(2005) (2005) 1 2 ( 1 ) 20km 2 4km 20km 40km 400km 10 1km 2km Ruscher and Deardroff (1982) Dempsey and Rotunno (1988) Smolarkiewcz et al. (1988) Smola

Similar documents
,, Mellor 1973),, Mellor and Yamada 1974) Mellor 1973), Mellor and Yamada 1974) 4 2 3, 2 4,

hPa ( ) hPa

mains.dvi


Study of the "Vortex of Naruto" through multilevel remote sensing. Abstract Hydrodynamic characteristics of the "Vortex of Naruto" were investigated b

No pp The Relationship between Southeast Asian Summer Monsoon and Upper Atmospheric Field over Eurasia Takeshi MORI and Shuji YAMAKAWA

7 OpenFOAM 6) OpenFOAM (Fujitsu PRIMERGY BX9, TFLOPS) Fluent 8) ( ) 9, 1) 11 13) OpenFOAM - realizable k-ε 1) Launder-Gibson 15) OpenFOAM 1.6 CFD ( )

D v D F v/d F v D F η v D (3.2) (a) F=0 (b) v=const. D F v Newtonian fluid σ ė σ = ηė (2.2) ė kl σ ij = D ijkl ė kl D ijkl (2.14) ė ij (3.3) µ η visco

1 flux flux Plumb (1985) flux F s Plumb (1985) Karoly et al. (1989) flux flux Plumb (1985) Plumb (1986) Trenberth (1986) Andrews (1983) review flux Pl

P00表紙.ai

20 $P_{S}=v_{0}\tau_{0}/r_{0}$ (3) $v_{0}$ $r_{0}$ $l(r)$ $l(r)=p_{s}r$ $[3 $ $1+P_{s}$ $P_{s}\ll 1$ $P_{s}\gg 1$ ( ) $P_{s}$ ( ) 2 (2) (2) $t=0$ $P(t

1

, 1.,,,.,., (Lin, 1955).,.,.,.,. f, 2,. main.tex 2011/08/13( )

Venkatram and Wyngaard, Lectures on Air Pollution Modeling, m km 6.2 Stull, An Introduction to Boundary Layer Meteorology,

* Meso- -scale Features of the Tokai Heavy Rainfall in September 2000 Shin-ichi SUZUKI Disaster Prevention Research Group, National R

<32322D8EA D89CD8D8797B294C E8A968388DF814589C193A1899B E5290EC8F438EA12D966B8A4393B98F5C8F9F926E95FB82CC8BC7926E F5

カルマン渦列の消滅と再生成のメカニズム

( ) a C n ( R n ) R a R C n. a C n (or R n ) a 0 2. α C( R ) a C n αa = α a 3. a, b C n a + b a + b ( ) p 8..2 (p ) a = [a a n ] T C n p n a

広報ひめじ2015年9月号

広報ひめじ2015年8月号

Web Two-phase Flow Analyses Using Interface Volume Tracking Tomoaki Kunugi Kyoto University 1) 2) 3)

????? 1???

SSI MUCAPE3km SReH 3kmMEANSHR VGP EHIMAX (a) (b) 1 ae (c)


HRBusinessReview_vol5

all

空間多次元 Navier-Stokes 方程式に対する無反射境界条件

A Higher Weissenberg Number Analysis of Die-swell Flow of Viscoelastic Fluids Using a Decoupled Finite Element Method Iwata, Shuichi * 1/Aragaki, Tsut


最新耐震構造解析 ( 第 3 版 ) サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 第 3 版 1 刷発行時のものです.

I z n+1 = zn 2 + c (c ) c pd L.V. K. 2

untitled

Fig. 3 Coordinate system and notation Fig. 1 The hydrodynamic force and wave measured system Fig. 2 Apparatus of model testing

CM1-GTX

プラズマ・核融合学会誌

NUMERICAL CALCULATION OF TURBULENT OPEN-CHANNEL FLOWS BY USING A MODIFIED /g-e TURBULENCE MODEL By Iehisa NEZU and Hiroji NAKAGA WA Numerical calculat

IHIMU Energy-Saving Principle of the IHIMU Semicircular Duct and Its Application to the Flow Field Around Full Scale Ships IHI GHG IHIMU CFD PIV IHI M

untitled

工学的な設計のための流れと熱の数値シミュレーション


三校永谷.indd


: u i = (2) x i Smagorinsky τ ij τ [3] ij u i u j u i u j = 2ν SGS S ij, (3) ν SGS = (C s ) 2 S (4) x i a u i ρ p P T u ν τ ij S c ν SGS S csgs

U Fig. : Physical state Navier-Stokes u t +(u grad)u = ρ gradp + ν u, () divu =. () u p ρ ν ω =(,,ω) b ω t +(u grad) ω = ν ω. (3) u Biot-Savart u = ω(

第62巻 第1号 平成24年4月/石こうを用いた木材ペレット

Title 渦度場の特異性 ( 流体力学におけるトポロジーの問題 ) Author(s) 福湯, 章夫 Citation 数理解析研究所講究録 (1992), 817: Issue Date URL R

Natural Convection Heat Transfer in a Horizontal Porous Enclosure with High Porosity Yasuaki SHIINA*4, Kota ISHIKAWA and Makoto HISHIDA Nuclear Applie

Print

¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤® - No.7, No.8, No.9

untitled

Undulator.dvi

untitled

Ax001_P001_目次-1.ai

1

pdf

untitled


untitled

untitled




2012専門分科会_new_4.pptx

1.3 (heat transfer with phase change) (phase change) (evaporation) (boiling) (condensation) (melting) (solidification) 1.4 (thermal radiation)

非線形長波モデルと流体粒子法による津波シミュレータの開発 I_ m ρ v p h g a b a 2h b r ab a b Fang W r ab h 5 Wendland 1995 q= r ab /h a d W r ab h

(Hiroshi Okamoto) (Jiro Mizushima) (Hiroshi Yamaguchi) 1,.,,,,.,,.,.,,,.. $-$,,. -i.,,..,, Fearn, Mullin&Cliffe (1990),,.,,.,, $E

RX501NC_LTE Mobile Router取説.indb

105†^Ÿ_Ł¶†^åM“è‡Ù‡©.pwd

Flow Around a Circular Cylinder with Tangential Blowing near a Plane Boundary (2nd Report, A Study on Unsteady Characteristics) Shimpei OKAYASU, Kotar

, 3, STUDY ON IMPORTANCE OF OPTIMIZED GRID STRUCTURE IN GENERAL COORDINATE SYSTEM 1 2 Hiroyasu YASUDA and Tsuyoshi HOSHINO

Fig. Division of unbounded domain into closed interior domain and its eterior domain. Zienkiewicz [5, 6] Burnett [7, 8] [3] The conjugated Ast


200708_LesHouches_02.ppt

a L = Ψ éiγ c pa qaa mc ù êë ( - )- úû Ψ 1 Ψ 4 γ a a 0, 1,, 3 {γ a, γ b } η ab æi O ö æo ö β, σ = ço I α = è - ø çèσ O ø γ 0 x iβ γ i x iβα i

阪神5年PDF.PDF

12 1



untitled

Microsoft Word - 01_表紙

第4回 小平市の文化振興を考える市民委員会

<4D F736F F D2089AB93EA8CA48F43838C837C815B83675F8FAC97D1>

2

渋谷区耐震改修促進計画

2

Microsoft Word - 第8回問題(3級)


1,000m 875m1 6km

Ⅰ.市区町村事例ヒアリング結果の詳細

一太郎 13/12/11/10/9/8 文書

Microsoft Word - NEWホノルル.docx

私にとっての沖縄と独自性.PDF

00.pdf

Microsoft Word - P01_導水路はいらない!愛知の会 会報11号-1 .docx




10 km!

H29-p06-07

, , km 9.8km 10.5km 11.9km 14.4km 14.4km 34.1km 3.4km 31.7km 6.2km 7.3k

Transcription:

(2005) (2005) 1 2 ( 1 ) 20km 2 4km 20km 40km 400km 10 1km 2km Ruscher and Deardroff (1982) Dempsey and Rotunno (1988) Smolarkiewcz et al. (1988) Smolarkiwicz and Rotunno (1989) F r = 0.15 0.5 ( F r = u/nh, N :, H : ) Kang et al. (1998) F r F r =0.48 F r =0.22 ( 1 ) Smolarkiwicz and Rotunno (1989) F r = 0.15 0.5 ( 1) ( 2 ) (2005) Kang et al. (1998)

1: 2000 2 21 ( ) ( URL http://weather.is.kochiu.ac.jp/) Kang et al.(1998) F r = 0.22 3.57 1km 2: (Kimura, 1988) (Etling,1989)

( 2 ) Kang et al. (1998) (2005) 2 ARPS ARPS m km Kang et al. (1998) 3 576km 195km 3km 3km 15km 50 z = 7.14km 170m 7.14km 10km (x, y) = (60, 97.5)km 3 x 10m/s 296.3K N = 14s 1 965hPa (open boundary) Orlanski (1976) Klemp and Durran (1983) 8000m Rayleigh damping ( 3) Altitude 2.3 0 0 U=10(m/s) Klemp-Durran Stratified lauer(n=14) Central Stratified layer(t=296.3k) Free Slip X-direction 600 Y-direction 200 0 0 600 X-direction 3: ( ( ) ( )

3 3.1 4 t = 154800s (43h) t = 241200s (67h) 08:30Z Sat 18 Dec 2004 t=4140 s (11:30:00) 08:30Z Sat 18 Dec 2004 t=4140 s (11:30:00) 08:30Z Sat 18 Dec 2004 t=4140 s (11:30:00) 100. 80. 40. 20. -20. -40. - -80. 20 30 40 50 Umin=-15.41 Umax=5.18 Vmin=-7.11 Vmax=9.14 20:00Z Sat 18 Dec 2004 t=8280 s (23:00:00) 20 30 40 50 20:00Z Sat 18 Dec 2004 t=8280 s (23:00:00) Min=-224. Max=158. 20:00Z Sat 18 Dec 2004 t=8280 s (23:00:00) -100. 100. 80. 40. 20. -20. -40. - -80. 20 30 40 50 Umin=-13.48 Umax=5.89 Vmin=-8.71 Vmax=9.23 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 20 30 40 50 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) Min=-318. Max=265. 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) -100. 100. 80. 40. 20. -20. -40. - -80. 20 30 40 50 20 30 40 50-100. Umin=-15.74 Umax=7.89 Vmin=-7.61 Vmax=8.14 t=24120 s (67:00:00) t=24120 s (67:00:00) Min=-341. Max=235. t=24120 s (67:00:00) 100. 80. 40. 20. -20. -40. - -80. 20 30 40 50 Umin=-14.04 Umax=6.22 Vmin=-15 Vmax=8.43 20 30 40 50-100. Min=-252. Max=285. ARPS/ZXPLOT myrun1, Version 4.5.2, Kang-Kimura Sounding ARPS/ZXPLOT myrun1, Version 4.5.2, Kang-Kimura Sounding 4: 1000m ( ) z ( ) 11h30m, 23h, 43h, 67h 3.2 t = 67h z 5 y xz 5 y = 97.5km y = 76.5km y =76.5km y 0.6km y =97.5km 1.5km λ x λ x 35km λ z λ z 1km y = 76.5km λ x 70km λ z 2 3km

-0.8 t=24120 s (67:00:00) t=24120 s (67:00:00) 0.8 0.64 t=24120 s (67:00:00) X-Z plane at y=97.5 km 0.48 0.32 0.16-1.19E-07-0.16-0.32-0.48-0.64 w (m/s, shaded) 20 30 40 50 Min=-.873 Max=0 t=24120 s (67:00:00) t=24120 s (67:00:00) - - 297.9 297.8-297.6 297.4-29 297. 296.8 296.6 9 48 57-296.4 296.2 Min=-662. Max=879. pt (K, shaded) 20 30 40 50 Min=296. Max=298. t=24120 s (67:00:00) t=24120 s (67:00:00) 296. 300. t=24120 s (67:00:00) 240. 180. 120. X-Z plane at y=76.5 km - -120. -180. -240. 20 30 40 50 Min=-252. Max=285. t=24120 s (67:00:00) -300. - - - - 9 48 57-20 30 40 50 Umin=-14.04 Umax=6.22 Vmin=-15 Vmax=8.43 Min=-688. Max=564. ARPS/ZXPLOT myrun1, Version 4.5.2, Kang-Kimura Sounding ARPS/ZXPLOT 5: 1000m (m/s) (K) z ( 10 5 1/s) (m/s) y xz y = 97.5km( ) y = 76.5km( ) 3.2.1 z =2300m 6 07:00Z Sun 19 Dec 2004 t=12240 s (34:00:00) 306 302 320 324 316 316 312 312 310 310 300 314 308 308 298 X-Z plane at y=97.5 km 322 326 318 304 302 320 306 324 300 314 298 322 318 304 9 48 57 pt (K, contour) Min=296. Max=334. Inc=1.00 6: y = 97.5km( ) xz c = U ± N kx 2 + k z 2 (3.1)

z c gz Nk x k z = (k 2 x + k 2. (3.2) z ) 3/2 c 7m/s U 10m/s U 6 m/s c U > 0 (3.1) (3.2) c gz > 0 (3.2) k x k z k z k x N c U = ± 2 kx + k, (3.3) 2 z N k z (3.4) c U 1(m/s) (3.5) N 1.4 10 2 (s 1 ) k z = N c U 1.4 10 2 1 1.4 10 2 (1/m) () λ z = 2π k z 0.5 10 3 (m) (3.7) c U 3(m/s) k z = N c U 1.4 10 2 3 0.4 10 2 (1/m) (3.8) λ z = 2π k z 1.5 10 3 (m) (3.9) λ z 1km λ z 2 3km N N 1.4 10 2 (s 1 ) N 3.2.2 z ( 7 ) y y xz ( 7 ). x = 250km ( 7 ) y = 76.5km y y = 97.5km z = 1.5km y x = 300km ( 7 ) y = 106.5km y 8 xz

t=24120 s (67:00:00) X-Z plane at y=79.5 km t=24120 s (67:00:00) X-Z plane at y=85.5 km - - - - - - - - 9 48 57-9 Min=-626. Vort*10^5 Max=602. (1/s, shaded) t=24120 s (67:00:00) 57 Min=-501. Max=843. t=24120 s (67:00:00) X-Z plane at y=97.5 km 48 X-Z plane at y=91.5 km - - - - - - - - - 9 48 57-9 Min=-575. Vort*10^5 Max=817. (1/s, shaded) t=24120 s (67:00:00) 57 Min=-662. Max=879. t=24120 s (67:00:00) X-Z plane at y=109.5 km 48 X-Z plane at y=103.5 km - - - - - - - - 9 48 57 - Min=-601. Max=0.101E+04 - - 9 48 57 Min=-533. Max=848. ARPS/ZXPLOT 図 7: 互い違いの渦列時の渦度 z 成分 ( 105 1/s) 左図は xy 断面図で 高度は上から 1000m 1500m 2000m 2500m 右図は xz 断面図で 上左は y = 79.5km 上右は y = 85.5km 中左は y = 91.5km 中右は y = 97.5km 下左は y = 103.5km 下右は y = 109.5km 図 8: 互い違いになったカルマン渦列の渦のつながり概念図

0.8 0.64 0.48 0.32 0.16-1.19E-07-0.16-0.32-0.48-0.64-0.8 297.9 297.8 297.6 297.4 29 297. 296.8 296.6 296.4 296.2 296. 300. 240. 180. 120. - -120. -180. -240. -300. 3.3 3.3.1 t = 43h z 9 y = 76.5km y xz ( 9 ) (y = 97.5km) z = 1.5km λ x 50km λ z 1km y = 76.5km λ x 50km λ z 2 3 km 3.3.2 c 6.5m/s U 6m/s U 10m/s c U 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) X-Z plane at y=97.5 km w (m/s, shaded) 20 30 40 50 Min=-.794 Max=0.875 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) - - - - 9 48 57 - Min=-551. Max=544. pt (K, shaded) 20 30 40 50 Min=296. Max=297. 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) X-Z plane at y=76.5 km 20 30 40 50 Min=-341. Max=235. 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) - - - - 9 48 57-20 30 40 50 Umin=-15.74 Umax=7.89 Vmin=-7.61 Vmax=8.14 Min=-493. Max=515. ARPS/ZXPLOT myrun1, Version 4.5.2, Kang-Kimura Sounding ARPS/ZXPLOT 9: 1000m ( ) (m/s) (K) z ( 10 5 1/s) (m/s) 1000m y ( ) 3.3.3 z ( 10 ) y y xz ( 10 ) x = 260km ( ( 10 )) 10 x = 260km 11 λ x

- - - - - - - - - - - - - - - 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) X-Z plane at y=79.5 km 9 48 57 X-Z plane at y=85.5 km Min=-522. Max=630. 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) 9 48 57 Min=-572. Max=785. 16:00Z Sun 19 Dec 2004 t=15480 s (43:00:00) X-Z plane at y=91.5 km 9 48 57 Min=-593. Max=706. ARPS/ZXPLOT 10: z ( 10 5 1/s) 1000m 1500m 2000m 2500m xz y = 79.5km y = 85.5km y = 91.5km z z y y x 11:

4 (2005) 1. Dempsey, D P. and Rotunno, R., 1988: Topographic generation of mesoscale vortices in mixed-layer models. J. Atmos. Sci., 45, 2961-2978. 2. Etling, D., 1989: On Atmospheric Vortex Streets in the Wake of Large Islands. Meteorol. Atmos. Phys., 41, 157-164 3., 2004:., 2004, 85, 115 4., 2005:., 2005, 88, 284 5. Kang, S. D., F. Kimura and S.Takahashi., 1998: A Numerical Study On the Karman Vortex Generated by Divergence of Momentum Flux in Flow Past an Isolated Mountain. J. Meteor. Soc. Japan, 76, 925-935 6. Kimura, R., 1988: The process of generation of Karman Vortex streets in the lee side of Cheju island. J. Jap. Soc. Fluid Mech., 7, 1-2 7. Klemp, J. B., and D. R. Durran, 1983: An upper boundary condition permitting internal gravity wave radiation in numerical mesoscale models. Mon. Wea. Rev., 111, 430-444 8. Orlanski, I., 1976: A simple boundary condition for unbounded hyperbolic flows. J. Comput. Phy., 21, 251-269 9. Ruscher, P. H. and Deardorff. J. W., 1982: A numerical simulation of atmospheric vortex streets., Tellus, 34, 555-566 10. Smolarkiewicz, P. K., Rassmussen and R. M., Clark, T. L., 1988: On the dynamics of Hawaiian cloud bands: island forcing. J. Atoms. Sci., 45, 1872-1905 11. Smolarkiewicz, P. K. and R. Rotunno, 1989: Low Froude Number Flow past Three-Dimensional Obstacles. Part1: Baroclinically Generated Lee Vortices. J. Atmos. Sci., 46, 1154-1165