@@ -434,6 +434,15 @@ def zero_inertia(cls) -> "Inertia":
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"""
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return cls (0.0 , 0.0 , 0.0 , 0.0 , 0.0 , 0.0 )
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+ @property
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+ def to_matrix (self ) -> np .array :
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+ return np .array ([
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+ [self .ixx , self .ixy , self .ixz ],
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+ [self .ixy , self .iyy , self .iyz ],
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+ [self .ixz , self .iyz , self .izz ]
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+ ])
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+
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+
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@dataclass
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class Material :
@@ -602,6 +611,77 @@ def to_mjcf(self, root: ET.Element) -> None:
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self .origin .to_mjcf (inertial )
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self .inertia .to_mjcf (inertial )
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+ # Adding a method to transform (rotate and translate) an Inertia Matrix
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+ def transform (self , tf_matrix : np .matrix , inplace : bool = False ) -> Union ["InertialLink" , None ]:
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+ """
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+ Apply a transformation matrix to the Inertial Properties of the a link.
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+
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+ Args:
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+ matrix: The transformation matrix to apply to the origin.
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+ inplace: Whether to apply the transformation in place.
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+
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+ Returns:
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+ An updated Inertial Link with the transformation applied to both:
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+ * the inertia tensor (giving a transformed "inertia tensor prime" = [ixx', iyy', izz', ixy', ixz', iyz'])
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+ * AND to the origin too (via the Origin class's transform logic [~line 100])
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+
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+ Examples {@}:
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+ >>> origin = Origin(xyz=(1.0, 2.0, 3.0), rpy=(0.0, 0.0, 0.0))
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+ >>> matrix = np.eye(4)
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+ >>> inertial.transform(matrix)
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+
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+ Analysis and References:
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+ The essence is to convert the Inertia tensor to a matrix and then transform the matrix via the equation
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+ I_prime = R·I·Transpose[R] + m(||d||^2·I - d·Transpose[d])
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+ Then we put the components into the resultant Inertial Link
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+ An analysis (on 100k runs) suggests that this is 3× faster than a direct approach on the tensor elements likely because numpy's libraries are optimized for matrix operations.
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+ Ref: https://chatgpt.com/share/6781b6ac-772c-8006-b1a9-7f2dc3e3ef4d
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+ """
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+ # Extract the rotation matrix R and translation vector d from T
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+ R = tf_matrix [:3 , :3 ] # Top-left 3x3 block is the rotation matrix
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+ p = tf_matrix [:3 , 3 ] # Top-right 3x1 block is the translation vector
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+
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+ # Unpack the inertia tensor components
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+ # Example is ixx=1.0, iyy=2.0, izz=3.0, ixy=0.0, ixz=0.0, iyz=0.
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+
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+ # Construct the original inertia matrix
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+ inertia_matrix = self .inertia .to_matrix
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+
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+ # Rotate the inertia matrix
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+ I_rot = R @ inertia_matrix @ R .T
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+
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+ # Compute the parallel axis theorem adjustment
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+ parallel_axis_adjustment = self .mass * (np .dot (p , p ) * np .eye (3 ) - np .outer (p , p ))
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+
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+ # Final transformed inertia matrix
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+ I_transformed = I_rot + parallel_axis_adjustment
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+
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+ # Extract the components of the transformed inertia tensor
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+ ixx_prime = I_transformed [0 , 0 ]
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+ iyy_prime = I_transformed [1 , 1 ]
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+ izz_prime = I_transformed [2 , 2 ]
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+ ixy_prime = I_transformed [0 , 1 ]
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+ ixz_prime = I_transformed [0 , 2 ]
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+ iyz_prime = I_transformed [1 , 2 ]
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+
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+ # Transform the Origin (Don't replace the original in case the user keeps the inplace flag false)
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+ Origin_prime = self .origin .transform (tf_matrix )
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+
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+ # Update values and (if requested) put the extracted values into a new_InertialLink
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+ if inplace :
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+ # mass stays the same :-) ==> self.mass = new_InertialLink.mass
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+ self .inertia .ixx = ixx_prime
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+ self .inertia .iyy = iyy_prime
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+ self .inertia .izz = izz_prime
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+ self .inertia .ixy = ixy_prime
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+ self .inertia .ixz = ixz_prime
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+ self .inertia .iyz = iyz_prime
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+ self .origin = Origin_prime
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+ return None
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+ else :
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+ new_InertialLink = InertialLink (mass = self .mass , inertia = Inertia (ixx_prime , iyy_prime , izz_prime , ixy_prime , ixz_prime , iyz_prime ), origin = Origin_prime )
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+ return new_InertialLink
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+
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@classmethod
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def from_xml (cls , xml : ET .Element ) -> "InertialLink" :
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"""
@@ -661,7 +741,7 @@ class VisualLink:
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<Element 'visual' at 0x7f8b3c0b4c70>
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"""
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- name : str
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+ name : Union [ str , None ]
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origin : Origin
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geometry : BaseGeometry
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material : Material
@@ -700,7 +780,8 @@ def to_xml(self, root: Optional[ET.Element] = None) -> ET.Element:
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<Element 'visual' at 0x7f8b3c0b4c70>
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"""
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visual = ET .Element ("visual" ) if root is None else ET .SubElement (root , "visual" )
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- visual .set ("name" , self .name )
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+ if self .name :
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+ visual .set ("name" , self .name )
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self .origin .to_xml (visual )
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self .geometry .to_xml (visual )
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self .material .to_xml (visual )
@@ -722,7 +803,8 @@ def to_mjcf(self, root: ET.Element) -> None:
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<Element 'visual' at 0x7f8b3c0b4c70>
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"""
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visual = root if root .tag == "geom" else ET .SubElement (root , "geom" )
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- visual .set ("name" , self .name )
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+ if self .name :
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+ visual .set ("name" , self .name )
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# TODO: Parent body uses visual origin, these share the same?
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self .origin .to_mjcf (visual )
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@@ -754,7 +836,6 @@ def from_xml(cls, xml: ET.Element) -> "VisualLink":
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VisualLink(name='visual', origin=None, geometry=None, material=None)
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"""
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name = xml .get ("name" )
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-
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origin_element = xml .find ("origin" )
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origin = Origin .from_xml (origin_element ) if origin_element is not None else None
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@@ -784,7 +865,7 @@ class CollisionLink:
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<Element 'collision' at 0x7f8b3c0b4c70>
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"""
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- name : str
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+ name : Union [ str , None ]
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origin : Origin
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geometry : BaseGeometry
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@@ -824,7 +905,8 @@ def to_xml(self, root: Optional[ET.Element] = None) -> ET.Element:
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<Element 'collision' at 0x7f8b3c0b4c70>
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"""
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collision = ET .Element ("collision" ) if root is None else ET .SubElement (root , "collision" )
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- collision .set ("name" , self .name )
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+ if self .name :
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+ collision .set ("name" , self .name )
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self .origin .to_xml (collision )
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self .geometry .to_xml (collision )
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return collision
@@ -858,7 +940,8 @@ def to_mjcf(self, root: ET.Element) -> None:
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<Element 'collision' at 0x7f8b3c0b4c70>
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"""
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collision = root if root .tag == "geom" else ET .SubElement (root , "geom" )
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- collision .set ("name" , self .name )
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+ if self .name :
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+ collision .set ("name" , self .name )
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collision .set ("contype" , "1" )
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collision .set ("conaffinity" , "1" )
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self .origin .to_mjcf (collision )
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