# Particle Size Variation and Prediction of Molecular Weight of Bi(III) Hydrolyzed Polymer Using Light Scattering Technique

Authors: N. Priyadarshini; M. Sampath; Shekhar Kumar; U. Kamachi Mudali
Journal: ISRN Inorganic Chemistry
 (2013)

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## Abstract

The present paper gives an overview of the hydrolysis reactions up to colloid formation of Bi(III) in aqueous nitric acid medium using light-scattering measurements. The hydrolysis products of Bi were polynuclear complexes such as dimers, pentamers, and the most important is the hexameric species. In the present investigation Bi3+ polymers were prepared by diluting different concentrations of Bi(NO3)3·5H2O solutions to pH 1 ± 0.1 by adding 0.1 M NaOH solution as it starts to precipitates at pH 1.4. The degree of polymerization was found to be 5-6 units. Particle size measurements were performed, and it has been found that particle size increases at high concentration of Bi due to aggregation. Refractive index measurements were also performed. The molecular weight of hydrolyzed polymeric species of Bi was determined by using Debye plot, and it was estimated as 1236 Da. The second virial coefficient was found to be 6.24 × 10−3 mLg−1 Da. The present investigation confirms that the predominant complex in the solution has 5-6 Bi atoms.


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## Body

## 1. Introduction

Among numerous reactions that govern the chemical behavior of metal ions in aqueous medium, the knowledge of hydrolysis, colloid formation, and precipitation is of highest priority. In general, metal ions in aqueous solutions form a variety of hydrolysis complexes, such as mono- and polynuclear hydroxospecies [1]. The polynuclear complexes are formed followed by hydrolysis, and in general it can be represented as
(1)xMn++yH2O⟺[Mx(OH)y](nx-y)+yH+
The pH is the most governing factor where soluble hydrolysis species are present. It is limited due to the formation of colloids or precipitation of hydroxides and oxides.Aqueous chemistry of Bi is primarily dominated by trivalent complexes(Bi3+) [2]. Bi(III) readily hydrolyzes in aqueous solutions (pKa=1.51) and has high affinity to oxygen. In addition to that Bismuth is a strong Lewis acid and begins to undergo hydrolysis at low pH values (pH~1) [3, 4]. The Bi3+ aqua ion [Bi(H2O)n]3+ has been characterized using many techniques which includes extended X-ray absorption fine structure (EXAFS) and low angle X-ray scattering (LAXS) spectroscopy and concluded that 8 water molecules are coordinated to Bi3+. But dynamic simulations show that the number of coordinated water molecules is 9 (i.e., [Bi(H2O)9]3+) and is found analogous to structures found among lanthanides [5]. Numerous studies on hydrolysis of Bi show that the predominant species at higher H+ concentration is Bi3+. It has been widely agreed that the hydrolyzed species of Bi are polymeric existing as dimers Bi2O22+, pentamers Bi5O55+, and the most important among them is the hexameric species Bi6O66+ at moderate Bi concentrations (≥10−2m) in acidic solutions with pH ~ 2–5. Further hydrolysis over pH range of 4–6 leads to the formation of Bi9 polynuclear complexes [6]. Sedimentation equilibrium measurements indicate that there were 5 or 6 bismuth atoms in the predominant complex present in solutions with approximately 2 hydroxide ions bound per bismuth atom [7]. Since Bi-Pb eutectic composition are heavy liquid coolant for nuclear reactors and several recent reactor prototypes use steam-generation modules in direct contact with liquid metal coolant, Bi speciation under hydrothermal conditions is very important to optimize the separation of Bi from concentrates such as Cu, Pb, and Mo [8, 9]. Hence an attempt has been made to study the hydrolysis and polymerization reactions of Bi using light-scattering technique. The use of light scattering to determine the molecular weight of polymers has increased interest because of the several advantages associated with this technique. It provides a nondestructive analytical technique for probing structure and dynamics of polymeric solution. The main aim of this study is to determine the particle size and its changes with change in concentration using dynamic light scattering and weight average molecular weight of Bi polynuclear complexes by static light scattering.


## 2. Theoretical

### 2.1. Dynamic Light Scattering

Dynamic light-scattering measurements measure the time dependence of scattered light fluctuations that can be related to the translational diffusion coefficient of the macromolecules. In order to quantify the time dependence, the autocorrelation functionG(τ) is calculated from the product of two photon counts at time t and t+τ such that G(τ)=〈I(t)I(T+τ)〉 [10]. The normalized intensity autocorrelation function g(τ) is given by
(2)gint(τ)=〈I(t)I(t+τ)〉〈I(t)I(t)〉.
The intensity autocorrelation function is related to the field autocorrelation function gfield(τ) by the Siegert relationship
(3)gfield=1+C|gint(τ)|2,
where τ is the delay time and C is the Siegert constant (experimental parameter of the measuring device). For dilute dispersion of macromolecules, gint(τ)  becomes
(4)gint(τ)=e-Γτ,
where Γ is the diffusion of particles under investigation. The relation between the diffusion coefficient (D) and the parameter Γ can be related by
(5)D=Γq2,
where q is the scattering vector.From the diffusion coefficient, the hydrodynamic particle radiusRh can be derived via the Stokes-Einstein relation
(6)Rh=KBT6πηD,
where KB is Boltzmann’s constant, T  is the temperature, and  η  is viscosity of the solvent.


### 2.2. Static Light Scattering

Static light scattering (SLS) has been widely used to determine the molecular weight of a polymer. SLS measures the time-averaged scattering intensity that can be related to the second virial coefficient and molecular weight by constructing the Debye plot according to the equation(7)KCRθ=(1Mw+2A2C),
where the optical constant K=[2πn(dn/dC)]2/NAλ°4, Rθ is the excess Rayleigh ratio, Mw is the weight average molecular weight of the solute, C is the concentration (in g/mL), A2 is the second virial coefficient, λo is the wavelength of light used, NA is Avogadro’s number, and dn/dC is the refractive index increment due to the solute under a given set of solution conditions. A positive value of A2 indicates repulsion between molecules, whereas a negative value indicates the presence of intermolecular interactions. The Debye plot is KC/Rθ versus concentration in g/mL. The intercept of the plot gives 1/Mw, and the slope is used to calculate the second virial coefficient [11, 12].


### 2.3. Materials and Methods

Bi(NO3)3·5H2O in crystalline form was obtained from Glaxo laboratories (minimum assay of 98.0%). Four different solutions of Bismuth were prepared by dissolving nitrate, Bi(NO3)3·5H2O in 1 M nitric acid (AR-Fisher, assay of 69–71%) to a concentration of 0.0064, 0.0121, 0.0246, and 0.0367 g mL−1. Bi(NO3)3·5H2O is of AR grade and used as such. The resulting solutions were diluted by gradually adding 0.1 M NaOH until slight turbidity occurs. The pH of the solution was maintained as 1±0.1. All the solutions were prepared at room temperature. Water used in the experiments was ASTM Grade-I water (from a Millipore Simplicity System with organic removal, 18.2 M.Ω.cm). Samples were weighed using Shimadzu (AUW220D) analytical balance with measurement uncertainty of        ±0.01 mg.


### 2.4. Measurement of pH and Refractive Index

The changes in the pH of the solutions were monitored using Thermo Scientific Orion Star pH meter. The glass electrode used for the measurement was calibrated with buffer solutions of pH 4.01 and 7.00. The accuracy of pH measurements was ±0.01 units. Refractive index(nD) of solutions of different concentration of Bi was measured on Anton Paar RXA 156 refractometer equipped with integrated Peltier thermostat with standard deviation of 2*10-5nD at 298 K.


### 2.5. Light-Scattering Measurements

Both SLS and DLS experiments were performed using Microtrac (Nanotrac ULTRA) particle size analyzer. Figures1(a) and 1(b) represent the experimental light-scattering system used for the present study. The light source was a 780 nm, 3 mW diode laser. An external fiber-optic probe measuring 1.5 m in length was dipped inside a beaker containing the sample solution. The interface between the sample and the probe is the sapphire window. Initially it reflects the original laser back through the beam splitter to a photodetector. This signal which has the same frequency as the original laser acts as a reference signal, offering heterodyne detection. And then, the laser passes through the sapphire window and is scattered by the particles under Brownian motion. According to the Doppler effect, the laser is frequency shifted relative to the velocity of the particle. Light is scattered in all directions including 180° backwards. This scattered, frequency shifted light is transmitted through the sapphire window to the optical splitter in the probe to the photodetector. These signals of various frequencies combine with the reflected signal of unshifted frequency (controlled reference) to generate a wide spectrum of heterodyne difference frequencies. The power spectrum of the interference signal is calculated with dedicated high speed FFT (Fast Fourier Transform) digital signal processor hardware. The power spectrum is then inverted to give the particle size distribution. The schematic of the instrument is shown in Figure 1. The scattered light was measured at an angle of 180°. Scattering experiments were performed at a temperature of 27±1°C. The performance of the instrument was checked with the reference material (100 nm polystyrene microsphere suspended in water) prior to particle size measurements. The uncertainty in the measurement was found to be ±1 nm.(a) Schematics of the light-scattering system showing the development of controlled reference at the probe tip and fluid interface. (b) Microtrac particle size analyzer with measurement range of 0.8 nm to 6.4μm used for the present study.
(a)
(b)


## 2.1. Dynamic Light Scattering

Dynamic light-scattering measurements measure the time dependence of scattered light fluctuations that can be related to the translational diffusion coefficient of the macromolecules. In order to quantify the time dependence, the autocorrelation functionG(τ) is calculated from the product of two photon counts at time t and t+τ such that G(τ)=〈I(t)I(T+τ)〉 [10]. The normalized intensity autocorrelation function g(τ) is given by
(2)gint(τ)=〈I(t)I(t+τ)〉〈I(t)I(t)〉.
The intensity autocorrelation function is related to the field autocorrelation function gfield(τ) by the Siegert relationship
(3)gfield=1+C|gint(τ)|2,
where τ is the delay time and C is the Siegert constant (experimental parameter of the measuring device). For dilute dispersion of macromolecules, gint(τ)  becomes
(4)gint(τ)=e-Γτ,
where Γ is the diffusion of particles under investigation. The relation between the diffusion coefficient (D) and the parameter Γ can be related by
(5)D=Γq2,
where q is the scattering vector.From the diffusion coefficient, the hydrodynamic particle radiusRh can be derived via the Stokes-Einstein relation
(6)Rh=KBT6πηD,
where KB is Boltzmann’s constant, T  is the temperature, and  η  is viscosity of the solvent.


## 2.2. Static Light Scattering

Static light scattering (SLS) has been widely used to determine the molecular weight of a polymer. SLS measures the time-averaged scattering intensity that can be related to the second virial coefficient and molecular weight by constructing the Debye plot according to the equation(7)KCRθ=(1Mw+2A2C),
where the optical constant K=[2πn(dn/dC)]2/NAλ°4, Rθ is the excess Rayleigh ratio, Mw is the weight average molecular weight of the solute, C is the concentration (in g/mL), A2 is the second virial coefficient, λo is the wavelength of light used, NA is Avogadro’s number, and dn/dC is the refractive index increment due to the solute under a given set of solution conditions. A positive value of A2 indicates repulsion between molecules, whereas a negative value indicates the presence of intermolecular interactions. The Debye plot is KC/Rθ versus concentration in g/mL. The intercept of the plot gives 1/Mw, and the slope is used to calculate the second virial coefficient [11, 12].


## 2.3. Materials and Methods

Bi(NO3)3·5H2O in crystalline form was obtained from Glaxo laboratories (minimum assay of 98.0%). Four different solutions of Bismuth were prepared by dissolving nitrate, Bi(NO3)3·5H2O in 1 M nitric acid (AR-Fisher, assay of 69–71%) to a concentration of 0.0064, 0.0121, 0.0246, and 0.0367 g mL−1. Bi(NO3)3·5H2O is of AR grade and used as such. The resulting solutions were diluted by gradually adding 0.1 M NaOH until slight turbidity occurs. The pH of the solution was maintained as 1±0.1. All the solutions were prepared at room temperature. Water used in the experiments was ASTM Grade-I water (from a Millipore Simplicity System with organic removal, 18.2 M.Ω.cm). Samples were weighed using Shimadzu (AUW220D) analytical balance with measurement uncertainty of        ±0.01 mg.


## 2.4. Measurement of pH and Refractive Index

The changes in the pH of the solutions were monitored using Thermo Scientific Orion Star pH meter. The glass electrode used for the measurement was calibrated with buffer solutions of pH 4.01 and 7.00. The accuracy of pH measurements was ±0.01 units. Refractive index(nD) of solutions of different concentration of Bi was measured on Anton Paar RXA 156 refractometer equipped with integrated Peltier thermostat with standard deviation of 2*10-5nD at 298 K.


## 2.5. Light-Scattering Measurements

Both SLS and DLS experiments were performed using Microtrac (Nanotrac ULTRA) particle size analyzer. Figures1(a) and 1(b) represent the experimental light-scattering system used for the present study. The light source was a 780 nm, 3 mW diode laser. An external fiber-optic probe measuring 1.5 m in length was dipped inside a beaker containing the sample solution. The interface between the sample and the probe is the sapphire window. Initially it reflects the original laser back through the beam splitter to a photodetector. This signal which has the same frequency as the original laser acts as a reference signal, offering heterodyne detection. And then, the laser passes through the sapphire window and is scattered by the particles under Brownian motion. According to the Doppler effect, the laser is frequency shifted relative to the velocity of the particle. Light is scattered in all directions including 180° backwards. This scattered, frequency shifted light is transmitted through the sapphire window to the optical splitter in the probe to the photodetector. These signals of various frequencies combine with the reflected signal of unshifted frequency (controlled reference) to generate a wide spectrum of heterodyne difference frequencies. The power spectrum of the interference signal is calculated with dedicated high speed FFT (Fast Fourier Transform) digital signal processor hardware. The power spectrum is then inverted to give the particle size distribution. The schematic of the instrument is shown in Figure 1. The scattered light was measured at an angle of 180°. Scattering experiments were performed at a temperature of 27±1°C. The performance of the instrument was checked with the reference material (100 nm polystyrene microsphere suspended in water) prior to particle size measurements. The uncertainty in the measurement was found to be ±1 nm.(a) Schematics of the light-scattering system showing the development of controlled reference at the probe tip and fluid interface. (b) Microtrac particle size analyzer with measurement range of 0.8 nm to 6.4μm used for the present study.
(a)
(b)


## 3. Results and Discussion

Figure2 shows the comparison plot for varying particle size as the concentration of the solution varies. The d50 values range from 121 to 190 nm. The details of each peak are given in Table 1.Table 1
Peak summary.
Concentration(g/mL)
Particle diameter(nm)
Volume %
Width
0.0064
121.3
97.7
54.7
0.0121
153.4
100.0
51.8
0.0246
160.4
100.0
81.8
0.0367
192.2
100.0
29.53Figure 2
A comparison plot for intensity-averaged particle diameter (d50) variation with different concentration of polymeric Bi solutions prepared in aqueous nitric acid medium.The increase in particle diameter is due to aggregation of smaller particles as the concentration increases. The polymer is formed as a result of the condensation reaction between the monomeric species. The general equilibrium reaction is given(8)nBi3++2nH2O⟺Bin(OH)2nn++2nH+Figure3 shows the refractive index increment for different concentrations of Bi, and the values are given in Table 2. As the concentration increases, the refractive index of the solution also increases giving a positive slope, dn/dC=0.1304 mL g−1. This value has been used as an input for generating the Debye plot. Values of 4.36 gcc−1 and 1.9 were assumed as particle density and particle refractive index. Figure 4 shows the Debye plot for different concentration of Bi. It is a straight line with a positive slope. The particles were assumed spherical and ensured that the prepared solution was free of impurities. The molecular weight of the polymer was determined as 1236 Da from the intercept of the plot. Second virial coefficient was determined as 6.24E-03 mLg−1Da. The positive value of A2 shows that the overall net interactive force is repulsive between the solute species and hence stable in the aqueous nitric acid medium. The positive value of the second virial coefficient shows a positive ΔG for polymer chain interpenetration which leads to steric stabilization. The resulting stabilization could be the result of positive ΔH or negative ΔS, where positive enthalpy reflects the release of bound solvent and negative entropy reflects the loss of configurational freedom as the polymer chains interpenetrate. At this condition the dispersion is sterically stabilized. Thus nitric acid is found to be a good solvent medium. The values of KC/Rop, mean diameter, and hydro molecular weight of each concentration are given in Table 3. With increasing concentration of Bi the degree of polymerization increases. The calculated parameters from the Debye plot are given in Table 4. The results show that Bi undergoes hydrolysis at low pH and forms polymers with more than 5 units.Table 2
Refractive indices for different concentration of Bi solutions.
Wt. concentration(gmL−1)
Refractive index
RI increment(dn/dC in mLg−1)
0.00634
1.33715
0.01212
1.33750
0.0842
0.02460
1.33866Table 3
Values of mean diameter,KC/Rop, and hydro-MW for different concentrations of Bi.
Weight concentration (g/mL)
Mean diameter (µm)
KC/Rop (1/Da)
Hydro-MW
0.00640
0.4530
8.27
E
-
04
1.28
E
+
07
0.01212
0.0518
8.50
E
-
04
1.91
E
+
08
0.02460
0.1262
8.85
E
-
04
2.76
E
+
09Table 4
Calculated parameters from the Debye plot.
Substance
Measured atλ=780 nm
Bi (III)  hydrous polymer
M
w (Da)
Second virial coefficient,A2 (mLg−1 Da)
1,236
6.24
E
-
03Figure 3
Thedn/dC curves obtained for different concentration of Bi(III) solution (R2=0.9827).Figure 4
Debye plot for various concentrations ofBi3+ with R2 of 0.9834.


## 4. Conclusion

A new approach was applied to interpret the hydrolytic behaviour of Bi using light-scattering technique. X-ray diffraction, centrifugation, electrophoretic, and tyndallometric studies reported the different species of Bi present in aqueous medium. The present investigation attempts to determine the molecular weight of the hydrolyzed species. It was shown that the particle size increases due to increased aggregation of solute. This shows that polymerization of Bi strongly depends on concentration. The second virial coefficient has also been determined, and the positive value shows that there is repulsion between the molecules making the polymeric solution stable. The weight average molecular weight of polymers of Bi(III) formed in aqueous nitric acid medium has confirmed that the hydrolyzed species has 5-6 atoms of Bismuth.



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*Source: 194120-2013-02-12.xml*