x,y, and zcoordinates, so there are a total of 3N(Nnumber of atoms) to-
tal coordinates for the molecule. Furthermore, one needs to keep track of the
original positive directions of the x,y, and zaxes, as shown in Figure 13.17.
Instead of the 3 3 matrices defined above, we therefore have to construct a
9 9 matrix to describe the complete spatial effect of each symmetry opera-
tion, shown visually in Figure 13.18:E(H 2 O)
xH1
yH1
zH1
xO
yO
zO
xH2
yH2
zH2xH1
yH1
zH1
xO
yO
zO
xH2
yH2
zH20 0 0 0 0 0 0 0 1
0 0 0 0 0 0 0 1 0
0 0 0 0 0 0 1 0 0
0 0 0 0 0 1 0 0 0
0 0 0 0 1 0 0 0 0
0 0 0 1 0 0 0 0 0
0 0 1 0 0 0 0 0 0
0 1 0 0 0 0 0 0 0
1 0 0 0 0 0 0 0 0
13.5 Character Tables 431yO
xOzOOyH
xHzH1H yH
xHzH2HyO
xOzOOyH
xHzH1H yH
xHzH2HEyO
xOzOOyH
xHzH1H yH
xHzH2HyOzO xOC 2yO
xOzOOyH
xHzH1H yH
xHzH2HyOzO xOOyH1xH1zH1H yH2xH2zH2H(yz)yO
xOzOOyH
xHzH1H yH
xHzH2HyO
xOzOOyH2
xH2zH2H yH1
xH1zH1H(xz)yH2zH2xH2yH1zH1xH1OHHFigure 13.18 The effect of the four symmetry
operations ofC2von the degrees of freedom of
the H 2 O molecule.Edoes nothing.C 2 and (xz)
exchange the two hydrogens and reverse the di-
rections of some of the coordinate unit vectors.
(yz) does not move any atoms but reverses some
coordinate vectors. You should be able to recon-
cile the above diagrams with the matrices in equa-
tion 13.2.