为生物医学磁刺激设计的脉冲磁通密度传感器

M. Yarita
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引用次数: 1

摘要

生物医学磁刺激应用广泛。然而,目前还没有合适的刺激强度测量方法可供临床应用。提出了一种由2an2传感器线圈和2Oms时间常数积分器组成的脉冲磁通密度测量传感器(PMFS)。该PMFS无需电源即可工作,可以简单地用于临床磁刺激。高磁通密度和频繁的磁刺激使大鼠头部皮层神经区产生微空泡改变[1]。测量磁刺激前后的刺激强度是磁刺激的基本要求。但是,没有提供适当的刺激强度指标,而是使用最大输出的%或电容器组充电电压。为了解决上述问题,本文提出了能够测量磁通量密度B及其时间导数dB/dt[2]作为刺激强度指标的PMFS。方法对传感器线圈尺寸进行优化设计。1:计算环形激励线圈的磁通密度分布Bz(内半径33.5mm,外半径54mm,N=9匝,电流I4600A)。2:计算不同传感器线圈尺寸的Bz畸变。3:设计了原型PMFS。Fig.lA。刺激线圈的多边形近似。.Fig.lB (K = 32)。d. 1点处磁通密度B由Biot Savart定律计算:磁通密度Bz由式(1)计算。采用多边形近似法(图1,K=32)和BiotSavart定律计算每个多边形段的磁通密度。每个多边形段的磁通密度贡献在一个观测点求和。2:有限传感器线圈测量的磁通密度分布Bz畸变如图2所示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Pulse magnetic flux density sensor designed for biomedical magnetic stimulation
Biomedical magnetic stimulations are widely used. However, proper stimulus intensity measurement has not been provided for clinical application. This paper proposes a Pulse Magnetic Flux density measuring Sensor (PMFS) that consists of 2an2 sensor coil and 2Oms time constant integrator. This PMFS works without the need of power supply which allows simple use for clinical magnetic stimulation. Introduction High magnetic flux density and frequent magnetic stimulations to rat heads produced microvacuolar changes on the neuropil portion of cortex [l]. It is an essential requirement for magnetic stimulation to measure the stimulus intensity before and after the practices. However, proper stimulus intensity index is not provided but using % of the maximum output or the capacitor bank charged voltage . As a solution to the raised problem, this paper proposes the PMFS that is able to measure magnetic flux density B and its time derivative dB/dt [2) as stimulus intensity indexes. Methods An optimal sensor coil size design is investigated. 1: Magnetic flux density distribution Bz by a donut shaped stimulation coil is calculated (inner radius 33.5mm,outer radius 54mm,N=9 turns, current I4600A). 2: Bz distortions by various sensor coil sizes are calculated. 3:Prototype PMFS is designed. Fig.lA. Polygon approximation for the stimulation coil. (K=32).Fig.lB. Magnetic flux density B calculation by Biot Savart’s law at the point d. 1:Magnetic flux density Bz is calculated by Eq.(l). A polygon approximation (Fig.l,K=32) and BiotSavart’s law are applied for the magnetic flux density calculations by each polygon segment. The magnetic flux density contributions from each polygon semnent are summed at an observation point. 2:Flux density distributions Bz measured by finite sensor coils are distorted as Bzs as Fig.2.
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