• Acta Physica Sinica
  • Vol. 68, Issue 18, 188401-1 (2019)
Wei Shi*, Qiang Zhou, and Bin Liu
DOI: 10.7498/aps.68.20190339 Cite this Article
Wei Shi, Qiang Zhou, Bin Liu. Performance analysis of spinning magnet as mechanical antenna[J]. Acta Physica Sinica, 2019, 68(18): 188401-1 Copy Citation Text show less
Schematic illustration of permanent magnet and equivalent magnetic dipole: (a) Permanent magnet; (b) equivalent magnetic dipole.永磁体和等效磁偶极子坐标示意图 (a) 永磁体; (b) 电流环(磁偶极子)
Fig. 1. Schematic illustration of permanent magnet and equivalent magnetic dipole: (a) Permanent magnet; (b) equivalent magnetic dipole.永磁体和等效磁偶极子坐标示意图 (a) 永磁体; (b) 电流环(磁偶极子)
Variation of |Bz| versus distance (rectangular permanent magnet and ideal magnetic dipole): (a) y = 0, z = 0, along x-axis; (b) x = 0, z = 160 mm, along y-axis; (c) x = 0, y = 0, along z-axis; (d) x = 0, y = 180 mm, along z-axis.|Bz|随距离的变化(矩形永磁体和理想磁偶极子) (a) y = 0, z = 0, 沿x轴变化; (b) x = 0, z = 160 mm, 沿y轴变化; (c) x = 0, y = 0, 沿z轴变化; (d) x = 0, y = 180 mm, 沿z轴变化
Fig. 2. Variation of |Bz| versus distance (rectangular permanent magnet and ideal magnetic dipole): (a) y = 0, z = 0, along x-axis; (b) x = 0, z = 160 mm, along y-axis; (c) x = 0, y = 0, along z-axis; (d) x = 0, y = 180 mm, along z-axis. |Bz|随距离的变化(矩形永磁体和理想磁偶极子) (a) y = 0, z = 0, 沿x轴变化; (b) x = 0, z = 160 mm, 沿y轴变化; (c) x = 0, y = 0, 沿z轴变化; (d) x = 0, y = 180 mm, 沿z轴变化
Schematic illustration of the equivalence between spinning permanent magnet and spinning magnetic dipole: (a) Spinning permanent magnet; (b) spinning magnetic dipole.旋转永磁体与旋转磁偶极子的等效 (a) 旋转永磁体; (b) 旋转磁偶极子
Fig. 3. Schematic illustration of the equivalence between spinning permanent magnet and spinning magnetic dipole: (a) Spinning permanent magnet; (b) spinning magnetic dipole.旋转永磁体与旋转磁偶极子的等效 (a) 旋转永磁体; (b) 旋转磁偶极子
Schematic illustration of the equivalence between spinning magnet dipole and orthogonal magnetic dipoles: (a) Spinning magnet dipole; (b) orthogonal magnetic dipoles; (c) orthogonal magnetic currents旋转磁偶极子与正交磁流元的等效关系 (a) 旋转磁偶极子; (b) 正交磁偶极子; (c) 正交磁流元
Fig. 4. Schematic illustration of the equivalence between spinning magnet dipole and orthogonal magnetic dipoles: (a) Spinning magnet dipole; (b) orthogonal magnetic dipoles; (c) orthogonal magnetic currents旋转磁偶极子与正交磁流元的等效关系 (a) 旋转磁偶极子; (b) 正交磁偶极子; (c) 正交磁流元
Coordinate system of the orthogonal electric dipoles.正交电偶极子的坐标系
Fig. 5. Coordinate system of the orthogonal electric dipoles.正交电偶极子的坐标系
Results comparison between the proposed method and the formula in Ref. [13] (along x-axis, the spherical coordinate parameters: , ).两种计算方法的结果对比(沿x轴, 球坐标变量为, )
Fig. 6. Results comparison between the proposed method and the formula in Ref. [13] (along x-axis, the spherical coordinate parameters: , ). 两种计算方法的结果对比(沿x轴, 球坐标变量为 , )
Simulated magnetic flux density versus distance: (a) Air; (b) seawater.旋转永磁体的磁感应强度随距离的变化 (a) 空气; (b) 海水
Fig. 7. Simulated magnetic flux density versus distance: (a) Air; (b) seawater. 旋转永磁体的磁感应强度 随距离的变化 (a) 空气; (b) 海水
Variation of simulated magnetic flux density with material and frequency: (a) 160 Hz; (b) seawater.旋转永磁体磁感应强度的一般变化规律 (a) 160 Hz; (b) 海水
Fig. 8. Variation of simulated magnetic flux density with material and frequency: (a) 160 Hz; (b) seawater. 旋转永磁体磁感应强度的一般变化规律 (a) 160 Hz; (b) 海水
Spinning permanent magnets array with two elements.旋转永磁体二元阵列
Fig. 9. Spinning permanent magnets array with two elements.旋转永磁体二元阵列
Performance comparison between spinning magnet array and single spinning magnet: (a) Along x-axis, the spherical coordinate parameters , ; (b) magnetic near field pattern at the horizontal plane (d = 50 m, r = 1000m, )二元旋转永磁体和单个旋转永磁体的场强对比 (a) 沿x轴, 球坐标变量为, ; (b) 近场水平面方向图(d = 50 m, r = 1000 m, )
Fig. 10. Performance comparison between spinning magnet array and single spinning magnet: (a) Along x-axis, the spherical coordinate parameters , ; (b) magnetic near field pattern at the horizontal plane (d = 50 m, r = 1000m, ) 二元旋转永磁体和单个旋转永磁体的场强对比 (a) 沿x轴, 球坐标变量为 , ; (b) 近场水平面方向图(d = 50 m, r = 1000 m, )
Simulated magnetic flux density in the elevation plane.二元阵列俯仰面磁场分布
Fig. 11. Simulated magnetic flux density in the elevation plane. 二元阵列俯仰面磁场分布
Simulated magnetic flux density of the spinning magnet array with two elements: (a) r = 1000 m; (b) r = 2000 m.改变初始旋转角, 二元阵列的水平面磁场方向图(a) r = 1000 m; (b) r = 2000 m
Fig. 12. Simulated magnetic flux density of the spinning magnet array with two elements: (a) r = 1000 m; (b) r = 2000 m. 改变初始旋转角, 二元阵列的水平面磁场方向图(a) r = 1000 m; (b) r = 2000 m
Wei Shi, Qiang Zhou, Bin Liu. Performance analysis of spinning magnet as mechanical antenna[J]. Acta Physica Sinica, 2019, 68(18): 188401-1
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