Precipitation over the tropical open oceans (i.e., areas at least 200 km away from coastlines) generally shows a diurnal cycle that peaks in the early morning (Dai, 2001;Mapes & Houze, 1993;Yang & Slingo, 2001;Zuidema, 2003). Previous studies have indicated that the early-morning precipitation peak is closely related to diurnal radiative effects (e.g., Gray & Jacobson, 1977;Liu & Moncrieff, 1998;Randall et al., 1991). During the nighttime, net radiative cooling at the cloud top is stronger than that below the cloud base. This process destabilizes the atmosphere and provides a favorable thermodynamical condition for the initiation and development of nocturnal convection (i.e., lapse rate mechanism, Liu & Moncrieff, 1998;Randall et al., 1991). Additionally, different radiative cooling intensities between the cloudy and clear-sky regions enhance the convergence below clouds, thus facilitates the development of nocturnal convection (i.e., differential radiation mechanism, Gray & Jacobson, 1977). Unlike most tropical open oceans with early-morning precipitation peaks, some have a prominent afternoon precipitation peak. Most of these areas are partially enclosed by coastlines, such as the open oceans between northwestern South America and the isthmus of Central America, the Gulf of Guinea, the South China Sea, and the Bay of Bengal (the BoB hereafter; Johnson, 2010). Among these areas, the BoB has been most extensively investigated due to its strong precipitation intensity.