• 대한전기학회논문지:전기기기및에너지변환시스템부문B
• /
• 제51권10호
• /
• pp.545-553
• /
• 2002

This paper is about the analysis of 3-dimensional magnetic field distribution in CPM(Convergence Purity Magnet) considering magnetization vector and the optimum design of CPM. The magnetization vector of CPM is obtained using 2-dimensional magnetization FEA(Finite Element Analysis) coupled with Priesach model. Using this magnetization vector of CPM, we analysed the 2-dimensional and 3-dimensional magnetostatic field of CPM and know that these analysis results are not equal. From experimental result, we know that the 3-dimensional analysis is accurate because the magnetic field distribution in CPM cannot be considered correctly by 2-dimensional analysis because of the shape of CPM. Finally, the optimum designing of CPM which control accurately the electron beam deflection in CRT(Cathode Ray Tube) was possible using 3-dimensional magnetic field analysis result.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 2000년도 추계학술대회 논문집 학회본부 B
• /
• pp.241-243
• /
• 2000

In this paper, we analyze three-dimensional magnetic field distribution of a convergence purity maget(C.P.M) which is used for a cathode ray tube. The magnetization vector distribution of the C.P.M is obtained from the result of magnetization process analysis using the 2D F.E.M. Then the motion of electron beam passing through the inner space of the C.P.M is determined and compared with experimental result.

• 대한전기학회논문지:전기기기및에너지변환시스템부문B
• /
• 제49권11호
• /
• pp.729-736
• /
• 2000

This paper deals with the characteristic analysis of magnetizer for convergence purity magnet by the finite element method. The analysis utilizes combined method of the time-stepped finite element analysis and the Preisach model with hysteresis phenomena. In the finite element analysis, the non-linearity and the eddy current of the magnetizing fixure and permanent-magnet are taken account. The magnetization distribution in the permanent magnet is determined by using Preisach model which are composed of Everett function table and the first order transition curves is obtained by the Vibrating Sample Magnetometer. The calculated flux density values on the surface of the permanent magnet are led to the approximated gauss density values measured by the gauss meter. As a result, winding current, copper loss, eddy current loss of the magnetizing yoke, flux plot, surface gauss plot, temperature rise of the coil and resistor variation, vector diagram of magnetization distribution are shown.

• 한국전기전자재료학회논문지
• /
• 제11권9호
• /
• pp.752-757
• /
• 1998

Rotational Magnetization-vector measurements have been performed on a polycrystalline $Y_1Ba_2Cu_3O_{7-\delta}$ sample in field-cooled condition at 4.2 K. The experimental results show that vortex flux density(B) consists of 3 groups :(1) a weak pinning part ($B_w$) which stays at a fixed angle relative to the magnetic field f(H) ; (2) a strong pining part($B_s$) which rotates rigidly with the sample and has same magnitude with the sample rotation, and(3) and intermediated pining part ($B_i$) which rotates rigidly with the sample, but whose magnitude changes with the sample rotation Our results have been explained in terms of a distribution in the strength of the vortex pinning torque and a repulsive intervortex torque.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 1996년도 하계학술대회 논문집 A
• /
• pp.62-64
• /
• 1996

Two current approaches for modeling the vector magnetic hysteretic process are the vector Preisach models and those models based on a system of noninteracting pseudo-particles. The pseudo-particles are intended to mimic the average behavior of real media particles. The simplest switching mechanisms of pseudoparticles is the Stoner-Wholfarth model. The Preisach models are quite precise in specifying the experimental input to the models. The vector properties of the Preisach models are, however, inadequate. This is partly because of the questionable assumptions used in coupling the various vector hysteresis components. Also these models do not include reversible magnetization changes. Unlike Preisach counterpart, the Stoner-Wholfarth model is inherently vector in nature. This is because spatial distribution and switching mechanisms are imposed on the system of pseudo-particles, so they come closer to representing the physical reality. The lack of interaction between pseudo-particles exclude the usefulness of the Stoner-Wholfarth model for small fields when the medium is traversing minor loops. The present work is an attempt at combining the advantages of above two models into one composite model, including the effect of particle interaction.

• 지구물리와물리탐사
• /
• 제23권1호
• /
• pp.22-37
• /
• 2020

이 연구는 남서태평양 통가열도에 위치한 TA (Tofua Arc) 12 해저산에 대한 해저지형, 자력자료를 이용한 자화벡터역산 모델링을 통해 해저면에서 심부층까지의 종합적인 3차원 자력구조 특징을 분석하였다. 북서-남동 방향성을 가진 타원형의 칼데라 해저지형이 TA 12 해저산 정상부에서 나타나며, 두 개의 작은 콘 모양의 지형이 칼데라 정상부 함몰지형에 존재한다. 또한 해저산 정상부 서쪽 사면에서는 콘 지형이 나타나는 지역부터 해저산 기저부 남서쪽 사면까지 큰 규모의 사면 해저곡이 보인다. TA 12 해저산에서는 칼데라 함몰지형에 저자기이상대가 나타나고 그 주변 칼데라 정상부 및 사면 지역에 고자기이상대가 둘러싸여 있다. 이는 함몰지형을 포함한 칼데라 정상부 지역에 강한 자성체의 분포 또는 마그마 관입 가능성이 있다고 해석될 수 있다. 3차원으로 해석된 자화벡터역산 결과에서는 해저 -3000 m부터 해저산의 주변 사면지역에서의 고이상대 존재와 자기 감수율이 칼데라 정상부 및 함몰지형의 천부층으로 향해 증가함을 보여 준다. 한편 주로 칼데라 정상부의 해저면 근처에서 소규모 고이상대들이 곳곳에 나타나고 있다. 따라서 TA 12 해저산에서는 마그마가 심부에서 천부로 올라올 때 해저산 주변 사면부에서 칼데라 정상부 및 함몰지형으로 이동했음이 예상된다. 그리고 해저면 근처의 복잡한 자력분포는 잔류자화의 영향으로 추정된다.