jueves, 20 de febrero de 2025

funciones-elípticas y termodinámica y física-rotación y psiquiatría

Teorema:

sin[n](x) = sum[k_{i} = q & k_{j} = 1]-[oo][ ...

... (-1)^{k_{i}}·( 1/(2k_{1}...k_{n}+1)! )·x^{2k_{1}...k_{n}+1} ]+...

sum[k_{i} = q & k_{j} = p > 1]-[oo][ ...

... (-1)^{k_{i}}·( 3p^{n+(-1)}+(-1)·(2k_{i}+1)·p^{n+(-1)} )·...

... ( 1/(2k_{1}...k_{n}+p^{n+(-1)})! )·x^{2k_{1}...k_{n}+p^{n+(-1)}} ]

cos[n](x) = sum[k_{i} = q & k_{j} = 1]-[oo][ ...

... (-1)^{k_{i}}·( 1/(2k_{1}...k_{n})! )·x^{2k_{1}...k_{n}} ]+...

sum[k_{i} = q & k_{j} = p > 1]-[oo][ ...

... (-1)^{k_{i}}·( 2p^{n+(-1)}+(-1)·(2k_{i})·p^{n+(-1)} )·...

... ( 1/(2k_{1}...k_{n})! )·x^{2k_{1}...k_{n}} ]

Teorema:

(-1)·sin[n](x) = sum[j_{i} = q+(-1) & j_{j} = 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 1/(2j_{1}...j_{n}+1)! )·x^{2j_{1}...j_{n}+1} ]+...

sum[j_{i} = q+(-1) & j_{j} = p > 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 3p^{n+(-1)}+(-1)·(2j_{i}+1)·p^{n+(-1)} )·......

... ( 1/(2j_{1}...j_{n}+p^{n+(-1)})! )·x^{2j_{1}...j_{n}+p^{n+(-1)}} ]

(-1)·cos[n](x) = sum[j_{i} = q+(-1) & j_{j} = 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 1/(2j_{1}...j_{n})! )·x^{2j_{1}...j_{n}} ]+...

sum[j_{i} = q+(-1) & j_{j} = p > 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 2p^{n+(-1)}+(-1)·(2j_{i})·p^{n+(-1)} )·...

... ( 1/(2j_{1}...j_{n})! )·x^{2j_{1}...j_{n}} ]

Teorema:

Sea sn[0](x) = 0 ==>

sin[n](x) = n·sin(x)+sn[n+(-1)](x)

Sea cs[0](x) = 0 ==>

cos[n](x) = n·cos(x)+cs[n+(-1)](x)

Teorema:

d_{x}[ sn[n+(-1)](x) ] = cs[n+(-1)](x)

d_{x}[ cs[n+(-1)](x) ] = (-1)·sn[n+(-1)](x)

Teorema:

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

sum[j_{i} = q+(-1) & j_{j} = 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 1/(2j_{1}...j_{n}+2)! )·x^{2j_{1}...j_{n}+2} ]+...

sum[j_{i} = q+(-1) & j_{j} = p > 1]-[oo][ ...

... (-1)^{j_{i}+1}·( 1/(2j_{1}...j_{n}+2p^{n+(-1)})! )·x^{2j_{1}...j_{n}+2p^{n+(-1)}} ] ) = (-n)·(1/2)



Ley:

Sea d_{V}[P_{0}]·V^{2}+d_{P}[V_{0}]·P^{2} = kT ==>

Si d_{V}[ T(V,P) ]·v = qR ==> v = qR·( k/(2V) )·( 1/d_{V}[P_{0}] )

Si d_{P}[ T(V,P) ]·p = qR ==> p = qR·( k/(2P) )·( 1/d_{P}[V_{0}] )

Ley:

Sea d_{V}[P_{0}]·V^{2}+d_{P}[V_{0}]·P^{2} = kT ==>

Si d_{VV}^{2}[ T(V,P) ]·v^{2} = qR ==> v = ( qR·(k/2)·(1/d_{V}[P_{0}]) )^{(1/2)}

Si d_{PP}^{2}[ T(V,P) ]·p^{2} = qR ==> p = ( qR·(k/2)·(1/d_{P}[V_{0}]) )^{(1/2)}

Ley:

Sea d_{V}[P_{0}]·V^{2}+d_{P}[V_{0}]·P^{2} = kT ==>

Si d_{VV}^{2}[ T(V,P) ]·v^{2}+d_{V}[ T(V,P) ]·v = (1/2)·qR ==> ...

... v = (1/2)·( k/d_{V}[P_{0}] )·...

... ( (-1)·(V/k)·d_{V}[P_{0}]+( (V/k)^{2}·d_{V}[P_{0}]^{2}+(1/k)·d_{V}[P_{0}]·qR )^{(1/2)} )

Si d_{PP}^{2}[ T(V,P) ]·p^{2}+d_{P}[ T(V,P) ]·p = (1/2)·qR ==> ...

... p = (1/2)·( k/d_{P}[V_{0}] )·...

... ( (-1)·(P/k)·d_{P}[V_{0}]+( (P/k)^{2}·d_{P}[V_{0}]^{2}+(1/k)·d_{P}[V_{0}]·qR )^{(1/2)} )



Examen de termodinámica:

Ley:

Sea d_{VV}^{2}[P_{0}]·V^{3}+d_{PP}^{2}[V_{0}]·P^{3} = kT ==>

Si d_{V}[ T(V,P) ]·v = qR ==> v = ?

Si d_{P}[ T(V,P) ]·p = qR ==> p = ?

Ley:

Sea d_{VV}^{2}[P_{0}]·V^{3}+d_{PP}^{2}[V_{0}]·P^{3} = kT ==>

Si d_{VV}^{2}[ T(V,P) ]·v^{2} = qR ==> v = ?

Si d_{PP}^{2}[ T(V,P) ]·p^{2} = qR ==> p = ?

Ley:

Sea d_{VV}^{2}[P_{0}]·V^{3}+d_{PP}^{2}[V_{0}]·P^{3} = kT ==>

Si d_{VV}^{2}[ T(V,P) ]·v^{2}+d_{V}[ T(V,P) ]·v = (3/8)·qR ==> v = ?

Si d_{PP}^{2}[ T(V,P) ]·p^{2}+d_{P}[ T(V,P) ]·p = (3/8)·qR ==> p = ?



Ley: [ de la Luz del Técnics ]

Sea m·d_{t}[x]^{2} = Fr ==>

Si d_{t}[y] = d_{t}[x]+d_{t}[w]·r ==> ...

... ( d_{t}[y] = 0 <==> d_{t}[w] = (-1)·( (F/m)·(1/r) )^{(1/2)} )

Ley: [ de aguja de Técnics con pitch negativo ]

Sea m·d_{t}[x]^{2} = Fr  & d_{t}[h(t)] = a·h(t) ==>

Si d_{t}[y] = d_{t}[x]+d_{t}[w]·h(t) ==> ...

... ( d_{tt}^{2}[y] = 0 <==> d_{t}[w] = ue^{(-a)·t} )

... d_{t}[y] = ( (F/m)·r )^{(1/2)}+uh

... ( d_{t}[y] = 0 <==> u = (-1)·(1/h)·( (F/m)·r )^{(1/2)} )

Ley: [ de aguja de Técnics con pitch positivo ]

Sea m·d_{t}[x]^{2} = Fr  & d_{t}[h(t)] = (-a)·h(t) ==>

Si d_{t}[y] = d_{t}[x]+d_{t}[w]·h(t) ==> ...

... ( d_{tt}^{2}[y] = 0 <==> d_{t}[w] = ue^{at} )

... d_{t}[y] = ( (F/m)·r )^{(1/2)}+uh

... ( d_{t}[y] = 0 <==> u = (-1)·(1/h)·( (F/m)·r )^{(1/2)} )

Ley: [ de aguja de Técnics orto-fone ]

Sea m·d_{t}[x]^{2} = Fr  & d_{t}[h(t)]^{2} = ar·h(t) ==>

Si d_{t}[y] = d_{t}[x]+d_{t}[w]·h^{(1/2)}·( h(t) )^{(1/2)} ==> ...

... ( d_{tt}^{2}[y] = 0 <==> w(t) = (-1)·ln(ut)

... d_{t}[y] = ( (F/m)·r )^{(1/2)}+(-1)·(1/2)·(arh)^{(1/2)}

... ( d_{t}[y] = 0 <==> a = (F/m)·(1/h) )



No entiendo porque enfadar-se tanto Francisco,

de querer matar-me para siempre,

por hacer-le un txotxo bonito con el dual del Jalisco.

Y no quiere matar al que le está diciendo que un Jalisco es una pitxa,

en vez de un txotxo para tener un txotxo bueno.

El o la que dice que un Jalisco es una pitxa ni se ha visto,

que ha mutado su sexo a algo muy feo seguro.

Ley:

La mujeres que se creen que un Jalisco es una pitxa,

mutan a un clítoris pitxa que todos hemos visto.

Los hombres que se creen que un Jalisca es un txotxo,

mutan a unos cojones enormes que todos hemos visto como txotxo.



Ley:

No salir de casa,

robando la libertad.

No dutxar-se,

robando la intimidad.

Anexo:

Esta enfermedad la tengo yo.

Ley:

No usar tecnología escrita,

robando la libertad en imagen.

No usar tecnología auditiva,

robando la libertar en sonido.

Anexo:

Esta enfermedad la tiene mi amigo Dj.Voltio,

y tiene que tener pensión.

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