“…and we will find the solution of Problems (2.10), (2.11), considering loaded part as known, 36 Let us introduce the notations v 0 (x, t, 𝜏) = U(x, t, 𝜏) and v k (x, t, 𝜏) = G k v 0 (x, t, 𝜏). In these notation, Problems (2.10), (2.11) are equivalent to the following problem about v k (x, t, 𝜏), k = 0, m − 1, finding functions of equations…”