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EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE

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doi: 10.3969/j.issn.1006-8775.2012.02.007

  • In this study, the effect of vertical wind shear (VWS) on the intensification of tropical cyclone (TC) is investigated via the numerical simulations. Results indicate that weak shear tends to facilitate the development of TC while strong shear appears to inhibit the intensification of TC. As the VWS is imposed on the TC, the vortex of the cyclone tends to tilt vertically and significantly in the upper troposphere. Consequently, the upward motion is considerably enhanced in the downshear side of the storm center and correspondingly, the low- to mid-level potential temperature decreases under the effect of adiabatic cooling, which leads to the increase of the low- to mid-level static instability and relative humidity and then facilitates the burst of convection. In the case of weak shear, the vertical tilting of the vortex is weak and the increase of ascent, static instability and relative humidity occur in the area close to the TC center. Therefore, active convection happens in the TC center region and facilitates the enhancement of vorticity in the inner core region and then the intensification of TC. In contrast, due to strong VWS, the increase of the ascent, static instability and relative humidity induced by the vertical tilting mainly appear in the outer region of TC in the case with stronger shear, and the convection in the inner-core area of TC is rather weak and convective activity mainly happens in the outer-region of the TC. Therefore, the development of a warm core is inhibited and then the intensification of TC is delayed. Different from previous numerical results obtained by imposing VWS suddenly to a strong TC, the simulation performed in this work shows that, even when the VWS is as strong as 12 m s-1, the tropical storm can still experience rapid intensification and finally develop into a strong tropical cyclone after a relatively long period of adjustment. It is found that the convection plays an important role in the adjusting period. On one hand, the convection leads to the horizontal convergence of the low-level vorticity flux and therefore leads to the enhancement of the low-level vorticity in the inner-core area of the cyclone. On the other hand, the active ascent accompanying the convection tends to transport the low-level vorticity to the middle levels. The enhanced vorticity in the lower to middle troposphere strengths the interaction between the low- and mid-level cyclonical circulation and the upper-level circulation deviated from the storm center under the effect of VWS. As a result, the vertical tilting of the vortex is considerably decreased, and then the cyclone starts to develop rapidly.
  • [1] RAMAGE C S. Hurricane Development [J]. J. Meteor., 1959, 16(3): 227-237.
    [2] MERRILL R T. Environmental influences on hurricane intensification [J]. J. Atmos. Sci., 1988, 45(11): 1678-1687.
    [3] GRAY W M. Global view of the origin of tropical disturbances and storms [J]. Mon. Wea. Rev., 1968, 96(10): 669-700.
    [4] McBRIDE J L, ZEHR R M. Observational analysis of tropical cyclone formation. Part II: Comparison of non-developing versus developing systems [J]. J. Atmos. Sci., 1981, 38(6): 1132-1151.
    [5] TULEYA R E, KURIHARA Y. A numerical study on the effects of environmental flow on tropical storm genesis [J]. Mon. Wea. Rev., 1981, 109(12): 2487-2506.
    [6] ZEHR R M. Tropical cyclogenesis in the western North Pacific [R]. NOAA Tech. Rep., NESDIS, 1992, 61: 181pp.
    [7] GALLINA G M, VELDEN C S. Environmental vertical wind shear and tropical cyclone intensity change utilizing enhanced satellite derived wind information [C]// Extended Abstracts, 25th Conf. on Hurricanes and Tropical Meteorology, San Diego: Amer. Meteor. Soc., 2002: 172-173.
    [8] SIMPSON R H, RIEHL H. Mid-tropospheric ventilation as a constraint on hurricane development and maintenance [C]// Proc. Technical Conf. on Hurricanes, Miami Beach: Amer. Meteor Soc., 1958: D4.1-D4.10.
    [9] JONES S C. The evolution of vortices in vertical shear. I: Initially barotropic vortices [J]. Quart. J. Roy. Meteor. Soc., 1995, 121(524): 821-851.
    [10] MARKS F D Jr, HOUZE R A Jr, GAMACHE J F. Dual-aircraft investigation of the inner core of Hurricane Norbert. Part I: Kinematic structure [J]. J. Atmos. Sci., 1992, 49(11): 919-942.
    [11] FRANKLIN J L, LORD S J, FEUER S E, et al. The kinematic structure of Hurricane Gloria (1985) determined from nested analyses of dropwinsonde and Doppler wind data[J]. Mon. Wea. Rev., 1993, 121(9): 2433-2451.
    [12] CORBOSIERO K L, MOLINARI J. The effects of vertical wind shear on the distribution of convection in tropical cyclones [J]. Mon. Wea. Rev., 2002, 130(8): 2100-2123.
    [13] CORBOSIERIO K L, MOLINARI J. The relationship between storm motion, vertical wind shear and convection asymmetries in tropical cyclones [J]. J. Atmos. Sci., 2003, 60(2): 366-376.
    [14] DeMARIA M. The effect of vertical wind shear on tropical cyclone intensity change [J]. J. Atmos. Sci., 1996, 53(14): 2076-2087.
    [15] FRANK W M, RITCHIE E A. Effects of vertical wind shear on the intensity and structure of numerically simulated hurricanes [J]. Mon. Wea. Rev., 2001, 129(9): 2249-2269.
    [16] FRANK W M, RITCHIE E A. Tropical cyclones in complex vertical shears [C]// Extended Abstracts, 25th Conf. on Hurricanes and Tropical Meteorology, San Diego: Amer. Meteor. Soc., 2002: 315-316.
    [17] BLACK M L, GAMACHE J F, MARKS JR F D, et al. Eastern Pacific Hurricanes Jimena of 1991and Olivia of 1994: The effect of vertical shear on structure and intensity [J]. Mon. Wea. Rev., 2002, 130(9): 2291-2312.
    [18] MOLINARI J, VOLLARO D, CORBOSIERIO K L. Tropical cyclone formation in a sheared environment: A case study [J]. J. Atmos. Sci., 2004, 61(21): 2493-2509.
    [19] JONES S C. The evolution of vortices in vertical shear. II: Large-scale asymmetries [J]. Quart. J. Roy. Meteor. Soc., 2000, 126(570): 3137-3159.
    [20] JONES S C. The evolution of vortices in vertical shear. III: Baro-clinic vortices [J]. Quart. J. Roy. Meteor. Soc., 2000, 126(570): 3161-3185.
    [21] JONES S C. On the ability of dry tropical-cyclone-like vortices to withstand vertical shear [J]. J. Atmos. Sci., 2004, 61(1): 114-119.
    [22] WONG M L M, CHAN J C L. Tropical cyclone intensity in vertical wind shear [J]. J. Atmos. Sci., 2004, 61(15): 1859-1876.
    [23] ZHANG D L, KIEU C Q. Shear-forced vertical circulations in tropical cyclones [J]. Geophys. Res. Lett., 2005, 32(L13822): 1-4.
    [24] REASOR P D, MONTGOMERY M T, GRASSO L D. A new look at the problem of tropical cyclones in vertical shear flow: Vortex resiliency [J]. J. Atmos. Sci., 2004, 61(1): 3-22.
    [25] SCHECTER D A, MONTGOMERY M T. Waves in a cloudy vortex [J]. J. Atmos. Sci., 2007, 64(2): 314-337.
    [26] HONG S Y, DUDHIA J, CHEN S H. A revised approach to ice microphysical processes for the bulk parameterization of clouds and precipitation [J]. Mon. Wea. Rev., 2004, 132(1): 103-120.
    [27] NOH Y, CHEON W G, HONG S Y, et al. Improvement of the K-profile model for the planetary boundary layer based on large eddy simulation data [J]. Bound.-Layer Meteor., 2003, 107(2): 401-427.
    [28] NGUYEN V S, SMITH R K, MONTGOMERY M T. Tropical cyclone intensification and predictability in three dimensions [J]. Quart. J. Roy. Meteor. Soc., 2008, 134(632): 563-582.
    [29] NOLAN D S. What is the trigger for tropical cyclogenesis?[J]. Aust. Meteor. Mag., 2007, 56(4): 241-266.
    [30] JORDAN C L. Mean soundings for the West Indies area[J]. J. Meteor., 1958, 15(1): 91-97.
    [31] ROTUNNO R, EMANUEL K A. An air�Csea interaction theory for tropical cyclones. Part II: Evolutionary study using a nonhydrostatic axisymmetric numerical model [J]. J. Atmos. Sci., 1987, 44(3): 542-561.
    [32] FRANK W M, RITCHIE E A. Effects of environmental flow on tropical cyclone structure [J]. Mon. Wea. Rev., 1999, 127(9): 2044-2061.
    [33] KNAFF J A, SESESKE S A, DEMARIA M, et al. On the influences of vertical wind shear on symmetric tropical cyclone structure derived from AMSU [J]. Mon. Wea. Rev., 2004, 132(10): 2503-2510.
    [34] YUTER S E, HOUZE JR R A. Three-dimensional kinematic and microphysical evolution of Florida cumulonimbus. Part III: Vertical mass transport, mass divergence, and synthesis [J]. Mon. Wea. Rev., 1995, 123(7): 1964-1983.
    [35] BLACK M L, BURPEE R W, MARKS JR F D. Vertical motion characteristics of tropical cyclones determined with airborne Doppler radial velocities [J]. J. Atmos. Sci., 1996, 53(13): 1887-1909.
    [36] ROGERS R F, BLACK M L, CHEN S S, et al. An evaluation of microphysics fields from mesoscale model simulation of tropical cyclones. Part I: Comparisons with observations [J]. J. Atmos. Sci., 2007, 64(6): 1811-1834.
    [37] ZHANG F, SIPPEL J A. Effects of moist convection on hurricane predictability [J]. J. Atmos. Sci., 2009, 66(7): 1944-1961.
    [38] FAMG J, ZHANG F. Initial development and genesis of Hurricane Dolly (2008) [J]. J. Atmos. Sci., 2010, 67(3): 655-672.
    [39] MONTGOMERY M T, NICHOLLS M E, CRAM T A, et al. A vortical hot tower route to tropical cyclogenesis [J]. J. Atmos. Sci., 2006, 63(1): 355-386.
    [40] TORY K J, MONTGOMERY M T. Tropical cyclone formation: A synopsis of the internal dynamics [C/OL]. Preprints, 28th Conf. on Hurricanes and Tropical Meteorology, Orlando: Amer. Meteor. Soc, 2008, 10A.1. [2011-09-30] http://ams.confex.com/ams/28Hurricanes/techprogram/paper_1 38062.htm
    [41] SKAMAROCK W C, COAUTHORS. A description of the Advanced Research WRF version 2 [R]. NCAR Tech. Note NCAR/TN-4681STR, 2005: 88pp.

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CHEN Qi-zhi, FANG Juan. EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE [J]. Journal of Tropical Meteorology, 2012, 18(2): 172-186, https://doi.org/10.3969/j.issn.1006-8775.2012.02.007
CHEN Qi-zhi, FANG Juan. EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE [J]. Journal of Tropical Meteorology, 2012, 18(2): 172-186, https://doi.org/10.3969/j.issn.1006-8775.2012.02.007
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Manuscript received: 30 September 2011
Manuscript revised: 16 February 2012
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EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE

doi: 10.3969/j.issn.1006-8775.2012.02.007

Abstract: In this study, the effect of vertical wind shear (VWS) on the intensification of tropical cyclone (TC) is investigated via the numerical simulations. Results indicate that weak shear tends to facilitate the development of TC while strong shear appears to inhibit the intensification of TC. As the VWS is imposed on the TC, the vortex of the cyclone tends to tilt vertically and significantly in the upper troposphere. Consequently, the upward motion is considerably enhanced in the downshear side of the storm center and correspondingly, the low- to mid-level potential temperature decreases under the effect of adiabatic cooling, which leads to the increase of the low- to mid-level static instability and relative humidity and then facilitates the burst of convection. In the case of weak shear, the vertical tilting of the vortex is weak and the increase of ascent, static instability and relative humidity occur in the area close to the TC center. Therefore, active convection happens in the TC center region and facilitates the enhancement of vorticity in the inner core region and then the intensification of TC. In contrast, due to strong VWS, the increase of the ascent, static instability and relative humidity induced by the vertical tilting mainly appear in the outer region of TC in the case with stronger shear, and the convection in the inner-core area of TC is rather weak and convective activity mainly happens in the outer-region of the TC. Therefore, the development of a warm core is inhibited and then the intensification of TC is delayed. Different from previous numerical results obtained by imposing VWS suddenly to a strong TC, the simulation performed in this work shows that, even when the VWS is as strong as 12 m s-1, the tropical storm can still experience rapid intensification and finally develop into a strong tropical cyclone after a relatively long period of adjustment. It is found that the convection plays an important role in the adjusting period. On one hand, the convection leads to the horizontal convergence of the low-level vorticity flux and therefore leads to the enhancement of the low-level vorticity in the inner-core area of the cyclone. On the other hand, the active ascent accompanying the convection tends to transport the low-level vorticity to the middle levels. The enhanced vorticity in the lower to middle troposphere strengths the interaction between the low- and mid-level cyclonical circulation and the upper-level circulation deviated from the storm center under the effect of VWS. As a result, the vertical tilting of the vortex is considerably decreased, and then the cyclone starts to develop rapidly.

CHEN Qi-zhi, FANG Juan. EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE [J]. Journal of Tropical Meteorology, 2012, 18(2): 172-186, https://doi.org/10.3969/j.issn.1006-8775.2012.02.007
Citation: CHEN Qi-zhi, FANG Juan. EFFECTS OF VERTICAL WIND SHEAR ON INTENSITY AND STRUCTURE OF TROPICAL CYCLONE [J]. Journal of Tropical Meteorology, 2012, 18(2): 172-186, https://doi.org/10.3969/j.issn.1006-8775.2012.02.007
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