Avoid common mistakes on your manuscript.
[Rheol Acta (2005) 44:305–314. DOI: 10.1007/s00397-005-0003-0
The text above Eq. (16) should read: “Using (4) and (5), and the scaling suggested by (6a)–(6 g) we find that the dimensionless storage modulus \({\left( {\widetilde{G}\prime = G\prime H^{2} /K_{{33}} } \right)}\), loss modulus \({\left( {\widetilde{G}\prime \prime = G\prime \prime H^{2} /K_{{33}} } \right)}\) and loss tangent \({\left( {\tan \,\delta = \widetilde{G}\prime \prime /\widetilde{G}\prime } \right)}\) (Burghardt 1991) are:”
The text below Eqs. (40a,b) should read: “and hence the impact of geometry is almost insignificant. For large frequencies, \(U_{1} {\left( {\widetilde{\omega }} \right)} \approx U_{2} {\left( {\widetilde{\omega }} \right)}\), for both flows”.
References: de Andrade Lima and Rey (2004a,b,c) should be located between Chandrasekhar (1992) and de Gennes and Prost (1993).
Author information
Authors and Affiliations
Corresponding author
Additional information
The online version of the original article can be found at http://dx.doi.org/10.1007/s00397-005-0003-0.
Rights and permissions
About this article
Cite this article
de Andrade Lima, L.R.P., Rey, A.D. Corrigendum to “Superposition principles for small amplitude oscillatory shearing of nematic mesophases”. Rheol Acta 45, 601 (2006). https://doi.org/10.1007/s00397-005-0048-0
Published:
Issue Date:
DOI: https://doi.org/10.1007/s00397-005-0048-0