Collisional interactions between neutral and plasma particles at the E-region heights (ca. 90-150 km) lead to the production of electric fields and currents, which can be expressed as follows:where J is the current density, ˆ is the ionospheric conductivity tensor, E is the electric field, U is the neutral wind, and B is the ambient magnetic field. Large-scale motion of the atmosphere across the geomagnetic field drives electric currents on the dayside ionosphere, where the conductivity is enhanced due to photoionization mainly by solar extreme ultraviolet radiation. Electric fields are generated in such a manner that the total currents (i.e., the sum of wind-driven currents and electric field-driven currents) are divergence free (Richmond & Roble, 1987). Under geomagnetically quiet conditions, the electric field in the low-latitude ionosphere is usually eastward on the dayside. The zonal electric field sets up a vertical polarization electric field near the magnetic equator, which drives the zonal current in the same direction as the current driven by the zonal electric field. As a result, there is a band of enhanced current flowing along the magnetic equator, which is known as the equatorial electrojet (EEJ) (e.g., Forbes, 1981;Yamazaki & Maute, 2017).The EEJ shows large day-to-day variation, which is closely connected to changes in the zonal electric field and equatorial ionization anomaly (e.g., Stolle et al., 2008). The variation is large enough so that the usually eastward EEJ sometimes turns westward (e.g., Soares et al., 2018;Zhou et al., 2018). The driving mechanism of the westward EEJ is not well understood. This study discusses the possible contributions of neutral winds