Official Ratings/Rankings of ÖTTV, NÖTTV, STTV, KTTV, BTTV, TTTV, StTTV, WTTV, VTTV, OÖTTV, TTQ, TTSA, TTTA, TTV, and ELTTL.
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Kröll, Roland

All Events
DateEventInitial
Rating
Point
Change
Final
Rating
2016-10-16TTTV MM 16/17, H05918±55−5913±53
2016-10-02TTTV MM 16/17, H03951±58−33918±53
2016-09-25TTTV MM 16/17, H02928±63+23951±57
2016-09-18TTTV MM 16/17, H01931±63−3928±62
2016-04-17TTTV MM 15/16 X/Y PO, F11911±47+20931±43
2016-04-03TTTV MM 15/16 X/Y PO, F09920±47−9911±45
2016-03-20TTTV MM 15/16 X/Y PO, F08926±46−6920±45
2016-03-13TTTV MM 15/16 X/Y PO, F07899±51+27926±45
2016-03-06TTTV MM 15/16 X/Y PO, F06878±57+21899±50
2016-02-28TTTV MM 15/16 X/Y PO, F05895±60−17878±56
2016-02-21TTTV MM 15/16 X/Y PO, F04902±60−7895±59
2016-02-14TTTV MM 15/16 X/Y PO, F03905±61−3902±60
2016-01-24TTTV MM 15/16 X/Y PO, F01885±69+20905±58
2015-10-11TTTV MM 15/16, H04888±60−3885±58
2015-10-04TTTV MM 15/16, H03899±61−11888±59
2015-09-27TTTV MM 15/16, H02904±62−5899±60
2015-09-20TTTV MM 15/16, H01894±69+10904±61
2015-04-19TTTV MM 14/15 X/Y PO, F11895±53−1894±52
2015-04-12TTTV MM 14/15 X/Y PO, F10895±520895±52
2015-03-29TTTV MM 14/15 X/Y PO, F09874±54+21895±50
2015-03-22TTTV MM 14/15 X/Y PO, F08884±55−10874±53
2015-03-15TTTV MM 14/15 X/Y PO, F07889±55−5884±54
2015-03-08TTTV MM 14/15 X/Y PO, F06893±59−4889±54
2015-03-01TTTV MM 14/15 X/Y PO, F05894±59−1893±59
2015-02-22TTTV MM 14/15 X/Y PO, F04855±64+39894±58
2015-02-15TTTV MM 14/15 X/Y PO, F03855±640855±64
2015-02-01TTTV MM 14/15 X/Y PO, F02861±64−6855±62
2015-01-25TTTV MM 14/15 X/Y PO, F01802±66+59861±63
2014-11-30TTTV MM 14/15, H11802±600802±60
2014-11-23TTTV MM 14/15, H10802±590802±59
2014-11-02TTTV MM 14/15, H07805±58−3802±57
2014-10-26TTTV MM 14/15, H06805±570805±57
2014-10-19TTTV MM 14/15, H05805±560805±56
2014-10-12TTTV MM 14/15, H04791±61+14805±55
2014-10-05TTTV MM 14/15, H03792±61−1791±61
2014-09-28TTTV MM 14/15, H02793±61−1792±60
2014-09-21TTTV MM 14/15, H01793±600793±60
2014-04-13TTTV MM 13/14, F11794±39−1793±37
2014-04-06TTTV MM 13/14, F10796±38−2794±37
2014-03-30TTTV MM 13/14, F09804±38−8796±37
2014-03-23TTTV MM 13/14, F08785±40+19804±37
2014-03-16TTTV MM 13/14, F07788±39−3785±39
2014-03-09TTTV MM 13/14, F06779±41+9788±38
2014-03-02TTTV MM 13/14, F05791±43−12779±40
2014-02-23TTTV MM 13/14, F04803±47−12791±42
2014-02-16TTTV MM 13/14, F03782±53+21803±46
2014-02-02TTTV MM 13/14 X/YPO, F02782±510782±51
2014-01-26TTTV MM 13/14, F01764±55+18782±50
2013-12-08TTTV MM 13/14, H11763±50+1764±49
2013-12-01TTTV MM 13/14, H10768±50−5763±49
2013-11-24TTTV MM 13/14, H09778±52−10768±49
2013-11-17TTTV MM 13/14, H08790±56−12778±51
2013-11-10TTTV MM 13/14, H07745±58+45790±55
2013-11-03TMM MM 13/14, H06787±62−42745±58
2013-10-28TMM MM 13/14, H05780±69+7787±61
2013-10-14TMM MM 13/14, H03785±79−5780±67
2013-09-22TMM MM 13/14, H01718±94+67785±77
2012-04-01TTTV MM 11/12, F10724±44−6718±41
2012-03-25TTTV MM 11/12, F09732±45−8724±43
2012-03-11TTTV MM 11/12, F07741±44−9732±42
2012-03-04TTTV MM 11/12, F06700±48+41741±43
2012-02-26TTTV MM 11/12, F05706±50−6700±47
2012-02-19TTTV MM 11/12, F04706±490706±49
2012-02-05TTTV MM 11/12, F03722±50−16706±47
2012-01-29TTTV MM 11/12, F02733±51−11722±49
2012-01-22TTTV MM 11/12, F01710±54+23733±50
2011-11-27TTTV MM 11/12, H10696±53+14710±47
2011-11-20TTTV MM 11/12, H09661±58+35696±52
2011-11-13TTTV MM 11/12, H08665±58−4661±57
2011-10-30TTTV MM 11/12, H06680±58−15665±56
2011-10-16TTTV MM 11/12, H04682±57−2680±57
2011-10-09TTTV MM 11/12, H03644±63+38682±56
2011-10-02TTTV MM 11/12, H02654±65−10644±63
2011-09-25TTTV MM 11/12, H01667±69−13654±65
2011-04-03TTTV MM 10/11, Runde 10708±53−41667±49
2011-03-27TTTV MM 10/11, Runde 9728±61−20708±52
2010-11-21TTTV MM 10/11, Runde 10689±55+39728±45
2010-11-14TTTV MM 10/11, Runde 9675±61+14689±54
2010-11-07TTTV MM 10/11, Runde 8723±62−48675±60
2010-10-31TTTV MM 10/11, Runde 7742±64−19723±62
2010-10-24TTTV MM 10/11, Runde 6691±77+51742±63
2010-10-17TTTV MM 10/11, Runde 5714±79−23691±77
2010-10-10TTTV MM 10/11, Runde 4716±79−2714±78
2010-10-03TTTV MM 10/11, Runde 3722±80−6716±78
2010-09-26TTTV MM 10/11, Runde 2846±105−124722±79
2010-09-19TTTV MM 10/11, Runde 1850±175−4846±105

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