m2q_c |
Table of contents
Procedurem2q_c ( Matrix to quaternion ) void m2q_c ( ConstSpiceDouble r[3][3], SpiceDouble q[4] ) AbstractFind a unit quaternion corresponding to a specified rotation matrix. Required_ReadingROTATION KeywordsMATH MATRIX ROTATION Brief_I/OVARIABLE I/O DESCRIPTION -------- --- -------------------------------------------------- r I A rotation matrix. q O A unit quaternion representing `r'. Detailed_Inputr is a rotation matrix. Detailed_Outputq is a unit-length SPICE-style quaternion representing `r'. See the discussion of quaternion styles in -Particulars below. `q' is a 4-dimensional vector. If `r' rotates vectors in the counterclockwise sense by an angle of `theta' radians about a unit vector `a', where 0 < theta < pi - - then letting h = theta/2, q = ( cos(h), sin(h)a , sin(h)a , sin(h)a ). 1 2 3 The restriction that `theta' must be in the range [0, pi] determines the output quaternion `q' uniquely except when theta = pi; in this special case, both of the quaternions q = ( 0, a , a , a ) 1 2 3 and q = ( 0, -a , -a , -a ) 1 2 3 are possible outputs. ParametersNone. Exceptions1) If `r' is not a rotation matrix, the error SPICE(NOTAROTATION) is signaled by a routine in the call tree of this routine. FilesNone. ParticularsA unit quaternion is a 4-dimensional vector for which the sum of the squares of the components is 1. Unit quaternions can be used to represent rotations in the following way: given a rotation angle `theta', where 0 < theta < pi - - and a unit vector `a', we can represent the transformation that rotates vectors in the counterclockwise sense by theta radians about `a' using the quaternion `q', where q = ( cos(theta/2), sin(theta/2)a , sin(theta/2)a , sin(theta/2)a ) 1 2 3 As mentioned in Detailed Output, our restriction on the range of `theta' determines `q' uniquely, except when theta = pi. The CSPICE routine q2m_c is an one-sided inverse of this routine: given any rotation matrix `r', the calls m2q_c ( r, q ); q2m_c ( q, r ); leave `r' unchanged, except for round-off error. However, the calls q2m_c ( q, r ); m2q_c ( r, q ); might preserve `q' or convert `q' to -q. Quaternion Styles ----------------- There are different "styles" of quaternions used in science and engineering applications. Quaternion styles are characterized by - The order of quaternion elements - The quaternion multiplication formula - The convention for associating quaternions with rotation matrices Two of the commonly used styles are - "SPICE" > Invented by Sir William Rowan Hamilton > Frequently used in mathematics and physics textbooks - "Engineering" > Widely used in aerospace engineering applications CSPICE function interfaces ALWAYS use SPICE quaternions. Quaternions of any other style must be converted to SPICE quaternions before they are passed to CSPICE functions. Relationship between SPICE and Engineering Quaternions ------------------------------------------------------ Let M be a rotation matrix such that for any vector V, M*V is the result of rotating V by theta radians in the counterclockwise direction about unit rotation axis vector A. Then the SPICE quaternions representing M are (+/-) ( cos(theta/2), sin(theta/2) A(1), sin(theta/2) A(2), sin(theta/2) A(3) ) while the engineering quaternions representing M are (+/-) ( -sin(theta/2) A(1), -sin(theta/2) A(2), -sin(theta/2) A(3), cos(theta/2) ) For both styles of quaternions, if a quaternion q represents a rotation matrix M, then -q represents M as well. Given an engineering quaternion QENG = ( q0, q1, q2, q3 ) the equivalent SPICE quaternion is QSPICE = ( q3, -q0, -q1, -q2 ) Associating SPICE Quaternions with Rotation Matrices ---------------------------------------------------- Let FROM and TO be two right-handed reference frames, for example, an inertial frame and a spacecraft-fixed frame. Let the symbols V , V FROM TO denote, respectively, an arbitrary vector expressed relative to the FROM and TO frames. Let M denote the transformation matrix that transforms vectors from frame FROM to frame TO; then V = M * V TO FROM where the expression on the right hand side represents left multiplication of the vector by the matrix. Then if the unit-length SPICE quaternion q represents M, where q = (q0, q1, q2, q3) the elements of M are derived from the elements of q as follows: +- -+ | 2 2 | | 1 - 2*( q2 + q3 ) 2*(q1*q2 - q0*q3) 2*(q1*q3 + q0*q2) | | | | | | 2 2 | M = | 2*(q1*q2 + q0*q3) 1 - 2*( q1 + q3 ) 2*(q2*q3 - q0*q1) | | | | | | 2 2 | | 2*(q1*q3 - q0*q2) 2*(q2*q3 + q0*q1) 1 - 2*( q1 + q2 ) | | | +- -+ Note that substituting the elements of -q for those of q in the right hand side leaves each element of M unchanged; this shows that if a quaternion q represents a matrix M, then so does the quaternion -q. To map the rotation matrix M to a unit quaternion, we start by decomposing the rotation matrix as a sum of symmetric and skew-symmetric parts: 2 M = [ I + (1-cos(theta)) OMEGA ] + [ sin(theta) OMEGA ] symmetric skew-symmetric OMEGA is a skew-symmetric matrix of the form +- -+ | 0 -n3 n2 | | | OMEGA = | n3 0 -n1 | | | | -n2 n1 0 | +- -+ The vector N of matrix entries (n1, n2, n3) is the rotation axis of M and theta is M's rotation angle. Note that N and theta are not unique. Let C = cos(theta/2) S = sin(theta/2) Then the unit quaternions Q corresponding to M are Q = +/- ( C, S*n1, S*n2, S*n3 ) The mappings between quaternions and the corresponding rotations are carried out by the CSPICE routines q2m_c {quaternion to matrix} m2q_c {matrix to quaternion} m2q_c always returns a quaternion with scalar part greater than or equal to zero. SPICE Quaternion Multiplication Formula --------------------------------------- Given a SPICE quaternion Q = ( q0, q1, q2, q3 ) corresponding to rotation axis A and angle theta as above, we can represent Q using "scalar + vector" notation as follows: s = q0 = cos(theta/2) v = ( q1, q2, q3 ) = sin(theta/2) * A Q = s + v Let Q1 and Q2 be SPICE quaternions with respective scalar and vector parts s1, s2 and v1, v2: Q1 = s1 + v1 Q2 = s2 + v2 We represent the dot product of v1 and v2 by <v1, v2> and the cross product of v1 and v2 by v1 x v2 Then the SPICE quaternion product is Q1*Q2 = s1*s2 - <v1,v2> + s1*v2 + s2*v1 + (v1 x v2) If Q1 and Q2 represent the rotation matrices M1 and M2 respectively, then the quaternion product Q1*Q2 represents the matrix product M1*M2 Examples1) A case amenable to checking by hand calculation: To convert the rotation matrix +- -+ | 0 1 0 | | | r = | -1 0 0 | | | | 0 0 1 | +- -+ also represented as [ pi/2 ] 3 to a quaternion, we can use the code fragment rotate_c ( halfpi_c(), 3, r ); m2q_c ( r, q ); m2q_c will return `q' as ( sqrt(2)/2, 0, 0, -sqrt(2)/2 ) Why? Well, `r' is a reference frame transformation that rotates vectors by -pi/2 radians about the axis vector a = ( 0, 0, 1 ) Equivalently, `r' rotates vectors by pi/2 radians in the counterclockwise sense about the axis vector -a = ( 0, 0, -1 ) so our definition of `q', h = theta/2 q = ( cos(h), sin(h)a , sin(h)a , sin(h)a ) 1 2 3 implies that in this case, q = ( cos(pi/4), 0, 0, -sin(pi/4) ) = ( sqrt(2)/2, 0, 0, -sqrt(2)/2 ) 2) Finding a quaternion that represents a rotation specified by a set of Euler angles: Suppose our original rotation `r' is the product [ tau ] [ pi/2 - delta ] [ alpha ] . 3 2 3 The code fragment eul2m_c ( tau, halfpi_c() - delta, alpha, 3, 2, 3, r ); m2q_c ( r, q ); yields a quaternion `q' that represents `r'. RestrictionsNone. Literature_ReferencesNone. Author_and_InstitutionN.J. Bachman (JPL) J. Diaz del Rio (ODC Space) W.L. Taber (JPL) E.D. Wright (JPL) Version-CSPICE Version 1.1.2, 24-AUG-2021 (JDR) Edited the header to comply with NAIF standard. Moved ROTATIONS required reading from -Literature_References to -Required_Reading section. -CSPICE Version 1.1.1, 27-FEB-2008 (NJB) Updated header; added information about SPICE quaternion conventions. Made minor edits throughout header. -CSPICE Version 1.1.0, 21-OCT-1998 (NJB) Made input matrix const. -CSPICE Version 1.0.1, 13-FEB-1998 (EDW) Minor corrections to header. -CSPICE Version 1.0.0, 08-FEB-1998 (NJB) (WLT) Based on SPICELIB Version 1.0.1, 10-MAR-1992 (WLT) Index_Entriesmatrix to quaternion |
Fri Dec 31 18:41:09 2021