| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 2 | 3.760 | 64/4:00.640 |
| 2 | 2 | 3.380 | 68/4:02.760 |
| 3 | 2 | 3.280 | 70/4:03.133 |
| 4 | 2 | 3.920 | 67/4:00.195 |
| 5 | 2 | 3.420 | 68/4:01.536 |
| 6 | 2 | 3.470 | 68/4:00.607 |
| 7 | 2 | 3.520 | 68/4:00.429 |
| 8 | 2 | 3.530 | 68/4:00.380 |
| 9 | 2 | 3.770 | 68/4:02.156 |
| 10 | 2 | 3.580 | 68/4:02.284 |
| 11 | 2 | 3.520 | 68/4:02.018 |
| 12 | 2 | 3.620 | 68/4:02.363 |
| 13 | 2 | 3.400 | 68/4:01.505 |
| 14 | 2 | 3.610 | 68/4:01.789 |
| 15 | 2 | 7.830 | 63/4:01.962 |
| 16 | 2 | 3.710 | 63/4:01.447 |
| 17 | 2 | 3.870 | 63/4:01.586 |
| 18 | 2 | 3.820 | 63/4:01.535 |
| 19 | 2 | 3.740 | 63/4:01.224 |
| 20 | 2 | 3.810 | 63/4:01.164 |
| 21 | 2 | 3.610 | 63/4:00.510 |
| 22 | 2 | 3.500 | 64/4:03.404 |
| 23 | 2 | 3.560 | 64/4:02.727 |
| 24 | 2 | 3.470 | 64/4:01.867 |
| 25 | 2 | 3.620 | 64/4:01.459 |
| 26 | 2 | 3.810 | 64/4:01.551 |
| 27 | 2 | 3.300 | 64/4:00.427 |
| 28 | 2 | 3.610 | 64/4:00.091 |
| 29 | 2 | 7.690 | 62/4:01.009 |
| 30 | 2 | 3.810 | 62/4:00.849 |
| 31 | 2 | 3.630 | 62/4:00.340 |
| 32 | 2 | 3.610 | 63/4:03.692 |
| 33 | 2 | 7.550 | 61/4:02.762 |
| 34 | 2 | 3.670 | 61/4:02.206 |
| 35 | 2 | 3.770 | 61/4:01.856 |
| 36 | 2 | 3.750 | 61/4:01.492 |
| 37 | 2 | 3.400 | 61/4:00.571 |
| 38 | 2 | 3.700 | 61/4:00.179 |
| 39 | 2 | 3.830 | 61/4:00.012 |
| 40 | 2 | 3.750 | 62/4:03.660 |
| 41 | 2 | 3.390 | 62/4:02.843 |
| 42 | 2 | 3.380 | 62/4:02.051 |
| 43 | 2 | 3.450 | 62/4:01.396 |
| 44 | 2 | 3.400 | 62/4:00.701 |
| 45 | 2 | 3.520 | 62/4:00.202 |
| 46 | 2 | 3.440 | 63/4:03.481 |
| 47 | 2 | 3.760 | 63/4:03.341 |
| 48 | 2 | 6.750 | 62/4:03.208 |
| 49 | 2 | 3.440 | 62/4:02.597 |
| 50 | 2 | 3.720 | 62/4:02.358 |
| 51 | 2 | 4.470 | 62/4:03.040 |
| 52 | 2 | 4.410 | 62/4:03.624 |
| 53 | 2 | 3.410 | 62/4:03.017 |
| 54 | 2 | 6.600 | 61/4:02.125 |
| 55 | 2 | 3.390 | 61/4:01.482 |
| 56 | 2 | 3.580 | 61/4:01.070 |
| 57 | 2 | 3.550 | 61/4:00.640 |
| 58 | 2 | 6.310 | 61/4:03.127 |
| 59 | 2 | 3.650 | 61/4:02.780 |
| 60 | 2 | 3.510 | 61/4:02.302 |
| 61 | 2 | 4.060 | 61/4:02.390 |