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<record version="3" id="1111">
 <title>quaternion series overview and article guide</title>
 <name>QuaternionSeriesOverviewAndArticleGuide</name>
 <created>2026-08-24 23:53:02</created>
 <modified>2026-08-26 02:20:14</modified>
 <type>Topic</type>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <comment>clean up and update to other article updates</comment>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="pacs" code="02.40.Yy"/>
	<category scheme="pacs" code="02.10.Hh"/>
	<category scheme="pacs" code="45.40.-f"/>
 </classification>
 <keywords>
	<term>quaternion</term>
	<term>rotation</term>
	<term>attitude</term>
	<term>orientation</term>
	<term>direction cosine matrix</term>
	<term>Euler angles</term>
	<term>angular velocity</term>
	<term>IMU</term>
	<term>attitude estimation</term>
	<term>inertial navigation</term>
	<term>learning path</term>
	<term>article guide</term>
 </keywords>
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 <content>\section*{Quaternion series overview and article guide}

The PhysicsLibrary quaternion collection is organized as an engineering and
physics learning path rather than as a purely algebraic development.  It begins
with notation and convention discipline, establishes the quaternion algebra
needed for computation, develops three-dimensional orientation and
frame to frame coordinate transformations, and then proceeds to angular rate
kinematics, relative attitude, estimation errors, and inertial measurement unit
propagation.

The collection is intended for students and practitioners in mechanics,
rigid-body dynamics, spacecraft attitude determination and control, inertial
navigation, robotics, simulation, and related fields.  The deeper algebraic
structure of quaternions remains important, but the first objective is to make
quaternion formulas unambiguous and usable in physical applications.

The quaternion and Euler angle series share one geometric convention:
\emph{passive coordinate transformations} are the primary attitude maps, and
named rotation sequences are interpreted \emph{intrinsically}, meaning that
successive rotations are about axes of the current, already-rotated frame.

\section{PhysicsLibrary quaternion convention}

Unless an article explicitly states otherwise, PhysicsLibrary uses Hamilton
multiplication, scalar-first mathematical notation, right-handed orthonormal
frames, positive frame rotation according to the right-hand screw rule, passive
frame to frame coordinate transformations, and intrinsic moving axis
interpretation for named Euler sequences.

The canonical attitude quaternion is written ${}^{B}q_A$.  It maps coordinates
from frame $A$ into frame $B$, in the same direction as the passive
direction cosine matrix ${}^{B}C_A$:

\begin{equation}
{}^{B}v
=
{}^{B}q_A\,{}^{A}v\,({}^{B}q_A)^*
=
{}^{B}C_A\,{}^{A}v.
\end{equation}

If frame $B$ is obtained from frame $A$ by a positive right-handed rotation of
the axes through angle $\theta$ about unit axis $\widehat{\mathbf u}$, then the
passive axis angle quaternion is

\begin{equation}
{}^{B}q_A
=
\cos\frac{\theta}{2}
-
\widehat{\mathbf u}\sin\frac{\theta}{2}.
\end{equation}

The minus sign is the passive counterpart of the familiar positive angle active
rotor.  For example, a positive $90^\circ$ frame rotation about $+z$ gives
${}^{B}q_A=\sqrt{2}/2-(\sqrt{2}/2)\mathbf k$, and a fixed physical vector with
coordinates $[1,0,0]^T$ in $A$ has coordinates $[0,-1,0]^T$ in $B$.

The inverse map is ${}^{A}q_B=({}^{B}q_A)^*$.  Hamilton multiplication then
chains passive quaternion maps in the same written order as passive DCMs:

\begin{equation}
{}^{C}q_A
=
{}^{C}q_B\,{}^{B}q_A,
\qquad
{}^{C}C_A
=
{}^{C}C_B\,{}^{B}C_A.
\end{equation}

This common frame direction is a central design choice of the revised
PhysicsLibrary orientation series.

The detailed convention discussion belongs in
Quaternions for Physics and Engineering: Orientation, Notation, and Conventions.

\section{Convention migration status}

Older PhysicsLibrary quaternion entries were written around an active vector
interpretation.  The revised series instead uses the passive frame map declared
above.

During the cleanup, an older linked article may temporarily retain an explicit
active convention.  Its local declaration controls until that article is
converted.  New and revised quaternion entries should use the passive convention
of this overview and of the convention reference article.

The algebraic articles on quaternion definition, multiplication, conjugation,
norm, and inverse require little or no mathematical change because Hamilton's
algebra is unchanged.  Convention sensitive entries require explicit revision,
particularly those dealing with axis angle orientation, vector or coordinate
transformation, composition, quaternion DCM conversion, quaternion Euler
conversion, kinematics, attitude error, and IMU propagation.

\section{How the articles fit together}

The material naturally falls into three stages.

\subsection*{1. Conventions and algebra}

Begin with
Quaternions for Physics and Engineering: Orientation, Notation, and Conventions,
then read
quaternion,
quaternion product in scalar vector form,
quaternion conjugate,
quaternion norm, and
quaternion inverse.

These entries establish the Hamilton basis rule
$\mathbf i\mathbf j=\mathbf k$, scalar/vector decomposition, the Hamilton
product, conjugation, norm, and the identity $q^{-1}=q^*/\lVert q\rVert^2$.
For a unit quaternion, $q^{-1}=q^*$.

Storage order is treated separately from algebra.  A program may store
$[q_w,q_x,q_y,q_z]$ or $[q_x,q_y,q_z,q_w]$ while still using the same Hamilton
multiplication.

\subsection*{2. Frame transformations and attitude representations}

Continue with
axis-angle representation and unit quaternion,
coordinate transformations with quaternions,
composition of rotations and quaternion order,
quaternions and direction cosine matrices,
and
quaternions and Euler angles.

The axis angle article develops the fundamental passive parameterization and
its quaternion exponential,

\begin{equation}
{}^{B}q_A
=
\exp\left(-\frac{\theta}{2}\widehat{\mathbf u}\right).
\end{equation}

The coordinate-transformation article then derives the passive quaternion
sandwich and its Rodrigues equivalent.  The composition article shows why
finite transformations do not commute and why explicit frame labels determine
factor order more reliably than verbal mnemonics.

The DCM article establishes the direct correspondence

\begin{equation}
{}^{B}C_A=C({}^{B}q_A),
\qquad
C(q^*)=C(q)^T,
\qquad
C(-q)=C(q).
\end{equation}

The Euler angle article connects the quaternion series to the revised
PhysicsLibrary passive/intrinsic Euler convention.  For intrinsic
$3$--$2$--$1$ yaw--pitch--roll, with $\psi$ yaw, $\theta$ pitch, and $\phi$
roll, define passive elementary quaternions
$q_1^P(\phi)$, $q_2^P(\theta)$, and $q_3^P(\psi)$.  Then

\begin{equation}
{}^{B}q_A
=
q_1^P(\phi)\,q_2^P(\theta)\,q_3^P(\psi),
\qquad
{}^{B}C_A
=
C_1(\phi)\,C_2(\theta)\,C_3(\psi).
\end{equation}

Thus quaternion and DCM sequence products have the same factor order.

\subsection*{3. Dynamics, estimation, and IMU propagation}

Finish the main engineering path with
quaternion kinematics and angular velocity,
relative attitude and error quaternions,
and
numerical quaternion propagation and IMU attitude state integration.

Let $q={}^{B}q_I$ map inertial coordinates into body coordinates.  If
$\omega^B$ is the angular velocity of $B$ relative to $I$, resolved in the body
frame and embedded as a pure quaternion, the passive kinematic equation is

\begin{equation}
\dot q=-\frac12\omega^B q.
\end{equation}

If the same physical angular velocity is resolved in the inertial frame, the
equivalent form is $\dot q=-\tfrac12 q\omega^I$.

For relative attitude, if $q={}^{B}q_I$ is the actual attitude and
$q_d={}^{D}q_I$ is the desired attitude, then the passive coordinate map from
the actual body frame $B$ into the desired frame $D$ is

\begin{equation}
{}^{D}q_B=q_dq^*,
\qquad
{}^{B}q_D=qq_d^*.
\end{equation}

For a small positive passive frame rotation error,
$\delta q\approx[1,-\tfrac12\delta\boldsymbol\theta^T]^T$ in scalar-first
notation.  Estimation articles must always identify which relative frame map is
being represented before assigning a sign to the local error vector.

For sampled body rate propagation, the incremental passive quaternion
$\delta q_k={}^{B_{k+1}}q_{B_k}$ left multiplies the current inertial to body
state:

\begin{equation}
q_{k+1}
=
\delta q_k q_k,
\qquad
\delta q_k
=
\begin{bmatrix}
\cos(\Delta\theta/2)\\
-\dfrac{\sin(\Delta\theta/2)}{\Delta\theta}\,
\Delta\boldsymbol\theta
\end{bmatrix}.
\end{equation}

The numerical propagation article develops bias correction, exact exponential
increments, numerical integration, normalization, sign continuity, coning, and
the relationship between attitude propagation and body/navigation vector
transformation.

\section{Self-study companions}

Beginning with the axis angle article, each main engineering entry has a
separate self study companion.  The exercises are stated first and complete
worked solutions follow afterward.

The companion articles are:

\begin{itemize}

\item axis-angle representation and unit quaternion: examples, exercises, and solutions;

\item coordinate transformations with quaternions: examples, exercises, and solutions;

\item composition of rotations and quaternion order: examples, exercises, and solutions;

\item quaternions and direction cosine matrices: examples, exercises, and solutions;

\item quaternions and Euler angles: examples, exercises, and solutions;

\item quaternion kinematics and angular velocity: examples, exercises, and solutions;

\item relative attitude and error quaternions: examples, exercises, and solutions;

\item numerical quaternion propagation and IMU attitude state integration: examples, exercises, and solutions.

\end{itemize}

During the active to passive convention migration, a companion should be
revised together with, or immediately after, its parent article so that its
examples do not silently use an obsolete sign or map direction.

\section{Recommended reading paths}

\subsection*{First engineering introduction}

A compact first route is:

\begin{enumerate}
\item the convention reference article;
\item quaternion;
\item conjugate, norm, and inverse;
\item axis-angle representation and unit quaternion;
\item coordinate transformations with quaternions;
\item quaternions and direction cosine matrices.
\end{enumerate}

This path establishes enough algebra and geometry to construct and apply
passive attitude quaternions without immediately requiring rigid-body
kinematics.

\subsection*{Spacecraft attitude, robotics, and rigid-body simulation}

After the transformation articles, continue with
quaternions and Euler angles,
quaternion kinematics and angular velocity,
and
relative attitude and error quaternions.

\subsection*{Inertial navigation and IMU propagation}

For strapdown applications, emphasize axis angle, coordinate transformations,
quaternion DCM conversion, quaternion kinematics, relative attitude/error
quaternions, and
numerical quaternion propagation and IMU attitude state integration.

The kinematics article supplies the continuous passive rate equation, the
relative attitude article supplies the local multiplicative error concept, and
the numerical article applies both to sampled gyro measurements.

\section{Core formula map}

The main formulas of the engineering sequence can be summarized compactly as

\begin{align*}
q&amp;=q_w+q_x\mathbf i+q_y\mathbf j+q_z\mathbf k,\\
q^{-1}&amp;=q^*/\lVert q\rVert^2,\\
{}^{B}q_A&amp;=\cos(\theta/2)-\widehat{\mathbf u}\sin(\theta/2),\\
{}^{B}v&amp;={}^Bq_A\,{}^Av\,({}^{B}q_A)^*,\\
{}^{C}q_A&amp;={}^Cq_B\,{}^Bq_A,\\
{}^{B}C_A&amp;=C({}^{B}q_A),\\
{}^{B}q_A&amp;=q_1^P(\phi)q_2^P(\theta)q_3^P(\psi)
\quad\hbox{for intrinsic $3$--$2$--$1$},\\
\dot q&amp;=-\tfrac12\omega^Bq
\quad\hbox{for $q={}^Bq_I$},\\
{}^{D}q_B&amp;=q_dq^*,\\
\delta q&amp;\approx[1,-\tfrac12\delta\boldsymbol\theta^T]^T,\\
q_{k+1}&amp;=\delta q_kq_k.
\end{align*}

This map is a guide, not a substitute for the individual derivations.

\section{Conceptual relationships}

Several relationships recur throughout the series.

\begin{enumerate}

\item \textbf{Quaternion algebra and quaternion attitude convention are
different layers.}
Hamilton multiplication remains unchanged when the application convention is
changed from active vector rotation to passive coordinate transformation.

\item \textbf{Storage order is not multiplication convention.}
Scalar-first and scalar-last arrays can represent the same Hamilton quaternion.

\item \textbf{The PhysicsLibrary attitude quaternion is a passive coordinate
map.}
The physical vector is held fixed while its components are transformed between
reference frames.

\item \textbf{Quaternion and DCM frame directions are deliberately aligned.}
Both ${}^{B}q_A$ and ${}^{B}C_A$ map $A$ coordinates into $B$ coordinates.

\item \textbf{Intrinsic describes a sequence construction.}
For a named Euler sequence, successive elementary rotations are about axes of
the moving frame.

\item \textbf{Positive passive and active axis angle quaternions are
conjugates.}
For the same positive geometric angle, the passive frame quaternion has the
opposite vector part sign from the positive active rotor.

\item \textbf{Euler angles are local coordinates.}
They remain valuable for interpretation but have coordinate singularities;
quaternions and DCMs provide globally nonsingular orientation propagation.

\item \textbf{A global quaternion and a local three component error are
complementary.}
The nominal state may remain a unit quaternion while an estimator linearizes a
small relative frame transformation.

\item \textbf{IMU propagation is repeated frame composition.}
Each gyro sample produces a small passive body frame increment whose sign,
multiplication order, and bias correction must agree with the declared
attitude state.

\end{enumerate}

\section{Where deeper mathematics fits}

The engineering sequence intentionally reaches applications before pursuing the
deeper algebra.  A later mathematical branch can develop division algebras, the
geometry of the unit three sphere, $SU(2)$, the double covering of $SO(3)$, Lie
groups and Lie algebras, and exponential and logarithmic maps.

Those subjects explain why the engineering formulas have the structure they
do, but they are not prerequisites for beginning quaternion attitude work.

\section{Summary}

The PhysicsLibrary quaternion series proceeds from convention discipline and
Hamilton algebra to passive frame transformations, direction cosine matrices,
intrinsic Euler angles, angular rate kinematics, attitude errors, and sampled
IMU propagation.

Its convention can be remembered from three statements:

\begin{equation}
{}^{B}v
=
{}^{B}q_A\,{}^{A}v\,({}^{B}q_A)^*,
\qquad
{}^{B}q_A
=
\cos\frac{\theta}{2}
-
\widehat{\mathbf u}\sin\frac{\theta}{2},
\qquad
{}^{C}q_A
=
{}^{C}q_B\,{}^{B}q_A.
\end{equation}

A reader who follows the collection should be able not only to quote quaternion
formulas, but also to determine what a formula means, identify its convention,
derive multiplication order from frame labels, test a transformation with a
simple coordinate example, and use the result consistently in a physical or
numerical application.

\section*{License}

This article is an original synthesis prepared for PhysicsLibrary and intended
for release under CC BY-SA 4.0.</content>
</record>
