Chapter
3 An introduction to molecular symmetry
TOPICS
& Symmetry operators and symmetry elements & Point groups & An introduction to character tables & Infrared spectroscopy & Chiral molecules
the resulting structure is indistinguishable from the first; 3.1 Introduction another 1208 rotation results in a third indistinguishable molecular orientation (Figure 3.1). This is not true if we Within chemistry, symmetry is important both at a molecu- carry out the same rotational operations on BF2H. lar level and within crystalline systems, and an understand- Group theory is the mathematical treatment of symmetry. ing of symmetry is essential in discussions of molecular In this chapter, we introduce the fundamental language of spectroscopy and calculations of molecular properties. A dis- group theory (symmetry operator, symmetry element, point cussion of crystal symmetry is not appropriate in this book, group and character table). The chapter does not set out to and we introduce only molecular symmetry. For qualitative give a comprehensive survey of molecular symmetry, but purposes, it is sufficient to refer to the shape of a molecule rather to introduce some common terminology and its using terms such as tetrahedral, octahedral or square meaning. We include in this chapter an introduction to the planar. However, the common use of these descriptors is vibrational spectra of simple inorganic molecules, with an not always precise, e.g. consider the structures of BF3, 3.1, emphasis on using this technique to distinguish between pos- and BF2H, 3.2, both of which are planar. A molecule of sible structures for XY2,XY3 and XY4 molecules. Complete BF3 is correctly described as being trigonal planar, since its normal coordinate analysis of such species is beyond the symmetry properties are fully consistent with this descrip- remit of this book. tion; all the F B F bond angles are 1208 and the B F bond distances are all identical (131 pm). It is correct to say that the boron centre in BF2H, 3.2,isinapseudo-trigonal planar environment but the molecular symmetry properties 3.2 Symmetry operations and symmetry are not the same as those of BF3. The F B F bond angle elements in BF2H is smaller than the two H B F angles, and the B H bond is shorter (119 pm) than the B F bonds In Figure 3.1, we applied 1208 rotations to BF and saw that (131 pm). 3 each rotation generated a representation of the molecule that F H was indistinguishable from the first. Each rotation is an example of a symmetry operation. 120˚ 120˚ 121˚ 121˚ B B A symmetry operation is an operation performed on an FF FF 120˚ 118˚ object which leaves it in a configuration that is (3.1) (3.2) indistinguishable from, and superimposable on, the original configuration. The descriptor symmetrical implies that a species possesses a number of indistinguishable configurations. When struc- The rotations described in Figure 3.1 were performed ture 3.1 is rotated in the plane of the paper through 1208, about an axis perpendicular to the plane of the paper and 80 Chapter 3 . An introduction to molecular symmetry
F 120˚ rotationF 120˚ rotation F
B B B FF F F F F
Fig. 3.1 Rotation of the trigonal planar BF3 molecule through 1208 generates a representation of the structure that is indistinguishable from the first; one F atom is marked in red simply as a label. A second 1208 rotation gives another indistinguishable structural representation.
passing through the boron atom; the axis is an example of a example, in square planar XeF4, the principal axis is a C4 symmetry element. axis but this also coincides with a C2 axis (see Figure 3.4). Where a molecule contains more than one type of Cn axis, A symmetry operation is carried out with respect to points, they are distinguished by using prime marks, e.g. C2, C2’ and lines or planes, the latter being the symmetry elements. C2’’. We return to this in the discussion of XeF4 (see Figure 3.4). Rotation about an n-fold axis of symmetry The symmetry operation of rotation about an n-fold axis Self-study exercises (the symmetry element) is denoted by the symbol C ,in n 1. Each of the following contains a 6-membered ring: benzene, 3608 which the angle of rotation is ; n is an integer, e.g. 2, 3 borazine (see Figure 12.19), pyridine and S6 (see Box 1.1). n Explain why only benzene contains a 6-fold principal rotation or 4. Applying this notation to the BF3 molecule in Figure axis. 3.1 gives a value of n ¼ 3 (equation 3.1), and therefore we 2. Among the following, why does only XeF4 contain a 4-fold say that the BF molecule contains a C rotation axis;in 3 3 principal rotation axis: CF ,SF, [BF ] and XeF ? this case, the axis lies perpendicular to the plane containing 4 4 4 4 C the molecule. 3. Draw the structure of [XeF5] . On the diagram, mark the 5 axis. The molecule contains five C axes. Where are these 3608 2 Angle of rotation ¼ 1208 ¼ ð3:1Þ axes? [Ans. for structure, see worked example 1.14] n 4. Look at the structure of B H in Figure 12.23b. Where is the In addition, BF also contains three 2-fold (C ) rotation 5 9 3 2 C axis in this molecule? axes, each coincident with a B F bond as shown in Figure 4 3.2. If a molecule possesses more than one type of n-axis, the axis of highest value of n is called the principal axis;itis Reflection through a plane of symmetry the axis of highest molecular symmetry. For example, in (mirror plane) BF , the C axis is the principal axis. 3 3 If reflection of all parts of a molecule through a plane In some molecules, rotation axes of lower orders than the produces an indistinguishable configuration, the plane is a principal axis may be coincident with the principal axis. For plane of symmetry; the symmetry operation is one of reflec- tion and the symmetry element is the mirror plane (denoted by ). For BF3, the plane containing the molecular frame- work (the yellow plane shown in Figure 3.2) is a mirror plane. In this case, the plane lies perpendicular to the vertical principal axis and is denoted by the symbol h. The framework of atoms in a linear, bent or planar molecule can always be drawn in a plane, but this plane can
be labelled h only if the molecule possesses a Cn axis perpen- dicular to the plane. If the plane contains the principal axis, it is labelled v. Consider the H2O molecule. This possesses a C2 axis (Figure 3.3) but it also contains two mirror planes, one containing the H2O framework, and one perpendicular to it. Each plane contains the principal axis of rotation and so may be denoted as v but in order to distinguish between them, we use the notations v and v’.The v label refers to the plane that bisects the H O H bond angle and the v’ label refers to the plane in which the molecule lies. Fig. 3.2 The 3-fold (C3) and three 2-fold (C2) axes of A special type of plane which contains the principal symmetry possessed by the trigonal planar BF3 molecule. rotation axis, but which bisects the angle between two Chapter 3 . Symmetry operations and symmetry elements 81
adjacent 2-fold axes, is labelled d. A square planar molecule such as XeF4 provides an example. Figure 3.4a shows that XeF4 contains a C4 axis (the principal axis) and perpen- dicular to this is the h plane in which the molecule lies. Coincident with the C4 axis is a C2 axis. Within the plane of the molecule, there are two sets of C2 axes. One type (the C2’ axis) coincides with F–Xe–F bonds, while the second type (the C2’’ axis) bisects the F–Xe–F 908 angle (Figure 3.4). We can now define two sets of mirror planes: one type ( v) contains the principal axis and a C2’ axis (Figure 3.4b), while the second type ( d) contains the principal axis and a C2’’ axis (Figure 3.4c). Each d plane bisects the angle between two C2’ axes. In the notation for planes of symmetry, , the subscripts h, v and d stand for horizontal, vertical and dihedral
Fig. 3.3 The H2O molecule possesses one C2 axis and respectively. two mirror planes. (a) The C2 axis and the plane of symmetry that contains the H2O molecule. (b) The C2 axis and the plane of symmetry that is perpendicular to the plane Self-study exercises of the H2O molecule. (c) Planes of symmetry in a molecule are often shown together on one diagram; this representation for 1. N2O4 is planar (Figure 14.14). Show that it possesses three H2O combines diagrams (a) and (b). planes of symmetry.
Fig. 3.4 The square planar molecule XeF4. (a) One C2 axis coincides with the principal (C4) axis; the molecule lies in a h plane which contains two C2’ and two C2’’ axes. (b) Each of the two v planes contains the C4 axis and one C2’ axis. (c) Each of the two d planes contains the C4 axis and one C2’’ axis. 82 Chapter 3 . An introduction to molecular symmetry
2. B2Br4 has the following staggered structure:
(3.7) (3.8)
Show that B2Br4 has one less plane of symmetry than B2F4 Self-study exercises which is planar. 1. Draw the structures of each of the following species and 3. Ga2H6 has the following structure in the gas phase: confirm that each possesses a centre of symmetry: CS2, [PF6] , XeF4,I2, [ICl2] . 2 2 2. [PtCl4] has a centre of symmetry, but [CoCl4] does not. One is square planar and the other is tetrahedral. Which is which?
3. Why does CO2 possess an inversion centre, but NO2 does not?
4. CS2 and HCN are both linear. Explain why CS2 possesses a centre of symmetry whereas HCN does not.
Show that it possesses three planes of symmetry. 4. Show that the planes of symmetry in benzene are one h, three Rotation about an axis, followed by and three . v d reflection through a plane perpendicular to this axis 3608 Reflection through a centre of symmetry If rotation through about an axis, followed by reflection n (inversion centre) through a plane perpendicular to that axis, yields an indistin- If reflection of all parts of a molecule through the centre of the guishable configuration, the axis is an n-fold rotation– molecule produces an indistinguishable configuration, the reflection axis, also called an n-fold improper rotation axis. centre is a centre of symmetry, also called a centre of It is denoted by the symbol Sn. Tetrahedral species of the inversion (see also Box 1.9); it is designated by the symbol i. type XY4 (all Y groups must be equivalent) possess three S axes, and the operation of one S rotation–reflection in Each of the molecules CO2 (3.3), trans-N2F2 (see worked 4 4 the CH molecule is illustrated in Figure 3.5. example 3.1), SF6 (3.4)andbenzene(3.5) possesses a 4 centre of symmetry, but H2S(3.6), cis-N2F2 (3.7) and SiH4 (3.8)donot. Self-study exercises
1. Explain why BF3 possesses an S3 axis, but NF3 does not.
2. C2H6 in a staggered conformation possesses an S6 axis. Show that this axis lies along the C–C bond.
3. Figure 3.5 shows one of the S4 axes in CH4. On going from CH4 to CH2Cl2, are the S4 axes retained?
(3.3) (3.4) Identity operator All objects can be operated upon by the identity operator E. This is the simplest operator (although it may not be easy to appreciate why we identify such an operator!) and effectively identifies the molecular configuration. The operator E leaves (3.5) (3.6) the molecule unchanged. Chapter 3 . Symmetry operations and symmetry elements 83
3608 Fig. 3.5 An improper rotation (or rotation–reflection), S , involves rotation about followed by reflection through a n n plane that is perpendicular to the rotation axis. The diagram illustrates the operation about one of the S4 axes in CH4; three S4 operations are possible for the CH4 molecule. [Exercise: where are the three rotation axes for the three S4 operations in CH4?]
Worked example 3.1 Symmetry properties of cis- and trans -N2F2
How do the rotation axes and planes of symmetry in cis- and trans-N2F2 differ?
First draw the structures of cis- and trans-N2F2; both are 5. The consequence of the different types of C2 axes, planar molecules. and the presence of the v plane in the cis-isomer, is that the symmetry planes containing the cis- and F trans-N2F2 molecular frameworks are labelled v’ and NN NN h respectively.
F F F cis trans Self-study exercises
1. The identity operator E applies to each isomer. 1. How do the rotation axes and planes of symmetry in Z- and E- CFH¼CFH differ? 2. Each isomer possesses a plane of symmetry which con-
tains the molecular framework. However, their labels 2. How many planes of symmetry do (a) F2C¼O, (b) ClFC¼O differ (see point 5 below). and (c) [HCO2] possess? [Ans. (a) 2; (b) 1; (c) 2] 3. The cis-isomer contains a C2 axis which lies in the plane of the molecule, but the trans-isomer contains a C2 axis which bisects the N N bond and is perpendicular to the plane of the molecule. Worked example 3.2 Symmetry operations in NH3
The symmetry operators for NH3 are E, C3 and 3 v. (a) Draw the structure of NH3. (b) What is the meaning of the E opera- tor? (c) Draw a diagram to show the rotation and reflection symmetry operations.
(a) The molecule is trigonal pyramidal.
4. The cis- (but not the trans-) isomer contains a mirror N H plane, v, lying perpendicular to the plane of the H molecule and bisecting the N N bond: H 84 Chapter 3 . An introduction to molecular symmetry
(b) The E operator is the identity operator and it leaves the In addition, BCl3 contains a h plane and three C2 axes molecule unchanged. (see Figure 3.2). (c) The C3 axis passes through the N atom, perpendicular to a plane containing the three H atoms. Each v plane contains one N H bond and bisects the opposite H N H bond angle.
Rotation through 1208 about the C3 axis, followed by reflec- tion through the plane perpendicular to this axis (the h plane), generates a molecular configuration indistinguishable from the first – this is an improper rotation S3.
Self-study exercises Conclusion: The symmetry elements that BCl3 and PCl3 have in common 1. What symmetry operators are lost in going from NH3 to are E, C3 and 3 v. NH2Cl? [Ans. C3; two v] The symmetry elements possessed by BCl3 but not by PCl3 2. Compare the symmetry operators possessed by NH3,NH2Cl, are h,3C2 and S3. NHCl2 and NCl3.
3. Draw a diagram to show the symmetry operators of NClF2. Self-study exercises [Ans. Show one v; only other operator is E] 1. Show that BF3 and F2C¼O have the following symmetry ele- ments in common: E, two mirror planes, one C2.
2. How do the symmetry elements of ClF3 and BF3 differ? E ’ C versus [Ans:BF3, as for BCl3 above; ClF3, , v , v, 2] Worked example 3.3 Trigonal planar BCl3 trigonal pyramidal PCl3
What symmetry elements do BCl3 and PCl3 (a) have in common and (b) not have in common? 3.3 Successive operations PCl3 is trigonal pyramidal (use VSEPR theory) and so possesses the same symmetry elements as NH3 in worked example 3.2. These are E, C3 and 3 v. As we have seen in Section 3.2, a particular symbol is used to BCl is trigonal planar (use VSEPR) and possesses all the 3 denote a specific symmetry operation. To say that NH3 above symmetry elements: possesses a C3 axis tells us that we can rotate the molecule through 1208 and end up with a molecular configuration that is indistinguishable from the first. However, it takes
three such operations to give a configuration of the NH3 molecule that exactly coincides with the first. The three separate 1208 rotations are identified by using the notation in Figure 3.6. We cannot actually distinguish between the three H atoms, but for clarity they are labelled H(1), H(2) 3 and H(3) in the figure. Since the third rotation, C3, returns the NH3 molecule to its initial configuration, we can write equation 3.2, or, in general, equation 3.3. 3 C3 ¼ E ð3:2Þ n Cn ¼ E ð3:3Þ Chapter 3 . Point groups 85
2 3 Fig. 3.6 Successive C3 rotations in NH3 are distinguished using the notation C3, C3 and C3. The effect of the last operation is the same as that of the identity operator acting on NH3 in the initial configuration.
Similar statements can be written to show the combined character tables (see Sections 3.5 and 4.4) which are effects of successive operations. For example, in planar widely available. BCl3,theS3 improper axis of rotation corresponds to rotation Table 3.1 summarizes the most important classes of point about the C3 axis followed by reflection through the h plane. group and gives their characteristic types of symmetry This can be written in the form of equation 3.4. elements; E is, of course, common to every group. Some particular features of significance are given below. S3 ¼ C3 h ð3:4Þ C 1 point group Self-study exercises Molecules that appear to have no symmetry at all, e.g. 3.9, 2 2 1. [PtCl4] is square planar; to what rotational operation is C4 must possess the symmetry element E and effectively possess equivalent? at least one C1 axis of rotation. They therefore belong to the 4 C1 point group, although since C1 ¼ E, the rotational 2. Draw a diagram to illustrate what the notation C6 means with respect to rotational operations in benzene. symmetry operation is ignored when we list the symmetry elements of this point group.
H 3.4 Point groups Br C F The number and nature of the symmetry elements of a given Cl molecule are conveniently denoted by its point group, and (3.9) give rise to labels such as C2, C3v, D3h, D2d, Td, Oh or Ih. These point groups belong to the classes of C groups, D C groups and special groups, the latter containing groups 1v point group that possess special symmetries, i.e. tetrahedral, octahedral C1 signifies the presence of an 1-fold axis of rotation, i.e. that and icosahedral. possessed by a linear molecule (Figure 3.7); for the molecular To describe the symmetry of a molecule in terms of one species to belong to the C1v point group, it must also possess symmetry element (e.g. a rotation axis) provides information an infinite number of v planes but no h plane or inversion only about this property. Each of BF3 and NH3 possesses a centre. These criteria are met by asymmetrical diatomics 3-fold axis of symmetry, but their structures and overall such as HF, CO and [CN] (Figure 3.7a), and linear poly- symmetries are different; BF3 is trigonal planar and NH3 is atomics (throughout this book, polyatomic is used to mean a trigonal pyramidal. On the other hand, if we describe the species containing three or more atoms) that do not possess symmetries of these molecules in terms of their respective a centre of symmetry, e.g. OCS and HCN. point groups (D3h and C3v), we are providing information about all their symmetry elements. D1 point group Before we look at some representative point groups, we h 2 emphasize that it is not essential to memorize the symmetry Symmetrical diatomics (e.g. H2,[O2] ) and linear poly- elements of a particular point group. These are listed in atomics that contain a centre of symmetry (e.g. [N3] , 86 Chapter 3 . An introduction to molecular symmetry
Table 3.1 Characteristic symmetry elements of some important classes of point groups. The characteristic symmetry elements of the Td, Oh and Ih are omitted because the point groups are readily identified (see Figure 3.8). No distinction is made in this table between v and d planes of symmetry. For complete lists of symmetry elements, character tables should be consulted.
Point group Characteristic symmetry elements Comments
Cs E, one plane Ci E, inversion centre Cn E, one (principal) n-fold axis Cnv E, one (principal) n-fold axis, n v planes Cnh E, one (principal) n-fold axis, one h plane, one The Sn axis necessarily follows from the Cn axis and h plane. Sn-fold axis which is coincident with the Cn axis For n ¼ 2, 4 or 6, there is also an inversion centre. Dnh E, one (principal) n-fold axis, n C2 axes, one h The Sn axis necessarily follows from the Cn axis and h plane. plane, n v planes, one Sn-fold axis For n ¼ 2, 4 or 6, there is also an inversion centre. Dnd E, one (principal) n-fold axis, n C2 axes, n v For n ¼ 3 or 5, there is also an inversion centre. planes, one S2n-fold axis Td Tetrahedral Oh Octahedral Ih Icosahedral
CO2,HC CH) possess a h plane in addition to a C1 axis observed electronic spectra of tetrahedral and octahedral and an infinite number of v planes (Figure 3.7). These metal complexes (see Section 20.6). Members of the 2 species belong to the D1h point group. icosahedral point group are uncommon, e.g. [B12H12] (Figure 3.9d). T O I d, h or h point groups Determining the point group of a molecule Molecular species that belong to the Td, Oh or Ih point or molecular ion groups (Figure 3.8) possess many symmetry elements, although it is seldom necessary to identify them all before The application of a systematic approach to the assignment of the appropriate point group can be assigned. Species with a point group is essential, otherwise there is the risk that sym- 2 tetrahedral symmetry include SiF4, [ClO4] , [CoCl4] , metry elements will be missed with the consequence that an þ [NH4] ,P4 (Figure 3.9a) and B4Cl4 (Figure 3.9b). Those incorrect assignment is made. Figure 3.10 shows a procedure with octahedral symmetry include SF6, [PF6] , W(CO)6 that may be adopted; some of the less common point groups 3 (Figure 3.9c) and [Fe(CN)6] . There is no centre of sym- (e.g. Sn, T, O) are omitted from the scheme. Notice that it is metry in a tetrahedron but there is one in an octahedron, not necessary to find all the symmetry elements (e.g. improper and this distinction has consequences with regard to the axes) in order to determine the point group.
Fig. 3.7 Linear molecular species can be classified according to whether they possess a centre of symmetry (inversion centre) or not. All linear species possess a C1 axis of rotation and an infinite number of v planes; in (a), two such planes are shown and these planes are omitted from (b) for clarity. Diagram (a) shows an asymmetrical diatomic belonging to the point group C1v, and (b) shows a symmetrical diatomic belonging to the point group D1h. Chapter 3 . Point groups 87
Tetrahedron Octahedron Icosahedron
Fig. 3.8 The tetrahedron (Td symmetry), octahedron (Oh symmetry) and icosahedron (Ih symmetry) possess four, six and twelve vertices respectively, and four, eight and twenty equilateral-triangular faces respectively.
We illustrate the application of Figure 3.10 with reference to four worked examples, with an additional example in Section 3.8. Before assigning a point group to a molecule, its structure must be determined by, for example, microwave spectroscopy, or X-ray, electron or neutron diffraction methods.
Worked example 3.4 Point group assignments: 1
Determine the point group of trans-N2F2.
First draw the structure. Fig. 3.9 The molecular structures of (a) P4, (b) B4Cl4 F (the B atoms are shown in blue), (c) [W(CO)6] (the W atom is shown in yellow and the C atoms in grey) and (d) 2 NN [B12H12] (the B atoms are shown in blue).
F Apply the strategy shown in Figure 3.10: Worked example 3.5 Point group assignments: 2 START
Is the molecule linear? No Determine the point group of PF5. Does trans-N2F2 have Td, Oh or Ih symmetry? No First, draw the structure. Is there a C axis? Yes; a C axis perpendicular n 2 F to the plane of the paper F and passing through the F P midpoint of the N N bond F Are there two C2 axes F perpendicular to the principal axis? No In the trigonal bipyramidal arrangement, the three equator- ial F atoms are equivalent, and the two axial F atoms are Is there a h plane (perpendicular to the equivalent. principal axis)? Yes Apply the strategy shown in Figure 3.10: STOP START Is the molecule linear? No The point group is C2h. Does PF5 have Td, Oh or Ih symmetry? No Self-study exercises Is there a Cn axis? Yes; a C3 axis containing the P and two axial F atoms 1. Show that the point group of cis-N2F2 is C2v. Are there three C2 axes 2. Show that the point group of E-CHCl¼CHCl is C . 2h perpendicular to the Yes; each lies along a P Feq principal axis? bond 88 Chapter 3 . An introduction to molecular symmetry
Fig. 3.10 Scheme for assigning point groups of molecules and molecular ions. Apart from the cases of n ¼ 1or1, n most commonly has values of 2, 3, 4, 5 or 6.
Is there a h plane Apply the strategy shown in Figure 3.10: (perpendicular to the Yes; it contains the P and principal axis)? three F atoms. START eq Is the molecule linear? No STOP Does POCl3 have Td, Oh or No (remember that The point group is D3h. Ih symmetry? although this molecule is loosely considered as Self-study exercises being tetrahedral in shape, it does not D 1. Show that BF3 belongs to the 3h point group. possess tetrahedral symmetry) 2. Show that OF2 belongs to the C2v point group. Is there a Cn axis? Yes; a C3 axis running along the O P bond Are there 3 C2 axes Worked example 3.6 Point group assignments: 3 perpendicular to the principal axis? No To what point group does POCl3 belong ? Is there a h plane (perpendicular to the
The structure of POCl3 is: principal axis)? No Are there n planes Yes; each contains the O v (containing the principal one Cl and the O and P P axis)? atoms Cl Cl STOP
Cl The point group is C3v. Chapter 3 . Character tables: an introduction 89
Self-study exercises 2. S6 has the chair conformation shown in Box 1.1. Confirm that this molecule contains a centre of inversion. 1. Show that CHCl3 possesses C3v symmetry, but that CCl4 belongs to the Td point group. þ 2. Assign point groups to (a) [NH4] and (b) NH3. [Ans. (a) T ; (b) C ] d 3v 3.5 Character tables: an introduction
While Figure 3.10 provides a point group assignment using certain diagnostic symmetry elements, it may be necessary Worked example 3.7 Point group assignments: 4 to establish whether any additional symmetry elements are exhibited by a molecule in a given point group. Three projections of the cyclic structure of S are shown below; 8 Each point group has an associated character table, and all S S bond distances are equivalent, as are all S S S bond that for the C point group is shown in Table 3.2. The angles. To what point group does S belong? 2v 8 point group is indicated at the top left-hand corner and the symmetry elements possessed by a member of the point group are given across the top row of the character table. The H2O molecule has C2v symmetry and when we looked at the symmetry elements of H2O in Figure 3.3, we labelled the two perpendicular planes. In the character table, taking the z axis as coincident with the principal axis, the v and v’ planes are defined as lying in the xz and yz planes, respec- tively. Placing the molecular framework in a convenient orientation with respect to a Cartesian set of axes has many advantages, one of which is that the atomic orbitals on the central atom point in convenient directions. We return to this in Chapter 4. Table 3.3 shows the character table for the C3v point Follow the scheme in Figure 3.10: group. The NH3 molecule possesses C3v symmetry, and worked example 3.2 illustrated the principal axis of rotation START and planes of symmetry in NH3. In the character table, the Is the molecule linear? No presence of three v planes in NH3 is represented by the Does S have T , O or I notation ‘3 v’ in the top line of the table. The notation 8 d h h 1 2 symmetry? No ‘2C3’ summarizes the two operations C3 and C3. The opera- tion C3 is equivalent to the identity operator, E, and so is not Is there a Cn axis? Yes; a C4 axis running 3 through the centre of the specified again. ring; perpendicular to the Figure 3.4 showed the proper axes of rotation and planes plane of the paper in of symmetry in the square planar molecule XeF4. This has diagram (a) D4h symmetry. The D4h character table is given in Appendix 3, and the top row of the character table that summarizes the Are there 4 C2 axes perpendicular to the principal Yes; these are most easily symmetry operations for this point group is as follows: axis? seen from diagram (c) ’ ’’ Is there a h plane D4h E 2C4 C2 2C2 2C2 i 2S4 h 2 v 2 d (perpendicular to the principal axis)? No
Are there n d planes Yes; these are most easily (containing the principal seen from diagrams (a)
axis)? and (c) Table 3.2 The character table for the C2v point group. For more character tables, see Appendix 3. STOP ð Þ ’ð Þ The point group is D4d. C2v EC2 v xz v yz
2 2 2 A1 111 1 zx, y , z Self-study exercises A2 11 1 1 Rz xy B1 1 11 1 x; Ry x; xz 1. Copy diagram (a) above. Show on the figure where the C4 axis B2 1 1 11 y, Rx y, yz and the four C2 axes lie. 90 Chapter 3 . An introduction to molecular symmetry
Table 3.3 The character table for the C3v point group. For The next two sections deal briefly with the consequences of more character tables, see Appendix 3. symmetry on observed bands in infrared spectra and with the relationship between molecular symmetry and chirality. C3v E 2C3 3 v In Chapter 20, we consider the electronic spectra of octa-
2 2 2 hedral and tetrahedral d-block metal complexes and discuss A1 111z x + y , z the effects that molecular symmetry has on electronic A2 11 1 Rz 2 2 spectroscopic properties. E 2 10(x, y)(Rx, Ry)(x – y , xy)(xz, yz)
In Figure 3.4 we showed that a C2 axis is coincident with the 2 C4 axis in XeF4. The C2 operation is equivalent to C4. The 3.7 Infrared spectroscopy character table summarizes this information by stating 1 3 2 ‘2C4 C2’, referring to C4 and C4, and C4 ¼ C2. The opera- 4 The discussion that follows is necessarily selective and is tion C4 is taken care of in the identity operator E. The two pitched at a simplistic level. Although in this section we sets of C2 axes that we showed in Figure 3.4 and labelled derive the number of vibrational modes for some simple ’ ’’ as C2 and C2 are apparent in the character table, as are molecules, for more complicated species it is necessary to the h, two v and two d planes of symmetry. The symmetry use character tables. The reading list at the end of the chapter operations that we did not show in Figure 3.4 but that are gives sources of detailed discussions of the relationship included in the character table are the centre of symmetry, between group theory and normal modes of vibration. i, (which is located on the Xe atom in XeF4), and the S4 Infrared (IR) and Raman (see Box 3.1) spectroscopies Þ: axes. Each S4 operation can be represented as (C4 h are branches of vibrational spectroscopy and the former The left-hand column in a character table gives a list of technique is the more widely available of the two in student symmetry labels. These are used in conjunction with the teaching laboratories. numbers, or characters, from the main part of the table to label the symmetry properties of, for example, molecular How many vibrational modes are there for a orbitals or modes of molecular vibrations. As we shall see given molecular species? in Chapter 4, although the symmetry labels in the character tables are upper case (e.g. A1, E, T2g), the corresponding Vibrational spectroscopy is concerned with the observation symmetry labels for orbitals are lower case (e.g. a1, e, t2g). of the degrees of vibrational freedom, the number of which In Chapter 4, we use character tables to label the symmetries can be determined as follows. The motion of a molecule of orbitals, and to understand what orbital symmetries are containing n atoms can conveniently be described in terms allowed for a molecule possessing a particular symmetry. of the three Cartesian axes; the molecule has 3n degrees of Appendix 3 gives character tables for the most commonly freedom which together describe the translational, vibrational encountered point groups, and each table has the same and rotational motions of the molecule. format as those in Tables 3.2 and 3.3. The translational motion of a molecule (i.e. movement through space) can be described in terms of three degrees of freedom relating to the three Cartesian axes. If there are 3n degrees of freedom in total and three degrees of freedom 3.6 Why do we need to recognize for translational motion, it follows that there must be symmetry elements? (3n 3) degrees of freedom for rotational and vibrational motion. For a non-linear molecule there are three degrees of rotational freedom, but for a linear molecule, there are So far in this chapter, we have described the possible sym- two degrees of rotational freedom. This difference arises metry elements that a molecule might possess and, on the because there is no rotation about the molecular axis in a basis of these symmetry properties, we have illustrated how linear molecule. Having taken account of translational and a molecular species can be assigned to a particular point rotational motion, the number of degrees of vibrational group. Now we address some of the reasons why the freedom can be determined (equations 3.5 and 3.6). recognition of symmetry elements in a molecule is important to the inorganic chemist. Number of degrees of vibrational freedom for a Most of the applications of symmetry fall into one of the non-linear molecule ¼ 3n 6 ð3:5Þ following categories: Number of degrees of vibrational freedom for a . constructing molecular and hybrid orbitals (see Chapter linear molecule ¼ 3n 5 ð3:6Þ 4); . interpreting spectroscopic (e.g. vibrational and electronic) For example, from equation 3.6, the linear CO2 molecule has properties; four normal modes of vibration and these are shown in Figure . determining whether a molecular species is chiral. 3.11. Two of the modes are degenerate; i.e. they possess the Chapter 3 . Infrared spectroscopy 91
CHEMICAL AND THEORETICAL BACKGROUND
Box 3.1 Raman spectroscopy
Infrared and Raman spectroscopies are both concerned with subject to the rule of mutual exclusion which states that in the study of molecular vibrations, and while IR spectroscopy such a molecule, a vibrational mode which is IR active is is used routinely in the practical laboratory, Raman spectro- Raman inactive, and vice versa. Thus, for a molecule with scopy is a more specialized technique. When radiation of a an inversion centre, a ‘missing’ absorption in the IR spectrum particular frequency, (usually from a laser source), falls may be observed in the Raman spectrum. However, the pre- on a molecule, some radiation is scattered. The scattered sence of symmetry elements other than the inversion centre radiation is of two types: does result in some exceptions to the rule of mutual exclusion and it must be applied with caution. We exemplify the rule . Rayleigh scattering involves radiation of frequency, , 0 with reference to CO (Figure 3.11). The two vibrational equal to that of the incident radiation, and 2 modes which are asymmetric with respect to the inversion . Raman scattering involves radiation of frequencies 0 centre (i.e. the carbon atom) are IR active and Raman inac- where is a fundamental frequency of a vibrational mode tive, while the symmetric stretch is IR inactive but Raman of the molecule. active. Thus, the value of 1333 cm 1 for this latter vibration The selection rules for Raman and IR active vibrations are can be confirmed from a Raman spectrum. different. A vibrational mode is Raman active if the polarizabil- ity of the molecule changes during the vibration. Changes in For more detailed accounts of the Raman effect, see: polarizability (for Raman spectra) are not as easy to E.A.V. Ebsworth, D.W.H. Rankin and S. Cradock (1991) visualize as changes in electric dipole moments (for IR Structural Methods in Inorganic Chemistry, 2nd edn, spectra) and in most cases it is necessary to use group theory Blackwell Scientific Publications, Oxford, Chapter 5. to determine whether or not a mode will be Raman active. K. Nakamoto (1997) Infrared and Raman Spectra of A combination of IR and Raman spectroscopic data is Inorganic and Coordination Compounds, 5th edn, Wiley, often of great use. Molecules with a centre of symmetry are New York.
same energy and could be represented in a single diagram Selection rule for an infrared active mode of with the understanding that one vibration occurs in the vibration plane of the paper and another, identical in energy, takes place in a plane perpendicular to the first. One of the important consequences of precisely denoting molecular symmetry is seen in infrared spectroscopy. An IR spectrum records the frequency of a molecular vibration, Self-study exercises but not all modes of vibration of a particular molecule give 1. Using VSEPR theory to help you, draw the structures of rise to observable absorption bands in the IR spectrum. CF4, XeF4 and SF4. Assign a point group to each molecule. This is because the following selection rule must be obeyed: Show that the number of degrees of vibrational freedom is for a vibrational mode to be IR active, it must give rise to a independent of the molecular symmetry. change in the molecular dipole moment (see Section 1.16). [Ans. Td; D4h; C2v ] For a mode of vibration to be infrared (IR) active, it must 2. Why do CO and SO have a different number of degrees of 2 2 give rise to a change in the molecular electric dipole moment. vibrational freedom? 3. How many degrees of vibrational freedom do each of the In the discussions of IR spectroscopy that follow, we are following possess: SiCl4, BrF3, POCl3?[Ans.9;6;9] concerned only with fundamental absorptions, these being the dominant features of IR spectra.
Fig. 3.11 The vibrational modes of CO2 (D1h); in each mode of vibration, the carbon atom remains stationary. Vibrations (a) and (b) are stretching modes. Bending mode (c) occurs in the plane of the paper, while bend (d) occurs in a plane perpendicular to that of the paper; the þ signs designate motion towards the reader. The two bending modes require the same amount of energy and are therefore degenerate. 92 Chapter 3 . An introduction to molecular symmetry
Fig. 3.12 The vibrational modes of SO2 (C2v).
The transition from the vibrational ground state to the first Worked example 3.8 Infrared spectra of triatomic excited state is the fundamental transition. molecules
The IR spectrum of SnCl2 exhibits absorptions at 352, 334 and D C C Linear ( 1h or 1v) and bent ( 2v) triatomic 120 cm 1. What shape do these data suggest for the molecule, molecules and is this result consistent with VSEPR theory? We can readily illustrate the effect of molecular symmetry on For linear SnCl (D1 ), the asymmetric stretch and the molecular dipole moments, and thus on infrared active 2 h bend are IR active, but the symmetric stretch is IR inactive modes of vibration, by considering the linear molecule (no change in molecular dipole moment). CO . The two C O bond distances are equal (116 pm) and 2 For bent SnCl , C , the symmetric stretching, asymmetric the molecule is readily identified as being ‘symmetrical’; 2 2v stretching and scissoring modes are all IR active. strictly, CO possesses D1 symmetry. As a consequence 2 h The data therefore suggest that SnCl is bent, and this is of its symmetry, CO is non-polar. Although both the 2 2 consistent with the VSEPR model since there is a lone pair asymmetric stretch and the bend (Figure 3.11) give rise to in addition to two bonding pairs of electrons: a change in dipole moment (generated transiently as the vibration occurs), the symmetric stretch does not. Thus, only two fundamental absorptions are observed in the IR spectrum of CO2. Sn Now consider SO2 which is a bent molecule (C2v). Figure Cl Cl 3.12 shows the three normal modes of vibration; all give rise to a change in molecular dipole moment and are therefore Self-study exercises IR active. A comparison of these results for CO2 and SO2 1 illustrates that vibrational spectroscopy can be used to 1. The vibrational modes of XeF2 are at 555, 515 and 213 cm determine whether an X3 or XY2 species is linear or bent. but only two are IR active. Explain why this is consistent Linear molecules of the general type XYZ (e.g. OCS or with XeF2 having a linear structure. HCN) possess C1 symmetry and their IR spectra are v 2. How many IR active vibrational modes does CS possess, and expected to show three absorptions; the symmetric stretch- 2 why? Hint: CS2 is isostructural with CO2. ing, asymmetric stretching and bending modes are all IR active. In a linear molecule XYZ, provided that the atomic 3. The IR spectrum of SF2 has absorptions at 838, 813 and 1 masses of X and Z are significantly different, the absorptions 357 cm . Explain why these data are consistent with SF2 belonging to the C rather than D1 point group. observed in the IR spectrum can be assigned to the X–Y 2v h stretch, the Y–Z stretch and the XYZ bend. The reason 4. To what point group does F2O belong? Explain why the vibra- that the stretching modes can be assigned to individual tional modes at 928, 831 and 461 cm 1 are all IR active. C bond vibrations rather than to a vibration involving the [Ans. 2v ] whole molecule is that each of the symmetric and asymmetric stretches is dominated by the stretching of one of the two bonds. For example, absorptions at 3311, 2097 and D C 712 cm 1 in the IR spectrum of HCN are assigned to XY3 molecules with 3h or 3v symmetry the H–C stretch, the C N stretch and the HCN bend, A molecule of the type XY3 with D3h symmetry undergoes respectively. the normal modes of vibration shown in Figure 3.13. The symmetric stretch is not accompanied by a change in A stretching mode is designated by the symbol , while a molecular dipole moment and is not IR active. The remain- deformation (bending) is denoted by . ing three normal modes are IR active and so molecules For example, CO stands for the stretch of a C O bond. such as SO3,BF3 and BCl3 exhibit three absorptions in Chapter 3 . Infrared spectroscopy 93
Fig. 3.13 The vibrational modes of SO3 (D3h); only three are IR active. The þ and notation is used to show the ‘up’ and ‘down’ motion of the atoms during the mode of vibration. [Exercise: Two of the modes are labelled as being degenerate: why is this?]