Synthesis and characterization of poly-aluminum silicate sulphate (PASS) for ultra-low density fiberboard (ULDF)

Tingjie Chena, Min Niua, Xiaodong Wangb, Wei Weia, Jinghong Liu*a and Yongqun Xie*a
aCollege of Material Engineering, Fujian Agriculture and Forestry University, 350002, Fuzhou, Fujian, China. E-mail: fjxieyq@hotmail.com; 314515363@qq.com; Fax: +86 591 83789135; Tel: +86 591 83789307
bDivision of Wood Technology and Engineering, Luleå University of Technology, 93187, Forskargatan 1, Skellefteå, Sweden

Received 16th July 2015 , Accepted 13th October 2015

First published on 15th October 2015


Abstract

Poly-aluminum silicate sulphate (PASS) was synthesized in a mixed aqueous solution of sodium silicate and aluminum silicate via a sol–gel method for use in ultra-low density fiberboard (ULDF). The preparation conditions were optimized by using response surface methodology. The effects and interactions of the Si/Al molar ratio (X1), pH value (X2) and temperature (X3) on the internal bond strength of ULDF were investigated. Research showed that the optimum internal bond strength (10.23 ± 0.64 kPa) was obtained under a Si/Al molar ratio of 2[thin space (1/6-em)]:[thin space (1/6-em)]1, pH value of 8, and a temperature of 50 °C. Analyses of the Fourier transform infra-red spectroscopy spectra confirmed that Al–O–Si bonds were formed between polysilicate and Al or its hydrolysate. The particle size analysis showed that the average size of PASS was 7.52 μm. Some of the PASS entered the cell wall and made a contribution to the improvement of the mechanical properties of ULDF.


1. Introduction

Ultra-low density fiberboards (ULDFs) are manufactured using a liquid frothing method.1 These materials have many excellent properties including low thermal conductivities, and good sound absorption, etc.1–5 They are a promising alternative to petroleum based products because they are made from plant fibers and could be used for building insulation materials and packaging buffer materials. However, their applications are restricted due to their poor mechanical properties which correspond to their ultra-low density (ranging from 10 to 90 kg m−3) and porosity.4,5 Recently, interest has increased in modifying the mechanical properties of wood-based materials through a variety of methods such as using inorganic compounds.5–10

Silicon materials such as water glass and aluminum compounds can improve the heat resistance of wood-based materials. When aluminum salts are heated, they absorb a lot of heat from the dehydration reaction.11 In addition, silicon materials can also ameliorate the mechanical properties of wood composites.7,8,12 Poly-aluminum silicate sulphate (PASS) is one of the inorganic polymer coagulants which can be prepared through polymerization of poly-silicic acid and hydroxylated aluminium salts.13 The polysilicic acid can neutralize the positive charge in polyaluminum and also combine with Al and its hydrolysis products through Al–O–Si bonds to form hydroxyl-aluminosilicate due to its negatively charged polymer.14,15 PASS has many distinct abilities including charge neutralization, adsorption bridging and sweep coagulation. When it is stirred with fibers, it covers the surface of the fibers or even interacts with plant fibers which improves the properties of the fibers or fiber composites.16,17

It’s worth noting that the properties of inorganic polymer coagulants are affected by many factors such as aging temperature, silicon dose, pH value, and Si/Al ratio. For example, the coagulation efficiency of an aluminum–silicate polymer composite (PASiC) increases with rising basicity, however, the PASiC products tend to become cloudy or partly gelatinous in this case.18 Li et al. showed that the coagulation performance of a poly-silicic-cation coagulant was affected by the pH value. The Si/Al ratio also played a crucial role in the properties of inorganic polymer coagulants. Different positive charges and molecular weights of PASiC coagulants were obtained when they were prepared in different Si/Al ratios. For example, an increase in the Si/Al ratio would increase the amount of polymeric coordination.18–21

Although the coagulation performances of various inorganic polymer coagulants in water and waste water treatment have been already studied by many researchers, there is still no research on the effects of PASS with different characteristics on the mechanical properties of ULDF. To systemically study the influence of PASS on the mechanical properties of ULDF, PASS materials with different Si/Al molar ratios, pH values, and temperatures were prepared and added into the preparation of ULDF. Additionally, to obtain the optimal preparation conditions of PASS, a standard response surface methodology (RSM) called central composite design (CCD) was used. The chemical structures and particle sizes of the PASS materials were examined and analyzed.

2. Experimental

2.1 Materials

Kraft pulp (KP, spruce-pine-fir; Tembec Inc., Canada) was utilized as a raw material to manufacture ULDF. Aluminum sulfate and sodium silicate, purchased from Tianjin Fuchen Chemical Reagents Factory (China), were used to generate the poly-aluminum silicate sulphate (PASS). Sodium dodecylbenzene sulfonate, a foaming agent, was purchased from Jiangsu Qingting Washing Products Co., Ltd. (China). Sulfuric acid was purchased from Tianjin Fuchen Chemical Reagents Factory (China) to acidize the sodium silicate.

2.2 Methods

2.2.1 Preparation of poly-aluminum silicate sulphate. A PASS solution was formed through a mutual reaction between sodium silicate and aluminum sulfate in a sol–gel process. The aluminum sulfate solution was added to a 500 mL tri-necked round-bottom flask with a magnetic stir bar, experiencing a vigorous stirring for 10 min at a set temperature. The sodium silicate solution was acidized using a dilute sulfuric acid to obtain the desired pH value. Then the quantitative polysilicic acid solution was added into the flask slowly to obtain the PASS. A schematic representation of the manufacture of PASS is shown in Fig. 1.
image file: c5ra13996a-f1.tif
Fig. 1 Schematic representation of the manufacture of PASS.
2.2.2 Preparation of ultra-low density fibreboard. Ultra-low density fiberboards of 200 mm × 200 mm × 50 mm (L × W × H) were manufactured separately using various parameters in a demonstration line as described by Chen et al.,22 with a target bulk density of 50–90 kg m−3. The preparation process of the fiberboards is described in Fig. 2. The amount of dry pulp fiber was 55 g. The 500 mL PASS solution, which was approximately 22.7% of the dry pulp fiber, was added into this paper. Additionally, the additives polyacrylamide resin, alkyl ketene dimer water repellent (AKD), chlorinated paraffin fire retardant, and sodium dodecylbenzene sulfonate surfactant (10% concentration, foaming agent) were added during different manufacturing stages for all of the specimens, at 20 mL, 50 mL, 46 g and 80 mL, respectively.
image file: c5ra13996a-f2.tif
Fig. 2 The preparation process of ULDFs.

2.3 Experimental design

The Si/Al molar ratio (X1), pH value (X2, the pH value of sodium silicate solutions) and temperature (X3, the aging temperature of PASS) were chosen as the variables. The internal bond strength (Y) was regarded as their function. A standard RSM design CCD was applied to study the effects of X1, X2 and X3 on Y. The software Design-Expert (Trial Version 8.0.6) was used to analyze the data and build the models. The selection range of each variable which was determined by the previous single factor experiment is shown in Table 1. The CCD consisted of 20 experiments including eight factorial experiments, six star points and another six replicated at the central point of the designed model to estimate the pure error sum of squares. The detailed parameter variables of PASS are given in Table 1.
Table 1 Levels of parameter variables used in the RSM design for ULDFs
  Levels
Coded-variables (Xi) −1.682 −1 0 1 1.682
Si/Al molar ratio (X1) 0.32[thin space (1/6-em)]:[thin space (1/6-em)]1 1[thin space (1/6-em)]:[thin space (1/6-em)]1 2[thin space (1/6-em)]:[thin space (1/6-em)]1 3[thin space (1/6-em)]:[thin space (1/6-em)]1 3.68[thin space (1/6-em)]:[thin space (1/6-em)]1
pH values (X2) 4.64 6.0 8.0 10.0 11.36
Temperature (X3, °C) 16.36 30 50 70 83.64


2.4 Internal bond strength of ultra-low density fibreboard

The internal bond strength (IB) of each ULDF was tested in accordance with GB/T 17657.23 The size of the specimens for the testing of the internal bond strength was 50 mm × 50 mm × 40 mm (L × W × H). All of the results were the average of five replications for each ULDF group.

2.5 Functional groups and particle sizes of PASS

The functional groups in the PASS were characterized using Fourier transform infrared (FTIR) spectroscopy. The FTIR analysis of PASS was performed by means of a Nicolet 380 FTIR spectrometer (Thermo Electron Instruments, USA), employing the KBr pellet method, and taking 32 scans for each sample with a resolution of 4 cm−1, ranging from 4000 to 400 cm−1. The particle sizes of the PASS were determined using a laser particle size analyzer (BT-9300H, Bettersize Instruments Ltd., China). Each sample, with a concentration of 0.5%, was tested over nearly 3 minutes with measurements ranging from 0.1 to 340.0 μm.

3. Results and discussion

3.1 Model fitting

The design matrix and the results of the RSM experiments for determining the effects of the three independent variables are shown in Table 2. The mathematical model representing the IB of ULDF against the function of the independent variables within the range under investigation is expressed as follows:
 
Y = 10.23 + 0.63X1 + 0.41X2 + 0.33X3 − 0.055X1X2 + 0.078X1X3 − 0.077X2X3 − 2.31X12 − 1.48X22 − 0.81X32 (1)
where Y is the IB of the ULDF, whereas X1, X2 and X3 are the coded variables for the Si–Al molar ratio, pH value, and temperature, respectively.
Table 2 Central composite design and the response to the internal bond strength
Run no. Coded levels Internal bond strength (kPa)
Si–Al molar ratio (X1) pH value (X2) Temperature (X3, °C) Experimental Predicted
1 −1(1[thin space (1/6-em)]:[thin space (1/6-em)]1) −1(6.0) −1(30) 3.61 4.20
2 1(3[thin space (1/6-em)]:[thin space (1/6-em)]1) −1 −1 5.15 5.43
3 −1 1(10.0) −1 4.83 5.28
4 1 1 −1 5.94 6.29
5 −1 −1 1(70) 4.48 4.87
6 1 −1 1 6.12 6.41
7 −1 1 1 5.18 5.64
8 1 1 1 6.81 6.96
9 −1.68(0.32[thin space (1/6-em)]:[thin space (1/6-em)]1) 0(8.0) 0(50) 3.40 2.63
10 1.68(3.68[thin space (1/6-em)]:[thin space (1/6-em)]1) 0 0 5.03 4.76
11 0(2[thin space (1/6-em)]:[thin space (1/6-em)]1) −1.68(4.64) 0 5.94 5.38
12 0 1.68(11.36) 0 7.22 6.74
13 0 0 −1.68(16.36) 8.01 7.38
14 0 0 1.68(83.64) 8.91 8.50
15 0 0 0 10.10 10.23
16 0 0 0 10.31 10.23
17 0 0 0 9.97 10.23
18 0 0 0 10.77 10.23
19 0 0 0 10.48 10.23
20 0 0 0 9.59 10.23


In general, the exploration and optimization of a fitted response surface may produce poor or misleading results unless the model exhibits a good fit.24–27 As shown in Table 3, the model’s fit was good because its p-value was less than 0.0001 and the lack of fit value was 0.0956. The determination coefficient (R2) of this model was 0.9667, which implied that 96.67% of the variations could be explained by the fitted model. The value of R2 was in reasonable agreement with Radj2 which indicated a high degree of correlation between the observed and predicted value.28 So, the values of R2 (0.9667) and Radj2 (0.9368) in this model proved that the regression model could explain the true behavior of the system well.

Table 3 Analysis of variance for the regression model for the internal bond strengtha
Source Sum of squares Degrees of freedom Mean square F-Value p-Value
a p < 0.01 highly significant; 0.01 < p < 0.05 significant; p > 0.05 insignificant.
Model 112.28 9 12.48 32.29 <0.0001
X1 5.49 1 5.49 14.22 0.0037
X2 2.26 1 2.26 5.84 0.0362
X3 1.53 1 1.53 3.96 0.0745
X1X2 0.024 1 0.024 0.063 0.8075
X1X3 0.048 1 0.048 0.12 0.7317
X2X3 0.048 1 0.048 0.12 0.7317
X12 77.04 1 77.04 199.38 <0.0001
X22 31.39 1 31.39 81.25 <0.0001
X32 9.49 1 9.49 24.55 0.0006
Residual 3.86 10 0.39    
Lack of fit 3.01 5 0.60 3.54 0.0956
Pure error 0.85 5 0.17    
Correlation total 116.15 19      


The corresponding variables would be more significant with greater F-values and smaller p-values.29 As can be seen in Table 3, the F-value (32.29) and p-value (less than 0.0001) implied that this model was significant and only a 0.01% chance that it could occur due to noise. On the contrary, the F-value (3.54) and p-value (0.0956) of the lack of fit implied that it was not significant and a 9.56% chance that it could occur due to noise. The p-values in this model indicated that X1, X2, and the three quadratic terms (X12, X22, and X32) affected the IB of the ULDFs significantly, whereas X3, X1X2, X2X3, and X1X3 were all insignificant to the response. The results also showed that the independent variable X1 was the most significant factor on the experimental effect of the IB of ULDF.

3.2 Analysis of response surface and optimization

The effects of the variables on the IB of ULDF are shown in Fig. 3. Here, the relationship between the parameters and response variable are illustrated in a 3D representation of the response surface and the corresponding contour plot.
image file: c5ra13996a-f3.tif
Fig. 3 Response surface plots for the maximum IB of ULDFs. (a) Effects of the Si/Al molar ratio and pH value on the IB of ULDFs; (b) effects of the Si/Al molar ratio and temperature on the IB of ULDFs; (c) effects of the pH value and temperature on the IB of ULDFs.

The results showed that the variables X1 and X2 played an important role in the IB of ULDFs, whereas X3 did not. At a Si/Al molar ratio of 1.8[thin space (1/6-em)]:[thin space (1/6-em)]1–2.2[thin space (1/6-em)]:[thin space (1/6-em)]1 and a pH value of 7.8–8.1, a maximal IB (10.23 kPa) could be determined (Fig. 3a). But, at a given Si/Al molar ratio, the IB of ULDFs decreased with too low or too high pH values. This was because the morphostructure of the fibers and the foaming system of the ULDF might be affected by the low or high pH value. Additionally, the particle size of PASS was small at low pH values which might limit them leaving in ULDFs, whereas the particle size was large at high pH values which would not be helpful to the distribution of Si/Al compounds on the fiber surfaces. On the other hand, the decrease in IB at higher Si/Al molar ratios was possibly due to the distribution of additives and their charge neutralization which was the major and effective mechanism for the absorption of PASS on the fiber surface.22,30 The IB of ULDFs increased with temperature, especially within the range from 45 to 60 °C, but declined slightly at higher temperatures (Fig. 3b). This was because the particle sizes of PASS were larger at higher temperatures which are always prone to agglomerate on the fiber surface. Fig. 3c shows the combined effect of pH value and temperature on the IB of ULDFs at a constant Si/Al molar ratio (2[thin space (1/6-em)]:[thin space (1/6-em)]1). The result was elliptical, indicating significant interactive effects of the two independent variables on the IB of ULDFs.31

As seen in Fig. 3, the interaction between the Si–Al molar ratio (X1) and the other two variables (X2, X3) was significant. This was because more and more hydroxyl ions were added as the pH value increased which made the formation of sediment between aluminium and silicate ions easier. The hydrolyses of aluminium and silicate were significantly affected by the temperature of the solution. Meanwhile, there was almost no interaction between the pH value (X2) and temperature (X3). The pH value of the solution might be affected by the temperature but not significantly.

Based on eqn (1) which was derived from the computational program, the optimal PASS conditions for ULDFs were a Si/Al molar ratio of 2.14[thin space (1/6-em)]:[thin space (1/6-em)]1, pH value of 8.26, and a temperature of 54.13 °C. Taking the practical operating conditions into consideration, some conditions were modified as follows: a Si/Al molar ratio of 2[thin space (1/6-em)]:[thin space (1/6-em)]1, pH value of 8, and a temperature of 50 °C. Under these conditions, an average of 10.23 ± 0.64 kPa was obtained, which is close to the model predicted value of 10.34 kPa. Compared to the control specimen (2.5 kPa), the IB of ULDF under the optimal conditions was increased by 313.6%. These results confirmed that the model adequately reflected the expected optimization and eqn (1) was satisfactory and accurate.

3.3 Functional groups in PASS

Schematics of the synthesis of a Si sol and PASS are illustrated in Fig. 5. First, the Si sol was obtained under H2SO4 catalysis conditions. PASS was developed after the Si sol was added slowly to an Al2(SO4)3 solution under ultrasound-assisted conditions. The FT-IR spectrum provided much information about the structure of the material, clearly revealing the combined mode of the Si and Al compounds.32 In order to explore the functional groups in the PASS, the infrared spectra of polysilicic acid, aluminum sulfate, and PASS are shown in Fig. 4.
image file: c5ra13996a-f4.tif
Fig. 4 FTIR profiles of polysilicic acid, aluminum sulfate and PASS.

The peaks at around 3400 and 1666 cm−1 were attributed to the –OH stretching vibrations and –OH bending vibrations, respectively. The peaks for aluminum sulfate at 1104, 931, and 606 cm−1 were attributed to the SO42−, Al–O–Al, and Al–OH vibrations, respectively. The peaks for polysilicic acid at around 1380, 1114, 798, 619 and 441 cm−1 were ascribed to the contribution of the silicon–oxygen tetrahedral, Si–O–Si or SO42−, Si–O–Si, SO42−, and O–Si–O vibrations, respectively. Comparing the infrared spectra of PASS to polysilicic acid and aluminum sulfate, the peak at 1100 cm−1 might be attributed to the Si–O–Si, SO42−, or Si–O–Al vibration. This is due to the broad band in the range of 1200–1000 cm−1 which usually corresponds to the mixed overlap of Si–O–Si and Al–O–Si bonds.33 In addition, the peak for PASS at 931 cm−1 was weakened. This is due to the polysilicic acid which could combine with Al and its hydrolysis product through Al–O–Si bonds to form hydroxyl-aluminosilicate, which led to the decrease in Al–O–Al bonds. Combining the results of Tang et al. and this study, the structure of the Si sol and PASS could be deduced as shown in Fig. 5.32


image file: c5ra13996a-f5.tif
Fig. 5 Schematic synthesis of Si sol and PASS.

3.4 Particle size of PASS

The particle size of PASS under the optimal preparation conditions is shown in Fig. 6.
image file: c5ra13996a-f6.tif
Fig. 6 Particle size of PASS under the optimal preparation conditions.

As can be seen, the distribution of PASS' particle size in Fig. 6, they was mainly distributed from 2 μm to 15 μm. The average and largest particle sizes were 7.52 μm and 18.98 μm, respectively. Combined with the cumulative curve, it could be found that there was 26.02% of PASS whose particle size was less than or equal to 5.25 μm. Due to the porosity of the fibers which have many pits ranging from 0.1 μm to 5.0 μm on their cell wall, some of the PASS with a smaller particle size could enter and leave the cell wall or cell cavity.22 Therefore, the PASS could not only deposit on the fiber surface through charge neutralization or adsorption bridging, but enter the cell cavity through the fiber pits and then become a sediment to enhance the mechanical properties of ULDF.4

On the contrary, the efficiency of coagulants in waste water treatment might be influenced by increasing the Si/Al ratio and pH value. The results were different from the PASS for ULDFs. The study by Yang et al. showed that for a given Si/Al ratio, an increase in pH value increased the DOC removal efficiency.21 This was because that higher pH value produced larger molecular sized products which would enhance aggregating efficiency. Additionally, for a given pH value, the DOC removal efficiency increased then decreased when the Si/Al ratio increased. This was because of the interaction between hydrolyzed Al species and polysilicic acid which would decrease the positive charge and increased the molecular weight of the coagulant.11

In this study, for a given Si/Al ratio and temperature, an increase in pH value would increase the particle size of PASS. Different particle sizes of PASS were obtained at different pH values so the IB increased and later decreased in Table 4. The smaller particle size of PASS which was obtained under the conditions of lower pH values could enter into fibers; they might easy to run off when they were added in the preparation of ULDF.30 On the other hand, an increase in pH value would promote agglomeration and probably increased the molecular weight in PASS. The mechanical properties of ULDF would be affected by the large particle size of PASS which could influence the distribution of PASS on the fiber surface.

Table 4 Particle size of PASS and the internal bond strength of ultra-low density fiberboards and similar coagulants for waste water treatment in the literature
PASS Si–Al molar ratio Temperature (°C) pH value Particle size (μm) IB (kPa) DOC removal efficiency
This study 2 30–40 4 0.40 6.24
6 0.90 7.41
8 5.13 9.95
12 12.59 8.73
Yang et al.21 0.05 Ambient temperature 4 9.1%
6 27.1%
8 20.8%
0.02 Ambient temperature 4 7.7%
0.05 9.1%
0.10 3.4%


Taking these factors into consideration, the suitable particle size of PASS which played an important role in the mechanical properties of ULDF should be prepared. Combined with the results of FTIR and particle size, the optimal preparation conditions of PASS were valid for preparing ULDFs.

4. Conclusions

The mechanical properties of ULDFs could be effectively improved with PASS. The optimal conditions of PASS were predicted using response surface methodology, and a good internal bond strength of 10.23 ± 0.64 kPa was obtained. Taking the practical operating conditions into consideration, the optimal preparation conditions of PASS were: a Si/Al molar ratio of 2[thin space (1/6-em)]:[thin space (1/6-em)]1, pH value of 8, and a temperature of 50 °C. FTIR analysis confirmed that the added polysilicate reacted with Al and its hydrolysate. The particle size analysis indicated that the PASS could not only deposit on the fiber surface, but enters the cell cavity through the fiber pits to enhance the mechanical properties of ULDF.

Acknowledgements

This paper was supported by the Scientific Research Foundation of Graduate School of Fujian Agriculture and Forestry University (1122YB020) and the Studying Abroad Scholarships of China. The authors are also grateful for the financial support of the National Science and Technology Support Program (2008BADA9B01), the National Natural Science Foundation of China (NSFC) (30781982) and the Natural Science Foundation of Fujian Province (2015J01604).

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