Research Article  Open Access
Anis Ghazouani, Sondes Boughammoura, Jalel M'Halla, "Studies of Electrolytic Conductivity of Some Polyelectrolyte Solutions: Importance of the Dielectric Friction Effect at High Dilution", Journal of Chemistry, vol. 2013, Article ID 852752, 15 pages, 2013. https://doi.org/10.1155/2013/852752
Studies of Electrolytic Conductivity of Some Polyelectrolyte Solutions: Importance of the Dielectric Friction Effect at High Dilution
Abstract
We present a general description of conductivity behavior of highly charged strong polyelectrolytes in dilute aqueous solutions taking into account the translational dielectric friction on the moving polyions modeled as chains of charged spheres successively bounded and surrounded by solvent molecules. A general formal limiting expression of the equivalent conductivity of these polyelectrolytes is presented in order to distinguish between two concentration regimes and to evaluate the relative interdependence between the ionic condensation effect and the dielectric friction effect, in the range of very dilute solutions for which the stretched conformation is favored. This approach is illustrated by the limiting behaviors of three polyelectrolytes (sodium heparinate, sodium chondroitin sulfate, and sodium polystyrene sulphonate) characterized by different chain lengths and by different discontinuous charge distributions.
1. Introduction
Conductivity is a powerful technique of high accuracy allowing the qualitative and the quantitative detection of ionic species even at low concentrations. On the other hand, it is well known that for electrolytes (or for electrolytes mixtures), it exists a universal linear limiting law relating the equivalent conductivity at high dilution to the square root of ionic strength . This concentration effect is caused by two sorts of ionic frictions: the electrophoretic effect and the ionic relaxation effect. This limiting law has been extended in the case of semidilute simple electrolytes [1–4]. In contrast, a completely satisfactory theory to describe the dynamic behavior in general and particularly the electrolytic conductivity of dilute flexible polyelectrolytes in aqueous solution is not yet available despite some interesting progress toward this objective [5–16]. This difficulty arises from the complex interdependence between polyion conformation, ionic condensation, screening effect, and frictional forces. Moreover, it is important to underline that these different attempts have ignored the influence of the translational dielectric friction on moving polyions as well as its dependence on concentration [17, 18]. The present paper is a supplementary contribution toward this goal in order to propose a general formal limiting equation expressing the influence of the effects cited above on the equivalent conductivity of polyelectrolytes, and applicable in the range of very dilute solutions for which the stretched conformation is favored and for which the electrophoretic effects and ionic relaxation effects are negligible. This approach will be illustrated by the behaviors of three polyelectrolytes (sodium heparinate, sodium chondroitin sulfate, and sodium polystyrene sulphonate) characterized by different chain lengths and by different discontinuous charge distributions.
2. Theoretical Model and Parameters
2.1. Presentation of the Cylindrical Model
For dilute polyelectrolyte solutions the long chains of ionized polymers are generally assumed to be completely stretched [5–13], so that each chain can be modeled as a cylinder of radius, structural length () and structural charge. On the other hand, as the linear distribution of the total charge is uniform, then the distance of separation between two successive ionizable groups is . Because of the ionic condensation effect, these charged groups are, in absence of additional salt (saltfree), partially neutralized only by counterions “” of charge and effective radius. According to Manning’s rodlike model () [6–12], the degree of ionic condensation () is independent on the counterions concentration so that , where is the Bjerrum length, is the Boltzmann constant, and is the permittivity of the solvent. In fact, experimental conductivity results are not in general in conformity with the current polyelectrolyte theories [10, 11, 14, 15]. In particular, we have proved that for more realistic polyelectrolyte models (rodlike or cylindrical models with finite length and models having ellipsoidal conformations of , focuses with ) [9–11], the corresponding degree of dissociation obeys in general to the Ostwald’s principle of dilution and consequently when . The degree was calculated on the basis of the twostate model [10] (double layer) proposed by Sélégny, Manning, Dobrynin, and Rubinstein [6–8], but in a different way. According to this approach, the condensed counterions are distributed on an ellipsoidal first layer of , focuses and minor axis, whereas the free counterions constitute the ionic atmosphere which can be represented by an ellipsoidal second layer having the same focuses , and a minor axis (see Figure 1). The thickness is a function of , and via the DebyeMSA screen parameter [1] and the Debye length . Notice that both first and second layers are equipotential surfaces of total charges equal, respectively, to and . In the case of the cylindrical model (, and ), calculation of needs the resolution of the following ensemble of implicit equations: and are the microscopic concentrations (number of particles/Å^{3}) of, respectively, the counterions and the polyions. is the structural volume of the cylindrical polyion. and are “the configuration functions” which depend on the conformation of the polyion. Notice first that (1) is a generalization to cylindrical polyions, of the Fuoss expression relative to the ionic association of simple electrolytes; and second, that in the restrictive case of Manning’s model () and for dilute solutions (), increases very slowly with dilution so that remains approximately constant in a large range of low concentrations. However, approaches toward only for some particular polyelectrolytes [10].
Notice also that (1) can be applied for ellipsoidal polyions of any shape (i.e., , and for all ).
2.2. Theoretical Conductivity of Cylindrical Polyelectrolytes in Dilute Solutions
In practice we measure the specific conductance of the polyelectrolyte solution in S·cm^{−1}. is related to the equivalent ionic conductivities and , respectively, of the polyion and the counterion as follows: where is the molar concentration of the polyions and is the total molar concentration of the counterions so that is the molar concentration of the free counterions, and () is the apparent (effective) charge of the polyion partially neutralized by the condensed counterions. The electroneutrality condition implies that . The equivalent conductivity of the polyelectrolyte is therefore defined by and depend on the concentration of the free counterions because of the brake effects on the moving ions (or on polyions) due to their ionic atmosphere. In general one distinguishes two different ionic friction effects [2–4, 9, 12]: (a) the electrophoretic effect which is a hydrodynamic friction on the ionic atmosphere transmitted to the central ion (or polyion) via solvent molecules, (b) the ionic relaxation effect due to the perturbation of the charge distribution of the ionic atmosphere by the external electrical field . This polarization effect induces on the moving central ion (or polyion) a local field opposed to . Quantitatively, these two effects appear in the expression of the ionic conductivity of simple ions (in our case, the counterions) via the corrective term and the relaxation term as follows: is the ionic equivalent conductivity of the counterion at infinite dilution which expresses both the hydrodynamic friction, due to the viscosity of the solvent (Robinson and Stokes [2]), and the dielectric friction effect (Zwanzig [19]). is determined experimentally by linear extrapolation at infinite dilution and according to the DebyeOnsager limiting equation [2], of the equivalent conductivity () (with the square root of the ionic strength ) of any corresponding simple electrolyte (e.g., if , we can choose ; extrapolation of in water at 25°C leads to ). The term is the Faraday, is the effective radius of the solvated counterion “”, is the radius of its ionic atmosphere, and is its corresponding DebyeMSA screen parameter. Notice that differs from the screen parameter relating to the polyion, because considering the high repulsion between polyions, we have assumed that the ionic atmosphere of the polyions is constituted only by free counterions; on the contrary, the ionic atmosphere of a counterion encloses both polyions and counterions. is the mean radius of the polyion (analog to the radius of gyration) which is also equal to the electrostatic capacitance (in c.g.s.u.e units) of the ellipsoidal (or cylindrical) polyion [17, 20]. Finally, the explicit expression of the ionic relaxation term will be examined at the end of this section because of its interdependence with the term relating to the polyions.
The expression of the equivalent conductivity of the polyion is more complex because its ionic equivalent conductivity at infinite dilution expressing both hydrodynamic friction and dielectric friction effect is experimentally inaccessible. Indeed, in contrast with simple electrolytes, ionic transport behavior of polyelectrolytes is not governed by any universal limiting law [5] allowing the determination of by an extrapolation method at infinite dilution. For this reason we decomposed the expression as follows [9]: The justification of the above equation is the following: the external electric field acting on the polyion polarizes its ionic atmosphere as well as its surrounding solvent molecules, which gives place to an ionic relaxation field and to a dielectric relaxation field slowing down the movement of the polyion. The velocity of the polyion can thus be written in two manners: is the actual electrical mobility of the polyion and is the Henry mobility [9, 21] so that and express, respectively, the ionic relaxation effect and the dielectric friction effect acting on the polyion. Equation (12) implies that The explicit expression of the Henry equivalent conductivity of the polyion is, [9], Accordingly, we can separate into two contributions: the purely hydrodynamic term due to the viscosity of the solvent, and the socalled electrophoretic term , so that It is remarkable to underline that the expression of coincides with the HubbardDouglass general relation [20] expressing the hydrodynamic mobility: of an arbitrarily shaped unspecified macroion of charge, in terms of its capacitance (generalization of Stokes’ law): We can therefore generalize the HubbardDouglass relation given by (17) to the Henry equivalent conductivity as follows [17]: is now the electrostatic Gouy capacitance (in c.g.s.u.e units) of the ellipsoidal (or cylindrical) capacitor constituted by the polyion and by its ionic atmosphere of mean radius : Notice that the relative importance of the electrophoretic effect can be evaluated by the ratio: This last equation implies that the electrophoretic effect vanishes in the range of highly dilute solutions, that is, when . It is also interesting to notice that certain authors [22] have described the electrophoretic mobility of polyions in polyelectrolyte solutions by means of the DebyeOnsagerMSA approach using the mean spherical approximation for the coil conformation of the polyion chain. The corresponding spherical hydrodynamic radius was evaluated according to StokesEinstein relation: , where is the self diffusion coefficient of the polyion at high dilution. The same spherical approximation could be used for the calculation of the ionic relaxation effect using Onsager relation applicable to spherical simple ions [3], therefore with: , if we assume that the ionic atmosphere is free of polyions. However, Manning has demonstrated that for infinite rodlike model (), remains sensibly constant, equal to 0.13. In order to conciliate the two results into a general expression one of the authors has proposed the following relation [9, 10]: so that when , then ; this limiting expression converges toward the DebyeOnsager relation concerning spherical ions. In contrast, for polyions of large length, , for all if .
On the other hand, according to linear irreversible thermodynamics (T.I.P) the different relaxation terms of all the “” species (ions or polyions) in solution are interdependent via the general relation [9, 14]: , with . This means that in the case of our binary system the two relaxation terms and , respectively, of the polyions and the counterions are equal: Lastly, because of the importance of the dielectric friction effect on a stretched polyion (which is the main subject of this paper) the friction term will be discussed in detail in the next paragraph.
2.3. Importance of the Dielectric Friction Effect on a Stretched Polyion
The aim of the present paragraph is to evaluate succinctly the frictional force on a slowly moving polyion due to dielectric loss in its surrounding medium. In fact, this dielectric friction effect depends on the conformation (shape) of the polyion. In order to show the link with previous works, we will start by presenting the general formal treatment adopted in all cases; hence we will recall the computation results relating to the spherical and ellipsoidal models. Then, we will treat, without going into the mathematical details, the specific case of a stretched polyion modeled as a chain of identical charged spheres, each one having a charge and a radius (a linear discontinuous distribution of ionized groups).
The general mechanism of dielectric friction is the following: when a sphere of charge and radius is submitted to a moderate external alternating field along the axis, it acquires a velocity , where is its electrical mobility. We indicate by the position of the center of the sphere at time . During its movement the charge induces at each point of the dielectric medium (solvent) defined by its radiusvector a timedependent polarization which is proportional to the displacement field created by at different anterior times : The module is the distance between the point and the center of the sphere at time . This noninstantaneous response results from the fact that each solvent molecule needs a relaxation time to be oriented along the radial field . Mathematically, the linear relation between and is given by the following convolution integral [17, 19]: with is the after effect function which depends on the delta function representing electronic relaxation and on the permittivities and , respectively, the static and the highfrequency dielectric constants of the solvent. For water at 25°C, and . Note that we have set the upper limit of the above integral to , because in general the dielectric relaxation time is small by comparison to t so that (vanishes rapidly) when .
In turn, this induced polarization exerts back on the charged sphere a resulting dielectric frictional force where is the so called dielectric relaxation field having a direction opposed to the external field . The general integral relation between the component of and the , , components of via and therefore is, [17], is the so called key integral defined by where . Integration is taken over the whole volume except the finite region including the charged sphere (or the polyion in general) from which the dielectric medium is excluded.
It is obvious that no dielectric friction occurs, when (immobile sphere) or when (instantaneous response so that ). In other words, the delay effect () causes a perturbation of the equilibrium distribution of solvent molecules around the moving sphere and therefore leads to a nonsymmetrical polarization responsible of the resulting dielectric relaxation field: . Consequently, linearity between causes and response implies that . On the other hand, as the dimension of the electrical relaxation force is , scaling analysis yields to .
More rigorous derivations of the expression of the dielectric frictional force on a charged sphere were performed successively by Zwanzig [19], Hubbard and Onsager [23], and Wolynes [24]. In particular, if the charged sphere of large radius is assumed to be a conductor then, hydrodynamic effects become small and all theories reduce to Zwanzig’s original result [19] which can be derived from (27) and (28) following the substituting of the explicit expression of given by (25) into (29): We can use the above equation to compute the dielectric friction effect on a spherical polyion of effective charge and radius . Indeed, according to (12) and (14), its velocity is given by with and the relative dielectric friction effect is defined by , therefore (30) leads to . If we explicit the expression of according to (19) and after replacing the relaxation time by its Debye expression in terms of the solvent radius and the viscosity so that , we obtain More recently, authors of [17] have demonstrated that this last expression remains valid even in the case of an ellipsoidal polyion of minor axis , interfocuses distance , and effective charge but with the proviso of replacing the spherical radius by an apparent ray which is a function of the eccentricity so that for and for .
Now, in the case of stretched chain of successive charged spheres of charge and of radius (, ), each sphere moving along direction with velocity undergoes from the polarized solvent molecules a dielectric frictional force , where is the local dielectric relaxation field. Because of the axial symmetry of the system around the axis, only the component of is different from zero: The corresponding key integral is defined by , , and are the components of the vector separating a point of the dielectric medium and the position of the charge at time . The principal difference between (25)–(29) relating to a spherical polyion and (32) and (33), comes primarily from the fact that the expression of the displacement field created by the stretched chain of charged spheres at is now This equation results from the principle of superposition so that (34) differs from (25) by the sum expressing the interference of the displacement field created at by at an anterior time , with the different due to the charges of the moving chain. Notice however that, if the distance: , between two successive charged groups, is sufficiently large (, i.e., ) so that: , then the dielectric friction undergone by the sphere is essentially due to polarized solvent molecules of its entourage. We could therefore neglect the interference effect and is reduced thus to ; in other words, each charged sphere of the moving polyion of radius and charge behaves as if it were alone to polarize the dielectric medium. Consequently, simple direct application of Zwanzig’s original result leads by analogy to (31) to the following obvious equation: Recent calculations [18] based on (14), (27), and (32)–(34) including the interference effect lead to the following corrected expression in replacement to the above expression of : Notice that (35) and (36) are valid only in the case of slowly moving polyions so that . The evaluation of the interference effect in terms of the “interference parameter” is quantified by the ratio between in presence of interference and in absence of interference: This equation shows that for a discontinuous charge distribution, that is, , the interference effect becomes negligible. In contrast, it is maximal for a chain of tangent spheres () and increases with .
It is interesting to note that increases with dilution as and it reaches its maximal value at infinite dilution, that is, when (Ostwald) and : Finally it is important to underline the singular case of Manning’s polyions ( and , ). Because of the infinite length of its moving chain, the structural state of the polyion (distribution of charges, distribution of solvent molecules, and therefore ) varies periodically with time with a period equal to: . As for slowly moving polyions, , therefore , that is, the solvent molecules have not sufficient time to reorient themselves toward the new field during the periodic variation. Consequently, the polyion seems to be immobile () and thus surrounded by its initial symmetrical cylindrical distribution of solvent molecules. This conservation of the equilibrium symmetry implies the absence of any resulting dielectric relaxation field (). It is the reason for which the dielectric relaxation effect is completely absent in the restrictive case of the Manning’s model.
3. Results and Discussion
In order to emphasize the importance of the dielectric friction on stretched polyions at high dilution we studied the conductivity behaviors of the following polyelectrolytes: sodium heparinate of high molecular weight (RB21055), sodium chondroitin sulfate, and sodium polystyrene sulphonate (NaPSS). Details of the experimental protocols of conductivity measurements are given in previous papers [9–11]. Notice that conductivity results concerning (NaPSS) are those published by Vink [14]. Comparisons for each polyelectrolyte, between experimental equivalent conductivities and theoretical equivalent conductivities calculated in absence or in presence of dielectric friction and also in absence or in presence of interference effect, are given in Tables 1–3 and Figures 2, 3, and 4. In each table we show the different molar total concentrations of counterions, the experimental equivalent conductivities , the degrees of condensation () on polyions, the apparent charge numbers of the polyions, the theoretical equivalent conductivities in absence of dielectric friction (i.e., only: hydrodynamic, electrophoretic, and ionic relaxation effects), the group radius , the theoretical equivalent conductivities in absence of interference, the theoretical equivalent conductivities in presence of interference, the % of the dielectric friction effect (36) in presence of interference, and the ratios (37) expressing the relative importance of the interference effect ( is the dielectric friction effect in absence of interference).



3.1. Conductivity of Sodium Heparinate (RB21055)
The biological polyelectrolyte sodium heparinate (RB21055) is a linear polysaccharide, well known for its anticoagulant activity. Its monomer unity is a hexasaccharide, in which each disaccharide consists in a glucosamine followed by an uronic acid. The charged groups are ( or ) and with a ratio . This heparin is provided by Sigma as a sodium salt extracted from pork stomach. The physical characteristics of the Sodium heparinate (RB21055) are as follows: is the average molecular weight of the Sodium Heparinate (RB21055). at is the structural charge number. Å is the structural length. Å is the chargetocharge distance. Å is the cylindrical radius of the polyion chain.
Table 1 shows that the variation of the degree of dissociation of from heparin in the concentration range: is in conformity with the dilution principle so that increases with dilution from 0.59 to 0.76 and it differs from its Manning’s value . Consequently, the apparent charge number varies with the concentration from −37.8 for to −29.5 for . Notice that this last value seems to be different from the value obtained from electrophoretic mobility using NernstEinstein relation: with cm^{2}·s^{−1} [22]. In fact differs from because it depends at the same time on ionic condensation and on ionic friction effects via . Table 1 and Figure 2 show that the experimental conductivity of sodium heparinate (RB21055) decreases sharply from 82.6 to in the low concentration range: . Theoretically, the hydrodynamic contribution (at infinite dilution) to is obtained in absence of ionic condensation , of ionic frictions (, ) and in absence of dielectric friction . According to (6), (10), (16), and (17), with , . The mean radius of heparinate (RB21055) is calculated from (10). We found , , and . Table 1 shows that the dielectric friction is the most significant retarding effect by comparison to the electrophoretic effect and the ionic relaxation effect even when taking into account the interference of the local displacement fields. Now, as is proportional to then , which means that increases with dilution toward its maximal value at infinite dilution (). According to (38), depends on the interference factor . Adjustment between experimental conductivities and theoretical conductivities of heparinate (RB21055) leads to a group radius equal to so that (a succession of tangent charged spheres). The maximal value is therefore equal to , for , , and . Consequently, the correct limiting conductivity at infinite dilution must take into account the limiting dielectric friction effect in addition to the hydrodynamic friction as follows: . This is experimentally inaccessible because of the nonexistence of a universal limiting law allowing a rigorous extrapolation of at infinite dilution. This impossibility is due primarily to ionic condensation effect. However, according to (6), (7), and (11), and after neglecting ionic friction effects, we can derive the following approximate complex relation between and applicable in the range of very dilute solutions for which the stretched conformation is favored and for which the electrophoretic effects and ionic relaxation effects are negligible: This expression can be used as an indirect method to evaluate experimentally the degree of ionic condensation from experimental measurements of the equivalent conductivity of the polyelectrolyte at high dilution. Calculation shows that for , in conformity with theoretical values ((1)–(4)) but incompatible with the Manning’s value . It is important to notice at this stage that the constancy of the condensation parameter at high dilution with would imply that increases first with dilution then attains a “palier” (platform) in the range of very low concentrations in which obeys to the Manning’s model. This kind of behavior is not in general experimentally observed [14].
In order to reinforce the hypothesis of the stretched conformation at high dilution we will compare the equivalent conductivity of sodium heparinate calculated in the case of coiled conformation (quasispherical) having a mean radius , to its corresponding experimental equivalent conductivity . According to ZwanzigFrank notation [19, 25] the expression of the equivalent conductivity of the spherical polyion at very high dilution is , with , at 25°C in water, Å, and . The equivalent conductivity of the (spherical) sodium heparinate is therefore . Now, according to the ionic association theory of Fuoss [3] the degree of dissociation: for M, therefore . This expected result is at least twenty percent larger (20%) than the experimental equivalent conductivity (), and it therefore invalidates the hypothesis of spherical conformation for heparin RB21055 polyions at high dilution. Finally it is important to underline the following principal conclusions.(i)The interference effect decreases by 70%–60% the dielectric friction on the stretched polyion. However, despite this important attenuation, the resulting dielectric friction remains the principal frictional effect ( decreases with concentration from 78% to 50%) in comparison to ionic relaxation effect and electrophoretic effect. (ii)The adjustment of the experimental equivalent conductivities with the theoretical conductivities leads to a group radius sensibly constant, of about Å, that is, equal to the half of the distance Å between two successive spherical charged groups, so that the coherent condition: is verified in the studied concentration range. (iii)The ionic relaxation effect on polyions and counterions becomes important (10%–20%) for M, while is for highly dilute solutions. This result is not in conformity with the Manning prediction: . (iv)The electrophoretic effect is relatively weak for counterions (), while it decreases as expected with dilution from 28% to 4% in the case of stretched heparin polyions. (v)The degree of ionic condensation () of on heparin RB21055 increases in % with the concentration from 24% to 41% and differs from the Manning value: 56%.(vi)The sharp increasing with dilution of the equivalent conductivity of sodium heparinate proves that both thermodynamics behavior and electrolytic conductivity behavior of this polyelectrolyte are governed by the Ostwald concentration regime despite the stretched conformation of heparin polyions.
3.2. Conductivity of Sodium Chondroitin Sulfate
The biological polyion chondroitin sulfate is a large linear polysaccharide composed of repeating disaccharide units altering an amino sugar acetylgalactosamine4sulfate and an glucuronic acid. The sulfate groups as well as the uronic acids result in linear chains having a negative charge. Chondroitin sulfate is provided by Sigma as a sodium salt from bovine trachea. The physical characteristics of the macroion are [10, 11] as follows: is the average molecular weight of the used polyelectrolyte. is the structural charge number. Å is the structural length. Å is the chargetocharge distance. Å is the cylindrical radius of the polyion chain.
This polyion is therefore about three times longer than heparin RB, and regarding its significant charge separation , it presents a more discontinuous linear charge distribution. On the other hand, according to Manning’s theory, we expect a weaker degree of condensation () despite the relative importance of its structural charge number. Table 2 shows that the degree of dissociation of from chondroitin increases slightly with dilution from 0.804 to 0.852 in the concentration range: . Sodium chondroitin sulfate is one of peculiar polyelectrolytes for which the behavior of ionic condensation in aqueous solution is compatible at the same time with the model of Manning and with the principle of dilution [10, 11]. Indeed, the Manning’s value of the condensation parameter is . Consequently, the apparent charge number varies slightly with the concentration from −63.9 for to −60.3 for .
Table 2 and Figure 3 show that the experimental conductivity of sodium chondroitin increases with dilution in a monotonous way from 65.3 to 78.54 in the concentration range: , (i.e., without the appearance of any palier). The hydrodynamic contribution (at infinite dilution) to is obtained in absence of ionic condensation and in absence of other frictional effects from (6), (10), (16), and (17), so that with with . The mean radius of the chondroitin sulfate is equal to 50.8 Å, therefore and . Table 2 shows also that the dielectric friction () is the most significant retarding effect by comparison to the electrophoretic effect and the ionic relaxation effect even when taking into account the interference of the local displacement fields. depends on the interference factor . Adjustment between experimental and theoretical conductivities of chondroitin sulfate leads to a group radius equal to Å so that (a discontinuous linear charge distribution), the maximal value is, according to (38), equal to for , , and . Consequently, the new limiting must take into account the limiting dielectric friction effect in addition to the hydrodynamic friction as follows: . This is experimentally inaccessible. However, according to our previous analysis and to (6), (7), and (11), we can proceed in the same manner that for Heparin RB21055 in order to derive the following approximate relation between the experimental equivalent conductivity of chondroitin sulfate and the degree of dissociation in the range of very dilute solutions for which the stretched conformation is favored and for which the electrophoretic effects and ionic relaxation effects are negligible, we obtain