Published online by Cambridge University Press: 31 January 2013
We report on near-turbulent thermal convection of a nematic liquid crystal heated from below in a cylindrical cell with an aspect ratio (diameter/height) equal to 0.50 for Rayleigh numbers  
 $2\times 1{0}^{7} \lesssim \mathit{Ra}\lesssim 3\times 1{0}^{8} $  and a Prandtl number of about 355. The Nusselt number  
 $\mathit{Nu}$  as a function of  
 $\mathit{Ra}$  did not differ significantly from that of an isotropic fluid. In a vertical magnetic field  
 $\mathbi{H}$ , we found  
 $\mathit{Nu}(H)/ \mathit{Nu}(0)= 1+ a(\mathit{Ra}){H}^{2} $ , with  
 $a(\mathit{Ra})= 0. 24{\mathit{Ra}}^{0. 75} ~{\mathrm{G} }^{- 2} $ . We present a model that describes the  
 $H$  dependence in terms of a change of the thermal conductivity in the thermal boundary layers due to a field-induced director alignment.
Current address: Department of Physics & Center for the Study of Complex Systems, University of Michigan, Ann Arbor, MI 48109, USA.