“…So, matching the electric field (2) to the fields (4) in two grooves on the corrugated surface @ = a ) and integrating the expression over the angular period, we obtain (the fin thickness is assumed to be zero for simplicity) the equation (3) and (1) on the corrugated surface for each of .two neighbor grooves gives us two more equations Dividing now the left and right parts of (7) by the left and right parts of (S), respectively, and talung into account the relation BdBI=hJl(hla)~h?fi(h2)~ resulting from (8) and (9), we obtain the dispersion equation E--, 1 Jl(g0) (10) g J , ( g 4 which should be solved together with (5). Note that if &2=.3, then h2=hl, and, from (6), f2(hzp)=J(hrp), and (10) is reduced to a dispersion equation given in (1) for corrugations of identical groove fiIling.…”