Definición: [ de tensor de curvatura ]
R_{ijk}^{s}·d_{t}[x_{i}]·d_{t}[x_{j}]·d_{t}[x_{k}] = d_{t}[x_{s}]^{3}
Definición: [ de tensor de Cristoffel ]
R_{ij}^{s}·d_{t}[x_{i}]·d_{t}[x_{j}] = d_{t}[x_{s}]^{2}
Definición: [ de tensor de Ricci ]
R_{k}^{s}·d_{t}[x_{k}] = d_{t}[x_{s}]
Definición: [ de curvatura de un plano ]
R_{ijs}^{s}·d_{t}[x_{i}]·d_{t}[x_{j}] = d_{t}[x_{s}]^{2}
Definición: [ de curvatura de una recta ]
R_{ssk}^{s}·d_{t}[x_{k}] = d_{t}[x_{s}]
Teorema:
x_{s} = ( x_{i} [o(t)o] x_{j} [o(t)o] int[ R_{ijs}^{s} ]d[t] )^{[o(t)o](1/2)}
x_{s} = x_{k} [o(t)o] int[ R_{ssk}^{s} ]d[t]
Teorema:
Si R_{ijs}^{s} = 1 ==> x_{s} = ( x_{i} [o(t)o] x_{j} )^{[o(t)o](1/2)}
Si R_{ssk}^{s} = 1 ==> x_{s} = x_{k}
Teorema:
( R_{k}^{s} )^{3} = R_{kkk}^{s}
Teorema:
( R_{k}^{s} )^{2} = R_{kk}^{s}
Teorema:
R_{ijs}^{s} = R_{ij}^{s}
Teorema:
R_{ssk}^{s} = R_{k}^{s}
Teorema:
R_{sk}^{s} = R_{k}^{s}
Definición: [ de Métrica Bi-lineal ]
m_{ij} = d[x_{i}]·d[x_{j}]
Definición: [ de Métrica lineal ]
m_{k} = d[x_{k}]
Teorema:
m_{ij} = ( 1/R_{ij}^{s} )·d[x_{s}]d[x_{s}]
Teorema:
m_{ij} = ( 1/R_{ijs}^{s} )·d[x_{s}]d[x_{s}]
Teorema:
m_{k} = ( 1/R_{k}^{s} )·d[x_{s}]
Teorema:
m_{k} = ( 1/R_{ssk}^{s} )·d[x_{s}]
Ley: [ de Einstein Lagraniana de curvatura esférica interior ]
Es invariante Lorentz en la energía en reposo:
( 1/( 1+(-1)·(1/c)^{2}·(1/2)·sum[s = 1]-[3][ m_{ij}·R_{ijs}^{s} ] ) )·...
... m·sum[s = 1]-[3][ d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... sum[s = 1]-[3][ U(x_{s}) ]·d[t]d[t]
Deducción:
m·( d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ) = (m/2)·d_{t}[x_{s}]^{2}·d[t]d[t]
Ley: [ de Einstein Hamiltoniana de curvatura toroidal exterior ]
Es invariante Lorentz en la energía en reposo:
( 1/( 1+(-1)·(1/c)·(1/2)·sum[s = 1]-[3][ m_{k}·R_{ssk}^{s} ] ) )·...
... mc·sum[s = 1]-[3][ d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = sum[s = 1]-[3][ U(x_{s}) ]·d[t]
Deducción:
mc·( d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ) = (m/2)·c·d_{t}[x_{s}]·d[t]
Ley: [ de niebla en valle ]
m·sum[s = 1]-[3][ d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... qgh·sum[s = 1]-[3][ T_{s} ]·d[t]d[t]
T_{s} = ax_{s}
Ley: [ de niebla en montaña ]
m·sum[s = 1]-[3][ d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... qgh·sum[s = 1]-[3][ T_{s} ]·d[t]d[t]
T_{s} = (-1)·ax_{s}
Ley: [ de viento en valle ]
mc·sum[s = 1]-[3][ d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... qgh·sum[s = 1]-[3][ T_{s} ]·d[t]
T_{s} = ax_{s}
Ley: [ de viento en montaña ]
mc·sum[s = 1]-[3][ d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... qgh·sum[s = 1]-[3][ T_{s} ]·d[t]
T_{s} = (-1)·ax_{s}
Ley: [ de temporal en alta mar ]
m·sum[s = 1]-[3][ d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... d_{xyz}[q(x,y,z)]·Vgh·sum[s = 1]-[3][ T_{s} ]·d[t]d[t]
T_{s} = ax_{s}
Ley: [ de temporal en costa ]
m·sum[s = 1]-[3][ d[x_{s}]d[x_{s}]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... d_{xyz}[q(x,y,z)]·Vgh·sum[s = 1]-[3][ T_{s} ]·d[t]d[t]
T_{s} = (-1)·ax_{s}
Ley: [ de corriente submarina en abismo ]
mc·sum[s = 1]-[3][ d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... d_{xyz}[q(x,y,z)]·Vgh·sum[s = 1]-[3][ T_{s} ]·d[t]
T_{s} = ax_{s}
Ley: [ de corriente submarina en isla ]
mc·sum[s = 1]-[3][ d[x_{s}]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... d_{xyz}[q(x,y,z)]·Vgh·sum[s = 1]-[3][ T_{s} ]·d[t]
T_{s} = (-1)·ax_{s}
Irodov-Garriga problems de rotación en dos sistemas de coordenadas:
Ley: [ de Irodov ]
Sea d_{t}[x] = d_{t}[ r(t) ]+d_{t}[w]·( r(t) ) ==>
Si d_{t}[ r(t) ] = u·r(t) ==> ...
... d_{tt}^{2}[x] = re^{ut}·( u^{2}+d_{tt}^{2}[w]+d_{t}[w]·u )
Deducción:
r(t) = re^{ut}
Ley:
Sea d_{t}[x] = d_{t}[ r(t) ]+d_{t}[w]·( r(t) ) ==>
Si ( d_{t}[ r(t) ] = a·( y(t) )^{n+1} & d_{t}[y] = b·( 1/y(t) )^{n} ) ==> ...
... d_{tt}^{2}[x] = (n+1)·ab·( 1+d_{tt}^{2}[w]·(1/2)·t^{2}+d_{t}[w]·t )
Deducción:
( y(t) )^{n+1} = (n+1)·bt
Ley:
Sea d_{t}[x] = d_{t}[ r(t) ]+d_{t}[w]·( r(t) ) ==>
Si ( d_{t}[ r(t) ] = ve^{nay} & d_{t}[y] = ve^{(-n)·ay} ) ==> ...
... d_{tt}^{2}[x] = nav^{2}·( 1+d_{tt}^{2}[w]·(1/2)·t^{2}+d_{t}[w]·t )
Deducción:
e^{nay} = nav·t
Ley:
Sea d_{t}[x] = d_{t}[ r(t) ]+d_{t}[w]·( r(t) ) ==>
Si ( d_{t}[ r(t) ] = v·ln( ay(t) ) & d_{t}[y] = u·y(t) ) ==> ...
... d_{tt}^{2}[x] = vu·( 1+d_{tt}^{2}[w]·(1/2)·t^{2}+d_{t}[w]·t )
Deducción:
y(t) = (1/a)·e^{ut}
Ley:
Sea d_{t}[x] = d_{t}[ r(t) ]+d_{t}[w]·( r(t) ) ==>
Si ( d_{t}[ r(t) ] = a·( y(t) )^{n+1}·e^{ut} & d_{t}[y] = b·( 1/y(t) )^{n} ) ==> ...
... d_{tt}^{2}[x] = ...
... (n+1)·ab·( ( 1+ut )·e^{ut}+d_{tt}^{2}[w]·t^{2}·er-h[2](ut)+d_{t}[w]·t·e^{ut} )
Deducción:
( y(t) )^{n+1} = (n+1)·bt
Irodov-Garriga problems de cinemática:
Ley: [ de Irodov ]
Si d_{t}[x] = ax^{(1/2)} ==>
d_{tt}^{2}[x] = (1/2)·a^{2}
Ley:
Si ( d_{t}[x] = ax^{n} & d_{t}[y] = bx^{(-n)+1} ) ==>
d_{tt}^{2}[y] = ((-n)+1)·ab
Ley:
Si ( d_{t}[x] = (-v)·e^{nax} & d_{t}[y] = ve^{(-1)·nax} ) ==>
d_{tt}^{2}[y] = nav^{2}
Ley:
Si ( d_{t}[x] = ux & d_{t}[y] = v·ln(ax) ) ==>
d_{tt}^{2}[y] = uv
Ley: [ de Einstein-Srôdinguer Lagraniana ]
( 1/( 1+(-1)·(1/c)^{2}·(1/2)·sum[s = 1]-[3][ m_{ij}·R_{ijs}^{s} ] ) )·...
... (-1)·( h^{2}/m )·sum[s = 1]-[3][ d[f(x_{s})]d[f(x_{s})]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... sum[s = 1]-[3][ U( f(x_{s}) ) ]·d[x_{s}]d[x_{s}]
Deducción:
(-1)·( h^{2}/m )·( d[f(x_{s})]d[f(x_{s})]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ) = ...
... (-1)·( h^{2}/(2m) )·d_{x_{s}}[f(x_{s})]^{2}·d[x_{s}]d[x_{s}]
Ley: [ de la función de onda del fotón ]
f(x) = cx·cos(w)·cos(s)
f(y) = cy·sin(w)·cos(s)
f(z) = cz·sin(s)
( 1/( 1+(-1)·(1/c)^{2}·(1/2)·sum[s = 1]-[3][ m_{ij}·R_{ijs}^{s} ] ) )·...
... (-1)·( h^{2}/m )·sum[s = 1]-[3][ d[f(x_{s})]d[f(x_{s})]+(-1)·(1/2)·m_{ij}·R_{ijs}^{s} ] = ...
... sum[s = 1]-[3][ (-1)·( h^{2}/m )·( f(x_{s})/x_{s} )^{2} ]·d[x_{s}]d[x_{s}]
Ley: [ de Einstein-Heisenberg Lagraniana ]
( 1/( 1+(-1)·(1/c)^{2}·(1/2)·m_{ij}·R_{ij1}^{1} ) )·...
... (-1)·( h^{2}/(mc^{2}) )·( d[f(t)]d[f(t)]+(-1)·(1/2)·m_{ij}·R_{ij1}^{1} ) = U( f(t) )·d[t]d[t]
Deducción:
(-1)·( h^{2}/(mc^{2}) )·( d[f(t)]d[f(t)]+(-1)·(1/2)·m_{ij}·R_{ij1}^{1} ) = ...
... (-1)·( h^{2}/(2·mc^{2}) )·d_{t}[f(t)]^{2}·d[t]d[t]
Ley:
f(t) = ct
( 1/( 1+(-1)·(1/c)^{2}·(1/2)·m_{ij}·R_{ij1}^{1} ) )·...
... (-1)·( h^{2}/(mc^{2}) )·( d[f(t)]d[f(t)]+(-1)·(1/2)·m_{ij}·R_{ij1}^{1} ) = ...
... (-1)·( h^{2}/(mc^{2}) )·( f(t)/t )^{2}·d[t]d[t]
Ley: [ de Einstein-Heisenberg Hamiltoniana ]
( 1/( 1+(-1)·(1/c)·(1/2)·sum[s = 1]-[3][ m_{k}·R_{ssk}^{s} ] ) )·...
... ihc·sum[s = 1]-[3][ d[f(x_{s})]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... sum[s = 1]-[3][ U( f(x_{s}) ) ]·d[x_{s}]
Deducción:
ihc·( d[f(x_{s})]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ) = (1/2)·ihc·d_{x_{s}}[f(x_{s})]·d[x_{s}]
Ley: [ de la función de onda del fotón ]
f(x) = cx·( cos(w)·cos(s) )^{2}
f(y) = cy·( sin(w)·cos(s) )^{2}
f(z) = cz·( sin(s) )^{2}
( 1/( 1+(-1)·(1/c)·(1/2)·sum[s = 1]-[3][ m_{k}·R_{ssk}^{s} ] ) )·...
... ihc·sum[s = 1]-[3][ d[f(x_{s})]+(-1)·(1/2)·m_{k}·R_{ssk}^{s} ] = ...
... sum[s = 1]-[3][ ihc·(1/x_{s})·f(x_{s}) ]·d[x_{s}]
Ley: [ de Einstein-Srôdinguer Hamiltoniana ]
( 1/( 1+(-1)·(1/c)·(1/2)·m_{k}·R_{11k}^{1} ) )·...
... ih·( d[f(t)]+(-1)·(1/2)·m_{k}·R_{11k}^{1} ) = U( f(t) )·d[t]
Deducción:
ih·( d[f(t)]+(-1)·(1/2)·m_{k}·R_{11k}^{1} ) = (1/2)·ih·d_{t}[f(t)]·d[t]
Ley:
f(t) = ct
( 1/( 1+(-1)·(1/c)·(1/2)·m_{k}·R_{11k}^{1} ) )·...
... ih·( d[f(t)]+(-1)·(1/2)·m_{k}·R_{11k}^{1} ) = ih·(1/t)·f(t)·d[t]