4,218 publications from this institution
Triboelectric nanogenerator (TENG) has been considered as a new type of energy harvesting technology, which employs the coupling effects of triboelectrification and electrostatic induction. One key factor having limited its application is the energy storage. In this work, a high performance Li3V2(PO4)3/C material synthesized by low-cost hydrothermal method followed with subsequent annealing treatment was studied to efficiently store the power generated by a radial-arrayed rotary TENG. Not only does the Li3V2(PO4)3/C exhibit a discharge capacity of 128 mAh g–1 at 1 C with excellent cyclic stability (capacity retention is 90% after 1000 cycles at a rate of 5 C) in Li-ion battery, but also shows outstanding energy conversion efficiency (83.4%) compared with the most popular cathodic materials: LiFePO4 (74.4%), LiCoO2 (66.1%), and LiMn2O4 (73.6%) when it was charged by high frequency and large current electricity directly from by TENG.
Abstract Super graphene‐skinned (Gr‐skinned) materials are emerging members of the graphene composite family, which are synthesized through the high‐temperature chemical vapor deposition of continuous graphene on engineering materials, followed by ingenious postprocessing techniques. The continuous high‐performance graphene “skin” endows the engineering materials with excellent thermal conductivity. The Gr‐skinned Cu is taken as an example and conducted a multi‐scale study of their heat transfer mechanism by combining molecular dynamics with physical models. The results show that the heat transfer at the Cu/Gr interface is the rate‐limiting step within the Gr‐skinned Cu, where phonon heat transfer accounts for 86.59% and electrons contribute to 13.41%. This phonon‐electron synergistic effect enhances interfacial heat transfer. Compared to other Cu(hkl) surfaces, the Cu(111) surface has stronger interfacial phonon coupling with graphene, which is further enhanced by specific graphene defects, improving interfacial heat transport. Macroscopically, Gr‐skinned Cu foil and powder units can be composited into bulk to build up a well‐connected conductivity network. The thermal conductivity increment of Gr‐skinned Cu powder bulk is eight times that of Gr‐doped Cu composites with an identical number of graphene layers. This confirms the advantages of Gr‐skinned Cu in heat conduction, offering a novel strategy for optimizing graphene composites.
Abstract ZnS particles consisting of nanocrystallites have potential applications as light emitters for displays. The possibility of encapsulating chemicals into porous particles and the temperature-controlled release of them could also be of interest in chemical engineering. The objective of this study is to determine the size distribution, shape and morphology of ZnS particles synthesized under different conditions, since they strongly influence the optical and electric properties. The ZnS powders were prepared by precipitation from homogeneous aqueous solutions, following a procedure described elsewhere1-3 The initial solution consists of a zincsalt precursor dissolved in ultrapure water under acidic pH conditions. Adding Thioacetamide (TAA: CH3C(S)NH2) to this acidic solution at elevated temperature leads to the precipitation of ZnS nanocrystals. Four different types of zincsalt precursors were used to study their influence on the precipitation process and the final powder morphology: acetate (CH3COO), chloride (Cl-), trifluoromethanesulfonate (tFMS: CF3SO3 -) and dimethyldithiocarbamate (dMdTC: S4N2C6H12 -). The dried powder were subjected to 350°C and 700°C heat treatments, respectively.
The `frozen-lattice' model is a semi-classical approach for calculating electron diffuse scattering in crystals that has arisen from thermal vibration of crystal atoms. This quasi-elastic scattering approach is, however, unproven since its equivalence with the incoherent phonon-excitation model is not yet established. As quantitative electron microscopy is becoming a realistic method, it is necessary to examine the accuracy of the model. In this paper, based on a rigorous quantum-mechanical phonon excitation theory, it is proved that an identical result would be obtained using the frozen-lattice model and the formal phonon-excitation model if (i) the incoherence between different orders of thermal diffuse scattering is considered in the frozen-lattice-model calculation and (ii) the specimen thickness and the mean-free-path length for phonon excitation are both smaller than the distance travelled by the electron within the lifetime of the phonon (τ0v, which is 5 µm for 100 kV electrons). Condition (ii) is usually absolutely satisfied and condition (i) can be precisely accounted for in the calculation with the introduction of the mixed dynamic form factor S(Q, Q′). The conclusion holds for each and all orders of diffuse scattering, thus, the quantum-mechanical basis of the frozen-lattice model is established, confirming the validity, reliability and accuracy of using this model in quantitative dynamical electron diffraction and imaging calculations. It has also been shown that the frozen-lattice model is suitable for low-energy electrons.