Large-amplitude vibrations of the symmetric triatomic molecule are con
sidered as the coupled rotations of two diatomic fragments. This proce
dure does not require a molecule-fixed coordinate system to be defined
. Thus Eckart conditions, Coriolis coupling, and similar concerns are
avoided. An algebraic approach is used to generate a Hamiltonian which
describes the stretching vibrations and a second Hamiltonian which de
scribes the bend. A model potential is used which treats the stretches
as coupled Morse oscillators and the bend as a bond-length-dependent
anharmonic oscillator. This paper gives detailed results only for stat
es of zero angular momentum. However it can be used for all rotational
states.