gprMax/tests/analytical_solutions.py

import numpy as np

from gprMax.constants import c, e0
from gprMax.utilities import rvalue
from gprMax.waveforms import Waveform


def hertzian_dipole_fs(timewindow, dt, dxdydz, rx):
    """Analytical solution of a z-directed Hertzian dipole in free space with a Gaussian current waveform (http://dx.doi.org/10.1016/0021-9991(83)90103-1).
    
    Args:
        timewindow (float): Length of time window (seconds).
        dt (float): Time step (seconds).
        dxdydz (float): Tuple of spatial resolution (metres).
        rx (float): Tuple of coordinates of receiver position relative to transmitter position (metres).
        
    Returns:
        fields (float): Array contain electric and magnetic field components.
    """

    # Waveform
    w = Waveform()
    w.type = 'gaussiandot'
    w.amp = 1
    w.freq = 1e9
    
    # Waveform integral
    wint = Waveform()
    wint.type = 'gaussian'
    wint.amp = w.amp
    wint.freq = w.freq

    # Waveform first derivative
    wdot = Waveform()
    wdot.type = 'gaussiandotdot'
    wdot.amp = w.amp
    wdot.freq = w.freq

    # Time
    iterations = rvalue(timewindow / dt)
    time = np.linspace(0, timewindow, iterations)

    # Spatial resolution
    dx = dxdydz[0]
    dy = dxdydz[1]
    dz = dxdydz[2]

    # Coordinates of Rx relative to Tx
    x = rx[0]
    y = rx[1]
    z = rx[2]
    if z == 0:
        sign_z = 1
    else:
        sign_z = np.sign(z)

    # Coordinates of Rx for Ex FDTD component
    Ex_x = x + 0.5 * dx
    Ex_y = y
    Ex_z = z - 0.5 * dz
    Er_x = np.sqrt((Ex_x**2 + Ex_y**2 + Ex_z**2))
    tau_Ex = Er_x / c

    # Coordinates of Rx for Ey FDTD component
    Ey_x = x
    Ey_y = y + 0.5 * dy
    Ey_z = z - 0.5 * dz
    Er_y = np.sqrt((Ey_x**2 + Ey_y**2 + Ey_z**2))
    tau_Ey = Er_y / c

    # Coordinates of Rx for Ez FDTD component
    Ez_x = x
    Ez_y = y
    Ez_z = z
    Er_z = np.sqrt((Ez_x**2 + Ez_y**2 + Ez_z**2))
    tau_Ez = Er_z / c

    # Coordinates of Rx for Hx FDTD component
    Hx_x = x
    Hx_y = y + 0.5 * dy
    Hx_z = z
    Hr_x = np.sqrt((Hx_x**2 + Hx_y**2 + Hx_z**2))
    tau_Hx = Hr_x / c

    # Coordinates of Rx for Hy FDTD component
    Hy_x = x + 0.5 * dx
    Hy_y = y
    Hy_z = z
    Hr_y = np.sqrt((Hy_x**2 + Hy_y**2 + Hy_z**2))
    tau_Hy = Hr_y / c

    # Coordinates of Rx for Hz FDTD component
    Hz_x = x + 0.5 * dx
    Hz_y = y + 0.5 * dy
    Hz_z = z - 0.5 * dz
    Hr_z = np.sqrt((Hz_x**2 + Hz_y**2 + Hz_z**2))
    tau_Hz = Hr_z / c

    # Initialise fields
    fields = np.zeros((iterations, 6))

    # Calculate fields
    for timestep in range(iterations):
        
        # Calculate values for waveform
        fint_Ex = wint.calculate_value((timestep * dt) - tau_Ex, dt) * dx
        f_Ex = w.calculate_value((timestep * dt) - tau_Ex, dt) * dx
        fdot_Ex = wdot.calculate_value((timestep * dt) - tau_Ex, dt) * dx
        
        fint_Ey = wint.calculate_value((timestep * dt) - tau_Ey, dt) * dy
        f_Ey= w.calculate_value((timestep * dt) - tau_Ey, dt) * dy
        fdot_Ey = wdot.calculate_value((timestep * dt) - tau_Ey, dt) * dy
        
        fint_Ez = wint.calculate_value((timestep * dt) - tau_Ez, dt) * dz
        f_Ez = w.calculate_value((timestep * dt) - tau_Ez, dt) * dz
        fdot_Ez = wdot.calculate_value((timestep * dt) - tau_Ez, dt) * dz
        
        fint_Hx = wint.calculate_value((timestep * dt) - tau_Hx, dt) * dx
        f_Hx = w.calculate_value((timestep * dt) - tau_Hx, dt) * dx
        fdot_Hx = wdot.calculate_value((timestep * dt) - tau_Hx, dt) * dx
        
        fint_Hy = wint.calculate_value((timestep * dt) - tau_Hy, dt) * dy
        f_Hy= w.calculate_value((timestep * dt) - tau_Hy, dt) * dy
        fdot_Hy = wdot.calculate_value((timestep * dt) - tau_Hy, dt) * dy
        
        fint_Hz = wint.calculate_value((timestep * dt) - tau_Hz, dt) * dz
        f_Hz = w.calculate_value((timestep * dt) - tau_Hz, dt) * dz
        fdot_Hz = wdot.calculate_value((timestep * dt) - tau_Hz, dt) * dz
        
        # Ex
        fields[timestep, 0] = ((Ex_x * Ex_z) / (4 * np.pi * e0 * Er_x**5)) * (3 * (fint_Ex + (tau_Ex * f_Ex)) + (tau_Ex**2 * fdot_Ex))
        
        # Ey
        try:
            tmp = Ey_y / Ey_x
        except ZeroDivisionError:
            tmp = 0
        fields[timestep, 1] = tmp * ((Ey_x * Ey_z) / (4 * np.pi * e0 * Er_y**5)) * (3 * (fint_Ey + (tau_Ey * f_Ey)) + (tau_Ey**2 * fdot_Ey))

        # Ez
        fields[timestep, 2] = (1 / (4 * np.pi * e0 * Er_z**5)) * ((2 * Ez_z**2 - (Ez_x**2 + Ez_y**2)) * (fint_Ez + (tau_Ez * f_Ez)) - (Ez_x**2 + Ez_y**2) * tau_Ez**2 * fdot_Ez)

        # Hx
        fields[timestep, 3] = - (Hx_y / (4 * np.pi * Hr_x**3)) * (f_Hx + (tau_Hx * fdot_Hx))

        # Hy
        try:
            tmp = Hy_x / Hy_y
        except ZeroDivisionError:
            tmp = 0
        fields[timestep, 4] = - tmp * (- (Hy_y / (4 * np.pi * Hr_y**3)) * (f_Hy + (tau_Hy * fdot_Hy)))

        # Hz
        fields[timestep, 5] = 0

    return fields