Toward a refined estimation of typhoon wind hazards: Parametric modeling and upstream terrain effects
Introduction
Typhoon or hurricane (typhoon hereafter is a general representation of tropical cyclone unless otherwise stated) is a large-scale air rotating system around a low atmospheric pressure center, frequently causing devastating economic loss and human casualties along coastal regions due to violent winds, heavy rainfall, massive storm surges, flash flooding or even landslides in mountainous areas. The Western Pacific Basin is the most active typhoon basin on earth, accounting for almost one-third of global annual storms. Seven or eight typhoons per year make landfall over the coastal region of China, where is characterized by high population densities and highly developed cities. It was estimated that averaged 472 people lost their lives and annual direct economic loss reached 28.7 billion RMB as a result of landfall typhoons from year 1983–2016 in China (Zhang et al., 2009). The losses are expected to continuously increase because of growing population and increasing wealth in coastal regions as well as the potential rise of typhoon frequency and intensity due to climate change. The investigation of typhoon wind characteristics and prediction of typhoon-induced hazards are of great importance to facilitate the disaster prevention and mitigation (Fang et al., 2019, 2020).
The quantification of typhoon boundary layer with the depth about 2–3 km, within which we live and carry out most human activities, has received intensive attention in past several decades (Batts et al., 1980; Meng et al., 1995; Vickery et al., 2000a, Vickery et al., 2000b; Kepert, 2010; Snaiki and Wu, 2017; Fang et al., 2018a) for the uses of engineering applications and wind hazard estimations. Parametric typhoon wind field model was commonly adopted for its high efficiency on Monte Carlo simulations as well as its continuous improvements with the help of the more measurement data. Recent years, the ever-increasing observation data have enabled a further investigation on typhoon inner structures. Taking the advantages of flight-level aircraft and dropsondes measurements in Atlantic Basin, a series of pioneering studies have been conducted to examine the characteristics of two typical typhoon field parameters, say the radius to maximum wind speed () and radial pressure profile shape parameter (), and model them with some statistically-based equations for the convenience of stochastic simulations (Powell et al., 2005; Vickery and Wadhera, 2008). Recently, some parameter models have also been successively developed in Western Pacific region using observation data (Xiao et al., 2011; Zhao et al., 2013; Fang et al., 2018b).
However, several issues remain to be discussed about these two parameters with respect to their height-variation, region-dependent and time duration characteristics. As discussed by Willoughby and Rahn (2004), it showed that the mean value of increases slightly with height while witnesses a 45% increase from the altitude about 750 m–2500 m based on a flight-level database. Holland et al. (2010) also tried to revise the pressure-wind model by addressing the differences between surface and gradient layers. In addition, these typhoon field parameters are usually region-dependent due to the difference of atmospheric circulation features, suggesting the cross-adoption of these parameter models could result in some unreasonable predictions. Furthermore, the agency-specified wind speed averaging period varies considerably (from 1 min to 10 min), resulting in the difference of central pressure estimation based on Dvorak method (Dvorak, 1984; Velden et al., 2006). This could be extended to the misunderstanding of and during their extractions and applications. Another issue is that the statistical models of and were always formulated as the function of central pressure deficit, typhoon center latitude and sea surface temperature . The autocorrelations between different timesteps are indirectly propagated from the central pressure deficit, and sea surface temperature during empirical full track simulations. This could result in the storm structure and size fluctuate notably with timesteps, which is inconsistent with the real cases.
To extract the parameters of and , a parametric typhoon pressure or wind field model should be introduced. However, most parametric wind field models are simplified from Navier-Stokes equations, i.e. several nonlinear terms and non-symmetric characteristics are customarily eliminated. If the Holland parametric pressure model described by and is derived from real pressure observations, the pressure field would be well reconstructed. But it could lead to unreal wind field due to the use of simplified model solutions. Alternatively, if and are extracted from the fitting results of real winds, the modeled wind field is as close to the reality as possible regardless of whether the pressure field is real or unreal. This can be achieved using the archived wind information in some best track dataset, such as HURDAT2 in Atlantic Basin and RSMC Best Track Data in Northwestern Pacific Ocean provided by Japan Meteorological Agency. It also allows the consideration of autocorrelations and between different timesteps to better conduct the stochastic simulations of wind hazard. Moreover, the evolutions of wind speed for each historical typhoon event can be reconstructed to facilitate the typhoon hazard assessment and mitigation.
Conventionally, to reproduce the over-land wind snapshots or footprints of typhoon storms, the underlying exposure was assumed as the open-flat terrain. However, local terrain roughness and topographic features as well as surrounding obstacles would determine the development of a boundary layer and evolution of turbulence. In reality, a sudden change of elevation or topography would have an obvious impact on surface wind speed over a very short distance (Miller et al., 2013), especially the speeds near the crests of ridges and hills, which show marked increases when compared with the wind speed measured at same height above the flat terrain. Some studies (Lemelin et al., 1988; Weng et al., 2000) found that the wind speed at top of the hill could even double the speed that over flat terrain due to topographic effects, which represents a structure on top of hill would experience an increase of 400% in the wind load than that in flat area. Accordingly, quantification of directional roughness and topographic effects is essentially important for typhoon wind hazards assessments. Some pioneer studies (Jackson and Hunt, 1975; Taylor et al., 1983; Hunt et al., 1988) have well developed the theory of boundary layer flow over low-slope topography. These methods provide a good estimation of topography effects for low slope hills but require massive computation resource if they are applied to a large area.
In this study, and at surface level are optimally fitted with a high-resolving typhoon boundary layer wind field model using the JMA best track dataset. The correlations between multiple typhoon field parameters are investigated before the development of recursive models for and accounting for the autocorrelations with previous timesteps. They are used to reconstruct the wind hazards of historical typhoon events. The upstream roughness and topographic effects for sites of interest are quantitatively estimated with a directional equivalent roughness length and a topographic speed-up factor.
Section snippets
Parametric pressure field
The typhoon’s surface pressure profile along the radial direction from storm center is always prescribed before solving the pressure term of Navier-Stokes equations in an analytical wind field model. Holland (1980) described the radial surface pressure of a typhoon with two typical parameters, i.e. the radius to maximum wind speed () and a shape parameter of pressure profile () in the form ofin which subscripts and denote surface values at the radius of
Description of JMA best-track dataset
In western North Pacific and the South China Sea (0°~60°N, 100°~180°N), the Japan Meteorological Agency (JMA), was designated by the World Meteorological Organization (WMO) as the responsible agency to provide information on typhoons to support disaster mitigation activities. JMA publicly releases the best track dataset of typhoons in its responsible area from the year of 1951. The dataset contains the following information recorded at a 6- 3- or 1-h interval for each storm: (1) storm timestep
Upstream terrain effects
After the extraction of and , the wind speed field of a typhoon at each timestep can be reproduced using the present boundary layer model to facilitate the estimation of wind hazards of historical typhoons. As shown in Fig. 12, a set of grid points for the provinces along the coastal region of China is generated. The resolution for coastline area within the range of about 50 km is (or about 2.2 km) while the 400-km inland region and exclusive economic zone (EEZ) are divided by
Conclusions
The present study develops a dataset of wind parameters, i.e. and in Western Pacific Ocean using the wind data information from JMA best track dataset coupled with a semi-analytical typhoon wind field model. Although the parametric pressure model using present and would result in significant difference from the real pressure field, the modeled wind field is forced to match the observations as closely as possible to increase the accuracy of wind hazards estimation. Each
CRediT authorship contribution statement
Genshen Fang: Writing - original draft, Visualization, Software. Weichiang Pang: Methodology, Supervision. Lin Zhao: Conceptualization, Project administration. Prashant Rawal: Data curation. Shuyang Cao: Resources. Yaojun Ge: Writing - review & editing, Funding acquisition.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
The authors gratefully acknowledge the support of the National Key Research and Development Program of China (2018YFC0809600, 2018YFC0809604), the National Natural Science Foundation of China (51678451, 51778495, 51978527), the Shanghai Pujiang Program (20PJ1413600), , the China Scholarship Council and the technical support of Palmetto Cluster in Clemson University.
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