Department of Mechanical Engineering, Chiang Mai University, Chiang Mai, Thailand.
Ultrasonics. 2010 Jun;50(7):654-65. doi: 10.1016/j.ultras.2010.01.003. Epub 2010 Jan 14.
Arterial stiffness has been shown to be a good indicator of arterial wall disease. However, a single parameter is insufficient to describe the complex stress-strain relationship of a multi-component, non-linear tissue such as the aorta. We therefore propose a new approach to measure the stress-strain relationship locally in vivo noninvasively, and present a clinically relevant parameter describing the mechanical interaction between aortic wall constituents. The slope change of the circumferential stress-strain curve was hypothesized to be related to the contribution of elastin and collagen, and was defined as the transition strain (epsilon(theta)(T)). A two-parallel spring model was employed and three Young's moduli were accordingly evaluated, i.e., corresponding to the: elastic lamellae (E(1)), elastin-collagen fibers (E(2)) and collagen fibers (E(3)). Our study was performed on normal and Angiotensin II (AngII)-treated mouse abdominal aortas using the aortic pressure after catheterization and the local aortic wall diameters change from a cross-correlation technique on the radio frequency (RF) ultrasound signal at 30 MHz and frame rate of 8 kHz. Using our technique, the transition strain and three Young's moduli in both normal and pathological aortas were mapped in 2D. The slope change of the circumferential stress-strain curve was first observed in vivo under physiologic conditions. The transition strain was found at a lower strain level in the AngII-treated case, i.e., 0.029+/-0.006 for the normal and 0.012+/-0.004 for the AngII-treated aortas. E(1), E(2) and E(3) were equal to 69.7+/-18.6, 214.5+/-65.8 and 144.8+/-55.2 kPa for the normal aortas, and 222.1+/-114.8, 775.0+/-586.4 and 552.9+/-519.1 kPa for the AngII-treated aortas, respectively. This is because of the alteration of structures and content of the wall constituents, the degradation of elastic lamella and collagen formation due to AngII treatment. While such values illustrate the alteration of structure and content of the wall constituents related to AngII treatment, limitations regarding physical assumptions (isotropic, linear elastic) should be kept in mind. The transition strain, however, was shown to be a pressure independent parameter that can be clinically relevant and noninvasively measured using ultrasound-based motion estimation techniques. In conclusion, our novel methodology can assess the stress-strain relationship of the aortic wall locally in vivo and quantify important parameters for the detection and characterization of vascular disease.
动脉僵硬度已被证明是动脉壁疾病的一个良好指标。然而,单一参数不足以描述主动脉等多成分、非线性组织的复杂应力-应变关系。因此,我们提出了一种新的方法来无创地在体内局部测量应力-应变关系,并提出了一个描述主动脉壁成分之间力学相互作用的临床相关参数。我们假设周向应力-应变曲线的斜率变化与弹性蛋白和胶原蛋白的贡献有关,并将其定义为过渡应变(epsilon(theta)(T))。采用双平行弹簧模型,并相应评估了三个杨氏模量,即弹性层片(E(1))、弹性蛋白-胶原纤维(E(2))和胶原纤维(E(3))。我们的研究使用导管后主动脉压力和射频(RF)超声信号的局部主动脉壁直径变化,通过相关技术在 30MHz 和 8kHz 的帧频下,对正常和血管紧张素 II(AngII)处理的小鼠腹主动脉进行。使用我们的技术,在正常和病理主动脉中以 2D 形式绘制了过渡应变和三个杨氏模量。在生理条件下,首次在体内观察到周向应力-应变曲线的斜率变化。在 AngII 处理的情况下,发现过渡应变出现在较低的应变水平,即正常主动脉为 0.029+/-0.006,AngII 处理的主动脉为 0.012+/-0.004。E(1)、E(2)和 E(3)分别等于正常主动脉的 69.7+/-18.6、214.5+/-65.8 和 144.8+/-55.2kPa,AngII 处理的主动脉为 222.1+/-114.8、775.0+/-586.4 和 552.9+/-519.1kPa。这是由于壁成分的结构和含量的改变,弹性层片和胶原蛋白的降解由于 AngII 处理。虽然这些值说明了与 AngII 处理相关的壁成分的结构和含量的改变,但应牢记物理假设(各向同性、线性弹性)的局限性。然而,过渡应变是一个与压力无关的参数,可使用基于超声的运动估计技术进行临床相关和无创测量。总之,我们的新方法可以在体内局部评估主动脉壁的应力-应变关系,并量化用于检测和表征血管疾病的重要参数。