“…As a matter of fact, these deformations can be described by using a deformed boundary operator∂ ↤ ∂, see [1,10,11,12] for more detailed exposition. Theorem 6.2 (operadic Stokes law [10,11,12], cf [1]). The variations of the operadic flows result as superpositions over the corresponding deformed boundaries, δ =δ ∂ i.eδ ⟨⋅ ⋅⟩ =δ ∂ ⟨⋅⟩ ⟨⋅ ⋅⟩ ,δ ⟨⋅ ⋅ ⋅⟩ =δ ∂ ⟨⋅⋅⟩ ⟨⋅ ⋅ ⋅⟩ ,δ ⟨⋅ ⋯⟩ = ⟨⋅ ⋯⟩ , .…”