Esempio n. 1
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def _compute_parameters(k, a_0, a_f, inc_0, inc_f):
    """Compute parameters of the model.

    """
    delta_inc = abs(inc_f - inc_0)
    V_0 = circular_velocity(k, a_0)
    V_f = circular_velocity(k, a_f)
    beta_0_ = beta_0(V_0, V_f, inc_0, inc_f)

    return V_0, beta_0_, delta_inc
Esempio n. 2
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def _compute_parameters(k, a_0, a_f, inc_0, inc_f):
    """Compute parameters of the model.

    """
    delta_inc = abs(inc_f - inc_0)
    V_0 = circular_velocity(k, a_0)
    V_f = circular_velocity(k, a_f)
    beta_0_ = beta_0(V_0, V_f, inc_0, inc_f)

    return V_0, beta_0_, delta_inc
def plot_problem(k=398600.0, a_0=7000.0, a_f=42166.0, inc_0=np.radians(28.5), i_f=0.0, f=3.5e-7, t_f=200):
    """Plot interesting quantities.

    """
    t_domain = np.linspace(0, t_f, num=2000) * 86400  # s

    V_0 = circular_velocity(k, a_0)
    V_f = circular_velocity(k, a_f)

    beta_0_ = beta_0(V_0, V_f, inc_0, i_f)

    _, ax_l1 = plt.subplots()
    ax_l1.set_xlabel("Time, days")

    ax_l1.plot(t_domain / 86400, np.degrees(beta(
        t_domain,
        V_0=V_0,
        f=f,
        beta_0=beta_0_
    )), color='k', linestyle='solid')
    ax_l1.set_ylabel("Yaw, degrees")

    ax_r1 = ax_l1.twinx()
    ax_r1.plot(t_domain / 86400, 1e-3 * a(
        t_domain,
        k=k,
        V_0=V_0,
        f=f,
        beta_0=beta_0_
    ), color='k', linestyle='dashed')
    ax_r1.set_ylabel("Semimajor axis, km (thousands)")

    _, ax_l2 = plt.subplots()
    ax_l2.set_xlabel("Time, days")

    ax_l2.plot(t_domain / 86400, V(
        t_domain,
        V_0=V_0,
        f=f,
        beta_0=beta_0_
    ), color='k', linestyle='solid')
    ax_l2.set_ylabel("Velocity, km/s")

    ax_r2 = ax_l2.twinx()
    ax_r2.plot(t_domain / 86400, np.degrees(inc_0 - delta_inc(
        t_domain,
        V_0=V_0,
        f=f,
        beta_0=beta_0_
    )), color='k', linestyle='solid')
    ax_r2.set_ylabel("Inclination, degrees")

    return ax_l1, ax_r1, ax_l2, ax_r2
Esempio n. 4
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def plot_problem(k=398600.0,
                 a_0=7000.0,
                 a_f=42166.0,
                 inc_0=np.radians(28.5),
                 i_f=0.0,
                 f=3.5e-7,
                 t_f=200):
    """Plot interesting quantities.

    """
    t_domain = np.linspace(0, t_f, num=2000) * 86400  # s

    V_0 = circular_velocity(k, a_0)
    V_f = circular_velocity(k, a_f)

    beta_0_ = beta_0(V_0, V_f, inc_0, i_f)

    _, ax_l1 = plt.subplots()
    ax_l1.set_xlabel("Time, days")

    ax_l1.plot(t_domain / 86400,
               np.degrees(beta(t_domain, V_0=V_0, f=f, beta_0=beta_0_)),
               color='k',
               linestyle='solid')
    ax_l1.set_ylabel("Yaw, degrees")

    ax_r1 = ax_l1.twinx()
    ax_r1.plot(t_domain / 86400,
               1e-3 * a(t_domain, k=k, V_0=V_0, f=f, beta_0=beta_0_),
               color='k',
               linestyle='dashed')
    ax_r1.set_ylabel("Semimajor axis, km (thousands)")

    _, ax_l2 = plt.subplots()
    ax_l2.set_xlabel("Time, days")

    ax_l2.plot(t_domain / 86400,
               V(t_domain, V_0=V_0, f=f, beta_0=beta_0_),
               color='k',
               linestyle='solid')
    ax_l2.set_ylabel("Velocity, km/s")

    ax_r2 = ax_l2.twinx()
    ax_r2.plot(t_domain / 86400,
               np.degrees(inc_0 -
                          delta_inc(t_domain, V_0=V_0, f=f, beta_0=beta_0_)),
               color='k',
               linestyle='solid')
    ax_r2.set_ylabel("Inclination, degrees")

    return ax_l1, ax_r1, ax_l2, ax_r2
Esempio n. 5
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def test_simple_circular_velocity():
    k = 398600 * u.km**3 / u.s**2
    a = 7000 * u.km

    expected_V = 7.5460491 * u.km / u.s

    V = util.circular_velocity(k, a)

    assert_quantity_allclose(V, expected_V)
Esempio n. 6
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def extra_quantities(k, a, ecc, argp_0, argp_f, f, A=0.0):
    """Extra quantities given by the model.

    """
    V = circular_velocity(k, a)
    delta_V_ = delta_V(V, ecc, argp_0, argp_f, f, A)
    t_f_ = delta_V_ / f

    return delta_V_, t_f_
Esempio n. 7
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def extra_quantities(k, a, ecc, argp_0, argp_f, f, A=0.0):
    """Extra quantities given by the model.

    """
    V = circular_velocity(k, a)
    delta_V_ = delta_V(V, ecc, argp_0, argp_f, f, A)
    t_f_ = delta_V_ / f

    return delta_V_, t_f_
Esempio n. 8
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def test_simple_circular_velocity():
    k = 398600 * u.km ** 3 / u.s ** 2
    a = 7000 * u.km

    expected_V = 7.5460491 * u.km / u.s

    V = util.circular_velocity(k, a)

    assert_quantity_allclose(V, expected_V)
Esempio n. 9
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def extra_quantities(k, a, ecc_0, ecc_f, f):
    """Extra quantities given by the model.

    """
    V_0 = circular_velocity(k, a)
    delta_V_ = delta_V(V_0, ecc_0, ecc_f)
    t_f_ = delta_V_ / f

    return delta_V_, t_f_
Esempio n. 10
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def extra_quantities(k, a, ecc_0, ecc_f, inc_0, inc_f, argp, f):
    """Extra quantities given by the model.

    """
    beta_ = beta(ecc_0, ecc_f, inc_0, inc_f, argp)
    V_0 = circular_velocity(k, a)
    delta_V_ = delta_V(V_0, ecc_0, ecc_f, beta_)
    t_f_ = delta_V_ / f

    return delta_V_, beta_, t_f_
Esempio n. 11
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def main():
    # http://matplotlib.org/users/pgf.html#custom-preamble
    # http://sbillaudelle.de/2015/02/23/seamlessly-embedding-matplotlib-output-into-latex.html
    rc("pgf", rcfonts=False)
    rc("text", usetex=True)

    k = 398600
    a = 42164
    inc_domain = np.radians(np.linspace(0, 30))

    fig1, ax = plt.subplots(figsize=(6, 6))

    eccentricities = 0.1, 0.2, 0.4, 0.6, 0.8
    beta_data = np.zeros((inc_domain.shape[0], len(eccentricities)))
    for ii, ecc in enumerate(eccentricities):
        beta_data[:, ii] = beta(ecc, 0.0, 0.0, inc_domain, 0.0)
        ax.plot(np.degrees(inc_domain),
                np.degrees(beta_data[:, ii]),
                label="$e = %.1f$" % ecc)

    ax.set_xlabel("Inclination change (deg)")
    ax.set_ylabel(r"Yaw angle $|\beta| (deg)$")
    ax.set_xlim(0, 30)
    ax.set_ylim(0, 90)
    ax.grid(True)
    ax.legend()

    fig1.savefig("combined_ei/chart_beta.pgf")

    fig2, ax = plt.subplots(figsize=(6, 6))

    eccentricities = 0.1, 0.2, 0.4, 0.6, 0.8
    delta_V_data = np.zeros((inc_domain.shape[0], len(eccentricities)))
    for ii, ecc in enumerate(eccentricities):
        delta_V_data[:, ii] = delta_V(circular_velocity(k, a), ecc, 0.0,
                                      beta_data[:, ii])
        ax.plot(np.degrees(inc_domain),
                delta_V_data[:, ii],
                label="$e = %.1f$" % ecc)

    ax.set_xlabel("Inclination change (deg)")
    ax.set_ylabel(r"$\Delta V$ (km/s)")
    ax.set_xlim(0, 30)
    ax.set_ylim(0, 2.5)
    ax.grid(True)
    ax.legend()

    fig2.savefig("combined_ei/chart_dV.pgf")

    return fig1, fig2
def main():
    # http://matplotlib.org/users/pgf.html#custom-preamble
    # http://sbillaudelle.de/2015/02/23/seamlessly-embedding-matplotlib-output-into-latex.html
    rc("pgf", rcfonts=False)
    rc("text", usetex=True)

    k = 398600
    a = 42164
    inc_domain = np.radians(np.linspace(0, 30))

    fig1, ax = plt.subplots(figsize=(6, 6))

    eccentricities = 0.1, 0.2, 0.4, 0.6, 0.8
    beta_data = np.zeros((inc_domain.shape[0], len(eccentricities)))
    for ii, ecc in enumerate(eccentricities):
        beta_data[:, ii] = beta(ecc, 0.0, 0.0, inc_domain, 0.0)
        ax.plot(np.degrees(inc_domain), np.degrees(beta_data[:, ii]), label="$e = %.1f$" % ecc)

    ax.set_xlabel("Inclination change (deg)")
    ax.set_ylabel(r"Yaw angle $|\beta| (deg)$")
    ax.set_xlim(0, 30)
    ax.set_ylim(0, 90)
    ax.grid(True)
    ax.legend()

    fig1.savefig("combined_ei/chart_beta.pgf")

    fig2, ax = plt.subplots(figsize=(6, 6))

    eccentricities = 0.1, 0.2, 0.4, 0.6, 0.8
    delta_V_data = np.zeros((inc_domain.shape[0], len(eccentricities)))
    for ii, ecc in enumerate(eccentricities):
        delta_V_data[:, ii] = delta_V(circular_velocity(k, a), ecc, 0.0, beta_data[:, ii])
        ax.plot(np.degrees(inc_domain), delta_V_data[:, ii], label="$e = %.1f$" % ecc)

    ax.set_xlabel("Inclination change (deg)")
    ax.set_ylabel(r"$\Delta V$ (km/s)")
    ax.set_xlim(0, 30)
    ax.set_ylim(0, 2.5)
    ax.grid(True)
    ax.legend()

    fig2.savefig("combined_ei/chart_dV.pgf")

    return fig1, fig2