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1.
A proton-conducting polymer electrolyte based on agar and ammonium nitrate (NH4NO3) has been prepared through solution casting technique. The prepared polymer electrolytes were characterized by impedance spectroscopy, X-ray diffraction, and Fourier transform infra-red spectroscopy. Impedance analysis shows that sample with 60 wt.% NH4NO3 has the highest ionic conductivity of 6.57 × 10−4 S cm−1 at room temperature. As a function of temperature, the ionic conductivity exhibits an Arrhenius behaviour increasing from 6.57 × 10−4 S cm−1 at room temperature to 1.09 × 10−3 S cm−1 at 70 °C. Transport parameters of the samples were calculated using Wagner’s polarization method and thus shows that the increase in conductivity is due to the increase in the number of mobile ions. Fuel cell has been constructed with the highest proton conductivity polymer 40agar/60NH4NO3 and the open circuit voltage is found to be 558 mV. 相似文献
2.
In the present work, a novel blend polymer electrolyte membrane using poly(vinyl acetate) (PVAc), poly(methyl methacrylate)
(PMMA), and lithium per chlorate (LiClO 4) in different compositions has been prepared by the solution-casting technique. Their chemical, structural characters, thermal
behavior, surface morphology, and ionic conductivity were studied using Fourier transform infrared spectroscopy, X-ray diffraction,
thermogravimetric/differential thermal analyzer, scanning electron microscopy, and AC impedance analyzer, respectively. A
maximum ionic conductivity value of 1.67 × 10 −4 S/cm at 303 K is obtained for PVAc–PMMA–LiClO 4 complexes in the ratio of 25 × 75, keeping LiClO 4 constant as 10 wt.% among all the compositions studied. 相似文献
3.
We investigate the room temperature frequency dependence of electrical modulus for the polymer electrolytes consisting of chitosan and oxalic acid in the frequency range from 50 Hz to 1 MHz. Oxalic acid serves as the proton provider. It is found that the lowest imaginary electrical modulus is shown by the highest conducting sample OA40, which contains 60 wt.% chitosan and 40 wt.% oxalic acid. The electrical moduli for OA40 sample membrane at different temperatures are also studied, and the peak of the imaginary electrical modulus has been observed to shift towards higher frequency with increasing temperature. This indicates that relaxation is thermally assisted. Analysis of electrical modulus shows that the main relaxation process in chitosan–oxalic acid polymer electrolyte system is a non-Debye process associated with viscoelastic relaxation. 相似文献
4.
The ZnO filler has been introduced into a solid polymeric electrolyte of polyvinyl chloride (PVC)–ZnO–LiClO 4, replacing costly organic filler for conductivity improvement. Ionic conductivity of PVC–ZnO–LiClO 4 as a function of ZnO concentration and temperature has been studied. The electrolyte samples were prepared by solution casting
technique. The ionic conductivity was measured using impedance spectroscopy technique. It was observed that the conductivity
of the electrolyte varies with ZnO concentration and temperature. The temperature dependence on the conductivity of electrolyte
was modelled by Arrhenius and Vogel–Tammann–Fulcher equations, respectively. The temperature dependence on the conductivity
does not fit in both models. The highest room temperature conductivity of the electrolyte of 3.7 × 10 −7 Scm −1 was obtained at 20% by weight of ZnO and that without ZnO filler was found to be 8.8 × 10 −10 Scm −1. The conductivity has been improved by 420 times when the ZnO filler was introduced into the PVC–LiClO 4 electrolyte system. It was also found that the glass transition temperature of the electrolyte PVC–ZnO–LiClO 4 is about the same as PVC–LiClO 4. The increase in conductivity of the electrolyte with the ZnO filler was explained in terms of its surface morphology. 相似文献
5.
The proton conducting solid-state polymer electrolyte comprising blend of poly(vinyl alcohol) (PVA) and poly( N-vinylimidazole) (PVIM), ammonium tetrafluoroborate (NH 4BF 4) as salt, and polyethylene glycol (PEG) (molecular weight 300 and 600) as plasticizer is prepared at various compositions by solution cast technique. The prepared films are characterized by Fourier transform infrared spectroscopy, differential scanning calorimetry, X-ray diffraction, and scanning electron microscopy analysis. The conductivity–temperature plots are found to follow an Arrhenius nature. The conductivity of solid polymer electrolytes is found to depend on salt and plasticizer content and also on the dielectric constant value and molecular weight of the plasticizer. Maximum ionic conductivity values of 2.20?×?10 ?4 and 1.28?×?10 ?4?S?cm ?1 at 30 °C are obtained for the system (PVA–PVIM)?+?20 wt.% NH 4BF 4?+?150 wt.% PEG300 and (PVA–PVIM)?+?20 wt.% NH 4BF 4?+?150 wt.% PEG300, respectively. The blended polymer, complexed with salt and plasticizer, is shown to be a predominantly ionic conductor. The proton transport in the system may be expected to follow Grotthuss-type mechanism. 相似文献
6.
In this paper, Al 2TiO 5 ceramic material has been synthesised and used as filler in polymer electrolyte system to enhance the conductivity. The precursor sintered at 1,050 °C and contained 0.08 mole of aluminium nitrate gives the best and complete formation of Al 2TiO 5. Composite polymer electrolytes of chitosan–NH 4SCN containing different amount of home-made Al 2TiO 5 were prepared by solution casting. The addition of filler has enhanced the conductivity of polymer electrolyte. The sample 57 wt% chitosan–38 wt% NH 4SCN–5 wt% Al 2TiO 5 exhibited the highest electrical conductivity of 2.10?×?10 ?4 S cm ?1 at room temperature. The presence of the Al 2TiO 5 creates favourable pathways for ionic conduction through Lewis acid–base type interactions between ionic species and O/OH surface groups on alumina filler grains. In addition, the space charge region created by the presence of Al 3+ could attract SCN ?1 ions, thus immobilise it and increase the transport number of the cation. Degree of crystallinity is calculated from the deconvoluted X-ray diffraction patterns and it shows that the lowest degree of crystallinity is achieved when 5 wt% of filler is added. In Fourier transform infrared study, the carboxamide band of the polymer is observed to shift to higher wave number from 1,629 to 1,634 cm ?1, confirming the formation of chitosan–NH 4SCN–Al 2TiO 5 complexes. The morphology of composite polymer electrolyte has been studied using scanning electron microscopy at room temperature. 相似文献
7.
We grew Cu 2S nanowires vertically on Cu foil by gas–solid reaction with a gas mixture of O 2 and H 2S. The electrical contact properties between the Cu 2S nanowires and Cu foil were investigated using a modified current–voltage–temperature plot. The Cu/Cu 2S layer exhibited the characteristics of a Schottky barrier with a barrier height of ∼0.72 eV, which was closer to the value for Cu/Cu 2O than to Cu/Cu 2S. Energy dispersive spectroscopy results showed the presence of Cu-oxide between the Cu 2S nanowires and Cu foil. The overall structure was Cu/Cu-oxide/Cu 2S and the electrical properties were controlled by the Cu/Cu-oxide. 相似文献
8.
Chitosan–ZnO nanostructures were prepared by chemical precipitation method using different concentration of zinc chloride and sodium hydroxide solutions. Nanorod-shaped grains with hexagonal structure for samples annealed at 300 °C and porous structure with amorphous morphology for samples annealed at 600 °C were revealed in SEM analysis. X-ray diffraction patterns confirmed the hexagonal phase ZnO with crystallite size found to be in the range of ~24.15–34.83 nm. Blue shift of UV–Vis absorption shows formation of nanocrystals/nanorods of ZnO with marginal increase in band gap. Photoluminescence spectra show that blue–green emission band at 380–580 nm. The chitosan–ZnO nanostructures used on surface of a glassy carbon electrode gives the oxidation peak potential at ~0.6 V. The electrical conductivity of chitosan–ZnO composites were observed at 2.1?×?10 ?5 to 2.85?×?10 ?5?S/m. The nanorods with high surface area and nontoxicity nature of chitosan–ZnO nanostructures observed in samples annealed at 300 °C were suitable as a potential material for biosensing. 相似文献
9.
DNA has attracted the interest of physicists for a long time. One interesting theoretical question is its melting behavior. The Rényi dimension spectrum of the melting transition of DNA, reveals the multifractal nature of the dynamics of the Peyrard–Bishop model. In this Letter, the effects of different parameters involved in the Peyrard–Bishop model on the multifractal nature of the melting dynamics of a DNA chain are investigated in details. As a result, it can be concluded that not only the best multifractality nature of the model arises from the Morse potential term which is taken in the model but also the multifractal nature of the model is independent of the homogeneity, the length of chain, stacking terms, the thermal bath simulation methods and even the potentials which describe the interaction between the two bases in a pair. Furthermore, our results confirm that, the best potential to describe the interactions between the bases in pairs in the PB and PBD models is the Morse potential. 相似文献
10.
In high energy density capacitors, the electrical conduction in the dielectric may result in the leakage and the reduction of the energy efficiency. This paper investigates the electrical conduction mechanism of metallized biaxially oriented polypropylene (BOPP) film based on a revised Poole–Frenkel (PF) effect and field-enhanced carrier mobility. The field-enhanced carrier mobility which is not taken into account in traditional PF effect is investigated in the revised PF effect based on the carrier hopping mechanism. Moreover, the coefficient of the PF effect ( βPF) which stands for the variation of the barrier height is discussed. Experiments are performed to measure the electrical conductivity of the BOPP film under different electric fields. Influencing factors such as metallized electrodes, the interlayer pressure in the winding, and the crystallinity may decrease the conductivity. With a fitted jump distance of 0.6 nm, the calculated conductivities based on the revised PF effect do match well with experimental results. 相似文献
11.
Films of composites (Co 45Fe 45Zr 10) x(Al 2O 3) 100–x, (Co 84Nb 14Ta 2) x(SiO 2) 100–x, (Co 41Fe 39B 20) x(SiO 2) 100–x and multilayer heterogeneous composite–composite structures {[(Co 45Fe 45Zr 10) x(Al 2O 3) 100–x]/[(Co 45Fe 45Zr 10) x(Al 2O 3) 100–x + N 2]} n, {[(Co 45Fe 45Zr 10) x(Al 2O 3) 100–x]/[(Co 45Fe 45Zr 10) x(Al 2O 3) 100–x + O 2]} n, {[(Co 41Fe 39B 20) x(SiO 2) 100–x]/[(Co 41Fe 39B 20) x(SiO 2) 100–x + O 2]} n, and {[(Co 84Nb 14Ta 2) x(SiO 2) 100–x]/[(Co 84Nb 14Ta 2) x(SiO 2) 100–x + O 2]} n have been deposited using the ionbeam sputtering method with a cyclic supply of reaction gases during deposition. The structure and magnetic properties of the films have been studied. It has been shown that the introduction of an oxidized interlayer makes it possible to suppress the perpendicular magnetic anisotropy in the (Co 45Fe 45Zr 10) x(Al 2O 3) 100–x composite with the metallic phase concentration higher than the percolation threshold. 相似文献
12.
In this article, a type of core–shell nanostructure, Au 2S/AuAgS/Ag 3AuS 2-coated gold nanorods (GNRs) with unique optical properties was used as a sensing platform to detect fish sperm DNA (fsDNA).
The prepared core–shell nanorods are positively charged due to the adsorption of the positively charged cetyltrimethylammonium
bromide (CTAB) cations on their surface. fsDNA can form ternary fsDNA–CTAB–nanorod complexes together with CTAB and nanorod,
which provides a useful platform to detect fsDNA through absorption spectra and resonance light scattering (RLS) spectroscopy.
In this sensitive core–shell nanorod sensor, CTAB concentration and the nanoparticle dosage play important roles and have
been investigated. Moreover, the fsDNA–CTAB–nanorod complexes induce a great enhancement of RLS intensity of the core–shell
GNRs and directly proportional to the concentration of fsDNA, reaching a detection limit of about 10 −9 mg/mL. This study will be significant for as-prepared core–shell GNRs for future application in biological systems. 相似文献
13.
Organic–inorganic hybrid electrolytes based on the reaction of tri-block copolymer poly(propylene glycol)- block-poly(ethylene glycol)- block-poly(propylene glycol) bis(2-aminopropyl ether), poly(ethylene glycol diglycidyl ether, and (3-glycidyloxypropyl)trimethoxysilane doped with LiClO 4 and SiO2 nanoparticles were synthesized by a sol–gel process. The structural and dynamic properties of the materials thus obtained were systematically investigated by Fourier transform infrared spectroscopy, differential scanning calorimetry, thermogravimetric analysis, alternate current impedance, and 13C solid-state NMR measurements. A maximum ionic conductivity of 3.2?×?10 ?5 S cm ?1 was obtained at 30 °C for the solid hybrid electrolyte with a [O]/[Li] ratio of 16 and 7 wt% of SiO2 nanoparticles. A Vogel–Tamman–Fulcher-like temperature dependence of ionic conductivity was observed for the hybrid electrolytes, implying that the diffusion of charge carriers was assisted by the segmental motions of the polymer chains. 相似文献
14.
Ionics - Blend polymer electrolytes with optimized composition (92.5 PVA:7.5 PAN) doped with lithium triflate (LiCF3SO3) have been prepared in different concentrations by solution casting... 相似文献
15.
The dc electrical conductivity of as deposited thin films of a-Se xTe 100?x ( x=3, 6, 9 and 12) is measured as a function of temperature range from 298 to 383 K. It is observed that the dc conductivity increases exponentially with the increase in temperature in this glassy system. The value of activation energy calculated from the slope of ln σdc vs. 1000/ T plot, is found to decrease on incorporation of dopant (Se) content in the Te system. On the basis of pre-exponetial factor ( σ0), it is suggested that the conduction is due to thermally assisted tunneling of the carriers in the localized states near the band edges. The optical absorption measurements show an indirect optical band gap in this system and it decreases on increasing Se concentration. The optical constants (extinction coefficient ( k) and refractive index ( n)) do change significantly with the photon energy and also with the dopant Se concentration. The decrease in optical band gap may be due to the decrease in activation energy in the present system. It is also found that the real and imaginary parts of dielectric constants show a significant change with the photon energy as well as with the dopant concentration. With large absorption coefficients and compositional dependence of optical band gap and optical constants ( n and k), these materials may be suitable for optical disk applications. 相似文献
16.
The blend-based polymer electrolyte consisting of poly (vinyl chloride) (PVC) and poly (ethylene glycol) (PEG) as host polymers
and lithium perchlorate (LiClO 4) as the complexing salt was studied. An attempt was made to investigate the effect of TiO 2 concentration in the unplasticized PVC–PEG polymer electrolyte system. The XRD and FTIR studies confirm the formation of
a polymer–salt complex. The conductivity results indicate that the incorporation of ceramic filler up to a certain concentration
(15 wt.%) increases the ionic conductivity and upon further addition the conductivity decreases. The maximum ionic conductivity
0.012 × 10 −4 S cm −1 is obtained for PVC–PEG–LiClO 4–TiO 2 (75–25–5–15) system. Thermal stability of the polymer electrolyte is ascertained from TG/DTA studies. 相似文献
17.
In order to enhance the ionic conductivity of polyethylene oxide (PEO)–KI(80:20) based alkaline polymer electrolytes, nanosized inorganic filler ZnS has been incorporated into PEO–KI matrix and the corresponding nanocomposite polymer electrolytes are synthesized by the usual solution casting procedure. Atomic force microscope image of composite polymer electrolyte exhibits that the introduction of ZnS nanoparticles changes the surface morphology and aggregates them to form an arborization pattern. The prepared nanocomposite polymer electrolyte reveals an ionic conductivity of about 10 ?4 S cm ?1 for 5 wt% ZnS at room temperature. 相似文献
18.
Polymer electrolyte membranes, comprising of poly(methyl methacrylate) (PMMA), lithium tetraborate (Li 2B 4O 7) as salt and dibutyl phthalate (DBP) as plasticizer were prepared using a solution casting method. The incorporation of DBP
enhanced the ionic conductivity of the polymer electrolyte. The polymer electrolyte containing 70 wt.% of poly(methyl methacrylate)–lithium
tetraborate and 30 wt.% of DBP presents the highest ionic conductivity of 1.58 × 10 −7 S/cm. The temperature dependence of ionic conductivity study showed that these polymer electrolytes obey Vogel–Tamman–Fulcher
(VTF) type behaviour. Thermogravimetric analysis (TGA) was employed to analyse the thermal stability of the polymer electrolytes.
Fourier transform infrared (FTIR) studies confirmed the complexation between poly(methyl methacrylate), lithium tetraborate
and DBP. 相似文献
19.
We study and calculate the mobility and conductivity of proton transfer and influence of temperature on it by pang's dynamic model in hydrogen bonded systems, which coincide with experiments. We further study the mechanism of magnetization of ciguid water in the basis of this model. 相似文献
20.
Zn–Sb based alloys with Cu 2Sb addition were prepared using spark plasma sintering technique and the effects of a Cu-contained intermetallic phase on the microstructures and thermoelectric properties were examined. Rietveld refinement reveals that there are many phases in the alloys, which involve β-Zn 4Sb 3, a major phase ZnSb, a small amount of an intermetallic compound Cu 5Zn 8 and unidentified impurity phases, the quantities of ZnSb and Cu 5Zn 8 increase from 67.3 wt.% to 91.8 wt.% and 0–4.3 wt.% with Cu 2Sb additive increasing, respectively. The ZnSb plays a fundamental role in controlling the thermoelectric properties, and Cu 5Zn 8 is of great significance to optimize the transport properties. The maximum thermoelectric figure of merit ZT of 0.72 is obtained for the alloy (Cu 2Sb) 0.05–(Zn 4Sb 3) 0.95 at 654 K, which is 0.25 higher than that of undoped β-Zn 4Sb 3 at the same conditions. Therefore, we conclude that a proper addition of Cu 2Sb can contribute to the improvement of thermoelectric properties of Zn–Sb based alloys. 相似文献
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