3.1. Anomaly Maps for 2023 and 2022
Examination of the annual mean precipitation map for 2023 (
Figure 1, top panel) indicates the typical features across the globe, with precipitation maxima of the tropics and mid-latitudes and dry zones in the subtropics. However, the bottom panel of
Figure 1 shows that there are significant anomaly features from the long-term (1979–2022) climatology. La Nina conditions were still dominant in January 2023 in the central tropical Pacific (Nino 3.4 Index of −0.72). A rapid warming in the central Pacific Ocean evolved over the next few months, resulting in a change to a positive Index by April with continued SST warming as the El Nino emerged, reaching a December Index of +2.07. For all of 2023, the mean Nino 3.4 Index was +0.83.
Because the El Nino-type conditions dominate the year, the tropical anomaly pattern has a stronger weight in that category, although the overall annual pattern is affected by the La Nina conditions in the early part of the year. Across the central Pacific there is a strong positive anomaly along the ITCZ, with negative anomalies to the north and south, indicating an intensification of the ITCZ in this region [
7,
8,
9]. The western Pacific Ocean also has a wet anomaly, but wider compared to the central Pacific. Over the Maritime Continent there is a general negative anomaly with some small positive areas. To the southwest of the Maritime Continent, stronger negative anomalies extend into the Indian Ocean. Over the western Indian Ocean, a positively anomaly exists overlapping the Equator and reaching into Africa. A strong negative anomaly is present over southern Africa. Australia was generally dry, as is expected during generally El Nino conditions. The Amazon in South America has a large rainfall deficit amid continuing drought conditions there. However, just to the south, surrounding the border between Brazil and Argentina a small area of precipitation surplus is present.
It is useful to extend our analysis back through 2022 to set the recent context. In early 2020, central Pacific Ocean surface temperatures cooled with the start of the 2020–2023 La Nina, one of the longest on record. The year 2022 had La Nina conditions for the entire year.
Figure 2 shows the anomaly fields for 2022 and 2023, along with annual composites for La Nina and El Nino conditions using previous years, based on the Nino 3.4 Index. The annual 2022 anomaly field matches the La Nina composite very well, especially over both tropical ocean and land areas, but even to a fair degree at higher latitudes. The La Nina and El Nino composites are very close mirror images of each other. For 2022, the La Nina resulted in central Pacific dryness, Maritime Continent wet conditions, dryness over much of the Indian Ocean, extending well south of the Equator, and wet conditions over southern Africa and northern South America. The wet feature over the Maritime Continent extends far to the southeast to the Straits of Magellan. Somewhat weaker matches are found over the North Pacific and Atlantic Oceans and North America.
To quantify the relation of the annual anomaly map to El Nino conditions, the pattern correlation is computed between the anomaly maps for 2023 and the El Nino composite for the 40° N–40° S band. For the whole year it is positive +0.34, but small compared to December 2023 with +0.59, when the El Nino was very intense with a Nino 3.4 of +2.07. Therefore, the annual anomaly map shows generally El Nino conditions, but not overwhelmingly so, due to the La Nina conditions during the early months of the year.
North America for 2023 was generally drier than normal, but interrupted by a relatively wet zone from the Pacific into the U.S. west coast and extending eastward. This general pattern is dissimilar from that of typical El Nino years.
Over Europe and northern Asia, positive precipitation anomalies dominated for the year, except for the Iberian Peninsula and the Mediterranean Sea. The South Asian monsoon produced positive anomalies over the water and a varying result over land, as was the case over China.
3.2. Evolution of Precipitation Patterns during 2023
The evolution of the anomaly patterns through the year is shown in
Figure 3. The January–March pattern (
Figure 3a) indicates a La Nina in the Pacific and elsewhere (Nino 3.4 Index of −0.4). This La Nina-like pattern has a large deficit of rain over the central equatorial Pacific, with the V-shaped positive anomaly to the west over the Maritime Continent, with arms reaching to the northeast and southeast, and a mostly dry Indian Ocean. The Australia and Amazon regions are unexpectedly dry due to the weakening phase of the La Nina. The dry feature over the Amazon in these early months continues throughout the year into the El Nino phase, exasperating the drought there.
The El Nino begins to show in the April–June pattern (
Figure 3b) with the start of a Pacific ITCZ and western Pacific wet anomaly (Nino 3.4 Index +0.47). This El Nino pattern continues to intensify through July–September (
Figure 3c, Nino 3.4 Index +1.1) into the full tropical El Nino pattern of the final period (
Figure 3d, Index +1.9). Floods and landslides, for example over Somalia and eastern Africa (see
https://floodlist.com/africa/east-africa-floods-november-2023-somalia-ethiopia-kenya-burundi-malawi, accessed on 20 January 2024), are associated with this El Nino pattern, as is the continuation of the drought over the Amazon. Independent of ENSO, over Europe and northern Asia positive anomalies exist over the cool months and negative anomalies over the warm months.
This transition from La Nina to El Nino is quantified in
Figure 4, examining the pattern correlation over the latitude band 40° N–40° S. This band was chosen to cover the deep tropics and much of the subtropics and include both wet and dry regions where ENSO has significant effect. For the entirety of 2022, when the Nino 3.4 SST Index was near −1.0, the correlation between the monthly anomaly patterns and the composite La Nina patterns is about +0.4 (and about -0.4 against the El Nino composites). As time crosses into 2023, the Nino 3.4 Index begins to increase, crossing into positive territory in March on its way to a maximum of ~+2.0 at the end of 2023. The anomaly/composite correlations also rapidly change, with the positive El Nino correlation continuously increasing until the last few months, reaching a value of +0.6 at the end of 2023.
3.3. Global Regional Trends and 2023 Anomalies
The global trend map based on the GPCP analysis of satellite and gauge observations has been described [
3,
10] and compared to climate model results [
11].
Figure 5 (top panel) shows a 1983–2022 version of the GPCP trend map. In the tropical Pacific, the ITCZ has intensified and shifted northward during the last 40+ years. The western Pacific shows a positive change, along with the tropical Indian Ocean and the Atlantic ITCZ region. Land areas also show trends, e.g., wet and dry trends over South America and drying over southwest North America. Regional trends are obviously the accumulation over the years of regional annual departures from climatology. So, how does 2023 fit in to that long-term trend map? The 2023 anomaly map is repeated in the bottom panel of
Figure 5 for comparison and shows some positive overlaps with the long-term trend map, indicating 2023 playing a role in the long-term changes. Examples include matching positive signs between the two panels in the western Pacific, western Indian Ocean, and the Pacific ITCZ, and matching negative signs over the southwestern U.S. and the Amazon. The pattern of trends and anomalies also are similar over the South Pacific Convergence Zone (SPCZ) and the high latitudes of the Northern Hemisphere. As one would expect, the comparison is noisy, however, the correlation between the two fields (40° N–40° S) is positive, at +0.21, indicating that overall the anomaly field from 2023 has contributed positively to the long-term trend pattern.
Comparison of the GPCP trend map with climate model results, but for the earlier GPCP V2.3, has been discussed in [
11].
Figure 6 shows a similar set of maps but for the new GPCP V3.2, with the time period of the GPCP maps and climate model results shortened to overlap exactly (1983–2014) in three of the panels, with a fourth panel (top right) showing the entire GPCP V3.2 record (as in
Figure 5).
For this analysis, we utilized the monthly calculated precipitation from the climate model outputs [
12], with one realization (the first) chosen from each. The models used are:
(1) the coupled ocean-atmosphere, full radiative forcing runs (CMIP6-hist; here referred to as CMIP6, 28 models) driven by natural (solar variation, volcanic eruptions, etc.) and anthropogenic (GHG and aerosols) radiative forcings, and (2) the atmosphere-only (AMIP6, 28 models) simulations from the CMIP6 models forced by observed SST and sea ice extent, along with the radiative forcings used in the CMIP6 historical full forcing experiments.
The results with the new GPCP V3.2 are very similar to that with V2.3 in the earlier paper [
11], and readers are referred to that paper for a detailed discussion. In brief, the trend patterns between
Figure 6a (GPCP) and 6c (AMIP) are broadly similar, despite the coarser resolution and multiple ensemble members producing smoother patterns. This similarity is not unexpected because the forcing from the observed SSTs helps to drive the large-scale pattern and intensity of the resulting precipitation features. However, there are differences, for example, along the central-eastern Pacific ITCZ, where the distinct, but narrow, GPCP feature of increase becomes near zero or even a decrease in AMIP6. However, the precipitation trends in the CMIP6 ensemble (
Figure 6d) tend to show broader and weaker features from those in the GPCP. However, regional similarities between CMIP6-hist and either GPCP or AMIP6 results can readily be seen in the deep tropics and over the mid–high latitudes. For example, all of the trend maps have positive trends along the Pacific ITCZ and SPCZ, in the Indian Ocean, and along the Atlantic ITCZ extending across part of the West African continent. Subtropical drying and high-latitude wetting are generally seen as well in all three. These general similarities indicate the climate-change (GHG) effect on precipitation change in these regions. It is also important to note that the magnitudes of regional trends in the CMIP6 results are generally smaller than those in either the GPCP or AMIP6 (a different scale is used in the CMIP6 panel). As the global precipitation observed record (e.g., GPCP) becomes longer, the effects of inter-annual and inter-decadal variations should become more subdued and the effects of long-term changes (e.g., GHG effects) should become more obvious and can be a better tool with which to compare to the CMIP6-hist results which naturally smooth out those shorter term variations.
3.4. Global Total Precipitation
Global total precipitation has remained nearly steady over the GPCP era, with only a small 1.5%/K rise (not statistically significant) compared to global surface temperature, and similar to climate models [
11]. But, the annual global precipitation mean value does fluctuate, mainly due to ENSO, with years dominated by El Nino conditions having a positive global anomaly and La Nina years having the opposite. With El Nino dominating during 2023, the global total is 2.82 mm day
−1, just higher than (+0.01 mm day
−1) the long-term mean (2.81 mm day
−1). For the ocean, the mean for 2023 is 3.13 mm day
−1 (a +0.05 anomaly) and the land mean is 2.10 mm day
−1 (a −0.08 anomaly). This land–ocean offset is also characteristic of El Nino conditions.
Figure 7 is a plot of annual global total precipitation anomalies from 1983 to 2023. The variations have about a 3% range around the mean of 2.81 mm day
−1 and there is a slight upward trend (not statistically significant) as previously mentioned, which may be more of an effect of a shift in the Pacific Decadal Oscillation (PDO) around 1998 [
11]. The peaks and valleys in the curve are closely associated with ENSO, with letters designating years or times with either El Nino or La Nina conditions. The minimum for 1991, the record low for this span of time, is related not to a La Nina, but to the effect of the Pinatubo volcano negatively affecting solar radiance at the surface and causing lower than normal surface temperatures and ocean evaporation and atmospheric convection [
10].
3.6. Variations in Two Latitude Bands
Examination of the observed trend maps in
Figure 5 and
Figure 6 indicates the ITCZ zone (0–10° N) is dominated by upward trends, over both land and ocean regions. In examining the 2023 results, a key finding was the record-setting mean annual value for the 0–10° N zone (land plus ocean) as seen in
Figure 9. In addition, the latitude band 30–40° N (land plus ocean) shows a relatively low mean value, indicating a very strong gradient in mean rainfall between these two latitude bands. The first zone is along the ITCZ in the deep tropics and the second in the dry northern hemisphere subtropics. Looking at the entire record (1983–2023) for these zones indicates a definite wet-getting-wetter and dry-getting-drier type of climate trend at a large scale as the mean values in these two bands are different by about a factor of two, with the larger value at the lower latitude. The year 2023 obviously contributes to this trend, and indeed sets the record by a significant amount for the ITCZ latitude zone, likely an effect of the added contribution of the ongoing El Nino. Indeed, the effect of ENSO is noticeable, with maxima associated with the El Nino years (e.g., 1998, 2015, 2023) and relative minima with La Nina periods (e.g., 1998–2000, 2020–2022) in the figure. The subtropical band shows a negative trend over the period shown, with 2022 and 2023 showing the lowest values in recent years, giving a record value of the gradient between the two bands as seen in the figure.