The simplest group of the type CnRI is the group
RI (n=1) generated by an inversion in the circle with
the center in the singular point O of the plane E2. The
inversion RI is the equivalent of the reflection in the
invariant plane of the symmetry groups of tablets G320. From
the existing isomorphism between the symmetry groups of tablets
G320 and conformal symmetry groups of the category C21,
by comparing the transformation RI with the plane reflection
mentioned, corresponding to it in this isomorphism, one can
directly note the properties of the inversion RI - its
involutionality and the relations between the inversion RI and
the other conformal symmetry transformations.
An inversion transforms a point A of the plane E2\{O} onto
the point A' of the same plane, where the vector relationship
(O,A)°(O,A') = r2 holds, and r is the length of a
radius of the inversion circle. An important characteristic of the inversion
RI is the property of equiangularity - the maintenance of the angle
between two arbitrary vectors in the plane E2\{O},
transformed by the inversion RI. The non-metric construction of the
inverse point RI(A) of a point A is based on the fact that the base
point of the hypotenuse altitude and a vertex that belongs to the
hypotenuse are the homologous points of the inversion in the circle with the
center in the other vertex of the hypotenuse and with the radius equal to
the cathete to which this vertex belongs (Figure 4.2). All the lines
containing point O and points of the inversion circle mI are,
respectively, the invariant lines and points of the inversion RI.
Circle lines containing the point O are transformed onto the lines that
do not contain the point O, circle lines that do not contain the point
O are transformed onto the circle lines that do not contain the point
O, while to all the lines not containing the point O correspond the
circle lines containing the point O. Hence, the following relationships
hold:
RI(A) = A iff A Î mI, RI(l) = l iff O Î l,
RI(l) = c iff O not Î l and O Î c,
RI(c) = c1 iff O not Î c and O not Î c1.
Every circle perpendicular to the inversion circle mI is
transformed by the inversion RI onto itself and represents its invariant,
so the relationship RI(c) = c iff c^ mI holds. All the
constructions in which an inversion takes part can be considerably
simplified by using those invariance relations - the invariance of all the
points of the inversion circle mI, of lines containing the singular
point O and of circles perpendicular to the inversion circle mI.
Very important for the simplification of constructions is the fact that
every circle line containing the point O and touching the inversion
circle mI, is transformed onto the tangent line of the circle
mI in the touch point and vice versa, and also every secant of the
inversion circle mI is transformed onto the circle line containing
the singular point O and the intersection points of the secant and
inversion circle. The reverse transformations also hold. Owing to those
characteristics of the non-metric construction of inverse figures,
according to the criterion of maximal constructional simplicity, the metric
construction was rarely used.
Figure 4.2
The construction of homologous points of the inversion RI.
|
Every conformal symmetry group of the type CnRI is the
direct product of the symmetry groups Cn (n) and RI.
Hence, visual interpretations of conformal symmetry groups of the type
CnRI (Figure 4.3, 4.4) can be constructed multiplying by the inversion
RI a rosette with the symmetry group Cn (n), belonging to a
fundamental region of the group RI, or multiplying by the n-fold
rotation a figure with the symmetry group RI, belonging
to the fundamental region of the group Cn (n). A
fundamental region of the group CnRI is the section
of the fundamental regions of the groups Cn (n)
and RI. Owing to the presence of the indirect symmetry
transformation - inversion RI - in groups of the type
CnRI enantiomorphic modifications do not occur. The
visual effect and degree of visual dynamism in rosettes with the
conformal symmetry group CnRI depend exclusively on
the choice of the form of a fundamental region, or on the
position and form of an elementary asymmetric figure within a
fundamental region. A degree of visual dynamism goes from
conformal symmetry rosettes alike to rosettes with the symmetry
group Cn (n) (Figure 4.3), to the conformal
symmetry rosettes with a fully expressed stationary visual
component resulting from the visual effect of the
inversion RI, similar to the visual effect
of a reflection. Those "static" conformal symmetry rosettes with the group
CnRI can be constructed by using an asymmetric figure,
with its shape very close to the inversion circle, or by using a
fundamental region of a similar form (Figure 4.4). A fundamental
region of the group CnRI offers a change of
non-inversional boundaries, i.e. boundaries that do not belong to
the inversion circle mI. This is the only restriction to
the choice of a fundamental region, since the invariance of all
the points of the inversion circle must be preserved.
Figure 4.3
Conformal symmetry rosettes with the symmetry groups of the type
CnRI, which satisfy the principle of maximal constructional simplicity.
|
Figure 4.4
Examples of conformal symmetry rosettes with the symmetry groups of
the type CnRI, with dominant static visual component produced
by the inversion RI.
|
Owing to their low degree of symmetry and visual dynamism
conditioned by the polarity of rotations, conformal symmetry rosettes with
the symmetry group CnRI are very rare in ornamental art. Such
examples as exist are constructed mostly by using half-circles containing
the singular point O, touching the inversion circle and forming a rosette
with the symmetry group Cn (n). They are transformed by the
inversion RI onto the corresponding half-tangents in the touch points
(Figure 4.3). In ornamental art, the frequent use of that construction is
dictated by the principle of maximal constructional and visual simplicity,
while other aspects of conformal symmetry rosettes with the symmetry group
CnRI are rarely found in ornamental art. Conformal symmetry groups
of the type CnRI can be obtained by desymmetrizations of groups of
the type DnRI, the most frequent discrete conformal symmetry groups
of the category C21 in ornamental art. Besides classical-symmetry
desymmetrizations, frequently occurring is the antisymmetry
desymmetrization resulting in the conformal antisymmetry group
DnRI/CnRI, which in the classical theory of symmetry can be
discussed as the group CnRI.
Every group of the type DnRI (Figure 4.5-4.7) is the direct
product of the symmetry groups Dn (nm) and RI. Hence,
visual interpretations of the group DnRI can be constructed
multiplying by the inversion RI a rosette with the symmetry group
Dn (nm), belonging to a fundamental region of the group RI
or, less frequently, multiplying by symmetry transformations of the group
Dn (nm) a figure with the symmetry group RI, belonging
to a fundamental region of the group Dn (nm). A fundamental
region of the group DnRI is the section of fundamental regions of
the groups Dn (nm) and RI. In groups of the type
DnRI, there are no enantiomorphic modifications.
Conformal symmetry rosettes with the symmetry group DnRI
have visual characteristics similar to that of generating rosettes with the
symmetry group Dn (nm). Owing to the presence of reflections
and inversions, these conformal symmetry groups belong to the family of
visually static symmetry groups with non-polar rotations.
Since groups of the type DnRI are generated by reflections
(reflections and inversions), there is no possibility for changing
boundaries of a fundamental region. Owing to the fixed shape of a
fundamental region, tilings corresponding to the group DnRI, for
fixed n, are reduced to only one figure (Figure 4.5). In ornamental art, the
variety, richness and visual interest of conformal symmetry rosettes with
the symmetry group DnRI, is achieved by applying different
elementary asymmetric figures within a fundamental region. The visual
effect of the inversion RI, within the group DnRI depends on the
shape of that elementary asymmetric figure and its position within a
fundamental region. The static visual function of the inversion RI comes
to its full expression for an elementary asymmetric figure, by the shape
and position being very close to the inversion circle.
Figure 4.5
Examples of conformal symmetry rosettes with the symmetry groups of
the type DnRI, constructed according to the principle of
maximal constructional simplicity.
|
In ornamental art, there are many examples of conformal symmetry
rosettes with symmetry groups of the type DnRI. The frequency of
occurrence of a particular group depends on the frequency of occurrence of
its generating group Dn (nm). Therefore, the groups
DnRI, for n - an even natural number, especially for
n = 2,4,6,8,12..., occur most often. These groups satisfy the
principle of visual entropy and offer the possibility of choosing
the position of a corresponding conformal symmetry rosette, such
that its reflection lines coincide with the fundamental natural
directions - the vertical and horizontal line.
Owing to maximal constructional simplicity, groups of the type
DnRI have a special role in ornamental art. Very interesting visual
interpretations of these groups are obtained, reproducing by the inversion
RI a rosette with the symmetry group Dn (nm), constructed by
circles (or their arcs) containing the singular point O and touching the
inversion circle mI. The inversion RI transforms these circles
(arcs) onto the tangent lines (parts of tangent lines) of the inversion
circle in the touch points (Figure 4.6, 4.7). These conformal symmetry
rosettes are used in ornamental art by almost all cultures. They have a
special place in Romanesque and Gothic art, within rosettes used in
architecture.
Figure 4.6
Examples of conformal symmetry rosettes with the symmetry groups of
the type DnRI, which are used in ornamental art.
|
The continuous conformal symmetry group D¥ RI possesses
adequate visual interpretations. One of them is a circle. Regarded from the
point of view of the isometric theory of symmetry, a circle possesses the
continuous symmetry group of rosettes D¥ , but for conformal
symmetry, its symmetry group is D¥ RI. Such
a possibility for different symmetry treatments of the same figure occurs in all situations
when a certain theory (e.g., the isometric theory of symmetry) is extended
to a larger, more general theory (e.g., the theory of conformal symmetry).
Figure 4.7
Examples of conformal symmetry rosettes with the symmetry groups of
the type DnRI, which are used in ornamental art.
|
The simplest group of the type CnZI is the group ZI
(n = 1), generated by the inversional reflection ZI, the
commutative composition of a reflection and an inversion. The
inversional reflection ZI is an equivalent of a two-fold
rotation with the axis belonging to the invariant plane of the
symmetry groups of tablets
G320. Those isomorphism between
conformal symmetry groups of the category C21 and the
symmetry groups of tablets
G320, in which the inversional
reflection ZI corresponds to this two-fold rotation,
indicates the properties of the inversional reflection ZI -
its involutionality and relations to the other conformal symmetry
transformations.
Since the inversional reflection ZI can be represented in the
form ZI = RRI = RIR,
as the commutative product of the reflection R with
the reflection line containing the singular point O and the inversion
RI, many properties of the inversion RI (e.g., the property of
equiangularity, etc.) and the construction methods given analyzing the
symmetry group RI, hold and can be transferred to the inversional
reflection ZI. A fundamental region of the group ZI can coincide
with that of the group RI, but offers a change of the shape of all
its boundaries.
Every group of the type CnZI (Figure 4.8, 4.9) is a
dihedral group derived as a superposition of the groups Cn (n)
and ZI. Their visual interpretations can be constructed multiplying
by the inversional reflection ZI a rosette with the symmetry group
Cn (n), belonging to a fundamental region of the group ZI
or, less frequently, multiplying by the n-fold rotation a conformal
symmetry rosette with the symmetry group ZI, belonging to a fundamental
region of the symmetry group Cn (n). According to the
relationship ZI = RRI = RIR, conformal symmetry rosettes with the symmetry
group CnZI can be directly derived from conformal symmetry rosettes
with the symmetry group
CnRI, by reproducing by the reflection R with the reflection line
defined by the singular point O and by the section of the boundaries of
the fundamental region of the group CnRI with the inversion circle
mI, one class of fundamental regions of the group CnRI (the
internal or external fundamental regions) (Figure 4.8). Conformal symmetry
groups of the type CnZI offer the possibility for the
enantiomorphism. All the other properties of groups of the type CnRI
can be attributed to groups of the type CnZI.
Figure 4.8
Examples of conformal symmetry rosettes with the symmetry groups of
the type CnZI, constructed according to the principle of
maximal constructional simplicity.
|
Figure 4.9
Examples of conformal symmetry rosettes with the symmetry groups of
the type CnZI.
|
Figure 4.10
Examples of conformal symmetry rosettes with the symmetry groups of
the type NI, which satisfy the principle of maximal
constructional simplicity.
|
Figure 4.11
Examples of conformal symmetry rosettes with the symmetry groups of
the type NI.
|
Like the symmetry groups of the type CnRI, the groups of the
type CnZI can be derived by a desymmetrization of the symmetry
groups of the type DnRI. Besides the classical-symmetry
desymmetrizations, antisymmetry desymmetrizations resulting in conformal
antisymmetry groups of the type DnRI/CnZI, discussed in the
classical theory of symmetry within the type CnZI, can
be obtained.
Groups of the type NI (Figure 4.10, 4.11) are generated by
the inversional rotation SI, the commutative composition of the rotation
S of the order 2n and the inversion RI, so that the relationship
SI = SRI = RIS holds.
Hence, conformal symmetry rosettes with the symmetry
group NI can be directly derived from conformal symmetry rosettes
with the symmetry group CnRI, by transforming by the rotation S
one class of fundamental regions (internal or external fundamental regions)
of the group CnRI. A fundamental region of the group NI may
coincide with that of the group CnRI, but it allows the varying
of all the boundaries. Conformal symmetry rosettes with the symmetry group
NI can also be constructed multiplying by the inversional rotation
SI a conformal symmetry rosette with the symmetry group Cn (
n), belonging to a fundamental region of the group RI. Groups of the type
NI are an equivalent of the symmetry groups of tablets G320 of
the type ([2ñ]), generated by n-fold rotational reflection,
so that the relationship S1 = SI2 holds,
where by S1 is denoted the
n-fold rotation. Despite the choice of a fundamental region or an
elementary asymmetric figure within a fundamental region, among all the
conformal symmetry groups of the category C21, conformal rosettes with
groups of the type NI produce the maximal degree of visual dynamism.
Consequently, corresponding conformal symmetry rosettes are very rare in
ornamental art. Owing to their maximal constructional simplicity, the most
frequent are examples of conformal symmetry rosettes with the symmetry group
NI, which consist of half-circles containing the singular point O
and touching the inversion circle mI, and of corresponding
half-tangent lines onto which these half-circles are transformed by the
inversional rotation SI (Figure 4.10). The enantiomorphism does not occur
in groups of the type NI.
Groups of the type NI can also be obtained by
desymmetrizations of groups of the type C2nRI. Besides the
classical-symmetry desymmetrizations, the antisymmetry desymmetrizations
resulting in conformal antisymmetry groups of the type
C2nRI/NI, discussed in the classical theory of
symmetry within the type NI, are very frequent.
According to the relationship SI = SRI = RIS, where by S is
denoted the rotation of the order 2n, a connection, analogous to
that existing between the types CnRI and NI,
exists between the types DnRI and D1NI.
Hence, conformal symmetry rosettes with the symmetry group
D1NI (Figure 4.12, 4.13) can be directly derived from
conformal symmetry rosettes with the symmetry group
DnRI, by reproducing by the rotation S one class of the
fundamental regions (the internal or external fundamental
regions) of the group DnRI. The same result can be
obtained multiplying by the inversional rotation SI a
conformal symmetry rosette with the symmetry group D1
(m), or multiplying by the reflection a conformal
symmetry rosette with the symmetry group NI. All the
other properties of groups of the type D1NI - the
absence of the enantiomorphism, visual characteristics of
corresponding conformal symmetry rosettes, etc. - are similar
to the properties of groups of the type DnRI.
Groups of the type D1NI are isomorphic to the symmetry
groups of tablets G320 of the type ([2ñ])m, generated
by the n-fold rotational reflection and the reflection in the plane
containing the tablet axis.
The variety of conformal symmetry rosettes with the symmetry group
D1NI can be accomplished by the choice of the form of
non-reflectional boundaries of a fundamental region or by using different
elementary asymmetric figures belonging to a fundamental region. In that
way, a large spectrum of the possible degree of visual dynamism can be
achieved (Figure 4.12). It goes from static conformal symmetry rosettes with
the symmetry group D1NI, without the application of an elementary
asymmetric figure within a fundamental region, to conformal symmetry
rosettes of a higher degree of visual dynamism, which can be, for instance,
formed by circle and line segments alternating along a radial line.
By applying the desymmetrization method on groups of the type
D2nRI, groups of the type D1NI can be obtained. Besides
classical-symmetry desymmetrizations, the antisymmetry desymmetrizations
resulting in the conformal antisymmetry groups of the type
D2nRI/D1NI, discussed in the classical
theory of symmetry within the type D1NI, can also be
used.
The symmetry groups of polar rods G31, isomorphic to conformal
symmetry groups of the category C2, can be derived by extending by the
translation, twist and glide reflection, the symmetry groups of tablets
G320, isomorphic to conformal symmetry groups of the category C21.
Hence, conformal symmetry groups of the category C2 can be derived by
extending by the similarity transformations K, L, M, conformal
symmetry groups of the category C21.
Figure 4.12
Examples of conformal symmetry rosettes with the symmetry groups of
the type D1NI.
|
Figure 4.13
Examples of conformal symmetry rosettes with the symmetry groups of
the type D1NI, which are used in ornamental art.
|
According to the theorem that the product of two reflections with
parallel reflection lines is a translation, the modulus of the translation
vector of which is twice the distance between the reflection lines, in the
field of conformal symmetry a dual theorem holds: the product of two circle
inversions with concentric inversion circles is a dilatation with the
dilatation coefficient k = r2/r12,
where r, r1 are the lengths of the radii
of the inversion circles. It indicates the possibility of deriving
conformal symmetry groups of the category C2 that contain a dilatation,
by using inversions in concentric inversion circles.
Figure 4.14
The conformal symmetry rosette with the symmetry group K4I.
|
Conformal symmetry rosettes with the symmetry group KNI
(Figure 4.14) can be constructed multiplying by the dilatation K (with
k > 0) a conformal symmetry rosette with the symmetry group NI,
belonging to a fundamental region of the group K. A fundamental region
of the group KNI is the section of fundamental regions of the groups
K and NI, and it allows a varying of the form of all the
boundaries. Since the dilatation K
is the element of every group of the type KNI, to efficiently
construct the corresponding visual interpretations one applies two
inversions in the concentric inversion circles. All the visual properties of
a generating conformal symmetry rosette with the symmetry group NI,
after the introduction of the dilatation K, are maintained in the derived
conformal symmetry rosette with the symmetry group KNI. The
dilatation K stimulates their visual dynamism, producing the suggestion of
centrifugal expansion. Owing to their low degree of symmetry and to their
visual properties mentioned, the corresponding conformal symmetry rosettes
are very rare in ornamental art. Those examples that exist in ornamental
art, in the first place respect the principle of visual entropy.
For a derivation of groups of the type KNI, desymmetrizations
of groups of the type KC2nRI, somewhat more frequent in ornamental
art, are also used. Besides the classical-symmetry desymmetrizations, the
antisymmetry desymmetrizations resulting in the conformal antisymmetry
groups of the type KC2nRI/KNI, discussed
in the classical theory of symmetry within the type KNI,
are frequent.
Figure 4.15
The conformal symmetry rosette with the symmetry group M6I.
|
The type MNI consists of the groups derived by the
superposition of the groups M and NI. Hence, corresponding
conformal symmetry rosettes with the group MNI can be constructed
multiplying by the dilative reflection M (with k > 0) a conformal symmetry
rosette with the group NI, belonging to a fundamental region of the
group M (Figure 4.15). A fundamental region of the group MNI is
the section of fundamental regions of the groups M and NI, and
allows a varying of all the boundaries.
After the introduction of the dilative reflection M, the visual
properties of a generating conformal symmetry rosette with the symmetry
group NI, remain unchanged. In the conformal symmetry rosette with
the symmetry group MNI obtained, the presence of the dilative
reflection M increases the visual dynamism, suggesting alternating
centrifugal expansion. Since conformal symmetry rosettes with the symmetry
group MNI belong to a family of dynamic, complicated conformal
symmetry rosettes, the construction and symmetry of which is not
comprehensible by empirical methods, they are very rare in ornamental art.
In aiming to obtain groups of the type MNI, the
desymmetrization method can be applied on groups of the type KD1NI.
Besides the classical-symmetry desymmetrizations, also the antisymmetry
desymmetrizations resulting in antisymmetry groups of the type
KD1NI/MNI, discussed in the classical theory of symmetry within
the type MNI, can also be derived.
Figure 4.16
The conformal symmetry rosette with the symmetry group KD12I.
|
Conformal symmetry rosettes with the symmetry group KD1NI
(Figure 4.16) can be constructed multiplying by the dilatation K (with
k > 0) a conformal symmetry rosette with the symmetry group D1NI,
belonging to a fundamental region of the symmetry group K. A
fundamental region of the group KD1NI is the section of fundamental
regions of the groups K and D1NI, and it allows a varying of
non-reflectional boundaries.
The visual properties of generating conformal symmetry rosettes with
the symmetry group D1NI are maintained in derived conformal symmetry
rosettes with the symmetry group KD1NI. The introduction of the
dilatation K results in the appearance of a new dynamic visual component
- the suggestion of centrifugal expansion. As in all the other cases of
conformal symmetry groups of the category C2 containing a dilatation, for
the construction of conformal symmetry rosettes with the symmetry group
KD1NI, it is very efficient to make the use of two circle inversions with
the concentric inversion circles. Owing to the static visual component
produced by reflections and the non-polarity of rotations, examples of
conformal symmetry rosettes with the symmetry group KD1NI are more
frequent in ornamental art, than conformal symmetry rosettes with the
symmetry group KNI or MNI.
By using the desymmetrization method, besides classical-symmetry
desymmetrizations, the antisymmetry desymmetrizations of groups of the type
KD2nRI, resulting in conformal antisymmetry groups of the type
KD2nRI/KD1NI, discussed in the classical theory of
symmetry within the type KD1NI, can be obtained.
The type KCnZI consists of conformal symmetry groups formed
by the superposition of the groups K and CnZI. Corresponding
conformal symmetry rosettes can be constructed multiplying by the dilatation
K (with k > 0) a conformal symmetry rosette with the symmetry group
CnZI, belonging to the fundamental region of the group K, or by
applying an inversion with the inversion circle concentric to a conformal
symmetry rosette with the symmetry group CnZI. A fundamental region
of the group KCnZI is the section of fundamental regions of the
groups K and CnZI, and allows a varying of all boundaries.
Visual properties of a derived conformal symmetry rosette with the symmetry
group KCnZI are similar to that of the generating conformal symmetry
rosette with the symmetry group CnZI. By introducing a new visual
dynamic component - an impression of centrifugal expansion - the
dilatation K contributes to the increase in the visual dynamism of the
conformal symmetry rosette derived, with respect to the generating conformal
symmetry rosette. Due to their visual dynamism conditioned by the bipolarity
of rotations, enantiomorphism, visual function of the dilatation K, etc.,
examples of conformal symmetry rosettes with the symmetry group
KCnZI, are very rare in ornamental art (Figure 4.17).
By desymmetrizations of groups of the type
KDnRI - the most frequent conformal symmetry groups of
the category C2 in ornamental art - it is possible to derive
groups of the type KCnZI. Besides classical-symmetry
desymmetrizations, the antisymmetry desymmetrizations resulting
in conformal antisymmetry groups of the type
KDnRI/KCnZI, discussed in the classical theory
of symmetry within the type KCnZI, can be obtained.
Figure 4.17
The conformal symmetry rosette with the symmetry group
KC4ZI.
|
The type LCnZI consists of conformal symmetry groups that
are the result of the superposition of the groups L and CnZI.
Visual examples of conformal symmetry groups of the type LCnZI can
be constructed multiplying by the dilative rotation L (with k > 0) a
conformal symmetry rosette with the symmetry group CnZI, belonging
to a fundamental region of the group L (Figure 4.18). The visual
effect of the dilative rotation L is the appearance of a dynamic
spiral-motion component. For a rational angle q of the dilative
rotation L, q = pp/q, (p,q) = 1, p,q Î Z, it is possible to
divide a conformal symmetry rosette with the symmetry group LCnZI
into sectors of the dilatation K((-1)pkq). A fundamental region of the
group LCnZI is the section of fundamental regions of the groups
L and CnZI. Hence, a varying of the shape of all the boundaries of
a fundamental region is allowed. Since the dilative rotation L is a
composite transformation, the relationship L = KS = SK holds, where a rotation
with the rotation angle q is denoted by S. Conformal symmetry
rosettes with the symmetry group KCnZI can be constructed by using
a generating conformal symmetry rosette with the symmetry group
CnZI, but such a construction is, in a certain degree, complicated. The
conformal rosette mentioned, must be first transformed by an inversion with
the inversion circle mI concentric to this rosette. After that, the
image obtained must be transformed by the reflection R with the reflection
line containing the singular point O, and finally, by the rotation S.
Figure 4.18
The conformal symmetry rosette with the symmetry group
LC3ZI.
|
Groups of the type LCnZI belong to a family of visually
dynamic conformal symmetry groups with bipolar rotations, and with the
possibility for the enantiomorphism. The impression of visual dynamism,
suggested by the corresponding conformal symmetry rosettes, is greater than
that suggested by the generating conformal symmetry rosettes with a symmetry
group of the type CnZI. It is the result of the presence of the
dilative rotation L, producing the visual impression of spiral-motion
rotational expansion, and representing by itself a visual interpretation of
a twist within the plane. The desired intensity of a visual dynamic
impression can be achieved by varying the form of a fundamental region,
applying different elementary asymmetric figures within a fundamental
region and choosing the parameters k, q. In ornamental art, the
variety of conformal symmetry rosettes with symmetry groups of the type
LCnZI is restricted by the principle of visual entropy. Therefore, the
most frequent conformal symmetry rosettes with the symmetry group
LCnZI are constructed multiplying by a dilative rotation, the simplest
conformal symmetry rosettes with the symmetry group CnZI (Figure
4.18). For the same reason, more frequent are conformal symmetry rosettes
with symmetry groups of the type LCnZI, with a rational angle of
the dilative rotation L. Very important in ornamental art are conformal
symmetry rosettes with a symmetry group of the subtype
L2nCnZI (L2n = L(k,p/n)). The symmetry group
mentioned is the subgroup of the index 2 of the group
LDnRI. According to the relationship K = L(k,0) = L0, a
consequent application of the criterion of subordination requires
also that the type KCnZI must be considered as the
subtype of the type LCnZI. This would result in the
complete elimination of the type KCnZI. A similar
situation occurs in all the cases of overlapping types or
individual conformal symmetry groups of the category C2. When
solving such a problem, an approach analogous to that already
discussed with the similarity symmetry groups of rosettes
S20, can be used.
By desymmetrizations of groups of the type LDnRI, the
corresponding groups of the subtype L2nCnZI, can be derived.
Adequate antisymmetry desymmetrizations of groups of the type LDnRI
result in conformal antisymmetry groups of the type LDnRI/
L2nCnZI, in the classical theory of symmetry included in the type
LCnZI, as groups of the subtype L2nCnZI.
Conformal symmetry rosettes with the symmetry group KCnRI
can be constructed multiplying by the dilatation K (with k > 0) a
conformal symmetry rosette with the symmetry group CnRI, belonging
to a fundamental region of the group K, or multiplying the same
conformal symmetry rosette by an inversion with the inversion circle
concentric with it (Figure 4.19). A fundamental region of the group
KCnRI is the section of fundamental regions of the groups K and
CnRI, and allows a varying of boundaries that do not belong to the
inversion circles, i.e. a varying of radial boundaries. The visual effect of
the conformal symmetry rosettes derived is very similar to that produced by
the generating conformal symmetry rosette with the symmetry group
CnRI. The introduction of the dilatation K representing the new
dynamic visual component - the suggestion of centrifugal
expansion - results in an increase in the visual dynamism.
Owing to their dynamic visual qualities, we would expect that
conformal symmetry rosettes with symmetry groups of the type
KCnRI are not so frequent in ornamental art. However, the
possibility of deriving conformal symmetry groups of the type
KCnRI by desymmetrizations of groups of the type
KDnRI, the most
frequently used conformal symmetry groups of the category C2 in
ornamental art, caused their more frequent occurrence. Besides
classical-symmetry desymmetrizations, the antisymmetry desymmetrizations,
resulting in the conformal antisymmetry groups of the type
KDnRI/KCnRI, discussed in the classical theory of symmetry within
the type KCnRI, can be obtained.
Figure 4.19
The conformal symmetry rosette with the symmetry group
KC4RI.
|
The type MCnRI consists of conformal symmetry groups derived
by extending by the dilative reflection M (with k > 0) conformal symmetry
groups of the type CnRI. Corresponding conformal symmetry rosettes
can be constructed multiplying by the dilative reflection M a conformal
symmetry rosette with the symmetry group CnRI, belonging to a
fundamental region of the group M. The same conformal symmetry
rosettes can be constructed transforming by an inversion with the inversion
circle mI concentric to it, a generating conformal symmetry rosette
with the symmetry group CnRI. Afterward, that image obtained we
must to copy by a reflection in the reflection line containing the singular
point O (Figure 4.20). The extension of the symmetry group CnRI by
the dilative reflection M will result, in the visual sense, in the
appearance of a new dynamic visual component - centrifugal alternating
expansion. The dominance of dynamic components caused the relatively rare
occurrence of conformal symmetry groups of the type MCnRI in
ornamental art.
Figure 4.20
The conformal symmetry rosette with the symmetry group MC8RI.
|
By desymmetrizations of groups of the type KDnRI, conformal
symmetry groups of the type MCnRI can be derived. In particular,
antisymmetry desymmetrizations, resulting in antisymmetry groups of the type
KDnRI/MCnRI, discussed by the classical theory of symmetry
within the type MCnRI, can be obtained.
The group KDnRI can be derived extending by the dilatation
K the conformal symmetry group DnRI. Corresponding conformal
symmetry rosettes can be constructed multiplying by the dilatation K a
conformal symmetry rosette with the symmetry group DnRI, belonging
to a fundamental region of the group K (with k > 0), or multiplying
the same conformal symmetry rosette by an inversion with the inversion
circle mI concentric to it (Figure 4.21). A fundamental region of
the group KDnRI is the section of fundamental regions of the groups
K and DnRI. Since the group KDnRI is generated by
reflections (reflections and inversions), its fundamental region is fixed.
Therefore, a fundamental region of the group KDnRI is defined by two
successive reflection lines and two successive inversion circles,
corresponding to this conformal symmetry group. The varying of conformal
symmetry rosettes with the symmetry group KDnRI is reduced to the
use of different elementary asymmetric figures belonging to a fundamental
region and to a change in the value of the parameter k.
Figure 4.21
The conformal symmetry rosette with the symmetry group
KD6RI.
|
The effect of the dilatation K on a generating conformal symmetry
rosette with the symmetry group DnRI is reduced, in the visual
sense, to the increase in the visual dynamism and the suggestion of
centrifugal expansion. Since there are a large number of models in nature
with the symmetry group of rosettes Dn, with a high degree of
constructional and visual simplicity and symmetry, and with the dominance of
the static visual impression, conformal symmetry groups of the type
KDnRI are the most frequent discrete conformal symmetry groups of the
category C2, in ornamental art. Besides their individual use, groups of
the type KDnRI form the basis for applying the desymmetrization
method, aiming to derive the other types of conformal symmetry groups of
the category C21.
Figure 4.22
The conformal symmetry rosette with the symmetry group
L12C6RI.
|
The group LCnRI can be derived extending by the
"centering" dilative rotation L = L2n = L(k,p/n) (with k > 0) the
conformal symmetry group CnRI. Hence, conformal symmetry rosettes
with the symmetry group LCnRI can be constructed multiplying by the
dilative rotation mentioned, a generating conformal symmetry rosette with
the symmetry group CnRI, belonging to a fundamental region of the
group L (Figure 4.22). The same conformal symmetry rosettes can be
constructed by using an inversion with the inversion circle concentric to
the generating rosette. In that case, after transforming it by the
inversion, the image obtained must be rotated through the angle
q = p/n. A fundamental region of the group LCnRI is the section of
fundamental regions of the groups L2n and
CnRI, and allows a varying of the form of non-inversional
boundaries, while the remaining boundaries are defined by the
concentric inversion circles (their corresponding arcs).
The influence of the dilative rotation L = L2n on a generating
conformal symmetry rosette with the symmetry group CnRI results in
the formation of the visual impression of a spiral motion. All the other
visual properties of the generating conformal symmetry rosette remain
unchanged. Because of the rational dilative rotation angle
q = p/n, there are sectors of the dilatation K(kn).
In ornamental art, apart from by those construction methods,
groups of the type LCnRI can be obtained by desymmetrizations of
groups of the type LDnRI. Since the group LCnRI is the
subgroup of the index 2 of the group LDnRI, besides
classical-symmetry desymmetrizations, very frequent are antisymmetry
desymmetrizations, resulting in antisymmetry groups of the type
LDnRI/LCnRI, discussed in the classical theory of symmetry within
the type LCnRI.
Figure 4.23
The conformal symmetry rosette with the symmetry group
LD4RI.
|
The group LDnRI can be derived extending the group
DnRI by the "centering" dilative rotation L = L2n = L(k,p/n) (with
k > 0). In ornamental art, conformal symmetry rosettes with the symmetry
group LDnRI are very frequent, since they can be derived
multiplying by the dilative rotation L = L2n a conformal symmetry rosette
with a symmetry group of the type DnRI, the most frequent conformal
symmetry group of the category C2, which belongs to a fundamental region
of the group L (Figure 4.23). The same conformal symmetry rosettes can
be constructed transforming by a circle inversion with the concentric
inversion circle mI, the generating rosette mentioned. Afterward,
the image obtained must be rotated through the angle q = p/n. A
fundamental region of the group LDnRI is the section of fundamental
regions of the groups DnRI and L. Hence, a varying of the form
of a fundamental region is restricted to a change in the shape of boundaries
that do not belong to the reflection lines or inversion circles.
The dilative rotation L produces, in the visual sense, a dynamic
effect and gives the impression of a spiral motion. Although, since the
"centered dihedral" similarity symmetry group LDn is the subgroup of
the index 2 of the group LDnRI, there exists a specific balance
between static and dynamic visual components in conformal symmetry rosettes
with the symmetry group LDnRI, and even a dominance of the static
ones. Because of the rational dilative rotation angle q = p/n ,
there are sectors of the dilatation K(kn).
In ornamental art, conformal symmetry rosettes with the symmetry
group LDnRI are very frequently used as individual ones, or as a
basis for applications of the desymmetrization method. Various examples are
obtained by applying a different elementary asymmetric figure within a
fundamental region or by varying the form of a fundamental region and the
value of the parameter k.
The complete survey of continuous conformal symmetry groups of the
categories C21 and C2 can be derived directly from the data on the
continuous symmetry groups of tablets G320 and non-polar rods G31,
respectively (A.V. Shubnikov, V.A. Koptsik, 1974). According to the
restrictions imposed by ornamental art, if textures are not applied,
visually presentable are continuous conformal symmetry groups of the
category C21 of the type D¥RI, and continuous conformal
symmetry groups of the category C2 of the types KD¥RI,
K1CnRI, K1DnRI, L1D
¥RI and L1CnZI, where a continuous dilatation
group and continuous dilative rotation group is denoted by
K1, L1, respectively. In terms of ornamental art,
the most interesting are continuous conformal symmetry rosettes
with the symmetry group L1CnZI, which can be
constructed multiplying by the n-fold rotation a logarithmic
spiral - the invariant line of the continuous conformal
symmetry group L1ZI. All the other visually
non-presentable continuous conformal symmetry groups can be
visually interpreted by using textures. Regarding the physical
interpretations, all the continuous conformal symmetry groups of
the categories C21 and C2 can be modeled in the plane
E2\{O} , by means of physical desymmetrization
factors (e.g., by the uniform rotation around the singular point
O, by adequate physical fields, etc.), as was done with the
continuous symmetry groups of tablets G320 and rods
G31, isomorphic to them (A.V. Shubnikov, V.A. Koptsik,
1974).
*
*
*
As with all the previously discussed symmetry groups occurring in
ornamental art, a significant prerequisite for their early appearance and
frequent use in ornamental art is that they satisfy the principle of visual
entropy - maximal constructional and visual simplicity and maximal
symmetry. For many ornamental art motifs, their origin and use is not
directly a function of the existence of models in nature with the
corresponding symmetry. This especially refers to conformal symmetry
rosettes. Hence, probably the most significant of the three mentioned
criteria conditioning the time of origin and frequency of occurrence of
different conformal symmetry groups in ornamental art, is the principle of
maximal constructional simplicity.
An inversion is a constituent part of all the conformal symmetry
transformations, as an independent symmetry transformation, or as a
component of the composite transformations - inversional reflection ZI
or inversional rotation SI, the commutative compositions of an inversion
with a reflection or with n-fold rotation. All the other conformal
symmetry transformations of the plane E2\{O} belong to
isometries or similarity symmetry transformations. Therefore, all the
construction problems in conformal symmetry rosettes with a symmetry group
of the category C21 or C2, can be solved, in principle, by using the
non-metric construction to obtain homologous points of the inversion RI.
Since a non-metric construction fully satisfies the criterion of maximal
constructional simplicity, for the conformal symmetry transformations RI,
ZI, SI, there is no reason to use the metric construction method.
The property of equiangularity is satisfied by every inversion and
by all the other isometries and similarity symmetry transformations
consisting of conformal symmetry groups. Hence, this property is an
invariant of all the conformal symmetry groups. When constructing conformal
symmetry rosettes with an elementary asymmetric figure of an arbitrary
form, belonging to a fundamental region, as with the similarity symmetry
groups of rosettes S2, a construction of the type "point by point" is
unavoidable. Since such a construction is very complicated, the invariance
of the points of the inversion circle mI and the fact that circles
and lines are homologous figures of an inversion, expressed by the
relationships: RI(A) = A iff A Î mI,
RI(l) = l iff
O Î l, RI(l) = c iff O not Î l and O Î c,
RI(c) = c1
iff O not Î c and O not Î c1, RI(c) = c
iff c^mI are a basis upon which we can simplify constructions of
all conformal symmetry rosettes.
For conformal symmetry groups of the category C21, this is
sufficient for the construction of their visual interpretations. Besides the
fact that they can be constructed multiplying by similarity transformations
K, L, M a generating conformal symmetry rosette with a symmetry group
of the category C21, for a construction of the conformal symmetry
groups of the category C2 it is possible to use an inversion with the
inversion circle concentric to the generating rosette mentioned. Due to the
simplicity of constructions by circles and lines, in many cases this is the
most suitable construction method. Whatever the approach is, the
construction of visual interpretations of conformal symmetry rosettes with a
symmetry group of the category C2 is reduced to a multiplication of a
conformal symmetry rosette with the conformal symmetry group of the category
C21. Since conformal symmetry groups of the category
C21 are the extensions of the symmetry groups of rosettes
Cn (n), Dn (nm), every
construction of conformal symmetry rosettes can be reduced to the
following procedure: the transformation of a generating rosette
with the symmetry group Cn (n) or Dn
(nm) by two circle inversions with the concentric inversion
circles, by rotations with the singular point O and by
reflections with the reflection line containing the point O.
For constructions of conformal symmetry rosettes with the desired
symmetry, the desymmetrization method is also used. This indirect
construction method is mainly applied to the conformal symmetry rosettes of
the types DnRI, KDnRI, LDnRI. Such conformal
symmetry rosettes, possessing a high degree of symmetry and representing the
most frequent conformal symmetry groups in ornamental art, are a suitable
medium for constructions of other conformal symmetry rosettes of a lower
degree of symmetry.
Using the desymmetrization method, besides classical-symmetry
desymmetrizations, antisymmetry desymmetrizations can be used in all the
cases when the desired symmetry group is the subgroup of the index 2 of a
certain larger group. With conformal symmetry groups of the category
C21, a complete survey of them is given in the table of the
antisymmetry desymmetrizations, i.e. of the corresponding conformal
antisymmetry groups of the category C21'. In this table, symbols of
antisymmetry groups are given in the group/subgroup notation G/H.
The table of antisymmetry desymmetrizations of conformal symmetry groups of
category C21:
NI/Cn | CnRI/Cn | DnRI/Dn
|
| C2nRI/CnRI | D2nRI/DnRI
|
D1NI/Dn | C2nRI/CnZI | DnRI/CnRI
|
D1NI/NI | | D2nRI/D1NI
|
D1NI/CnZI | CnZI/Cn | DnRI/CnZI
|
| C2nZI/CnZI
|
|
Besides being the basis for applications of the antisymmetry
desymmetrization method, this table is an indicator of all the subgroups of
the index 2 of conformal symmetry groups of the category C21.
The complete derivation and catalogue of conformal antisymmetry
groups of the categories C21' and C2' is given by S.V. Jablan
(1985).
Information on some possible color-symmetry desymmetrizations of
crystallographic conformal symmetry groups of the categories C21 and
C2, can be obtained from the work of
A.M. Zamorzaev, E.I. Galyarski,
A.F. Palistrant (1978), A.F. Palistrant (1980c),
and E.I. Galyarski (1986),
who discuss the color-symmetry groups of tablets G320 and non-polar
rods G31.
With conformal symmetry groups of the category C21, it is
possible to establish a connection between these and the corresponding
symmetry groups of friezes G21. The following relationships hold:
CnRI @ m1, DnRI @ mm, CnZI
@ 12, D1NI @ mg, NI @
1g. In this way, the problem of color-symmetry groups derived from
conformal symmetry groups of the category C21 can be reduced to the
color-symmetry groups of friezes (J.D. Jarratt, R.L.E. Schwarzenberger,
1981), i.e. to the use of the table of color-symmetry desymmetrizations of
the corresponding symmetry groupsof friezes. In doing so, it is necessary
to be aware on the identification pxn = E.
Conformal symmetry tilings of the plane E2\{O} , are
discussed by E.A. Zamorzaeva (1985). In this work, a connection is
established between the different types of conformal symmetry groups of the
category C2, the symmetry groups of non-polar rods G31 and the
symmetry groups of ornaments G2. The following relationships hold :
KCnZI, LCnZI @ p2, KNI @ pg,
KCnRI @ pm, LCnRI @ cm,
MNI @ pgg, KD1NI, MCnRI @ pmg,
LDnRI @ cmm, KDnRI @ pmm. Using
such an approach, the problem of isogonal tilings, which correspond to
conformal symmetry groups of the category C2, is solved.
The discussion on the visual properties of conformal symmetry groups
of the category C21, can be reduced to an analysis of the effects of
the conformal transformations RI, ZI, SI on generating rosettes
with the symmetry groups Cn (n), Dn (nm).
In groups of the type CnRI, the inversion RI causes the
absence of the enantiomorphism, existing in the symmetry group Cn
(n). The intensity of the static visual impression produced by an
inversion depends on the position and form of an elementary asymmetric
figure belonging to a fundamental region of the conformal symmetry group
containing this inversion. It comes to its full expression only for figures
that are, by their shape, close to the inversion circle. In the
geometric sense, the inversion RI causes the constancy of the
shape of the boundary of a fundamental region, which coincides
with the inversion circle mI (its arc), and the
non-polarity of radial rays.
The inversional rotation SI mainly keeps the properties of
generating rosettes with symmetry groups of the category G20 and
somewhat intensifies their dynamic visual properties. The inversional
reflection ZI causes the bipolarity of rotations and of radial rays, and
preserves the property of the enantiomorphism. The dynamic or static visual
properties of conformal symmetry rosettes with symmetry groups of the
category C21 will depend on the analogous properties of generating
rosettes with symmetry groups of the category G20.
Conformal symmetry groups of the category C2 are derived
extending by the similarity transformations K, L, M, conformal
symmetry groups of the category C21. The dilatation K and dilative
rotation L maintain all the geometric-visual properties of the generating
conformal symmetry groups of the category C21 and introduce a new
dynamic visual component - a suggestion of centrifugal expansion, or of
rotational centrifugal expansion. The dilative reflection M, in the visual
sense, produces the impression of centrifugal alternating expansion. In the
geometric sense, it eliminates the possibility for the enantiomorphism.
The form of a fundamental region of conformal symmetry groups is
defined by the invariance of all the points of inversion circles and
reflection lines. In this way, the conformal symmetry groups of the types
NI, CnZI, KNI, KCnZI, LCnZI,
MNI, offer the possibility to change the shape of all the boundaries of a
fundamental region; groups of the types CnRI, MCnRI,
LCnRI offer the possibility to change the shape of non-inversional
boundaries; groups of the types D1NI, KD1NI offer the
possibility to change the shape of non-reflectional boundaries; groups of
the type LDnRI type offer the possibility to change the shape of
non-reflectional and non-inversional boundaries, while groups of the types
DnRI, KDnRI, generated by reflections and inversions, do not
offer the possibility to change the shape of boundaries of a fundamental
region.
In conformal symmetry groups that do not require the constancy of
the form of a fundamental region, a variety of corresponding conformal
symmetry rosettes in ornamental art is achieved by varying the boundaries
of a fundamental region or the form of an elementary asymmetric figure
belonging to a fundamental region. In the remaining conformal rosettes the
variety is achieved exclusively by the second of these possibilities.
In the geometric-visual sense, the inversion RI represents an
adequate interpretation of "two-sideness" in the "one-sided" plane, i.e. the
interpretation of the symmetry transformation of the space E3
- the plane reflection in the invariant plane of the symmetry
groups of tablets G320, in the plane E2\{O}.
In the same way, because of the isomorphism between the symmetry
groups of tablets G320 and conformal symmetry groups of the
category C21, and the isomorphism between the symmetry
groups of non-polar rods G31 and conformal symmetry groups
of the category C2, apart from the schematic visual
interpretations - Cayley diagrams and tables of the graphic
symbols of symmetry elements - conformal symmetry rosettes
represent a completely adequate visual model of the symmetry
groups of tablets G320 and non-polar rods G31. The
symmetry groups of polar rods
G31 possess a similar visual
interpretation in the plane E2 - similarity symmetry rosettes.
On the basis of those isomorphisms, the presentations, the
geometric and visual properties of conformal symmetry groups of
the categories C21, C2 can be fully transferred,
respectively, to the symmetry groups of tablets G320 and
non-polar rods G31.
In the table of the group-subgroup relations (Figure 4.24), a survey
is given of all the group-subgroup relations between the
visually-presentable continuous conformal symmetry groups, the discrete
conformal symmetry groups of the categories C21, C2 and
group-subgroup relations between conformal symmetry groups of the category
C2 and the similarity symmetry groups of the category S20. Although
incomplete, as they do not include all the group-subgroup relations but only
the most important ones, the tables can serve as a basis on which to apply
the desymmetrization method for obtaining conformal symmetry groups or
similarity symmetry groups and also for the geometric-visual evidence of
symmetry substructures of conformal symmetry groups. Aiming for a more
complete consideration of those problems, the given tables can be used with
the analogous tables corresponding to similarity symmetry groups of the
category S20.
Figure 4.24
The time and frequency of occurrence of different conformal symmetry
groups in ornamental art are related to the periods when various
constructional problems were solved. According to the criterion of maximal
constructional and visual simplicity, constructions of conformal symmetry
rosettes are mostly based on the use of circles and lines as homologous
elements of conformal symmetry transformations. Combinations of elementary
geometric figures (regular polygons, circles) with a common singular point,
found in the earliest periods of ornamental art, gave as a result the first
examples of conformal symmetry rosettes with symmetry groups of the category
C21, mostly of the type DnRI
(n =1,2,3,4,6,8,...). In the
further development of ornamental art, examples of all other conformal
symmetry groups of the category C21 appeared. The dominance of visually
static conformal symmetry rosettes with a higher degree of symmetry, is
expressed throughout the history of ornamental art.
Very important in the formation of conformal symmetry rosettes was
the existence of certain models in nature - the flowers of different
plants, forms of growth, etc., possessing or suggesting different kinds of
conformal symmetry.
Conformal symmetry rosettes with a symmetry group of the category
C2 are constructed multiplying by similarity transformations K, L,
M, a generating conformal symmetry rosette with the symmetry group of the
category C21, or multiplying a generating rosette with the same
symmetry group, by an inversion with the inversion circle concentric to it.
The second construction, based on the non-metric construction method,
using invariance of all the points of inversion circles and reflection
lines, and circles and lines as homologous figures of conformal symmetry
transformations, offers better possibilities, in the sense of maximal
constructional simplicity. It came to its fullest expression in the
corresponding elementary geometric constructions by means of circles and
lines used in ornamental art. In ornamental art, conformal symmetry
rosettes came to their peak in the work of Romanesque and Gothic
architects, artisans and artists. Examples of almost all the conformal
symmetry groups date from these periods. When calculating a building
proportions and other architectural elements, especially when drawing-up the
plans of the decorative architectural elements - window and floor rosettes
- Medieval architects used those constructions.
Directly linked to these problems, and covered by the theory of
similarity symmetry and conformal symmetry, are the questions of the theory
of proportions, the roots of which date from Greek geometry. It held a
special place in Medieval and Renaissance architectural planning and it
reached its fullest expression in applications of the "aurea sectio"
(or the "golden section") and musical harmonies used in architecture and in
the visual arts.
In more recent periods, examples of conformal
symmetry rosettes with symmetry groups of the category C2 can
be found in the work of M.C. Escher (1971a, b; 1986),
who, besides classical-symmetry, often used conformal
antisymmetry and color-symmetry rosettes, and greatly contributed
to the analysis of different conformal color-symmetry groups and
conformal tilings.
The problems of visual perception, referring here to conformal
symmetry rosettes, can be solved analogously to the same problems previously
discussed in the other categories of symmetry groups, through the analysis
of the symmetrization and desymmetrization factors caused by the visual
effects of the physiological-psychological elements of visual perception.
The approach to ornamental art from the theory of symmetry, makes possible
the recognition, classification and the exact analysis of all the various
kinds of conformal symmetry rosettes occurring in ornamental art, and also
highlights the different possibilities for constructing these conformal
symmetry rosettes possessing the symmetry and geometric-visual properties
already anticipated.