Synoptic analysis of the Pacific–North American teleconnection pattern

In this study, we use various diagnostic techniques to investigate the synoptic evolution of the Pacific–North American teleconnection pattern (PNA). National Center for Environment Prediction/National Center for Atmospheric Research reanalysis data are used. These data cover the years 1948–2008 for the months of November–March. It is found that the positive PNA is initiated by enhanced convection over the western tropical Pacific and weakened convection over the tropical Indian Ocean. The excitation of the negative PNA exhibits opposite features. For both phases, the response to tropical convection excites a small-amplitude PNA about 8–12 days prior to the pattern attaining its maximum amplitude. This is followed by slow, steady growth for about 5 days, after which driving by synoptic scale waves, via their eddy vorticity flux, together with stationary eddy advection lead to much more rapid growth and the establishment of the full PNA. For the positive PNA, the synoptic scale waves propagate eastward into the midlatitude northeastern Pacific, where they are observed to undergo cyclonic wave breaking. For the negative PNA, the synoptic scale waves first amplify over the midlatitude northeastern Pacific and then propagate equatorward into the Subtropics where they undergo anticyclonic wave breaking. Once established, for both phases, the PNA appears to be maintained through a positive feedback that involves a succession of wave breakings. These results suggest that preconditioning may play an important role in the formation of the PNA. For the positive PNA, in its early development, the strengthening and eastward extension of the subtropical jet result in an increase in the cyclonic shear and a decrease in the meridional potential vorticity gradient, features that are known to favour cyclonic wave breaking. For the negative PNA, opposite changes were observed for the background flow, which favour equatorward wave propagation and anticyclonic wave breaking. The role of optimal growth is also discussed. Our results also suggest that the PNA is potentially predictable 1–2 weeks in advance. Copyright © 2011 Royal Meteorological Society

[1]  G. Branstator Analysis of General Circulation Model Sea-Surface Temperature Anomaly Simulations Using a Linear Model. Part II: Eigenanalysis , 1985 .

[2]  S. Feldstein The dynamics of NAO teleconnection pattern growth and decay , 2003 .

[3]  Sukyoung Lee,et al.  Synoptic View of the North Atlantic Oscillation , 2004 .

[4]  Michiko Masutani,et al.  The global response to tropical heating in the Madden–Julian oscillation during the northern winter , 2004 .

[5]  Grant Branstator,et al.  Low-Frequency Patterns Induced by Stationary Waves , 1990 .

[6]  A. Simmons The forcing of stationary wave motion by tropical diabatic heating , 1982 .

[7]  N. Bond,et al.  The influence of the 1997–99 El Niňo Southern Oscillation on extratropical baroclinic life cycles over the eastern North Pacific , 2001 .

[8]  S. Schubert,et al.  Simulated Life Cycles of Persistent Anticyclonic Anomalies over the North Pacific: Role of Synoptic-Scale Eddies. , 1994 .

[9]  B. Hoskins,et al.  The Generation of Global Rotational Flow by Steady Idealized Tropical Divergence , 1988 .

[10]  P. R. Julian,et al.  Detection of a 40–50 Day Oscillation in the Zonal Wind in the Tropical Pacific , 1971 .

[11]  J. Frederiksen A Unified Three-Dimensional Instability Theory of the Onset of Blocking and Cyclogenesis. II. Teleconnection Patterns , 1983 .

[12]  J. Wallace,et al.  Barotropic Wave Propagation and Instability, and Atmospheric Teleconnection Patterns. , 1983 .

[13]  Grant Branstator,et al.  The Maintenance of Low-Frequency Atmospheric Anomalies , 1992 .

[14]  A. Lupo,et al.  Dynamics of Eddy-Driven Low-Frequency Dipole Modes. Part II: Free Mode Characteristics of NAO and Diagnostic Study , 2007 .

[15]  Sukyoung Lee,et al.  Observed Nonmodal Growth of the Pacific–North American Teleconnection Pattern , 2001 .

[16]  R. K. Scott,et al.  Wave Breaking and Mixing at the Subtropical Tropopause , 2002 .

[17]  I. Held,et al.  Linear and nonlinear barotropic decay on the sphere , 1987 .

[18]  I. Held,et al.  Barotropic Decay of Baroclinic Waves in a Two-Layer Beta-Plane Model , 1989 .

[19]  A. Barnston,et al.  Classification, seasonality and persistence of low-frequency atmospheric circulation patterns , 1987 .

[20]  J. Sheng GCM experiments on changes in atmospheric predictability associated with the PNA pattern and tropical SST anomalies , 2002 .

[21]  J. Egger,et al.  On the Theory of the Long-Term Variability of the Atmosphere , 1983 .

[22]  Brian J. Hoskins,et al.  Rossby Wave Propagation on a Realistic Longitudinally Varying Flow , 1993 .

[23]  Arun Kumar,et al.  Role of the Pacific‐North American (PNA) pattern in the 2007 Arctic sea ice decline , 2008 .

[24]  W. Collins,et al.  The NCEP–NCAR 50-Year Reanalysis: Monthly Means CD-ROM and Documentation , 2001 .

[25]  J. Abatzoglou,et al.  Opposing Effects of Reflective and Nonreflective Planetary Wave Breaking on the NAO , 2005 .

[26]  R. Dole,et al.  The Dynamics of Large-Scale Cyclogenesis over the North Pacific Ocean , 1993 .

[27]  F. Jin,et al.  Dynamics of Synoptic Eddy and Low-Frequency Flow Interaction. Part III: Baroclinic Model Results , 2006 .

[28]  I. Orlanski A New Look at the Pacific Storm Track Variability: Sensitivity to Tropical SSTs and to Upstream Seeding , 2005 .

[29]  Paul Berrisford,et al.  A New Rossby Wave–Breaking Interpretation of the North Atlantic Oscillation , 2008 .

[30]  John W. Nielsen-Gammon,et al.  Using Tropopause Maps to Diagnose Midlatitude Weather Systems , 1998 .

[31]  Brian J. Hoskins,et al.  The Steady Linear Response of a Spherical Atmosphere to Thermal and Orographic Forcing , 1981 .

[32]  S. Feldstein The Timescale, Power Spectra, and Climate Noise Properties of Teleconnection Patterns , 2000 .

[33]  M. Watanabe,et al.  Dynamics of Synoptic Eddy and Low-Frequency Flow Interaction. Part I: A Linear Closure , 2006 .

[34]  Ngar-Cheung Lau,et al.  Variability of the observed midlatitude storm tracks in relation to low-frequency changes in the circulation pattern , 1988 .

[35]  R. Wayne Higgins,et al.  Persistent North Pacific Circulation Anomalies and the Tropical Intraseasonal Oscillation , 1997 .

[36]  M. Watanabe,et al.  The Growth and Triggering Mechanisms of the PNA : A MJO-PNA Coherence , 2008 .

[37]  N. Bond,et al.  Decadal Variability of the Aleutian Low and Its Relation to High-Latitude Circulation* , 1999 .

[38]  Nathaniel C. Johnson,et al.  The Continuum of North Pacific Sea Level Pressure Patterns: Intraseasonal, Interannual, and Interdecadal Variability , 2009 .

[39]  N. Lau,et al.  A Diagnostic and Modeling Study of the Monthly Mean Wintertime Anomalies Appearing in a 100-Year GCM Experiment , 1993 .

[40]  Klaus M. Weickmann,et al.  Circulation anomalies associated with tropical convection during northern winter , 1992 .

[41]  John M. Wallace,et al.  Planetary-Scale Atmospheric Phenomena Associated with the Southern Oscillation , 1981 .

[42]  T. Palmer Medium and extended range predictability and stability of the Pacific/North American mode , 2006 .

[43]  S. Feldstein Fundamental mechanisms of the growth and decay of the PNA teleconnection pattern , 2002 .

[44]  C. Franzke,et al.  Are the North Atlantic Oscillation and the Northern Annular Mode Distinguishable , 2006 .

[45]  S. Schubert,et al.  Low-Frequency Intraseasonal Tropical-Extratropical Interactions , 1991 .

[46]  G. Branstator Analysis of General Circulation Model Sea-Surface Temperature Anomaly Simulations Using a Linear Model. Part I: Forced Solutions , 1985 .

[47]  Huw C. Davies,et al.  Breaking Waves at the Tropopause in the Wintertime Northern Hemisphere: Climatological Analyses of the Orientation and the Theoretical LC1/2 Classification , 2007 .

[48]  Linhao Zhong,et al.  Dynamical Relationship between the Phase of North Atlantic Oscillations and the Meridional Excursion of a Preexisting Jet: An Analytical Study , 2008 .

[49]  Gwendal Rivière,et al.  Characteristics of the Atlantic Storm-Track Eddy Activity and Its Relation with the North Atlantic Oscillation , 2005 .

[50]  R. Reynolds,et al.  The NCEP/NCAR 40-Year Reanalysis Project , 1996, Renewable Energy.

[51]  D. Luo,et al.  Dynamics of Eddy-Driven Low-Frequency Dipole Modes. Part IV: Planetary and Synoptic Wave-Breaking Processes during the NAO Life Cycle , 2008 .

[52]  I. Orlanski Bifurcation in Eddy Life Cycles: Implications for Storm Track Variability , 2003 .

[53]  Christian Franzke,et al.  Is the North Atlantic Oscillation a Breaking Wave , 2004 .

[54]  C. Franzke,et al.  The continuum and dynamics of Northern Hemisphere teleconnection patterns , 2005 .

[55]  J. Wallace,et al.  Teleconnections in the Geopotential Height Field during the Northern Hemisphere Winter , 1981 .

[56]  J. Frederiksen A Unified Three-Dimensional Instability Theory of the Onset of Blocking and Cyclogenesis , 1982 .

[57]  R. Dole,et al.  Life cycles of persistent anomalies. II - The development of persistent negative height anomalies over the North Pacific Ocean , 1990 .

[58]  M. Hitchman,et al.  A Climatology of Rossby Wave Breaking along the Subtropical Tropopause , 1999 .

[59]  B. Hoskins,et al.  The Direct Response to Tropical Heating in a Baroclinic Atmosphere , 1995 .

[60]  P. R. Julian,et al.  Description of Global-Scale Circulation Cells in the Tropics with a 40–50 Day Period , 1972 .

[61]  B. Hoskins,et al.  Two paradigms of baroclinic‐wave life‐cycle behaviour , 1993 .

[62]  A. Lupo,et al.  Dynamics of Eddy-Driven Low-Frequency Dipole Modes. Part I: A Simple Model of North Atlantic Oscillations , 2007 .

[63]  The tropical-extratropical interaction between high-frequency transients and the Madden-Julian oscillation , 1999 .