The Minkowski tensor gives gM = nu/c (I) for the momentum density g of a plane-wave electromagnetic
field in a stationary medium, whereas the Abraham tensor gives gA = u/nc (II), where u is the energy
density and n the refractive index. Expression (I) cannot be reconciled with J = μν (III), where μ is the
mass of the wave packet and ν is its velocity if, according to Einstein, μ = E/c2, where J is the
momentum and E the energy of the wave packet. On the other hand, the expression for the
"pseudomomentum" JM = nE/c (IV), which follows from (I), is identical with the expression for the
momentum of the quantum photon J = nhν/c (V), whereas the formula the follows from (II), i.e.,
JA = E/nc (VI) is in agreement with the Einstein equation (III) but is in conflict with (V). Simple
calculation for stationary medium and source shows that (IV) and (VI) can be reconciled if one takes into
account the fact that, under certain assumptions, JM = JA + ΔJ (VII), where ΔJ is the momentum
communicated to the medium in the photon emission process. It is shown in this paper that, within the
framework of the adopted assumptions and, probably, classical models generally, expression (VII) cannot
be generalized to the case of a source moving relative to the medium. This result is in conflict with the
conclusions reported by V. L. Ginzberg and V. A. Ugarov [Usp. Fiz. Nauk 118, 175 (1976)] [Sov. Phys.
Usp. 19, 94 (1976)]. Moreover, it is shown that, if (VII) is introduced as a postulate for a source moving
relative to the medium, one can satisfy at the same time both the quantum conditions and (V), on the one
hand, and the fundamental Einstein relation (III), on the other.