共查询到15条相似文献,搜索用时 140 毫秒
1.
根据理想封闭矩形腔体内电磁场表达式,分析了对混响室内场特性有影响的因素;结合混响室的参数要求,对混响室模型的设计进行了研究,并确立了适用于短脉冲激励下的混响室的场均匀性分析指标;通过对比电场分布的均匀性,重点研究腔体形状和源搅拌方法对腔体内场分布的影响,采用连续10次移动激励源的方法可以将场分布标准差降低约0.4 dB。数值模拟结果表明:采用类似复杂腔的结构,在矩形腔的基础上引入若干复杂结构,可以有效地提高场分布的均匀性,有利于在腔内构造均匀的电磁环境;证明了连续移动激励源位置这一源搅拌方法的可行性,通过该方法可以有效地提高场分布的均匀性。 相似文献
2.
研究了在短脉冲波激励下,源搅拌方法对混响室内场分布的影响效果。分析了混响室内场分布特征的影响因素,得到了影响源搅拌的相关参量。研究改变激励源的位置对腔体内场分布的影响效果,主要对比了电场的最大值、分布标准差等电场统计特征。结果表明:通过连续地移动激励源对场分布进行搅拌,混响室内的电场最大值可以达到约6.7 kV/m,而且场值的空间分布标准差降至3 dB以下,能量分布也更加均衡。因此,采用源搅拌方法可以有效地改善腔内的场分布,提高场分布的均匀性,有利于构造均匀的电磁场环境。 相似文献
3.
4.
以带有返波结构的混响室为基础,研究了在复杂腔体内部返波结构的改变对场分布的影响效果。根据微波混沌理论分析了不规则腔内的场分布特征;结合统计电磁学,确立了在高功率微波短脉冲激励下的混响室中进行场均匀性和各向同性验证的指标;对复杂腔体中返波体的大小、数量及分布范围等因素进行了研究。数值模拟结果显示:凸起结构的尺寸越大,其对腔内电场的影响效果越为明显,尤其是腔内电场分布的统计均匀性和各向同性结果,都能得到很好的改善。同时凸起结构越多,分布的范围越广,腔内电场的统计均匀性和能流的统计均衡性就越好。 相似文献
5.
以带有返波结构的混响室为基础,研究了在复杂腔体内部返波结构的改变对场分布的影响效果。根据微波混沌理论分析了不规则腔内的场分布特征;结合统计电磁学,确立了在高功率微波短脉冲激励下的混响室中进行场均匀性和各向同性验证的指标;对复杂腔体中返波体的大小、数量及分布范围等因素进行了研究。数值模拟结果显示:凸起结构的尺寸越大,其对腔内电场的影响效果越为明显,尤其是腔内电场分布的统计均匀性和各向同性结果,都能得到很好的改善。同时凸起结构越多,分布的范围越广,腔内电场的统计均匀性和能流的统计均衡性就越好。 相似文献
6.
从本征模的角度阐明了频率搅拌技术的混响原理,并根据激励信号的频域特征,系统研究了频率搅拌方式下获取实时均匀场与统计均匀场的三种有效实现途径。选取线性扫频这一搅拌方式为主要研究对象,检验了混响室频率搅拌下的最低可用频率、场均匀性与统计特性三项主要技术指标。试验结果表明:线性扫频搅拌方式下,混响室的最低可用频域与机械搅拌方式基本一致;场均匀性满足IEC 61000-4-21标准规定的容差要求;场值波动规律符合理论分布模型。 相似文献
7.
使用微扰理论分析了腔体形变对谐振频率漂移的影响规律,从理论上论证了边界形变混响室的可行性,计算得到了边界形变参数对混响室空间电场均匀性的影响规律;采用了一种由柔性屏蔽布作为腔体材料、步进电机控制腔体表面形变的边界形变混响室设计方法,并对研制的几何尺寸为2.5 m×1.8 m×1.5 m的混响室的内部电场统计特性进行了试验测试。结果表明:混响室内部电场服从Rician分布,且随频率升高与理论模型的一致性变好;当形变幅度达到400 mm时,腔体内部电场扰动比大于20 dB,空间电场标准偏差小于3 dB,满足电磁兼容对混响室平台均匀性的限制要求。 相似文献
8.
9.
10.
11.
I. N. Didenkulov A. I. Martyanov N. V. Pronchatov-Rubtsov 《Bulletin of the Russian Academy of Sciences: Physics》2016,80(10):1197-1202
Results from studying the interaction between gas bubbles and the field of a flow-through acoustic resonator, and the Raman scattering of acoustic waves by moving bubbles, are presented. The structure of the distribution of bubble concentration in the resonator is studied. It is shown that nonlinear scattering by moving bubbles can be used to image bubble objects. 相似文献
12.
An optimally arranged multiple-channel active-control system is known to be able to create a large quiet zone in free space for a stationary primary noise source. When the primary noise source moves, the active control of the noise becomes much more difficult, as the primary noise field changes with time in space. In this case, the controller of the control system must respond fast enough to compensate for the change; much research has been focused on this issue. In this paper, it is shown that a moving source also causes difficulties from an acoustical perspective. A moving source not only changes continuously the strengths and phases of the sound field in the space, but also changes the wavefront of the primary sound field continuously. It is known that the efficiency of active noise control is determined mainly by the wavefront matching between the primary and control fields. To keep the control system effective in the case of a moving source, the wavefront of the control field needs to change, in order to continuously match the primary-wavefront change. This paper shows that there are limitations to the control-wavefront change. An optimally pre-arranged, multiple-channel control system is not able to construct a matching wavefront when the primary source moves outside a certain range. In other words, the control system is still able to create a large quiet zone only when the primary source moves within a range around the central axis of the control system. Both the location and the size of the quiet zone change with the location of the primary source. 相似文献
13.
At high frequencies, e.g., Q- and W-bands, it is advantageous to make the axial length of loop-gap resonators (LGRs) at least as long as a free-space wavelength. The opposite scaling of capacitance and inductance with LGR length suggests that the length of an LGR can be increased without limit, with the axial radio frequency (rf) field profiles and resonance frequency independent of length. This scaling is accurate for resonator dimensions much less than one free-space wavelength. When the resonator length approaches one-tenth of a free-space wavelength, the rf field uniformity degrades. From one-tenth to one free-space wavelength, computer simulations and experimental measurements show that the axial magnetic field energy density profile is peaked in the center of the LGR, gradually decreases from 25 to 50% at a distance one radius from the end, and rapidly there-after. The nonuniformity is of two types. One type, in the vicinity of one radius of the end, is caused by the flaring of the field as it curves from the central loop to the end region, into the larger return loop(s). The other type, in the central part of the resonator, is caused by impedance mismatch at the ends of the LGR. The LGR may be viewed as a strongly reentrant (ridge) waveguide nearly open at both ends and supporting a standing wave. A transmission line model relates the central nonuniformity to the fringing capacitance and inductance at the ends of the resonator. This nonuniformity can be eliminated in several ways including modifying the ends of the LGR by adding a small metal bridge or a dielectric ring. These uniformity trimming elements increase the fringing capacitance and/or decrease the fringing inductance. With trimmed ends, LGRs can be made many free-space wavelengths long. The maximum resonator length is determined by the proximity in frequency of the fundamental LGR mode to the next highest frequency mode as well as the quality factor. Results of this theory are compared and conformed with finite-element simulations. This theory connects the uniform LGR with the uniform field cavity resonators previously introduced by this laboratory. 相似文献
14.
A. D. Lapin 《Acoustical Physics》2000,46(4):491-493
The sound field generated by a point source of volume velocity in a room with a Helmholtz resonator is determined. The shift produced by the resonator in the natural frequencies of the room is calculated. 相似文献
15.
He G Petryakov S Samouilov A Chzhan M Kuppusamy P Zweier JL 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2001,149(2):218-227
EPR spectroscopy has been applied to measure free radicals in vivo; however, respiratory, cardiac, and other movements of living animals are a major source of noise and spectral distortion. Sample motions result in changes in resonator frequency, Q, and coupling. These instabilities limit the applications that can be performed and the quality of data that can be obtained. Therefore, it is of great importance to develop resonators with automatic tuning and automatic coupling capability. We report the development of automatic tuning and automatic coupling provisions for a 750-MHz transversely oriented electric field reentrant resonator using two electronically tunable high Q hyperabrupt varactor diodes and feedback loops. In both moving phantoms and living mice, these automatic coupling control and automatic tuning control provisions resulted in an 8- to 10-fold increase in signal-to-noise ratio. 相似文献