We provide a set of rules to define several spinful quantum Hall model states. The method extends the one that is known for spin-polarized states. It is achieved by specifying an undressed root partition, a squeezing procedure, and rules to dress the configurations with spin. It applies to both the excitationless and the quasihole states. In particular, we show that the naive generalization where one preserves the spin information during the squeezing sequence, may fail. We give numerous examples such as the Halperin states, the non-abelian spin singlet states, or the spin-charge separated states. The squeezing procedure for the series (k = 2, r) of spinless quantum Hall states, which vanish as r powers when k + 1 particles coincide, is generalized to the spinful case. As an application of our method, we show that the counting observed in the particle entanglement spectrum of several spinful states matches the one obtained through the root partitions and our rules. This counting also matches the counting of quasihole states of the corresponding model Hamiltonians, when the latter are available.PACS numbers: 05.30.Pr, Recent developments in generating candidate quantum Hall wave functions gave rise to a framework based on root partitions, squeezing, and highest weight conditions that provides an elegant manner to address several can-arXiv:1107.2232v2 [cond-mat.str-el]