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1.
Iron oxyhydroxides and hydroxides were synthesized from chemically beneficiated high SiO2/Al2O3 low-grade iron ore (57.49% Fe2O3) rejects and heated to get iron oxides of 96–99.73% purity. The infrared band positions, isothermal weight loss and thermogravimetric and chemical analysis established the chemical formulas of iron-oxyhydroxides as γ-FeOOH.0.3H2O; α-FeOOH.0.2H2O and amorphous FeOOH. The thermal products of all these were α-Fe2O3 excepting that of γ-FeOOH.0.3H2O which gave mainly γ-Fe2O3 and some admixture of α-Fe2O3. The hydrazinated iron hydroxides and oxyhydroxides, on the other hand, decomposed autocatalytically to mainly γ-Fe2O3. Hydrazine method modifies the thermal decomposition path of the hydroxides. The saturation magnetization,J s, values were found to be in the range 60–71 emu g−1 which are close to the reported values for γ-Fe2O3. Mechanism of the γ-Fe2O3 formation by hydrazine method is discussed.  相似文献   

2.
Dielectric behaviour of samples of the system Ca1 −x La x Ti1 −x Co x O3 withx ⩽ 0·20 has been studied in the temperature range 300–525 K as a function of frequency. The strong dispersion ofɛ andD observed in these materials indicate the significant contribution of interfacial polarisation to the observed dielectric properties. The interfacial polarisation arises due to the presence of microscopic chemical heterogeneities arising out of the slow diffusion-controlled solid state sintering process used for their preparation.  相似文献   

3.
Glasses with varying molar ratios of PbO/BaO in the system BaO-PbO-TiO2-B2O3-SiO2 were prepared keeping (BaO + PbO)/TiO2 ratio equal to one. The glasses were ceramized by two-stage heat treatment. X-ray diffraction indicates that PbTiO3 crystallizes in lead-rich glasses while BaTiO3 precipitates in barium-rich compositions. Solid solution (Ba, Pb)TiO3 does not seem to crystallize over the entire range of compositions. Simultaneous presence of PbO and BaO in the initial glass composition reduces the yield of ferroelectric phase. Dielectric properties have been interpreted in terms of microstructural features.  相似文献   

4.
Dielectric constant (ɛ), dielectric loss (tan δ) and conductivity (σ) for K2Zn2(SO4)3 and (NH4)2 Mg2(SO4)3 have been measured over the frequency range 100 Hz — 100 kHz and in temperature range 30°C — 400°C. The values of static dielectric constant at room temperature are 7.67 and 4.80 for K2Zn2(SO4)3 and (NH4)2 Mg2(SO4)3 respectively. The plots of log σ against reciprocal temperature at different frequencies of these samples merge into a straight line beyond 250°C and the activation energies calculated in this region are found to be 0.67 eV and 1.98 eV for K2Zn2(SO4)3 and (NH4)2 Mg2(SO4)3 respectively.  相似文献   

5.
通过固相化学反应合成了MexZn1-xFe2O4(Me=Co,Mn;x=0,0.5,0.6)三种复合氧化物,利用TG-DTA,XRD,SEM等对复合氧化物的热分解性质,物相和形貌进行了表征,同时测定了复合氧化物的相对复介电常数和相对复磁导率,以损耗角正切值表征了它们的吸波性能,结果表明MexZn1-xFe2O4复合氧化物在高频段对电磁波有较大的吸收,并且三种复合氧化物之间有明显差异.  相似文献   

6.
This paper reports the electrical and spectroscopic investigation of the gamma ferrite synthesized through combustion route. The electrical study and dielectric behaviour showed a typical ferrite nature for the samples. The γ → α transition is observed from the electrical conductivity data. Infrared spectral study showed the transition of a typical ferrite. The effect of the presence of α-impurities in γ-Fe2O3 is also explained here.  相似文献   

7.
Ferroelectromagnetic composites with compositions, X Ni0·5Zn0·5Fe1·95O4−δ + (1 − X) Ba0·8Pb0·2TiO3, in which X varies as 0, 0·005, 0·010, 0·015, 0·020, 0·040, 0·060, 0·080 and 1 in mole %, were prepared by conventional ceramic double sintering process. The presence of two phases was confirmed by X-ray diffraction. The temperature variation of dielectric constant, ɛ′, dielectric loss, tan δ, d.c. conductivity, a.c. conductivity, elastic and anelastic behaviour of ferrite-ferroelectric composites were studied in the temperature range 30–350°C. The a.c. conductivity measurements on these composites in the frequency range 100 Hz-1 MHz at room temperature reveal that the conduction mechanism is due to small polaron hopping. The dielectric and elastic data were discussed in the light of phase transitions.  相似文献   

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