1 | 15: L. Reichert - P. Wojtczak, 1.0, -/LB |
17 | NS |
3 | S | 3 | -1 |
-50 | 53.22 |
1 | 15: L. Reichert - P. Wojtczak, 1.0, -/LB |
18 | NS |
3 | W | J | -1 |
50 | 51.56 |
1 | 15: L. Reichert - P. Wojtczak, 1.0, -/LB |
19 | NS |
1 | W | 8 | = |
-90 | 56.25 |
1 | 15: L. Reichert - P. Wojtczak, 1.0, -/LB |
20 | NS |
PASS | | | |
0 | 74.99 |
2 | 10: M. Zacharewicz - W. Skowron, 8.0, LB |
13 | NS |
2 | E | 9 | +1 |
-140 | 39.07 |
2 | 10: M. Zacharewicz - W. Skowron, 8.0, LB |
14 | NS |
2 | E | J | +1 |
-140 | 71.09 |
2 | 10: M. Zacharewicz - W. Skowron, 8.0, LB |
15 | NS |
3 | E | 3 | +1 |
-430 | 3.14 |
2 | 10: M. Zacharewicz - W. Skowron, 8.0, LB |
16 | NS |
5 | E | 3 | = |
-650 | 45.31 |
4 | 14: K. Lindner - R. Boberski, 5.5, LB |
21 | EW |
3 | S | K | -1 |
-100 | 76.92 |
4 | 14: K. Lindner - R. Boberski, 5.5, LB |
22 | EW |
3 | N | K | = |
140 | 30.77 |
4 | 14: K. Lindner - R. Boberski, 5.5, LB |
23 | EW |
2 | W | 5 | -2 |
200 | 33.08 |
4 | 14: K. Lindner - R. Boberski, 5.5, LB |
24 | EW |
4 x | S | Q | -2 |
-300 | 21.54 |
5 | 16: S. Kozar - S. Kotas, 10.0, LB |
5 | EW |
4 | S | K | -1 |
-100 | 34.38 |
5 | 16: S. Kozar - S. Kotas, 10.0, LB |
6 | EW |
5 | E | K | = |
-650 | 69.53 |
5 | 16: S. Kozar - S. Kotas, 10.0, LB |
7 | EW |
3 | N | 10 | +1 |
130 | 71.09 |
5 | 16: S. Kozar - S. Kotas, 10.0, LB |
8 | EW |
2 | E | 10 | -1 |
50 | 46.09 |
6 | 11: C. Plachimowicz - M. Nieznański, 12.0, LB |
25 | NS |
4 | E | 5 | = |
-620 | 12.31 |
6 | 11: C. Plachimowicz - M. Nieznański, 12.0, LB |
26 | NS |
2 | W | A | = |
-110 | 43.08 |
6 | 11: C. Plachimowicz - M. Nieznański, 12.0, LB |
27 | NS |
2 | N | K | -3 |
-150 | 11.23 |
6 | 11: C. Plachimowicz - M. Nieznański, 12.0, LB |
28 | NS |
1 | W | 6 | +1 |
-120 | 14.32 |
7 | 13: A. Niziałek - R. Góralski, 5.0, LB |
1 | EW |
4 | N | 3 | -2 |
-100 | 67.96 |
7 | 13: A. Niziałek - R. Góralski, 5.0, LB |
2 | EW |
2 | E | 8 | -1 |
50 | 21.88 |
7 | 13: A. Niziałek - R. Góralski, 5.0, LB |
3 | EW |
4 | N | K | -1 |
-50 | 91.40 |
7 | 13: A. Niziałek - R. Góralski, 5.0, LB |
4 | EW |
4 x | N | J | +2 |
1190 | 1.57 |