1 / 22

赵旭 电子科技大学生命科学与技术学院 20041202

边界元法求解脑电正问题初探 -- A Modifield Boundary Element Methed for the Estimation of Potential Fields on the Scalp. 赵旭 电子科技大学生命科学与技术学院 20041202. 内容提要. 1· 课题及边界元法简介 2·Modifield BEM 简介 3·Modifield BEM 的实现 4· 初步总结以及展望. 1· 课题及边界元法简介. 电流偶极子源的假设 脑电 正问题 ( Forward Problem) 脑电 逆问题 (Inverse Problem).

jena-sykes
Télécharger la présentation

赵旭 电子科技大学生命科学与技术学院 20041202

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. 边界元法求解脑电正问题初探--A Modifield Boundary Element Methed for the Estimation of Potential Fields on the Scalp 赵旭 电子科技大学生命科学与技术学院 20041202

  2. 内容提要 • 1·课题及边界元法简介 • 2·Modifield BEM 简介 • 3·Modifield BEM 的实现 • 4·初步总结以及展望

  3. 1·课题及边界元法简介 • 电流偶极子源的假设 • 脑电正问题(Forward Problem) • 脑电逆问题(Inverse Problem)

  4. 1·课题及边界元法简介 • 边界元法的一般原理 • 许多物理问题可通过不同的途径归结为不同的 • 数学模型(大多数没有解析解): • a· 偏微分方程的边值问题--有限差分法 • b· 区域上的变分问题--有限元法 • C· 边界上的积分问题--边界元法

  5. 1·课题及边界元法简介 • 边界元法是将区域内微分方程 • 通过积分定理变为边界上的积分方程 • 再将积分方程在边界上离散为代数方程。

  6. 2·Modifield BEM 简介 • Let us start by formulating the BEM equations as • Where Vi and gi are vectors of potentials on the • Ith surface,and Bij is a matrix.

  7. 2·Modifield BEM 简介

  8. 2·Modifield BEM 简介 • Consider the expression for the potentials on the inner surface S3 of a three-surface head model • For V1 and V2are much more smaller than V3,we can ignore V1and V2 entirely and still achieve a good estimate of V3 .

  9. 2·Modifield BEM 简介 • By Green’s theorem we can get : • Pxya matrix with coefficients equal to ¼pi • times the solid angle subtended by an element of unit area on surface y at a point on surface x; • Gxya matrix with coefficients equal to • ds an areal element of surface y, r the distance between a point on surface x and element ds; • the normal component of the gradient of V3

  10. 2·Modifield BEM 简介 • First,since the surfaces are relatively smooth ,the ‘self’ matrices,P11,P33,and G33 are strongly diagonal.Also ,as already noted,we do not have to maintain the accuracy of the magnitude of the scalp field,so we can take the self matrices as identity matrity matrices.Thus

  11. 2·Modifield BEM 简介 • We can get: • Premultiply by G13 to give • However ,all the terms of the matrix product G13P13 are much smaller than one and

  12. 2·Modifield BEM 简介 • (I-G13P31) is dominated by the identity matrix,so

  13. 3·Modifield BEM 的实现 • 采用三层球模型并归一化半径为一。 • 每层都离散成642个点,1280个三角形。 • 第一层为头皮层,二层为颅骨层,三层为大脑组织层。 • 三层的电导率分别取为:1;1/80;1

  14. 3·Modifield BEM 的实现 • 由上面的分析可知要求头皮的电位必须求:g3,B33,P13,G13. • G3= • D为电流偶极子极矩;r0为偶极子位置;r为场点位置。

  15. 3·Modifield BEM 的实现 • B33(I,j)= • Ώ为立体角;k=l=3 • Ώ的计算: • a,b,c为相对于参考点的三角形的三个顶点

  16. 3·Modifield BEM 的实现 • P13(I,j)= ¼pi×B13 • B13的计算方法与B33相同 • G13(I,j)= ¼pi×ds(j)/r(I,j) • ds为三角形的面积;r为点到三角形的距离

  17. 4·初步总结以及展望 • vp=[0 0 1]; r=[0.8 0 0];(jxf)

  18. 4·初步总结以及展望 • vp=[0 0 1];vr0=[0.8 0 0];(BEM)

  19. 4·初步总结以及展望 • vp=[0 0 1]; r=[0.5 0 0];(jxf)

  20. 4·初步总结以及展望 • vp=[0 0 1];vr0=[0.5 0 0];(BEM)

  21. 4·初步总结以及展望 • Modifield BEM直观上看比起解析解要模糊一些。 • 这个结果不太理想,要仔细分析模糊的原因。 1立体角?2V3的计算?3矩阵处理?4······ • Modifield BEM方法只是一种尝试,目的是加深对课题的理解。 • 课题的目标是作一个精度与速度都比较好的算法(在综合文献的各种优点的基础上提出自己的综合算法)。 • ······

  22. 谢谢大家!

More Related