from ET import * B = Function('B') A = Function('A') t = Symbol('t') r = Symbol('r') theta = Symbol('theta') phi = Symbol('phi') g = Metric((-B(r), 0, 0, 0), (0, A(r), 0, 0), (0, 0, r**2, 0), (0, 0, 0, r**2 * sin(theta)**2)) x = (t, r, theta, phi) C = Christoffel(g, x) Rie = Riemann(C, x) Ric = Ricci(Rie, x) Rs = Rscalar(Ric) G = ET(Ric, g, Rs) print 'Initial metric:' pprint(g.matrix()) #C.nonzero() Ric.nonzero() #Rie.nonzero() #Rs.printing() G.nonzero() print 'Initial metric:' pprint(gdd) Gamma.nonzero() Ric.nonzero()
t=Symbol('t') r=Symbol('r') theta=Symbol('theta') phi=Symbol('phi') A= Function('A') K = Symbol('K') #general, spherically symmetric metric gdd=Matrix(( (-1,0,0,0), (0, A(t)/(1 - K*r**2), 0, 0), (0, 0, A(t)*r**2, 0), (0, 0, 0, A(t)*r**2*sin(theta)**2) )) g=Metric(gdd) x=(t,r,theta,phi) C=Christoffel(g,x) Rie = Riemann(C,x) Ric=Ricci( Rie,x) Rs =Rscalar(Ric) print 'Initial metric:' pprint(gdd) C.nonzero() Ric.nonzero() #Rie.nonzero() #Rs.printing()
theta=Symbol('theta') phi=Symbol('phi') #general, spherically symmetric metric gdd=Matrix(( (-B(r),0,0,0), (0, A(r), 0, 0), (0, 0, r**2, 0), (0, 0, 0, r**2*sin(theta)**2) )) g=Metric(gdd) X=(t,r,theta,phi) Gamma=Christoffel(g,X) Rie = Riemann(Gamma,X) Ric=Ricci(Rie,X) Rs =Rscalar(Ric) print 'Initial metric:' pprint(gdd) Gamma.nonzero() Ric.nonzero() #Rie.nonzero() Rs.printing() print '-'*40 #Solving EFE for A and B s = ( Ric.dd(1,1)/ A(r) ) + ( Ric.dd(0,0)/ B(r) ) pprint (s) t = dsolve(s, A(r))
r=Symbol('r') theta=Symbol('theta') phi=Symbol('phi') #general, spherically symmetric metric gdd=Matrix(( (-B(r),0,0,0), (0, A(r), 0, 0), (0, 0, r**2, 0), (0, 0, 0, r**2*sin(theta)**2) )) g=Metric(gdd) X=(t,r,theta,phi) Gamma=Christoffel(g,X) Ric=Ricci(Riemann(Gamma,X),X) def pprint_Gamma_udd(i,k,l): pprint(Eq(Symbol('Gamma^%i_%i%i' % (i,k,l)), Gamma.udd(i,k,l))) def pprint_Ric_dd(i,j): pprint(Eq(Symbol('R_%i%i' % (i,j)), Ric.dd(i,j))) print 'Initial metric:' pprint(gdd) print '-'*40 print 'Christoffel symbols:' for i in [0,1,2,3]: for k in [0,1,2,3]: for l in [0,1,2,3]: if Gamma.udd(i,k,l) != 0 :
import Ricci from sympy import * from sympy.abc import phi, theta coordinate = [theta, phi] g = Matrix([[1, 0], [0, sin(theta) * sin(theta)]]) S2 = Ricci.Ricci(coordinate, g) CF = S2.ChristoffelSymbol() print(CF)
from Christoffel import * from Riemann import * from Ricci import * from Rscalar import * t = Symbol('t') r = Symbol('r') theta = Symbol('theta') phi = Symbol('phi') A = Function('A') K = Symbol('K') #general, spherically symmetric metric gdd = Matrix(((-1, 0, 0, 0), (0, A(t) / (1 - K * r**2), 0, 0), (0, 0, A(t) * r**2, 0), (0, 0, 0, A(t) * r**2 * sin(theta)**2))) g = Metric(gdd) x = (t, r, theta, phi) C = Christoffel(g, x) Rie = Riemann(C, x) Ric = Ricci(Rie, x) Rs = Rscalar(Ric) print 'Initial metric:' pprint(gdd) C.nonzero() Ric.nonzero() #Rie.nonzero() #Rs.printing()
theta=Symbol('theta') phi=Symbol('phi') #general, spherically symmetric metric gdd=Matrix(( (-B(r),0,0,0), (0, A(r), 0, 0), (0, 0, r**2, 0), (0, 0, 0, r**2*sin(theta)**2) )) g=Metric(gdd) X=(t,r,theta,phi) Gamma=Christoffel(g,X) Rie = Riemann(Gamma,X) Ric=Ricci(Rie,X) print 'Initial metric:' pprint(gdd) print '-'*40 print 'Christoffel symbols:' for i in [0,1,2,3]: for k in [0,1,2,3]: for l in [0,1,2,3]: if Gamma.udd(i,k,l) != 0 : Gamma.printing(i,k,l) print'-'*40 print'Ricci tensor:' for i in [0,1,2,3]: for j in [0,1,2,3]: