Math
123H - Symmetry
Questions on Readings (Hargittai &
Hargittai)
Q1: What is the difference between geometric symmetry and symmetry in
nature or the real world?
Geometric symmetry can be
thought of in our minds as perfectly precise and exact (though it is
often realized through our somewhat imperfect drawings of
examples). Symmetry in nature or the real world is often only
approximate and we must fill in or fix the missing or imperfect detail
in order to create complete symmetry.
Q2: How does the material we have already studied relate to the point
group and space group symmetries (p. xvi, xvii) and to symmetry
operations and symmetry elements (p. 2, 39)? More specifically:
- What terms have we used for the "special points" mentioned on
page xvi?
The description given says that
a special point is one that remains unchanged under symmetry
operations, so this is similar to what we have been calling a fixed
point. For the rotation in particular, it is the same as what we
called a rotocenter.
- What terms or ideas that we have studied are used in space group
symmetry?
Space group symmetries must
involve translation and can also involve reflections, glide
reflections, and rotations.
- What term(s) have we used for what Hargittai and Hargittai call
symmetry elements?
The symmetry operations
they describe are the rigid motions we have studied. The symmetry
elements are the tools used to perform those symmetries or rigid
motions.
Q3: Why do they refer to a mirror plane rather than a mirror
line? Hint: where do the objects that Hargittai and Hargittai
consider naturally live? Where do the objects that we have
reflected so far live?
The objects considered in the
book by Hargittai & Hargittai are primarily three-dimensional, so
to reflect them they use a two-dimensional plane. The objects we
have considered previously are primarily two-dimensional, so to reflect
them we used a one-dimensional line.
Q4: Why do they refer to a rotation axis rather than a rotocenter on
page 39? Same type of hint as for Q3.
The objects considered in the
book by Hargittai & Hargittai are primarily three-dimensional, so
to rotate them they use a one-dimensional line (think of the axis for
the wheels on a car or the Earth's axis of rotation). The objects
we have
considered previously are primarily two-dimensional, so to rotate them
we used a zero-dimensional point, the rotocenter.
Q5: Explain the reason behind the "Fact to Consider" on page
68.
Do you agree with their statement that the "only case where reflection
is not accompanied by rotation is when there is bilateral symmetry?
It is true that bilateral
symmetry involves one reflectional symmetry and only one other
symmetry, the identity, so figures with bilateral symmetry do not
appear to have any rotational symmetry. However, bilateral
symmetry is the same as symmetry type D_1. When discussing
dihedral symmetry type D_n, it is most natural to include the identity
symmetry as a rotation so that the figure can be considered to have n
reflection symmetries and n rotation symmetries (as opposed to n
reflection symmetries and n-1 rotation symmetries). Thus it is
reasonable to consider the identity to be a rotational symmetry, in
which case one might dispute or at least want to clarify the statement
on page 68.
Q6: Is the comment on page 45 about jellyfish consistent with the
discussion of symmetry in animals in Bunch, Chapter 1? Explain.
The comment that the 4-fold
rotational symmetry of the jellyfish may be due to a circling motion in
capturing food is consistent with Bunch's point that symmetry often
occurs in the absence of any differentiating or distinguishing
force. Since the jellyfish is not moving in a straight line
direction, but rather in a circle, it is reasonable for the jellyfish
to not have a front and a back. This does not explain however why
there is 4-fold rotational symmetry as opposed to some other type C_n
symmetry.
Questions on Rosen
Q1 (Foreword, Preface, and Chapter 1): How many symmetries does
he view a square as having? What are the additional symmetries
and why do they arise?
Rosen identifies 12 symmetries
of the square. He finds more than the eight we have already
studied because he is considering the square to be sitting in a
3-dimensional space.
In addition to the rotations by
0, 90, 180, and 270 degrees about an axis through the center
perpendicular to the plane of the square, and reflection in planes
perpendicular to the plane of the square and passing through the axes
formed by diagonals and lines through midpoints of opposite sides, he
also find rotations by 180 degrees about these same lines. When
viewing the square as simply a 2-dimensional object, the effects of
these additional 4 rotations and the 4 reflections are the same.
Q2 (Chapter 1): Rosen takes a much broader view of what
constitutes a symmetry transformation than we have so far. Name 3
types of symmetry transformations that he mentions but we have not
considered.
Q3 (Chapter 2): Suppose the depressions labelled A, B, and C are
arranged in an equilateral triangle with A at the top vertex, B at the
bottom left vertex and C at the bottom right vertex. Give the
symmetries described on page 10 in terms of Farmer's standard notation
(using r and m). (It may help to draw out the triangle diagrams
and show the effect of the maps Rosen describes on the diagram.
Remember that standard notation means the m is written on the left, but
as always, the motion on the right is applied first.)
Q4 (Chapter 2): Write an equation, using the symbols a and b to
stand for two general symmetry transformations, that shows the property
Rosen describes in the last three paragraphs of Chapter 2 (page 16-17)
before the group theory section. (Let a stand for covering the
pot and b stand for filling the pot. Notice that Rosen is
discussing how to find the inverse of a combined transformation.
Write an equation for this using the symbols a and b. It may help
to think of this as translating the sentences on the bottom of page 16
and top of page 17 into symbols, or as translating part of Figure 2.13
into symbols.)
(ab)^{-1}=b^{-1}a^{-1}
The crucial observation is that
the inverse is NOT a^{-1}b^{-1} unless a and b commute, i.e., satisfy
ab=ba.
Q5: Write one or more questions you have after reading Chapters 1
and 2.