Page 126 - YORAM RUDY BOOK FINAL
P. 126

P. 126
        BEM is derived from Green’s second theorem        260 , which relates the potential in a volume to the

        potential on its bounding surfaces via integration:




                            2
                                                 2
                   ∫ [Φ▼ (1/r) – (1/r)▼ Φ]dv = ∫ [Φ{∂(1/r)/∂n} – 1/r{∂ Φ/∂n}]ds    (5.4)
                    v                                          s


        Where the surface S includes the epicardial and torso surfaces and v is the torso volume enclosed
        by these surfaces; r is the Euclidian distance in three-dimensional space. Manipulation of equation
                                 2
        5.4 considering that ▼ Φ = 0 in the volume v, and discretization of the epicardial and torso
        surfaces into triangular elements, leads to the following matrix equation relating Φ  and Φ :
                                                                                                   T
                                                                                                            E
                                                       Φ  = AΦ                                                          (5.5)
                                                          T         E


        Where Φ  is a vector of torso potentials and Φ  is a vector of epicardial potentials; A is a transfer
                  T
                                                           E
        matrix that contains the geometric relationship between the heart surface and torso surface.
        The potential over each triangular element can be assumed to be constant or to vary as a linear

        or higher order function of the intrinsic element coordinates. Equation (5.5) computes Φ  from a
                                                                                                         T
        given Φ  in a specific heart-torso geometry (contained in the transfer matrix A). This formulation
                 E
        constitutes the forward problem of electrocardiography. The objective of ECGI is to invert this
        relationship to compute Φ  from a known Φ , a formulation that constitutes the inverse
                                                         T
                                     E
        problem of electrocardiography. The inverse problem is mathematically ill-posed in the sense
        that even low-level noise or error in the data (the measured torso potential, Φ ) can cause large,
                                                                                             T
        unbounded errors in the solution (the epicardial potentials, Φ ). Because of this property, one
                                                                            E
        cannot simply invert the (ill-conditioned) matrix A to obtain Φ . To overcome this difficulty, we
                                                                            E
        have applied different computational schemes in the ECGI application: Tikhonov regularization
        (TR) 260  and the generalized minimal residual (GMRes)    262  method.

               TR stabilizes the computation by imposing constraints on the solution through the

        following objective function:


                                                                      2
                                                                                       2
                                        Min  [║Φ  - AΦ ║  + t║RΦ ║ ]                         (5.6)
                                              Φ E        T        E                E
        By minimizing this function with respect to Φ , one finds the Φ  that best approximates (in the
                                                                              E
                                                           E
        least-square sense) a solution to equation (5.5) subject to a given constraint. The first term in
        equation (5.6) represents the solution and the second term is the constraint (regularization) term
        that imposes bounds on the magnitude of Φ  (for R=I, the unit matrix), its steepness (for R=G, the
                                                          E
        surface gradient operator), or its curvature (for R=L, the surface Laplacian operator); t is a regular-
        ization parameter that determines the weight of the imposed constraint.
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