Depending on the material and the results required, the treating temperature and time are chosen in advance.
|
no environmental and safety problems, as neither dangerous nitriding materials are used nor produced
|
|
minimal requirement of gas, as, by ionizing the gas used may be exploited effectively
|
|
the structure of the nitride layer may be controlled
|
|
surface parts which may not be treated, can be protected by covering
|
|
steels containing chrome may be nitrided without previous depassivation
|
|
if required the temperature of work pieces may be kept very low; thus it is possible to treat cold work steel.
|
PULSED TECHNIQUE |  | D.C. TECHNIQUE |
|
only energy required for the process will be added metered, especially if low temperature treating is required |
|
|
energy surplus has to be carried off (e.g. by cooling the wall of the vessel) |
|
|
minimal energy losses by cooling water, as wall of vessel is insulated (energy saving by the factor 3 to 5 compared to cooled wall) |
|
|
high energy losses by a large area cooled furnace wall |
|
|
good homogeneity of temperature in vessel, due to low temperature difference between charge and wall |
|
|
high temperature gradient between charge and cooled vessel |
|
|
complete usage of the charge volume due to good temperature homogeneity |
|
|
using of the charge zone is limited by overheating of work pieces in the center of charge |
|
|
excellent results due to an easy controllability and reproducability of treatment for different charge sizes, as plasma parameters, important for the results, are independent from load density |
|
|
treatment results depend on the loading density as plasma paramenters are linked with temperature regulation |
|
|
arcing is impossible as its development is periodically interrupted by the pulsed current mode. If necessary during each pulse a switch off in less than 1 µs. |
|
|
arcing is always possible and has to be interrupted immediately. In spite of short reaction times arc traces on the surface of parts |
|
|
total surface nitriding, even into smallest bores |
|
|
contour tracing on surface is limited |
|
|
short heating time of charge by using a seperate heating |
|
|
long heating time, because charge can be heated directly or indirectly by plasma only |
|