We consider a two-dimensional infinitely long acoustic waveguide formed by
two parallel lines containing an arbitrarily shaped obstacle. The existence
of trapped modes that are the eigenfunctions of the Laplace operator in th
e corresponding domain subject to Neumann boundary conditions was proved by
Evans, Levitin and Vassiliev (J. Fluid Mech. 261 1994) for obstacles symme
tric about the centreline of the waveguide. In our paper we deal with the s
ituation when the obstacle is shifted with respect to the centreline and st
udy the resulting complex resonances. We are particularly interested in tho
se resonances which are perturbations of (real) eigenvalues. We study how a
n eigenvalue becomes a complex resonance moving from the real axis into the
upper half-plane as the obstacle is shifted from its original position. Th
e shift of the eigenvalue along the imaginary axis is predicted theoretical
ly and the result is compared with numerical computations. The total number
of resonances lying inside a sequence of expanding circles is also calcula
ted numerically.