Following Eq. (4b) to the end of the paper in Secs. II–IV and VI, b(t) and bx(t) should be replaced by1 

b^(t)=δ−1GR b(t).

In Sec. V, b→ should be replaced by

b^→=δ−1GR b→.

All the results of the paper remain unchanged since only dimensional values were effectively used in the investigation.

1.
E.
 
Sterman-Cohen
,
M.
 
Bestehorn
, and
A.
 
Oron
, “
Rayleigh-Taylor instability in thin liquid films subjected to harmonic vibration
,”
Phys. Fluids
 
29
,
052105
(
2017
).
https://doi.org/10.1063/1.4984082
Google Scholar
Crossref
Search ADS
 
View Original Article
© 2017 Author(s).
2017
Author(s)