基于电磁弹簧的隔振方案

IF 0.2 Q4 MULTIDISCIPLINARY SCIENCES Suranaree Journal of Science and Technology Pub Date : 2023-04-26 DOI:10.55766/sujst-2023-02-e01602
P. Thamboon, Tanatip Mayoon, N. Tanasanchai, Puripong Suthisopapan, Waranont Anukool
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引用次数: 0

摘要

敏感的测量需要隔振系统来防止有害的震动。两种类型的隔振系统-被动和主动-目前实施。基于弹簧的无源设计通常伴随着无效的低频响应。因此,由传感器、反馈控制系统和执行器组成的主动设计被整合,以提高抵消性能的总体有效性。在这项工作中,我们重点开发了基于电磁弹簧的致动器,并将其集成到我们的紧凑型量子重力仪中。每个弹簧驱动部分包括两个排斥性钕磁铁,它们面对面地放置在螺线管内。通过这种配置,弹簧也可以通过排斥磁力在被动模式下工作。在主动模式下,施加的力是由磁铁和电流控制的螺线管线圈形成的磁场的结果。通过改变线圈电流,可以改变弹簧的刚度,从而可以控制位移。研究了不同尺寸的磁体,并对其在被动和主动模式下的受力行为进行了表征。讨论了量子重力仪中致动器的实现方案。
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VIBRATION ISOLATION SCHEME BASED ON ELECTROMAGNETIC SPRING
Sensitive measurements require a vibration isolation system to safeguard against detrimental tremble. Two types of vibration isolation systems - passive and active - are currently implemented. The spring-based passive designs usually accompany with ineffective low-frequency response. Therefore, the active designs, consisting of sensors, feedback control systems, and actuators, are consolidated to improve the total effectiveness of the cancellation performance. In this work, we focus on developing the actuator founded on electromagnetic spring to be incorporated into our compact quantum gravimeter. Each spring-actuated part comprises two repelling Nd magnets positioned face to face inside a solenoid. With this configuration, the spring can also work in the passive mode via repulsive magnetic force. In the active mode, the exerted force is a result of magnetic fields formed by the magnets and the current-controlled solenoid coils. By changing the coil current, the stiffness of the spring can be modified, and thus the displacement can be controlled.  Different sizes of magnets are explored, and their force behaviors in passive and active modes are characterized. The implementation scheme of the actuator in the quantum gravimeter is also discussed.
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来源期刊
Suranaree Journal of Science and Technology
Suranaree Journal of Science and Technology MULTIDISCIPLINARY SCIENCES-
CiteScore
0.30
自引率
50.00%
发文量
0
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