get values for v~ by carrying out experiments at various values of CA. Using the logarithm of v~ with these data, we get the following: logv I ~" log flkq + txlOgCA PB ( 18 ) Experimental adjustment to this straight line enables us to find the chemical constant (kq) and the order ( a ) of reagent A, and several values of kq obtained in experiments at constant CA and different temperatures will allow us to determine the activation energy. 3. A general kinetic model for discs Let us consider a disc like the one in Fig. 2, in which 2ro > lo. After a certain time the chemical reaction makes the disc thinner; in this case the greatest input to the dissolution comes from the solid dissolved at the base of the cylinder. The disc finally disappears w h e n / = 0 , but at this time r > 0 and we cannot use the model of Eq. (15 ) to describe the kinetic behaviour of the disc. Since the disc begins to react when l = lo and disappears when l = 0, the model to be deduced must be expressed in terms of/. To do this we solve for r in Eq. (9) and substitute this value in Eqs. ( 10) and ( 1 1 ) to arrive at the following equations for the volume (V) and surface area (S) of the disc: V=4[132(lo2ro)/2+ (lo  2ro)2l] (19) S=213124(lo  2ro)/+ ( l o  2 r o ) 2] (20) C. Nft~ez et al. / Hydrometallurgy 36 (1994) 285294 I ~ 289 ,_ ro i 21 m / h~ u~!l L_J I Fig. 2. The dimensions of interest in modelling a disc of 1o< 2ro. R is the radius of a sphere inscribed in the disc, or the kinetic radius. Differentiating with respect to l in Eq. ( 19 ) and dividing it by Eq. (20), the result is: dV dl dh S 2 (21) If we say that l/2=R, with R as the radius of a sphere inscribed in the disc tangent to its two bases, called a kinetic sphere [4], and therefore a function of the radius of the kinetic sphere, then dl/2 = d R and lo/2 =Ro; substituting the value of d V/S in Eq. (6) with dR and solving, we get: R flkqC~] t v ~ I ~o = [ ~ _ ~ o =~ool (22) This is the general kinetic model for all discs of the type 2Ro = lo < 2to in terms of the radius of the socalled kinetic sphere (R), which takes a shape like the one inEq. (15). The chemical followup of the reaction is based on the ratio between volume and fraction reacted (see Eq. 16 ), substituting l or lo with 2R or 2Ro, respectively, and r with its value in (roRo) +R. Substituting these values, operating and ordering, we get: R 3  2 (ro Ro)R2 4 (to Ro)2RroR~( 1  x ) = 0 (23) For each experimental value of x, Eq. (23 ) gives the corresponding value for R, which satisfies Eq. (22). From here on we proceed in the same way as described for finding kq and o~ in the case of cylinders. 4. D i s c u s s i o n A particular case in the family of cylinders is the one in which 2ro = 1o (an 'isometric' cylinder). In this case, Eqs. (15) and (22) are still valid, since ro=Ro C. Nfi~ez et al. / Hydrometallurgy 36 (1994) 285294 290 and r=R; that is, the radius of the sphere inscribed in the cylinder (R) coincides at all times with the radius (r) of the cylinder base. Nonetheless, an exact model has been proposed for this isometric cylinder [6 ] in terms of an initial equivalent radius of the solid and its sphericity factor. Note that ro in Eq. ( 15 ) and Ro in Eq. (22) are actually the radius of the sphere inscribed in the cylinder and in the disc, respectively; therefore, these two equations are exactly the same, if we consider that the r or R that must always be introduced into the model is the radius of the inscribed sphere. For the purpose of comparing the approximate model ofEq. ( 1 ) with the model for a toroid, we can briefly deduce the kinetic model for dissolving a toroid like the one in Fig. 3 under chemical control. At any given time during the reaction, the volume of the toroid is given by: 7~2 V=~(a+b)(ba) 2 (24) and the surface area by: S=nZ(a+b)(ba) (25) Considering that for the toroid: (a+b)=(ao +bo) ba=2r (26) (27) Eqs. (24) and (25) become: V=n2(ao +bo)r 2 (28) %,\ • I, _ ' i/ Fig. 3. The dimensions of interest in the crosssection o f a toroid. C. N~t~ez et al. / Hydrometallurgy 36 (1994) 285294 S=2nZ(ao +bo)r 291 (29) Differentiating Eq. (28) for r and dividing it by Eq. (29), we get: dV=dr= dh S (30) Substituting this value for d V/S in Eq. (6) and integrating, we get Eq. ( 15 ). The basis for expressing it in terms of fraction reacted is: V= Vo( 1  x ) . From this we deduce that: r=ro(1x) ½ (31) If we then substitute this value in Eq. ( 15 ), we get Eq. ( 1 ), which turns out to be the exact model to describe the reaction of a toroid under chemical control. In order to look at the x curves (fraction reacted) against time (t), we chose a range of values for ro and lo, but always with the condition that the volume of the bodies analyzed is the same and equal to 10n: ( 1 ) a reference sphere: V= 10n; ro= 1.957; (2) a cylinder of lo>2ro: V= 10n; ro= 1.581; •0=4; (3) a disc oflo< 2ro: V= 10n; ro=2.236;/0=2; (4) a cylinder like (2) but with the approximate Eq. ( 1 ) applied to it, using the actual data for the fraction reacted of cylinder 2; (5) a toroid: V= 10n; ro= 1; bo= 1 + ( 5 / n ) ; ao= ( 5 / n )  1. We took the arbitrary value of vl =0.2 for all cases. We then proceeded to calculate the fraction reacted (x) in terms of time (t), and the values of vtt/ro in terms of the fraction reacted for each of the five bodies listed above. ( 1 ) For the reference sphere we took: V i i _ 1_ ( l _ x ) ~ (32) r0 The final time that it takes for this sphere to dissolve is calculated from Eq. (7), using r = 0; considering that h = v~t and solving for t, we get: t = 9.787. (2) The final dissolution time for the cylinder will be: t = 7.906. (3) The final dissolution time for the disc, depending on the dimensions chosen, will be: t = 5. (4) The actual values for the fraction reacted of cylinder 2 were applied to the approximate model in Eq. ( 1 ), calculating v~t/ro. In this case the dissolution time for the cylinder is the same as for cylinder 2: t = 7.906. (5) We used Eq. ( 1 ) for the toroid, which is its exact equation. The final dissolution time for the toroid is: t = 5. Fig. 4 shows the fraction reacted (x) plotted against time. In the first place, the final dissolution time depends on the value chosen for the minimum thickness of each body. We can see that the sphere, as a body of minimum surface area per unit of volume, is the one that takes the longest to dissolve, when it and all the C. Nt~ftez et al. /Hydrometallurgy 36 (1994) 285294 292 ),0 O / 016 / ~ Or4 / 0 A • • 1 2 3 4 • 5 0¢2 t I I 2 I I 4 i I 6 I I I 8 Fig. 4. The fraction reacted (x) plotted against time (t) for the bodies referred to in the text. 1 = sphere; 2 = cylinder; 3 = disc; 4 cylinder; 5 = toroid. bodies are of the same volume. The x/t curves for discs and toroids give larger fractions reacted for each reaction time since they have much more surface area per unit of volume than the sphere. The fraction reacted for cylinder 4 calculated with the value of x taken from the approximate model of Eq. ( 1 ) leads to errors by default, with lower fraction reacted predictions than for cylinder 2 and even for the sphere, which is unacceptable. The x/t curve for cylinder 2 is the correct one and does not differ greatly from the curve for the sphere since we chose a near equiaxial cylinder in order to see clearly the consequences of ignoring the reaction on the base area. The straight lines obtained in Fig. 5 terminate at the final dissolution time values previously chosen for the bodies. We can see that the approximate model of Eq. ( 1 ) applied to a cylinder with dimensions like number 2 does not give a straight line. Nevertheless, up to fraction reacted values of 0.8 we can assume that the slope corresponds to the dotted line, which would lead to errors of up to approximately 30% in estimating kq for the cylinder being analyzed. Finally, since real solids are not uniform or rigorously isotropic, dissolution is not homothetic and the reaction takes place preferably in areas that are more active in energy terms, leading to pitting, caused by the presence of impurities, concentration of dislocations, residual stresses, etc. Nevertheless, we can expect that for low concentrations of defects and moderate fraction reacted rates, we can use these models for an acceptable determination of the chemical constants in a reaction. Furthermore, this is the first time that an exact model has been pre C. Nftgez et al. I Hydrometallurgy 36 (1994) 285294 ,,o,.,. 293 i, _;'°/ / //..// o,8 / /,* / d IS// OI4 Oa2 5 t I I 2 I I 4 I I 6 I I I 8 Fig. 5. Plot of vlt/ro against time (t) for the bodies referred to in the text. 1 =sphere; 2=cylinder; 3 = disc; 4 = cylinder; 5 = toroid. sented to describe the kinetic behaviour of cylinders, discs and toroids of all types, which completes the set of simple basic models in heterogeneous kinetics. 5. Conclusions The mathematical treatment presented in this paper makes it possible to propose a single model, in terms of the radius of the inscribed sphere, to describe the kinetic behaviour of cylinders and make exact predictions for the behaviour of cylinders, discs or toroids in reactions under chemical control. It can also be used to determine the kinetic constant, the order of reagent A and activation energy of the reaction system, as long as the solid is reacted uniformly, because in the basic models of heterogeneous kinetics the solid is assumed to be pure, homogeneous and isotropic. References [ 1 ] Levenspiel, O., Ingenieria de las Reacciones Quimicas. Table 121. Revertr, Barcelona ( 1974 ), p. 409. [ 2] Sohn, H.Y. and Wadsworth, M.E., Rate Processes of Extractive Metallurgy. Plenum Press, New York (1979), p. 144. [ 3 ] Habashi, F., Principles of Extractive Metallurgy. Vol. I. Gordon and Breach, New York ( 1969 ), p. 137. 294 C. N ~ e z et al. / Hydrometallurgy 36 (1994) 285294 [4] Ntifiez, C., Vifials, J., Roca, A. and GarciaSoto, L., A general shrinkingparticle model for the chemical dissolution of crystalline forms. Hydrometallurgy 36 (1994), in press. [ 5 ] B. Delmon, Introduction ~ la Cin6tique H6t6rogbne. Technip, Paris ( 1969 ), 281 pp. [ 6 ] Ntifiez, C. and Espiell, F., The shape of bodies and its consequences on the chemical attack of solids. Chem. Eng. Sci. 41 (8) ( 1986): 20752083.