1 | 311: P. Wydra - K. Barnat, 4.5, MA |
4 | NS |
3  | S | 8 | -5 |
-500 | 3.89 |
1 | 311: P. Wydra - K. Barnat, 4.5, MA |
5 | NS |
2  | W | Q | = |
-110 | 58.99 |
1 | 311: P. Wydra - K. Barnat, 4.5, MA |
6 | NS |
4  | S | 8 | = |
420 | 11.85 |
2 | 309: J. Otulak - M. Smolińska, 3.0, MA |
1 | NS |
3  | S | 6 | -1 |
-50 | 19.13 |
2 | 309: J. Otulak - M. Smolińska, 3.0, MA |
2 | NS |
3  | W | 6 | +2 |
-200 | 88.69 |
2 | 309: J. Otulak - M. Smolińska, 3.0, MA |
3 | NS |
3  | W | 3 | -4 |
400 | 86.31 |
3 | 307: B. Rożek - M. Jakubisiak, 4.0, MA |
25 | NS |
3  | S | 2 | -1 |
-50 | 54.00 |
3 | 307: B. Rożek - M. Jakubisiak, 4.0, MA |
26 | NS |
4  | N | 8 | = |
620 | 61.14 |
3 | 307: B. Rożek - M. Jakubisiak, 4.0, MA |
27 | NS |
3  | N | 2 | +3 |
490 | 87.50 |
4 | 305: M. Borkowski - M. Rożek, 5.5, MA |
22 | NS |
4 x | N | K | +1 |
690 | 97.86 |
4 | 305: M. Borkowski - M. Rożek, 5.5, MA |
23 | NS |
3  | S | K | = |
140 | 51.14 |
4 | 305: M. Borkowski - M. Rożek, 5.5, MA |
24 | NS |
3  | S | 10 | = |
400 | 74.64 |
5 | 303: B. Długosz - M. Budzyński, 1.5, MA |
19 | NS |
2  | S | J | +2 |
130 | 70.34 |
5 | 303: B. Długosz - M. Budzyński, 1.5, MA |
20 | NS |
4  | E | A | = |
-620 | 17.91 |
5 | 303: B. Długosz - M. Budzyński, 1.5, MA |
21 | NS |
5  | N | 6 | +1 |
620 | 10.17 |
7 | 299: J. Jaworski - S. Rokicki, 4.5, MA |
13 | EW |
3  | N | 8 | -1 |
-100 | 26.39 |
7 | 299: J. Jaworski - S. Rokicki, 4.5, MA |
14 | EW |
3  | S | 5 | = |
110 | 34.87 |
7 | 299: J. Jaworski - S. Rokicki, 4.5, MA |
15 | EW |
3  | E | J | +2 |
-150 | 21.45 |
8 | 296: M. Hołowacz - W. Turant, 0.5, MA |
10 | EW |
4  | W | A | +2 |
-680 | 81.21 |
8 | 296: M. Hołowacz - W. Turant, 0.5, MA |
11 | EW |
3  | W | 5 | +1 |
-430 | 79.25 |
8 | 296: M. Hołowacz - W. Turant, 0.5, MA |
12 | EW |
3  | E | J | +2 |
-460 | 91.93 |
9 | 292: M. Hołowacz - W. Wnuk, 5.5, MA |
7 | EW |
3  | N | 3 | +1 |
630 | 39.45 |
9 | 292: M. Hołowacz - W. Wnuk, 5.5, MA |
8 | EW |
3  | S | A | -3 |
-150 | 91.62 |
9 | 292: M. Hołowacz - W. Wnuk, 5.5, MA |
9 | EW |
3  | W | 10 | = |
-600 | 91.01 |