Oscillatory fl ow effects on a fi xed bed of solids in contact with a single liquid phase were fi rst studied in detail by Krasuk and Smith (1965). They measured the rate of dissolution of cast particles of a sparingly soluble organic solid (β-naphthol) in water in a column of diameter 47.6 mm. Cylinders and spheres were studied with equivalent spherical diameters in the range 5.7 to 7.6 mm. Reynolds numbers, based on the particle diameters, system properties and liquid velocities, were in the range 4.5 to 20 for both the steady and oscillatory fl ows. Condoret et al. (1989) used an electrochemical method to study mass transfer in pulsatile fl ow around an active brass sphere within a packed bed of equal sized inert glass spheres, of diameter 4 or 6 mm. The amplitudes (up to 27 mm) and frequencies (up to 3.7 Hz) resulted in oscillatory Reynolds numbers up to 700. Approximately the same Reynolds number range was covered by Takahashi et al. (1992) who also used an electrochemical method to study mass transfer around a mechanicallyThe liquid-solid mass transfer behaviour of a fi xed bed of cylinders has been studied using the dissolution of copper in acidifi ed dichromate solution under pulsating fl ow conditions. The bed diameter was 100 mm. The depth of the working section was 95 mm and the length and diameter of the cylinders were 19.1 mm. Variables studied were steady fl ow superfi cial liquid velocity, and oscillation amplitude and frequency. Data have been correlated as the Sherwood number in terms of Schmidt number and the cylinder Reynolds numbers for steady and oscillatory fl ow. The form of the correlation permits comparison with literature data for the limiting cases where either of these Reynolds numbers is zero.On a étudié le transfert de matière liquide-solides dans un lit fi xe composé de cylindres dans le cas de la dissolution de cuivre dans une solution de dichromate acidifi é avec des conditions d'écoulement pulsé. Le diamètre de lit est de 100 mm, la profondeur de la section transversale de 95 mm et la longueur et le diamètre des cylindres de 19,1 mm.Les variables étudiées sont la vitesse de liquide superfi cielle en écoulement stationnaire, l'amplitude de l'oscillation et la fréquence. Les données ont été corrélées par le nombre de Sherwood en fonction du nombre de Schmidt et des nombres de Reynolds des cylindres pour l'écoulement stationnaire et oscillatoire. La forme de la corrélation permet la comparaison avec les données de la littérature scientifi que pour les cas limites lorsque l'un de ces nombres de Reynolds est nul.