bonding to surfaces two classifications distinguished by the magnitude of their enthalpies of...
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Bonding to surfaces
Two classifications distinguished by the magnitude of their enthalpies of adsorption
Physisorption: long-range but weak van der Waals-type interactions with negligible exchange of electrons and enthalpies~Hcond (-HAD<35 kJ/mol)
Chemisorption: formation of a chemical bond (covalent, ionic, metallic) with exchange of electrons and –HAD>35 kJ/mol
Enthalpy of chemisorption depends strongly on surface coverage (interactions)
Spectroscopic techniques (see later) are used to confirm chemisorption
(IR or XPS for example)
Adsorption kinetics
Probability of molecule being associatively adsorbed may defined in terms of a sticking probability, s.
(Z) surface with themolecules ofcollison of rate
surface by the molecules of adsorption of rates
We can write: )1(0 ss
Thus the greater the number of vacant sites, the greater is s.
However, s is often not a linear function of θ. Invoke the precursor state
Precursor stateIf adsorbate collides with the surface and doesn’t stick, it may not simply rebound, but rather form a weak bond (physisorption) and diffuse for a period (losing energy) until a vacant site is located for chemisorption to occur. If the weak bond is initially at a vacant site one refers to intrinsic precursor states, whereas if it is at an occupied site this corresponds to extrinsic precursor states.
For adsorption to proceed, the gas needs to “dump” energy into the solid, if not it will desorb. The longer the gas molecule resides on the surface, the more likely is energy exchange with the surface. Can write an Arrhenius-type relationship between residence time and the enthalpy of adsorption at the precursor adsorption site. See p.11 Attard & Barnes
Lennard-Jones Potentialphysisorption
z
pote
ntia
l en e
rgy
ads < 35 kJmol-1
attractive van der Waals interactions
repulsive Coulombic interactionsPauli repulsion
ads
0
Potential energy profiles
Not activated Activated
Potential energy profilesFor an introduction to PE curves for adsorption see section 2.4 of:
http://www.chem.qmw.ac.uk/surfaces/scc/
MO diagram for chemisorption
1s 1s
σ*
σ
σ* orbitalsσ orbitals
Metal Adsorbed molecule Free molecule
PHYSISORPTION CHEMISORPTION
WEAK, LONG RANGE BONDING
Van der Waals interactions (e.g. London dispersion, dipole-dipole)..
STRONG, SHORT RANGE BONDING
Chemical bonding involving orbital overlap and charge transfer.
NOT SURFACE SPECIFIC
Physisorption takes place between all molecules on any surface providing the
temperature is low enough.
SURFACE SPECIFIC
E.g. Chemisorption of hydrogen takes place on transition metals but not on gold or mercury.
ads = 5 ….. 35 kJ mol-1 ads = 35 ….. 500 kJ mol-1
Non activated with equilibrium achieved relatively quickly. Increasing temperature
always reduces surface coverage.
Can be activated, in which case equilibrium can be slow and increasing temperature can
favour adsorption.
No surface reactions. Surface reactions may take place:- Dissociation, reconstruction, catalysis.
MULTILAYER ADSORPTION
BET Isotherm used to model adsorption equilibrium.
MONOLAYER ADSORPTION
Langmuir Isotherm used to model adsorption equilibrium..
Adsorption and Reaction at Surfaces
Surface structure
Surface defects
Surface science
In order to ensure reproducible results between experiments precise definition of the chemical and structural state of the surface: well-defined surfaces required.
Review 2nd and 3rd year lectures from D. Cunningham on naming crystal and solid structures
Overview
bcc body-centred cubic
fcc face-centred cubic
hcphexagonal close
packed
Close-packed solids
ABA ABC
Close-packed solids
hcp ccp (fcc)
bcc
http://www.chem.qmw.ac.uk/surfaces/scc/
Miller indices
Miller indicesIdentify the intercepts on the x- , y- and z- axes
x = a (at the point (a,0,0) )parallel to the y- and z-axes
Intercepts : a , ,
Specify the intercepts in fractional co-ordinates In the case of a cubic unit cell each co-ordinate will
simply be divided by the cubic cell constant a a/a , /a, /a i.e. 1 , ,
Take the reciprocals of the fractional intercepts yielding
Miller Indices : (100)
Try these
And this
Miller indicesAtkins & dePaula p. 700
fcc (100)
Rotate 45o
CN=8 for surface layer (12 for bulk)
http://www.chem.qmw.ac.uk/surfaces/scc/
fcc(110)
Rotate 45o
CN=7 for surface layer (12 for bulk)
http://www.chem.qmw.ac.uk/surfaces/scc/
fcc(111)
Rotate 45o
CN=9 for surface layer (12 for bulk)
http://www.chem.qmw.ac.uk/surfaces/scc/
Surface energetics
• The most stable solid surfaces are those with :
a high surface atom density
surface atoms of high coordination number
expect
fcc (111) > fcc (100) > fcc (110)
Intersection of surfaces
Surface relaxation
Surface relaxation
Surface reconstruction