- freely available
- re-usable

*Polymers*
**2014**,
*6*(4),
1207-1231;
doi:10.3390/polym6041207

Published: 22 April 2014

## Abstract

**:**In this review, we focus on the electrical conductivity of aqueous polyelectrolyte solutions in the light of the dynamic scaling laws, recently proposed by Dobrynin and Rubinstein, to take into account the polymer conformations in different concentration regimes, both in good and poor solvent conditions. This approach allows us to separate contributions due to polymer conformation from those due to the ionic character of the chain, and offers the possibility to extend the validity of the Manning conductivity model to dilute and semidilute regimes. The electrical conductivity in the light of the scaling approach compares reasonably well with the observed values for different polyelectrolytes in aqueous solutions, over an extended concentration range, from the dilute to the semidilute regime.

## 1. Introduction

Polyelectrolytes are polymers that bear a large number of ionizable groups distributed along their chain. In aqueous solution and under appropriate conditions, these polymers dissociate, leaving ionized charged groups on the polyion backbone and counterions in the bulk solution [1,2,3]. Examples of polyelectrolytes include poly(styrenesulfonate), poly(acrylic acid), poly(methacrylic acid) and their salts, DNA, and other polyacids and polybases.

Polyelectrolytes have attracted much attention in the last decades because of their unusual properties, since the long-range nature of the electrostatic interactions due to the charge distribution along the chain introduces new length and time scales. The delicate balance between attractive hydrophobic interactions and repulsive electrostatic interactions governs the structural and dynamical properties of these systems. One of the most important property of polyelectrolytes is that, because of the dissociation of the ionizable groups along the chain, there is only a partial release of counterions into solution, resulting in an effective (renormalized) charge of the polyion chain significantly lower than its bare structural charge (counterion condensation).

This phenomenon is due to a fine interplay between electrostatic attractions of counterions to the polymer chain and the loss of their conformational entropy due to the localization in the vicinity of the polymer backbone. Counterion condensation strongly influences the transport and the thermodynamic properties of polyelectrolyte solutions.

In order to give a unifying picture of the conductometric properties of these systems, we have proposed a scenario able to take into account different concentration regimes, based on a scaling approach to the dynamic properties of a polyelectrolyte chain.

In this review, we summarize the main results and collect the relevant expressions governing the electrical conductivity of a polyelectrolyte solution in different experimental conditions, on the basis of a series of our own papers, appeared in the last few years [4,5,6,7,8,9,10,11,12,13,14,15,16].

Electrical conductivity is the key parameter for the understanding of the coupling between chain conformation and counterion condensation. This coupling is of particular importance in biological polyelectrolytes, such as DNA, where the conformation influences the biological functions. Moreover, in the light of this coupling, the knowledge of the electrical conductivity allows the evaluation of the effective charge of the polymer chain in the solution and the scaling approach can be used to calculate this charge in the most general conditions, i.e., for polyion of different molecular weights, at different concentrations and in the presence or absence of added salt.

The scaling concepts applied to polyelectrolyte solutions have been successfully proposed many years ago, and more recently, Dobrynin, Rubinstein et al. [17,18,19,20] have given a description of the charged polymer conformation in different concentration regimes, covering both the dilute and semidilute region.

On the basis of this scaling treatment, we have proposed a modified version of the Manning counterion condensation model [21,22,23] in order to take into account the different chain conformations, which dominate in the low-concentration limit from those which become prominent with increasing concentration (semidilute and concentrated regimes). The scaling theory predicts the dependences of observables, such as the chain extension in the different concentration regimes on various parameters, such as the fraction f of free counterions and the number and the size of each characteristic unit along the polymer chain.

We will begin our analysis by listing the basic features of the counterion condensation theory originally proposed by Manning [21,22,23], based on the charge renormalization due to the partial collapse of counterions on the polyion backbone.

Consider an aqueous polyelectrolyte solution, made up of polyion chains, each with a degree of polymerization N, contour length L, at a concentration C_{p}. Each monomer, of size b_{struct} = L/N, bears an ionizable group of valence z_{p}. In fully ionization condition, each chain will have a charge Q_{p} = z_{p}eN and will release in the solution Nv_{1} counterions, each of charge q_{1} = z_{1}e.

However, at finite concentration, some counterions, owing to the interplay between the electrostatic interactions and the change in entropy due to their spatial confinement, may condense on the polyion itself, thus, reducing its effective charge. This phenomenon, known as counterion condensation, has been described in detail by Manning [24,25,26]. According to the Manning model, the system is characterized by a charge-density parameter ξ, defined as the ratio of the Bjerrum length l_{B} and the structural charge spacing b_{struct} :

_{w}is the permittivity of the aqueous phase and K

_{B}T the thermal energy. Here, the Bjerrum length is defined as the length scale at which the Coulomb interaction between two elementary charges in a dielectric medium with a dielectric constant ε

_{w}is equal to the thermal energy K

_{B}T.

If the charge spacing is too small, the electric field becomes so strong that the system can lower its free energy by condensing some of the counterions on the polyion chain. If:

Counterions of valence z_{1} become trapped close to the polyion chain (counterion condensation) to reduce its effective charge from the value Q_{p} = z_{p}eN (before condensation) to the effective value:

So that the fraction of free (un-condensed) counterions will be:

The charged polyion, together with the condensed counterions, can be considered as a single entity with an effective charge Q_{p eff} which is considerably lower than the bare structural charge Q_{p}.

Within this model, polyion and condensed counterions, under the influence of an external electric field, move together with the same mobility u_{p}. However, in the infinite polyion length limit and in the presence of high salt content, simulations have recently shown that this motion decouples and condensed counterions acquire a mobility with respect to the polyion itself [27].

It must be noted that condition (1.4) strictly holds in the case of an infinite isolated linear polyion chain. In the case of finite length rod-like polyions, at a finite concentration, a counterion condensation theory has been, more recently, developed by Netz [28] and Manning and Mohanty [29] who derived a more general condition, depending on the length of the polyion chain. However, in practice, in most cases, polyions are long enough to be in the regime described by Equation (1.4) and only short oligomers, exhibiting an incomplete condensation, deviate from this behavior.

From a physical point of view, counterion condensation is due to a balance between a favorable gain in electrostatic energy as a consequence of the ion collapse and an unfavorable loss of entropy when counterions bind to the polymer chain. This phenomenon plays an important role in biological polyelectrolyte solutions since the effective charge on the polyion backbone affects the morphology of the polyelectrolyte itself and, moreover, its response to external stimuli.

A typical example of counterion condensation occurs in DNA chains, where data obtained from optical tweezers experiments [30] indicate that the effective charge is −050 ± 0.05 per base pair, much less than the bare charge −2 per base pair (two phosphates per base pair), equivalent to a reduction of the bare charge by 75% ± 3%, in excellent agreement with the reduction predicted by the Manning counterion condensation theory of 76%.

During the last decades, a number of studies have focused on the phenomenon of counterion condensation, both experimental [31,32] and theoretical, and by simulations [33,34].

## 2. The Electrical Conductivity. Theoretical Background and Basic Equations

In order to put things into their proper perspective, we will start by describing the theory of the electrical conductivity of an aqueous solution.

From a phenomenological point of view, the electrical conductivity of an aqueous solution of polyelectrolytes originated by the movement of any charged entity in response to an external applied electric field, depends on three independent contributions, i.e., the numerical concentration n_{i} of the charge carriers of type i, their electrical charge (z_{i}e) and their mobility u_{i}, according to the relationship:

Here, the mobility u is defined as the ratio of the average velocity of the charged carrier to an applied electric field of unit strength. From an experimental point of view, the usual definition of the conductivity σ is given by the linear relationship:

Equation (2.1) can be written in a more usual way if we express the numeric concentration n_{i} through the molar concentration C_{i} (n_{i} = N_{A}C_{i}, where N_{A} is the Avogadro number) and the mobility u_{i} through the equivalent conductance λ_{i} (u_{i} = λ_{i} / F, where F = eN_{A} is the Faraday constant). We obtain:

In cgs units, the concentrations C_{i} are expressed in [mol/cm^{3}] and the equivalent conductances in [statohm^{−1}·cm^{2}·mol^{−1}] (for the conversion to SI units, 1 statohm ≈ 9 × 10^{11} ohm). Equation (2.5) is the basic equation that governs the whole transport process, depending on the concentration C_{i} and the equivalent conductance λ_{i} of each charge carrier.

In the case of a polyelectrolyte solution, charge carriers derive from the partial dissociation of the polyion chain and Equation (2.5) can be rewritten as:

_{1}|C

_{1}λ

_{1}+ |Z

_{p}|C

_{p}λ

_{p}

Because of the counterion condensation effect, the following relationships hold, i.e., C_{1} = v_{1}N f C_{p}, Z_{1} = z_{1}, Z_{p} = N f z_{p}, and Equation (2.5) reduces to:

_{p}(v

_{1}|z

_{1}|λ

_{1}+ |z

_{p}|λ

_{p})

The equivalent conductance λ_{1} differs from the value of the counterion in the absence of the polyelectrolyte, according to:

With this substitution, Equation (2.7) becomes:

_{p}| − v

_{1}|z

_{1}| = 0. In the light of this framework, the parameters which define the electrical conductivity of the polyelectrolyte solution are the equivalent conductance λ

_{p}of the polyion chain, the fraction f of free (un-condensed) counterions, besides the degree of polymerization N and the polyion concentration C

_{p}.

#### The Equivalent Conductance in the Manning Model

Before going on, we summarize the main results of the Manning model [24,25,26] as far as the equivalent conductance λ_{p} is concerned. In this context, the equivalent conductance λ_{p} can be written as the ratio of the polyion charge Q_{p} and the total electrophoretic coefficient f_{Etot} according to the expression:

If the electrophoretic coefficient f_{E} is calculated according to the general expression given by Kirkwood and Riseman [32], modeling the polyion as an ensemble of N_{b} simple spherical units of radius R_{b}, following the Manning derivation, we have:

_{b}= 6πηR

_{b}is the friction coefficient, with η the viscosity of the aqueous phase. The final expression for the equivalent conductance λ

_{p}of the polyion can be written as:

**Figure 1.**A sketch of a polyelectrolyte chain in good-solvent conditions, for different (salt free) concentration regimes. The chain is an extended rodlike configuration of electrostatic blobs and a random walk of correlation blobs for dilute (C < C*) and semidilute (C > C*) regimes, respectively.

The second example is taken from reference [12]. We have investigated the electrical behavior of poly(N-methyl-2-vinyl pyridinium chloride) [PMVP-Cl] at two different charge densities in two different solvents, i.e., pure water (poor-solvent condition) and ethylene glycol (good-solvent condition). These polymers possess a carbon-based backbone for which water is a poor solvent and ethylene glycol behaves as a good solvent.

## 3. Good Solvent Condition

#### 3.1. Dilute Solutions

In dilute solution, at very low concentrations, and consequently at a very low ionic strength, the Debye screening length is much larger than the average distance between chains and charges are obliged to interact by means of an unscreened Coulombic potential. In these conditions, the polymer chain is represented by an extended rod-like configuration of N_{D} electrostatic blobs of size D to form a fully extended chain of length L = N_{D}D. Each electrostatic blob contains g_{e} monomers and bears a charge q_{D} = z_{p}e f g_{e}. As usual, f is the fraction of ionized charged groups on the polymer chain and consequently the fraction of free counterions. The total charge of each polyion chain is Q_{p} = q_{D}N_{D} ≡ z_{p}e f g_{e}N_{D}.

A sketch of a polyelectrolyte chain in good-solvent conditions is shown in Figure 1.

In this case, the derivation of the expression for the equivalent conductance λ_{p} of the polyion proceeds analogously to what previously done, with the substitution of the elementary unit of length R_{b} of the Manning model by the electrostatic blob of size D. This means that the following substitutions hold:

_{b}→ N

_{D}

R

_{b}→ D

ζ

_{b}→ ζ

_{D}

Consequently, the electrophoretic coefficient f_{E} becomes:

_{p}of the polyion results:

In this way, the relevant parameters of the model reduce to the number of electrostatic blobs N_{D} and their size D. In the light of the scaling approach, these parameters scale as:

_{D}D ~ Nb(l

_{B}/ b)

^{2/7}f

^{4/7}

N

_{D}~ N(l

_{B}/ b)

^{5/7}f

^{10/7}

Equation (2.9), together with Equations (3.1.3) and (3.1.4) furnishes the final expression of the electrical conductivity of the polyelectrolyte solution in dilute condition. Note that here and throughout the paper, we drop numerical coefficients and keep our discussion at the scaling level.

#### 3.2. Semidilute Solutions

In the semidilute solutions, the polyion chain is modeled as random walk of N_{ξ0} correlation blobs of size ξ_{0}, each of them containing monomers. The number of correlation blobs is N_{ξ0} = N / g. Consequently, each correlation blob bears an electric charge = z_{p}efg and the charge of the full chain is Q_{p} = N_{ξ0} = z_{p}efgN_{ξ0}. In this case, the following substitutions hold:

_{b}→ N

_{ξ0}

R

_{b}→ ξ

_{0}

ζ

_{b}→ ζ

_{ξ}

_{E}becomes:

The friction coefficient ζ_{ξ} can be easily derived taking into account that now we are dealing with a rodlike unit of size ξ_{0} containing N_{ξ0} = N_{D} / ξ_{0} correlation blobs:

In this concentration regime, the characteristic parameters are the contour length N_{ξ0}ξ_{0} of the random walk chain of correlation blobs, the number N_{ξ0} of correlation blobs within each polymer chain and the ratio g/g_{e} of monomer inside a correlation blob to the ones inside an electrostatic blob. According to the scaling theory, these quantities scale as:

_{ξ0}ξ

_{0}− Nb(l

_{b}/ b)

^{2/7}f

^{4/7}

N

_{ξ0}− Nb

^{3/2}c

^{1/2}(l

_{b}/ b)

^{3/7}f

^{6/7}

g / g

_{e}− b

^{−3/2}c

^{−1/2}(l

_{b}/ b)

^{2/7}f

^{4/7}

Here, c is the polymer concentration expressed as monomers per unit volume (c = CNN_{A}, with N_{A} the Avogadro number). Analogously to the previous case, Equation (2.9) together with Equations (3.2.3) and (3.2.4) allows the electrical conductivity of the polyelectrolyte solution to be calculated.

## 4. Poor Solvent Condition

Polymer-solvent interactions are of primary importance in determining the spatial configuration of the polymer chain in solution. In the light of the scaling approach, the configuration of a hydrophobic chain in a poor solvent condition has been discussed extensively by Dobrynin and Rubinstein [36], who developed a scaling theory of hydrophobic polyelectrolytes over the entire range of polyelectrolyte concentrations and postulated the so-called necklace globule model.

Due to the strong hydrophobic interactions between the polymer backbone and the water molecules, in poor solvent conditions, the electrostatic blobs or the correlation blobs, present when good solvent condition applies, will split into a set of smaller charged globules (beads) connected by long and narrow tubules (strings). As pointed out by Dobrynin [36], this structure optimizes the correlation-induced attraction of condensed counterions to charged monomers and electrostatic repulsion between ionized charges.

The situation is even more interesting in the case of semidilute regime (C > C*), where two new different concentration regimes appear, i.e., string controlled regime (C* < C < C_{b}) and bead controlled regime (C_{b} < C < C_{D}), where a different concentration dependence of the chain size occurs.

In string-controlled regime, the correlation length is much larger than the size of the beads and the chains assume a bead-necklace structure on length scales smaller than the correlation length. Conversely, in bead-controlled regime, the correlation length is of the order of the size of the beads and the chains assume a bead structure on length scales smaller than the correlation length [37]. This effect is analogous to the splitting of a charged liquid droplet into an array of smaller ones, as predicted by Rayleigh long ago [38]. These different regimes imply a different picture of counterion condensation, which will condense on the necklace globule in an avalanche-like fashion. As pointed out by Jeon and Dobrynin [39], with the increase of the polyion concentration, counterions condense inside beads of the necklace globule, favoring the reduction of its charge and the increase of its mass which further promote the counterion condensation giving rise to the avalanche-like process. The necklace conformation is supported by experiments [40] and computer simulations [41,42].

A sketch of the necklace globule model is shown in Figure 2.

**Figure 2.**A sketch of the necklace globule model for a polyion in poor solvent condition, in dilute (C < C*) and semidilute (C > C*) concentrations. The semidilute concentration splits into string controlled regime (C* < C < C

_{b}) and bead controlled regime (C

_{b}< C < C

_{D}).

#### 4.1. Dilute Solutions

When the total effective charge of a polyion Q_{p} = zefN becomes larger than Q'= ze(Nτb / l_{b})^{1/2} and the Coulomb repulsion becomes comparable to the surface energy, the system tends to reduce its total free energy giving rise to N_{b} beads of size D_{b} containing monomers each and joined (N_{b} − 1) strings of length l_{s}. The length of the necklace is given by L_{nec} = N_{b}l_{s}, since the most of the length is stored in the string (l_{s} >> D_{b}).

The quality of the solvent is taken into account by the solvent quality parameter τ defined as τ = , where θ is the temperature at which the net excluded volume for uncharged monomers is zero.

In this case, the friction coefficient f_{E} can be written as:

The characteristic quantities scale as:

D

_{b}~ b(l

_{b}/ b)

^{−1/3}f

^{−2/3}

l

_{s}~ b(l

_{b}/ b)

^{−1/2}f

^{−1}τ

^{1/2}

#### 4.2. Semidilute Solutions

The overlapping concentration C_{b} between the string controlled regime (C* < C < C_{b}) and the bead-controlled regime (C_{b} < C < C_{D}) depends, in addition to the monomer size b and the fraction f, on the solvent quality parameter τ and scales according to the relationship:

_{b}− b

^{−3}τ

^{−1/2}(l

_{b}/ b)

^{1/2}f

In the string-controlled regime C* < C < C_{b}, the chain is assumed to be a random walk of N_{ξ0} = N / g_{ξ} correlation segments of size ξ_{0}, each of them containing g_{ξ} monomers.

The electrophoretic friction coefficient is given by:

_{ξ}is given by:

The characteristic quantities scale as:

_{0}− b

^{−1/2}C

^{−1/2}τ

^{1/4}(l

_{b}/ b)

^{−1/4}f

^{−1/2}

g

_{ξ}− b

^{−3/2}C

^{−1/2}τ

^{3/4}(l

_{b}/ b)

^{−3/4}f

^{−3/2}

In the bead-controlled regime C_{b}* < C < C_{D}, owing to the screening of the electrostatic interactions between beads, the model predicts only one bead per correlation globule of size ξ_{0}, containing g_{ξ} monomers.

The electrophoretic friction coefficient is given by:

_{ξ}is given by:

The characteristic quantities scale as:

_{0}− c

^{1/3}τ

^{1/3}(l

_{b}/ b)

^{−1/3}f

^{−2/3}

g

_{ξ}− τ(l

_{b}/ b)

^{−1}f

^{−2}

#### 4.3. The Diffusion Coefficients and in the Light of the Scaling Approach

To proceed further to the calculation of the polyion equivalent conductance λ_{p} and, finally, to the electrical conductivity σ of the polyelectrolyte solution, the ratio / must be appropriately evaluated in the light of the scaling laws. In the presence of counterion condensation (but in the absence of added salt), Manning [25] derived the following expression:

_{1},m

_{2}) ≠ (0,0) and ξ = 1/|z

_{1}z

_{p}|. In the case of uni-univalent polyion (z

_{1}= z

_{p}= 1), for ξ = 1, numerical evaluation of Equation (4.3.1) yields a constant value / ≃ 0.866.

Within the scaling picture, the charge density parameter ξ can be written as:

Consequently, the ratio / assumes the expression:

In the light of the scaling laws, the two relevant quantities D / g_{e} and ξ_{0} / g scale, in good solvent condition, as:

In poor solvent condition, in dilute regime the following substitution hold:

Typical behavior of the ratio / as a function f of the fraction of the free counterions, in dilute and semidilute regimes, is shown in Figure 3.

As can be seen in Equation (4.3.9), in bead controlled regime, there is, contrarily to the other regimes, a dependence on the polyelectrolyte concentration c (expressed as monomers per unit volume). In Figure 4, the typical dependence of / on the concentration c, for different values of the fraction f is shown in Figure 4. In this case, the value of the parameter τ is assumed fixed to τ = 0.4.

**Figure 3.**(Upper panel): the ratio / for polyelectrolytes solution in dilute regime; full line: good solvent condition; dotted lines: poor solvent condition, with four different values of the parameter τ (τ = 0.2, 0.4, 0.6, 0.8). (Bottom panel): the ratio / for polyelectrolytes solution in semidilute regime. Full line: good solvent condition. Dotted lines: poor solvent condition, in string-controlled regime. Dashed lines: poor solvent condition, in bead-controlled regime with different values of the parameter τ (τ = 0.4, 0.6, 0.8, in the order marked by the arrow).

**Figure 4.**Bead-controlled regime. Dependence of the ratio / on the polyelectrolyte concentration C and on the fraction f for a fixed value of the solvent quality parameter (τ = 0.4).

From the above analysis, it turns out that the electrical conductivity of a polyelectrolyte solution in the absence of added salt depends essentially on two parameters, the fraction f of free counterions and the solvent quality parameter τ. These parameters control the polyion equivalent conductance λ_{p} in the different concentration regimes (dilute and semidilute concentrations), according to the above stated scaling relationships.

A typical dependence of the equivalent conductance λ_{p} of the polyion in poor-solvent condition as a function of the polymer concentration, covering both the dilute and semidilute regime, is shown in Figure 5. As can be seen, the dependence is rather complex, reflecting the different conformations assumed by the polyion chain in the different concentration regimes.

**Figure 5.**Behavior of the equivalent conductance λ

_{p}of polyions in poor-solvent condition, as a function of the polyion concentration. According to the scaling picture, three different concentration regimes are clearly shown. In the dilute regime, the conductance is independent of the concentration. In the semidilute regime, a string-controlled regime and a beads-controlled regime are dependent on the concentration.

## 5. Polyelectrolyte Solutions in the Presence of Added Salt

Following an additive rule, in the presence of added salt, Equation (2.7) must be replaced by:

In this case too, the equivalent conductances λ can be writes as:

Substitution of Equation (5.2) into Equation (5.1) yields:

The general expression for the ratio (D_{i} / ) (i = 1,2), according to the derivation proposed by Manning [24,25], can be written as:

Here, ξ is, as usual, the charge density parameter and X, that takes into account the ratio of salt and polyion concentration, is defined as X = NC_{p} / C_{s}.

To a first approximation, Equations (5.4) and (5.5) can be simplified according to the following expression:

_{p}z

_{1}|, Equation (5.3) becomes:

Equation (5.7) reduces to the usual expression in the case of uni-univalent salt and for univalent charges on the polyion chain. In this case, z_{p} = 1; z_{1} = 1; v_{1} =1; =1; = 1; = 1; = 1 and the expression for the conducibility becomes:

In the presence of counterion condensation, i.e., ξ > 1/|z_{p}z_{1}|, Equation (5.3) can be written as:

As can be seen, in Equations (5.5) and (5.7), or equivalently, in the Equations (5.6) and (5.8), the key parameter that governs the conductometric behavior of the polyion solution is represented by the polyion equivalent conductance λ_{p} which contains all the relevant information concerning the concentration regimes and the polyion conformation.

As previously done, we will start considering the equivalent conductance λ_{p} within the Manning model and how, in the framework of the scaling relationships, this parameter has to be modified as a function of the polyion concentration, the quality of the solvent.

Taking into account the “asymmetry field” correction, in the presence of added salt, the general expression for the polyion equivalent conductance λ_{p} given by Manning, reads:

_{E}is the electrophoretic coefficient (without the asymmetry field correction), X = Nn

_{p}/ n

_{s}≡ c / n

_{s}takes into account the ratio of the salt and polyion concentration and and are the cation and anion mobilities in the aqueous phase (in the absence of the polyion). Here, the polyion charge Q

_{p}depends on the charge density parameter and stands for Q

_{p}= z

_{p}eNf in the presence of counterion condensation and for Q

_{p}= z

_{p}eN (the structural value) in the absence of counterion condensation.

The electrophoretic coefficient f_{E} in the light of the Manning model is approximated by:

#### 5.1. The Scaling Approach

In the presence of added salt, the polyion conformation is characterized by three different concentrations that define different concentration regimes. These concentrations are the concentration C* at which the distance between chains equals their extended length, the concentration C_{D} where the electrostatic blobs begins to overlap, and the concentration C_{e} (in between C* and C_{D}) at which polymer chains begin to entangle. Consequently, the polymer solution behaves as dilute solution for C < C*, as un-entangled semidilute solution for C* < C < C_{e} and as entangled semidilute solution for C_{e} < C < C_{D}. Finally, polymer solution behaves as concentrated solution for C > C_{D}.

In analogy with what we have done in the previous section, we will discuss good-solvent and poor-solvent conditions, separately.

#### 5.1.1. Good-Solvent Condition

In the dilute concentration regime, the polyion chain is represented by a self-avoiding walk of N_{rB} electrostatic blobs of size r_{B} inside which the polyion conformation is extended. Each electrostatic blob contains g_{B} monomers and bears an electric charge q_{rB} = z_{p}efg_{B}. The polyion bears a charge Q_{p} = N_{rB}q_{rB}, assuming a flexible conformation with an end-to-end distance given by R = r_{B}(N / g_{B})^{3/5}.

In the semidilute concentration regime, the polyion chain is modeled as a random walk of N_{ξ0} = N / g correlation blobs of size ξ_{0}. Each correlation blob bears an electric charge = z_{p}efg while the polyion charge is Q_{p} = N_{ξ0}. In this case, the polyion end-to-end length is given by R = ξ_{0}(N / g)^{1/2}.

Contrarily to what happens in the absence of added salt, in this case, electrostatic interactions are reduced by the presence of the added salt and in both the two regimes a random-walk structure dominates.

#### 5.1.2. Poor-Solvent Condition

In dilute concentration regime, when the effective polyion charge becomes larger than a critical value and the Coulombic repulsion becomes comparably with the surface energy, the polyion splits into N_{b} beads of size D_{b} and joined by (N_{b} − 1) strings of length l_{s}. In the semidilute concentration regime, the concentration C_{b} introduces, in analogy with the case in absence of added salt, two different regimes. In string-controlled regime (C* < C < C_{b}), the chain is composed of N_{ξ0} = N / correlation segment of size ξ_{0} each of them containing monomers. The chain is assumed to be a random walk of size R = ξ_{0}(N / )^{1/2}. In the bead-controlled regime (C_{b} < C < C_{D}), the screening of the electrostatic interactions produces one bead per correlation globule with a random walk chain conformation of size R = ξ_{0}(N / )^{1/2}, analogous to the size of the chain in string-controlled regime.

#### 5.2. The Electrophoretic Coefficient f_{E}

As in the previous cases, in the presence of added salt too, the electrophoretic coefficient f_{E} depends on the different concentration regimes, since the elementary unit that contributes to the conductivity, in the light of the Manning theory, differs from a regime to the other.

In good solvent condition and in dilute regime, the elementary unit is the electrostatic blob of size D_{b} and the electrophoretic coefficient f_{E} is given by:

In good-solvent condition, but in semidilute regime, the elementary unit is the correlation blob of size ξ_{0} and the electrophoretic coefficient f_{E} is given by:

_{ξ0}given by:

In the poor solvent condition, when the necklace model applies, the electrophoretic coefficient f_{E} in the dilute regime (the elementary unit is the bead of size D_{b}) is given by:

_{0}) is given by:

In this latter case, the friction coefficient ζ_{ξ0}, depending on the basic unit of the chain, can be written as:

_{b}) and as:

_{b}< C < C

_{D}).

In good solvent condition, according to the scaling theory, the characteristic quantities are D_{b} and N_{b} in dilute regime and ξ_{0}, N_{ξ0} and g / g_{e} in semidilute regime. These quantities scale as:

_{b}~ N(l

_{B}/ b)

^{−1/3}f

^{−2/3}

N

_{b}~ N(l

_{B}/ b) f

^{−2}

_{b}~ N(l

_{B}/ b)

^{−1/3}f

^{−2/3}

N

_{b}~ N(l

_{B}/ b) f

^{−2}

In poor solvent condition, according to the scaling relationships, the characteristic quantities entering Equations (5.2.4) and (5.2.5) are N_{b}, D_{b} and l_{s} in the dilute regime and ξ_{0}, N_{ξ0} in the semidilute regime. These quantities scale as:

D

_{b}~ b(l

_{B}/ b)

^{−1/3}f

^{−2/3}

Here, the quantity X_{s}, that takes into account the concentration of free ions present in the solution, is defined as:

For uni-univalent salt and for univalent counterions, the equation reduces to:

On the basis of these scaling relationships, the equivalent conductance λ_{p} can be conveniently evaluated in each concentration regime we are dealing with, taking into account the appropriate quality of the solvent. Once the equivalent conductance λ_{p} is known, the electrical conductivity σ of the whole polyelectrolyte solution derives directly from the Manning expression. As an example, in Figure 6 we report the equivalent conductance λ_{p} for polyions in good-solvent condition, in dilute and semidilute regime and in the presence of added salt.

**Figure 6.**The equivalent conductance λ

_{p}of polyions in good solvent regime, for dilute and semidilute conditions, calculated according to Equations (5.2.1) and (5.2.2) in the presence of added salt, for three different values of the parameter X. Dotted lines show the calculated values in the dilute region extrapolated to semidilute region. The parameters are: N = 2250; l

_{B}= 7 × 10

^{−8}cm; b = 2.52 × 10

^{−8}cm; η = 1 cP; = 0.137 cgs units; = 0.235 cgs units. Here, X is defined as X = c/n

_{s}.

## 6. Comparison with Experiments

In what follows, we will compare some representative results from the recent literature with the ones predicted by the scaling theory. We confine ourselves to one’s own measurements [4,5,8,12], but in the recent literature many other appropriate examples can be easily found.

Electrical conductivity measurements of Sodium polyacrylate salts [−CH_{2}CH(CO_{2}Na)−]_{n}, [NaPAA] as a function of polymer concentration to cover the dilute and semidilute regime have been extensively reported in Reference [5]. Measurements have been carried out at three different values of the ratio X = c / n_{s} (X = 0.1, 1, 10), by adding appropriate amount of NaCl electrolyte solution, maintaining constant the ratio between the number of monomers and the number of ions derived from the added salt. In these experiments, good-solvent condition applies. In Figure 7, we show a comparison between the polyion equivalent conductance λ_{p} directly derived from the experimental values of the electrical conductivity σ and the values calculated on the basis of the scaling approach we have above discussed. As can be seen, both in the dilute regime and in the semidulute regime, the agreement is quite good. In particular, we observe that transition from dilute and semidilute regime occurs exactly at the polyion concentrations predicted by the theory.

**Figure 7.**The equivalent conductance of NaPAA polyions in aqueous solutions in the presence of added salt (X = 0.1, = 1, X = 10) as a function of the polyion concentration. Polymer in good solvent condition. Panel (

**A**) Dilute solution, X = 0.1; (■) experimental values derived from the measured electrical conductivity. Full curve is calculated on the basis of Equation (5.2.1). Panel (

**B**) Dilute and semidilute solution, the transition region being marked by the arrow, X = 1; (●) experimental values derived from the measured electrical conductivity. Upper full curve is calculated on the basis of Equation (5.2.1) in the dilute regime and lower full curve calculated on the basis of Equation (5.2.2) in the semidilute regime. Panel (

**C**) Dilute and semidilute solution, the transition region being marked by the arrow. X = 10; (●) experimental values derived from the measured electrical conductivity. Upper full curve is calculated on the basis of Equation (5.2.1) in the dilute regime and lower full curve calculated on the basis of Equation (5.2.2) in the semidilute regime. Data redrawn from Reference [5].

The second example is taken from reference [12]. We have investigated the electrical behavior of poly(N-methyl-2-vinyl pyridinium chloride) [PMVP-Cl] at two different charge densities in two different solvents, i.e., pure water (poor-solvent condition) and ethylene glycol (good-solvent condition). These polymers possess a carbon-based backbone for which water is a poor solvent and ethylene glycol behaves as a good solvent.

We report here some typical results showing the behavior of the equivalent conductance λ_{p} of the polyion as a function of the polyion concentration, derived from the measured electrical conductivity and compared with the values calculated, on the basis of the scaling approach, for semidilute regime in string-controlled conditions. We present two limiting cases, i.e., polyions in water (poor-solvent condition) and in ethylene glycol (good-solvent condition) in cases of differently charged poyions (Figure 8, degree of quaternization Q = 55% and Figure 9, degree of quaternization Q = 17%). As can be seen, the agreement with the expected behavior is quite good over the whole concentration range, where the semidilute regime holds. This agreement is further enforced if we compare the values of the equivalent conductance for water solution with the ones calculated for good solvent condition (dotted line in Figure 8 Panel A) or for ethylene glycol with the ones for poor-solvent conditions (dotted line in Figure 8. Panel B).

These results are a strong support for the necklace model for hydrophobic polyions in the light of the dynamic scaling models.

**Figure 8.**The equivalent conductance of 55% PMVP-Cl (Q = 55%) polyion as a function of concentration C. Panel (

**A**) polyion in water solution (poor-solvent condition). (●): values derived from the measured electrical conductivity. Full line represents the corresponding values calculated according to the necklace model in the semidilute string-controlled condition, assuming = 0.6. The dotted line represents the calculated values in the semidilute good-solvent condition. Panel (

**B**) polyion in ethylene glycol solvent (good-solvent condition). (●): values derived from the measured electrical conductivity. Full line represents the corresponding values calculated according to the semidilute good-solvent condition. The dotted line represents the calculated values in the necklace model in semidilute-string-controlled condition. The arrow marks the concentration c *, indicating the transition between the dilute and the semidilute regime. Data from Reference [12].

**Figure 9.**The equivalent conductance of 17% PMVP-Cl (Q = 17%) polyion as a function of concentration C. Panel (

**A**) polyion in water solution (poor-solvent condition). (●): values derived from the measured electrical conductivity. Full line represents the corresponding values calculated according to the necklace model in the semidilute string-controlled condition, assuming τ = 0.6. The dotted line represents the calculated values in the semidilute good-solvent condition. Panel (

**B**) polyion in ethylene glycol solvent (good-solvent condition). (●): values derived from the measured electrical conductivity. Full line represents the corresponding values calculated according to the semidilute good-solvent condition. The dotted line represents the calculated values in the necklace model in semidilute-string-controlled condition. The arrow marks the concentration c *, indicating the transition between the dilute and the semidilute regime. Data from Reference [12].

## 7. Conclusions

The conductometric properties of aqueous polyelectrolyte solutions in the absence and in the presence of added salt have been reviewed in the light of the dynamic scaling models for polyion conformation in different concentration regimes, proposed some years ago by Dobrynin and Rubinstein. Starting from the basic relationship derived by Manning for the equivalent conductance of a polyelectrolyte in high dilution limit, we have extended this approach on the basis of the scaling picture, to more concentrated systems. In the dilute regime, where stretched rod-like polymer conformation prevails, the basic entity that contributes to the electrical conductivity is the electrostatic blob and the polymer chain is represented by a rod-like configuration of electrostatic blobs. In the semidilute regime, where a random walk statistics applies, the polymer chain is modeled as a random walk of correlation blobs. For each of these regimes, it is possible to identify the elementary unit that contributes to the conductive process, together with the characteristic parameters, which model these units. The further step is the introduction of the scaling relationships, which allow the knowledge of the conformal evolution of the polymer chain in the different concentration regimes and in consequence of the solvent quality. This approach furnishes a comprehensive picture of the conductometric behavior of polyelectrolyte solutions in different experimental conditions in good agreement with experimental results.

## Acknowledgments

I acknowledge support from the Department of Physics at the University of Rome “La Sapienza”.

## Conflicts of Interest

The author declares no conflict of interest.

## References

- Morawetz, H. Polyelectrolytes; Marcel Dekker: New York, NY, USA, 1993.
- Russel, W.B.; Saville, D.A.; Schowalter, W.R. Colloidal Dispersions; Cambridge University Press: Cambridge, UK, 1983.
- Mandel, M. Physical Properties of Polyelectrolyte Solutions; Pacini: Florence, Italy, 1999.
- Bordi, F.; Cametti, C.; Gili, T. Electrical conductivity of aqueous polyelectrolyte solutions in the presence of counterion condensation: The scaling approach revisited. Phys. Rev. E
**2002**, 66, doi:10.1103/PhysRevE.66.021803. - Bordi, F.; Cametti, C.; Gili, T. Electrical conductivity of polyelectrolyte solutions in the presence of added salt: The role of the solvent quality factor in the light of the scaling approach. Phys. Rev. E
**2003**, 68, doi:10.1103/PhysRevE.68.011805. - Truzzolillo, D.; Bordi, F.; Cametti, C.; Sennato, S. Counterion condensation of differently flexible polyelectrolytes in aqueous solution in the dilute and semidilute regime. Phys. Rev. E
**2009**, 79, doi:10.1103/PhysRevE.79.011804. - Bordi, F.; Cametti, C.; Gili, T.; Colby, R.H. Dielectric relaxations in aqueous polyelectrolyte solutions: A scaling approach and the role of their solvent quality parameter. Langmuir
**2002**, 18, 6404–6409, doi:10.1021/la020175h. - Bordi, F.; Colby, R.H.; Cametti, C.; de Lorenzo, L.; Gili, T. Electrical conductivity of polyelectrolyte solutions in the semidilute and concentrated regime: The role of counterion condensation. J. Phys. Chem. B
**2002**, 106, 6887–6893, doi:10.1021/jp020262i. - Bordi, F.; Cametti, C.; Motta, A. Scaling behavior of the high-frequency dielectric properties of Poly-l-lysine aqueous solutions. Macromolecules
**2000**, 33, 1910–1916, doi:10.1021/ma991383s. - Bordi, F.; Cametti, C.; Colby, R.H. Dielectric spectroscopy and conductivity of polyelectrolyte solutions. J. Phys. Cond. Matter
**2004**, 16, R1423–R1463, doi:10.1088/0953-8984/16/49/R01. - Bordi, F.; Cametti, C.; Gili, T.; Sennato, S.; Zuzzi, S.; Dou, S.; Colby, R.H. Solvent quality influence on the dielectric properties of polyelectrolyte solutions: A scaling approach. Phys. Rev. E
**2005**, 72, doi:10.1103/PhysRevE.72.031806. - Bordi, F.; Cametti, C.; Gili, T.; Sennato, S.; Zuzzi, S.; Dou, S.; Colby, R.H. Conductometric properties of linear polyelectrolytes in poor-solvent condition: the necklace model. J. Chem. Phys.
**2005**, 122, doi:10.1063/1.1931607. - Bordi, F.; Cametti, C.; Sennato, S.; Zuzzi, S.; Dou, S.; Colby, R.H. Dielectric scaling in polyelectrolyte solutions with different solvent quality in the dilute concentration regime. Phys. Chem. Chem. Phys.
**2006**, 8, 3653–3658, doi:10.1039/b605624e. - Cametti, C. Dielectric and conductometric properties of highly heterogeneous systems. Riv. Nuovo Cimento
**2009**, 32, 185–260. - Truzzolillo, D.; Cametti, C.; Sennato, S. Dielectric properties of differently flexible polyions: A scaling approach. Phys. Chem. Chem. Phys.
**2009**, 11, 1780–1786. - Cametti, C.; Zuzzi, S. Radiowave dielectric properties of sodium maleate copolymers in aqueous solutions in light of a scaling approach. J. Phys. Chem. B
**2010**, 114, 7140–7147, doi:10.1021/jp100593z. - Dobrynin, A.V. Effect of counterion condensation on rigidity of semiflexible polyelectrolytes. Macromolecules
**2006**, 39, 9519–9527, doi:10.1021/ma061030a. - Dobrynin, A.V.; Rubinstein, M. Theory of polyelectrolyte in solutions and at surfaces. Prog. Polym. Sci.
**2005**, 30, 1049–1118, doi:10.1016/j.progpolymsci.2005.07.006. - Dobrynin, A.V.; Rubinstein, M.; Obukhov, S.P. Cascade of transitions of polyelectrolytes in poor solvent. Macromolecules
**1996**, 29, 2974–2979, doi:10.1021/ma9507958. - Dobrynin, A.V.; Rubinstein, M. Hydrophobic polyelectrolytes. Macromolecules
**1999**, 32, 915–922, doi:10.1021/ma981412j. - Manning, G.S. Counterion binding in polyelectrolyte theory. Acc. Chem. Res.
**1979**, 12, 443–449, doi:10.1021/ar50144a004. - Manning, G.S. The critical onset of counterion condensation. A survey of its experimental and theoretical basis. Ber. Bunsenges. Phys. Chem.
**1996**, 100, 909–922, doi:10.1002/bbpc.19961000637. - Manning, G.S. Counterion condensation on charged spheres, cylinders and planes. J. Phys. Chem.
**2007**, 111, 8554–8559, doi:10.1021/jp0670844. - Manning, G.S. Limiting laws and counterion condensation in polyelectrolyte solutions. I. Colligative properties. J. Chem. Phys.
**1969**, 51, 924–933, doi:10.1063/1.1672157. - Manning, G.S. Limiting laws and counterion condensation in polyelectrolyte solutions. II. Self diffusion of the small ions. J. Chem. Phys.
**1969**, 51, 934–947, doi:10.1063/1.1672158. - Manning, G.S. The molecular theory of polyelectrolyte solutions with applications to the electrostatic properties of polynucleotides. Q. Rev. Biophys.
**1978**, 11, 179–246, doi:10.1017/S0033583500002031. - Fischer, S.; Naji, A.; Netz, R.R. Salt-induced counterion-mobility anomaly in polyelectriolyte electrophoresis. Phys. Rev. Lett.
**2008**, 101, doi:10.1103/PhysRevLett.101.176103. - Netz, R.R. Polyelectrolytes in electric fields. J. Phys. Chem. B
**2003**, 107, 8208–8217, doi:10.1021/jp022618w. - Manning, G.S.; Mohanty, U. Counterion condensation on ionic oligomers. Phys. A
**1997**, 247, 196–204, doi:10.1016/S0378-4371(97)00413-5. - Keyser, U.F.; Koeleman, B.N.; van Dorp, S.; Krapf, D.; Smeets, R.M.M.; Lemay, S.G.; Dekker, N.H.; Dekker, C. Direct force measurements on DNA in a solid state nanopore. Nat. Phys.
**2006**, 2, 473–477, doi:10.1038/nphys344. - Wette, P.; Schope, H.J.; Palberg, T. Comparison of colloidal effective charges from different experiments. J. Chem. Phys.
**2002**, 116, 10981–10988, doi:10.1063/1.1480010. - Essafi, W.; Lafuma, F.; Williams, C.E. Structural evidence of charge renormalization in semi-dilute solutions of highly charged polyelectrolytes. Eur. Phys. J. B
**1999**, 9, 261–266, doi:10.1007/s100510050765. - Aubouy, M.; Trizc, E.; Bocquet, L. Effective charge versus bare charge: An analytical estimate for colloids in the infinite dilution limit. J. Phys. A Math. Gen.
**2003**, 36, 5835–5840, doi:10.1088/0305-4470/36/22/302. - Naji, A.; Netz, R.R. Scaling and universality in the counterion condensation transition at charged cylinders. Phys. Rev. E
**2006**, 96, doi:10.1103/PhysRevE.73.056105. - Kirkwood, J.K.; Riseman, J. The intrinsic viscosities and diffusion constants of flexible macromolecules in solution. J. Chem. Phys.
**1948**, 16, 565–572, doi:10.1063/1.1746947. - Dobrynin, A.V.; Rubinstein, M. Counterion condensation and phase separation in solutions of hydrophobic polyelectrolytes. Macromolecules
**2001**, 34, 1964–1972, doi:10.1021/ma001619o. - Chang, R.; Yethiraj, A. Strongly charged flexible polyelectrolytes in poor solvents: Molecular dynamics simulations with explicit solvent. J. Chem. Phys.
**2003**, 118, 6634–6647, doi:10.1063/1.1558312. - Rayleight, L. On the equilibrium of liquid conducting masses charged with electricity. Philos. Mag.
**1882**, 14, 184–186, doi:10.1080/14786448208628425. - Jeon, J.; Dobrynin, A.V. Necklace globule and counterion condensation. Macromolecules
**2007**, 40, 7695–7706, doi:10.1021/ma071005k. - Aseyev, V.O.; Klenin, S.I.; Tenhu, H.; Grillo, I.; Geissler, E. Neutron scattering studies of the structure of a polyelectrolyte globule in a water-acetone mixture. Macromolecules
**2001**, 34, 3706–3709, doi:10.1021/ma0016331. - Lyulin, A.V.; Dunveg, B.; Borisov, O.V.; Darinskii, A.A. Computer simulation studies of a single polyelectrolyte chain in poor solvent. Macromolecules
**1999**, 32, 3264–3278, doi:10.1021/ma981818w. - Micka, U.; Kremer, K. Strongly charged flexible polyelectrolytes in poor solvent. From stable spheres to necklace chain. Europhys. Lett.
**2000**, 49, 189–195, doi:10.1209/epl/i2000-00133-6.

© 2014 by the authors; licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution license (http://creativecommons.org/licenses/by/3.0/).