The biharmonic equation arises in areas of continuum mechanics including linear elasticity theory and the Stokes flows, as well as in a radar imaging problem. We discuss the reflection formulas for the biharmonic functions u(x, y) ∈ R 2 subject to different boundary conditions on a real-analytic curve in the plane. The obtained formulas, generalizing the celebrated Schwarz symmetry principle for harmonic functions, have different structures.In particular, in the special case of the boundary, Γ 0 := {y = 0}, reflections are point-topoint when the given on Γ 0 conditions are u = ∂ n u = 0, u = u = 0 or ∂ n u = ∂ n u = 0, and point to a continuous set when u = ∂ n u = 0 or ∂ n u = u = 0 on Γ 0 .