MONTHLY ANTICYCLONICITY AND CYCLONICITY IN THE SOUTHERN HEMISPHERE: AVERAGES FOR MARCH AND SEPTEMBER

Similar documents
Lecture 14. Heat lows and the TCZ

ENSO Cycle: Recent Evolution, Current Status and Predictions. Update prepared by Climate Prediction Center / NCEP 8 March 2010

Typhoon Vamei: An Equatorial Tropical Cyclone Formation

Influence of enhanced convection over Southeast Asia on blocking ridge and associated surface high over Siberia in winter

Weather drivers in Victoria

McKnight's Physical Geography 11e

Lecture 20. Active-weak spells and breaks in the monsoon: Part 1

9/25/2014. Scales of Atmospheric Motion. Scales of Atmospheric Motion. Chapter 7: Circulation of the Atmosphere

The Morphology of the Subtropical Anticyclone. By Y. Neyama

The Effects of Gap Wind Induced Vorticity, the ITCZ, and Monsoon Trough on Tropical Cyclogenesis

Atmospheric Waves James Cayer, Wesley Rondinelli, Kayla Schuster. Abstract

Weather drivers in South Australia

Climate briefing. Wellington region, February Alex Pezza and Mike Thompson Environmental Science Department

Lecture 13 El Niño/La Niña Ocean-Atmosphere Interaction. Idealized 3-Cell Model of Wind Patterns on a Rotating Earth. Previous Lecture!

Climatology of the 10-m wind along the west coast of South American from 30 years of high-resolution reanalysis

3. Climatic Variability. El Niño and the Southern Oscillation Madden-Julian Oscillation Equatorial waves

Air Pressure and Wind

Atmospheric Rossby Waves in Fall 2011: Analysis of Zonal Wind Speed and 500hPa Heights in the Northern and Southern Hemispheres

APPENDIX B NOAA DROUGHT ANALYSIS 29 OCTOBER 2007

RELATIONSHIP BETWEEN CROSS-EQUATORIAL FLOW, TRADE WIND FLOW AND FAVOURABLE CONDITIONS OF THE CYCLOGENESIS OVER THE MOZAMBICA CHANNEL

Chapter. Air Pressure and Wind

GEOS 201 Lab 13 Climate of Change InTeGrate Module Case studies 2.2 & 3.1

AT350 EXAM #2 November 18, 2003

ATMOSPHERIC CIRCULATION. WIND = The horizontal movement of air. Results from the differences in air pressure. Always moves from HIGH to LOW.

Ocean Currents Shortcut method by to learn faster

Ocean Currents Shortcut method by to learn faster

Lecture 8: Pressure and Wind

Atmospheric Circulation. Recall Vertical Circulation

PHYSICAL GEOGRAPHY. By Brett Lucas

Effect of sea surface temperature on monsoon rainfall in a coastal region of India


CHAPTER 7 Ocean Circulation

CLIMATOLOGY. GEOGRAPHY Grade 12

Global Circulations. GEOG/ENST 2331 Lecture 15 Ahrens: Chapter 10

Recent Atmospheric and Oceanic Circulation Changes Affecting Winter Weather in North America. Dr. Art Douglas Professor Emeritus Creighton University

Effect of Orography on Land and Ocean Surface Temperature

Chapter 6: Atmospheric Pressure, Wind, and Global Circulation

18.1 Understanding Air Pressure 18.1 Understanding Air Pressure Air Pressure Defined Measuring Air Pressure Air pressure barometer

WEATHER SYSTEMS OF MIDDLE LATITUDES

Atmospheric Rossby Waves Fall 2012: Analysis of Northern and Southern 500hPa Height Fields and Zonal Wind Speed

Atmosphere Circulation

Prof. Geraint Vaughan. Centre for Atmospheric Science School of Earth, Atmospheric and Environmental Sciences. Bogdan Antonescu

Meteorology. Circle the letter that corresponds to the correct answer

Tropical Pacific Ocean remains on track for El Niño in 2014

ATOMOSPERIC PRESSURE, WIND & CIRCULATION

Understanding El Nino-Monsoon teleconnections

Canada s vast size creates a diverse range of weather conditions and climatic conditions. Warming trend for last 10 years Wet Spring Dry five summers

Chapter 22, Section 1 - Ocean Currents. Section Objectives

Length of day for a full year. Ocean Gyres. Wet. Adiabatic. lapse rate, starts at. dewpoint Dry Adiabatic lapse rate

National Weather Service

The General Circulation and El Niño. Dr. Christopher M. Godfrey University of North Carolina at Asheville

Section 3: Atmospheric Circulation

Intraseasonal Variability of the Low-Level Jet Stream of the Asian Summer Monsoon

Introduction to Oceanography OCE 1001

Large-Scale Overview of YOTC Period (ENSO, MJO, CCEWs,.)

ENSO Cycle: Recent Evolution, Current Status and Predictions. Update prepared by Climate Prediction Center / NCEP 4 September 2012

Analysis of 2012 Indian Ocean Dipole Behavior

REMINDERS: UPCOMING REVIEW SESSIONS: - Thursday, Feb 27, 6:30-8:00pm in HSS 1330

THE ATMOSPHERE. WEATHER and CLIMATE. The Atmosphere 10/12/2018 R E M I N D E R S. PART II: People and their. weather. climate?

Organized Deep Cumulus Convection Over the South China Sea and its Interaction with Cold Surges

Chapter 10: Global Wind Systems

Abrupt seasonal variation of the ITCZ and the Hadley circulation

Wind Driven Circulation Indian Ocean and Southern Ocean

3/22/11. General Circulation of the Atmosphere. General Circulation of the Atmosphere

Currents. History. Pressure Cells 3/13/17. El Nino Southern Oscillation ENSO. Teleconnections and Oscillations. Neutral Conditions

Historical Analysis of Montañita, Ecuador for April 6-14 and March 16-24

SESSION THREE: FACTORS THAT INFLUENCE WEATHER IN SOUTH AFRICA

ESS15 Lecture 12. Review, tropical oceans & El Nino, and the thermohaline ocean circulation. Please see new reading material on website.

2.2 Southwest Monsoon

RECTIFICATION OF THE MADDEN-JULIAN OSCILLATION INTO THE ENSO CYCLE

Ocean Currents Lecture Notes

ENSO and monsoon induced sea level changes and their impacts along the Indian coastline

Some characteristics of low pressure systems and summer monsoon rainfall over Orissa

Your web browser (Safari 7) is out of date. For more security, comfort and the best experience on this site: Update your browser Ignore

Local vs. Remote SST Forcing in Shaping the Asian-Australian Monsoon Variability

Lesson: Atmospheric Dynamics

Finish Characteristics of Climate

The Air-Sea Interaction. Masanori Konda Kyoto University

Polar storms and polar jets: Mesoscale weather systems in the Arctic & Antarctic

The ocean water is dynamic. Its physical

Foundations of Earth Science, 6e Lutgens, Tarbuck, & Tasa

Record-breaking La Niña events

Interannual variation of northeast monsoon rainfall over southern peninsular India

8.4 COASTAL WIND ANOMALIES AND THEIR IMPACT ON SURFACE FLUXES AND PROCESSES OVER THE EASTERN PACIFIC DURING SUMMER

Biennial Oscillation of Tropical Ocean-Atmosphere System Associated with Indian Summer Monsoon

Impacts of intraseasonal oscillation on the onset and interannual variation of the Indian summer monsoon

W3 Global Circulation Systems

Lightning distribution with respect to the monsoon trough position during the Indian summer monsoon season

Lecture 33. Indian Ocean Dipole: part 2

Cold Air Damming. Introduction. Learning Objectives. Cold Air Damming. Cold Air Damming. Cold Air Damming 9/28/17. After this class you should

Wednesday, September 27, 2017 Test Monday, about half-way through grading. No D2L Assessment this week, watch for one next week

ATMS 310 Tropical Dynamics

The atmospheric circulation system

Atmospheric and Ocean Circulation Lab

Changes of The Hadley Circulation Since 1950

SERIES ARTICLE The Indian Monsoon

Atmospheric Circulation. Density of Air. Density of Air: H 2 O and Pressure effects

The impacts of explicitly simulated gravity waves on large-scale circulation in the

Currents & Gyres Notes

Lecture Outlines PowerPoint. Chapter 18 Earth Science 11e Tarbuck/Lutgens

Transcription:

76 Weather and Climate (1992) 12: 76-82 MONTHLY ANTICYCLONICITY AND CYCLONICITY IN THE SOUTHERN HEMISPHERE: AVERAGES FOR MARCH AND R. M. Leighton National Meteorological Centre Bureau of Meteorology, Melbourne, Australia ABSTRACT Geographical distributions across the Southern Hemisphere of 15-year averages (23-year averages in the Australian region) of monthly anticyclonicity and cyclonicity as well as monthly anticyclone and cyclone immobility times, for the months of March and September for the years 1973-1987 (1965-1987 in the Australian region) are presented in the form of maps. Comparisons are made with an existing atmospheric climatology of the Southern Hemisphere by the National Climate Centre of the Bureau of Meteorology, Melbourne covering the period 1976-1990 calculated from numerical analyses, and with relevant climatologies contained in the World Survey of Climatology. References are made to past works relating to the climatology of the Southern Hemisphere and synoptic features of the climatology are discussed. INTRODUCTION An excellent account of the early history of synoptic meteorology and climatology is given by Klein (1957) with references to the tracking and frequency of cyclones and anticyclones in the Northern Hemisphere. By the end of the nineteenth century many studies of cyclone frequency and tracks were made not only for the U.S. but for Europe, the Atlantic, India, the west Indies and the Far East. The first thorough investigation for the Northern Hemisphere was completed in 1894 which contained the average frequency of cyclones during each of the 12 months and their principal tracks. During the twentieth century notable work on various aspects of synoptic climatology in the Southern Hemisphere has been completed. Streten and Troup (1973) developed a classification scheme for observed cloud vortices. Streten (1980) developed a series of indices relating to the subtropical highs, the westerlies, the sub-antarctic trough and the high pressure region south of the sub-antarctic trough and Streten and Pike (1980) applied these monthly indices to the year of the first GARP global experiment (FGGE) of 1978-79. Trenberth (1984) studied the interannual variability of the Southern Hemisphere circulation as represented by the FGGE year. Le Marshall et al. (1985) produced ten-year monthly mean sea level pressure charts based on 10 years of daily numerical analyses (1972-1982) for both January and July, and a comparison of these charts with averages of anticyclonicity and cyclonicity for the Australasian region (90 E-1800E) are discussed by Leighton and Deslandes (1991). A comprehensive account of the history of the study of blocking in the Southern Hemisphere is given by Trenberth and Mo (1985). Trenberth (1991) provided a description of atmospheric variables which have a strong signature in baroclinic storm tracks in the Southern Hemisphere. Jones (1991) used a principal components regression scheme on station mean sea level pressure data to reconstruct gridded data back to 1951 and 1911.

For the Australian region (including New Zealand) the method of representation of the surface circulation for long periods (i.e. months, season, etc) by charts of anticyclonicity and cyclonicity was developed during 1951-53 in connection with the problem of extended and long-range forecasting in Australia. Later charts of 7-year averages (1946-1952) of monthly and seasonal anticyclonicity and cyclonicity and their description were published by Karelsky (1954). Charts of monthly and seasonal anticyclonicity and cyclonicity for the Australian region for 15 years (1946-1960) were published by Karelsky (1961). Leighton and Deslandes (1991) published monthly charts for 23 years (1965-1987) for the Australian region including the eastern Indian Ocean. ANTICYCLONICITY AND CYCLONICITY The term anticyclonicity (cyclonicity) is defined as the time in hours during which anticyclone (cyclone) centres occupied a given 5* cell during a given period (i.e., week, month, season, etc.). (South of 55'S cells are 5' latitude by 10' longitude.) Cyclonicity and anticyclonicity were computed from the plotted locations of cyclone (anticyclone) centres at 00 UTC and 12 UTC and, assuming a uniform speed of movement, the systems could be tracked. Single centres which were not part of a track were assigned a lifetime of 6 hours. Cyclones whose centres were tracked fitted into one or more of the following classes: identifiable closed circulation with or without an associated front, wave lows which developed into closed circulations, thermal (heat) low, tropical lows and tropical cyclones. Anticyclones in general covered much larger areas than cyclones. On occasions when anticyclones were shown to have a double centre, both centres were considered when budding (an anticyclone centre forming in a ridge which is extending from an established anticyclone) was the obvious cause. Centres in ridges were taken into account when there was an identifiable outflow, or when they were seen as a prelude to anticyclogenesis. In general the cut-off value for weak cyclones was about 1008 hpa except in cases when cyclogenesis was evident. For anticyclones, weak cells below 1018 hpa in tropical regions and in high-latitude ridges were taken into account, but for mid latitudes these cells were considered only when anticyclogenesis was apparent. A certain amount of identification of centres relates to the pressure of the centre compared with that of surrounding areas rather than the absolute pressure value of the centre. Manually drawn archive charts prepared by the National Meteorological Centre of the Australian Bureau of Meteorology were used to obtain means of cyclonicity, anticyclonicity, and immobility for March and September from 1973-1987 (1965-1987 in the Australian Region (90 E-180 E)). Charts of mean monthly anticyclonicity, anticyclone immobility, cyclonicity, and cyclone immobility are presented in Figs. la-d and 2a-d. CHARTS OF ANTICYCLONE (CYCLONE) IMMOBILITY Immobility of an anticyclone (cyclone) centre is defined as the time taken by the anticyclone (cyclone) centre to traverse a 5' cell. The average immobility of anticyclone (cyclone) centres across a 5' cell was calculated by dividing the anticylonicity (cyclonicity) of a 5 cell by the number of anticyclone (cyclone) centres which have occupied that square during the same period. ACCURACY OF CHARTS OF ANTICYCLONICITY AND CYCLONICITY Cloud satellite photos were available from 1965 for the Australian Region and from 1973 for the Southern Hemisphere, greatly increasing the data base for synoptic analyses. Additional data has been supplied by drifting buoys deployed at various times since 1978 at differing locations in the oceans around the Southern Hemisphere. The author believes that the ability of analysts to identify centres of lows from cloud photos could affect the accuracy of the charts. Wave lows forming under heavy cloud cover may not be obvious until the clouds display a definite wave or hook shape. Old lows can be difficult to assess because an apparent circulation may remain visible in the cold air after the surface low itself has decayed. Lows situated under clouds associated with warm air advection may give no visible evidence of formation, particularly in the initial stages of development. Surface lows in the monsoon trough are difficult to determine due to lack of data. Areas showing 77

78 ANT IC YCL ONICITY MARCH RHISY CYCLONICITY MARCH rema 06 oz, N ANTICYCLONE IMMOBILIT MARCH Fig 1: March average (a) anticyclonicity (c) cyclonicity Isopleths are hours for each 5 square (b) anticyclone immobility index (d) cyclone immobility index Isopleths are hour/system for each 5' square. (e) Hemispheric mean sea level pressure 1.85,11 1

79 ANTICYCLONICITY Ft, 13 CYCLONICIT Y 11265,11 15 ANTICYCLONE IMMOBILITY CYCLONE IMMOBILITY R285,14 Fig 2: September average (a) anticyclonicity (c) cyclonicity Isopleths are hours for each 5' square (b) anticyclone immobility index (d) cyclone immobility index Isopleths are hour/system for each 5' square. (e) Hemispheric mean sea level pressure R285,

80 large cloud masses of convective activity in the tropics are regarded as regions of potential surface low development. On occasions analyses identify ephemeral centres in these areas. DISCUSSION Differing approaches to the climatology of synoptic systems for a region add detail to the understanding of the overall climatology of that region. Charts of (anti)cyclonicity help show how the centres of pressure systems can relate to the results of other climatological studies and indicate areas of fast or slow centre movement, thus suggesting regions favourable for the development of synoptic blocking patterns. The 15-year (1976-1990) average hemispheric mean sea level pressure charts for March and September as produced by the National Climate Centre (NCC) of the Bureau of Meteorology, Melbourne appear in Figs. le, 2e. Climatologies contained in the World Survey of Climatology volumes 12 (Climates of Central and South America) and 15 (Climates of the Oceans) will be referred to as well as results from other works previously mentioned. Anticyclonicity The hemispheric mean sea level charts for both months show that the maximum pressures in the subtropical ridge are across the eastern half of the oceans. Anticyclonicity maxima coincide well with the maximum pressure values in the eastern Pacific Ocean and the eastern Atlantic Ocean in March. Around the hemisphere various other anticyclonicity maxima are located in the ridge mainly to the south of the ridge axis particularly in the western half of the oceans. In September the anticyclonicity centres are notably south of the high pressure ridge. The anticyclonicity maxima highlight where anticyclone centres are predominant in or near the ridge. Most anticyclones would appear to move eastwards to the south of the pressure ridge axis. This finding is consistent with Taljaard and van Loon (1984) when discussing the climate of the Indian Ocean south of 35'S, who state that the high pressure axis is located about 3 degrees equatorward of the core of highest anticylonic frequency. This is due to the fact that frontal or intercell troughs and occasional cyclones also occur in the anticyclonicity belt, in which cases the highest pressures (in the cols) are found well to the north. Across the Australian region the anticyclonicity chart for March has distinct maxima at latitudes higher than 35'S in the Bight and the Tasman Sea. Notable maxima occur south of the west coast of Australia, across southeastern Australia and across New Zealand. Anticyclones located in the east Indian Ocean can extend a ridge under W.A. into the Bight where a new anticyclone centre forms in the ridge a process known as budding. Anticyclones are known to remain in the Bight before a similar budding process occurs across southeastern Australia and anticyclone centres strengthen in the Tasman Sea. New Zealand is also a notable region for budding. In September the anticyclonicity maxima are located between 30'S and 35'S at longitudes similar to that of March. East of New Zealand between 40'S and 50'S the anticyclonicity charts for both March and September have anticyclonicity maxima located at the highest latitudes around the hemisphere. The September maximum is small but distinct. The anticyclone immobility value for both months indicate that anticyclones tend to be slow moving when located in this region. Across the mid Pacific in March the anticyclonicity maxima values lie between 35'S and 45'S whereas in September the maxima are between 30'S and 40'S. In the eastern Pacific the anticyclones mostly are located between 30'S and 35"S near 90'W in March and between 25'S and 35'S east of 90'W in September. The anticyclone immobility values indicate that the less common anticyclones which are located at high latitudes across the Pacific can be slow moving particularly in September. In the western Atlantic Ocean near 40'W the anticylonicity maximum in March is between 35'S and 40'S and in September between 30'S and 35'S. In the eastern Atlantic Ocean near 0' the March maximum lies between 30'S and 35'S whereas the September maximum is between 25'S and 30'S. The March maxima values are notably higher than the September values which is similar to the other oceans. The immobility values show that the irregular anticyclone centres which form off the Antarctic Peninsula north of the Weddell Sea are likely to be slow moving.

In the Indian Ocean the anticyclonicity chart for March shows a broad maximum lying across the ocean between 35'S and 40'S. By contrast the anticyclonicity for September lies across the ocean between 30'S and 35'S. Peaks in the maxima are comparable in both months near 60'E and near 100"E. These months clearly show the seasonal shift in latitude of the paths preferred by anticyclones. The anticyclone immobility values in the Indian Ocean are lower than in the other oceans particularly in the eastern sector suggesting that the eastern Indian Ocean is not as great an anchor point for single anticyclones as the eastern Pacific or eastern Atlantic Oceans. Cycloni city For both March and September the largest cyclonicity maximum is placed in the sub- Antarctic trough near the mean minimum sea level pressure value south of Western Australia. Other cyclonicity maxima coincide reasonably with minimum pressure values around the trough. For both months in the New Zealand sector, both the Tasman Sea and the Pacific Ocean have cyclonicity maxima and cyclone immobility maxima indicating slow moving lows are common. These regions also favour slow moving anticyclones as suggested by the anticyclonicity and anticyclone immobility values which support the findings of Trenberth and Mo that the New Zealand sector is a primary location for the occurrence of blocking patterns. Across the Pacific Ocean the cyclonicity chart for September shows distinct maxima between 40'S and 50'S and another strong maximum in the sub-antarctic trough. A notable minimum is evident through the Ocean between 50'S and 60'S. The mid-pacific cyclones which have originated in the Southwest Pacific or on the South Pacific Convergence Zone are usually separated from the large southern depressions by either a col region or occasionally a narrow latitudinal ridge located between 50'S and 60'S. In March the cyclonicity values across the central Pacific are less than in September and the latitudinal split in cyclonicity maxima is not as definite. These differences in cyclonicity values suggest that September is a more favoured month for cut-off lows to be located in the Pacific than March. In the southwestern Atlantic Ocean cyclonicity maxima in both months are associated with cyclogenesis in the frontal zone off South America (Hoflich, 1984) and developments in easterlies over or near the South American continent. Both months show a cyclonicity maximum near 4005 40'W indicating that cut-off lows are favoured in this region. Across the Indian Ocean at high latitudes both months show cyclonicity maxima at the same locations, but cyclonicity at mid latitudes is less in the Indian Ocean than the other two oceans. For both months the Atlantic- Indian Ocean sector has an extended minimum cyclone immobility value along 50'S suggesting that movement of cyclones at this latitude is rapid. By contrast cyclone immobility minima in the Pacific Ocean are not continuous particularly in September indicating that cyclone movement can be slower than in the other oceans. In both months the cyclonicity maxima across northwestern Australia and northern Argentina are related to heat lows. The Australian heat low is more evident than the corresponding heat low in South America because Schwerdtfeger (1984) states that the location in Argentina is over relatively high and dry terrain east of the Andes where the reduction of station level pressure to mean sea level pressure is a problematic procedure. In March the cyclonicity maxima across tropical waters in the Indian Ocean, the Australian region and the western Pacific Ocean relate to tropical lows and cyclones. The cyclone immobility chart shows a large number of centres across these tropical regions but the author feels that a longer time average and a denser network of surface observations would be needed to confirm such a pattern of centres. CONCLUSION (Anti)cyclonicity and (anti)cyclone immobility averages supplement conventional climatologies by showing preferred locations of surface centres, regions of slow and rapid movement of centres and location of potential blocking areas. Averages for March and September show how positions of anticyclone and cyclone centres differ in contrasting seasons (in this case late summer and late winter). Some regions show a significant seasonal dif- 81

82 ference, for example latitudinal positions of anticyclones in subtropical regions and locations of lows in the tropics; whereas some regions do not, for example positions of lows off the coast of Antarctica. Blocking appears more common in the Pacific Ocean in September and speed of cyclone movement across the Atlantic-Indian Ocean sector near 50'S shows little difference between the two months. The averages could be useful for verifying the realism of Regional and Global Numerical Weather Prediction and the basic figures, being on a five degree grid, could be used as a data base in models. Anomalies can be calculated for ongoing current months and these could help in defining severe weather occurrences or possible climate change. ACKNOWLEDGEMENTS The author wishes to thank Roger Deslandes for assistance in the Australian Region, Terry Skinner for comments on the work and on the manuscript, Cheryl Hatcher for data calculation and typing the manuscript and to the Drafting Section of the Australian Bureau of Meteorology for the production of the charts. gion: 23 year (1965-1987) Averages, Bureau of Meteorology and Technical Report No. 64, 29 pp. Le Marshall, J.R., Kelly, G.A.M. and Karoly, D.J. 1985. An atmospheric climatology of the Southern Hemisphere based on the ten years of daily numerical analyses (1972-1982): I overview, Aust. Meteor. Mag. 33, 65-85. Schwerdtfeger, W. 1984. Climates of Central and South America, World Survey of Climatology, Vol. 12, Elsevier Amsterdam, 1-11. Streten, N.A. 1980. Some synoptic indices of the Southern Hemisphere mean sea level circulation 1972-1977, Mon. Wea. Rev. 108, 18-36. Streten, N.A. and Pike, D.J. 1980. Indices of the mean monthly surface circulation over the Southern Hemisphere during FGGE, Aust Meteorol. Mag. 28, 201-215. Streten, N.A. and Troup, Al. 1973. A synoptic Climatology of satellite observed cloud vortices over the Southern Hemisphere, Quart. J. R. Met. Soc. 99, 56-72. Taljaard, J.J. and van Loon, H. 1984. Climate of the Indian Ocean South of 35'S, in van Loon, H. (ed.), Climates of the Oceans, World Survey of Climatology, Vol 15, Elsevier, Amsterdam 505-588. Trenberth, K.E. 1984. Interannual variability of the Southern Hemisphere circulation: representativeness of the year of the Global Weather Experiment, Mon. Wea. Rev. 112, 108-123. Trenberth, K.E. 1991. Storm tracks in the Southern Hemisphere, J. Atmos. Sci. 48, 2159-2178. Trenberth, K.E. and Mo, K.C. 1985. Blocking in the Southern Hemisphere, Mon. Wea. Rev. 113, 3-21. REFERENCES Berry, KA., Owens, G.V. and Wilson, M.P. 1952. Arctic Weather Maps, U.S. Navy Bureau of Aeronautics, Project AROWA, 102 pp. Guymer, L.B. and Le Marshall, J.F. 1980. Impact of FGGE buoy data on Southern Hemisphere Analyses, Aust Meterol. Mag. 28, 19-42. Hoflich, O. 1984. Climate of the South Atlantic Ocean, in Van Loon, H. (ed.), Climates of the Oceans. World Survey of Climatology, Vol. 15, Elsevier, Amsterdam, pp 1-131. Jones, P.D. 1991. Southern Hemisphere Sea-Level Pressure Data: An Analysis and Reconstruction back to 1951 and 1911, J Climatol. 11, 585-607. Kareslky, S. 1954. Surface circulation in the Australasian region, Bureau of Meteorology Study No. 3, AGPS, Canberra 45 pp. Karelsky, S. 1961. Monthly and seasonal anticyclonicity and cyclonicity in the Australian region 15 year average (1946-1960), Bureau of Meteorology Study No. 13, AGPS, Canberra, 11 pp. Klein, W.K. 1957. Principal tracks and mean frequencies of cyclones and anticyclones in the Northern Hemisphere. Research Paper No. 40, U.S. Weather Bureau, Washington D.C. Leighton, R.M. and Deslandes, R. 1991. Monthly Anticyclonicity and Cyclonicity in the Australasian Region: Averages for January, April, July and October, Aust. Met. Mag, 39, 149-154. Leighton, R.M. and Deslandes, R. 1.991.Monthly Anticyclonicity and Cyclonicity in the Australian Re-