Yang, M.-J., T.-C. Chen Wang, Y. Zhang, and C.-Y. Weng, 2011:

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Presentation transcript:

Momentum budget evolution of Typhoon Nari (2001) during the landfall process Yang, M.-J., T.-C. Chen Wang, Y. Zhang, and C.-Y. Weng, 2011: Momentum budget evolution of Typhoon Nari (2001) during the landfall process. Terr., Atmos., and Oceanic Sci., 22, 595–612, doi: 10.3319/TAO.2011.05.31.01(TM)

Outline Keywords Introduction Methodology Axisymmetric AAM and Radial momentum Budgets over ocean Asymmetric AAM and Radial momentum Budgets over land Conclusions

Keywords Supergradient wind Momentum budget

Supergradient wind L GWB model(Gradient-wind balance) V>Vg Vg centrifugal force Coriolis force Pressure gradient force http://ww2010.atmos.uiuc.edu/(Gh)/guides/mtr/fw/grad.rxml Gradient Wind: A steady horizontal air motion along curved parallel isobars or contours in an unchanging pressure or contour field, assuming there is no friction and no divergence or convergence. A wind of greater speed than the gradient wind required by the existing pressure gradient and centrifugal force. ( http://encyclopedia2.thefreedictionary.com/supergradient+wind ) ( http://www.superglossary.com/Definition/Weather/Gradient_Wind.html ) Gradient Wind. A wind induced in a certain direction by flow of air balancing the pressure gradient caused by the earth's rotation and centrifugal force ( http://en.mimi.hu/aviation/gradient_wind.html ) (其他在 “file:meeting paper reference” 裡面) V>Vg

Momentum budget Momentum = m * V angular momentum = r * m * V Absolute angular momentum (AAM,M) Caused by earth rotation 在絕對座標內 角動量,就如動量一般,是一個可用來表徵物體運動特徵的物理量。 Relate to earth Equations will be discussed later. The law of conservation of angular momentum states that when no external torque acts on an object or a closed system of objects, no change of angular momentum can occur.

Introduction GWB assumption for the tangential wind has been widely used in theoretical studies for TCs.(Shapiro and Willoughby 1982; Emanuel 1986) GWB model is a good approximation to the azimuthally-averaged tangential winds in the inner-core region for flows above the MBL and below the upper outflow layer.(La Seur and Hawkins 1963; Willoughby 1990, 1991) Systematic GW unbalance flows in the eyewall, especially near the radius of maximum wind(RMW).(Gray and Shea 1973) Utilizing AAM and radial momentum budget, Zhang indicated that both conclusions are correct for the levels of observations they analyzed.(Zhang et al. 2001) These studies are only for marine TCs , and it remains unknown whether the GWB model is still applicable when a TC makes landfall, such as CMR in Taiwan.

Case : Typhoon Nari(2001) - Struck Taiwan on UTC 16 Sep. - More than 1400mm/3days 92 death tolls. (Sui et al. 2002) 9/16: marine to land. Picture originated from CWB

Objectives of the study Investigate the evolution of tangential and radial flows of Nari during its landfall in Taiwan.(From more axisymmetric structure over ocean to asymmetric features over mountains. ) Understand the extent that GWB is still valid for a TC made landfall. Gain insight and examine the physical mechanism responsible of the sloping midlevel radial flow over terrain.

Methodology PSU-NCAR MM5 model ver.3.5 PSU-NCAR MM5 model ver.3.5 Horizontal :54 ,18, 6, 2km (quadruply nested-grid ) Vertical:32 σ levels (top= 50 hPa ) Time period : 1200 UTC 16 Sep. ~ 0000 UTC 19 Sep. (84 h) SST is constant I.C. and B.C. : ECMWF/TOGA (1.125°*1.125° horizontal resolution) TC initialization : Davis and Low-Nam (2001) Parameterization : cumulus (Grell 1993)(54, 18 km) microphysics( Reisner et al. 1998) with graupel included PBL (MRF model)(Hong and Pan 1996) atmospheric radiation(Dudhia1989) Output interval : 2-min and 2-km governing eq. based on PSU-NCAR MM5 model (Dudhia 1993; Grell et al. 1995) This study is high temporal and spatial resolution.

Methodology Governing equation for radial and tangential wind Radial Pressure Gradient Force(PGFR; Up) Centrifugal Force(UE) Coriolis Force(Uc) Including The Effect of Vertical Motion PBL Effects And Turbulent Mixing(UTB) (Residues) PBL Effects And Turbulence Mixing(VTB) Coriolis Force(Vc) including the effect of vertical motion Centrifugal Force(VE) Tangential Pressure Gradient Force(PGFR; Vp) Local tendency Horizontal advection Vertical advection λ – azimuthal angle. r – radius from TC center, pointing outward. z – vertical height. U – radial wind in cylindrical coordinate. V – tangential wind in cylindrical coordinate. W – vertical wind in cylindrical coordinate. Ω – angular velocity on the earth. Ф – latitude. U’ – storm relative radial wind. V’ – storm relative tangential wind.

Lagrangian derivative of AAM equation Caused by earth rotation β – df/dФ Vm – projections of U and V onto longitudinal axes. Relate to earth’s rotation Pressure Torque Beta Torque Longitudinally-Oriented Coriolis Torque By The Vertical Motion Torque Due To The PBL Effects And Turbulent Mixing

NW SW SW For the different terrain imposed on the simulated storm due to the landfall position error. SW Time lag

Axisymmetric AAM and Radial momentum Budgets over ocean

A1 B1 Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) B1 A1 NE: stronger and more upright. SW: low level inflow stronger and deeper. Solid: positive (upward, outflow) Dashed: negative (downward, inflow) Less degree of asymmetry. B1 A1 小時時間平均,A1B1剖面。 TC still at its developing stage. And some degree of asymmetry induced by storm’s internal dynamical process can be seen. A1 B1

Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) inflow outflow UP RMW DN eye wall :12km wall UP Radial advection MBL friction 方位角、小時時間平均 kinetic and AAM field of Nari. (c) Friction cause vertical (tangential??) wind shear? How? Where? MBL top: V’ max=57 m/s

UP Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) Solid: positive Solid: positive (source) Dashed: negative (sink) Solid: positive (upward, inflow) Dashed: negative (downward, outflow) AAM Slightly conserved UP Inward AAM Outward AAM Upward AAM Indicate a slow spindown of tangential wind inside the eye. 方位角、小時時間平均 AMM budget. 水平、垂直異號。 AAM Sink

Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) Same as gradient-wind imbalance Outward Inward UP Up max Same structure as Up , opposite sign. Cyclostrophic imbalance = Up+UE Gradient –wind imbalance = Up+UE +Uc SuperCyclostrophic UE>Up Supergradient-wind SubCyclostrophic UE<Up Subgradient-wind 方位角 、 小時時間平均 Radial momentum budget terms and the extent of different balanced-wind approximation since its on the sea. Proof Zhang? Solid: positive (outward) Dashed: negative (inward) Solid: positive Dashed: negative

Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) Solid: positive (outward) Dashed: negative (inward) Strengthen upper level outflow Low level from eye to wall : further reduce the central pressure In the wall : increase radial inflow Out of wall : decrease inflow Upper level: outflow Below the up axis : slightly decrease radial outflow; Above then increase. 方向角、小時時間平均。 Tendency << Lagrangian  Suggested that the oceanic Nari ‘s radial flow evolved very slowly during its intensifying stage. Solid: positive (outward, upward ) Dashed: negative (inward, downward )

Oceanic Nari:0100-0200 UTC 16 Sep. 2001 (t=13-14h) Supercyclostrophic wind = 6 m/s Subcyclostrophic wind Supergradient wind > 6 m/s Subgradient wind 方向角、小時時間平均。 非氣旋流、非梯度風。 Acyclostrophic wind = V-Vc Agradient wind = V -Vg

Asymmetric AAM and Radial momentum Budgets over land

Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) B Snow Mountain Range 30km 60km Z=3 km Contour – V’ Shaded – midlevel (σ =0.4~0.8) radar reflectivity (t=22.5 h) Vector – horizontal wind (t=22.5h)

Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) Buckling height AB剖面 小時平均 Buckling height reduce the vertical gradient above the lower level , which occurs at a higher altitude in the outer region(r>40) over land than over the ocean. Indicating the rapid spindown of V due to the enhanced sfc.

( ) * M Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) Land: mostly negative. Ocean: very small. AB剖面,小時時間平均。

Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) Negative: inward. Peak value decreased: -500 m/s*h (ocean)  -450 m/s*h (land) > 800 m/s > 500 m/s Supergradient wind (UE>UP) (stronger at off shore ) AB剖面。 UPEC(GW unbalance) is similar to UPE(cyclostrophic unbalance). UTB –(< 0) by turbulence mixing in the eye (< 30 km) dU/dt – low level slightlr outward (> 0 ); up level outward flow is decreased by UTB. Solid: positive (outward) Dashed: negative (inward)

Supergradient wind Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) AB剖面。 Supergradient wind

Contour – dU/dt , V-Vg solid(positive) dashed(negative) Shaded – U’ Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) Over ocean: R < 40 km in eye dU/dt >0 reduce the inward. Over land: Accompanied by the vertical transport (outward). Contour – dU/dt , V-Vg solid(positive) dashed(negative) Shaded – U’ 10 m/s 15 m/s 5 m/s Over ocean: In the eye Strong supergradient wind Upper outflow level Weak supergradient wind Over land: Sub- and super- oscillation AB剖面。

Landfall Nari:1000-1100 UTC 16 Sep Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h), R=35km (large GW imbalance near eye.) Supercyclostrphic wind (Since in th eye) Supergradient wind R=35 km UPEC is similar to UPE (since C acceleration is small.) UTB works over the land than over the ocean (north). Similar to GW imbalance, but with fluctuation (turbulent mixing).

Landfall Nari:1000-1100 UTC 16 Sep Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h), R=60 km (outer principal rainband.) Only over the terrain and the rainband (NW) : UE overcompensates UP (supergradient wind) R=60 km UTB works beneath PBL and over the terrain  retard radial inflow. Similar to GW imbalance, but with fluctuation (turbulent mixing).

Contour – agradient wind solid(positive), dashed(negative) Shaded – U’ Landfall Nari:1000-1100 UTC 16 Sep. 2001 (t=22-23h) Contour – agradient wind solid(positive), dashed(negative) Shaded – U’ -24 m/s 21 m/s 9 m/s R=35 km N Semicircle/ near the wall and mid-low level: Strong supergradient winds (by terrain). SE quadrant- (lee side of Snow Mountain Range): Subgradient winds at low level and lee Side. R=60 km North Semicircle: Strong supergradient winds near the wall and low level. Southeastern quadrant (lee side of Snow Mountain Range): Strong subgradient winds lee Side. 6 m/s -24 m/s

Conclusions

Tangential wind Budget Oceanic Nari Landfall Nari AAM Budget Conserved: outside the eye, above MBL. Sink: Eye, MBL. Tangential wind Budget Radial wind Budget Supergradient wind (UE(V)>UP): the bottom of the eye to the upper outflow layer inside the eyewall.(Gray and Shea 1973) Subgradient wind (UE(V)<UP): Below the MBL outside the wall. Low level inflow stronger and thicker. Outflow maximum over the terrain. 35 km over the terrain. Leeside the terrain. 60 km The same. GWB’s validation Below the outflow region and over MBL. (La Seur and Hawkins 1963; Willoughby 1990, 1991) Invalid. Leads to more quickly-evolved vortex flows and 2nd circulations above terrain.

Reference CWB 氣象名詞查詢表 http://photino.cwb.gov.tw/rdcweb/lib/h/g_000853.htm http://www.phy.ncu.edu.tw/notes/angular/purpose.htm wikipedia :http://en.wikipedia.org/wiki/Angular_momentum http://encyclopedia2.thefreedictionary.com/supergradient+wind http://www.superglossary.com/Definition/Weather/Gradient_Wind.html http://en.mimi.hu/aviation/gradient_wind.html

THANKS FOR YOUR ATTENTION.

Cyclostrophic Flow centrifugal force Pressure gradient force L Vc

Domain D1 D2 D3 D4 Dimensions (x,y) 81*71 100*100 166*166 271*301 Grid size (km) 54 18 6 2 Area coverage(Km^2) 4320*3780 1782*1782 990*990 540*660 Time step(s) 90 30 10 3.3 Integration hours 0-84