Chen Shuai, Lu Zhongliang, Huang Qiang, Zhao Gaowei, Sun Zheng, Zhou Jing, Liao Yupeng
School of Medical Information Engineering, Gannan Medical University, Ganzhou, China.
School of Information Engineering, Jiangxi University of Science and Technology, Ganzhou, China.
Front Bioeng Biotechnol. 2025 Aug 29;13:1575142. doi: 10.3389/fbioe.2025.1575142. eCollection 2025.
The open-ended coaxial probe (OECP) method has demonstrated promising potential in biological tissue measurements. However, it still faces challenges such as significant measurement errors and poor repeatability. Research indicates that a substantial portion of these errors originates from tissue heterogeneity. To mitigate errors associated with tissue heterogeneity and accurately interpret the relationship between the dielectric properties and histology of heterogeneous tissue samples, detailed knowledge of the probe's effective sensing volume is essential.
In this study, the effective sensing volumes of two commonly used small-aperture probes (with diameters of 2.20 mm and 3.58 mm) were measured. The vertical sensing volume is represented by the sensing depth, while the horizontal sensing volume is characterized by the sensing radius. A measurement model for the sensing volume of the OECP method was established using a heterogeneous dielectric property layered model combined with an optimized sliding rail-assisted micrometer system. Dielectric property bilayer models were constructed using materials with distinct dielectric parameters (Teflon, ethanol, methanol, deionized water) and biological tissue simulants (dimethyl sulfoxide, salt-sugar mixed solution). To validate the sensing volume derived from the aforementioned bilayer model, we conducted experimental measurements on porcine tissue and human breast tissue, both of which exhibit well-defined layered structures. In this experiment, the geometric center of a Teflon cube was designated as the origin for probe movement.
The measured sensing depth ranges were 0.44 to 0.62 mm for a 2.20 mm diameter probe and 0.75 to 0.98 mm for a 3.58 mm diameter probe. While the corresponding sensing radius ranges of 0.36 to 0.63 mm for the 2.20 mm diameter probe and 0.71 to 0.99 mm for the 3.58 mm diameter probe.
The results indicate that both the sensing depth and radius of the probe increase significantly with larger coaxial probe aperture sizes. Furthermore, a smaller aperture reduces the influence of tissue heterogeneity on measurements, while the effective sensing volume remains consistent across frequencies.
开放式同轴探头(OECP)方法在生物组织测量中已展现出可观的潜力。然而,它仍面临诸如显著的测量误差和较差的重复性等挑战。研究表明,这些误差的很大一部分源于组织异质性。为了减轻与组织异质性相关的误差,并准确解释异质组织样本的介电特性与组织学之间的关系,详细了解探头的有效传感体积至关重要。
在本研究中,测量了两种常用小孔径探头(直径分别为2.20毫米和3.58毫米)的有效传感体积。垂直传感体积由传感深度表示,而水平传感体积由传感半径表征。使用异质介电特性分层模型结合优化的滑轨辅助微米系统,建立了OECP方法传感体积的测量模型。使用具有不同介电参数的材料(聚四氟乙烯、乙醇、甲醇、去离子水)和生物组织模拟物(二甲基亚砜、盐 - 糖混合溶液)构建介电特性双层模型。为了验证从上述双层模型得出的传感体积,我们对猪组织和人乳腺组织进行了实验测量,这两种组织均呈现出明确的分层结构。在本实验中,将聚四氟乙烯立方体的几何中心指定为探头移动的原点。
直径为2.20毫米的探头测得的传感深度范围为0.44至0.62毫米,直径为3.58毫米的探头测得的传感深度范围为0.75至0.98毫米。而直径为2.20毫米的探头相应的传感半径范围为0.36至0.63毫米,直径为3.58毫米的探头相应的传感半径范围为0.71至0.99毫米。
结果表明,随着同轴探头孔径尺寸增大,探头的传感深度和半径均显著增加。此外,较小的孔径可降低组织异质性对测量的影响,且有效传感体积在不同频率下保持一致。