Many recent studies have aimed to better understand changes in the characteristics of the intertropical convergence zone (ITCZ), including ITCZ location, width, and precipitation intensity. However, very few studies have looked at the relationship between characteristics of convection within the ITCZ and ITCZ width. The present work uses information from an ITCZ identification database and Tropical Rainfall Measuring Mission (TRMM) precipitation feature (PF) database to quantify variations in convective characteristics across the ITCZ in the Pacific Ocean. Data are partitioned into wide and narrow ITCZ regimes to quantify differences in convection between different ITCZ regimes. Under the wide regime, convection deeper than 5 km, with areas greater than 100 km2, or stratiform rain fractions greater than 0.5 is, on average, 24%, 23%, and 12% more frequent, respectively. In the narrow regime, the signal is reversed, with average increases in the frequency of convection with heights below 5 km, areas less than 100 km2, or stratiform rain fractions less than 0.5 of 15%, 4%, and 6%, respectively. Positive and negative anomalies in columnar water vapor (CWV) and sea surface temperature (SST) across the ITCZ are observed in the wide and narrow regimes, respectively. There is also a strong positive correlation between an El Niño–Southern Oscillation (ENSO) index and ITCZ width anomalies, with wide (narrow) ITCZs occurring during warm (cold) phases of ENSO. This implies that the strengthening and weakening of the Walker circulation associated with ENSO may play a role in modulating the convective populations that contribute to the Pacific ITCZ width variations.
The accurate prediction of changes in the hydrologic cycle is of great importance as water is essential for life. Shifts in the locations of the world’s deserts and rain belts could spell disaster through loss of crops, property, and even life. In the tropics and extratropics, changes in the hydrologic cycle can broadly be linked to changes in the Hadley and Walker circulations. Numerous studies have aimed to quantify changes in the Hadley circulation in a warming climate using data from reanalyses (e.g., Mitas and Clement 2005; Stachnik and Schumacher 2011; Nguyen et al. 2013), general circulation models (e.g., Mitas and Clement 2006; Lu et al. 2007; Lau and Kim 2015; Su et al. 2014), and observations (e.g., Hu and Fu 2007; Seidel et al. 2008; Hu et al. 2011). There is disagreement between studies as to how the strength of the Hadley circulation has changed in recent decades (Hu et al. 2018); however, the general consensus is that the Hadley circulation has expanded poleward. While studies of changes in the future climate generally agree that the Hadley circulation will become weaker, Su et al. (2014) noted that the circulation goes through complex structure changes as the climate warms. Similar studies of the Walker circulation also disagree on the change of the circulation’s strength; some found weakening and a westward shift (e.g., Tanaka et al. 2004; Vecchi et al. 2006; Power and Smith 2007; Schwendike et al. 2015), while others found strengthening (e.g., Meng et al. 2012; L’Heureux et al. 2013; Sohn et al. 2013). As the intertropical convergence zone (ITCZ) is the main driver of the Hadley circulation and influences the Walker circulation, changes in the intensity of convection within the ITCZ impact both of these circulations (Hack et al. 1989; Hou and Lindzen 1992; Dodd and James 1997; Webster 2004). Therefore, it is important to understand the link between broader ITCZ characteristics and the convective systems within the ITCZ.
One of the first major studies of the ITCZ’s climatological location and seasonal migration used observations of highly reflective clouds to identify the ITCZ (Waliser and Gautier 1993), while more recent studies have applied statistical models to observations (Bain et al. 2011) and thresholding techniques to reanalysis data (Berry and Reeder 2014) to study the ITCZ. Building off the methods of Berry and Reeder (2014), Wodzicki and Rapp (2016) quantified the ITCZ width and precipitation intensity and determined that the ITCZ has been narrowing and intensifying over the past 30+ years, possibly due to an increase in the frequency of midtropospheric dry layers (Bartos et al. 2018). Their findings are in line with other observational studies that noted long-term increases in tropical precipitation rate, mainly in the ITCZ region (Lau and Wu 2007; Zhou et al. 2011), and lend support to climate model predictions of further narrowing and intensification in the future (Lau et al. 2013; Lau and Kim 2015; Su et al. 2017, 2019). While the aforementioned studies focused on long-term trends in ITCZ characteristics, many studies have also noted a link between convective systems and ITCZ width variations at other time scales, from synoptic to interseasonal.
At synoptic time scales, Straub and Kiladis (2002) and Serra and Houze (2002) found that as Kelvin waves passed over a region, convection rapidly initiated and organized along the central axis of the ITCZ. This increase in organized convection widened the ITCZ, with the increase in ITCZ width propagating with convection associated with the Kelvin waves as they moved across the ocean basin. Serra and Houze (2002) also noted that the passage of Kelvin waves initiated hurricane development after which the ITCZ tends to completely break down, with deep convection disappearing and ITCZ width decreasing to near zero. A more recent study by Dias and Pauluis (2011) found a relationship between ITCZ location and width and the speed of convectively coupled Kelvin wave (CCKWs). They suggest that the meridional circulation associated with the CCKWs modulates ITCZ width and precipitation, indicating a link between the broader ITCZ width and the characteristics of the convective systems within.
Dias and Pauluis (2011) also noted that the ITCZ is abnormally wide during El Niño events in the central Pacific (180°–130°W), consistent with the observational findings of Wodzicki and Rapp (2016, 160°E–160°W). Simple Walker circulation models (e.g., Bretherton and Sobel 2002) also show a wider zone of convection when the sea surface temperature (SST) gradient across the Walker circulation weakens during El Niño. Insomuch as the ITCZ tends to be wide during El Niño and narrow during La Niña, some studies have indirectly looked at variations in characteristics of convection in different ITCZ width regimes. Masunaga et al. (2005) used Tropical Rainfall Measuring Mission (TRMM) satellite data to show that during El Niño events, deep stratiform and convective systems became much larger and more frequent, taking the place of shallow convection, when compared to La Niña. Henderson et al. (2018) found very similar changes from deep isolated systems in the La Niña phase to large, organized systems with increased stratiform rain area during El Niño. This is further supported by Stephens et al. (2018), who found evidence for the Bjerknes feedback in observations that show large positive latent and radiative heating perturbations with super-Clausius–Clapeyron precipitation responses in the warming, moistening ITCZ region during El Niño. However, it remains unclear how the population and character of convective clouds within the ITCZ vary to produce the observed precipitation and heating rate perturbations that feedback on these large-scale circulations as similar radiative and latent heating perturbations could come from very different cloud populations. There are some indications that the character of convective systems in the tropics may be shifting as the convective zones narrow at longer (decadal) time scales (Tan et al. 2015), but this has not been specifically analyzed in the context of expansion and contraction of the ITCZ at shorter (annual or seasonal) time scales.
The aim of the present study is to better understand the relationship between the variations in large-scale ITCZ width and characteristics of convection [e.g., rain rate (RR), maximum height, and stratiform/convective partitioning]. This will be done through the analysis of convective features located within the ITCZ based on the Pacific ITCZ identifications from Wodzicki and Rapp (2016). While previous studies have focused on long-term changes in ITCZ precipitation intensity and location, the relatively short TRMM data record limits the present study to shorter time scales. Thus, features in two different ITCZ width regimes (wide and narrow based on the upper and lower quartiles of the width distribution, respectively) are compared to understand the relationship between the distribution of convection characteristics and variations in ITCZ width.
2. Data and methods
Wodzicki and Rapp (2016) created an ITCZ climatology that provides information about the location, width, and RRs within the Pacific ITCZ (160°E–100°W) on a monthly-mean time scale. To identify the ITCZ they used monthly 1000–850-hPa layer mean u- and υ-wind components to compute divergence, gradient of divergence, and Laplacian of divergence. Locations where the gradient of divergence equaled zero were taken as the first-guess ITCZ center, with the divergence and Laplacian of divergence fields used to mask out regions of divergence and relative minima in the divergence field, respectively. The 850-hPa wet-bulb potential temperature was used as a final mask, limiting identifications to tropical regions. After the ITCZ center was identified, ITCZ boundaries were located by iterating from the ITCZ center to the north and south to find the latitude where RR fell below a threshold of 2.5 mm day−1. While their work focused on long-term trends in ITCZ characteristics using long time series Global Precipitation Climatology Project (GPCP) RRs (Adler et al. 2003), the present study utilizes TRMM Microwave Imager (TMI) RRs for boundary identifications. The two major benefits of using TMI-based ITCZ identification over GPCP are 1) the TMI ITCZ climatology is already available from Wodzicki and Rapp (2016) and 2) the TMI sensor is on the TRMM satellite with the precipitation radar (PR), which is used to define convective features.
The TRMM satellite was launched in 1997 to further the understanding of precipitation in the tropics (Simpson et al. 1988; Kummerow et al. 1998). As the first satellite to feature a PR, TRMM provided invaluable information about internal precipitation structures, allowing for improved characterizations of precipitating convection in the tropics. However, with over 16 years of data, studying the distributions and morphology of precipitating systems using pixel-level data can be cumbersome. The work of Nesbitt et al. (2000) and Liu et al. (2008) greatly reduced data processing requirements through the development of a precipitation feature (PF) database. The current study uses their radar PF definition, defined as a single or contiguous group of PR pixels that have RRs greater than 0 mm h−1, because the convective characteristics used here to quantify convective intensity (i.e., maximum height reached by the PF, RR, area, and stratiform and convective partitioning) are all derived from the PR. It is worth noting that the spatial and temporal resolutions of radar PFs are highly variable as they are limited by the presence of rain and the spatial and temporal resolutions of TRMM. The relatively narrow swath width (~215 km) of TRMM also limits the maximum size of PFs that can be sampled; however, Nesbitt et al. (2000) found that only 17% of PFs are affected and noted that while this does cause some truncation in the area distribution of PFs, other characteristics remain unbiased. As convection can be greatly influenced by its environment (Derbyshire et al. 2004; Rapp et al. 2011; Hohenegger and Stevens 2013), it is advantageous to consider changes in convective characteristics with changes in the ITCZ environment.
To do this, PFs are matched to Remote Sensing Systems (RSS) TMI version 7 (Wentz 1997; Hilburn and Wentz 2008) data on a 0.25° × 0.25° grid at daily resolution. PFs are matched to the closest possible TMI time and the nearest grid box using a nearest neighbor method based on the center latitude and longitude of an ellipse fitted to the PF (Liu 2013). Using the monthly ITCZ center and boundary locations, each PF and TMI grid box are assigned an ITCZ flag and a distance from the ITCZ center; PFs within the ITCZ are hereafter referred to as ITCZ PFs. The variables of interest in the present study are PF area, RR, stratiform fraction, and maximum height, and TMI columnar water vapor (CWV) and SST. PF area is calculated by multiplying the number of pixels in the feature by the size of each pixel and the RR is average RR over the entire feature. To reduce bias, PFs with fewer than four pixels are excluded from the analysis as these very small, very frequent features can introduce noise (Nesbitt et al. 2000).
As previously discussed, modeling studies suggest a link between the width of the ITCZ and the characteristics of convection within the ITCZ (Chou and Neelin 2004; Neggers et al. 2007). Thus, we partition our data into wide and narrow ITCZ regimes where a wide (narrow) ITCZ is any ITCZ that has a deseasonalized zonal-mean width anomaly (%) above (below) the 75th (25th) percentile of the ITCZ width anomaly distribution for the 17-yr period from December 1997 through September 2014. All analysis is also performed across the bulk of the Pacific basin from 160°E to 100°W. The far eastern Pacific and far western Pacific are excluded to reduce the influence of spurious ITCZ identification in the North American monsoon region and the South Pacific convergence zone (SPCZ), respectively. While continental areas may be present in the northern and southern regions of the domain, any PFs over such areas are excluded so that only PFs over the ocean are considered.
Using the matched PF database, monthly zonal median values for PF area, maximum height, and RR are computed for 2.5° bins centered on the ITCZ center. Median values are used as there tends to be many small and very few large PFs, which skews the mean values. These data are then deseasonalized to calculate percent anomalies. Using the deseasonalized anomalies from months above the upper and below the lower quartiles of the ITCZ width distribution, the average deviations from the mean state of the PF characteristics are determined. The significance of anomalies throughout the analysis are determined using a simple bootstrapping method wherein all deseasonalized anomalies are randomly resampled, with replacement, 10 000 times. A sampling size of 50 is used because that is roughly one-quarter the number of months analyzed, giving a sample size equal to the number of months above (below) the upper (lower) quartile of the ITCZ width distribution. The average of each resample is computed, giving 10 000 realizations of the mean anomalies. An anomaly is determined to be significant if it falls in the top or bottom 2.5% of the bootstrapped distribution, giving a two-tailed test at the 95% confidence level.
a. PF populations
To gain a general understanding of the changes in convection in different ITCZ width regimes, Fig. 1 shows the average zonal anomalies with wide ITCZ months (above upper quartile) in red and narrow ITCZ months (below lower quartile) in blue. Anomalies that are significantly different from the mean at the 95% level are indicated with an “X”. From Figs. 1a and 1b, PFs tend to be larger and deeper when the ITCZ is wide, with maximum heights 5%–14% higher than average across the ITCZ. RR shows a more interesting picture (Fig. 1c), with wide months having below average RRs across the ITCZ region while narrow months have above average RRs. While this seems at odds with previous studies that have shown RRs increasing as convection becomes larger and deeper (DeMott and Rutledge 1998; Nesbitt et al. 2006), this result is due to the use of conditional PF-averaged RR, not area-averaged RR, in the present study. As PFs become larger they will contain larger stratiform areas that tend to have a much lower instantaneous RR than small cumulus dominated by convective RRs. This acts to suppress the storm-averaged RR, while area-averaged RR would still be above normal.
To gain a better sense of how the PF population differs between the narrow and wide ITCZ regimes, PFs are partitioned into cumulus, congestus, and cumulonimbus regimes, based on maximum height of the PF, using a slightly modified version of the definitions from Johnson et al. (1999) with bins of 0–5 km for cumulus, 5–10 km for congestus, and 10–20 km for cumulonimbus. Figure 2 shows the zonal distribution of clouds by fractional occurrence for cumulus, congestus, and cumulonimbus for narrow and wide months. It is worth noting that, on average, cumulus, congestus, and cumulonimbus clouds generate roughly 7%, 27%, and 67% of all rain, respectively, across the ITCZ. From this figure it is clear that most of the anomalies observed in Fig. 1 are due to differences in cumulus and congestus clouds, with cumulus (congestus) clouds occurring more frequently when the ITCZ is narrow (wide). Figure 2c shows that cumulonimbus are roughly 30%–50% more frequent in the wide regime than the narrow across the ITCZ; however, cumulonimbus account for a small percentage (<10%) of all clouds. What is perhaps more interesting is that there are roughly the same number of clouds across the ITCZ during wide and narrow months (not shown), which means that as the ITCZ narrows cumulonimbus clouds become less frequent and there is a shift from congestus to cumulus, indicating a shift to shallow, weaker convection. Along with this shift in cloud frequency is a shift in the percent contribution to total rain in the wide (narrow) regime to 5% (10%) for cumulus, 24% (31%) for congestus, and 71% (59%) for cumulonimbus.
b. PF convection characteristics
To further study the changes in PF characteristics in different ITCZ width regimes, joint histograms of PF characteristics are used. Figures 3 and 4 show joint histograms for PF maximum height and area, respectively. To create these figures, monthly joint histograms are generated for the entire TRMM period (December 1997 through September 2014), showing the frequency of PFs with a given characteristic (e.g., maximum height of 5 km) at a given distance from the ITCZ center (e.g., ±1.25°). Each monthly histogram is then scaled to show the percentage of PFs with a given attribute. Figure 3a shows the average distribution for all months where, as an example, 10%–15% of PFs that are ±1.25° from the ITCZ center have maximum heights of 5–5.5 km. The monthly joint histograms are then deseasonalized and converted to percent anomalies using data from the full TRMM period. These anomalies are then averaged for months that fall above the upper (wide) and below the lower (narrow) quartiles of the ITCZ width distribution, with the average anomalies shown in Figs. 3b and 4b and in Figs 3c and 4c, respectively. Vertical gray lines show the average locations of the ITCZ boundaries over the respective months of each panel and stippling in Figs 3b,c and 4b,c indicate significant departures from the mean state at the 95% level. Note that in Fig. 4, only data before August 2001 are included in the smallest area bin (~55–81 km2) when computing means and anomalies because of the difference in pre- and postboost pixel sizes.
From Fig. 3a it is clear that the majority of PFs have heights between 2 and 8 km, with the frequency of deeper storms (i.e., heights greater than 8 km) increasing slightly toward the center of the ITCZ. On the northern edge of the ITCZ the distribution shifts to shallower PFs (i.e., heights less than 5 km), with 20%–30% of PFs having heights around 3 km at 10°N of the ITCZ center. This is indicative of shallow cumulus in the subtropics; the ITCZ is typically located around 8°N, placing the PFs around 15°–20°N. At the southern edge of the ITCZ, the picture is similar to that north of the ITCZ; however, PFs with heights greater than 6 km become more frequent, likely due to the SPCZ, or double ITCZ.
Looking at the anomalies in PF maximum height distribution for wide ITCZs (Fig. 3b) PFs with heights less than 4 km become less frequent across the domain, with increases in PFs taller than 4 km. Note that some of the large increases occur near the southern boundary of the ITCZ. This suggests that when the ITCZ is wide, shallower convection is less common within the ITCZ and deep convection is more common, especially near the edges. For narrow ITCZs (Fig. 3c), PFs with heights below 4 km become much more frequent across the domain, with all PFs with heights greater than 4 km becoming less frequent. This indicates a general shift toward shallower convection when the ITCZ is narrow. Note that most of the bins within the ITCZ are stippled, indicating high confidence in these changes. However, outside of the ITCZ confidence diminishes (no stippling) suggesting a large spread in the anomalies observed.
Focusing now on variability in PF frequency based on PF area, Fig. 4 shows the joint histograms of PF area and distance from the ITCZ center. While the orbital boost of TRMM did cause a reduction in the frequency of very light rain detected by the PR (Liu et al. 2012), RRs greater than 1 mm h−1 are not significantly affected. As the current study neglects very small PFs, many PFs with very low RRs have already been excluded. PFs with RRs less than 1 mm h−1 actually make up a larger percentage of PFs after the boost (~20%) than before the boost (~18%) and so the impact of the orbital boost is small. With PFs that have areas greater than 1000 km2 making up a small portion of the total distribution (~20%), small changes in the frequency of larger PFs lead to large percent changes; for example, if a PF of a given area appears only once in a given month’s climatology but twice when the ITCZ is wide, a 100% increase in frequency will be observed.
Figure 4b shows that when the ITCZ is wide, PFs with areas greater than ~100 km2 become more frequent while PFs with areas less than ~100 km2 become less frequent. Note that because the majority of PFs have areas less than 500 km2 a small percentage change in frequency can equate to a large number of PFs. From these anomalies a shift from cumulus (small and shallow) to congestus (moderately large and deep) and cumulonimbus (large and deep) features is apparent; however, the increases in the frequency of PFs with areas between 100 and 1000 km2 are not significant, indicating a large amount of variability in the frequency of PFs of this size. In contrast to the wide ITCZs, narrow ITCZs (Fig. 4c) show a reduction in PFs with areas greater than ~100 km2, with increases in smaller PFs. This signifies a distinct shift toward smaller PFs in narrow ITCZs. To understand how PFs grow in the wide ITCZ regime, joint histograms of stratiform area fraction are created.
Stratiform area fraction is defined here as the number of PR pixels within a PF that are identified as stratiform rain by the 2A23 algorithm (Steiner et al. 1995; Awaka 1998) divided by the total number of PR pixels in the feature. Figure 5a shows the climatology of joint histograms of stratiform area fraction and distance from ITCZ center. PFs with very low stratiform area (<5%) account for over 50% of all PFs across the entire ITCZ. This is expected as congestus and cumulus type systems (i.e., convection that has little to no stratiform component) account for nearly all PFs (Fig. 2). As expected based on the shifts shown in PF area under wide ITCZs (Fig. 4b), Fig. 5b shows a shift toward PFs with predominantly stratiform rain when the ITCZ is wide, with Fig. 5c showing a shift toward predominantly convective rain when narrow. While it is not surprising that the stratiform area increases as PFs get larger, it is not immediately obvious why a wider ITCZ should be associated with larger, more organized individual storms.
c. Environmental influences on PF populations
Recent studies have shown a strong relationship between thermodynamics and precipitation over the ocean, with stratiform rain intensity and area being highly sensitive to water vapor above a critical value (Bretherton et al. 2004; Ahmed and Schumacher 2015). Therefore, it is possible that these different ITCZ regimes correspond to different large-scale thermodynamic variability associated with El Niño–Southern Oscillation (ENSO) or other large-scale drivers. As SST, CWV, and convection are all interconnected (Graham and Barnett 1987; Zhang 1993), TMI SST and CWV data are compared across the ITCZ for anomalously wide and narrow months.
All TMI grid boxes that contain at least one PF are used to create zonal median plots of SST and CWV for wide and narrow ITCZs (Fig. 6). While the differences are not large, both CWV and SST are significantly higher than average (at the 95% level) across the ITCZ region when the ITCZ is wide. Bretherton et al. (2004, their Fig. 2a) shows that precipitation rates begin to pickup quickly above 50-mm water vapor path, with rapid increases occurring above 55 mm. While Ahmed and Schumacher (2015) used column saturation fraction, a similar increase in stratiform RR was observed for very moist columns. Ahmed and Schumacher (2015) also noted that RR increases driven by changes in stratiform area were more pronounced than precipitation intensity changes. Thus, the changes in the morphology of PFs under the wide ITCZ regime are likely a result of increased moisture and SST over the tropics, either through increased evaporation locally or increased moisture convergence from remote sources. It is worth noting that near the northern boundary of the ITCZ CWV decreases rapidly, falling below the 48-mm threshold defining the moist tropics (Mapes et al. 2018) north of the ITCZ. However, at the southern boundary, CWV does not fall below 50 mm, which we attribute to SPCZ influence in the central Pacific region. With ENSO being a major source of both SST and CWV variability in the Pacific (Rasmusson and Carpenter 1982; Trenberth et al. 2005), the relationship between ENSO on ITCZ width is examined.
Using the multivariate ENSO index (MEI; Wolter and Timlin 1993, 1998), the influence of ENSO on ITCZ width and PFs is determined by regressing MEI against the ITCZ width anomalies. As the MEI is a 2-month index, the value for a single month is computed by averaging the two surrounding 2-month values; that is, the MEI value for December is the average of the November/December and December/January values. Figure 7 indicates a strong relationship between monthly ITCZ width anomalies and ENSO, with a correlation coefficient of 0.63. Defining El Niño (La Niña) events as any month where the MEI is greater than 0.5 (less than −0.5) shows that 41 of the 50 anomalously wide ITCZ months occurred during an El Niño with 36 of the 50 anomalously narrow ITCZ months during a La Niña. However, we note that the patterns shown above also hold when we attempt to mitigate the ENSO influence by excluding ENSO events using the MEI thresholds defined above; general patterns remain similar, although the magnitude and significance of anomalies is greatly reduced.
4. Summary and discussion
TRMM PFs are used to study changes in the characteristics of convection within the ITCZ in the Pacific Ocean. Using the ITCZ climatology of Wodzicki and Rapp (2016), monthly ITCZ widths are partitioned into anomalously wide and narrow regimes, with the wide (narrow) regime consisting of months where percent anomalies of ITCZ width are above the upper (below the lower) quartile of the ITCZ width distribution.
PFs tend to be larger and deeper when the ITCZ is wide, with large increases in stratiform areas. While PF RRs are lower when the ITCZ is wide, this was determined to be a result of using conditional-average PF RR because PFs with large areas consist of mainly weakly raining stratiform clouds, which act to suppress storm-average RR. The large increases in PF and stratiform area in the wide ITCZ regime may be linked to deep convection changes associated with SST and CWV increases based on a strong correlation between ITCZ width and the MEI and the anomalously high (low) SSTs and CWV in the wide (narrow) ITCZ width regime. This indicates a strong link between ITCZ width and PF characteristics to ENSO and the Walker circulation. While this may seem to be discrepant with model studies of the Walker circulation indicating that convection should be more intense during the contraction of the deep convection area (e.g., Bretherton and Sobel 2002), this analysis composites convection across the full longitudinal extent of the Pacific ITCZ. When the east–west temperature gradient is strong during La Niña, the ITCZ is narrow and the deeper, more intense convection is confined to a small portion of the averaging domain, so the composite convection is weaker when averaged across the longitudinal ITCZ extent. When the ITCZ is wide during El Niño as the east–west temperature gradient breaks down, the deep convection covers a larger fractional area of the ITCZ averaging domain. Studies of the relation between the strength of the Hadley circulation and the phases of ENSO also lend support to the current study’s findings, with many studies (e.g., Oort and Yienger 1996; Stachnik and Schumacher 2011; Nguyen et al. 2013; Hu et al. 2018) showing an anticorrelation between the Hadley circulation and ENSO. This means that under El Niño (La Niña), when the ITCZ is wide (narrow), the Hadley circulation is narrow (wide).
The observed shift from shallow to deep convection between La Niña and El Niño coupled with the modulation of the Walker circulation also provides a mechanism for the large latent and radiative heating perturbations shown in models and observations (Rädel et al. 2016; Stephens et al. 2018). The increase in upper-level cloud is the result of the shift from congestus across the bulk of the ITCZ in the narrow regime to larger systems with more widespread stratiform areas in the wide ITCZ regime. The expansion of more organized systems with large stratiform rain regions across the ITCZ during El Niño provide the large positive latent heating anomalies in the warming and moistening regions of the tropics that can feedback on the large-scale circulation.
It is clear from this analysis that variations in ITCZ width and PFs at interseasonal and interannual time scales may not be a good proxy for examining the relationship between convection characteristics and long-term ITCZ width variations due to changes in the Hadley circulation. This is likely due to the differences in the spatial and temporal scales as well as the complex balance of net energy input, atmospheric energy transport, ENSO, and Hadley and Walker circulation influences that drive changes in the Pacific ITCZ at different time scales (Adam et al. 2016).
More work is needed to unravel the connections between the convection distribution and the large-scale ITCZ state. Further efforts will also be focused on determining a proxy for the changes in convective characteristics observed in the present study that can be applied to long-time series reanalysis and model datasets to determine whether the relationship between the large-scale ITCZ characteristics and the convective systems within the ITCZ hold at longer time scales.
This research was partially supported by NASA Grants NNX13AG91G and NNX15AD13G. K. Wodzicki also acknowledges support for this work from the Texas A&M Hagler Institute for Advanced Study. The Pacific ITCZ mask dataset is available from the Texas Data Digital Repository at https://doi.org/10.18738/T8/T5PH8N and the TRMM Precipitation Feature Database is available at http://atmos.tamucc.edu/trmm/. TMI data are produced by Remote Sensing Systems and sponsored by the NASA Earth Science MEaSUREs DISCOVER Project. Data are available at www.remss.com.