mecánica-física y electrónica y análisis-funcional y evangelio-stronikiano

Principio: [ de no gloria ]

Ecuación de 1º grado

Ecuación de 2º grado

Principio: [ de no gloria ]

Derivada y integral de 1º grado

Derivada y integral de 2º grado

Principio: [ de no gloria ]

Serie de 1º grado (1/k!)

Serie de 2º grado (1/(2k+r)!)

No hay logaritmos ni funciones trigonométricas inversas.

Ley: [ de barcos y aviones en un mundo glorificado ]

m·d_{tt}^{2}[x] = F+(-1)·p·h(ut)·g

d_{tt}^{2}[x] = 0 <==> t = (1/u)·Anti-h( (1/p)·(F/g) )

m·d_{t}[x] = Ft+(-1)·p·(1/u)·H(ut)·g

d_{t}[x] = 0 <==> t = (1/u)·Anti-[ (1/s)·H(s) ]-( F/(pg) )

Ley: [ de vehículos terrestres en un mundo glorificado ]

m·d_{tt}^{2}[x] = F+(-1)·( p·h(ut)+q )·g

d_{tt}^{2}[x] = 0 <==> t = (1/u)·Anti-h( (1/p)·( (-q)+(F/g) ) )

m·d_{t}[x] = Ft+(-1)·( p·(1/u)·H(ut)+qt )·g

d_{t}[x] = 0 <==> t = (1/u)·Anti-[ (p/q)·(1/s)·H(s)+1 ]-( F/(qg) )

Ley: [ de ascensores en un mundo glorificado ]

Sea d_{tt}^{2}[z] = d_{tt}^{2}[x] = d_{tt}^{2}[y] ==>

m·d_{tt}^{2}[x] = (-1)·p·h(ut)·g+T

m·d_{tt}^{2}[y] = qg+(-T)

m·d_{tt}^{2}[z] =  (1/2)·( (-1)·p·h(ut)+q )·g

T = (1/2)·( p·h(ut)+q )·g

m·d_{tt}^{2}[z] = 0  <==> t = (1/u)·Anti-h(q/p)

m·d_{t}[z] = (1/2)·( (-1)·p·(1/u)·H(ut)+qt )·g

d_{t}[z] = 0 <==> t = (1/u)·Anti-[ (p/q)·(1/s)·H(s)+1 ]-(0)

Ley: [ de submarinos en un mundo glorificado ]

m·d_{tt}^{2}[x] = p·h(ut)·g+(-b)·d_{t}[x]

d_{t}[x] = e^{(-1)·(b/m)·t}·int[ (p/m)·h(ut)·g·e^{(b/m)·t} ]d[t]

m·d_{tt}^{2}[x] = 0 <==> t = (1/u)·Anti-h( (b/(pg))·d_{t}[x] )

Ley: [ de colchones en un mundo glorificado ]

m·d_{tt}^{2}[x] = p·h(ut)·g+(-k)·x

x(t) = ...

... int[ cos( (k/m)^{(1/2)}·t )·int[ cos( (k/m)^{(1/2)}·t )·(p/m)·h(ut)·g ]d[t] ]d[t]

... int[ sin( (k/m)^{(1/2)}·t )·int[ sin( (k/m)^{(1/2)}·t )·(p/m)·h(ut)·g ]d[t] ]d[t]

m·d_{tt}^{2}[x] = 0 <==> t = (1/u)·Anti-h( (k/(pg))·x )

Ley: [ de ecualizador de voltaje espiral ]

L·d_{tt}^{2}[q] = C·( 1+(C/L)·t^{2} )·q(t)

q(t) = pe^{(C/L)·(1/2)·t^{2}}

L·d_{tt}^{2}[q] = (-C)·( 1+(C/L)·t^{2} )·q(t)

q(t) = pe^{(-1)·(C/L)·(1/2)·t^{2}}

Ley: [ de ecualizador de carga espiral ]

(L/R)^{2}·d_{tt}^{2}[q] = t·d_{t}[q]

d_{t}[q] = Ie^{(R/L)^{2}·(1/2)·t^{2}}

q(t) = I·(L/R)^{2}·e^{(R/L)^{2}·(1/2)·t^{2}} [o(t)o] ln(ut)

(L/R)^{2}·d_{tt}^{2}[q] = (-t)·d_{t}[q]

d_{t}[q] = Ie^{(-1)·(R/L)^{2}·(1/2)·t^{2}}

q(t) = (-I)·(L/R)^{2}·e^{(-1)·(R/L)^{2}·(1/2)·t^{2}} [o(t)o] ln(ut)

Ley: [ de dron de voltaje espiral ]

(r/t)·( d_{t}[q]/q(t) ) = g

q(t) = pe^{(C/L)·(1/2)·t^{2}}

Ley: [ de dron de carga espiral ]

(r/t)·( d_{tt}^{2}[q]/d_{t}[q] ) = g

d_{t}[q] = Ie^{(R/L)^{2}·(1/2)·t^{2}}

Definició: [ d'espectre d'un operador ]

Esp(A) = { H(t) : [Ex][ A[x]+(-1)·L(t) = H(t) ] }

Fun-Prop(A) = { L(t) : [Ex][ A[x]+(-1)·L(t) = H(t) ] }

Teorema:

Sea A[x] = kx ==>

Esp(A) = {0} <==> lim[x = (1/k)·L(t)][ A[x] ] = L(t)

Demostració:

[=>] Sigui x(t) = (1/k)·L(t) ==>

A[x]+(-1)·L(t) = H(t)

| A[ (1/k)·L(t) ]+(-1)·L(t) | = | A[x]+(-1)·L(t) | = | H(t) | = 0 < s

lim[x = (1/k)·L(t)][ A[x] ] = L(t)

[<=] Sigui x(t) = (1/k)·L(t) ==>

A[x]+(-1)·L(t) = H(t)

| H(t) | = | A[x]+(-1)·L(t) | = | A[ (1/k)·L(t) ]+(-1)·L(t) | = | k·(1/k)·L(t)+(-1)·L(t) | = | L(t)+(-1)·L(t) | = 0

H(t) = 0

Teorema:

Sea A[x] = d_{t}[x] ==>

Si x(t) = e^{t} ==>

Fun-Prop(A) = { e^{t} } <==> Esp(A) = {0}

lim[x = e^{t}][ A[x] ] = e^{t}

Demostració:

Sigui s > 0 ==> 

| A[x]+(-1)·e^{t} | = | d_{t}[x]+(-1)·e^{t} | = | e^{t}+(-1)·e^{t} | < s

Teorema:

Sea A[x] = d_{t}[x] ==>

Si x(t) = t ==>

Fun-Prop(A) = { t+(-1) } <==> Esp(A) = {t}

Teorema:

Sea A[x] = d_{t}[x]+kx ==>

Si x(t) = e^{kt} ==>

Fun-Prop(A) = { 2ke^{kt} } <==> Esp(A) = {0}

lim[x = e^{kt}][ A[x] ] = 2ke^{kt}

Demostració:

Sigui s > 0 ==> 

| A[x]+(-1)·2ke^{kt} | = | d_{t}[x]+kx+(-1)·2ke^{kt} | = | ke^{kt}+ke^{kt}+(-1)·2ke^{kt} | < s

Teorema:

Sea A[x] = d_{t}[x]+kx ==>

Si x(t) = t ==>

Fun-Prop(A) = { (1+(-k))·t+(-1) } <==> Esp(A) = {t}

Teorema:

Sea A[x] = int[x]d[t] ==>

Si x(t) = e^{t} ==>

Fun-Prop(A) = { e^{t} } <==> Esp(A) = {0}

lim[x = e^{t}][ A[x] ] = e^{t}

Demostració:

Sigui s > 0 ==> 

| A[x]+(-1)·e^{t} | = | int[x]d[t]+(-1)·e^{t} | = | e^{t}+(-1)·e^{t} | < s

Teorema:

Sea A[x] = int[x]d[t] ==>

Si x(t) = 1 ==>

Fun-Prop(A) = { 0 } <==> Esp(A) = {t}

Teorema:

Sea A[x] = int[x]d[t]+kx ==>

Si x(t) = e^{(1/k)·t} ==>

Fun-Prop(A) = { 2ke^{(1/k)·t} } <==> Esp(A) = {0}

lim[x = e^{(1/k)·t}][ A[x] ] = 2ke^{(1/k)·t}

Demostració:

Sigui s > 0 ==> 

| A[x]+(-1)·2ke^{(1/k)·t} | = | int[x]d[t]+kx+(-1)·2ke^{(1/k)·t} | = ...

... | ke^{(1/k)·t}+ke^{(1/k)·t}+(-1)·2ke^{(1/k)·t} | < s

Teorema:

Sea A[x] = int[x]d[t]+kx ==>

Si x(t) = 1 ==>

Fun-Prop(A) = { (-k) } <==> Esp(A) = {t}

Teorema:

int[x = 0]-[1][ e^{nx}+(3/2)^{sig(1,1)}·(1/n) ]d[x] [o] int[x = 0]-[1][ e^{(-1)·nx}+(2/n) ]d[x] = 1

int[x = 0]-[1][ e^{nx}+(2/3)^{sig(2,2)}·(1/n) ]d[x] [o] int[x = 0]-[1][ e^{(-1)·nx}+(3/n) ]d[x] = 0

Teorema:

int[x = 0]-[1][ e^{nx}+(3/2)^{sig(1,2)}·(1/n) ]d[x] [o] int[x = 0]-[1][ e^{(-1)·nx}+(3/n) ]d[x] = 0

int[x = 0]-[1][ e^{nx}+(2/3)^{sig(2,1)}·(1/n) ]d[x] [o] int[x = 0]-[1][ e^{(-1)·nx}+(2/n) ]d[x] = 1

Teorema:

int[x = 0]-[1][ x^{n}+( n^{2}+2n+2 )^{sig(1,1)}·(1/(n+1)) ]d[x] [o] ...

... int[x = 0]-[1][ (-1)·x^{n}+(1/(n+1)) ]d[x] = 1

int[x = 0]-[1][ x^{n}+( 1/(n^{2}+2n+2) )^{sig(2,2)}·(1/(n+1)) ]d[x] [o] ...

... int[x = 0]-[1][ (-1)·x^{n}+( n^{2}+2n+2 )·(1/(n+1)) ]d[x] = 0

Teorema:

int[x = 0]-[1][ x^{n}+( n^{2}+2n+2 )^{sig(1,2)}·(1/(n+1)) ]d[x] [o] ...

... int[x = 0]-[1][ (-1)·x^{n}+( n^{2}+2n+2 )·(1/(n+1)) ]d[x] = 0

int[x = 0]-[1][ x^{n}+( 1/(n^{2}+2n+2) )^{sig(2,1)}·(1/(n+1)) ]d[x] [o] ...

... int[x = 0]-[1][ (-1)·x^{n}+(1/(n+1)) ]d[x] = 1

Teorema:

int[x = 0]-[(pi/2)][ sin(nx)+2^{sig(1,1)}·(2/pi)·(1/n) ]d[x] [o] ...

... int[x = 0]-[(pi/2)][ (-1)·sin(nx)+(2/pi)·(1/n) ]d[x] = 1

int[x = 0]-[(pi/2)][ sin(nx)+(1/2)^{sig(2,2)}·(2/pi)·(1/n) ]d[x] [o] ...

... int[x = 0]-[(pi/2)][ (-1)·sin(nx)+(4/pi)·(1/n) ]d[x] = 0

Teorema:

int[x = 0]-[(pi/2)][ sin(nx)+2^{sig(1,2)}·(2/pi)·(1/n) ]d[x] [o] ...

... int[x = 0]-[(pi/2)][ (-1)·sin(nx)+(4/pi)·(1/n) ]d[x] = 0

int[x = 0]-[(pi/2)][ sin(nx)+(1/2)^{sig(2,1)}·(2/pi)·(1/n) ]d[x] [o] ...

... int[x = 0]-[(pi/2)][ (-1)·sin(nx)+(2/pi)·(1/n) ]d[x] = 1

El que odiaba a los hombres odiando-me a mi,

está loco de odiar al prójimo no como a si mismo,

en ser yo un dios solo con cuerpo de hombre,

pero no soy un hombre.

Estos tíos odiaban a los hombres,

y Dios me ha hecho hombre,

para destruir-los con la condenación,

de no ser yo un hombre.

Me deberían de seguir muchos hombres,

porque contra más hombres,

más condenación de yo no ser un hombre.

Soy el profesor tornasol cap rodó.

Juan:

El que quiera ser esclavo del pecado,

que tire la primera piedra.

El que quiera ser libre del pecado,

que no tire ninguna piedra.