Another example with this P-to-H at recovery time 172:Jormungant wrote: ↑January 22nd, 2021, 1:18 pmI was not sure that this periodic [BR176P] was connectable to anything, but it turns out it is possible to use it somehow:Code: Select all
x = 77, y = 61, rule = LifeHistory 3$54.2A$54.2A2$23.2A$14.2A6.B2AB$13.B2AB5.3B$13.3B7.B$14.B.2B3.5B14. 2A$8.B.2BC10BA4B13.A26.2A$6.7BC.7BABA4B12.A.A24.A$5.8B2C7BABA4B13.2A 22.A.A$5.7B2C9BA4B38.2A$6.6BC13B$8.16B$11.13B$11.12B27.3D14.A.2A$11. 13B28.D14.2A.A$11.12B27.3D$12.10B$14.8B34.D$17.5B34.D.D$17.6B33.3D$ 16.7B34.D$17.5B$17.5B12.2A14.2A$18.DB2D13.A14.A$18.3D11.3A16.A$19.D 12.A17.2A7$24.2A$24.2A$10.2A$10.2A45.3D$59.D$58.3D2$13.2A8.2A$14.A8.A .A$11.3A11.A$11.A13.2A$20.A$19.BAB$17.BA.2A$17.2A4B$18.B.BA$20.2A$21. 2A$20.3A$21.B!
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x = 54, y = 54, rule = LifeHistory
13.2A$4.2A7.2A22.A$4.2A30.A.A$36.A.A$34.3A.2A$2.A10.A19.A$3.A8.A.A19.
3A.2A$3.2A7.A.A21.A.2A$2.2A9.A$2.A12$24.2A26.2A$25.A26.2A$22.3A$22.A
4$41.2A$41.2A$33.2A$14.2A18.A$14.2A18.A.A$2A33.2A$2A4$3.2A8.2A$4.A8.A
.A26.3A$.3A11.A26.A$.A13.2A24.2A3$8.3A$9.A2$8.3A$7.A3.A$6.A5.A$6.A.A.
A.A$5.2A.A.A.2A$4.A2.2A.2A2.A$4.2A7.2A!
The p360 gun in DRH-oscillators.rle uses a p8 R-to-2H implicitly:
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x = 42, y = 26, rule = LifeHistory
2.2A$2.A$3A9$7.A$7.2A32.A$6.2A31.3A$22.2A15.A$22.2A15.A6$9.2A8.2A$8.
3A8.A$7.A.A2.A2.2A3.A$7.2A2.2A2.2A2.2A$11.2A!
EDIT: the last pattern in this post works! The recovery time is exactly 256 ticks, and the upward Herschel must enter a conduit that is 1)not using a transparent block reaction (i.e. not classically dependent) and 2)capable of cleaning the block without the usual block-eating eater. Here I connected a Fx169.
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x = 87, y = 83, rule = LifeHistory
35.B$34.3D$34.BDB$33.2B3D$33.5B$33.6B$33.6B$33.5B$32.6B$33.6B$32.7B$
32.6B$32.6B$32.6B$31.8B$32.8B$31.9B$31.9B$31.10B$31.5B2A3B$31.5B2A4B
3.2A$31.11B3.A$31.4BD7BA.A$33.B3D4B2.2A$33.D2B2D2B$B28.2A2.5B$2B26.A.
A7B$3B25.A3.6B$4B23.2A4.5B9.2A$.4B28.6B8.A$2.4B24.B.8B4.BA.A$3.4B22.
2A9B.2B.B2A$4.4B21.2AB.12B$5.4B21.B2.12B4.2A$6.4B23.12B5.A$7.4B12.2A
6.14B2.3A$8.4B12.A5.17BA$9.4B11.A.AB3.15B$10.4B11.2AB.16B$11.4B12.18B
$12.4B11.17B.B.2A3.2A$13.4B10.B2A17BA.A.A.A$B13.4B10.2A16B.B.A.A$2B
13.4B10.19B2A.2A$3B13.4B9.3B.14B.B$4B13.4B16.10B$.4B13.4B16.8B$2.4B
13.4B15.7B$3.4B13.4B13.11B$4.4B13.4B12.12B$5.4B13.4B11.12B$6.4B13.4B
10.B2D9B8.2A$7.4B13.4B8.B.2D.4B3DB2.2A5.A$8.4B13.4B6.3B4.4BD2B2.A.A.
3A$9.4B13.4B5.3B4.2B3D2B4.A.A$10.4B7.2A4.4B3.5B4.6B3.B2AB$11.4B5.B2AB
4.4B.7B3.7B.4B19.A$12.4B5.3B5.25B20.3A$13.4B3.B.B6.27B21.A$14.4B.6B4.
28B19.2A$15.10B2.30B$7.2A7.43B5.7B.B$8.A8.42B5.13B.B$8.A.AB6.33BD10BD
21B$9.2AB.3B2.33B2D10BD21BD$11.21B3D15B2D11B2D18B3DB$11.23BD27B2D2B2A
15BDBD$12.20B3D27BD3B2A15BD$11.62B3.2B2.2B$9.45B.B3.B2.10B$7.19B3.25B
9.6B$7.2BA15B5.10B.11B12.3B$6.3BABA4B.7B7.8B.12B12.B$7.2B3A4B2.6B7.7B
2.10B2.3B8.2A$6.5BA4B3.6B6.2A7.9B3.3B2A2.B3.A$5.10B6.4B7.A8.7B3.2ABA
2BAB2A3.A$4.4B12.B2A2B4.3A10.6B3.2A2BA4BA2.2A$4.3B14.2A.B2A2.A13.B2.B
5.B2.BA3B$2.4B18.BA.A.A27.ABA$2.2A23.A.2A$3.A23.A$3A23.2A$A!
EDIT3: minor rewording and adding a quote that explains the necessity of this thread.Sphenocorona wrote: ↑December 18th, 2014, 2:00 amThis p15 R -> LWSS unfortunately doesn't work with ny of the -> R conduits I am aware of....
It's also unfortunate that it doesn't work with any of the p2^n oscillators I tried to use, but that's not as great of an issue.Code: Select all
x = 25, y = 15, rule = B3/S23 4bobo2bobo$2obo2bo2bo2bob2o$4bobo2bobo4$4bo6bo11b2o$2bo2bo4bo2bo9b2o$ 2bo2bo4bo2bo$2bo2bo4bo2bo$4bo6bo2$19bo$18b3o$18bo!
dvgrn wrote: ↑February 25th, 2014, 2:35 pm...
If you'd like a more specific suggestion, how about period 8? That's a corner of Life-logic-circuitry-space that I've always thought should get more attention; hardly any p8 circuitry has ever been built, and none since the Snark came along. See, the Snark is a color-preserving glider reflector, and the standard p8 reflector is a color-changing glider reflector -- it's a lot easier to have both types of reflector available when you're trying to get a glider to a particular spacetime location.
Period 8 is maximally Hashlife-compatible. There are lots of p2 and p4 and p8 oscillators that can be used in phase adjusters and suchlike. The p8 glider-to-Herschel converter is a reasonable size, which means you can split signals very easily... easier than with a full-sized Silver reflector
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