• Journal of the Korean Society of Manufacturing Technology Engineers
• /
• v.6 no.3
• /
• pp.17-25
• /
• 1997

This paper aims to clarify the effects of grinding conditions on the grinding force, ground surface and chipping size of workpiece in surface grinding of various ferrites with the resin bond diamond wheel. The main conclusions obtained were as follows: In a constant peripheral wheel speed, the specific grinding energy is fitted by straight lines with grinding depth coefficient($\delta$) in a logarithmic graph. The effect of both depth of cut and workpiece speed on grinding energy becomes larger in the order of Mn-Zn, Cu-Ni-Zn and Sr. When using the diamond grain of the lower toughness, the roughness of the ground surface becomes lower. The ground surfaces show that the fracture process during grinding becomes more brittle in the order of Sr, Mn-Zn and Cu-Ni-Zn. The chipping size at the corner of workpiece in grinding increases with the the increases of the depth of cut and workpiece speed, and the decrease of peripheral wheel speed. The effect of both depth of cut and workpiece speed on chipping size becomes more larger in the order of Sr, Mn-Zn and Cu-Ni-Zn.

• Proceedings of the KIEE Conference
• /
• 2001.07c
• /
• pp.1460-1462
• /
• 2001

초고속 전력선 통신을 위한 고주파수 대역에서 안정적인 자기적 특성을 갖는 Ni-Zn ferrite를 개발하기 위해서 투자율은 낮지만 주파수 특성이 우수한 $Ni_{0.8}Zn_{0.2}Fe_2O_4$를 기본조성으로 입자를 성장시키는 $Bi_2O_3$를 0.7, 비저항을 증가 시키는 CaO를 0.3, 그리고 입자를 균일하게 하는 $V_2O_5$를 0.1 wt% 첨가하여 미세구조를 제어하고, 다시 고주파 특성을 향상시킬 것으로 기대되는 $Co_3O_4$를 0, 0.3, 0.5, 0.7 wt%로 변화시켜 자기적 특성을 조사하였다. $Co_3O_4$가 밀도 및 미세구조에는 영향을 미치지 않았으나 0.3, 0.5 wt% 첨가시 첨가하지 않은 조성보다 투자율은 감소하였으나 사용 한계 주파수로 여겨지는 공명주파수가 각각 19.905, 19.205 MHz로 크게 증가하였다. 그리고 전체 전력 손실도 $Co_3O_4$를 첨가했을 때 감소하였으나 첨가량에는 큰 변화가 없었다. 와전류 손실이 전체 전력손실에 지배적인 영향을 미치고 있다.

• Electrical & Electronic Materials
• /
• v.4 no.3
• /
• pp.211-219
• /
• 1991

본 논문은 고주파에서의 Ni-Zn페라이트의 첨가물에 따른 소결특성에 관하여 연구한 것이다. 연구에서 사용한 시편은 20mol% NiO, 30mol% ZnO 및 50mol% Fe$_{2}$ $O_{3}$이 조성으로된 페라이트를 모재로 하고 첨가물로서 각각 0.0025mol%, 0.005mol% 및 0.001mol%의 비율로 Nb$_{2}$ $O_{5}$, Bi$_{2}$ $O_{3}$ 및 V$_{2}$ $O_{5}$를 첨가하였다. 그리고 소결을 1100.deg.C에서 이루어졌다. 초투자율은 V$_{2}$ $O_{2}$가 첨가된 시편의 100KHz-1000KHz주파수대에서 4*$10^{2}$~8*$10^{2}$의 높은 값을 얻었다. 손실계수는 100KHz~500KHz주파수대에서 1*10~3*$10^{-2}$이었다. 1/(.mu.*Q)값은 0.005mo;% Bi$_{2}$ $O_{3}$가 첨가된 시편에서 가장 높은 값을 나타내었다. 자기저항은 초유자율과 반비례의 관계를 나타내었다. 실험의 결과 첨가물에 의한 소결특성은 액상형성에 의하여 고른 입자성장을 확인할 수 있었다. 따라서 0.01mol% V$_{2}$ $O_{5}$를 첨가한 시편이 가장 우수한 자기특성을 나타내고 있음을 확인하였다.

• Journal of Powder Materials
• /
• v.2 no.1
• /
• pp.29-35
• /
• 1995

In this study the calcined condition and characteristic of Cu-Ni-Zn ferrite powder were investigated. The Cu-Ni-Zn ferrite powder has been synthesized by the thermal decomposition of the organic acid salt. This process did not require a strict pH control and provided the uniform composition and fine powder with about 0.3 $\mu\textrm{m}$. The XRD diffraction pattern of this powder showed about 50% spinel phase. The optimum calcination was found to be done at $700^{\circ}C$ for one hour. After the calcination, the amount of spinel increased to 90%. The distribution of the particle size showed bimodal peaks, one was about 0.5 $\mu\textrm{m}$ and the other was about 20 $\mu\textrm{m}$. The large particles of 20 $\mu\textrm{m}$ were the agglomeration of fine Particles. The mean Particle size of the powder was about 0.4 $\mu\textrm{m}$. The powder was compacted under 100 MPa pressure and sintered at 1100~ $1250^{\circ}C$ for one hour in air. The density of ferrites specimen was a function of the sintering temperature. The higher the temperature, the denser the ferrite. The maximum relative density of the sintered ferrite was about 93% at $1250^{\circ}C$. The grain size of sintered specimen at $1200^{\circ}C$ was 5 $\mu\textrm{m}$ and homogeneous.

• Korean Journal of Materials Research
• /
• v.13 no.8
• /
• pp.531-536
• /
• 2003

The electromagnetic properties and microstructures of the ferrites based on ($Ni_{0.2}$ $Cu_{0.2}$ $Zn_{0.6}$)$_{1.085}$($Fe_2$$O_3$)$_{0.915}$ were investigated by changing the amount of additive SnO$_2$and CaO and the sintering temperatures. Addition of $SnO_2$caused pores in the specimen. There was no variation of grain size by changing the amount of additives. Total loss was reduced when ($Ni_{0.2} $Cu_{0.2}$ $Zn_{ 0.6}$)$_{1.085}$ ($Fe_2$$O_3$)$_{0.915}$ composition was sintered at $1150^{\circ}C$ rather than $1300^{\circ}C$. Addition of CaO was useful to reduce the total loss because it increased the sintering density. The lowest total loss was obtained when 0.06 wt% $SnO_2$and 0.4 wt% CaO were added at the same time.

• Proceedings of the Korean Magnestics Society Conference
• /
• 2002.12a
• /
• pp.38-39
• /
• 2002

일반적인 세라믹스 분말 합성방법으로서 고상법과 침전법 등은 성분 원소들간의 균일한 혼합이 어렵고, 대부분 최종 생성물의 합성 온도가 높아서 다성분계에 대하여 단일 상을 유지하면서 미세한 분말을 얻기가 힘들다. 그러나, 최근 들어 이러한 단점을 보완하기 위한 방법으로서 비정질 citrate법, 무기 금속염을 이용한 sol-gel법 등과 같이 비교적 공정이 단순하면서 입도 분포가 좁고 재현성이 우수한 구형의 초미립 또는 나노 분말의 제조에 적합한 방법들이 많이 연구되고 있다[1]. (중략)

• Proceedings of the Korean Magnestics Society Conference
• /
• 2007.05a
• /
• pp.58.1-58.1
• /
• 2007

• Resources Recycling
• /
• v.9 no.5
• /
• pp.16-21
• /
• 2000

Generation of abnormally large grains in the microstructure of small grains has been investigated on some ferrites. Some fractions of large grains were observed in the microstructue of sintered ZnFe$_2$O$_4$, Mn-ZnFe$_2$O$_4$, Fe$_3$O$_4$(in $N_2$) and MnFe$_2$O$_4$(in air). On the other hand, the large grains were not observed in $NiFe_2$$O_4$ and $CoFe_2$$O_4$, independent of calcining and sintering conditions. The large grains seem to be generated in such ferrites that are easy to very their compositions or valencies at high temperatures. as the sintering proceeded, the number of large grains was increasing to from a continuous structure consisting of large grains, while the size of large grains did not increase remarkably. In addition, the growth of small grains was also very slow during the generation of the large grains. The large grains appeared be suddenly generated after some induction periods. Avrami equation could be applied to the relation between net volume of large grains and sintering time. Thus, the grain boundaries may be strongly stabilized when the large grains are generated. The large grain is generated y the local activation of the stabilized rain boundaries, which is caused by the variation of composition or valencies during sintering. It is concluded that the essence of the abnormal gain growth is not the generation of abnormally large grains, but the abnormal stabilization and the local activation of he grain boundaries.

• Journal of the Korean Ceramic Society
• /
• v.50 no.3
• /
• pp.231-237
• /
• 2013

Thermodynamic modeling of the $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ complex ferrite system has been adopted as a rational approach to establish routes to better synthesis conditions for pure phase $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ complex ferrite. Quantitative analysis of the different reaction equilibria involved in the precipitation of $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ from aqueous solutions has been used to determine the optimum synthesis conditions. The spinel ferrites, such as magnetite and substitutes for magnetite, with the general formula $MFe_2O_4$, where M= $Fe^{2+}$, $Co^{2+}$, and $Ni^{2+}$ are prepared by coprecipitation of $Fe^{3+}$ and $M^{2+}$ ions with a stoichiometry of $M^{2+}/Fe^{3+}$= 0.5. The average particle size of the as synthesized $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$, measured by transmission electron microscopy (TEM), is 14.2 nm, with a standard deviation of 3.5 nm the size when calculated using X-ray diffraction (XRD) is 16 nm. When $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ ferrite is annealed at elevated temperature, larger grains are formed by the necking and mass transport between the $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ ferrite nanoparticles. Thus, the grain sizes of the $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ gradually increase as heat treatment temperature increases. Based on the results of Thermogravimetric Analysis (TGA) and Differential Scanning Calorimeter (DSC) analysis, it is found that the hydroxyl groups on the surface of the as synthesized ferrite nanoparticles finally decompose to $Ni_{0.5}Zn_{0.4}Cu_{0.1}Fe_2O_4$ crystal with heat treatment. The results of XRD and TEM confirmed the nanoscale dimensions and spinel structure of the samples.

• Journal of Magnetics
• /
• v.8 no.4
• /
• pp.138-141
• /
• 2003

$Ni_{0.65}Zn_{0.35}Fe_2O_4$thin films were prepared by using a sol-gel method. Their crystallographic, dielectric and magnetic properties were investigated as a function of Cu contents by means of an X-ray diffractometer (XRD), X-ray reflectivity, LCZ meter (NF2232), a vibrating sample magnetometer (VSM), and an atomic force microscope (AFM). From typical C-V measurements for $Ni_{0.65}Zn_{0.35}Fe_2O_4$ thin films on p-type silicon substrate, the surface charge density was calculated as 1.4 ${\mu}$C/$m^2$. The dielectric constant evaluated from the capacitance at the accumulation state was 28. The high $H_{c}$ and low $M_{sat}$ at x=0.0 and 0.1 were due to the growth of the ${\alpha}$-$Fe_2O_3$ phase having antiferromagnetic properties. The rapidly decreased $H_{c}$ and increased $M_{sat}$ at x=0.2 and 0.3 can be explained that the ${\alpha}$-$Fe_2O_3$ phases have completely disappeared at x=0.3 and so, non-magnetic defects are minimized. The $M_{sat}$ was slightly decreased and the $H_{c}$ was increased above at x=0.3 because the increase of grain boundary due to smaller grain size acts as defects during magnetization process.