Beispiel #1
0
    def __init__(self, return_states=False, use_penalty=False):
        # self.dyn = Dynamics(dt=0.02)
        self.fw = FixedWing()
        self.x0 = self.fw._start
        self.dt = 0.01
        self.Q = np.diag([0, 0, 100, 0, 0, 0, 50, 50, 50, 0, 0, 0])
        # self.Qf = np.array([10,10,100,4.5,4.5,5,0.8,0.8,1])
        # self.x0 = np.array([0,0,-5.,0,0,0,0,0,0])
        # self.x_des = self.x0.copy()

        phi0 = 0.0  # roll angle
        theta0 = 0.  # pitch angle
        psi0 = 0.0  # yaw angle

        e = Euler2Quaternion(phi0, theta0, psi0, 1)
        e0 = e.item(0)
        e1 = e.item(1)
        e2 = e.item(2)
        e3 = e.item(3)

        self.x_des = np.array([
            [0],  # (0)
            [0],  # (1)
            [-100],  # (2)
            [25],  # (3)
            [0],  # (4)
            [0],  # (5)
            [e0],  # (6)
            [e1],  # (7)
            [e2],  # (8)
            [e3],  # (9)
            [0],  # (10)
            [0],  # (11)
            [0]
        ])  # (12)

        # self.initialized = False
        self.return_states = return_states
        w_max = np.pi / 1.5
        self.u_max = np.array([w_max, w_max, 1, w_max])
        self.u_min = np.array([-w_max, -w_max, 0, -w_max])
        self.mu = 10.
#   Initial conditions for MAV
pn0 = 0.  # initial north position
pe0 = 0.  # initial east position
pd0 = -100.0  # initial down position
u0 = 4.  # initial velocity along body x-axis
v0 = 0.  # initial velocity along body y-axis
w0 = 0.  # initial velocity along body z-axis
phi0 = 0.  # initial roll angle
theta0 =  0.  # initial pitch angle
psi0 = 0.0  # initial yaw angle
p0 = 0  # initial roll rate
q0 = 0  # initial pitch rate
r0 = 0  # initial yaw rate
Va0 = np.sqrt(u0**2+v0**2+w0**2)
#   Quaternion State
e = Euler2Quaternion(phi0, theta0, psi0, 1)
e0 = e.item(0)
e1 = e.item(1)
e2 = e.item(2)
e3 = e.item(3)


######################################################################################
                #   Physical Parameters
######################################################################################
mass = 0.015 #kg
Jx = 0.00002 #kg m^2
Jy = 0.0001
Jz = 0.00011
Jxz = 0.00001
S_wing = 0.043
Beispiel #3
0
def follow_orbit(state):

    # p = np.array([state[0], state[1], state[2]]).T
    g = 9.81
    Vg = state[3]

    e2 = np.array([0, 1, 0])
    e3 = np.array([0, 0, 1])

    # psi = state.psi

    phi, theta, psi = Quaternion2Euler(normalize(state[6:10]))
    chi = psi

    k_orbit = 0.75

    c = np.array([0, 0, -100])
    rho = 20
    dir = -1
    d = np.sqrt((state[1] - c.item(1))**2 + (state[0] - c.item(0))**2)
    varphi = np.arctan2(state[1] - c.item(1), state[0] - c.item(0))
    while any(varphi - chi < -np.pi):
        # pdb.set_trace()
        varphi = varphi + 2 * np.pi * (varphi - chi < -np.pi).astype(int)
    while any(varphi - chi > np.pi):
        # pdb.set_trace()
        varphi = varphi - 2 * np.pi * (varphi - chi > np.pi).astype(int)

    chi_c = varphi + dir * (np.pi / 2 + np.arctan(k_orbit * (d - rho) / rho))

    # self.autopilot_commands.course_command = chi_c
    # self.autopilot_commands.altitude_command = c.item(2)
    phi_feedforward = dir * np.arctan(Vg**2. / (g * rho * np.cos(chi_c - psi)))

    R_90 = np.array([[0, 1, 0], [-1, 0, 0], [0, 0, 1]])
    pos_noZ = np.array([state[0][0], state[1][0], 0])
    closest_to_cir = 2.5 * normalize(pos_noZ)
    closest_to_cir[2] = c[2]
    # line_dir = R_90 @ normalize(pos_noZ)
    # line_err = state[0:3].T - closest_to_cir

    phi_feedforward = 0
    wp = np.array([[100], [0], [-100]])
    wp_prev = np.array([[0], [0], [-100]])
    line_dir = (wp - wp_prev) / np.linalg.norm(wp - wp_prev)
    # set_trace()
    line_err = (np.eye(3) - line_dir * line_dir.T) @ (state[0:3] - wp_prev)
    line_err = line_err.T

    chi_l = np.arctan2(line_dir[1], line_dir[0])

    gamma_l = np.arctan(-line_dir[2] /
                        np.sum(np.abs(line_dir[0:2])**2, axis=0)**(1. / 2))
    gamma = theta

    R_I2l = np.identity(3)
    R_I2l[0, 0] = np.cos(chi_l)
    R_I2l[0, 1] = np.sin(chi_l)
    R_I2l[1, 0] = -np.sin(chi_l)
    R_I2l[1, 1] = np.cos(chi_l)

    k_orbit = 0.1
    chi_ref = chi_l - 0.2618 * 2.0 / np.pi * np.arctan(
        k_orbit * e2.dot(R_I2l @ line_err.T))
    chi_c = chi_ref

    k_path = 0.5
    gamma_ref = gamma_l + 0.2618 * 2.0 / np.pi * np.arctan(
        k_path * e3.dot(R_I2l @ line_err.T))
    # gamma_ref += 0.5

    # return normalize(Euler2Quaternion(0.0*np.ones(state.shape[1]),
    #     0.0*np.ones(state.shape[1]),
    #     chi_c*np.ones(state.shape[1]),
    #     state.shape[1]))
    # pdb.set_trace()
    return normalize(
        Euler2Quaternion(phi_feedforward * np.ones(state.shape[1]),
                         gamma_ref[0] * np.ones(state.shape[1]),
                         chi_c * np.ones(state.shape[1]), state.shape[1]))