The lithosphere‐atmosphere‐ionosphere coupling problem is a challenge nowadays. It requires understanding of (a) the physical mechanism that is responsible for plasma disturbances generation at ionospheric heights, (b) the penetration of seismogenic impact from the ground into the ionosphere through the underlying neutral atmosphere, and (c) on‐the‐ground (in‐the‐ground) sources generation. Kuo et al. (2014) reported an improved model of lithosphere‐atmosphere‐ionosphere coupling that includes the ionosphere as well as the underlying neutral atmosphere (from the ground up to the ionosphere altitudes, i.e., 60–80 km above the Earth's surface). The main feature of the Kuo et al. (2014) approach is that they find ground‐to‐ionosphere currents from
∇·trueJ→=0,
trueJ→≡−∇ψ system of equations. In contrast to Kuo et al. (2011), where well‐known
∇·trueJ→=0,trueJ→=trueσ̂trueE→,trueE→=−∇ϕ equations are used, Kuo et al. (2014) looks better as it does not require the knowledge of electric conductivity σ profile. In this paper we show that the Kuo et al. (2014) equations can be obtained as a special case of the Kuo et al. (2011) ones, given the electric conductivity tensor is a spatially invariant scalar. Therefore, Kuo et al. (2014) formulation may not describe correctly electric currents flowing between the Earth and the ionosphere.