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  • Liuli CHEN, Yan CHEN, Xuanrong JI
    Journal of the Chinese Ceramic Society. 2024, 52(1): 154-160.
    Introduction

    1-3 type piezoelectric composites are widely used to fabricate high-sensitivity and broadband ultrasonic transducers due to the advantages like a low dielectric constant, a low acoustic impedance, and a high electromechanical coupling coefficient. However, some conventional manufacturing methods such as the cut-and-fill method, the arrangement-casting process, and the injection molding method have challenges to emanate from geometric complexity and structural integrity. Stereolithography technology based on the mask projection approach is an alternative method for manufacturing piezoelectric ceramics with a rapid prototyping and a high precision. Lead-free barium titanate BaTiO3 (BTO) ceramics are widely investigated for piezoelectric sensors and dielectric capacitors applications because of their high dielectric constant, good piezoelectric coefficient, and favorable electromechanical coupling coefficient. In this work, digital light processing (DLP) technology was used to manufacture barium titanate based 1-3 type piezoelectric composites. The influence of piezoelectric phase volume fraction (i.e., 20%-45%) on the micrograph, acoustic impedance and electrical properties of BTO 1-3 composites was investigated.

    Methods

    The printed ceramic slurries with 84% (in mass fraction) BTO content, including BTO powders (d50=500 nm), dispersant, and liquid photopolymers, were mixed by a model ZYMC-180V homogenizer (ZYE) at 2 000 r/min for 90 s. The printed models were built by a software named Computer-Aided Design (CAD) and sliced to a thickness of 7 μm. The piezoelectric pillars (150 μm) with a support were printed layer by layer to form the physical models (i.e., Soon solid, TC-Ⅱ). The printed samples were washed in alcohol by aultrasonic cleaner to remove the residual slurry. Afterwards, the green bodies were treated by a two-step heating treatment, i.e., a debonding process and a sintering process, to obtain the piezoelectric phase structures. Two-time vacuum treatments below -100 kPa were introduced to remove air bubbles in epoxy resin (EPO-TEK301) that filled in the kerfs between piezoelectric pillars (width of 120 μm, height of 330 μm). The samples filled with epoxy resin were heat treated at 60 ℃ for 12 h and then coated with gold electrodes. The BTO 1-3 composites were polarized in an electric field of 4 kV/mm in silicone oil. The microstructures of samples were characterized by a model TM4 000 Plus scanning electron microscope (Hitachi Co., Lted., Japan). The dielectric constant εr, dielectric loss δ, and frequency impedance spectrum were measured by a model 6500B precision impedance analyzer (Wayne Kerr Co., Ltd., UK). Piezoelectric constant d33 was determined by a model ZJ-3A piezo-d33 meter (Institute of Acoustics, Chinese Academy of Sciences, China). The ferroelectric hysteresis loop was measured by a model 2000E ferroelectric analyzer (aixACCT Co., Germany).

    Results and discussion

    The uniform piezoelectric pillars with a width of (150±10) μm are printed through optimizing the slurry formula, and the minimum distance between pillars is approximately 100 μm. The bending deformation of BTO pillars is negligible, and the lateral shrinkage rate is 20%. The forming mechanism of DLP technology results in a clear lamination of the piezoelectric pillar along the printing direction. The shrinkage of ceramics and the growth of grains fill the gap between interlayers, thus reducing the lamination after sintering. There are no residual bubbles in the epoxy resin after vacuum treatment. The density and acoustic impedance of the piezoelectric composites increase with the growth of the piezoelectric phase volume proportion. Compared with the acoustic impedance of BTO ceramics (i.e., Z=31.64 MRayl, 1Rayl=1 Pa·s/m=10-6 MRayl), the acoustic impedance of composites (45%, in volume fraction) is decreased by 67%.

    The piezoelectric constant d33 and electromechanical coupling coefficient kt enhance with the piezoelectric phase volume proportion of the composites, meeting their maximum values of 74 pC/N and 0.48, respectively. Compared with the BTO ceramics (kt=0.37), the electromechanical coupling coefficient is improved by 30%. According to the frequency impedance spectra of piezoelectric composites, 1-3 type composites have a pure thickness vibration mode. The dielectric constant εr increases linearly with increasing the piezoelectric phase volume fraction, reaching its maximum of 1 167. The dielectric loss tanδ is lower than 3%, which can enhance the receiving sensitivity of ultrasound transducers. The residual polarization intensity increases with the increase of volume fraction of the piezoelectric phase. The residual polarization intensity of the piezoelectric composite with a volume fraction of 45% reaches a maximum of 1.77 μC/cm2 at 4 kV/mm.

    Conclusions

    1-3 type barium titanate/epoxy resin piezoelectric composites were fabricated by the DLP technology. The effect of volume fraction of piezoelectric phases on the electrical performances of composites was investigated. The electrical properties such as piezoelectric constant d33, electromechanical coupling coefficient kt, and dielectric constant εr were optimized as the volume fraction of the piezoelectric phase (≤45%) was increased. The polymer phase could effectively reduced the acoustic impedance of piezoelectric materials, thus obtaining an acoustic matching between the piezoelectric materials and tissues or water. Compared to pure barium titanate ceramics, 1-3 type composites as a material of ultrasound transducers could effectively suppress the lateral vibration of the material and enhance the thickness vibration mode, which could improve the pulse echo response. The DLP technology with a high resolution provides an effective and low-cost method for fabricating the piezoelectric composites.

  • Teng ZHANG, Yuan ZHANG, Dahua REN, Qiang LI, Jiying YU, Jinneng ZHOU, Jinqiao YI
    Journal of the Chinese Ceramic Society. 2024, 52(1): 161-169.
    Introduction

    Ga2O3 is an ultra-wide bandgap semiconductor, which has a direct bandgap of 4.9 eV. Also, it has the superior thermodynamic and chemical stability, making it suitable for the development of deep ultraviolet optoelectronic devices. Ga2O3 exhibits the superior photosensitive and resistive properties, which has a promising application in sensor-memory integrated optoelectronic devices. In this paper, the crystal structure, composition, and morphology of the Ga2O3 thin film grown via pulsed laser deposition (PLD) was discussed, and then an optoelectronic device with Pt/Ga2O3/NSTO/In structure was designed and constructed. The physical mechanism of the Ga2O3-based device was investigated. The device process was optimized to achieve both high sensitivity ultraviolet photo-response and stable resistive switching characteristics. This work can provide theoretical guidance and technical support for the development of novel Ga2O3-based multifunctional optoelectronic devices.

    Methods

    Ga2O3 thin films were grown on (100) Nd∶ SrTiO3 (NSTO) substrates by the PLD method. The target material used was a pure Ga2O3 ceramic target prepared by a solid-state method. Before thin film deposition, the ceramic target was pre-ablated for 3 min to remove surface contaminants. The film deposition was performed at pulse laser energy of 300 mJ, O2 partial pressure of 3.0 Pa, and substrate temperature of 650 ℃. The target rotation speed was 5 r/min, the substrate rotation speed was 10 r/min, the pulse laser frequency was 5 Hz, and the deposition time was 30 min. Based on the deposited Ga2O3 thin films, a device with metal/Ga2O3/electrode sandwich structure was further constructed. At room temperature, Pt metal dot electrodes were fabricated on the surface of Ga2O3 thin films by a DC magnetron sputtering method as a top electrode of the device, and then weld the metal indium (In) directly onto the back of the NSTO substrate as a bottom contact electrode. The above Pt metal electrode preparation process was run at DC source power of 100 W, working pressure of 1.5 Pa, Ar flow rate of 10 mL/min, substrate rotation of 10 r/min, and sputtering time of 60 s.

    The structure of Ga2O3 thin films was characterized by a model D8 Discover type high-resolution four circle single crystal X-ray diffractometer. The elemental composition of Ga2O3 thin film material was analyzed by a model Escalab 250Xi X-ray photoelectron spectroscope. The surface and cross-sectional morphology of the films was characterized by a model Sigma 500 field emission scanning electron microscope. A semiconductor electrical performance testing system was constructed by a model Keithley 2635 digital source meter, probe station, and electromagnetic shielding dark box, to examine the I-V scanning loop, multi-level resistive state, retention, and fatigue resistance characteristics of the device. A 255 nm LED light source was driven by a digital signal generator to test the time-dependent UV photoresponse characteristics. A Omni-λ 3027 setup consisting of monochromator, 150 W xenon lamp light source, chopper, collimating light converter, and phase-locked amplifier, was utilized to measure the dark current, spectral response, UV-visible suppression ratio, and detectivity of the photodetector.

    Results and discussion

    The deposited β-Ga2O3 film with small particles and a flat and dense surface exhibits (004) plane preferential orientation. The Pt/Ga2O3/NSTO/In device with both fast self-driven ultraviolet photoresponse and stable resistive switching characteristics was fabricated. Under illumination, the photocurrent of the device rapidly increases to its maximum value and then gradually decreases to a steady state possibly due to the reduction in the Schottky junction built-in electric field caused by the injection of photogenerated carriers into the barrier region. The self-driven photoresponse is attributed to the efficient separation of photo-generated carriers by a built-in electric field formed at the Pt/Ga2O3 interface. On the other side, the device exhibits a stable bipolar resistive switching behavior. Alternating -5 V and +3 V pulse voltages with a 10 ms pulse width results in a resistive switching ratio of nearly 104. A rapid switching between multi-level resistance states occurs at different pulse voltages. The intrinsic oxygen vacancy defect in Ga2O3 thin film as the trap center dominates the capture/release process of charge carriers, thereby maintaining the resistance state. Changing the pulse voltage can control the amount of electron injection, thus affecting the height of the interface barrier, which can explain the multi-level resistive characteristics of the device. The resistance state shows a good retention, and there is no significant degradation within 104 s, showing the nonvolatile characteristics. In addition, the device also exhibits stable and fast switching characteristics after multiple repeats, indicating potential applications in memory devices. The mechanism of resistive switching effect can be attributed to the interface type resistance mechanism. The variation of the Schottky barrier caused by external electrical injection and the carrier trapping/detrapping process caused by the oxygen vacancy defect trap center jointly determine the resistive switching effect.

    Conclusions

    The fabricated device had a fast UV photoresponse (τr/τd=60 ms/120 ms) with a peak responsivity of 13.4 mA/W and 1.49×1011 Jones (λ=250 nm) at 0 V bias. According to the analysis, the Schottky contact formed at the Pt/Ga2O3 interface resulted in a fast self-driven photoresponse at 0 V bias. In addition, the fabricated device also exhibited a stable bipolar resistive switching behavior with a high/low resistance ratio of 104. The fast switching between multiple resistance state was achieved with the superior anti-fatigue and retention characteristics at different pulse voltages. The external electric field and oxygen-vacancy trap centers was considered as the main origin of resistive switching effect in Ga2O3-based optoelectronic device.

  • Xiangnan KANG, Shengxu ZHONG, Rui DING, Jun MA, Liang LI, Yuqin ZHU
    Journal of the Chinese Ceramic Society. 2024, 52(1): 170-179.
    Introduction

    Machinery and equipment are prone to equipment failure and even safety accidents caused by insufficient lubrication under severe working conditions. Adding additives with some superior performance in lubricant is an effective approach to improve the lubricant performance, reduce the friction and wear, and extend the service life of machinery. Lubricants are widely used in machinery and equipment as an important method of anti-wear and friction reduction. Silicate minerals are harmless to the environment and the humanbeing. A low roughness, high hardness friction reaction film can be formed by silicate minerals as lubricant additives during the lubrication process, which can effectively reduce wear. Organic molybdenum as a commonly used lubricant additive has superior antioxidant properties, and can decompose when pressure, temperature and other conditions meet the requirements, and then lead to a chemical reaction and form the protective film containing molybdenum elements, thus preventing the surface oxidation reactions to improve the tribological properties of the lubricant. In this paper, the friction and wear reduction properties of composite lubricant additives of montmorillonite (MMT) and organomolybdenum were investigated to obtain superior lubrication, thereby improving the operational stability and safety of machinery and equipment under severe operating conditions.

    Methods

    The lubrication performance of three molybdenum-based lubricants, i.e., MoDDP (C28H60O4P2S4Mo), MoDTC (C34H72Mo2N2O2S6) and RS-568, was evaluated by a four-ball friction and wear tester to determine the organic molybdenum type and the optimal mass fraction of organic molybdenum in the composite lubricant additives. Tribological tests were then carried out on lubricant samples at different concentrations of MMT to determine the optimal mass fraction of MMT in the composite additives. After the preparation of the composite additive, the lubricating properties of the MMT/MoDDP composite additives were examined, and the friction reduction and anti-wear mechanism of the composite additive was investigated by energy dispersive spectroscopy, X-ray photoelectron spectroscopyand Raman spectroscopy.

    Results and discussion

    The results show that among the organic molybdenum additives, molybdenum dialkyldithiophosphate (MoDDP) exhibits the optimum lubricant properties. The friction coefficient and wear spot diameter firstly decrease and then increase with the increase in the mass fraction of MMT and MoDDP in the oil, and the optimal mass fractions of MMT and MoDDP are 3.0% and 1.5%, respectively. Compared with the base oil, the friction coefficient is reduced by 41.0% and the wear spot diameteris decreased by 48.9% for oil sample at 1.5% MoDDP, and the friction coefficient is reduced by 40.6% and the wear spot diameter is decreased by 48.2% for the oil sample at 3.0% MMT.

    Compared with the oil samples at 3.0% MMT, the friction coefficient and the wear spot diameter was reduced by 26.3% and 7.9%, respectively, for the oil sample with the composite additives. Compared with the oil samples at 1.5% MoDDP, the friction coefficient and the wear spot diameter are reduced by 26.6% and 6.6%, respectively, for the oil sample with the composite additives. The 3.0% MMT/1.5% MoDDP composite lubricant additives can further improve the friction reduction and anti-wear performance of the lubricant. Compared with the base oil, the friction coefficient and wear spot diameter are reduced by 56.3% and 52.3%, respectively, for the oil sample with the composite additives.

    During the friction process, a SiO2 physical adsorption film was deposited on the friction surface due to the adsorption property of MMT additives. Under the action of shear force, the layered MMT particles are subjected to shear, resulting in an interlayer slip, which can reduce the friction between the contact surfaces. The fractured MMT particles are mechanically filled in the surface wear area to improve the carrying capacity of the oil film. Moreover, a layered MoS2 film with a low shear strength and a high melting point can be generated due to the chemical reaction of the MoDDP additive. Also, the MoO2, FeS2, Fe2O3 metal compound reaction film can be generated to prevent the direct contact of the friction interfaces. Although the single additive has a great lubrication effect, the MMT and MoDDP composite additives show a better lubrication performance and synergistic effects in the friction process. The composite metal compound layer and the physical adsorption film can be generated during friction to form the high load-bearing capacity of the lubricant film, thus increasing the strength and stability of the lubricant film, and it was able to continuously and effectively reduce friction and wear. The friction tests also verify that MoDDP and MMT have a positive synergistic effect in the friction process. During the lubrication process, chemical reaction films with MoS2, MoO2, FeS2, and Fe2O3 and SiO2 physical adsorption films were generated, thus effectively reducing thefriction and wear.

    Conclusions

    The 3.0% (in mass fraction) MMT/1.5% (in mass fraction) MoDDP composite additives exhibited the better lubricating properties, compared with a single additive. It was indicated that the MMT/MoDDP composite lubricant underwent a chemical reaction during the friction process, which produced molybdenum sulfides and oxides containing molybdenum (MoS2, MoO2) and iron sulfides and oxides containing FeS2, Fe2O3, as well as physically adsorbent films containing SiO2. The compound lubrication film could effectively reduce the friction of the interface.

  • Gang LU, Longhua LUO, Xiao CHEN, Qingsong YAN, Hang YU, Yisi CHEN, Yongguang GUO
    Journal of the Chinese Ceramic Society. 2024, 52(1): 180-188.
    Introduction

    With the increasing demand for turbine engine performance, turbine blade structure becomes increasingly complex. The investment of precision casting ceramic core is a serious challenge. The existing solubility is the most important issue restricting the application of alumina-based ceramic cores. Increasing the porosity can enhance the substrate material and the interaction of chemical solutions. The main research direction is to improve the corrosion performance of alumina-based ceramic core. However, the increase of porosity will cause the core strength to plummet, affecting the performance of alumina-based ceramic core. To meet the requirements of investment casting, the organic-inorganic hybrid fiber can improve the porosity and strength of alumna-based ceramic core system. The synergic strengthening mechanism of hybrid fiber modified aluminum ceramic cores pore-system was investigated.

    Methods

    Capacitive corundum powder, fused mullite, and quartz glass powder were used as matrix material, mineralizer, and firing aid, respectively. Meanwhile, organic short-cut fiber as a pore-making agent, inorganic short-cut alumina fiber as reinforcement, coupling agent solution, and hydroxypropyl methylcellulose modified fiber were used to prepare alumina ceramic cores with different hybrid fiber ratios via hot pressing injection. According to aviation industry standard HB 5353.1-3—2004, the key performance parameters of each core sample were obtained. A scanning electron microscope was used to observe the pore characteristics, fracture morphology, and fiber distribution of the core, and analyze the fiber fracture mode. The synergic strengthening mechanism and the pore strength of the hybrid fiber-modified alumina-based ceramic core were investigated.

    Results and discussion

    The introduction of hybrid fibers changes the pore characteristics of the alumina-based ceramic core, and irregularly connected pores and nearly circular closed pores appear in the ceramic core. The fracture mode of the alumina-based ceramic core changes from "transcrystalline fracture" of like-metal to "intergranular fracture" as the proportion of hybrid fibers decreases.

    The addition of hybrid fiber reduces the sintering shrinkage rate of the alumina-based ceramic core, the shrinkage rate of the sample NA67 is only 0.2%. For the comparison, the rate is reduced by 77.8% for the sample NA60 without alumina fibers, which may be since an appropriate amount of alumina fiber can effectively increase the center separation of sintered particles, hinder the migration and diffusion of substances, offset the sintering shrinkage stress, and inhibit the sintering shrinkage of the core. The mass-burn loss of alumina-based ceramic core is 19.5% as the proportion of hybrid fibers decreases. As the mass loss mainly comes from the oxidation burn loss of plasticizer and nylon fiber, the alumina fiber has an impact on the migration of crystal water in the sintering process, so the mass-burn loss rate fluctuates slightly.

    The number of large pores in the aluminum ceramic core increases, the number of small pores decreases, and the apparent pores in the ceramic core firstly increase and then become stable with the decrease in the proportion of hybrid fibers. Small-aperture pores are mainly composed of closed pores lost by chopped organic nylon fiber (Nsf) fiber, while large-aperture pores are mainly connected pores formed by chopped inorganic alumina fiber (Asf) crossing closed pores when the hybrid fiber ratio is less than 6∶7. The apparent porosity of the core tends to be stable at 43.31% because the intersected Asf fibers are clustered among the sintered particles. The effect of Asf fibers on the increase of the distance between the sintered particles becomes slight, the number and size of connected pores in the ceramic core almost unchange, and the apparent porosity tends to be stable.

    The bending strength of the alumina-based ceramic core increases firstly and then decreases as the proportion of hybrid fiber decreases. This is because the appropriate amount of Asf fiber effectively increases the fiber-matrix interface bonding area. When the core is subjected to external loads, Asf fiber consumes the more crack propagation energy through the behavior of debonding, fracture, and pull-out, and the bending strength of cores increases significantly. The excessive Asf fiber is unevenly dispersed in the matrix material, dividing the matrix, reducing the interface bonding area between the agglomerated fiber and the core matrix, weakening the strengthening effect of the fiber on the core, and leading to a slight decline in the bending strength of the core.

    Conclusions

    The shrinkage rate of the alumina-based ceramic core decreased after firing as the hybrid Nsf/Asf fiber ratio decreased. The Asf fibers interspersed in the core matrix effectively hindered the diffusion and migration of sintered particles and reduced the core densification. The shrinkage rate of the sample NA67 after firing was 0.2% when the hybrid fiber ratio was 6∶7, which was 77.8% lower than that of the sample NA60 without hybrid fiber, showing a good dimensional stability.

    The increase of apparent porosity of hybrid fiber reinforced alumina-based ceramic core was mainly due to the loss of residual closed porosity by oxidation of Nsf fiber at a high temperature and the formation of connected porosity by Asf fiber interpenetrating matrix. The number of connected pores, the volume proportion of open pores and the apparent porosity increased, while the volume density decreased as the hybrid fiber proportion decreased.

    An appropriate amount of Asf fiber consumed the crack propagation energy through the mechanism of de-bonding, pulling out, and breaking, and improved the bending strength of alumina-based ceramic core, effectively making up for the strength loss caused by in-situ burning of Nsf. The bending strength of the alumina-based ceramic core reached a maximum value of 20.1 MPa when the hybrid fiber ratio was 6∶7. However, the agglomeration and cross of Asf fibers could form some penetrating cracks in the core matrix and cut the matrix, affecting the strengthening effect of the fibers when the proportion of hybrid fibers further decreased.

  • Zhou ZHANG, Gang MA, Jiayin ZHANG, Sizhe DU, Yakun CHANG, Bo LI
    Journal of the Chinese Ceramic Society. 2024, 52(1): 189-202.
    Introduction

    Ordinary concrete rapidly loses its bearing capacity under impact, while the addition of steel fibers effectively enhances the overall integrity and matrix toughness of concrete, thus meeting the concrete performance requirements of high strength, high durability, and high toughness in practical engineering. The existing work on the strengthening and toughening mechanism and failure mechanism of steel fiber reinforced concrete is mainly based on the macroscopic experiments. It is thus difficult to reflect the randomness and non-uniformity of concrete. In this paper, the dynamic response of steel fiber reinforced concrete beam specimens at a low-speed impact was investigated by a drop hammer testing machine to comprehensively reveal the internal damage and failure process of concrete and the toughening mechanism of steel fibers. A three-dimensional microscopic model of steel fiber reinforced concrete beams was proposed, and the mechanical properties and crack development of steel fiber reinforced concrete beams under dynamic impact were analyzed. In addition, the effects of steel fiber volume fraction and impact velocity on the impact resistance and failure morphology of steel fiber reinforced concrete beams were also discussed.

    Methods

    Steel fiber reinforced concrete beams with different steel fiber volume fractions (i.e., 0%, 0.5%, 1.0%, 1.5%, 2.0%, and 2.5%) were prepared based on the experimental mix proportion. The effect of steel fiber volume fraction on the impact performance of steel fiber reinforced concrete beams was analyzed via dynamic three-point bending performance in a model INSTRON-9530 drop hammer impact testing machine.

    A steel fiber model was randomly proposed based on the Monte Carlo method, and a spring element was used to simulate the bond slip between steel fibers and concrete matrix. Based on its bond slip relationship, a three-dimensional fine calculation model for steel fiber concrete was established. The dynamic response and failure forms of steel fiber concrete were simulated at different volume fractions (i.e., 0%, 0.5%, 1.0%, 1.5%, 2.0%) and different impact rates (i.e., 1, 2, 3, 4, 5, 10, 20 m/s), respectively, The effects of steel fiber content and impact rate on the impact resistance and failure morphology of steel fiber reinforced concrete beams were analyzed.

    Results and discussion

    The drop hammer impact test is widely used to test the dynamic bending performance of concrete beams, but the hammer impact force measured by a hammer force sensor is not an actual impact force due to its inclusion of structural inertia force. In the low-speed impact test of steel fiber reinforced concrete beams, this study integrated some force sensors with roller bearings to accurately obtain the support reaction force of the beam during the impact process and reduce the influence of inertial force, thereby revealing the true dynamic response of the tested specimens.

    The key to improving the mechanical properties of fiber reinforced materials lies in the micro bridging effect of fibers on the concrete matrix. Steel fiber exhibit a large number and random distribution in the concrete matrix, making it difficult to quantitatively evaluate the fiber reinforcement effect at an impact load. This study used the Monte Carlo method to propose a fiber microscopic model and determine the range based on the unique three-dimensional position and direction information of each fiber. The numerical analysis methods were used to more intuitively clarify the deformation and damage situation of steel fibers and concrete matrix during the impact process to obtain the accurate energy quantification evaluation.

    The key to improving the mechanical properties of steel fiber reinforced concrete lies in the bond slip between steel fibers and concrete matrix. Simulating the bond slip between concrete matrix and steel fibers accurately becomes a key to simulating steel fiber reinforced concrete. In this paper, spring elements were used to simulate steel fibers. The stiffness of the spring element adopts a "two-stage" model. The simulation data by the model are in reasonable agreement with the experimental results.

    Conclusions

    The simulation data of three-dimensional steel fiber reinforced concrete beams based on bonded slip spring elements were in reasonable agreement with the experimental results.

    The bearing capacity and energy dissipation capacity of steel fiber reinforced concrete beams increased with the increase of steel fiber volume fraction when the fiber volume fraction was small. The peak impact force of the concrete beam was increased by 16.71% at the optimal dosage of steel fiber of 1.5%. However, the energy dissipation capacity and impact resistance of steel fiber reinforced concrete beams decreased as the volume fraction of steel fibers further increased.

    The bearing capacity of steel fiber reinforced concrete beams was positively correlated to the rate when the impact rate was in the range of 1 m/s to 20 m/s. The peak impact force of steel fiber reinforced concrete beams increased, but the reinforcement effect of steel fiber on the steel fiber reinforced concrete gradually weakened as the rate continues to increased. The reinforcement effect of steel fiber was slight when the rate increased to 20 m/s. Therefore, for steel fibers with a length of 12.5 mm and an aspect ratio of 20, their enhancement effect on the dynamic mechanical properties of concrete beams was more significant in a low-speed impact range of less than 10 m/s.

  • Zhiyuan LIU, Xicheng GUAN, Zhou LI, Ni MA, Junjie MA, Qian BA, Ailin XIA, Chuangui JIN
    Journal of the Chinese Ceramic Society. 2024, 52(1): 203-217.

    Bi2Te3 based alloys have attracted considerable attention in low-temperature thermoelectric materials due to their superior electrical transport properties and low thermal conductivity. However, the conversion efficiency of thermoelectric power generation or refrigeration devices made of Bi2Te3-based alloys is still low. It is thus crucial to further improve the thermoelectric figure of merit zT of Bi2Te3 based materials. There are some correlations between lattice thermal conductivity and electrical performance parameter. Reducing the lattice thermal conductivity by phonon engineering becomes an important method to increase zT without deteriorating the electrical performance. This review summarized the main research progress in recent years to optimize the thermoelectric properties of Bi2Te3 based materials by phonon engineering, such as nano-modification, superlattice structure, nanocomposing, doping and adding dislocation arrays. The effect of the optimization method on the specific heat capacity, phonon group velocity and phonon mean free path was discussed. The specific heat capacity, phonon group velocity or phonon mean free path of Bi2Te3 based materials can be significantly reduced by the optimization methods. As a result, the lattice thermal conductivity of Bi2Te3 based materials is significantly reduced, leading to a significant increase in the thermoelectric properties.

    Nano-modification: The interface density is increased via low dimensionalization and grain refinement, resulting in an enhanced scattering of low-frequency phonons, reduced phonon mean free path and phonon group velocity, significantly reducing the lattice thermal conductivity. Nowadays, the grain size and morphology of Bi2Te3-based alloys can be precisely controlled by mechanical milling, MBE method, hydrothermal method, chemical vapour deposition and wet chemical method. Bi2Te3 nanostructures with a ultra-low grain size can be prepared. However, heat conduction cannot be completely prevented even at rather small sizes due to the incomplete suppression of low-frequency phonons. Therefore, it is difficult to improve zT by a single low-dimensionalisation and grain refinement method. The specific surface area can be increased either by combining the phases of different nanostructures to form a heterogeneous interface or by introducing special nanostructures such as twins and nanopores, which can strongly scatter the low-frequency phonons caused by lattice mismatch and lattice vibration, and further reduce the lattice thermal conductivity.

    Bi2Te3-based superlattice structure: Furthermore, in the microscopic and mesoscopic scales, the superlattice structure generated by artificially controlling the ordered arrangement of atomic layers of Bi2Te3-based materials is considered as the optimum candidate material to achieve the 'phonon glass-electron crystal' thermoelectric material standard. Especifically, the quantum well structure in the thin film superlattice produces an intense boundary scattering effect and a quantum confinement effect on phonons, resulting in a decrease in the mean free path and group velocity of phonons, greatly reducing the thermal conductivity of Bi2Te3-based thermoelectric materials. The bulk superlattice structure of the Bi2Te3-based alloy relies on its complex crystal structure and acousto-optic coupling effect, causing a low cut-off frequency of phonon mode and an intense phonon resonance scattering, and resulting in a low intrinsic thermal conductivity. In addition, the low phonon group velocity caused by chemical bond softening and lattice anharmonicity is also a reason for the low intrinsic thermal conductivity of the bulk superlattice structure of Bi2Te3-based alloy.

    Nanocomposites, doping modification and dislocation arrays: Nanocomposite and doping modification are the main approaches to improve the thermoelectric properties of Bi2Te3-based materials. In the nanocomposite process, the nanoparticles dispersed in the thermoelectric material do not enter the matrix lattice, but attach onto the surface of the matrix grain, forming a heterogeneous interface with the matrix. Also, introducing nanoparticles increases the grain boundary density, resulting in a further scattering of low frequency phonons. Doping modification is achieved by doping elements entering the Bi2Te3 lattice, replacing Bi site (or Te site) or entering the van der Waals gap for interstitial doping. This process can introduce multiple scattering centers such as grain boundaries, point defects, in-situ precipitates and dislocations into Bi2Te3-based alloy, enhancing a multi-scale scattering of phonons and effectively reducing the mean free path of phonons. Combined with the preparation process such as sintering, the dislocation array is increased, which leads to a higher scattering intensity of intermediate frequency phonons, further reducing the lattice thermal conductivity.

    Summary and prospects

    The phonon specific heat capacity, phonon group velocity and mean free path of the Bi2Te3-based alloy could be effectively controlled by phonon engineering including nano-modification, superlattice structure, nanocomposite, doping and introduction of the dislocation array to achieve a sufficiently low lattice thermal conductivity. The electrical transport properties were optimized by the carrier engineering and energy band engineering techniques, and the synergistic regulation of the electrical and thermal transport properties was realized. As a result, the thermoelectric properties of Bi2Te3-based alloys were significantly improved. This provided a scientific and technical support for the application of thermoelectric devices. However, a lot of work remained in improving the thermoelectric properties of Bi2Te3 materials by phonon, carrier and energy band engineering. Nevertheless, the large-scale commercialization of Bi2Te3-based alloys as thermoelectric materials still attracts much attention. Also, interdisciplinary research in thermoelectricity and other disciplines becomes popular. The future research and large-scale application of Bi2Te3 thermoelectric materials are expected.

  • Zixing WANG, Jiajia LI, Ying LIU, Kefeng CAI
    Journal of the Chinese Ceramic Society. 2024, 52(1): 218-228.

    Thermoelectric (TE) materials as one of clean energy materials can realize the direct conversion between heat and electricity. Flexible TE films have attracted recent attention because they can be used to fabricate flexible TE generators (f-TEGs) to replace batteries that need to be charged or replaced frequently to power rapidly developing wearable electronic devices. Bi2Te3-based films exhibit the optimum TE performance at room temperature (RT), but Bi2Te3-based films are easy to oxidize, and Te is expensive, rare, and toxic, so suitable alternatives need to be explored. Silver selenide (Ag2Se) is a narrow bandgap semiconductor and has a superior TE performance at RT. Furthermore, compared with element Te, element Se is less toxic and more abundant. However, the TE properties of Ag2Se are still lower than that of Bi2Te3. This review summarized the mechanism of improving the TE properties and flexibility of Ag2Se by functional unit order strategy, and provided a route to enhance the TE properties and flexibility of Ag2Se.

    Typical strategies for improving the zT values of Ag2Se-based films include the introduction of secondary phase, defect engineering, stoichiometry manipulation, etc.. However, charge carrier and phonon transport in TE material are strongly coupled with each other, seriously restricting the improvement of TE performance. The functional unit order is an effective strategy to optimize the performance of materials. Functional units with different roles constructed orderly in materials can enhance a synergistic effect between functional units and thus improve the performance. For Ag2Se-based flexible TE films, the effect of functional unit ordering and the synergetic effect between functional units on the electronic, phonon transport, and flexibility were discussed. The S-doped Ag2Se film shows a power factor ~954 μW·m-1·K-2 at 300 K and superior flexibility (94.4% of the original electrical conductivity was preserved after bending for 2 000 times around a rod with a radius of 4 mm). The S-doped Ag2Se film consists of a special "core-shell" microstructure, namely, the "core" is an S-doped Ag2Se phase and the "shell" (thickness of 15 nm) is Se-doped Ag2S and amorphous S mixed phase. The formation of the "core-shell" microstructure is mainly due to the different affinities between Ag and Se and Ag and S. The "core" acts as TE functional units because of the well-preserved conductive paths formed by well-crystallized S-doped Ag2Se grains, thus maintaining a high electrical conductivity of the film. The "shell" acts as a flexible functional unit to enhance the flexibility of the film mainly due to the inherently flexible amorphous S phase and the ductile Se-doped Ag2S. Moreover, the thermal conductivity of the film is low because of the strengthened phonon scattering resulting from the hetero-interfaces and the intrinsically low thermal conductivity of the amorphous S phase and the Se-doped Ag2S nanograins.

    The Ag2Se/PVP composite film has a high power factor of ~1 910 μW·m-1·K-2 and a superior flexibility at 300 K. Most Ag2Se grains with coherent interfaces in the Ag2Se/PVP composite film indicate that the Ag2Se TE functional unit is constructed, leading to a high electrical conductivity. The formation of the unique microstructure is related to the special sintering mechanism and the effect of PVP. The superior flexibility (i.e., 98% of the original electrical conductivity is preserved after bending for 1 000 times around a rod with a radius of 4 mm) is due to the good adhesion and viscosity of PVP acting as a flexible functional unit. The composite film has a pretty low thermal conductivity because of PVP with an extremely low intrinsic thermal conductivity and it contains numerous nano-sized- to micron-sized-pores and Ag2Se/PVP hetero-interfaces.

    The Ag2Se/Se/PPy composite film has an exceptionally high power factor of ~2 240 μW·m-1·K-2 and excellent flexibility at 300 K. The Ag2Se/Se/PPy composite film has a superior crystallinity of Ag2Se grains and continuous grain boundaries without defects, indicating that the Ag2Se TE functional unit is constructed, leading to a high electrical conductivity. There exist energy-filtering effects at the heterointerfaces of Ag2Se/Se and Ag2Se/PPy in the film, leading to a high Seebeck coefficient. The formation of the unique microstructure is related to the special sintering mechanism. The superior flexibility (i.e., 92.5% of the original electrical conductivity is preserved after bending for 1 500 times around a rod with a radius of 4 mm) is due to the good adhesion and viscosity of PPy acting as a flexible functional unit. Moreover, the nano-sized to submicron-sized pores, and the Ag2Se/PPy and Ag2Se/Se heterointerfaces in the composite film can scatter short- to long-wavelength phonons because PPy has an intrinsic low thermal conductivity, the composite film has a low thermal conductivity.

    Summary and prospects

    The functional unit order is an effective strategy to optimize the performance of materials. For Ag2Se-based TE films, the TE functional units ordering (such as coherent adjacent Ag2Se grains, good crystalline qualities, continuous grain boundaries, and core-shell nanostructure) and flexible functional units were constructed in Ag2Se-based films. The effective regulation of electron and phonon transport and flexibility was realized due to the synergistic effect between different functional units, thus increasing the electrical conductivity, reducing the thermal conductivity, and improving the flexibility. The more work are needed to verify whether the relevant strategies are universal.

  • Dekun SHEN, Zihan YANG, Peiyuan GUO, Mengling ZHAO, Jian GE, Gongxun DENG, Aiji WANG
    Journal of the Chinese Ceramic Society. 2024, 52(1): 229-239.

    Conventional metal materials affect the development of microwave integrated circuits, while the use of microwave electric materials can achieve the miniaturization and high-performance requirements. With the continuous exploration of modern microwave communication technology, microwave devices will face some opportunities and challenges like multi-frequency, and multi-mode capabilities. Tunable microwave devices are also an essential core of phased array radar and modern mobile technology, with the broad application prospects.

    BaxSr1-xTiO3 (BST) film material is considered as one of the most materials for tunable microwave devices due to its high dielectric tunability and low dielectric loss with a high figure of merit (FOM). However, BST thin film material still has some problems in applications, such as the synergistic optimization of tunability and dielectric loss, as well as temperature stability. To optimize the performance of films, the dielectric properties are adjusted through the improved preparation processes, annealing modification, controlled composition ratio, and doping modification as well. These optimization measures provide some opportunities for the design and preparation of microwave devices based on the BST films.

    To investigate the dielectric properties of BST thin film, high-annealing in the preparation process can repair defects and improve grain growth, while controlling growth atmosphere can optimize the surface roughness and grain boundary characteristics of the film. Selecting appropriate substrates or inserting buffer to control stress can optimize the film structure and improve the dielectric performance. In addition, the Ba/Sr/Ti molar ratio regulation has a significant impact on the ferro-dielectric properties (i.e., the Curie temperature) of the film. The use of oxide molecular beam epitaxy (MBE) can achieve a better stoichiometric control and a low defect density. Doping regulation can change the lattice parameters and ion interactions of BST films. Some methods such as acceptor doping donor doping, and multicomponent doping are used. For instance, the FOM of La/Fe co-doped Ba0.65Sr0.35TiO3 films prepared by a solid-phase reaction is increase by 5 times, compared to pure BST. The super lattice structures prepared by alternate doping and the multilayer films prepared by different material combinations indicate better comprehensive dielectric properties.

    The BST thin film materials have nonlinear characteristics, in which the dielectric constant changes with the applied electric field, and these dielectric properties play an important role as parameter indicators in microwaveable devices. It is indicated that the oxide bottom electrode is of great significance to improve the performance of BST thin film variable capacitors in high-frequency applications. The BST film capacitors with SrMoO3 (SMO) oxide was designed as a bottom electrode instead of conventional precious metal electrode materials, which avoids an acoustic resonance at high frequencies. Using the BST tunable filters instead of conventional filters composed of multiple filters is more in line with the needs of miniaturized and integrated devices in radar and communication fields. However, current research is limited due to the high insertion losses in practical devices, and reducing the insertion losses remains an important issue for BST-based microwave devices. Some phase shifters made using BST films were reported, demonstrating a large phase shift range and a high figure-of-merit, and achieving continuous tunable phase shift capability at different frequency ranges. Film phase shifters are applied in antenna arrays and end-fire arrays, realizing radiation directionality steering and linear beam scanning, thus promoting the development of radar and antenna systems. The power oscillators using BST films and single-chip AlGaN/GaN high electron mobility transistors voltage controlled oscillator were reported, showing the potential of BST films in the field of microwave oscillators.

    Summary and prospects

    The dielectric properties were reduced via optimizing film growth conditions. However, some related problems were not solved, i.e., decoupling the physical mechanism of dielectric tunability and dielectric loss, and the optimization of high-frequency film dielectric performance testing and extraction. In terms of microwave devices, more efforts need to be made in microwave device design, simulation, preparation, and testing. In summary, to commercialize ferroelectric thin film-based tunable microwave devices, we need to clarify the physical mechanisms of thin film dielectric properties, optimize the growth conditions preparation processes (i.e., synergistic optimization of dielectric tunability and dielectric loss), and obtain high-quality films, thus laying a foundation for the application prospects of tunable microwave devices.

  • Xueqi XING, Yu NI, Zekai WANG, Hongyu LU, Xiaoxia JIANG, Ning BAI
    Journal of the Chinese Ceramic Society. 2024, 52(1): 240-254.

    Solid-state lithium-ion batteries (SSLBs) are one of the most promising next-generation batteries due to their excellent safety, higher energy density and longer cycle life. Solid-state electrolytes (SSEs) with a high ionic conductivity, a wide electrochemical window, and good mechanical properties are the importance of the high-performance SSLBs. The organic polymer SSEs have some advantages of flexibility and good mechanical property, that makes them almost have no serious interfacial problems. However, the low ionic conductivity is a major drawback for most polymer SSEs. Inorganic SSEs show a high ionic conductivity, a good electrochemical stability, and a high thermal stability, but their main disadvantages are a weak mechanical property (i.e., brittle and fragile), a poor air stability and an inferior compatibility with metal lithium anode. Compared to inorganic and organic polymer SSEs, composite solid-state electrolytes (CSSEs) integrating the merits of organic polymers and inorganic electrolytes exhibit a good electrochemical performance and an excellent interface compatibility, which have attracted extensive attention in the SSEs research. This review detailly summarized the research progress on CSSEs in lithium batteries.

    The CSSEs are usually composed of inorganic fillers, organic polymers and lithium salts. The inorganic fillers are classified into inert and active fillers. The inert fillers, such as SiO2, Al2O3 and TiO2, do not transport Li+ themselves, but can promote the ionic properties of polymer matrices. The active fillers conduct Li+ themselves including oxides (i.e., perovskite-type, garnet-type, NASICON-type), sulfides, and halides, etc.. Lithium salts used for the investigation of CSSEs include LiPF6, LiBF4 and LiN(CF3SO2)2(LiTFSI), etc..

    The first CSSE with an inert filler was prepared via introducing an Al2O3 into a matrix, thus improving the mechanical property of LiClO4/PEO CSSEs at 100 ℃. SiO2 and TiO2 were a commonly used inert ceramic filler for the fabrication of CSSEs. The content, particle size and shape of metal oxide inert fillers affect the performance of CSSEs. The layered nano-sized claylike montmorillonite (MMT) as a passive filler was doped into polyvinylidene fluoride (PVDF)-hexafluoropropylene (HFP) polymer to prepare a ultraviolet (UV)-crosslinked MMT/PVDF-HFP membrane, having a room-temperature ionic conductivity of 1.6×10-3 S/cm. Carbon materials were also served as inert fillers to prepare CSSEs.

    The CSSEs with active fillers were synthesized via adding active fillers to polymers. Li0.5La0.5TiO3 (LLTO) is a typical perovskite-type active filler. The reduction of Ti ions in LLTO with lithium was prevented as combining LLZO with polymers, and the LLZO CSSEs exhibited a wide electrochemical window and a good stability. For instance, a PVDF polymer CSSEs with LLTO nanowires delivers a room temperature ion conductivity of 5.8×10-4 S/cm, an electrochemical window of 5.2 V, and a mechanical strength of 10 MPa. The cell of Li|PVDF/LLTO-15%/Li+|LiFePO4 (LFP) has a superior Coulomb efficiency of approaching 100% after 200 cycles. The garnet-type active filler Li7La3Zr2O12 (LLZO) and Li6.4La3Zr1.4Ta0.6O12 (LLZTO) were divided into zero-dimensional nanoparticles, one-dimensional nanowires and nanotubes, two-dimensional nanosheets, and three-dimensional structures according to the geometric structures. For instance, a LLZTO/PEO CSSEs was prepared by dispersing a zero-dimensional LLZTO powder into acetonitrile solution of PEO/LiTFSI. The room-temperature ion conductivity and electrochemical stability window of LLZTO/PEO CSSEs are 4.76×10-4 S/cm and 4.75 V, respectively. The multi-mixing CSSE membrane consisting of LLZTO, PEO, PVDF-HFP, and LiTFSI has a high ionic conductivity of 1.05×10-4 S/cm at 35 ℃, an electrochemical window of 5.2 V, and a high Li+ transference number of 0.52 at 60 ℃. A three-dimensional PVDF/LLZO/LiClO4 CSSEs was obtained by adding 3D coral-like LLZO nanofiller into PVDF/LiClO4. This CSSE membrane structured 3D interconnected framework has an enhanced ionic conductivity of 1.51×10-4 S/cm at room temperature. The assembled battery delivers a capacity retention of 95.2% after 200 cycles at 1 C. The NASICON-type Li1.3Al0.3Ti1.7(PO4)3 (LATP) and Li1.5Al0.5Ge1.5(PO4)3 (LAGP) ceramics as active fillers were added into PEO and PVDF-HFP polymers. A PVDF-HFP/LiTFSI CSSE containing 50% (in mass fraction) LAGP displays the maximum ionic conductivity of 9.2×10-4 to 9.6×10-4 S/cm at room temperature. After 50 cycles, the cell with PVDF-HFP/50% LAGP/LiTFSI CSSE remains 141.3 mA·h/g and a capacity retention rate of 89.5%.

    Besides, sulfide fillers were investigated. However, sulfides are instability in air because it intrinsically tends to react with moisture to generate toxic H2S gas. The CSSEs prepared with sulfide fillers improve asulfide stability and offer a high ion conductivity. For instance, adding sulfide active filler Li10GeP2S12 (LGPS) to PEO polymer can prepare a PEO/LGPS/LiTFSI CSSE membrane with a stability in air. The CSSE has an ionic conductivity of 1.18×10-4 S/cm at room temperature. After 150 cycles at 0.5 C, the cells using PEO/LGPS/LiTFSI as a membrane demonstrates superior capacity retention and rate performance.

    To meet high-voltage cathodes and lithium metal, CSSEs with bi-layered or multi-layered structures maximize the synergistic effect of each layer without or withless sacrificing their properties, particularly for adjustable interphase. A bi-layer structure used Li6.4La3Zr2Al0.2O12/PEO/LiTFSI and I2/PEO/LiTFSI CSSE layers to contact with cathode and anode, respectively. After 500 cycles at 0.2 C, the LFP||Li cell maintains a specific capacity of 146.20 mA·h/g. A sandwich structure CSSE with PAN/PVDF-80% (in mass) LLTO/PEO was prepared by a casting method, having an ionic conductivity of 2.81×10-4 S/cm and an electrochemical window of 4.92 V. The assembled battery delivers the Coulomb efficiency of 99.2% and a capacity retention rate of 88% at 0.5 C after 500 cycles.

    The mechanism of ion transport in CSSEs has not yet clarified due to itscomplexity. The current well-known ion transport pathways in CSSEs include polymer matrix, inorganic active fillers and interfacial regions between polymer matrix and active fillers. Among them, the ion-transport pathway at the interfaces is relatively complex, and more efforts are needed to reveal the mechanism.

    Summary and prospects

    CSSEs have attracted great attention for the development of SSLBs because they can improve ionic conductivity and enhance the mechanical strength and stability of the SSEs by incorporating inorganic fillers into polymer electrolytes. Recent research progress on the CSSEs were summarized. The main components of the key materials of CSSEs, i.e., inert and active fillers in the polymer matrix, were classified and summarized. The advanced structures of CSSEs to withstand lithium metal reduction and high-voltage positive electrode oxidation were explored. In addition, the possible mechanism of ion conductivity in CSSEs wasalso discussed. Although CSSEs were used in battery applications, they still had some challenges in ion conductivity, lithium-ion transport mechanism, and interface compatibility. Some key issues need to be considered for the future studies, i.e., further increasing in the room-temperature ionic conductivity of CSSEs, understanding of ion conduction mechanism in different types of CSSEs, and optimizing the interphase between the solid electrolytes and the electrodes.

  • Zijie XU, Xiuchun YANG, Yufan WANG
    Journal of the Chinese Ceramic Society. 2024, 52(1): 255-272.

    With the rapid growth of population and the development of industry, the lack of clean water resources becomes increasingly prominent. For the shortage of clean water resources, China as a country rich in seawater resources vigorously promotes seawater desalination technology, which has gradually developed into a strategic industry. Compared with the existing desalination technologies such as multi-effect distillation, multi-stage flash evaporation, reverse osmosis membrane, electrodialysis and so on, the desalination technology based on the principle of solar photothermal conversion has unparalleled advantages, i.e., environmental-friendly, high efficiency and low cost. Solar-driven steam generation (SSG) could be widely applied in seawater desalination, sewage treatment and other fields, which is of great significance in acquiring pure water and solving the problem of water resource shortage.

    Ultra-high solar steam conversion efficiency could be achieved by increasing photothermal conversion efficiency, water transfer rate and heat management of the SSG system. In recent years, the evaporation models underwent a gradual transition from using photothermal particles dispersed in volume water to interface water evaporation with porous insulation layer or 1D or 2D water transport channels to the hydrophilic gel evaporation structure. It is reported that TiN hyperbranched nanowires have a better solar light absorption and a higher specific surface area to evaporate water rather than TiN nanoparticles and nanotubes. Its solar water evaporation rate and solar thermal conversion efficiency are 1.525 2 kg·m-2·h-1 and 94.01%, respectively, under 1 kW·m-2 simulated solar irradiation. Zhu et al. demonstrated that a carbon foam with a three-dimensional interconnected porous structure enables a sufficient diffusion of vapor with a convective flow and realizes an evaporation rate of 10.9 kg·m-2·h-1. Solar-driven steam-electricity system expands the functionary of SSG, providing an innovative pattern for the electricity supply for tiny electronic devices, flexible wearable devices and remote area. Solar-driven steam-electricity system is mainly divided into integrating electricity generation module and self-powered electricity generation module. In SSG and PV cell integration modules, Xu et al. experimentally demonstrated that a prototype hybrid tandem solar device with WTIL can generate electricity with a power output of 204 W·m-2 and purify water at 0.80 kg·m-2·h-1 under 1-sun illumination. Deng et al. realized that the evaporation rate of the prepared TEC in seawater electrolyte is 1.1 kg·m-2·h-1, and the solar vapor conversion efficiency of the TEC is 60% with a peak output power of 0.5 mW·m-2. In self-powered electricity generation modules, Guo et al. presented a device prototype for enhanced power generation from ambient humidity, the device to ambient humidity can produce voltages of 0.78 V and a current of 7.5 μA, both of which can be sustained for more than 10 d. In this review, we summarized recent research work on the solar-driven steam-electricity system, and analyzef the advantages and disadvantages of different electricity generation modules.

    Summary and prospects

    Selection of solar absorbers: Three categories of solar-absorbing materials including carbon materials (such as carbon nanotubes, carbon nanoparticles, and graphene), plasmonic metals (such as Al, Au, Ag, Cu) and ceramic nanomaterials (such as transition metal nitrides and carbides) and semiconducting nanomaterials (such as TiO2-x, MoS2) were developed. The present research focuses on the preparation of high-light-absorption photothermal absorbers with a low-cost and a superior chemical stability.

    1) Structural design of solar steam generation system: The solar-vapor conversion efficiency (η) can be calculated by

    where Qs is the incident light power (1 kW·m-2); Qe is the water evaporation power; Hv is the evaporation heat of water (~2 260 kJ·kg-1); m is the evaporated water mass; t is time.

    Based on Eq. (1), the solar steam conversion efficiency is directly proportional to water evaporation enthalpy and water evaporation rate. It is proved that the latent heat of water vaporization in a porous nanostructure is lower than the standard value. However, it is still unclear how to obtain a low water evaporation enthalpy by regulating the porous structure of the solar photothermal materials. It is crucial to obtain hierarchical nanostructures and evaluate its water vaporization latent heat. In order to increase the specific surface area of solar photothermal materials, porous foams and gels are designed and prepared, but the preparation of these artificially hierarchical materials is a time-consuming and costly process. It is thus imperative to explore naturally hierarchical plants that are low-cost and easy to obtain.

    2) Efficiency and mechanism of VOCs photodegradation in water: Solar-driven steam generation is utilized to produce fresh water by removing salts, heavy metals, micro-organisms, and most organic pollutants in raw water. However, it also accelerates the volatility of the volatile organic compounds (VOCs) and enrich them in the distilled water if the water source is contaminated by VOCs because of their similar boiling point with water, which poses a serious threat to the atmospheric environment and human-being health. VOCs such as alcohols, aldehydes, ketones, olefins, and aromatic compounds tend to migrate and accumulate in different environmental media such as soil, water, and air. The World Health Organization and China's sanitary standards for drinking water quality both have established limit values for VOCs. Consequently, it is crucial to efficiently remove VOC during the solar-driven interfacial evaporation.

    3) The relative merits of different electricity generation systems: Solar-driven steam-electricity system is mainly divided into integrating electricity generation system and self-powered electricity generation system. The integrating electricity generation module integrates a solar water evaporation module and an electricity generation module by rationally connecting the solar water evaporation module with photovoltaic device harvesting light energy, thermoelectric module recovering heat energy from water vapor, membrane structure utilizing salt concentration gradients and triboelectric nanogenerator based on steam condensation process. The electricity generation capacity of an integrated electricity generation system typically depends on the electrical output performance of the power generation module itself. Though the integrated electricity generation system can be commercially produced and has a stable performance, it has some problems such as complex structure, high cost and non-adaptability of different modules, which limit its practical application. The self-powered electricity generation system does not connect solar water evaporation module with other auxiliary equipment for electricity generation. It generates electricity directly by a hydrovoltaic effect, and its evaporation-electricity generation performance mainly depends on the microstructure of the photothermal material, such as the size of micro-/nano-pore channels and the zeta potential. The currently reported output currents range from nanoamps to microamps, and exploring current output in the milliamp range is a further research direction.