Several attempts to model the entire plasma cross section have been reporte
d in the last few years. Two possibilities are to either couple a core code
to a scrape-off layer (SOL) code at a specified interface or to extend the
computational region of an SOL-code all the way to the plasma centre. The
most advanced global code is the code COCONUT which is based on the former
principle and comprises the Monte-Carlo code NIMBUS, the 2D scrape-off laye
r code EDGE2D, the core transport code JETTO and the core impurity transpor
t code SANCO. A main feature of COCONUT is its modular structure which ensu
res a high degree of flexibility and the capability to cover a large range
of time-scales. The influence of the SOL on the core is illustrated with a
range of global simulations carried out with COCONUT. The simulations show
that the primary effect of the SOL is the control of the particle sources a
nd sinks with a secondary effect on plasma dilution, radiation and perhaps
pedestal temperatures.