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I awoke to thunderstorms in Madison, Wisconsin this morning. The elevated storms were riding a warm front at 850 mb, fueled by moderate-to-strong warm-air advection.This was a good opportunity to look at ProbSevere LightningCast version 2, which includes Multi-Radar Multi-Sensor (MRMS) Reflectivity -10C as a predictor, along with several visible, near-infrared,... Read More
I awoke to thunderstorms in Madison, Wisconsin this morning. The elevated storms were riding a warm front at 850 mb, fueled by moderate-to-strong warm-air advection.
Figure 1: 850 mb winds, heights, and temperate advection, from 09Z to 11Z, as analyzed by the Storm Prediction Center’s mesoanalysis page. Note the warm-air advection over Wisconsin.
This was a good opportunity to look at ProbSevere LightningCast version 2, which includes Multi-Radar Multi-Sensor (MRMS) Reflectivity -10C as a predictor, along with several visible, near-infrared, and longwave-infrared bands from the GOES-R Advanced Baseline Imager (ABI). In the animation below, the contours in the left images were produced by LightningCast v1 (ABI-only predictors), whereas the contours in the right images were produced by LightningCast v2 (ABI + MRMS predictors). The background imagery is the GOES-16 IR-only cloud phase RGB and the blue foreground pixels are observed flash-extent density from the GOES-16 Geostationary Lightning Mapper (GLM).
The LightningCast v1 probabilities were lower for the storms in southern Wisconsin compared to LightningCast v2, which had elevated probabilities before lightning initiation. There are likely a couple of reasons that v1 probabilities are lower: 1) the short-wave reflective bands are not contributing at this time, and 2) overlapping mid- and high-level clouds may be obscuring the convective signal for the long-wave infrared predictors.
Overall, we’ve found that LightningCast v2 is very similar to v1, but outperforms v1 in important situations such as in new convective development under thick ice (e.g., anvil clouds), for convective decay, and sometimes in nocturnal convection. We have not seen significant degradation in regions without MRMS coverage or drops in lead time to lightning initiation when applying LightningCast v2.
This new version of LightningCast will be evaluated at the NOAA Hazardous Weather Testbed in May and June of this year.
Figure 2: Left: LightningCast v1 probabilities (contours). Right: LightningCat v2 probabilities. The higher probabilities correspond with GLM observations of lightning, highlighting better performance for the v2 model in this case.
Imagery from the VIIRS Today website, shown below, shows the stark effects of the Lunar Eclipse on Day Night Band imagery. Suomi NPP and NOAA-20 passes over the east coast (shown below; it happened with NOAA-21 too!) lack the reflected moonlight that was available over the central/western United States after the lunar eclipse... Read More
Imagery from the VIIRS Today website, shown below, shows the stark effects of the Lunar Eclipse on Day Night Band imagery. Suomi NPP and NOAA-20 passes over the east coast (shown below; it happened with NOAA-21 too!) lack the reflected moonlight that was available over the central/western United States after the lunar eclipse had ended. This will happen again on September 7th this year. Mark your calendars.
Suomi-NPP Day Night Band visible (0.7 µm) imagery, 14 March 2025 (Click to enlarge)NOAA-20 Day Night Band visible (0.7 µm) imagery, 14 March 2025 (Click to enlarge)
Contrast, below, NOAA-21 overpasses (imagery taken from the CIMSS VIIRS Viewer) at 0651 and 0831 UTC. With no reflected lunar illumination in the earlier overpass, aurora over northern Canada are far easier to view (Note also the lightning streaks over the ocean). It’s a bit harder to see the full extent of the aurora in the more illuminated overpass at 0831 UTC.
NOAA-21 Day Night Band visible (0.7 µm) imagery along the east coast ca. 0651 UTC (mostly dark), and over the central USA ca. 0831 UTC (illuminated) on 15 March 2025 (Click to enlarge)
Bob Carp, SSEC, created the following animation using McIDAS-V. It shows swaths from Suomi-NPP, NOAA-20 and NOAA-21. You’ll see that DNB imagery is starting to dim at 0507 UTC and starts to brighten up by 0832 UTC. This website gives times when the effects of the eclipse were expected: The penumbral part of the eclipse was from 0357 UTC to 1000 UTC; a partial eclipse was from 0509 UTC to 0847 UTC; totality was from 0626 UTC to 0731 UTC.
In addition, shown below is a similar animation (created using AWIPS) that steps through Day/Night Band images from Suomi-NPP + NOAA-21 (white labels) and NOAA-20 (cyan labels).
VIIRS Day/Night Band images from Suomi-NPP + NOAA-21 (white labels) and NOAA-20 (cyan labels) [courtesy Scott Bachmeier, CIMSS; click to enlarge]
Clean-window infrared imagery centered on the Samoan Islands on 9 March 2025, above, show convective development north of Upolu that subsequently shows a cyclonic circulation. This system was accompanied by Flood Warnings, Heavy Rain Warnings and Marine Warnings and Wind Advisories over all of Samoa (Facebook link). Gusts exceeding 70 km/hr... Read More
GOES-18 Clean Window infrared (Band 13, 10.3 µm) imagery, 0000-1300 UTC on 9 March 2025 (Click to enlarge)
Clean-window infrared imagery centered on the Samoan Islands on 9 March 2025, above, show convective development north of Upolu that subsequently shows a cyclonic circulation. This system was accompanied by Flood Warnings, Heavy Rain Warnings and Marine Warnings and Wind Advisories over all of Samoa (Facebook link). Gusts exceeding 70 km/hr were reported. A very timely MetopC overpass, below (courtesy Joe LaPlante from the NWS in Pago Pago), shows the low-level circulation that developed. It does not appear to have cut off into a closed circulation at that time.
Metop-C ASCAT Winds, 0842 UTC on 9 March 2025 (Click to enlarge)
How well can a strong spin-up like this be anticipated? A deterministic ECMWF forecast initialized on 0000 UTC on 8 March, below, showed a region of active weather moving southward through the Samoan Island chain after 1800 UTC on 8 March. Note the small box drawn around the Samoan Islands. (Here is the 1200UTC/8 March ECMWF run that shows a similar evolution). Imagery is taken from the excellent TropicalTidbits website.
ECMWF Surface Predictions initialized 0000 UTC/8 March 2025; forecasts are every 3 hours from 0300 UTC 8 March 2025 through 1200 UTC 9 March 2025. A black box is centered on the Samoan Islands (Click to enlarge)
Deterministic models from the GFS (imagery also from the Tropical Tidbits site), below, show a similar scenario, both from the model initialized at 0000 UTC/8 March below, and the one starting at 1200 UTC/8 March at this link. All of the forecasts show a system sagging towards the south across Samoa.
GFS Surface Predictions initialized 0000 UTC/8 March 2025; forecasts are every 6 hours from 0600 UTC 8 March 2025 through 1200 UTC 9 March 2025. A black box is centered on the Samoan Islands (Click to enlarge)
MIMIC Total Precipitable Water (TPW) fields from 0000 UTC 8 March through 1200 UTC 9 March 2025, below (from this site), suggest a local maximum in moisture over the islands, and the fields also show the southward motion.
MIMIC Total Precipitable Water (TPW) fields over the south Pacific, 0000 UTC 8 March through 1200 UTC 9 March 2025 (Click to enlarge)
Visible imagery (from the CSPP Geosphere website) below shows active weather north of Samoa. It moves south throughout the animation.
GOES-18 Band 2 Visible (0.64) imagery, 1800 UTC 8 March 2025 – 0600 UTC 9 March 2025
Now consider the Metop-B ASCAT winds below, from ca. 2100 UTC on 8 March 2025. A local maximum in wind (in red) is north of Savai’i, and the leading edge of a region of stronger winds. Is this single observational plot sufficient for a forecaster to prepare the weather that was observed?
Metop-B 25-km ASCAT winds, 2057 UTC on 8 March 2025 (Click to enlarge)
The GOES-18 imagery at that time (pulled from the visible animation above) shows strong convection (circled in black) near that region of stronger winds. If you trace that convective region southward to Upolu and Savai’i, does it overspread the region that saw damage (downed trees, taken from here, for example) and heavy rain?
GOES-18 Visible Imagery (Band 2, 0.64) at 2100 UTC on 8 March 2025 (Click to enlarge)
Clean window infrared imagery, below (the end of the animation below overlaps with the start of the infrared animation shown above), suggests that perhaps that region of strong winds in the ASCAT fields, if associated with strong convection can be tracked to the south.
GOES-18 Clean Window infrared (Band 13, 10.3 µm) imagery, 1800 8 March 2025 – 0100 UTC on 9 March 2025 (Click to enlarge)
Once the cyclonic circulation is apparent, would you expect it to persist in the environment? That is — are we seeing the development of a tropical cyclone? Shear values (from the CIMSS Tropical Weather Website), show a narrow region of favorable shear where the spin-up occurred. Like the forecasts and other fields, the favorable shear region is shifting south with time.
Diagnosed Deep-Layer Shear (850-250 mb), 1200 UTC 8 March – 1200 UTC 9 March 2025 (Click to enlarge)
Upper-level divergence is similarly shifting southward, with strong values where the convection and spin-up occurred.
Diagnosed Upper-Level Divergence (150-300 mb), 1200 UTC 8 March – 1200 UTC 9 March 2025 (Click to enlarge)
Low level convergence fields also show a southward progression, but are not as organized as upper levels. Maybe that’s why this cyclone did not persist with time.
Low-level convergence fields (850-925 mb), 1200 UTC 8 March – 1200 UTC 9 March 2025 (Click to enlarge)
Thanks to the Forecast Office in Pago Pago for alerting me to this interesting event.
Early this morning at around 3:15 AM local time, an EF-0 tornado touched down in Pico Rivera, a community in Los Angeles County, California. It damaged several homes and knocked down numerous trees over the course of its mile-long path. Numerous instances of damaging winds were also reported, as seen... Read More
Early this morning at around 3:15 AM local time, an EF-0 tornado touched down in Pico Rivera, a community in Los Angeles County, California. It damaged several homes and knocked down numerous trees over the course of its mile-long path. Numerous instances of damaging winds were also reported, as seen on the NOAA SPC Storm Reports page. Fortunately, there were no reports of injuries.
NOAA SPC storm reports for this event. Due to the way that SPC organizes data from 1200 to 1159 UTC each day, this event is assigned to March 12th even though it happened on March 13th. The red dot in California indicates the location of the tornado.
Tornadoes in Los Angeles County are comparatively rare, but not unheard of. This is the 50th recorded tornado in the county since 1950, and every month of the year has had at least one tornado report. The peak season for LA County tornadoes is winter and spring with more tornadoes recorded in January than any other month; with today’s event, March is now tied for second on that list. The NOAA NCEI Storm Events Database is an invaluable tool for analyses like these.
This particular storm event was driven by an advancing cold front linked to a low pressure system offshore. A steady stream of moist air from the Pacific ensured sufficient moisture to support convection. That is evident in the GOES-18 Band 8 upper level water vapor imagery, which shows a plume of moisture pointed directly at the greater Los Angeles area.
Band 8 upper water vapor imagery from 0830 – 1030 UTC (1:30 AM – 3:30 AM local time).
A polar-orbiting overpass at 0930 UTC (2:30 AM local time, approximately 45 minutes before tornadogenesis) provided Gridded NUCAPS observations. The 700-500 mb lapse rate product from Gridded NUCAPS shows lapse rates over LA County to be close to the critical conditionally unstable value of 6.0 C/km, with more unstable air aloft coming onshore from the south. The elevated lifting from the advancing front coupled with the elevated instability was enough to support deep convection.
Gridded NUCAPS 700-500 mb lapse rate for 0930 UTC (2:30 AM local time).
Forecasters anticipated the potential weather overnight and the GOES-18 mesoscale sector was active for this event, providing images every minute. Since it was nighttime, none of the products that depend on shortwave channels were available, but many interesting things can be discerned from the longwave imagery. The Channel 13 IR window view shows the cold cloud top temperatures associated with the deep, moist convection, while the speckled orange portions of the Night Microphysics RGB help to confirm that the clouds over LA are deep, thick, and moisture-laden. Mesoscale sectors are available in AWIPS, or are freely available to everyone at SSEC RealEarth.
One-minute mesoscale sector scans of Band 13 from GOES-18 from 1000 to 1030 UTC (3:00 AM – 3:30 AM UTC)As in the figure above, but for the night microphysics product.