Lecture Notes: Symmetries & Symmetry Groups

For more information about symmetry, see chapter 11 of your text.  In particular, see section 11.7.

The symmetry of an object or shape is a motion that moves the object back onto itself.  In other words the object looks the same after applying the motion as it did before. 

 

Examples:

 
1. Symmetries of a Square:  As discussed in class, the symmetries of the square are rotations by 90°, 180°, 270° and 360°, as well reflections about the horizontal (l4), the vertical (l3), and the two diagonal axis (l1 and l2).

°

l1

l2

l3

l4

R90

R180

R270

e = R360

l1

   R360    

   R180    

   R90    

   R270    

   l3 

  l2 

   l4    

l1

l2

   R180    

   R360    

   R270    

   R90    

   l4    

  l1

   l3 

l2

l3

   R270    

   R90    

   R360    

   R180    

  l2 

   l4    

   l1 

l3 

l4

   R90    

   R270    

   R180   

   R360    

 l1

   l3 

  l2

  l4  

R90

 l3   

     l4    

l1

  l2

   R180    

   R270    

   R360    

   R90  

R180

l2 

  l1

   l4    

   l3  

   R270    

   R360    

   R90    

   R180    

R270

 l3  

   l4    

  l2

  l1

   R360    

   R90    

   R180    

   R270    

e = R360

l1

  l2

l3  

   l4    

   R90    

    R180  

   R270    

   R360    

            Filling in the above table shows that, the set of symmetries of the square along with the operation composition, , forms a group known as the Dihedral group D4.  The square is said to have D4 symmetry type.   Note:  The element in the R90 row and the l3 column corresponds to l3 ° R90 , i.e. perform a rotation counter-clockwise 90 degrees and then flip around the l3 axis and you'll get the same thing as if you flip around the l1 axis.  

2. Symmetries of an equilateral triangle:  The symmetries of an equilateral triangle are rotations by 120°, 240°, and 360°, as well as reflections about the three symmetry axes, l1, l2, and l3.

 

3. Symmetries of a propeller:  The symmetries of a propeller are rotations by 90°, 180°, 270°, and 360°.  The set of symmetries of a propeller with the composition operation form an Albelian group, as shown in the following table.  Clearly, rotations or 360° act as the identity element under composition.  All rotations have an inverse under composition.  Example, the composition of a 270° rotation and a 90° rotation is the same as a 360° rotation, or no rotation at all.  The group formed by the symmetries of a propeller and the composition operation is known as Z4.  The propeller is said to have Z4 symmetry.

°

R90

R180

R270

e = R360

R90

R180

R270

e

R90

R180

R270

e

R90

R180

R270

e

R90

R180

R270

e = R360

R90

R180

R270

R360

 

4. Z2 symmetry:  We’ve already seen examples of shapes with D4 and Z2 symmetry.  There are also shapes with what is known as Z2 symmetry.  These are shapes whose symmetry is just the set of two elements, Rotations of 180° and rotations of 360°.  The face cards of most decks have Z2 symmetry, as do the letters Z, and S.  The set {R360, R180} along with composition forms an Albelian group known as Z2.   The following shapes all have Z2 symmetry.

°

R180

e = R360

R180

e

R180

e = R360

R180

R360

          

 

5.  D1 symmetry:  The set {R360, l1}, i.e. rotation of 360° and reflection about one axis, also form an albelian group with composition.  This group is called D1.   Examples of D1 symmetry are shown below.  

°

l1

e = R360

l1

e

l1

e = R360

l1

e

      

 

6. Z1 symmetry:  The R360 forms a rather trivial one element group known as Z1.  Elements whose only symmetry is rotation by 360° are said to have Z1 symmetry.   Examples of Z1 symmetry are shown below.

°

e = R360

e = R360

e