Example #1
0
 def M2g(t, y):
     vec = y[:-1, -1]
     out = eom_func(vec, *args)
     g = rn(dim + 1)
     g.set_vector(out)
     return g
Example #2
0
    def __call__(self, eom_func, quad_func, tspan, y0, q0, *args, **kwargs):
        r"""
        Propagates the differential equations over a defined time interval.

        :param eom_func: Function representing the equations of motion.
        :param quad_func: Function representing the quadratures.
        :param tspan: Independent time interval.
        :param y0: Initial state position.
        :param q0: Initial quad position.
        :param args: Additional arguments required by EOM files.
        :param kwargs: Unused.
        :return: A full reconstructed trajectory, :math:`\gamma`.
        """
        y0 = np.array(y0, dtype=np.float64)

        if self.program == 'scipy':
            if self.variable_step is True:
                int_sol = solve_ivp(lambda t, y: eom_func(y, *args),
                                    [tspan[0], tspan[-1]],
                                    y0,
                                    rtol=self.reltol,
                                    atol=self.abstol,
                                    max_step=self.maxstep,
                                    method=self.stepper)
            else:
                T = np.arange(tspan[0], tspan[-1], self.maxstep)
                if T[-1] != tspan[-1]:
                    T = np.hstack((T, tspan[-1]))
                int_sol = solve_ivp(lambda t, y: eom_func(y, *args),
                                    [tspan[0], tspan[-1]],
                                    y0,
                                    rtol=self.reltol,
                                    atol=self.abstol,
                                    method=self.stepper,
                                    t_eval=T)
            gamma = Trajectory(int_sol.t, int_sol.y.T)

        elif self.program == 'lie':
            dim = y0.shape[0]
            g = rn(dim + 1)
            g.set_vector(y0)
            y = HManifold(RN(dim + 1, exp(g)))
            vf = VectorField(y)
            vf.set_equationtype('general')

            def M2g(t, y):
                vec = y[:-1, -1]
                out = eom_func(vec, *args)
                g = rn(dim + 1)
                g.set_vector(out)
                return g

            vf.set_M2g(M2g)
            if self.method == 'RKMK':
                ts = RKMK()
            else:
                raise NotImplementedError

            ts.setmethod(self.stepper)
            f = Flow(ts, vf, variablestep=self.variable_step)
            ti, yi = f(y, tspan[0], tspan[-1], self.maxstep)
            gamma = Trajectory(ti, np.vstack([_[:-1, -1] for _ in yi
                                              ]))  # Hardcoded assuming RN

        else:
            raise NotImplementedError

        if quad_func is not None and len(q0) is not 0:
            if self.quick_reconstruct:
                qf = integrate_quads(quad_func, tspan, gamma, *args)
                gamma.q = np.vstack((q0, np.zeros(
                    (len(gamma.t) - 2, len(q0))), qf + q0))
            else:
                gamma = reconstruct(quad_func, gamma, q0, *args)

        return gamma
Example #3
0
 def m2g(_, _y):
     vec = _y[:-1, -1]
     out = eom_func(vec, *args)
     _g = rn(dim+1)
     _g.set_vector(out)
     return _g