Abstract:Y 2 O 3 -doped Zn 1x Ni x O (x = 0, 0.3, 0.4, 0.5, 0.6, 0.7, and 0.9) powders were prepared by a wet chemical synthesis method, and the related ceramics were obtained by the traditional ceramic sintering technology. The phases and related electrical properties of the ceramics were investigated. The analysis of X-ray diffraction (XRD) indicates that the prepared ceramics with Ni substitution have a cubic crystalline structure. The resistance-temperature feature indicates that all the ceramics show a typical ef… Show more
“…This can be used to transform the resistance versus temperature function of a thermistor into a linear lnR versus T 1 function. The average slope of this function would then yield an approximation of the B parameter value [1,8,[34][35][36]. The set of graphs with 1/T on the X-axis and lnR on the Y-axis were plotted to obtain the thermistor parameters.…”
“…T is the temperature in Kelvin and R is the resistance in ohms. In the measurement of temperature in the range of 200 °C, the error in the Steinhart-Hart equation is usually less than 0.02 °C[1,8,[34][35][36].…”
The influence of Cu and Li doping in the structural and R-T characteristics of Ni-Mn-based spinel oxide negative temperature coefficient (NTC) thermistors prepared using the conventional solid-state synthesis method was investigated in this study. The doping of Cu and Li in nickel manganite plays an important role in tailoring the thermistor parameters. The structural characterization of the prepared samples using XRD revealed that the basic structure of the samples is not altered by the addition of the dopants Cu and Li. The particle size of the samples was obtained at less than 50 nm. R-T characteristics showed a decrease in resistance with temperature. It was observed that the addition of dopant Cu in a minimal amount helps to tune the resistance of the thermistor in the required range and Li addition, as a dopant, stabilized the thermistor parameters B and alpha.
“…This can be used to transform the resistance versus temperature function of a thermistor into a linear lnR versus T 1 function. The average slope of this function would then yield an approximation of the B parameter value [1,8,[34][35][36]. The set of graphs with 1/T on the X-axis and lnR on the Y-axis were plotted to obtain the thermistor parameters.…”
“…T is the temperature in Kelvin and R is the resistance in ohms. In the measurement of temperature in the range of 200 °C, the error in the Steinhart-Hart equation is usually less than 0.02 °C[1,8,[34][35][36].…”
The influence of Cu and Li doping in the structural and R-T characteristics of Ni-Mn-based spinel oxide negative temperature coefficient (NTC) thermistors prepared using the conventional solid-state synthesis method was investigated in this study. The doping of Cu and Li in nickel manganite plays an important role in tailoring the thermistor parameters. The structural characterization of the prepared samples using XRD revealed that the basic structure of the samples is not altered by the addition of the dopants Cu and Li. The particle size of the samples was obtained at less than 50 nm. R-T characteristics showed a decrease in resistance with temperature. It was observed that the addition of dopant Cu in a minimal amount helps to tune the resistance of the thermistor in the required range and Li addition, as a dopant, stabilized the thermistor parameters B and alpha.
“…Because of its unique properties like non-toxic nature, abundance in nature, low cost, suitability for doping, high thermal and chemical stability and is an important semiconductor materials [9]. ZnO has versatile applications like UV photodetectors [10] gas sensors [11], solar cells [12], spintronics [13] luminescent materials [14], piezoelectric devices [15], light emitting devices [16], Thermistor [17] and cancer treatment [18].…”
Section: Introductionmentioning
confidence: 99%
“…Chromium has been utilized to upgrade the optical, electrical, magnetic and luminescent behaviour of ZnO [38]. By doping ZnO with different metals like Ni [17], Sr [20], Ca [39], Mn [40], La [41] etc. into ZnO shows NTCR behaviour which is very much suitable for thermistor application.…”
Cr doped ZnO (x = 0-0.04) nanoceramics was successfully synthesized by high energy ball milling (HEBM) technique. The structural and electrical properties of the synthesized sample has been studied in detail. The doping of Cr into ZnO has been verified by X-ray diffraction (XRD) and also from the variation in structural parameters. Rietveld refinement XRD pattern of calcined sample showed the hexagonal wurtzite structure and it did not induce impurity phases. From the XRD, it has been confirm that maximum result confirms that up to 4 atomic% of Cr can be doped into ZnO. The strain of the sample reduced with increase in particle size. After sintering, there is a growth of particle size of Cr doped ZnO sample. The impedance spectroscopy data shows a single semicircle in the high frequency region corresponding to the bulk properties of the nanoceramic sample. The decrease in real part of the impedance with temperature suggests the NTCR behavior of the sample in the temperature range of 300-500 ºC. The temperature dependent relaxation phenomena are also observed for the synthesized ceramic sample at high temperature. Distributed relaxation time suggests that the relaxation in the synthesized samples is of non-Debye type. The equivalent electrical circuit of the semicircular pattern in the impedance spectrum of ZnO and Zn1-xCrxO nanoceramics sample is a parallel combination of bulk resistance (Rb) and bulk capacitance (Cb).
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