Hademenos G J, Massoud T, Valentino D J, Duckwiler G, Viñuela F
Division of Medical Imaging, University of California, Los Angeles 90024-1721.
Neurol Res. 1994 Oct;16(5):376-84. doi: 10.1080/01616412.1994.11740257.
Mathematical models of aneurysms are typically based on Laplace's law which defines a linear relation between the circumferential tension and the radius. However, since the aneurysm wall is viscoelastic, a nonlinear model was developed to characterize the development and rupture of intracranial spherical aneurysms within an arterial bifurcation and describes the aneurysm in terms of biophysical and geometric variables at static equilibrium. A comparison is made between mathematical models of a spherical aneurysm based on linear and nonlinear forms of Laplace's law. The first form is the standard Laplace's law which states that a linear relation exists between the circumferential tension, T, and the radius, R, of the aneurysm given by T = PR/2t where P is the systolic pressure. The second is a 'modified' Laplace's law which describes a nonlinear power relation between the tension and the radius defined by T = ARP/2At where A is the elastic modulus for collagen and t is the wall thickness. Differential expressions of these two relations were used to describe the critical radius or the radius prior to aneurysm rupture. Using the standard Laplace's law, the critical radius was derived to be Rc = 2Et/P where E is the elastic modulus of the aneurysm. The critical radius from the modified Laplace's law was R = [2Et/P]2At/P. Substituting typical values of E = 1.0 MPa, t = 40 microns, P = 150 mmHg, and A = 2.8 MPa, the critical radius is 4.0 mm using the standard Laplace's law and 4.8 mm for the modified Laplace's law.(ABSTRACT TRUNCATED AT 250 WORDS)
动脉瘤的数学模型通常基于拉普拉斯定律,该定律定义了圆周张力与半径之间的线性关系。然而,由于动脉瘤壁是粘弹性的,因此开发了一种非线性模型来描述动脉分叉处颅内球形动脉瘤的发展和破裂,并根据静态平衡时的生物物理和几何变量来描述动脉瘤。本文对基于线性和非线性形式拉普拉斯定律的球形动脉瘤数学模型进行了比较。第一种形式是标准拉普拉斯定律,该定律指出圆周张力T与动脉瘤半径R之间存在线性关系,表达式为T = PR/2t,其中P为收缩压。第二种是“修正”拉普拉斯定律,它描述了张力与半径之间的非线性幂关系,表达式为T = ARP/2At,其中A为胶原蛋白的弹性模量,t为壁厚。利用这两种关系的微分表达式来描述动脉瘤破裂前的临界半径。根据标准拉普拉斯定律,临界半径为Rc = 2Et/P,其中E为动脉瘤的弹性模量。修正拉普拉斯定律的临界半径为R = [2Et/P]2At/P。代入E = 1.0 MPa、t = 40微米、P = 150 mmHg和A = 2.8 MPa的典型值,使用标准拉普拉斯定律时临界半径为4.0 mm,使用修正拉普拉斯定律时临界半径为4.8 mm。(摘要截短为250字)