The presence of a crack in a structural member introduces a local flex
ibility that affects its vibration response. Moreover, the crack will
open and close in time depending on the rotation and vibration amplitu
de. In this case the system is nonlinear. Furthermore, if general moti
on is considered, the local stiffness matrix description of the cracke
d section of the shaft leads to a coupled system, while for an uncrack
ed shaft the system is decoupled. This means that the crack introduces
new harmonics in the spectrum. In fact, in addition to the second har
monic of rotation and the subharmonic of the critical speed, two more
families of harmonics are observed: (1) higher harmonics of the rotati
ng speed due to the nonlinearity of the closing crack, and (2) longitu
dinal and torsional harmonics are present in the start-up lateral vibr
ation spectrum due to the coupling. Over 500 papers on the subject wer
e published in the past 10 yrs. A wealth of analytical, numerical and
experimental investigations now exists. However, a consistent cracked
bar vibration theory is yet to be developed. There are still many unan
swered questions, especially in the area of closing cracks in rotating
shafts. Copyright (C) 1996 Elsevier Science Ltd.