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- # FOR THE UNCANNY THIS IS A "PYTHON" PROGRAM.
- # It's more unclear what or how this program does
- # but that's half the fun
- #
- # todo: add 27.818133whatver for ZY+1.44
- # e-mail maplecat@protonmail.com for stuff or whatever questions
- # or something?
- # IMPORTANT INFO ABOUT HOW IT MIGHT WORK
- # ANYWAY:
- #
- # most of the "pentacle" functions except the "pent3" one's
- # was defined first and all these "pentacle" formulas
- # can be used but most practical is those with "constant"
- # output even if a "variable" (n) are used in the equation
- #
- # this above is feed into the yzz() "function" developed last
- # to use perhaps type yzz(128,harmonic(64)) to get ouput on the screen
- # N.B. One should never use the stable() function with anything it
- # will burn at least ..
- #
- # The resulting integers can be fed into the "cathie" formulas
- # which was the original one's maybe used during ww2 in.fact
- # personally I use cathie32(n) or as it would be typed:
- #
- # print(x,yzz(129,harmonic(64)),cathie32(yzz(129,harmonic(64)))
- #
- # I think it's important to have the digits all the same with and
- # without piping through cathie32 but who cares about that?!
- #
- # also for the above print that displays output on the screen from
- # python also even if harmonic(64) usually is equal to 2.9
- # there are always inteferrence which might make subtle CHANGE
- # for the output though the functions are pretty stable you
- # can run a stability check with just typing stable(333) i.e. and
- # others like stable(454) and same with harmonic(n) to see if
- # both give output exact 0.16 and 2.9 not i.e. 2.90000002 but
- # apparently some of these "pentacles" are designed in such a way
- # that they usually are stable hence the names maybe.
- #
- # there are other cathie equations and my own dabbeling is
- # the function enew() whish introduce an array for each output
- # based on cosinus or sinus
- #
- # SO this is a "python" computer program language "script" i.e.
- # it's different from a normal computer executable but then again
- # it can even run on your telephone / android
- #
- # Usually anyway it would have a "front-end" but this does not
- # have a front-end (yet) only these comments and to look at the "code"
- # below:
- # END intro currently.
- # Here is the script / code it's alot to look through but even worse
- # too look through is the output for some!
- #importing seperatly so I know what I use
- from math import cos
- from math import log
- from math import e #trying 2.71453
- #e=2.71453
- #from math import e #trying e again
- from math import pi
- from operator import lshift
- from operator import rshift
- from math import sqrt
- #from math import e
- from math import trunc
- # lets void PI
- pi=3.14625
- # defining Buckinster Fuller's "Synergetics Constants"
- syn=[]
- for x in range(1,13):
- syn.append((9/8)**(x/6))
- # Old way of doing the above this is the integers HE used:
- syn2=[1.019824451,1.040041912,1.060660172,1.081687178,1.103131033,1.125,1.193242683,1.265625] #find formula
- # square it mother fu->>> p.s also 64/27
- lsic=((8/(3*sqrt(3)))**2) #liebs square ice constant (or 8/9*sqrt(3)!
- #or Wadsworth constant 640*(3/10)/81
- light_meter=299792458 # this should be clear it's
- # light in wrong kilmeters per hours
- # probably they no-one figured it was paramount
- # to ~= 3 though this is actually 29..
- phi=((1+sqrt(5))/ 2.0) # NOTICE 5/2 sdtuf. defining ph--
- gamma=(4*log(2)-2*log(3)) # forumla!!! ;)
- print("gamma",gamma)
- print("computer e",e)
- e=(16/9)**(1/gamma) # coputer e gives a fractional error from
- # 1.7777..with it's e-value. this one better.
- print("my e",e)
- #alpha=1.37318 # fine structure constants
- alpha=1/(2**11)*6**7
- print("alpha",alpha)
- lsi=1/(1024/6/6/6/2) #converts 2**n to 6**n ? 216 */ n
- test=(1/(((e**(4*log(2)-2*log(3))))/2**9))
- speed=(1/(((e**gamma))/2**9)) #give 144*2 must make test
- # below are future components of the program
- # based on american "bucky" from his book on
- # Synergetics, it's from Him that we got the
- # idea for the "pentacle"'s to use only
- # primes in designing them,
- # "Synegetics" are actually two books / compendiums
- # interexchangable his major technical work..and
- # contain many of these equations here; gemoteric ..
- # stuff..
- def angles(c,n=180):
- return((c-2*n))
- def fuller_sp(n):
- # number of
- sp=0
- for x in range(1,n+1):
- sp=sp+10*(x**2)
- #print("layer",x,sp)
- sp=sp+(2*n)+1
- return(sp)
- #def fuller_sph(n):
- # sp=0
- # for x in range(1,n+1):
- # sp=sp+fuller_n(x)
- # return(sp)
- # some stuff here used previously following below
- # we tried finding some resonant frequencies
- # because this program obviously has many layers
- # or is so-called multi-functional
- #
- # this below the next is routine to find physical
- # coils etc physical material stuff to build
- # something that works for mankind free stuff
- def test6(c):
- n=c
- return(1/((e**gamma)/n))
- def m_str(I,N=288,l=45,c=0):
- ''' N=vindings, l=spool-length (arc?) I=power(watt)
- currently using fuller_n() for windings..
- !! using 50/1.125/1.125 instead of 10 cm/2.54
- also suggesting 50 as in HZ so use maybe 40 or whatever.
- '''
- if c==0:
- return((I*N)/(l))
- else:
- return((I*N)/(l/2.54))
- def search_h(x=256000,y=25600,z=256000):
- print("Searching for harmonics of Coils")
- ''' Routine to (try) to find if Harmonic Equation 2 can correspond to Coild strength
- '''
- I=25
- N=25
- harmonics=()
- while I<x:
- while N<y:
- coil=m_str(I,N)
- for a in range(1,z):
- #print("Cathie:",cathie2((a*sqrt(2)**2)),"Coil:",coil)
- if trunc(cathie((a*sqrt(2)**2)))==coil:# trunc only cathie2 as it is supposed to give
- # whole integers.
- # --maybe remove formule and just use plain c,
- # since 'coil' doesnt give whole number output
- print('Coil Strength',coil,'Cathie 2:',cathie((a*sqrt(2)**2)))
- N=N+1
- #print(N)
- I=I+1
- N=25
- print(I)
- def search_h2(x=256000,y=25600,z=256000,zz=25600): # errorenous procedure but gives me more hits
- print("Searching for harmonics of Coils")
- ''' Routine to (try) to find if Harmonic Equation 2 can correspond to Coild strength
- '''
- I=25
- N=25
- l=1
- harmonics=()
- while I<x:
- while N<y:
- while l<zz:
- coil=m_str(I,N,l)
- for a in range(1,z):
- #print("Cathie:",cathie2((a*sqrt(2)**2)),"Coil:",coil)
- if trunc(cathie2(z))==coil:# here it should be cathie()
- # not cathie2()
- #
- # remember a*sqrt(2)**2 was c
- print('Coil Strength',coil,'Cathie 2:',cathie2((a*sqrt(2)**2)))
- zz=zz+1
- N=N+1
- zz=1
- #print(N)
- I=I+1
- N=25
- print(I)
- # END of that part of the program.
- #
- psi=147.81557937222715 # derived from 6 see 144-.py
- black=2*(225|144^256) # 99.4% dont worry it doesnt get blacker
- black2=(225|144^256&225) # ? going around like the code also
- # it is a "belt"
- two88=[2,3,4,6,8,9,12,16,18,24,32,36,48,72,96,144]
- three84=[2,3,4,6,8,12,16,24,32,48,64,96,128,192]
- x360=1/(29/10440) #10440 is !144
- two=96/43.62 #any from tuble tw88 x16 / x7.2
- # the below here is testingr something don't remember what
- def loop(c=(e**gamma)):
- x=pentacle(c)
- y=1/x
- while y < 144:
- x=pentacle(c)
- print(x,y)
- loop
- def analyse(c,d=32):
- a=cathie(c)
- for x in range(1,d):
- z=(rshift(int(a),x))
- print(x,c,z,z/c,'abc=',(1/(z/c)),'sqrt-abc=',sqrt(1/(z/c)),'sqrt z',sqrt(z))
- if z==1:
- break
- # Reciprocal & reverse-pentacle:
- def multacle(n):return (pentacle(n)*repentacle(n))
- def pentsum(n):return (pentacle(n)+repentacle(n))
- def binary_shift(n,m):return(lshift(n,m))
- def pentacle(n):return 1/(n*5/2)
- def repentacle(n):return 1/(n*2/5)
- def harmonic(n):return(pentsum(n)*n) # returns approx. 29...always..
- # above, equals 29/10..but we need the variable n(N)
- #def stable(n):return n*2 # ,n/(pentacle(n)/repentacle(n)) #last figure is always 0.16
- def pentacle3(n):return(1/(n*5/3))
- def repentacle3(n):return(1/(n*3/5))
- def pentsum3(n):return (pentacle3(n)+repentacle3(n))
- def harmonic3(n):return(pentsum3(n)*n) # 2.2666666666.. 34/15!!
- def harmonic31(n):return(((1/(n*5/3))+(1/(n*3/5)))*n)
- #from the above i ducted furter not next but next
- def stable(n):return(pentacle(n)/repentacle(n)) #last figure is always 0.16
- ## above equls 4/25 but we want n(N)
- # this is for getting sum of an "array" which is all digits
- # from x to y.
- def sum(n):
- x=0
- for y in range(1,n):
- x=x+y
- return(x+n) #phase-
- #here thats
- def nos(n):return(pentsum(n)/pentacle(n)) #always return 7.25
- def nos2(n):return((1/(n*5/2)+1/(n*2/5))/(1/(n*5/2))) # same as above
- def son(n):return(pentsum(n)/n) #this oen was col.
- def boss(n): # 4.915960401250875 constant/static..
- x=(((n/3)*(n*5)/2)*2.9)
- y=sqrt(x)
- z=y/n
- return(z)
- def boss2(n): # 3.6514837167011076 constant/static..
- x=(((n/3)*(n*5)/2)*0.16)
- y=sqrt(x)
- z=y/n
- return(z)
- def boss3(n,nn): # as above without the 0.16 static instead nnany
- x=(((n/3)*(n*5)/2)*nn)
- y=sqrt(x)
- z=y/n
- return(z)
- # HERE is the stuff we pipe around in a circle with both this
- # being our way of Enigma calculating stuff which is then
- # processed in a circle with / through the E=xyz (einstein)
- # formulas which read like cake..
- def yzz(n,a=2.9): #returns some multiples of 4 or 5 per 29..
- y=0
- for x in range(1,n):
- y=y+(x/a)
- #print(y) #enable this one to show stuff important remove first #
- return(y/n)
- ten=yzz(59)
- anti_matter=boss2(87)*boss(87)*0.16
- #### buckminster fuller equations!!::
- def sq_triangle(n):
- ''' N='square' triangle how many times.'''
- return((n*(n+1))/2)
- def fuller_n(f,n=5,a=2):
- return(a*n*(f**2)+2)
- def relation(n): #number of tangible relationshops n!
- return(((n**2)-n)/2)
- def spheres(f): #number of closest packed spheres
- n=0
- for x in range(f):
- n=n+((x**2))
- #print(x,n)
- #print(n)
- n=n*10
- #print(n)
- n=n+((2*f**2)+1)
- return(n)
- ## END FULLER.
- def test1(x,y): #print table something
- for z in range(0,x):
- print(bin(z))
- print(bin(y),y)
- print(bin((z&y)))
- print('-----')
- def test2(x=9,y=256,z=8): #not sure what this one does.
- for n in range(0,y):
- for m in range(0,z):
- print((x<<m),'&',n,'=',((x<<m)^n))
- print('-----')
- placer=fuller_n(6)-fuller_n(2) #from NWSE. obsiouyy 6/22
- #spectacle
- zy=(harmonic(21)*stable(21)*nos(21)*boss(89))
- print('hello and:',zy,'test')
- def cathie(c):
- '''
- Bruce Cathie relativity equations two. c is a variable speed of
- special frame of reference or singular entitiy. Value. Function
- seems to vaugely relate to one coincidental Buckminster Fuller
- equations.
- '''
- return((2*c*sqrt(1/(2*c)))*(2*c)**2)
- def cathie2(c):
- ''' This is a variant of the one above just using a differnt formula
- according to wolfram alpha, but i t gives different output?
- And with x6 as was shown by triel good be.
- Use this at least with 'Standard Atonic Weight'.s
- '''
- return((4*(sqrt(2))/((1/c)*5/2)))
- def cathie3(c):
- '''Relativity equation 3'''
- return( sqrt((2*c)+sqrt(1/(2*c))*(2*c)**2))
- def cathie32(c):
- '''Relativity equation 3, wolfram alpha version'''
- return(sqrt(2*c+(2*sqrt(2))/((1/c)**(3/2))))
- def cathie33(c):
- ''' Another substuture of H3 assuming c is positive
- which I suppose it is, because how can speed of light be
- negative or?'''
- return(sqrt(2*sqrt(2) *c**(3/2)+2* c))
- def sunfact(n): # dnot know what this is. doesnt work either
- if n < 1:
- return(1)
- else:
- return(n*sunfact(n-1)+1-2*(n%2))
- def pi_c(x): #this can give closer and closer aprox of PI
- area = 0 #but we never reach a perfect sphere in anything may
- hypot=2 #so we only need approximations.
- for n in range(0,x):
- height=1-(1-(hypot/2)**2)**0.5
- area=area+2**n*height*hypot
- hypot=(height**2+(hypot/2)**2)**0.5
- return(area)
- def test4(n,f,x=216,y=8): m# dont know about this
- flr=fuller_n(f,n)
- #print(flr)
- return((1/(flr*lsic)*x)*2**y)
- # future \use
- def approximate_size(size, a_kilobyte_is_1024_bytes=True):
- '''Convert a file size to human-readable form.
- Keyword arguments:
- size -- file size in bytes
- a_kiloyte_is_1024_bytes -- if True (default), use multiples of 1024
- if False, use multiples of 1000
- Returns: string
- '''
- if size < 0:
- raise ValueError('number must be non-negative')
- multiple = 1152 if a_kilobyte_is_1024_bytes else 1024
- for suffix in SUFFIXES[multiple]:
- size /= multiple
- if size < multiple:
- return '{0:.1f} {1}'.format(size, suffix)
- raise ValueError('number too large')
- print(cathie2(alpha*sqrt(2)),'alpha x sqrt2 -> cathie2')
- # new functions.
- def enew(x,c):
- z=(cos(x)*c+1/(1/c)**(3/2))
- return(z)
- def crack(depth=16):
- x=1/58*(2**(3+depth)*5**depth-1)
- x=x*sqrt(2)
- #print('1.Cathie Wolfram 2b X is qual to: ',x,'Hertz is equal to: ',cathie2(x),'ok.. With this reciprocal / inverse: ',1/cathie2(x))
- #..DO NOT EVEN THINK ABOUT THESE NEVER.
- #print('2.Cathie 3 W/A:',x,'Hertz is equal to: ',cathie32(x),'ok.. With this reciprocal / inverse:..')
- #print('3.Cathie Pos W/A:: ',x,'Hertz is equal to: ',cathie33(x),'ok.. With this reciprocal / inverse: ',1/cathie33(x))
- return(x)
- def wad(n,f): #this one is what makes the dimensional tables part of it
- return(f/6480)**(n-1) #other version of wadt
- #doesnt give complex numbers
- #with negative values for n
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