Met Office College – Course Notes Precipitation Forecasting Contents 1 Introduction 2 Frontal Precipitation 3 Non-frontal precipitation 3.1 3.2 4 Instability precipitation 4.1 4.2 5 Organised precipitation Precipitation from stratiform cloud Showers Cumulonimbus and thunderstorms Type of precipitation 5.1 5.2 5.3 5.4 Hail Drizzle Rain or snow? Freezing precipitation 6 Quantity of precipitation 7 Snow Predictors 7.1 7.2 7.3 7.4 7.5 8 Boyden’s technique using 1000 - 850 Thickness Height of wet bulb zero degree isotherm above ground level Hand's rule Height of zero degree isotherm above ground level Screen wet-bulb temperature technique (Lumb) Further Reading Crown Copyright. Permission to quote from this document must be obtained from The Principal, Met Office College. Page 1 of 16 Last saved date: 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College 1 Introduction We have seen previously the mechanisms, which produce precipitation. In this section we will look at the problem of forecasting precipitation both from layer and convective cloud. Forecasting precipitation requires the consideration of many aspects: 1. Type, e.g. drizzle, rain, hail or snow. 2. Area of coverage, i.e. local or widespread. 3. Intensity i.e. slight, moderate or heavy. 4. Length of time precipitation will last. 5. Total quantity of precipitation. We can split the problem into three main parts:1. Frontal precipitation 2. Non-frontal precipitation 3. Instability precipitation 2 Frontal Precipitation Synoptic chart - Study the chart and try to identify the fronts. In the case of an active front this may be relatively simple; inactive fronts are more difficult to position, especially over sea areas. In both cases the satellite pictures are very useful. Colour in the precipitation areas in green. Nimbus - Can be used effectively to track areas of precipitation by overlaying the weather elements on the satellite products. This will give an idea of which cloud produces what precipitation. Then overlaying the model wind fields for 700 hPa gives an idea of advection. Use the radar option to track elements, and hence find the speed of movement. Beware of development, dissipation and orographic effects when timing rain bands. History - Look at earlier charts and see how the front has moved and also how the precipitation area has grown or diminished. Draw up continuity charts of the movement of the fronts and associated rain areas. Look at the isallobaric pattern, which will show whether the parent depression is deepening or filling. Usually if the depression is deepening the front is becoming more active, and vice versa. Page 2 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting Tephigram - A study of the tephigram will help in the positioning of the front (T analysis). Consider how moist or dry the ascents are. Are there regions of instability which may lead to heavy rain? Upper air - A useful guide to precipitation forecasting is the 700 hPa wind. The precipitation area will often move in the direction and at the speed of the 700 hPa wind. Are there any upper air troughs or jet streams present? A front will become more active if an upper air trough such as one at 300 hPa over-runs a surface front. 3 Non-frontal precipitation Assuming an area of non-frontal precipitation can be tied in with a significant feature then, because we have a good idea of the development of these features, we should be able to make a reasonable forecast for changes in the precipitation area. For example, if we forecast a feature to become more intense, say as a upper trough sharpens, then we would expect the precipitation to become heavier due to increased vertical motion. Similarly if we expected a polar low to track across land then we would expect the precipitation to gradually die out as the system loses its heat source. Areas of non-frontal precipitation which are not readily associated with any significant feature are more difficult to handle. Causes of non-frontal precipitation can be divided into two main categories:1. Those connected with organised features 2. Those not connected with organised features 3.1 Organised precipitation Surface The main surface features are troughs and polar lows. These tend to be less conservative than fronts. The main method used is to move the rain area associated with troughs with the 700 hPa wind. The rain area associated with the polar low tends to move more erratically and is best tracked using continuity or as a rough guide move with the 850 hPa wind. — Upper air Cold pools and troughs in the thickness pattern and troughs in the contour pattern are useful indications of the probability of instability rain, showers or thunderstorm. Both in summer and winter these features are — Page 3 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College responsible for mesoscale differences in precipitation distribution. In winter they are often responsible for significant variations in local accumulations of snowfall. The most vigorous convection associated with a thermal pool or trough will often give precipitation in areas which under normal streamline flow would not receive any. An obvious example of this would be well inland or to the lee of high ground, where organised features may bring significant precipitation because they maintain vertical momentum better than non-organised systems. In summer the effect is similar but the most vigorous activity will occur overland (not at sea as in winter) where there is maximum heating. Any showers will be enhanced by upper troughs or cold pools due to increased instability and may be the mechanism which provides the trigger for thunderstorms. Upper troughs or cold pools may give rise to shower activity outside the period that daytime heating would suggest. 3.2 Precipitation from stratiform cloud Precipitation produced from stratiform cloud which is nonfrontal e.g. drizzle or light rain, is related to the microphysics of the cloud rather than the broader dynamics involved with the previous sections. We need to consider the temperature and depth of layered cloud to see if the cloud droplets will grow sufficiently large to fall to the ground without evaporating. Drizzle is often associated with haar/sea fret and affects similar areas, i.e. east and north coasts, and is cleared inland by radiation and near the coasts by advection. Drizzle tends to be more frequent during the latter part of the night and early morning as the ST/SC thickens due to nocturnal cooling. For drizzle to reach the ground it must fall from ST cloud with its base less than 1000 ft. The dew-point depression in the air below the cloud should be less than 20C, otherwise the drizzle will evaporate before reaching the ground. Heavier drizzle is mainly associated with orographic cloud. Sporadic light rain can often be associated with thicker layers of SC in the circulation of an anticyclone. As SC is notoriously difficult to forecast, the forecasting of this type of rain is also difficult. If the high pressure builds Page 4 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting enough then the SC will become thinner and the rain will cease. The satellite imagery on NIMBUS can help to identify areas of colder ST/SC tops where rain or drizzle is more likely. Again the overlay of actual weather on these satellites can be useful. 4 Instability precipitation Synoptic chart - Study the charts and decide whether showers and thunderstorm are already occurring. Are they associated with any topographical feature (e.g. over the sea, land, mountains, etc)? Are they associated with any isobaric pattern (e.g. troughs, thundery lows, etc.)? NIMBUS - The satellite facility can be used to see the spatial distribution of showers. By using the temperature scale an estimate of the cloud tops temperatures can be found hence from an adjacent tephigram an estimate of the cloud heights can be made. History - Study yesterday’s charts. Did showers or thunderstorm develop in the sea air mass and if so at what time? Tephigrams - Choose a representative ascent. Is it unstable? Is it moist or dry? In general the higher the moisture content, the more likely it is that convection will be vigorous with showers or thunderstorm. Find the temperature required to release instability. Using the heating curve this will give you a good idea when showers will occur. If the ascent is very unstable then the larger CU will build up quite rapidly and the showers will start earlier. Possible changes - We are interested in whether the ascent will become more unstable, less unstable, moister or drier. 4.1 Showers The distinction between the conditions which give rise to showers, and those which do not, is a fine one. There is no technique which enables a forecaster to say exactly when any specific place will have a shower. As a summary of shower formation we can say that showers are likely if the cloud is greater than 5000 ft in depth with cloud top temperatures colder than -120C. From the study of radar imagery has shown that showers are not always randomly distributed. As an example the North Channel between Scotland and Northern Ireland can produce semi-permanent shower patterns due to the long warm and Page 5 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College moist sea track. This has the effect of producing significant rain/snow falls in parts of Wales and Cornwall while the majority of the country is cloud free. Significant wind shears can deplete large CU of their rainfall, allowing only lighter precipitation to reach the ground. More detail is given in the Convective Cloud Forecasting notes. 4.2 Cumulonimbus and thunderstorms Cumulonimbus(CB) are important because we associate thunderstorms, hail and flash floods with larger CB, and heavy rain even with smaller CB. These are easy to track using radar and satellite but remember about daughter cell formation when tracking larger storms. The large amounts of heavy localised precipitation can cause most havoc when falling on very dry ground which is unable to absorb the larger quantities of water. The water quickly accumulated in rivers and roads producing the summer flash floods which can destroy bridges and roads on occasions. The Environment Agency and other customers are interested in the amounts of precipitation falling over a short period. Some local accumulations can be in excess of 100 mm in a few hours. For the development of thunderstorm, we need a large depth of convection with a large amount of moisture. The temperature of the top of the cloud should be colder than 200C. Look out for reports of heavy rain, SFLOC activity or large echoes on the radar. Note that CB and thunderstorms are often embedded within fronts, especially cold fronts, and in these circumstances can be very difficult to spot. Polar lows in winter, heat lows and convergence lines in summer are other favoured mechanisms for CB and thunderstorm formation. 5 Type of precipitation So far we have only discussed precipitation in general, but it is necessary to distinguish between the various types of precipitation. 5.1 Hail Hail is usually forecast whenever large CB are possible. The temperature of the top of the cloud should be -200C or colder. Little conclusive work has yet been done on hail in Page 6 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting this country but the following technique has been suggested:forecast hail if the parcel method of convection gives cloud tops of 15 000 ft or more and the path and environment curves are at least 40C apart A similar method, based on the parcel curve, is:1. On a representative sounding, construct the parcel curve. 2. At the point where this curve reaches -200C, measure the difference between this temperature and the environment temperature. 3. If this difference is equal to or greater than 50C, forecast hail. If this difference lies between 50C and 2.50C, forecast soft hail or rain. If this difference is less than 2.50C, forecast rain. For large hail then a ‘steady state’ storm is required where the hail can circulate within the CB for a sufficient time to allow the hail to increase in size. Page 7 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College Figure 1. 5.2 Conditions required for hail. Drizzle When drizzle forms, the rarity of ice crystals in cloud with cloud-top temperatures greater than -50C indicates that the coalescence mechanism is predominantly responsible. The minimum depth of cloud for producing drizzle is around 2000 ft (this also implies that in a stratus situation if it begins to drizzle then the cloud will probably be at least 2000 ft thick!). The main problem in winter is determining if the precipitation will reach the ground as rain, snow or rain and snow mixed. The temperatures in the lowest part of the atmosphere are the most critical in determining what will fall at the surface hence most of the snow predictors we use are based on the temperatures in the lowest 100 hPa. Wet bulb temperature is an important feature to watch because when rain commences the dry bulb temperature is reduced by evaporative cooling to the wet bulb, often within a period of one or two hours. Page 8 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting 5.3 Rain or snow? Whether precipitation will fall as rain or snow can be difficult to forecast. There are many factors to consider. Site - Higher inland sites are more prone to snow than low coastal sites. Snow cover - If snow is already lying and quite extensive then precipitation is more likely to fall as snow since the lowest layers of the atmosphere will be cooler. This implies that if there is extensive snow cover snow can be forecast with a higher 1000-850 hPa thickness value than would be expected. Wind direction - If on a coastal site the winds are blowing from the sea this effectively warms the lowest part of the atmosphere. Most of the precipitation is rain or rain and snow mixed, but if the wind changes slightly, and has a cooler land track, especially when snow is already lying inland, then the precipitation can readily change to snow. If the situation arises where there is a cold easterly wind at low-level undercutting the warmer moister air then the potential for large amounts of snow increases, as the lowlevel thickness values fall. Warm front approaching - This scenario is one which causes many problems for forecasters because of the potential for large accumulations of snow. If the air at low levels ahead of the front is very cold (e.g. after good radiation conditions) then precipitation can start of as snow before turning to rain as the warm air approaches. The situations which cause problems is when the warm from becomes slow moving or stationary to the south of you and your station remain in the cold air. In this circumstance most of the frontal precipitation tends to be slight but if a shallow wave develops upstream then the potential for significant accumulations of snow in enhanced. Guidelines given in the Handbook of Weather Forecasting, paragraph 19.7.6.3, suggest that if the warm air mass is tropical maritime, with wet-bulb temperatures around +100C then in the cold air snow rarely falls within 50 miles of the front. On the other hand, if the warm air mass is polar maritime, with a wet bulb temperature of the order of 4.50C then in the cold air snow may extend right up to the front. Polar Lows - They tend to be very important features in the northern parts of Scotland and Ireland due to the significant snow falls associated with them. They can be identified from satellite and tracked before coming into radar range. Don’t ignore ships with high winds and weather Page 9 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College which are at odds with the chart - they may be right! Remember the model cannot handle these small scale features well. Snow showers - One significant feature of winter snow showers in a westerly is the great depth of instability giving large CB which produce heavy and sometimes prolonged precipitation. With frequent heavy showers precipitation can turn to snow with higher initial temperatures than from frontal precipitation - see table 1. Initial wet bulb temperature Type of precipitation To which snow will descend To which snow is unlikely Prolonged frontal precipitation +2.0 C +2.5 C Extensive areas of moderate or heavy instability precipitation +3.0 C +3.5 C Table 1. The relationship between downward penetration of snow beneath the 0C level and initial wet bulb temperature, from Handbook of Weather Forecasting, paragraph 19.7.61f Drifting or blowing snow - Can be a serious aviation hazard. It can also be a more widespread problem bringing communications to a stand still with large snow drifts and terrible visibility. With air temperatures less than zero and dry snow we need: wind <12 kn for no significant drifting wind 12-16 kn for slight to moderate accumulations wind >17 kn severe drifting or blowing snow There are several snow predictors available to the forecaster and these are shown in the Annex. One of the more reliable methods is Boyden’s adjusted 1000-850 hPa thickness method and as with most methods relates the mean temperature for the lower part of the atmosphere to the risk of snow. The 1000-500 hPa thickness is unreliable because it can be affected by warm or cold air aloft which has little influence to the precipitation near the surface. Page 10 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting 5.4 Freezing precipitation Freezing precipitation can be in the form of rain or drizzle. Freezing rain is caused when solid precipitation falls through a layer with positive air temperatures and melts before falling through a shallow sub-zero layer near the surface. When the rain hits the cold ground it spreads out before freezing forming a sheet of glazed ice. This is a very dangerous phenomena and can cause many accidents on the roads, with pedestrians and is a severe hazard for aircraft operations. A typical ascent for freezing rain is shown in Figure 2. This ascent is most often found in a situation where the surface has been intensely cooled due to radiation (or cold low level advection) with an approaching warm front. As the front approaches the precipitation falls as freezing rain before the ground warms to positive temperatures due to the warm airmass. Freezing drizzle normally occurs from a similar process to that of freezing rain but it is possible to get freezing drizzle from a complete sub-zero ascent. If no ice particles are present in the stratiform cloud, which could easily be the case with temperatures just below zero, then coalescence can still occur with supercooled droplets which then freeze on reaching the ground. Page 11 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College Figure 1. The typical ascent for freezing rain. Page 12 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting 6 Quantity of precipitation The public often want to know how much rain they are likely to get, rather than just whether it is going to rain. To aid you in determining this, some stations broadcast reports of the amount of rainfall that has fallen in the past hour. These messages are of the form SREW iiiRRR, where RRR is the rainfall in tenths of a millimetre. These are readily available on NIMBUS, so by continuity you can get a rough idea of the totals expected in your area, bearing in mind the effects of orography on the precipitation pattern. For short-term forecasting of precipitation, rainfall radar displays and UKMO’s NIMROD system are the best guide in timing the onset and cessation of rain and for assessing the movement and intensity of rain areas. Development of showers and systems can also be monitored in this way. 7 Snow Predictors 7.1 Boyden’s technique using 1000 - 850 Thickness The 1000–850 hPa thickness needs adjustment using the following formula: C= A + (H1000 - HGR)/30 Where: C = corrected value for 1000 - 850 hPa thickness A = actual 1000 - 850 hPa thickness (gpm) (H1000) = the 1000 hPa height (HGR) = height of station or ground above sea level Using the corrected values of 1000–850 hPa thickness the probability of snow is as follows: Percentage probability of snow Adjusted value of 1000–850 Technique hPa thickness (gpm) 90% 70% 50% 30% 10% 1281 1290 1293 1298 1303 Figure 3 incorporates these corrections and it illustrates how a snow probability may be estimated. Page 13 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College Figure 3. Forecasting the probability of precipitation as snow. How to find the probability of snow at a station with an elevation of 750 ft (230 m), a surface pressure of 990 hPa and a 1000–850 hPa thickness of 1295 gpm. 7.2 Height of wet bulb zero degree isotherm above ground level The height of the 0 °C wet-bulb temperature additionally takes into account latent cooling effects. Beware of cold surface air undercutting warm; Hand uses mean temperature of the lowest 100 hPa. Height of 0 °C wet-bulb temperature Form of precipitation Below 1000 ft Mostly snow; only light or occasional precipitation Page 14 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Precipitation Forecasting falls as rain. 7.3 1000–2000 ft Persistent rain readily turns to snow 2000–3000 ft Mostly rain; snow unlikely 3000 ft or over Almost always rain; snow rare Hand's rule Use of mean temperature of lowest 100 hPa above ground to predict type of precipitation at the surface. In heavy and persistent precipitation lowest layers will be further cooled by latent heat of evaporation. 7.4 Mean temperature (°C) in lowest 100 hPa above surface Precipitation type usually reaching surface < -1.5 snow -1.5 to 0.5 sleet > 0.5 rain Height of zero degree isotherm above ground level o Height of 0 C isotherm agl (hPa) Probability of snow 7.5 12 25 35 45 61 90% 70% 50% 30% 10% Screen wet-bulb temperature technique (Lumb) For an exposed station at height H (in hundreds of metres) in central and western regions of the UK under moderate easterly, or stronger, winds: 1. for elevations up to 170 m: Page 15 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc Met Office College Rain turns to melting snow if: Tw < (2.1 - 0.6H) °C Rain turns to lying snow if: Tw < (0.6H) °C where Tw is surface wet-bulb temperature when precipitation begins. 2. for elevations 170 to 350 m: Snow probable if: Tw < (2.1 - 0.6H) °C 3. If Tw > 2.5 °C rain is more likely than sleet, irrespective of elevation. Winds should be at least moderate with a good cover of low or medium level cloud. Figure 2. Diagrammatic form of Lumb’s method for snow prediction. 8 Further Reading For further details on this topic the best reference source is Met 0875, Handbook of Weather Forecasting, Chapter 19. Section 19.7 deals specifically with the forecasting of precipitation. Page 16 of 16 Last Saved Date : 15 February 2016 File: MS-TRAIN-COLLEGE-WORK-d:\533546845.doc