Carbonate rocks (i.e., rocks containing at least 50% of calcite or dolomite) are among the most common rocks at the surface of the Earth (∼20% of sedimentary rocks) and form an important source of drinkable water aquifers (e.g., Ford & Williams, 2007) and 40% of the oil and gas reservoirs (e.g., Brigaud et al., 2014). The electrical conductivity of carbonate rocks has been broadly investigated in the literature (e.g., Cerepi, 2004;Focke & Munn, 1987;Regnet et al., 2019;Winn, 1957). It is generally assumed that conductivity of these rocks is dominated by the bulk conductivity associated with conduction in the pore water located in the connected pore network. Similarly, the Maxwell-Wagner polarization of carbonate rocks (occurring at intermediate frequency range ∼100 Hz-10 MHz) has also been broadly described (e.g., Hizem et al., 2008). The Maxwell-Wagner or interfacial polarization is related to the discontinuity of the displacement current density at the interface between the different phases of a porous composite. That said, little quantitative investigations have been performed regarding their induced (low-frequency, <∼10 kHz) polarization properties despite the need for a simple physics-based model of induced polarization in carbonate rocks that can be applied to field data.Induced polarization refers to the reversible charge accumulation in charged porous media under the influence of a primary electrical field and at low frequencies (i.e., typically <10 kHz, e.g., Abdulsamad et al., 2019;Börner, 1992). These charge accumulations occur mostly at grain or pore scales (e.g., Weller et al., 2015), which correspond to polarization length scales controlling a distribution of relaxation times. In the field, induced polarization imaging is nowadays broadly used in the realm of hydrogeophysics (Bin-