92 lines
34 KiB
JSON
92 lines
34 KiB
JSON
[
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{
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"id": 1,
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"chunk": "# Terpolymer-based SIPN coating with excellent antifogging and frost-resisting properties† \n\nJie Zhao,a Anthony Meyer,a Li Ma,b Xiaojun Wangb and Weihua Ming\\*a \n\nDOI: 10.1039/c5ra21399a \n\nwww.rsc.org/advances",
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"category": " Abstract"
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},
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{
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"id": 2,
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"chunk": "# Introduction \n\nFogging and/or frosting can severely reduce visibility and transparency of a substrate because of the prism effect of small water droplets. Many coatings have recently been developed1–20 to mitigate fogging problems for various applications such as eyeglasses, cameras, mirrors, goggles, and display devices in analytical instrument. An extensively used strategy has been to apply a superhydrophilic coating, primarily due to its ability to signicantly reduce light scattering by only allowing water to condensate like a thin lm.8–19 However, it generally requires complicated procedures to fabricate textured surfaces8–16 or UV illumination17–19 for $\\mathrm{TiO}_{2}$ based coatings to obtain superhydrophilicity. Moreover, these superhydrophilic surfaces may fail to resist frost formation since ice would still form from the thin water layer when conditions are right. \n\nIt has been recently demonstrated that antifogging behavior does not have to reply on superhydrophilicity and can be obtained by cleverly combining hydrophilic and hydrophobic segments in a coating.1,21–24 For instance, Youngblood et al. developed self-cleaning and antifogging coatings by \n\nWe prepared an effective antifogging/frost-resisting coating by forming a semi-interpenetrating polymer network (SIPN) on the basis of a linear, random terpolymer poly(2-(dimethylamino)ethyl methacrylateco-N-vinylpyrrolidone-co-methyl methacrylate), poly(DMAEMA-co-NVP-co-MMA), and a network of poly(ethylene glycol dimethacrylate). The excellent antifogging/frost-resisting property was mainly attributed to a balanced hydrophilicity/hydrophobicity of the terpolymer with the optimal DMAEMA/NVP/ MMA molar ratio at 40/30/30. Compared to our previous work using poly(DMAEMA-co-MMA), the terpolymer-based coating demonstrated excellent antifogging property against both low- and hightemperature moist air, by eliminating the lower critical solution temperature related to the DMAEMA segments in the binary copolymer. By monitoring the coating thickness change during the fogging/ frosting test, it appeared that water molecules could rapidly be absorbed into and desorbed from the terpolymer-based coating, implying long-term effectiveness of the antifogging/frost-resisting coating. \n\ncombining both peruoroalkyl groups and poly(ethylene glycol) (PEG) segments.21 Cohen and Rubner et al. designed and prepared zwitter-wettable coatings showing excellent antifogging/frost-resisting properties via layer-by-layer assembly involving PEG segments22 or a chitosan/cellulose complex.23 Compared to a superhydrophilic antifogging surface, the coatings with balanced hydrophilicity/ hydrophobicity can imbibe rapidly water molecules from the surrounding vapor, thus preventing the formation of water droplets on the coating surface. \n\nRecently, we developed an effective antifogging/frostresisting coating on the basis of a semi-interpenetrating polymer network (SIPN) comprising a linear, binary acrylic copolymer poly(2-(dimethylamino)ethyl methacrylate-co-methyl methacrylate), poly(DMAEMA-co-MMA), and a cross-linked network due to ethylene glycol dimethacrylate (EGDMA).1 The SIPN coating showed excellent antifogging/frost-resisting properties against cold moist air; however, its antifogging performance became poor when exposed to hot moist air due to the lower critical solution temperature (LCST) associated with the DMAEMA segments.1 We envisage that partial replacement of the DMAEMA segments by another hydrophilic monomer may help eliminate the LCST effect in the binary copolymer poly(DMAEMA-co-MMA). Here we report the design and synthesis of a series of terpolymers, poly(2-(dimethylamino) ethyl methacrylate-co-N-vinylpyrrolidone-co-methyl methacrylate), poly(DMAEMA-co-NVP-co-MMA), and the subsequent preparation of antifogging/frost-resisting coatings on the basis of a SIPN from poly(DMAEMA-co-NVP-co-MMA) and PEGDMA against both cold and hot moist air.",
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"category": " Introduction"
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},
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{
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"id": 3,
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"chunk": "# Experimental section",
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"category": " Materials and methods"
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},
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{
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"id": 4,
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"chunk": "# Materials \n\nMonomers including DMAEMA $(98\\%)$ , $N$ -vinylpyrrolidone (NVP, $99\\%$ ), and EGDMA $(99\\%)$ were purchased from Aldrich, and MMA $(99\\%)$ was obtained from Alfa Aesar. Free radical initiators, 2-hydroxy-4-(2-hydroxyethoxy)-2-methylpropiophenone (HHMP, $98\\%$ ) and azobisisobutyronitrile (AIBN, $99\\%$ ), were obtained from Aldrich. Solvents such as dimethylformamide (DMF), toluene, and chloroform were purchased from Fisher. All chemicals were used as received.",
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"category": " Materials and methods"
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},
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"id": 5,
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"chunk": "# Synthesis of poly(DMAEMA-co-NVP-co-MMA) terpolymer \n\nAll terpolymers were synthesized by free radical polymerization. A typical procedure is described as follows. Three monomers, DMAEMA (4.8 g), NVP (4.5 g) and MMA $\\left(3.0{\\ g}\\right)$ (molar percentage: $30\\%$ DMAEMA, $40\\%$ NVP, and $30\\%$ MMA) were added into DMF in a $100~\\mathrm{{mL}}$ ask to obtain $10~\\mathrm{wt\\%}$ solution; then, the thermal initiator AIBN $[0.5\\mathrm{wt\\%}$ with respect to the total monomer mass) was added. Aer being purged by argon for $20\\ \\mathrm{min}$ , the polymerization was carried out at $70~^{\\circ}\\mathbf{C}$ for $^{24\\mathrm{~h~}}$ under magnetic stirring $\\left(200\\mathrm{\\rpm}\\right)$ . The nal terpolymer, designated as $\\mathrm{T}{-}30$ according to the DMAEMA molar percentage, was puried by dissolution in chloroform and precipitation in cyclohexane (twice), and dried in a vacuum oven. Similarly, other terpolymers were synthesized with the MMA amount xed at $30~\\mathrm{mol\\%}$ : T-40, $40\\%$ DMAEMA and $30\\%$ NVP; T-50: $50\\%$ DMAEMA and $20\\%$ NVP.",
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"category": " Materials and methods"
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},
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"id": 6,
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"chunk": "# Preparation of SIPN coatings \n\nGlass slides $(1.5\\ \\times\\ 1.5\\ \\mathrm{cm}^{2})$ ) were sonicated consecutively in acetone and ethanol for $30\\mathrm{min}$ , followed by blow-drying with air. A terpolymer $(2.0\\mathrm{~g})$ , EGDMA $(0.5~\\mathrm{\\wt\\%}$ with respect to the terpolymer), and HHMP $2.0~\\mathrm{wt\\%}$ relative to EGDMA) were dissolved in toluene $\\mathrm{(20.0~mL)}$ to obtain a homogeneous solution. The mixture was then spun-coated on clean glass slides at various rates (400, 800, 1500 and $3000\\mathrm{rpm}$ ) for $15{\\mathrm{~s}}.$ The spun-coated lm was then cured under UV irradiation in a UVP CL-1000 ultraviolet cross-linker apparatus ( $365~\\mathrm{nm}$ , 15 W) for $45~\\mathrm{min}$ , and dried in a vacuum oven at $70~^{\\circ}\\mathrm{C}$ for $24\\mathrm{~h~}$ . The smooth SIPN coatings (on glass) based on terpolymers T-30, T-40, and $\\mathrm{T}{\\cdot}50$ were labelled as SIPN-T-30, SIPN-T-40, and SIPN-T-50, respectively. The root-meansquare (RMS) surface roughness of SIPN coatings was typically 2–3 nm over an area of $2\\times2~\\upmu\\mathrm{m}^{2}$ , as determined by atom force microscopy (AFM) on an NT-MDT NTEGRA Prima instrument in the semi-contact mode with a gold-coated cantilever NSG 10.",
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"category": " Materials and methods"
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},
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"id": 7,
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"chunk": "# Fogging/frosting test \n\nAntifogging tests against hot moist air were conducted by holding the samples $5\\ \\mathrm{cm}$ above a hot water bath $(80~^{\\circ}\\mathbf{C})$ for different periods of time (15, 30, 45 and 60 s) with a glass as the control. A more aggressive fogging/frosting test was performed by placing these samples in a freezer at $-20{}^{\\circ}\\mathbf{C}$ for $30\\mathrm{min}$ and photographs were taken aer the samples were exposed to ambient conditions $({\\sim}20\\ ^{\\circ}{\\bf C}$ , $50\\%$ relative humidity) for 5 s. To evaluate the antifogging/frost-resisting performance more quantitatively, light transmission over the $400{\\mathrm{-}}700\\ \\mathrm{nm}$ range was collected on an Agilent 8453 UV-Vis spectrophotometer during fogging/frosting tests. To examine antifogging mechanism, time-dependent water contact angles on all SIPN coatings were collected on a Ram´e-Hart 290 instrument (every 10 s over 600 s period).",
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"category": " Materials and methods"
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},
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"id": 8,
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"chunk": "# Monitoring lm thickness change during fogging/frosting tests \n\nLight transmission data collected from UV-Vis measurements were also used to monitor the coating thickness change for the coatings that remained to be transparent during fogging/ frosting tests. Refraction index and coating thickness were simultaneously determined by tting the interference fringes in the transmission prole, $T(\\lambda)$ , as a function of wavelength, $\\lambda,^{25}$ \n\n$$\nT(\\lambda)=\\frac{T_{\\mathrm{sa}}(\\lambda)T_{\\mathrm{afs}}(\\lambda)}{1-R_{\\mathrm{sfa}}(\\lambda)R_{\\mathrm{sa}}(\\lambda)},\n$$ \n\nwhere $T_{\\mathrm{sa}}(\\lambda)$ and $T_{\\mathrm{afs}}(\\lambda)$ are the interference upon transmissions through the substrate-air and air-lm-substrate systems, respectively, and $R_{\\mathrm{sfa}}(\\lambda)$ and $R_{\\mathrm{sa}}(\\lambda)$ are the interference upon reections from the substrate-lm-air and substrate-air systems, respectively. Both $T_{\\mathrm{afs}}$ and $R_{\\mathrm{sfa}}$ are dependent on the refractive index and thickness of the test lm.25 Transmission spectrum of the glass slide was also needed and measured before lm coating, which was tted to a two-coefficient Cauchy equation.26 Normal incidence on the test lm was adopted for measurement conguration. By curve tting the raw data, the coating thickness was determined according to eqn (1). This method provides a noninvasive and instantaneous measurement of thickness and refractive index of a transparent lm. The coating thickness was veried by AFM on an NT-MDT NTEGRA Prima instrument in the semi-contact mode.",
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"category": " Materials and methods"
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},
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"id": 9,
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"chunk": "# Other measurements \n\nGlass transition temperature $\\left(T_{\\mathrm{g}}\\right)$ was measured on a TA Instruments DSC Q100 instrument, over the range of $-50$ to 120 ${}^{\\circ}\\mathbf{C}$ at a heating rate of $10^{\\circ}{\\bf C}\\operatorname*{min}^{-1}$ . NMR spectra were collected on an Agilent $400~\\mathrm{{MHz}}$ instrument with $\\mathbf{CDCl}_{3}$ as the solvent. Number-average molecular weight $\\left(M_{\\mathrm{n}}\\right)$ and polydispersity index, PDI $\\left(M_{\\mathrm{w}}/M_{\\mathrm{n}}\\right)$ of the terpolymers were determined by gel permeation chromatography (GPC) equipped with a Waters 515 HPLC pump and Water Styragel HT3/HT4 columns, using DAWN EOS 18-Angle Laser Light Scattering Instrument (Wyatt Technology) and OPTILAB DSP Interferometric Refractometer (Wyatt Technology) as detectors, with DMF as the elute (ow rate: $1\\mathrm{mL}\\mathrm{min}^{-1}$ , at room temperature); the molecular weights were calibrated with polystyrene standards.",
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"category": " Materials and methods"
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},
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"id": 10,
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"chunk": "# Results and discussion",
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"category": " Results and discussion"
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},
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"id": 11,
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"chunk": "# Preparation and properties of terpolymer poly(DMAEMA-coNVP-co-MMA) \n\nAs mentioned earlier, we already developed SIPN coatings on the basis of a binary copolymer, poly(DMAEMA-co-MMA) with the optimal DMAEMA/MMA molar ratio at 70/30 and PEGDMA (0.5 $\\mathrm{wt\\%}$ relative to the copolymer), which demonstrated excellent antifogging/frost-resisting properties against cold moist air.1 However, due to the LCST associated with the DMAEMA segments, the antifogging performance became poor when the coating was exposed to hot moist air (the temperature of the water bath was 80 ${}^{\\circ}\\mathbf{C}]$ . A logical solution to this issue appeared to be to replace some of the DMAEMA segments with another hydrophilic monomer that, when polymerized, would not lead to a LCST while maintaining the desired hydrophilic/hydrophobic balance in a new terpolymer. \n\nWe decided to incorporate a third, hydrophilic monomer, NVP, to partially replace DMAEMA to obtain the terpolymer (poly(DMAEMA-co-NVP-co-MMA), Scheme 1) and, subsequently, to form a SIPN coating comprising the terpolymer and a network of polymerized EGDMA $(0.5~\\mathrm{wt\\%}$ relative to the copolymer1). We rst synthesized terpolymers with balanced hydrophobicity and hydrophilicity from three monomers, DMAEMA, NVP, and MMA, by conventional free radical polymerization. The $M_{\\mathrm{n}}$ of the terpolymers, measured from GPC, was about 30 000 (Table 1). The molar ratio of the three monomeric units in the nal terpolymers, as determined via $\\mathbf{\\Omega}^{1}\\mathbf{H}\\mathbf{-}\\mathbf{NMR}$ , was in good agreement with the feed ratio (Table 1). It should be noted that a single glass transition temperature $\\left(T_{\\mathrm{g}}\\right)$ was observed for each of three terpolymers (Table 1), clearly pointing to the random distribution of the three monomeric units in the nal terpolymers. This is crucial for the terpolymers to be used in antifogging/frostresisting coatings, since a random copolymer would not lead to (micro)phase separation in the coating, thus ensuring optical clarity of the coating. In addition, the $T_{\\mathrm{g}}$ of the terpolymer could be easily tuned by varying its composition (Table 1): a higher NVP content, with the MMA content being xed at about $30\\mathrm{mol\\%}$ , led to a higher $T_{\\mathrm{g}}$ for the terpolymer.",
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"category": " Materials and methods"
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},
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"id": 12,
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"chunk": "# Antifogging performance against hot moist air \n\nWe rst examined the antifogging performance of terpolymerbased coatings against hot moist air. Compared to the completely fogged control glass, different antifogging performances were observed on the SIPN-T coating surfaces. Aer 15 s exposure to the hot water vapor, no fogging was observed for both SIPN-T-30 and SIPN-T-40 (Fig. 1a). However, some fogging was observed for SIPN-T-50 (photo not shown). Exposure to hot moist air for longer periods of time further revealed difference between SIPN-T-30 and SIPN-T-40 (Fig. $1\\mathrm{c}\\ \\&\\ \\mathrm{d}$ , and video clip in $\\mathrm{ESI\\dagger}_{\\mathrm{\\Phi}}$ ): while SIPN-T40 clearly maintained high transparency, SIPN-T-30 did show some compromise in optical clarity (the le part of the sample, in particular) despite that its surface remained to be free of fog. The observed slight whitening for SIPN-T-30 resembles the water-blushing effect of a water-borne polymer coating,27,28 which is due to water sorption into the coating and subsequent formation of water domain. Therefore, the slightly reduced transparency of SIPN-T-30 (more below) aer exposure to hot moist air for more than 30 s may be attributed to the excessive water-absorbing capacity due to the larger amount of very hydrophilic NVP segments, which in turn might have led to the formation of free water domains in the coating. \n\nTable 1 Properties of terpolymers synthesized by free radical polymerization \n\n\n<html><body><table><tr><td></td><td colspan=\"2\">DMAEMA:NVP:MMA</td><td colspan=\"3\"></td></tr><tr><td>Terpolymer</td><td>Feed molar ratio</td><td>Final molar ratio</td><td>Mn</td><td>PDI</td><td>Tg (C)</td></tr><tr><td>T-30</td><td>30:40:30</td><td>27:39:34</td><td>33000</td><td>2.5</td><td>72</td></tr><tr><td>T-40</td><td>40:30:30</td><td>40:30:30</td><td>30000</td><td>2.3</td><td>61</td></tr><tr><td>T-50</td><td>50:20:30</td><td>48:20:32</td><td>31000</td><td>2.4</td><td>43</td></tr></table></body></html> \n\nTo evaluate the antifogging performance more quantitatively, light transmission over the $400{\\mathrm{-}}700\\ \\mathrm{\\nm}$ range was collected before and aer all samples were exposed to hot moist air for $60~\\mathrm{s}.$ . Prior to the fogging test, SIPN-T-40 and SIPN-T-50 showed comparable light transmission, about $92\\%$ , to the control glass, indicating that the SIPN coating based on the random terpolymer had a negligible effect on the glass transmission (Fig. 2a), while for SIPN-T-30, the coating with the highest NVP content, there appeared to be slight reduction in light transmission, especially in the short wavelength range. Upon exposure to hot moist air for $60~\\mathrm{s}$ , the light transmission decreased to below $40\\%$ for the control glass (Fig. 2b), obviously due to severe fogging. For the three SIPN coatings, the light transmission appeared to strongly depend on the NVP content in the terpolymer (Fig. 2b): the largest reduction in light transmission was observed for SIPN-T-50 (from $92\\%$ to ${\\sim}60\\%$ ) and there was about $10\\%$ decrease for SIPN-T-30; in contrast, SIPN-T-40 maintained high light transmission $(\\sim90\\%)$ . \n\n \nScheme 1 Chemical structure of a random terpolymer poly(DMAEMA-co-NVP-co-MMA), and the subsequent preparation of a SIPN coating on the basis of the terpolymer. \n\n \nFig. 1 Photos of different samples: (left) control glass, (middle) SIPNT-40, and (right) SIPN-T-30: (a) $15\\mathsf{s,}$ (b) $30\\mathsf{s},$ (c) 45 s and (d) 60 s after exposure to hot moist air (5 cm above a $80~^{\\circ}\\mathsf{C}$ water bath) under ambient lab conditions $(\\sim20^{\\circ}\\mathsf C,$ $50\\%$ relative humidity). \n\nThe poor antifogging performance for SIPN-T-50 was likely due to the relatively high DMAEMA content $(\\sim50\\mathrm{\\mol\\%})$ in the terpolymer $\\mathrm{T}{\\cdot}50$ , which might have failed in overcoming the LCST effect in the binary copolymer poly(DMAEMA-co-MMA). Therefore, it appeared to be critical to reduce the total DMAEMA content in the terpolymer below a threshold to eliminate LCST. On the other hand, if there was too much NVP segments in the terpolymer (T-30), the SIPN coating may become too hydrophilic, potentially allowing free water domain to form which would in turn lead to light scattering and reduced light transmission27,28 (water blushing, as discussed above). Therefore, the DMAEMA/NVP molar ratio (with the MMA amount being xed) in the terpolymer played a vital role in designing effective antifogging coating, and the DMAEMA/NVP/MMA molar ratio of 40/30/30 has proven to the optimal ratio for excellent antifogging effect against hot moist air.",
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"category": " Results and discussion"
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},
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"id": 13,
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"chunk": "# Frost-resisting performance \n\nThe frost-resisting performance was evaluated by visually examining the sample appearance 5 s aer it was taken out of a freezer at $-20{}^{\\circ}\\mathbf{C}$ for $30~\\mathrm{min}$ . The control glass lost its transparency completely (Fig. 3a), due to severe frosting that later turned into fog under ambient condition. For SIPN-T-30, some haziness was clearly seen (Fig. 3b), likely due to the presence of the free water domain (which might crystallize into ice initially), as discussed above. In sharp contrast, neither frost nor fog formation was observed on SIPN-T-40 that retained high transparency throughout the test (Fig. 3c and video clip in $\\mathrm{ESI\\dagger}$ . \n\nLight transmission data were also collected for the samples undergoing the frost test. Not surprisingly, the control glass suffered the biggest drop in light transmission due to frosting (Fig. 4), followed by SIPN-T-30 for which only $70\\%$ transmission remained aer 5 s under ambient conditions. High transmission $(\\sim90\\%)$ was observed for SIPN-T-40, indicating that frost formation was completely suppressed. SIPN-T-50 also demonstrated acceptable frost-resisting performance with the transmission value at ${\\sim}88\\%$ (the LCST effect due to the DMAEMA segments was not a factor for frost-resisting property). Once again, the DMAEMA/NVP molar ratio in the terpolymer (with the MMA content being xed) had signicant impact on the frost-resisting performance of the coatings. The sample SIPN-T-40 appeared to have the optimal hydrophilic/ hydrophobic balance, allowing it to excel in both antifogging and frost-resisting performance. \n\nSince the antifogging/frost-resisting property of our SIPN coating is directly related to its water-absorbing capability, we examined the inuence of coating thickness on the antifogging performance. A thicker coating, presumably with higher waterabsorbing capacity, would likely lead to better antifogging behavior. By adjusting the spin-coating rate, we were able to tune the thickness of SIPN-T-40 from $390\\pm30\\mathrm{nm}$ $3000~\\mathrm{rpm})$ , to $490\\pm20\\mathrm{nm}$ $(1500~\\mathrm{rpm})$ , $780\\pm50\\mathrm{nm}$ $\\left({800}~\\mathrm{rpm}\\right)$ , and $920\\pm$ 60 $\\left(400\\mathrm{rpm}\\right)$ , as determined by AFM. It turned out that only the thinnest coating of $390\\mathrm{nm}$ developed some haziness during the frosting test and the rest all demonstrated excellent antifogging/frost-resisting behavior. To guarantee good antifogging/frost-resisting performance for our SIPN coatings, the coating has to be sufficiently thick to be capable of absorbing, rapidly and fully, water molecules from the surrounding into the coating. \n\n \nFig. 2 Light transmission at the normal incident angle for various samples (a) before and (b) after 60 s exposure to hot moist air (5 cm above a 80 $^{\\circ}{\\mathsf C}$ water bath) under ambient lab conditions $(\\sim20^{\\circ}C,$ $50\\%$ relative humidity). \n\n \nFig. 3 Photos of different samples: (a) control glass, (b) SIPN-T-30, and (c) SIPN-T-40, which were first stored at $-20^{\\circ}\\mathsf C$ for $30\\mathrm{\\min}$ and then exposed for 5 s to ambient lab conditions ${\\mathrm{\\sim}}20^{\\circ}\\mathsf{C}.$ , $50\\%$ relative humidity). \n\n \nFig. 4 Light transmission at the normal incident angle for various samples, exposed for $5s$ to ambient conditions ${\\mathrm{.}}{\\sim}20^{\\circ}\\mathsf{C}.$ , $50\\%$ relative humidity) after being stored at $-20^{\\circ}C$ for $30\\mathrm{\\min}$ . \n\nIt should be noted that we also prepared SIPN coatings on the basis of a binary random copolymer poly(NVP-co-MMA) with varying NVP/MMA molar ratios. However, these coatings did not show antifogging/frost-resisting performance as good as SIPNT-40, probably due to the strong water-absorbing NVP segments in the copolymer that might have easily led to the formation of discrete free water domain, thus reducing light transmission.",
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"category": " Results and discussion"
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},
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{
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"id": 14,
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"chunk": "# Surface wettability of SIPN coating \n\nTo investigate the origin of the antifogging/frost-resisting property of the SIPN coatings, we collected time-dependent water contact angles (CA) on these samples under ambient conditions. The initial water CA on all SIPN coatings was greater than $60^{\\circ}$ , which signicantly differs with the CA (approaching $0^{\\circ^{\\circ}}$ ) on a superhydrophilic antifogging coating and reinforces the recent ndings from us1 and others21–24 that a coating does not have to be superhydrophilic to be effectively antifogging. During the 600 s time interval, the water CAs on all SIPN coatings showed a substantial decrease (Fig. 5a), much more than the decrease due to water evaporation (e.g., on the control glass). This clearly indicated that some water had been imbibed into the coating layer. The higher the NVP content in the terpolymer, the more signicant the CA decrease was observed $\\left(\\mathrm{SIPN–T–30}>\\mathrm{SIPN–T–40}>\\mathrm{SIPN–T–50}\\right)$ , which is consistent with the high water-absorbing capability of the hydrophilic NVP segments. \n\nThe changes in the diameter of the water contact area on the sample surface were also simultaneously monitored (Fig. 5b). No change (even slight decrease) in the diameter was observed on the control glass, while the water contact diameter increased by about $9\\%$ for SIPN-T-50 over the 600 s period, similar to the increase we observed previously for the antifogging coating1 based on the binary copolymer poly(DMAEMA- $_{\\cdot c o}$ -MMA) (DMAEMA/MMA molar ratio: 70/30). On the other hand, the water contact diameter dramatically increased by ${\\sim}40\\%$ and $53\\%$ (Fig. 5b) for SIPN-T-40 and SIPN-T-30, respectively. Obviously, water molecules had diffused into these terpolymerbased SIPN coatings and led to signicant expansion of the droplet contact area with the coating surface. The much greater increase of the water contact diameter in these two coatings further indicated that the NVP segments in the terpolymer were indeed more “water-loving” than the DMAEMA segments. However, too many NVP units in the terpolymer would lead to too much water being imbibed into the coating and the formation of discrete free domain, thus compromising its antifogging performance (as in the case of SIPN-T-30). Therefore, the ability we render to a coating to allow rapid diffusion of water molecules into the coating, while not forming discrete water domain in the coating, appears to be the key in obtaining highly effective antifogging/frost-resisting coating, such as SIPN-T-40.",
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"category": " Results and discussion"
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},
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{
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"id": 15,
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"chunk": "# Long-term effectiveness of SIPN coating \n\nTo evaluate long-term effectiveness of our SIPN coatings, SIPNT-40 was subject to multiple cycles of fogging/frosting tests and a more practical, bathroom test. The optical transparency of the SIPN-T-40 coating maintained throughout the fogging/frosting test allowed us to monitor the variation of the coating thickness, as derived from the light transmission data.25 Aer the 920 nm thick SIPN-T-40 was stored at $-20\\ ^{\\circ}\\mathbf{C}$ for $30\\ \\mathrm{min}$ , it was exposed to ambient conditions ( ${\\bf\\sim}20^{\\circ}{\\bf C}$ , $50\\%$ relative humidity). \n\n \nFig. 5 (a) Water contact angle evolution on various samples as a function of time. (b) Diameter change of the water droplet on various samples over the $600\\ s$ period as expressed as $\\Delta D/D_{0}$ , where $\\Delta D=D-D_{0}$ , and $D_{0}$ and $D$ (shown in the inset) are the initial diameter (time zero) and the diameter at different times, respectively, of the wetted area by the water droplet. \n\nThe coating thickness increased by $36\\%$ aer 30 s (Fig. 6a) relative to the initial thickness, suggesting the coating had taken up a substantial amount of water. Water molecules should exist as bound water (non-freezing water) to the hydrophilic segments of the terpolymer.1,22 In addition, since SIPN-T40 remained completely transparent over the test period, there should be no discrete free water domain in the coating; otherwise, reduced light transmission would have been observed.27,28 Aer $60~\\mathrm{s}$ , the coating thickness decreased signicantly (Fig. 6a) to about $17\\%$ above its initial thickness, revealing that some water molecules had somehow “le” the coating. It was interesting to notice that, aer about $150~\\mathrm{s}$ , the coating had almost recovered to its original thickness; in other words, most of the absorbed water had been released from the coating, despite that the exact mechanism of water departure remained unclear. \n\nThe rapid recovery of the thickness for the antifogging/frostresisting coating is an obvious advantage: the coating is ready for the next antifogging action. SIPN-T-40 was subject to four more frosting tests and, indeed, during each test the variation of the coating thickness followed the similar trend to Fig. 6a. The original coating thickness was restored in a short period of time $\\left(2.5\\mathrm{-}3\\mathrm{min}\\right)$ ) under ambient conditions. The variation in the coating thickness at room temperature was also directly reected in the transmission prole (Fig. 6b). The coating aer 30 s at room temperature following the rst freezing ( $30\\mathrm{min}$ at $-20$ ${}^{\\circ}\\mathbf{C}]$ , Fig. 6b-ii, appeared to have very similar transmission spectrum with the same coating aer $30~\\mathrm{s}$ at room temperature following the h freezing (Fig. 6b-iii), indicating there was a similar amount of bound water in the coating during the rst and h frosting test. Furthermore, the transmission spectrum (Fig. 6b-iv) for the coating aer $200\\mathrm{~s~}$ at room temperature following the h freezing resembled closely to the original coating (Fig. 6b-i), revealing that the coating thickness had restored to its original thickness. The reversible change of the coating thickness implied that the antifogging property of our coating would be long-term effective. \n\nSIPN-T-40, together with a control glass, was mounted on a bathroom mirror and visually examined for possible fogging immediately aer a shower for 6 months (with typically one shower a day being taken). As clearly shown in Fig. 7, SIPN-T-40 remained to be perfectly antifogging aer about 180 showers, while the control glass as well as the mirror completely fogged up. Indeed, the terpolymer-based SIPN coating has remained antifogging aer at least 6 months. \n\n \nFig. 6 (a) Thickness change for SIPN-T-40, relative to the original coating thickness, following a frosting test: 30–150 s at room temperature after the coating was stored at $-20^{\\circ}\\mathsf C$ for $30\\mathrm{min}$ . (b) Zoomed-in transmission raw data (in dots) and fitting solid lines by eqn (1) for SIPN-T-40: (i) the original coating; (ii) 30 s at room temperature after first freezing (stored at $-20^{\\circ}C$ for $30\\mathrm{min})$ ); (iii) 30 s at room temperature after 5th freezing; and (iv) 200 s at room temperature after 5th freezing. \n\n \nFig. 7 Photo of two samples (a) SIPN-T-40 and (b) control glass on a bathroom mirror, immediately after a shower on day 181. \n\nIn summary, we prepared antifogging/frost-resisting coatings on the basis of a SIPN comprising random, linear terpolymer poly(DMAEMA-co-NVP-co-MMA) and cross-linked PEGDMA. By carefully balancing the hydrophilic DMAEMA and NVP segments and hydrophobic MMA segments in the terpolymer, the LCST effect in a binary poly(DMAEMA-co-MMA)-based coating was completely eliminated, leading to excellent antifogging/frost-resisting properties against both hot and cold moist air for a terpolymer coating (SIPN-T-40) with the optimal DMAEMA/NVP/MMA molar ratio of 40/30/30. The antifogging/ frost-resisting property of the SIPN-based coating can be attributed to its capability of absorbing rapidly water vapour from the surrounding, yet not allowing the formation of discrete water domain in the coating, thus ensuring optical transparency for the coating during fogging/frosting tests. The fact that water molecules can quickly depart from the coating renders this type of antifogging/frost-resisting coating longterm effective.",
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"category": " Results and discussion"
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},
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{
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"id": 16,
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"chunk": "# Acknowledgements \n\nFinancial support of this research from USDA/NIFA (Award No. \n2011-67022-30229) is gratefully acknowledged.",
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"category": " References"
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},
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{
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"id": 17,
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"chunk": "# Notes and references \n\n1 J. Zhao, A. Meyer, L. Ma and W. Ming, Chem. Commun., 2013, 49, 11764. \n2 A. Tricoli, M. Righettoni and S. Pratsinis, Langmuir, 2009, 25, 12578. \n3 P. Chevallier, S. Turgeon, C. Sarra-Bournet, R. Turcotte and G. Laroche, ACS Appl. Mater. Interfaces, 2011, 3, 750. \n4 L. Introzzi, J. M. Fuentes-Alventosa, C. A. Cozzolino, S. Trabattoni, S. Tavazzi, C. L. Bianchi, A. Schiraldi, L. Piergiovanni and S. Farris, ACS Appl. Mater. Interfaces, 2012, 4, 3692. \n5 L. Zhang, Z. Qiao, M. Zheng, Q. Huo and J. Sun, J. Mater. Chem., 2010, 20, 6125. \n6 J. A. Howarter and J. P. Youngblood, Adv. Mater., 2007, 19, 3838. \n7 X. Zhang and J. He, Chem. Commun., 2015, 51, 12661. \n8 J. Xiong, S. N. Das, J. P. Kar, J. H. Choi and J. M. Myoung, J. Mater. Chem., 2010, 20, 10246. \n9 H. Dong, P. Ye, M. Zhong, J. Pietrasik, R. Drumright and K. Matyjaszewski, Langmuir, 2010, 26, 15567. \n10 D. Lee, M. F. Rubner and R. E. Cohen, Nano Lett., 2006, 6, 2305. \n11 F. C. Cebeci, Z. Wu, L. Zhai, R. E. Cohen and M. F. Rubner, Langmuir, 2006, 22, 2856. \n12 N. Nuraje, R. Asmatulu, R. E. Cohen and M. F. Rubner, Langmuir, 2010, 27, 782. \n13 Y. Li, J. Zhang, S. Zhu, H. Dong, F. Jia, Z. Wang, Z. Sun, L. Zhang, Y. Li, H. Li, W. Xu and B. Yang, Adv. Mater., 2009, 21, 4731. \n14 X. Liu, X. Du and J. He, ChemPhysChem, 2008, 9, 305. \n15 L. Xu and J. He, ACS Appl. Mater. Interfaces, 2012, 4, 3293. \n16 L. Zhang, Y. Li, J. Sun and J. Shen, Langmuir, 2008, 24, 10851. \n17 R. Wang, K. Hashimoto, A. Fujishima, M. Chikuni, E. Kojima, A. Kitamura, M. Shimohigoshi and T. Watanabe, Nature, 1997, 388, 431. \n18 M. Miyauchi, A. Nakajima, K. Hashimoto and T. Watanable, Adv. Mater., 2000, 12, 1923. \n19 Y. Lai, Y. Tang, J. Gong, D. Gong, L. Chi, C. Lin and Z. Chen, J. Mater. Chem., 2012, 22, 7420. \n20 X. F. Gao, X. Yan, X. Yao, L. Xu, K. Zhang, J. Zhang, B. Yang and L. Jiang, Adv. Mater., 2007, 19, 2213. \n21 J. A. Howarter and J. P. Youngblood, Macromol. Rapid Commun., 2008, 29, 455. \n22 H. Lee, M. L. Alcaraz, M. F. Rubner and R. E. Cohen, ACS Nano, 2013, 7, 2172. \n23 H. Lee, J. B. Gilbert, F. E. Angile, R. Yang, D. Lee, M. F. Rubner and R. E. Cohen, ACS Appl. Mater. Interfaces, 2015, 7, 1004. \n24 X. Zhang and J. He, Sci. Rep., 2015, 5, 9227. \n25 K. C. Jena and D. K. Horea, Am. J. Phys., 2011, 79, 256. \n26 D. J. Griffiths, Introduction to Electrodynamics, Prentice-Hall, Upper Saddle River, NJ 07458, 1999, p. 404. \n27 N. Starostin, S. Harvey and G. Carlson, Scanning, 2008, 30, 78. \n28 Z. Aguirreurreta, J. Dimmer, I. Willerich, J. de la Cal and J. R. Leiza, Macromol. Mater. Eng., 2015, 9, 925.",
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"category": " References"
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},
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{
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"id": 18,
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"chunk": "# Conclusions",
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"category": " Conclusions"
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}
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] |