Nomenclature

$\mathbb{SO}(3)$

Special orthogonal group in $3$ dimensions

$\boldsymbol{R}_X({\cdot})$

Rotation matrix for rotation about the $X$ -axis

$\boldsymbol{R}_Y({\cdot})$

Rotation matrix for rotation about the $Y$ -axis

$\boldsymbol{R}_Z({\cdot})$

Rotation matrix for rotation about the $Z$ -axis

$\{\alpha, \beta, \gamma \}$

The sequence of three Euler angles used in this article

$\underline{({\cdot})}$

Lower limit of Euler angle $({\cdot})$

$\overline{({\cdot})}$

Upper limit of Euler angle $({\cdot})$

$\boldsymbol{k}$

A unit vector in ${\mathbb{R}}^3$ describing the axis of rotation

$\psi$

Angle of rotation about the axis $\boldsymbol{k}$

$\phi$

Critical value of $\psi$

$\mathcal{E}$

Space of Euler angles

${\mathcal{R}}$

Space of Rodrigues parameters

$\mathcal{V}_{\mathcal{E}}$

A cuboid in $\mathcal{E}$

$\mathcal{F}_{({\cdot})}$

A face ( $\cdot$ ) of $\mathcal{V}_{\mathcal{E}}$ ; e.g., $\mathcal{F}_{{\overline{\gamma }}}$ , $\mathcal{F}_{{\underline{\gamma }}}$ , etc.

$\mathcal{V}_{\mathcal{R}}$

A region in $\mathcal{R}$

${\mathcal{Q}}_{({\cdot})}$

A bounding surface of $\mathcal{R}$ , corresponding to $\mathcal{F}_{({\cdot})}$

$\mathcal{S}$

A sphere that is tangent to one or more surfaces of $\mathcal{V}_{\mathcal{R}}$

$r$

The radius of $\mathcal{S}$

$\overline{{\mathcal{S}}}$

The largest sphere that fits inside $\mathcal{V}_{\mathcal{R}}$

$\overline{r}$

The radius of $\overline{{\mathcal{S}}}$

$\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$

Global frame of reference in $\mathcal{R}$

$\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$

Local frame of reference in $\mathcal{R}$

$\mathcal{U}_{({\cdot})}$

A quadric in $\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$ corresponding to the face $\mathcal{F}_{({\cdot})}$ in $\mathcal{E}$

$\mathcal{U}^{\prime}_{({\cdot})}$

A quadric in $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ corresponding to the face $\mathcal{F}_{({\cdot})}$ in $\mathcal{E}$

$\mathcal{P}^{\prime}_2$

A plane in $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ defined as $d^{\prime}_2=0$

$\mathcal{P}^{\prime}_3$

A plane in $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ defined as $d^{\prime}_3=0$

${\mathcal{S}}^{\prime}$

A sphere in $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$

$\mathcal{X}_{\text{e}}$

An ellipse resulting from the intersection of $\mathcal{P}_2$ with ${\mathcal{U}^{\prime}_{{\overline{\gamma }}}}$

$\mathcal{C}_{\text{e}}$

A circle resulting from the intersection of $\mathcal{P}_2$ with ${\mathcal{S}}^{\prime}$

$\mathcal{X}_{\text{h}}$

A hyperbola resulting from the intersection of $\mathcal{P}_3$ with ${\mathcal{U}^{\prime}_{{\overline{\gamma }}}}$

$\mathcal{C}_{\text{h}}$

A circle resulting from the intersection of $\mathcal{P}_3$ with ${\mathcal{S}}^{\prime}$

CAS

Computer algebra system

2. Mapping of a subset of $\mathbb{SO}(3)$ described in Euler angles to the space of Rodrigues parameters

The orientations of a rigid body form the special orthogonal group of three dimensions, denoted by $\mathbb{SO}(3)$ . A summary of the geometric/algebraic properties of this group has been presented in Appendix A. This group admits numerous representations, the most popular among which, perhaps, are the rotation matrices, $\boldsymbol{R} \in{\mathbb{R}}^{3\times 3}$ , where $\boldsymbol{R}$ is orthogonal and $\text{det}(\boldsymbol{R}) = 1$ . These matrices can themselves be expressed variously in terms of different parametrisations, among which the most common may be a sequence of three Euler angles. A generic rotation matrix, $\boldsymbol{R}$ , may be expressed as a concatenation of three successive simple rotations about the coordinate axes. For instance, in the body-fixed convention, one could write $\boldsymbol{R}={\boldsymbol{R}_Z(\alpha ) \boldsymbol{R}_Y(\beta ) \boldsymbol{R}_X(\gamma )}$ , which constitutes a Z-Y-X or $3$ - $2$ - $1$ type of rotation, $\alpha, \beta$ , and $\gamma$ being the corresponding Euler angles, respectively. It is known that in the space-fixed convention, the same rotation may be represented by $\boldsymbol{R}^{\prime}={\boldsymbol{R}_X(\gamma ) \boldsymbol{R}_Y(\beta )\boldsymbol{R}_Z(\alpha )}$ . Considering both the body-fixed and space-fixed conventions, and the sequences of the types Z-Y-X as well as $Z$ - $X$ - $Z$ , there can be a total of 24 valid sequences of Euler anglesFootnote ² (for the details, see, e.g., [Reference Craig24], Appendix B). This article will follow the body-fixed convention primarily.

In the Z-Y-X sequence, by choosing $\alpha, \beta, \gamma \in [{-}\pi, \pi ]$ , one covers $\mathbb{SO}(3)$ entirely. However, in most practical examples, only proper subsets of $\mathbb{SO}(3)$ are of interest, since the end-effector of a serial manipulator or the moving platform of a parallel one cannot typically achieve all possible orientations due to practical constraints.Footnote ³ Such a subset is often described via a box or a cuboid $\mathcal{V}_{\mathcal{E}}$ in the same manner as one would in a Cartesian space [Reference Monsarrat and Gosselin18–Reference Merlet20]:

(1) \begin{align} & \alpha \in [{\underline{\alpha }},{\overline{\alpha }}], \ \beta \in [{\underline{\beta }},{\overline{\beta }}], \ \gamma \in [{\underline{\gamma }},{\overline{\gamma }}]; \\[-3pt]\nonumber \end{align}

(2) \begin{align} \Rightarrow &{\mathcal{V}_{\mathcal{E}}} \equiv [{\underline{\alpha }},{\overline{\alpha }}]\times [{\underline{\beta }},{\overline{\beta }}]\times [{\underline{\gamma }},{\overline{\gamma }}]. \\[15pt]\nonumber \end{align}

In the above and henceforth, $\underline{({\cdot})}$ and $\overline{({\cdot})}$ denote the lower and upper limits of the individual Euler angles, respectively. As in most of the cases reported in the literature, it is assumed in this work that the ranges of individual Euler angles are symmetric about the origin; that is:

(3) \begin{equation}{\overline{\alpha }} = -{\underline{\alpha }}, \quad{\overline{\beta }} = -{\underline{\beta }}, \quad{\overline{\gamma }} = -{\underline{\gamma }}. \end{equation}

The symmetric ranges of Euler angles discussed in the following are divided into two categories, namely: (a) uniform and (b) non-uniform ranges. The ranges are called uniform when ${\overline{\alpha }}={\overline{\beta }}={\overline{\gamma }}$ and consequently ${\underline{\alpha }}={\underline{\beta }}={\underline{\gamma }}$ , and non-uniform otherwise. Such ranges are widely used for describing the orientation workspaces of spatial parallel manipulators, such as the Stewart platforms, of which a few examples are listed in Table I. Furthermore, the minimum and maximum limits of Euler angles are required to lie within the ranges $(-\pi /2,0)$ and $(0,\pi /2)$ , respectively, to avoid parametrisation singularities (see, e.g., [Reference Ghosal21], pp. 28–29 and [Reference Murray, Sastry and Zexiang26], p. 33) or gimbal locks, as these are popularly known, in the description of successive rotations.

Figure 1. Faces and vertices of ${\mathcal{V}_{\mathcal{E}}} \in{\mathcal{E}}$ represented as a cuboid in Euler angles for non-uniform ranges of Euler angles. The numerical values of the limits are listed in Table III.

Figure 1 shows the schematic of the corresponding cuboid, that is, an instance of $\mathcal{V}_{\mathcal{E}}$ . The faces of $\mathcal{V}_{\mathcal{E}}$ are termed as $\mathcal{F}_{({\cdot})}$ , for example, the face associated with $\gamma = \overline{\gamma }$ is denoted by $\mathcal{F}_{{\overline{\gamma }}}$ . Similarly, the $\mathcal{F}_{\underline{\gamma }}$ is defined by $\gamma ={\underline{\gamma }}$ and so on. The coordinates of the vertices of $\mathcal{V}_{\mathcal{E}}$ are listed in Table II. However, it is known that $\mathbb{SO}(3)$ is not Cartesian in nature, since it is neither a linear space, nor does it admit the Euclidean metric, at least in the global sense. Hence, the utility of the schematic in Figure 1 is limited only to a familiar visual representation, beyond which it has no mathematical significance. Nevertheless, from Table II, one can confirm what may be observed in Figure 1 as well, that points in $\mathcal{V}_{\mathcal{E}}$ possess central symmetry w.r.t. the origin of $\mathcal{E}$ , denoted by $\boldsymbol{o}$ ; see, for example, the terminal points of the body-diagonal $\boldsymbol{p}_1$ and $\boldsymbol{p}_7$ , and their coordinates.

Table II. Vertices of $\mathcal{V}_{\mathcal{E}}$ , as seen in Fig. 1, in terms of the limits of Euler angles.

Figure 2. A pictorial depiction of $\boldsymbol{k}$ , which may be expressed as $\boldsymbol{k} = [\cos \zeta \cos \xi, \cos \zeta \sin \xi, \sin \zeta ]^{\top }$ .

In order to describe appropriately the subset of $\mathbb{SO}(3)$ demarcated as $\mathcal{V}_{\mathcal{E}}$ and to analyse its extent in a physically pertinent manner, it is mapped to the space of Rodrigues parameters, $\mathcal{R}$ . This choice of parametrisation is made to take advantage of two facts: (a) Rodrigues parameters are related to the axis-angle representation intrinsically, which affords them physical significance; (b) the Euclidean norm is defined in the neighbourhood of the origin in this space, making it possible to define subsets of $\mathbb{SO}(3)$ as spheres centred at the origin (see, e.g., [Reference Nag and Bandyopadhyay11]) and compare their sizes in terms of the radii of these spheres. The details of the mapping are presented below.

2.1. Mapping of Euler angles into Rodrigues parameters

The relationship between a rotation matrix $\boldsymbol{R}$ and the vector of Rodrigues parameters,Footnote ⁴ $\boldsymbol{c}=[c_1,c_2,c_3]^{\top } \in{\mathbb{R}}^3$ , is shown in Table 1(a) of [Reference Spring16] and Eq. (204) of [Reference Shuster13]. The derivation is simple and compact; it is presented below for the sake of completeness and to introduce certain notations. It is preceded by a geometric perspective to the Rodrigue’s vector.

The description of $\mathbb{SO}(3)$ via Rodrigues parameters is closely related to a geometric representation due to Euler, who proved that any generic rotation of a rigid body in space is equivalent to a simple rotation about a corresponding axis in space. This leads directly to the so-called axis-angle representation, which is given by the pair $(\boldsymbol{k}, \psi )$ , where $\boldsymbol{k} \in \mathbb{S}^2$ , that is, $\boldsymbol{k}$ is a unit vector in ${\mathbb{R}}^3$ (see Figure 2) which lies along the said axis of rotation, and $\psi \in \mathbb{S}^1$ is the corresponding angle, measured about $\boldsymbol{k}$ in the CCW sense. A visual depiction of this interpretation of $\mathbb{SO}(3)$ may be found, e.g., in Figure 3 of [Reference Nag and Bandyopadhyay11]. In terms of the axis angle-pair, the Gibbs/Rodrigues vector or the vector of Rodrigues parameters can be expressed explicitly asFootnote ⁵

(4) \begin{align} \boldsymbol{c} = \boldsymbol{k} \tan \frac{\psi }{2}. \end{align}

Considering the norms of both sides of Eq. (4), one arrives at an important result:

(5) \begin{align}{\| \boldsymbol{c}\|} = \left |\tan \frac{\psi }{2} \right |{\| \boldsymbol{k}\|} = \left |\tan \frac{\psi }{2} \right |, \quad \text{since\; $\boldsymbol{k}$ is a unit vector}. \end{align}

Figure 3. Visualisation of subsets of $\mathbb{SO}(3)$ as spheres in ${\mathbb{R}}^3$ , as described by Rodrigues parameters. Two sets of Rodrigues vectors are shown, which lie along two unit vectors $\boldsymbol{k}_1, \boldsymbol{k}_2$ in ${\mathbb{R}}^3$ and describe rotations through the angles $\psi ^{\prime}$ and $\psi ^{\prime\prime}$ about these.

Eqs. (4, 5) show that the Rodrigues vector representing a given rotation is along the axis of rotation and has a magnitude equalling the absolute value of the tangent of half of the angle of rotation. This property leads to a visual representation of the Rodrigues vector, as depicted in Figure 3. It shows two pairs of Rodrigues vectors, namely, $\{\boldsymbol{c}^{\prime}_1,\boldsymbol{c}^{\prime}_2\}$ , and $\{\boldsymbol{c}^{\prime\prime}_1,\boldsymbol{c}^{\prime\prime}_2\}$ which lie along the axes $\boldsymbol{k}_1, \boldsymbol{k}_2$ . The vectors $\{\boldsymbol{c}^{\prime}_1, \boldsymbol{c}^{\prime}_2\}$ correspond to rotations through $\psi ^{\prime}$ CCW about $\boldsymbol{k}_1$ and $\boldsymbol{k}_2$ , respectively, while $\{\boldsymbol{c}^{\prime\prime}_1, \boldsymbol{c}^{\prime\prime}_2\}$ describe CCW rotations through $\psi ^{\prime\prime}$ about the same set of axes. Further, Figure 3 suggests that the elements $\{c_1,c_2,c_3\}$ of $\boldsymbol{c}$ may be interpreted as local coordinates of ${\mathbb{R}}^3$ around its origin, and subsets of $\mathbb{SO}(3)$ can be described by spheres centred at the origin. The radii of these spheres indicate the extent of rotations permissible within the respective subsets, about any axis in space. Obviously, this description is only valid for rotation angles in $(0, \pi )$ .

An expression for $\boldsymbol{k}$ corresponding to any $\boldsymbol{R} \in{\mathbb{SO}(3)}$ may be found as

(6) \begin{align} \boldsymbol{k} = \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{2\sin \psi }, \quad \text{provided $\psi \in (0, \pi )$.} \end{align}

The operator $({\cdot})^{\vee }\,:\,{so(3)} \to{\mathbb{R}}^3$ appearing in Eq. (6) produces the so-called vector equivalent of a skew-symmetric matrix; that is, $\boldsymbol{A}\boldsymbol{x} = \boldsymbol{A}^\vee \times \boldsymbol{x}, \forall \boldsymbol{x} \in{\mathbb{R}}^3$ and $\forall \boldsymbol{A} \in{\mathbb{R}}^{3\times 3}$ such that $\boldsymbol{A}+\boldsymbol{A}^{\top } = \textbf{0} \in{\mathbb{R}}^{3\times 3}$ . Since it has been assumed in the above that $\psi \in (0, \pi )$ , null/full rotations and half-turns about any axis are not included in the following analysis.

Using Eq. (6) in Eq. (4), one obtains

(7) \begin{align} \boldsymbol{c} & = \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{2\sin \psi } \tan (\psi /2)\nonumber, \\ & = \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{4 \cos ^2(\psi /2)}\nonumber, \\ &= \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{2+2 \cos \psi }. \end{align}

Noting that $\text{tr}({\boldsymbol{R}}) = 1 + 2 \cos \psi$ , an expression for $\boldsymbol{c}$ is obtained in terms of $\boldsymbol{R}$ explicitly:

(8) \begin{align} \boldsymbol{c} = \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{1 + \text{tr}({\boldsymbol{R}})}. \end{align}

For the sake of brevity, an operator $\stackrel{\frown }{({\cdot})}\,:\,{\mathbb{SO}(3)} \to{\mathbb{R}}^3$ is introduced as follows:

(9) \begin{align} \stackrel{\frown }{\boldsymbol{R}}\,=\, \frac{(\boldsymbol{R}-\boldsymbol{R}^{\top })^\vee }{1 + \text{tr}({\boldsymbol{R}})}, \end{align}

Thus, one can express Eq. (8) compactly as

(10) \begin{align} \boldsymbol{c} =\, \stackrel{\frown }{\boldsymbol{R}}. \end{align}

Furthermore, expressing $\boldsymbol{R}$ in Eq. (8) as $\boldsymbol{R}_Z(\alpha ) \boldsymbol{R}_Y(\beta ) \boldsymbol{R}_X(\gamma )$ , one can relate the corresponding Rodrigues parameters, denoted by $\{d_1, d_2, d_3\}$ , to the Euler angles analytically:

(11a) \begin{align} & d_1 = \frac{{\sin \gamma }({\cos \alpha } +{\cos \beta }) -{\sin \alpha }\,{\sin \beta }\,{\cos \gamma }}{A + B}, \\[-3pt]\nonumber \end{align}

(11b) \begin{align} & d_2 = \frac{{\sin \beta } (1 +{\cos \alpha }\,{\cos \gamma }) +{\sin \alpha }\,{\sin \gamma }}{A + B}, \\[-3pt]\nonumber \end{align}

(11c) \begin{align} & d_3 = \frac{{\sin \alpha } ({\cos \beta } +{\cos \gamma }) -{\cos \alpha }\,{\sin \beta }\,{\sin \gamma }}{A + B}; \quad \text{where} \\[-3pt]\nonumber \end{align}

(11d) \begin{align} & A = 1 +{\cos \alpha }\,{\cos \beta }+{\cos \beta }\,{\cos \gamma } +{\cos \gamma }\,{\cos \alpha }, \quad \text{and} \\[-3pt]\nonumber \end{align}

(11e) \begin{align} & B ={\sin \alpha }\,{\sin \beta}\,{\sin \gamma }. \\[15pt]\nonumber \end{align}

Considering the equivalent space-fixed rotation matrix $\boldsymbol{R}^{\prime} =\,\boldsymbol{R}_X(\gamma )\boldsymbol{R}_Y(\beta )\boldsymbol{R}_Z(\alpha )$ , the corresponding Rodrigues parameters are found as

(12a) \begin{align} & e_1 = \frac{{\sin \gamma } ({\cos \alpha } +{\cos \beta }) +{\sin \alpha }\,{\sin \beta }\,{\cos \gamma }}{A - B}, \\[-3pt]\nonumber \end{align}

(12b) \begin{align} & e_2 = \frac{{\sin \beta } (1 +{\cos \alpha }\,{\cos \gamma }) -{\sin \alpha }\,{\sin \gamma }}{A - B}, \\[-3pt]\nonumber \end{align}

(12c) \begin{align} & e_3 = \frac{{\sin \alpha } ({\cos \beta } +{\cos \gamma }) +{\cos \alpha }\,{\sin \beta }\,{\sin \gamma }}{A - B}.\\[15pt]\nonumber \end{align}

Eqs. (11a–11c) and (12a–12c) are valid iff $A+B$ and $A-B$ do not vanish, respectively. The real combinations of $\{\alpha, \beta, \gamma \}$ for which these vanish have been studied in Appendix B.

The expressions derived above afford the means of mapping $\mathcal{V}_{\mathcal{E}}$ in Figure 1 to the corresponding solid, namely, ${\mathcal{V}_{\mathcal{R}}} \in \;{\mathcal{R}}$ , as explained in the following. The bounding surface $\mathcal{F}_{({\cdot})}$ is mapped to the surface ${\mathcal{Q}}_{({\cdot})}$ bounding $\mathcal{V}_{\mathcal{R}}$ ; e.g., ${\mathcal{Q}}_{{\overline{\gamma }}}$ is the mapped surface corresponding to the face $\mathcal{F}_{{\overline{\gamma }}}$ and so on.

2.2. Mapping of the cuboid $\mathcal{V}_{\mathcal{E}}$ in the space of Euler angles $\mathcal{E}$ into solid regions $\mathcal{V}_{\mathcal{R}}$ in the space of Rodrigues parameters $\mathcal{R}$

In order to map $\mathcal{V}_{\mathcal{E}}$ to $\mathcal{V}_{\mathcal{R}}$ , its faces are transformed individually. The process is explained in the context of the face $\mathcal{F}_{{\overline{\gamma }}}$ (see Figure 4a). The remaining faces are treated similarly.

Figure 4. One of the faces of $\mathcal{V}_{\mathcal{E}}$ and the corresponding surfaces of $\mathcal{V}_{\mathcal{R}}$ ; (a) face $\mathcal{F}_{{\overline{\gamma }}}$ , (b) surface ${\mathcal{Q}}_{{\overline{\gamma }}}$ ,and (c) surface ${\mathcal{Q}}_{{\overline{\gamma }}}^{\prime}$ . The point $\boldsymbol{p}$ on the face $\gamma ={\overline{\gamma }}=50^\circ$ corresponds to the parameter values $\{u,v\}=\{0.8,0.8\}$ (see Eq. (13)).

The face $\mathcal{F}_{{\overline{\gamma }}}$ is spanned by two linearly independent vectors, given by $\boldsymbol{a}_1 = \boldsymbol{p}_8 - \boldsymbol{p}_5$ , and $\boldsymbol{a}_2 = \boldsymbol{p}_6 - \boldsymbol{p}_5$ , as shown in Figure 4a. Any point on this face, say, $\boldsymbol{p}=[\alpha, \beta, \gamma ]^{\top }$ , may be represented in terms of the pair of parameters $\{u,v\}$ as

(13) \begin{align} & \quad \boldsymbol{p} = \boldsymbol{p}_5 + \boldsymbol{a}_1 u + \boldsymbol{a}_2 v; \nonumber \\ & \Rightarrow [ \alpha, \beta, \gamma ]^{\top } = [ ({\overline{\alpha }} -{\underline{\alpha }}) u +{\underline{\alpha }}, ({\overline{\beta }} -{\underline{\beta }}) v +{\underline{\beta }},{\overline{\gamma }} ]^{\top }, \quad \text{where}\; u,v \in [ 0, 1 ]. \end{align}

Using Eq. (13) in Eq. (11), one obtains a $\{u,v\}$ parametrisation of the desired surface in $\mathcal{R}$ , denoted by ${\mathcal{Q}}_{{\overline{\gamma }}}$ , using the Z-Y-X sequence of Euler angles. This surface has been visualised in Figure 4b. Similarly, a combination of Eq. (13) and Eq. (12) results in the surface, denoted by ${\mathcal{Q}}^{\prime}_{{\overline{\gamma }}}$ , corresponding to the X-Y-Z sequence, as shown in Figure 4c.

The same procedure is followed for the remaining five faces in both conventions, whence they enclose two different instances of $\mathcal{V}_{\mathcal{R}}$ , denoted by $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ , respectively. These may be seen individually in Figures 6a, 6b, and together in Figure 6c. The corresponding instances of $\mathcal{V}_{\mathcal{R}}$ for uniform symmetric ranges of Euler angles are shown in Figures 5a, 5b, and 5c, respectively. The coordinates of the points $\boldsymbol{p}_i$ are listed in Table II, and their numerical values are tabulated in Table III. The coordinates of the vertices $\boldsymbol{m}_i$ are obtained by using Eq. (13) and its counterparts for the other faces of $\mathcal{V}_{\mathcal{E}}$ in Eqs. (11). These are shown in Figures 5a–5c. Similarly, the vertices $\boldsymbol{n}_i$ are obtained via Eqs. (12), and these are shown in Figures 6a–6c.

Table III. Uniform and non-uniform ranges of Euler angles used in this article.

Figure 5. Solids $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ corresponding to uniform symmetric ranges of Euler angles $\alpha, \beta, \gamma \in [-30^\circ, 30^\circ ]$ (see Table III).

Figure 6. Solids $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ corresponding to non-uniform symmetric ranges of Euler angles $\{\alpha, \beta, \gamma \}\in [-30^\circ, 30^\circ ]\times [-40^\circ, 40^\circ ]\times [-50^\circ, 50^\circ ]$ (refer to Table III).

2.3. Relations between $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ for symmetric ranges of Euler angles

If the limits of Euler angles are chosen in a symmetric manner, then it is easy to see that the pairs of vertices of $\mathcal{V}_{\mathcal{E}}$ delimiting each of its body-diagonal maps to their respective inverses in $\mathbb{SO}(3)$ ; that is., if the line segment joining the vertices $\boldsymbol{p}_i$ and $\boldsymbol{p}_j$ , $i\ne j$ constitutes a body diagonal, and the corresponding rotation matrices are given by $\boldsymbol{R}_{\boldsymbol{p}_i}$ and $\boldsymbol{R}^{\prime}_{\boldsymbol{p}_j}$ , respectively, then $\boldsymbol{R}^{\prime}_{\boldsymbol{p}_j} = \boldsymbol{R}^{\top }_{\boldsymbol{p}_i}$ , where $\boldsymbol{R}^{\prime}$ denotes the space-fixed counterpart of any body-fixed rotation matrix $\boldsymbol{R}$ . This relation is a consequence of the intrinsic central symmetry among the points in $\mathcal{V}_{\mathcal{E}}$ . Obviously, in this case, this symmetry must be interpreted in the context of the group operation of $\mathbb{SO}(3)$ ; that is, matrix multiplications, since $\boldsymbol{R}_{\boldsymbol{p}_i} \boldsymbol{R}^{\prime}_{\boldsymbol{p}_j} = \boldsymbol{I}_{3\times 3}$ , $\boldsymbol{I}_{3\times 3} = \operatorname{diag}(1,1,1)$ being the multiplicative identity in $\mathbb{SO}(3)$ . In the following, this symmetry is demonstrated in the context of the body diagonal connecting the vertices $\boldsymbol{p}_3$ and $\boldsymbol{p}_5$ (see Figure 1).

Given the coordinates of $\boldsymbol{p}_3,\boldsymbol{p}_5$ in Table II, one can write

(14a) \begin{align} & \boldsymbol{R}_{\boldsymbol{p}_3}=\boldsymbol{R}_Z({\overline{\alpha }})\boldsymbol{R}_Y({\overline{\beta }})\boldsymbol{R}_X({\underline{\gamma }}), \\[-3pt]\nonumber \end{align}

(14b) \begin{align} & \boldsymbol{R}^{\prime}_{\boldsymbol{p}_5}=\boldsymbol{R}_X({\overline{\gamma }})\boldsymbol{R}_Y({\underline{\beta }})\boldsymbol{R}_Z({\underline{\alpha }}). \\[15pt]\nonumber \end{align}

Further, the matrix $\boldsymbol{R}^{\prime}_{\boldsymbol{p}_5}$ may be obtained as

(15) \begin{align} \boldsymbol{R}^{\prime}_{\boldsymbol{p}_5} & =\boldsymbol{R}_X^{\top }(-{\overline{\gamma }})\boldsymbol{R}_Y^{\top }(-{\underline{\beta }})\boldsymbol{R}_Z^{\top }(-{\underline{\alpha }}),\nonumber \\ & =\boldsymbol{R}_X^{\top }({\underline{\gamma }})\boldsymbol{R}_Y^{\top }({\overline{\beta }})\boldsymbol{R}_Z^{\top }({\overline{\alpha }}), \quad \text{since ${\overline{\alpha }} = -{\underline{\alpha }}$ and so on, as per Eq. (3)};\nonumber \\ \Rightarrow \boldsymbol{R}^{\prime}_{\boldsymbol{p}_5} & = \left (\boldsymbol{R}_Z({\overline{\alpha }})\boldsymbol{R}_Y({\overline{\beta }})\boldsymbol{R}_X({\underline{\gamma }})\right )^{\top }, \nonumber \\ & = \boldsymbol{R}_{\boldsymbol{p}_3}^{\top }, \ \text{following Eq. (14a)};\nonumber \\ \Rightarrow \boldsymbol{R}^{\top }_{\boldsymbol{p}_3} & = \boldsymbol{R}^{\prime}_{\boldsymbol{p}_5}. \end{align}

This symmetry persists in $\mathcal{R}$ . The images of $\boldsymbol{p}_i\in{\mathcal{V}_{\mathcal{E}}}$ in $\mathcal{R}$ are the points $\boldsymbol{m}_i = \stackrel{\frown }{\boldsymbol{R}}_{\boldsymbol{p}_i} \in{\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)}$ and $\boldsymbol{n}_i = \stackrel{\frown }{\boldsymbol{R}^{\prime}}_{\boldsymbol{p}_i} \in{\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)}$ , respectively, $i = 1,\ldots, 8$ . Therefore, one can write

\begin{align*} \boldsymbol{m}_3 = \stackrel{\frown }{\boldsymbol{R}}_{\boldsymbol{p}_3} = -\stackrel{\frown }{\boldsymbol{R}}^{\top }_{\boldsymbol{p}_3}\ \quad \text{since} \ \stackrel{\frown }{\boldsymbol{R}} = -\stackrel{\frown }{\boldsymbol{R}}^{\top } \ \forall \boldsymbol{R} \in{\mathbb{SO}(3)}, \quad \text{as per Eq. (9)}. \end{align*}

Considering Eq. (15), this becomes

(16) \begin{align} \Rightarrow & \boldsymbol{m}_3 = -\stackrel{\frown }{\boldsymbol{R}^{\prime}}_{\boldsymbol{p}_5}, \quad \text{following Eq. (15)}; \nonumber \\ \Rightarrow & \boldsymbol{m}_3 = - \boldsymbol{n}_5. \end{align}

This relation can be observed numerically in Table IV, wherein the corresponding entries have been presented in bold fonts. Similarly, the point $\boldsymbol{n}_j$ has been placed on the same row as the corresponding $\boldsymbol{m}_i$ . From these derivations and discussions, it may be concluded that for symmetric ranges of Euler angles, points in $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ bear central symmetry with respect to the origin of $\mathcal{R}$ (i.e., point corresponding to zero rotation) with the corresponding points in $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ .

Table IV. Coordinates of the vertices of $\mathcal{V}_{\mathcal{E}}$ (see Figure 1), $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ , as shown in Figure 6.

3. Identification of the largest spheres centred at the origin and contained within $\mathcal{V}_{\mathcal{R}}$

The instances of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ obtained by mapping $\mathcal{V}_{\mathcal{E}}$ into $\mathcal{R}$ have complicated shapes, as seen in Figure 5, and Figure 6, respectively. Most importantly, these are seen to be non-convex solids, and hence, not favourable for a convenient yet accurate description of the orientation workspace. Spherical shapes are preferred for this purpose given the obvious advantages they provide, in addition to being convex: (a) spatial homogeneity – a sphere extends to identical extents in all spatial directions and (b) ease of point classification – any given point in $\mathbb{SO}(3)$ may be trivially identified as being “inside” or “outside” or “on” such a sphere, based simply on a comparison of the distance of the point from the centre of the sphere (the origin, in the present case) with the radius of the said sphere.Footnote ⁶

Naturally, in addition to making sure that the desired sphere is centred at the origin and contained fully inside $\mathcal{V}_{\mathcal{R}}$ , it is of interest to maximise its radius, so as to maximise the set of accessible orientations within the said sphere. Such a sphere would obviously be tangent to at least one of the bounding surfaces of $\mathcal{V}_{\mathcal{R}}$ . Therefore, the desired sphere may be identified in two steps: (a) finding all the spheres tangent to each of the bounding surfaces individually and (b) choosing the smallest among them (since the larger ones may intersect one or more boundary surfaces at other points). The computations involved in step (a) are explained below in the context of the surface ${\mathcal{Q}}_{{\overline{\gamma }}}$ shown in Figure 4.

Let, the desired sphere be denoted by $\mathcal{S}$ and have the radius $r$ . Obviously, the radius represents a critical value of the distance of the surface from the centre of $\mathcal{S}$ , that is, the origin. An arbitrary point on the surface may be located by the corresponding Rodrigues parameters $\{d_1, d_2, d_3\}$ , as per Eq. (11). As shown in Eq. (13) (in the context of a different face of $\mathcal{V}_{\mathcal{E}}$ ), these coordinates may be expressed explicitly in terms of the surface parameters, $\{u,v\}$ :

(17a) \begin{align} & d_1 = \frac{\sin{\overline{\gamma }} (\cos u^{\prime}+\cos v^{\prime}) - \cos{\overline{\gamma }}\sin u^{\prime} \sin v^{\prime}}{A^{\prime} + B^{\prime}}, \\[-3pt]\nonumber \end{align}

(17b) \begin{align} & d_2 = \frac{\sin{\overline{\gamma }} \sin u^{\prime}+\sin v^{\prime} (\cos{\overline{\gamma }} \cos u^{\prime}+1)}{A^{\prime} + B^{\prime}}, \\[-3pt]\nonumber \end{align}

(17c) \begin{align} & d_3 = \frac{\cos{\overline{\gamma }} \sin u^{\prime}-\sin{\overline{\gamma }} \cos u^{\prime} \sin v^{\prime}+\sin u^{\prime} \cos v^{\prime}}{A^{\prime} + B^{\prime}}, \\[-3pt]\nonumber \end{align}

(17d) \begin{align} &\text{where}\nonumber \\ &u^{\prime}={\underline{\alpha }} + ({\overline{\alpha }} -{\underline{\alpha }})u, \\[-3pt]\nonumber \end{align}

(17e) \begin{align} & v^{\prime}={\underline{\beta }} + ({\overline{\beta }} -{\underline{\beta }})v \\[-3pt]\nonumber \end{align}

(17f) \begin{align} & A^{\prime} = 1 + \cos{\overline{\gamma }} \cos v^{\prime} +\cos{\overline{\gamma }} \cos u^{\prime} + \cos u^{\prime} \cos v^{\prime}, \\[-3pt]\nonumber \end{align}

(17g) \begin{align} & B^{\prime} = \sin{\overline{\gamma }} \sin u^{\prime} \sin v^{\prime}. \\[20pt]\nonumber \end{align}

Eqs. (17a–17c) is valid iff $A^{\prime}+B^{\prime} \ne 0$ and that the same has been discussed further in Appendix B. Therefore, the task reduces to finding the critical points of the squared distance function from the origin, which is given by

(18) \begin{align} r^2 := d_1^2 + d_2^2 + d_3^2. \\[-4pt]\nonumber \end{align}

From Eq. (5), $r^2$ equals $\tan ^2\frac{\phi }{2}$ , where $\phi \in (0, \pi )$ denotes the critical value of the rotation that may be achieved. In view of the expressions of $d_i$ in terms of $\{u,v\}$ , $r^2$ may be written explicitly in terms of $\{u,v\}$ , leading to the formulation of the following optimisation problem:

(19) \begin{align} \begin{aligned} &\underset{\{u,v\}}{\text{Maximise}} & & f(u,v)= r^2, \\ &\text{subject to} & & u,v \in [0,1]. \end{aligned} \\[-4pt]\nonumber \end{align}

Using the constrained Lagrangian formulation to incorporate the boundary constraints, the objective function becomes

(20) \begin{equation}{\mathcal{L}}(u,v) = f - \lambda _1 (u-s_1)- \lambda _2(u-1+s_2)- \lambda _3(v-s_3)-\lambda _4(v-1+s_4), \end{equation}

where $\lambda _i,i=1,\dots, 4$ are the Lagrange multipliers and $s_j,j=1,\dots, 4$ , the slack variables (see [Reference Deb28], p. 361). Setting the partial derivatives of $\mathcal{L}$ w.r.t. $\{u,v,\lambda _i,s_j\}$ to zero, the corresponding equations are obtained as follows:

(21a) \begin{align} & \frac{\partial{\mathcal{L}}}{\partial u}:=-\lambda _1-\lambda _2+f_u(u,v)=0; \quad \text{where} \quad f_u(u,v) = \frac{\partial f}{\partial u}; \\[-3pt]\nonumber \end{align}

(21b) \begin{align} & \frac{\partial{\mathcal{L}}}{\partial v}:=-\lambda _3-\lambda _4+f_v(u,v)=0; \quad \text{where} \quad f_v(u,v) = \frac{\partial f}{\partial v}; \\[-3pt]\nonumber \end{align}

(21c) \begin{align} &\frac{\partial{\mathcal{L}}}{\partial \lambda _1}:= s_1-u=0, \quad \frac{\partial{\mathcal{L}}}{\partial \lambda _2}:= 1-s_2-u=0,\quad \frac{\partial{\mathcal{L}}}{\partial \lambda _3}:= s_3-v=0,\quad \nonumber \\ &\frac{\partial{\mathcal{L}}}{\partial \lambda _4}:=1-s_4-v=0, \\[-3pt]\nonumber \end{align}

(21d) \begin{align} &\frac{\partial{\mathcal{L}}}{\partial s_1}:=\lambda _1=0,\quad \frac{\partial{\mathcal{L}}}{\partial s_2}:=-\lambda _2=0,\quad \frac{\partial{\mathcal{L}}}{\partial s_3}:=\lambda _3=0,\quad \frac{\partial{\mathcal{L}}}{\partial s_4}:=-\lambda _4=0. \\[15pt]\nonumber \end{align}

Eq. (21d) shows that $\lambda _i = 0, i=1,\dots, 4$ . Therefore, Eqs. (21a, 21b) reduce to two transcendental equations, respectively:

(22a) \begin{align} & f_u(u,v)=0, \\[-3pt]\nonumber \end{align}

(22b) \begin{align} & f_v(u,v)=0. \\[15pt]\nonumber \end{align}

The real solutions of $\{u,v\}$ obtained from Eqs. (22a, 22b) are used in Eqs. (21c) to obtain the corresponding values of $s_j$ . If $s_j \gt 0\; \forall j$ , then the solutions $\{u,v\}$ are deemed feasible. If $s_j=0$ for some $j$ , then the critical point lies on the corresponding boundary of the domain of $\{u,v\}$ . The solutions leading to $s_j\lt 0$ for any $j$ are infeasible. Thus, the above method of solving a constrained optimisation problem is seen to be equivalent to the solutions of the corresponding unconstrained problem, followed by imposing the boundary constraints on the real solutions to identify the feasible ones among those.

The critical points are identified as follows. Expressions of $f_u(u,v)$ and $f_v(u,v)$ are quoted below.

(23a) \begin{align} &f_u(u,v) = \frac{2{\underline{\alpha }} \left (\cos u^{\prime\prime} \sin v^{\prime\prime}\sin \frac{{\overline{\gamma }}}{2} -\sin u^{\prime\prime} \cos v^{\prime\prime}\cos \frac{{\overline{\gamma }}}{2}\right )}{C}, \\[-3pt]\nonumber \end{align}

(23b) \begin{align} &f_v(u,v) = \frac{2{\underline{\beta }} \left (\sin u^{\prime\prime} \cos v^{\prime\prime}\sin \frac{{\overline{\gamma }}}{2} -\cos u^{\prime\prime} \sin v^{\prime\prime}\cos \frac{{\overline{\gamma }}}{2} \right )}{C}, \quad \text{where} \\[-3pt]\nonumber \end{align}

(23c) \begin{align} &u^{\prime\prime}=\frac{{\underline{\alpha }}}{2}(1-2u), \\[-3pt]\nonumber \end{align}

(23d) \begin{align} & v^{\prime\prime}= \frac{{\underline{\beta }}}{2} (1-2v), \\[-3pt]\nonumber \end{align}

(23e) \begin{align} &C = \left (\sin u^{\prime\prime} \sin v^{\prime\prime} \sin \frac{{\overline{\gamma }}}{2} + \cos u^{\prime\prime} \cos v^{\prime\prime}\cos \frac{{\overline{\gamma }}}{2}\right )^3. \\[15pt]\nonumber \end{align}

Since ${\underline{\alpha }},{\underline{\beta }}$ cannot vanish, the larger factors appearing in the numerators of $f_u(u,v)$ and $f_v(u,v)$ form a system of linear equations in $\{\sin u^{\prime\prime},\cos u^{\prime\prime}\}$ , which may be written in the form:

(24a) \begin{align} &\boldsymbol{A} \boldsymbol{x} = \boldsymbol{0}, \quad \text{where}, \\[-3pt]\nonumber \end{align}

(24b) \begin{align} &\boldsymbol{A}= \begin{bmatrix} \cos v^{\prime\prime} \cos \frac{{\overline{\gamma }}}{2} & -\sin v^{\prime\prime} \sin \frac{{\overline{\gamma }}}{2} \\ -\cos v^{\prime\prime} \sin \frac{{\overline{\gamma }}}{2} & \sin v^{\prime\prime} \cos \frac{{\overline{\gamma }}}{2} \end{bmatrix}, \quad \text{and} \\[-3pt]\nonumber \end{align}

(24c) \begin{align} & \boldsymbol{x} = \begin{bmatrix} \sin u^{\prime\prime} \\ \cos u^{\prime\prime} \end{bmatrix}. \\[15pt]\nonumber \end{align}

Given that ${\| \boldsymbol{x}\|} = 1\; \forall u^{\prime\prime}\in{\mathbb{R}}$ , for Eq. (24a) to be consistent, one must have $\det (\boldsymbol{A}) = 0$ and $\boldsymbol{x} \in \mathcal{N}(\boldsymbol{A})$ , where $\mathcal{N}({\cdot})$ denotes the nullspace of a matrix. The determinantal equation may be expanded as

(25) \begin{align} \det (\boldsymbol{A}):=\frac{\cos{\overline{\gamma }}}{2} \sin \left ({\underline{\beta }}(1-2 v)\right ) = 0. \end{align}

The solution of Eq. (25) is obtained as

(26) \begin{align}{\underline{\beta }}(1-2 v) = 0 \ \text{or} \ \pm N\pi, \ N \in \mathbb{Z}; \\[-3pt]\nonumber \end{align}

(27) \begin{align} \Rightarrow v ={\frac{1}{2}}, \quad \text{since} \ v \in [0, 1]. \\[15pt]\nonumber \end{align}

Similarly, it is found that

(28) \begin{align} u ={\frac{1}{2}}. \end{align}

Thus, $\{u,v\}=\{1/2,1/2\}$ is the unique critical point, which is also feasible, as can be verified trivially. Also, at this point, one can verify that

(29) \begin{equation} C = \cos ^3 \frac{{\overline{\gamma }}}{2} \ne 0, \quad \text{since}\;{\overline{\gamma }}\in \left (0,\frac{\pi }{2}\right ), \end{equation}

which bolsters the validity of the solution.

The value of the objective function at this critical point is computed from Eqs. (17a–17c, 18, 19) as

(30a) \begin{align} &r^2 = \tan ^{2}\frac{{\overline{\gamma }}}{2}, \\[-3pt]\nonumber \end{align}

(30b) \begin{align} \Rightarrow & r = \pm \left |\tan \frac{{\overline{\gamma }}}{2}\right | = \tan \frac{{\overline{\gamma }}}{2}, \ \text{and} \ \tan \frac{{\underline{\gamma }}}{2}, \; \text{as}\;{\underline{\gamma }} = -{\overline{\gamma }}. \\[15pt]\nonumber \end{align}

Corresponding to the pair of solutions above, there are two points of tangency between the maximal sphere and two of the surfaces delimiting $\mathcal{V}_{\mathcal{R}}$ , namely, ${\mathcal{Q}}_{{\overline{\gamma }}}$ , and ${\mathcal{Q}}_{{\underline{\gamma }}}$ . The locations of these points, respectively, are obtained from Eqs. (11) as

(31a) \begin{align} & \overline{\boldsymbol{m}}^* = \tan \frac{{\overline{\gamma }}}{2}\left [1,0,0\right ]^{\top }, \\[-3pt]\nonumber \end{align}

(31b) \begin{align} & \underline{\boldsymbol{m}}^* = \tan \frac{{\underline{\gamma }}}{2}\left [1,0,0\right ]^{\top }. \\[15pt]\nonumber \end{align}

These points of tangency and parts of the corresponding surfaces are shown in Figures 7a and 7b, respectively.

Figure 7. Spheres tangent to (a) ${\mathcal{Q}}_{{\overline{\gamma }}}$ and (b) ${\mathcal{Q}}_{{\underline{\gamma }}}$ of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ corresponding to the faces $\mathcal{F}_{{\overline{\gamma }}}$ and $\mathcal{F}_{{\underline{\gamma }}}$ , respectively (refer to Table III for corresponding numeric details).

The above computations need to be repeated only for two of the remaining four surfaces due to the symmetry in the limits of Euler angles. It may be verified that the surfaces ${\mathcal{Q}}_{{\overline{\beta }}}$ and ${\mathcal{Q}}_{{\overline{\alpha }}}$ are tangent to two spheres, with radii $\left |\tan \frac{{\overline{\beta }}}{2}\right |$ and $\left |\tan \frac{{\overline{\alpha }}}{2}\right |$ , respectively. Finally, taking all of these into consideration, the largest sphere ( $\overline{{\mathcal{S}}}$ ) that fits completely inside $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ is found to be the one with the following radius ( $\overline{r}$ ):

(32) \begin{align} {\overline{r}} = \min \left \{ \left |\tan \frac{{\overline{\alpha }}}{2}\right |, \left |\tan \frac{{\overline{\beta }}}{2}\right |, \left |\tan \frac{{\overline{\gamma }}}{2}\right | \right \}. \end{align}

The sphere $\overline{{\mathcal{S}}}$ with radius $\overline{r}$ in $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ are shown in Figures 8a and 8b, respectively. Due to the central symmetry (as explained in Section 2.3) between the vertices of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ , $\overline{{\mathcal{S}}}$ is tangent to the surfaces ${\mathcal{Q}}_{{\overline{\alpha }}}$ and ${\mathcal{Q}}_{{\underline{\alpha }}}$ in both cases.

Figure 8. Sphere $\overline{{\mathcal{S}}}$ inside $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ corresponding to the non-uniform ranges of Euler angles $\{\alpha, \beta, \gamma \}\in [-30^\circ, 30^\circ ]\times [-40^\circ, 40^\circ ]\times [-50^\circ, 50^\circ ]$ (refer to Table III). In each case, $\overline{{\mathcal{S}}}$ is tangent to the surface corresponding to $\alpha =30^\circ$ .

The surfaces ${\mathcal{Q}}_{{\overline{\alpha }}}$ , etc., are derived in their implicit forms and characterised geometrically in the following section .

4. Geometric Characterisation of ${\mathcal{Q}}_{\overline{\gamma}}$ , ${\mathcal{Q}}_{\text{\underline{$\gamma$}}}$ , etc

The parametric forms of the surfaces ${\mathcal{Q}}_{{\overline{\alpha }}}$ , etc., accomplish the main goal of this work, namely, the identification of the largest contained sphere $\overline{{\mathcal{S}}}$ analytically. However, it is of interest to study these surfaces further to understand their geometric natures. This has been presented in the following by first converting these surfaces to their respective implicit forms, followed by a comprehensive characterisation. It is found that each of the surfaces ${\mathcal{Q}}_{{\overline{\alpha }}}$ , etc., are quadrics in nature; more precisely, they form hyperboloids of one sheet. The largest contained sphere is computed in this new geometric framework as well, which serves as an alternative derivation as well as a formal confirmation of the results obtained in Section 3.

4.1. Derivation of the implicit forms of the bounding surfaces ${\mathcal{Q}}_{\overline{\gamma}}$ , ${\mathcal{Q}}_{\text{\underline{$\gamma$}}}$ , etc

The trigonometric parametrisation of the surfaces ${\mathcal{Q}}_{{\overline{\gamma }}}$ , ${\mathcal{Q}}_{{\underline{\gamma }}}$ , etc., (presented in Eqs. (17a-17c)) makes it difficult to understand their geometric nature. Hence, these trigonometric functions are converted to their algebraic counterparts in the variables $\{{t_\alpha },{t_\beta },{t_\gamma }\}$ using the standard tangent of half angle transformations:

(33) \begin{align} &{t_\alpha } = \tan \frac{\alpha }{2}, \quad{t_\beta } = \tan \frac{\beta }{2}, \quad{t_\gamma } = \tan \frac{\gamma }{2}, \quad \text{such that} \\[-3pt]\nonumber \end{align}

(34) \begin{align} & \sin \alpha = \frac{2{t_\alpha }}{1+{t_\alpha }^2}, \quad \cos \alpha = \frac{1-{t_\alpha }^2}{1+{t_\alpha }^2}, \quad \text{and so on.} \\[15pt]\nonumber \end{align}

Further, two new parameters, namely, $\{{\tilde{u}},{\tilde{v}}\}$ , are introduced to describe each of the surfaces. For example, the surface ${\mathcal{Q}}_{{\overline{\alpha }}}$ is re-parametrised as

(35a) \begin{align} &{t_\alpha } ={t_{{\overline{\alpha }}}}, \ \text{and} \\[-3pt]\nonumber \end{align}

(35b) \begin{align} &{t_\beta } ={t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}} -{t_{{\underline{\beta }}}} ){\tilde{u}}, \\[-3pt]\nonumber \end{align}

(35c) \begin{align} &{t_\gamma } ={t_{{\underline{\gamma }}}} + ({t_{{\overline{\gamma }}}} -{t_{{\underline{\gamma }}}}){\tilde{v}}, \ \text{where} \\[-3pt]\nonumber \end{align}

(35d) \begin{align} &{t_{{\overline{\alpha }}}} =\tan \frac{{\overline{\alpha }}}{2}, \quad{t_{{\underline{\alpha }}}} =\tan \frac{{\underline{\alpha }}}{2}. \\[15pt]\nonumber \end{align}

Similarly, ${\mathcal{Q}}_{{\overline{\beta }}}$ , ${\mathcal{Q}}_{{\overline{\gamma }}}$ may be described by, respectively:

(36a) \begin{align} &{{\mathcal{Q}}_{{\overline{\beta }}}}\,:\,{t_\alpha } ={t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}} -{t_{{\underline{\alpha }}}} ){\tilde{u}}, \quad{t_\beta } ={t_{{\overline{\beta }}}}, \quad{t_\gamma } ={t_{{\underline{\gamma }}}} + ({t_{{\overline{\gamma }}}} -{t_{{\underline{\gamma }}}}){\tilde{v}}, \\[-3pt]\nonumber \end{align}

(36b) \begin{align} &{{\mathcal{Q}}_{{\overline{\gamma }}}}\,:\,{t_\alpha } ={t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}} -{t_{{\underline{\alpha }}}} ){\tilde{u}}, \quad{t_\beta } ={t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}} -{t_{{\underline{\beta }}}} ){\tilde{v}}, \quad{t_\gamma } ={t_{{\overline{\gamma }}}}, \quad \text{where} \\[-3pt]\nonumber \end{align}

(36c) \begin{align} &{t_{{\overline{\beta }}}} =\tan \frac{{\overline{\beta }}}{2}, \quad{t_{{\underline{\beta }}}} =\tan \frac{{\underline{\beta }}}{2},\quad{t_{{\overline{\gamma }}}} =\tan \frac{{\overline{\gamma }}}{2}, \quad \text{and}\;{t_{{\underline{\gamma }}}} =\tan \frac{{\underline{\gamma }}}{2}. \\[15pt]\nonumber \end{align}

Parametrisation of ${\mathcal{Q}}_{{\underline{\alpha }}}$ , ${\mathcal{Q}}_{{\underline{\beta }}}$ and ${\mathcal{Q}}_{{\underline{\gamma }}}$ in terms of $\tilde{u}$ and $\tilde{v}$ may be performed in an analogous manner. Derivation of the implicit forms of these surfaces requires the elimination of the parameters $\tilde{u}$ , $\tilde{v}$ from the parametric forms of these surfaces. The process is described below in the context of the surface ${\mathcal{Q}}_{{\overline{\gamma }}}$ , using the Z-Y-X sequence of Euler angles.

Using Eqs. (34), and (36b) in Eqs. (11), the Rodrigues parameters $\{d_1,d_2,d_3\}$ are expressed in terms of $\tilde{u}$ , $\tilde{v}$ :

(37a) \begin{align} &d_1 = \frac{-\left ({t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}){\tilde{u}}\right ) \left ({t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}} -{t_{{\underline{\beta }}}}){\tilde{v}}\right )+{t_{{\overline{\gamma }}}}}{D}, \\[-3pt]\nonumber \end{align}

(37b) \begin{align} &d_2 = \frac{\left ({t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}} -{t_{{\underline{\alpha }}}}){\tilde{u}}\right ){t_{{\overline{\gamma }}}} +{t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}} -{t_{{\underline{\beta }}}}){\tilde{v}}}{D}, \\[-3pt]\nonumber \end{align}

(37c) \begin{align} &d_3 = \frac{{t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}} -{t_{{\underline{\alpha }}}}){\tilde{u}} -\left ({t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}){\tilde{v}}\right ){t_{{\overline{\gamma }}}}}{D}, \quad \text{where} \\[-3pt]\nonumber \end{align}

(37d) \begin{align} &D = 1+ \left (({t_{{\underline{\alpha }}}} + ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}){\tilde{u}})({t_{{\underline{\beta }}}} + ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}){\tilde{v}})\right ){t_{{\overline{\gamma }}}}. \\[15pt]\nonumber \end{align}

In the following, it would be assumed that $D \ne 0$ , which would be verified later (see Section 4.4).

Eq. (37a–37c) is bilinear in $\{{\tilde{u}},{\tilde{v}}\}$ ; that is, they contain the following monomials Footnote ⁷ (see, e.g., [Reference Cox, Little and O’Shea29], pp. 1–2): $\{{\tilde{u}},{\tilde{v}},{\tilde{u}}{\tilde{v}}\}$ . These equations may be organised into the following linear system:

(38a) \begin{align} &\widetilde{\boldsymbol{M}} \tilde{\boldsymbol{x}} = \tilde{\boldsymbol{b}}, \quad \text{where} \\[-3pt]\nonumber \end{align}

(38b) \begin{align} &\widetilde{\boldsymbol{M}} = \begin{bmatrix} -({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}){t_{{\underline{\beta }}}} (d_1{t_{{\overline{\gamma }}}}+1) & -{t_{{\underline{\alpha }}}} ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}) (d_1{t_{{\overline{\gamma }}}}+1) & - ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}) (d_1{t_{{\overline{\gamma }}}}+1) \\ -({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}})(d_2{t_{{\underline{\beta }}}}-1){t_{{\overline{\gamma }}}} & -({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}) (d_2{t_{{\underline{\alpha }}}}{t_{{\overline{\gamma }}}}-1)& - ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}) d_2{t_{{\overline{\gamma }}}} \\ -({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) (d_3{t_{{\underline{\beta }}}}{t_{{\overline{\gamma }}}}-1) & - (d_3{t_{{\underline{\alpha }}}}+1) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}){t_{{\overline{\gamma }}}} & -d_3 ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}}){t_{{\overline{\gamma }}}} \end{bmatrix}, \\[-3pt]\nonumber \end{align}

(38c) \begin{align} &\tilde{\boldsymbol{b}} = [d_1 (1+{t_{{\underline{\alpha }}}}{t_{{\underline{\beta }}}}{t_{{\overline{\gamma }}}})+{t_{{\underline{\alpha }}}}{t_{{\underline{\beta }}}}-{t_{{\overline{\gamma }}}},d_2 (1 +{t_{{\underline{\alpha }}}}{t_{{\underline{\beta }}}}{t_{{\overline{\gamma }}}})-({t_{{\underline{\alpha }}}}{t_{{\overline{\gamma }}}}+{t_{{\underline{\beta }}}}),d_3(1+{t_{{\underline{\alpha }}}}{t_{{\underline{\beta }}}}{t_{{\overline{\gamma }}}})-{t_{{\underline{\alpha }}}} +{t_{{\overline{\beta }}}}{t_{{\overline{\gamma }}}}]^{\top }, \\[-3pt]\nonumber \end{align}

(38d) \begin{align} & \tilde{\boldsymbol{x}} = [{\tilde{u}},{\tilde{v}}, w]^{\top }, \quad \text{and} \\[-3pt]\nonumber \end{align}

(38e) \begin{align} & w ={\tilde{u}}{\tilde{v}}. \\[15pt]\nonumber \end{align}

The determinant of $\det (\widetilde{M})$ is given by

(39) \begin{align} \det \left (\widetilde{\boldsymbol{M}}\right ) =({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}})^2 ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}})^2 \left (1+{t_{{\overline{\gamma }}}}^2\right ) (1 +{t_{{\overline{\gamma }}}} d_1). \end{align}

Eq. (38a) can yield a non-trivial solution iff $\det (\widetilde{M}) \ne 0$ , which is always the case. It is obvious that the first two factors in the R.H.S. of Eq. (39) cannot vanish. The third factor is always greater than unity, but it becomes infinite at a half-turn, which is excluded from this study (see Section 2). The last factor cannot vanish either, since it may be verified that the corresponding expression of $d_1$ , when substituted back in Eqs. (37a–37c) makes the system inconsistent. Therefore, the solution for $\tilde{\boldsymbol{x}}$ is obtained as

(40a) \begin{align} &\tilde{\boldsymbol{x}} = \frac{\text{adj}\left (\widetilde{\boldsymbol{M}}\right )}{\det \left (\widetilde{\boldsymbol{M}}\right )}\widetilde{\boldsymbol{b}}; \\[-3pt]\nonumber \end{align}

(40b) \begin{align} \Rightarrow &{\tilde{u}} = \frac{-{t_{{\underline{\alpha }}}} (1+{t_{{\overline{\gamma }}}} d_1)+d_2{t_{{\overline{\gamma }}}}+d_3}{({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}})(1+{t_{{\overline{\gamma }}}} d_1)}, \\[-3pt]\nonumber \end{align}

(40c) \begin{align} &{\tilde{v}} = \frac{{t_{{\underline{\beta }}}}(1+{t_{{\overline{\gamma }}}} d_1)+d_3{t_{{\overline{\gamma }}}}-d_2}{({t_{{\underline{\beta }}}}-{t_{{\overline{\beta }}}})(1+{t_{{\overline{\gamma }}}} d_1)}, \\[-3pt]\nonumber \end{align}

(40d) \begin{align} &w =\frac{{t_{{\underline{\alpha }}}}{t_{{\underline{\beta }}}}(1 +{t_{{\overline{\gamma }}}} d_1) -{t_{{\underline{\beta }}}}(d_3 +{t_{{\overline{\gamma }}}} d_2) +{t_{{\overline{\gamma }}}}(1 +{t_{{\underline{\alpha }}}} d_3)-d_2{t_{{\underline{\alpha }}}} -d_1}{({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}})(1+{t_{{\overline{\gamma }}}} d_1)}. \\[15pt]\nonumber \end{align}

Using Eqs. (40b–40d) in the identity $w ={\tilde{u}}{\tilde{v}}$ (see Eq. (38e)), one can eliminate $\tilde{u}$ , $\tilde{v}$ simultaneously from Eqs. (37a–37c) to obtain the desired implicit form of ${\mathcal{Q}}_{{\overline{\gamma }}}$ in terms of $d_i$ :

(41) \begin{align} \frac{d_1 (1+d_1{t_{{\overline{\gamma }}}}-{t_{{\overline{\gamma }}}}^2)+(d_2{t_{{\overline{\gamma }}}}+d_3) (d_2-d_3{t_{{\overline{\gamma }}}})-{t_{{\overline{\gamma }}}}}{(1+d_1{t_{{\overline{\gamma }}}})^2 ({t_{{\overline{\alpha }}}}-{t_{{\underline{\alpha }}}}) ({t_{{\overline{\beta }}}}-{t_{{\underline{\beta }}}})} =0. \end{align}

The numerator of Eq. (41) defines an algebraic surface of degree two in $\{d_1,d_2,d_3\}$ :

(42) \begin{align}{ U_{{\overline{\gamma }}}:= d_1^2+ d_2^2 - d_3^2 + \frac{2}{\tan{\overline{\gamma }} }d_2 d_3 + \frac{2}{\tan{\overline{\gamma }}} d_1 - 1 = 0, \quad \text{(since\; ${t_{{\overline{\gamma }}}} = \tan ({\overline{\gamma }}/2)$)}. } \end{align}

In geometry, such a surface is known as a quadric. In the following, this quadric has been referred to as $\mathcal{U}_{{\overline{\gamma }}}$ and analysed further to ascertain its nature.

4.2. Characterisation of the quadric $\mathcal{U}_{{\overline{\gamma }}}$

Eq. (42) may be cast in the following form:

(43a) \begin{align} &\boldsymbol{\rho }^{\top } \boldsymbol{E} \boldsymbol{\rho }=0,\quad \text{where} \\[-3pt]\nonumber \end{align}

(43b) \begin{align} &\boldsymbol{E} = \begin{bmatrix} \boldsymbol{B} & \boldsymbol{\kappa } \\ \boldsymbol{\kappa }^{\top } & -{t_{{\overline{\gamma }}}} \end{bmatrix}, \\[-3pt]\nonumber \end{align}

(43c) \begin{align} &{\boldsymbol{B} = \begin{bmatrix} 1 & 0 & 0\\ 0 & 1 & \frac{1}{\tan{\overline{\gamma }}}\\ 0 & \frac{1}{\tan{\overline{\gamma }}} & -1 \end{bmatrix}}, \\[-3pt]\nonumber \end{align}

(43d) \begin{align} &{\boldsymbol{\kappa } = \frac{1}{\tan{\overline{\gamma }}}[1,0,0]^{\top }}, \ \text{and} \\[-3pt]\nonumber \end{align}

(43e) \begin{align} & \boldsymbol{\rho } = [d_1, d_2, d_3, 1]^{\top }. \\[15pt]\nonumber \end{align}

To comprehensively characterise the quadric one, $\mathcal{U}_{{\overline{\gamma }}}$ , needs to assess the ranks of $\boldsymbol{E}$ and $\boldsymbol{B}$ , the sign of $\det (\boldsymbol{E})$ and the signs of eigenvalues of $\boldsymbol{B}$ (see, e.g., [Reference Zwillinger30], pp. 219–221). It may be readily verified that both $\boldsymbol{E}$ and $\boldsymbol{B}$ are of full rank, since

(44) \begin{align} {\det (\boldsymbol{E}) = \frac{1}{\mu ^4} \gt 0},\qquad\qquad\qquad\qquad\qquad\end{align}

(45) \begin{align} {\det (\boldsymbol{B}) = -\frac{1}{\mu ^2} \lt 0, \quad \forall{\overline{\gamma }} \in \left (0,\frac{\pi }{2}\right ),\; \text{where}} \end{align}

\begin{align*} &{\mu = 1+ \cos{\overline{\gamma }}}.\end{align*}

The eigenvalues of $\boldsymbol{B}$ , denoted by ${\lambda }_i, i=1,\dots, 3$ , are obtained as

(46) \begin{align}{\lambda }_1 = 1,\quad{{\lambda }_2 = -\frac{1}{\sin{\overline{\gamma }}},} \quad{\lambda }_3 = -{\lambda }_2. \end{align}

Therefore, ${\lambda }_1,{\lambda }_3\gt 0,{\lambda }_2\lt 0 \ \forall{\overline{\gamma }} \in (0,\pi /2)$ . Based on these, it may be inferred that $\mathcal{U}_{{\overline{\gamma }}}$ is a hyperboloid of one sheet (see Figure 9). The sphere $\mathcal{S}$ may now be identified as the largest one centred at the origin and tangent to $\mathcal{U}_{{\overline{\gamma }}}$ . In order to simplify subsequent computations, the quadric $\mathcal{U}_{{\overline{\gamma }}}$ is first reduced to its canonical form, as described below.

Figure 9. Hyperboloid of sheet corresponding to the face $\mathcal{F}_{{\overline{\gamma }}}$ $(\gamma ={\overline{\gamma }}=50^\circ )$ and its local frame of reference ( $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ ) represented in the global reference frame $\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$ .

Figure 10. Intersection of the plane $\mathcal{P}^{\prime}_2$ with the quadric $\mathcal{U}_{{\overline{\gamma }}}$ and the sphere $\mathcal{S}$ .

4.3. Reduction of $\mathcal{U}_{{\overline{\gamma }}}$ to its canonical form

The centre of a central quadric (denoted by $\boldsymbol{o}^{\prime}$ in the case of $\mathcal{U}_{{\overline{\gamma }}}$ ) is characterised by the vanishing of the gradient vector to the quadratic expression of the surface at that point, that is:

(47) \begin{align} &\nabla U_{{\overline{\gamma }}}:=\left (\frac{\partial U_{{\overline{\gamma }}}}{\partial \boldsymbol{d}}\right )\bigg |_{\boldsymbol{d}=\boldsymbol{o}^{\prime}}= \boldsymbol{0}. \end{align}

Upon solving Eq. (47), the desired centre, $\boldsymbol{o}^{\prime}$ , is obtained as

(48) \begin{align}{\boldsymbol{o}^{\prime} = - \frac{1}{\tan{\overline{\gamma }}}\left [1,0,0\right ]^{\top }}. \end{align}

Eq. (48) places the centre $\boldsymbol{o}^{\prime}$ on the axis $\boldsymbol{d}_1$ of the global frame of reference, $\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$ , as shown in Figure 9. The canonical frame of reference of the hyperboloid (denoted by $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ ) is determined by eigenvectors of $\boldsymbol{B}$ , which are computed as

(49) \begin{align} \boldsymbol{d}^{\prime}_1 = [1,0,0]^{\top },\quad \boldsymbol{d}^{\prime}_2= [0,({t_{{\overline{\gamma }}}}-1),(1+{t_{{\overline{\gamma }}}})]^{\top },\quad \boldsymbol{d}^{\prime}_3 = [0,(1+{t_{{\overline{\gamma }}}}),(1-{t_{{\overline{\gamma }}}})]. \end{align}

Given that the eigenvalues are distinct, the eigenvectors form an orthogonal basis, as shown in Figure 9. The axis $\boldsymbol{d}^{\prime}_1$ is aligned with the global coordinate axis $\boldsymbol{d}_1$ , while $\boldsymbol{d}^{\prime}_2,\boldsymbol{d}^{\prime}_3$ span the plane $d_1 = 0$ . The principal planes in $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ passing through $\boldsymbol{d}^{\prime}_1$ are denoted as $\mathcal{P}^{\prime}_2$ (i.e., $d^{\prime}_2=0)$ and $\mathcal{P}^{\prime}_3$ (i.e., $d^{\prime}_3=0)$ and are shown in Figures 10a and 11a, respectively. Finally, $\mathcal{U}_{{\overline{\gamma }}}$ may be expressed in its canonical form using the coordinates $\boldsymbol{d}^{\prime}=[d^{\prime}_1,d^{\prime}_2,d^{\prime}_3]^{\top }$ through the following rigid transformation:

(50a) \begin{align} &\boldsymbol{d} = \boldsymbol{o}_{\text{l}} + \boldsymbol{R}_{\boldsymbol{X}}(\theta )\boldsymbol{d}^{\prime}, \quad \text{since}\; \boldsymbol{d}_1, \boldsymbol{d}^{\prime}_1 \ \text{align with} \; [0,0,1]^{\top };\; \text{and}\\[-3pt]\nonumber \end{align}

(50b) \begin{align} & \theta = \arccos \left (\frac{\boldsymbol{d}^{\prime}_2\cdot \boldsymbol{d}_2}{\sqrt{\boldsymbol{d}^{\prime}_2 \cdot \boldsymbol{d}^{\prime}_2}}\right ) ={\frac{1}{4}(3\pi - 2{\overline{\gamma }})}.\\[15pt]\nonumber \end{align}

Using Eq. (50a) in Eq. (42) results in the standard form of the equation of the hyperboloid, denoted by $U^{\prime}_{{\overline{\gamma }}}$ :

(51) \begin{align} & U^{\prime}_{{\overline{\gamma }}}:=\left (\frac{{d^{\prime}_1}}{a^{\prime}}\right )^2-\left (\frac{{d^{\prime}_2}}{b^{\prime}}\right )^2+\left (\frac{{d^{\prime}_3}}{c^{\prime}}\right )^2 -1 = 0, \ \text{where} \\[-3pt]\nonumber\end{align}

(52) \begin{align} &{a^{\prime} =\frac{1}{\sin{\overline{\gamma }}}}, \\[-3pt]\nonumber\end{align}

(53) \begin{align} & b^{\prime}= \ c^{\prime}= \ \sqrt{a^{\prime}}.\\[15pt]\nonumber \end{align}

Figures 10b and 11b depict the hyperboloid in its canonical frame (labelled as ${\mathcal{U}_{{\overline{\gamma }}}}^{\prime}$ ).

Figure 11. Intersection of the plane $\mathcal{P}^{\prime}_3$ with the quadric $\mathcal{U}_{{\overline{\gamma }}}$ and the sphere $\mathcal{S}$ .

4.4. Identification of the largest contained sphere, $\mathcal{S}$

The sphere $\mathcal{S}$ in $\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$ may also be transformed to the canonical frame $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ by substituting $\boldsymbol{d}$ from Eq. (50a) in Eq. (18). This results in the following equation:

(54) \begin{align}{S^{\prime}:={d^{\prime}_1}^2 +{d^{\prime}_2}^2 +{d^{\prime}_3}^2 - \frac{2}{\tan{\overline{\gamma }}} d^{\prime}_1 - \left (r^2 + \frac{8}{\cos 2{\overline{\gamma }} - 1} + \frac{5}{2}\right )=0}. \end{align}

In Eq. (54), the variable $r$ denotes the radius of the original sphere $\mathcal{S}$ in $\boldsymbol{o}\text{-}\boldsymbol{d}_1\boldsymbol{d}_2\boldsymbol{d}_3$ , as seen in Figure 14. The new sphere, labelled as ${\mathcal{S}}^{\prime}$ , in the frame $\boldsymbol{o}^{\prime}\text{-}\boldsymbol{d}^{\prime}_1\boldsymbol{d}^{\prime}_2\boldsymbol{d}^{\prime}_3$ is shown in Figures 10b and 11b. The centre of the sphere lies on the axis $\boldsymbol{d}^{\prime}_1$ as well. It is located at

(55) \begin{align}{\boldsymbol{o}_{\text{s}}= \frac{1}{\tan{\overline{\gamma }}}\left [1,0,0\right ]^{\top }}. \end{align}

Because of this, the problem of determining the point of tangency between $\mathcal{S}$ and $\mathcal{U}_{{\overline{\gamma }}}$ becomes a trivial one, since it now suffices to study the problem in either of the principal planes of the hyperboloid, given by $\mathcal{P}^{\prime}_2$ or $\mathcal{P}^{\prime}_3$ . The plane $\mathcal{P}^{\prime}_2$ is considered first.

Setting $d^{\prime}_2$ to zero reduces Eq. (51) to that of an ellipse (denoted by $\mathcal{X}_{\text{e}}$ ), given by

(56) \begin{align} X_{\text{e}}:=\left (\frac{d^{\prime}_1}{a^{\prime}}\right )^2+ \left (\frac{d^{\prime}_3}{b^{\prime}}\right )^2 -1= 0. \end{align}

The centre of the ellipse is at the origin of the $\mathcal{P}^{\prime}_2$ plane, that is, $[0,0]^{\top }$ . The orientation of the ellipse can be determined by identifying its major axis. Given that

\begin{align*} \frac{a^{\prime}}{b^{\prime}} & = \frac{a^{\prime}}{\sqrt{a^{\prime}}} \quad \text{(see Eq.\; (53))}\\ & = \frac{1}{\sqrt{\sin{\overline{\gamma }}}}. \end{align*}

Hence, $a^{\prime}\gt b^{\prime} \ \forall{\overline{\gamma }} \in (0, \pi /2)$ . Thus, the major axis of the ellipse $\mathcal{X}_{\text{e}}$ is along the axis $\boldsymbol{d}^{\prime}_1$ .

Similarly, ${\mathcal{S}}^{\prime}$ reduces to a circle (denoted by $\mathcal{C}_{\text{e}}$ ) in the plane $\mathcal{P}^{\prime}_2$ , whose equation is given by

(57) \begin{align}{C_{\text{e}}:={d^{\prime}_1}^2 +{d^{\prime}_3}^2 - \frac{2}{\tan{\overline{\gamma }}} d^{\prime}_1 - \left (r^2 -\frac{2}{1-\cos 2{\overline{\gamma }}} + 1\right )=0}. \end{align}

The centre of $\mathcal{C}_{\text{e}}$ also lies on the axis $\boldsymbol{d}^{\prime}_1$ and is located at $\boldsymbol{o}^{\prime}_{\text{e}}=(1/\tan{\overline{\gamma }})[1,0]^{\top }$ (in the $\mathcal{P}^{\prime}_2$ plane).

Figure 12. Ellipse and circle resulting from intersection of $\mathcal{P}^{\prime}_2$ with ${\mathcal{U}^{\prime}_{{\overline{\gamma }}}}$ and ${\mathcal{S}}^{\prime}$ , respectively.

Figure 13. Hyperbola and circle resulting from intersection of $\mathcal{P}^{\prime}_3$ with ${\mathcal{U}^{\prime}_{{\overline{\gamma }}}}$ and ${\mathcal{S}}^{\prime}$ , respectively.

Furthermore, the centre of $\mathcal{C}_{\text{e}}$ lies inside $\mathcal{X}_{\text{e}}$ , since $\operatorname{sgn}(C_{\text{e}}) = \operatorname{sgn}(X_{\text{e}}) = -1$ , when evaluated at their respective centres. Therefore, the radii of the circles tangent to $\mathcal{X}_{\text{e}}$ and centred at $\boldsymbol{o}^{\prime}_{\text{e}}$ are given by (see Figure 12):

(58a) \begin{align} &r^{\prime}_1=a^{\prime}-{\| \boldsymbol{o}^{\prime}_{\text{e}}-\boldsymbol{o}^{\prime}\|}= \frac{1+{t_{{\overline{\gamma }}}}^2}{2{t_{{\overline{\gamma }}}}} - \frac{1-{t_{{\overline{\gamma }}}}^2}{2{t_{{\overline{\gamma }}}}}={t_{{\overline{\gamma }}}} = \tan \frac{{\overline{\gamma }}}{2},\quad \text{and} \\[-3pt]\nonumber \end{align}

(58b) \begin{align} \text{similarly},\ &r^{\prime}_2=a^{\prime}+{\| \boldsymbol{o}^{\prime}_{\text{e}}-\boldsymbol{o}^{\prime}\|} = \frac{1+{t_{{\overline{\gamma }}}}^2}{2{t_{{\overline{\gamma }}}}} + \frac{1-{t_{{\overline{\gamma }}}}^2}{2{t_{{\overline{\gamma }}}}} = \frac{1}{{t_{{\overline{\gamma }}}}} = \frac{1}{\tan \frac{{\overline{\gamma }}}{2}}. \\[15pt]\nonumber\end{align}

Obviously, $r^{\prime}_1 \le r^{\prime}_2\;\forall{\overline{\gamma }} \in (0,\pi /2)$ (as mentioned in Section 2). Hence, the largest circle centred at $\boldsymbol{o}^{\prime}_{\text{e}}$ and contained within $\mathcal{X}_{\text{e}}$ , and consequently, the desired largest sphere centred at $\boldsymbol{d}$ contained inside $\mathcal{U}_{{\overline{\gamma }}}$ share the radius $r^{\prime}_1=r ={t_{{\overline{\gamma }}}}$ . Furthermore, the relevant point of tangency is found to be the terminal point of the major axis of the ellipse/hyperbola lying on the positive $\boldsymbol{d}^{\prime}_1$ coordinate axis. Hence, in the 3D space of Rodrigues parameters $\{d_1,d_2,d_3\}$ , the relevant point of tangency is given by

(59a) \begin{align} \overline{\boldsymbol{m}}^* & = [r_1,0,0]^{\top }\\[-3pt]\nonumber\end{align}

(59b) \begin{align} &{= \tan \frac{{\overline{\gamma }}}{2}[1,0,0]^{\top }}.\\[15pt]\nonumber\end{align}

Identical results may be obtained by considering $\mathcal{P}^{\prime}_3$ plane, wherein the same problem is reduced to the tangency between a circle, $\mathcal{C}_{\text{h}}$ , and a hyperbola, $\mathcal{X}_{\text{h}}$ , as shown in Figure 13. The computations involved are trivial in nature, and are, therefore, omitted for the sake of brevity.

Figure 14. Sphere $\mathcal{S}$ that is tangent to ${\mathcal{Q}}_{{\overline{\gamma }}}$ (and $\mathcal{U}_{{\overline{\gamma }}}$ ) at $\overline{\boldsymbol{m}}^*$ .

Figures 12 and 13 depict $\mathcal{C}_{\text{e}}$ and $\mathcal{C}_{\text{h}}$ of radius $r^{\prime}_1$ that are tangent to $\mathcal{X}_{\text{e}}$ and $\mathcal{X}_{\text{h}}$ , respectively. Similarly, Figure 14 shows that $\mathcal{S}$ is tangent to both ${\mathcal{Q}}_{{\overline{\gamma }}}$ and $\mathcal{U}_{{\overline{\gamma }}}$ at $\overline{\boldsymbol{m}}^*$ . Finally, to determine the parameters $\{{\tilde{u}},{\tilde{v}}\}$ corresponding to the point of tangency, the coordinates of the point $\overline{\boldsymbol{m}}^*$ are inserted in Eqs. (40b) and (40c), resulting in the following expressions:

(60a) \begin{align} &{\tilde{u}} = \frac{{t_{{\underline{\alpha }}}}}{{t_{{\underline{\alpha }}}}-{t_{{\overline{\alpha }}}}}, \\[-3pt]\nonumber\end{align}

(60b) \begin{align} &{\tilde{v}} = \frac{{t_{{\underline{\beta }}}}}{{t_{{\underline{\beta }}}}-{t_{{\overline{\beta }}}}}.\\[15pt]\nonumber\end{align}

Given that the ranges of Euler angles used in this work are symmetric, the corresponding numerical values are

(61) \begin{align} &{\tilde{u}} = \frac{1}{2}, \quad{\tilde{v}} = \frac{1}{2}. \end{align}

An assumption made earlier in this work, namely, $D \ne 0$ (see Section 4.1), may now be verified. Using Eqs. (61) and (3) in Eq. (37d), one finds

(62) \begin{equation} D=1. \end{equation}

5. Numerical Examples

The theoretical results derived above are numerically illustrated in this section. All the computations have been performed using a computer algebra system (CAS), namely, Mathematica 13.1 [31]. The ranges of Euler angles are chosen to be symmetric. However, both the cases of uniform and non-uniform ranges are studied. The corresponding numerical data are presented in Table III, while the locations of the corner points of corresponding $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ have been listed in Table IV.

From Table IV, it is evident that for the non-uniform rangesFootnote ⁸ of Euler angles, the corresponding vertices of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ maintain the central symmetry about the origin. The points $\boldsymbol{m}_i$ and their counterparts $\boldsymbol{n}_j$ have been placed in the same rows in Table IV to accentuate this fact.

5.1. Computation of the largest sphere $\overline{{\mathcal{S}}}$ contained in $\mathcal{V}_{\mathcal{R}}$

Both uniform and non-uniform ranges are used for demonstrating the computation of the largest contained spheres. The formulation and analytical computations were elaborated above in the context of the Z-Y-X and X-Y-Z sequences of Euler angles. However, the method has been applied to all the other asymmetric/Tait–Bryan sequences, that is, X-Z-Y, Y-X-Z, Y-Z-X, and Z-X-Y, for the sake of completeness. The corresponding results are summarised in Table VII. In all the cases, the analytical results are verified against results obtained from independently performed numerical optimisation, employing the in-built module NMinimize Footnote ⁹ of Mathematica 13.1. In all the cases, the corresponding results are found to agree up to 5 digits after the decimal.

For the “proper” Euler angle sequences, e.g., $Z$ - $Y$ - $Z$ , $Z$ - $X$ - $Z$ and so on, the bounding hyperboloids pass through the origin, as shown in Figures 15a and 15b. Therefore, the volume contained between these around the origin vanishes identically, as shown in Figure 16. While this fact has been depicted visually in the context of the surfaces corresponding to $\mathcal{F}_{{\overline{\gamma }}}$ and $\mathcal{F}_{{\overline{\alpha }}}$ in the said figures, respectively (using the $Z$ - $Y$ - $Z$ Euler angle sequence), it holds in all the other such cases as well. As can be seen in Figure 16, multiple bounding surfaces of $\mathcal{V}_{\mathcal{R}}$ intersect at the origin for such sequences, which, in turn, reduces the radius of the largest sphere centred at the origin of $\mathcal{V}_{\mathcal{R}}$ to zero. Therefore, such Euler angle sequences are not included in the above study.

Figure 15. Surfaces corresponding to the non-uniform ranges of Euler angles $\{\alpha, \beta, \gamma \}\in\times$ $ [-30^\circ, 30^\circ ] [-40^\circ, 40^\circ ]\times [-50^\circ, 50^\circ ]$ .

Figure 16. Intersection of the surfaces of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}Z)$ for one instance of proper Euler angles.

5.1.1. Computation of the sphere $\overline{{\mathcal{S}}}$ corresponding to the Z-Y-X and X-Y-Z sequences of rotations for non-uniform ranges of Euler angles

The computation of ${\mathcal{S}} \subset{\mathcal{V}_{\mathcal{R}}(Z\text{-}X\text{-}Y)}$ is considered first. The face $\mathcal{F}_{{\overline{\gamma }}}$ is used for the sake of illustration. As explained before, $\{u,v\}=\{1/2,1/2\}$ is the only real critical point obtained for the face $\gamma ={\overline{\gamma }} = 50^\circ$ , as shown in Figure 7a. Corresponding to the values of $\{u,v\}$ , the critical value of the radius $r$ is computed from Eq. (30b) as $r = \tan (25^\circ ) \approx 0.4663$ .

The results corresponding to the remaining five faces may be found in a similar manner. In all the cases, the critical point in the parameter space corresponds to $\{1/2, 1/2\}$ , and the critical value of the radius matches the tangent of half of the limiting value of the Euler angle defining the face (see Table V). The details are skipped to avoid the repetition of identical analytical steps. As mentioned in Eq. (32), the radius of the largest fully contained sphere, $\overline{{\mathcal{S}}}$ , is obtained as ${\overline{r}} = \tan (15^\circ ) \approx 0.2679$ and corresponding points of tangency are $\overline{\boldsymbol{m}}^*=[0,0,0.2679]^{\top }$ and $\underline{\boldsymbol{m}}^*=[0,0,-0.2679]^{\top }$ . This corresponds to the smallest limit among the three Euler angles, namely, ${\overline{\alpha }} = 30^\circ$ , as shown in Figure 8a. The same process is repeated to find ${\overline{{\mathcal{S}}}} \subset{\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)}$ . Not surprisingly, the results are identical to the case of ${\overline{{\mathcal{S}}}} \subset{\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)}$ as depicted in Figure 8b.

Table V. Critical values of $\{u,v\}$ , and the corresponding points of tangency and radii of the largest included spheres in $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ for non-uniform ranges of Euler angles.

Table VI. Values of $\{u,v\}$ , corresponding $\underline{\boldsymbol{m}}^*$ , $\overline{\boldsymbol{m}}^*$ , $\underline{\boldsymbol{n}}^*$ , $\overline{\boldsymbol{n}}^*$ and $r$ of $\mathcal{S}$ in $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ for uniform ranges of Euler angles.

5.1.2. Computation of the sphere $\overline{{\mathcal{S}}}$ corresponding to the Z-Y-X and X-Y-Z rotation sequences using uniform ranges of Euler angles

The uniform Euler angles listed in Table III are used for the computation of $\overline{{\mathcal{S}}}$ . Similar to the case of non-uniform Euler angles, the solution of the optimisation problem is $\{u,v\}=\{1/2,1/2\}$ for each surface of $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ . The radii of the spheres tangent to the bounding surfaces, as well as the corresponding points of tangency, are listed in Table VI. As can be seen from the table, due to the symmetry in the limits of Euler angles, the radii of the said spheres are identical. Hence, the radius $\overline{r}$ of the largest sphere $\overline{{\mathcal{S}}}$ that fits inside $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ is evaluated as ${\overline{r}}=\tan (15^\circ ) \approx 0.2679$ , as shown in Figure 17a. As $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ are related through the aforementioned central symmetry, and due to the uniformity in the ranges of Euler angles, the sphere $\overline{{\mathcal{S}}}$ corresponding to $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ is identical to the one corresponding to the Z-Y-X rotations, as shown in Figure 17b.

Table VII. Results corresponding to Tait–Bryan sequence of rotations for non-uniform ranges of Euler angles listed in Table III.

Figure 17. Sphere $\overline{{\mathcal{S}}}$ inside $\mathcal{V}_{\mathcal{R}}(Z\text{-}Y\text{-}X)$ and $\mathcal{V}_{\mathcal{R}}(X\text{-}Y\text{-}Z)$ corresponding to the uniform ranges of Euler angles $\alpha, \beta, \gamma \in [-30^\circ, 30^\circ ]$ (refer to Table III). In each case, $\overline{{\mathcal{S}}}$ is tangent to all the surfaces of the solid.

5.1.3. Computation of the spheres corresponding to the X-Z-Y, Y-Z-X, Y-X-Z and Z-X-Y sequences for non-uniform ranges of Euler angles

The same procedure, as mentioned in Section 5.1.1, is followed to compute the largest sphere $\overline{{\mathcal{S}}}$ that fits inside ${\mathcal{V}_{\mathcal{R}}}(\text{{X}-{Z}-{Y}})$ , ${\mathcal{V}_{\mathcal{R}}}(\text{{Y}-{Z}-{X})}$ , ${\mathcal{V}_{\mathcal{R}}}(\text{{Y}-{X}-{Z}})$ , and ${\mathcal{V}_{\mathcal{R}}}(\text{{Z}-{X}-{Y}})$ , respectively, to cover comprehensively the remaining cases of Tait–Bryan sequences. The ranges of Euler angles are specified numerically in Table III. The included largest spheres are shown in Figures 18a, 18b, 18c and 18d, respectively.

Table VII summarises the results for all of the six possible cases of Tait–Bryan angles. The results are identical since the radius of the largest included sphere, $\overline{r}$ , is given by the tangent of the half-angle corresponding to the smallest of the limiting values, that is, $\overline{\phi } = \min \{{\overline{\alpha }},{\overline{\beta }},{\overline{\gamma }}\} ={\overline{\alpha }}$ , in this case (see Table III).

Figure 18. Solids corresponding to the non-uniform ranges of Euler angles $\{\alpha, \beta, \gamma \}\in$ $[-30^\circ, 30^\circ ]\times [-40^\circ, 40^\circ ]\times [-50^\circ, 50^\circ ]$ (refer to Table III). In each case, $\overline{{\mathcal{S}}}$ is tangent to the surface of the solids corresponding to the face $\alpha =30^\circ$ .

6. Summary and discussions

The main results and the contributions of this article are discussed briefly in this section.

This article studies different representations of $\mathbb{SO}(3)$ , in order to explore the possibility of using them to describe subsets of $\mathbb{SO}(3)$ geometrically, in a manner that is both simple and physically meaningful. This is a non-trivial problem since not all mathematical structures are compatible with all the parametrisations of $\mathbb{SO}(3)$ ; for example, it is meaningless to employ the Euclidean metric to compute the “distance between two rotations” in the Euler angle parametrisation. Therefore, proper combinations of parametrisations and choice of geometric shapes to describe the subsets are important. This is achieved in this article by using the Rodrigues parameters for computations, owing to the existence of a valid measure of distance from the origin in its own neighbourhood.

The theme of this article is entirely novel. It looks into descriptions of subsets in $\mathbb{SO}(3)$ and their relations, which, surprisingly, find no mention in the existing literature. For example, cuboids in the space of Euler angles are used quite commonly for this purpose, even though the validity or physical implications of the same have not been documented ever, to the best of the knowledge of the authors. This leaves some pertinent questions unanswered; for instance, given two cuboids, how does one find the set of rotations which are included in both? Or, how does one decide which one is “bigger” based on a physically meaningful and mathematically admissible scalar quantifier?

In order to investigate these cuboids further, they are first mapped to the space of Rodrigues parameters. This causes significant changes in their geometry, as each face of the cuboids transforms into a patch on the corresponding hyperboloid of one sheet. Accordingly, the cuboids map into solids which look as though they have been twisted about all the three coordinate axes (see Figure 6). Since these complicated shapes impede further analysis, such as a quantitative assessment of their extents, it is sought to identify the largest sphere, centred at the origin, that they enclose. This makes these solids comparable, in terms of the largest spheres (centred at the origin) that they fully enclose.

Furthermore, such a sphere has a great physical significance, as its radius equals $\tan (\overline{\phi }/2)$ , where $\overline{\phi }$ is the maximum angle of rotation that one can achieve about all the spatial directions without violating the limits on the Euler angles specified originally. It is also shown, via direct computation, that irrespective of the Euler angle sequence considered (albeit with a restriction to the Tait–Bryan/Cardan types), the value of $\overline{\phi }$ always equals the least absolute value of the limits on the individual Euler angles. Thus, the radius $\overline{r}$ affords a physically significant quantifiable measure for the extent of rotations permissible within the original cuboid of Euler angles. Moreover, given the simplicity and closed-form nature of the final expression of $\overline{\phi }$ , no computation is required for practical applications of this measure in design and path planning. Moreover, in instances of design applications, Rodrigues parametrisation can be more appropriate than Euler angles. For example, [Reference Kingsley, Martin and Gasho32] describes a Stewart platform manipulator, which is to be used to mount an antenna that tracks the satellite, as it travels over an entire hemisphere. In this case, it is intuitive and trivial to express the desired range of orientations of the moving platform in terms of the normal to the platform, and eventually in terms of Rodrigues parameters, considering the normal to be the axis of non-zero net rotations. In contrast, it is not clear as to what might the required range of Euler angles be to cover the specified range of orientations.

This study legitimises the use of the cuboids in Euler angles (of the Tait–Bryan/Cardan types) to describe subsets of $\mathbb{SO}(3)$ . It can be stated with confidence that any specification of the orientation workspace of a manipulator in terms of permissible Euler angles as $\alpha \in [{\underline{\alpha }},{\overline{\alpha }}]$ , $\beta \in [{\underline{\beta }},{\overline{\beta }}]$ and $\gamma \in [{\underline{\gamma }},{\overline{\gamma }}]$ implies that all rotations about all possible axes in space are permissible to the extent of $\overline{\phi } = \operatorname{min}\{|{\underline{\alpha }}|,|{\overline{\alpha }}|, |{\underline{\beta }}|,|{\overline{\beta }}|,|{\underline{\gamma }}|,|{\overline{\gamma }}|\}$ . Such a result does not seem to exist in the present literature.

All the studies presented in this article have been performed in the analytical form via symbolic computations using a CAS, so as to preserve the generality and exactness of the results. The numerical results have been added only for the sake of illustrations and verifications. It is expected that the novel insights and quantitative measures generated in this study regarding the specifications of orientation workspaces and their physical implications would be beneficial in the process of path planning and design of spatial manipulators, especially those of parallel architecture, as these typically have limited orientation workspaces as opposed to their serial counterparts.