Plasma irregularities are mostly generated after the local sunset on some nights over the dip-equatorial regions, and their effects extend to low latitudes. These irregularities span over seven orders of magnitude in scale sizes and manifest themselves in different ways. For example, they are observed as a spread (both in frequency and range) in reflected echoes in ionosondes, intensity depleted regions or plasma bubbles in airglow imagers, backscatter plumes in incoherent radar measurements, and scintillations in GPS signals. In the evening hours, the ionospheric F-layer gets lifted to higher altitudes due to enhancement in the eastward electric field (known as the pre-reversal enhancement [PRE] of the electric field). Further, plasma recombination in the lower heights contributes to an apparent rise in the F-layer. These cause a sharp gradient in the bottom side plasma density, which can potentially become unstable and generate plasma irregularities through the Rayleigh-Taylor (R-T) instability process. As the ion-neutral collision frequency reduces with altitude, the amplitude of any plasma density perturbation in the bottom side of the equatorial ionosphere grows while moving upward. Studies on the growth rate of these irregularities in the F-region as a function of different background conditions can be found