formas-diferenciales-aplicadas-a-la-física y geometría-diferencial y topología y cinemática-física y análisis-matemático

Principio: [ de súper-conducción de electrones coherentes ]

H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[&]-d[ax]+cos(ut)·g(ay)·d[ut]-[&]-d[ay] ] 

T·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = T+(-1)·T_{0}

Principio: [ de súper-conducción de gravitones coherentes ]

H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[&]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[&]-d[ay] ] 

T·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = T+(-1)·T_{0}

Principio: [ de láser de fotones eléctricos coherentes ]

H(x,y,t) = int-int[ e^{uti}·f(ax)·d[uti]-[&]-d[ax]+e^{(-1)·uti}·g(ay)·d[uti]-[&]-d[ay] ] 

z·( e^{uti}·F(ax)+(-1)·e^{(-1)·uti}·G(ay) [o] H(x,y,t) ) = z+(-1)·z_{0}

Principio: [ de láser de fotones gravitatorios coherentes ]

H(x,y,t) = int-int[ e^{ut}·f(ax)·d[ut]-[&]-d[ax]+e^{(-1)·ut}·g(ay)·d[ut]-[&]-d[ay] ] 

z·( e^{ut}·F(ax)+(-1)·e^{(-1)·ut}·G(ay) [o] H(x,y,t) ) = z+(-1)·z_{0}

Principio: [ de estabilizador de carga de electrones ]

H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[ || ]-d[ax]+cos(ut)·g(ay)·d[ut]-[ || ]-d[ay] ] 

q·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = 2q+(-1)·q_{0}

H(x,y,t) = (-1)·cos(ut)·(1/F(ax))+sin(ut)·(1/G(ay))

Principio: [ de estabilizador de carga de gravitones ]

H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[ || ]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[ || ]-d[ay] ] 

p·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = 2p+(-1)·p_{0}

H(x,y,t) = cosh(ut)·(1/F(ax))+(1/i)·sinh(ut)·(1/G(ay))

Anexo:

El estabilizador de conducción,

es un chip de diagonal-hipérbola y semi-círculo y hipérbola-diagonal.

Principio: [ de estabilizador de rotación de corriente eléctrico ]

H(x,y,t) = int-int[ sin(ut)·f(ax)·d[ut]-[ || ]-d[ax]+cos(ut)·g(ay)·d[ut]-[ || ]-d[ay] ] 

v·( (-1)·cos(ut)·F(ax)+sin(ut)·G(ay) [o] H(x,y,t) ) = 2v+(-1)·v_{0}

H(x,y,t) = (-1)·cos(ut)·(1/F(ax))+sin(ut)·(1/G(ay))

Principio: [ de estabilizador de rotación de corriente gravitatorio ]

H(x,y,t) = int-int[ sinh(ut)·f(ax)·d[ut]-[ || ]-d[ax]+(1/i)·cosh(ut)·g(ay)·d[ut]-[ || ]-d[ay] ] 

v·( cosh(ut)·F(ax)+(1/i)·sinh(ut)·G(ay) [o] H(x,y,t) ) = 2v+(-1)·v_{0}

H(x,y,t) = cosh(ut)·(1/F(ax))+(1/i)·sinh(ut)·(1/G(ay))

Anexo:

El estabilizador de rotación,

es un mecanismo donde circula un corriente,

de diagonal-hipérbola y semi-circulo y hipérbola-diagonal.

Teorema:

int-int[ z^{2n+(-1)}·d[y]-[&]-d[z]+z^{2n+(-1)}·d[z]-[&]-d[x]+(-1)·d[x]-[&]-d[y] ] = ...

... nx+ny+z^{2n}

Teorema:

int-int[ e^{2nz}·d[y]-[&]-d[z]+e^{2nz}·d[z]-[&]-d[x]+(-1)·d[x]-[&]-d[y] ] = ...

... nx+ny+e^{2nz}

Teorema:

int-int[ z^{3n+(-1)}·d[y]-[ || ]-d[z]+x^{3n+(-1)}·d[z]-[ || ]-d[x]+y^{3n+(-1)}·d[x]-[ || ]-d[y] ] = ...

... (1/z)^{3n}·(n/y)+(1/x)^{3n}·(n/z)+(1/y)^{3n}·(n/x)

Teorema:

int-int[ e^{3nz}·d[y]-[ || ]-d[z]+e^{3nx}·d[z]-[ || ]-d[x]+e^{3ny}·d[x]-[ || ]-d[y] ] = ...

... e^{(-3)·nz}·(n/y)+e^{(-3)·nx}·(n/z)+e^{(-3)·ny}·(n/x)

Geodésicas y Símbolos de Cristoffel:

Teorema:

Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>

Si H_{kk}^{k} = d_{t}[ f_{k}(t) ] ==> x_{k}(t) = ( t /o(t)o/ int[ f_{k}(t) ]d[t] )

H_{ij}^{k} = ( 1/f_{k}(t) )^{2}·d_{t}[ f_{k}(t) ]·f_{i}(t)·f_{j}(t)

Demostración:

(-1)·( 1/d_{t}[x_{k}] )^{2}·d_{tt}^{2}[x_{k}] = H_{kk}^{k} = d_{t}[ f_{k}(t) ]

( 1/d_{t}[x_{k}] ) = f_{k}(t)

( 1/f_{k}(t) ) = d_{t}[x_{k}]

x_{k}(t) = ( t /o(t)o/ int[ f_{k}(t) ]d[t] )

Teorema:

Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>

Si H_{kk}^{k} = k ==> x_{k}(t) = (1/k)·ln(t)

H_{ij}^{k} = (1/k)·ij

Demostración:

(-1)·( 1/d_{t}[x_{k}] )^{2}·d_{tt}^{2}[x_{k}] = H_{kk}^{k} = k

( 1/d_{t}[x_{k}] ) = kt

(1/(kt)) = d_{t}[x_{k}]

x_{k}(t) = (1/k)·ln(t)

Teorema:

Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>

Si H_{kk}^{k} = e^{kt} ==> x_{k}(t) = (-1)·e^{(-1)·kt}

H_{ij}^{k} = k^{2}·e^{(-1)·kt}·(1/(ij))·e^{it+jt}

Teorema:

Sea d_{tt}^{2}[x_{k}]+H_{ij}^{k}·d_{t}[x_{i}]·d_{t}[x_{j}] = 0 ==>

Si H_{kk}^{k} = t^{k} ==> x_{k}(t) = (-1)·( (k+1)/k )·t^{(-k)}

H_{ij}^{k} = (k+1)^{2}·t^{(-k)+(-2)}·(1/(i+1))·(1/(j+1))·t^{i+1+j+1}

Teorema:

Si f(x) = x+s ==> f(x) es un morfismo topológico

Demostración:

f(max{x,y}) = max{x,y}+s = max{x+s,y+s} = max{f(x),f(y)}

x+s [< y+s

x [< y

max{x+s,y+s} = y+s = max{x,y}+s

Ley:

Si y(t) = (-1)·(1/2)·(q/m)·gt^{2}+h ==> d_{t}[y] = ( (q/m)·2g·(h+(-y)) )^{(1/2)}

Ley:

Si y(t) = (-1)·(1/6)·(I/m)·gt^{3}+h ==> d_{t}[y] = (1/2)·( (I/m)^{(1/2)}·6g^{(1/2)}·(h+(-y)) )^{(2/3)}

Teorema:

Sea Q(x) = f(t) ==>

A(x,t) = P(x)+(-1)·h(t)·x [o(x)o] ( Q(x)+(-1)·f(t) )

h(t) = ( d_{x}[P(x)]/d_{x}[Q(x)] )

Demostración: [ por doble destrocter ponens ]

Si Q(x_{k}) = f(t) ==> d_{k}[ Q(x_{k})+(-1)·f(t) ] = d_{k}[ Q(x_{k}) ]

Si [EF][ F(x_{k}) = f(t) ] ==> [AF][ F(x_{k}) != f(t) ]

Estando en la falsedad.

Si [AG][ G(x_{k}) != h(t) ] ==> [EG][ G(x_{k}) = h(t) ]

Estando en la verdad.

Teorema:

Sea x = f(t) ==>

F(x,t) = x^{n+1}+(-1)·h(t)·x [o(x)o] ( x+(-1)·f(t) )

h(t) = (n+1)·( f(t) )^{n}

Teorema:

Sea x^{m} = f(t) ==>

F(x,t) = x^{n+1}+(-1)·h(t)·x [o(x)o] ( x^{m}+(-1)·f(t) )

h(t) = ( (n+1)/m )·( f(t) )^{( (n+1)/m )+(-1)}

Teorema:

int[ sum[k = 1]-[n][ x_{1}·...d_{t}[x_{k}]·...·x_{n}·d[t] ] ] = n·x_{1}·...·x_{n}

Demostración: [ por doble destrocter ponens ]

Si [En][ x_{n+1} = 1 ] ==> [An][ x_{n+1} != 1 ]

Estando en la falsedad.

Si [An][ n != n+1 ] ==> [En][ n = n+1 ]

Estando en la verdad.

int[ sum[k = 1]-[n+1][ x_{1}·...d_{t}[x_{k}]·...·x_{n+1}·d[t] ] ] = ...

int[ sum[k = 1]-[n][ x_{1}·...d_{t}[x_{k}]·...·x_{n}·d[t] ] ] = n·x_{1}·...·x_{n} = ...

n·x_{1}·...·x_{n}·x_{n+1} = (n+1)·x_{1}·...·x_{n}·x_{n+1}