20 different methods of inverting the Mandelbrot set
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- Опубліковано 26 сер 2024
- Or: how to get from c to 1/c, and back again.
First the cardioid of the main body of the Mandelbrot set is converted to a circle After the inversion the process is reversed so that when a second inversion is applied one gets back to the original image.
In the unlikely event that someone is interested in the formulas used, please ask and I won't show any hesitation in sharing them.
I'd like to take a look at the formula...thanks
Well, there's 20 of them, as the title of the video suggests, on how to get from c to 1/c.
But they all group in 3 families:
1. addition: c -> c-c*t+t/c and t=0..1
2. multiplication: c -> c/(t*(c*c-1)+1) and t=0..1
3. exponentiation: c -> c^t and t=1..-1
The first 2 are pretty elementary to work out. The 3rd makes use of the fact that:
c = a+ib = r*exp(i*phi) where r=sqrt(a*a+b*b) and phi=arctan(b/a)
then c^t = r^t*exp(t*i*phi) = r^t*[cos(t*phi)+i*sin(t*phi)]
Thanks for prompt reply
@@GawdonBennett Say Thanks!
@@00001__ bro?
I HAVE FORMULA
That pop on the 3rd, 5th and 7th one 😳
You kind of want to flip the bulbs over the cardioid, and (or perhaps not) flip the feature on the right side of the set as well.
ج
0:30 inverted Monobar
0:21 spider on the 6th
hi! would you please share formulas for the 3, 15 and 16 ones? counting left to right, top to bottom. thank you!
Well, first there's the transformation from the cardioid of the body of the set to a circle. This is done in c-space (a+ib) as follows:
rho=sqrt(a*a+b*b)-1/4
phi=arctan(b/a)
a-new=rho*(2*cos(phi)-cos(2*phi))/3
b-new=rho*(2*sin(phi)-sin(2*phi))/3
Frame 3, 15 and 16 are based on an inversion through exponentiation, i.e.:
c -> c^t and t=1..-1
Making use of the fact that:
c = a+ib = rho*exp(i*phi) where rho=sqrt(a*a+b*b) and phi=arctan(b/a)
then c^t = rho^t*exp(t*i*phi) = rho^t*[cos(t*phi)+i*sin(t*phi)]
This is frame 3.
Frame 15 and 16 is a variant where rho^t in the equation above is substituted with rho/(t*(rho*rho-1)+1) and t=0..1
Additionally, frame 16 substitutes cos(t*phi) with cos(phi), in other words, the transition is cancelled for Re(c) but kept for Im(c).
I hope this all makes sense to you.
@@Arneauxtje it does! thank you so much for a prompt reply! it's an awesome job!
0:18 19th one *eclipse with glasses 15th without
Holographic Holo-Fractal Stochastic Super-Tension Shape Dynamics!.
0:07 Monobar
I'm interested in the formulas used. Please share them.
Happy to oblige. But could you be a bit more specific though?
Also, in the comments below a lot has been disclosed already. If you would like some additional explanations on some of the procedures, please let me know.
@@Arneauxtje right ( I see them after expandig the comments tree ) Thx
@@Arneauxtje i want formula for 4
@@truongquangduylop33yyuh34
First there's the transformation from the cardioid of the body of the set to a circle. This is done in c-space (a+ib) as follows:
rho=sqrt(a*a+b*b)-1/4
phi=arctan(b/a)
a-new=rho*(2*cos(phi)-cos(2*phi))/3
b-new=rho*(2*sin(phi)-sin(2*phi))/3
Frame 4 is based on an inversion through exponentiation, i.e.:
c -> c^t and t=1..-1
Making use of the fact that:
c = a+ib = rho*exp(i*phi) where rho=sqrt(a*a+b*b) and phi=arctan(b/a)
then c^t = rho^t*exp(t*i*phi) = rho^t*[cos(t*phi)+i*sin(t*phi)]
This is frame 3.
For frame 4 the t in in cos(t*phi) is dropped, i.e.:
c^t = rho^t*[cos(phi)+i*sin(t*phi)]
Hope this helps.
John
Is this not just an inversion of the human body?
or at least the human psyche.
Ok, now what do I do with my newfound confusedness
Wow!!
0:19 is this me or did it lag?
I think it's you
0:05 - 20 monobars?
A 1st what ap? At 2nd I want formulas for 1 and 2.
No app, write my own code, mainly in assembly.
1: c -> c-c*t+t/c and t=0..1
2: c -> c/(t*(c*c-1)+1) and t=0..1
Make 100 Diffrent Ones
Or 36
other method of plane transformations : commons.wikimedia.org/wiki/File:Feigenbaum_stretch_3.png
Very interesting, I'll look into it. Thanks.
0:05 everything is monobar LOL
Monobar formula:
z^2 + (c iabs c+0.25)
@@KingGreenscreenKid420 wrong it's actually
complex p;
complex t;
complex r;
complex d;
complex y;
complex o;
complex pa;
pa = 1;
y = (0.1);
d = c^w;
o = 1;
p = arg(d);
r = cos(2/o*arg(cos(p* o/2)));
d = d * r;
r = rad(d) - 0.25;
p = arg(d);
d = r * (2*exp(1i*p) - exp(2*1i*p)) / 3;
bailout = 10;
t = pa;
z = (z)^po + t * d + (1 - t) * c;
@LatinNegativeElolnoma no shit sherlock i didn't know
Obviously not, it is not a monobar, It is a half lambda or a circle body mandelbrot
@@DoNotExpose5624 No, I thought that 2 years ago
ı am dızzy 😵
0:19 DONOT look at the 2th mandelbrot to the top
Takes one to know one
0:19 DONOT look at the 2th mandelbrot to the top
Uhm actually its
"1st"
"2nd"
"3rd"
"4th"
🤓
hmmm
@@tesscruzat5277stop copying him