An attempt is made to explain the nature of the electric signal observed in He II in a second-sound standing wave. Using the general quantum-mechanical principles, we show that, due to interatomic interaction, each atom of He-II acquires a small fluctuating induced dipole moment with the average value of its modulus dat = 2eδ, δ ≃ 2.6 × 10 −4 Å. A directed flux of microscopic vortex ringswhich, together with phonons, are thermal excitations of He II -forms in the second-sound standing halfwave. This flux partially orders the chaotically oriented dipole moments of the atoms, which results in volume polarization of He II. The observed electric induction △U ≈ k B △T /2e can be explained theoretically under the assumption that each vortex ring possesses a dipole moment d vr of the order of ten atomic moments, d vr ∼ 10 dat .It is shown also that the theoretical value of the voltage △U induced in He II by the volume system of dipoles strongly depends on the dimensions of the resonator for dipoles of any origin. The experimental value of △U is the same for two resonators of different size; therefore, this voltage may be not connected with the volume polarization of He II.