### 抄録

The magnetic field distributions of an HTS bulk magnet system were precisely measured between the face-to-face 3.4-T magnetic poles. After the activation by 5-T field cooling magnetization, the magnetic flux density has reached the value of 2.26 T at the center of the 34-mm gap. The sum of the local magnetic fields generated from each magnetic pole coincides with the local field strength in the gap. We estimated the homogeneity of the magnetic flux densities of B_{z} and B_{y}, which were measured at various positions along z and y-axes in the center portion of the 60-mm gap. Since the magnetic flux density becomes smooth with increasing distance, we obtained the smallest distribution range of 123 ppm of Bz = 1.62 T at the center of the gap as for B_{z}. On the other, as for B_{y}, the smallest distribution range of 1125 ppm of B_{z} = 1.20 T was obtained at z = 1.7 mm distant from the center point. Since there must exist a certain plane which has no vector components along the radius direction at the center of the gap, the closer the z-positions come to the null point, the more homogeneous the field distribution becomes.

元の言語 | English |
---|---|

記事番号 | 6626624 |

ジャーナル | IEEE Transactions on Applied Superconductivity |

巻 | 24 |

発行部数 | 3 |

DOI | |

出版物ステータス | Published - 2014 1 1 |

外部発表 | Yes |

### Fingerprint

### ASJC Scopus subject areas

- Electronic, Optical and Magnetic Materials
- Condensed Matter Physics
- Electrical and Electronic Engineering

### これを引用

*IEEE Transactions on Applied Superconductivity*,

*24*(3), [6626624]. https://doi.org/10.1109/TASC.2013.2284859

**Strong magnetic field generator containing HTS bulk magnets and compact refrigerators.** / Oka, Tetsuo; Hirayama, Eri; Kanai, Tomoaki; Ogawa, Jun; Fukui, Satoshi; Sato, Takao; Yokoyama, Kazuya; Nakamura, Takashi.

研究成果: Article

*IEEE Transactions on Applied Superconductivity*, 巻. 24, 番号 3, 6626624. https://doi.org/10.1109/TASC.2013.2284859

}

TY - JOUR

T1 - Strong magnetic field generator containing HTS bulk magnets and compact refrigerators

AU - Oka, Tetsuo

AU - Hirayama, Eri

AU - Kanai, Tomoaki

AU - Ogawa, Jun

AU - Fukui, Satoshi

AU - Sato, Takao

AU - Yokoyama, Kazuya

AU - Nakamura, Takashi

PY - 2014/1/1

Y1 - 2014/1/1

N2 - The magnetic field distributions of an HTS bulk magnet system were precisely measured between the face-to-face 3.4-T magnetic poles. After the activation by 5-T field cooling magnetization, the magnetic flux density has reached the value of 2.26 T at the center of the 34-mm gap. The sum of the local magnetic fields generated from each magnetic pole coincides with the local field strength in the gap. We estimated the homogeneity of the magnetic flux densities of Bz and By, which were measured at various positions along z and y-axes in the center portion of the 60-mm gap. Since the magnetic flux density becomes smooth with increasing distance, we obtained the smallest distribution range of 123 ppm of Bz = 1.62 T at the center of the gap as for Bz. On the other, as for By, the smallest distribution range of 1125 ppm of Bz = 1.20 T was obtained at z = 1.7 mm distant from the center point. Since there must exist a certain plane which has no vector components along the radius direction at the center of the gap, the closer the z-positions come to the null point, the more homogeneous the field distribution becomes.

AB - The magnetic field distributions of an HTS bulk magnet system were precisely measured between the face-to-face 3.4-T magnetic poles. After the activation by 5-T field cooling magnetization, the magnetic flux density has reached the value of 2.26 T at the center of the 34-mm gap. The sum of the local magnetic fields generated from each magnetic pole coincides with the local field strength in the gap. We estimated the homogeneity of the magnetic flux densities of Bz and By, which were measured at various positions along z and y-axes in the center portion of the 60-mm gap. Since the magnetic flux density becomes smooth with increasing distance, we obtained the smallest distribution range of 123 ppm of Bz = 1.62 T at the center of the gap as for Bz. On the other, as for By, the smallest distribution range of 1125 ppm of Bz = 1.20 T was obtained at z = 1.7 mm distant from the center point. Since there must exist a certain plane which has no vector components along the radius direction at the center of the gap, the closer the z-positions come to the null point, the more homogeneous the field distribution becomes.

KW - Bulk superconductor

KW - Field distribution

KW - Magnetic field generator

KW - Refrigerator

UR - http://www.scopus.com/inward/record.url?scp=84904598034&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=84904598034&partnerID=8YFLogxK

U2 - 10.1109/TASC.2013.2284859

DO - 10.1109/TASC.2013.2284859

M3 - Article

AN - SCOPUS:84904598034

VL - 24

JO - IEEE Transactions on Applied Superconductivity

JF - IEEE Transactions on Applied Superconductivity

SN - 1051-8223

IS - 3

M1 - 6626624

ER -