| 1 | 24: Z. Mróz - J. Poznar, 5.5, DS |
17 | NS |
1  | E | 8 | -2 |
100 | -0.45 |
| 1 | 24: Z. Mróz - J. Poznar, 5.5, DS |
18 | NS |
6  | E | 9 | +1 |
-1010 | -4.41 |
| 1 | 24: Z. Mróz - J. Poznar, 5.5, DS |
19 | NS |
2  | E | 4 | +1 |
-140 | -1.65 |
| 1 | 24: Z. Mróz - J. Poznar, 5.5, DS |
20 | NS |
4  | S | 8 | = |
620 | 4.55 |
| 3 | 26: R. Rączkowski - S. Grybel, 8.0, DS |
9 | EW |
1  | S | 8 | -1 |
-50 | 0.93 |
| 3 | 26: R. Rączkowski - S. Grybel, 8.0, DS |
10 | EW |
2  | E | 2 | = |
-110 | 0.74 |
| 3 | 26: R. Rączkowski - S. Grybel, 8.0, DS |
11 | EW |
1  | W | 4 | +3 |
-170 | -0.84 |
| 3 | 26: R. Rączkowski - S. Grybel, 8.0, DS |
12 | EW |
4  | W | 5 | = |
-420 | 1.39 |
| 4 | 23: K. Jankowiak - L. Jarząb, 4.0, DS |
21 | EW |
3  | W | 5 | -3 |
150 | 1.22 |
| 4 | 23: K. Jankowiak - L. Jarząb, 4.0, DS |
22 | EW |
5 x | W | 3 | -2 |
500 | -1.72 |
| 4 | 23: K. Jankowiak - L. Jarząb, 4.0, DS |
23 | EW |
2  | N | 3 | -2 |
-200 | 1.05 |
| 4 | 23: K. Jankowiak - L. Jarząb, 4.0, DS |
24 | EW |
2  | N | J | = |
110 | -1.42 |
| 5 | 25: A. Janiak - E. Gąska, 10.0, DS |
5 | EW |
2  | W | K | +1 |
-140 | 0.76 |
| 5 | 25: A. Janiak - E. Gąska, 10.0, DS |
6 | EW |
3  | N | J | +1 |
430 | -2.13 |
| 5 | 25: A. Janiak - E. Gąska, 10.0, DS |
7 | EW |
4  | N | Q | +1 |
650 | -0.78 |
| 5 | 25: A. Janiak - E. Gąska, 10.0, DS |
8 | EW |
4  | W | 3 | +2 |
-480 | 1.10 |
| 6 | 20: R. Siwak - R. Siwiec, 6.5, DS |
25 | NS |
4  | N | 3 | = |
420 | 1.26 |
| 6 | 20: R. Siwak - R. Siwiec, 6.5, DS |
26 | NS |
2  | E | A | = |
-110 | -1.48 |
| 6 | 20: R. Siwak - R. Siwiec, 6.5, DS |
27 | NS |
3  | E | 7 | +2 |
-460 | -3.04 |
| 6 | 20: R. Siwak - R. Siwiec, 6.5, DS |
28 | NS |
4  | W | 8 | = |
-420 | -5.90 |
| 7 | 22: T. Błażejowska - G. Czapulak, 6.5, DS |
1 | EW |
3  | N | A | +1 |
130 | 5.02 |
| 7 | 22: T. Błażejowska - G. Czapulak, 6.5, DS |
2 | EW |
4  | S | K | -1 |
-100 | 4.29 |
| 7 | 22: T. Błażejowska - G. Czapulak, 6.5, DS |
3 | EW |
3  | W | K | +3 |
-690 | -0.25 |
| 7 | 22: T. Błażejowska - G. Czapulak, 6.5, DS |
4 | EW |
3  | W | K | = |
-140 | 4.93 |