Sergiu
Ruta
*a,
Yilian
Fernández-Afonso
b,
Samuel E.
Rannala
c,
M. Puerto
Morales
d,
Sabino
Veintemillas-Verdaguer
d,
Carlton
Jones
e,
Lucía
Gutiérrez
*b,
Roy W.
Chantrell
c and
David
Serantes
fg
aCollege of Business, Technology and Engineering, Sheffield Hallam University, UK. E-mail: sergiu.ruta@shu.ac.uk
bInstituto de Nanociencia y Materiales de Aragón (INMA), CSIC-Universidad de Zaragoza and CIBER-BBN, Spain. E-mail: lu@unizar.es
cDepartment of Physics, University of York, UK
dMaterials Science Institute of Madrid (ICMM/CSIC), Spain
enanoTherics Ltd, Brookside Farm, Dig Lane, Warrington, WA2 0SH, UK
fApplied Physics Department, Universidade de Santiago de Compostela, Spain
gInstituto de Materiais (iMATUS), Universidade de Santiago de Compostela, Spain
First published on 22nd July 2024
Correction for ‘Beyond Newton's law of cooling in evaluating magnetic hyperthermia performance: a device-independent procedure’ by Sergiu Ruta et al., Nanoscale Adv., 2024, https://doi.org/10.1039/d4na00383g.
All calculations were carried out using the 1D heat transport model (eqn (5)). Eqn (6)–(8) indicate the correction to the SLP taking into account the instantaneous losses. The notation is intended to indicate derivatives during heating and cooling rather than absolute values.
In general, the expectation is that the second term in eqn (8) is negative, therefore the correction will be an increase in SLP prediction based on the heating part only. The correct notation is to use square brackets rather than vertical lines around the derivatives, as seen below:
![]() | (6) |
![]() | (7) |
![]() | (8) |
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
This journal is © The Royal Society of Chemistry 2024 |