A new concept of pseudo mean wave resistance is introduced to find the
oretical mean wave resistances of the precursor soliton generation in
two-layer how over a localized topography at near-resonance in this pa
per. The pseudo mean wave resistance of the precursor soliton generati
on of two-layer how is determined in terms of the AfKdV equation. From
the theoretical results it is shown that the theoretical mean wave re
sistance is equal to the pseudo mean wave resistance times 1/m(1), whe
re m(1) is the coefficient of the fKdV equation. From the regional dis
tribution of the energy of the precursor soliton generation at the res
onant points, it is shown that ratios of the theoretical mean wave res
istance and regional mean energy to the total mean energy are invarian
t constants, i.e. <(E)over circle (1)>/(E) over circle : <(E)over circ
le (2)>/(E) over circle: <(E)over circle (3)>(E) over circle :< D > /(
E) over circle = (1/2) : (-1/2) : 1 : 1, in which <(E)over circle 1>,<
(E)over circle (2)> and <(E)over circle (3)> are the mean energy of th
e generating regions of the precursor solitons, of the depression and
of the trailing wavetrain at the resonant points respectively, (E) ove
r circle and < D > are the total energy of the system and the theoreti
cal mean wave resistance at the resonant points. A prediction of the t
heoretical mean wave resistances of two-layer how over the semicircula
r topography is carried out in terms of the theoretical results of the
present paper. The comparison shows that the theoretical mean wave re
sistance is in good agreement with the numerical calculation.