コード例 #1
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
    def test2D(potential, field):
        potAccept2D = np.zeros((NX_2D + 1, NY_2D + 1))
        fieldAccept2D = np.zeros((NX_2D + 1, NY_2D + 1, 2))
        for i, j in np.ndindex(potAccept2D.shape):
            potAccept2D[i, j] = potential(X0_2D + DX_2D * i, Y0_2D + DY_2D * j)
            fieldAccept2D[i, j] = field(X0_2D + DX_2D * i, Y0_2D + DY_2D * j)

        test(esSolve.potentialToElectricField(potAccept2D, [DX_2D, DY_2D]),
             fieldAccept2D)
コード例 #2
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
    def test1D(potential, field):
        potAccept1D = np.zeros(NX_1D + 1)
        fieldAccept1D = np.zeros((NX_1D + 1, 1))
        for i in range(NX_1D + 1):
            potAccept1D[i] = potential(X0_1D + DX_1D * i)
            fieldAccept1D[i] = field(X0_1D + DX_1D * i)

        test(esSolve.potentialToElectricField(potAccept1D, [DX_1D]),
             fieldAccept1D)
コード例 #3
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
 def test2D(potential,field):
   potAccept2D   = np.zeros((NX_2D+1,NY_2D+1))
   fieldAccept2D = np.zeros((NX_2D+1,NY_2D+1,2))
   for i,j in np.ndindex(potAccept2D.shape):
     potAccept2D[i,j]   = potential(X0_2D+DX_2D*i,Y0_2D+DY_2D*j)
     fieldAccept2D[i,j] = field(    X0_2D+DX_2D*i,Y0_2D+DY_2D*j)
   
   test(esSolve.potentialToElectricField(potAccept2D,[DX_2D,DY_2D]),
        fieldAccept2D)
コード例 #4
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
  def test1D(potential,field):
    potAccept1D   = np.zeros(NX_1D+1)
    fieldAccept1D = np.zeros((NX_1D+1,1))
    for i in range(NX_1D+1):
      potAccept1D[i]   = potential(X0_1D+DX_1D*i)
      fieldAccept1D[i] = field(    X0_1D+DX_1D*i)

    test(esSolve.potentialToElectricField(potAccept1D,[DX_1D]),
         fieldAccept1D)
コード例 #5
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
 def test3D(potential,field):
   potAccept3D   = np.zeros((NX_3D+1,NY_3D+1,NZ_3D+1))
   fieldAccept3D = np.zeros((NX_3D+1,NY_3D+1,NZ_3D+1,3))
   for i,j,k in np.ndindex(potAccept3D.shape):
     # consider using np.fromfunction here
     potAccept3D[i,j,k]   = potential(X0_3D+DX_3D*i,Y0_3D+DY_3D*j,Z0_3D+DZ_3D*k)
     fieldAccept3D[i,j,k] = field(    X0_3D+DX_3D*i,Y0_3D+DY_3D*j,Z0_3D+DZ_3D*k)
   
   test(esSolve.potentialToElectricField(potAccept3D,[DX_3D,DY_3D,DZ_3D]),
        fieldAccept3D)
コード例 #6
0
ファイル: testEsSolve.py プロジェクト: ericangle/esPic
    def test3D(potential, field):
        potAccept3D = np.zeros((NX_3D + 1, NY_3D + 1, NZ_3D + 1))
        fieldAccept3D = np.zeros((NX_3D + 1, NY_3D + 1, NZ_3D + 1, 3))
        for i, j, k in np.ndindex(potAccept3D.shape):
            # consider using np.fromfunction here
            potAccept3D[i, j,
                        k] = potential(X0_3D + DX_3D * i, Y0_3D + DY_3D * j,
                                       Z0_3D + DZ_3D * k)
            fieldAccept3D[i, j,
                          k] = field(X0_3D + DX_3D * i, Y0_3D + DY_3D * j,
                                     Z0_3D + DZ_3D * k)

        test(
            esSolve.potentialToElectricField(potAccept3D,
                                             [DX_3D, DY_3D, DZ_3D]),
            fieldAccept3D)
コード例 #7
0
                             VN_NR,
                             "gaussSeidel",
                             relTol=0.0,
                             absTol=1.0e-3 * (deltaV_NR),
                             useCython=False)
pot1D_R = esSolve.laplace1D(NX,
                            DX,
                            V0,
                            VN_R,
                            "gaussSeidel",
                            relTol=0.0,
                            absTol=1.0e-3 * (deltaV_R),
                            useCython=False)

# Compute E = - grad V on grid
electricFieldOnGrid_NR = esSolve.potentialToElectricField(pot1D_NR, [DX])
electricFieldOnGrid_R = esSolve.potentialToElectricField(pot1D_R, [DX])

positions_NR = [electron_NR.position[0]]
velocities_NR = [electron_NR.velocity[0]]
positions_R_Rpush = [electron_R_Rpush.position[0]]
velocities_R_Rpush = [electron_R_Rpush.velocity[0]]
positions_R_NRpush = [electron_R_NRpush.position[0]]
velocities_R_NRpush = [electron_R_NRpush.velocity[0]]

for step in xrange(steps + 1):
    # Compute E at particle position
    electricFieldAtPoint_NR = esSolve.electricFieldAtPoint(
        electricFieldOnGrid_NR, [DX], [X0], electron_NR.position)
    electricFieldAtPoint_R_Rpush = esSolve.electricFieldAtPoint(
        electricFieldOnGrid_R, [DX], [X0], electron_R_Rpush.position)
コード例 #8
0
ファイル: ex_1d_particles.py プロジェクト: ericangle/esPic
electron_R_Rpush  = particle(mass,charge,[X0_particle],[V0_particle])
electron_R_NRpush = particle(mass,charge,[X0_particle],[V0_particle])

# Time steps
T_NR  = 0.99*pow(-2.0*mass*pow(LX,2.0)/(charge*deltaV_NR),0.5)
T_R   = 0.99*pow(-2.0*mass*pow(LX,2.0)/(charge*deltaV_R),0.5)
steps = 100
DT_NR = T_NR/steps
DT_R  = T_R/steps

# Solve for potential
pot1D_NR = esSolve.laplace1D(NX,DX,V0,VN_NR,"gaussSeidel",relTol=0.0,absTol=1.0e-3*(deltaV_NR),useCython=False)
pot1D_R  = esSolve.laplace1D(NX,DX,V0,VN_R,"gaussSeidel",relTol=0.0,absTol=1.0e-3*(deltaV_R),useCython=False)

# Compute E = - grad V on grid
electricFieldOnGrid_NR = esSolve.potentialToElectricField(pot1D_NR,[DX])
electricFieldOnGrid_R  = esSolve.potentialToElectricField(pot1D_R,[DX])
 
positions_NR        = [electron_NR.position[0]]
velocities_NR       = [electron_NR.velocity[0]]
positions_R_Rpush   = [electron_R_Rpush.position[0]]
velocities_R_Rpush  = [electron_R_Rpush.velocity[0]]
positions_R_NRpush  = [electron_R_NRpush.position[0]]
velocities_R_NRpush = [electron_R_NRpush.velocity[0]]

for step in xrange(steps+1):
  # Compute E at particle position
  electricFieldAtPoint_NR       = esSolve.electricFieldAtPoint(electricFieldOnGrid_NR,[DX],[X0],electron_NR.position)
  electricFieldAtPoint_R_Rpush  = esSolve.electricFieldAtPoint(electricFieldOnGrid_R,[DX],[X0],electron_R_Rpush.position)
  electricFieldAtPoint_R_NRpush = esSolve.electricFieldAtPoint(electricFieldOnGrid_R,[DX],[X0],electron_R_NRpush.position)