Three physical mechanisms behind the modeled convective behavior were suggested and explored through an additional experiment in which time-and space-independent surface fluxes were applied and through a set of dry simulations involving the nonlinear atmospheric response to the ITCZ-like heat sources located at various latitudes. The first was the wind-induced surface flux variability which played a vital role in the formation of the single ITCZ on the equator in the control simulation. The second was the enhanced low-level convergence by the planetary rotation regarding the response to convective heating, which favored an ITCZ displaced from the equator. The third concerned the trapping of convection-generated subsidence warming and drying by the Coriolis force, which preferred an equatorial ITCZ. The combination of the last two conflicting dynamical processes resulted in a double ITCZs positioned at a finite distance (approximately 800~1500 km) away from the equator in the control simulation and also in the sensitivity experiment with uniform surface fluxes.
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