Exploring the Effects of Polyacrylic Acid on Triton-X-100 Aqueous Solutions: Density, Viscosity and Ultrasonic Velocity Analysis

 

Anil D. Kakuste1, Sachin S. Borse1*, Gunvant H. Sonawane2

1Department of Chemistry, V. U. Patil Arts and Late. Dr. B. S. Desale Science College,

Sakri, Taluka- Sakri, District- Dhule, Maharashtra, India.

2Department of Chemistry, Kisan Arts, Commerce and Science College, Parola, Dist- Jalgaon, Maharashtra, India.

*Corresponding Author E-mail: anilkakuste@ymail.com, sachinborseld32@gmail.com, drgunvantsonawane@gmail.com

 

ABSTRACT:

This study explore the intricate interplay between Triton-X-100 surfactant and polyacrylic acid (PAA) polymer in aqueous solutions, focusing on the influence of temperature variations and PAA concentrations on the physical properties. Through experimental analysis, including measurements of density, viscosity, and ultrasonic velocity, various interaction parameters were calculated to elucidate the underlying phenomena. Notably, the viscosity of the surfactant solution increases with increasing PAA concentration. Temperature alterations revealed nuanced effects: while ultrasonic velocity displayed an initial rise from 298.15 K to 308.15 K, followed by a decline at 313.15 K, density, adiabatic compressibility, and intermolecular free length decreased with rising temperatures. Conversely, ultrasonic velocities, acoustic impedance, molar volumes, and molar sound velocities exhibited an upward trend with increasing temperature. Moreover, the ultrasonic velocities demonstrated a complex relationship with PAA concentration, the ultrasonic velocities initially increases then decreases with increasing concentration of PAA. For 0.03% PAA it shows maximum ultrasonic velocities and maximum velocity observed at 0.03% PAA concentration. This comprehensive analysis sheds light on the thermodynamic and acoustic behavior of Triton-X-100/PAA aqueous solutions, offering valuable insights into their physical interactions.

 

KEYWORDS: Surfactant, Nonionic surfactant Triton-X-100, Ultrasonic velocity, Acoustic parameter, Polymer Polyacrylic acid.

 


INTRODUCTION

Surfactants play a very crucial role in our daily used products and in research fields1. The last decade has seen the extension of cationic surfactant application to high technology areas such as electronic printing, magnetic recording, biotechnology and microelectronics2,3. The solution properties of nonionic surfactants and polymers alone and mixture has been extensively studied4,5.

 

 

 

The study of binary and ternary liquid systems comprising surfactants and polymers has garnered significant interest due to their diverse industrial applications, ranging from pharmaceuticals to enhanced oil recovery.

 

The physicochemical studies of polymer-surfactant solution have created much interest regarding their industrial importance6,7.

 

Triton-X-100, a widely-used nonionic surfactant, exhibits complex behavior when mixed with water-soluble polymers like polyacrylic acid (PAA). Understanding the interactions within such systems is crucial for optimizing their performance in various applications. In this article, we studied the interactions properties of aqueous solutions containing Triton-X-100, a commonly used nonionic surfactant, in conjunction with polyacrylic acid (PAA), a water-soluble polymer. By employing experimental techniques to measure density, viscosity, and ultrasonic velocity across varying concentrations and temperatures, we aim to unravel the intricate interplay between Triton-X-100 and PAA molecules.

 

MATERIALS AND METHODS:

Materials:

Nonionic surfactant Triton-X-100 was purchased from Loba Chemie, India. The Additive used is water soluble polymer Polyacrylic acid (PAA) (Mol. Wt. 50,000) was purchase from Otto Chemica India. Doubly distilled water was used for preparation of all solutions. Triton-X-100 solutions were prepared in 30% ethanol.

 

Surfactant-Triton-X-100-

 

 

Additive-PAA-

 

Methods:

 

Ultrasonic Velocity Measurement:

The ultrasonic velocity measurement is useful in understanding interaction between surfactant-polymer systems and provides the information of micelle in solution8. The interferometer cell was filled with the solution under test and connected to output terminals of the high frequency generator through the shielded cable. Water was circulated around the measuring cell from a thermostat to maintain require temperature. When the solution in cell attains the temperature of bath, the micrometer screw was slowly moved till the anode current meter showed at maximum. The frequency ‘f’ of the crystal is accurately known. Here the frequency of the crystal is 2 MHz, the ultrasound velocity (U) was calculated by using formula: U= λ x f

 

The various physical parameters calculated from the measured values of density (ρ), viscosity (η) and ultrasound velocity (U) using the standard formula9,10.

Adiabatic Compressibility                                 (βad) = 1/ρU2

Intermolecular free length                  (Lf) = K (βad) ½

Molar Sound Velocity                         (Rm) = (/ρ) U 1/3

Specific Acoustic Impedance           (Z) = (ρU)

Molar Volume                                      (Vm) =/ρ)

Surface Tension                           (γ) = (U 3/2) (6.3 x 10-4) ρ

 

Where U is the ultrasonic velocity, ρ is the density; K is the Jacobson’s temperature depended constant [(84.875+0.375T) x 10-8],  is the effective molecular weight and can be calculated using relation.

 

= X1M1+ X2M2

 

Where M1 and M2 are molecular weights and X1 and X2 are the mole fractions of component-1 additive and component-2 surfactant solution as solvent.

 

RESULT AND DISCUSSION:

Density Measurement:

The densities of Triton-X-100 (0.0155%) were assessed at various temperatures (Table 1). It was noted that within a specific concentration of solution, density decreases with rising temperature, because on increasing temperature, kinetic energy of particles, thermal agitation, and volume of solution increases11.

 

The densities of Triton-X-100 (0.0155%) exhibit an upward trend with the increase in concentration of PAA and decreases with increasing temperature (Table 2 a and b). Such density increments signify enhanced solvent-solvent and solute-solvent interactions, potentially stemming from volume contraction induced by the presence of solute molecules. The fluctuations in densities can be elucidated through the co-sphere overlap model. Here, the overlapping of hydration co-spheres between hydrophobic-hydrophobic and ion-hydrophobic groups leads to a net reduction in volume. Conversely, interactions involving ion-hydrophilic and hydrophilic-hydrophilic groups contribute to volume expansion12-16.

 

Viscosity Measurement:

It was noted that as temperatures increases, the viscosity of Triton-X-100 (0.0155% w/v) decreases. Furthermore, viscosity measurements were conducted on Triton-X-100 (0.0155%) in the presence of polymer PAA across diverse concentrations and temperatures. Remarkably, the viscosity of Triton-X-100 increases with increasing PAA concentration but declines with increasing temperatures (Table 3). The increase in viscosity with increase in concentration of PAA indicates the increase in cohesiveness present in the solute-solvent molecules17. The rise in viscosity attributed to stronger hydrophilic-hydrophobic interactions in aqueous media. The hydrophobic segments of surfactant congregate forming hydrophobic domain. These domains serve as intermolecular cross links which boosting viscosity.

 

Ultrasonic Velocity of Triton-X-100 (0.0155% w/v):

The data indicates that, according to Table 1, for the Triton-X-100 system, as temperature increases, density, adiabatic compressibility, and intermolecular free length decreases, consequently leading to increases in ultrasonic velocities, acoustic impedance, molar volumes, molar sound velocities, and surface tension. The rise in ultrasonic velocities with increasing temperature is attributed to structural reorganization resulting from hydration18,19.

 

Ultrasonic Velocity of Triton-X-100 and PAA Mixed System:

This study investigates the ultrasonic velocity measurement of Triton-X-100 and polyacrylic acid (PAA) mixed systems, with the concentration of Triton-X-100 maintained at its critical micelle concentration (CMC) while varying the concentration of PAA additive and temperature of mixed system (Table 2 a and b). Measurements were conducted at temperatures of 298.15 K, 303.15 K, 308.15 K, and 313.15 K to explore the effects of temperature on the physical interactions within the system. On experimental analysis it was noted that, density (ρ), adiabatic compressibility ad) and intermolecular free length (Lf) decreased with increasing temperatures, while ultrasonic velocities (U), specific acoustic impedance (Z), molar volumes (Vm), and molar sound velocities (Rm) demonstrated an upward trend. Additionally, at particular temperature, the ultrasonic velocities displayed a non-linear relationship with PAA concentration, reaching a peak at 0.03% PAA concentration. This indicates complete dissolution of Triton-X-100 and making the medium more and clearer. The ultrasonic velocity then decreases with increase in concentration of PAA, the hydrophobic potion of surfactant may associate to form micelle rods. Formation of such rods may interfere with ultrasonic velocity. Hence ultrasonic velocity decreases with increase in concentration of PAA. These findings contribute to a deeper understanding of the thermodynamic and acoustic behavior of Triton-X-100/PAA mixed systems, providing insights into their physical interactions under varying conditions.

 

In the data provided in Table 2(a) and Table 2(b), concerning the nonionic surfactant-PAA mixed system, it is observed that the ultrasonic velocity exhibits an upward trend with increasing temperature. But at a fixed temperature, there is a rise in ultrasonic velocities, followed by a subsequent decline with increasing concentrations of PAA. Notably, at a PAA concentration of 0.03%, the ultrasonic velocities reach their maximum value due to structural rearrangement induced by hydration20,21. Additionally, this phenomenon may be attributed to alterations in overall free energy and changes in micelle shape from spherical to cylindrical/rod-like structures and that interfere the propagation of ultrasonic waves. The peak ultrasonic velocity corresponds to the aggregation of monomers into micelles. The subsequent decrease in velocity could be linked to a transition in micelle shape from cylindrical/rod-like to spherical configurations. This intriguing observation is closely associated with the well-established interpolymeric association reactions occurring between polyethylene oxide and polycarboxylic acids.

 

The variation of sound velocity with concentration of surfactant is given by the relation.

 

dU/dc = - (U/2) [(1/ρ) (dρ/dc) + (1/ βad) (dβad / dc)]  

 

According to the Eyring and Kincaid model of sound wave propagation, the intermolecular free length decreases as the ultrasonic velocity value increases22,223. This concept is reinforced by the anticipated decrease in βad with higher concentrations of surfactant, indicating potential interactions between the solute and solvent. As ultrasonic velocity increases, the intermolecular free length (Lf) and adiabatic compressibility (βad) decrease, and vice versa. This inverse relationship aligns with the Eyring and Kincaid model. The decrease in Lf and βad values with increase in ultrasonic velocity suggests substantial interaction between PAA and the surfactant, influencing the structural arrangement within the solution mixture, indicative of strong solute-solvent interactions and less closely packed molecules. The variation of βad reveals insights: minimal compressibility enhances bond strength, while maximal compressibility signifies weaker bond strength between molecules. The increase in βad values, attributed to the removal of solvent molecules around ions, supports weak interactions. Furthermore, βad values decrease with increasing concentrations of PAA, further emphasizing the intricate interplay between the components in the solution mixture. The increase in specific acoustic impedance (Z) with increase in concentration and temperature are an indicative of the increase in intermolecular forces with the addition of PAA with surfactant because of aggregation of solvent molecules around solute, which induces strong solute-solvent interaction24. Further, the higher value of specific acoustic impedance (Z) confirms the stronger interaction between the PAA and surfactant.


 

 

Table 1. Ultrasound velocities of Triton-X-100 (0.0155 %)

Temp

(K)

ρ

(Kgm-3)

U

(ms-1)

βad x10-10

(Kg-1ms2)

Lf

(Ao)

Z x106

(Kgm-2s-1)

Vm x10-3

(L.mol-1)

Rm x 10-4 mmol-1 (N/m1/2)-1/3

γ x104

(Nm-1)

298.15

997.0875

2328.00

1.8505

0.2675

2.3212

128.73293

1706.15

7.056

303.15

995.6825

2816.00

1.2665

0.2213

2.8038

159.73767

2255.72

9.374

308.15

994.0916

2840.00

1.2472

0.2196

2.8232

190.86571

2702.93

9.479

313.15

992.2569

2944.00

1.1628

0.2120

2.9212

253.07761

3627.16

9.986

 

Table 2 (a). Ultrasonic Velocity for 0.0155 % Triton-X-100 + PAA

Temp

(K)

ρ

(Kgm-3)

U

(ms-1)

βad x10-10

(Kg-1ms2)

Lf

(Ao)

Z x106

(Kgm-2s-1)

Vm x10-3

(L.mol-1)

Rm x 10-4 mmol-1 (N/m1/2)-1/3

γ x104

(Nm-1)

298.15 K

0.005

997.8623

1992.00

2.5255

0.3125

1.9877

128.63298

1618.51

5.589

0.01

998.1791

2076.00

2.3245

0.2998

2.0722

159.33814

2032.65

5.948

0.02

998.7047

2280.00

1.9262

0.2729

2.2770

189.98409

2500.51

6.850

0.03

999.2999

2440.00

1.6808

0.2549

2.4383

251.29393

3383.08

7.588

0.04

999.8415

2128.00

2.2086

0.2922

2.1277

312.54754

4020.13

6.183

0.05

1000.0998

2088.00

2.2935

0.2978

2.0882

373.84069

4778.19

6.011

303.15 K

0.005

995.7543

2160.00

2.1525

0.2912

2.1508

128.90529

1666.31

6.298

0.01

996.3531

2276.00

1.9375

0.2763

2.2677

159.63016

2099.77

6.816

0.02

996.8691

2320.00

1.8637

0.2710

2.3127

190.33392

2519.68

7.018

0.03

997.6727

2600.00

1.4827

0.2417

2.5939

251.70379

3461.10

8.333

0.04

998.5258

2304.00

1.8866

0.2726

2.3006

312.95936

4133.48

6.957

0.05

999.6450

2160.00

2.1441

0.2907

2.1592

374.01077

4834.69

6.322

 

Table 2 (b). Ultrasonic Velocity for 0.0155 % Triton-X-100 + PAA

Temp

(K)

ρ

(Kgm-3)

U

(ms-1)

βad x10-10

(Kg-1ms2)

Lf

(Ao)

Z x106

(Kgm-2s-1)

Vm x10-3

(L.mol-1)

Rm x 10-4 mmol-1 (N/m1/2)-1/3

γ x104

(Nm-1)

308.15 K

0.005

994.6692

2224.00

2.0326

0.2857

2.2121

129.04592

1684.44

6.572

0.01

994.2291

2260.00

1.9692

0.2812

2.2470

159.97118

2099.32

6.730

0.02

994.8458

2472.00

1.6449

0.2570

2.4593

190.72101

2578.78

7.703

0.03

995.5977

2576.00

1.5136

0.2465

2.5647

252.22839

3457.61

8.201

0.04

996.6254

2512.00

1.5901

0.2527

2.5035

313.55613

4262.41

7.905

0.05

997.3687

2304.00

1.8888

0.2754

2.2979

374.86438

4951.10

6.949

313.15 K

0.005

992.7568

2312.00

1.8844

0.2776

2.2953

129.29451

1709.66

6.953

0.01

993.3988

2280.00

1.9365

0.2814

2.2649

160.10488

2107.25

6.813

0.02

993.8996

2528.00

1.5744

0.2538

2.5126

190.90258

2600.58

7.959

0.03

994.5153

2880.00

1.2123

0.2227

2.8642

252.50290

3592.50

9.684

0.04

995.3549

2536.00

1.5622

0.2528

2.5242

313.95636

4281.40

8.008

0.05

996.1707

2360.00

1.8024

0.2715

2.3510

375.31519

4996.89

7.195

 


Table 3. Viscosity of Triton-X-100 (0.0155 %) in presence of PAA at various temperatures and concentrations

Conc. %

(w/v)

PAA

298.15 K

303.15 K

308.15 K

313.15 K

0.005

0.9354

0.8667

0.7217

0.6985

0.01

0.9496

0.8887

0.7238

0.7081

0.02

0.9621

0.9208

0.7311

0.7317

0.03

0.9866

0.9491

0.7464

0.7434

0.04

1.0190

0.9653

0.7686

0.7592

0.05

1.0521

0.9903

0.8059

0.7908

 

CONCLUSION:

The investigation encompassed measurements of density, viscosity, and ultrasonic velocity of Triton-X-100 (at 0.0155% concentration) in aqueous solutions containing water-soluble polymer PAA across diverse temperatures and concentrations. The viscosity of Triton-X-100 increases with increasing PAA concentration but declines with increasing temperatures. This may be due to stronger hydrophilic-hydrophobic interactions in aqueous media. Notably, the observed increase in ultrasonic velocity is intricately linked to the structural characteristics of both solutes and surfactants within the system. With rising temperatures, the potential for structural rearrangement due to hydration increases, leading to a more ordered state. Analysis of density, viscosity, ultrasonic velocity, and additional thermodynamic properties such as adiabatic compressibility, acoustic impedance, and intermolecular free length unveiled a non-linear relationship. This non-linearity provides evidence of diverse interactions including solute-solvent, dipole-dipole, and ion-solvent interactions within the system, underscoring the complexity of the molecular dynamics at play. For 0.03% PAA, it shows maximum ultrasonic velocities. This may be due to structural rearrangement as a result of hydration.

 

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Received on 20.04.2024                    Modified on 23.05.2024

Accepted on 21.06.2024                   ©AJRC All right reserved

Asian J. Research Chem. 2024; 17(3):134-138.

DOI: 10.52711/0974-4150.2024.00025