• 대한기계학회논문집B
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• 제25권12호
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• pp.1667-1675
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• 2001

Numerical simulations are carried out for the liquid encapsulant Czochralski(LEC) by imposing a magnetic field. The use of a magnetic field to the crystal growth is to suppress melt convection and to improve the homogeneity of the crystal. In the present numerical investigation, we focus on the range of 0-0.3Tesla strength for the axial and cusped magnetic field and the effect of the magnetic field on the melt-crystal interface, flow field and temperature distribution which are the major factors to determine the quality of the single crystal are of particular interest. For both axial and cusped magnetic field, increase of the magnetic field strength causes a more convex interface to the crystal. In general, the flow is weakened by the application of magnetic field so that the shape of the melt-crystal interface and the transport phenomena are affected by the change of the flow and temperature field.

• Investigative Magnetic Resonance Imaging
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• 제7권2호
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• pp.137-143
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• 2003

목적 : 자기공명영상(MRI)에서 두부영상촬영을 위하여 가장 많이 사용되는 birdcage RF (Radiofrequency) 코일의 RF B1 필드가 코일 중앙부에서 endring영역으로 갈수록 줄어드는 것을 볼 수 있다. Birdcage RF 코일에서 endcap 쉴드가 코일 중앙부에서 endring영역으로 갈수록 RF B1 필드 균질성에 얼마나 영향을 주는지에 대하여 분석하였다. 대상 및 방법 : Lowpass, highpass, hybrid birdcage RF 코일들에 대해 각각 FDTD (Finite Difference Time Domain) 모의실험으로 RF B1 자속밀도 분포를 비교하였다. 모의 실험결과 RF Bl 필드가 가장 높은 조건인 highpass birdcage RF코일을 선택하여 RF코일 endring 근처에 endcap 쉴드를 적용함으로써 RF B1 균질성에 얼마나 영향이 있는 지 조사하였다. 결과 : FDTD모의실험결과 highpass birdcage RF코일은 코일 내부에서 RF B1 필드가 lowpass나 hybrid 형태의 birdcage RF 코일들 보다 우수하나 코일 중앙부에서 endring 영역까지의 균질성은 떨어졌다. 그러나 highpass birdcage RF 코일에 endcap 쉴드를 적용하면 hybrid birdcage RF 코일의 RF B1 필드와 비슷한 수준이면서 sagittal 방향의 전체적인 RF B1 균질성은 우수하였다. 결론 : 본 논문에서 제안한 방법은 임상에서 MRI자장의 세기가 커질수록 RF코일 내부의 RF B1 균질성이 현저히 떨어지는 문제점이 있는데 이를 개선하는데 적용 할 수 있다고 사료된다.

• 한국초전도저온공학회:학술대회논문집
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• 한국초전도저온공학회 1999년도 제1회 학술대회논문집(KIASC 1st conference 99)
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• pp.113-116
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• 1999

The shield effects of the actively shielded superconducting magnet systems for MRI were investigated. The magnetic field was calculated by FEM considering the winding error and the homogeneity of the magnetic field at the 30cm DSV was presented. The 5 gauss stray field line was restricted within 5m form the magnet center.

• 한국초전도저온공학회:학술대회논문집
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• 한국초전도저온공학회 2001년도 학술대회 논문집
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• pp.178-181
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• 2001

Two methods can be used to correct the undesirable magnetic field of MRI. One is active shimming method and the other is ferro-magnetic shimming. Ferro-magnetic shimming method is more inexpensive, more convenient in operation and more effective on correcting magnetic field. So, nowadays, it is the general method for shimming the commercialized MRI magnet. We have developed a 1.5T MRI magnet and its ferromagnetic shimming system. Using the ferro-magnetic shimming system, we have improved the field homogeneity of the 1.5T MRI magnet.

• 한국초전도ㆍ저온공학회논문지
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• 제18권1호
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• pp.50-54
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• 2016

In this paper, a hybrid method is proposed to design an air-core superconducting solenoid system for 6 T axial uniform magnetic field using Niobium Titanium (NbTi) superconducting wire. In order to minimize the volume of conductor, the hybrid optimization method including a linear programming and a nonlinear programming was adopted. The feasible space of solenoid is divided by several grids and the magnetic field at target point is approximated by the sum of magnetic field generated by an ideal current loop at the center of each grid. Using the linear programming, a global optimal current distribution in the feasible space can be indicated by non-zero current grids. Furthermore the clusters of the non-zero current grids also give the information of probable solenoids in the feasible space, such as the number, the shape, and so on. Applying these probable solenoids as the initial model, the final practical configuration of solenoids with integer layers can be obtained by the nonlinear programming. The design result illustrates the efficiency and the flexibility of the hybrid method. And this method can also be used for the magnet design which is required the high homogeneity within several ppm (parts per million).

• 한국초전도저온공학회:학술대회논문집
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• 한국초전도저온공학회 2000년도 KIASC Conference 2000 / 2000년도 학술대회 논문집
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• pp.150-153
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• 2000

NMR researches are required high field and high homogeneous super-conducting magnet. Thus superconducting magnets for NMR applications are designed with minimization of coil winding volume satisfied constraints such as field strength, field homogeneity, etc. In this paper, we are discussed optimal design of high field super-conducting magnet for NMR applications. For a design example, we designed unshielded superconducting magnet for 600MHz NMR spectrometer with 100mm room temperature bore size and obtained 14.1011[T] field strength and 1.33 ppm field homogeneity.

• 한국초전도ㆍ저온공학회논문지
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• 제11권1호
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• pp.20-24
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• 2009

The superconducting property measurement system is used to acquire electrical and thermal properties on short HTS tape samples and the system is composed of specimen holder for mounting HTS tape and a magnet for applying magnetic fields externally. The magnet consists of two split racetrack windings and is designed to produce maximum 3T of center field. The temperature of specimen holder can be varied in range from 10K to 77K. The field homogeneity is required less than 300 gauss stray field contour within 20cm axially and 3cm radially from origin. We have worked on the conceptual designs of the conduction-cooled magnet for the superconducting characteristic measurement system. The measurement system will be fabricated in near future based on the design parameters presented in this paper.

• Investigative Magnetic Resonance Imaging
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• 제24권3호
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• pp.95-122
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• 2020

In this article, we evaluated the performance of radiofrequency (RF) coils in terms of the signal-to-noise ratio (S/N) and homogeneity of magnetic resonance images when used for ultrahigh-frequency (UHF) 7T magnetic resonance imaging (MRI). High-quality MRI can be obtained when these two basic requirements are met. However, because of the dielectric effect, 7T magnetic resonance imaging still produces essentially a non-uniform magnetic flux (|B₁|) density distribution. In general, heterogeneous and homogeneous RF coils may be designed using electromagnetic (EM) modeling. Heterogeneous coils, which are surface coils, are used in consideration of scalability in the |B₁| region with a high S/N as multichannel loop coils rather than selecting a single loop. Loop coils are considered state of the art for their simplicity yet effective |B₁|-field distribution and intensity. In addition, combining multiple loop coils allows phase arrays (PA). PA coils have gained great interest for use in receiving signals because of parallel imaging (PI) techniques, such as sensitivity encoding (SENSE) and generalized autocalibrating partial parallel acquisition (GRAPPA), which drastically reduce the acquisition time. With the introduction of a parallel transmit coil (pTx) system, a form of transceiver loop arrays has also been proposed. In this article, we discussed the applications and proposed designs of loop coils. RF homogeneous coils for volume imaging include Alderman-Grant resonators, birdcage coils, saddle coils, traveling wave coils, transmission line arrays, composite right-/left-handed arrays, and fusion coils. In this article, we also discussed the basic operation, design, and applications of these coils.

• 전기학회논문지
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• 제65권10호
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• pp.1727-1730
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• 2016

Magnetic resonance imaging has a potential to produce clear anatomical as well as functional images of human body. However, the ability to diagnose is limited by signal to noise ratio (SNR) and the resolution of current medical systems. To remove the challenges prevalent due to the use of high field scanners, dedicated radio frequency coils are used. Transverse electromagnetic coils have an advantage of providing homogeneous magnetic field throughout the region but with low signal to noise ratio while surface coils have an advantage of providing higher signal to noise ratio but with low homogeneity. This research combines both the advantage into one by utilizing transmit only transverse electromagnetic radio frequency coils (8 channel) along with receive only surface coils (by varying the number) for better imaging of brain. A 7 Tesla 32-channel close fitting helmet shaped phased-array surface coils along with the combination of 8 channel transmit only transverse electromagnetic coils provided good homogeneity as well as significant SNR improvements throughout the human brain.

• 전자공학회논문지SC
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• 제48권6호
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• pp.57-62
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• 2011

본 논문에서는 초전도 자석의 자장 균일도를 개선하기 위한 방법으로 3가지 형태의 magnet 모델을 제안하고 각각의 자석 형태에 대하여 같은 세기의 자장을 (Magnet field strength) 가질 경우에 최소전력 방식으로 최적화된 전류 분포에 해당하는 coil wire의 길이, 그리고 해당 조건에서의 자장의 불균일도를 시뮬레이션을 통하여 비교, 분석하였다. 구성된 3가지 magnet type을 동일한 조건 (계산 점의 개수 18개, 20cm DSV)에 대해서 wire길이와 main field inhomogeneity를 비교하였으며, 이러한 시뮬레이션 결과를 통하여 얻을 수 있는 결론은 계산점의 수가 적을수록 wire의 길이는 짧아지나 field inhomogeneity는 높아진다는 것이다. 즉, Magnet shim을 수행할 경우 계산점을 줄이는 방법으로는 짧은 wire의 길이와 main field homogeneity를 동시에 만족하도록 최적화 하는 것이 거의 불가능함을 의미하는 것이다. 그러나 DSV를 줄였을 경우에 계산점을 줄였을 때에 비해 우수한 결과 값을 얻을 수 있었다. 결론적으로 공간적으로 개방되어 있는 magnet model의 경우 계산점을 줄여 shimming을 진행할 경우 동일한 imaging region의 크기에 대해 더 많은 전류(또는 wire 길이)가 필요하고 field 균일도도 떨어졌으나 작은 ROI를 대상으로 영상을 얻는 경우 유용하게 사용될 수 있다.