An Urban Heat Island Tale of Two Cities: New York City vs. Los Angeles

November 13th, 2026

John Christy and I just submitted a paper for publication in the AMS Journal of Applied Meteorology and Climatology called “Average Summer Heat Island Effects Relative to Landsat Impervious Surface Area for 50 Major U.S. Cities, 1985-2025“. You can tell what it’s about from the title.

As you might recall, a couple of years ago we published a paper relating GHCN station air temperatures to population density, and I made maps of the global distributions of UHI warming based upon those calculations.

But population density is not the best choice as a proxy for urbanization when it comes to the urban heat island (UHI) effect. The reason I used it is that there are global gridpoint datasets of population density going back to at least 1800, and how much UHI warming there has been in cities should be compared to what temperatures would be if the city was not there. The very first published study of the UHI effect was in 1818 by Luke Howard for London.

So, a couple years ago, I started a new analysis using Landsat satellite-based impervious surface area (ISA), which should be the single most direct physical influence on UHI warming. ISA measures the spatial coverage (in percent) of roads, parking lots, roofs, and many more types of human-built structures and modified soil surfaces (e.g. railways). The spatial resolution is 30×30 meters, and the dataset begins in 1985, now updated through 2025.

Methodology

I analyzed all of the June, July, and August GHCN station data within 30 to 100 km of the center of the 50 most populous Metropolitan Statistical Areas (MSAs) used by the U.S. Census Bureau. The following image shows those station locations.

This was a tedious, time-consuming process, partly because I also wanted to see if the UHI effect was magnified in these cities during excessively hot weather (warmer than the 97th percentile threshold temperature in Tmax). Determining that threshold from many stations in each of the 50 MSAs (which averaged 27 stations) was not straightforward.

I also simplified the methodology compared to our previous population-density related work: the example plots that follow are based upon how much each GHCN station’s daily Tmax or Tmin temperature departs from the average of all stations within the MSA (rural, suburban, and urban). This is basically what many of us experience on a daily basis as we commute from more rural locations to more urban locations, or drive across the city. Those individual station departures from the MSA-wide multi-station averages were then related to the impervious surface area centered on that GHCN station at 7 different averaging spatial resolutions (from 30×30 m to 10×10 km). The ISA averaging resolution producing the greatest magnitude correlation (positive or negative) was then chosen for further analysis.

The First City: NYC and its Strong Nighttime Warming, But Slight Daytime Cooling

New York City skyline at dusk. Photo by Bruce Emmerling.

It was quite a coincidence that two of the most extreme, and yet somewhat opposite, examples came from the two most populous MSAs: New York City and Los Angeles. The following plot shows how the New York City MSA GHCN station temperatures related to their impervious surface area.

Fig. 1. New York City Metropolitan Statistical Area GHCN station daily-average summertime temperature departures from the average of all other stations, related to Landsat-based impervious surface area (ISA) at the indicated ISA spatial averaging resolutions centered on each GHCN station. Panel (a) is for Tmin on non-excessive heat days, (b) is for Tmin on excessive heat days, (c) is for Tmax on non-excessive heat days, and (d) is for Tmax on excessive heat days. The linear regression-based change in temperature per 100% ISA coverage is shown in red in the lower right of each panel, corresponding to the dashed red regression line. The dotted blue curved lines are 2nd order polynomial regression fits, just for reference in case there is some evidence of a nonlinearity.

As in virtually all of the 50 cities I analyzed, there was quite a bit of scatter in the resulting plots. This is because there are other influences I could not quantify, such as local spurious heat sources (brick walls, heat pumps, etc.), local microclimate effects, the use of only one “best” spatial averaging resolution out of seven, and station temperature sensor biases. For stations with substantial differences in elevation, I made lapse rate adjustments based upon regressions for that MSA.

For daily minimum temperature (Tmin) on non-excessive heat days (Fig. 1a) the average warming sensitivity to ISA across all stations was +3.1 deg. C per 100% ISA coverage. LaGuardia Airport looks like it has the most warming for its ISA coverage (over 3 deg. C at ~45% ISA coverage over a 2×2 km area). Central Park is also quite warm, as is Brooklyn and Bronx.

During excessively hot days (exceeding the 97th percentile threshold in Tmax for that station’s entire period of record) the UHI warming was amplified somewhat, increasing from +3.1 to +3.9 deg. C per 100% ISA coverage.

But for Tmax on non-excessive heat days (Fig. 1, panel c) there is a slight urban cool island effect (yes, it’s a real thing), at -0.5 deg. C per 100% ISA coverage. The daytime cool island effect is due to the same reason why the nights are so warm in urban areas: the much higher heat storage capacity of impervious surfaces such as roads and parking lots causes a time delay in the air temperature response compared to natural soil surfaces or vegetation. Just as it takes time overnight for roads and parking lots to release their extra heat energy, it takes time for those surfaces to heat up during the day from solar energy input after cooling off overnight. This creates a slight cooling effect during the day relative to rural areas (even though both obviously heat up during the day). But that effect seems to disappear on excessively hot days (Fig. 1d) where there is an average warming of +2.1 deg. C per 100% ISA coverage, albeit with a lot of variation between stations (low explained variance in the regessions, R-squared).

The relationships shown in Fig. 1 are strictly based upon spatial differences between stations, averaged across all summers, 1985-2025. A natural question is, how has the UHI effect changed over those years? While not in the paper, I’ve just started to look at this. In Fig. 2, I show how the +3.1 deg. C multi-station average Tmin warming per 100% ISA, when applied to the yearly average ISA in every county contained in that metropolitan statistical area, results in an estimate of how the Tmin warming has increased in time over the 1985 to 2025 period.

Fig. 2. Increases in the New York City Tmin UHI warming effect relative to 1985, for individual counties in the NYC MSA, based upon the 1985-2025 average GHCN stations’ relationship to Landsat impervious surface area multiplied by the increase in ISA during every individual year, 1985 through 2025.

As can be seen in Fig. 2, all 22 counties in the New York City MSA experienced increasing impervious surface area, which then translates into increases in UHI warming. It should be emphasized that these calculations are based upon a single Tmin-vs-ISA relationship (+3.1 deg. C per 100% ISA) representing an average relationship across all GHCN stations (Fig. 1a). There is no way to know how accurate the individual county UHI warming amounts shown in Fig. 2 are.

The thick purple curve in Fig. 2 is the population-weighted average UHI warming increase across all counties. It is not very large: about +0.1 deg. C across 40 years, which is only +0.025 C per decade. So, while the UHI effect in NYC is quite large (+3 to +4 deg. C at several GHCN stations), since 1985 the increase in UHI has been rather weak, at least using the small increases in impervious surface area coverage as a proxy for increased urbanization. Other potential influences (e.g. increased localized spurious heat produced by more traffic and air conditioning) are not accounted for.

The Second City: Could Los Angeles Daytime Temperatures Decrease with Warming?

The Los Angeles skyline at dawn. Photo by mjhbower on flickr.com.

The second most populous U.S. MSA, Los Angeles, shows some stark differences compared to New York City (Fig. 3).

Fig. 3. As in Fig. 1, but for Los Angeles.

The biggest difference with New York City is in the daytime maximum temperature (Tmax). In Fig 3d we see see very strong cooling of the urban areas relative to the rural areas on excessively hot days, with an average relationship of -6.8 deg. C per 100% ISA coverage. This is likely because when hotter than normal summer air masses settle over the U.S. Southwest, the daytime thermal low pressure which forms inland, away from the Pacific Ocean, increases the strength of the sea breeze. As a result, the most urbanized locations (which tend to be nearer the coast) that are normally cooler anyway during the daytime (Fig. 3c) cool even more on days when the all-station average temperature across the Los Angeles metropolitan statistical area is well above the normal summer average temperature.

The other Pacific Coast cities I analyzed show similar results, although not quite as strong as L.A. Given this strong UHI-cooling effect from the sea breeze, there is no way to determine just how much daytime UHI warming (or cooling) is due to the presence of impervious surface area. The signal is confounded by the sea breeze since the more urbanized station locations tend to be closer to the sea breeze-influenced coast.

If you are confused at this point about how hotter weather causes the cooler temperatures shown in Fig. 3, remember that these plots (Figs. 1 and 3) are for how individual GHCN station’s temperatures depart from the all-station average temperatures. Thus, they are temperature differences, and say nothing about what the absolute temperatures are. So, while excessively hot summer days might actually be warmer than usual in downtown Los Angeles, there is a strong offsetting cooling effect from stronger sea breezes on those days compared to inland stations, which tend to be less urbanized.

On this point, I have looked at the official NOAA daytime Tmax temperatures for the summers in Los Angeles (LAX airport), and I do not see any evidence of this cooling effect; NOAA data shows the long-term warming at LAX has been at least as strong as at other southern California stations. I have no explanation for this discrepancy, other than the possibility that the homogenization process NOAA uses might make rather large trend adjustments to the LAX temperatures if the LAX trends depart from the surrounding stations farther from the coast. Homogenization is essentially a “voting” process and the few coastal GHCN stations might have gotten out-voted.

Regarding nighttime minimum temperatures (Tmin), Los Angeles shows a modest UHI warming effect during non-excessive heat days (+1.9 deg. C per 100% ISA, Fig. 3a), increasing to +2.3 deg. C on excessively hot days (Fig. 3d). Of course, the cooling effects of the sea breeze mostly disappear at night.

Thanks To Everyone, and The Future

The 50-city UHI study paper might be the last research article I publish if we are unsuccessful in getting a new contract to keep me employed. I have funding for several more months, then retirement might be a necessity.

As you already know, our “peers” who will review our current proposal don’t like us very much, and government funding of science contracts and grants is unavoidably political. The political winds in DC have just shifted strongly to the left, which will impact, directly or indirectly, congressional appropriations for what kinds of scientific research are deemed acceptable.

I’d like to thank everyone who has been contributing to this website on a monthly basis. I get an email every month for every contribution, along with the contributor’s name, and it always helps to brighten my day. The fact that people take the time to contribute means more to me than the actual $$ amount.

We will see how the funding situation sorts itself out in the coming months.

UAH v6.1 Global Temperature Update for October, 2026: +0.69 deg. C

November 3rd, 2026

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for October, 2026 was +0.69 deg. C departure from the 1991-2020 mean, up from the September, 2026 value of +0.61 deg. C.

The Version 6.1 global area-averaged linear temperature trend (January 1979 through October 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 34 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.79+1.02+0.57+1.20-0.20+0.40+1.11+0.97
2024Feb+0.87+0.94+0.81+1.16+1.30+0.86+1.15+2.45
2024Mar+0.88+0.95+0.80+1.25+0.21+1.05+1.33+1.12
2024Apr+0.94+1.11+0.76+1.14+0.85+0.88+0.53+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.77+0.60+0.84+1.36+0.64+0.90+0.19
2024July+0.73+0.85+0.61+0.96+0.43+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.74+1.36
2024Sep+0.80+1.04+0.57+0.81+1.31+1.48+0.97+2.40
2024Oct+0.74+0.89+0.60+0.63+1.89+0.81+1.08+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+0.99+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.53+1.65
2025Jan+0.45+0.69+0.20+0.23-1.07+0.74+0.47+1.04
2025Feb+0.50+0.55+0.45+0.25+1.03+2.10+0.86-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.44+0.55+0.30+0.14+0.75+0.98+0.81
2025June+0.47+0.48+0.47+0.29+0.80+0.05+0.38-0.22
2025July+0.36+0.49+0.23+0.44+0.32+0.40+0.52-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.52+0.55+0.49+0.35+0.37+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.66+2.59
2025Nov+0.43+0.58+0.27+0.24+1.31+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.18+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.38+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.46+0.60+0.58+0.21+0.34+0.10+0.21
2026June+0.46+0.54+0.38+0.57+0.64+1.01+0.38+0.99
2026July+0.48+0.68+0.27+0.85+1.14+0.53-0.22+0.78
2026Aug+0.67+0.76+0.59+0.90+0.59+0.80+0.39+0.71
2026Sep+0.61+0.78+0.44+0.89+1.32+0.80+1.13+0.99
2026Oct+0.69+0.82+0.57+0.88+2.13+1.18+0.46+0.80
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for Tropics, USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for October, 2026 and a more detailed analysis by John Christy, should be available within the next several days here.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Statosphere

UAH v6.1 Global Temperature Update for September, 2026: +0.61 deg. C

October 2nd, 2026

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for September, 2026 was +0.61 deg. C departure from the 1991-2020 mean, down from the August, 2026 value of +0.68 deg. C.

The Version 6.1 global area-averaged linear temperature trend (January 1979 through September 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 33 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.46+0.60+0.58+0.21+0.34+0.10+0.21
2026June+0.46+0.54+0.38+0.57+0.64+1.01+0.38+0.99
2026July+0.48+0.68+0.27+0.85+1.14+0.53-0.22+0.78
2026Aug+0.68+0.76+0.59+0.90+0.60+0.80+0.39+0.71
2026Sep+0.61+0.78+0.44+0.89+1.32+0.80+1.13+0.99
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for Tropics, USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for September, 2026 and a more detailed analysis by John Christy, should be available within the next several days here.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere

UAH v6.1 Global Temperature Update for August, 2026: +0.68 deg. C

September 2nd, 2026

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for August, 2026 was +0.68 deg. C departure from the 1991-2020 mean, up from the July, 2026 value of +0.48 deg. C. It appears the effects of the strengthening major El Nino event are beginning to appear in the global average tropospheric temperature, with an August temperature anomaly of +0.9 deg. C in the tropics. This month I’ve added a plot of tropical temperatures (below).

The Version 6.1 global area-averaged linear temperature trend (January 1979 through August 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 32 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.46+0.60+0.58+0.21+0.34+0.10+0.21
2026June+0.46+0.54+0.38+0.57+0.64+1.01+0.38+0.99
2026July+0.48+0.68+0.27+0.85+1.14+0.53-0.22+0.78
2026August+0.68+0.76+0.59+0.90+0.60+0.80+0.39+0.71
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for Tropics, USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for August, 2026 and a more detailed analysis by John Christy, should be available within the next several days here. John officially retired with emeritus professor status on July 1, 2026, and is now working as a part-time employee of UAH.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere

Record Low Lake Mead: “Millennium Drought” or Inevitable Result of Demand Exceeding Supply?

August 12th, 2026
Recent photo of Lake Mead behind Hoover Dam (Newsweek).

NOTE: I’ve made a couple of updates/clarifications below based upon comments on this post.

Lake Mead behind Hoover Dam is now within several feet of the lowest level at which turbine power generation must be greatly curtailed. Recent news articles often blame the cause on a “millennium drought” being experienced in the West. Of course, much of the western U.S. experiences drought conditions every summer, which is part of the normal climate there. Tens of millions of people like to live where it is sunny most of the year, and agriculture thrives where photosynthesis (lots of sunshine) is abundant… assuming enough water supply for irrigation.

Obviously, people need water, which is why virtually no one lives in the Sahara Desert. Add in the beauty of the Pacific Ocean, and it was inevitable that water demand would exceed supply. Even in 1922, before most people moved out west, the Colorado River Compact was negotiated to divide up the Colorado River’s water among seven southwestern states: California, Nevada, New Mexico, Arizona, Colorado, Utah, and Wyoming.

Most of the water in the Colorado River is from snowmelt in the Rocky Mountains. Most (50% to 70%) goes to agriculture. And, yes, the annual runoff flows into Lake Mead (which was filled after construction of Hoover Dam was mostly completed in 1935) have been below “normal” in recent years. But calling recent reduced streamflow (and as a result, lower Lake Mead water levels) the result of a “millennium drought” is sloppy reporting.

Numerous studies suggest that the original Colorado River Compact of 1922 was based upon a period of unusually high precipitation. This was discussed in a paper entitled “New Streamflow Reconstructions for the Upper Colorado River Basin: Placing Recent Droughts into a Centuries-Long Context“, which is a very readable review of various studies that have reconstructed Colorado River flows at Lee Ferry over the last 500 years from tree ring data. While the paper is a little dated (2006), the conclusions remain the same today.

Here are a couple of noteworthy quotes from that paper (bold added):

“The Stockton and Jacoby reconstruction of the annual flows from 1520 to 1961 contained several important findings, including that the highest sustained flows in the entire record occurred in the first part of the 20th century, the period upon which the Colorado River Compact of 1922 was negotiated, while the most persistent and severe drought occurred in the late 16th century.“

“…Colorado River allocations were based on one of the wettest periods in the past five centuries, while droughts more severe than any 20th-21st century event have occurred in the past.”

I’ve created a chart of the annual streamflows at Lee Ferry with some annotations showing periods of 3+ year droughts, the long-term trend (5th order polynomial fit) since stream gage data started in 1906, and four different estimates of the long-term (500-year) normal streamflow at Lee Ferry reconstructed from tree ring data.(UPDATE: the 2026 estimate is not just a repeat of the 2025 measurement, it is the central estimate of several quantitative evaluations of what the 2026 water year [October through September] will be based upon Lee Ferry gage measurements.)

As can be seen, the period before Hoover Dam was constructed was unusually wet. From the 1930s onward, there has been little net trend with some very wet years and very dry years, with up to a factor of 4-to-5 variations in the annual flows into Lake Mead. Six drought periods of at least 3 consecutive years are shown in red. Note that it took only 5 years to completely fill Lake Mead, which was accomplished by reducing the streamflow below the dam by about 30% to 40% of what the normal flows have been in recent decades.

From the above graph, I think one would be hard pressed to say there has been a statistically significant decrease in streamflow since the 1930s. (UPDATE: the linear trend for 1932 [a wet year] to 2025 is -0.013 +/- 0.016 million acre-feet per year, so it is not significant at the 68% confidence level). The major problem is that water usage exceeds what Mother Nature can reliably provide on a long-term basis. Several years ago I discussed this problem in a post in which I included the following graph (also rather dated) of Colorado River water supply versus usage.

SOURCE: https://www.usbr.gov/watersmart/bsp/docs/finalreport/ColoradoRiver/CRBS_Executive_Summary_FINAL.pdf

As can be seen, since about 2000, usage has exceeded supply, and given the natural multi-year variations in streamflow, it was only a matter of time before Lake Mead water levels would fall to operationally low levels.

In that same post I showed the average of over 100 CMIP6 climate model runs that show precipitation in the Colorado River watershed increasing substantially with global warming, so blaming the recent dry years on human-caused climate change seems a stretch. (UPDATE: While it is true that drought is a function of both precipitation and evaporation, and warming can cause drought even if precipitation does not change, water releases from Hoover Dam have been declining since 1998, so increased evapotranspiration from irrigation uses downstream of the dam [the main use of Colorado River water] cannot explain decreasing Lake Mead water levels. Direct evaporation from the lake surface is very small and changes little with warming. And there has been no statistically significant trend in streamflow input at Lee Ferry since 1932.)

And calling the recent dry years a “millennium drought” is just fake news

UAH v6.1 Global Temperature Update for July, 2026: +0.48 deg. C

August 4th, 2026

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for July, 2026 was +0.48 deg. C departure from the 1991-2020 mean, which is statistically unchanged from the June, 2026 value of +0.46 deg. C.

The Version 6.1 global area-averaged linear temperature trend (January 1979 through July 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 31 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.46+0.60+0.58+0.21+0.34+0.10+0.21
2026June+0.46+0.54+0.38+0.57+0.64+1.01+0.38+0.99
2026July+0.48+0.68+0.27+0.85+1.14+0.53-0.22+0.78
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for July, 2026 and a more detailed analysis by John Christy, should be available within the next several days here. John officially retired on July 1, 2026, but will continue working as a part-time employee of UAH.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere

UAH v6.1 Global Temperature Update for June, 2026: +0.46 deg. C

July 2nd, 2026

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for June, 2026 was +0.46 deg. C departure from the 1991-2020 mean, which is down from the May, 2026 value of +0.53 deg. C.

The Version 6.1 global area-averaged linear temperature trend (January 1979 through June 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 30 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.46+0.60+0.58+0.21+0.34+0.10+0.21
2026June+0.46+0.54+0.38+0.57+0.64+1.01+0.38+0.99
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for June, 2026 and a more detailed analysis by John Christy, should be available within the next several days here. John officially retired yesterday, July 1, 2026, but will continue working as a part-time employee of UAH.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere

UAH v6.1 Global Temperature Update for May, 2026: +0.53 deg. C

June 2nd, 2026

This month I’m adding Australia to the Global, USA48, and Canada time series plots.

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for May, 2026 was +0.53 deg. C departure from the 1991-2020 mean, which is up from the April, 2026 value of +0.39 deg. C..

The Version 6.1 global area-averaged linear temperature trend (January 1979 through May 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

A Note on These Tropospheric Temperature Anomalies vs. Surface Temperature Anomalies

It has been a while since I have discussed the main reason why our global monthly satellite-based tropospheric temperature anomalies can sometimes differ by quite a lot from the global monthly surface temperature anomalies. A good example is the last 2 months. In April, our +0.39 deg. C anomaly was statistically identical to the +0.38 deg. C surface temperature anomaly from the NOAA Climate Data Assimilation System (CDAS, which I take from WeatherBell.com maps). But then last month (May) the CDAS anomaly went down slightly (+ 0.34 deg. C), while our UAH anomaly went up considerably (+0.53 deg. C). These month-to-month fluctuations in the relationship between surface and tropospheric temperature changes are almost certainly dominated by fluctuations in moist convective heat transfer from the surface to the free troposphere. When there is a burst of extra convection (usually in the tropics), it cools the surface and warms the free troposphere more than normal, which is probably what happened last month (May).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 29 months (record highs are in red).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
2026May+0.53+0.53+0.53+0.58+0.21+0.33+0.10+0.21
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for USA48, Canada, and Australia

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for May, 2026 and a more detailed analysis by John Christy, should be available within the next several days here.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere

Pressure Causes Temperature? It’s Time to Climb Down from “Mount Stupid”

May 28th, 2026

There was a recent weeks-long exchange of emails between many climate people — professional and amateur — regarding the idea that air pressure (in combination with absorbed solar energy) is what causes temperature. There were insults launched at those who refused to believe what a certain physics-trained person says should be a revolution in our understanding of planetary temperatures. That person even managed to get a paper published in a journal that (in my opinion) used reviewers who were in over their heads on the subject.

The whole ordeal makes me think of the Dunning-Kruger Effect, which is the tendency for people who start to understand a complex subject to overestimate their level of understanding. This then leads to a point of peak overconfidence (climbing “Mount Stupid”), which then gradually relaxes as more is learned and the person increasingly realizes that the subject is more complicated and nuanced than they originally thought.

I claim that the person in question who thinks [pressure + absorbed solar energy = temperature] is still stuck on Mount Stupid.

The reason I bring this up again (I’ve preached on it before) is that many have been misled into believing the “theory”. As a result, I have spent many years responding to questions from the public (including science-savvy citizens) regarding the issue. Many have been convinced by the “theory”, and have joined the proponent of the theory on Mount Stupid.

After lurking in the weeks-long email discussion, I finally responded with the following summary of the issue. I have removed the person’s name to protect the not-so-innocent.

SUBJECT: Where <NAME REDACTED> Is Right… and Where <PRONOUN REDACTED> Is Wrong

All:

After working in meteorology and then climate during my 40+ year career, I think I can offer some insight into the issues being discussed in these emails. Like <NAME REDACTED>, I have always been skeptical of what I have been told until I could fully understand an issue for myself.

I’m sure the following explanations will be of help to many of you. (I suspect <NAME REDACTED> is too invested in theories to change <PRONOUN REDACTED> mind.) Many of the concepts are not trivial, and I will admit it wasn’t until many years after all of my education (PhD Meteorology) that I finally understood a few of them, because they were not taught in school. Dick Lindzen helped me in this in the early climate research years.

Most of what follows is fundamental atmospheric thermodynamics, and I question whether <NAME REDACTED> really did take a university-level Atmospheric Thermodynamics course. If he did, I’d like to know where.

And if <PRONOUN REDACTED> shows me <PRONOUN REDACTED> grades, I’ll show <PRONOUN REDACTED> mine.

A THOUGHT EXPERIMENT

Imagine you could suddenly dump an extra 1 atmosphere of air on top of the existing atmosphere, what would happen to air temperature in the 1 ATM below? Just as <NAME REDACTED> would predict, the temperature of the original atmosphere below would increase greatly through adiabatic compression.

But what would happen NEXT?….

The high [hot] atmospheric temperatures in the lower atmosphere would then be far out of energy balance compared to what existed before. The result would be cooling of all of that air that was heated through adiabatic (or nearly so) compression (work done on the lower atmosphere) until a new state of energy equilibrium was reached. The energy loss would be through infrared radiation of the hotter air.

In fact is it always ENERGY BALANCE that determines temperature, through the 1st Law of Thermodynamics. A change in temperature is proportional to the rate of energy input minus the energy output (which includes any work done in the process).

In contrast, the Ideal Gas Law (PV=nRT) cannot tell you what the temperature “should be”. It only says how the variables P, V, and T are interrelated during the process of re-equilibration and in the final equilibrium state. What <NAME REDACTED> misses in <PRONOUN REDACTED> theory is the “n” part of the equation (the number of moles, or mass… which is in the density form of the equation, P = rho RT). In my hypothetical 2-atmosphere thought experiment, as the lower atmosphere cools to reach a new state of energy equilibrium with the solar input, the decreasing temperature causes an increase in the air density (“shrinkage”), and the pressure remains the same… even while the temperature is changing.

Specifically, following the 1st Law, the internal temperature of a volume of atmosphere exposed to an energy INPUT will increase until the temperature-dependent energy OUTPUT processes equal the rate of energy gain. This is true of every physical system… the atmosphere, a pot of water on the stove, a car’s engine, the human body, the interior of the sun, etc. That energy equilibrium is what determines the final temperature. (In the real atmosphere, there are constant energy imbalances and thus changes in temperature; Trenberth’s global-average energy balance diagram is only useful to gain a conceptual understanding of the relative role of the major energy flows in the global-average climate system.)

THE IDEAL GAS LAW

Again, the Ideal Gas Law equation (PV=nRT) cannot tell you what the temperature of a gas should be, only energy flows in and out can do that. The gas law just tells you how the P, n, and T are interrelated for a given volume (V) of air. Yes, <NAME REDACTED>, on short time scales, ascending air cools and descending air warms, but if all of that motion was to stop, energy flow processes would then determine what the final temperature would be… not what the air pressure is.

For a given surface air pressure, a huge range of temperatures is possible, and that huge range is all due to energy flow processes. Again, if the near-surface air temperature over the whole planet is much higher than local energy flow processes can support, the temperature falls, and the air’s volume shrinks (or density, rho, increases, according to the equivalent Ideal Gas Law equation, P=rhoRT). The surface air pressure remains the same because the total mass of the atmosphere is unchanged.

SO WHY MIGHT THERE BE A CLOSE RELATIONSHIP BETWEEN DIFFERENT PLANET’S LOWER ATMOSPHERIC TEMPERATURE AND PRESSURE?

I haven’t studied the atmospheres of other planets, because I don’t care. Even if those other planets did not exist, they are not necessary for understanding our own atmosphere. But if indeed <NAME REDACTED> is correct about a close statistical relationship between different planets’ surface air pressure and temperature, after adjusting for solar input, then I suspect it’s because the more atmosphere there is, the more greenhouse gases there are.

On the subject of GHGs, I’ve forgotten… does <NAME REDACTED> believe that air absorbs and emits IR energy? Because the greenhouse effect is a necessary consequence of that absorption/emission. Energetically, the GHE is a radiative insulator. It’s analogous to adding insulation to a heated building’s walls in winter. For a given energy input into the building, the air temperature inside will rise, and the outside of the walls will experience a temperature fall. This is exactly what the GHE does to the atmospheric temperature profile (in an energetic sense.. clearly involving radiation rather than conduction as a heat transfer mechanism).

If <NAME REDACTED> doesn’t believe air absorbs IR energy, how does <PRONOUN REDACTED> explain all of the thousands of spectroscopic measurements of CO2, water vapor, and methane as a function of temperature and pressure? And if <PRONOUN REDACTED> does believe the atmosphere absorbs and emits IR energy, then <PRONOUN REDACTED> must also believe in a greenhouse effect, because it is a necessary consequence…. the greenhouse effect in planetary atmospheres always causes warming of the lower atmosphere and cooling of the upper atmosphere.

(BTW, it is a common misconception that air which absorbs IR energy immediately loses that energy through emission of IR. Not true. Look up the “kinetic theory of gases” and related concepts. When CO2 or H2O vapor molecules absorb IR photons they extremely rapidly lose their extra energy to other air molecules through collisions. This happens much faster [by a factor of ~50,000] than the time it takes to re-emit energy through IR photons. This is how IR absorption immediately leads to “thermalization” [a term I hate].

Furthermore, it is crucial to understand that since IR absorption is largely independent of temperature, but IR loss is VERY dependent upon temperature, almost all air in the atmosphere is in a continual state of IR energy imbalance. Much of that imbalance is what [is balanced by] convective overturning.

WHAT IS THE ROLE OF THE ADIABATIC LAPSE RATE?

The adiabatic lapse rate in the troposphere (9.8 deg C per km without moisture condensation) is the RESULT OF convective overturning. If condensation of moisture is involved in updrafts, then the lapse rate is lower. Like the Ideal Gas Law, it doesn’t tell you what the temperature “should” be. It just tells you how the temperature of an air parcel changes during ascent or descent, if there is no energy gain or loss (“a-diabatic”). [But there are energy gains and losses occurring everywhere, all the time, and those determine what the absolute temperature will be — not pressure.]

HOW DOES THE GREENHOUSE EFFECT PLAY INTO THE LAPSE RATE?

This is a very interesting subject. It is something that even many atmospheric scientists and climate researchers don’t really understand. The combination of solar heating of the surface and IR absorption and emission by the surface and atmosphere ALONE, WITHOUT ANY CONVECTIVE OVERTURNING would result in an extremely steep tropospheric lapse rate, with very high surface temperatures and exceedingly cold upper tropospheric temperatures. This was first demonstrated by Manabe & Strickler (1964), and it’s called the “pure radiative equilibrium” case. It is sort of what makes the term “greenhouse effect” technically correct; like a real greenhouse inhibiting convective heat loss [because it has a roof], the greenhouse effect is, by definition, what happens WITHOUT the resulting convective overturning.

But in the real world, convective overturning is the RESPONSE to this GHE destabilization! So, that 33 deg. GHE warming people talk about? That’s not the GHE. It’s the GHE + CONVECTION. Without convection, that 33 deg. C figure would be more like 65 or 75 deg. C. Which then leads to another fascinating question…

WHAT WOULD HAPPEN IF THE ATMOSPHERE DID NOT ABSORB AND EMIT IR ENERGY?

Imagine a cold planetary atmosphere with no energy input. Then, turn on the sun. Solar heating of the surface would warm the atmosphere through convective overturning. But the [deep] atmosphere would have no way to shed that energy to cool in the presence of all of that energy input. The temperature of the [deep] atmosphere would then continue to rise until it had the same temperature as the surface, through its entire depth. Long before that process finished convective overturning would have stopped, because the atmosphere would be too stable to support convection. The atmosphere would eventually become isothermal (or nearly so, since there might be some planetary scale overturning between the tropics and the poles, due to their different rates of solar input), with the same temperature as the surface. Interestingly, as a result all weather activity would cease. All clouds would probably disappear, resulting in higher temperatures. Any [remaining] circulation systems would have a planetary scale, because the horizontal scale of those systems are related to the lapse rate (through the “Rossby radius of deformation”), which is also why the stratosphere only has planetary-scale circulations.

-Roy

UAH v6.1 Global Temperature Update for April, 2026: +0.39 deg. C

May 7th, 2026

This month I’m adding plots for USA48 and Canada, too.

The Version 6.1 global average lower tropospheric temperature (LT) anomaly for April, 2026 was +0.39 deg. C departure from the 1991-2020 mean, which remains statistically unchanged for 4 months now.

The Version 6.1 global area-averaged linear temperature trend (January 1979 through April 2026) remains at +0.16 deg/ C/decade (+0.22 C/decade over land, +0.13 C/decade over oceans).

The following table lists various regional Version 6.1 LT departures from the 30-year (1991-2020) average for the last 28 months (record highs are in red). Note I’ve added Canada to the table this month, by request (although WordPress won’t allow me to add September 2024 for some reason). The warmest April in Canada was in 2010 (+2.61 deg. C), while the warmest anomaly out of all months was in January 1981 (+3.75 deg. C).

YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.
2024Jan+0.80+1.02+0.57+1.20-0.19+0.40+1.12+0.97
2024Feb+0.88+0.94+0.81+1.16+1.31+0.85+1.16+2.45
2024Mar+0.88+0.96+0.80+1.25+0.22+1.05+1.34+1.12
2024Apr+0.94+1.12+0.76+1.15+0.86+0.88+0.54+1.39
2024May+0.77+0.77+0.78+1.20+0.04+0.20+0.52+0.67
2024June+0.69+0.78+0.60+0.85+1.36+0.63+0.91+0.19
2024July+0.73+0.86+0.61+0.96+0.44+0.56-0.07+1.15
2024Aug+0.75+0.81+0.69+0.74+0.40+0.88+1.75+1.36
2024Sep+0.81+1.04+0.58+0.82+1.31+1.48+0.98
2024Oct+0.75+0.89+0.60+0.63+1.89+0.81+1.09+0.89
2024Nov+0.64+0.87+0.40+0.53+1.11+0.79+1.00+1.61
2024Dec+0.61+0.75+0.47+0.52+1.41+1.12+1.54+1.65
2025Jan+0.45+0.70+0.21+0.24-1.07+0.74+0.48+1.04
2025Feb+0.50+0.55+0.45+0.26+1.03+2.10+0.87-0.35
2025Mar+0.57+0.73+0.41+0.40+1.24+1.23+1.20+0.80
2025Apr+0.61+0.76+0.46+0.36+0.81+0.85+1.21+0.45
2025May+0.50+0.45+0.55+0.30+0.15+0.75+0.98+0.81
2025June+0.48+0.48+0.47+0.30+0.80+0.05+0.39-0.22
2025July+0.36+0.49+0.23+0.45+0.32+0.40+0.53-0.23
2025Aug+0.39+0.39+0.39+0.16-0.06+0.82+0.11+0.62
2025Sep+0.53+0.56+0.49+0.35+0.38+0.77+0.30+2.44
2025Oct+0.53+0.52+0.55+0.24+1.12+1.42+1.67+2.59
2025Nov+0.43+0.59+0.27+0.24+1.32+0.78+0.36+1.47
2025Dec+0.30+0.45+0.15+0.19+2.10+0.32+0.37-1.86
2026Jan+0.35+0.51+0.19+0.09+0.30+1.40+0.95+1.17
2026Feb+0.39+0.54+0.23+0.03+1.91-0.48+0.73+0.32
2026Mar+0.38+0.33+0.42+0.07+3.74-0.48+1.14-3.17
2026Apr+0.39+0.43+0.34+0.23+1.20+0.30+0.70-0.89
YearMonGlobeNHemSHemTropicUS48ArcticAust.Can.

Time Series Plots for USA48 and Canada

Starting this month I will include time series graphs for USA48 and Canada, in addition to the usual global plot. Note that for the previous month (March) the record warmth in USA48 (+3.74 deg. C) was in stark contrast to the coldest March in Canada in the 48-year satellite record (-3.17 deg. C).

The full UAH Global Temperature Report, along with the LT global gridpoint anomaly map for April, 2026 and a more detailed analysis by John Christy, should be available within the next several days here.

The monthly anomalies for various regions for the four deep layers we monitor from satellites will be available in the next several days at the following locations:

Lower Troposphere

Mid-Troposphere

Tropopause

Lower Stratosphere