# Conformal Method of Moments

The Method of Moments (MoM) is a technique used to convert the EFIE into a system of linear equations that then can be solved by standard methods. For simplicity, the integral (linear) operator in the **Electric Field Integral Equation >** (EFIE) will be denoted by *L*. Then, the EFIE takes the form:

where *E _{T}* is the tangential component of the incident electric field. The current distribution is approximated by a sum of

*N*basis functions with unknown amplitudes

*I*, giving:

_{n}With this expansion and using the linearity of the operator *L*, we can write:

To obtain a set of *N* equations, the functional equation (3) is weighted with a set of *N* independent testing functions *w _{m}*, giving:

where the integrals are calculated over the domain of *L*. Now we have as many independent equations as unknowns, so (4) can be written as:

where

[*Z*]: impedance matrix with dimension *NxN* and the elements

[*I*]: current matrix with dimension *Nx1* and the elements *I _{n}*.

[*U*]: voltage matrix with dimension *Nx1* and the elements

This fully occupied equation system must be solved for the unknown currents *I _{n}*. LU decomposition is used in AN-SOF. The MoM is applied by first dividing the wire structure into

*N*segments, and then defining the basis and testing functions on the segments. Triangular basis and pulse testing functions are used in AN-SOF, Fig. 1.

When a curved wire is described parametrically by a vector function as in **Eq. (5) here >**, the basis and testing functions are curved in the sense that their support is a curved subset of the wire. Therefore, when curved basis and testing functions are used, the **Conformal Method of Moments (CMoM)** is obtained.

To fill the impedance matrix [*Z*], an adaptive Gauss-Legendre quadrature rule is applied to compute the involved integrals. After having solved the equation system, the currents *I _{n}* are known and other parameters of interest, such as input impedances, voltages, radiated power, directivity, and gain can be computed.

The MoM can also be used to calculate the electromagnetic response of metallic surfaces, which are modeled using wire grids. In AN-SOF, with the CMoM the accuracy of the calculation of wire grids is remarkably improved compared to the traditional MoM, as demonstrated in **this article >** . Another extension of the calculation includes wires that do not have a circular cross section. In AN-SOF an equivalent radius is calculated for these wires.