Chapter 9: Observation, Analysis, and Prediction

9.6 Forecast Verification and Validation »
9.6.2 General Methods for Forecast Verification »
9.6.2.6 Methods for Verification of Ensemble Forecasts

As we discussed in Section 9.4.5Section 9.4.5, ensembles consist of many versions of a single dynamical model or many different dynamical models. The ensemble forecast captures the uncertainty in the forecast and provides a range of outcomes.

Many methods for evaluating probability forecasts can also be implemented for evaluating ensemble forecasts, where the spread of the ensemble members indicates probability. However, since ensembles provide information on the range of possible outcomes given the particular initial conditions, other measures of skill can also be applied to ensembles. We review just a few. You are encouraged to explore further using the cited references and resource links.

  • Rank histogram The rank histogram is a quantitative, multi-category method of verification that is represented visually (e.g., Fig. 9.82). It measures how well the ensemble spread of the forecast represents the true variability (uncertainty) of the observations. It is also known as a “Talagrand diagram”.116,117
Example rank histogram for a 15 member ensemble
Fig. 9.82. An example rank histogram for a 15-member ensemble. Typically, N ensemble members will have N+1 bins with the lowest and highest valued bins being open-ended. In this example, the highest valued bin is repeated as Bin 0.

In an ensemble with perfect spread, an observation is equally likely to fall between any pair of ensemble members since each ensemble member represents an equally likely scenario. Therefore, we can evaluate the success of the ensemble spread by looking at the shape of the rank histogram. If the histogram is:

  • Flat, the ensemble spread is acceptable for representing the forecast uncertainty. Note that a flat rank histogram does not necessarily indicate a good forecast, only that the ensemble is a reasonable representation of the observed probability distribution;
  • U-shaped, the ensemble spread is too small since many observations fall outside the range spanned by all of the ensemble members.
  • Dome-shaped, the ensemble spread is too large since most observations fall near the center of the range of the ensemble set;
  • Asymmetric, the ensemble has an overall bias compared to observations.

Verifying forecasts of rare and/or extreme events

Since we are interested in verification for ensemble forecasts of TC, we will briefly review two methods for verifying ensemble forecasts of rare and extreme events.

  • Deterministic limit
    The deterministic limit118 is the forecast lead time at which the number of misses plus false alarms in the ensemble forecast set equals the number of hits for a chosen weather system. It measures the forecast lead time for which the forecast is more likely to be correct than incorrect (Fig. 9.83). While this may not sound too exciting, it could help the forecaster to decide how much weight to give that forecast and, possibly, to decide to switch from deterministic to probabilistic guidance.

One example of the use of a deterministic limit would be the statement that “The deterministic limit for forecasts of TC intensity by the XXX model is 24 hours.”

Example of the calculation of the deterministic limit
Fig. 9.83. Example of the calculation of the deterministic limit for a chosen weather system and forecast model.
  • Extreme Dependency Score
    The Extreme Dependency Score (EDS) measures the reliability of a model to forecast a specific weather system, such as a TC. The EDS119 is a measure of the forecast skill for observed rare events. It ranges between -1 and 1, where a perfect score is EDS=1.

9.6 Forecast Verification and Validation »
9.6.3 Summary: Advantages and Inadequacies of Current TC Forecast Models

Based on results from the current verification methods, we can make some general comments on the skill of the current generation of forecast models.

While it is possible for the human forecaster to show skill over the operational forecast models from time to time, model performance has improved significantly over the years, and they are now very difficult to beat on a consistent basis, at least for track forecasts.

Intensity forecasting is much more complex than track forecasting. For a start, intensity forecasts rely in some measure on the track forecasts (e.g., to get interactions with other weather systems and SST information). Further, intensity depends on details of the TC core structure, such as the distribution of deep convection, and other internal storm processes. Thus, dynamical forecast models still have little skill in predicting TC intensity change.

Statistical models for TC intensity are beginning to provide useful guidance, although since they are built using historical storm information, their skill is restricted to “typical” TC intensity evolution. Events such as rapid intensity change are not well forecast in either statistical or dynamical models. Current statistical models of rapid intensity change are based on a very small set of storms, which limits the range of possible intensity changes that underlie the statistical model.

Consensus forecast systems offer hope for improvements in forecast accuracy. Ensemble prediction systems are beginning to address the problem of TC forecasting directly101,120 by targeting TC when the ensemble perturbations are developed,80 rather than developing the perturbations as part of a larger forecasting problem. These offer hope of improved forecasts, not only of TC track and intensity, but on wind and rainfall distributions and storm structure evolution. Forecasting of extratropically transitioning TC121 (ET, Section 8.5ET, Section 8.5) and the influence of these ET systems on the midlatitude flow122,123 is also a critical problem being studied using these targeted model ensembles.

Focus Areas

Focus Areas »
Focus 1: The Australian-Indonesian Monsoon

Focus 1: The Australian-Indonesian Monsoon »
9F1.1 Overview of the North Australian Monsoon

by Dr. Mick Pope of the Australian Bureau of Meteorology (BoM)

The monsoon refers to the tropical and subtropical seasonal reversals in the atmospheric circulation and associated precipitation,124 leading to two distinct phases, “wet” and “dry” (Fig. 9F1.1).125 The changes in the atmospheric circulations arise from reversals in temperature gradients between continental regions and the adjacent oceans. In many cases this is accompanied by the seasonal migration of the Hadley cell and associated monsoon trough or ITCZ. However, in the case of the American monsoons (Fig.9F1.1, left panels), no seasonal reversal of the winds has been identified.125 Equatorial regions have two rainy seasons and the trade wind flow collects moisture over the warm tropical oceans. In locations like Australia and India, one rainy season occurs when the cross equatorial flow turns westerly (Fig. 9F1.1, right panels). The corresponding trade wind easterlies are dry and characterized by a low-level inversion which caps deep convection.

This focus section will examine the Australian-Indonesian monsoon as a case study of monsoon dynamics, with a particular focus on the differences between the various intraseasonal phases.

Mean OLR, 200hPa streamlines, and 850 hPa wind vectors
Fig. 9F1.1. Mean OLR, 200 hPa streamlines, and 850 hPa wind vectors (1979-1995) for the American, African, and Asian-Australian monsoons. Top panels are peak boreal summer monsoon periods. Bottom panels are peak austral summer monsoon periods. Red arrows show the general monsoon flow. Inset maps show colour-shaded digital elevation.

Focus 1: The Australian-Indonesian Monsoon »
9F1.1 Overview of the North Australian Monsoon »
9F1.1.1 The Seasonal Cycle

Like the Indian monsoon,126 the Australian-Indonesian monsoon undergoes intraseasonal variation consisting of active and break phases, characterized by widespread and isolated precipitation respectively (Fig.9F1.2).

Map of Australian-Indonesian monsoon region
Mean daily zonal winds (b) and precipitation (c) at Darwin, Australia
Fig. 9F1.2. (a) Map of Australian-Indonesian monsoon region. Mean daily zonal winds (b) and precipitation (c) at Darwin, Australia.

The NAM forms part of the global monsoon driven by the Hadley Cell. Up motion occurs in the hot towers due to condensational heating, resulting in lower pressures near the surface in the tropics and hence a cross equatorial pressure gradient with the winter hemisphere mid-latitudes. The column heating in the hot tower also produces a much stronger reverse pressure gradient in the upper troposphere which drives the upper return flow into the winter hemisphere.127 Modeling studies show that the response to the tropospheric heating is stronger when the heating is off the equator.128 Superimposed on this is the land-sea thermal contrast that develops during Austral Spring.125 A heat low develops over the Pilbara region, often resulting in shallow westerly flow over northern Australia, which moistens and pre-conditions the environment for deep convection (Fig.9F1.3). The period during which this pre-conditioning and isolated shallow convection occurs is known as the buildup. There is also a forcing due to the seasonal migration of the warmest sea surface temperatures.129

MSLP (contours) and 900 hPa vorticity
Fig. 9F1.3. MSLP (contours) and 900 hPa vorticity (shading) (a) prior to monsoon onset on 6 December 2005 and (b) during an active monsoon phase, 23 March 2006 from the Bureau of Meteorology TXLAPS model. Contours are every 2 hPa; shading every 15 x 10-6 s-1. Negative values in the Southern Hemisphere indicate cyclonic vorticity.

think icon A significant amount of rainfall occurs outside of the period of westerly winds. What weather systems would be responsible for this? We will answer this question in a later section.

Mean month values of CAPE, CIN and number of zero CAPE days
Fig. 9F1.4. Mean month values of CAPE, CIN and number of zero CAPE days for the 2300 UTC Darwin sounding. CAPE and CIN are calculated using the unmodified 2300 UTC surface values. The mean monthly CIN values exclude zero CAPE days.130

The seasonal cycle can also be considered in terms of the CAPE—a proxy for the strength of convective updrafts. The most energetic updrafts occur on average during November to January. Figure 9F1.4 shows the month values of CAPE, Convective Inhibition (CIN) and number of zero CAPE days for the 2300 UTC Darwin sounding. The amount of CAPE almost doubles during the late dry season (September through November), with a rapid decrease in the number of zero CAPE days. The increase in the CIN during this period is likely an artifact of the large number of zero CAPE days during September and October. Zero CAPE days reach a minimum at the peak of the monsoon during February, although this is not the time of maximum mean monthly CAPE.

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.1 TWP-ICE

The NAM undergoes significant intraseasonal variability. Figure 9F1.5 shows the area average rain accumulation for January and February 2006 from the Tropical Warm Pool – International Cloud Experiment (TWP-ICE).131 The active period of the monsoon was marked by deep zonal westerly winds over Darwin and, during 23-26 January, an intense mesoscale convective system (MCS) produced an area averaged rainfall rate of approximately 45 mm day-1. The period starting February 6th is referred to as a break monsoon with deep tropospheric easterly winds, which produced an area averaged rainfall rate of approximately 8 mm day-1.

Rainfall accumulation averaged over the 300-km-diameter circle
Fig. 9F1.5. Rainfall accumulation averaged over the 300-km-diameter circle sampled by polarimetric radar during TWP-ICE. The heavy vertical lines mark the beginning and end of the intensive observing period and dotted lines are regime transitions.131

The NAM is characterized by active and break periods.132,133,134 During periods when the MJO is active (which it is not during all summers) there is a strong synchronization between the active-break cycle and the MJO.135,136 Likewise, the greatest probabilities of rainfall in the highest quintile are observed during the active MJO phase. Other influences on the monsoon at Darwin include upper troughs137 and equatorially-trapped Rossby wavesequatorially-trapped Rossby waves.138

The unusual phenomenon observed during TWP-ICE was the suppressed period of relatively small rainfall, together with the three days of clear conditions over Darwin with no rainfall. We now consider these three monsoon regimes in more detail.

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.2 The active monsoon

IR satellite image, MSLP and 900 hPa vorticity, 2300 UTC sounding, radar image of active phase convection
Fig. 9F1.6. (a) An IR satellite image for 1930 UTC or 1000 LST, (b) Bureau of Meteorology model analysis of MSLP and 900 hPa vorticity at 0000 UTC, 18 Jan 2006 and (c) 2300 UTC sounding at Darwin for an active phase of the monsoon on 17 Jan 2006. (d) Sample radar image of active phase convection.
video icon Animation of enhanced IR images of the active monsoon period

The active monsoon is associated with widespread, deep tropical convection, indicated by cold clouds in the IR image (Fig. 9F1.6a); although some cold clouds may be cirrus as IR cannot distinguish between precipitating convection and cold cirrus (Chapter 2, Section 2.5.2Chapter 2, Section 2.5.2). The associated synoptic pattern is a deep low over the Kimberley, directing west to northwesterly winds over northwest Australia and surrounding waters. The Monsoon Trough (MT) is indicated by the east-west oriented cyclonic vorticity maximum. Equatorward of the MT, the flow is converging into the low, resulting in the observed cloudiness and vertical motion profile (Fig. 9F1.6a,c). The sounding shows a typical active monsoon profile with a small dewpoint depression through the depth of the troposphere and a lapse rate close to moist adiabatic. The CAPE is typically small during the active monsoon. The wind profile is westerly to approximately 400 hPa with easterly winds above that. Drosdowsky (1984)139 defined the active monsoon in terms of the wind profile, with mean westerly zonal winds to 500 hPa and mean easterly zonal winds above 300 hPa.

Which weather elements are likely to be important in an active monsoon environment? What timing for the onset and cessation of these events might be appropriate and why? (Type your answer in box.)

Feedback:

Below is an example of the evolution of convective weather expected during an active monsoon; as expressed in a Terminal Aerodrome Forecast (TAF).

TAF YPDN 171802Z 1718/1818 34015KT 9999 SCT020
TEMPO 1718/1802 30020G40KT 1000 TSRA BKN010 SCT020CB
INTER 1802/1810 30020G40KT 3000 +SHRA BKN010
TEMPO 1810/1818 31020G40KT 1000 TSRA BKN010 SCT020CB

The Terminal Aerodrome Forecast (TAF) for Darwin shows periods of reduced visibility, lowered cloud base and precipitation in the form of heavy rain showers (+SHRA) and thunderstorms with rain (TSRA) throughout the validity period of the forecast which is 24 hours from 1800 UTC (0330 LST). An INTER means that conditions persist for periods of 30 minutes or less, a TEMPO for periods between 30 minutes and 1 hour.

During the thunderstorms described by the TAF above, the visibility is down to 1 km and in heavy showers to 3 km. The term BKN010 refers to low cloud with a base of 1000 feet, covering between 5 and 7 oktas (eighths) of the sky. The 24-hour coverage is consistent with the widespread cloud cover observed and the presence of synoptic-scale convergence and upward motion (Fig. 11F1.6). The focus of deep convection during the night and morning hours (between 1000 UTC = 1930 LST and 0200 UTC = 1130 LST) implies that deep convection is more likely to be nocturnal during the active monsoon, characterizing the airmass as maritime. The use of the TEMPO for this length of time is designed to include the time of potential enhanced convection and associated reduced visibility and cloud base due to the convection and enhanced by the wet bulb process. The peak in number and strength of updrafts does not typically occur until after dawn (about 0700 – 0900 LST).

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.3 The Break Monsoon

In contrast to the active monsoon, clouds are more isolated during the break periods (Fig. 9F1.7), often coastal, due to triggering on the sea breeze, and westward propagating. The MSLP/vorticity plot shows that the MT is to the north of Darwin, extending from the Arafura Sea into the Coral Sea. A region of cyclonic vorticity lies along the west coast of Australia extending into a heat low.

What differences do you observe between the trace (sounding) for the break monsoon period (shown below in 9F1.7c) ) and the active monsoon? (Type your answer in box.)

IR satellite image, MSLP and 900 hPa vorticity, sounding, radar images of break phase convection
Fig. 9F1.7. (a) An IR satellite image for 0230 UTC or 1700 LST, (b) Bureau of Meteorology model analysis of MSLP and 900 hPa vorticity at 0000 UTC 7 Feb 2006, and (c) Darwin 2300 UTC sounding for a break phase of the monsoon on 6 Feb 2006. (d) Sample radar images of break phase convection.

video icon Animation of enhanced IR images of the active monsoon period

Feedback:

The main features of the sounding are easterlies through most of the troposphere compared to the westerlies of the active monsoon. The shallow westerlies near the surface are a result of the heat low. The zig-zag pattern in the dewpoint profile indicate dry air in mid-levels, referred to as dry slots.

Where on the satellite image, in Fig. 9F1.7, do you expect the sea-breeze front to be found over northern Australia? (Type your answer in box.)

Feedback:

Where on the satellite image do you expect the sea-breeze front to be found?

IR satellite, radar reflectivity,
Fig. 9F1.8. (a) An IR satellite image and (b) radar reflectivity image (right) for a break monsoon period. (c) Radar reflectivity images showing before and (d) after westward propagating convection encounters the sea breeze.

Convection usually occurs at the leading edge of the sea-breeze front,140 where the warm and moist inland air of the prevailing flow is lifted to its level of free convection. The orientation of the prevailing flow determines the preferred locations of convective development (Fig. 9F1.8). Convective rolls are also generated inland. The air mass coastward of the sea-breeze front is indicated by the cloud free region along the coast. On the radar image, the sea-breeze front is indicated by the line of convection parallel to the coast. Convection along the Coburg peninsula is indicative of the convergence of sea breezes (Fig. 9F1.8b).

The sea-breeze front also interacts with existing convection. In Fig. 9F1.8c, the sea-breeze front is seen as a light blue line oriented from Humpty Doo (HDoo) to Finnis Range (Finn). A thunderstorm propagates in from the southeast. Once the storm reaches the sea-breeze front, the outflow interacts with the sea breeze to initiate fresh convection, in this case, a squall line propagating to the northwest.

Compare the Darwin TAF for the break period (below) with the one for the active periodactive period. What differences do you observed for the wind? How does this relate to the differences in synoptic regime? What differences are observed in the key weather elements and timing?

TAF YPDN 061611Z 0618/1818 22007KT 9999 SCT020 FM0802 30014KT 9999 SCT030
TEMPO 0706/0612 10015G35KT 1000 TSRA BKN010 SCT020CB

(Type your answer in box.)

Feedback:

The winds are northwesterly in the active monsoon but here the wind is southwesterly turning northwest during the morning. Thunderstorms are forecast during the afternoon and evening, compared to showers and storms for the active monsoon. The TEMPO is diurnal rather than through the period, indicating that the trigger convection is due to the sea breeze and surface heating.

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.4 Comparison Between the Active and Break Periods

Given the mean diurnal cycle for the Australian-Indonesian monsoon shown in Section 5.3.7.2Section 5.3.7.2, what differences would you expect between the active and break periods for a place like Darwin?

(Type your answer in box.)

Feedback:

The active and break monsoon environments have different synoptic forcing and air masses. These differences should be reflected in the diurnal cycle of the resulting deep convection, as has been suggested by the TAFs of the activeactive and break break periods shown earlier. Figures 9F1.9 and 9F1.10 compare the diurnal cycles of convection for different phases of the monsoon.

diurnal cycle of the number of cells per day
Fig. 9F1.9. The diurnal cycle of the number of cells per day with 45 dBZ reflectivities for the active monsoon (left) and break monsoon (right) at Darwin.

The break period has a strong diurnal signal, with a peak at 1400 LST. The timing of this peak is location dependent. It depends on the day to day synoptic forcing, sea-breeze cycle, and occurrence of earlier convection which may suppress the environment. The active period has a relatively flat diurnal cycle, with a weaker diurnal maximum at 1600 LST, compared to the break, and a morning peak at 0700 LST. The relatively flat diurnal cycle is consistent with the maritime nature of the air mass.

mean reflectivity versus height
Fig. 9F1.10. The mean reflectivity versus height for the active monsoon (left), break monsoon (middle) and buildup environment (right) from Gunn Point Radar, Darwin.141

Another way to illustrate the diurnal cycle is to compare the mean reflectivity versus height (Fig. 9F1.10). The active monsoon has a very weak diurnal cycle with maximum values at 0930 and 1530 LST. The break period has a flat diurnal cycle except for the pronounced afternoon peak at 1530 LST when the mean reflectivity increases by 10 dBZ over most of the depth of the troposphere. The buildup profile is typical of the early wet season, when the surface moisture is still increasing. The echoes are not as deep as the break period or as large for a given height, indicating weaker updrafts. This is due to the entrainment of drier environmental air in the boundary layer. The gradual increase in reflectivity during the diurnal cycle is consistent with the mechanism by which multiple plumes moisten the atmosphere and allow larger rain droplets to form.

icon_think What differences will the amount of convection make to the thermodynamics of the active and break regions and vice versa?

Active or break environments occur relative to the monsoon trough, as shown in Fig. 9F1.11. In the southeasterly stream poleward of the monsoon trough at O, dry air advection results in the dry slots observed in the dewpoint profile. Equatorward of the monsoon trough at X, moist maritime air is lifted in the convergent region to produce a deep moist profile. Fig. 9F1.11 illustrates that, as the monsoon trough migrates poleward, winds shift from easterly to northeasterly with southeasterly flow in the upper troposphere to deep monsoon westerly with easterly flow aloft. Tropospheric moisture increases with the change in trajectories and synoptic forcing.

Time 00 Hour

   Click the O to see an aerological profile. Click the X to see a cross section animation.

Time 00 Hour
Image Image

Time 12 Hour

   Click the O to see an aerological profile.

Time 00 Hour
Image

Time 24 Hour

   Click the O to see an aerological profile.

Time 00 Hour
Image
Fig. 9F1.11. Schematic of active and break environments relative to the monsoon trough. Cross section, seen in the Time 00 Hour tab, adapted from McBride and Frank 1999.142

Figure for print version
4-panel image showing sample profiles and cross section for active and break environments (Fig. 9F1.11).

The cross section (shown by clicking the X on the image in the Time 00 Hour tab of Fig. 9F1.11) illustrates the difference in CAPE and lapse rate between the active and break period environments. Latent heat release in the mid to upper troposphere warms the environment while evaporation of precipitation cools the lower troposphere, stabilizing the lapse rate. Spreading near surface cold pools reduces the CAPE by bringing down cooler and drier air from aloft. During break periods, shortwave heating of the surface and longwave cooling of the atmosphere destabilize the troposphere and allow CAPE to recover.

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.5 The Suppressed Monsoon

Refer back to Fig 9F1.5. What kind of synoptic environment could produce a suppressed regime?

(Type your answer in box.)

Feedback:

IR satellite, mslp and 900 hPa vorticity, sounding and radar images of suppressed monsoon
Fig. 9F1.12. (a) IR satellite image for 1930 UTC or 1000 LST, (b) BoM model analysis of MSLP and 900 hPa vorticity for 0000 UTC 28 Jan 2006 and (c) 2300 UTC Darwin sounding for a suppressed phase of the monsoon, 27 Jan 2006 (d) Sample radar images of a suppressed monsoon phase.
video iconAnimation of enhanced IR images of the suppressed monsoon period.

The suppressed monsoon over Darwin is due to a deep low over central Australia (Fig. 9F1.12). Such deep lows are referred to colloquially as ‘landfoons’ due to their structural similarity to tropical cyclones (also known as typhoons) in the satellite imagery and their potential to become tropical cyclones were they over the warm, tropical ocean.143 The MSLP/vorticity chart shows that the monsoon trough is well to the south of Darwin, together with the associated convergence. The flow is southwesterly rather than the west to northwesterly flow associated with an active monsoon.

Compare the trace (sounding) of the suppressed monsoon to the trace for the active monsoon. How is the wind profile similar/different? How is the dewpoint profile different?

(Type your answer in box.)

Feedback:

The winds are strong westerly as is the case for the active monsoon, but the meridional component is southerly. The ‘dry slots’ in the dewpoint profile look like those in the break period monsoon profile. The suggestion is that the trajectories are different due to the location of the low; advecting drier air from further south. Examination of model moisture fields and backward trajectories confirms this.

What differences will the drier trajectories produce in the Darwin? Is deep convection likely?

(Type your answer in box.)

Feedback:

Below is a description of the weather situation including an example TAF.

TAF YPDN 271613Z 2718/2818 27020G30KT 9999 BKN020
INTER 2718/2818 26020G40KT 4000 SHRA BKN010

The TAF indicates an INTER (less than 30 minutes at a time) showers only which indicates a relatively suppressed environment, i.e., no deep convection. Note that Fig. 9F1.5 indicates that, as the low moved further south, conditions became more suppressed so that eventually no showers were observed.

The occurrence of the suppressed monsoon highlights the shortcomings of zonal wind only based definitions of monsoon onset. More work is required to more rigorously define the regimes of the NAM.141

Focus 1: The Australian-Indonesian Monsoon »
9F1.2 Regimes of the North Australian Monsoon »
9F1.2.6 Summary of NAM Regime Differences

derived mean vertical motion and cloud frequency from the Millimeter Cloud Radar
Fig. 9F1.13. The derived mean vertical motion (left) and cloud frequency from the millimeter cloud radar that corresponds to the different observed monsoon regimes during TWP-ICE (and marked in Fig. 9F1.5).131

The active monsoon is dominated by deep upward motion, reaching a maximum near 6 km, and a large cloud frequency (red line in Fig. 9F1.13). Although the break monsoon period contains some intense storms, their isolated nature and differences in the large scale forcing means that the mean vertical motion is much less than the active monsoon (blue line in Fig. 9F1.13). The suppressed monsoon has very weak mean vertical motion, and the vertical cloud frequency profile shows the prevalence of shallow convective cloud mostly below 3 km, together with the cirrus between about 10 and 14 km. The cloud free period is unsurprisingly associated largely with subsidence.

Focus 1: The Australian-Indonesian Monsoon »
9F1.3 Storm Types of the North Australian Monsoon

This section examines some of the convective weather systems associated with the NAM. It is not an exhaustive treatment.

Focus 1: The Australian-Indonesian Monsoon »
9F1.3 Storm Types of the North Australian Monsoon »
9F1.3.1 Wet Microbursts

A wet microburst is a thunderstorm which produces damaging surface winds associated with significant precipitation at the surface and a low cloud base (Fig 9F1.14). Typically, the moisture extends to about 500 hPa with a dry layer above and the wind shear is weak. The low cloud base is due to high relative humidity near the surface, inhibiting evaporation. A warm cloud depth of greater than 10000 ft allows the collision and coalescence process to produce large rain drops. These conditions imply that precipitation drag is important in forming the downdraft. These storms occur during active and break monsoon conditions.

A schematic (left) and sounding (right) for a wet microburst
Fig. 9F1.14. A schematic (left) and sounding (right) for a wet microburst for Darwin, 2300 UTC 31 January 2000.

On 31 January 2000 wind gusts of 100 and 150 km h-1 were produced by a sustained wet microburst of about 30 minutes in duration. Figure 9F1.15 shows the Doppler velocities for a wet microburst. Figure 9F1.15 also shows the effect of large CAPE on a wet microburst environment. Large CAPE result in strong updrafts which produce elevated strong reflectivity echoes, making it possible to detect an impending downburst before it occurs. For small to moderate CAPE (< 2000 J kg-1) the first echoes are observed at about 3–6 km (10–19000 ft). These typically produce non-severe wind gusts. For larger CAPE, first echoes are observed at about 7–9 km (22000–30000 ft).

Doppler velocities for a wet microburst, 20000 feet CAPPI reflectivity
Fig. 9F1.15. (a) Doppler velocities for a wet microburst and (b) 20000 feet CAPPI reflectivity scan (top) and RHI through the same storm (bottom) for a wet microburst for Darwin radar 14 November 2001.

Focus 1: The Australian-Indonesian Monsoon »
9F1.3 Storm Types of the North Australian Monsoon »
9F1.3.2 Dry Microbursts

Schematic and sounding for a dry microburst
Fig. 9F1.16. (a) Schematic and (b) sounding for a dry microburst for Alice Springs, 2300 UTC 2 November 1992.144

Dry microbursts are a feature of inland Australia in an environment of deep easterly flow where the boundary layer is deep (up to 16000 ft above ground level) and dry. These storms produce damaging winds at the surface with no precipitation. Updrafts are weak due to low CAPE and vertical wind shear is weak. Hence, the downburst is produced by evaporation. The trace shown in Figure 9F1.16 was observed at Alice Springs aerodrome in 1992, and produced wind gusts of 72 and 94 km h-1. These storms are difficult to forecast because mixing with the hot environmental air and weakens the negative buoyancy of the downdraft. These storms occur during active and break monsoon conditions.

Focus 1: The Australian-Indonesian Monsoon »
9F1.3 Storm Types of the North Australian Monsoon »
9F1.3.3 Continental Squall Lines

Continental squall lines occur during break phases of the monsoon and can produce potentially damaging surface winds. A typical continental squall line, approaching Darwin from the east, consists of a leading edge of deep convection with a trailing stratiform region (Fig. 9F1.17).

Darwin radar reflectivity image from 3 February 2003 of a squall line
Fig. 9F1.17. Darwin radar reflectivity image from 3 February 2003 of a squall line approaching Darwin.
video icon Animation of radar reflectivity showing bookend vortices.

The basic conceptual model of a squall line is a line of convection propagating perpendicular to the mean wind shear vector or mean steering flow (COMET’s Convective Storm Matrix). The strong unidirectional wind flow provides wind shear to balance the vorticity generated at the leading edge of the spreading cold pool by buoyancy gradients to generating new convective cells at the leading edge (Fig. 9F1.18). The wind profile also provides winds to ingest in the convective downdraft as surface gusts. The cold pool is produced by the evaporation of precipitation falling through unsaturated environmental air, known as the dry slot.

developing break period continental squall line and A 2300 UTC sounding at Darwin
Fig. 9F1.18. (a) Structure of the initial development of a break period continental squall. (b) A 2300 UTC sounding at Darwin showing the wind, temperature and moisture profile typical of a break period continental squall line.

One of the signatures of a severe squall line is the rear inflow jet. Strong rear inflow jets occur in large CAPE, strong vertical wind shear environments. The rear inflow jet accelerates the flow into the rear of the squall line and hence increases the potential surface wind gusts.

Eventually, the cold pool outruns its parent convection and the squall dies. At this stage, the strongest surface winds occur as the rear inflow jet reaches the surface in the downdraft (Fig. 9F1.19). Evidence of a rear inflow jet and imminent surface wind gusts can be obtained from Doppler radar. Fig. 9F1.19 shows Doppler imagery with double range folding to 25 m s-1 (~ 50 kts) 9 minutes before the measured gust of 58 knots at the surface. A thin region of dark blue indicates this range folding, moving through orange shades and then through again to dark blue "circular" regions.

squall line in the late stages of its development and  the Doppler velocity image
Fig. 9F1.19. (a) A schematic of a squall line in the late stages of its development and (b) the Doppler velocity image of a squall line 9 minutes prior to damaging winds being observed near the surface.

Another feature of potential severity for squall lines is the bookend vortex. Bookend vortices result from vorticity at the leading edge of the cold pool being lifted and tilted by the updraft (reference). The bookend vortices can increase the strength of the rear inflow jet and cause part of the squall line to bow outwards as a bow echo. Figure 9F1.17 shows a bow echo, as well as curved elements in the reflectivity at either end of the leading edge, indicative of bookend vortices.

Focus 1: The Australian-Indonesian Monsoon »
9F1.3 Storm Types of the North Australian Monsoon »
9F1.3.4 Monsoon Squalls

A monsoon squall, also referred to as maritime squalls, form in an environment of deep westerly winds. The lines occur in regions of moderate to strong wind shear in the lower troposphere, and with a block of strong westerly winds. Figure 9F1.20 shows an example of a series of linear features with strong surface winds moving over the Tiwi Islands. A large dry slot exists between 800 and 500 hPa. One monsoon squall on 3 January 2005 produced several convective lines resulting in gusts observed up to 110 km h-1.

Radar reflectivity image and (b) radiosonde ascent
Fig. 9F1.20. (a) Radar reflectivity image and (b) radiosonde ascent (bottom right) for 1 Feb 2006.

Focus 1: The Australian-Indonesian Monsoon »
9F1.4 The Monsoon over the Maritime Continent

Focus 1: The Australian-Indonesian Monsoon »
9F1.4 The Monsoon over the Maritime Continent »
9F1.4.1 Hector and Convection over Flat Islands

Hector is a thunderstorm complex occurring over the Tiwi Islands, with a height > 15 km, and a horizontal extent of the > 30 dBZ echo of at least 200 km2.145 Hector forms during the break periods of the monsoon. The zonal tropospheric wind flow during this period is easterly, providing the steering flow as is the case for tropical squall lines. The direction of the low-level flow determines where convective initiation starts (Fig. 9F1.21). Figure 9F1.21 also shows the evolution of Hector when the low-level flow is westerly, such as occurs when there is an active heat low over mainland Australia. Convection is preferentially initiated on the eastern side of the Tiwis on the sea-breeze front (Fig. 9F1.21). Weaker convection is initiated on the western coast on a weak sea-breeze front. As the initial convection evolves from updraft dominated (a) to downdraft dominated (b), the spreading cold pool becomes the new site of convective initiation as the cold pool vorticity balances the wind shear. Further lifting occurs as Hector propagates westward and the cold pool interacts with the western sea-breeze front. A radar sequence of a developing Hector is shown in Fig. 9F1.22.

Fig. 9F1.21. A schematic of the evolution of Hector, a propagating mesoscale convective system over the Tiwi Islands. Adapted from Carbone et al. 2000.146
radar reflectivity sequence showing the evolution of Hector
Fig. 9F1.22. A radar reflectivity sequence showing the evolution of Hector. White lines indicate sea-breeze boundaries, red lines are the outflow from the east coast convection and the green line the outflow boundary of the west coast convection (Wilson et al. 2001).145

The key element of Hector is that it occurs on an island with little rugged topography, allowing the entire mesoscale convective system to propagate across the island. The site of initial convective initiation is determined by the low-level flow, and thereafter Hector propagates to the west.

What do you think happens in the case of islands with significant rugged topography?

(Type your answer in box.)

Feedback:

We will explore those situations in the following section.

Focus 1: The Australian-Indonesian Monsoon »
9F1.4 The Monsoon over the Maritime Continent »
9F1.4.2 Timor and Convection over Significant Topography

Timor is an island with significant mountains. The highest point reaches 2963 m (9721 ft). Figure 9F1.23 shows the situation for two days in February 2006 with similar gradient level wind flow (3000’ above sea level). However differences in the wind profiles give rise to differences in convective cloud initiation and evolution (compare the left and right panels of Fig. 9F1.23). On the 8th the flow is east to northeast whereas on the 10th (11th was unavailable) flow is weak for much of the depth of the troposphere. On the 8th, the convection appears to form further inland along the spine of the island and is steered along the ranges. Later on the 8th, shallower convection in the Timor Sea is steered towards the northeast by the lower tropospheric flow. The slightly weaker near surface flow on the 11th allows convection to be generated near the coast, and on the ranges to the West of Dili. The steering flow then carries this convection into the Savu Sea.

What impact will these different situations have on forecasting for Dili airport? Review Fig. 9F1.23 before making your forecast.

Infrared (IR) satellite imagery

streamline/isotach analysis at gradient level and Skew T log P diagrams
Fig. 9F1.23. Infrared (IR) satellite imagery (top), streamline/isotach analysis at gradient level (3000 feet above sea level; middle) and Skew T log P diagrams of 0000 UTC soundings from Kupang (bottom) for 8 Feb (left) and 11 Feb (right) 2006.

(Type your answer in box.)

Feedback:

An expert response:

TAF WPDL 080105Z 0801/0814 31008KT 9999 BKN025
FM0813 14003KT 9999 SCT020
PROB30 INTER 0805/0810 5000 SHRA BKN010

TAF WPDL 110107Z 1101/1114 29011KT 9999 SCT025
PROB30 TEMPO1105/1111 1000 TSRA BKN010 SCT020CB

A chance of thunderstorms and rain (30% probability) at Dili was forecast on the 11th as the steering flow was easterly, possibly advecting the storms off the ranges and over Dili. On the 8th the steering was along the ranges so only showers and fewer clouds were forecast at Dili.

Focus 1: The Australian-Indonesian Monsoon »
9F1.4 The Monsoon over the Maritime Continent »
9F1.4.3 Papua New Guinea

Flow relative to terrain during trade wind flow, May to August, and monsoonal flow, January to April. Yellow and white arrows show prevailing flow and point to general locations of rainfall maxima
Fig. 9F1.24. Flow relative to terrain during trade wind flow, May to August, and monsoonal flow, January to April. Yellow and white arrows show prevailing flow and point to general locations of rainfall maxima during the trade wind and monsoon season, respectively.

Papua New Guinea’s (PNG) climate may not be described as truly monsoonal as there are no reliable periods of nil or near nil monthly rainfall as there is in Darwin, for example. Rainfall on the highlands is in the range 2500-3500 mm, with somewhat lesser values in the lowland areas. For example, Port Moresby has less than 1000 mm per year. Despite being tropical, frosts can occur above 2200 m and snow settles above 4000 m.

PNG rainfall is enhanced over the tropical oceanic regions due to two factors:

  1. the mountains of the Maritime Continent
  2. the West Pacific warm pool

Both contribute to the maintenance of high θe air in this area. From routine satellite imagery, it can be seen that, cloud associated with the ITCZ affects PNG all year. However, the associated wind circulation patterns and the nature of the weather disturbances vary seasonally (Fig. 9.24).

During the southeasterly trades, convergence occurs where flow is onshore and undergoing frictional convergence and collision with nighttime land breezes (Fig. 9F1.24). During the monsoon, these convergences occur in different locations (Fig. 9F1.24). Throughout the year, enhanced uplift due to local topography leads to convection.146 Mountain-valley circulations also contribute to local convergence and convection.

Focus 1: The Australian-Indonesian Monsoon »
9F1.4 The Monsoon over the Maritime Continent »
9F1.4.4 The Indonesian-Malaysian Region

Annual rainfall statistics for Peninsular Malaysia and Singapore
Fig. 9F1.25. Annual rainfall statistics for Peninsular Malaysia and Singapore.

As was the case for PNG, enhanced topography can play a key role in the seasonal variation of rainfall throughout the Maritime Continent.147 Close to the equator there is a much less marked difference between wet and dry seasons than for the NAM. For example, Singapore has a relatively flat rainfall distribution (Fig. 9F1.25). The local rainfall minima occur in July and February under the influence of dry trade wind flows. The further north along the east coast, the greater the topographical enhancement of rainfall during the Boreal Winter (northeast) Monsoon. For example, the November rainfall at Kota Bahru is twice that of Singapore. Likewise, on the northwest coast a secondary peak exists in rainfall during April-May due to the southwesterly cross equatorial flow and the elevated topography.

Annual rainfall statistics for Java
Fig. 9F1.26. Annual rainfall statistics for Java.

Java has a distinct dry season (Fig. 9F1.26), particularly in the south when under influence of southeast trade winds in the southern hemisphere (May to September). Likewise, there is a distinct wet season when influenced by Boreal Winter Monsoon (northeast trade winds). Sumatra (Fig. 9F1.27) also has a dry season under the influence of the southern hemisphere trades (May to September). The wet season is bimodal where mountains are able to enhance the northeast and southwest flows during boreal winter and summer respectively.

Annual rainfall statistics for Sumatra
Fig. 9F1.27. Annual rainfall statistics for Sumatra.

Intraseasonal variability

As with northern Australia, the MJO and various tropical wave modes such as the Kelvin wave, n=1 equatorial Rossby wave and mixed Rossby-gravity wave are responsible for intraseasonal variability over the Maritime Continent (Chapter 4, Section 4.1Chapter 4, Section 4.1) and references therein). Real-time monitoring of the MJO (Table 4.1)Real-time monitoring of the MJO (Table 4.1) and various tropical wave modes (Table 4.2various tropical wave modes (Table 4.2) is done routinely by NOAA and the Australian BoM.

However, as illustrated earlier in this section, knowledge of local topography is essential for forecasting rainfall over the Maritime Continent. For example, Haylock and McBride (2001)148 showed that the coherence of rainfall anomalies during December to February for two rainfall stations on Java separated by less than 100 km was small (correlation of 0.18).

Focus 1: The Australian-Indonesian Monsoon »
9F1.5 Summary of the North Australian Monsoon

The differences between active, break and suppressed monsoon regimes for the North Australian Monsoon (NAM) are summarized in Fig. 9F1.28. The NAM is a result of the annual land-sea thermal contrast that develops during Austral Spring superimposed on the seasonal migration of the Hadley cell. The NAM is modulated by the Madden Julian Oscillation, upper troughs and equatorial waves, as well as by an inherent transient component of monsoon systems.125 Deep lows that move inland over Australia can produce dry southwesterly winds known as a suppressed or inactive monsoon. Significant enhanced topography over the Maritime Continent modifies the large scale synoptic flow such that knowledge of local topography is necessary to determine the seasonality and intraseasonality of deep convection.

Summary of differences between the different regimes of the North Australian Monsoon
Fig. 9F1.28. Summary of differences between the different regimes of the North Australian Monsoon.

Figure 9F1.28 shows a summary of the major features of the NAM. Like the Indian monsoon, the NAM undergoes alternating active and break monsoon periods with the migrating monsoon trough. The location of the trough exhibits an inherent transient nature but is also modulated by the MJO and equatorially trapped waves such as Rossby waves.

During the active monsoon, there is large scale forcing due to the monsoon trough, advecting a deep westerly, moist maritime air mass. Widespread cloud and precipitation occurs with relatively weak convective updrafts. The diurnal cycle is weak, with an overnight and morning maximum in convective activity due to its maritime nature but also an afternoon maximum over land due to boundary layer heating. Weather hazards, apart from tropical cyclones, include monsoonal squalls and flooding due to widespread, persistent rainfall from MCSs.

During break monsoon periods, widespread subsidence means that convection is forced locally on sea-breeze boundaries and is largely diurnal in nature. Short wave heating of the surface and long wave cooling of the mid troposphere contrast to the cold pool driven cooling of the surface and latent heating of the mid troposphere during the active monsoon. The result is isolated but more intense deep convection during the break period in the form of pulse convection, and various propagating lines of convection such as continental squall lines and Hector.

A third regime of the monsoon occurs when the monsoon trough is found in central Australia. Under these conditions, dry air wraps around a deep low, sometimes in the form of a “landfoon”, resulting in dry westerly winds over northern Australia and convectively suppressed conditions.

Focus 2: The Tropical Forecasters' Perspective

In order to understand how a tropical cyclone forecast is created, we interviewed two forecasters from NOAA's NHC (RSMC with responsibilities for the North Atlantic and Eastern Pacific) and one forecaster from Météo-France La Réunion (RSMC with responsibility for the South Indian Ocean). They also tell us about the path they took to tropical cyclone forecasting and changes in the forecast process during their careers.

Focus 2: The Tropical Forecasters' Perspective »
9F2.1 National Hurricane Center Forecasters (Audio Interviews)

Audio interviews were conducted with the NHC forecasters, Dr. James Franklin and Dr. Lixion Avila, on 9 June 2009. Here are edited versions of those interviews.

Dr. James Franklin, National Hurricane Center Forecaster

Dr. James Franklin

Question 1

How and when did you decide to become a tropical cyclone forecaster? What was your path? Did you do anything special in elementary or high school to further your goals?

Answer:

The path really began as a 6 year-old experiencing Hurricane Cleo when it went over my house, … but that's really what triggered my interest.

I didn't start out in forecasting at all. I was a researcher for 17 years, flying into storms with the hurricane research division of NOAA; did some operationally related research towards the end of that period when the GPS dropwindsonde got developed and spent some time looking at how hurricane winds behaved, the structure of those winds with height in the eye wall. That work caught the attention of some of the folks at the National Hurricane Center and they actually approached me about whether I had some interest in doing it. I hadn't really thought about it at all until they talked to me about it.

A lot of things in life I think are fortuitous. Being exposed to some hurricanes growing up; while I was in school at MIT, Bob Burpee who was at the Hurricane Research Division, was on sabbatical. I took his course on tropical meteorology, I guess I did well enough to have him approach me about a position.

All through high school, I had two main interests: one was meteorology the other was astronomy. Meteorology seemed to be the more interesting field, at least had more of an influence on people's lives and was a little bit more exciting. So that was the field I ended up taking. But I knew that going into college, that that's the kind of thing that I wanted to do, weather in general, I didn't know it was going to be hurricanes at the time.

I did spend a fair amount of my undergraduate time at MIT taking meteorology with folks like Fred Sanders, Pauline Austin, and spent some time with Fred, Kerry Emanuel going back and forth across the New England coastal front in Fred's Rabbit. My master's thesis was going to be on the New England coastal front. My good friend, Frank Marks, who was at MIT at the time, agreed to look over the collection of the data, while we went out and took the observations. Came back and found out the Frank had erased all the data instead of saving it and I was left with no thesis. Bob Burpee took me at the Hurricane Research Division anyway. A couple of years later, we came up with another thesis topic.

Question 2

What process do you use to forecast TC? What tools? Does your answer differ between track, intensity, size and rainfall forecasts?

Answer:

Track
Many years ago people could outfox the guidance at least in terms of track forecasting, but the numerical models have gotten so much better over the last 15, 20 years, in fact, our track forecasts are now about twice as good as they were 15 years ago. It's really very difficult for a forecaster to out integrate numerical models.

A very powerful technique in all of meteorology not just hurricanes is the idea of consensus. Get 3 or 4 or some group of skillful numerical models and you combine them. That's our goal; every time we sit down to make a forecast, that there is something that we can add to try and improve on that consensus. Is there a model that isn't initialized well? Do we recognize a situation when a certain model tends to perform well or tend to perform less well in? Very often your expectations for intensity play into the track forecast, but it all centers around the notion of a consensus and then trying to make moves in one direction or another from that.

One aspect of the forecast process has to do with presenting a consistent picture to our users. We have a very strong continuity constraint from one forecast to the next. We tend to make small increments on the forecast that came before us, improve what you inherited. I haven't talked about intensity so let me go on to that a little bit.

Intensity
Intensity forecasting is a little bit different then the track forecasting in the sense that guidance is not nearly so advanced. The forecast on the other hand does a better job than our intensity guidance. We have 4 intensity guidance models, 2 are dynamical, and 2 are statistical. The human forecaster can see a lot more of what's going on with the storm in terms of its convective structure and how the wind field is organized in terms of concentric eyewalls. None of the kinds of core factors is really well incorporated into our existing intensity guidance. By seeing what's going on in the core, that's where it is the forecaster really adds value to the guidance and is able to contribute a lot more to the process.

Size
We also forecast the size of tropical cyclones to issue these wind radii forecasts, the maximum extent of hurricane force winds in each of 4 quadrants around the center. So we are actually ahead of ourselves there in terms of what we provide relative to what we can do skillfully. So our error in even estimating that parameter is on the order of 50%. That a really tough one. About all that we have to help us with those are climatology and persistence models, the CLIPER model for example for wind radii. We have presumption that as a storm strengthens generally is it going to larger. After a storm is complete, we do what's called a best track, a post analysis of all the available data to create a permanent record, our best record of what happened with that particular storm: location, pressure, maximum sustained wind speed and the status, whether it's a tropical, subtropical, extra tropical. Until very recently we did not do a best track on the wind radius. Until you get to 2004, 2005, those are all operational estimates. They were not reviewed after the fact, those data certainly are not the same quality as the final best track intensity estimates. We've also got very few, sometimes no, real measurements of how large these radii really ought to be. From looking at the cloud shields, surface observations (these are very few), we have some additional tools to help us there. The AMSU, microwave instrument also gives us some size estimates.

Rainfall
Responsibility for rainfall forecasts lies with the Hydrometeorological Prediction Center. They are looking at model guidance, analogs, and previous storms. In our advisories now, we get the guidance for rainfall from HPC.

Question 3

Have ensemble model predictions changed your process?

Answer:

Ensembles are a big part of the tropical cyclone forecast process. Two primary methods would be to take a single model and run it repeatedly using slightly different initial conditions. That's one way. That has not been very successful in operational tropical cyclone forecasts. You can also form a consensus from different models.

When the members that make up an ensemble are independent you get a much better ensemble mean. We're also finding for intensity forecasting, if you form a consensus of the four main intensity models, it is much better on average than any of those four models individually. I think part of the reason for that is those models are very independent. They're not even the same type, you have two statistical models and you have two dynamical models and they're quite independent and it's that independence that really helps you. When members of an ensemble are independent, the errors tend to cancel, particularly when the synoptic situation is relatively simple, so we see this a lot in the eastern Pacific when the synoptic flows are simple. A lot of the errors in the models are random so if you can combine 3 or 4 of them you get a much better forecast then any individual one.

In the Atlantic the signal is not so strong. In the Atlantic we have stronger synoptic scale forcing, more complicated environments, midlatitude troughs coming down and a lot of other features in the environment and in that situation the different models are handling these features in different ways. The consensus concept in the Atlantic is a little bit less effective than it is in the east Pacific because there is more of a systematic component to how the models behave.

Question 4

What's your day like when there is a TC to forecast? How is it different if there are a number of TC? Is it any different if the TC are in different basins or in the same basin?

Answer:

Forecasting shifts are divided in to three: day, evening and midnight shifts. The day shift is responsible for 2 forecasts at 11:00 AM and 5:00 PM. The evening shift is responsible for the 11 PM advisory. The midnight shift is responsible for the 5:00 AM advisory. The day shift is longer, more tiring, much more hectic with more people floating around and more of a media presence.

The forecast cycle basically runs for 3 hours. The 11:00 AM advisory, for example, starts at 8:00 AM with an aircraft reconnaissance fix. You spend about 15 minutes analyzing the data from the reconnaissance aircraft, initial location, initial intensity, initial motion, initial size, all the parameters that are going to go into initializing the numerical model guidance. You update the best track and then submit guidance. We get it back and from about 8:30 AM and in this case up until 10:00 AM is spent making the forecast, looking at the models, the guidance, water vapor imagery, sea surface temperature all the different parameters that are important to track and intensity. By 10:00 AM you have your forecast prepared and we do a conference call with other weather service forecast offices as well as other agencies in the federal government. HPC will be on there, to talk about rainfall; the Storm Prediction Center will be on there, to talk about tornado threats; the Navy is there; Homeland Security is there; a whole host of agencies are there where we discuss the forecast, coordinate any issues that need to be coordinated, like where watches and warnings might be. That call can last from 3 or 4 minutes to a half an hour.

After the conference call is done we then prepare the forecast. We write our discussions and a summary of our rational behind the forecast. We talk about things like forecast uncertainty, why we've analyzed it to be the intensity that we have, why we've chosen the forecast that we have. That's a very important product for us used by emergency managers, the general public helps to provide some context for the forecast. In that last 45 minutes we're writing the discussion, we're preparing the public advisory.

If there are multiple storms you may have to do that for two and on occasion I've had to write even three advisories at once in that three hour period. We do have 2 forecasters on shift, but sometimes we may be working as many as 5 storms simultaneously between the Atlantic and east Pacific. There are times where you really have to compress it. It really depends on what kind of storms you have to deal with. If we have a significant landfall going on or imminent, within a couple of days of landfall, one of the forecasters will focus on that storm exclusively and leave 2 or even 3 to the other person if they are a less difficult forecast situation. We will try, when we have more than 3 systems, to bring in somebody to help us out. They are called hurricane support meteorologists; they have some experience in putting together advisory packages. They come in and help us with the least complicated of the systems that we're working on so that folks from the marine tropical forecasting unit, they're the folks that do the marine forecasting, or they might be from the technical support branch here at the hurricane center. They do have meteorology degrees, so some of them do have experience writing advisory packages. They're all Hurricane Center employees.


Dr. Lixion Avila, National Hurricane Center Forecaster

Dr. Lixion Avila (English)

Question 1

How and when did you decide to become a tropical cyclone forecaster? What was your path? Did you do anything special in elementary or high school to further your goals?

Answer:

I wanted to be a hurricane forecaster since I was a kid in Cuba and I was always asking questions to the farmers and to the fishermen. But, actually, I didn't start doing that until I was able to finish what you call pre-university degree in Cuba. I entered the Met Service in Cuba but I always wanted to be a hurricane forecaster. After that I went to the United States and I got my Masters and Ph.D. and I was lucky enough to enter the National Hurricane Center and I've been a forecaster for almost 25 years.

I got my degree in Cuba and I worked as a forecaster. But you take care of all the weather systems including hurricanes and I did that for about 5 years.

What I didn't know when I was in elementary school is that you needed a lot of math and physics to study meteorology but actually I love math and physics so it turned out to be good. That's one of the things that really got me by surprise. When you're a kid you don't know that you need those tools, you thought it was more like a fun thing to do than really study hard.

When I was a little kid, one of the things that I enjoyed was to wait for the afternoon thunderstorms, especially in the hurricane season. I grew up near the beach so there was some hills in between the ocean and the beach. Sometimes, I see the thunderstorms coming from south and sometimes I see the storms coming from the ocean. And it was really wonderful for me to enjoy the development of the clouds. And it was really interesting to see that. I am glad that my parents put up with that and they always pleased me with that craziness. But it turned out to be the best for me in the world.

Question 2

What process do you use to forecast TC? What tools? Does your answer differ between track, intensity, size and rainfall forecasts?

Answer:

I've been doing this since 1971. I have seen how the tools have changed. Tremendously! In the '70s we were plotting the surface data by hand. We were getting, maybe, one map a day of a forecast of 24 hours at 500 mb. The facsimile; we even got 1 satellite picture or two satellite pictures a day. And that was probably the case in most of the Caribbean countries and probably not very different in the United States.

We began to get more and more satellite pictures…What really changed the way of forecasting is the development of numerical models and computer science. And, nowadays, we can use all these sophisticated computer models and the physics and dynamics that goes into models to predict hurricanes.

First thing we do in the morning, is to look at the entire globe and all the satellite pictures and look at the different systems. Then we emphasize the system that we think is going to do something or not. We look at the analysis of what's going on through the computer models, of course, using the, also, the conventional data. Before I wasn't able to integrate in my head 5 days in advance, now the computer models are able to give me a better estimate, at least, what could happen, or the possibilities that could happen in terms of the distribution of high pressures and low pressures.

Nowadays we make a 5-day forecast and the weather pattern that is going to affect that cyclone today, if it's in the Caribbean, that weather system is, perhaps, in the western Pacific now, then move to the east. So we need to look at the whole pattern. Either track or intensity, you have to look at the whole thing because the intensity change is related to, perhaps, an upper trough coming. It is more difficult, of course, the forecast of the intensity.

Size
At this moment when we make a prediction, if we don't have data, we don't even know the size of the system. So what we do is try to extrapolate. But we don't have any tools to predict changes in size other than climatology. Perhaps some of the numerical models would give us the size of the storm when they are moving and becoming extratropical in higher latitude. The models are doing a little better, but in terms of the deep tropics the change and size, it's very difficult to predict. What we do is just basically use extrapolation and when we get new data that tell us that the size is larger, we adjust with the new data.

Rainfall
In terms of rainfall, it's even more difficult. Rainfall is probably the cause of most of the deaths, for example, in the region of the Caribbean. But it's the same in most of the tropics when you even have a small, weak tropical depression that could produce 20 inches of rain and produce a tremendous amount of damage. And, unfortunately, many people are killed by the rainfall, especially by flash floods and all this orographic rain that you have when you have a weak tropical depression. Those are very difficult, difficult processes, both the size and the rainfall.

You know, the intensity of a tropical cyclone has nothing to do with the rainfall. It's basically the speed and the amount of convection that the system has. You can have a hurricane that can produce less rain then a weak tropical depression.

There are some old rules I learned from the old-timers and they use the number 100 divided by the speed of the tropical cyclone and you get the amount of inches of rain. And it's so interesting to see that some models, like the GFDL and others, when you compare with that rule the numbers on average turn out to be very close. The bottom line is that it's the speed of the system what matters.

Question 3

Have ensemble model predictions changed your process?

Answer:

Here at the National Hurricane Center, what we have been using is another type of ensemble. What we call the "consensus", which is not just the ensemble of one model but the consensus of different models. And, actually, that turns out to be one of the best ways of making a forecast. It appears that, when you make the consensus of different models, you cancel all the biases of the models and you end up having a better forecast by using all these consensus models.

Yes, it changed the process and makes my life, I would say, a little bit easier. But, still, you have to understand why each particular model is doing what it's doing. You cannot use models as a black box, you have to understand what goes into each model.

In many cases here, when we do the verification, the forecaster turns out to be better than all the different independent models. Because we are using all the information and we process it and we get, as I mentioned, we understand the strength and weakness of each model and we try to improve on that.

Question 4

What's your day like when there is a TC to forecast? How is it different if there are a number of TC? Is it any different if the TC are in different basins or in the same basin?

Answer:

Things have changed too, throughout the years. I do remember when we were 5 hurricane specialists and I have to do almost all of them. And now, luckily, we have more specialists and we get help from other colleagues here at the National Hurricane Center. We are prepared to have simultaneous tropical cyclones. Of course, the pressure is tremendous, especially if you have a hurricane that is threatening land areas. If it's a strong hurricane, we have to take care of the media. But, our emphasis is to be able to get all the information and try to make the best forecast possible.

Do I get nervous? No. Do I get excited? Yes! I do get very excited. I have to be in control, but always, what I like to do is emphasize on the science. I don't want to be biased by any of my feelings and I want to do the best job possible. But, it's a very interesting day. It's a very interesting day when you have a tropical cyclone. I presume that it is the same with a doctor when they have somebody that they want to cure or they want to improve their health. I want to make the best forecast.

I've been offered to work for insurance companies. I have been offered to work for TV. But, there is something about being here at the National Hurricane Center; that I have the "power" to name a system. You might think it's not important, but for me, it kind of means that I'm on top of the science and I'm doing this. For me, it's one of the fun things that I get from the job.

Focus 2: The Tropical Forecasters' Perspective »
9F2.2 Tropical Cyclone Centre Météo-France, La Réunion

Interview with Dr. Anne-Claire Fontan, tropical cyclone forecaster

1. How and when did you decide to become a tropical cyclone forecaster? What was your path? Did you do anything special in elementary or high school to further your goals?

I became a tropical cyclone forecaster at the RSMC/Tropical Cyclone Centre Météo-France/La Réunion 12 years ago, once I finished studying at the French school dedicated to meteorology “ENM” (Ecole Nationale de la Météorologie de Météo-France / Météo-France National School of Meteorology), located in Toulouse, France. This school gives a diploma in meteorology, which takes three years to complete (after either two years in a university-level college, or a Master of Science at the university).

Before this school, I was at university where I studied for a Masters degree in oceanography and meteorology at Marseille and Paris. In France, there is no way to specialize in meteorology until you have completed a bachelor or Masters degree or the “ENM”, but you need to choose a scientific path from high school.

Once you have graduated, and got the job at the RSMC/TCC La Réunion, you have to follow an extra two weeks formation in tropical meteorology. Afterwards you become a “trainee” in operations during several months at the RSMC. During this period you are given an additional formation and practice through tutoring with experienced TC forecasters. A TC forecaster is considered to be accomplished after one or two complete cyclonic seasons.

2. What process do you use to forecast TC? What tools? Does your answer differ between track, intensity, size and rainfall forecasts?

To forecast at the RSMC/La Réunion, we use a powerful workstation called SYNERGIE. This workstation displays and superimposes all the data a forecaster needs to work: observations, models, satellite imageries, radar, etc. There is a specific module dedicated to tropical cyclones called SYNERGIE CYCLONE which allows us to focus on tropical cyclone analysis and track and intensity forecasts. In addition to models, observations, images, and TC tracks plots, we have recently implemented the possibility to display directly the websites data we use daily in operation. These websites are mainly – and so not exhaustively - the tropical cyclones pages from the NRL, the CIMSS, the NOAA (QuikSCAT), the AOML (heat potential), the Australian BoM (MJO), ….

Our area of responsibility (Equator to 40°S and African coastline to 90°E) is mainly a maritime basin, except the western part between African coasts and 60°E. We rely indeed a lot on satellite data. Size and rainfall associated to the systems are “observed”, not yet specifically forecast. Every 6 hours, as we issue our warnings, we describe the size of the TC, based on the 30 knots and 50 knots winds, by using all the available observations; these are mainly received through scatterometer data - due to the maritime characteristic of our basin. We also describe the weather and the rainfall associated with the system. When a TC is forecast to approach or hit a landmass the “comments part” of the warnings specifies as well the inhabited areas the rainfall can concern in the next 24 to 36 hours. In this case, we use forecast fields as the precipitation rate, humidity, vertical velocity, …, of the best model.

Track forecast

We get the fields from the numerical models developed by different countries/centres to be able to track forecast; two models from Météo-France, a global one and a limited area one (over Southern Indian Ocean), one from the UKMO (United Kingdom Met Office), and the Ensemble Prediction System (EPS) average and the deterministic models from the ECMWF (European Centre). Since season 2004-2005 we get as well the “geopoints” (i.e. position and MSLP (Mean Seal Level Pressure) of the TC each 6 or 12 hours) of some of the American numerical models via the JTWC; GFDN, NOGAPS, AVNO, and consensus of different models computed at the JTWC. These models tracks are displayed on the workstation.

Thanks to the analysis of the fields from the models, the forecaster decides which scenario is the best. Afterwards, as statistics tend to show consensus of models lead to the better results, we average chosen models to make the track forecast. If philosophy of some of the models totally differs from the chosen one, we do not involve them in the average.

Intensity forecast

To forecast intensity, we need to know the current and follow-on environment of the system. Several tools are used. We study the products of the CIMSS to get the current environment and to get it for the few hours to come; upper level divergence and winds, low level convergence and winds, wind shear, shear tendency, and so on. We get the heat content thanks to the SSTs satellite data and the AOML website heat potential (depth of the 26°C isotherm). Humidity is assessed thanks to WV and MW imageries. Then we use the fields of the model estimated to be the best for the situation: θ’w at 700 hPa, divergence, convergence. And we have a look on the tendency of the different models, if ever they deepen or weaken the system.

3. Have ensemble model predictions changed your process?

For the past few years we received data from the Ensemble Prediction System (EPS) and it has changed the way we work and our results. We use it to further several goals. First of all, the EPS is used to assess the probability of cyclogenesis over the basin for the 10 coming days. Then the average of the 51 runs of the EPS is used as a ”deterministic model” and can be involved into a consensus of models to make the TC track forecast. Strike probabilities provided on each system by the ECMWF is used to manage the risk at La Réunion Island. The last goal, still under investigation, would be to use the EPS to provide cones of uncertainty for the RSMC forecast track.

4. What’s your day like when there is a TC to forecast? How is it different if there are a number of TC? Is it any different if the TC are in different basins or in the same basin?

We work in 12 hour shifts either day or night. These shifts range between 7.00 AM to 7.00 PM and 7.00 PM to 7.00 AM. We issue four series of warnings a day at 00, 06, 12, 18Z. So for example, for a day shift we have the 06 and 12Z warnings to issue.

At first we have the changeover and a detailed study of the current situation. At 08.30 AM we have the briefing for the people working at the centre. Straight afterwards starts the entry of the data in the software we use to prepare the 6 or 7 warnings which will be issued in both English and French at 10.30 AM (0630Z). Then we brief the local weather forecast service and if necessary (i.e. if the TC directly or indirectly concerns the weather on Réunion Island), we provide it with guidance and directives. We have a break between 11.00 AM and 12.00 PM.

Afterwards, we have a database dedicated to cyclogenesis to fill in, and the writing of the tropical weather outlook in both English and French, which will be issued at 03.00 PM. Meanwhile we write the “connection bulletin” which allows to keep the information within the team, and to give instruction for the three following days to the local forecast team.

The following warnings are prepared and issued at 04.30 PM. At the end of the shift, we have to update the archives of the day with messages, pertinent satellite images, and so on.

When there is a risk to manage on Réunion Island, we issue some extra warnings at 1.00 PM and 7.00 PM for the local authorities and for the public, and we answer to the media.

If ever there are two TC to deal with, it is double the workload! If there are two systems to monitor, with a risk to manage on the Island, a second cyclone forecaster comes to help. We get somebody in extra as well if ever there are more than two systems over the basin.

We have a single basin to monitor. But this basin has a “virtual border” with two others ones; the south-east Indian Ocean (the Australian area of responsibility starts at 90E) and the Indonesian area of responsibility (east of 90E, north of 10S). If ever a TC comes from one of their areas of responsibility to ours or vice versa, the different centres (Perth, Jakarta and Réunion Island) send e-mails or phone to manage the handover.

Focus 2: The Tropical Forecasters' Perspective »
9F2.3 Météorologique Régional Spécialisé / Centre des Cyclones Tropicaux de La Réunion, Météo-France

Entretien avec Anne-Claire Fontan, ingénieur prévisionniste cyclone

1. Comment et quand avez-vous décidé de devenir un prévisionniste cyclone? Quel a été votre cursus? Avez-vous suivi un parcours spécifique que cela soit en primaire, collège ou lycée pour atteindre votre but?

Je suis devenue ingénieur prévisionniste cyclone au CMRS/ Centre des Cyclones Tropicaux de La Réunion il y a 12 ans, une fois mes études terminées à l’ENM (Ecole Nationale de la Météorologie), l’école d’ingénieurs dédiée à la météorologie, dépendant de Météo-France, et située à Toulouse, en France. Cette école délivre un diplôme en météorologie qui nécessite trois ans d’étude ( qui viennent après deux ans de classes préparatoires aux grandes écoles ou une maîtrise de sciences de l’université). Avant l’ENM, j’ai fait mes études dans les Universités de Marseille et Paris pour obtenir un Master d’océanographie et de météorologie. En France, il n’est pas possible de se spécialiser en météorologie avant l’université et le niveau licence ou maîtrise -ou avant d’aller à l’ENM, mais il est toutefois nécessaire de choisir une filière scientifique dès le lycée.

Une fois diplômé et une fois obtenu le poste au Centre des Cyclones Tropicaux de La Réunion, il faut suivre deux formations supplémentaires; une première formation théorique de deux semaines en météorologie tropicale à l’ENM, puis une deuxième formation, opérationnelle, pendant plusieurs mois, au Centre des Cyclones. Cette période consiste à travailler avec et sous la supervision d’ingénieurs prévisionnistes cyclone expérimentés. Un prévisionniste cyclone est dit confirmé après avoir travaillé pendant une ou deux saisons cycloniques complètes.

2. Quelle(s) méthode(s) utilisez-vous pour prévoir les cyclones tropicaux (CT)? Avec quels outils travaillez-vous? Si l'on distingue les prévisions à effectuer: trajectoire, intensité, taille ou précipitations, vos réponses sont-elles différentes?

Pour élaborer les prévisions au Centre des Cyclones de La Réunion, nous utilisons une puissante station de travail appelée SYNERGIE, sur laquelle nous pouvons visualiser et superposer toutes les données dont un prévisionniste a besoin pour travailler: observations, modèles, imageries satellite, radar, etc. Cette station de travail possède un module spécifiquement dédié aux cyclones tropicaux (SYNERGIE CYCLONE), avec lequel nous travaillons pour procéder à l’analyse du système tropical et établir les prévisions de trajectoire et d’intensité. En plus des modèles, observations, images et tracé des trajectoires issues des modèles numériques …, nous avons récemment installé la visualisation directe des données des sites Internet utilisés quotidiennement en opération. Ces sites sont principalement – et donc de manière non exhaustive- les pages dédiées aux cyclones tropicaux du NRL, du CIMSS, de la NOAA (QuikSCAT), de l’AOML (pour le contenu énergétique), du BoM australien (MJO), ….

Notre zone de responsabilité (de l’équateur à 40S et des côtes africaines à 90E) est essentiellement un domaine maritime, exceptée la partie ouest du bassin, entre les côtes africaines et le 60E. Nous dépendons donc fortement des données satellitaires.

La taille et les précipitations associées aux systèmes tropicaux sont « observées », mais ne sont pas encore spécifiquement prévues. Toutes les six heures, lors de la diffusion de nos bulletins, nous décrivons la taille des systèmes via l’extension des vents à 30 nœuds et 50 nœuds, essentiellement grâce aux données des diffusiomètres (du fait du caractère maritime du bassin). Nous décrivons également le temps et donc les précipitations associées au système. Lorsqu’un système tropical est prévu approcher ou frapper une terre, la partie « commentaires » de nos bulletins spécifie de plus les zones habitées que les précipitations peuvent concerner dans les 24 à 36 prochaines heures. Pour ce faire, nous utilisons les champs prévus comme le taux de précipitation, l’humidité, la vitesse verticale, …, du meilleur modèle.

Prévision de trajectoire:

Pour élaborer nos prévisions de trajectoire, nous disposons des champs des modèles numériques développés par différents pays ou centres; deux modèles de Météo-France, un global et un à aire limitée sur l’Océan Indien Sud, le modèle anglais du Met Office, le modèle déterministe et la moyenne de la prévision d’ensemble du Centre Européen de Prévision (CEP). Depuis la saison 2004-2005, via le JTWC, nous avons également accès aux « géopoints » (i.e. position et pression minimale au centre du système tropical, toutes les 6 ou 12 heures) de quelques-uns des modèles américains comme le GFDN, le NOGAPS, le AVNO, et consensus de modèles calculés au JTWC. Les trajectoires proposées par tous ces modèles sont visualisées sur la station de travail.

Grâce à l’analyse des champs des modèles, le prévisionniste décide quel scénario est le meilleur. Par la suite, comme les statistiques tendent à montrer que les consensus de modèles mènent aux meilleurs résultats, nous moyennons les modèles choisis pour élaborer la prévision de trajectoire. Si la philosophie de certains modèles ne correspond pas à celle retenue, nous ne les incluons pas dans la moyenne.

Prévision d’intensité:

La prévision d’intensité nécessite la connaissance de l’environnement du système et son évolution. Nous utilisons pour ce faire plusieurs outils. Nous étudions les produits du site du CIMSS pour connaître l’environnement; la divergence et les vents d’altitude, la convergence et les vents de basses couches, le cisaillement vertical de vent et sa tendance, etc. Nous regardons le potentiel énergétique océanique via les températures de surface de la mer données par l’imagerie satellite et le contenu énergétique du site de l’AOML (profondeur de l’isotherme 26°C). L’humidité est évaluée grâce aux imageries vapeur d’eau et micro-onde, et nous utilisons également les champs du modèle estimé être le meilleur; θ’w à 700 hPa, divergence, convergence. Pour finir, nous regardons la tendance donnée par les modèles, s’ils creusent ou affaiblissent le système tropical.

3. La Prévision d'Ensemble a-t-elle changé votre méthode de travail?

Nous somme destinataires des produits de la Prévision d’Ensemble (PE) depuis plusieurs années et cela a changé notre façon de travailler et nos résultats. Nous l’utilisons à différentes fins. Tout d‘abord, la PE est utilisée pour évaluer la probabilité de cyclogenèse à 10 jours sur le bassin. Ensuite, la moyenne des 51 runs de la PE est utilisée comme un modèle déterministe et peut être incluse dans un consensus de modèles pour élaborer la prévision de trajectoire. Le panache de probabilité (« strike probabilities ») fourni par le CEP sert à la gestion du risque sur l’Ile de La Réunion. Enfin, la dernière application, toujours à l’étude, serait d’utiliser la PE pour calculer des cônes d’incertitude appliqués à la prévision de trajectoire du CMRS.

4. Comment se déroule une journée de travail lorsqu’un système tropical évolue sur le bassin? En quoi est-ce différent s’il y a plusieurs systèmes tropicaux à la fois? Suivant si les systèmes tropicaux évoluent sur le même bassin ou bien sur des bassins différents, cela fait-il une différence dans votre journée de travail?

Nous travaillons selon des tours de service de 12 heures, qui peuvent être de jour ou de nuit. Les horaires de ces tours de service sont de 07h00 à 19h00 et de 19h00 à 07h00. Nous émettons quatre séries de bulletins par jour, en français et en anglais, à 00, 06, 12 et 18Z. Nous avons donc lors d’une journée de travail, les bulletins de 06 et 12Z à élaborer et diffuser.

La journée commence avec la relève et l’étude approfondie de la situation, exposée lors d’un briefing pour le personnel du centre à 08h30. Nous enchaînons avec la saisie de données dans le logiciel avec lequel nous préparons nos 6 à 7 bulletins, qui sont diffusés en bilingue pour 10h30. Vient ensuite le briefing interne avec le service de prévision du temps local et si nécessaire (i.e. si un CT concerne directement ou indirectement le temps sur La Réunion), nous lui fournissons des directives.

Nous avons une pause entre 11.00 AM et 12.00 PM.

Après cela, nous devons remplir une base de données concernant la cyclogenèse, et débuter la rédaction du bulletin en anglais et français sur l’activité cyclonique et les conditions météorologiques du bassin (« tropical outlook »). Ce bulletin est diffusé à 03h00. Entre-temps, nous élaborons le bulletin dit de « liaison » permettant de tenir l’équipe informée des actions de la journée et de donner des instructions à l’équipe de prévision locale pour les 3 jours à venir.

Les bulletins du réseau suivant sont ensuite préparés et diffusés pour 04h30. A la fin du service, nous procédons à l’archivage des messages, des images satellitaires pertinentes, etc, de la journée.

Si jamais nous avons deux CT à gérer, c’est double travail! S’il y a deux systèmes à suivre, avec une gestion de risque sur La Réunion, un deuxième prévisionniste cyclone vient donner de l’aide. Quelqu’un vient également en renfort lorsqu’il y a trois systèmes à gérer sur le bassin.

Nous avons un seul bassin à surveiller, mais il a une frontière « virtuelle » avec deux autres zones; le sud-est de l’océan Indien (la zone de responsabilité australienne débute à 90E) et la zone de responsabilité indonésienne (est de 90 E et nord de 10S). Si jamais un CT nous arrive d’une de ces deux zones (ou vice et versa), les centres concernés (Perth, Jakarta, La Réunion) s’envoient des mels ou s’appellent pour assurer la passation de responsabilité de suivi du système.

Summary

Tropical weather observation, analysis, and forecasting are challenging but continue to improve thanks to new instruments (mostly satellite and some in situ), derived variables, and tools for synthesizing observations and numerical model output. Forecasters add value to the automated systems using their knowledge of model biases, rapidly updated satellite information, and past cases. Satellite data analysis is one of the most critical skills for tropical weather forecasters. Since radars are sparse in the tropics, high resolution geostationary images aid in nowcasting mesoscale and convective-scale weather systems. High resolution, non-hydrostatic models are producing realistic convective weather systems at many scales, however, data assimilation methods are challenged by increasing amounts and types of satellite data. Ensemble techniques are providing information on model forecasts uncertainty. Multi-model ensemble (consensus) models have led to better tropical cyclone track forecasts. While tropical cyclone intensity forecast skill is lagging, ensembles of statistical and high-resolution dynamical models provide the best numerical guidance currently. Intraseasonal forecasting is becoming mature enough to be used as guidance for the probability of tropical cyclogenesis. New and traditional forecast verification and validation techniques are helping tropical forecaster evaluate numerical forecasts. As knowledge of tropical meteorology and confidence in NWP increases, we expect to see more improvements in tropical weather forecasting.

Appendix A: Station Plot and Weather Symbols

Surface station data are plotted at its location on a weather map in a format shown in Fig. 9A.1. To the upper right is mean sea-level pressure (MSLP); the leading digit(s) is dropped (9 or 10 in the case of MSLP). Therefore, a MSLP value of 998.6 hPa is plotted as “986” while 1011.5 is plotted as "115". The circle shows the sky cover in eighths or oktas (Fig. 9A.2). The wind barb represents speed and the direction from which the wind is blowing. For standard upper-air horizontal analyses (1000, 850, 700, 500, 300, 200 hPa), the station plots show temperature, dewpoint, wind velocity, and geopotential height. A sample 850 hPa data plot is shown in Fig. 9A.1b, where geopotential height of 1564m is plotted as “564”. Other commonly used weather symbols are shown in Fig. 9A.2.

surface station model
upper air station model
Fig. 9A.1. (a) A surface station model plot and (b) an upper air station model plot at 850 hPa.
weather symbols
Fig. 9.A.2. Some commonly used weather symbols.

Questions for Review

  1. Describe at least two challenges that are unique to tropical weather forecasting.
  2. List three types of point measurements.
  3. List three sources of observation error.
  4. What are the advantages and weaknesses of satellite observations when compared to station observations of the tropics?
  5. Describe two advantages and two limitations of weather radar observations for tropical weather analysis and forecasting.
  6. Why is streamline/isotach analysis more useful for tropical weather forecasting than isobaric analysis?
  7. List at least two instruments (in situ or remote-sensing) developed for research that have been applied to tropical weather forecasting since the 1990s.
  8. How does monitoring intraseasonal circulations, such as equatorial waves and the MJO, help tropical forecasters?
  9. List uses and limitations of trajectory analysis for tropical weather forecasting.
  10. List three variables forecasted for tropical marine weather.
  11. Describe how satellite and radar images are used to analyze the evolution of tropical mesoscale convection.
  12. Describe at least four sources of numerical weather prediction model error.
  13. What is the purpose of data assimilation?
  14. What are the fundamental principles represented by the “primitive equations” used in dynamical models?
  15. Why are non-hydrostatic models better for tropical weather prediction than hydrostatic models?
  16. Explain what constitutes an ensemble numerical forecast.
  17. Describe the advantages and limitations of three-dimensional (3D-VAR), four-dimensional variational (4D-VAR), and Ensemble Kalman Filter data assimilation techniques.
  18. Describe three methods for verification of NWP model forecasts including their strengths, weaknesses, and at least one example of their application in tropical weather.
  19. List three factors that must be considered when forecasting tropical cyclone motion.
  20. List three factors that must be considered when forecasting tropical cyclone intensity change.
  21. When are statistical models most useful in tropical cyclone forecasting?
  22. What are some of the key physical variables included in a typical statistical model used for tropical cyclone forecasting?
  23. Give a basic description of two dynamical models used for tropical cyclone motion forecasts.
  24. When are ensemble techniques most useful for tropical cyclone prediction and why?
  25. Describe two techniques used to validate tropical cyclone motion or intensity forecasts.
  26. List the major differences between active and break monsoon periods over Northern Australia in terms of dynamics and thermodynamics.
  27. Describe the differences in the diurnal cycle of convection between active and break monsoon periods. What impact does this have on aviation forecasting at Darwin, Australia?
  28. List as many of the severe storm types you can and at least one feature in the radiosonde that would alert you to potential severity.
  29. Briefly describe why suppressed monsoon periods occur over northern Australia. How are these periods different to the typical active monsoon?
  30. What role does orography play in the seasonal cycle of precipitation over the Maritime Continent (SE Asia)?

QUIZ

You may also take a quiz and email your results to your instructor.

Brief Biographies

Dr. Akio Arakawa

Dr. Akio Arakawa is a pioneer in global numerical weather prediction (NWP). He received his B.Sc. in physics and D.Sc. in meteorology from Tokyo University in 1950 and 1961, respectively. While working at the Japan Meteorological Agency during the 1950s, he developed his first global atmospheric circulation model, having been inspired by Norman Phillips’s first general circulation simulation. He came to the University of California Los Angeles (UCLA) as a visiting scientist in 1961 after being recruited by Yale Mintz. In 1963 they completed the first UCLA General Circulation Model, which later became known as the Mintz-Arakawa Model. It was the first global model to include realistic land-sea distributions and surface topography. Arakawa returned to UCLA in 1965 after a two-year period in Japan. He remained at UCLA as a faculty member for the rest of his career while leading the development of increasingly sophisticated general circulation and earth system models.

Using his brilliant mathematical skills and meteorological expertise, he developed numerical methods for representing fluid dynamics including finite difference techniques first published in 1966. He also developed robust schemes for representing the interaction of cumulus convection and large-scale circulations, creating with Wayne Schubert, the “Arakawa-Schubert cumulus parameterization scheme” in 1974. These contributions have led to major advances in tropical weather prediction and earth system modeling in general. He received the Carl-Gustaf Rossby Research Medal in 1977, the highest award granted by the AMS. His career was celebrated at UCLA in 1998 with, “General Circulation Modeling Past Present, and Future: A symposium in honor of Akio Arakawa. He was made a Fellow of the AMS and an AMS symposium was held in his honor in 2007. He was a recipient of the UCLA Dickson Award for 2008. Most recently, he was awarded the 2010 Vilhelm Bjerknes Medal by the European Geosciences Union in recognition of his pioneering and fundamental contributions not only to numerical modeling in atmospheric sciences but to geophysical fluid dynamics in general. Although retired, he continues to be involved in ongoing efforts to refine global models including climate models. He is regarded as a “living legend”.

Benito Viñes (1837-1893)

Known as the “Hurricane Priest”, Father Benito Viñes, laid the foundation for the modern observational and hurricane warning network. He was the director of the Magnetic and Meteorological Observatory of the Royal College of Belen in Havana, Cuba from 1870 until his death in 1893. He was born in Poboleda, Spain, received training in physics, and came to Cuba via France. He organized hundreds of observers to monitor weather along the coast of Cuba, thereby establishing the first observational network that delivered hurricane warnings by pony express and later by telegraph. From his meticulous observations of surface weather, cloud motion, sea-swells, and post-landfall assessment, he developed a fairly accurate conceptual model for the three-dimensional structure of hurricanes. By observing cloud motion and sea swells, he also created a technique for finding the center of hurricanes. He became famous for pioneering forecasts of hurricane motion based on the movement of high cloud outflow from the center of tropical storms. In September 1875, he became a legend after he issued his first printed forecast and accurately forecasted the landfall of an intense hurricane in southern Cuba. Subsequent success later that year and in the following years resulted in Viñes gaining funding from private companies to aid with observation stations and free message service from telegraph and railroad companies. He published his now famous Practical Hints in Regard to West Indian Hurricanes in 1877 and it became a standard training resource for mariners and others. His technical report on the Cyclonic Circulation and Translatory Movement of West Indian Hurricanes was delivered posthumously to the U.S. Weather Bureau, having been mailed three days before his death.

Thanks to Patrick Fitzpatrick for sharing biographical information from his book, "Hurricanes; a reference handbook, 2nd Edition", Contemporary World Issues, ABC CLIO, 412pp, 2006.

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146. Carbone, R. E., J. W. Wilson, T. D. Keenan, and J. M. Hacker, 2000: Tropical island convection in the absence of significant topography. Part I: Life cycle of diurnally forced convection. Mon. Wea. Rev., 128, 3459-3480.
147. Chang, C., Z. Wang, J. McBride, and C. Liu, 2005: Annual cycle of southeast Asia-maritime continent rainfall and the asymmetric monsoon transition. J. Climate, 18, 287-301.
148. Haylock, M., J. McBride, 2001: Spatial coherence and predictability of Indonesian wet season rainfall. J. Climate, 14, 3882-3887.

A

Absolute angular momentum
For the atmosphere, the absolute angular momentum, per unit mass of air, is the sum of the angular momentum relative to the earth and the angular momentum due to the rotation of the earth.
Absolute vorticity
See Vorticity.
Absorber
Anything that retains incident electromagnetic radiation due its physical composition.
Absorption
The process by which incident radiant energy is retained by a material due to the material's physical composition.
Absorption band
A portion of the electromagnetic spectrum where radiation is absorbed and emitted by atmospheric gases such as water vapor, carbon dioxide, and ozone.
African easterly wave
A trough or cyclonic curvature maximum in the trade-wind easterlies. The wave may reach maximum amplitude in the lower middle troposphere.
Aggregation
The clumping together of ice crystals after they collide.
Anomaly
The deviation of a quantity over a specified period from the normal value for the same region. For example, El Niño is identified by sea surface temperature anomalies.
Atlantic Multidecadal Oscillation (AMO)
A natural oscillation of the North Atlantic SST between warm and cool phases. The SST difference between these warm and cool phases is about 0.5°C and the period of the oscillation is roughly 20-40 years (the period is variable, but is a few decades long). Evidence suggests that the AMO has been active for at least the last 1,000 years.
Attenuation
Any process in which the intensity of radiation decreases due to scattering or absorption.
Atmospheric Window
A portion of the electromagnetic spectrum where radiation passes through the atmosphere without absorption by atmospheric gases such as water vapor, carbon dioxide, and ozone.
Available potential energy (APE)
The portion of the total potential energy available for adiabatic conversion to kinetic energy. The total potential energy is a combination of the APE and the potential energy representing the mass distribution needed to balance the mean atmospheric motions.

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B

Backscatter
That portion of radiation scattered back toward the source.
Baroclinic
Dependence on the horizontal temperature contrast between warm and cold air masses., In a baroclinic atmosphere, the geostrophic wind varies with height in direction as well as speed and its shear is a function of the horizontal temperature gradient (the thermal wind equation).
Barotropic
The atmosphere has the same horizontal structure at all levels in the vertical. This is equivalent to the absence of horizontal temperature gradients.
Barotropic-Baroclinic Instability
Barotropic and baroclinic instability analyses are used to explain the growth of a small perturbation to the flow. A perturbation growing due to baroclinic instability draws its energy from the available potential energy (APE). A perturbation growing due to barotropic instability draws its energy from the kinetic energy of the background flow. A perturbation growing through both APE and mean kinetic energy conversion to kinetic energy of the growing system (intensifying the system) is developing through combined barotropic baroclinic instability.
Best track
As defined by the National Hurricane Center, it is a subjectively-smoothed representation of a tropical cyclone's location and intensity over its lifetime. The best track contains the cyclone's latitude, longitude, maximum sustained surface winds, and minimum sea-level pressure at 6-hourly intervals. Best track positions and intensities, which are based on a post-storm assessment of all available data, may differ from values contained in storm advisories. They also generally will not reflect the erratic motion implied by connecting individual center positions fixed during operations.
Beta (β) effect
Denotes how fluid motion is affected by spatial changes of the Coriolis parameter, for example, due to the earth's curvature. The term takes its name from the symbol β representing the meridional gradient of the Coriolis parameter at a fixed latitude. The asymmetric flows resulting from the interaction of the vortex with the changing Coriolis parameter is known as the β-gyres.
Beta (β) plane
An approximation of the Coriolis parameter in which f = f0 + βy, where β is a constant. The Coriolis parameter is assumed to vary linearly in the north-south direction. The term takes its name from the symbol β representing the meridional gradient of the Coriolis parameter at a fixed latitude.
Blackbody
An object that absorbs all incident radiation and emits the maximum amount of energy at all wavelengths.
Blended precipitation estimate
An estimate that is derived by combining low earth-orbiting microwave measurements, which have high resolution but low frequency, with the more frequently available geostationary IR.
Bow echo
An organized mesoscale convective system, so named because of its characteristic bow shape on radar reflectivity displays. Bow echoes are typically 20–200 km long and last for 3–6 hours. They are associated with severe weather, especially high, straight-line surface winds, which are the result of a strong rear-inflow jet descending to the surface.
Brightness temperature
The Planck temperature associated with the radiance for a given wavelength.

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C

Center
Location of the vertical axis of a tropical cyclone, usually defined by the location of minimum wind or minimum pressure. The cyclone center position can vary with altitude.
Cloud track winds
Winds derived from tracking movement of cloud elements using IR and water vapor images from geostationary satellites.
Conditional Instability of the Second Kind (CISK)
A theory for tropical cyclone development that relates boundary layer moisture convergence (driven by Ekman pumping) to the potential for tropical cyclone intensification. As the storm intensifies, the moisture convergence must increase, providing a feedback to the system. As with WISHE, CISK relies on the presence of an incipient disturbance.
Coordinated Universal Time (UTC)
Same as Zulu (Z) and Greenwich Mean Time (GMT).
Coriolis parameter, f
A measure that is twice the local vertical component of the angular velocity of a spherical planet, 2Ω sinφ, where Ω is the angular speed of the planet and φ is the latitude.
Cyclogenesis
The formation of a cyclone.
Cyclone
An closed circulation of low pressure, rotating counter-clockwise in the Northern Hemisphere and clockwise in the SH.
Cyclone Phase Space (CPS)
A concise, three-parameter summary of the structure of a storm. It can be used to describe the structure of any synoptic or meso-synoptic cyclone.

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D

Deposition
The process by which molecules are changed from the vapor phase directly to the solid phase, such as from water vapor to ice.
Doppler Effect
The apparent shift in the frequency and wavelength of a wave perceived by an observer moving relative to the source of the wave.
Doppler radar
Radar that uses the Doppler effect to detect radial velocity of targets based on the phase shift between the transmitted pulse and the received backscatter.
Dvorak Technique
a classification scheme for estimating the intensity of TCs from enhanced IR and visible satellite imagery. It is the primary method of estimating intensity everywhere, except the North Atlantic and North Pacific where aircraft reconnaissance is routine.

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E

Eddy angular momentum flux (EAMF)
Flux (net transport) of angular momentum into a circle centered on the storm. If EAMF is positive, the flow inside the circle will become more cyclonic; negative EAMF render the system less cyclonic (more anticyclonic). See Box 8-6 for a definition and discussion of angular momentum in tropical cyclones.
Ekman layer
Thin horizontal layer of water at top of the ocean that is affected by wind.  That layer has a force balance between pressure gradient force, Coriolis force and frictional drag.
Ekman layer instability
A shearing instability in a boundary layer where the mean flow results from a balance between the forces of friction, pressure gradient, and Coriolis. The instability appears as vortex rolls in the form of a spiral band.
Ekman pumping
The force balance determining the vector wind is modified by friction at the Earth's surface. The addition of friction changes the force balance to slow the winds and change their direction: winds now flow into a low and out of a high pressure system. Winds flowing into a low because of friction are forced upwards and out of the boundary layer. This process is known as Ekman pumping.
El Niño-Southern Oscillation (ENSO)
An oscillation of the ocean-atmosphere system in the tropical Pacific which affects global  weather and climate. El Niño, the warm phase of ENSO, is a quasi-periodic (2-7 years) warming of ocean surface waters in the equatorial and eastern tropical Pacific and an eastward shift in convection from the western Pacific climatological maximum. Changes occur in the tropical trade easterlies, vertical wind shear,  and ocean height. Cool ocean temperature anomalies are observed in the tropical western Pacific extending eastward into the subtropics of both hemispheres. "La Niña" refers to the less intense, anomalous  cool phase of ENSO. The Southern Oscillation refers to the atmospheric pressure difference between Darwin and Tahiti that is correlated with El Niño.
Electromagnetic (EM)
Energy carried by electric and magnetic waves.
Emission
The process by which a material generates electromagnetic radiation due to its temperature and composition.
Emissivity
The emitting efficiency of an object compared to an ideal emitter (or blackbody). A blackbody has an emissivity of one.
Emitter
Anything that radiates measurable electromagnetic radiation.
Empirical Orthogonal Function (EOF)
See Principal Component Analysis.
Energy
The capacity to do work or transfer heat. Measured in SI units as Joules.
Entrainment
The integration of unsaturated environmental air into the turbulent cloud-scale circulation. The antonym of entrainment is detrainment.
Explosive Deepening
A decrease in the minimum sea-level pressure of a tropical cyclone of 2.5 hPa hr-1 for at least 12 hours or 5 hPa hr-1 for at least six hours.
Extratropical
A term used to indicate that a cyclone has lost its “tropical” characteristics. The term implies both poleward displacement of the cyclone and the conversion of the cyclone’s primary energy source from the release of latent heat of condensation to baroclinic processes.

It is important to note that cyclones can become extratropical and still retain winds of hurricane or tropical storm force. Given that these dangerous winds can persist after the cyclone is classified as extratropical, the Canadian Hurricane Centre (for example) follows them as “Former hurricane XXX.”
Extratropical Transition (ET)
The evolution of a poleward-moving initially tropical cyclone resulting in an extratropical cyclone. In the process of this evolution the energy source of the storm shifts from latent heat release to baroclinic development.
Eye (of tropical cyclone)
The approximately circular area of light winds at the center of a tropical cyclone. It is surrounded entirely or partially by clouds in the eyewall.
Eyewall / Wall Cloud
The full or partial ring of thunderstorms that surround the eye of a tropical cyclone. The strongest sustained winds in a tropical cyclone occur in the eyewall.

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F

Field of View (FOV)
Generally associated with the ground resolution from the detector standard viewing location, field of view is the solid angle through which a detector observes radiation.
Fraction of Photosynthetically Active Radiation (FPAR)
An index that measures how much sunlight the leaves are absorbing.
Frequency
The number of recurrences of a periodic phenomenon per unit time. The frequency, v, of electromagnetic energy is usually specified in Hertz (Hz), which represents one cycle per second.
Fujiwhara Effect
The mutual advection of two or more nearby tropical cyclones about each other. This results in cyclonic rotation of the storms about each other.

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G

Gale Force Wind
A sustained surface wind in the range 17 m s-1 (39 mph, 63 km hr‑1 or 34 knot) to 24 m s-1 (54 mph, 87 km hr‑1 or 47 knot) inclusive, and not directly associated with a tropical cyclone.
Geostationary or Geosynchronous orbit
An orbit whose rotation period equals that of the Earth. The altitude of a geostationary orbit is approximately 35,800 km. Its orbit keeps it above a single point on the equator.
GOES
Geostationary Operational Environmental Satellite (operated by NOAA).
GOES Precipitation Index
An estimate of precipitation that uses 235K as the IR temperature with the best correlation to average precipitation for areas spanning 50-250 km over 3-24 hours.
GPS
Global Positioning System, a network of defense satellites established in 1993. Each satellite broadcasts a digital radio signal that includes its own position and the time, accurate to one billionth of a second. GPS receivers use the signals to calculate their position to with a few hundred feet.
GPS radio occultation
The technique by which satellite receivers intercept signals from GPS and infer the deviations in the signal's path caused by temperature and moisture gradients.
Gravity waves
Oscillations usually of high frequency and short horizontal scale, relative to synoptic- scale motions, which arise in a stably stratified fluid when parcels are displaced vertically. Gravity is the restoring force.
Greenwich Mean Time (GMT)
Mean solar time of the meridian at Greenwich, England, used as the basis for standard time throughout most of the world. Also referred to as Zulu (Z) and Coordinated Universal Time (UTC).

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H

Hadley Cells
Circulation cells in which air rises in the ITCZ, sinks into the subtropical highs, and returns to the equatorial low along the trade winds. George Hadley proposed a model (1735) of the global atmospheric circulation with rising motion at the equator, where there is surplus heating, and sinking motion at the poles, where there is net cooling. Hadley's model did not account for the Coriolis effect, which leads to average westerly motion in the mid-latitudes. The Hadley model does explain the circulation within 30 degrees of the equator.
Horizontal Convective Rolls
Lines of overturning motion with axes parallel to the local surface. These rolls result from a convective instability (high density over low density – often corresponding to cool air over warm) and can mix strong winds from above down towards the surface.
Hurricane
A tropical cyclone in which the maximum sustained surface wind (using the local time averaging convention) is at least 33 m s-1 (74 mph, 119 km hr-1 or 64 knot). The term "hurricane" is used for in the Northern Atlantic and Northeast Pacific; "tropical cyclone" east of the International Dateline to the Greenwich Meridian; and "typhoon" in the Pacific north of the Equator and west of the International Dateline.

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I

Inertial period
The time taken to complete one rotation. In the tropical cyclone this is calculated by dividing the circumference at the radius of interest (commonly, the radius of maximum winds) by the wind speed at that radius.
Infrared (IR)
Electromagnetic energy within the wavelength interval generally defined from 0.7 to 100 microns.
Irradiance
The energy per unit time incident upon a unit area of a given surface, measured in SI units as Wattsm-2.
Insolation
The incoming solar radiation that reaches the earth and its atmosphere.
Intensity
The peak sustained surface wind in the region immediately surrounding the storm center, or the minimum central pressure measured in the eye.
Intertropical Convergence Zone (ITCZ)
The zone where the northeast and southeast trade winds converge. It is marked by low pressure, rising motion, and thunderstorms, which occur with strong surface heating. Its latitudinal position shifts in response to the solar maximum and heating response of the surface. It is recognized in satellite images as a band of thunderstorms across the tropics. It is often, but not always, co-located with the zone of low pressure known as the "Equatorial Trough".
Intraseasonal
Varying on time scales shorter than one season.

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J

Joule
SI unit of energy equal to 0.2389 calories.

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K

Kelvin waves
At the equator, eastward propagating waves with negligible meridional velocity component and Gaussian latitudinal structure in zonal velocity, geopotential, and temperature, symmetric about the equator.

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L

Landfall
The intersection of the surface center of a tropical cyclone with a coastline. Because the strongest winds in a tropical cyclone are not located precisely at the center, it is possible for the strongest winds to be experienced over land even if landfall does not occur.
Leaf Area Index (LAI)
The ratio of green leaf area to the total surface area occupied by vegetation.
Longwave (LW)
Electromagnetic energy lying in the wavelength interval generally defined from 4.0 microns to an indefinite upper limit.
Low earth orbit (LEO)
An orbit that is located at an altitude generally between 200 and 1000 km.
Low earth orbit satellite
A satellite that has a low earth orbit. Most have paths crossing the poles and can provide synchronous observations (e.g., the NOAA series or Defense Meteorological Satellite Program systems). The TRMM is an LEO satellite that orbits between ±35º latitude.

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M

Madden-Julian Oscillation (MJO)
Tropical rainfall exhibits strong variability on time scales shorter than the seasonal. These fluctuations in tropical rainfall often undergo a 30-60 day cycle that is referred to as the Madden-Julian Oscillation or intraseasonal oscillation. The MJO is a naturally occurring component of the Earth's coupled ocean-atmosphere system that significantly affects the atmospheric circulation throughout the global tropics and subtropics.
Maritime Continent
The region of Southeast Asia that comprises many islands, peninsulas, and shallow seas (including countries such as Indonesia, Malaysia, Papua New Guinea, and the Phillipines and covers approximately 12°S to 8°N, 95°E to 150°E).
Meridional
North-south, crossing latitudes; by convention the meridional wind from the south is positive.
Mesoscale
Spatial scale of 100-1000 km and temporal scale of hours to a day; between synoptic and convective scale. Tropical clouds are most often organized into mesoscale systems.
Mesoscale convective complex (MCC)
A large, quasi-circular mesoscale convective system that produces heavy rainfall and severe weather. In some MCCs, a mid-tropospheric vortex forms and remains after the deep convection has dissipated.
Mixed Rossby-Gravity (MRG) Wave
A divergent Rossby wave, resulting from conservation of potential vorticity and buoyancy forcing. These waves propagated westward along the equator. Meridional velocity is symmetric about the equator. Zonal wind, temperature, and geopotential area antisymmetric about the equator.
Monochromatic
Of or pertaining to a single wavelength, or in practice, perhaps a very narrow spectral interval.
Monsoon
A term whose roots are from the Arabic for "season", it is a seasonal wind reversal. The monsoon has inflow to a surface heat low and an offshore flow from high pressure during the winter when the land cools relative to the ocean. The Indian monsoon is the most prominent but it has been recognized that that monsoon region extends from Southeast Asia to West Africa. The summer monsoon is a vital source of moisture; its arrival, duration, and amount of precipitation modulates the economies of these regions.
Monsoon Gyre
A closed, symmetric circulation at 850 hPa with horizontal extent of 25° latitude that persists for at least two weeks. The circulation is accompanied by abundant convective precipitation around the south-southeast rim of the gyre.
Monsoon Region
Refers to the combination of features including a monsoon trough, confluence zone, and the ITCZ.

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N

Nadir
The satellite viewing angle directly downward (viewing zenith angle = 0 degrees). Also used to refer to the sub-satellite point location.

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0

Ocean conveyor belt
The name given to summarize the pattern of global ocean currents. The surface ocean currents generally transport warm salty water polewards, out of the tropics. The water cools as it moves polewards, becoming increasingly dense (remember that salty water is more dense than fresh water). This water sinks in the North Atlantic and also in the Southern Ocean near Antarctica. The deep water currents transport the water around the globe until it rises to the surface again, once more part of the surface ocean currents.
Opaque
A physical description of a material which attenuates electromagnetic radiation.
Optical depth
A measure of the cumulative attenuation of a beam of radiation as a result of its travel through the atmosphere.

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P

Pacific Decadal Oscillation (PDO)
The PDO is a basin-scale pattern of Pacific climate variability; PDO climate anomalies are most visible in the North Pacific and North American regions, with secondary features in the tropics. The phases of the PDO persist for 20-to-30 years. Causes for the PDO have not yet been explained.
Planck's Law
An expression for the variation of monochromatic radiance as a function of wavelength for a blackbody at a given temperature.
Planetary Boundary Layer (PBL)
The layer of the atmosphere that extends upward from the surface to heights of 100 to 3000 m. The boundary layer is directly influenced by surface forcing such as friction, heating, and evapotranspiration.
Polar orbit
An orbit whose path crosses the polar regions. This type of orbit is located at an altitude generally between 200 and 1000 km, and can provide sun-synchronous observations.
Polar Orbiting Environmental Satellite (POES)
A satellite which has a polar orbit, such as the NOAA series or Defense Meteorological Satellite Program systems.
Potential evapotranspiration
A measure of the maximum possible water loss from an area under a specified set of weather conditions.
Potential Intensity (PI)
The largest possible intensity (maximum wind, minimum pressure) expected to be possible for a particular tropical cyclone.
Potential vorticity
A scalar measure of the balance between the vorticity and the thermal structure of the atmosphere.
Principal component analysis
A mathematical technique for identifying patterns in data by reducing multidimensional data to a smaller number of dimensions. A number of variables that are (possibly) correlated are transformed into a new coordinate system. The transformation identifies the components that account for variability in the data. The first principal component often accounts for the most of variability in the data. Also known as Empirical Orthogonal Function (EOF) analysis.

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Q

Quasi-Biennial Oscillation (QBO)
An oscillation in the lower stratospheric zonal winds averaged around the equator. It is typically diagnosed from the zonal winds between 30-70 hPa (although it is evident as high as 10 hPa). The QBO has a varying from about 24 to 30 months. The zonal winds change by about 40 m s-1 between the maximum easterly and maximum westerly phase.

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R

Radar (Radio Detection And Range)
An instrument that detects objects remotely by transmitting high-frequency pulses to the atmosphere and measuring the "backscatter" or echoed pulses from that object. Weather radar transmits microwave (mm-cm) pulses; the returned signal is interpreted to determine where it is precipitating.
Radiance
A measure of radiant intensity produced by a material in a given direction and per unit wavelength interval, measured in Watts/m 2 /steradian/micron. Monochromatic radiance is the most fundamental unit measured by satellite instruments.
Radiation
Energy transferred by electromagnetic waves.
Radius of Maximum Winds
The distance from the center of a tropical cyclone to the location of the cyclone's maximum winds. In well-developed systems, the radius of maximum winds is generally found at the inner edge of the eyewall.
Rapid Deepening
A decrease in the minimum sea-level pressure of a tropical cyclone of 1.75 hPa hr-1 or 42 hPa for 24 hours.
Recurvature
The poleward motion of a tropical cyclone taking it from the mean tropical easterlies to the midlatitudes westerlies. This change in the advection of the storm results in curvature in the storm track.
Reflection
The process by which incident radiation is scattered in the backward direction (backscattered).
Reflectivity
The fraction of incident radiation reflected by a material.
Relative vorticity
See Vorticity.
Remnant Low
Used for systems no longer having the sufficient convective organization required of a tropical cyclone (e.g., the swirls of stratocumulus in the eastern North Pacific).
Retrieval
The process or end result of a process where physical quantities such as water vapor, temperature, and/or pressure are extracted from measurements of total upwelling radiance to space; here involving the GOES sounder.
Reyleigh Instability
Instability of a horizontal fluid layer heated from below or cooled from above. The onset of convection due to this thermal instability was first documented by Lord Rayleigh and Henri Bérnard (although the latter discovery was an instability due to surface tension differences that occur when a fluid is unevenly heated). Mesoscale cellular convection in the atmospheric boundary layer appears similar to Rayleigh-Bérnard convection.
Riming
The formation of ice by the rapid freezing of supercooled water drops as they impinge upon an object such as an ice crystal or aeroplane wing.
Rossby Radius of Deformation
The Rossby radius is the critical scale at which rotation becomes as important as buoyancy, which allows an initial disturbance to be sustained. It is a function of the absolute vorticity, stability, and depth of the disturbance. When a disturbance is wider than LR, it will persist; systems that are smaller than LR will dissipate.
Rossby Wave
A planetary wave, resulting from conservation of potential vorticity. Gradients of potential vorticity provide a restoring mechanism to allow propagation of the waves. This text focuses on Rossby waves centered on the equator equatorial (n=1) Rossby waves.

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S

Saffir-Simpson scale
A scale that links the observed damage and the effects of wind, pressure and storm surge that could lead to such damage. Initial wind damage scale was defined by Herbert Saffir and later expanded by Robert Simpson to include storm surge.
Scattering
The process by which a material interacts with and redirects incident radiation (in any given direction).
Scatterometer
A radar that infers near-surface wind velocity by sending pulses of microwave energy to the ocean surface and measuring the backscatter from small-scale waves. Scatterometry wind retrievals can be ambiguous during rain, since rain creates additional backscatter and attenuates the radar beam.
Shortwave (SW)
Electromagnetic radiation generally defined as having a wavelength shorter than 4.0 microns.
Size
The mean radius of a tropical cyclone enclose by winds of at least 17 m s-1. Size may also be defined as the outer closed isobar of the surface pressure.
Solar declination angle
The angle between the rays of the Sun and the equatorial plane of the Earth. It is zero during an equinox and 23.5° during a solstice.
Southern Oscillation Index (SOI)
The normalized difference in sea level pressure between Darwin, Australia and Tahiti, French Polynesia.
Specific humidity
The mass of water vapor per unit mass of air (including water vapor), usually denoted by q and measured in units of grams per kilograms.
Spectral
A descriptor for radiometric quantities or measurements which have a limited wavelength range.
Split window
A pair of regions of the electromagnetic spectrum which are closely located in wavelength, but have slightly different attenuation characteristics. Used to denote the 11- and 12-micron regions in which greater water vapor attenuation at 12 microns causes slightly different brightness temperatures.
Stefan-Boltzmann Law
The energy emitted per unit area (from all wavelengths and represented by the area under the blackbody curve) is proportional to the 4 th power of the absolute temperature
Steradian
The unit of measure of solid angles, equal to the angle subtended at the center of a sphere.
Storm Surge
An abnormal rise in sea level accompanying a tropical cyclone or other intense storm, and whose height is the difference between the observed level of the sea surface and the level that would have occurred in the absence of the cyclone. Storm surge is usually estimated by subtracting the normal or astronomic high tide from the observed storm tide.
Storm Tide
The actual level of sea water resulting from the astronomic tide combined with the storm surge.
Subtropical Cyclone
A non-frontal low pressure system that has characteristics of both tropical and extratropical cyclones.

The most common type is an upper-level cold low with circulation extending to the surface layer and maximum sustained winds generally occurring at a radius of about 100 miles or more from the center. In comparison to tropical cyclones, such systems have a relatively broad zone of maximum winds that is located farther from the center, and typically have a less symmetric wind field and distribution of convection.

A second type of subtropical cyclone is a mesoscale low originating in or near a frontolyzing (dying frontal) zone of horizontal wind shear, with radius of maximum sustained winds generally less than about 50 km (30 miles). The entire circulation may initially have a diameter less than 160 km (100 miles). These generally short-lived systems may be either cold core or warm core.
Subtropical Depression
A subtropical cyclone in which the maximum sustained surface wind speed does not exceed 17 m s-1 (39 mph, 63 km hr‑1 or 34 knot).
Subtropical Storm
A subtropical cyclone in which the maximum sustained surface wind speed is at least 17 m s-1 (39 mph, 63 km hr‑1 or 34 knot).
Synthetic Aperture Radar (SAR)
Works like other radars except that it has very fine resolution in the azimuthal direction. It synthesizes the fine resolution normally achieved with a large antenna by combining signals from an object along a radar flight track and processing the signals as if obtained simultaneously from a single large antenna. The distance over which the signals are collected is known as the synthetic aperture.

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T

Trade Winds
Prevailing easterly winds flowing from the subtropical highs that affect equatorial and subtropical regions. Trade winds are mostly east to northeasterly in the Northern Hemisphere and east to southeasterly in the Southern Hemisphere. During the monsoon, easterly trades are replaced by mostly westerly winds.
Transmission
The process by which incident radiation propagates forward through a material.
Transpiration
The process by which water vapor enters the atmosphere through the stomata in the leaves of plants.
Thermocline
The inversion layer separating the near-surface warm waters from the colder, deeper layers of oceans and lakes.  It is about 1km deep and is thermally stratified. In the ocean, it also separates the fresher waters near the surface from the saltier waters below.
Total Precipitable Water (TPW)
The depth of water in a vertical column of unit cross-sectional area if the total atmospheric water vapor contained in that column, extending between the surface and the "top" of the atmosphere, completely condensed.
Tropical Cyclone
A warm-core non-frontal synoptic-scale cyclone, originating over tropical or subtropical waters, with organized deep convection and a closed surface wind circulation about a well-defined center. Once formed, a tropical cyclone is maintained by the extraction of heat energy from the ocean at high temperatures and heat export at the low temperatures of the upper troposphere. In this they differ from extratropical cyclones, which derive their energy from horizontal temperature contrasts in the atmosphere (baroclinic effects). Also see Hurricane.
Tropical Cyclone Season
The portion of the year having a relatively high incidence of tropical cyclones. Also known as "Hurricane Season" or "Typhoon Season".
Tropical Depression
A tropical cyclone in which the maximum sustained surface wind speed is not more than 17 ms-1 (39 mph, 63 km hr‑1 or 34 knot).
Tropical Disturbance
A discrete tropical weather system of apparently organized convection – generally 185 to 550 km (100-300 n mi) in diameter – originating in the tropics or subtropics, having a nonfrontal migratory character, and maintaining its identity for 24 hours or more. It may or may not be associated with a detectable perturbation of the wind field.
Tropical Storm
A tropical cyclone in which the maximum sustained surface wind speed ranges from 17 ms-1 (39 mph, 63 km hr‑1 or 34 knot) to 33 ms-1 (74 mph, 119 km hr-1, 64 knot).
Typhoon
See Tropical Cyclone and Hurricane.

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U

Ultraviolet (UV)
Electromagnetic radiation of shorter wavelength than visible radiation but longer than x-rays (approximately 0.03 to 0.4 microns)

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V

Virtual Potential Temperature
In a system of moist air the potential temperature of dry air having the same density and pressure as the moist air.
Visible
The region of the electromagnetic spectrum which is detectable to the human eye (approximately 0.4 to 0.7 microns).
Vorticity
The local rotation of the flow, calculated as the the curl (cross product) of the vector wind. Vorticity has units of inverse seconds (s-1).

“Relative vorticity” is the vorticity calculated for the observed winds. It is called “relative” since the winds are the flow relative to the Earth’s rotation.
The vertical component of the vorticity vector is most often used since it is much larger than the other vorticity components. This is because the horizontal winds in tropical cyclones are much greater than the vertical wind component.

“Absolute vorticity” is the vorticity calculated for the total motion of the atmosphere the combination of the observed winds and the Earth’s rotation.

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W

Walker Circulation
The east-west circulation cells that form along the equator in response to differential surface heating.
Warning
A warning that sustained winds exceeding the threshold for either tropical storm or tropical cyclone and associated with such a storm are expected in a specified coastal area in 24 hours or less.
Watch
An announcement for specific coastal areas that either tropical storm or tropical cyclone conditions are possible within 36 hours.
Wavelength
The distance a wave will travel in the time required to generate 1 cycle, denoted by λ. A length measured from the midpoint of a crest (or trough) to the midpoint of the next crest (or trough).
Wavenumber
The reciprocal of the wavelength, denoted by κ.
Water Vapor Channel (or water vapor IR channel)
A spectral band in which the radiance is attenuated by water vapor. This usually refers to the 6.7 micron channel in this module.
Weighting function
A mathematical expression representing the relative radiance contribution provided from a given level of the atmosphere (usually a function of atmospheric pressure).
Wind-Induced Surface Heat Exchange (WISHE)
A tropical cyclone development theory based on a conceptual model of a tropical cyclone as an atmospheric Carnot engine. Consistent with its Carnot engine roots, WISHE relates (i) fluxes of heat and moisture from the ocean surface and (ii) the temperature of the tropical cyclone outflow layer to the potential for continued storm development. The fluxes increase with surface wind speed providing a feedback to the system. As with CISK, WISHE relies on the presence of an incipient disturbance.
Wind profiler
Vertically pointing radar which operates on the same principle as horizontally-scanning Doppler radar; provides best measurements of vertical air motion inside convective storms
Wien's Displacement Law
The wavelength of maximum blackbody emission is inversely proportional to its absolute temperature.

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X

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Y

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Z

Zonal
East-west, crossing longitudes; by convention, the zonal wind from the west is positive.
Zulu (Z)
Used to represent the same clocktime at GMT and UTC. See Greenwich Mean Time (GMT), or Coordinated Universal Time (UTC)

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