On a 3D manifold, a Weyl geometry consists of pairs (g, A) = (metric, 1-form) modulo gauge g = e 2ϕ g, A = A + dϕ. In 1943, Cartan showed that every solution to the Einstein-Weyl equations R (µν) − 1 3 Rg µν = 0 comes from an appropriate 3D leaf space quotient of a 7D connection bundle associated with a 3 rd order ODE y = H(x, y, y , y ) modulo point transformations, provided 2 among 3 primary point invariants vanishWe find that point equivalence of a single PDE z y = F (x, y, z, z x ) with para-CR integrability DF := F x + z x F z ≡ 0 leads to a completely similar 7D Cartan bundle and connection. Then magically, the (complicated) equation Wünschmann(H) ≡ 0 becomeswhose solutions are just conics in the {p, F }-plane. As an ansatz, we takewith 9 arbitrary functions α, . . . , ν of y. This F satisfies DF ≡ 0 ≡ Monge(F ), and we show that the condition Cartan(H) ≡ 0 passes to a certain K(F ) ≡ 0 which holds for any choice of α(y), . . . , ν(y). Descending to the leaf space quotient, we gain ∞-dimensional functionally parametrized and explicit families of Einstein-Weyl structures (g, A) in 3D. These structures are nontrivial in the sense that dA ≡ 0 and Cotton([g]) ≡ 0.