Department of Physics, Ryerson University, Toronto, Canada.
IEEE Trans Ultrason Ferroelectr Freq Control. 2010 Nov;57(11):2391-402. doi: 10.1109/TUFFC.2010.1707.
Magneto-acousto-electrical tomography (MAET) is a potential imaging modality which can provide high-spatial-resolution images of the impedance of conductive media. In MAET, the impedance is reconstructed from the mapped current density distribution J(ab)(r) that would exist in a sample if a current/voltage source were to be applied through measurement electrodes a and b. To map J(ab)(r) without applying a current/voltage source, the sample is placed in a static magnetic field and a focused ultrasonic pulse is directed to a point r to generate a point-like dipole source via the Lorentz force mechanism. The MAET voltage U(ab), which is directly proportional to J(ab)(r), is measured through electrodes a and b for each scanning point. To reconstruct the electrical impedance, we need to map the current density distribution at every point inside the sample. However, with the MAET experimental setup reported in our previous paper on MAET, the MAET signal from a homogenous interior of the sample is undetectable because of the spatially-oscillating nature of the ultrasound field inside the sample. In this paper, we propose to use dual-frequency ultrasound to generate the MAET signal at the difference frequency through the ultrasound radiation force mechanism. The dynamic radiation force causes vibrations inside the sample (and consequently, generates the electric field) with a wavelength much larger than the dimension of the sample along the transducer's axis. Therefore, the MAET signal caused by the radiation force will not be canceled out. We create a dynamic radiation force by applying an amplitude-modulated signal with a modulation frequency fm of several kilohertz and a carrier frequency f(0) of 2.25 MHz to drive the transducer. The dependence of the DF-MAET signal in experiments on the modulation frequency and on the density of the sample agrees with the prediction based on the radiation force mechanism. The spatial resolution of DF-MAET is also studied to verify the radiation force mechanism. Finally, we will prove that the parametric effect in the coupling oil is not a significant source of the DF-MAET signal by imaging a sample at different distances from the transducer. Potential improvements to the present DF-MAET experimental configuration are also discussed.
磁声电层析成像(MAET)是一种潜在的成像方式,可以提供导电介质阻抗的高空间分辨率图像。在 MAET 中,通过测量电极 a 和 b 测量到的电流密度分布 J(ab)(r)来重建阻抗,如果在样品中施加电流/电压源,那么就会存在该电流密度分布。为了在不施加电流/电压源的情况下绘制 J(ab)(r),将样品放置在静态磁场中,并将聚焦超声脉冲引导到点 r,通过洛伦兹力机制产生点状偶极子源。MAET 电压 U(ab)与 J(ab)(r)直接成正比,通过电极 a 和 b 测量每个扫描点的 MAET 电压。为了重建电导率,我们需要在样品内部的每个点上绘制电流密度分布。然而,在我们之前关于 MAET 的论文中报道的 MAET 实验设置中,由于样品内部超声场的空间振荡性质,样品均匀内部的 MAET 信号是不可检测的。在本文中,我们建议使用双频超声通过超声辐射力机制在差频处产生 MAET 信号。动态辐射力会引起样品内部的振动(因此会产生电场),其波长比样品沿换能器轴的尺寸大得多。因此,辐射力引起的 MAET 信号不会被抵消。我们通过施加调制频率 fm 为几 kHz 且载波频率 f(0)为 2.25 MHz 的调幅信号来产生动态辐射力,以驱动换能器。实验中 DF-MAET 信号对调制频率和样品密度的依赖性与基于辐射力机制的预测相符。还研究了 DF-MAET 的空间分辨率,以验证辐射力机制。最后,我们将通过对距离换能器不同距离的样品进行成像,证明耦合油中的参数效应不是 DF-MAET 信号的主要来源。还讨论了对当前 DF-MAET 实验配置的潜在改进。