Abstract
In this work, lamellar MnFe2O4 was successfully planted on a wood surface through the association of hydrogen bonds via the one-pot hydrothermal method. Simultaneously, the fluoroalkylsilane (FAS-17) on the surface of the MnFe2O4 layer formed long-chain or network macromolecules through a poly-condensation process and provided a lower surface energy on the wood surface. The MnFe2O4/wood composite (FMW) presented superior superparamagnetism, superhydrophobicity and electromagnetic wave absorption performance. The results indicated a saturation magnetization of the FMW with excellent superparamagnetism of 28.24 emu·g−1. The minimum value of reflection loss of the FMW reached −8.29 dB at 16.39 GHz with a thickness of 3 mm. Even after mechanical impact and exposure to corrosive liquids, the FMW still maintained a superior superhydrophobicity performance.
Currently, bamboo, wood and various other natural organic materials are usually considered good candidates as host materials for composites, and as-prepared composites can still retain their special morphology while obtaining some unique properties1,2,3,4,5. In particular, wood or wood-based products feature superior physical properties and a warm appearance and have excellent functions in penetrability, accessibility and reactivity, which are essentially different from other materials. However, when facing sources of environmental erosion such as acid rain and high temperatures, wood surfaces typically loses their efficacy with clouding, roughening, discolouring and checking. Therefore, potential mechanical, thermal, optical, magnetic and biological applications of wood-inorganic hybrid materials have attracted significant attention6,7,8. More importantly, through solutions combining inorganic particles on wood surfaces, the wood receives efficient protection from environmental erosion, which improves durability and robustness and extends the application range and service life9,10.
Oxide metal particles, such as CoFe2O411,12,13, Fe3O414, MnFe2O413,15,16, and others17, are very useful inorganic materials because of their distinct size-dependent physicochemical, magnetic and other excellent properties. Among these oxide metals particles, superparamagnetic MnFe2O4 particles are a highly active area of research and can be applied to a wide range of applications, including air and water purification, ultraviolet resistance, and electromagnetic shielding. Furthermore, MnFe2O4 particles have massive hydroxyl groups on their surfaces, which can produce an effective combination with the surface of wood and may provide superior magnetic and electromagnetic wave absorption properties18,19.
Superhydrophobicity is of great interest in various fields. Superhydrophobic materials, because of their self-cleaning surfaces, biocompatibility and other excellent properties, are widely used in applications in waterproofing, anti-fouling, and bacteriostasis20,21,22. Often, clouding, discolouring and checking defects in wood are caused by the hydrophilicity of the wood surface. Therefore, to overcome the wood’s defects and prolong the wood’s service life, the preparation of superhydrophobic wood is necessary23,24. In general, a superhydrophobic wood surface can be prepared by two approaches: forming a layer of inorganic particles on the wood surface to create a rough structure or chemically modifying a rough surface with a low surface free energy (such as FAS-17)25,26. Most of the preparation methods for these materials are complicated and require at least two or three steps for the formation of the superhydrophobic surface. In this work, we employed a simple one-step hydrothermal method for the growth of MnFe2O4 on a wood surface, and the as-prepared MnFe2O4/wood composite exhibited superior superparamagnetism, superhydrophobic and electromagnetic wave absorption properties. In addition, the chemical and mechanical stability of superhydrophobic surfaces are very important to the performance of the material and have received broad interest. Thus, we tested the superhydrophobicity of the wood surface by sand abrasion and a test of resistance against corrosive liquids, which indicated a good chemical and mechanical stability of the wood surface when facing environmental erosion.
Results
Figure 1 shows the X-ray diffraction (XRD) patterns of the wood and the MnFe2O4/wood composite. As shown in Fig. 1a,b, strong diffraction peaks at 16.0° and 22.5° appear in the wood and the FMW spectra, which originated from the crystalline region of the cellulose in the wood27. Seven crystalline peaks were observed at 2θ° of 17.96°, 30.31°, 35.67°, 43.33°, 53.52°, 57.09° and 62.78° and were related to the 111, 220, 311, 400, 422, 511 and 440 crystallographic planes, corresponding to the MnFe2O4 crystals (JCPDS 73-1964) with a spinel structure28. Therefore, MnFe2O4 had been successfully grown on the wood surface.
Figure 1.

X-ray diffraction (XRD) analyses of (a) the wood and (b) the FMW.
Figure 2 shows the surface morphologies of the wood and the FMW. As shown in Fig. 2a, the microstructure of the wood in a longitudinal section and the inner surface of the lumen and the vessels were observed on the wood surface. Figure 2b shows the surface of the FMW with a very low magnification. After the one-step hydrothermal process, the MnFe2O4 was packed tightly on the wood surface, masking the vessels and other details. The magnified SEM image of the FMW revealed that the MnFe2O4 layer was composed of a number of lamellas with different sizes (Fig. 2c,d). Therefore, these results indicate that the lamella MnFe2O4 had been successfully coated onto the wood surface.
Figure 2.
SEM micrographs of (a) the wood, (b) the surfaces of the FMW with a low-magnification and (c,d) local partial enlarged images of (b).
Figure 3 shows the typical FT-IR spectra of the wood and the FMW. The peaks at 3450–3400 cm−1 were attributed to the -OH stretching absorption bands arising from the hydroxyl groups of the wood, which shifted to lower wavenumbers. This result indicates the formation of a strong interaction between the hydroxyl groups of the wood surface and the MnFe2O4 through hydrogen bonds29. Then, as shown in Fig. 3a, the peaks at 2921 cm−1, 2852 cm−1 and 1740 cm−1 were ascribed to the stretching vibrations of -CH3, -CH2 and C=O, respectively30. These peaks in the FMW spectra (Fig. 3b) had significantly decreased, which might have occurred by the hydrolysis of fatty acids through the alkaline hydrothermal process. More importantly, the peaks at 1202 cm−1 and 1332 cm−1 were assigned to the C-F stretching vibration, which corresponds to the FAS-17 that is incorporated into the MnFe2O4 surface31. In addition, a strong adsorption peak appeared at 576 cm−1, which was attributed to the intrinsic vibrations of the manganese ferrite (Fe-O or Mn-O)32. Therefore, the analysis of the FT-IR spectra of the FMW exhibited the existence of FAS-17 and hydrogen bonds between the wood surface and the MnFe2O4.
Figure 3.

FT-IR spectra of (a) the wood and (b) the FMW.
X-ray photoelectron spectroscopy (XPS) was employed as a potent technique to analyze the chemical structure characteristics and surface modification of the FMW after the hydrothermal process. The survey-scan spectra of the FMW exhibited the existence of C, O, Mn, Fe, F and Si in the FMW surface, as shown in Fig. 4a. The wood substrate provided the major source of C and O, and the MnFe2O4 growing in the wood surface provided the Fe, Mn and O. F, Si, and a portion of C and O originated from the hydrophobic layer (FAS-17) on the surface of the MnFe2O4.
Figure 4.
(a) Survey-scan XPS spectra of the FMW, (b) Fe2p XPS spectra of the FMW, (c) Mn2P XPS spectra of the FMW, (d) O1s XPS spectra of the FMW, (e) C1s XPS spectra of the FMW and (f) F1s XPS spectra of the FMW.
The Fe 2p peak (Fig. 4b) was a doublet with a spin-orbit separation of 13.7 eV, and the Fe3+ cation had a well-defined structure at 8 eV after the Fe 2p3/2 peak (711.58 eV). However, this peak in the Fe3O4 was smeared and almost equal in proportion because of the presence of both Fe2+ and Fe3+ 33. As shown in Fig. 4c, the Mn 2p spectra consisted of spin-orbit-split 2p3/2 and 2p1/2 with a separation of 11.7 eV, which was approaching the spin-orbit separation (11.6 eV) of the MnO34. In addition, the satellite peak at 647.08 eV was approximately 5 eV distant from the 2p1/2 peak of the Mn 2p spectra, which is the typical Mn2+ ion behaviour35. Therefore, these results provided powerful evidence of the presence of Mn2+ and Fe3+ in the FMW surface.
The O 1s region (Fig. 4d) was dominated by three components centred at 530.18, 531.78 and 533.08 eV, arising from the photoelectrons ejected from the oxygen 1 s orbital. The dominant peak at 533.08 eV was attributed to the Fe-O and Mn-O from the MnFe2O4 layer36. The peak at 531.78 eV included a carbon-oxygen double bond (such as lignin), -OH groups (such as adsorbed water, hydroxyl groups from the wood or hydrogen bonds between the wood surface and MnFe2O4) and a Si-O bond (FAS-17 layer)31. Finally, the C-H bond at 533.08 eV was provided by the FAS-17 and the wood substrate.
The C 1 s spectrum (Fig. 4e) of the FMW surface could be resolved into eight components, namely, CF3-CF2 (293.13 eV), CF2-CF2 (291.30 eV), CF2-CH2 (289.13 eV), O=C-O (288.10 eV), C=O or O-C-O (287.05 eV), C-O (285.61 eV), C-H or C-C (284.30 eV) and C-Si (282.5 eV)31. The presence of the CF3-CF2, CF2-CF2, CF2-CH2 and C-Si in the spectrum provided powerful evidence that the hydrolytic FAS-17 had been incorporated into the MnFe2O4 surface and formed the hydrophobic layer through the self-assembly process. The other peaks originated from the wood surface (cellulose, hemicellulose and lignin), and a small amount of the hydrocarbon originated from the XPS instrument itself37. Figure 4f shows the high-resolution XPS F 1 s spectra of the FMW surface. The peak at 693 eV was attributed to the F 1 s from the FAS-17 layer. In summary, all of the XPS results demonstrated that the FMW sample consisted of C, O, Mn, Fe, F and Si elements with an anomic ratio of Fe:Mn at 2.35:1 and proved the presence of the MnFe2O4 and the hydrophobic layer (FAS-17 layer) on the wood surface.
Figure 5 shows the magnetization-hysteresis (M-H) curves of the FMW. The magnetic property of the MnFe2O4/wood composite was analyzed by room temperature VSM with an applied field of −10 KOe ≤ H ≤ 10 KOe. The value of the saturation magnetization (Ms) of the FMW was 28.08 emu·g−1. The lower right corner inset shows that the remnant magnetization (Mr) and coercivity field were 1.2 emu·g−1 and 25 Oe, respectively. These results show that the FMW had superior superparamagnetic properties, small hysteresis loops and low coercivity38. Therefore, the MnFe2O4/wood composite showed superparamagnetism via a one-pot hydrothermal process with low temperature.
Figure 5. Magnetization of the FMW as a function of the applied magnetic field.

The inset shows a magnification of one segment of the FMW magnetization-hysteresis curves.
The mechanism of the formation of the MnFe2O4 can be expressed by reaction Equations (1)–(3), , :
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According to previous results, the possible mechanism can be described as follows (Fig. 6). First, when the ammonia solution was added into the Fe3+, Mn2+ and FAS-17 mixed solution containing the wood substrate, the Fe3+ and Mn2+ ions transformed into Fe and Mn hydroxides, respectively. Then, part of the Fe and Mn hydroxides dissolved in the mixed solution because of the presence of high concentrations of the ammonia and converted to the Mn(OH)n2−n and Fe(OH)n3−n with massive hydroxyl groups. Second, the Mn(OH)n2−n and Fe(OH)n3−n, as a growth unit, formed the MnFe2O4 crystal nucleus on the wood surface by the dehydration reaction. Then, the MnFe2O4 crystal grew with the deposition of the MnFe2O4 nucleus, which eventually formed a more stable MnFe2O4/wood composite. More importantly, inset a shows the combination mechanism of the MnFe2O4 and the wood surface by the hydrogen bonds. As shown in inset b, the Si-OCH3 groups in the FAS-17 molecules participate in a hydrolysis reaction, which caused the elimination of CH3OH and the formation of the Si-OH groups. Subsequently, after hydrolysis, the FAS-17 molecules on the MnFe2O4 crystal nucleus surface formed long-chain or network macromolecules by a polycondensation reaction. Then, the MnFe2O4 crystal grew in the constraint of the fluoroalkylsilane macromolecule structure and, ultimately, formed the lamellar MnFe2O4 on the wood surface. Finally, when water was dropped onto the wood surface, the FMW displayed a superior superhydrophobic property.
Figure 6. Possible schematic illustration of the preparation of the FMW.
Insets (a,b) show the combination mechanism of the MnFe2O4 layer and the wood surface and the formation mechanism of the hydrophobic lamellar MnFe2O4, respectively.
To provide a more visible demonstration of the superhydrophobic performance, four types of corrosive liquids were placed on the surface of the wood and FMW, including water, acid, salt, and alkali droplets. Figure 7a shows that all of the liquid profiles on the wood surface were approximately zero, which proved the hydrophilicity of the pristine wood. In contrast, the surface of the FMW was highly repellent to the water and other liquids, and the droplets exhibited spherical shapes on the sample surface (Fig. 7b). Figure 7b shows the contact angle values and profiles of several typical liquids. The CA value of the water droplet on the FMW surface was approximately 156°, and all of the CA values of the acid, salt, and alkali droplets on the sample surface were over 150° because the high surface concentration of -CF3 and -CF2 from the FAS-17 layer provided a low surface energy on the FMW surface, which is conducive for superior superhydrophobic performance.
Figure 7.
Optical images of water, HCl solution (pH 1), NaCl solution (pH 7) and NaOH solution (pH 14) droplets on the surfaces of (a) wood and (b) FMW, and (c) the contact angle values and profiles of the FMW.
The superhydrophobic property of the FMW was further evaluated by a sand abrasion experiment. In this test, sand grains (10 g) with an average diameter of approximately 100 μm were flowed to the FMW surface from a height of 30 cm, and the sand grains repeatedly impacted the FMW surface 10 times (100 g of sand). As shown in Fig. 8b, it is intuitive to show that the values of the contact angles of water (WCA) and the saturation magnetization (Ms) of the FMW gradually decreased with increases in the experiment frequency. The WCA images and Ms curves of the FMW with its values were recorded at 0 g, 10 g, 20 g, 40 g, 60 g and 100 g, shown in Fig. 8c–h, respectively. Before the experiment, the WCA of the FMW was 156°. After 10 cycles of the sands abrasion test, the WCA of the FMW was 149.1°. In addition, the value of the Ms of the FMW had only decreased by 1.61 emu g−1, indicating its stable performance for superhydrophobicity and superparamagnetism. Therefore, these results indicate that the samples have excellent durability magnetism and mechanical stability when confronted with external abrasion, and the FMW might have great potential in a wide range of applications.
Figure 8.
Schematic description of the experimental set-up for (a) the sand abrasion experiment of the FMW. (b) The trend graph of Ms and WCA of the FMW as a function of the amount of sand dropped onto the surface. (c–h) The values of saturation magnetization (Ms) and WCAs with its corresponding curves or image varied with the mass of sand dropped onto the surface.
To evaluate the durability of the superhydrophobic wood surface for mild acids and strong bases, the as-prepared FMW samples were placed into a NaCl solution of 0.1 mol/L (Fig. 9a) HCl solution with a pH of 1 (Fig. 9b) and a NaOH solution with a pH of 14 (Fig. 9c) for 4 h at 50 °C. In contrast to the baseline condition, the WCA of the FMW surface displayed only a small change, and the water contact angles were larger than 150°. These results showed that all of the samples maintained their superhydrophobic properties after the acid and base corrosion tests and had good durability towards acidic (152°) and basic (151°) liquids. In addition, the salt solution corrosion test demonstrated that Cl and Na ions had almost no effect on the superhydrophobic performance under the same conditions (Fig. 9a). Figure 9b,c show that the acid resistance of the FMW was appreciably stronger than the base resistance. Therefore, this superhydrophobic MnFe2O4/wood composite might have applications in outdoor building materials to protect wood substrates from acid rain erosion by the environment.
Figure 9.
The water contact angle profiles and values of the samples with an immersion time in solutions of (a) NaCl (0.1 mol/L), (b) HCl (pH 1) and (c) NaOH (pH 14) at 50 °C for 4 h.
To investigate the electromagnetic absorption property of the wood and the FMW, the reflection loss (RL) values were calculated by the transmission line theory39.
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where Zin is the input impedance of the samples, Z0 is the impedance of air, εr is the complex permittivity, μr is the complex permeability, d is the thickness of the samples, c is the velocity of light and f is the microwave frequency. The values of the reflection loss (RL) of the wood and the FMW are exhibited by three-dimensional and colour-filling pattern images in the frequency range of 2–18 GHz in Fig. 10. Figure 10a,b show that both the wood and FMW had a minimum value at the thickness of 3 mm, and the corresponding values of the reflection loss were −2.37 dB at 16.64 GHz and −8.29 dB at 16.39 GHz, respectively. Since the magnetic loss of MnFe2O4 after the lamellate MnFe2O4 formed on the wood surface, the absorption bandwidth of the FMW improved significantly compared with the wood. These results indicate that the electromagnetic absorption property of the MnFe2O4/wood composite was improved via a simple one-step hydrothermal method, which might provide potential applications in electromagnetic wave-absorbing materials and electromagnetic shielding.
Figure 10.
Frequency dependence of the reflection loss for (a) the wood and (b) the FMW by three-dimensional and colour-filling patterns in the frequency range of 2–18 GHz.
Conclusions
In summary, we developed a simple one-step hydrothermal method to fabricate a superparamagnetic MnFe2O4/wood composite with good chemical and mechanical stability of its superhydrophobic and electromagnetic wave absorption properties. The reaction involved hydrogen bond assembly and a polycondensation process. The hydrogen bond assembly appeared in the formation process of the lamellar MnFe2O4 layer, causing the tight adhesion of the lamellar MnFe2O4 onto the wood surface. The fluoroalkylsilane macromolecules on the MnFe2O4 layer surface via the polycondensation process provided a low surface energy to achieve superhydrophobicity. After a one-step hydrothermal reaction, the value of the saturation magnetization of the FMW reached 28.08 emu·g−1 and presented excellent superparamagnetism properties. The value of the water contact angles of FMW reached 156°, and the FMW maintained its superhydrophobic properties even after sand abrasion and exposure to corrosive liquids. In addition, the value of the minimum reflection loss of the FMW reached −8.29 dB at 16.39 GHz with a thickness of 3 mm, and the absorption bandwidth improved. These findings suggest that the MnFe2O4/wood composite has potential applications in electromagnetic wave-absorbing materials, electromagnetic shielding and outdoor building materials.
Methods
Materials
All chemicals were supplied by Shanghai Boyle Chemical Co. Ltd (Shanghai. China). and used without further purification. The wood slices were cut to dimensions of 10 mm (length) × 10 mm (width) × 10 mm (height), and then the slices were ultrasonically rinsed with deionized water for 30 minutes and dried at 80 °C in a vacuum.
One-pot hydrothermal synthesis of FMW
In a typical synthesis, FeCl3∙6H2O (3.24 g) and MnCl2∙4H2O (0.94 g) in a stoichiometric ratio of 2:1 were dissolved in 80 mL of a deionized water solution with the wood samples under magnetic stirring for 2 h at room temperature. During the stirring process, FAS-17 (1 mL) and the proper amount of ammonia (3 mL) were added dropwise into the solution. Then, the obtained homogeneous mixture was transferred into a 100 mL Teflon-lined stainless autoclave, and this vessel was sealed and heated to 120 °C for 8 hours. Subsequently, the autoclave was left to cool to room temperature. Finally, the prepared magnetic wood samples were removed from the solution, ultrasonically rinsed with deionized water for 30 minutes, and dried at 45 °C for over 24 hours in vacuum.
Characterizations
The surface morphologies of the samples were characterized by scanning electron microscopy (SEM, FEI, Quanta 200). Crystalline structures of the samples were identified by the X-ray diffraction technique (XRD, Rigaku, D/MAX 2200), operated with Cu Kα radiation (λ = 1.5418 Å) at a scan rate (2θ) of 4° min−1, an accelerated voltage of 40 kV and the applied current of 30 mA ranging from 10° to 70°. Changes in the chemical groups were recorded via Fourier transform infrared spectroscopy (FT-IR, Magna-IR 560, Nicolet). XPS analysis was characterized by an X-ray photoelectron spectrometer (ESCALAB 250 XI, ThermoFisher Co.). The magnetic properties of the composites were measured by a vibrating sample magnetometer (VSM, LakeShore, Model 7404, USA) at 300 K. The contact angle analyzer (CAA, JC2000C, Powereach Co., China) at ambient temperature with a droplet volume of 5 μL was employed to measure the contact angles (CAs) of the samples. An average of the five measurements taken at different positions on each sample was applied to calculate the final CA value. The sand abrasion test evaluated the mechanical resistance of the MnFe2O4/wood composite. Sand (10 g in each test with an average particle size of 100 μm) was dropped from a 30 cm height onto the fabricated films, at a tilt angle of 45° with respect to the axis vertical to the bottom surface of the experimental set-up. The microwave parameters of the samples were measured at 2–18 GHz with an AV3618 network analyzer. The reflection losses (dB) of the composites were calculated according to the transmission line theory, using the measured data of relative complex permeability and permittivity.
Additional Information
How to cite this article: Wang, H. et al. A simple, one-step hydrothermal approach to durable and robust superparamagnetic, superhydrophobic and electromagnetic wave-absorbing wood. Sci. Rep. 6, 35549; doi: 10.1038/srep35549 (2016).
Acknowledgments
This research was supported by Zhejiang Provincial Natural Science Foundation of China (Grant No. LZ15C160002), the Scientific Research Foundation of Zhejiang A&F University (Grant No. 2014FR077), the Special Fund for Forest Scientific Research in the Public Welfare (Grant No. 201504501), and the Fund for Innovative Research Team of Forestry Engineering Discipline (101-206001000713).
Footnotes
Author Contributions Q.F. conceived the project and revised the manuscript; H.W. and Q.Y. designed the experiments and wrote the paper. C.W., B.F., Y.X. and Y.C. prepared figures 1–12; C.J. provided project support and contributed to the revisions of the manuscript. All authors reviewed the manuscript.
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