“…We prescribe the adiabatic approximation, that is to say, that the transition in the axis depth of the sound channel with latitude is sufficiently gradual that no significant interaction occurs between different modes and different frequencies: the energy within a narrow frequency band of a fixed mode is conserved. This model is equivalent to an action-conserving ray model (Munk, 1991). In practice the adiabatic approximation implies a small fractional change in the channel over one ray loop span (order 50 km), and this condition is not grossly violated.…”