WESTERN REGION TECHNICAL ATTACHMENT
NO. 03-05
May 28, 2003
A LOW LEVEL BLOCKING
RIDGE ALONG WITH DOWNWARD MOTION ALOFT IN THE RIGHT FRONT QUADRANT OF THE UPPER
LEVEL JET -
A RECIPE FOR MINOR FLOODING AND HIGH WINDS
Ivory J. Small and Joseph Dandrea
Weather Forecast Office, San Diego, California
INTRODUCTION
During the period 7-9 November 2002, urban and small stream flooding along
with damaging mountain/desert wind developed over southern California (Fig.
1). Over 10 inches of rain fell in the San Bernardino mountains, tapering
off to about 4 inches in the southernmost mountains. Urban and small stream
flooding was reported in Mill Creek Canyon below Yucaipa Ridge, 40 miles east
of Ontario CA (a location open to westerly flow with shear, rocky faces lining
the canyon). No flash flooding was reported. In the mountain and desert areas
mountain wave wind gusted to over 90 mph. Interestingly, although southern California
was in the front-right quadrant of the jet with downward motion aloft (Moore
and VanKnowe, 1992) nearly a foot of rain fell in the northern mountains. The
very high 850 mb dew point (near 8 degrees C), usually more commonly associated
with strong summer thunderstorms than winter rainfall, points toward extremely
high moisture content and a warm rain process. The 850 mb temperature was well
over the 5 degree C value generally needed to bring the snow level down to the
ski resorts near the 6500 - 7000 foot level. (The freezing level was above 10,000
feet for the entire event). Coupled with a nearly saturated 850-700 mb layer,
a strong, slow-moving low level jet at 850 mb of at least 20 knots, and a precipitation
band slowed by very strong 850 mb blocking, it is suspected that a very efficient,
warm rain process, amplified by upslope flow in the mountains, helped generate
the copious rainfall. Mountain rainfall totals were about 4-7 times higher than
coastal totals in the north, with even higher ratios in the south. Cross-sections,
along with other data were taken to evaluate this scenario (figure
2). In this Technical Attachment (TA) we will analyze the event using the
MesoETA model.
CASE COMPARISON
Many high accumulation events in southern California involve a very slow
moving mean trough, its associated very strong jet, and a series of strong waves
moving through the mean trough position as the trough moves slowly through California.
In this case, figures 3a-d show a large, slow moving
"anchor" low with an "anchor jet" that exceeded 200 knots
at one time. Figures 3a-d show conditions at 1800 UTC
8 November 2002, 0000 UTC 9 November 2002, 1200 UTC 9 November 2002 and 0000
UTC 10 November 2002, respectively. The anchor jet, with two 160 + knot jet
streaks (waves) moving through it (figure 3b), remains north of southern California
during the entire event. Such strong 250 mb anchor jets and strong imbedded
waves have been important features in the past for identifying strong pacific
storms with copious rains in southern California. Small (1993) noted a "130
knot jet streak approaching the coast" as a key feature in the flash flood
events in February 1992. For comparison, figure 4 shows
the 2 large troughs and their associated strong 130+ knot (150 mph) jet streaks
rotating through the mean anchor trough/anchor jet position during the 10-12
February 1992 cases. The anchor jet was oscillating from about 130 knots to
over 170 knots as the waves moved through the mean trough/mean jet position.
The jet streaks associated with the waves can be seen at 33N/130W and 33N/145W.
In this case, the 130 knot jet streaks south of Southern California were strong
enough to generate strong "negative tilt diffluent" troughs with very
high rainfall rates in the convection and dynamics at and north of the jet axis.
The first trough can be seen along the coast. During the 10-12 February 1992
event 1.55 inches of rain fell in one hour with 0.65 inches in 15 minutes on
the 10th, and 1.64 inches fell in one hour on the 12th. Since the amounts were
above 1.25 inches in one hour, they were at least good candidates for flash
flooding in southern California. Flash flooding occurred on both the 10th and
12th of February 1992.
In contrast, the 7-9 November 2002 case had mainly light-moderate stratiform precipitation and no flash flooding. There was a strong upper level jet to the north, but no strong vorticity centers (no strong synoptic scale ascent) over southern California (Fig. 3a-d). Notice the relatively warm flow shown by the very high (mid 570's in decameters) 500 mb heights. There is also a very high (around 560 decameter) 1000-500 mb thickness over southern California. Infrared satellite imagery in figures 5 and 6 show the very powerful jet pulling moisture from a decaying tropical system at 1200 UTC 6 November 2002, adding copious moisture to the moisture stream seen flowing into southern California at 1200 UTC 9 November 2002. Figure 7a-d shows the 850 mb heights, wind, and 850-700 mb mean relative humidity at 1200 UTC 8 November 2002, 0000 UTC 9 November 2002, 1200 UTC 9 November 2002, and 0000 UTC 10 November 2002 respectively. From about KSNA northward there were a whopping 4 consecutive sounding times (a 36 hour period from 1200 UTC 8 November 2002 to 0000 UTC 10 November 2002) with 850-700 mb mean relative humidity greater than 80-85 %, along with relatively warm 850 mb winds between 20 and 40 mph for high rain accumulations at both coastal and mountain sites.
The pattern and timing of moisture increases in the vertical prior to rainfall depends on the event type ("bottom up", "top down", or both) and is critical for beginning and ending the rainfall event. During many of the lighter rainfall events in southern California, the moisture is generally surface based with little moisture aloft. These "marine layer events" are topped out around 3000 to 6000 feet with mainly night and morning precipitation. Similar to the effects of a "low strong inversion" (about 1300 feet/10 degree C) at the beaches, these 3000 foot and deeper marine layers usually result in low clouds lingering into the afternoon, and sometimes all day. They are characterized by a "bottom up" type deepening trend, during which the moisture deepens from the surface upward in moist zonal or cyclonic westerly flow (with an onshore flow and/or trend). Measurable rain can begin at about 4-6 thousand feet deep. Clouds around 2000 feet thick accompany "trace" events and about 3500-5000 foot thick clouds accompany the more isolated - scattered, measurable light rain events. Saturated layers 5000-6000 feet thick have delivered scattered - widespread 0.10-0.25 inch amounts with marine layers of only 6000 feet deep at KNKX. This is especially true when an eddy or fairly strong low level onshore flow (about 10-15 knots near 850 mb) results in upslope flow, a locally deeper marine layer, and highest rainfall in/near the mountains. With enough cold advection near 850 mb the inversion can weaken and "bust up" the solid cloud deck. In these cases the boundary layer will "convect", resulting in a transition from steady light rain to convective showers (especially when the air aloft is cold enough and the surface moist layer is a few thousand feet deep or deeper). As the event winds down, broken cloud decks can still be generated via solar heating with surface based moist layers that have thinned to only about 1500 feet deep. If the clearing progresses from the coast inland as the cool, stabilizing sea breeze air sweeps over the area ("reverse clearing"), then the moisture left over from rainfall can result in fog overnight in the inland areas that have cleared. [Some discussion and satellite imagery of a "showery/reverse clearing" pattern is shown in Small (1999)]. With the saturated, stationary/warm frontal type airmass such as the 7-9 November 2002 case, the fog actually develops with the rain rather than during the night after the rain event ends and the clouds clear.
As is common for cases
with huge rainfall accumulations, the 7-9 November 2002 event started out as
a "top down" event, with the moisture moving in aloft first. This
"top down" moistening can occur any time of year via overrunning precipitation
as a storm approaches, or when the flow turns south around the summer subtropical
high. The precipitation from high based showers or isolated thunderstorms helps
to moisten the lower layers. (Cold pool or heating-related convection is frequently
reduced or delayed til the higher clouds move out, leaving a moist low/mid level
airmass to convect. Consequently, until then, the tendency is toward a more
"stratiform" precipitation). Figure 8a at
0000 UTC 8 November 2002 shows this upper level moisture moving in aloft to
begin moistening the lower levels, partially by raining into it (usually rain
finally reaches the ground when the 50 % relative humidity level lowers to about
the 650 to 700 mb level). Next, the "bottom up" processes develop
in the boundary layer as low level onshore flow increases, as seen in figure
8b. Figure 8b at 1200 UTC 8 November 2002 shows the classic warm advection
sounding. There is a nearly saturated layer of increased stability (an inversion
in this case) between about 900 mb and 700 mb with a very impressive 8 degree
C 850 mb dew point and strong winds. Figure 8c shows summer-like precipitable
water values [locally in excess of 1.5 inches (well over 2 times normal for
the cool season)] which persisted between 1.25 and 1.50 inches for the entire
event. Even 1 inch of precipitable water is quite high for the cool season.
The very moist airmass in the lower-mid levels is apparent in this case. There
was strong low level flow at 850 mb (20 knots or greater). The high freezing
level/snow level confirms that the airmass was very warm. The high heights (mainly
around 570 decameters ), high thicknesses (mainly in the low 560s in decameters),
along with high precipitable water values (above 1.25 inches, which is above
2 times normal) resulted in a very efficient warm rain process. As a matter
of fact, the 850-700 mb airmass was nearly saturated (above 90 percent) much
of the time with 850 mb wind speeds in the 25-40 knot range.
As for blocking, the strong gradient in the 850 mb heights, or a "low level
blocking 850 mb ridge" (for example, figure 9a)
is a good indicator that the baroclinic band and possibly heavy rain, snow,
etc, may linger over an area, making the area vulnerable to additional waves
in the baroclinic zone. The 850 mb height difference of over 110 meters between
the Tucson (KTUS) and Desert Rock (KDRA) indicated a strong south to north height
gradient, strong westerly flow, and very slow southward movement of the front
for continued large rainfall accumulations northern coastal areas. The coastal
rain amounts were then dramatically magnified in the mountain areas. This height
gradient reflects the surface pressure gradient shown in figure
9b.
On the other hand, potentially higher rainfall rates can occur when this 850 mb gradient is more east-west [blocking ridge in the form of a large 850 mb height gradient between Miramar (KNKX) and Tucson (KTUS)]. Figure 10a-b shows examples of very strong south-north and east-west blocking for comparison using the 850 mb heights and winds. Figure 10a shows the "zonal" case, with very strong (about 140 meters over 400 miles) south to north blocking and a 45 knot westerly low level jet. In this type of situation the stronger portion of the wave and associated dynamics pass by to the north. Figure 10b is the more "volatile" case, with a very strong (about 80 meters over 400 miles) east to west blocking and a 30 knot jet (southerly flow). In these cases the negative tilt trough and strong dynamics approach from the west. Usually, for the volatile east-west (or "front-side') blocked cases, about 30-60 meters of blocking (strong) is a significant concern. [As a matter of fact, of the 7 storms with blocking that reached at least 60 meters (very strong front-side blocking) between 1998 and 2002, 6 resulted in at least 1.25 inches of rain at KSAN, which is about one-eighth of the annual rainfall]. During these "east-west blocked" events (commonly seen with negative tilt diffluent troughs) there is a strong southerly (or even southeast) flow as the surface low wraps up and moves north. Consequently, the strong low level jet and the frontal band with very high rainfall rates stalls, or moves very slowly east across southern California. Also, this pattern can result in a strong subtropical or even tropical connection and rapidly bring up huge amounts of moisture from the ITCZ and surrounding area well to the south (between the equator and about 10 degrees north).
As for wind, figure 9a shows the 850 mb heights, 700 mb wind and the 850 mb wind at 0000 UTC 9 November 2002, near the period of strongest surface wind [maximum sustained wind of 66 mph with a gust to 93 mph at Burns Canyon (BNY) on the eastern slopes of the San Bernardino Mountains]. The 850 mb winds of 30-40 knots, the 50-60 knots at 700 mb, and the synoptic scale downward motion associated with the right front quadrant of the upper level jet easily supplied the upper level support to generate these surface winds. Sustained surface winds that equaled the 850 mb winds, and isolated gusts around twice the 850 mb wind speed (well above the maximum 700 mb wind speed) developed. The strong south to north 850 mb height gradient accurately reflects the south to north surface pressure gradients of over 14 mb from the KLAX/KSAN area on the southern California coast to a 999 mb low over southern Nevada in the KLAS/KTPH area (figure 9b). Unlike the strong east-west blocking usually found with the negative tilt diffluent trough events, the east-west blocking was only a paltry 20 meters. It was the huge south-north blocking of over 110 meters (indicative of a strong westerly low level jet) that stalled the baroclinic band and slowed the movement of the region of heaviest precipitation in this case.
Figure 2 shows the location of the cross section used in figure 11a-b. Figure 11a at 0000 UTC 9 November 2002 shows deep moisture in westerly flow up to the mountain crest, with downslope flow and drying below mountain crest east of the mountains [Although there was over 10 inches of rain in the mountains, the southern deserts (KPSP and KTRM) did not receive measurable rain, which is an interesting characteristic of many westerly zonal flow events]. Deeper moisture and/or a more easterly flow is usually needed for significant precipitation in the southern deserts.
SUMMARY AND CONCLUSION
Long-duration high accumulation events are a significant forecast problem. They
can develop when the region of moderate or heavy precipitation along a baroclinic
band slows or stalls (possibly due to blocking of the 850 mb jet by a strong
height gradient/blocking ridge at 850 mb). In these cases the potential exists
for waves in the flow to periodically enhance the precipitation on these slow
moving, blocked bands. The wind driven moisture flux/moisture convergence results
in a very moist airmass (mean relative humidity of 80-85 percent or more) in
the 850-700 mb layer. (During many southern California rain events, the deep
moisture will extend no higher than the 850-700 mb region, so the characteristics
of a storm can often be determined by looking at the wind, relative humidity,
and instability in this layer). During the more extreme cases, a nearly saturated
airmass extends from the surface to well above 500 mb. With 4 raobs meeting
this 850-700 mb 80-85 % value, the isolated urban and small stream flooding
during the 7-9 November 2002 storm was more of a "duration" (prolonged
rainfall) and "frequency" (back to back waves in moist westerly flow)
problem rather than an "intensity" (rainfall rate) problem. Basic
ingredients in the case include a very powerful jet aloft driving a strong low
level flow of 20-30 knots or more at 850 mb. This is coupled with a warm airmass
extending upward into the 850-700 mb layer, moistened to at least 80-85 % mean
relative humidity. Just as important are 850 mb dew points in excess of about
5 degrees C (usually associated with strong summer thunderstorms), which indicate
a very warm (and usually saturated) airmass during the cool season. Dew points
of that magnitude generally correspond to precipitable water values over an
inch (approximately 2 times normal). The 5+ degree C 850 mb temperature also
indicates a high freezing level (above about 6500-7000 feet) and a warm rain
process in place. Very powerful jet streams that exceed about 200 mph (or about
175 knots) in southern California can easily produce these parameters, especially
with a subtropical moisture fetch. One of these monsters can easily produce
storm total precipitation of a foot or more from multiple imbedded waves or
a series of storms. This is especially true north of the jet axis in the dynamics
and convection, where very high rainfall rates can more frequently occur resulting
in periods of high rainfall frequency (waves rotating through the mean trough
position) and duration. Although the synoptic scale downward motion associated
with the right front quadrant of the upper level jet helps transport some momentum
downward to the low level jet, the drying effect of the subsidence aloft is
easily counteracted by the strong moisture convergence and upslope flow near
the surface over and west of the mountains. In this case the low level mechanics
prevail over upper level jet dynamics and high rainfall totals still occur.
As for wind, flow direction
is important for offshore flow patterns as well as for southwest through northwest
wind patterns. Due to mountain/canyon orientation, northeast (southwest) winds
are optimal for waves and gap flow in the northern portions of the San Diego
CWFA, whereas a more easterly (westerly) flow favors waves and gap flow in the
southern portions of the CWFA. When the flow direction is optimal (and usually
associated with surface pressure gradients of about 3.5 mb or more between the
coast and local deserts), gusts seem to reach about 2 times the 850 mb wind
speed in the favored areas where the wave surfaces. This is especially true
for winds upward of about 25-30 knots at 850 mb (or about 50 knots at 700 mb).
In this 7-9 November 2002 west wind case, synoptic scale downward motion in
the right front quadrant of the jet, although not able to reduce the rainfall
west of the mountain ridge line, actually couples with mountain wave activity
to help surface the winds in the mountains and deserts. The 850 mb and 700 mb
winds near 40 knots and 60 knots respectively resulted in local mountain wave
winds in excess of 60 mph with gusts over 90 mph at BNY, (a "favored area"
during west wind patterns). To further complicated matters, a "Palm Springs
Rotor" brought east wind gusts to18 knots to KPSP, while at the same time
west wind gusts reached 44 knots 20 miles away at KTRM. With little rain, wind
gusts to 40 mph can result in at least local visibilities of 1/4 mile or less
in blowing sand and dust, making the forecast problem surrounding wind events
even more challenging. This 7-9 November 2002 case was no exception.
REFERENCES
Moore, J. T., and G.
E. VanKnowe, 1992: The Effect of Jet Streak Curvature on Kinematic Fields. Mon.
Wea. Rev., 120, 2429-2441
Small, I. J., 1999: An Observational Study of a California Bight Coastal Convergence
Zone Produced by Flow Interaction With Mainland Topography: Precipitation Producer
in Southern California. Western Region Technical Attachment No. 99-19, http://www.wrh.noaa.gov/wrh/99TAs/9919/index.html
Small, I. J., 1993:
The February 1992 Record Flash Flood Events In Southern California. Post-Print
Volume, Third National Heavy Precipitation Workshop, Pittsburgh, Pennsylvania,
November 16-20, 1992. NOAA Technical Memorandum No. ER-87, 139-148, 8 pp.
http://www.ntis.gov/