# Interaction between Aqueous Solutions of Hydrophobically Associating Polyacrylamide and Dodecyl Dimethyl Betaine

Authors: Zhongbin Ye; Guangfan Guo; Hong Chen; Zheng Shu
Journal: Journal of Chemistry
 (2014)

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## Abstract

The interaction between hydrophobically associating polyacrylamide (HAPAM) and dodecyl dimethyl betaine (BS-12) is studied through surface tension, interfacial tension (IFT), apparent viscosity, aggregation behavior, and microscopic morphologies. Results show that surface and interface properties of BS-12 are largely affected by HAPAM. BS-12 critical micelle concentrations are increased with the increment of polymer concentrations. Abilities of reduced air-water surface tension and oil-water interfacial tension are dropped. The oil-water interfacial tension to reach minimum time is increased. HAPAM can form network structures in the aqueous solution. Mixed micelles are formed by the interaction between BS-12 micelles and hydrophobic groups of HAPAM in aqueous solution and self-assembly behavior of HAPAM is affected. With the increment of surfactant concentrations, the apparent viscosity, apparent weight average molecular weights (Mw, a), root mean square radius of gyration (〈Rg〉), and hydrodynamic radius of HAPAM increase first and then decline. Moreover, microscopic morphologies of the mixed system are formed from relatively loose network structures to dense network structures and then become looser network structures and the part of network structures fracture.


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## Body

## 1. Introduction

Water-soluble polymers modified with a small amount of hydrophobic groups (<2%, mole fraction) have become of great interest in recent years. They have broad application prospects, such as oil exploration, paint, mineral separation, and cosmetic and pharmaceutical preparations et al. [1–4]. Hydrophobically associating polymer molecules in aqueous solution, three-dimensional network structures are formed through the intermolecular interaction. Therefore, hydrophobically modified polymers have the good increasing viscosity, heat resistance, salt resistance and shear resistance, and so on [5–7], and they have a good application prospect.Polymer-surfactant mixed system is a kind of very important soft substance. Usually adding surfactants into polymer solutions, the dosage of polymers or surfactants can be reduced, and solution performances are improved [8–10]. The mixed system has many unique properties, for example, the system viscosity, interfacial adsorption, solubilization, drug delivery, and so on. So the study of polymer-surfactant mixed system is that people are very interested in research subjects [11–14]. In recent years, the interaction between hydrophobically associating polyacrylamide (HAPAM) and surfactant is studied by some scholars [15–18]. These studies find that the system can form mixed micelles and rheological properties of polymer solutions can be changed to a great extent. The interaction between polymer and surfactant is mainly decided by the polymer hydrophobicity and the surfactant structure. Betaine is a main type of zwitterionic surfactant. It shows characteristics of different ionic surfactant under different conditions owing to having anionic and cationic groups at the same time. Now the interaction between HAPAM and betaine surfactants is very little researched [19]. In this paper, the interaction of hydrophobically associating polyacrylamide (HAPAM) and dodecyl dimethyl betaine is studied. Expecting polymer-surfactant mixed system has good application prospects in washing textile, daily chemical and oil field development, and so on.


## 2. Experiment

### 2.1. Materials and Instruments

Acrylamide (AM), acrylic acid (AA), anhydrous sodium carbonate (Na2CO3), potassium persulfate (K2S2O8), and sodium hydrogen sulfite (NaHSO3) were provided by Chengdu Kelong Chemical Reagents Corporation, China, and all drugs were analytical pure. 18-Alkyl-dimethyl diallyl ammonium chloride (C18DMAAC, its molecular structure be shown in Figure 1) and dodecyl dimethyl betaine (BS-12) were supplied by Southwest Petroleum University. TX-500C full range tensiometer was purchased from the United States Bowing Industry Corporation. Brookfield DV-III viscometer was purchased from the United States Brookfield Instrument Corporation. BI-200SM dynamic/static wide angle laser light scattering apparatus was purchased from the United States Brooke Haven Instrument Corporation. Nanoscope IIIa atomic force microscope was purchased from the United States Digital Instrument Corporation.Figure 1
Molecular structure of 18-alkyl-dimethyl diallyl ammonium chloride (C18DMAAC).


### 2.2. Synthesis of Hydrophobically Associating Polyacrylamide

Hydrophobically associating polyacrylamide (HAPAM) synthesis is as follows. 80 g distilled water, 14.9 g acrylamide (AM), 5 g sodium acrylate (acrylic acid and anhydrous sodium carbonate), and 0.1 g 18-alkyl-dimethyl diallyl ammonium chloride (C18DMAAC) were added into a three-necked flask according to the literature [20]. Adjusting the pH value of the system was 6.0-7.0, and potassium persulfate/sodium hydrogen sulfite redox (0.03%–0.05%) were added. The solution was mixed and then bubbled with nitrogen for 30 min to displace dissolved oxygen then quickly capped. The polymerization was carried out at 50°C for 24 h. Products were precipitated and purified by ethanol to remove unreacted monomers and oligomers and then were baked in a vacuum drying oven at the 50°C to constant quality. The polymer molecular structure was shown in Figure 2, and characteristic parameters were shown in Table 1.Table 1
Characteristic parameters of hydrophobically associating polyacrylamide (HAPAM).
Sample
Molecular weight
Degree of hydrolysis (%)
Critical association concentration (ppm)
Polydispersity index
HAPAM
6000000
25.0
800
1.46Figure 2
Molecular structure of hydrophobically associating polyacrylamide (HAPAM) (theoretical mole percents ofx, y, and z were about 79.7%, 20.2%, and 0.1%, resp.).


### 2.3. Solution Preparation

The aqueous solutions (5000 ppm) of surfactant and polymer were always freshly prepared using a mechanical stirrer for 8–10 h to form a consistent homogeneous solution at a low rotation per minute. Appropriate quantity of zwitterionic surfactants and hydrophobically associating polymers were dissolved carefully in distilled water for about 40 min [21, 22].


### 2.4. Measurement of Surface Tension and Interfacial Tension

In polymer-surfactant mixed systems, polymer concentrations were 500, 1000, 1500, and 2000 ppm, respectively, and BS-12 concentrations were 10–2000 ppm. The surfactant solution with or without HAPAM as outer-phase was injected into the glass tube, and 2μL air or oil as inner-phase was put into the middle of the tube. Then the tube was enveloped with the plastic cover and put into the apparatus measuring the surface tension or interfacial tension at a temperature of 25°C [3]. In surface tension experiment, the outer-phase was polymer-surfactant mixed system and the inner-phase was air. Surface tensions of polymer-surfactant mixed systems were measured at a rotating velocity of 6000 rpm, when surface tension reached a minimum value and stopped the test. In interfacial tension (IFT) experiment, the outer-phase was polymer-surfactant mixed system and the inner-phase was dodecane. Interfacial tensions of mixed systems were measured at a rotating velocity of 5000 rpm, when interfacial tension reached a minimum value and stopped the test. In dynamic interfacial tension (DIFT) experiment, surfactant concentration was selected to make oil-water interfacial tension minimum in different polymer concentrations, and then interfacial tensions of the mixed system as time changing were measured a at a rotating velocity of 5000 rpm.


### 2.5. Measurement of Apparent Viscosity

In polymer-surfactant mixed systems, the polymer concentration was 1500 ppm and BS-12 concentrations were 10–2000 ppm. The viscosities of polymer-surfactant mixed systems were measured by Brookfield DV-III viscometer with a shearing rate of 7.34 s−1 and at a temperature of 25°C.


### 2.6. Laser Light Scattering Experiment

The diluted polymer-surfactant mixed system was dusted and filtered by the Millipore Corporation production of the disposable filter with a 0.8μm aperture. The filtrate was collected in the sample pool. In the laser light scattering experiment, toluene as a standard solution, the laser wavelength was 532 nm and the measured temperature was 25°C [23, 24].According to the light scattering theory [25–27], weight average molecular weight (Mw) and root mean square radius of gyration (〈Rg〉) of polymers were measured by static light scattering. For high molecular weight polymers, the light scattering of polymer dilute solution can be expressed as:
(1)(KCRvv(q))1/2≈(1MW)1/2(1+16〈Rg2〉q2)×(1+A2MwC),
where K=4π2n02(dn/dC)2/(Nλ04), K was associated with the constant of solvent nature and incident light frequency; n0 was the refractive index of solution; C was the solution concentration, ppm; Rvv(q) was the solvent effect of scattering intensity for different angles; λ0 was the incident light wavelength; λ was the wavelength of incident light in solution, λ=λ0/n0; dn/dC was the refractive index increment and the ratio of solution refractive index and concentration, ppm; N was the Avogadro constant; 〈Rg〉 was root mean square radius of gyration and the chain quality centre to each chain segment average of squared distance. When the scattering angles were θ→0 and concentrations were C→0, some parameters were obtained such as 〈Rg〉 and Mw by extrapolation [28, 29].Hydrodynamic radius〈Rh〉 of polymer molecules under different surfactant concentrations was measured by dynamic light scattering (DLS) [24]. In the dynamic light scattering, measurements were the light intensity-light intensity time related spectroscopy:
(2)G(2)(τ)=A·(1+β·|g(1)(τ)|2),
where G(2)(τ) was the autocorrelation function of light intensity; A was the baseline of the autocorrelation function; β was the experimental constant of constraint signal noise ratio, associated with the measuring experimental device; g(1)(τ) was autocorrelation function of electric field. Its relationship with the line width distribution G(Γ) is as follows:
(3)g(1)(τ)=∫0∞G(Γ)exp⁡(-Γτ)dΓ.
If the relaxation is caused entirely by diffusion, under the conditions of C→0 and q→0, Γ=Dq2, D was the particle diffusion coefficient and q was the scattering vector. This moment, when the concentration was very low, D extrapolated to zero point and particle size distributions were obtained through Stokes-Einstein formulas D=KBT/(3πηd), where: KB was Boltzmann constant; T was absolute temperature; η was solvent viscosity; d was particle diameter.


### 2.7. Measurement of Molecular Aggregation Morphologies

AFM operating mode was tapping; Probe model was RTESP; operating frequency was 86 kHz; force constants were 1~5 Nm−1. The system was stirred at a low velocity for 5 min to obtain a homogeneous solution concentration. For the AFM measurements, 0.1 mL of the prepared polymer-surfactant mixed system was dropped onto freshly cleaved mica, and the redundant solution was blown off by a stream of high purity nitrogen. Samples were measured by Nanoscope IIIa microscope in air at the ambient temperature [30].


## 2.1. Materials and Instruments

Acrylamide (AM), acrylic acid (AA), anhydrous sodium carbonate (Na2CO3), potassium persulfate (K2S2O8), and sodium hydrogen sulfite (NaHSO3) were provided by Chengdu Kelong Chemical Reagents Corporation, China, and all drugs were analytical pure. 18-Alkyl-dimethyl diallyl ammonium chloride (C18DMAAC, its molecular structure be shown in Figure 1) and dodecyl dimethyl betaine (BS-12) were supplied by Southwest Petroleum University. TX-500C full range tensiometer was purchased from the United States Bowing Industry Corporation. Brookfield DV-III viscometer was purchased from the United States Brookfield Instrument Corporation. BI-200SM dynamic/static wide angle laser light scattering apparatus was purchased from the United States Brooke Haven Instrument Corporation. Nanoscope IIIa atomic force microscope was purchased from the United States Digital Instrument Corporation.Figure 1
Molecular structure of 18-alkyl-dimethyl diallyl ammonium chloride (C18DMAAC).


## 2.2. Synthesis of Hydrophobically Associating Polyacrylamide

Hydrophobically associating polyacrylamide (HAPAM) synthesis is as follows. 80 g distilled water, 14.9 g acrylamide (AM), 5 g sodium acrylate (acrylic acid and anhydrous sodium carbonate), and 0.1 g 18-alkyl-dimethyl diallyl ammonium chloride (C18DMAAC) were added into a three-necked flask according to the literature [20]. Adjusting the pH value of the system was 6.0-7.0, and potassium persulfate/sodium hydrogen sulfite redox (0.03%–0.05%) were added. The solution was mixed and then bubbled with nitrogen for 30 min to displace dissolved oxygen then quickly capped. The polymerization was carried out at 50°C for 24 h. Products were precipitated and purified by ethanol to remove unreacted monomers and oligomers and then were baked in a vacuum drying oven at the 50°C to constant quality. The polymer molecular structure was shown in Figure 2, and characteristic parameters were shown in Table 1.Table 1
Characteristic parameters of hydrophobically associating polyacrylamide (HAPAM).
Sample
Molecular weight
Degree of hydrolysis (%)
Critical association concentration (ppm)
Polydispersity index
HAPAM
6000000
25.0
800
1.46Figure 2
Molecular structure of hydrophobically associating polyacrylamide (HAPAM) (theoretical mole percents ofx, y, and z were about 79.7%, 20.2%, and 0.1%, resp.).


## 2.3. Solution Preparation

The aqueous solutions (5000 ppm) of surfactant and polymer were always freshly prepared using a mechanical stirrer for 8–10 h to form a consistent homogeneous solution at a low rotation per minute. Appropriate quantity of zwitterionic surfactants and hydrophobically associating polymers were dissolved carefully in distilled water for about 40 min [21, 22].


## 2.4. Measurement of Surface Tension and Interfacial Tension

In polymer-surfactant mixed systems, polymer concentrations were 500, 1000, 1500, and 2000 ppm, respectively, and BS-12 concentrations were 10–2000 ppm. The surfactant solution with or without HAPAM as outer-phase was injected into the glass tube, and 2μL air or oil as inner-phase was put into the middle of the tube. Then the tube was enveloped with the plastic cover and put into the apparatus measuring the surface tension or interfacial tension at a temperature of 25°C [3]. In surface tension experiment, the outer-phase was polymer-surfactant mixed system and the inner-phase was air. Surface tensions of polymer-surfactant mixed systems were measured at a rotating velocity of 6000 rpm, when surface tension reached a minimum value and stopped the test. In interfacial tension (IFT) experiment, the outer-phase was polymer-surfactant mixed system and the inner-phase was dodecane. Interfacial tensions of mixed systems were measured at a rotating velocity of 5000 rpm, when interfacial tension reached a minimum value and stopped the test. In dynamic interfacial tension (DIFT) experiment, surfactant concentration was selected to make oil-water interfacial tension minimum in different polymer concentrations, and then interfacial tensions of the mixed system as time changing were measured a at a rotating velocity of 5000 rpm.


## 2.5. Measurement of Apparent Viscosity

In polymer-surfactant mixed systems, the polymer concentration was 1500 ppm and BS-12 concentrations were 10–2000 ppm. The viscosities of polymer-surfactant mixed systems were measured by Brookfield DV-III viscometer with a shearing rate of 7.34 s−1 and at a temperature of 25°C.


## 2.6. Laser Light Scattering Experiment

The diluted polymer-surfactant mixed system was dusted and filtered by the Millipore Corporation production of the disposable filter with a 0.8μm aperture. The filtrate was collected in the sample pool. In the laser light scattering experiment, toluene as a standard solution, the laser wavelength was 532 nm and the measured temperature was 25°C [23, 24].According to the light scattering theory [25–27], weight average molecular weight (Mw) and root mean square radius of gyration (〈Rg〉) of polymers were measured by static light scattering. For high molecular weight polymers, the light scattering of polymer dilute solution can be expressed as:
(1)(KCRvv(q))1/2≈(1MW)1/2(1+16〈Rg2〉q2)×(1+A2MwC),
where K=4π2n02(dn/dC)2/(Nλ04), K was associated with the constant of solvent nature and incident light frequency; n0 was the refractive index of solution; C was the solution concentration, ppm; Rvv(q) was the solvent effect of scattering intensity for different angles; λ0 was the incident light wavelength; λ was the wavelength of incident light in solution, λ=λ0/n0; dn/dC was the refractive index increment and the ratio of solution refractive index and concentration, ppm; N was the Avogadro constant; 〈Rg〉 was root mean square radius of gyration and the chain quality centre to each chain segment average of squared distance. When the scattering angles were θ→0 and concentrations were C→0, some parameters were obtained such as 〈Rg〉 and Mw by extrapolation [28, 29].Hydrodynamic radius〈Rh〉 of polymer molecules under different surfactant concentrations was measured by dynamic light scattering (DLS) [24]. In the dynamic light scattering, measurements were the light intensity-light intensity time related spectroscopy:
(2)G(2)(τ)=A·(1+β·|g(1)(τ)|2),
where G(2)(τ) was the autocorrelation function of light intensity; A was the baseline of the autocorrelation function; β was the experimental constant of constraint signal noise ratio, associated with the measuring experimental device; g(1)(τ) was autocorrelation function of electric field. Its relationship with the line width distribution G(Γ) is as follows:
(3)g(1)(τ)=∫0∞G(Γ)exp⁡(-Γτ)dΓ.
If the relaxation is caused entirely by diffusion, under the conditions of C→0 and q→0, Γ=Dq2, D was the particle diffusion coefficient and q was the scattering vector. This moment, when the concentration was very low, D extrapolated to zero point and particle size distributions were obtained through Stokes-Einstein formulas D=KBT/(3πηd), where: KB was Boltzmann constant; T was absolute temperature; η was solvent viscosity; d was particle diameter.


## 2.7. Measurement of Molecular Aggregation Morphologies

AFM operating mode was tapping; Probe model was RTESP; operating frequency was 86 kHz; force constants were 1~5 Nm−1. The system was stirred at a low velocity for 5 min to obtain a homogeneous solution concentration. For the AFM measurements, 0.1 mL of the prepared polymer-surfactant mixed system was dropped onto freshly cleaved mica, and the redundant solution was blown off by a stream of high purity nitrogen. Samples were measured by Nanoscope IIIa microscope in air at the ambient temperature [30].


## 3. Results and Discussions

### 3.1. Surface Tension of Polymer-Surfactant Mixed System

It is well known that surfactants reduce the surface tension of water by getting adsorbed on the liquid-gas interface. The CMC, one of the main parameters for surfactants, is the concentration at which surfactant solutions begin to form micelles in large amounts [22]. Different techniques are used to examine the water-soluble polymer-surfactant aggregates formed in solution [31, 32]. Surface tensions of surfactant (BS-12) solutions at different concentrations were measured and plotted as a function of concentrations (Figure 3). Figure 3 shows that the CMC and the surface tension have been a large change after adding polymers into surfactant solutions. When polymers are not added, the CMC and the CMC of the surface tension are minimal. The CMC value of BS-12 is about 300 ppm and the surface tension is about 31.3 mN/m. After the polymers being added, the surfactant CMC and the CMC of surface tensions gradually increase with the increment of polymer concentrations. When HAPAM concentration is about 2000 ppm, the CMC of the mixed system is about 500 ppm and the surface tension increases to 33.4 mN/m. Khan et al. also found the same behavior of polyacrylamide solutions in the presence of SDBS [22]. The reason for this phenomenon is that hydrophobic groups of polymers will interact with surfactant hydrophobic parts, and some surfactants are shackled in the bulk phase. Shackled surfactants increase with the increment of polymer concentrations. They need to consume more surfactants to form micelles [3]. Therefore, reaching critical micelles requires higher surfactant concentrations. Mixed micelles of polymers/surfactants that are formed have been inhibitory effect to the surface tension of surfactants in solution.Figure 3
Effect of HAPAM concentrations on surface tensions of BS-12.


### 3.2. Interfacial Tension of Polymer-Surfactant Mixed System

The polymer-surfactant mixed system has been applied in the oil field owing to reducing the mobility ratio decrease interfacial tension (IFT) between the water and the oil [33, 34]. It has been reported that addition of polymers increases the IFT of ionic surfactants [3, 35]. Interfacial tensions of surfactant (BS-12) solutions at different concentrations are measured, and results are shown in Figure 4. Figure 4 shows that oil-water IFT is decreased with the increment of surfactant concentrations. After a turning point, the IFT becomes to balance. If there are no polymers, the turning point of surfactant concentration and the IFT is minimal. The turning point of surfactant concentration is about 300 ppm and the IFT is about 0.29 mN/m. With the increment of polymer concentrations, the turning point of surfactant concentration and the IFT have shown a trend of increment. This phenomenon is similar to Figure 2. Hydrophobic groups of polymers will interact with surfactant hydrophobic parts and bound part surfactants in the bulk phase. Ultimately, the ability of reduced oil-water IFT is declined. The shackled effect is enhanced with the polymer concentrations increasing. Therefore the reduced oil-water IFT needs to consume more surfactants. On the other hand, the IFT of surfactants can be inhibited by the viscosity of polymer solutions. Chen et al. also confirm the result [3].Figure 4
Effect of HAPAM concentrations on interfacial tensions of BS-12.Figure5 shows the result that the oil-water dynamic interfacial tension (DIFT) of BS-12 is affected by the HAPAM concentrations. The DIFT is changed with time increasing. The reduced surfactant IFT and reaching steady state that required time can be reflected by DIFT characteristics. When surfactant concentrations are 500 ppm, the DIFT change is faster at lower polymer concentrations. Therefore oil-water IFT reaching a minimum need less time. The higher concentrations the polymer is, the longer the time reaching a minimum of IFT is. The reason is that surfactants and associating polymers have the strong interaction and oil-water interface diffusion rates of surfactants which are significantly affected. In addition, the system viscosity increases with the increment of polymer concentrations, and the surfactant spread speed is also slowed. As a result, the IFT reaching a minimum needs longer times at the higher polymer concentrations.Figure 5
Effect of HAPAM concentrations on the dynamic interfacial tensions of BS-12.


### 3.3. Apparent Viscosity of Polymer-Surfactant Mixed System

The effect of BS-12 concentrations on the viscosity of polymers is shown in Figure6. Figure 6 shows that the system viscosity increases first and then declines with the increment of BS-12 concentrations. When the BS-12 concentration is about 100 ppm, the system viscosity is the largest. Badoga et al. [36] and Jiang et al. [37] have reported that the viscosity of polymer-surfactant mixed systems increases first and then declines with the increment of surfactant concentrations. When the addition of surfactant concentrations is lower, surfactant molecules in single molecule state are distributed in aqueous solution. Surfactant molecular ions and HAPAM molecular chains interacting with each other make the interaction of hydrophobic groups forming inner salt keys be opened, and the intermolecular association is formed. At this moment, the association between polymer molecules promoted role and polymer molecular chains is more diastolic because of the addition of surfactants. The solution viscosity is increased with the increment of surfactant concentrations. When surfactant concentrations exceed a certain value, the interaction between surfactants and hydrophobic groups of polymer chain segments is further enhanced. Mixed micelles of polymer-surfactant are formed. On the other hand, the intermolecular association of polymers is shielded with the increase of surfactant micellar numbers; thus polymer network structures are damaged and collapsed. The viscosity of mixed systems is decreased.Figure 6
Effect of BS-12 concentrations on the viscosity of 1500 ppm HAPAM.


### 3.4. Laser Light Scattering Experiments

It has been reported [23, 38] that addition of ionic surfactants influences the molecular structure of the polymer. The effects of BS-12 concentrations on apparent weight average molecular weights (Mw,a) of polymers are tested at a 25°C. Their result is shown in Figure 7. The root mean square radius of gyration (〈Rg〉) is characteristic parameters of the polymer and directly reflects the conformation of polymer chains. In order to reduce the effect of polymer concentrations, the preparation concentration of polymers is 2 ppm in experiment. For the dilute polymer solution, 〈Rg〉 can be concluded through extrapolation of the same concentrations with different angles in solution; then some 〈Rg〉 are received under different surfactant concentrations in the same way. Their results are shown in Figure 8.Figure 7
Effect of BS-12 concentrations on apparent weight average molecular weight (Mw,a) of HAPAM.Figure 8
Effect of BS-12 concentrations on root mean square radius of gyration (〈Rg〉) of HAPAM.Figures7 and 8 show that Mw,a and 〈Rg〉 of HAPAM increase first and then decline with the increment of BS-12 concentrations. When there are a few surfactants in the polymer-surfactant mixed system, the surfactant molecules interacting with polymer hydrophobic groups, intermolecular association of polymers is strengthened and polymers are more likely to gather to form super molecular structures. Mw,a and 〈Rg〉 show a trend of increment. When surfactant concentrations are about 100 ppm, the system viscosity is the largest. With the further increment of surfactant concentrations, hydrophobic groups of polymer molecules are inhibited by cationic groups of surfactant molecular chains. The intramolecular association of associating polymers forms inner salt key. Mw,a and  〈Rg〉 become smaller. When surfactant concentrations are more than its critical micelle concentrations, the number of surfactant micelles is increased. Hydrophobic groups of associating polymers are separated by surfactant micelles. The intermolecular association is weakened and supramolecular aggregations are dismantled. Thus, Mw,a and 〈Rg〉 are further smaller.In order to study zwitterionic surfactant (BS-12) effect on hydrodynamic sizes of polymers in solution, the preparation concentration of polymers is 2 ppm in the experiment. Particle size distributions and hydrodynamic radius (〈Rh〉) of the polymer under different surfactant concentrations are measured by dynamic light scattering at a 25°C and the scattering angle is 90°. Their results are shown in Figures 9 and 10. Figure 9 shows that particle sizes of HAPAM are unimodal distribution under no surfactant condition. When surfactant concentrations are about 100 ppm, the particle size distribution of HAPAM is a wider unimodal and moves to the right. Surfactants can enhance intermolecular association of polymers and make polymer chains stretch and hydrodynamic radius increase. When surfactant concentrations are more than 400 ppm, particle sizes of HAPAM are multimodal distributions and wider unimodal move to left. The reason is that surfactant micelles are increased with the increment of surfactant concentrations in solution. Some polymer hydrophobic groups are embedded by surfactant micelles. The intermolecular association of HAPAM is partially blocked, and the hydrodynamic radius appears to be reducing.Figure 9
Particle size distributions of HAPAM with different BS-12 concentrations.Figure 10
Effect of BS-12 concentrations on the hydrodynamic radius(〈Rh〉) of HAPAM.Figure10 shows that 〈Rh〉 is increased because of a small amount of surfactants to be added. When surfactant concentrations are lower, the intermolecular association of HAPAM is strengthened, and 〈Rh〉 is increased. But the surfactant concentrations exceed a certain value; polymer aggregations are dismantled; therefore, 〈Rh〉 is reduced.


### 3.5. Molecular Aggregation Morphologies of Polymer-Surfactant Mixed System

The previous research results had been confirmed that space network structures of hydrophobically associating polymer are formed exceeding the critical association concentration (CAC) of polymer [3, 24]. When ionic surfactants are added, molecular aggregation morphologies of HAPAM are affected. Different BS-12 concentrations affecting molecular aggregation morphologies are observed. Their results are shown in Figure 11. Figure 11(a) is an AFM photo of HAPAM without surfactants. When the HAPAM concentration exceeds the CAC, it can be formed obvious spatial network structures in distilled water [39]. Figure 11(b) is an AFM photo of HAPAM solution to add 100 ppm surfactants. Compared with Figures 11(a) and 11(b), when BS-12 concentrations are about 100 ppm, the space network structures become more intense in solution, and the connecting mesh chain beams are thicker, especially the intersection part of chain beam. Figure 11(c) is an AFM photo of HAPAM solution to add 400 ppm surfactants. Compared with Figures 11(b) and 11(c), when BS-12 concentrations are about 400 ppm, the space network structures become sparser. When surfactants continue to be added, the connecting network chain beams are thinner. These results show that adding a few surfactants has a promoting effect on the self-assembly of polymer molecules, but the self-assembly of polymer molecules is inhibited for adding too many surfactants.AFM images of 1500 ppm HAPAM with different BS-12 concentrations: (a) 0 ppm BS-12, (b) 100 ppm BS-12, and (c) 400 ppm BS-12.
(a)
(b)
(c)


## 3.1. Surface Tension of Polymer-Surfactant Mixed System

It is well known that surfactants reduce the surface tension of water by getting adsorbed on the liquid-gas interface. The CMC, one of the main parameters for surfactants, is the concentration at which surfactant solutions begin to form micelles in large amounts [22]. Different techniques are used to examine the water-soluble polymer-surfactant aggregates formed in solution [31, 32]. Surface tensions of surfactant (BS-12) solutions at different concentrations were measured and plotted as a function of concentrations (Figure 3). Figure 3 shows that the CMC and the surface tension have been a large change after adding polymers into surfactant solutions. When polymers are not added, the CMC and the CMC of the surface tension are minimal. The CMC value of BS-12 is about 300 ppm and the surface tension is about 31.3 mN/m. After the polymers being added, the surfactant CMC and the CMC of surface tensions gradually increase with the increment of polymer concentrations. When HAPAM concentration is about 2000 ppm, the CMC of the mixed system is about 500 ppm and the surface tension increases to 33.4 mN/m. Khan et al. also found the same behavior of polyacrylamide solutions in the presence of SDBS [22]. The reason for this phenomenon is that hydrophobic groups of polymers will interact with surfactant hydrophobic parts, and some surfactants are shackled in the bulk phase. Shackled surfactants increase with the increment of polymer concentrations. They need to consume more surfactants to form micelles [3]. Therefore, reaching critical micelles requires higher surfactant concentrations. Mixed micelles of polymers/surfactants that are formed have been inhibitory effect to the surface tension of surfactants in solution.Figure 3
Effect of HAPAM concentrations on surface tensions of BS-12.


## 3.2. Interfacial Tension of Polymer-Surfactant Mixed System

The polymer-surfactant mixed system has been applied in the oil field owing to reducing the mobility ratio decrease interfacial tension (IFT) between the water and the oil [33, 34]. It has been reported that addition of polymers increases the IFT of ionic surfactants [3, 35]. Interfacial tensions of surfactant (BS-12) solutions at different concentrations are measured, and results are shown in Figure 4. Figure 4 shows that oil-water IFT is decreased with the increment of surfactant concentrations. After a turning point, the IFT becomes to balance. If there are no polymers, the turning point of surfactant concentration and the IFT is minimal. The turning point of surfactant concentration is about 300 ppm and the IFT is about 0.29 mN/m. With the increment of polymer concentrations, the turning point of surfactant concentration and the IFT have shown a trend of increment. This phenomenon is similar to Figure 2. Hydrophobic groups of polymers will interact with surfactant hydrophobic parts and bound part surfactants in the bulk phase. Ultimately, the ability of reduced oil-water IFT is declined. The shackled effect is enhanced with the polymer concentrations increasing. Therefore the reduced oil-water IFT needs to consume more surfactants. On the other hand, the IFT of surfactants can be inhibited by the viscosity of polymer solutions. Chen et al. also confirm the result [3].Figure 4
Effect of HAPAM concentrations on interfacial tensions of BS-12.Figure5 shows the result that the oil-water dynamic interfacial tension (DIFT) of BS-12 is affected by the HAPAM concentrations. The DIFT is changed with time increasing. The reduced surfactant IFT and reaching steady state that required time can be reflected by DIFT characteristics. When surfactant concentrations are 500 ppm, the DIFT change is faster at lower polymer concentrations. Therefore oil-water IFT reaching a minimum need less time. The higher concentrations the polymer is, the longer the time reaching a minimum of IFT is. The reason is that surfactants and associating polymers have the strong interaction and oil-water interface diffusion rates of surfactants which are significantly affected. In addition, the system viscosity increases with the increment of polymer concentrations, and the surfactant spread speed is also slowed. As a result, the IFT reaching a minimum needs longer times at the higher polymer concentrations.Figure 5
Effect of HAPAM concentrations on the dynamic interfacial tensions of BS-12.


## 3.3. Apparent Viscosity of Polymer-Surfactant Mixed System

The effect of BS-12 concentrations on the viscosity of polymers is shown in Figure6. Figure 6 shows that the system viscosity increases first and then declines with the increment of BS-12 concentrations. When the BS-12 concentration is about 100 ppm, the system viscosity is the largest. Badoga et al. [36] and Jiang et al. [37] have reported that the viscosity of polymer-surfactant mixed systems increases first and then declines with the increment of surfactant concentrations. When the addition of surfactant concentrations is lower, surfactant molecules in single molecule state are distributed in aqueous solution. Surfactant molecular ions and HAPAM molecular chains interacting with each other make the interaction of hydrophobic groups forming inner salt keys be opened, and the intermolecular association is formed. At this moment, the association between polymer molecules promoted role and polymer molecular chains is more diastolic because of the addition of surfactants. The solution viscosity is increased with the increment of surfactant concentrations. When surfactant concentrations exceed a certain value, the interaction between surfactants and hydrophobic groups of polymer chain segments is further enhanced. Mixed micelles of polymer-surfactant are formed. On the other hand, the intermolecular association of polymers is shielded with the increase of surfactant micellar numbers; thus polymer network structures are damaged and collapsed. The viscosity of mixed systems is decreased.Figure 6
Effect of BS-12 concentrations on the viscosity of 1500 ppm HAPAM.


## 3.4. Laser Light Scattering Experiments

It has been reported [23, 38] that addition of ionic surfactants influences the molecular structure of the polymer. The effects of BS-12 concentrations on apparent weight average molecular weights (Mw,a) of polymers are tested at a 25°C. Their result is shown in Figure 7. The root mean square radius of gyration (〈Rg〉) is characteristic parameters of the polymer and directly reflects the conformation of polymer chains. In order to reduce the effect of polymer concentrations, the preparation concentration of polymers is 2 ppm in experiment. For the dilute polymer solution, 〈Rg〉 can be concluded through extrapolation of the same concentrations with different angles in solution; then some 〈Rg〉 are received under different surfactant concentrations in the same way. Their results are shown in Figure 8.Figure 7
Effect of BS-12 concentrations on apparent weight average molecular weight (Mw,a) of HAPAM.Figure 8
Effect of BS-12 concentrations on root mean square radius of gyration (〈Rg〉) of HAPAM.Figures7 and 8 show that Mw,a and 〈Rg〉 of HAPAM increase first and then decline with the increment of BS-12 concentrations. When there are a few surfactants in the polymer-surfactant mixed system, the surfactant molecules interacting with polymer hydrophobic groups, intermolecular association of polymers is strengthened and polymers are more likely to gather to form super molecular structures. Mw,a and 〈Rg〉 show a trend of increment. When surfactant concentrations are about 100 ppm, the system viscosity is the largest. With the further increment of surfactant concentrations, hydrophobic groups of polymer molecules are inhibited by cationic groups of surfactant molecular chains. The intramolecular association of associating polymers forms inner salt key. Mw,a and  〈Rg〉 become smaller. When surfactant concentrations are more than its critical micelle concentrations, the number of surfactant micelles is increased. Hydrophobic groups of associating polymers are separated by surfactant micelles. The intermolecular association is weakened and supramolecular aggregations are dismantled. Thus, Mw,a and 〈Rg〉 are further smaller.In order to study zwitterionic surfactant (BS-12) effect on hydrodynamic sizes of polymers in solution, the preparation concentration of polymers is 2 ppm in the experiment. Particle size distributions and hydrodynamic radius (〈Rh〉) of the polymer under different surfactant concentrations are measured by dynamic light scattering at a 25°C and the scattering angle is 90°. Their results are shown in Figures 9 and 10. Figure 9 shows that particle sizes of HAPAM are unimodal distribution under no surfactant condition. When surfactant concentrations are about 100 ppm, the particle size distribution of HAPAM is a wider unimodal and moves to the right. Surfactants can enhance intermolecular association of polymers and make polymer chains stretch and hydrodynamic radius increase. When surfactant concentrations are more than 400 ppm, particle sizes of HAPAM are multimodal distributions and wider unimodal move to left. The reason is that surfactant micelles are increased with the increment of surfactant concentrations in solution. Some polymer hydrophobic groups are embedded by surfactant micelles. The intermolecular association of HAPAM is partially blocked, and the hydrodynamic radius appears to be reducing.Figure 9
Particle size distributions of HAPAM with different BS-12 concentrations.Figure 10
Effect of BS-12 concentrations on the hydrodynamic radius(〈Rh〉) of HAPAM.Figure10 shows that 〈Rh〉 is increased because of a small amount of surfactants to be added. When surfactant concentrations are lower, the intermolecular association of HAPAM is strengthened, and 〈Rh〉 is increased. But the surfactant concentrations exceed a certain value; polymer aggregations are dismantled; therefore, 〈Rh〉 is reduced.


## 3.5. Molecular Aggregation Morphologies of Polymer-Surfactant Mixed System

The previous research results had been confirmed that space network structures of hydrophobically associating polymer are formed exceeding the critical association concentration (CAC) of polymer [3, 24]. When ionic surfactants are added, molecular aggregation morphologies of HAPAM are affected. Different BS-12 concentrations affecting molecular aggregation morphologies are observed. Their results are shown in Figure 11. Figure 11(a) is an AFM photo of HAPAM without surfactants. When the HAPAM concentration exceeds the CAC, it can be formed obvious spatial network structures in distilled water [39]. Figure 11(b) is an AFM photo of HAPAM solution to add 100 ppm surfactants. Compared with Figures 11(a) and 11(b), when BS-12 concentrations are about 100 ppm, the space network structures become more intense in solution, and the connecting mesh chain beams are thicker, especially the intersection part of chain beam. Figure 11(c) is an AFM photo of HAPAM solution to add 400 ppm surfactants. Compared with Figures 11(b) and 11(c), when BS-12 concentrations are about 400 ppm, the space network structures become sparser. When surfactants continue to be added, the connecting network chain beams are thinner. These results show that adding a few surfactants has a promoting effect on the self-assembly of polymer molecules, but the self-assembly of polymer molecules is inhibited for adding too many surfactants.AFM images of 1500 ppm HAPAM with different BS-12 concentrations: (a) 0 ppm BS-12, (b) 100 ppm BS-12, and (c) 400 ppm BS-12.
(a)
(b)
(c)


## 4. Conclusions

(1)
Adding polymers into dodecyl dimethyl betaine (BS-12) solutions, the CMC and surface tensions of the CMC are increased with the increment of HAPAM concentrations.
(2)
Zwitterionic surfactant (BS-12) can reduce dodecanoic-water interfacial tension to about 0.3 mN/m. BS-12 has been a good ability to reduce the oil-water interfacial tension. The surfactant (BS-12) interface activity is affected by HAPAM. The required time of interfacial tension balance is longer with polymer concentrations increasing.
(3)
When the surfactant (BS-12) concentrations are lower, the apparent viscosity, apparent weight average molecular weights (Mw,a), root mean square radius of gyration (〈Rg〉), and hydrodynamic radius (〈Rh〉) of HAPAM increase with the increment of BS-12 concentrations. When surfactant concentrations are 100 ppm, they are maximum; surfactant concentrations continue to increase and they begin to decline. BS-12 has a great influence on performances of HAPAM solutions.
(4)
The hydrophobically associating polymer (HAPAM) can form the obvious spatial network structures exceeding the critical association concentration (CAC) in distilled water. When added surfactant (BS-12) concentrations are about 100 ppm, the space network structures become more intense, and the connecting network chain beams are thicker. BS-12 concentrations continue to increase, when concentrations are about 400 ppm, loose network structures are formed, and partially loose network structures are broken.



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*Source: 932082-2014-02-23.xml*