• Title/Summary/Keyword: MRI Coil

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Experimental study of open head coil in vertical field MRI (수직자계 MRI용 개방형 머리영상 코일에 대한 실험적 연구)

  • Yi, J.H.;Kang, D.H.;Kim, J.H.;Yi, W.
    • Proceedings of the KOSOMBE Conference
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    • v.1996 no.05
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    • pp.108-110
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    • 1996
  • Open MRI is a new concept in clinical application of the MRI such as interventional study. Receiving RF coils used in the open MRI must have open structures to insure convenient manipulations fur the patient. In this paper, we presented experimental study fur open head coil suitable to 0.3 Tesla vertical field MRI system with its experimental results.

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Design and Test Results of an Actively Shielded Superconducting Magnet for Magnetic Resonance Imaging

  • Jin, Hong-Beom;Ryu, Kang-Sik;Oh, Bong-Hwan;Ryu, Kyung-Woo;Jeoun, In-Young
    • Journal of Electrical Engineering and information Science
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    • v.2 no.6
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    • pp.95-105
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    • 1997
  • In this paper, we have studied about design and fabrication of the actively shielded superconducting MRI magnet. Nonlinear optimization methods are usually used to find optimum coil configurations. However the selection of initial coil configurations is very difficult. In case bad initial data are used, it is even impossible to find optimum coil configurations which satisfy predefined constraints. We have developed computer optimization program which consists of two steps. Initial coil configurations are easily selected through linear optimization in the first step and optimum coil configurations are found through nonlinear optimization in the second step. We have also studied about superconducting shim coils to cancel error fields caused by coil fabrication errors. Many researchers published design concepts of shim coil. However all these studies are for shim coil design using filamentary coils with single turn, Shim coils with multi-turns should be used to produce enough field strength to cancel error fields. We have developed computer program for the design of shim coils which have proper thickness and length. An actively shielded superconducting MRI magnet with a small warm bore was fabricated and four sets of superconducting shim coils were equipped. The magnetic field distributions were measured and field correction was carried out using shim coils.

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Surface Gradient/RF Coil Set for High-Resolution Skin MRI

  • 한재호;김용권;오정민;박상용;오칠환;최보영;오창현
    • Proceedings of the KSMRM Conference
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    • 2003.10a
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    • pp.74-74
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    • 2003
  • 목적: 피부표면에 가까운 고분해능 MR 영상을 얻기 위하여는 Surface RF Coil과 강력한 경사자계를 갖는 Gradient Coil이 필수적으로 요구된다. 본 연구에서는 High-Resolution MR Imaging을 위해 surface RF Coil과 Surface Gradient Coil을 제안하였다. Target Field Method를 사용하여 Gradient Coil의 전력 소모를 최소화하였으며 MR Microscopy가 가능한 50 mm∼100 mm의 해상도가 가능하도록 Coil을 설계하였다.

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A simulation-based design study of superconducting zonal shim coil for a 9.4 T whole-body MRI magnet

  • Kim, Geonyoung;Choi, Kibum;Park, Jeonghwan;Bong, Uijong;Bang, Jeseok;Hahn, Seungyong
    • Progress in Superconductivity and Cryogenics
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    • v.22 no.1
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    • pp.12-16
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    • 2020
  • As high homogeneity in magnetic field is required to increase the resolution of MRI magnets, various shimming methods have been researched. Using one of them, the design of the superconducting active zonal shim coil for MRI magnets is discussed in this paper. The magnetic field of the MRI magnet is expressed as the sum of spherical harmonic terms, and the optimized current density of shim coils capable of removing higher-order terms is calculated by the Tikhonov regularization method. To investigate all potential designs derived from calculated current density, 4 sweeping parameters are selected: (1) axial length of shim coil zone; (2) radius of shim coils; (3) exact axial position of shim coils; and (4) operating current. After adequate designs are determined with constraints of critical current margin and homogeneity criterion, the total wire length required for each is calculated and the design with a minimum of them is chosen. Using the superconducting wire length of 9.77 km, the field homogeneity over 50 cm DSV is improved from 24 ppm to 1.87 ppm in the case study for 9.4 T whole-body MRI shimming. Finally, the results are compared with the finite element method (FEM) simulation results to validate the feasibility and accuracy of the design.

FDTD 방법을 이용한 3T MRI용 RF 코일의 해석

  • 이종오;박준서;명노훈;박부식;김용권;정성택
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.11 no.6
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    • pp.976-983
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    • 2000
  • In this paper, Bridcage type RF coils used widely as RF coils for MRI and its applicable type, spiral type RF coil are analyzed and designed using FDTD method. In low tesla (IT, 1.5T) MRI system, several tools have been used for the analysis and design of the RF coils for MRI. This includes, so-called, LC equivalent circuit method for predicting the resonance frequency of the coil and the Biot-Savart law to determine the field distribution within the coil. Both of the circuit analysis and Biot-Savart law are low frequency techniques. Therefore, at high frequency applications, the circuit model approximation breaks down because the coil geometry is a significant fraction of the wavelength. In this paper, we analyzed and designed RF coils for 3T MRI using FDTD method. This method is a full wave analysis and very accurate at low and high frequencies. Also, this RF coils are actually fabricated and FDTD models of RF coils for MRI are proven.

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The Birdcage coil for small object in 3T MRI

  • 추명자;최보영;이형구;서태석
    • Proceedings of the KSMRM Conference
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    • 2001.11a
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    • pp.177-177
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    • 2001
  • 목적: Head coil이나 Knee coil로 촬영하기에 부피가 작은 신체의 부위나 동물을 촬영하기 위하여 3T small birdcage coil을 개발하고 실험을 통해 코일의 효율성을 조사하였다. 대상 및 방법: 원통형 아크릴과 구리테이프를 사용하여 원통의 내경이 Knee coil보다 작은 8개의 elements를 가진 birdcage coil을 설계 제작하였고 팬톰, 지원자, 동물에 대한 MR 영상으로 그 가치를 평가하였다.

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B1+ Comparison for Different RF Coils at 7 T MRI (7 T MRI에서의 다양한 RF 코일에 대한 B1+ 비교)

  • Kim, Hong-Joon;Yoo, Hyoung-Suk
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.23 no.8
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    • pp.1010-1013
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    • 2012
  • This paper demonstrates the use of the convex optimization to localize the transverse magnetic $B_1^+$ field in regions of interest for recently proposed multi-sectioned alternating impedance coils and the traditional transmission line coil. An approach based on different axial slices to identical RF coils except upper stripline structure is investigated. Electromagnetic simulation results are compared for RF coils and discussed in detail at 7.0 T.

The Treatment of Giant Middle Cerebral Artery Aneurysm with MDS Coil - Case Report - (기계적 분리코일(MDS coil)을 이용한 소아 거대 중대뇌동맥류의 치료)

  • Choi, Gwang-Shik;Kim, Sung-Ho;Bae, Jang-Ho;Kim, O-Lyong;Choi, Byung-Youn;Cho, Soo-Ho;Byun, Woo-Mok
    • Journal of Yeungnam Medical Science
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    • v.14 no.1
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    • pp.237-244
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    • 1997
  • A 14-year old boy was admitted with stuporous mentality. CT scan, MRI and cerebral angiogram revealed SAH and a giant aneurysm of right middle cerebral artery($4{\times}5{\times}5.3cm$). To minimize surgical risk, endovascular treatment was done with MDS(mechanical detachable system)-spiral coil. Follow up MRI showed intraluminal thrombus formation of the aneurysm.

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Signal Intensity Changes according to Coil Position Changes in MRI using 6 Channel SENSE Cardiac Array Coils (6채널 SENSE Cardiac Array 코일을 이용한 검사 시 코일의 위치 변화에 따른 신호강도)

  • Choi, Kwan-Woo;Son, Soon-Yong;Yoo, Beong-Gyu
    • Journal of the Korean Society of Radiology
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    • v.12 no.5
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    • pp.699-706
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    • 2018
  • In this study, we measured signal intensities according to array coil position changes to provide reference data of coil directions and the distances as it deters image quality unless the coils are aligned properly. The multi-purpose MRI phantom was placed in body array coils, and it was moved to the top, bottom, left, and right directions by 2 cm from the center to 10 cm. After obtaining images, signal intensities were measured and compared. The results of this study were as follows: Except for the upward direction, the signal intensities of the reference signal was not significantly different from that of the reference signal intensity within 2cm in both T1 and T2-weighted images. In conclusion, in clinical circumstances which various challenges exist to align the coils exactly on the same lines, array coils should be positioned at least within 2 cm from the center except for the upward direction, on the same line to prevent the image qualities are lowered.