The Experimental Blending of Polymers
Significance of impact and tensile test on the blend of wPP, PS and NR
The mechanical properties (impact and tensile strength) in the blend of experimental runs are presented in Table 3. Where, both impact and tensile strength of the blend showed significant improvement as compared to the control samples sp17, sp18 and sp19. As demonstrated in Table 3, it is a well-known fact that not all mechanical properties of a certain blend combination will yield high values in those attributes. But it turns out that sp5 (PP/PS/NR; 22.5/47.5/30) and sp11 (PP/PS/NR; 30/40/30) are different, with high impact and tensile strength values of 198.16 J/m, 158.71 J/m, 158.71 J/m, and 118.04 MPa, 114.97 MPa, and 26.93 MPa, respectively.
Sample
|
Independent Variable
|
Responses
|
Table 3
Effects of wPP, PS and NR concentrations on the impact and tensile strength
Runs
|
Sample code
|
PP
|
PS
|
NR
|
Impact strength (J/m)
|
Std. Error
|
Tensile strength (MPa)
|
Std. Error
|
1
|
sp1
|
35
|
60
|
5
|
108.78
|
± 11.56
|
105.44
|
± 2.67
|
2
|
sp2
|
15
|
60
|
25
|
126.00
|
± 11.00
|
78.11
|
± 7.02
|
3
|
sp3
|
25
|
60
|
15
|
96.89
|
± 3.86
|
50.22
|
± 3.11
|
4
|
sp4
|
35
|
40
|
25
|
98.67
|
± 2.00
|
11.63
|
± 3.69
|
5
|
sp5
|
22.5
|
47.5
|
30
|
251.67
|
± 15.57
|
118.04
|
± 7.07
|
6
|
sp6
|
26
|
51
|
23
|
80.11
|
± 5.06
|
109.41
|
± 4.52
|
7
|
sp7
|
30.5
|
45.5
|
24
|
106.11
|
± 13.11
|
102.30
|
± 4.03
|
8
|
sp8
|
35
|
50
|
15
|
92.11
|
± 2.61
|
51.07
|
± 7.18
|
9
|
sp9
|
20.5
|
55.5
|
24
|
91.33
|
± 10.60
|
35.52
|
± 2.32
|
10
|
sp10
|
35
|
50
|
15
|
93.24
|
± 4.44
|
27.30
|
± 0.71
|
11
|
sp11
|
30
|
40
|
30
|
201.56
|
± 12.40
|
26.93
|
± 1.18
|
12
|
sp12
|
25
|
60
|
15
|
96.78
|
± 1.93
|
49.95
|
± 2.80
|
13
|
sp13
|
22.5
|
47.5
|
30
|
227.56
|
± 7.18
|
114.97
|
± 4.12
|
14
|
sp14
|
15
|
60
|
25
|
119.11
|
± 1.22
|
12.11
|
± 0.45
|
15
|
sp15
|
35
|
60
|
5
|
116.78
|
± 9.89
|
96.44
|
± 6.44
|
16
|
sp16
|
30.5
|
55.5
|
14
|
66.22
|
± 2.98
|
11.63
|
± 0.30
|
Control Samples
|
17
|
sp17
|
100
|
0
|
0
|
72.89
|
± 4.78
|
20.19
|
± 2.49
|
18
|
sp18
|
0
|
100
|
0
|
121.33
|
± 9.33
|
93.89
|
± 2.51
|
19
|
sp19
|
0
|
0
|
100
|
72.22
|
± 4.84
|
38.71
|
± 1.76
|
Studying the mechanical properties' analysis of variance (ANOVA)
The significance of the models is to predict the experimental value, which is subject to validation. However, the models cannot be said to be reliable without checking for consistency and adequacy. Equations 4 and 5 present the models generated from the ANOVA of tensile and impact strengths of the polymer blend, where cubic and special quartic mixture models were used for the blend of wPP, PS and NR respectively. Through the use of probability values, ANOVA can help assess the importance of each linear, quadratic, cubic, quartic, and interaction factor in the models (P-value). P values less than 0.05 were used to establish the significance of the models produced in Tables 4 and 5 for all terms. The impact and tensile strengths had a considerable impact on all independent and interaction variables.
TS =
|
37.82A – 282.59B + 100.91C + 955.10AB – 92.65AC + 603.77BC – 1171.31ABC – 974.77AB (A – B) + 73.20AC (A – C) + 1251.93BC (B – C)
|
(4)
|
IS =
|
149.53A + 123.17B + 113.16C + 422.45AB – 126.44AC – 108.84BC – 3505.41A2BC – 1147.41 AB2C – 1861.57ABC2
|
(5)
|
Where; A = wPP, B = PS, C = NR
Given the Model F-value of 97.60, the model is most likely significant. Only 0.01 percent of cases might have an F-value this high due to noise. Model terms are regarded as significant when "Prob > F" is less than 0.05. A, B, C, AB, AC, BC, A2BC, and ABC2 are significant model terms in this situation. In cases where the value exceeds 0.1, model terms are not significant. The "Lack of Fit F-value" of 0.57 indicates that, in comparison to the pure error, the lack of fit is not substantial. The probability that noise is to blame for a "Lack of Fit F-value" this high is 60 percent. A negligible lack of fit is advantageous since we want the model to fit. Predictability R-Squared (Pred R-Squared) of 0.9614 and Adjustment R-Squared (Adj R-Squared) of 0.9810 are reasonably in agreement; the difference is less than 0.2. Accurate measurements are made of the signal-to-noise ratio. Preferable ratios range from 4 and up. Due to the ratio of 31.278 showing a sufficient signal, the model can be used to investigate the design space.
Given the Model F-value of 98.26, the model is most likely significant. Only 0.01 percent of cases might have an F-value this high due to noise. Model terms are regarded as significant when "Prob > F" is less than 0.05. The model terms B, C, AB, BC, ABC, AB(A - B), and BC(B - C) are significant in this case. If the value is more than 0.10, the model terms are not important. If your model has a lot of extraneous terms, model reduction may improve it (except those needed to maintain hierarchy). According to the "Lack of Fit F-value" of 2.43, there is no distinction between the lack of fit and a simple error. A "Lack of Fit F-value" this large could be caused by noise with a 17.94% probability. The model should fit; hence a non-significant lack of fit is excellent. It is not defined (N/A) what the projected R2 statistic is. Because a case with a leverage of 1.00 was achieved, that is why. While the adjusted R2 (0.9832) is close to unity (1.0000) and so validates the model, the R2 (0.9933) is not. The signal-to-noise ratio is calculated by "Adeq Precision". More than 4 is preferred as a ratio. The signal is strong enough when the ratio is 27.047. It is presented in Table 6 and can be utilized to move about the design space.
Blend optimization
The optimization process for the blend of wPP, PS, and NR was predicted by the software and three runs were proposed. The run with the highest desirability was chosen [25]. As indicated in Table 7, the anticipated ideal combination variables in this work were 21 percent, 49 percent, and 30 percent, with a desirability value close to unity.
Table 5: Analysis of variance (ANOVA) test of the developed cubic model for Tensile Strength on the blend of PP, PS and NR.
Source
|
|
df
|
|
|
|
R2
|
Adj R2
|
Error (%)
|
Pred R2
|
Adeq pre.
|
Model
|
21724.93
|
9
|
2413.88
|
98.26
|
< 0.0001
|
0.9933
|
0.9832
|
1.02
|
1.00
|
27.047
|
Linear Mixture
|
60.49
|
2
|
30.24
|
1.23
|
0.3564
|
|
|
|
|
|
AB
|
3602.25
|
1
|
3602.25
|
146.63
|
< 0.0001
|
|
|
|
|
|
AC
|
29.84
|
1
|
29.84
|
1.21
|
0.3127
|
|
|
|
|
|
BC
|
4363.99
|
1
|
4363.99
|
177.64
|
< 0.0001
|
|
|
|
|
|
ABC
|
756.76
|
1
|
756.76
|
30.80
|
0.0014
|
|
|
|
|
|
AB(A-B)
|
3544.89
|
1
|
3544.89
|
144.30
|
< 0.0001
|
|
|
|
|
|
AC(A-C)
|
8.02
|
1
|
8.02
|
0.33
|
0.5885
|
|
|
|
|
|
BC(B-C)
|
8411.56
|
1
|
8411.56
|
342.39
|
< 0.0001
|
|
|
|
|
|
Residual
|
147.40
|
6
|
24.57
|
|
|
|
|
|
|
|
Lack of Fit
|
48.27
|
1
|
48.27
|
2.43
|
0.1794
|
|
|
|
|
|
Pure Error
|
99.13
|
5
|
19.83
|
|
|
|
|
|
|
|
Cor Total
|
21872.33
|
15
|
|
|
|
|
|
|
|
|
Table 7
Optimum condition for a maximum impact and tensile strength
Parameter
|
Goal
|
Experimental region
|
Optimized conditions
|
Validated result
|
Error (%)
|
|
Lower Limit
|
Upper Limit
|
|
Fraction of wPP
|
In range
|
15
|
35
|
21
|
|
|
Fraction of PP
|
In range
|
40
|
60
|
49
|
|
|
Fraction of NR
|
In range
|
5
|
30
|
30
|
|
|
Tensile Strength (MPa)
|
Maximize
|
11.63
|
118.04
|
118.04
|
120.14
|
1.75
|
Impact Strength (J/m)
|
Maximize
|
66.23
|
251.67
|
241.62
|
248.9
|
2.93
|
Desirability
|
0.973
|
Diagnostics Plots and the three-Dimensional Graph for Impact and Tensile Strengths
According to the data distributions along the regression line in Fig. 1, which exhibit no outliers and demonstrate a high level of significance and a model that fits well thanks to positive interactions, the experimental study's data are in good agreement with those of the anticipated variables.
The impact strength model graph is also shown in Fig. 2. The 3D graph's elliptical shape demonstrates the model's importance. Additionally, as shown in the graph as proof, the shape of the related contour plots typically shows the significance of the reciprocal interactions between the independent variables and their responses.
Furthermore, in terms of tensile strength, comparable interaction trends were seen in the parity and 3D graphs, respectively. The usefulness of the model was further demonstrated by the good interactions seen in the plots, which demonstrated that the data were evenly distributed along the regression line and the contour form of the 3D surface plots as shown in Figs. 3 and 4, respectively.
Thermogravimetric analysis (TGA)
Thermogravimetric analysis (TGA) and derivative thermogravimetric analysis were used to examine the thermal analysis and thermal stability of polymer blends (DTG) as shown in Figs. 7 and 8.
Tables 8 and 9 present the summarized results for thermogravimetry and derivative thermogravimetry analysis for the blend of wPP/PS/NR
Table 8
Summary of TGA on weight loss on the polymer of wPP, PS, and NR
|
Initial Point
|
Mid-Point
|
Final Point (Max)
|
Residue
|
Sample
|
wt loss (m1)
|
Temp (T1)
|
wt loss (m2)
|
Temp (T2)
|
wt loss (m3)
|
Temp (T3)
|
(m4)
|
sp4
|
0
|
352
|
50
|
402
|
90.8
|
448
|
9.2
|
sp5
|
0
|
360
|
50
|
406
|
94
|
444
|
6
|
sp8
|
0
|
369
|
50
|
405
|
98
|
440
|
2
|
sp11
|
0
|
360
|
50
|
407
|
93.2
|
447
|
6.8
|
sp17
|
0
|
332
|
50
|
381
|
97.7
|
424
|
2.3
|
sp18
|
0
|
360
|
50
|
387
|
95
|
420
|
5
|
sp19
|
0
|
341
|
50
|
382
|
92
|
532
|
8
|
Table 9
Summary of the effect of DTG on temperature for the blend of wPP, PS, and NR
DTG
|
Sample
|
Td Onset
|
Td Peak
|
Td Offset
|
sp4
|
344
|
439
|
481
|
sp5
|
353
|
434
|
451
|
sp8
|
355
|
433
|
449
|
sp11
|
349
|
426
|
451
|
sp17
|
337
|
391
|
436
|
sp18
|
320
|
402
|
438
|
sp19
|
329
|
379
|
445
|
In some circumstances, this study can reveal details regarding the mechanisms of degradation that cause molecular weight reduction. Figures 7 and 8 show the weight loss versus temperature for the blends (wPP, PS, and NR), as well as the derivative of the weight over temperature (differential thermogravimetry) versus temperature for control samples (wPP, PS, and NR).
Intake of oxygen results in the creation of hydroperoxides and peroxy radicals, which are unstable at higher temperatures and soon change into other labile products before being evolved. Figure 8 shows this initial mass rise. For samples that have experienced degradation, the mass gain is larger because shorter chains react with oxygen more quickly. Since volatile chemicals evolved after the reaction with oxygen, the reprocessed samples begin to lose mass more quickly [24, 25]. However, all samples of the polymer mixes will remain stable up to about 350 oC. However, it was discovered that more than half of the polymer blend was lost when the material was heated to a temperature between 380 and 400 oC. Additionally, the bulk of the compounds decomposed at temperatures higher than 400 oC.
However, the polymer blends will be stable up to around 350 oC for all samples. But, when the material was subjected to a temperature between 380–400 oC, it was observed that over about 50% of the polymer blend was lost. Also, when the decomposition temperature was above 400 oC, the majority of the samples were decomposed leaving residue, as presented in Table 9. From the DTG curves, the loss was attributed to side group scission, which was for sp17, sp18 and sp19 having a single peak (Figure )(single stage degradation). While, sp4, sp5 sp8 and sp11 with double peaks degradation, indicate mass loss as a result of scissions and depolymerization [26, 27].
Furthermore, a detailed summary of the TGA (Table 8) gives an idea about the effect of temperatures corresponding to different mass losses at; the initial point (T100), mid-point (T50), and maximum degradation (Tmax). While, Table 9 gives the summary of the DTG curve via the onset of degradation (onset Td), peak degradation temperature (peak Td), and offset temperature at maximum degradation (offset Td).
Dynamic Mechanical Analysis (DMA)
Dynamic mechanical analysis (DMA) is a standard technique for defining a material's properties as a function of temperature, time, frequency, stress, atmosphere, or a combination of these elements [28, 29].
Storage modulus El
To investigate miscibility in polymer mixtures, DMA is frequently utilized. Temperature information is supplemented by data from DMA regarding the behaviour of mixes and phase morphology. Figure 9 shows how the temperature affects the mix of wPP, PS, and NR's storage modulus (El).
Theoretically, all samples should experience a general drop in storage modulus as the temperature rises. Chain mobility theory can be used to explain this [30]. As a result, a temperature rise will raise the enthalpy of the composite chain, which will release a lot of internal energy that can be used to weaken or dissolve the physical bonds and entanglements linked to the polymer chains. Again, if the molecular chains move more forcefully during heating, less energy will be stored, resulting in a decrease in storage modulus.
From Fig. 9, it can be observed that storage modulus (El) values for the control samples were higher than the blended samples, which was a result of the addition of NR in the blend making it more flexible as compared to the pure PS and PP. But generally, the storage modulus decreased with increasing temperature in all samples, with a notable drop in the regions between 80 and 100 oC, after which the storage moduli are relatively the same.
Loss modulus (Ell)
When comparing several systems at the same strain amplitude, the Ell is a measurement of the energy lost as heat per cycle of sinusoidal deformation. It is also known as the material's viscous reaction (viscoelasticity). The variation in loss modulus (Ell) with a temperature of the blend is illustrated in Fig. 10 and summarized in Table 10. There was no improvement in the Ell. The unbroken polymer chains and potential for stress transfer below the Tg value were represented in the more or less consistent values of Ell. Energy dissipation occurred when the temperature reached the Tg, and a corresponding peak was seen in the values Ell.
Damping (Tan ɗ)
Damping, which is measured as the tangent of the phase angle, is the energy dissipation in a material under cyclic load. A material's capability to absorb energy is determined by its Tan ɗ value; the higher Tan ɗ is, the better the capacity. The ratio of Ell to El is provided. It also varies according to the frequency, temperature, and state of the material. The glass transition temperature Tg of the substance is taken to be the highest temperature value of Tan ɗ. Figure 11 and Table 10 provide convincing evidence that the blended component has better damping effect and higher Tg then the control samples. They tend to absorbed more energy when subjected to engineering application. These result from the addition of three polymer, which typically causes a shift in the Tg toward higher temperatures and a peak in the loss factor (damping) due to the restriction of the movements of the matrix (polymer) chain molecules, raises the storage modulus and dampens the effect [31–33].
According to Joseph et al. (2010) [28], the inclusion of macro/microfibers reduces the damping properties of polymer fibre composites and increases storage modulus because the additional fibres obstruct the macromolecular chains' free motion. The empty matrix, in comparison, has the largest damping ratio, indicating a high level of mobility. Additionally, Sreekala et al. (2005) [29] used a DMA technique to report on the dynamic mechanical characteristics of composites made of oil palm fibre and phenol-formaldehyde. The addition of oil palm fibre was found to increase the dynamic modulus and decrease the damping properties of the composite.
Table 10
Summary of DMA values for polymer blend.
Samples
|
Onset El of Tg (oC)
|
El (MPa)
|
Peak T of Ell (oC)
|
Ell (MPa)
|
Peak T of Tan ɗ
|
Tan ɗ
|
sp5
|
79.4
|
199.74
|
27.1
|
29
|
109
|
0.171
|
sp6
|
68
|
65.34
|
33.4
|
31
|
88
|
0.18
|
sp17
|
52.5
|
696.59
|
39.9
|
63
|
81.1
|
0.089
|
sp18
|
93.7
|
590.02
|
90.4
|
60
|
104.3
|
0.061
|
Scanning Electron Micrograph Image of the Polymer Blend
The surface micrograph of the blend and optimized blend are presented in Fig. 12. SEM examines the surface appearance of bulk specimens and gathers signals using detectors positioned above the sample. It is the most common method for characterizing polymer surfaces.
The morphologies of the blend (sp5) and optimized (spopt) blend of terpolymer of wPP/PS/NR, are shown in Fig. 12. spopt shows a fine surface morphology with little cracks which account for high mechanical properties observed from the thermal and mechanical properties analysis. While, sp5 shows the coarsest morphological structure, which was a result of improper mixing of the polymers, leading to low mechanical properties.