You are viewing an old version of this page. View the current version.

Compare with Current View Page History

« Previous Version 35 Next »

Please note that numbering/ordering does not indicate/imply any sort of priority. Recent entries/changes/updates are shown in green.

Topic / titleDescriptionRelated activities
2m Temperature  
1. 2m temperature in the presence of inversionsIn common with all models, 2m temperature forecasts from the IFS tend to have much larger errors, on average, during low level inversion situations, which are particularly common at high latitudes in winter. The basic physical explanation is that a set change in atmospheric energy content has a much larger impact on screen temperature in inversion situations than in unstable situations, because the energy change is commuted through a much smaller depth of the atmosphere (e.g. metres rather than kilometres). The lower the inversion, the larger is the potential error. There is also sensitivity here to the method we use to interpolate between air temperature at the lowest model level (~10m) and skin temperature (2m temperature is a diagnostic, not direct model output). 
2. City temperatures too lowDue to the urban heat island effect not being represented, screen temperatures in large urban areas, particularly cities, are commonly too low compared to observations. The problem can be accentuated in winter by snow cover.'Urban tiles' due in land surface scheme in 2016/17
3. Screen temperatures fall too much near coastsAs a consequence of the radiation grid being larger than the model grid (due to computational constraints) night-time radiative cooling over land near to the coast is often too rapid. This is because cooling progresses according to T4, and at near-coast points T is approximately the average temperature of the land and (warmer) ocean. As a result screen temperatures drop too much - related errors can sometimes exceed 10C. The problem is enhanced (i) when there is snow cover, (ii) at high latitudes, and (iii) where coasts have a convex shape (land-relative).Improvements due to radiation code 'fixes' will come with the cycle 41R2 in early 2016. More substantial radiation code changes are likely in the longer term.
4. Meteogram temperature issues in complex topographyIn addition to the normal problems of representing screen temperatures in complex topography in current-generation global models, the user should be aware that the method by which screen temperatures on Meteograms are generated from model screen temperatures assumes a standard lapse rate (6.5oC drop per km increase in altitude), and so if the difference in height between the site chosen, and the nearest model gridpoint (as shown in the ENSgram title) is large, the scope for large errors/biases increases. This is especially true in winter-time when inversions are more common: by definition an inversion implies a temperature increase with height, not a decrease, so the temperature correction applied could even be in the wrong direction. This issue is compounded by item 1 above.Resolution upgrade early in 2016 will help. Re-calibration project  should help even more.
5. China cold spot

In products that intrinsically display 2m temperature output in some 'anomaly' form - such as monthly forecast anomalies, seasonal forecast anomalies, and in the shorter ranges EFI and SOT - there is a semi-permanent winter-time 'cold spot' over eastern China. It is not real in the sense that temperatures are not always 'below normal' in this area when they are shown to be. The cold spot owes its existence to incompatibilities between the current forecasting system, and ERA-Interim (ERA-I). ERA-I re-analyses are used to start the re-forecasts which form the 'climatology' against which current forecasts are compared. So whilst these re-forecasts are rightly performed with the latest model version, they also inherit, as a starting point, auxiliary data such as snow depth from ERA-I, in fact from the ERA-I 'offline fields'. In turn this offline snow depth inevitably derives, in part, from what the ERA-I model puts on the ground in the way of snowfall, and this model's climatology is such that there is less snowfall in this area, on average, than in the current HRES. In turn, an intrinsic part of the offline run is a re-scaling using GPCP climatology, and the GPCP climate meanwhile is much drier in winter than either the IFS or ERA-I. So HRES and other IFS components are inclined to have a much deeper snow cover in their analyses through the winter than the re-forecasts have in theirs, which encourages the development of 2m temperatures that are similarly much lower - ie the 'cold spot' anomalies.

The problem is compounded by a historical dearth of observations in this area which might have helped bring things back on track, and also by a snow analysis scheme 'feature' that excludes all observations above 1500m (the said area is around 4000m). This cut-off helps avoid problems in complex terrain, though could be improved by using instead a measure of sub-grid orography. The limited number of observations that do exist suggest that the winter-time snowfall climatology is rather better in IFS than in ERA-I offline, implying that the IFS' absolute 2m temperature forecasts should be more reliable than our anomaly-format products.

 
Precipitation  

6. Marine convection propagation

In reality shower cells have a finite lifetime, so precipitation associated moves with the showers, as one can see on radar. In the IFS showers are instantaneous (as they are parametrised) and the related precipitation does not propagate. So showers triggered over the sea do not generally move inland in the model as they should. This can lead to under-prediction errors of several mm in inland locations, 10mm or more in extremis. The degree to which the error extends inland depends on the windspeed at the steering level for showers. For stronger winds the errors extend further inland. For snow showers the errors can be worse still, compounded by the relatively slow fall speed of snowflakes (up to say one tenth of that of raindrops). So a snowflake starting its descent at the coast might end up on the ground 100km inland, if winds are strong, whereas a raindrop in equivalent summer conditions might only propagate 20km before reaching the ground. 
7. Underestimation of orographically-enhanced precipitationAs a consequence of topographical barriers being too low, in general (due to resolution), both the orographic enhancement of precipitation and the rain shadow effect tend to be underestimated in the IFS (more so in ENS than HRES, and more so in ENS after 10 days when resolution changes).Resolution upgrade in early 2016

8. Underestimation of convective precipitation extremes

As a consequence of resolution, and the related parametrisation of convection, localised extreme values in precipitation totals will be systematically "underestimated" in IFS output. Differences equal to about one order of magnitude are possible. However this is not as bad as it seems, because when verified over areas that are the same size as the effective model gridbox size the agreement is generally much better.

Resolution upgrade in early 2016. New ways of forecasting the degree of sub-grid variability in precipitation totals are under investigation.
9. Tropical rainfall extremes greatest on day 1

If one examines the distribution, in forecasts, of daily rainfall totals for locations in the tropics, the (wet) tails tend to be longer for very short lead times (eg T+0 to T+24), implying that ENS and HRES have a greater propensity to generate extreme rainfall in short range forecasts than they do in medium range forecasts. For example the 99th percentile of daily rainfall at some locations at day 1 is twice what it is at day 3. This would appear to be a 'spin down' issue, of sorts, related to the handling of convection. Formulation of the EFI and SOT is such that they intrinsically account for this (though note item 19 below), so the problem arises for the user particularly when referencing the direct model output.

 

10. Extreme rainfall at certain gridpoints ("rain bombs")

At particular gridpoints, that lie in areas of complex topography, IFS forecasts (notably HRES) can occasionally generate extreme localised precipitation totals in a matter of hours, say well over 100mm, when at neighbouring locations the amounts are far less. These extremes are incorrect; the error occurs in convective situations with light winds. Only a small number of gridpoints around the world are affected - mainly these lie in the following areas: southern China, parts of Eastern Africa, Papua New Guinea, along the Andes, southern Mexico. The cause is understood though is too involved to describe in detail here; in short it relates to a weakness in the semi-Lagrangian scheme (part of the model numerics). Tests have shown that the error will go away when the grid structure and model resolution are changed with the next cycle.Resolution upgrade in early 2016 will solve.
Snow  
11. Snow drift in convective situationsWhen snow falls through cloud or beneath cloud it drifts with the wind. For large-scale (dynamic) precipitation IFS physics accounts for this. For convective precipitation however it does not; there is no drift, the precipitation arrives at the surface instantaneously once the convection is diagnosed, in the place that it is diagnosed. As a result snow arising from convective processes may be misplaced in the model (too far upwind), and the errors will be larger if winds along the snowflake path are stronger. Errors can be of order 100km. Item 6 relates. The same issues exist for rain, but given the faster fallspeed of raindrops relative to the IFS model resolutions these errors are negligible. Clearly one also has to take account of the melting level. 
12. Snow on the ground takes too long to meltIn both ENS and HRES small amounts of snow on the ground tend to take too long to melt, even if the temperature of the overlying air is well above zero. This is because, for melting purposes, the snow that there is is assumed to be piled up high in one segment of a gridbox. For smaller nominal depths, the pile becomes higher, though at the same time covers a much smaller fraction of the box. The reason this is used is to improve the handling of screen temperature; by confining the snow to gridbox segments the impact on the temperature of that snow is reduced, and on average we find smaller errors and biases in 2m temperature as a result. The main downside is that snow cover pictures can look misleading, particularly at longer leads (when they can not of course be rectified by observational data). The cut-off above which snow is assumed to cover the full grid box is a 10cm depth - this is why a green hue used on standard snow depth charts on the web, which suggests to the eye the presence of some vegetation, disappears at 10cm.4-year project to address snow issues ("Earth2Observe")
13. Mixed rain/snow leads to snow accumulationIn marginal snow situations, when precipitation at the surface comprises both rain and snow, the snow component accumulates as lying snow. In the vast majority of cases this is wrong - it should melt instantaneously. This behaviour occurs because small snow depths within the model are assumed to be piled up into a small segment of a gridbox, and as such it is very difficult for them to melt quickly (as in item 12 above).4-year project to address snow issues
14. Spurious snowfall in freezing rain situationsIn certain winter situations, when snow descends through the atmosphere and melts to rain in a warm layer, before descending again through a cold (sub zero) layer, the model turns the precipitation back to snow far too readily. So surface precipitation in freezing rain situations commonly appears as snow, and that snow also accumulates on the ground. HOWEVER, it seems that where this precipitation is diagnosed as convective, this re-freezing problem does not exist.Resolved with physics changes implemented in May 2015, though monitoring still required.
15. Multiple snow layers

The model assumes that all snow on the ground has the same density (though that density does vary - e.g. increasing with age). So layers of different density, which arise in the real world, are not catered for. This can impact on several things, such as total snow water content, and upward heat conductivity, which in turn has the potential to adversely affect 2m temperature.

In addition, when new snow falls onto old, the change in snow depth is commonly less that it should be, because the density assigned to the fresh snow depends in part on the density of the pre-existing lying snow, and so tends to be greater than it should. The magnitude of the error (in snow depth change) increases when the pre-existing snow is deeper and/or has a greater density. Example: if 10cm of new snow (ratio 12:1) fell onto 10cm of old lying snow (ratio 2.5), snow depth in the model would increase by only 3.5cm.

4-year project to address snow issues
Tropical Cyclones  
16. Tropical cyclone intensityResolution limits our ability to fully capture the core of strong winds around many tropical cyclones; likewise depths can be under-estimated, by over 50hPa in extremis. The problems are larger for smaller systems, with a smaller eye - Haiyan was one such example. Often minimum pressure in HRES will be lower than in all the ENS members, and likewise winds stronger; this is because of the higher resolution of HRES. In such situations HRES guidance will often be better, but not always.With cycle 41R2 in early 2016 will come a major IFS resolution upgrade, and a substantial improvement to the resolution used in the EDA. Main impact will be to markedly reduce a positive depth bias in ENS analyses and forecasts.
17. Relatively slow-moving TCs can deepen too much in HRES

There is no coupling with the ocean in HRES. So for relatively slow moving TCs, when fluxes and mixing might in reality lead to a reduction in SST, the SST will remain at an elevated level and this can give the TC extra impetus to deepen too much (provided other factors such as shear remain favourable). For fast moving TCs the affected ocean is left behind, and so the problem is less acute or non-existent. Whilst item 16 above generates errors in the opposite sense that might sometimes fortuitously cancel, there are nonetheless recorded cases where TCs have been over-deepened, by as much as 50mb, because of the lack of coupling.

Coupling of HRES with the ocean may commence in 2017.
Miscellaneous  
18. Under-estimation of strong gusts in convective situationsAlthough there is a helpful convective contribution in the computation of maximum gusts (as used in direct model output and the EFI), experience has shown that extreme gusts are generally under-represented, particularly when vigorous convection is involved, such as one might see with MCSs or squall lines - eg 60kt gusts or more might be observed when 30-40kt gusts are predicted. This relates to (i) an inability, at current model resolution, to represent the 3-d circulation around convective systems, and (ii) the fact that it is impossible to design an adjustment in the gust computation that will work in all cases.New EFI parameters relating to severe convection were introduced in test mode in summer 2015; these can provide pointers to when errors of this type are likely.
19. Jumpiness in EFI and SOT, especially at short lead timesA consequence of the re-forecast strategy is that extreme events are sometimes not well sampled. Especially at short lead times, say 1 or 2 days, the 11 members that go up to make the re-forecast can be very similar, and so if the re-forecast dates (twice per week since May 2015) happen to be just before certain extreme events there may be some over-sampling, whilst if extreme events fall inbetween the re-forecast dates, there may be some under-sampling. Thus the tails of the model climate (M-Climate) distribution can be jumpy as we move from one lead time to another, and as EFI and SOT depend heavily on these tails, much more than they depend on solutions around the median, they can be jumpy too. The increase from 500 to 1980 re-forecast realisations effected in May 2015 has reduced the magnitude of this problem; we will continue to monitor and perhaps drop this issue in due course. 
20. Sunshine durationThe integrity of this post-processed output parameter is strongly compromised by the radiation timestep in the model (3 hours in ENS, 1 hour in HRES), which because of computational cost is longer than the basic model timestep. This manifests itself in the sunshine duration parameter being (a) an undesirable function of longitude and (b) more generally unreliable. 
21. Sea ice evolution and associated weather

Sea ice cover does not change in any interactive way in the forecasts as we do not have a sea ice model. So none of the following are represented: sea ice formation due to low air temperatures, break up due to wind effects or melting, and advection by currents and winds. In turn this affects weather that relates, such as 2m temperatures over and downwind of, and convection triggered over water but not over ice. Wave model output will naturally also be affected.

In the twice daily forecasts to day 15 sea ice cover is fixed. At longer ranges, to capture the seasonal cycle, there is relaxation towards the ice cover of the last five years; for monthly forecasts all ENS members use the average value, for seasonal forecasts members are divided into five sets (of 10) each one of which uses the pattern for one of those five years.

Sea ice model being developed
22. Very poor SST evolution near New YorkDue to the lack of resolution in the ocean component of the semi-coupled ENS system we are now running (introduced in Nov 2013 with 40R1), and an associated poor handling of the gulf stream wall, there is a major anomalous upward drift in SSTs over and S and E of the New York Bight (which itself lies just SE of New York city), in the first 10 days of the ENS forecasts. The area affected is about the size of England, and the size of the error that develops in 10 days can exceed 10C. 
23. 'Hot spots' near to glaciersWhen cycle 41R1 was introduced on 12 May 2015 an error began to appear, over certain glaciated/partly glaciated regions (e.g. Iceland, the fringes of Greenland), on 2m temperature products that represent, directly or indirectly, anomalies. Affected fields include EFI/SOT (large positive values), Meteograms with climate (M-Climate too cold) and monthly forecasts (positive anomalies regularly forecast). This error is not a reflection of the absolute forecast values themselves - those should generally be OK - but is instead indicative of an error that was inadvertently introduced into the re-forecast suite. This error makes the 2m temperature forecasts in those re-forecasts, close to glaciers, much colder than they should be, causing the actual forecasts to look like they are indicating strong positive anomalies. Initially, in May, the error was less or non-existent because it was masked by residual seasonal snow cover.The error has now been corrected. Affected re-forecasts will not themselves be rerun, although newly created re-forecasts should, from data times in early July onwards, be correct. This means that the mentioned issues slowly went away between early July and mid August 2015, as the fraction of the re-forecasts that were contaminated steadily reduced.
24. 'Cold ring' around sea ice after day 10Since the introduction of 41R1 on 12 May 2015 a ring of cold SST values (= -1.8C), about one gridbox wide, has appeared at the day 10/11 resolution change, along the edges of areas of sea ice. Locally SSTs may suddenly drop by more than 5C. This is a complex issue but relates to a change in the threshold at which sea ice cover is accepted (it is now 2%, it used to be 20%), the fact that we have to interpolate SST values onto a different grid when resolution changes, and the fact that SST is now set to -1.8C in gridboxes that include some sea ice.. A related complication is the fact that the two-way coupled ocean model runs on a different grid (1 degree). The ice cover threshold change was made to improve the handling of ocean waves in ice-margin zones, and to pave the way for introduction of a full sea ice model in the future. These advantages are considered to outweigh the 'cold ring' disadvantage. The day 10-15 EFI 2m temperature field can also be affected (showing a band of low values in the ice margin zones).Consideration is being given to perhaps removing the resolution change at day 10.
25. Missing islandsA new land-sea mask was introduced with cycle 41R1 on 12 May 2015, in order to improve representativeness. Unfortunately there were some deficiencies in the source dataset, which has meant that a few islands are no longer present in the IFS, for example Tahiti. This will clearly reduce the utility of some IFS output, for example the Tahiti meteogram, for which a sea point is now used. However we do know that this is not a widespread problem, and that only a few island grid points have been affected. There was no impact on the ocean wave model.This will be corrected in early 2016, with cycle 41R2.

  • No labels