The indirect heat transfer of steam-heated tube bundles in a moving be
d has been examined in an experimental apparatus. Heat transfer in sin
gle tubes is typified by a characteristic flow of the bulk solids alon
g the outer tube wall surface. A cuneiform rest zone is created at the
upper tube wall (stagnation point), in which the particles remain for
a long time. An 'insulating' effect is exhibited by the dammed bulk z
one and is reponsible for the poor heat transfer in this area.Near the
sides of the lateral tubes heat transfer is good and increases with i
ncreasing mass flux and bulk solids velocity. Bubbling occurs at the l
ower tube wall and the heat transfer again decreases due to the small
number of wall-particle contacts. The experimentally confirmed 'trace
theory' describes the temperature profile at the outlet of a moving be
d heat exchanger, being characterized by very good cross-mixing of the
bulk solids which allows the integral heat transition to be calculate
d. A modelling approach to the heat transfer and bulk solids movement
in the moving bed provides a physical model which describes the depend
ence of the heat transfer at a single tube on the flow profile between
two neighbouring tubes. In order to determine the flow profile, the c
ontinuity equation is solved vectorially, allowing an analytical relat
ionship of the velocity profile between two tubes to be obtained via t
he coaxiality of stress and deformation. To allow such a calculation,
the heat-transfer model makes use of the residence and contact time be
haviour resulting from the velocity profile, with the different compon
ents of heat transfer at a tube being determined from the friction pro
perties of the specific bulk material. Calculation of the integral hea
t transfer in the moving bed may be achieved via heat transfer at a si
ngle tube. By using the theory of 'extended contact time', the total r
esidence time of the bulk at the first tubes may be considered as a ca
se history for the other tubes. The integral overall heat-transfer coe
fficients of moving bed heat exchangers thereby determined have been v
erified experimentally.