\begin{table}%ta.2 \caption{\label{t:errpar}Star-to-star (individual) errors and cluster errors in atmospheric parameters and in the EWs.} %\centerline {\small \begin{tabular}{lrllllcrrrr} \hline\hline\noalign{\smallskip} &\multicolumn{5}{c}{Star-to-star errors} & \multicolumn{1}{c}{} &\multicolumn{4}{c}{Cluster errors} \\ \cline{2-6} \cline{8-11}\\ cluster &$T_{\rm eff}$& $\log g$ & [A/H] & $v_t$ & $EW$ & & $T_{\rm eff}$& $\log g$ & [A/H] & $v_t$\\ & (K) & dex & (dex) & (km~s$^{-1}$)&(dex) & & (K) & dex & (dex) & (km~s$^{-1}$) \\ &(1) & (2) & (3) & (4) &(5) & & (6) & (7) & (8) & (9) \\ \cline{2-6} \cline{8-11}\\ NGC 104 & 6 & 0.042 & 0.032 & 0.11 & 0.025 & & 40 & 0.059 & 0.026 & 0.009 \\ NGC 288 & 6 & 0.041 & 0.042 & 0.28 & 0.025 & & 63 & 0.061 & 0.070 & 0.027 \\ NGC~1904& 5 & 0.041 & 0.036 & 0.20 & 0.027 & & 57 & 0.060 & 0.069 & 0.026 \\ NGC~3201& 4 & 0.041 & 0.049 & 0.19 & 0.028 & & 62 & 0.061 & 0.073 & 0.016 \\ NGC~4590& 4 & 0.041 & 0.071 & 0.28 & 0.037 & & 69 & 0.061 & 0.068 & 0.025 \\ NGC~5904& 12 & 0.041 & 0.023 & 0.11 & 0.024 & & 54 & 0.060 & 0.062 & 0.009 \\ NGC~6121& 4 & 0.041 & 0.025 & 0.12 & 0.022 & & 54 & 0.060 & 0.053 & 0.012 \\ NGC~6171& 2 & 0.041 & 0.044 & 0.21 & 0.025 & & 26 & 0.057 & 0.026 & 0.037 \\ NGC~6254& 4 & 0.041 & 0.053 & 0.13 & 0.026 & & 67 & 0.061 & 0.074 & 0.011 \\ NGC~6388& 9 & 0.043 & 0.078 & 0.19 & 0.037 & & 57 & 0.061 & 0.028 & 0.032 \\ NGC~6397& 4 & 0.041 & 0.039 & 0.34 & 0.038 & & 64 & 0.060 & 0.060 & 0.028 \\ NGC~6808& 5 & 0.041 & 0.044 & 0.20 & 0.027 & & 58 & 0.060 & 0.072 & 0.016 \\ NGC~6838& 5 & 0.041 & 0.034 & 0.10 & 0.023 & & 45 & 0.059 & 0.048 & 0.016 \\ NGC~7078& 5 & 0.041 & 0.061 & 0.33 & 0.030 & & 67 & 0.061 & 0.067 & 0.036 \\ NGC~7099& 5 & 0.041 & 0.046 & 0.41 & 0.034 & & 71 & 0.061 & 0.067 & 0.051 \\ \hline \end{tabular}} \medskip (1) Slope relation $T_{\rm eff}$(V-K)$_{\rm Alonso}$ vs. mag~$V$ or $K$ + 0.02~mag error in $V$ or $K$; (2) slope $\log g$ vs. mag $V$ or $K$ +0.02~mag error + 10\% variation in mass; (3)~rms scatter in [Fe/H] of all analysed stars; (4) quadratic mean of 1$\sigma$ errors in the slope abundances Fe~I/line strength (minus systematic components) from stars with a large enough number of Fe~I lines (5)~(rms in Fe~I for stars with enough lines) divided the square root of typical number of lines; (6) slope relation $T_{\rm eff}$($V-K$)$_{\rm Alonso}$ vs. ($V-K$)$_0$ +0.02 error in E(B-V) + 0.02~mag error in $V-K$ colours zero point; (7)~0.1~mag error in modulus + systematic error in $T_{\rm eff}$ +10\% error in mass; (8)~statistical error+systematic error in $T_{\rm eff}$+systematic error in $\log g$~+~systematic error in $v_t$; (9)~internal error in $v_t$ divided the square root of $N_{\rm stars}$. \end{table}