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相关概念视频

Magnetic Damping01:17

Magnetic Damping

451
Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
451
Diamagnetism01:26

Diamagnetism

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Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
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The Hall Effect01:30

The Hall Effect

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Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
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Magnetic Field Of A Current Loop01:16

Magnetic Field Of A Current Loop

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Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
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Magnetic Field Due To A Thin Straight Wire01:28

Magnetic Field Due To A Thin Straight Wire

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Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
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Magnetic Field Due to Two Straight Wires01:18

Magnetic Field Due to Two Straight Wires

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Consider two parallel straight wires carrying a current of 10 A and 20 A in the same direction and separated by a distance of 20 cm. Calculate the magnetic field at a point "P2", midway between the wires. Also, evaluate the magnetic field when the direction of the current is reversed in the second wire.
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微型双翼∆E效应磁场传感器

Fatih Ilgaz1, Elizaveta Spetzler2, Patrick Wiegand3

  • 1Chair for Multicomponent Materials, Department of Materials Science, Faculty of Engineering, Kiel University, 24143, Kiel, Germany.

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概括

研究人员开发了一种用于磁弹性微电机系统 (MEMS) 的新方法,以克服压力诱导的问题. 这项创新显著提高了先进传感器和执行器的设备可重现性和性能.

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科学领域:

  • 材料科学 材料科学 材料科学
  • 微电子机械系统 (MEMS) 是一种微电子机械系统.
  • 磁力学 磁力学 是一种

背景情况:

  • 磁弹性MEMS依赖于磁阻力,但对应力诱导的磁性异性质敏感.
  • 制造过程引起的残余应力会损害设备的可重复性,性能和磁弹性层中的产量.
  • 尽量减少应力对于可靠和高性能磁弹性装置至关重要.

研究的目的:

  • 开发一种制造技术,防止残余应力转移到磁弹性层.
  • 为了研究在最小化压力条件下磁电微振解器的性能.
  • 为了提高磁弹性MEMS设备的可复制性和灵敏度.

主要方法:

  • 利用阴影面具沉积技术,以防止应力转移到磁层.
  • 采用免费的磁电微共振器设计,以减轻磁不均性.
  • 进行了磁电共振器的实验和理论分析,重点是应力异性质,磁性异性质和 ΔE 效应灵敏度.

主要成果:

  • 实现了非常小的设备对设备共振频率变化 (<0.2%).
  • 具有高的 ΔE 效应灵敏度,与宏观磁场传感器相当.
  • 验证了阴影面具沉积和自由无共振器设计的有效性.

结论:

  • 开发的方法显著提高了磁弹性装置的可重复性.
  • 这种方法为大规模的高性能磁弹性MEMS集成阵列铺平了道路.
  • 这些发现代表了磁弹性传感器和执行器的实际应用的有希望的进步.