journal article·2000-12

Spinel forming ceramics of the system FexNiyMn3–x–yO4 for high temperature NTC thermistor applications

Adalbert Feltz, Walter Pölzl

Journal of the European Ceramic Society· Volume 20· Issue 14-15
Publisher page

Abstract

Abstract The thermal stability and aging of spinels of the system Fe 2 O 3 –NiO–Mn-oxide are studied by measuring the electrical properties of ceramic samples obtained by sintering up to 1350°C. Based on the formula Fe III x Ni II y Mn z 3−x−y O 3+ x 2+δ , chemical analyses of ceramic samples with defined values of x and y make it possible to determine the average oxidation number z of manganese with z= 2δ 3−x−y +2 thus leading to the share of oxygen 2−x−2δ 4 O 2 which is liberated during sintering. X-ray diffraction measurements of samples with higher NiO and lower Fe 2 O 3 content indicate NiO separation. Hence, the analytical results are suitable to elucidate the phase constitution of the ceramics consisting of a mixture of NiO and of a spinel with modified composition. The formation of the spinel ceramics FeNi 0.5 Mn 1.5 O 4 ( x =1, y =0.5) and FeNi 0.7 Mn 1.3 O 4 ( x =1, y =0.7) in a single-phase state, i.e. without oxygen loss on sintering at 1350 or 1300°C in air, is due to the lower content of NiO at a sufficiently high fraction of Fe 2 O 3 in the composition. The compounds show ferrimagnetic behavior. FeNi 0.5 Mn 1.5 O 4 has a Curie temperature of 245 5°C. At increasing temperature, commonly above 150°C or 200°C up to 400°C the specific electrical resistivity ρ 25°C and the value of the B 25/100°C constant of both of the two compounds depend on time and on the thermal pre-treatment of the samples. Aging is due to the frozen-in state of the equilibrium of distribution of cations between the tetrahedral and octahedral sites of the spinel structure. This tends to shift towards equilibrium when the temperature is increased step by step during aging; it can be followed by measuring the electrical properties. The changes are observed to arise approaching the Curie temperature. Soaking of the samples at 650°C after aging for 72 and 144 h up to 500°C shows that the variations of the ρ 25°C and B 25/100°C values can be repeated in a following aging cycle, provided that the same cooling rate is applied. On the other hand, above 400 °C the ralaxation effects fail. Changes in this range of higher temperature involve fast rates of cation re-distribution thus leading to short waiting times until a constant value of the electrical resistivity is achieved. Hence, above 400°C, FeNi 0.5 Mn 1.5 O 4 ceramics appear completely stable against aging within common measuring times. Therefore, they should be suitable for high temperature NTC thermistor applications. The comparatively high value B 25/100°C =7470 K makes it possible to measure the temperature via the electrical resistivity with satisfactory sensitivity, e.g. α= 1 ρ d ρ dT =0.8% is achieved in the range around 750°C.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Electrical and Thermal Properties of Materials · Ferroelectric and Piezoelectric Materials · Microwave Dielectric Ceramics Synthesis

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (20)

Show source-provided references
1. Siemens Matsushita Components. Keramische Bauelemente, A-8530 Deutschlandsberg, Data Book. 1996.
2. Keystone Carbon Company, Thermistor Division. High-Temperature NTC Glass Encapsulated Thermistors. St. Marys, PA 15857, USA.
3. Ishikawa, K., Tamai, T., Kanasashi M., Miyama M. and Hata, T., Thermistor Sensor for Automotive Uses. National Technical Report, Vol.34, 1988, pp.25–34.10.5179/benthos1981.1988.25 ↗
4. Katsuki, N.,Tamal T., Moriwake H., LeGare J. and Yoshida S., Exhaust Gas High Temperature Sensor for LEV/ULEV and OBD Systems. SAE Technical Papers 960336. Int. Congr. & Expos. Detroit, MI, February 1996.10.4271/960336 ↗
5. Solid-phase equilibria in the system NiO–Mn2O3–O210.1016/0022-1902(64)80116-0 ↗
6. Temperaturabhängigkeit der Kationenverteilung im Spinell NiAl2O410.1007/BF00638282 ↗
7. Untersuchungen an elektronenleitenden Oxid-systemen XXIII: Struktur und Eigenschaften stabiler Spinelle in den Reihen MzNiMn2–zO4 (M=Li, Fe)10.1002/zaac.19936190108 ↗
8. Preparation and characterization of NTC thermistors based on Fe2+δMn1–x-δNixO410.1007/BF00362142 ↗
9. Feltz, A., Tendencies in the development and application of negative temperature coefficient oxide ceramics. In Proceed. Electroceramics IV, Vol. II, Aachen 1994, pp. 677–684.
10. Electrical conductivity of iron-doped NiO single crystal at equilibrium and during internal oxidation10.1111/j.1151-2916.1987.tb05737.x ↗
11. Etude cristallographique du manganite spinelle cubique NiMn2O4 par diffraction de neutrons10.1107/S0567740869005644 ↗
12. X-ray photoelectron spectroscopy study of the cation valencies in nickel managanite10.1016/0022-4596(83)90220-7 ↗
13. Electrical conductivity and cation distribution in nickel manganite10.1016/0022-3697(86)90074-0 ↗
14. Cation valencies and distribution in the spinels NiMn2O4 and MzNiMn2–zO4 (M=Li, Cu) studied by XPS10.1002/pssa.2211340211 ↗
15. Bildung von Defektspinellen und Phasenbeziehungen im System NiMn3-xO410.1002/zaac.19895760110 ↗
16. Feltz, A. and Rosc, F. Sinterkeramik für hochstabile Thermistoren und Verfahren zu ihrer Herstellung. Patentschrift DE 4420657 A1, EP 0 678 656 A1.
17. Wartewig, P., Personal communication, Department of Physics, University Leipzig.
18. Stabile Spinelle ZnzNiMn2–zO4 und Vergleich mit Spinellen MgzNiMn2–zO410.1002/zaac.19926080225 ↗
19. Schmalzried, H., Festkörperreaktionen. Akademieverlag, Berlin, 1973, p. 80.
20. Sr7Mn4O15 ceramics for high temperature NTC thermistors10.1023/A:1006681817330 ↗