Yifan Siab and
Zhiguang Guo*ab
aHubei Collaborative Innovation Centre for Advanced Organic Chemical Materials, Ministry of Education Key Laboratory for the Green Preparation and Application of Functional Materials, Hubei University, Wuhan 430062, People's Republic of China. E-mail: zguo@licp.cas.cn; Fax: +86-931-8277088; Tel: +86-931-4968105
bState Key Laboratory of Solid Lubrication, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China
First published on 11th March 2016
The papermaking industry always causes many disastrous problems to humans, such as energy consumption, environmental pollution and destruction to the ecosystem. However, paper is not only one kind of life's necessities but also a necessity of the office. But the service life of paper is reduced easily because of the invasion of water. Here we creatively prepared one kind of multifunctional inner and outer uniform-superhydrophobic paper by the secondary use of waste paper inspired by nature and traditional papermaking knowledge, which not only has a great water proof ability for various liquids, but also has wonderful self-cleaning, anti-fouling and oil absorption abilities. It is worth mentioning that superhydrophobic recycled paper still has good writability, suppleness, foldability and tailorability to meet our daily needs. Unique outer and inner uniform-superhydrophobicity make this paper able to tolerate any degree of abrasion. This groundbreaking work will not only avoid harm by the water invasion and expand the usable range of paper, but also it will ease the energy and environment crisis.
Cellulose is one important ingredient of both paper and recycled paper which is a hydrophilic and hydroscopic material by nature. It is well known that water has long been the leading destroyer of paper. Once wet, the strength of paper soon diminishes significantly because celluloses are bonded together through the phenomenon of hydrogen (H–O–H) bonding, but the presence of water molecules weakens the intermolecular forces. Even drying again after water evaporation, paper appears wrinkled with the deformation of small amounts of soluble components so that paper loses its aesthetic property and practicality.8,9 Thus, water-repellent paper has been one kind of much-anticipated functional product.
Recently, inspired by the micro- and nano-scale structure of the lotus in nature, a superhydrophobic surface which exhibit an extremely high water contact angle (WCA) (>150°) and low water sliding angle (SA) (<10°) has been a hot area of research in many areas.10–15 Numerous fabrication methods have been developed for chemical and physical preparations of superhydrophobic surfaces in the literature, each providing varying degrees of control of the nano–micro roughness and wettability to various substrates which, without question, provide feasible ideas for water-repellent paper.16–20 But it still will be a challenge to create water-repellent or superhydrophobic paper while keeping its intrinsic properties well. Actually, superhydrophobic paper has been reported by many groups before and these creative works have opened new doors to expand the range uses of traditional paper.21–24 However, it is also undeniable that these perpetration methods always have questions about the weak strength of the paper and the complex process, and cannot be prepared on a broad scale. Furthermore, these second modifications will also inflict damage to the aesthetic property and practicality. But above all, present research just concentrates on the surface treatment of paper. If only the surface of paper is modified, the superhydrophobicity of the modified paper is easily lost due to wear and tear from friction during repeated use. Considering the above situation, there is an urgent need to design one kind of novel, wear-proof and uniform both within and outside superhydrophobic paper.
In the traditional papermaking industry, fillers are the second most important component used to meet the needs of papermaking, such as decreasing the dependence on forestry resources and promoting drainage drying in the papermaking process with high benefits in terms of costs and energy saving. Importantly, fillers also can enhance and impact some essential properties of paper such as brightness, gloss, opacity, smoothness and printability. So, many types of fillers have been applied in the papermaking industry, including calcium silicate, precipitated calcium carbonate, calcium carbonate, titanium dioxide and so on.25–27 In the same way, the wettability of paper also can be regulated by superwetting the filler, as far as we know, which has never been reported before.
For their amazing adhesion ability to various kinds of surface or substance, mussels have been attracting much attention in the research community;28–31 this ability derives from L-3,4-dihydroxyphenylalanine (dopamine) with excellent biocompatibility and low cytotoxicity. Many studies found that the interfacial poly-dopamine (PDA) layers not only facilitate the dispersion of the filler, but also strengthen the stress transfer from the substrate to the filler, resulting in greatly improved mechanical properties.32,33 Inspired by a wise mentor of humans – nature – we creatively combined the lotus effect and the mussel adhesion effect into a recycled papermaking process and obtained one kind of multifunctional uniform both inside and outside the superhydrophobic recycled paper with wonderful self-cleaning, anti-fouling and oil absorption abilities while still keep the paper's intrinsic properties.
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| Fig. 1 Schematic illustration of the synthesis procedure of SRP from the waste paper via traditional papermaking processes. | ||
The cellulose fiber paper (CFP) and PDA/cellulose fiber paper (PCFP) were also prepared in a similar way as control experiments. All these three kinds of papers (CFP, PCFP and SRP) are uniform in composition with smooth surface. The PCFP and SRP have weaker whiteness than CFP due to the brown PDA layer and the optical images of CFP, PCFP and SRP are shown in Fig. S2, see ESI.† In fear of damage to the aesthetics and writable of the PDA layer, the original amount of dopamine was controlled within a small range (0.01 g) and the polymerization time is relatively short. The FESEM images of CFP, PCFP and SRP are shown in Fig. 2. According to low resolution images of CFP, the diameters of the original fibers vary from about ten to dozens of micrometers, which are of a criss-crossing, formed porous structure. PCFP is so compact due to the DPA layer's adhesion action, which can enhance the interaction forces of the fibers. The compactness of SRP is less than that of PCFP because SSGP, an inorganic filler, has a negative impact on the fiber-to-fiber bonding with the opposite effect to the PDA layer.36 Compared with the CFP, SRP is still more close-grained based upon the interaction of all of these factors. The high resolution FESEM images of CFP, PCFP and SRP can clearly display the surface topography of a single fiber. In Fig. 2d, the original fiber surface is smooth without a distinct wrinkle. The PDA/cellulose fiber surface shows a wavy integument with many grooves resulting from the PDA layer's cladding. The FTIR spectra of PCFP can also be proved from the band at 1400 cm−1 that can be assigned to C
C resonance vibrations and the bands at 867 cm−1 and 712 cm−1 that can be assigned to –H vibrations in the aromatic rings of PDA (Fig. S3, see ESI†). The surface topography of the SSGP/PDA/cellulose fiber is different from that of the previous two. There are lots of flaky objects attached to the surface. In the higher resolution image, the flaky object was composed of SSGP of around 30 nm in size (Fig. S4, ESI†). XPS spectra can also give proof of this preparation process. The XPS spectra of CFP mainly include two peaks at 532 eV and 284.8 eV which are, respectively, labeled as O 1s and C 1s. Compared to CFP, the XPS spectra of PCFP has one weak peak at 398.4 eV assigned to N 1s, which indicated the existence of PDA. And, apparently, the XPS spectra of SRP show Si 2s and Si 2p at 155.1 eV and 105.8 eV that be consistent with the XPS spectra of SSGP, thus proving the existence of SSGP (the XPS spectrum are shown in Fig. S5, ESI†).
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| Fig. 2 (a–c) Low resolution FESEM images of CFP, PCFP and SRP. (d–f) High resolution FESEM images of CFP, PCFP and SRP. | ||
![]() | (1) |
cos θw = r cos θ
| (2) |
Cassie & Baxter proposed the heterogeneous surfaces concept and they believed that the liquid drop will not penetrate into cavities on the rough surface in all cases and that air is trapped in these cavities to become air pockets. So, there is a new equation for this model:39
cos θCB = fSL(1 + cos θ) − 1
| (3) |
Based on the previous theoretical research, one can draw the conclusion that a smaller solid–liquid contact area and a lower solid surface energy are conducive to a higher water contact angle. Barthlott and Neinhuis40 held that a nano- and micro-scale hierarchical structure benefited an extreme repellence against liquid droplets, inspired by the lotus leaf, which shows fine-branched nanostructures on top of microsized papillae. Therefrom, researchers have committed to create such a special hierarchical roughness structure to achieve wonderful superhydrophobic surfaces.41 Besides, fluorine substances always have attracted much attention for a low surface energy in this research field. However, two nearly inevitable shortcomings are high toxicity and high price. In this work, we chose HMDS with the aid of rich hydrophobic –CH3 to avoid fluorine-substances successfully.42 So, this low toxicity SRP can satisfy the need of real life without worry. From the structural aspect, micron-scale PDA-cellulose and nano-scale SSGP can combine into a hierarchical structure of our SRP, see Fig. 2f. So, that is the reason why this SRP have excellent superhydrophobicity. In order to manifest its waterproof ability more intuitively, on dipping of the SRP into the water using tweezers, and then removing it out seconds later, there is no residual water and the SRP is as dry as before (see Movie S1, ESI†). More interestingly, when the SRP is immerged in water, a layer of silvery white mirror can be found. This is because there are abundant air pockets between water and the paper surface (Fig. 3c) which also proves that water on the paper surface exists in the Cassie & Baxter state. Therefore, the experiment results agree well with the theoretical analysis. Using an injection syringe to eject a water column into the SRP surface, the impacting water column bounces out without spread (Fig. 3d). In addition, the SRP has a strong acid and alkaline resistance as well. Let drops of HNO3 (1 M) and NaOH (1 M) fall onto the SRP surface. We can observe both drops keep a perfect spherical shape on the paper that can be sustained over time (Fig. 3e). All in all, the extreme goal for our artificial SRP is to serve the people's everyday life. So, some common liquids in our daily life are studied too. Coffee, milk, green tea, black tea, methylene blue and water drops are both placed on SRP surface and they all showed near-spherical shapes with high CA (Fig. 3f). This indicates that the SRP can meet people's basic needs and can handle various situations.
Different from traditional fillers in the papermaking industry, SSGP played a key role in regulating the wettability of recycled paper in this study but to improve the optical properties and smoothness. The impact of the weight ratio of SSGP (here we use the term W(SSGP) on the basis of the weight of waste paper fragments) was revealed by measured CA and SA values. When W(SSGP) = 0%, namely, PCFP was tested first and the CA was 0° for the superhydrophilicity of cellulose and PDA as mentioned before. Only on increasing W(SSGP) to 10% from 0%, could the CA also significantly increase to 139.3 ± 2.3°. However, the water drop (∼12 μL) cannot roll down at an inclination of ∼10°. Furthermore, when we continued to improve the W(SSGP) to 20%, the hydrophobicity of recycled paper also improved (CA achieved 143.7 ± 1.2°). This time, the water drop can roll down with an inclination of ∼10° but it cannot roll down with an inclination of ∼8 degrees. When W(SSGP) = 30%, the CA finally surpassed and reached 157.8 ± 0.7°. Strictly speaking, this time the recycled paper is still not superhydrophobic because the water drop cannot roll down with an inclination of ∼8 and ∼5°. In other words, the SA value is bigger than 5°. Only when W(SSGP) = 40%, did we eventually obtain SRP. The CA of SRP is 158.9 ± 1.1° and SA is lower than 5°. If the SRP is tilted only a little, the water drop can roll down easily and rapidly. As the W(SSGP) continues to improve, the CAs are 160.9 ± 0.8° and 158.3 ± 1.7°, respectively when W(SSGP) are 50% and 60%. Similarly, the SAs of these two situations are both lower than 5°. In general, W(SSGP) = 40% is the boundary between high-hydrophobicity and superhydrophobicity (the images of CAs and SAs from 10% to 60% are shown in Fig. S7†). It is interesting to note that in our control experiment, when the SSGP was added into original the cellulose fiber pulp without PDA and then made into paper under the same conditions and methods, the CA was only 151 ± 3° and the water drop (∼12 μL) could not roll down with an inclination of ∼8°, even when the W(SSGP) = 40% (see Fig. S8†). This result reveals that PDA has an important influence on the final results. So, TGA was used to characterize the thermal degradation of three kinds of papers (CFP, SSGP/CFP and SRP) and the weight loss curves in N2 are shown in Fig. S9.† The degradation of all of them occurs at around 300 °C, which was the result of the depolymerization of cellulose into volatile products (levoglucosan). But the residue weight percentages were significantly different at the end of degradation (800 °C). The weight percentage of residue of CFP was about 10%, which means a stable char residue of cellulose.43,44 As a control experiment, the weight percentages of residue of SSGP/CFP (W(SSGP) = 40%) increased to 25%. Obviously, difficult-to-decompose inorganic filler (SSGP) still existed. In contrast, the weight percentage of a residue of SRP was as high as 35% with 40 percent in the PDA situation. The adhesion effect of PDA can reduce the loss of SSGP and increase the SSGP content in SRP, which led to a better superhydrophobicity of SRP as well.
It is impossible to write with a water-based ink pen on this SRP due to the great water-proof ability. The surface energy of water is about 72 mN m−1, but oil is much low (20–30 mN m−1).45 Then, the superhydrophobic surface is superoleophilic in general and this SRP is no exception. On this understanding, an oil-based ink pen is undoubtedly a potential alternative and it is truly useful. According to Fig. 4a, using a blue oil-based ink marker pen, we write the word “writable” and draw a tree on the paper surface. Obviously, the smooth handwriting has not caused damage to the paper. It is worthwhile to indicate that water drops can still stand nearby-spherical even on the written place. This SRP has a very good suppleness as well and can be folded in half by tweezers, shown in Fig. 4b. Furthermore, the SRP can be cut into rectangle and then folded into a simple paper boat which can, different from the ordinary one, float on the water surface for quite a long time without wetting. Combining the above characteristics, we designed an artificial lotus colored by a green dye which also can float on water just like live one in nature (Fig. 4c and d). This work must open up new prospects for the application of paper crafts. The durability and instability of SRP are worth caring for as well. By clipping the middle area, the SRP can hang weights (50 g) easily without breakage and deformation (shown in Fig. 4e). High-temperature experiments were also conducted. In order to explain more objectively and intuitively, taking commercial tissues as a comparison, we can see that after heating at 100 °C for one half hour, there was no significant change of our SRP. However, commercial tissue folded slightly because of the loss of contained trace amounts of water, shown in Fig. 4f. These above two points illustrate that this SRP must be sufficient to meet the basic daily needs. In this lab-based fundamental research, the beating, deinking, bleaching and refining treatments of the traditional papermaking industry have been omitted for the mature development of these aspects and they are not our research focus. Likewise, we have avoided the use of industrial adhesives in this process. So, the mechanical property of SRP has certainly been a possible concern here. PCFP (SRP without PDA) shows very weak mechanical properties. No matter whether it is folded or stretched, both make it broken and we can't write on it. Considering accessibility and affordability factors, dopamine was chosen to solve this issue here. A PDA layer that covers the fiber surface enhances the interaction force between fiber–fiber and fiber-filler. This organic–inorganic composite construction not only helps maintain good superhydrophobicity, as mentioned before, but also contributes greatly to mechanical properties. Obviously, the mechanical property of SRP is associated with the initial content of dopamine increase. But the initial content of dopamine has to be controlled within a small value. The reason is that brown PDA has a negative impact on the brightness and appearance of SRP (see Fig. S2†). After comprehensive consideration, a small amount of dopamine is the best choice.
A water droplet can roll off instead of sliding on the superhydrophobic surface for the high CA and low SA. For a favorable decease of the surface energy, the powders adhered on the surface are easy attached to liquid so that the dirt on the superhydrophobic surface can always be taken away by the water droplet. This is the reason why the lotus leaves keep a clean appearance in an unclean natural environment, called the “self-cleaning” ability. It is important inherent this feature of a superhydrophobic surface and it has been researched a lot. The significance of the “self-cleaning” ability of the SRP is self-evident. So, a self-cleaning experiment has been conducted as well. A bit of black graphite powder was spread on the SRP evenly with an inclination of about 30 degrees. These powders did not slip off at beginning. Using an injection syringe, water droplets were dripped continuously and slowly from 1 cm above the paper. The water drop could roll down and take the touched powders away. After few drops of water, on the area where the water passed by almost no graphite powder remained (Fig. 5a–c). Generally speaking, the SRP can always keep it clean even in an outside environment for a long time with rain scouring but this situation also inevitably leads to new questions. The rainfall has a certain amount of dust and pollutants in it and can this SRP withstand this? Namely, whether this SRP has anti-fouling ability, which was investigated using muddy water. Similarly, the muddy water was poured out using a beaker and it flowed down in strands from the paper surface. The paper still keeps clean consistently without any residue or pollution. Furthermore, with the addition of muddy water in a petri dish, the SRP can float on the liquid surface but wetted as shown in Fig. 5d–f. So, this SRP, no doubt, will bring dramatic changes into the paper packaging industry with good dust and water proof ability.
Fantastically, different from previous research, the SRP has unique outer and inner uniform superhydrophobicity. Taking advantage of traditional papermaking industry knowledge here, the SSGP exists in each part of the SRP no matter the surface (outside or inside). So, even if the surface part is worn away by friction, the water-proof ability still exists. A sand paper abrasion test under a 50 g of load to the SRP was adopted as well. The SRP sample (1 cm × 1 cm) was adhered to a slide with double sided adhesive tape and then the sample was propelled for 8 cm on the sandpaper (800 Cw). One cycle experiment process of the sandpaper abrasion is shown in Fig. S10, see ESI.† After 5 cycles, the SRP clearly shows an edge with high roughness. But this did not impact the wettability of paper and water droplet can still “stand” on it. The CA value can reach ∼150° but fluctuates wildly (±4.3°) because of the uneven surface (Fig. 7a). The situation is also available over 10 cycles. But for 15 cycles, the instability of CA will drop because the sample is very thin now and it will turn flat. But what is astonishing is the CA can be up to 154.4 ± 1.2° after 20 cycles with almost no sample remaining on the double side adhesive tape, which can be seen with the naked eye clearly (Fig. 7a, the insets). This illustrates that the SRP can keep a great water proof ability even under an excessive wear situation. In order to clarify this property more intuitively, the SRP was torn apart from the middle to expose the internal part to air, as shown in Fig. 7b. Both the surface and the inner part can make a water droplet stand in a near-spherical shape, which also proves the unique outer and inner uniform superhydrophobicity of the SRP.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra04259g |
| This journal is © The Royal Society of Chemistry 2016 |