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Discussed in the following Daily reports:



Picture

1. Impact

Severe thunderstorm developed starting from around the town of Byala Slatina A severe thunderstorm was initiated over the Balkan mountain range (Stara planina in Bulgarian) in north-western Bulgaria moving eastwards and hitting Pleven. It moved to the east-northeast and developed quickly to a supercell badly affecting the town of Byala Slatina and Pleven, one of the biggest cities in northern Bulgaria in the afternoon hours on 15 May 2018. The storm quickly developed into a powerful long-lived supercell causing caused all possible types of convective hazards: strong winds, large hail, heavy rain and accompanying flash flooding. It caused inflicted a lot of damage on properties, cars and infrastructure. Strong winds uprooted trees and caused power outages. In the municipalities of Byala Slatina and Pleven has been declared a state of emergency.

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The development of the supercell is associated with very intense lightning activity as well. From the ESWD one can easily see the track of the supercell over northern BulgariaThe track of the supercell over the Danube plain can easily be tracked from the reports in the European Severe Weather Database (ESWD).

ATDnet lightning flash density (left) and ESWD reports (right).

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The radar imagery reveals a hook echo which is a sign of the mesocyclone development associated with the supercell.

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A sequence of consecutive CAPE-shear EFI forecasts starting from the latest one. The blue triangles denotes Pleven, one of the worst affected places in this storm.

ECMWF is just about to offer a number of new products to facilitate forecasting deep moist convection.

One of these products is the ensemble tephigrams part of which is the hodograph view. Hodographs of all 50 members, HRES and control forecast are shown with colours denoting wind at different layers in the atmosphere. This provides information about the ensemble spread at different layers alongside information about wind shear at different layers in the atmosphere. For this event, the spread in the medium range (left) is large especially going up in the atmosphere but the deep-layer shear is relatively biglarge. Low-level winds are weak with easterly components in some members. Winds become stronger higher up in the atmosphere with quite large spread in speed and direction but in general the winds they have a strong westerly component. In the short range (right plot below), the spread uncertainty decreases but still some spread is present at low levels and between 500 and 200 hPa while between 700 and 500 hPa and above 200 hPa the spread is smaller and the winds are south-westerly. The hodographs shown here suggest the presence of quite large wind shear which could favour favours organisation of convection if the latter can be initiated.

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To assess the convective instability and whether convection can be initiated, CAPE plot is provided with the ensemble tephigrams as well. CAPE is plotted in three categories depending on the range of CIN values. The fourth category is CAPE=0. In the first category CAPE is relatively easy to be released due to small CIN values less than 50 J/kg. In the second category, some substantial lift would be necessary to bring the air parcel to the level of free convection (LFC). In the third category convection is unlikely because the CIN is too high. In this case, in the medium range forecast (T+108h) ensemble members are distributed in all 4 groups. The most populated groups are the second one and  that with CAPE=0. A lot of members fall also in the third group where HRES and Control forecast belong to. In total there are 23 members (9+14) out of 50 which potentially can develop deep moist convection and HRES is not among them. The instability itself is moderate with CAPE values mostly between 300 and 800 J/kg. There are few members in the first category with CAPE greater than 1000 J/kg. In the short range, most members (28 out of 50) plus HRES and control forecast show convective instability in the forecast but most of them including Control forecast are in the second category requiring more substantial lift so that convection could be initiated. Still quite a lot of members (19) have very large CIN and in this group the CAPE is not particularly high in this group either.

CAPE plot showing CAPE distributed into 3 categories + CAPE=0 (shown in the title) for T+108h (left) and T+12h (right).


With the IFS cycle 45r1 lightning density is added as a new model parameter. HRES forecast in the medium range (T+114h) does not have much lightning over the affected area because of the very strong capping (large CIN values) while the short-range forecast (T+18h) have the signal in the right place over NW Bulgaria but overpredicted lightning intensity over southern Romania. In this case, one can see the value of having an ensemble system. Probabilistic forecast in the medium range (T+114h) provided very good guidance on the area under greatest threat of intense lightning activity.

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Probabilities of the new maximum CAPE parameter to be above 1000 J/kg highlights the affected area in the medium range whilst in the short-range forecasts that area stands out. It’s worth mentioning that the probability of high CAPE is very high over the central part of southern Romania but severe storms fail to develop there.

Probability of maximum CAPE greater than 1000 J/kg at T+114h (left) and T+18h (right).

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