“…According to Kudryavtsev et al. (
2019), the OML thickness for a fast‐moving TC is approximately proportional to,
where, N is the Brunt‐Väisälä frequency for the seasonal pycnocline, U 10 is ocean surface wind speed at 10‐m height, R max is the radius of maximum wind, and U h is the TC's translation speed. The wind‐driven current speed in the OML for a moving TC (Price,
1983) can be approximately expressed as
where, τ is wind stress (
) which can be estimated from air density ( ρ air ), drag coefficient ( C d ) and U 10 .…”