Braydon Buster
Current Personal Records
Event | NR | CR | WR | Single | Average | WR | CR | NR | Gold | Silver | Bronze | Solves/Attempts |
---|---|---|---|---|---|---|---|---|---|---|---|---|
3x3x3 Cube | 7441 | 9903 | 38859 | 12.96 | 15.27 | 36192 | 9188 | 6912 | 20/20 | |||
2x2x2 Cube | 12742 | 16725 | 59069 | 4.95 | 7.23 | 61287 | 17436 | 13304 | 5/5 |
Sum of Ranks
Sum of NR | NR | Sum of CR | CR | Sum of WR | WR | |
---|---|---|---|---|---|---|
Single | 124017 | 15073 | 161305 | 19607 | 556665 | 69121 |
Average | 99263 | 13862 | 129320 | 18050 | 449756 | 63449 |
3x3x3 Cube | |||||
Competition | Round | Place | Best | Average | Detail |
---|---|---|---|---|---|
Atomic Fools 2017 | Second round | 16 | 12.96 | 15.27 | 16.62 18.97 14.17 15.01 12.96 |
First round | 20 | 13.96 | 16.71 | 18.86 17.06 14.22 19.63 13.96 | |
Rexburg 2016 | Second round | 11 | 18.92 | 21.10 | 21.08 23.16 21.00 18.92 21.22 |
First round | 14 | 18.31 | 24.99 | 22.78 23.39 32.10 18.31 28.80 | |
2x2x2 Cube | |||||
Competition | Round | Place | Best | Average | Detail |
Rexburg 2016 | First round | 11 | 4.95 | 7.23 | 7.44 4.95 8.89 8.03 6.23 |
Atomic Fools 2017 | |||||
Event | Round | Place | Best | Average | Detail |
---|---|---|---|---|---|
3x3x3 Cube | Second round | 16 | 12.96 | 15.27 | 16.62 18.97 14.17 15.01 12.96 |
First round | 20 | 13.96 | 16.71 | 18.86 17.06 14.22 19.63 13.96 | |
Rexburg 2016 | |||||
Event | Round | Place | Best | Average | Detail |
3x3x3 Cube | Second round | 11 | 18.92 | 21.10 | 21.08 23.16 21.00 18.92 21.22 |
First round | 14 | 18.31 | 24.99 | 22.78 23.39 32.10 18.31 28.80 | |
2x2x2 Cube | First round | 11 | 4.95 | 7.23 | 7.44 4.95 8.89 8.03 6.23 |
No. | Date | Name | Region | City |
---|---|---|---|---|
2 | 2017-04-01 | Atomic Fools 2017 | United States | Richland, Washington |
1 | 2016-11-12 | Rexburg 2016 | United States | Rexburg, Idaho |
Closest Cubers
Person | Competitions |
---|---|
Dartagnan Mullins | 2 |
Kit Clement | 2 |
Lauren Klemz | 2 |
Seen Cubers
Times | Competitors |
---|---|
1 | 107 |
2 | 3 |
All | 110 |