peacock-data-public-datasets-idc-llm_eval
/
env-llmeval
/lib
/python3.10
/site-packages
/sympy
/physics
/mechanics
/system.py
from sympy.core.backend import eye, Matrix, zeros | |
from sympy.physics.mechanics import dynamicsymbols | |
from sympy.physics.mechanics.functions import find_dynamicsymbols | |
__all__ = ['SymbolicSystem'] | |
class SymbolicSystem: | |
"""SymbolicSystem is a class that contains all the information about a | |
system in a symbolic format such as the equations of motions and the bodies | |
and loads in the system. | |
There are three ways that the equations of motion can be described for | |
Symbolic System: | |
[1] Explicit form where the kinematics and dynamics are combined | |
x' = F_1(x, t, r, p) | |
[2] Implicit form where the kinematics and dynamics are combined | |
M_2(x, p) x' = F_2(x, t, r, p) | |
[3] Implicit form where the kinematics and dynamics are separate | |
M_3(q, p) u' = F_3(q, u, t, r, p) | |
q' = G(q, u, t, r, p) | |
where | |
x : states, e.g. [q, u] | |
t : time | |
r : specified (exogenous) inputs | |
p : constants | |
q : generalized coordinates | |
u : generalized speeds | |
F_1 : right hand side of the combined equations in explicit form | |
F_2 : right hand side of the combined equations in implicit form | |
F_3 : right hand side of the dynamical equations in implicit form | |
M_2 : mass matrix of the combined equations in implicit form | |
M_3 : mass matrix of the dynamical equations in implicit form | |
G : right hand side of the kinematical differential equations | |
Parameters | |
========== | |
coord_states : ordered iterable of functions of time | |
This input will either be a collection of the coordinates or states | |
of the system depending on whether or not the speeds are also | |
given. If speeds are specified this input will be assumed to | |
be the coordinates otherwise this input will be assumed to | |
be the states. | |
right_hand_side : Matrix | |
This variable is the right hand side of the equations of motion in | |
any of the forms. The specific form will be assumed depending on | |
whether a mass matrix or coordinate derivatives are given. | |
speeds : ordered iterable of functions of time, optional | |
This is a collection of the generalized speeds of the system. If | |
given it will be assumed that the first argument (coord_states) | |
will represent the generalized coordinates of the system. | |
mass_matrix : Matrix, optional | |
The matrix of the implicit forms of the equations of motion (forms | |
[2] and [3]). The distinction between the forms is determined by | |
whether or not the coordinate derivatives are passed in. If | |
they are given form [3] will be assumed otherwise form [2] is | |
assumed. | |
coordinate_derivatives : Matrix, optional | |
The right hand side of the kinematical equations in explicit form. | |
If given it will be assumed that the equations of motion are being | |
entered in form [3]. | |
alg_con : Iterable, optional | |
The indexes of the rows in the equations of motion that contain | |
algebraic constraints instead of differential equations. If the | |
equations are input in form [3], it will be assumed the indexes are | |
referencing the mass_matrix/right_hand_side combination and not the | |
coordinate_derivatives. | |
output_eqns : Dictionary, optional | |
Any output equations that are desired to be tracked are stored in a | |
dictionary where the key corresponds to the name given for the | |
specific equation and the value is the equation itself in symbolic | |
form | |
coord_idxs : Iterable, optional | |
If coord_states corresponds to the states rather than the | |
coordinates this variable will tell SymbolicSystem which indexes of | |
the states correspond to generalized coordinates. | |
speed_idxs : Iterable, optional | |
If coord_states corresponds to the states rather than the | |
coordinates this variable will tell SymbolicSystem which indexes of | |
the states correspond to generalized speeds. | |
bodies : iterable of Body/Rigidbody objects, optional | |
Iterable containing the bodies of the system | |
loads : iterable of load instances (described below), optional | |
Iterable containing the loads of the system where forces are given | |
by (point of application, force vector) and torques are given by | |
(reference frame acting upon, torque vector). Ex [(point, force), | |
(ref_frame, torque)] | |
Attributes | |
========== | |
coordinates : Matrix, shape(n, 1) | |
This is a matrix containing the generalized coordinates of the system | |
speeds : Matrix, shape(m, 1) | |
This is a matrix containing the generalized speeds of the system | |
states : Matrix, shape(o, 1) | |
This is a matrix containing the state variables of the system | |
alg_con : List | |
This list contains the indices of the algebraic constraints in the | |
combined equations of motion. The presence of these constraints | |
requires that a DAE solver be used instead of an ODE solver. | |
If the system is given in form [3] the alg_con variable will be | |
adjusted such that it is a representation of the combined kinematics | |
and dynamics thus make sure it always matches the mass matrix | |
entered. | |
dyn_implicit_mat : Matrix, shape(m, m) | |
This is the M matrix in form [3] of the equations of motion (the mass | |
matrix or generalized inertia matrix of the dynamical equations of | |
motion in implicit form). | |
dyn_implicit_rhs : Matrix, shape(m, 1) | |
This is the F vector in form [3] of the equations of motion (the right | |
hand side of the dynamical equations of motion in implicit form). | |
comb_implicit_mat : Matrix, shape(o, o) | |
This is the M matrix in form [2] of the equations of motion. | |
This matrix contains a block diagonal structure where the top | |
left block (the first rows) represent the matrix in the | |
implicit form of the kinematical equations and the bottom right | |
block (the last rows) represent the matrix in the implicit form | |
of the dynamical equations. | |
comb_implicit_rhs : Matrix, shape(o, 1) | |
This is the F vector in form [2] of the equations of motion. The top | |
part of the vector represents the right hand side of the implicit form | |
of the kinemaical equations and the bottom of the vector represents the | |
right hand side of the implicit form of the dynamical equations of | |
motion. | |
comb_explicit_rhs : Matrix, shape(o, 1) | |
This vector represents the right hand side of the combined equations of | |
motion in explicit form (form [1] from above). | |
kin_explicit_rhs : Matrix, shape(m, 1) | |
This is the right hand side of the explicit form of the kinematical | |
equations of motion as can be seen in form [3] (the G matrix). | |
output_eqns : Dictionary | |
If output equations were given they are stored in a dictionary where | |
the key corresponds to the name given for the specific equation and | |
the value is the equation itself in symbolic form | |
bodies : Tuple | |
If the bodies in the system were given they are stored in a tuple for | |
future access | |
loads : Tuple | |
If the loads in the system were given they are stored in a tuple for | |
future access. This includes forces and torques where forces are given | |
by (point of application, force vector) and torques are given by | |
(reference frame acted upon, torque vector). | |
Example | |
======= | |
As a simple example, the dynamics of a simple pendulum will be input into a | |
SymbolicSystem object manually. First some imports will be needed and then | |
symbols will be set up for the length of the pendulum (l), mass at the end | |
of the pendulum (m), and a constant for gravity (g). :: | |
>>> from sympy import Matrix, sin, symbols | |
>>> from sympy.physics.mechanics import dynamicsymbols, SymbolicSystem | |
>>> l, m, g = symbols('l m g') | |
The system will be defined by an angle of theta from the vertical and a | |
generalized speed of omega will be used where omega = theta_dot. :: | |
>>> theta, omega = dynamicsymbols('theta omega') | |
Now the equations of motion are ready to be formed and passed to the | |
SymbolicSystem object. :: | |
>>> kin_explicit_rhs = Matrix([omega]) | |
>>> dyn_implicit_mat = Matrix([l**2 * m]) | |
>>> dyn_implicit_rhs = Matrix([-g * l * m * sin(theta)]) | |
>>> symsystem = SymbolicSystem([theta], dyn_implicit_rhs, [omega], | |
... dyn_implicit_mat) | |
Notes | |
===== | |
m : number of generalized speeds | |
n : number of generalized coordinates | |
o : number of states | |
""" | |
def __init__(self, coord_states, right_hand_side, speeds=None, | |
mass_matrix=None, coordinate_derivatives=None, alg_con=None, | |
output_eqns={}, coord_idxs=None, speed_idxs=None, bodies=None, | |
loads=None): | |
"""Initializes a SymbolicSystem object""" | |
# Extract information on speeds, coordinates and states | |
if speeds is None: | |
self._states = Matrix(coord_states) | |
if coord_idxs is None: | |
self._coordinates = None | |
else: | |
coords = [coord_states[i] for i in coord_idxs] | |
self._coordinates = Matrix(coords) | |
if speed_idxs is None: | |
self._speeds = None | |
else: | |
speeds_inter = [coord_states[i] for i in speed_idxs] | |
self._speeds = Matrix(speeds_inter) | |
else: | |
self._coordinates = Matrix(coord_states) | |
self._speeds = Matrix(speeds) | |
self._states = self._coordinates.col_join(self._speeds) | |
# Extract equations of motion form | |
if coordinate_derivatives is not None: | |
self._kin_explicit_rhs = coordinate_derivatives | |
self._dyn_implicit_rhs = right_hand_side | |
self._dyn_implicit_mat = mass_matrix | |
self._comb_implicit_rhs = None | |
self._comb_implicit_mat = None | |
self._comb_explicit_rhs = None | |
elif mass_matrix is not None: | |
self._kin_explicit_rhs = None | |
self._dyn_implicit_rhs = None | |
self._dyn_implicit_mat = None | |
self._comb_implicit_rhs = right_hand_side | |
self._comb_implicit_mat = mass_matrix | |
self._comb_explicit_rhs = None | |
else: | |
self._kin_explicit_rhs = None | |
self._dyn_implicit_rhs = None | |
self._dyn_implicit_mat = None | |
self._comb_implicit_rhs = None | |
self._comb_implicit_mat = None | |
self._comb_explicit_rhs = right_hand_side | |
# Set the remainder of the inputs as instance attributes | |
if alg_con is not None and coordinate_derivatives is not None: | |
alg_con = [i + len(coordinate_derivatives) for i in alg_con] | |
self._alg_con = alg_con | |
self.output_eqns = output_eqns | |
# Change the body and loads iterables to tuples if they are not tuples | |
# already | |
if not isinstance(bodies, tuple) and bodies is not None: | |
bodies = tuple(bodies) | |
if not isinstance(loads, tuple) and loads is not None: | |
loads = tuple(loads) | |
self._bodies = bodies | |
self._loads = loads | |
def coordinates(self): | |
"""Returns the column matrix of the generalized coordinates""" | |
if self._coordinates is None: | |
raise AttributeError("The coordinates were not specified.") | |
else: | |
return self._coordinates | |
def speeds(self): | |
"""Returns the column matrix of generalized speeds""" | |
if self._speeds is None: | |
raise AttributeError("The speeds were not specified.") | |
else: | |
return self._speeds | |
def states(self): | |
"""Returns the column matrix of the state variables""" | |
return self._states | |
def alg_con(self): | |
"""Returns a list with the indices of the rows containing algebraic | |
constraints in the combined form of the equations of motion""" | |
return self._alg_con | |
def dyn_implicit_mat(self): | |
"""Returns the matrix, M, corresponding to the dynamic equations in | |
implicit form, M x' = F, where the kinematical equations are not | |
included""" | |
if self._dyn_implicit_mat is None: | |
raise AttributeError("dyn_implicit_mat is not specified for " | |
"equations of motion form [1] or [2].") | |
else: | |
return self._dyn_implicit_mat | |
def dyn_implicit_rhs(self): | |
"""Returns the column matrix, F, corresponding to the dynamic equations | |
in implicit form, M x' = F, where the kinematical equations are not | |
included""" | |
if self._dyn_implicit_rhs is None: | |
raise AttributeError("dyn_implicit_rhs is not specified for " | |
"equations of motion form [1] or [2].") | |
else: | |
return self._dyn_implicit_rhs | |
def comb_implicit_mat(self): | |
"""Returns the matrix, M, corresponding to the equations of motion in | |
implicit form (form [2]), M x' = F, where the kinematical equations are | |
included""" | |
if self._comb_implicit_mat is None: | |
if self._dyn_implicit_mat is not None: | |
num_kin_eqns = len(self._kin_explicit_rhs) | |
num_dyn_eqns = len(self._dyn_implicit_rhs) | |
zeros1 = zeros(num_kin_eqns, num_dyn_eqns) | |
zeros2 = zeros(num_dyn_eqns, num_kin_eqns) | |
inter1 = eye(num_kin_eqns).row_join(zeros1) | |
inter2 = zeros2.row_join(self._dyn_implicit_mat) | |
self._comb_implicit_mat = inter1.col_join(inter2) | |
return self._comb_implicit_mat | |
else: | |
raise AttributeError("comb_implicit_mat is not specified for " | |
"equations of motion form [1].") | |
else: | |
return self._comb_implicit_mat | |
def comb_implicit_rhs(self): | |
"""Returns the column matrix, F, corresponding to the equations of | |
motion in implicit form (form [2]), M x' = F, where the kinematical | |
equations are included""" | |
if self._comb_implicit_rhs is None: | |
if self._dyn_implicit_rhs is not None: | |
kin_inter = self._kin_explicit_rhs | |
dyn_inter = self._dyn_implicit_rhs | |
self._comb_implicit_rhs = kin_inter.col_join(dyn_inter) | |
return self._comb_implicit_rhs | |
else: | |
raise AttributeError("comb_implicit_mat is not specified for " | |
"equations of motion in form [1].") | |
else: | |
return self._comb_implicit_rhs | |
def compute_explicit_form(self): | |
"""If the explicit right hand side of the combined equations of motion | |
is to provided upon initialization, this method will calculate it. This | |
calculation can potentially take awhile to compute.""" | |
if self._comb_explicit_rhs is not None: | |
raise AttributeError("comb_explicit_rhs is already formed.") | |
inter1 = getattr(self, 'kin_explicit_rhs', None) | |
if inter1 is not None: | |
inter2 = self._dyn_implicit_mat.LUsolve(self._dyn_implicit_rhs) | |
out = inter1.col_join(inter2) | |
else: | |
out = self._comb_implicit_mat.LUsolve(self._comb_implicit_rhs) | |
self._comb_explicit_rhs = out | |
def comb_explicit_rhs(self): | |
"""Returns the right hand side of the equations of motion in explicit | |
form, x' = F, where the kinematical equations are included""" | |
if self._comb_explicit_rhs is None: | |
raise AttributeError("Please run .combute_explicit_form before " | |
"attempting to access comb_explicit_rhs.") | |
else: | |
return self._comb_explicit_rhs | |
def kin_explicit_rhs(self): | |
"""Returns the right hand side of the kinematical equations in explicit | |
form, q' = G""" | |
if self._kin_explicit_rhs is None: | |
raise AttributeError("kin_explicit_rhs is not specified for " | |
"equations of motion form [1] or [2].") | |
else: | |
return self._kin_explicit_rhs | |
def dynamic_symbols(self): | |
"""Returns a column matrix containing all of the symbols in the system | |
that depend on time""" | |
# Create a list of all of the expressions in the equations of motion | |
if self._comb_explicit_rhs is None: | |
eom_expressions = (self.comb_implicit_mat[:] + | |
self.comb_implicit_rhs[:]) | |
else: | |
eom_expressions = (self._comb_explicit_rhs[:]) | |
functions_of_time = set() | |
for expr in eom_expressions: | |
functions_of_time = functions_of_time.union( | |
find_dynamicsymbols(expr)) | |
functions_of_time = functions_of_time.union(self._states) | |
return tuple(functions_of_time) | |
def constant_symbols(self): | |
"""Returns a column matrix containing all of the symbols in the system | |
that do not depend on time""" | |
# Create a list of all of the expressions in the equations of motion | |
if self._comb_explicit_rhs is None: | |
eom_expressions = (self.comb_implicit_mat[:] + | |
self.comb_implicit_rhs[:]) | |
else: | |
eom_expressions = (self._comb_explicit_rhs[:]) | |
constants = set() | |
for expr in eom_expressions: | |
constants = constants.union(expr.free_symbols) | |
constants.remove(dynamicsymbols._t) | |
return tuple(constants) | |
def bodies(self): | |
"""Returns the bodies in the system""" | |
if self._bodies is None: | |
raise AttributeError("bodies were not specified for the system.") | |
else: | |
return self._bodies | |
def loads(self): | |
"""Returns the loads in the system""" | |
if self._loads is None: | |
raise AttributeError("loads were not specified for the system.") | |
else: | |
return self._loads | |