| Итого | За последние 12 месяцев | Apr | Mar | Feb |
| Всего | 12мес | Apr | Mar | Feb | Jan | Dec | Nov | Oct | Sep | Aug | Jul | Jun | May | 20 | 19 | 18 | 17 | 16 | 15 | 14 | 13 | 12 | 11 | 10 | 09 | 08 | 07 | 06 | 05 | 04 | 03 | 02 | 01 | 31 | 30 | 29 | 28 | 27 | 26 | 25 | 24 | 23 | 22 | 21 | 20 | 19 | 18 | 17 | 16 | 15 | 14 | 13 | 12 | 11 | 10 | 09 | 08 | 07 | 06 | 05 | 04 | 03 | 02 | 01 | 28 | 27 | 26 | 25 | 24 | 23 | 22 | 21 | 20 | 19 | 18 |
|
По разделу |
7048 | 210 |
22 |
26 |
25 |
22 |
14 |
18 |
10 |
14 |
4 |
14 |
18 |
23 |
1 |
2 |
1 |
1 |
0 |
2 |
2 |
1 |
1 |
1 |
0 |
1 |
0 |
1 |
1 |
2 |
2 |
2 |
1 |
0 |
2 |
0 |
0 |
1 |
0 |
2 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
2 |
1 |
0 |
2 |
1 |
0 |
0 |
1 |
1 |
0 |
2 |
1 |
1 |
3 |
2 |
2 |
1 |
1 |
1 |
0 |
1 |
0 |
2 |
0 |
2 |
1 |
0 |
2 |
|
Парадокс д'Аламбера для вязкой жидкости |
1935 | 96 |
11 |
13 |
13 |
9 |
8 |
9 |
2 |
6 |
3 |
6 |
6 |
10 |
1 |
0 |
0 |
1 |
0 |
2 |
2 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
1 |
0 |
1 |
1 |
1 |
0 |
2 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
2 |
0 |
0 |
0 |
0 |
1 |
0 |
1 |
1 |
0 |
1 |
0 |
2 |
1 |
1 |
1 |
0 |
0 |
0 |
2 |
0 |
0 |
0 |
0 |
1 |
|
Новая механика |
2131 | 92 |
9 |
9 |
16 |
11 |
5 |
6 |
5 |
6 |
1 |
7 |
8 |
9 |
0 |
0 |
0 |
1 |
0 |
1 |
1 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
2 |
1 |
1 |
1 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
1 |
1 |
0 |
2 |
1 |
1 |
1 |
0 |
1 |
0 |
0 |
0 |
1 |
0 |
2 |
1 |
0 |
2 |
|
Новая модель атома водорода |
1807 | 90 |
9 |
12 |
11 |
10 |
6 |
9 |
2 |
5 |
1 |
5 |
9 |
11 |
0 |
1 |
0 |
1 |
0 |
1 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
2 |
2 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
2 |
0 |
0 |
0 |
1 |
0 |
0 |
1 |
0 |
0 |
2 |
0 |
0 |
2 |
2 |
0 |
1 |
0 |
1 |
0 |
1 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
|
Информация о владельце раздела |
1175 | 85 |
12 |
10 |
10 |
11 |
5 |
5 |
6 |
7 |
0 |
5 |
6 |
8 |
0 |
2 |
1 |
1 |
0 |
1 |
1 |
1 |
1 |
0 |
0 |
0 |
0 |
1 |
1 |
0 |
0 |
2 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
2 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
1 |
3 |
1 |
1 |
1 |
1 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
2 |