コード例 #1
1
def _kepler(k, r0, v0, tof, numiter, rtol):
    # Cache some results
    dot_r0v0 = np.dot(r0, v0)
    norm_r0 = np.dot(r0, r0)**.5
    sqrt_mu = k**.5
    alpha = -np.dot(v0, v0) / k + 2 / norm_r0

    # First guess
    if alpha > 0:
        # Elliptic orbit
        xi_new = sqrt_mu * tof * alpha
    elif alpha < 0:
        # Hyperbolic orbit
        xi_new = (np.sign(tof) * (-1 / alpha)**.5 * np.log(
            (-2 * k * alpha * tof) /
            (dot_r0v0 + np.sign(tof) * np.sqrt(-k / alpha) *
             (1 - norm_r0 * alpha))))
    else:
        # Parabolic orbit
        # (Conservative initial guess)
        xi_new = sqrt_mu * tof / norm_r0

    # Newton-Raphson iteration on the Kepler equation
    count = 0
    while count < numiter:
        xi = xi_new
        psi = xi * xi * alpha
        c2_psi = c2(psi)
        c3_psi = c3(psi)
        norm_r = (xi * xi * c2_psi + dot_r0v0 / sqrt_mu * xi *
                  (1 - psi * c3_psi) + norm_r0 * (1 - psi * c2_psi))
        xi_new = xi + (sqrt_mu * tof - xi * xi * xi * c3_psi -
                       dot_r0v0 / sqrt_mu * xi * xi * c2_psi - norm_r0 * xi *
                       (1 - psi * c3_psi)) / norm_r
        if abs(np.divide(xi_new - xi,
                         xi_new)) < rtol or abs(xi_new - xi) < rtol:
            break
        else:
            count += 1
    else:
        raise RuntimeError("Maximum number of iterations reached")

    # Compute Lagrange coefficients
    f = 1 - xi**2 / norm_r0 * c2_psi
    g = tof - xi**3 / sqrt_mu * c3_psi

    gdot = 1 - xi**2 / norm_r * c2_psi
    fdot = sqrt_mu / (norm_r * norm_r0) * xi * (psi * c3_psi - 1)

    return f, g, fdot, gdot
コード例 #2
0
def _lambert(k, r0, r, tof, short, numiter, rtol):
    if short:
        t_m = +1
    else:
        t_m = -1

    norm_r0 = np.dot(r0, r0)**.5
    norm_r = np.dot(r, r)**.5
    norm_r0_times_norm_r = norm_r0 * norm_r
    norm_r0_plus_norm_r = norm_r0 + norm_r

    cos_dnu = np.dot(r0, r) / norm_r0_times_norm_r

    A = t_m * (norm_r * norm_r0 * (1 + cos_dnu))**.5

    if A == 0.0:
        raise RuntimeError("Cannot compute orbit, phase angle is 180 degrees")

    psi = 0.0
    psi_low = -4 * np.pi
    psi_up = 4 * np.pi

    count = 0

    while count < numiter:
        y = norm_r0_plus_norm_r + A * (psi * c3(psi) - 1) / c2(psi)**.5
        if A > 0.0:
            # Readjust xi_low until y > 0.0
            # Translated directly from Vallado
            while y < 0.0:
                psi_low = psi
                psi = (0.8 * (1.0 / c3(psi)) *
                       (1.0 - norm_r0_times_norm_r * np.sqrt(c2(psi)) / A))
                y = norm_r0_plus_norm_r + A * (psi * c3(psi) - 1) / c2(psi)**.5

        xi = np.sqrt(y / c2(psi))
        tof_new = (xi**3 * c3(psi) + A * np.sqrt(y)) / np.sqrt(k)

        # Convergence check
        if np.abs((tof_new - tof) / tof) < rtol:
            break
        count += 1
        # Bisection check
        condition = (tof_new <= tof)
        psi_low = psi_low + (psi - psi_low) * condition
        psi_up = psi_up + (psi - psi_up) * (not condition)

        psi = (psi_up + psi_low) / 2
    else:
        raise RuntimeError("Maximum number of iterations reached")

    f = 1 - y / norm_r0
    g = A * np.sqrt(y / k)

    gdot = 1 - y / norm_r

    v0 = (r - f * r0) / g
    v = (gdot * r - r0) / g

    return v0, v
コード例 #3
0
def _lambert(k, r0, r, tof, short, numiter, rtol):
    if short:
        t_m = +1
    else:
        t_m = -1

    norm_r0 = np.dot(r0, r0)**.5
    norm_r = np.dot(r, r)**.5
    cos_dnu = np.dot(r0, r) / (norm_r0 * norm_r)

    A = t_m * (norm_r * norm_r0 * (1 + cos_dnu))**.5

    if A == 0.0:
        raise RuntimeError("Cannot compute orbit, phase angle is 180 degrees")

    psi = 0.0
    psi_low = -4 * np.pi
    psi_up = 4 * np.pi

    count = 0
    while count < numiter:
        y = norm_r0 + norm_r + A * (psi * c3(psi) - 1) / c2(psi)**.5
        if A > 0.0 and y < 0.0:
            # Readjust xi_low until y > 0.0
            # Translated directly from Vallado
            while y < 0.0:
                psi_low = psi
                psi = (0.8 * (1.0 / c3(psi)) *
                       (1.0 - (norm_r0 + norm_r) * np.sqrt(c2(psi)) / A))
                y = norm_r0 + norm_r + A * (psi * c3(psi) - 1) / c2(psi)**.5

        xi = np.sqrt(y / c2(psi))
        tof_new = (xi**3 * c3(psi) + A * np.sqrt(y)) / np.sqrt(k)

        # Convergence check
        if np.abs((tof_new - tof) / tof) < rtol:
            break
        else:
            count += 1
            # Bisection check
            if tof_new <= tof:
                psi_low = psi
            else:
                psi_up = psi
            psi = (psi_up + psi_low) / 2
    else:
        raise RuntimeError("Maximum number of iterations reached")

    f = 1 - y / norm_r0
    g = A * np.sqrt(y / k)

    gdot = 1 - y / norm_r

    v0 = (r - f * r0) / g
    v = (gdot * r - r0) / g

    return v0, v
コード例 #4
0
ファイル: test_stumpff.py プロジェクト: huleg/poliastro
def test_stumpff_functions_near_zero():
    psi = 0.5
    expected_c2 = (1 - cos(psi**.5)) / psi
    expected_c3 = (psi**.5 - sin(psi**.5)) / psi**1.5

    assert_almost_equal(c2(psi), expected_c2)
    assert_almost_equal(c3(psi), expected_c3)
コード例 #5
0
ファイル: test_stumpff.py プロジェクト: huleg/poliastro
def test_stumpff_functions_under_zero():
    psi = -3.0
    expected_c2 = (cosh((-psi)**.5) - 1) / (-psi)
    expected_c3 = (sinh((-psi)**.5) - (-psi)**.5) / (-psi)**1.5

    assert_equal(c2(psi), expected_c2)
    assert_equal(c3(psi), expected_c3)
コード例 #6
0
ファイル: test_stumpff.py プロジェクト: huleg/poliastro
def test_stumpff_functions_above_zero():
    psi = 3.0
    expected_c2 = (1 - cos(psi**.5)) / psi
    expected_c3 = (psi**.5 - sin(psi**.5)) / psi**1.5

    assert_equal(c2(psi), expected_c2)
    assert_equal(c3(psi), expected_c3)
コード例 #7
0
ファイル: propagation.py プロジェクト: yothinix/poliastro
def _kepler(k, r0, v0, tof, numiter, rtol):
    # Cache some results
    dot_r0v0 = dot(r0, v0)
    norm_r0 = dot(r0, r0) ** .5
    sqrt_mu = k**.5
    alpha = -dot(v0, v0) / k + 2 / norm_r0

    # First guess
    if alpha > 0:
        # Elliptic orbit
        xi_new = sqrt_mu * tof * alpha
    elif alpha < 0:
        # Hyperbolic orbit
        xi_new = (np.sign(tof) * (-1 / alpha)**.5 *
                  np.log((-2 * k * alpha * tof) /
                         (dot_r0v0 + np.sign(tof) *
                          np.sqrt(-k / alpha) * (1 - norm_r0 * alpha))))
    else:
        # Parabolic orbit
        # (Conservative initial guess)
        xi_new = sqrt_mu * tof / norm_r0

    # Newton-Raphson iteration on the Kepler equation
    count = 0
    while count < numiter:
        xi = xi_new
        psi = xi * xi * alpha
        c2_psi = c2(psi)
        c3_psi = c3(psi)
        norm_r = (xi * xi * c2_psi +
                  dot_r0v0 / sqrt_mu * xi * (1 - psi * c3_psi) +
                  norm_r0 * (1 - psi * c2_psi))
        xi_new = xi + (sqrt_mu * tof - xi * xi * xi * c3_psi -
                       dot_r0v0 / sqrt_mu * xi * xi * c2_psi -
                       norm_r0 * xi * (1 - psi * c3_psi)) / norm_r
        if abs(np.divide(xi_new - xi, xi_new)) < rtol or abs(xi_new - xi) < rtol:
            break
        else:
            count += 1
    else:
        raise RuntimeError("Maximum number of iterations reached")

    # Compute Lagrange coefficients
    f = 1 - xi**2 / norm_r0 * c2_psi
    g = tof - xi**3 / sqrt_mu * c3_psi

    gdot = 1 - xi**2 / norm_r * c2_psi
    fdot = sqrt_mu / (norm_r * norm_r0) * xi * (psi * c3_psi - 1)

    return f, g, fdot, gdot