The quench protection system for the superconducting magnets of the CE
RN Large Hadron Collider (LHC) is described. The system is based on th
e so called ''cold diode'' concept. In a group of series connected mag
nets if one magnet quenches then the magnetic energy of all the magnet
s will be dissipated in the quenched magnet so destroying it. This is
avoided by by-passing the quenched magnet and then rapidly de-exciting
the unquenched magnets. For the LHC machine it is foreseen to use sil
icon diodes situated inside the cryostat as by-pass elements - so call
ed ''cold diodes''. The diodes are exposed to some 50 kGray of radiati
on during a 10 year operation life-time. The high energy density of th
e LHC magnets (500 kJ/m) coupled with the relatively slow propagation
speed of a ''natural'' quench (10 to 20 m/s) can lead to excessive hea
ting of the zone where the quench started and to high internal voltage
s. It is therefore necessary to detect quickly the incipient quench an
d fire strip heaters which spread the quench out more quickly over a l
arge volume of the magnet. After a quench the magnet chain must be de-
excited rapidly to avoid spreading the quench to other magnets and ove
r-heating the by-pass diode. This is done by switching high-power ener
gy-dump resistors in series with the magnets. The LHC main ring magnet
will be divided into 16 electrically separated units which has import
ant advantages.