gprMax/user_models/cylinder_2D_py.in

#python:
from gprMax.input_cmd_funcs import *
command('title', 'A or B scan from a metal cylinder buried in a dielectric half-space')
z_dim = 0.002
resolution = 0.002
tsim = 3e-9
B_scan = False

domain = domain(x=64e-2, y=30e-2, z=z_dim)
dx = dx_dy_dz(resolution, resolution, z_dim)
time_window(tsim)

material(permittivity=6, conductivity=0,
         permeability=1, magconductivity=0, name='half_space')

identifier = waveform('ricker', amplitude=1, frequency=1.5e9,
                      identifier='my_ricker')

if B_scan:
    x_ant = 8e-2
else:
    x_ant = domain.x/2 - 1e-2 # in the middle of the x-axis

tx = hertzian_dipole('z',
                     x_ant, domain.y - 4e-2, 0, # minus 4 cm in y-direction
                     identifier)
rx(tx.x + 2e-2, tx.y, tx.z)     # 2 cm away in x-direction from tx

if B_scan:
    src_steps(dx=0.8e-2/4)
    rx_steps(dx=0.8e-2/4)

b0, b1 = box(0, 0, 0,
             domain.x, domain.y - 4e-2, z_dim, # same as domain, minus 4 cm in y-direction
             'half_space')

c_x, c_y = (domain.x/2, b1.y - 5e-2) # in the middle of the x-axis and 5 cm down from the half_space
cylinder(c_x, c_y, 0,
         c_x, c_y, z_dim,
         radius=1e-2, material='pec')

# Outputs, geometry and snapshots
geometry_view(0, 0, 0,
              domain.x, domain.y, domain.z,
              dx.x, dx.y, dx.z,
              'cylinder', 'n')

N = 32
for i in range(1, N+1):
    snapshot(0, 0, 0,
             domain.x, domain.y, domain.z,
             dx.x, dx.y, dx.z, i*(tsim/N), 'snapshot' + str(i))
#end_python: