\begin{table}%t4 \par \caption {\label{tab_abundances}Mean NLTE abundances (on the scale in which $\log \epsilon$[H]~=~12) and total 1-$\sigma$ uncertainties (in brackets), in units of the last digits.} %\centerline {\begin{tabular}{lcccc} \hline\hline & HD~180~642 & B stars & Sun 1-D & Sun 3-D\\\hline He/H(4) & 0.088(18) & $\sim$0.089 & 0.085(1) & 0.085(2)\\ $\log \epsilon$(C)\ (9) & 8.21(10) & $\sim$8.20 & 8.52(6) & 8.39(5)\\ $\log \epsilon$(N) (21) & 8.00(19) & $\sim$7.79 & 7.92(6) & 7.78(6)\\ $\log \epsilon$(O) (25) & 8.53(14) & $\sim$8.58 & 8.83(6) & 8.66(5)\\ $\log \epsilon$(Ne) (6) & 7.86(16)$^a$ & $\sim$8.07 & 8.08(6) & 7.84(6)\\ $\log \epsilon$(Mg) (1) & 7.34(20) & $\sim$7.48 & 7.58(5) & 7.53(9)\\ $\log \epsilon$(Al) (3) & 6.22(15) & $\sim$6.08 & 6.47(7) & 6.37(6)\\ $\log \epsilon$(Si) (7) & 7.19(19) & $\sim$7.20 & 7.55(5) & 7.51(4)\\ $\log \epsilon$(S) (4) & 7.10(34) & $\sim$7.19 & 7.33(11) & 7.14(5)\\ $\log \epsilon$(Fe) (21) & 7.34(21) & $\sim$7.36 & 7.50(5) & 7.45(5)\\ \hline ${\rm [N/C]}$ & --0.21(22) & $\sim$--0.41 & --0.60(9) & --0.61(8)\\ ${\rm [N/O]}$ & --0.53(24) & $\sim$--0.79 & --0.91(9) & --0.88(8)\\ \hline $Z$ & 0.0099(16) & $\sim$0.0108 & 0.0172(12) & 0.0124(7)\\ \hline \end{tabular}} \par \smallskip {The number of spectral lines used is given in brackets in the first column. For comparison purposes, we provide typical values found for early B~dwarfs in the solar neighbourhood (Morel~\cite{morel09}, and references therein; B~stars), the standard solar composition of Grevesse \& Sauval\ (\cite{grevesse_sauval}, Sun 1-D), and updated values derived from three-dimensional hydrodynamical models (Asplund et~al.\ \cite{asplund}, Sun 3-D). We define [N/C] and [N/O] as $\log$[$\epsilon$(N)/$\epsilon$(C)] and $\log$[$\epsilon$(N)/$\epsilon$(O)], respectively. The metallicity, $Z$, is given in the last row. To compute this quantity, we assumed the abundances of Grevesse \& Sauval\ (\cite{grevesse_sauval}) for the trace elements not under study.\\ $^a$ A negligible difference amounting to 0.01~dex is obtained when using the $T_{\rm eff}$ derived from the Ne ionisation balance (Morel \& Butler\ \cite{morel_butler}).} \end{table}