Magnetic Moments
Magnetic moments are often used in conjunction with electronic
spectra to gain information about the oxidation state and
stereochemistry of the central metal ion in coordination
complexes.
(Determination of the magnetic moment using the
Gouy method has been simplified by the
use of an on-line template or spreadsheet.)
For first row transition metal ions in the free ion state, ie
isolated ions in a vacuum, all 5 of the 3d orbitals are
degenerate.
In octahedral complexes, a simple crystal field theory approach suggests
that for these ions the d orbitals are no longer degenerate but are split
such that 2 orbitals, the dx2-y2 and the dz2 are at higher energy than the
dxy, dxz, dyz.
For ions with between 4 and 7 d electrons, this gives rise to 2
possible arrangements called either high spin-low spin or weak
field-strong field respectively. See an interactive JAVA script for examples.
In tetrahedral complexes the orbitals are again split, such that
2 orbitals (the dx2-y2 and the dz2) are now at lower energy than
the remaining 3.
Tetrahedral complexes are ALL high spin since
the difference between the 2 subsets of orbitals is much smaller
than is found in octahedral complexes
(Δtet= 4/9 Δoct).
The formulae most frequently used to calculate magnetic moments
of first row transition metal ion complexes are given
below:
The first formula is known as the spin only formula, the second
takes into account possible contributions from orbital angular
momentum and the third is used to make small adjustments when the
ground term for the metal ion is either A or E.
Where:
S is the spin quantum number = 1/2 for each unpaired electron
L is the orbital angular momentum
α is a constant = 2 for E and 4 for A ground terms
λ is the spin orbit coupling constant
Δ is the crystal field splitting parameter found from the spectrum
of the complex.
To illustrate:
predict the variation of the magnetic moments for the series of
tetrahedral complexes Copyr2Cl2,
Copyr2Br2 and Copyr2I2.
Their visible spectra have been recorded in chloroform
and from the centre of their main absorption bands in the visible
region, ν (in wavenumbers cm-1) can be seen to be roughly:
1 Copyr2Cl2 16260 cm-1 (615 nm)
2 Copyr2Br2 15870 cm-1 (630 nm)
3 Copyr2I2 14925 cm-1 (670 nm)
These peaks represent the third electronic transition expected for these
complexes, the other bands occurring in the infrared region, so
although we may be able to place the halides into order of the
spectrochemical series, we need to consult an Orgel diagram
before trying to calculate Δ.
The Orgel diagram appropriate for these types of complexes is
given below:
oct d3,d8 tet d2,d7
←-----------------------------------→
oct d2,d7 tet d3,d8
and for d7 tetrahedral the ground term is
4A2.
Three peaks are predicted in their electronic spectra,
namely:
4T2 ← 4A2 ν1
4T1(F) ← 4A2 ν2
4T1(P) ← 4A2 ν3 ** the band observed in the visible region
The energy of the third transitions is approximately
ν3 = 6/5 Δ + 15B (where B is the Racah parameter and
ignoring configuration interactions). For Co(II)
tetrahedral complexes B has generally been found to be about 750
cm-1.
Hence Δ for the three complexes above can be
calculated to be roughly, Δ = (ν3 - 15x750) x 5/6, or:
Copyr2Cl2 (16260-15x750) x 5/6 = 4175 cm-1
Copyr2Br2 (15870-15x750) x 5/6 = 3850 cm-1
Copyr2I2 (14925-15x750) x 5/6 = 3063 cm-1
For three unpaired electrons the spin only magnetic moment is predicted to be 3.87 BM.
Using a value for the free ion spin orbit coupling constant
(λ) of -172 cm-1 then a better
approximation of the magnetic moment can be obtained by using
the third formula above. This would give a value of:
Copyr2Cl2 3.87*(1+ 688/4175) = 4.49 B.M. found 4.42 BM
Copyr2Br2 3.87*(1+ 688/3850) = 4.57 B.M. found 4.50 BM
Copyr2I2 3.87*(1+ 688/3063) = 4.76 B.M. found 4.48 BM
In the case of the series;
CoI42-, CoBr42-, CoCl42-, Co(NCS)42-
the magnetic moments have been recorded as
4.77, 4.65, 4.59, 4.40 BM
showing even more clearly the inverse effect of the
spectrochemical series on the magnetic moment.
return to the CHEM2101 (C21J) course
outline
Copyright © 1995-2010 by Robert John
Lancashire, all rights reserved.
Created and maintained by Prof. Robert J.
Lancashire,
The Department of Chemistry, University of the West Indies,
Mona Campus, Kingston 7, Jamaica.
Created Dec 1995. Links checked and/or last modified
12th October 2010.
URL
http://wwwchem.uwimona.edu.jm/spectra/MagMoment.html