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Correction of electric and magnetic fields and gradients measured within and around an insulating sensor capsule in seawater

机译:校正海水中绝缘传感器盒内和周围测得的电场和磁场以及梯度

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The presence of a highly conductive medium around a measurement capsule influences electromagnetic measurements made in the ocean and fundamentally alters the structure of the magnetic gradient tensor. Additional effects arise if seawater is flowing past the sensor package. This paper presents a quantitative analysis of these effects and describes the corrections that need to be applied to obtain accurate absolute measurements of electromagnetic fields and gradients in the ocean. For example, for a small spherical cavity within a 1D horizontal quasistatic electric current distribution, the electric field within the cavity is parallel to the unperturbed applied field and larger by 50%, and the magnetic field at the centre of the cavity is equal to the unperturbed magnetic field that existed at the same point in the conductive medium, prior to insertion of the measurement capsule. The symmetric magnetic gradient tensor within the cavity is uniform. If the unperturbed electric current is parallel to the x axis, the only non-zero components of the magnetic gradient tensor within the cavity are Byz = Bzy. These components are each equal to half the value of ∂By/∂z that is produced by the unperturbed current flow in the conductive medium. The external perturbation of the electric field around the cavity has the configuration of a dipole field and the external magnetic field due to the cavity is that of an elementary current dipole. An ellipsoidal cavity has an anisotropic response, except in the degenerate case where all axes are equal and the cavity is spherical. Unless the applied field lies along a principal axis of the ellipsoid, the internal field is not parallel to the applied field, but is deflected away from the major axis and towards the minor axis. An applied electric field is amplified within the cavity. For a disk-like cavity the amplification of the applied electric field normal to the disk can be very large wi--thin the cavity. The anomalous magnetic field within the ellipsoidal cavity due to electric current flow around the cavity is nonuniform, but has a uniform gradient. At the center of the ellipsoidal cavity the magnetic field is equal to the field that existed at that point before insertion of the cavity. The resultant internal magnetic gradient tensor is symmetric and traceless, as required. Seawater motion past a sensor package produces easily detectable effects that can represent an important source of electromagnetic noise. In the vicinity of a measurement capsule, water velocities of the order of 1 ms−1 produce perturbations of ∼45 µVm−1 in electric field, ∼75 pT in magnetic field, and produce magnetic gradients of ∼150 pT/m.
机译:测量胶囊周围存在高导电性介质会影响在海洋中进行的电磁测量,并从根本上改变磁梯度张量的结构。如果海水流过传感器包装,则会产生其他影响。本文对这些影响进行了定量分析,并描述了为获得海洋中电磁场和梯度的准确绝对测量值而需要进行的校正。例如,对于一维水平准静态电流分布内的小球形空腔,空腔内的电场与不受扰的外加电场平行,且电场大50%,并且空腔中心处的磁场等于在插入测量胶囊之前,存在于导电介质中同一点的无干扰磁场。腔内的对称磁梯度张量是均匀的。如果未扰动的电流平行于x轴,则腔内磁梯度张量的唯一非零分量为B yz = B zy 。这些分量分别等于∂B y /∂z的一半,后者是由导电介质中不受干扰的电流产生的。腔周围的电场的外部扰动具有偶极场的结构,并且由于腔引起的外部磁场是基本电流偶极子的场。椭圆形腔体具有各向异性的响应,除非在退化的情况下所有轴都相等并且腔体是球形。除非所施加的场沿椭圆体的主轴线放置,否则内部场不会平行于所施加的场,而是会偏离主轴线并偏向短轴。施加的电场在腔体内被放大。对于圆盘状的腔,垂直于圆盘的施加电场的放大可能会非常大。 -- 使腔变薄。由于电流在椭球腔周围流动,椭球腔内的异常磁场是不均匀的,但具有均匀的梯度。在椭圆形腔体的中心,磁场等于在腔体插入之前在该点处存在的磁场。根据需要,所得内部磁梯度张量是对称且无迹的。海水经过传感器包装会产生易于检测到的影响,这可能是电磁噪声的重要来源。在测量胶囊附近,水速为1 ms -1 时,在电场中产生的干扰约为45 µVmm -1 ,在磁场中的干扰约为75 pT。 ,产生约150 pT / m的磁梯度。

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