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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 大氣科學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/18318
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor吳健銘
dc.contributor.authorJia-Ying Tsaien
dc.contributor.author蔡佳穎zh_TW
dc.date.accessioned2021-06-08T00:59:32Z-
dc.date.copyright2015-03-13
dc.date.issued2015
dc.date.submitted2015-01-19
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Bretherton, C. S., and M. C. Wyant, 1997: Moisture transport, lower-tropospheric stability, and decoupling of cloud-topped boundary layers. J. Atmos. Sci., 54(1), 148-167. doi:http://dx.doi.org/10.1175/1520-0469(1997)054<0148:MTLTSA>2.0.CO;2
Chung, D., G. Matheou, and J. Teixeira, 2012: Steady-state large-eddy simulations to study the stratocumulus to shallow cumulus cloud transition. J. Atmos. Sci.,
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Jones, C. R., C. S. Bretherton, and P. N. Blossey, 2014: Fast stratocumulus time scale in mixed layer model and large eddy simulation. J. Adv. Model. Earth Syst., 6(1), 206-222. doi:10.1002/2013MS000289
Jones, C. R., C. S. Bretherton, and D. Leon, 2011: Coupled vs. decoupled boundary layers in VOCALS-REx. Atmos. Chem. Phys., 11, 7143-7153. doi:10.5194/acp-11-7143-2011
Jung, J. H., and A. Arakawa, 2008: A three-dimensional anelastic model based on the vorticity equation. Mon. Wea. Rev., 136(1), 276-294. doi:http://dx.doi.org/10.1175/2007MWR2095.1
Krueger, S. K., Q. Fu, K. N. Liou, and H.-N. Chin, 1995: Improvements of an ice-phase microphysics parameterization for use in numerical simulations of tropical convection. J. Appl. Meteor., 34(1), 281-287. doi:http://dx.doi.org/10.1175/1520-0450-34.1.281
Krueger, S. K., G. T. McLean, and Q. Fu, 1995a: Numerical simulation of the stratus-to-cumulus transition in the subtropical marine boundary layer. Part I: Boundary-layer structure. J. Atmos. Sci., 52(16), 2839-2850.
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Park, S., C. B. Leovy, and M. A. Rozendaal, 2004: A new heuristic Lagrangian marine boundary layer cloud model. J. Atmos. Sci., 61(24), 3002-3024. doi:http://dx.doi.org/10.1175/JAS-3344.1
Randall, D. A., 1980: Conditional instability of the rst kind upside-down. J. Atmos. Sci., 37(1), 125-130. doi:http://dx.doi.org/10.1175/1520-0469(1980)037<0125:CIOTFK>2.0.CO;2
Sandu, I., and B. Stevens, 2011: On the factors modulating the stratocumulus to cumulus transitions. J. Atmos. Sci., 68(9), 1865-1881. doi:http://dx.doi.org/10.1175/2011JAS3614.1
Savic-Jovcic, V., and B. Stevens, 2008: The structure and mesoscale organization of precipitating stratocumulus. J. Atmos. Sci., 65(5), 1587-1605. doi:http://dx.doi.org/10.1175/2007JAS2456.1
Schubert, W. H., J. S. Wake eld, E. J. Steiner, and S. K. Cox, 1979a: Marine stratocumulus convection. Part I: Governing equations and horizontally homogeneous
solutions. J. Atmos. Sci., 36(7), 1286-1307. doi:http://dx.doi.org/10.1175/1520-0469(1979)036<1286:MSCPIG>2.0.CO;2
Schubert, W. H., J. S. Wake eld, E. J. Steiner, and S. K. Cox, 1979b: Marine stratocumulus convection. Part II: Horizontally inhomogeneous solutions. J. Atmos. Sci., 36(7), 1308-1324. doi:http://dx.doi.org/10.1175/1520-0469(1979)036<1308:MSCPIH>2.0.CO;2
Stevens, B., and Coauthors, 2003: Dynamics and chemistry of marine stratocumulus-DYCOMS-II. Bull. Amer. Meteor. Soc., 84(5), 579-593. doi:http://dx.doi.org/10.1175/BAMS-84-5-579
Stevens, B., and Coauthors, 2005: Evaluation of large-eddy simulations via observations of nocturnal marine stratocumulus. Mon. Wea. Rev., 133(6), 1443-1462. doi:http://dx.doi.org/10.1175/MWR2930.1
Wood, R., 2012: Stratocumulus clouds. Mon. Wea. Rev., 140(8), 2373-2423. doi:http://dx.doi.org/10.1175/MWR-D-11-00121.1
Wood, R., and C. S. Bretherton, 2004: Boundary layer depth, entrainment, and decoupling in the cloud-capped subtropical and tropical marine boundary layer. J. Climate, 17(18), 3576-3588. doi:10.1175/1520-0442(2004)017<3576:BLDEAD>2.0.CO;2
Wood, R., and C. S. Bretherton, 2006: On the relationship between stratiform low cloud cover and lower-tropospheric stability. J. Climate, 19(24), 6425-6432. doi:10.1175/JCLI3988.1
Wu, C.-M., and A. Arakawa, 2011: Inclusion of the surface topography into the vector vorticity equation model (VVM). J. Adv. Model. Earth Syst., 3(2), M04002. doi:10.1029/2011MS000061
Wyant, M. C., C. S. Bretherton, H. A. Rand, and D. E. Stevens, 1997: Numerical simulations and a conceptual model of the stratocumulus to trade cumulus transition. J. Atmos. Sci., 54(1), 168-192. doi:10.1175/1520-0469(1997)054<0168:NSAACM>2.0.CO;2
Xiao, H., C.-M. Wu, and C. R. Mechoso, 2011: Buoyancy reversal, decoupling and the transition from stratocumulus-topped to trade-wind cumulus-topped marine
boundary layer. Climate Dyn., 37, 971-984. doi:10.1007/s00382-010-0882-3
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doi:http://dx.doi.org/10.1175/2009JCLI2891.1
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/18318-
dc.description.abstract本研究目的展示層積雲系統的雙穩態(bi-stable)行為以及海溫和大尺度沉降對層積雲雲量的遲滯(hysteresis)效應。透過以渦度方程為基礎的三維雲解析模式VVM (Vector Vorticity equation Model),理想化模擬建立在南加州外海海洋層積雲典型的環境條件。長時間模擬呈現一數學架構,在暖海溫和弱大尺度沉降環境條件下,不同自由大氣濕度初始條件的層積雲動力系統演化趨向兩吸引子(attractors):一是深厚層積雲,另一是淺積雲。分岐點被辨識在1至2天的中間熱力調整時間尺度。層積雲的演變因此被區分成在6至24小時快速逸入時間尺度上關係逸入與LWP負反饋的快動力以及在2天後多天緩慢逆溫層調整時間尺度上關係常數逸入率的慢動力。層積雲系統的破裂就發生在當上部邊界層開始變得乾,也就是,中間熱力調整時間尺度與緩慢逆溫層調整時間尺度的交界。另外,短時間模擬顯示大尺度沉降作用為立即性抑制逆溫層高度抗衡海溫,在乾自由大氣下立即性控制逆溫層上下濕度差異絕對值與LWP正反饋。海溫的作用是緩慢的,卻扮演協助乾自由大氣情境、控制濕自由大氣情境至關重要的角色。這份工作提出系統性且按照自然法則合理的框架,有助於層積雲轉換成淺積雲的現有知識。zh_TW
dc.description.abstractIn this study, we attempt to demonstrate the bi-stable behaviour of stratocumulus systems and the hysteresis effect forced by SST and large-scale subsidence on marine stratocumulus cloud amount. To address this aim, the idealized simulations are carried out with a 3D vector vorticity equation based cloud resolving model (VVM). The typical stratocumulus conditions over Southern California coast are considered as initial conditions and large-scale forcings. Simulations of long-term (8 days) responses to the warmer sea surface temperature and the weaker large-scale subsidence are conducted in order to clearly recognize the evolution of stratocumulus and to detect an occurrence of the stratocumulus to shallow cumulus cloud transition. Two experiments with different initial free atmospheric humidity under the fixed large-scale forcings are used to represent a mathematical framework for the stratocumulus dynamical systems. By analyzing characteristic time scales and instability, the results of this research support the idea that the initial free atmospheric humidity yields two attractors. During a critical transition when a bifurcation occurs, a decoupled and thick stratocumulus cloud boundary layer is evolved into either a deep and thick stratocumulus cloud boundary layer or a shallow and scattered cumulus cloud boundary layer. A critical transition is recognized on the intermediate thermodynamic adjustment time scale of 1 to 2 days. The evolution of stratocumulus is thus distinguished into fast dynamics concerning the entrainment-LWP negative feedback on the fast entrainment time scale of 6 to 24 hours and slow dynamics regarding constant entrainment rate on the slow inversion adjustment time scale of multiple days starting after the 2nd day. A breakdown of stratocumulus systems occurs just when the upper boundary layer becomes dry, that is, the border between the intermediate thermodynamic adjustment time scale and the slow inversion adjustment time scale. Simulations of short-term (6 hours) responses to the various perturbed large-scale environments lead to a better understanding of the sensitivities of strarocumulus properties to large-scale controlling variables such as SST, subsidence, and free tropospheric humidity. The large-scale subsidence functions as an immediate restraint on the inversion height against SST and on the positive feedback between absolute value of moisture jumps across the inversion and LWP against the dry upper troposphere. The effect of SST is tardy, but plays a crucial role to assist dry upper tropospheric scenarios and to control wet ones. This work contributes to existing knowledge about the stratocumulus to shallow cumulus cloud transition by proposing a systematic and physically reasonable framework.en
dc.description.provenanceMade available in DSpace on 2021-06-08T00:59:32Z (GMT). No. of bitstreams: 1
ntu-104-R00229023-1.pdf: 3845166 bytes, checksum: b18e477b0d0aa1ec5a18c856523fc72b (MD5)
Previous issue date: 2015
en
dc.description.tableofcontentsDEDICATION : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : iii
PREFACE : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : v
ACKNOWLEDGEMENTS : : : : : : : : : : : : : : : : : : : : : : : : : : vi
ABSTRACT in CHINESE : : : : : : : : : : : : : : : : : : : : : : : : : : : vii
ABSTRACT : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : ix
LIST OF ABBREVIATIONS : : : : : : : : : : : : : : : : : : : : : : : : : xi
LIST OF FIGURES : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : xv
CHAPTER
I. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.1 The Stratocumulus to Cumulus Tansition . . . . . . . . . . . 1
1.1.1 The Stratocumulus-Topped Marine Boundary Layer 1
1.1.2 Characteristics and Factors in the Transition . . . . 2
1.2 Hysteresis Phenomena and Multiple Equilibria . . . . . . . . 8
1.3 Characteristic Time Scales . . . . . . . . . . . . . . . . . . . 10
1.4 Research Purpose and Framework . . . . . . . . . . . . . . . 13
II. Model Settings . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.1 Model Description . . . . . . . . . . . . . . . . . . . . . . . . 15
2.2 DYCOMSII-RF01 . . . . . . . . . . . . . . . . . . . . . . . . 16
2.3 Simulations . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17
2.3.1 8-Day Simulations . . . . . . . . . . . . . . . . . . . 18
2.3.2 6-Hour Simulations . . . . . . . . . . . . . . . . . . 19
III. Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21
3.1 A Critical Transition for Slow-Fast Dynamics . . . . . . . . . 21
3.1.1 A Critical Transition in Simulations MHW and DHW 21
3.1.2 Fast Dynamics . . . . . . . . . . . . . . . . . . . . . 28
3.1.3 Slow Dynamics . . . . . . . . . . . . . . . . . . . . 30
3.2 A Critical Transition for Equilibria . . . . . . . . . . . . . . . 31
3.3 Fast Response to Large-Scale Forcings . . . . . . . . . . . . . 32
IV. Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35
4.1 A Conceptual Framework . . . . . . . . . . . . . . . . . . . . 35
4.2 Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.3 Simulations . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
V. Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41
BIBLIOGRAPHY : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 45
FIGURES AND TABLES : : : : : : : : : : : : : : : : : : : : : : : : : : : 51
dc.language.isoen
dc.title層積雲動力系統之分歧現象zh_TW
dc.titleCritical Transitions of Stratocumulus Dynamical Systemsen
dc.typeThesis
dc.date.schoolyear103-1
dc.description.degree碩士
dc.contributor.oralexamcommittee羅敏輝,林和,郭鴻基
dc.subject.keyword層積雲,快慢動力系統,時間尺度,雙穩態,分岐,遲滯,zh_TW
dc.subject.keywordcumulus under stratocumulus,slow-fast dynamical systems,time scales,bi-stable,bifurcation,hysteresis,en
dc.relation.page67
dc.rights.note未授權
dc.date.accepted2015-01-20
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept大氣科學研究所zh_TW
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