Common understanding of the Snoek-Koster (SK) relaxation in bcc metals
is based on Schoeck's and Seeger's models. The former considers dragg
ing of the cloud of foreign interstitial atoms (FIAs) by a dislocation
in terms of the string model. The latter is based on the concept of k
ink pair formation on dislocations. A new insight into the SK relaxati
on, however, can be obtained if the coupling model, developed by K. L.
Ngai, is used to interpret mechanical loss spectra induced by the mot
ion of dislocations dragging along the Cottrell cloud of FIAs. This ph
enomenological model opens a new line of thinking in mechanical spectr
oscopy of metals to describe complex cooperative phenomena. It provide
s a very general scenario for two distinct regions of the relaxation p
rocess: exponential and stretched exponential. This model implies that
the relaxation function may continuously cross over from a Debye func
tion to a stretched exponential function. The one-sided Fourier transf
orm of the derivative of the normalized relaxation function gives the
same asymmetry of a loss peak as that observed for the carbon SK peak
in deformed ultra-high purity alpha-Iron. This paper is a resume of th
e experimental observations of SK relaxation such as the effect of the
amount of plastic deformation, of deformation temperature, of conditi
ons for thermal stability of the SK peak, and its broadening. It is co
ncluded that the concept of the cooperative migration of FIAs in the C
ottrell cloud elucidates the primary and secondary features of SK peak
. Very low value of the activation enthalpy of the stable SK peak dete
cted in deformed ultra-high purity alpha-Iron doped with 25 at. ppm of
carbon (i.e. H-SK = 0.95 eV) is given. This small value is interprete
d in terms of the coupling model. It is concluded that the basic featu
res of the S-K peaks in Fe-C, Nb-O and Ta-O are essentially the same.
To test, however, the coupling model in other bcc alloys, special care
must be taken to 'design' favourable experimental conditions to revea
l secondary features of the SK peak.