Wind-generated ocean surface waves give rise to a near-surface velocity known as Stokes drift (SD) (Stokes, 1847), which can contribute substantially to near-surface mass transport. SD is widely applied in representation of nearshore circulation in coastal zones and in modeling of tracer transport as the difference between Lagrangian and Eulerian averages, and it is responsible for the Coriolis-Stokes force in the upper-ocean layer in Eulerian models (van den Bremer & Breivik, 2018). It has been shown that wave-induced water transport due to SD can affect a wide range of ocean states in dramatic ways (Hasselmann, 1971). The magnitude of SD can reach the same as that of wind transport in high-and mid-latitude oceans (McWilliams & Restrepo, 1999;Shi et al., 2016). Tamura et al. (2012) proposed that SD plays an important role in the momentum balance of the upper ocean through introduction into the average Eulerian flow. Moreover, SD also influences the mixed layer of the ocean by causing Langmuir turbulence generation (McWilliams et al., 2014).