Table 9: Comparison of average values of colour gradients for the subsample IR0 of objects with zero IRAS 100 $\mu $ flux and the subsample IR1 of objects with non zero flux (Knapp et al. 1989).
Y IR0 N Av0 IR1 N  
$\Delta _{BV}$ IR0 17 $-0.065\pm.005$ IR1 35 $-0.067\pm.004$
$\Delta _{UB}$ id 13 $-0.166\pm.015$ id 27 $-0.152\pm.007$
$\Delta_{BR}$ id 14 $-0.083\pm.008$ id 28 $-0.081\pm.005$
$\Delta_{VI}$ id 15 $-0.057\pm.009$ id 34 $-0.063\pm.006$
$\Delta _{VJ}$ id 17 $-0.106\pm.026$ id 35 $-0.147\pm.015$
id id 16 $-0.089\pm.014$ id 34 $-0.139\pm.013$
$\Delta _{VK}$ id 17 $-0.199\pm.029$ id 35 $-0.237\pm.018$
id id 16 $-0.175\pm.017$ id 34 $-0.227\pm.015$
$\Delta_{JK}$ id 17 $-0.090\pm.009$ id 35 $-0.092\pm.005$
1) Gradient Y; (2) subsample IR0; (3) N number of objects; (4) average Av0; (5) subsample IR1; (6) N number of objects; (7) average Av1. NB: the 2nd. line for $\Delta _{VJ}$, $\Delta _{VK}$ gives the solution after the rejection at $3\sigma$ of NGC 4660 from the subsample IR0 and 5866 from IR1.

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