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Platinum Metals Rev., 2000, 44, (4), 146

Relativistic Phenomena in the Chemistry of the Platinum Group Metals

Effects on Coordination and Chemisorption in Homogeneous and Heterogeneous Catalysis

  • By Geoffrey C. Bond
  • Brunel University, Uxbridge UB8 3PH, U.K.
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Article Synopsis

It may at first sight seem strange that concepts developed by Albert Einstein in the first decade of the 20th century to explain the structure and dynamics of the cosmos should have any relevance to chemistry. However, it is now quite clear that the chemical behaviour of the heavier elements in particular is dominated by what are termed “relativistic effects”. This article explores the implications of this for the coordination and chemisorption of carbon monoxide and unsaturated hydrocarbons, and their reactions in homogeneous and heterogeneous catalysis involving the platinum group metals.

A highly significant feature of the chemistry of the elements at the end of the three Transition Series of the Periodic Table is the close similarity that exists between the six elements with partially occupied 4d and 5d orbitals, that is, the group known as the “platinum metals”, and the marked difference between them and the three elements which have only 3d electrons, that is, the base metals (iron, cobalt, nickel). This difference also extends into Group 11, where gold and silver are much “nobler” than copper. Part of the reason for this behaviour is that the size of the atoms increases on passing from the 3d to the 4d metals, but there is no further increase on going to the 5d metals, see Table I. This size difference is seen right across the Transition Series, from Group 4 to Group 10 and beyond, and it has traditionally been explained by electron occupation of the 4f orbitals to create the Rare Earth elements before the 5d orbitals start to be filled. This has been held to produce what is termed the “lanthanide contraction”, caused by the inability of electrons in the 4f orbitals to shield effectively the s electrons from the increasing positive nuclear charge. The 6s orbital therefore contracts, and the expected increase in atomic size does not occur (1,2).

Table I

Atomic Numbers, Z, Electronic Structures, Melting Temperatures, Tm, Enthalpies of Sublimation, ΔHsub, and Metallic Radii, r, for the Platinum Group Metals

MetalZElectronic StructureTm, KΔHsub, kJ mol-1r, pm
Ru44(Kr)4d 75s 12655648132.5
Rh45(Kr)4d 85s 12239556134.5
Pd46(Kr) 4d 101825373137.5
Os76(Xe)5d 66s 23318784133.7
Ir77(Xe)5d 76s 22713663135.7
Pt78(Xe)5d 96s 12042469138.5

Chemistry of the Heavier Elements

The heavier elements, that is, those having 5d, 6s or 6p electrons, show a number of unusual physicochemical properties, many of which have been interpreted in terms of other measurable parameters, such as ionisation potential, or by assigning a label, such as “the 6s inert pair effect”, which provides a comforting sense of understanding. However the underlying causes have remained uncertain, and there has been an increasing suspicion, especially in the last 20 years, that the lanthanide contraction is not a full, perfect and sufficient explanation for all that is observed. Among the anomalies are the greater stability of the PtIV oxidation state compared to PdIV, the stability of the AuIII state, the varied colours of the Group 11 metals, the low melting temperature of mercury and the existence of the Hg22+ ion.

Numerous other unexplained aspects of the chemistry of the heavier elements have been noted (1, 2). The quite startling properties of gold have recently been reviewed in depth (3): it has high electronegativity and can form the auride ion, Au. It owes its nobility to the instability of its compounds with other electronegative elements, such as oxygen and sulfur.

The Relativistic Analogue of the Schrödinger Equation

The Schrödinger wave equation, describing subatomic particle motion, which we were taught to believe contained in principle the understanding of all chemistry, has in fact one major defect: it does not treat space and time as equivalent, as required by Einstein’s Theory of Special Relativity. P. A. M. Dirac and, independently, the Dutch physicist, H. A. Kramers, therefore devised a relativistic analogue of the Schrödinger equation, which incidentally predicted the existence of the positive electron (positron), and accounted for the occurrence of electrons having opposite “spins”. The difference which the relativistic correction made to the energetic description of the hydrogen atom was however very small, and it was therefore concluded that the chemical consequences were insignificant; but what was overlooked was the fact that, as the positive charge on the nucleus increases, the orbiting electrons must move faster in order to overcome the greater electrostatic attraction and hence to maintain their position. When the nuclear charge is about 50 (at the element tin), electrons in the 1s orbital are moving at about 60 per cent of the speed of light, and their mass is increased according to the equation:

where mass m moves with speed v, c is the speed of light and m 0 is the mass of the particle at rest. The 1s orbital therefore contracts, and the outer s orbitals have to contract in sympathy, but p orbitals are less affected, and d orbitals hardly at all: their shape determines that their electrons spend little time close to the nucleus, see Figure 1.

Fig. 1

The forms of atomic orbitals: (i) s orbitals are spherically symmetrical

(ii) p orbitals consist of three pairs of lobes, centred on each of the Cartesian axes (the px orbital is shown)

(iii) d orbitals comprise the eg family, that is the dz2 and dx2-y2 (shown), and the t2g family, which contains three four-fold lobes centred on two of the Cartesian axes, each set being mutually at right angles (the dxy set is shown)

The forms of atomic orbitals: (i) s orbitals are spherically symmetrical(ii) p orbitals consist of three pairs of lobes, centred on each of the Cartesian axes (the px orbital is shown)(iii) d orbitals comprise the eg family, that is the dz2 and dx2-y2 (shown), and the t2g  family, which contains three four-fold lobes centred on two of the Cartesian axes, each set being mutually at right angles (the dxy set is shown)

Relativistic Effects on the Properties of the Heavier Elements

The net effect of all this can be illustrated by the results of recent calculations for the metals molybdenum, tungsten and seaborgium, (4), see Figure 2. We may provisionally assume this also applies to palladium, platinum and eka-platinum (element 110), respectively. The 6s orbital, having contracted, is thus lowered in energy, while the 5d levels are raised in energy because the orbitals have expanded. The spin-orbital splitting of the p and d orbitals is a particular feature of the relativistic treatment (57).

Fig. 2

This shows the calculated outermost atomic energy levels for molybdenum, tungsten and seaborgium (4), (assumed to be analogous to palladium, platinum and eka-platinum). The left-hand part for each element shows the non-relativistic values (NR) and the right-hand part the values having the relativistic correction (Rel)

This shows the calculated outermost atomic energy levels for molybdenum, tungsten and seaborgium (4), (assumed to be analogous to palladium, platinum and eka-platinum). The left-hand part for each element shows the non-relativistic values (NR) and the right-hand part the values having the relativistic correction (Rel)

The extent of the relativistic correction to the size of the s orbitals (and its smaller effect on p orbitals) increases approximately as the square of the nuclear charge, and the total effect on the atomic size is expressed as a “relativistic contraction”, that is, the fractional decrease in the actual metallic radius compared to the calculated non-relativistic value, see Figure 3. This relativistic contraction is greatest for platinum and gold, but it subsequently decreases with increase in nuclear charge as the space occupied by the 6s orbital has a diminishing effect on atomic size.

Fig. 3

Relativistic contraction of the 6s electron level as a function of nuclear charge (redrawn from (4))

Relativistic contraction of the 6s electron level as a function of nuclear charge (redrawn from (4))

It is now generally thought that the relativistic contraction is at least as significant, if not more so, than the lanthanide contraction for the 5d metals, and that it is a dominant factor in the chemistry of elements having nuclear charge greater than 80 (mercury). From the energy level diagram of Figure 2 we can understand why the electron configuration of palladium is 4d 10 while that of platinum is 5d 96s 1, and why osmium and iridium have the 6s 2 configuration while ruthenium and rhodium are 5s 1 (because the lower energy levels are filled up first). It also follows that the 5d metals have higher ionisation potentials than the 4d (because the 6s level is of lower energy) and that they should have the greater bond strengths, with atoms both of different type and of the same type, as shown by the sublimation enthalpies and melting temperatures in Table I.

This also explains why the (100) and (110) surfaces of only the 5d metals undergo reconstruction in the absence of chemisorbed atoms. The small difference in the energies of the 6s and 5d levels, Figure 2, means that d -electrons can be more easily removed or mobilised for bonding purposes, thus accounting for the stabilities of the PtIV and AuIII oxidation states. Indeed, it would be an interesting exercise to try to predict the properties of eka-platinum on the basis of calculated energy levels of the type shown in Figure 2.

The above observations and their interpretation have been well described (3, 57), so it is of more interest to explore less well documented areas. Inorganic textbooks (1, 2) pay due regard to the phenomenon of coordination of ligands to metal atoms and ions, and to the related reactions that occur in homogeneous catalysis, but little attention is paid to the parallel phenomenon of chemisorption or to the resultant reactions of heterogeneous catalysis. These are no less interesting, and in practical terms more useful, aspects of the inorganic/organometallic chemistry of the elements. We ought therefore to look for evidence of the operation of relativistic effects in these areas, to see whether they assist in understanding and in rationalising what is seen. This will be done by considering:

(a) carbonyl complexes, chemisorption of carbon monoxide and relevant reactions, and

(b) complexes and chemisorption of unsaturated hydrocarbons, and their reactions. In doing so it will be necessary to engage in some rather broad generalisations.

Coordination and Chemisorption of Carbon Monoxide

A very great deal of research has been performed on the carbonyls formed by coordination of carbon monoxide to metal atoms (1,2). Stable neutral complexes containing one or more metal atoms exist for all the metals of Groups 8 to 10 except palladium and platinum, where the presence of either negative charge or of other ligands, such as halide ion, is required for stability. The same is true for the metals of Groups 11 and 12. Palladium is different from platinum, however, in that it cannot form polynuclear ionic complexes of the Chini type (8), but neutral monatomic complexes, M(CO), of both metals can be made at very low temperature using the matrix-isolation technique (9). The carbon monoxide can bond to one, two or three metal atoms, and the nature of the bonding is well understood (1, 2). In the linear form of coordinated carbon monoxide, the 5p molecular orbital donates charge to a vacant d orbital on the metal atom, and accepts charge from a filled atomic orbital into the 2π molecular orbital, Figure 4, but since both are antibonding the first strengthens the C-O bond and the second weakens it. The two effects therefore tend to cancel out, but the strength of the C-M bond depends on the extents of the two transfers of charge.

Fig. 4

Molecular orbital diagram for the linear bonding of carbon monoxide to a metal atom (14)

Molecular orbital diagram for the linear bonding of carbon monoxide to a metal atom (14)

The role of the relativistic effect is shown by recent density functional theory (DFT) calculations on the first bond dissociation energy of carbonyl complexes of the type M(CO)5 and M(CO)4 (10), see Table II. The agreement between theory and experiment, where possible, is satisfactory. It is one of the triumphs of modern computational chemistry that results can be obtained on molecules such as Pd(CO)4 and Pt(CO)4 which do not exist as stable entities, although the calculation correctly predicts very low M-CO dissociation energies for them. Estimates of force constants for the Group 10 molecules M(CO) in matrix isolation provide confirmation that nickel is a much better σ-donor and π-acceptor than either palladium or platinum, although the latter is the second best because the destabilised 5d levels, see Figure 2, allow more metal-to-ligand back donation (9). In Group 8, both theory and experiment show that the sequence of M-CO bond energies is Fe > Os > Ru, for the same reason (10).

Table II

Calculated and Experimental First Bond Dissociation Energies, D, of Mononuclear Carbonyls of Groups 8 and 10 (10)

D, kJ mol-1
CarbonylExperimentalCalculated
Fe(CO)5176192
Ru(CO)5118138
Os(CO)5130145
Ni(CO)4105124
Pd(CO)4-50.5
Pt(CO)4-65.6

Much is also known about the chemisorption of carbon monoxide on metal surfaces and particles: the nature of the bonding is very similar to that in carbonyl complexes, and the fact that a surface metal atom is linked to a number of others seems to have little effect. The significant difference is however that the M-CO bond is stronger at surfaces than in complexes, so that strong chemisorption is observed with palladium and platinum, and the adsorbed state can even be studied on the Group 11 metals.

In fact, it is in Group 11 that the relativistic effect is more clearly seen (1113), but results from a recent important paper which analyses the situation with the Group 10 metals in great depth must be examined (14). In summary it concludes that the chemisorption of a carbon monoxide molecule on platinum differs from that on nickel and palladium because there is:

• a larger differential shift in C-O vibration frequency between the atop and bridge sites, and

• a smaller change in the work function of the metal. These observations can only be explained theoretically on the basis of DFT calculations which incorporate the relativistic correction. This is however of much less importance in the case of palladium, see Figure 2.

Coordination of Hydrogen Atoms and Molecules

In homogeneously-catalysed reactions in which hydrogen is a reactant, it must first be coordinated to the metal centre: this usually occurs by dissociation and oxidative addition. The metals of Group 8 form complexes of the type M(PR3)3H4 (15). When M is osmium there are four hydride ligands, but if M is iron or ruthenium there are two hydrides and one hydrogen molecule, the latter acting as a σ* acceptor via its vacant antibonding σ* orbital. DFT calculations show that this changeover is due to the destabilisation of the osmium 5d orbitals, making osmium a stronger donor. It is not yet known whether there are parallel differences in hydrogen chemisorption.

Homogeneous and Heterogeneous Catalytic Reactions of Carbon Monoxide

The industrially and environmentally important catalysed reactions of carbon monoxide are:

(i) its reaction with hydrogen

(ii) its reaction with hydrogen and an alkene, that is, hydroformylation

(iii) its reaction with methanol, and

(iv) its oxidation to carbon monoxide.

The reaction with hydrogen can lead to many different products, including methane, methanol and, by the Fischer-Tropsch synthesis, higher alkenes, alkanes and oxygenated products, depending on the catalyst used, and on the temperature and the pressure at which the reaction is conducted.

There are no significant applications of homogeneously catalysed reactions of carbon monoxide with hydrogen alone. Laboratory studies have shown that HCo(CO)4 can catalyse the formation of methanol, and rhodium cluster complexes can give 1,2-dihydroxyethane (ethylene glycol), but vigorous conditions are needed, and they are not commercially attractive (1).

All the many important reactions of carbon monoxide and hydrogen require heterogeneous catalysts. The metals which feature in Fischer-Tropsch synthesis are the three base metals of Groups 8 to 10, and ruthenium and osmium. Ruthenium is able to give very high molecular weight hydrocarbons at high pressure. Palladium can catalyse the formation of methane, and rhodium can make C2 oxygenated products; the distinction here between these two metals and the others of Groups 8 to 10 is a clear reflection of the weaker bonding of carbon monoxide to their surfaces. In the same way, copper is the metal of choice for the industrial synthesis of methanol, although gold also works, but much less effectively (3).

The carbonylation of methanol to acetic acid was for many years operated with a homogeneous rhodium catalyst, although an iridium compound is now also used (the Cativa process) (16). This is one of the very few examples of the use of iridium in industrial homogeneous catalysis.

Coordination and Chemisorption of Unsaturated Hydrocarbons

Much work has been performed on these subjects (1, 2, 1719), so it is necessary to draw some broad generalisations and to select just a few examples for closer attention. Many metal atoms and ions coordinate alkenes, alkynes and alkadienes, and these molecules are also strongly chemisorbed by the metals of Groups 8 to 10.

Ethene

Most work has been done on ethene, so it will be discussed first. The archetypal complex is Zeise’s salt, K[PtCl3(C2H4)].H2O, in which the ethene molecule coordinates sideways on to the PtII ion. The C-C bond is stretched and the hydrogen atoms move backwards, see Figure 5. The bond is very similar to that described above for carbon monoxide: electrons pass from a filled π orbital into a vacant d orbital on the metal (giving the σ component) and there is a reciprocal transfer back of electrons from a filled orbital into a vacant antibonding π* orbital of the ethene (the π component). Similar coordination occurs with other metal atoms and ions of Groups 8 to 10, and with the univalent cations of Group 11, although here the bonding is weaker because there are no vacant d orbitals on the metal. There are also complexes of the type M0(PR3)2(C2H4) in which the geometry is distorted tetrahedral, see Figure 6. The bonding has predominantly π character, again because of the absence (in the case of palladium) or lesser availability (in the case of platinum) of d -orbital vacancies. The coordinated ethene molecule may therefore be considered to have a metallacyclopropane structure. The variable extents of the two types of orbital overlap, depending upon the electronic structure of the metal species, the nature of the other ligands and the substituents on the alkene, mean that there is a continuous range of structures, from an almost unaltered ethene molecule through the σπ complexed Zeise’s salt structure to the ethane-like metallocyclopropane mode, rather than there being clearly divided classes.

Fig. 5

Molecular orbital diagram for the bonding of ethene to PtII in [PtCl3(C2H4)] (the anion of Zeise’s salt). Note that there are other Cl ions in front of and behind the platinum atom

Molecular orbital diagram for the bonding of ethene to PtII in [PtCl3(C2H4)]− (the anion of Zeise’s salt). Note that there are other Cl− ions in front of and behind the platinum atom

Fig. 6

Molecular orbital diagram for the bonding of ethene to Pt0 in Pt0(PPh3)2(C2H4): electron donation from ethene is supposed to be to a partly-filled dp2 hybrid orbital on the metal. This complex is almost planar; the phenyl groups are not shown

Molecular orbital diagram for the bonding of ethene to Pt0 in Pt0(PPh3)2(C2H4): electron donation from ethene is supposed to be to a partly-filled dp2 hybrid orbital on the metal. This complex is almost planar; the phenyl groups are not shown

It is difficult to find quantitative information on the strengths of the coordinate bond between ethene and metal atoms or ions. There is however a general impression that platinum complexes are more strongly bonded than palladium, due to the greater spatial extension of the platinum’s 5d orbitals, and the larger orbital overlap which is therefore possible. This impression is confirmed by measurements of the equilibrium constant for the formation of M(PR3)2(C2H4) complexes in benzene solution at 298 K:

the values of which are ∼ 300 for nickel, 0.013 for palladium and 0.122 for platinum (20). Bond energies for these complexes and for those of the type M(CO)4(C2H4) have been calculated by relativistic DFT, and are, in both cases, smallest for palladium, see Table III, (21).

Table III

Ethene-Metal Bond Dissociation Energies Calculated by Relativistic Density Functional Theory (21)

ComplexBond dissociation energy, kJ mol-1
Ni(PH3)2(C2H4)38.0
Pd(PH3)2(C2H4)19.8
Pt(PH3)2(C2H4)22.8
Ni(CO)4(C2H4)38.9
Pd(CO)4(C2H4)30.7
Pt(CO)4(C2H4)39.3

Similar structures to those seen in coordination complexes have also been identified when ethene is chemisorbed by metal surfaces or particles (1719). Indeed, a simple-minded theoretical basis for the correspondence was presented in the mid-1960s (22). In particular the πσ form (as in Zeise’s salt) is seen at low temperature or high surface coverage on a number of surfaces, and an analogue of the metallacyclopropane form may also have been detected, see Figure 7. However, because multi-atom sites are available, other structures can arise, especially the σ-diadsorbed ethane-like structure where each carbon atom forms a σ-bond to two metal atoms, as shown in Figure 7, (23). The only analogy for this type of structure in organometallic chemistry is the complex Os2(CO)8(C2H4), which may also owe its existence to the relativistic d orbital destabilisation.

Fig. 7

Molecular orbital diagrams for ethene chemisorbed on metal surfaces:(a) the σ-diadsorbed form on platinum, (b) the πσ form on a platinum atom (the analogue of the structure shown in Fig. 6) and (c) on atoms of Group 11, where back-bonding from ethene to metal cannot occur because of the lack of a suitable vacant orbital

Molecular orbital diagrams for ethene chemisorbed on metal surfaces:(a) the σ-diadsorbed form on platinum, (b) the πσ form on a platinum atom (the analogue of the structure shown in Fig. 6) and (c) on atoms of Group 11, where back-bonding from ethene to metal cannot occur because of the lack of a suitable vacant orbital

The use of spectroscopic and structure-determining techniques such as FTIR and LEED have provided estimates of the stretching of the C-C bond following chemisorption, either by:

(i) a “π,σ parameter” derived from the change in vibration frequency of the C-C bond, taking values between zero (for the free molecule) and unity (for C2H4Br2) (24), or by

(ii) a bond order between unity and two derived from the length of the C-C bond (19).

Some values of both parameters are given in Table IV, and show that the distortion due to stretching is slight for the Group 11 metals but large for iron, ruthenium, nickel and platinum surfaces.

Table IV

Values of the π,σ Parameter (24) and of the C-C Bond Order (19) for Ethene Chemisorbed on Various Metal Surfaces

Surfaceπ,σ ParameterBond order
Fe(110)0.551.20
Ru(001)0.851.35
Rh(111)0.501.39
Ni(111)0.801.33
Pd(111)0.431.61
Pt(111)0.921.13
Cu(100)0.211.66
Ag film-1.88
Au foil0.25-

From the very extensive literature, the following generalisations may be made:

(i) The σ-diadsorbed form of ethene is commonly seen on platinum surfaces, but rarely on palladium, which usually shows the πσ type of structure.

(ii) The πσ type occurs together with the σ-diadsorbed form on stepped platinum surfaces.

(iii) Pre-adsorbed oxygen atoms favour the πσ form, or structures which tend towards this form. The clear conclusion is that here is a marked tendency for ethene to be more strongly chemisorbed (as the σ-diadsorbed form) on platinum than on palladium (where the πσ form is favoured); the parallels with coordination chemistry are also very marked, and the explanations are the same.

Other Alkenes

Alkenes having a methylene group adjacent to the double bond may on coordination lose a hydrogen atom to form a π-allylic ligand (1, 2). This occurs with a number of metal atoms and ions, but more readily and extensively with nickel and palladium than with platinum. Here is another distinction that may have its origin in relativistic effects. Dienes coordinate strongly through both double bonds to many metal species, for instance, on palladium, 1,3-butadiene is chemisorbed by both double bonds in the πσ mode, but on platinum, only through one double bond in the σ-diadsorbed form (18).

Homogeneous and Heterogeneous Catalysis of Reactions of Unsaturated Hydrocarbons

It would be possible to summarise the homogeneous catalysis of alkene reactions and of metal-mediated reactions of organic molecules in general by saying simply that (with the sole exception of hydrosilylation) all require a metal compound or complex drawn from the elements in the first two rows of Groups 8 to 10 . This remarkably clear generalisation is however not often noted. The distinction between the second and third row metals is strikingly confirmed by inspecting, for example, Number 3 of this Journal for 1999, where in the reviews on pages 103 and 114, and in the Homogeneous Catalysis’ Abstracts and New Patents sections, every reference concerns either ruthenium, rhodium or palladium. More generally, complexes of the three base metals: iron, cobalt and nickel, are also effective, while those of the 5d metals and compounds of the Group 11 metals are not. This illustrates the operation of a “Volcano Principle” in homogeneous catalysis: the 5d metals form complexes that are too strong, the Group 11 metal complexes are too weak, while those of the 3d and 4d metals fall in the acceptable range. Unfortunately there seems to be little quantitative information available (apart from that mentioned above) to underpin that statement.

It is only necessary to record briefly some of the observations which lead to this concept. Early work on homogeneous hydrogenation used compounds or complexes of iron, cobalt, ruthenium and rhodium (for example, Wilkinson’s complex Rh(PPh3)3Cl); hydroformylation used initially cobalt, but this was later replaced by rhodium which gave greater selectivity to terminal aldehydes (2). Complexes of NiII and Rh1 catalyse the dimerisation of alkenes (2), and complexes of FeII, NiII and PdII with suitable nitrogen-containing ligands catalyse the polymerisation of ethene either to (α-alkenes or to high-density polyethene, depending on the type of ligand (25). NiII complexes also polymerise ethyne to either benzene or cyclo-octatetraene.

In the case of hydrosilylation, the use of platinum is probably required in order that an alkene complex of sufficiently great stability can be formed in the presence of bulky -SiR3 ligands.

Alkenes coordinated to nickel and palladium species are susceptible to nucleophilic attack, for example by OH ions. The best-known case of this is the oxidation of ethene by PdII to ethanal (acetaldehyde), or in the presence of ethanoic (acetic) acid to ethenyl ethanoate (vinyl acetate). Here the PdII is reduced to Pd0, and an oxygen-carrying CuII species is needed to complete the catalytic cycle (1, 2).

In heterogeneous catalysis, the clearest proof of the operation of a relativistic effect lies in the reactions of unsaturated hydrocarbons with hydrogen or deuterium. There is a very clear distinction between:

(A) nickel and palladium (and copper) on the one hand, and

(B) platinum (and iridium) on the other, in the following reactions (26):

(i) Reaction of ethene with deuterium, where the A Group metals allow a much greater return of deuterium-substituted alkenes to the gas phase.

(ii) Reactions of C4 or higher alkenes where molecules altered by double-bond migration or E/Z -isomerisation appear in the gas phase to a much greater extent with the A Group than the B Group.

(iii) Hydrogenation of alkynes and alkadienes, for which the A Group metals are more active, and on which they afford the intermediate alkene with much higher selectivity, and preferential Z -addition of hydrogen; with 1,3-butadiene, for example, a high yield of 1-butene is obtained.

All of these observations are consistent with a weaker chemisorption of the alkene compared to that of the alkyne or alkadiene on the A Group metals, as indeed was suspected many years ago (26). These and other features of the reaction have been rationalised by proposing that πσ or π-allylic intermediates occur with the A Group, but σ-diadsorbed intermediates with the B Group. Once again there is a clear correspondence between the findings of organometallic chemistry and homogeneous catalysis and with those of heterogeneous catalysis.

The second point (ii) above also explains why fat-hardening is conducted with nickel (27) or palladium (28) catalysts, but not with platinum. Expressed briefly, a C18 chain containing three non-conjugated C=C bonds has to be hydrogenated so that only one C=C bond is left. This requires first an isomerisation to bring them into conjugation, and then a selective hydrogenation, for which nickel under hydrogen-diffusion-limited conditions is suitable. Palladium is also suitable.

We may also note that ethyne trimerises to benzene on palladium (best on the (111) surface), just as occurs with NiII complexes (29).

Finally we may ask why platinum was the metal of choice for petroleum reforming, since the opening step is dehydrogenation of an alkane, followed by desorption of an alkene and its migration to an acid site. In fact nickel was the metal first used, and recently palladium has found some use, so the answer probably lies in the fact that platinum, in conjunction with tin or rhenium, is much less susceptible to deactivation by carbon deposition than nickel or palladium would be.

Some Final Thoughts

This review has indicated that there are many respects in which the 5d metals (Os, Ir, Pt, Au) differ from the 3d base metals (Fe, Co, Ni, Cu) and the 4d metals (Ru, Rh, Pd, Ag) (30). These differences can be explained in terms of the stabilisation of the 6s level and the destabilisation of the 5d level, compared to the situation in the earlier series, see Figure 2. The origin of this phenomenon is the operation of a relativistic effect on all the s orbitals. Metal catalysts for those reactions involving only σ-bonded alkyl radicals or multiple C=M bonds (equilibration of alkanes with deuterium, alkane hydrogenolysis, etc.) do not show preferential activity related to this effect.

It may be wondered what other aspects of the chemistry of the elements may be traced to this cause. In the bioinorganic field, there is platinosis, but not palladosis; there is the well-known toxicity of many of the heavy elements, but the beneficial use of platinum complexes in chemotherapy (7) (but not so much those of palladium or other metals) and of gold (but not silver) in treating arthritis. It would be surprising if there were not some underlying connection.

So next time you touch gold, or drive a car with a platinum catalyst beneath it, or take your temperature with a mercury-in-glass thermometer do remember: you are now directly in touch with some consequences of the principles that shape the Universe and are determining its evolution.

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The Author

Geoffrey Bond has retired from Brunei University and is Emeritus Professor. He is also Visiting Professor at the University of Salford. His major interests are in metal-catalysed reactions of hydrocarbons, supported oxides and kinetics of catalysed reactions.

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