| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 2 | 3.963 | 61/4:01.743 |
| 2 | 2 | 3.917 | 61/4:00.340 |
| 3 | 2 | 3.921 | 62/4:03.887 |
| 4 | 2 | 3.985 | 61/4:00.737 |
| 5 | 2 | 3.901 | 61/4:00.181 |
| 6 | 2 | 4.028 | 61/4:01.102 |
| 7 | 2 | 3.940 | 61/4:00.994 |
| 8 | 2 | 3.924 | 61/4:00.790 |
| 9 | 2 | 3.945 | 61/4:00.774 |
| 10 | 2 | 3.986 | 61/4:01.011 |
| 11 | 2 | 3.904 | 61/4:00.750 |
| 12 | 2 | 3.940 | 61/4:00.716 |
| 13 | 2 | 5.408 | 60/4:03.517 |
| 14 | 2 | 4.182 | 60/4:04.046 |
| 15 | 2 | 4.101 | 59/4:00.110 |
| 16 | 2 | 3.958 | 60/4:03.761 |
| 17 | 2 | 4.045 | 60/4:03.699 |
| 18 | 2 | 3.938 | 60/4:03.287 |
| 19 | 2 | 3.883 | 60/4:02.744 |
| 20 | 2 | 3.942 | 60/4:02.433 |
| 21 | 2 | 3.947 | 60/4:02.166 |
| 22 | 2 | 3.951 | 60/4:01.934 |
| 23 | 2 | 3.897 | 60/4:01.581 |
| 24 | 2 | 3.909 | 60/4:01.287 |
| 25 | 2 | 3.924 | 60/4:01.054 |
| 26 | 2 | 3.900 | 60/4:00.782 |
| 27 | 2 | 3.994 | 60/4:00.740 |
| 28 | 2 | 4.102 | 60/4:00.932 |
| 29 | 2 | 3.890 | 60/4:00.672 |
| 30 | 2 | 3.945 | 60/4:00.540 |
| 31 | 2 | 4.010 | 60/4:00.542 |
| 32 | 2 | 3.923 | 60/4:00.381 |
| 33 | 2 | 3.989 | 60/4:00.349 |
| 34 | 2 | 3.901 | 60/4:00.164 |
| 35 | 2 | 3.905 | 61/4:03.997 |
| 36 | 2 | 4.040 | 60/4:00.063 |
| 37 | 2 | 3.974 | 60/4:00.019 |
| 38 | 2 | 3.904 | 61/4:03.865 |
| 39 | 2 | 4.676 | 60/4:00.911 |
| 40 | 2 | 3.955 | 60/4:00.821 |
| 41 | 2 | 3.907 | 60/4:00.664 |
| 42 | 2 | 3.900 | 60/4:00.506 |
| 43 | 2 | 3.911 | 60/4:00.370 |
| 44 | 2 | 3.933 | 60/4:00.270 |
| 45 | 2 | 3.968 | 60/4:00.221 |
| 46 | 2 | 3.933 | 60/4:00.129 |
| 47 | 2 | 3.894 | 61/4:03.991 |
| 48 | 2 | 4.082 | 60/4:00.094 |
| 49 | 2 | 4.071 | 60/4:00.179 |
| 50 | 2 | 4.025 | 60/4:00.205 |
| 51 | 2 | 3.966 | 60/4:00.161 |
| 52 | 2 | 3.894 | 60/4:00.036 |
| 53 | 2 | 3.924 | 61/4:03.948 |
| 54 | 2 | 4.038 | 61/4:03.992 |
| 55 | 2 | 4.086 | 60/4:00.086 |
| 56 | 2 | 4.087 | 60/4:00.178 |
| 57 | 2 | 3.967 | 60/4:00.140 |
| 58 | 2 | 3.980 | 60/4:00.117 |
| 59 | 2 | 3.933 | 60/4:00.047 |
| 60 | 2 | 3.939 | 61/4:03.985 |
| 61 | 2 | 6.305 | 61/4:06.290 |