ADSC with its periodical temperature programs combines the features of
DSC measured at high heating rate (high sensitivity) with those at lo
w heating rate (high temperature resolution). In addition, the ''rever
sing'' c(p) effects can be separated from the ''non-reversing'' latent
heat effects. Various periodical temperature programs can be applied.
This paper compares the different possible temperature programs and t
heir algorithms for the c(p) determination for metal, metal oxide and
polymer of various properties. Simulated and measured results for vari
ous wave shapes and samples are presented. The relevant sample propert
ies and their influence on the measurements are identified and guiding
rules for the proper choice of the various experimental parameters ar
e given. Measurements with different samples, performed with the new M
ETTLER TOLEDO STAR(e)-System, are shown and compared with the simulati
on results. The simulations and the measurements clearly show that the
alternating techniques can yield new information about sample propert
ies, but are susceptible to the proper choice of the various experimen
tal parameters.