2 | 56: M. Haldenby - C. Haldenby, 0.0, |
| NS |
3 | N | 2 | -2 |
-100 | 42.59 |
2 | 56: M. Haldenby - C. Haldenby, 0.0, |
| NS |
3 | E | 5 | -2 |
100 | 61.52 |
3 | 57: Z. Świderek - A. Rydz, 4.5, MP/SW |
| NS |
3 | N | 7 | = |
140 | 77.78 |
3 | 57: Z. Świderek - A. Rydz, 4.5, MP/SW |
| NS |
5 x | N | A | = |
850 | 100.00 |
4 | 54: K. Gliński - M. Matusiak, 0.0, PD |
| NS |
5 | W | 8 | +1 |
-420 | 98.15 |
4 | 54: K. Gliński - M. Matusiak, 0.0, PD |
| NS |
1 | E | 5 | +1 |
-120 | 29.63 |
5 | 55: R. Szopiński - A. Wójcik, 12.0, ZP |
| NS |
3 | W | 4 | -2 |
200 | 81.48 |
5 | 55: R. Szopiński - A. Wójcik, 12.0, ZP |
| NS |
3 | N | Q | -1 |
-50 | 5.56 |
6 | 52: I. Wróblewska - P. Wróblewski, 1.5, MA |
| NS |
5 | S | 6 | = |
400 | 83.33 |
6 | 52: I. Wróblewska - P. Wróblewski, 1.5, MA |
| NS |
6 | N | 4 | = |
1430 | 100.00 |
7 | 53: K. Marcinkiewicz - E. Kucewicz-Ciach, 0.0, |
| NS |
3 x | W | 10 | -4 |
800 | 100.00 |
7 | 53: K. Marcinkiewicz - E. Kucewicz-Ciach, 0.0, |
| NS |
3 | S | A | = |
110 | 99.38 |
8 | 64: K. Frąckiewicz - E. Brewińska, 0.0, -/MA |
| NS |
3 | N | 7 | = |
140 | 59.26 |
8 | 64: K. Frąckiewicz - E. Brewińska, 0.0, -/MA |
| NS |
3 | S | 8 | +2 |
660 | 73.05 |
9 | 62: W. Sadowski - P. Kowalewski, 0.0, -/MA |
| NS |
3 | N | 7 | -1 |
-50 | 24.07 |
9 | 62: W. Sadowski - P. Kowalewski, 0.0, -/MA |
| NS |
5 | N | 8 | = |
600 | 53.70 |
10 | 63: K. Tarabańska - G. Szatkowski, 0.0, KP |
| EW |
5 | E | A | = |
-450 | 81.48 |
10 | 63: K. Tarabańska - G. Szatkowski, 0.0, KP |
| EW |
5 | E | J | -1 |
100 | 57.41 |
11 | 60: R. Koszowska - Z. Koszowski, 9.0, SL |
| EW |
4 | W | Q | = |
-620 | 66.67 |
11 | 60: R. Koszowska - Z. Koszowski, 9.0, SL |
| EW |
3 | E | A | -2 |
100 | 22.22 |
12 | 61: A. Bułat - T. Cesarz, 2.5, MP/- |
| EW |
4 | E | 8 | +2 |
-680 | 85.19 |
12 | 61: A. Bułat - T. Cesarz, 2.5, MP/- |
| EW |
4 | N | 3 | = |
620 | 50.00 |
13 | 58: J. Bejma - J. Kilanowicz-Bosek, 2.5, MA |
| EW |
1 | E | A | = |
-80 | 48.15 |
13 | 58: J. Bejma - J. Kilanowicz-Bosek, 2.5, MA |
| EW |
4 | N | 7 | -1 |
-100 | 68.52 |