We have investigated the magnetic properties in the well localized compound NdFe${}_{2}$Al${}_{10}$ and the Kondo semiconductor Ce${T}_{2}$Al${}_{10}$ ($T=\text{Ru}$, Os) to clarify the origin of the unusual magnetic order in Ce${T}_{2}$Al${}_{10}$. In NdFe${}_{2}$Al${}_{10}$, the experimental results of the magnetic properties could be reproduced very well by the mean-field calculation for the two-sublattice model. In Ce${T}_{2}$Al${}_{10}$ we could reproduce the anisotropic magnetic susceptibility in the paramagnetic region above 60--100 K very well by the mean-field calculation for the two-sublattice model introducing an anisotropic exchange interaction and the recently determined crystalline electric field (CEF) level scheme from Strigari et al. [Phys. Rev. B 86, 081105 (2012)]. However, in the antiferromagnetic (AFM) ordered state, we could not reproduce the experimental results at all in the framework of the mean-field calculation for the two-sublattice model. We propose that although the magnetic properties in the paramagnetic region above 60--100 K could be understood well by a localized picture, the ordered state could not, and that the $c$-$f$ hybridization, especially along the $a$ axis, is associated with the unusual magnetic order in Ce${T}_{2}$Al${}_{10}$.