Correction

This article refers to:

Study of Casson nanofluid flow over a wedge with variable magnetic effect, thermal radiation, and melting effects

Article title: Study of Casson nanofluid flow over a wedge with variable magnetic effect, thermal radiation, and melting effects

Authors: Anomitra Chakraborty, and Pranitha Janapatla

Journal: Numerical Heat Transfer, Part B: Fundamentals

DOI: https://doi.org/10.1080/10407790.2023.2266128

When this article was originally published online, equation 11(11) $$u\frac{\partial T}{\partial x}+v\frac{\partial T}{\partial y}=\alpha \frac{{\partial }^{2}T}{\partial y^2}+\tau \left[D_B\frac{\partial C}{\partial y}\mathit{ }\frac{\partial T}{\partial y}+\frac{D_T}{T_{\infty }}{\left(\frac{\partial T}{\partial y}\right)}^2\mathit{ }\right]-\frac{\partial }{\partial y}\left(\frac{1}{\rho C_p}{q}_y^r\right)$$(11) showed a ‘plus (+)’ before the last term instead of ‘minus (−)’ sign. The appropriate equation 11(11) $$u\frac{\partial T}{\partial x}+v\frac{\partial T}{\partial y}=\alpha \frac{{\partial }^{2}T}{\partial y^2}+\tau \left[D_B\frac{\partial C}{\partial y}\mathit{ }\frac{\partial T}{\partial y}+\frac{D_T}{T_{\infty }}{\left(\frac{\partial T}{\partial y}\right)}^2\mathit{ }\right]-\frac{\partial }{\partial y}\left(\frac{1}{\rho C_p}{q}_y^r\right)$$(11) is provided below. (11) $$u\frac{\partial T}{\partial x}+v\frac{\partial T}{\partial y}=\alpha \frac{{\partial }^{2}T}{\partial y^2}+\tau \left[D_B\frac{\partial C}{\partial y}\mathit{ }\frac{\partial T}{\partial y}+\frac{D_T}{T_{\infty }}{\left(\frac{\partial T}{\partial y}\right)}^2\mathit{ }\right]-\frac{\partial }{\partial y}\left(\frac{1}{\rho C_p}{q}_y^r\right)$$(11)