From Wikipedia, the free encyclopedia
The NUMBER PI
There are many forms of PI and you can see them [1]
However the number of Pi is not just a circle but a series of geometric images such as an equilateral triangle, square, pentagon, etc.
unique pattern that I found 2004. Pi for all numbers is:
π
n
=
n
2
.
s
i
n
(
360
n
)
{\displaystyle \pi _{n}={\frac {n}{2}}.sin({\frac {360}{n}})}
sinus in degrees
n= {3,4,5,6........., infinity}
n=3 it is the equilateral triangle
π
3
=
3
2
sin
(
360
3
)
{\displaystyle \pi _{3}={\frac {3}{2}}\sin({\frac {360}{3}})}
π
3
=
1.299038105676657970145584756129404275207103940357785471041855234588949762681600027810859640067936431756719606061555027272477458821249214359108741634070780236396069923926729186550981115075813506192448761484257450177492164988004191001691378478420285348745275896191014287489903034894542100737760629932038067463761097204575710701640392743812359372142969874748342368381216535847874688010418122988440891548250968547863765249583132380335670783737076566229143676252517640533358216521993217274347815376373554674619972363212265589806452991554023153186737988373546994737255879027157790435027172484077780448014436830076173399466281730856066512557064076779745703123294923844606990748216673347110878468792671641139677682025389606048286479258495794767292154648948115366998523815015896613116458830885964900880276393737512516970811610634553457857999822195125972183078771421332595361479060232409486838841413231534260410498721433971667217832916432192792394148303696921223601631524640287512203987208937787304127.......
{\displaystyle \pi _{3}=1.299038105676657970145584756129404275207103940357785471041855234588949762681600027810859640067936431756719606061555027272477458821249214359108741634070780236396069923926729186550981115075813506192448761484257450177492164988004191001691378478420285348745275896191014287489903034894542100737760629932038067463761097204575710701640392743812359372142969874748342368381216535847874688010418122988440891548250968547863765249583132380335670783737076566229143676252517640533358216521993217274347815376373554674619972363212265589806452991554023153186737988373546994737255879027157790435027172484077780448014436830076173399466281730856066512557064076779745703123294923844606990748216673347110878468792671641139677682025389606048286479258495794767292154648948115366998523815015896613116458830885964900880276393737512516970811610634553457857999822195125972183078771421332595361479060232409486838841413231534260410498721433971667217832916432192792394148303696921223601631524640287512203987208937787304127.......}
Area of an equilateral triangle will be
R
2
π
3
{\displaystyle R^{2}\pi _{3}}
R -radius of the circle described about an equilateral triangle
The scope of the triangle will be
C
=
2
R
π
3
cos
α
2
:
α
=
360
3
{\displaystyle C={\frac {2R\pi _{3}}{\cos {\frac {\alpha }{2}}}}:\alpha ={\frac {360}{3}}}
See picture[]
n=4 it is a square
π
4
=
2
{\displaystyle \pi _{4}=2}
Area of squares will be
R
2
π
4
{\displaystyle R^{2}\pi _{4}}
R -radius of the circle described around the square
Perimeter of the square will be
C
=
2
R
π
4
cos
α
2
:
α
=
360
4
{\displaystyle C={\frac {2R\pi _{4}}{\cos {\frac {\alpha }{2}}}}:\alpha ={\frac {360}{4}}}
See picture[]
so on pentagon, hexagon .......
π
5
=
2.37764129073788393029109833344845535851424658531437555611826411107538292521298375429698202742702845418974929387850751052246766548442424981578803067578295594696444359492600258179554275230250379513151001423802924795917183008219605036301495148507880140322781045987090044531881885084349467130129921084258543849815492459549445122232219143670592470372285079329288667825627445956811065730153458201304781755172126659167760259062780734991737248477967564240583159502841310815397363785669533897013826055892072659996199853464482719029151537061472938008846993548889178745205678459542206169347872570742004980802724766701370391337077603044283323962631433827549038847681729685293628396669902392009519093871640782190843048473742646406880592139994355352920382189607783603508041226848456648980006775286567800517085352418736253370309354164490169821718538097751802464867296154739841155499816959251406543633373361369339814369337895730123108013172623915093695955211484250762466097770012856809360256952109203831071625
{\displaystyle \pi _{5}=2.37764129073788393029109833344845535851424658531437555611826411107538292521298375429698202742702845418974929387850751052246766548442424981578803067578295594696444359492600258179554275230250379513151001423802924795917183008219605036301495148507880140322781045987090044531881885084349467130129921084258543849815492459549445122232219143670592470372285079329288667825627445956811065730153458201304781755172126659167760259062780734991737248477967564240583159502841310815397363785669533897013826055892072659996199853464482719029151537061472938008846993548889178745205678459542206169347872570742004980802724766701370391337077603044283323962631433827549038847681729685293628396669902392009519093871640782190843048473742646406880592139994355352920382189607783603508041226848456648980006775286567800517085352418736253370309354164490169821718538097751802464867296154739841155499816959251406543633373361369339814369337895730123108013172623915093695955211484250762466097770012856809360256952109203831071625}
See picture[]
π
6
=
2.59807621135331594029116951225880855041420788071557094208371046917789952536320005562171928013587286351343921212311005454495491764249842871821748326814156047279213984785345837310196223015162701238489752296851490035498432997600838200338275695684057069749055179238202857497980606978908420147552125986407613492752219440915142140328078548762471874428593974949668473676243307169574937602083624597688178309650193709572753049916626476067134156747415313245828735250503528106671643304398643454869563075274710934923994472642453117961290598310804630637347597674709398947451175805431558087005434496815556089602887366015234679893256346171213302511412815355949140624658984768921398149643334669422175693758534328227935536405077921209657295851699158953458430929789623073399704763003179322623291766177192980176055278747502503394162322126910691571599964439025194436615754284266519072295812046481897367768282646306852082099744286794333443566583286438558478829660739384244720326304928057502440797441787557460825459
{\displaystyle \pi _{6}=2.59807621135331594029116951225880855041420788071557094208371046917789952536320005562171928013587286351343921212311005454495491764249842871821748326814156047279213984785345837310196223015162701238489752296851490035498432997600838200338275695684057069749055179238202857497980606978908420147552125986407613492752219440915142140328078548762471874428593974949668473676243307169574937602083624597688178309650193709572753049916626476067134156747415313245828735250503528106671643304398643454869563075274710934923994472642453117961290598310804630637347597674709398947451175805431558087005434496815556089602887366015234679893256346171213302511412815355949140624658984768921398149643334669422175693758534328227935536405077921209657295851699158953458430929789623073399704763003179322623291766177192980176055278747502503394162322126910691571599964439025194436615754284266519072295812046481897367768282646306852082099744286794333443566583286438558478829660739384244720326304928057502440797441787557460825459}
π
7
=
.
.
.
.
.
.
.
.
.
.
.
{\displaystyle \pi _{7}=...........}
π
8
=
.
.
.
.
.
.
.
.
.
.
.
{\displaystyle \pi _{8}=...........}
.
.
.
.
.
.
.
.
.
.
.
{\displaystyle ...........}
π
1
2
=
3
{\displaystyle \pi _{1}2=3}
.
.
.
.
.
.
.
.
.
.
.
{\displaystyle ...........}
π
=
3.14159265358979323846264338327950288419716939937510582097494459230781640628620899862803482534211706798214808651328230664709384460955058223172535940812848111745028410270193852110555964462294895493038196442881097566593344612847564823378678316527120190914564856692346034861045432664821339360726024914127372458700660631558817488152092096282925409171536436789259036001133053054882046652138414695194151160943305727036575959195309218611738193261179310511854807446237996274956735188575272489122793818301194912983367336244065664308602139494639522473719070217986094370277053921717629317675238467481846766940513200056812714526356082778577134275778960917363717872146844090122495343014654958537105079227968925892354201995611212902196086403441815981362977477130996051870721134999999837297804995105973173281609631859502445945534690830264252230825334468503526193118817101000313783875288658753320838142061717766914730359825349042875546873115956286388235378759375195778185778053217122680661300192787661119590922
{\displaystyle \pi =3.14159265358979323846264338327950288419716939937510582097494459230781640628620899862803482534211706798214808651328230664709384460955058223172535940812848111745028410270193852110555964462294895493038196442881097566593344612847564823378678316527120190914564856692346034861045432664821339360726024914127372458700660631558817488152092096282925409171536436789259036001133053054882046652138414695194151160943305727036575959195309218611738193261179310511854807446237996274956735188575272489122793818301194912983367336244065664308602139494639522473719070217986094370277053921717629317675238467481846766940513200056812714526356082778577134275778960917363717872146844090122495343014654958537105079227968925892354201995611212902196086403441815981362977477130996051870721134999999837297804995105973173281609631859502445945534690830264252230825334468503526193118817101000313783875288658753320838142061717766914730359825349042875546873115956286388235378759375195778185778053217122680661300192787661119590922}
evidence
π
=
n
2
.
s
i
n
(
360
n
)
{\displaystyle \pi ={\frac {n}{2}}.sin({\frac {360}{n}})}
l
i
m
n
→
∞
n
2
.
s
i
n
(
360
n
)
{\displaystyle lim_{n\to \infty }{\frac {n}{2}}.sin({\frac {360}{n}})}
1
2
l
i
m
n
→
∞
n
.
s
i
n
(
360
n
)
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }n.sin({\frac {360}{n}})}
1
2
l
i
m
n
→
∞
s
i
n
(
360
n
)
1
n
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {360}{n}})}{\frac {1}{n}}}}
1
2
l
i
m
n
→
∞
s
i
n
(
360
n
)
1
n
.
360
360
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {360}{n}})}{\frac {1}{n}}}.{\frac {360}{360}}}
360
2
l
i
m
n
→
∞
s
i
n
(
360
n
)
360
n
{\displaystyle {\frac {360}{2}}lim_{n\to \infty }{\frac {sin({\frac {360}{n}})}{\frac {360}{n}}}}
360
n
=
t
{\displaystyle {\frac {360}{n}}=t}
t
→
0
{\displaystyle t\rightarrow \ 0}
180
lim
t
→
0
s
i
n
t
t
=
180
0
{\displaystyle 180\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=180^{0}}
180
0
=
π
(
r
a
d
)
{\displaystyle 180^{0}=\pi (rad)}
-------------------------------------------------------
The following is another new form of PI, which I found in 2004
π
=
180.
m
.
s
i
n
(
1
m
)
{\displaystyle \pi =180.m.sin({\frac {1}{m}})}
lim
m
→
∞
180.
m
.
s
i
n
(
1
m
)
{\displaystyle \lim _{m\to \infty }180.m.sin({\frac {1}{m}})}
180
lim
m
→
∞
m
.
s
i
n
(
1
m
)
{\displaystyle 180\lim _{m\to \infty }m.sin({\frac {1}{m}})}
180
lim
m
→
∞
s
i
n
(
1
m
)
1
m
{\displaystyle 180\lim _{m\to \infty }{\frac {sin({\frac {1}{m}})}{\frac {1}{m}}}}
1
m
=
t
{\displaystyle {\frac {1}{m}}=t}
m
→
∞
{\displaystyle m\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
180
lim
t
→
0
s
i
n
t
t
=
180
0
{\displaystyle 180\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=180^{0}}
180
0
=
π
(
r
a
d
)
{\displaystyle 180^{0}=\pi (rad)}
-------------------------------------------------------
π
2
{\displaystyle {\frac {\pi }{2}}}
π
2
=
n
2
s
i
n
(
180
n
)
{\displaystyle {\frac {\pi }{2}}={\frac {n}{2}}sin({\frac {180}{n}})}
evidence
l
i
m
n
→
∞
n
2
.
s
i
n
(
180
n
)
{\displaystyle lim_{n\to \infty }{\frac {n}{2}}.sin({\frac {180}{n}})}
1
2
l
i
m
n
→
∞
n
.
s
i
n
(
180
n
)
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }n.sin({\frac {180}{n}})}
1
2
l
i
m
n
→
∞
s
i
n
(
180
n
)
1
n
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {180}{n}})}{\frac {1}{n}}}}
1
2
l
i
m
n
→
∞
s
i
n
(
180
n
)
1
n
.
180
180
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {180}{n}})}{\frac {1}{n}}}.{\frac {180}{180}}}
90
lim
m
→
∞
s
i
n
(
1
m
)
1
m
{\displaystyle 90\lim _{m\to \infty }{\frac {sin({\frac {1}{m}})}{\frac {1}{m}}}}
180
n
=
t
{\displaystyle {\frac {180}{n}}=t}
n
→
∞
{\displaystyle n\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
90
lim
t
→
0
s
i
n
t
t
=
90
0
{\displaystyle 90\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=90^{0}}
90
0
=
π
2
(
r
a
d
)
{\displaystyle 90^{0}={\frac {\pi }{2}}(rad)}
-------------------------------------------------------
π
3
{\displaystyle {\frac {\pi }{3}}}
π
3
=
n
2
s
i
n
(
120
n
)
{\displaystyle {\frac {\pi }{3}}={\frac {n}{2}}sin({\frac {120}{n}})}
evidence
l
i
m
n
→
∞
n
2
.
s
i
n
(
120
n
)
{\displaystyle lim_{n\to \infty }{\frac {n}{2}}.sin({\frac {120}{n}})}
1
2
l
i
m
n
→
∞
n
.
s
i
n
(
120
n
)
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }n.sin({\frac {120}{n}})}
1
2
l
i
m
n
→
∞
s
i
n
(
120
n
)
1
n
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {120}{n}})}{\frac {1}{n}}}}
1
2
l
i
m
n
→
∞
s
i
n
(
120
n
)
1
n
.
120
120
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {120}{n}})}{\frac {1}{n}}}.{\frac {120}{120}}}
60
lim
n
→
∞
s
i
n
(
120
n
)
120
n
{\displaystyle 60\lim _{n\to \infty }{\frac {sin({\frac {120}{n}})}{\frac {120}{n}}}}
120
n
=
t
{\displaystyle {\frac {120}{n}}=t}
n
→
∞
{\displaystyle n\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
60
lim
t
→
0
s
i
n
t
t
=
60
0
{\displaystyle 60\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=60^{0}}
60
0
=
π
3
(
r
a
d
)
{\displaystyle 60^{0}={\frac {\pi }{3}}(rad)}
-------------------------------------------------------
π
4
{\displaystyle {\frac {\pi }{4}}}
π
4
=
n
2
.
s
i
n
(
90
n
)
{\displaystyle {\frac {\pi }{4}}={\frac {n}{2}}.sin({\frac {90}{n}})}
evidence
l
i
m
n
→
∞
n
2
.
s
i
n
(
90
n
)
{\displaystyle lim_{n\to \infty }{\frac {n}{2}}.sin({\frac {90}{n}})}
1
2
l
i
m
n
→
∞
n
.
s
i
n
(
90
n
)
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }n.sin({\frac {90}{n}})}
1
2
l
i
m
n
→
∞
s
i
n
(
90
n
)
1
n
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {90}{n}})}{\frac {1}{n}}}}
1
2
l
i
m
n
→
∞
s
i
n
(
90
n
)
1
n
.
90
90
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {90}{n}})}{\frac {1}{n}}}.{\frac {90}{90}}}
90
2
l
i
m
n
→
∞
s
i
n
(
90
n
)
90
n
{\displaystyle {\frac {90}{2}}lim_{n\to \infty }{\frac {sin({\frac {90}{n}})}{\frac {90}{n}}}}
90
n
=
t
{\displaystyle {\frac {90}{n}}=t}
n
→
∞
{\displaystyle n\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
45
lim
t
→
0
s
i
n
t
t
=
45
0
{\displaystyle 45\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=45^{0}}
45
0
=
π
4
(
r
a
d
)
{\displaystyle 45^{0}={\frac {\pi }{4}}(rad)}
-------------------------------------------------------
π
5
{\displaystyle {\frac {\pi }{5}}}
π
5
=
n
2
s
i
n
(
72
n
)
{\displaystyle {\frac {\pi }{5}}={\frac {n}{2}}sin({\frac {72}{n}})}
evidence
l
i
m
n
→
∞
n
2
.
s
i
n
(
72
n
)
{\displaystyle lim_{n\to \infty }{\frac {n}{2}}.sin({\frac {72}{n}})}
1
2
l
i
m
n
→
∞
n
.
s
i
n
(
72
n
)
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }n.sin({\frac {72}{n}})}
1
2
l
i
m
n
→
∞
s
i
n
(
72
n
)
1
n
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {72}{n}})}{\frac {1}{n}}}}
1
2
l
i
m
n
→
∞
s
i
n
(
72
n
)
1
n
.
72
72
{\displaystyle {\frac {1}{2}}lim_{n\to \infty }{\frac {sin({\frac {72}{n}})}{\frac {1}{n}}}.{\frac {72}{72}}}
72
2
l
i
m
n
→
∞
s
i
n
(
72
n
)
72
n
{\displaystyle {\frac {72}{2}}lim_{n\to \infty }{\frac {sin({\frac {72}{n}})}{\frac {72}{n}}}}
72
n
=
t
{\displaystyle {\frac {72}{n}}=t}
n
→
∞
{\displaystyle n\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
72
2
l
i
m
t
→
0
s
i
n
t
t
=
72
2
{\displaystyle {\frac {72}{2}}lim_{t\to \mathbf {0} }{\frac {sint}{t}}={\frac {72}{2}}}
72
2
=
π
5
(
r
a
d
)
{\displaystyle {\frac {72}{2}}={\frac {\pi }{5}}(rad)}
-------------------------------------------------------
π
8
{\displaystyle {\frac {\pi }{8}}}
π
8
=
n
2
s
i
n
(
45
n
)
{\displaystyle {\frac {\pi }{8}}={\frac {n}{2}}sin({\frac {45}{n}})}
-------------------------------------------------------
The following is another new form of PI, which I found in 2004
π
=
n
.
sin
(
180
n
)
{\displaystyle \pi =n.\sin({\frac {180}{n}})}
evidence
l
i
m
n
→
∞
n
.
s
i
n
(
180
n
)
{\displaystyle \ lim_{n\to \infty }n.sin({\frac {180}{n}})}
l
i
m
n
→
∞
s
i
n
(
180
n
)
1
n
{\displaystyle \ lim_{n\to \infty }{\frac {sin({\frac {180}{n}})}{\frac {1}{n}}}}
l
i
m
n
→
∞
s
i
n
(
180
n
)
1
n
.
180
180
{\displaystyle \ lim_{n\to \infty }{\frac {sin({\frac {180}{n}})}{\frac {1}{n}}}.{\frac {180}{180}}}
180
lim
m
→
∞
s
i
n
(
180
n
)
180
n
{\displaystyle 180\lim _{m\to \infty }{\frac {sin({\frac {180}{n}})}{\frac {180}{n}}}}
180
n
=
t
{\displaystyle {\frac {180}{n}}=t}
n
→
∞
{\displaystyle n\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
180
lim
t
→
0
s
i
n
t
t
=
180
0
{\displaystyle 180\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=180^{0}}
180
0
=
π
(
r
a
d
)
{\displaystyle 180^{0}=\pi (rad)}
-------------------------------------------------------
π
2
{\displaystyle {\frac {\pi }{2}}}
π
2
=
n
.
sin
(
90
n
)
{\displaystyle {\frac {\pi }{2}}=n.\sin({\frac {90}{n}})}
-------------------------------------------------------
π
3
{\displaystyle {\frac {\pi }{3}}}
π
3
=
n
.
sin
(
60
n
)
{\displaystyle {\frac {\pi }{3}}=n.\sin({\frac {60}{n}})}
-------------------------------------------------------
π
5
{\displaystyle {\frac {\pi }{5}}}
π
5
=
n
.
sin
(
36
n
)
{\displaystyle {\frac {\pi }{5}}=n.\sin({\frac {36}{n}})}
-------------------------------------------------------
The following is another new form of PI, which I found in 2004
π
=
360.
m
.
s
i
n
(
1
2
m
)
{\displaystyle \pi =360.m.sin({\frac {1}{2m}})}
lim
m
→
∞
360.
m
.
s
i
n
(
1
2
m
)
{\displaystyle \lim _{m\to \infty }360.m.sin({\frac {1}{2m}})}
360
lim
m
→
∞
m
.
s
i
n
(
1
2
m
)
{\displaystyle 360\lim _{m\to \infty }m.sin({\frac {1}{2m}})}
360
lim
m
→
∞
s
i
n
(
1
2
m
)
1
m
{\displaystyle 360\lim _{m\to \infty }{\frac {sin({\frac {1}{2m}})}{\frac {1}{m}}}}
360
lim
m
→
∞
s
i
n
(
1
2
m
)
1
m
1
2
1
2
{\displaystyle 360\lim _{m\to \infty }{\frac {sin({\frac {1}{2m}})}{\frac {1}{m}}}{\frac {\frac {1}{2}}{\frac {1}{2}}}}
360.
1
2
lim
m
→
∞
s
i
n
(
1
2
m
)
1
2
m
{\displaystyle 360.{\frac {1}{2}}\lim _{m\to \infty }{\frac {sin({\frac {1}{2m}})}{\frac {1}{2m}}}}
1
2
m
=
t
{\displaystyle {\frac {1}{2m}}=t}
m
→
∞
{\displaystyle m\to \infty }
t
→
0
{\displaystyle t\rightarrow \ 0}
180
lim
t
→
0
s
i
n
t
t
=
180
0
{\displaystyle 180\lim _{t\to \mathbf {0} }{\frac {sint}{t}}=180^{0}}
180
0
=
π
(
r
a
d
)
{\displaystyle 180^{0}=\pi (rad)}
For the numerical values of PI recommend free extra precision calculator Harry-J-Smith XP,XM,….. recommend m=1.0E+10000000
to the success of the calculator you need to install netframework2.0
(Рајко Велимировић (talk ) 10:02, 21 December 2011 (UTC))