The paper studies the dynamics of a Bose-Einstein condensate loaded into a 1D parabolic optical lattice, and excited by a sudden shift of the lattice center. Depending on the magnitude of the initial shift, the condensate undergoes either dipole or Bloch oscillations. The effects of dephasing and of atom-atom interactions on these oscillations are discussed.1. Bloch oscillations (BO) of a quantum particle in a periodic potential are one of the most fascinating phenomena of quantum physics [1]. Since the pioneering experiment [2] in 1996, this phenomenon has been intensively studied for cold atoms in optical lattices [3], with recent emphasis on quantum statistical (Fermi or Bose) and atom-atom interaction effects. In particular, the dynamics of degenerate Bose gases, on which we will focus here, was studied experimentally in [4,5,6]. It should be stressed from the very beginning that, when addressing this problem theoretically, one has to distinguish between quasi one-dimensional lattices (created by two counterpropagating laser beams) and truly 1D lattices (or socalled modulated quantum tubes). Indeed, in the former case the number of atoms per well of the optical lattice can be as large as 10 3 − 10 4 , and a mean field approach (based on the Gross-Pitaevskii or nonlinear Schrödinger equation) is generally justified. This is not the case of the truly 1D lattices, where only few atoms occupy a single well, and, hence, a microscopic analysis is required. For a tilted infinite lattice such analysis, based on the BoseHubbard model, was presented in [7,8,9], where two regimes of BO -quasiperiodic and irreversible decaying -were identified.When referring to the typical laboratory experiments, an additional complication stems from the harmonic confinement along the lattice. Clearly, harmonic confinement should modify BO of bosonic atoms, and the aim of this work is to estimate its effect. At the same time, parabolic lattices have their own interest, because they allow to study dipole oscillations of BECs. Recent experiments [10] have shown that there is a fundamental difference between dipole oscillations in quasi-and truly 1D lattices. While in the former case the main effect of the periodic potential can be taken into account by simply substituting the atomic mass by its effective mass in the ground Bloch band [11], one observes a rapid decay of oscillations in the latter case. In the present paper we also briefly discuss dipole oscillations of a BEC in truly 1D lattices, partially overlapping in this part with recent theoretical work [12].2. We consider atoms in a parabolic lattice potential V (x) = M ω 2 x 2 /2 − V cos 2 (2πx/d), where the atoms are set into motion by a sudden shift of the trap origin. The relevant parameters of the system are the hopping matrix element J (defined by the amplitude of the periodic potential V ), the 'parabolicity' ν = M ω 2 d 2 , and the initial shift l 0 = ∆x/d. Using the single band approximation and neglecting atom-atom interactions, the dynamics of the system is described by t...