326. Charges with surface densities σ1 and σ2 are evenly distributed on two infinite parallel planes (Fig. 25). It is required: 1) using the Ostrogradsky-Gauss theorem and the principle of superposition of electric fields, find the expression E (x) of the electric field strength in three areas: I, II and III. Take σ1 = -4σ, σ2 = 2σ; 2) calculate the field strength E at a point located between the planes, and indicate the direction of the vector E, σ = 40 nC / m2; 3) build a graph of E (x).