Why not: Difference between revisions
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{{Oscillator|name=Why not|pname=whynot|p=2|h=15|v=0.68 | {{Oscillator | ||
|name = Why not | |||
|pname = whynot | |||
|c = 14 | |||
|bx = 7 | |||
|by = 7 | |||
|p = 2 | |||
|h = 15 | |||
|v = 0.68 | |||
|discoverer = David Buckingham | |||
|discoveryear = 1977 | |||
|rulemin = B3/S23 | |||
|rulemax = B3678/S2345678 | |||
|rulespecial = [[Conway's Game of Life|Conway Life]] | |||
|synthesis = 27 | |||
|synthesisRLE = true | |||
|life105 = true | |||
|life106 = true | |||
|plaintext = true | |||
|rle = true | |||
|animated = true | |||
}} | |||
'''Why not''' is a [[period]] [[:Category:Oscillators with period 2|2]] [[oscillator]] that was found by [[:Category:Patterns found by David Buckingham|David Buckingham]] in July [[:Category:Patterns found in 1977|1977]]. It is extremely similar to [[by flops]]. | '''Why not''' is a [[period]] [[:Category:Oscillators with period 2|2]] [[oscillator]] that was found by [[:Category:Patterns found by David Buckingham|David Buckingham]] in July [[:Category:Patterns found in 1977|1977]]. It is extremely similar to [[by flops]]. | ||
Revision as of 15:06, 19 June 2016
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| Pattern type | Oscillator | ||||||||
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| Number of cells | 14 | ||||||||
| Bounding box | 7 × 7 | ||||||||
| Period | 2 (mod: Unknown) | ||||||||
| Heat | 15 | ||||||||
| Volatility | 0.68 | 0.68 | ||||||||
| Kinetic symmetry | Unspecified | ||||||||
| Discovered by | David Buckingham | ||||||||
| Year of discovery | 1977 | ||||||||
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Why not is a period 2 oscillator that was found by David Buckingham in July 1977. It is extremely similar to by flops.
External links
- Why not at the Life Lexicon
Categories:
- Patterns
- Oscillators with 14 cells
- Periodic objects with minimum population 14
- Patterns with 14 cells
- Patterns found by David Buckingham
- Patterns found in 1977
- Patterns that can be constructed with 27 gliders
- Oscillators
- Oscillators with period 2
- Oscillators with heat 15
- Oscillators with volatility 0.68
- Oscillators with strict volatility 0.68
- Patterns with bilateral orthogonal symmetry