Preparation and Characterization of Binary and Ternary Blends with Poly ( Lactic Acid ) , Polystyrene , and Acrylonitrile-Butadiene-Styrene

Binary and ternary blends of poly(lactic acid) (PLA), polystyrene (PS) and acrylonitrile-butadiene-styrene (ABS) were prepared using a one-step extrusion process. Rheological and mechanical properties of the prepared blends were determined. Rheological properties were studied using a capillary rheometer, shear rate, shear stress, non-Newtonian index, shear viscosity and flow activation energy were determined. Mechanical properties were studied in term of tensile properties, stress at break, strain at break, and Young’s modulus was determined. The effect of the composition on the rheological and mechanical properties was investigated. The results show that the ternary blend exhibits shear-thinning behavior over the range of the studied shear rates where the true shear viscosity of the blend decreases with increasing true shear rate, also it was found that the true viscosity of the blend decreases with increasing ABS content. The mechanical results showed that, in the most cases, the stress at break and the Young’s modulus improved by the addition of ABS.

Preparation and characterization of PLA/PS polymer blends were reported in many works [12][13][14][15][16], it was found in these works that the thermal stability of the blend is better than that of pure PLA.Also it was found that the blend has good processability.Nevertheless, drawbacks were noted in this blend (PLA/PS), such as lower mechanical properties (tensile strength and modu-lus) comparing with those of pure PLA.From another side ABS was used for improving the impact strength of PLA, Li and Shimizu [21] used ABS for toughening PLA.Blends of PLA and ABS in different ratios were prepared and as the in-situ compatibilizer for PLA/ABS blends to improve the compatibility between PLA and ABS, the reactive styrene-acrylonitrile-glycidyl methacrylate copolymer (SAN-GMA) by incorporating with ethyltriphenyl phosphonium bromide (ETPB) as the catalyst was used.The mechanical results showed that impact strength of the compatibilized blend is higher than that of uncompatibilized and pure PLA, but the modulus of the compatibilized blend was less than that of pure PLA.In this work ternary blends of PLA, PS, ABS were prepared in efforts to obtain new materials with improved mechanical properties, such works are very important in the development of composites and blends from biodegradable polyesters.

Blends Preparation
Binary and ternary blends of PLA, PS, and ABS in different ratios were prepared using a laboratory scale single screw extruder (SSE) (D = 20 mm, L/D = 25) [SHAM EXTRUDER 25D Performance: Kreem Industrial Establishment, Damascus, Syria].The screw has a fluted type mixing section located before the metering zone [48], in this type of mixers the material is forced to pass at a high shear stress.This brings in some level of dispersing action besides reorienting the interfacial area, and increasing the imposed total strain.The screw speed was set at 40 rpm in the blends preparation, and the extruder temperature profile along the barrel was 130˚C, 140˚C, 150˚C, 160˚C (from feed zone to die).The blends were extruded through a multi holes die (3 mm), the extrudates were then fed into a granulator, which converted them into granules.The obtained granules were dried at 70˚C for 6 h before studying.The compositions of the blends are shown in Table 1.

Tensile Samples Preparation
The prepared granules were injection molded at 190˚C -210˚C using NEGRI BOSSI (NB 25) injection machine (Lessona Corporation, Italy).The tensile samples were prepared according to the following injection conditions, cooling time in the mold was 15 sec, the mold temperature was room temperature with water-cooling (25˚C) and injection pressure was 9 MPa.The molded samples were dog bone-shaped samples with a thickness and width of 4 mm and 10 mm respectively.The gauge length of the sample was 80 mm (Figure 1).The obtained products were immediately packed in plastics bags and stored in a dark cool surrounding.

Rheological Properties
Rheological experiments were carried out using a capillary rheometer (Davenport 3/80), the rheological experiments were carried out at 165, 175, 185 and 195˚C, and by using L/R = 8, 15, 25 and 36 capillaries.Bagley's correction [49] was performed by using the data from the four capillary dies.The apparent shear rate (γ a ) is given by: where R is the capillary radius, and Q is the volumetric flow rate.The true shear rate (γ r ) is given by: where n is the non-Newtonian index depending on temperature, the term 3 1 4 was the Rabinowitsch correction factor.The apparent shear stress (τ a ) is given by: where ΔP is the pressure at the capillary entrance, and L is the capillary length.The true shear stress (τ r ) is given by: where e is the Bagley's correction factor.The true viscosity (η r ) is given by: The values of flow activation energy at a constant shear rate (E γ ) were determined using Arrhenius equation form: where A is the consistency related to structure and formulation and R is the gas constant (8.314J/(mol·K)).

Mechanical Properties
Tensile testing to study stress at break (N/mm 2 ), strain at break (%) and Young's modulus (N/mm 2 ) were performed using Testometric M350-10KN (The Testometric Company Ltd., Rochdale, UK) at room temperature, all samples were strained at 50 mm/min.Samples were conditioned at room temperature for a period of 48 h prior to testing.Results from 6 -8 specimens were averaged.

Flow Curves
Polymer rheology in the molten state is very important for determining the processing conditions of the materials.Figure 2 shows the relationship between apparent shear rate and apparent shear stress (flow curves) for the ternary blend at 165˚C.
It is clearly seen from Figure 2 that the relationship between shear stress and shear rate obeys the power law in the range of the studied shear rates.
where K is the consistency index and n is the non-Newtonian index, which can be calculated from the slope of the lines in Figure 2. The same relationship was obtained for both polymers and binary polymer blends.Figure 3 shows the effect of ABS content on the n of the blend at 165˚C.It could be noted from Figure 3 that the values of n were less than 1, implying that PLA/PS/ABS blend melts were pseudo plastic; similar to most polymer and binary polymer blends in the molten state.No attention has been given in the past to flow behavior of the ternary polymer blends.Also it could be noted from Figure 3 that the values of n for the ternary blend (PLA/PS/ABS) is less than that of the binary blend (PLA/PS (50/50)).
The value of n describes the deviation from the Newtonian fluids about flow behavior, so it is also called the flow behavior index.A higher value of n reveals less influence of shear rate on flow behavior.In other words, the changes in viscosity upon shear rate are not obvious, so it could be said that the flow behavior of ternary blend melts is more sensitive to shear rate as compared with the binary blend (PLA/PS (50/50)).

Viscosity Curves
Figure 4 shows the relationship between true shear viscosity and true shear rate (viscosity curves) for the blends at 165˚C.It could be noted from Figure 4 that the true shear viscosity of the blends decreases with increasing true shear rate in the studied range of the shear rates, showing a typical property of shear-thinning, this behavior was attributed to the alignment or arrangement of chain segments of polymers in the direction of applied shear stress.The high shear viscosity at a low shear rate provide the integrity of the extrudate during extrusion, and the low shear viscosity at a high shear rate enables low injection pressure, high injection speed and less time of the injection cycle.
Figure 5 shows the plots of true viscosity versus blending ratio at 165˚C and at shear rate = 10 s -1 .It could be seen from Figure 5 that the true shear viscosity of the binary blend (PLA/PS) decreases with increasing PLA content in the blend and this behavior can be attributed to the low melt viscosity of PLA comparing with that of pure PS.Also it could be noted from Figure 5 that the viscosity of the binary blends is less than that of the ternary blends, where the addition of 5 phr of ABS to PLA/PS (50/50) enhanced the true shear viscosity by a factor of 2.22 and by a factor 2.62 at 10 phr ABS.

Flow Activation Energy
Figure 6 shows the relationship between true shear viscosity and 1/T of the ternary blends at shear rate = 10 s -1 , it could be noted from Fig. 6 that the true shear viscosity decreases with increasing temperature.With a rise of temperature the motion ability of polymer chains enhances, and the resistance between the melt layers decreases relevantly, leading to reduction of the melt viscosity.
The plots of true shear viscosity versus 1/T shown in Figure 6 give a group of straight lines, which indicates that the relationship between the true viscosity and temperature follows Arrhenius equation (Equation ( 6)).Flow activation energy at a constant shear rate (E γ ) could be calculated from the slopes of these lines.  Figure 7 shows the effect of ABS content on the flow activation energy at a constant shear rate (γ = 10 s -1 ).
It could be noted from Figure 7 that the flow activation energy of the binary blend (PLA/PS (50/50)) is less than that that of the ternary blends, so it could be said that adding ABS caused in increasing flow activation energy.It is well known that the value of flow activation energy reflects the temperature-sensitivity of viscosity, so the more E γ was the more sensitive the behavior of blends were to the temperature so it could be said that ternary blends are more sensitive to the temperature than the binary blend (PLA/PS (50/50)).

Mechanical Properties
Mechanical properties of the blends were determined in term of tensile properties, stress at break, strain at break, and Young's modulus were determined.Figure 8 shows the stress at break of the blends.
It could be noted from Figure 8 that the addition of ABS improves the stress at break of binary blend (PLA/ PS (50/50)), where adding 5 phr ABS to PLA/PS (50/50) enhanced the stress at break by a factor of 2.29, also adding 20 phr ABS to PLA/PS (30/70) and PLA/PS (50/ 50) enhanced the stress at break by factors 0.53 and 1.4 respectively.
Figure 9 shows the strain at break of the blends, it could be noted from Figure 9 that the strain at break of the ternary blends is more than that of the binary blend (PLA/PS (50/50)).Also it could be noted that the strain at break of PLA/PS (30/70) increases by a factor of 1.41 by the addition of 20 phr.
Figure 10 shows the Young's modulus of the blends, it could be noted from Figure 10 that the Young's modulus of the ternary blends is more than that of the binary blends.It could be noted from Figures 8 and 10 that the ternary blend (PS50/ABS5) has good mechanical properties  (stress at break and Young's modulus) which is similar to those of pure PLA (stress at break = 56 N/mm 2 and Young's modulus = 2220 N/mm 2 ).

Conclusion
In this work, rheological and mechanical properties of binary and ternary blends with poly(lactic acid), polystyrene, and acrylonitrile-butadiene-styrene were studied.The blends were prepared using a single screw extruder.Rheological results showed that the ternary blend (PLA/ PS/ABS) is pseudo plastic in nature; its viscosity decreases with increasing shear rate similar to most polymer and polymer blend melts.Also it was found that the true shear viscosity of the binary blend (PLA/PS) decreases with increasing PLA content which was attributed to PLA low viscosity, and the true shear viscosity of the ternary blend is more than that of the binary blend.The mechanical results showed that the stress at break and Young's modulus of the ternary blend are better than those of the binary blend.PS50/ABS5 blend showed good mechanical properties near to the mechanical properties of pure PLA.

Figure 4 .
Figure 4. True shear viscosity versus true shear rate of the blends at 165˚C.

Figure 7 .
Figure 7.The effect of ABS content on the flow activation energy at a constant shear rate (γ = 10 s -1 ).

Figure 8 .
Figure 8. Stress at break of the blends.

Figure 9 .
Figure 9. Strain at break of the blends.

Figure 10 .
Figure 10.Young's modulus of the blends.