It is shown that all the $K\to 2\pi$ decays are forbidden in the limit of complete S${\mathrm{U}}_3$ symmetry of strong interactions, provided only (a) that both $K$ and $\pi$ mesons belong to the same octet and (b) that the nonleptonic decay interactions belong to the $\mathrm{CP}$-invariant representation (the irreducible representation whose $Y=Q=0\mathrm{}$ members are $\mathrm{CP}$-invariant). This is more general than the conclusion of Cabibbo and Gell-Mann. In their proof, the nonleptonic decay Lagrangian is assumed to belong to a $\mathrm{CP}$-invariant octet. This result suggests that the observed large decay rate of ${K_1}^0\to 2\pi$ decay is due to the symmetry-breaking interactions and its large $Q$ value. Finally, a brief comment is given concerning the $({K_1}^0\to 2\pi )-(K^{+}\to 2\pi )$ puzzle in the $\Delta I=\frac{1}{2}$ rule. It is shown that, if one assumes the $\Delta I=\frac{1}{2}$ rule in addition to the above hypothesis (b), the $K^{\pm }\to 2\pi$ decay can occur only through the electromagnetic corrections and its effective decay Lagrangian should belong to the representations 10 and $\overline{1}\overline{0}$.

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