Essential Classes¶
CoordinateSym¶

class
sympy.physics.vector.frame.
CoordinateSym
[source]¶ A coordinate symbol/base scalar associated wrt a Reference Frame.
Ideally, users should not instantiate this class. Instances of this class must only be accessed through the corresponding frame as ‘frame[index]’.
CoordinateSyms having the same frame and index parameters are equal (even though they may be instantiated separately).
Parameters: name : string
The display name of the CoordinateSym
frame : ReferenceFrame
The reference frame this base scalar belongs to
index : 0, 1 or 2
The index of the dimension denoted by this coordinate variable
Examples
>>> from sympy.physics.vector import ReferenceFrame, CoordinateSym >>> A = ReferenceFrame('A') >>> A[1] A_y >>> type(A[0]) <class 'sympy.physics.vector.frame.CoordinateSym'> >>> a_y = CoordinateSym('a_y', A, 1) >>> a_y == A[1] True
ReferenceFrame¶

class
sympy.physics.vector.frame.
ReferenceFrame
(name, indices=None, latexs=None, variables=None)[source]¶ A reference frame in classical mechanics.
ReferenceFrame is a class used to represent a reference frame in classical mechanics. It has a standard basis of three unit vectors in the frame’s x, y, and z directions.
It also can have a rotation relative to a parent frame; this rotation is defined by a direction cosine matrix relating this frame’s basis vectors to the parent frame’s basis vectors. It can also have an angular velocity vector, defined in another frame.

ang_acc_in
(otherframe)[source]¶ Returns the angular acceleration Vector of the ReferenceFrame.
Effectively returns the Vector: ^N alpha ^B which represent the angular acceleration of B in N, where B is self, and N is otherframe.
Parameters: otherframe : ReferenceFrame
The ReferenceFrame which the angular acceleration is returned in.
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> N = ReferenceFrame('N') >>> A = ReferenceFrame('A') >>> V = 10 * N.x >>> A.set_ang_acc(N, V) >>> A.ang_acc_in(N) 10*N.x

ang_vel_in
(otherframe)[source]¶ Returns the angular velocity Vector of the ReferenceFrame.
Effectively returns the Vector: ^N omega ^B which represent the angular velocity of B in N, where B is self, and N is otherframe.
Parameters: otherframe : ReferenceFrame
The ReferenceFrame which the angular velocity is returned in.
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> N = ReferenceFrame('N') >>> A = ReferenceFrame('A') >>> V = 10 * N.x >>> A.set_ang_vel(N, V) >>> A.ang_vel_in(N) 10*N.x

dcm
(otherframe)[source]¶ The direction cosine matrix between frames.
This gives the DCM between this frame and the otherframe. The format is N.xyz = N.dcm(B) * B.xyz A SymPy Matrix is returned.
Parameters: otherframe : ReferenceFrame
The otherframe which the DCM is generated to.
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> from sympy import symbols >>> q1 = symbols('q1') >>> N = ReferenceFrame('N') >>> A = N.orientnew('A', 'Axis', [q1, N.x]) >>> N.dcm(A) Matrix([ [1, 0, 0], [0, cos(q1), sin(q1)], [0, sin(q1), cos(q1)]])

orient
(parent, rot_type, amounts, rot_order='')[source]¶ Defines the orientation of this frame relative to a parent frame.
Parameters: parent : ReferenceFrame
The frame that this ReferenceFrame will have its orientation matrix defined in relation to.
rot_type : str
The type of orientation matrix that is being created. Supported types are ‘Body’, ‘Space’, ‘Quaternion’, ‘Axis’, and ‘DCM’. See examples for correct usage.
amounts : list OR value
The quantities that the orientation matrix will be defined by. In case of rot_type=’DCM’, value must be a sympy.matrices.MatrixBase object (or subclasses of it).
rot_order : str
If applicable, the order of a series of rotations.
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> from sympy import symbols, eye, ImmutableMatrix >>> q0, q1, q2, q3 = symbols('q0 q1 q2 q3') >>> N = ReferenceFrame('N') >>> B = ReferenceFrame('B')
Now we have a choice of how to implement the orientation. First is Body. Body orientation takes this reference frame through three successive simple rotations. Acceptable rotation orders are of length 3, expressed in XYZ or 123, and cannot have a rotation about about an axis twice in a row.
>>> B.orient(N, 'Body', [q1, q2, q3], '123') >>> B.orient(N, 'Body', [q1, q2, 0], 'ZXZ') >>> B.orient(N, 'Body', [0, 0, 0], 'XYX')
Next is Space. Space is like Body, but the rotations are applied in the opposite order.
>>> B.orient(N, 'Space', [q1, q2, q3], '312')
Next is Quaternion. This orients the new ReferenceFrame with Quaternions, defined as a finite rotation about lambda, a unit vector, by some amount theta. This orientation is described by four parameters: q0 = cos(theta/2) q1 = lambda_x sin(theta/2) q2 = lambda_y sin(theta/2) q3 = lambda_z sin(theta/2) Quaternion does not take in a rotation order.
>>> B.orient(N, 'Quaternion', [q0, q1, q2, q3])
Next is Axis. This is a rotation about an arbitrary, nontimevarying axis by some angle. The axis is supplied as a Vector. This is how simple rotations are defined.
>>> B.orient(N, 'Axis', [q1, N.x + 2 * N.y])
Last is DCM (Direction Cosine Matrix). This is a rotation matrix given manually.
>>> B.orient(N, 'DCM', eye(3)) >>> B.orient(N, 'DCM', ImmutableMatrix([[0, 1, 0], [0, 0, 1], [1, 0, 0]]))

orientnew
(newname, rot_type, amounts, rot_order='', variables=None, indices=None, latexs=None)[source]¶ Creates a new ReferenceFrame oriented with respect to this Frame.
See ReferenceFrame.orient() for acceptable rotation types, amounts, and orders. Parent is going to be self.
Parameters: newname : str
The name for the new ReferenceFrame
rot_type : str
The type of orientation matrix that is being created.
amounts : list OR value
The quantities that the orientation matrix will be defined by.
rot_order : str
If applicable, the order of a series of rotations.
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> from sympy import symbols >>> q0, q1, q2, q3 = symbols('q0 q1 q2 q3') >>> N = ReferenceFrame('N')
Now we have a choice of how to implement the orientation. First is Body. Body orientation takes this reference frame through three successive simple rotations. Acceptable rotation orders are of length 3, expressed in XYZ or 123, and cannot have a rotation about about an axis twice in a row.
>>> A = N.orientnew('A', 'Body', [q1, q2, q3], '123') >>> A = N.orientnew('A', 'Body', [q1, q2, 0], 'ZXZ') >>> A = N.orientnew('A', 'Body', [0, 0, 0], 'XYX')
Next is Space. Space is like Body, but the rotations are applied in the opposite order.
>>> A = N.orientnew('A', 'Space', [q1, q2, q3], '312')
Next is Quaternion. This orients the new ReferenceFrame with Quaternions, defined as a finite rotation about lambda, a unit vector, by some amount theta. This orientation is described by four parameters: q0 = cos(theta/2) q1 = lambda_x sin(theta/2) q2 = lambda_y sin(theta/2) q3 = lambda_z sin(theta/2) Quaternion does not take in a rotation order.
>>> A = N.orientnew('A', 'Quaternion', [q0, q1, q2, q3])
Last is Axis. This is a rotation about an arbitrary, nontimevarying axis by some angle. The axis is supplied as a Vector. This is how simple rotations are defined.
>>> A = N.orientnew('A', 'Axis', [q1, N.x])

partial_velocity
(frame, *gen_speeds)[source]¶ Returns the partial angular velocities of this frame in the given frame with respect to one or more provided generalized speeds.
Parameters: frame : ReferenceFrame
The frame with which the angular velocity is defined in.
gen_speeds : functions of time
The generalized speeds.
Returns: partial_velocities : tuple of Vector
The partial angular velocity vectors corresponding to the provided generalized speeds.
Examples
>>> from sympy.physics.vector import ReferenceFrame, dynamicsymbols >>> N = ReferenceFrame('N') >>> A = ReferenceFrame('A') >>> u1, u2 = dynamicsymbols('u1, u2') >>> A.set_ang_vel(N, u1 * A.x + u2 * N.y) >>> A.partial_velocity(N, u1) A.x >>> A.partial_velocity(N, u1, u2) (A.x, N.y)

set_ang_acc
(otherframe, value)[source]¶ Define the angular acceleration Vector in a ReferenceFrame.
Defines the angular acceleration of this ReferenceFrame, in another. Angular acceleration can be defined with respect to multiple different ReferenceFrames. Care must be taken to not create loops which are inconsistent.
Parameters: otherframe : ReferenceFrame
A ReferenceFrame to define the angular acceleration in
value : Vector
The Vector representing angular acceleration
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> N = ReferenceFrame('N') >>> A = ReferenceFrame('A') >>> V = 10 * N.x >>> A.set_ang_acc(N, V) >>> A.ang_acc_in(N) 10*N.x

set_ang_vel
(otherframe, value)[source]¶ Define the angular velocity vector in a ReferenceFrame.
Defines the angular velocity of this ReferenceFrame, in another. Angular velocity can be defined with respect to multiple different ReferenceFrames. Care must be taken to not create loops which are inconsistent.
Parameters: otherframe : ReferenceFrame
A ReferenceFrame to define the angular velocity in
value : Vector
The Vector representing angular velocity
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> N = ReferenceFrame('N') >>> A = ReferenceFrame('A') >>> V = 10 * N.x >>> A.set_ang_vel(N, V) >>> A.ang_vel_in(N) 10*N.x

variable_map
(otherframe)[source]¶ Returns a dictionary which expresses the coordinate variables of this frame in terms of the variables of otherframe.
If Vector.simp is True, returns a simplified version of the mapped values. Else, returns them without simplification.
Simplification of the expressions may take time.
Parameters: otherframe : ReferenceFrame
The other frame to map the variables to
Examples
>>> from sympy.physics.vector import ReferenceFrame, dynamicsymbols >>> A = ReferenceFrame('A') >>> q = dynamicsymbols('q') >>> B = A.orientnew('B', 'Axis', [q, A.z]) >>> A.variable_map(B) {A_x: B_x*cos(q(t))  B_y*sin(q(t)), A_y: B_x*sin(q(t)) + B_y*cos(q(t)), A_z: B_z}

x
¶ The basis Vector for the ReferenceFrame, in the x direction.

y
¶ The basis Vector for the ReferenceFrame, in the y direction.

z
¶ The basis Vector for the ReferenceFrame, in the z direction.

Vector¶

class
sympy.physics.vector.vector.
Vector
(inlist)[source]¶ The class used to define vectors.
It along with ReferenceFrame are the building blocks of describing a classical mechanics system in PyDy and sympy.physics.vector.
Attributes
simp (Boolean) Let certain methods use trigsimp on their outputs 
cross
(other)[source]¶ The cross product operator for two Vectors.
Returns a Vector, expressed in the same ReferenceFrames as self.
Parameters: other : Vector
The Vector which we are crossing with
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector >>> from sympy import symbols >>> q1 = symbols('q1') >>> N = ReferenceFrame('N') >>> N.x ^ N.y N.z >>> A = N.orientnew('A', 'Axis', [q1, N.x]) >>> A.x ^ N.y N.z >>> N.y ^ A.x  sin(q1)*A.y  cos(q1)*A.z

diff
(var, frame, var_in_dcm=True)[source]¶ Returns the partial derivative of the vector with respect to a variable in the provided reference frame.
Parameters: var : Symbol
What the partial derivative is taken with respect to.
frame : ReferenceFrame
The reference frame that the partial derivative is taken in.
var_in_dcm : boolean
If true, the differentiation algorithm assumes that the variable may be present in any of the direction cosine matrices that relate the frame to the frames of any component of the vector. But if it is known that the variable is not present in the direction cosine matrices, false can be set to skip full reexpression in the desired frame.
Examples
>>> from sympy import Symbol >>> from sympy.physics.vector import dynamicsymbols, ReferenceFrame >>> from sympy.physics.vector import Vector >>> Vector.simp = True >>> t = Symbol('t') >>> q1 = dynamicsymbols('q1') >>> N = ReferenceFrame('N') >>> A = N.orientnew('A', 'Axis', [q1, N.y]) >>> A.x.diff(t, N)  q1'*A.z >>> B = ReferenceFrame('B') >>> u1, u2 = dynamicsymbols('u1, u2') >>> v = u1 * A.x + u2 * B.y >>> v.diff(u2, N, var_in_dcm=False) B.y

dot
(other)[source]¶ Dot product of two vectors.
Returns a scalar, the dot product of the two Vectors
Parameters: other : Vector
The Vector which we are dotting with
Examples
>>> from sympy.physics.vector import ReferenceFrame, dot >>> from sympy import symbols >>> q1 = symbols('q1') >>> N = ReferenceFrame('N') >>> dot(N.x, N.x) 1 >>> dot(N.x, N.y) 0 >>> A = N.orientnew('A', 'Axis', [q1, N.x]) >>> dot(N.y, A.y) cos(q1)

dt
(otherframe)[source]¶ Returns a Vector which is the time derivative of the self Vector, taken in frame otherframe.
Calls the global time_derivative method
Parameters: otherframe : ReferenceFrame
The frame to calculate the time derivative in

express
(otherframe, variables=False)[source]¶ Returns a Vector equivalent to this one, expressed in otherframe. Uses the global express method.
Parameters: otherframe : ReferenceFrame
The frame for this Vector to be described in
variables : boolean
If True, the coordinate symbols(if present) in this Vector are reexpressed in terms otherframe
Examples
>>> from sympy.physics.vector import ReferenceFrame, Vector, dynamicsymbols >>> q1 = dynamicsymbols('q1') >>> N = ReferenceFrame('N') >>> A = N.orientnew('A', 'Axis', [q1, N.y]) >>> A.x.express(N) cos(q1)*N.x  sin(q1)*N.z

free_symbols
(reference_frame)[source]¶ Returns the free symbols in the measure numbers of the vector expressed in the given reference frame.
Parameter
 reference_frame : ReferenceFrame
 The frame with respect to which the free symbols of the given vector is to be determined.

outer
(other)[source]¶ Outer product between two Vectors.
A rank increasing operation, which returns a Dyadic from two Vectors
Parameters: other : Vector
The Vector to take the outer product with
Examples
>>> from sympy.physics.vector import ReferenceFrame, outer >>> N = ReferenceFrame('N') >>> outer(N.x, N.x) (N.xN.x)

separate
()[source]¶ The constituents of this vector in different reference frames, as per its definition.
Returns a dict mapping each ReferenceFrame to the corresponding constituent Vector.
Examples
>>> from sympy.physics.vector import ReferenceFrame >>> R1 = ReferenceFrame('R1') >>> R2 = ReferenceFrame('R2') >>> v = R1.x + R2.x >>> v.separate() == {R1: R1.x, R2: R2.x} True

subs
(*args, **kwargs)[source]¶ Substitution on the Vector.
Examples
>>> from sympy.physics.vector import ReferenceFrame >>> from sympy import Symbol >>> N = ReferenceFrame('N') >>> s = Symbol('s') >>> a = N.x * s >>> a.subs({s: 2}) 2*N.x

to_matrix
(reference_frame)[source]¶ Returns the matrix form of the vector with respect to the given frame.
Parameters: reference_frame : ReferenceFrame
The reference frame that the rows of the matrix correspond to.
Returns: matrix : ImmutableMatrix, shape(3,1)
The matrix that gives the 1D vector.
Examples
>>> from sympy import symbols >>> from sympy.physics.vector import ReferenceFrame >>> from sympy.physics.mechanics.functions import inertia >>> a, b, c = symbols('a, b, c') >>> N = ReferenceFrame('N') >>> vector = a * N.x + b * N.y + c * N.z >>> vector.to_matrix(N) Matrix([ [a], [b], [c]]) >>> beta = symbols('beta') >>> A = N.orientnew('A', 'Axis', (beta, N.x)) >>> vector.to_matrix(A) Matrix([ [ a], [ b*cos(beta) + c*sin(beta)], [b*sin(beta) + c*cos(beta)]])

Dyadic¶

class
sympy.physics.vector.dyadic.
Dyadic
(inlist)[source]¶ A Dyadic object.
See: http://en.wikipedia.org/wiki/Dyadic_tensor Kane, T., Levinson, D. Dynamics Theory and Applications. 1985 McGrawHill
A more powerful way to represent a rigid body’s inertia. While it is more complex, by choosing Dyadic components to be in body fixed basis vectors, the resulting matrix is equivalent to the inertia tensor.

cross
(other)¶ For a cross product in the form: Dyadic x Vector.
Parameters: other : Vector
The Vector that we are crossing this Dyadic with
Examples
>>> from sympy.physics.vector import ReferenceFrame, outer, cross >>> N = ReferenceFrame('N') >>> d = outer(N.x, N.x) >>> cross(d, N.y) (N.xN.z)

dot
(other)¶ The inner product operator for a Dyadic and a Dyadic or Vector.
Parameters: other : Dyadic or Vector
The other Dyadic or Vector to take the inner product with
Examples
>>> from sympy.physics.vector import ReferenceFrame, outer >>> N = ReferenceFrame('N') >>> D1 = outer(N.x, N.y) >>> D2 = outer(N.y, N.y) >>> D1.dot(D2) (N.xN.y) >>> D1.dot(N.y) N.x

dt
(frame)[source]¶ Take the time derivative of this Dyadic in a frame.
This function calls the global time_derivative method
Parameters: frame : ReferenceFrame
The frame to take the time derivative in
Examples
>>> from sympy.physics.vector import ReferenceFrame, outer, dynamicsymbols >>> N = ReferenceFrame('N') >>> q = dynamicsymbols('q') >>> B = N.orientnew('B', 'Axis', [q, N.z]) >>> d = outer(N.x, N.x) >>> d.dt(B)  q'*(N.yN.x)  q'*(N.xN.y)

express
(frame1, frame2=None)[source]¶ Expresses this Dyadic in alternate frame(s)
The first frame is the list side expression, the second frame is the right side; if Dyadic is in form A.xB.y, you can express it in two different frames. If no second frame is given, the Dyadic is expressed in only one frame.
Calls the global express function
Parameters: frame1 : ReferenceFrame
The frame to express the left side of the Dyadic in
frame2 : ReferenceFrame
If provided, the frame to express the right side of the Dyadic in
Examples
>>> from sympy.physics.vector import ReferenceFrame, outer, dynamicsymbols >>> N = ReferenceFrame('N') >>> q = dynamicsymbols('q') >>> B = N.orientnew('B', 'Axis', [q, N.z]) >>> d = outer(N.x, N.x) >>> d.express(B, N) cos(q)*(B.xN.x)  sin(q)*(B.yN.x)

subs
(*args, **kwargs)[source]¶ Substitution on the Dyadic.
Examples
>>> from sympy.physics.vector import ReferenceFrame >>> from sympy import Symbol >>> N = ReferenceFrame('N') >>> s = Symbol('s') >>> a = s * (N.xN.x) >>> a.subs({s: 2}) 2*(N.xN.x)

to_matrix
(reference_frame, second_reference_frame=None)[source]¶ Returns the matrix form of the dyadic with respect to one or two reference frames.
Parameters: reference_frame : ReferenceFrame
The reference frame that the rows and columns of the matrix correspond to. If a second reference frame is provided, this only corresponds to the rows of the matrix.
second_reference_frame : ReferenceFrame, optional, default=None
The reference frame that the columns of the matrix correspond to.
Returns: matrix : ImmutableMatrix, shape(3,3)
The matrix that gives the 2D tensor form.
Examples
>>> from sympy import symbols >>> from sympy.physics.vector import ReferenceFrame, Vector >>> Vector.simp = True >>> from sympy.physics.mechanics import inertia >>> Ixx, Iyy, Izz, Ixy, Iyz, Ixz = symbols('Ixx, Iyy, Izz, Ixy, Iyz, Ixz') >>> N = ReferenceFrame('N') >>> inertia_dyadic = inertia(N, Ixx, Iyy, Izz, Ixy, Iyz, Ixz) >>> inertia_dyadic.to_matrix(N) Matrix([ [Ixx, Ixy, Ixz], [Ixy, Iyy, Iyz], [Ixz, Iyz, Izz]]) >>> beta = symbols('beta') >>> A = N.orientnew('A', 'Axis', (beta, N.x)) >>> inertia_dyadic.to_matrix(A) Matrix([ [ Ixx, Ixy*cos(beta) + Ixz*sin(beta), Ixy*sin(beta) + Ixz*cos(beta)], [ Ixy*cos(beta) + Ixz*sin(beta), Iyy*cos(2*beta)/2 + Iyy/2 + Iyz*sin(2*beta)  Izz*cos(2*beta)/2 + Izz/2, Iyy*sin(2*beta)/2 + Iyz*cos(2*beta) + Izz*sin(2*beta)/2], [Ixy*sin(beta) + Ixz*cos(beta), Iyy*sin(2*beta)/2 + Iyz*cos(2*beta) + Izz*sin(2*beta)/2, Iyy*cos(2*beta)/2 + Iyy/2  Iyz*sin(2*beta) + Izz*cos(2*beta)/2 + Izz/2]])
