| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 2 | 3.886 | 62/4:00.932 |
| 2 | 1 | 3.917 | 62/4:01.893 |
| 3 | 1 | 3.921 | 62/4:02.296 |
| 4 | 1 | 3.815 | 62/4:00.855 |
| 5 | 1 | 3.917 | 62/4:01.254 |
| 6 | 2 | 3.905 | 62/4:01.397 |
| 7 | 2 | 4.013 | 62/4:02.455 |
| 8 | 2 | 3.908 | 62/4:02.436 |
| 9 | 2 | 4.044 | 62/4:03.357 |
| 10 | 2 | 4.389 | 61/4:02.262 |
| 11 | 2 | 3.946 | 61/4:02.120 |
| 12 | 2 | 3.919 | 61/4:01.865 |
| 13 | 2 | 4.001 | 61/4:02.034 |
| 14 | 2 | 4.010 | 61/4:02.218 |
| 15 | 2 | 4.022 | 61/4:02.426 |
| 16 | 2 | 3.862 | 61/4:01.998 |
| 17 | 2 | 3.971 | 61/4:02.012 |
| 18 | 2 | 4.005 | 61/4:02.139 |
| 19 | 2 | 3.936 | 61/4:02.032 |
| 20 | 2 | 3.920 | 61/4:01.886 |
| 21 | 1 | 3.884 | 61/4:01.650 |
| 22 | 1 | 4.033 | 61/4:01.848 |
| 23 | 1 | 4.034 | 61/4:02.032 |
| 24 | 1 | 4.001 | 61/4:02.117 |
| 25 | 1 | 3.877 | 61/4:01.892 |
| 26 | 1 | 3.992 | 61/4:01.954 |
| 27 | 1 | 3.967 | 61/4:01.955 |
| 28 | 1 | 3.986 | 61/4:01.998 |
| 29 | 1 | 3.957 | 61/4:01.976 |
| 30 | 1 | 4.108 | 61/4:02.264 |
| 31 | 1 | 3.951 | 61/4:02.223 |
| 32 | 1 | 3.939 | 61/4:02.162 |
| 33 | 1 | 4.044 | 61/4:02.299 |
| 34 | 1 | 3.901 | 61/4:02.172 |
| 35 | 1 | 3.976 | 61/4:02.182 |
| 36 | 1 | 3.949 | 61/4:02.146 |
| 37 | 1 | 4.001 | 61/4:02.198 |
| 38 | 1 | 4.069 | 61/4:02.356 |
| 39 | 1 | 3.991 | 61/4:02.384 |
| 40 | 1 | 4.130 | 61/4:02.623 |
| 41 | 1 | 4.105 | 61/4:02.813 |
| 42 | 1 | 4.074 | 61/4:02.948 |
| 43 | 1 | 4.008 | 61/4:02.984 |
| 44 | 1 | 3.963 | 61/4:02.956 |
| 45 | 1 | 4.031 | 61/4:03.021 |
| 46 | 1 | 4.044 | 61/4:03.101 |
| 47 | 1 | 3.885 | 61/4:02.971 |
| 48 | 1 | 4.004 | 61/4:02.997 |
| 49 | 1 | 4.076 | 61/4:03.112 |
| 50 | 1 | 3.923 | 61/4:03.036 |
| 51 | 1 | 3.967 | 61/4:03.016 |
| 52 | 1 | 4.046 | 61/4:03.089 |
| 53 | 1 | 4.025 | 61/4:03.134 |
| 54 | 1 | 4.107 | 61/4:03.271 |
| 55 | 1 | 3.896 | 61/4:03.169 |
| 56 | 1 | 3.975 | 61/4:03.157 |
| 57 | 1 | 3.913 | 61/4:03.079 |
| 58 | 1 | 4.125 | 61/4:03.226 |
| 59 | 1 | 4.065 | 61/4:03.306 |
| 60 | 1 | 3.967 | 61/4:03.284 |
| 61 | 1 | 4.196 | 61/4:03.492 |