2016
DOI: 10.1175/jas-d-15-0165.1
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Quadrant-Dependent Evolution of Low-Level Tangential Wind of a Tropical Cyclone in the Shear Flow

Abstract: This study investigates the quadrant-by-quadrant evolution of the low-level tangential wind near the eyewall of an idealized simulated mature tropical cyclone embedded in a unidirectional shear flow. It is found that the quadrant-averaged tangential wind in the right-of-shear quadrants weakens continuously, while that in the left-of-shear quadrants experiences a two-stage evolution: a quasi-steady stage followed by a weakening stage after the imposing of vertical wind shear. This leads to a larger weakening ra… Show more

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Cited by 20 publications
(12 citation statements)
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“…Cha (2018) conducted a similar analysis on Hurricane Matthew and found the wavenumber‐1 maximum roughly in the same region of the eyewall, though slight differences in the location may be due to different methods used. Previous composite and modeling studies show that the strongest tangential winds in a sheared eyewall typically create a wavenumber‐1 asymmetry left of the shear vector with a maximum in the DL quadrant (Reasor et al, 2013; Uhlhorn et al, 2014; Zhang et al, 2013), a result of inward advection of angular momentum downshear (Gu et al, 2016). The wavenumber‐1 wind maximum in the downshear to DR region in Matthew could have contributions from other environmental or dynamic forcings.…”
Section: Kinematic Observations Of the Eyewallmentioning
confidence: 99%
“…Cha (2018) conducted a similar analysis on Hurricane Matthew and found the wavenumber‐1 maximum roughly in the same region of the eyewall, though slight differences in the location may be due to different methods used. Previous composite and modeling studies show that the strongest tangential winds in a sheared eyewall typically create a wavenumber‐1 asymmetry left of the shear vector with a maximum in the DL quadrant (Reasor et al, 2013; Uhlhorn et al, 2014; Zhang et al, 2013), a result of inward advection of angular momentum downshear (Gu et al, 2016). The wavenumber‐1 wind maximum in the downshear to DR region in Matthew could have contributions from other environmental or dynamic forcings.…”
Section: Kinematic Observations Of the Eyewallmentioning
confidence: 99%
“…Large-scale vertical wind shear (VWS), also referred to as deep-layer shear, is commonly defined as the difference between horizontal wind vectors in the 200-and 850-hPa layers, averaged over an area in an annular region or within a given radius from the tropical cyclone (TC) center. Although deep-layer shear is responsible for TC genesis (Gray 1968;Tuleya and Kurihara 1981), structure (Black et al 2002;Corbosiero and Molinari 2003;Reasor et al 2013;Zhang et al 2013;DeHart et al 2014;Gu et al 2016), and intensity change (Simpson and Riehl 1958;DeMaria 1996;Frank and Ritchie 2001;Wu and Braun 2004;Riemer et al 2010;Tang and Emanuel 2010;Gu et al 2015), it alone is not enough to represent the overall vertical structure of a large-scale environmental flow. For example, observational analysis (Wang et al 2015) and idealized simulations (Finocchio et al 2016) both found that low-level shear is more destructive to TC intensification than is deep-layer shear.…”
Section: Introductionmentioning
confidence: 99%
“…Important roles of environmental vertical shear in TC structure and intensity changes have long been known. Large vertical shear is generally negative to TC intensification (DeMaria 1996;Zeng, Wang, and Chen 2010;Riemer, Montgomery, and Nicholls 2010;Gu, Tan, and Qiu 2016;Wang et al 2015), and produces inner-core asymmetric convection with stronger convection downshear-left (Jones 1995;Rogers et al 2003). Recently, ambient vertical shear has also been found to cause outer-rainband formation in the downshear quadrant (Li, Wang, and Duan 2017).…”
Section: Introductionmentioning
confidence: 99%