1 | 223: A. Wódkowski - D. Kłodos, 8.0, MA |
16 | EW |
3 | N | K | +2 |
460 | -2.00 |
1 | 223: A. Wódkowski - D. Kłodos, 8.0, MA |
17 | EW |
6 | E | K | +1 |
-940 | 0.79 |
1 | 223: A. Wódkowski - D. Kłodos, 8.0, MA |
18 | EW |
2 | S | 2 | = |
110 | 0.20 |
2 | 225: K. Konopko - A. Rzechuła, 6.0, MA |
10 | EW |
4 | N | 5 | -1 |
-100 | 6.46 |
2 | 225: K. Konopko - A. Rzechuła, 6.0, MA |
11 | EW |
6 | W | 8 | = |
-980 | 4.18 |
2 | 225: K. Konopko - A. Rzechuła, 6.0, MA |
12 | EW |
3 | E | 9 | +1 |
-170 | 0.18 |
3 | 227: K. Najda - M. Kowalski, 19.0, MA |
4 | EW |
1 | W | 7 | = |
-80 | 6.43 |
3 | 227: K. Najda - M. Kowalski, 19.0, MA |
5 | EW |
3 | W | 6 | +1 |
-430 | 4.99 |
3 | 227: K. Najda - M. Kowalski, 19.0, MA |
6 | EW |
6 | S | Q | = |
980 | -10.32 |
4 | 229: J. Boczar - M. Boczar, 12.0, MA |
25 | EW |
3 | S | 10 | = |
110 | -3.07 |
4 | 229: J. Boczar - M. Boczar, 12.0, MA |
26 | EW |
4 | S | 8 | +1 |
650 | -1.36 |
4 | 229: J. Boczar - M. Boczar, 12.0, MA |
27 | EW |
3 | E | 7 | +2 |
-460 | 0.61 |
5 | 231: R. Łuczak - M. Łasiewicki, 10.0, MA |
19 | EW |
5 | S | K | = |
400 | -2.17 |
5 | 231: R. Łuczak - M. Łasiewicki, 10.0, MA |
20 | EW |
7 | N | 2 | -2 |
-200 | 5.88 |
5 | 231: R. Łuczak - M. Łasiewicki, 10.0, MA |
21 | EW |
3 | W | 10 | -2 |
100 | -3.20 |
6 | 233: T. Wolfke - S. Knothe, 12.0, MA |
13 | EW |
2 | S | 6 | = |
90 | -4.92 |
6 | 233: T. Wolfke - S. Knothe, 12.0, MA |
14 | EW |
4 | W | Q | +1 |
-450 | 0.10 |
6 | 233: T. Wolfke - S. Knothe, 12.0, MA |
15 | EW |
4 | N | 2 | = |
620 | -12.17 |
8 | 213: M. Miklaszewska - P. Piątkiewicz, 6.0, MA |
22 | NS |
3 | E | K | -1 |
100 | 8.36 |
8 | 213: M. Miklaszewska - P. Piątkiewicz, 6.0, MA |
23 | NS |
3 | W | 2 | = |
-600 | -7.27 |
8 | 213: M. Miklaszewska - P. Piątkiewicz, 6.0, MA |
24 | NS |
TD | | | |
| 0.00 |
9 | 215: M. Tuczyński - K. Marcinkowski, 7.0, MA |
1 | NS |
3 | W | J | +1 |
-430 | -0.43 |
9 | 215: M. Tuczyński - K. Marcinkowski, 7.0, MA |
2 | NS |
4 | S | 10 | +3 |
710 | -0.74 |
9 | 215: M. Tuczyński - K. Marcinkowski, 7.0, MA |
3 | NS |
1 | S | J | = |
90 | 1.96 |