In ITER, the electric field applied for ionization and to ramp up the
plasma current may be limited to approximate to 0.3 V m(-1). In this c
ase, based on established theories of the avalanche process, it is sho
wn that ohmic breakdown in ITER is only possible over a narrow range o
f pressure and magnetic error field. Therefore, ECRH may be necessary
to provide robust and reliable strut-up. ECRH can ensure prompt breakd
own over a wide range of prefill pressure and error field and can also
give control over the initial time and location of breakdown. For ECR
H-assisted start-up in ITER, the power and pulse length requirements a
re essentially determined by the need to ensure burnthrough, i.e. comp
lete ionization of hydrogen and the transition to high ionization stat
es of impurities. A zero-dimensional (0D) code (with inclusion of some
1D effects) has been developed to analyse burnthrough in ITER. The 0D
simulations indicate that control of the deuterium density is the key
factor for ensuring successful start-up in ITER, where the effects of
neutral screening and dynamic fuelling by the ex-plasma volume are al
so crucial. It is concluded that without ECRH, successful start-up wil
l only be possible over a very restricted range of parameters but 3 MW
of absorbed ECRH power will ensure reasonably robust start-up for a b
road range of conditions with beryllium impurity. In the case of carbo
n impurity, even with an absorbed ECRH power of 5 MW one may be restri
cted to low prefill pressure and/or low carbon concentration for succe
ssful start-up.