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The signal-to-noise ratio of nuclear magnetic resonance surface coils and application to a lossy dielectric cylinder model. II. The case of cylindrical window coils

机译:核磁共振表面线圈的信噪比及其在有损介质圆柱模型中的应用。二。圆柱窗线圈的情况

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For pt. I see ibid., vol. 42, no. 5, p. 497-506 (1995). In pt. I the authors developed complete expressions for the power dissipated by and for the signal-to-noise ratio (S/N) of a coil of arbitrary geometry facing an infinite lossy dielectric cylinder. They now consider an example coil geometry, a "cylindrical window", and demonstrate the effects of coil size and position, tissue properties, and source location on the S/N. Frequencies ranging from 1 to 170 MHz are investigated for two coil sizes, the larger having four times the surface area of the smaller. For a dipole source of strength assumed independent of frequency, the S/N is constant for frequencies up to about 10 MHz. Both coil sizes yield similar optimal S/N values when imaging structures deep within the body, the larger coil showing less dependence on the source location. For more superficial structures, the smaller coil has a better performance at all frequencies investigated while still being more sensitive to source position. Hence, when imaging superficial structures the choice of coil size should be balanced between image uniformity and the need for a higher S/N. For each coil size, there is an optimal position away from the tissues which yields the highest S/N when imaging deep. By contrast, the coil should be placed as close as possible to the body when the source is near the surface. From an electromagnetic standpoint and aside from the increased equilibrium magnetization in the tissues, the S/N of both coils is actually improved by operating at a higher frequency when imaging superficially, whereas it is degraded when imaging deep. Experimental results gathered on a saline-filled cylinder correlate very well with these simulations and show the model will also predict with good accuracy the S/N for a finite length cylinder as long as that length is at least three or four times the coil longitudinal dimension.
机译:对于pt。我看同上。 42号5,第497-506(1995)。在pt。作者针对面向无限损耗电介质圆柱体的任意几何形状的线圈的耗散功率以及信噪比(S / N)开发了完整的表达式。他们现在考虑示例线圈几何形状,“圆柱窗口”,并演示了线圈大小和位置,组织特性以及源位置对S / N的影响。对于两种线圈尺寸,研究了从1到170 MHz的频率,较大的线圈具有较小线圈表面积的四倍。对于假定的偶极子强度源,它与频率无关,对于高达约10 MHz的频率,S / N是恒定的。当在体内深处对结构进行成像时,两种线圈尺寸均会产生相似的最佳S / N值,较大的线圈对源位置的依赖性较小。对于更浅层的结构,较小的线圈在所研究的所有频率下均具有更好的性能,同时仍然对源位置更加敏感。因此,在对表层结构进行成像时,应在图像均匀性和对更高信噪比的需求之间平衡线圈尺寸的选择。对于每种线圈尺寸,都有一个远离组织的最佳位置,当进行深层成像时,它会产生最高的信噪比。相反,当源靠近表面时,应将线圈放置在尽可能靠近人体的位置。从电磁的角度来看,除了增加组织中的平衡磁化强度外,当在浅层成像时,通过以较高的频率工作,实际上可以提高两个线圈的S / N,而在深层成像时,S / N会降低。在充满盐水的钢瓶上收集的实验结果与这些模拟具有很好的相关性,并且表明该模型还将以良好的精度预测有限长度钢瓶的S / N,只要该长度至少是线圈纵向尺寸的三到四倍即可。

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