Thread for NonCA Academic Questions
 Saka
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Thread for NonCA Academic Questions
Have you ever had a big, huge, or deep nonCA question but was/is/are to lazy to post it on some other site? This is the place to post them to get answered!
My question:
Is it possible to grow animal cells inside plants? Like plants with nerve cells or muscle cells?
My question:
Is it possible to grow animal cells inside plants? Like plants with nerve cells or muscle cells?
Code: Select all
x = 17, y = 10, rule = B3/S23
b2ob2obo5b2o$11b4obo$2bob3o2bo2b3o$bo3b2o4b2o$o2bo2bob2o3b4o$bob2obo5b
o2b2o$2b2o4bobo2b3o$bo3b5ob2obobo$2bo5bob2o$4bob2o2bobobo!
Re: Thread for NonCA Academic Questions
Q:How would the following model evolve?And can you reduce it?
I made a model that simulates evolution before.
It has a tape. Programs and data are saved on it. There are also many tape readers on it. But unlike Turing machines,the readers execute the programs on the tape(Instead of running the rule saved in the reader),and they can read data or go to lines randomly.
Here are the commands. Each command is made of three 16bit numbers. The first one is the command ID. The second and the third are the parameters. They can be values or pointers.
0 x y:Halt whatever x and y are.
1 x y:*x=y
2 x y:*x=*y
3 x y:*x+=y
4 x y:*x+=*y
5 x y:*x=y
6 x y:*x=*y
7 x y:*x*=y
8 x y:*x*=*y
9 x y:*x/=y
10 x y:*x/=*y
11 x y:if(x!=0) go to the y th line (aka the 3*y th, 3*y+1 th,3*y+2 th number)
12 x y: make a new reader on the x th line whatever y is.
I made a model that simulates evolution before.
It has a tape. Programs and data are saved on it. There are also many tape readers on it. But unlike Turing machines,the readers execute the programs on the tape(Instead of running the rule saved in the reader),and they can read data or go to lines randomly.
Here are the commands. Each command is made of three 16bit numbers. The first one is the command ID. The second and the third are the parameters. They can be values or pointers.
0 x y:Halt whatever x and y are.
1 x y:*x=y
2 x y:*x=*y
3 x y:*x+=y
4 x y:*x+=*y
5 x y:*x=y
6 x y:*x=*y
7 x y:*x*=y
8 x y:*x*=*y
9 x y:*x/=y
10 x y:*x/=*y
11 x y:if(x!=0) go to the y th line (aka the 3*y th, 3*y+1 th,3*y+2 th number)
12 x y: make a new reader on the x th line whatever y is.
Code: Select all
x = 15, y = 36, rule = B38/S23
bo$2bo$3o14$13bo$12bo$12b3o2$11bo$12bo$10b3o4$12b3o$12bo$13bo2$10bo$8b
obo$9b2o$6b2o$5bobo$7bo!
Re: Thread for NonCA Academic Questions
Wow,a suitable place for the question in my signature:Is there any relationship between the R/S configuration of a chiral carbon atom and the right hand rule?
Skimmed to: Soup search results Pg59
To be done: butter synthesis
Why do others have so much time posting around?
GUYTU6J
To be done: butter synthesis
Why do others have so much time posting around?
GUYTU6J
Re: Thread for NonCA Academic Questions
Does the 24cell function as a caltrop?
Bored of using the Moore neighbourhood for everything? Introducing the Range2 von Neumann isotropic nontotalistic rulespace!
Re: Thread for NonCA Academic Questions
There is quite an issue on the sequence of executing.72c20e wrote:the readers execute the programs on the tape
Suppose that reader 1 and reader 2 have the following commands:
reader 1: *x=*y
reader 2: *y=*x
Different sequences of executing gives different results.
Still drifting.
 gameoflifeboy
 Posts: 474
 Joined: January 15th, 2015, 2:08 am
Re: Thread for NonCA Academic Questions
No, cells are opposite cells and vertices are opposite vertices.muzik wrote:Does the 24cell function as a caltrop?
Re: Thread for NonCA Academic Questions
...then how can it be selfdual?
Bored of using the Moore neighbourhood for everything? Introducing the Range2 von Neumann isotropic nontotalistic rulespace!
 gameoflifeboy
 Posts: 474
 Joined: January 15th, 2015, 2:08 am
Re: Thread for NonCA Academic Questions
Well, how can the square be selfdual if vertices are opposite other vertices?muzik wrote:...then how can it be selfdual?
I've touched on this topic before. An npolytope is selfdual if there exists a transformation composed of rotations and reflections that, applied to the polytope, exchanges d and (n  d  1)dimensional elements. As a polytope and its dual must have the same axes of symmetry, the axes of symmetry must remain invariant under this transformation. However, as a convex polytope cannot itself remain invariant under such a transformation, there must be more than one way to mark it with axes of symmetry. Thus, given fixed axes of symmetry, there are two ways to orient the polytope such that it aligns with them. Now a new symmetry is defined, with all the transformations that kept the polytope invariant ("even" transformations) plus all those that transform it to dual orientation ("odd" transformations).
Now choose a point P on an nD hypersphere. From this point, we can define a set of points, all on the hypersphere, which are equivalent to P under some transformation. This set can be divided into two subsets containing the results of "even" transformations and "odd" transformations. An "odd" transformation on any member of one set produces a member of the opposite set. Transforming the selfdual shape into its "dual" orientation can be done by any "odd" transformation.
For example, doubling tetrahedral symmetry this way produces octahedral symmetry. In this picture, each black triangle can represent an "odd" transformation, and each blue triangle an "even" one: https://upload.wikimedia.org/wikipedia/ ... omains.png
In odd dimensions, it seems that turning the shape upside down is always an odd transformation (is there a known proof of this?), and thus turning an odddimensional selfdual convex polytope (like the tetrahedron) upside down results in its dual orientation. However, in even dimensions this is not always the case, and in the case of the icositetrachoron (24cell), turning it by any multiple of 90 degrees is always an "even" transformation that maps the polytope to itself, not to its dual.
An example of an "odd" transformation turning the icositetrachoron into its dual can be realized by rotating 45 degrees in a rotation based on the Hopf fibration of the cube.
TL;DR: Selfdual convex shapes must have selfdual symmetries, which can be doubled by adding transformations that turn the base orientation into the dual orientation. It appears, but I'm not certain, that in odd dimensions, turning a shape upside down is always a transformation of the second type and thus selfdual convex polyhedra are their duals upsidedown.
By the way, if anyone knows more about this than I do, I would like to be informed if I have made any flaws in my reasoning.

 Posts: 796
 Joined: May 30th, 2016, 8:47 pm
 Location: Milky Way Galaxy: Planet Earth
Re: Thread for NonCA Academic Questions
Is there any way to stabilize superheavy elements through metastability? I'm thinking of something like tantalum180m.
Code: Select all
x = 81, y = 96, rule = LifeHistory
58.2A$58.2A3$59.2A17.2A$59.2A17.2A3$79.2A$79.2A2$57.A$56.A$56.3A4$27.
A$27.A.A$27.2A21$3.2A$3.2A2.2A$7.2A18$7.2A$7.2A2.2A$11.2A11$2A$2A2.2A
$4.2A18$4.2A$4.2A2.2A$8.2A!
 toroidalet
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Re: Thread for NonCA Academic Questions
There have been reports of Ub292 (unbibinum, element 122) with a halflife of about 7*10^8 years in a thorium deposit. Apparently evidence in the data points to it having an excited state but these results haven't been reproduced.Gamedziner wrote:Is there any way to stabilize superheavy elements through metastability? I'm thinking of something like tantalum180m.
Also, is this formula for the probability an X with halflife y (in seconds) will decay in k (seconds) correct?
Pd(k)=11/(2^(k/y))
(Pd stands for Probability of Decay, not pentadecathlon)
Sketch of proof:
The probability that an X will decay in y seconds is 1/2, so
Pd(y)=1/2
Ps(y)=11/2=1/2.
Pd(y)=1Ps(y)=11/2=1/2.
Pd(2y)=1Ps(y)^2=11/4=3/4.
Pd(3y)=1Ps(y)^3=7/8
... and so on.
Extrapolation:
Pd(cy)=1Ps(y)^c=11/(2^c)
Pd(y(1/y)=11/(2^(1/y))
Pd(1)=1(1/(2^(1/y)))
Ps(1)=1(11/(2^(1/y)))=1/(2^(1/y)).
Pd(k)=1Ps(1)^k=1(1/(2^(1/y)))^k=1/(2^(k/y)).
Pd(k)=11/(2^(k/y))
EDIT: typo
Last edited by toroidalet on July 26th, 2017, 9:19 pm, edited 1 time in total.
"Build a man a fire and he'll be warm for a day. Set a man on fire and he'll be warm for the rest of his life."
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 gameoflifemaniac
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Re: Thread for NonCA Academic Questions
Is it possible to emulate a normal computer in a quantum computer?
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 Saka
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Re: Thread for NonCA Academic Questions
You guys know about how a giant centrifuge can make artificial gravity?
Isn't that essentially a giant fidget spinnet that spins really fast (that has rooms in it of course.)?
Isn't that essentially a giant fidget spinnet that spins really fast (that has rooms in it of course.)?
Code: Select all
x = 17, y = 10, rule = B3/S23
b2ob2obo5b2o$11b4obo$2bob3o2bo2b3o$bo3b2o4b2o$o2bo2bob2o3b4o$bob2obo5b
o2b2o$2b2o4bobo2b3o$bo3b5ob2obobo$2bo5bob2o$4bob2o2bobobo!
Re: Thread for NonCA Academic Questions
Yes, there's a standard trick for this. Given a function f : {0, 1}^n > {0, 1}^m expressed as a circuit C of classical logic gates, you can replace the gates in the circuit with reversible equivalents to yield a reversible circuit C' (which may have lots of ancillary '0' inputs and some arbitrary messy outputs):gameoflifemaniac wrote:Is it possible to emulate a normal computer in a quantum computer?
[n input bits][k ancillary '0' bits] > [m output bits][n+km unwanted garbage bits]
Suppose we have another m ancillary '0' bits at this stage. Then we can CNOT the output bits with these ancillary bits to produce another copy of the output, like so:
[n input bits][k ancillary '0' bits][m extra '0' bits] > [m output bits][n+km unwanted garbage bits][m output bits]
Now apply C' in reverse to the first n+k bits to clean up the mess we created:
[n input bits][k ancillary '0' bits][m extra '0' bits] > [n input bits][k ancillary '0' bits][m output bits]
The upshot of this is that the ancillary '0' bits can be reused in a future computation. This combined circuit, ignoring the k ancillary '0' bits, actually computes the reversible function:
f : {0, 1}^(n+m) > {0, 1}^(n+m)
(x, y) > (x, f(x) XOR y)
Now, every reversible classical circuit is a quantum circuit (permutation matrices are unitary matrices), so this can be built out of quantum gates.
What do you do with ill crystallographers? Take them to the monoclinic!
Re: Thread for NonCA Academic Questions
I have a conjecture I'd like to prove. Take a k*k matrix P, where every item in P is >0 and less than or equal to b.
Then imagine a function E(k,b) which returns the amount of matrices that exist with those parameters which are antipalindromic. We'll define antipalindromic as meaning the subarrays that are the rows, the columns, and the diagonals are all nonpalindromes. If you need further clarification and/or discussion, see here.
Now, assuming b is constant, what is the asymptotic behaviour of E(k,b) as k increases? My conjecture states that it tends to 0, and I believe it happens exponentially. Here is my reasoning.
Premise 1: The probability that a length k string is a palindrome goes down exponentially as k increases.
Premise 2: The amount of subarrays in P only increaes linearly as k increases (2k+2).
Conclusion: The exponential part of the equation should overpower the linear one, and so palindromes should become less common in big matrices.
This is a rough line of reasoning, not a mathematical proof. I can't really grasp how I'd mathematically prove this when the subarrays intersect each other; maybe you could prove they're still independently random despite their intersections. Can anyone prove this?
Then imagine a function E(k,b) which returns the amount of matrices that exist with those parameters which are antipalindromic. We'll define antipalindromic as meaning the subarrays that are the rows, the columns, and the diagonals are all nonpalindromes. If you need further clarification and/or discussion, see here.
Now, assuming b is constant, what is the asymptotic behaviour of E(k,b) as k increases? My conjecture states that it tends to 0, and I believe it happens exponentially. Here is my reasoning.
Premise 1: The probability that a length k string is a palindrome goes down exponentially as k increases.
Premise 2: The amount of subarrays in P only increaes linearly as k increases (2k+2).
Conclusion: The exponential part of the equation should overpower the linear one, and so palindromes should become less common in big matrices.
This is a rough line of reasoning, not a mathematical proof. I can't really grasp how I'd mathematically prove this when the subarrays intersect each other; maybe you could prove they're still independently random despite their intersections. Can anyone prove this?
succ
 gameoflifemaniac
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Re: Thread for NonCA Academic Questions
Adam, you are smart as hell.calcyman wrote:Yes, there's a standard trick for this. Given a function f : {0, 1}^n > {0, 1}^m expressed as a circuit C of classical logic gates, you can replace the gates in the circuit with reversible equivalents to yield a reversible circuit C' (which may have lots of ancillary '0' inputs and some arbitrary messy outputs):gameoflifemaniac wrote:Is it possible to emulate a normal computer in a quantum computer?
[n input bits][k ancillary '0' bits] > [m output bits][n+km unwanted garbage bits]
Suppose we have another m ancillary '0' bits at this stage. Then we can CNOT the output bits with these ancillary bits to produce another copy of the output, like so:
[n input bits][k ancillary '0' bits][m extra '0' bits] > [m output bits][n+km unwanted garbage bits][m output bits]
Now apply C' in reverse to the first n+k bits to clean up the mess we created:
[n input bits][k ancillary '0' bits][m extra '0' bits] > [n input bits][k ancillary '0' bits][m output bits]
The upshot of this is that the ancillary '0' bits can be reused in a future computation. This combined circuit, ignoring the k ancillary '0' bits, actually computes the reversible function:
f : {0, 1}^(n+m) > {0, 1}^(n+m)
(x, y) > (x, f(x) XOR y)
Now, every reversible classical circuit is a quantum circuit (permutation matrices are unitary matrices), so this can be built out of quantum gates.
This is a signature
Re: Thread for NonCA Academic Questions
Wait, I didn't invent the technique; it's wellknown: https://en.wikipedia.org/wiki/Uncomputationgameoflifemaniac wrote:Adam, you are smart as hell.calcyman wrote:Yes, there's a standard trick for this. [...]gameoflifemaniac wrote:Is it possible to emulate a normal computer in a quantum computer?
Now, every reversible classical circuit is a quantum circuit (permutation matrices are unitary matrices), so this can be built out of quantum gates.
According to Scott Aaronson, it was 'proposed by Bennett in the 1980s' (which I assume refers to Charles Henry Bennett).
The best resource for learning about quantum computation is 'Quantum Computation and Quantum Information' by Nielsen and Chuang. I once had an interesting conversation in the Faculty about this, wherein I described it as 'the Kamasutra of quantum computing', only to be informed that the word 'Bible' is more commonly used as a metaphor for its authoritative status.
What do you do with ill crystallographers? Take them to the monoclinic!
 gameoflifemaniac
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 Saka
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Re: Thread for NonCA Academic Questions
not sure what you mean. But yes, there are tons of programs that find primes and you can easily multiply and add primes on a computer.gameoflifemaniac wrote:Are primes computable?
Is it possible to make a program that evolves itself? For example, it starts out as 1 file. The file is programmed to duplicate itself, but with some random "mutations" every duplication, like adding some specific code to a function wich gets called after a certain condition (Also mutable (e.g. function is called every 2 duplications)) and the worst files, determined by another program, the "fitness tester". Will this file be able to evolve so much with the right fitness tester and become an AI?
Code: Select all
x = 17, y = 10, rule = B3/S23
b2ob2obo5b2o$11b4obo$2bob3o2bo2b3o$bo3b2o4b2o$o2bo2bob2o3b4o$bob2obo5b
o2b2o$2b2o4bobo2b3o$bo3b5ob2obobo$2bo5bob2o$4bob2o2bobobo!

 Posts: 796
 Joined: May 30th, 2016, 8:47 pm
 Location: Milky Way Galaxy: Planet Earth
Re: Thread for NonCA Academic Questions
If two atomsharp needles were pushed together, would the extremely focused pressure cause nuclear fusion?
Code: Select all
x = 81, y = 96, rule = LifeHistory
58.2A$58.2A3$59.2A17.2A$59.2A17.2A3$79.2A$79.2A2$57.A$56.A$56.3A4$27.
A$27.A.A$27.2A21$3.2A$3.2A2.2A$7.2A18$7.2A$7.2A2.2A$11.2A11$2A$2A2.2A
$4.2A18$4.2A$4.2A2.2A$8.2A!
Re: Thread for NonCA Academic Questions
Disclaimer: I haven't looked at this topic recently so my observations may be out of date.Saka wrote:Is it possible to make a program that evolves itself? For example, it starts out as 1 file. The file is programmed to duplicate itself, but with some random "mutations" every duplication, like adding some specific code to a function wich gets called after a certain condition (Also mutable (e.g. function is called every 2 duplications)) and the worst files, determined by another program, the "fitness tester". Will this file be able to evolve so much with the right fitness tester and become an AI?
What you describe has been explored in a branch of artificial life research. All of the successful research efforts that I am aware of involve running programs in a simulated computing environment similar to a virtual machine. In this case though the architecture of the virtual machine and the instruction set it supports are specifically designed to ensure that "mutations" of a program result in another functional program. Two examples of this line of research are Tierra and Avida. These systems show evolutionary behaviour of the digital organisms which exist within them and all kinds of properties were observed. The result of evolution in these systems often favours smaller program size, because less computation time equals faster replication. In some cases programs analagous to viruses were observed, where the program no longer contained the functionality to replicate itself, but used the replication code from another program in the environment instead. You can find links to other examples of this type of artificial life here: https://en.wikipedia.org/wiki/Artificia ... simulators  look for entries classed as "Executable DNA".
Instruction sets for real computers are not designed to ensure that all or even most valid assembly code will actually result in an executable program. As a result, applying this kind of evolution through simple mutation of functional programs leads to almost all "children" being nonfunctional programs. This makes it very difficult to observe evolution which leads to any interesting behaviour in the resulting programs. Similarly with a system that tries to evolve programs written in a higher level language like C, nearly all possible "child programs" which are the result of mutations of a functioning C program will fail because the program is very unlikely to even be able to compile.
Maybe someone has tried combining a system like this with some kind of automatic program generator which is much more likely to produce functional programs  something like this RNN trained on the Linux code base (see the section titled "Linux Source Code"). If so, I'd be interested in seeing the results.
The latest version of the 5S Project contains over 226,000 spaceships. There is also a GitHub mirror of the collection. Tabulated pages up to period 160 (out of date) are available on the LifeWiki.
 gameoflifemaniac
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 gameoflifeboy
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Re: Thread for NonCA Academic Questions
Here is an article about someone's attempts to extend the second argument of tetration to the real numbers. I haven't really tried to understand it but I will probably do so when I am less busy.
A much simpler solution is to just use linear approximation, but this lacks the beauty of the original because the function is not smooth (i.e. cannot be differentiated everywhere an infinite number of times).
A much simpler solution is to just use linear approximation, but this lacks the beauty of the original because the function is not smooth (i.e. cannot be differentiated everywhere an infinite number of times).
 Saka
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Re: Thread for NonCA Academic Questions
Would it be possible to make an image of say, 1 city, so detailed, you can clearly see individual people?
Code: Select all
x = 17, y = 10, rule = B3/S23
b2ob2obo5b2o$11b4obo$2bob3o2bo2b3o$bo3b2o4b2o$o2bo2bob2o3b4o$bob2obo5b
o2b2o$2b2o4bobo2b3o$bo3b5ob2obobo$2bo5bob2o$4bob2o2bobobo!
 gameoflifemaniac
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Re: Thread for NonCA Academic Questions
What's the bounding box of the Mandelbrot set?
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Re: Thread for NonCA Academic Questions
I'm currently trying to figure out how a universe in which Newton's second law is F=mj would behave. So far, I've determined that particles travel in parabolas (possibly degenerate) when not acted upon by any force, objects falling under a constant force with zero horizontal acceleration descend cubic curves, and that colliding objects attracted by a force rebound either superelastically or inelastic with a probability of 1 depending on how the force varies with distance — no kind of energy is in any way conserved, at least if my intuition is correct. I'm wondering what kind of work has been done on this problem.
Also, is there anything known about a twodimensional universe in which Newton's second law is F=imv? Clearly, systems containing attractive and/or repulsive forces where the law is just F=mv either expand without limit, quickly lead to singularities, or both, but it seems like stable orbits would exist no matter how force varies with distance in the F=imv case. There might be a conserved quantity associated, as well, but I'm not sure exactly what it is.
Also, is there anything known about a twodimensional universe in which Newton's second law is F=imv? Clearly, systems containing attractive and/or repulsive forces where the law is just F=mv either expand without limit, quickly lead to singularities, or both, but it seems like stable orbits would exist no matter how force varies with distance in the F=imv case. There might be a conserved quantity associated, as well, but I'm not sure exactly what it is.
x₁=ηx
V ⃰_η=c²√(Λη)
K=(Λu²)/2
Pₐ=1−1/(∫^∞_t₀(p(t)ˡ⁽ᵗ⁾)dt)
$$x_1=\eta x$$
$$V^*_\eta=c^2\sqrt{\Lambda\eta}$$
$$K=\frac{\Lambda u^2}2$$
$$P_a=1\frac1{\int^\infty_{t_0}p(t)^{l(t)}dt}$$
http://conwaylife.com/wiki/A_for_all
Aidan F. Pierce
V ⃰_η=c²√(Λη)
K=(Λu²)/2
Pₐ=1−1/(∫^∞_t₀(p(t)ˡ⁽ᵗ⁾)dt)
$$x_1=\eta x$$
$$V^*_\eta=c^2\sqrt{\Lambda\eta}$$
$$K=\frac{\Lambda u^2}2$$
$$P_a=1\frac1{\int^\infty_{t_0}p(t)^{l(t)}dt}$$
http://conwaylife.com/wiki/A_for_all
Aidan F. Pierce