def sundials_rhs(self, t, y, ydot):
"""
The right hand side of the LLG equation
"""
self.t = t
# already synchronized when call this funciton
# self.spin[:]=y[:]
self.compute_effective_field(t)
clib.compute_llg_rhs(ydot,
self.spin,
self.field,
self._alpha,
self._pins,
self.gamma,
self.mesh.n,
self.do_precession,
self.default_c
)
# ydot[:] = self.dm_dt[:]
return 0
def step_rhs(self, t, y):
self.t = t
self.compute_effective_field(t)
clib.compute_llg_rhs(self.dm_dt,
self.spin,
self.field,
self.alpha,
self._pins,
self.gamma,
self.n,
self.do_procession,
self.default_c)
return self.dm_dt
def step_rhs(self, t, y):
self.t = t
self.compute_effective_field(t)
clib.compute_llg_rhs(self.dm_dt,
self.spin,
self.field,
self.alpha,
self._pins,
self.gamma,
self.n,
self.do_precession,
self.default_c)
return self.dm_dt
def sundials_rhs(self, t, y, ydot):
self.t = t
# already synchronized when call this funciton
# self.spin[:]=y[:]
self.compute_effective_field(t)
clib.compute_llg_rhs(
ydot, self.spin, self.field, self.alpha, self._pins, self.gamma, self.n, self.do_procession, self.default_c
)
# ydot[:] = self.dm_dt[:]
return 0
def sundials_rhs(self, t, y, ydot):
self.t = t
# already synchronized when call this funciton
# self.spin[:]=y[:]
self.compute_effective_field(t)
clib.compute_llg_rhs(ydot, self.spin, self.field, self.alpha,
self._pins, self.gamma, self.n,
self.do_precession, self.default_c)
#ydot[:] = self.dm_dt[:]
return 0
def step_rhs(self, t, y):
self.spin[:] = y[:]
self.t = t
# From the micro_driver class:
self.compute_effective_field(t)
clib.compute_llg_rhs(self.dm_dt,
self.spin,
self.field,
self.alpha,
self._pins,
self.gamma,
self.n,
self.do_precession,
self.default_c
)
return self.dm_dt
