Unit quaternions, known as versors, provide a convenient mathematical notation for representing spatial orientations and rotations of elements in three dimensional space. Specifically, they encode information about an axisangle rotation about an arbitrary axis. Rotation and orientation quaternions have applications in computer graphics,^{[1]} computer vision, robotics,^{[2]} navigation, molecular dynamics, flight dynamics,^{[3]} orbital mechanics of satellites,^{[4]} and crystallographic texture analysis.^{[5]}
When used to represent rotation, unit quaternions are also called rotation quaternions as they represent the 3D rotation group. When used to represent an orientation (rotation relative to a reference coordinate system), they are called orientation quaternions or attitude quaternions. A spatial rotation around a fixed point of radians about a unit axis that denotes the Euler axis is given by the quaternion , where and .
Compared to rotation matrices, quaternions are more compact, efficient, and numerically stable. Compared to Euler angles, they are simpler to compose. However, they are not as intuitive and easy to understand and, due to the periodic nature of sine and cosine, rotation angles differing precisely by the natural period will be encoded into identical quaternions and recovered angles in radians will be limited to .
In 3dimensional space, according to Euler's rotation theorem, any rotation or sequence of rotations of a rigid body or coordinate system about a fixed point is equivalent to a single rotation by a given angle about a fixed axis (called the Euler axis) that runs through the fixed point.^{[6]} The Euler axis is typically represented by a unit vector ( in the picture). Therefore, any rotation in three dimensions can be represented as via a vector and an angle .
Quaternions give a simple way to encode this ^{[7]} axis–angle representation using four real numbers, and can be used to apply (calculate) the corresponding rotation to a position vector (x,y,z), representing a point relative to the origin in R^{3}.
Euclidean vectors such as (2, 3, 4) or (a_{x}, a_{y}, a_{z}) can be rewritten as 2 i + 3 j + 4 k or a_{x} i + a_{y} j + a_{z} k, where i, j, k are unit vectors representing the three Cartesian axes (traditionally x, y, z), and also obey the multiplication rules of the fundamental quaternion units by interpreting the Euclidean vector (a_{x}, a_{y}, a_{z}) as the vector part of the pure quaternion (0, a_{x}, a_{y}, a_{z}).
A rotation of angle around the axis defined by the unit vector
can be represented by conjugation by a unit quaternion q. Since the quaternion product gives 1, using the Taylor series of the exponential function, the extension of Euler's formula results:
It can be shown^{[8]} that the desired rotation can be applied to an ordinary vector in 3dimensional space, considered as the vector part of the pure quaternion , by evaluating the conjugation of p′ by q, given by:
using the Hamilton product, where the vector part of the pure quaternion L(p′) = (0, r_{x}, r_{y}, r_{z}) is the new position vector of the point after the rotation. In a programmatic implementation, the conjugation is achieved by constructing a pure quaternion whose vector part is p, and then performing the quaternion conjugation. The vector part of the resulting pure quaternion is the desired vector r. Clearly, provides a linear transformation of the quaternion space to itself;^{[9]} also, since is unitary, the transformation is an isometry. Also, and so leaves vectors parallel to invariant. So, by decomposing as a vector parallel to the vector part of and a vector normal to the vector part of and showing that the application of to the normal component of rotates it, the claim is shown. So let be the component of orthogonal to the vector part of and let . It turns out that the vector part of is given by
The conjugation of p′ by q can be expressed with fewer arithmetic operations as:
A geometric fact independent of quaternions is the existence of a twotoone mapping from physical rotations to rotational transformation matrices. If 0 ⩽ ⩽ , a physical rotation about by and a physical rotation about by both achieve the same final orientation by disjoint paths through intermediate orientations. By inserting those vectors and angles into the formula for q above, one finds that if q represents the first rotation, −q represents the second rotation. This is a geometric proof that conjugation by q and by −q must produce the same rotational transformation matrix. That fact is confirmed algebraically by noting that the conjugation is quadratic in q, so the sign of q cancels, and does not affect the result. (See 2:1 mapping of SU(2) to SO(3)) If both rotations are a halfturn , both q and −q will have a real coordinate equal to zero. Otherwise, one will have a positive real part, representing a rotation by an angle less than , and the other will have a negative real part, representing a rotation by an angle greater than .
Mathematically, this operation carries the set of all "pure" quaternions p (those with real part equal to zero)—which constitute a 3dimensional space among the quaternions—into itself, by the desired rotation about the axis u, by the angle θ. (Each real quaternion is carried into itself by this operation. But for the purpose of rotations in 3dimensional space, we ignore the real quaternions.)
The rotation is clockwise if our line of sight points in the same direction as .
In this (which?) instance, q is a unit quaternion and
It follows that conjugation by the product of two quaternions is the composition of conjugations by these quaternions: If p and q are unit quaternions, then rotation (conjugation) by pq is
which is the same as rotating (conjugating) by q and then by p. The scalar component of the result is necessarily zero.
The quaternion inverse of a rotation is the opposite rotation, since . The square of a quaternion rotation is a rotation by twice the angle around the same axis. More generally q^{n} is a rotation by n times the angle around the same axis as q. This can be extended to arbitrary real n, allowing for smooth interpolation between spatial orientations; see Slerp.
Two rotation quaternions can be combined into one equivalent quaternion by the relation:
in which q′ corresponds to the rotation q_{1} followed by the rotation q_{2}. Thus, an arbitrary number of rotations can be composed together and then applied as a single rotation. (Note that quaternion multiplication is not commutative.)
Conjugating p by q refers to the operation p ↦ qpq^{−1}.
Consider the rotation f around the axis , with a rotation angle of 120°, or 2π/3 radians.
The length of is √3, the half angle is π/3 (60°) with cosine 1/2, (cos 60° = 0.5) and sine √3/2, (sin 60° ≈ 0.866). We are therefore dealing with a conjugation by the unit quaternion
If f is the rotation function,
It can be proven that the inverse of a unit quaternion is obtained simply by changing the sign of its imaginary components. As a consequence,
and
This can be simplified, using the ordinary rules for quaternion arithmetic, to
As expected, the rotation corresponds to keeping a cube held fixed at one point, and rotating it 120° about the long diagonal through the fixed point (observe how the three axes are permuted cyclically).
A quaternion rotation (with ) can be algebraically manipulated into a matrix rotation , where is the rotation matrix given by:^{[10]}
Here and if q is a unit quaternion, .
This can be obtained by using vector calculus and linear algebra if we express and as scalar and vector parts and use the formula for the multiplication operation in the equation . If we write as , as and as , where , our equation turns into . By using the formula for multiplication of two quaternions that are expressed as scalar and vector parts,
this equation can be rewritten as
where denotes the outer product, is the identity matrix and is the transformation matrix that when multiplied from the right with a vector gives the cross product .
Since , we can identify as , which upon expansion should result in the expression written in matrix form above.
The expression rotates any vector quaternion around an axis given by the vector by the angle , where and depends on the quaternion .
and can be found from the following equations:
where is the twoargument arctangent. While works, it is numerically unstable (inaccurate) near for numbers with finite precision.
Care should be taken when the quaternion approaches a scalar, since due to degeneracy the axis of an identity rotation is not welldefined.
A benefit of the quaternion formulation of the composition of two rotations R_{B} and R_{A} is that it yields directly the rotation axis and angle of the composite rotation R_{C} = R_{B}R_{A}.
Let the quaternion associated with a spatial rotation R be constructed from its rotation axis S with the rotation angle around this axis. The associated quaternion is given by Then the composition of the rotation R_{B} with R_{A} is the rotation R_{C} = R_{B}R_{A} with rotation axis and angle defined by the product of the quaternions that is
Expand this product to obtain
Divide both sides of this equation by the identity, which is the law of cosines on a sphere, and compute
This is Rodrigues' formula for the axis of a composite rotation defined in terms of the axes of the two rotations. He derived this formula in 1840 (see page 408).^{[11]}
The three rotation axes A, B, and C form a spherical triangle and the dihedral angles between the planes formed by the sides of this triangle are defined by the rotation angles. Hamilton^{[12]} presented the component form of these equations showing that the quaternion product computes the third vertex of a spherical triangle from two given vertices and their associated arclengths, which is also defines an algebra for points in Elliptic geometry.
The normalized rotation axis, removing the from the expanded product, leaves the vector which is the rotation axis, times some constant. Care should be taken normalizing the axis vector when is or where the vector is near ; which is identity, or 0 rotation around any axis.
Or with angle addition trigonometric substitutions...
finally normalizing the rotation axis: or .
The rotated quaternion p' = q p q^{−1} needs to be differentiated with respect to the rotating quaternion q, when the rotation is estimated from numerical optimization. The estimation of rotation angle is an essential procedure in 3D object registration or camera calibration. For unitary q and pure imaginary p, that is for a rotation in 3D space, the derivatives of the rotated quaternion can be represented using matrix calculus notation as
A derivation can be found in.^{[13]}
The complex numbers can be defined by introducing an abstract symbol i which satisfies the usual rules of algebra and additionally the rule i^{2} = −1. This is sufficient to reproduce all of the rules of complex number arithmetic: for example:
In the same way the quaternions can be defined by introducing abstract symbols i, j, k which satisfy the rules i^{2} = j^{2} = k^{2} = i j k = −1 and the usual algebraic rules except the commutative law of multiplication (a familiar example of such a noncommutative multiplication is matrix multiplication). From this all of the rules of quaternion arithmetic follow, such as the rules on multiplication of quaternion basis elements. Using these rules, one can show that:
The imaginary part of a quaternion behaves like a vector in threedimensional vector space, and the real part a behaves like a scalar in R. When quaternions are used in geometry, it is more convenient to define them as a scalar plus a vector:
Some might find it strange to add a number to a vector, as they are objects of very different natures, or to multiply two vectors together, as this operation is usually undefined. However, if one remembers that it is a mere notation for the real and imaginary parts of a quaternion, it becomes more legitimate. In other words, the correct reasoning is the addition of two quaternions, one with zero vector/imaginary part, and another one with zero scalar/real part:
We can express quaternion multiplication in the modern language of vector cross and dot products (which were actually inspired by the quaternions in the first place^{[14]}). When multiplying the vector/imaginary parts, in place of the rules i^{2} = j^{2} = k^{2} = ijk = −1 we have the quaternion multiplication rule:
where:
Quaternion multiplication is noncommutative (because of the cross product, which anticommutes), while scalar–scalar and scalar–vector multiplications commute. From these rules it follows immediately that (see Quaternions § Quaternions and threedimensional geometry):
The (left and right) multiplicative inverse or reciprocal of a nonzero quaternion is given by the conjugatetonorm ratio (see details):
as can be verified by direct calculation (note the similarity to the multiplicative inverse of complex numbers).
Let be a unit vector (the rotation axis) and let . Our goal is to show that
yields the vector rotated by an angle around the axis . Expanding out (and bearing in mind that ), we have
If we let and equal the components of perpendicular and parallel to respectively, then and , leading to
Using the trigonometric pythagorean and doubleangle identities, we then have
This is the formula of a rotation by around the u→ axis.
A very formal explanation of the properties used in this section is given by Altman.^{[15]}
Unit quaternions represent the group of Euclidean rotations in three dimensions in a very straightforward way. The correspondence between rotations and quaternions can be understood by first visualizing the space of rotations itself.
In order to visualize the space of rotations, it helps to consider a simpler case. Any rotation in three dimensions can be described by a rotation by some angle about some axis; for our purposes, we will use an axis vector to establish handedness for our angle. Consider the special case in which the axis of rotation lies in the xy plane. We can then specify the axis of one of these rotations by a point on a circle through which the vector crosses, and we can select the radius of the circle to denote the angle of rotation.
Similarly, a rotation whose axis of rotation lies in the xy plane can be described as a point on a sphere of fixed radius in three dimensions. Beginning at the north pole of a sphere in threedimensional space, we specify the point at the north pole to be the identity rotation (a zero angle rotation). Just as in the case of the identity rotation, no axis of rotation is defined, and the angle of rotation (zero) is irrelevant. A rotation having a very small rotation angle can be specified by a slice through the sphere parallel to the xy plane and very near the north pole. The circle defined by this slice will be very small, corresponding to the small angle of the rotation. As the rotation angles become larger, the slice moves in the negative z direction, and the circles become larger until the equator of the sphere is reached, which will correspond to a rotation angle of 180 degrees. Continuing southward, the radii of the circles now become smaller (corresponding to the absolute value of the angle of the rotation considered as a negative number). Finally, as the south pole is reached, the circles shrink once more to the identity rotation, which is also specified as the point at the south pole.
Notice that a number of characteristics of such rotations and their representations can be seen by this visualization. The space of rotations is continuous, each rotation has a neighborhood of rotations which are nearly the same, and this neighborhood becomes flat as the neighborhood shrinks. Also, each rotation is actually represented by two antipodal points on the sphere, which are at opposite ends of a line through the center of the sphere. This reflects the fact that each rotation can be represented as a rotation about some axis, or, equivalently, as a negative rotation about an axis pointing in the opposite direction (a socalled double cover). The "latitude" of a circle representing a particular rotation angle will be half of the angle represented by that rotation, since as the point is moved from the north to south pole, the latitude ranges from zero to 180 degrees, while the angle of rotation ranges from 0 to 360 degrees. (the "longitude" of a point then represents a particular axis of rotation.) Note however that this set of rotations is not closed under composition. Two successive rotations with axes in the xy plane will not necessarily give a rotation whose axis lies in the xy plane, and thus cannot be represented as a point on the sphere. This will not be the case with a general rotation in 3space, in which rotations do form a closed set under composition.
This visualization can be extended to a general rotation in 3dimensional space. The identity rotation is a point, and a small angle of rotation about some axis can be represented as a point on a sphere with a small radius. As the angle of rotation grows, the sphere grows, until the angle of rotation reaches 180 degrees, at which point the sphere begins to shrink, becoming a point as the angle approaches 360 degrees (or zero degrees from the negative direction). This set of expanding and contracting spheres represents a hypersphere in four dimensional space (a 3sphere). Just as in the simpler example above, each rotation represented as a point on the hypersphere is matched by its antipodal point on that hypersphere. The "latitude" on the hypersphere will be half of the corresponding angle of rotation, and the neighborhood of any point will become "flatter" (i.e. be represented by a 3D Euclidean space of points) as the neighborhood shrinks. This behavior is matched by the set of unit quaternions: A general quaternion represents a point in a four dimensional space, but constraining it to have unit magnitude yields a threedimensional space equivalent to the surface of a hypersphere. The magnitude of the unit quaternion will be unity, corresponding to a hypersphere of unit radius. The vector part of a unit quaternion represents the radius of the 2sphere corresponding to the axis of rotation, and its magnitude is the sine of half the angle of rotation. Each rotation is represented by two unit quaternions of opposite sign, and, as in the space of rotations in three dimensions, the quaternion product of two unit quaternions will yield a unit quaternion. Also, the space of unit quaternions is "flat" in any infinitesimal neighborhood of a given unit quaternion.
We can parameterize the surface of a sphere with two coordinates, such as latitude and longitude. But latitude and longitude are illbehaved (degenerate as described by the hairy ball theorem) at the north and south poles, though the poles are not intrinsically different from any other points on the sphere. At the poles (latitudes +90° and −90°), the longitude becomes meaningless.
It can be shown that no twoparameter coordinate system can avoid such degeneracy. We can avoid such problems by embedding the sphere in threedimensional space and parameterizing it with three Cartesian coordinates (w, x, y), placing the north pole at (w, x, y) = (1, 0, 0), the south pole at (w, x, y) = (−1, 0, 0), and the equator at w = 0, x^{2} + y^{2} = 1. Points on the sphere satisfy the constraint w^{2} + x^{2} + y^{2} = 1, so we still have just two degrees of freedom though there are three coordinates. A point (w, x, y) on the sphere represents a rotation in the ordinary space around the horizontal axis directed by the vector (x, y, 0) by an angle .
In the same way the hyperspherical space of 3D rotations can be parameterized by three angles (Euler angles), but any such parameterization is degenerate at some points on the hypersphere, leading to the problem of gimbal lock. We can avoid this by using four Euclidean coordinates w, x, y, z, with w^{2} + x^{2} + y^{2} + z^{2} = 1. The point (w, x, y, z) represents a rotation around the axis directed by the vector (x, y, z) by an angle
The multiplication of quaternions is noncommutative. This fact explains how the p ↦ q p q^{−1} formula can work at all, having q q^{−1} = 1 by definition. Since the multiplication of unit quaternions corresponds to the composition of threedimensional rotations, this property can be made intuitive by showing that threedimensional rotations are not commutative in general.
The figure to the right illustrates this with dice. Use your right hand to create a pair of 90 degree rotations. Both dice are initially configured as shown in the upper lefthand corner (with 1 dot on the top face.) Path A begins with a rotation about the –y axis (using the righthand rule.), followed by a rotation about the +z axis, resulting in the configuration shown in the lower left corner (5 dots on the top face.) Path B reverses the order of operations, resulting with 3 dots on top.
If you don't have dice, set two books next to each other. Rotate one of them 90 degrees clockwise around the z axis, then flip it 180 degrees around the x axis. Take the other book, flip it 180° around x axis first, and 90° clockwise around z later. The two books do not end up parallel. This shows that, in general, the composition of two different rotations around two distinct spatial axes will not commute.
The vector cross product, used to define the axis–angle representation, does confer an orientation ("handedness") to space: in a threedimensional vector space, the three vectors in the equation a × b = c will always form a righthanded set (or a lefthanded set, depending on how the cross product is defined), thus fixing an orientation in the vector space. Alternatively, the dependence on orientation is expressed in referring to such that specifies a rotation as to axial vectors. In quaternionic formalism the choice of an orientation of the space corresponds to order of multiplication: ij = k but ji = −k. If one reverses the orientation, then the formula above becomes p ↦ q^{−1} p q, i.e., a unit q is replaced with the conjugate quaternion – the same behaviour as of axial vectors.
It is reported^{[16]} that the existence and continued usage of an alternative quaternion convention in the aerospace and, to a lesser extent, robotics community is incurring a significant and ongoing cost [sic]. This alternative convention is proposed by Shuster M.D. in ^{[17]} and departs from tradition by reversing the definition for multiplying quaternion basis elements such that under Shuster's convention, whereas Hamilton's definition is . This convention is also referred to as "JPL convention" for its use in some parts of NASA's Jet Propulsion Laboratory.
Under Shuster's convention, the formula for multiplying two quaternions is altered such that
The formula for rotating a vector by a quaternion is altered to be
To identify the changes under Shuster's convention, see that the sign before the cross product is flipped from plus to minus.
Finally, the formula for converting a quaternion to a rotation matrix is altered to be
which is exactly the transpose of the rotation matrix converted under the traditional convention.
The table below groups applications by their adherence to either quaternion convention:^{[16]}
Hamilton multiplication convention  Shuster multiplication convention 



While use of either convention does not impact the capability or correctness of applications thus created, the authors of ^{[16]} argued that the Shuster convention should be abandoned because it departs from the much older quaternion multiplication convention by Hamilton and may never be adopted by the mathematical or theoretical physics areas.
The representation of a rotation as a quaternion (4 numbers) is more compact than the representation as an orthogonal matrix (9 numbers). Furthermore, for a given axis and angle, one can easily construct the corresponding quaternion, and conversely, for a given quaternion one can easily read off the axis and the angle. Both of these are much harder with matrices or Euler angles.
In video games and other applications, one is often interested in "smooth rotations", meaning that the scene should slowly rotate and not in a single step. This can be accomplished by choosing a curve such as the spherical linear interpolation in the quaternions, with one endpoint being the identity transformation 1 (or some other initial rotation) and the other being the intended final rotation. This is more problematic with other representations of rotations.
When composing several rotations on a computer, rounding errors necessarily accumulate. A quaternion that is slightly off still represents a rotation after being normalized: a matrix that is slightly off may not be orthogonal any more and is harder to convert back to a proper orthogonal matrix.
Quaternions also avoid a phenomenon called gimbal lock which can result when, for example in pitch/yaw/roll rotational systems, the pitch is rotated 90° up or down, so that yaw and roll then correspond to the same motion, and a degree of freedom of rotation is lost. In a gimbalbased aerospace inertial navigation system, for instance, this could have disastrous results if the aircraft is in a steep dive or ascent.
The orthogonal matrix corresponding to a rotation by the unit quaternion z = a + b i + c j + d k (with  z  = 1) when postmultiplying with a column vector is given by
This rotation matrix is used on vector w as . The quaternion representation of this rotation is given by:
where is the conjugate of the quaternion , given by
Also, quaternion multiplication is defined as (assuming a and b are quaternions, like z above):
where the order a, b is important since the cross product of two vectors is not commutative.
A more efficient calculation in which the quaternion does not need to be unit normalized is given by^{[20]}
where the following intermediate quantities have been defined:
One must be careful when converting a rotation matrix to a quaternion, as several straightforward methods tend to be unstable when the trace (sum of the diagonal elements) of the rotation matrix is zero or very small. For a stable method of converting an orthogonal matrix to a quaternion, see the Rotation matrix#Quaternion.
The above section described how to recover a quaternion q from a 3 × 3 rotation matrix Q. Suppose, however, that we have some matrix Q that is not a pure rotation—due to roundoff errors, for example—and we wish to find the quaternion q that most accurately represents Q. In that case we construct a symmetric 4 × 4 matrix
and find the eigenvector (x, y, z, w) corresponding to the largest eigenvalue (that value will be 1 if and only if Q is a pure rotation). The quaternion so obtained will correspond to the rotation closest to the original matrix Q ^{[dubious – discuss]}.^{[21]}
This section discusses the performance implications of using quaternions versus other methods (axis/angle or rotation matrices) to perform rotations in 3D.
Method  Storage 

Rotation matrix  9 or 6 (see below) 
Quaternion  4 or 3 (see below) 
Angle–axis  4 or 3 (see below) 
Only three of the quaternion components are independent, as a rotation is represented by a unit quaternion. For further calculation one usually needs all four elements, so all calculations would suffer additional expense from recovering the fourth component. Likewise, angle–axis can be stored in a threecomponent vector by multiplying the unit direction by the angle (or a function thereof), but this comes at additional computational cost when using it for calculations. Similarly, a rotation matrix requires orthogonal basis vectors, so in 3D space the third vector can unambiguously be calculated from the first two vectors with a cross product (though there is ambiguity in the sign of the third vector if improper rotations are allowed).
Method  # multiplies  # add/subtracts  total operations 

Rotation matrices  27  18  45 
Quaternions  16  12  28 
Method  # multiplies  # add/subtracts  # sin/cos  total operations  

Rotation matrix  9  6  0  15  
Quaternions *  Without intermediate matrix  15  15  0  30 
With intermediate matrix  21  18  0  39  
Angle–axis  Without intermediate matrix  18  13  2  30 + 3 
With intermediate matrix  21  16  2  37 + 2 
* Quaternions can be implicitly converted to a rotationlike matrix (12 multiplications and 12 additions/subtractions), which levels the following vectors rotating cost with the rotation matrix method.
There are three basic approaches to rotating a vector v→:
Method  # multiplies  # add/subtracts  # sin/cos  total operations  

Rotation matrix  9n  6n  0  15n  
Quaternions *  Without intermediate matrix  15n  15n  0  30n 
With intermediate matrix  9n + 12  6n + 12  0  15n + 24  
Angle–axis  Without intermediate matrix  18n  12n + 1  2  30n + 3 
With intermediate matrix  9n + 12  6n + 10  2  15n + 24 
A pair of unit quaternions z_{l} and z_{r} can represent any rotation in 4D space. Given a fourdimensional vector v→, and assuming that it is a quaternion, we can rotate the vector v→ like this:
The pair of matrices represents a rotation of . Note that since , the two matrices must commute. Therefore, there are two commuting subgroups of the group of four dimensional rotations. Arbitrary fourdimensional rotations have 6 degrees of freedom; each matrix represents 3 of those 6 degrees of freedom.
Since the generators of the fourdimensional rotations can be represented by pairs of quaternions (as follows), all fourdimensional rotations can also be represented.