Prerequisites
Definition of terms:
Equations
if:
- the matrix is orthoginal (det(matrix)=1)
- trace = m00 + m11 + m22 + 1 > 0 (the matrix is special orthogonal which cannot represent a reflection component)
then:
qw= sqrt (1 + m00 + m11 + m22) /2
qx = (m21 - m12)/( 4 *qw)
qy = (m02 - m20)/( 4 *qw)
qz = (m10 - m01)/( 4 *qw)
Java Code
Simple Code
public final void set(Matrix4f m1) {
w = Math.sqrt(1.0 + m1.m00 + m1.m11 + m1.m22) / 2.0;
double w4 = (4.0 * w);
x = (m1.m21 - m1.m12) / w4 ;
y = (m1.m02 - m1.m20) / w4 ;
z = (m1.m10 - m1.m01) / w4 ;
}
The above should work assuming that the matrix is orthogonal (it represents
a pure rotation), but if the matrix only represents a pure rotation then it
has a lot of redundant information (9 values which we are converting down to
4) . If it is not a pure rotation then the following algorithm may be more resilient.
Even with orthogonal matrix the value of qw could be very small (or just 0)
and produce big numerical errors when dividing. So it is better to use the following
code:
Better code
1) Calculate the trace(the sum of the diagonal elements) of the matrix T from
the equation:
T = 4 - 4*qx
2 - 4*qy
2 - 4*qz
2
= 4( 1 -qx
2 - qy
2 - qz
2 )
= m00 + m11 + m22 + 1
If the trace of the matrix is greater than zero, then the result is:
S = 0.5 / sqrt(T)
W = 0.25 / S
X = ( m21 - m12 ) * S
Y = ( m02 - m20 ) * S
Z = ( m10 - m01 ) * S
If the trace of the matrix is less than or equal to zero then identify which
major diagonal element has the greatest value.
if (m00 > m11)&(m00 > m22)) {
S = sqrt( 1.0 + m00 - m11 - m22 ) * 2; // S=4*qx
qw = (m12 - m21) / S;
qx = 0.25 * S;
qy = (m01 + m10) / S;
qz = (m02 + m20) / S;
} else if (m11 > m22)) {
S = sqrt( 1.0 + m11 - m00 - m22 ) * 2; // S=4*qy
qw = (m02 - m20) / S;
qx = (m01 + m10) / S;
qy = 0.25 * S;
qz = (m12 + m21) / S;
} else {
S = sqrt( 1.0 + m22 - m00 - m11 ) * 2; // S=4*qz
qw = (m01 - m10) / S;
qx = (m02 + m20) / S;
qy = (m12 + m21) / S;
qz = 0.25 * S;
}
C++ Code (kindly sent to me by Angel)
There is also code from minorlogic at the end of this page.
This includes code for both normalised and unnormalised quaternions.
inline void CalculateRotation( Quaternion& q ) const {
float trace = a[0][0] + a[1][1] + a[2][2] + 1.0f;
if( trace > M_EPSILON ) {
float s = 0.5f / sqrtf(trace);
q.w = 0.25f / s;
q.x = ( a[2][1] - a[1][2] ) * s;
q.y = ( a[0][2] - a[2][0] ) * s;
q.z = ( a[1][0] - a[0][1] ) * s;
} else {
if ( a[0][0] > a[1][1] && a[0][0] > a[2][2] ) {
float s = 2.0f * sqrtf( 1.0f + a[0][0] - a[1][1] - a[2][2]);
q.w = (a[1][2] - a[2][1] ) / s;
q.x = 0.25f * s;
q.y = (a[0][1] + a[1][0] ) / s;
q.z = (a[0][2] + a[2][0] ) / s;
} else if (a[1][1] > a[2][2]) {
float s = 2.0f * sqrtf( 1.0f + a[1][1] - a[0][0] - a[2][2]);
q.w = (a[0][2] - a[2][0] ) / s;
q.x = (a[0][1] + a[1][0] ) / s;
q.y = 0.25f * s;
q.z = (a[1][2] + a[2][1] ) / s;
} else {
float s = 2.0f * sqrtf( 1.0f + a[2][2] - a[0][0] - a[1][1] );
q.w = (a[0][1] - a[1][0] ) / s;
q.x = (a[0][2] + a[2][0] ) / s;
q.y = (a[1][2] + a[2][1] ) / s;
q.z = 0.25f * s;
}
}
}
Alternative Method
Christian has suggested an alternative algorithm and he makes a convincing argument that this is more efficient here.
quaternion.w = sqrt( max( 0, 1 + m00 + m11
+ m22 ) ) / 2;
quaternion.x = sqrt( max( 0, 1 + m00 - m11
- m22 ) ) / 2;
quaternion.y = sqrt( max( 0, 1 - m00 + m11
- m22 ) ) / 2;
quaternion.z = sqrt( max( 0, 1 - m00 - m11
+ m22 ) ) / 2;
Q.x = _copysign( Q.x, m21 - m12 )
Q.y = _copysign( Q.y, m02 - m20 )
Q.z = _copysign( Q.z, m10 - m01 )
- The max( 0, ... ) is just a
safeguard against rounding error.
- copysign takes the sign from the second term and sets the sign of the first without altering the magnitude, I don't know of a java equivalent.
Scaling
Since it is possible for both matrices and quaternions to represent scaling in addition to rotation, then it would be possible to include this in the convertion. In most cases this is not necessary, as we only want to represent rotations, but if you do need to include a scale factor then you might want to try this method suggested by Christian.
Of course, this will mean that the matrix is no longer orthogonal and that the quaternion is no longer normalised.
We first calculate absQ2 which is the cube root of the volume
spanned by the matrix axes.
absQ2 = det(
matrix )^(1/3)
quaternion.w = sqrt( max( 0,
absQ2 + m00 + m11 + m22 ) ) / 2;
...etc
Rounding Errors
When comparing different methods
of doing this conversion I think we should consider sensitivity to rounding errors. In other words, the matrix
contains redundant information so, althrough a matrix may initially be orthogonal, if we then do some rotation operations rounding errors may
de-orthogonalise the matrix, if this happens which method is most
likely to cancel out the errors?
I don't know
how best to tackle this? say, for instance, rounding errors
introduce an error 'delta e' to one element of
the matrix, but we don't know which element has the error. Which
method is most likely to cancel out this error? Which method is
most likely to produce a normalised
quaternion?
Derivation of Equations
Quaternion multiplication and orthogonal matrix multiplication can both be
used to represent rotation. If a quaternion is represented by qw + i
qx + j qy + k qz , then the equivalent matrix, to represent the
same rotation, is:
| 1 - 2*qy2 - 2*qz2 |
2*qx*qy - 2*qz*qw |
2*qx*qz + 2*qy*qw |
| 2*qx*qy + 2*qz*qw |
1 - 2*qx2 - 2*qz2 |
2*qy*qz - 2*qx*qw |
| 2*qx*qz - 2*qy*qw |
2*qy*qz + 2*qx*qw |
1 - 2*qx2 - 2*qy2 |
This assumes that the quaternion is normalised (qw2 + qx2
+ qy2 + qz2 =1) and that the matrix is orthogonal.
This
page discusses the equivalence of quaternion multiplication and orthogonal
matrix multiplication.
So this gives the following equations:
- m00 = 1 - 2*qy2 - 2*qz2
- m01 = 2*qx*qy - 2*qz*qw
- m02 = 2*qx*qz + 2*qy*qw
- m10 = 2*qx*qy + 2*qz*qw
- m11 = 1 - 2*qx2 - 2*qz2
- m12 = 2*qy*qz - 2*qx*qw
- m20 = 2*qx*qz - 2*qy*qw
- m21 = 2*qy*qz + 2*qx*qw
- m22 = 1 - 2*qx2 - 2*qy2
This contains more information than we need, so we need to choose a method
which is less sensitive to matrix not being orthogonal.
If the quaternion is normalised: qx2 + qy2 + qz2+
qw2 = 1
so,
qw2 = 1 - qx2 - qy2 - qz2
multiply both sides by 4 gives,
4 * qw2 = 4 - 4*qx2 - 4*qy2 - 4*qz2
4 * qw2 = 1 + 1 - 2*qy2 - 2*qz2 + 1 - 2*qx2
- 2*qz2 + 1 - 2*qx2 - 2*qy2
4 * qw2 = 1 + m00 + m11 + m22
so qw= sqrt (1 + m00 + m11 + m22) /2
the sum of the diagonal elements is known as the trace (Tr), this gives,
qw= sqrt (1 + Tr) /2
this method can only be used if we are taking the square root of a positive
number ie,
1 + Tr <= 0
Is this always the case for orthogonal
matrices ???
So we have an equation for qw, to get the other values we can use:
m21 - m12 = 2*qy*qz - 2*qx*qw - 2*qy*qz - 2*qx*qw
m21 - m12 = 4 *qx*qw
therefore:
qx = (m21 - m12)/( 4 *qw)
now calculate qy
m02 - m20 = 2*qx*qz + 2*qy*qw - 2*qx*qz + 2*qy*qw
m02 - m20 = 4*qy*qw
therefore:
qy = (m02 - m20)/( 4 *qw)
now calculate qz,
m10 - m01 = 2*qx*qy + 2*qz*qw - 2*qx*qy + 2*qz*qw
m10 - m01 = 4*qz*qw
therefore:
qz = (m10 - m01)/( 4 *qw)
so summarising the results:
- qw= sqrt (1 + m00 + m11 + m22) /2
- qx = (m21 - m12)/( 4 *qw)
- qy = (m02 - m20)/( 4 *qw)
- qz = (m10 - m01)/( 4 *qw)
Some other results:
|
1 + m00 - m11 - m22
= 1 + 1 - 2*qy2 - 2*qz2 - 1 + 2*qx2 +
2*qz2 - 1 + 2*qx2 + 2*qy2
= 4*qx2
therefore:
qx =sqrt (1 + m00 - m11 - m22) /2 |
|
1 + m11 - m00 - m22
= 1 + 1 - 2*qx2 - 2*qz2 - 1 + 2*qy2 +
2*qz2 - 1 + 2*qx2 + 2*qy2
= 4*qy2
therefore:
qy =sqrt (1 + m11 - m00 - m22) /2 |
|
1 + m22 - m00 - m11
= 1 +1 - 2*qx2 - 2*qy2 - 1 + 2*qy2 +
2*qz2 - 1 + 2*qx2 + 2*qz2
= 4*qz2
therefore:
qz =sqrt (1 + m22 - m00 - m11) /2 |
Issues
This page assumes:
If these conditions are satisfied then the resulting quaternion should be normalised.
Rotation about a point other than origin
Quaternions and 3x3 matrices alone can only represent rotations about the origin.
But if we include a 3D vector with the quaternion we can use this to represent
the point about which we are rotating. Also if we use a 4x4 matrix then this
can hold a translation (as explained
here) and therefore can specify a rotation about a point.
The following code generates a 3D vector (representing the centre of rotation)
from the 4x4 matrix. The theory is given
here.
|
|
= 1/det[m] * |
| (m11 - 1)*m22 - m12*m21 |
m02*m21 - m01*(m22 - 1) |
m01*m12 - m02*(m11 - 1) |
| m12*m20 - m10*(m22 - 1) |
m00*(m22 - 1) - m02*m20 |
m02*m10 - (m00 - 1)*m12 |
| m10*m21 - (m11 - 1)*m20 |
m01*m20 - (m00 - 1)*m21 |
m00*(m11 - 1) - m01*m10 |
|
|
Example
| we take the 90 degree rotation from this: |
 |
to this: |
 |
As shown here
the matrix for this rotation is:
So using the above result:
qw= sqrt (1 + m00 + m11 + m22) /2 = sqrt (2)/2 = 1.4142/2 = 0.7071
qx = (m21 - m12)/( 4 *qw) = 2/(4 * 0.7071) = 1/ 1.4142 = 0.7071
qy = (m02 - m20)/( 4 *qw) = 0
qz = (m10 - m01)/( 4 *qw) = 0
This gives the quaternion 0.7071 + i 0.7071
As you can see here,
this gives the result that we are looking for.
Angle Calculator and Further examples
I have put a java applet here which allows the values to be entered and the converted values shown along with a graphical representation of the orientation.
Also further examples in 90 degree steps here
This site may have errors. Don't use for critical systems.