Energetics of Nanomaterials and Zeolites Alexandra Navrotsky UC Davis.
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Transcript of Energetics of Nanomaterials and Zeolites Alexandra Navrotsky UC Davis.
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Energetics of Nanomaterials Energetics of Nanomaterials
and Zeolitesand Zeolites
Alexandra Navrotsky
UC Davis
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Control of Polymorphism Control of Polymorphism at the Nanoscaleat the Nanoscale
Competition between polymorphism and surface energy
Free energy crossovers as function of sizeMore metastable polymorphs have lower
surface energies in general
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0
4
8
12
16
0 4000 8000 12000
Surface area (m2/mol)
En
thalp
y (
kJ/m
ol)
0 50 100 150
Surface area (m2/g)
brookiterutile
anatase
Enthalpy of titania polymorphs as a function of surface area (8).
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Energetics of Nanocrystalline Zirconia
0
20
40
60
80
100
120
140
0 10000 20000 30000 40000 50000
Surface area measured (m2/mol)
H w
.r.t
. bu
lk m
-ZrO
2(k
J/m
ol)
monoclinic
tetragonal
amorphous
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ZEOLITES: NANOMATERIALS WITH INTERNAL SURFACES
• Many different framework types, all of enthalpy 8 - 14 kJ/mol above quartz
• Molar volume changes by a factor of two because of large internal pores and channels
• Internal surfaces generated by pores, can be modeled using Cerius2 software
• Can one define a physically meaningful surface energy from slope of trend between enthalpy and internal surface area?
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7.20
10.90
9.30
11.40
10.50
13.60
6.60
13.90
8.20
6.80
8.70
0.00
y = 0.6992x - 17.5 R
2 = 0.7147
0
4
8
12
16
25 30 35 40 45 50
Molar Volume (cm 3 /mol)
H
tra
ns (
kJ
/mo
l)
quartz
MTW
MFI
FER
MEL
AFI
AST
BEA
CHA
EMT
FAU
MEI
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Surface Energy of 40 nm Particle
Material Enthalpy relative to bulk(kJ/mol)
__________________________________________
Silicalite 0.5
Corundum 10
-alumina 6.5
Rutile 6.2
Brookite 3.1
Anatase 1.2
Low value of surface energy (internal and external) may be what allows many open polymorphs, the manganese oxides may be a test case.
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2 4 6 8 10 12 14 16 18 20 22 24 26 280
4
8
12
16
20
24
28
32
Ent
halp
y of
for
mat
ion
rela
tive
to q
uart
z (k
J/m
ol)
Pore size (nm)
Enthalpies of formation of pure-silica mesoporous materials relative to quartz as a function of pore size. represents SBA-15 and MCM-41 materials (Trofymluk et al. 2005); - MCM-48 and SBA-16 materials; - MCM-41 (Navrotsky et al. 1995) - MCM-41 materials from Lee, B. MS thesis 2003, UC Davis
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ChallengesChallengesof Hydrationof Hydration
Detailed structural rearrangements at surface and in frameworks related to degree of hydration
Energetics Is hydration a major driving force or
a by-product? Which is the tail, which the dog?
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Hydration control of growth
• High energy surface sites have highest heats of hydration, hold on to water
• Hydrated surface layers for enhanced reactivity, less hydration and more order as particle grows, e.g. apatite
• Hydrophilic-hydrophobic competition
• Control of shape
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Scanning heat flow curves of a zeolite synthesis mixture (5.15Na2O-1.00Al2O3-
3.28SiO2- 165H2O at a
constant heating rate of 0.10 ºC/min in a Setaram C-80 heat flux microcalorimeter. Repeated in situ experiments were performed and stopped at the selected temperatures denoted by capital letters. Apparent peaks below 30 oC are artifacts. Peaks between 40 and 70 oC represent several steps of gel formation
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Crystal Growth from Nanoclusters
• Attachment of nanoclusters, rather than atoms or molecules, to growing crystal
• Elimination of surface area and eentually of surface-adsorbed species
• Classical nucleation and growth not applicable
• Ostwald step rule rationalized
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Insight into Zeolite Growth Mechanisms
Alexandra Navrotsky
University of California at Davis, DMR-01-01391
A
B
C D
E
F
Increase of pH in solution
Increase of surface charge density
Vessel set used inin situ calorimetry
Teflon liner
Stainless steel vessel
Synthesis mixture
Exo Endo
Tim
e
Cal
orim
etri
c cu
rve
Framework structure of MFI zeolite
Schematic representation of zeolite crystal growth by aggregation of the pre-assembled nano-precursor particles from exothermic stage to endothermic stage.
Zeolites are widely used in ion exchange, Catalysis and separation because of theirUniform cages and channels of nanometerDimension. Design of zeolite materials forApplications demands a detailed under-Standing of zeolite formation mechanisms.
Here we demonstrate that in situ calorimetry reveals a two-stage crystallization process for MFI-type zeolite
Chem. Mater. 14, 2803 (2002)
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polymorph
nanoparticles
bulk phases
metastable polymorph
stable polymorph
species in solution or melt
nanoclusterscritical nucleus or cluster for assembly
.
Particle radius
Fre
e en
ergy
(sc
hem
atic
)
nanoparticlesnanoparticles
bulk phasesbulk phases
metastable polymorph
stable polymorph
species in solution or melt
nanoclusterscritical nucleus or cluster for assembly
.
Particle radius
Fre
e en
ergy
(sc
hem
atic
)
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• Control of polymorphism• Selection of hydrous precursors with low surface energy• Storage, transport and attachment of nanoparticles rather than of individual ions• Specific surface-protein interactions• Non-classical reinterpretation of nucleation, growth, Ostwald step rule
Nanoparticles andBiomineralization
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Other Possible Advantages of Nanoparticles
• Efficient concentration and storage of precursors, including sparingly soluble materials
• Tethering of particles to active sites
• Membrane transport
• Detox
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Synthesis of Silver ThiolatesSynthesis of Silver Thiolates
Atul Parikh et al 1999
AgS CH3
R-SH (sol)+Ag NO3(sol) → R-S Ag (solid)+HNO3(sol)
Self-assembled monolayersSelf-assembled monolayers
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6 8 10 12 14 16 18 20
20
25
30
35
a, Å
number of carbons
Micellar (columnar) mesophase
Structure of silver thiolates. Structure of silver thiolates. Phase transitions.Temperature-Phase transitions.Temperature-dependent XRDdependent XRD
ainterlayer d-spacing
16 20 24 28 32 3625
30
35
40
45
50
55
d = 8.14+1.21*(2N)
inte
rlaye
r d-
spa
cing
, Å
2(N-1)
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Phase Transitions in Silver Thiolates. DSC Phase Transitions in Silver Thiolates. DSC datadata
H, kJ/moln
9 130.5±0.5 35.3±0.5 86.2±1.0
11 131.1±0.3 39.3±2.7 97.2±6.2
15 131.0±0.5 53.7±1.2 132.9±3.8
T, °C S, J/K mol
17 131.1±0.3 58.8±2.2 145.5±7.5
0 50 100 150 200
20
40
60
Ent
halp
y, k
J/m
ol
Entropy, J/K mol
hydrocarbons
8 10 12 14 16 18 200
20
40
60
80
Ent
halp
y, k
J/m
ol
Number of carbons
8 10 12 14 16 18 2040
80
120
160
Ent
ropy
, J/K
mol
Number of carbons
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6 8 10 12 14 16 18 20
0
-20
-40
-60
-80
-100
melting
solution in toluene
En
tha
lpy,
kJ/
mo
l
Number of carbons
0 20 40 60 80 100 120 140
0
1
2
3
4
5
Hea
t flo
w, a
r.un
.
Time, min
0 10 20 30 40 50 60 70-1
0
1
2
3
4
5
0 2 4 6 8 10 12 14 16 18 20-50
-100
-150
-200
-250
R2 = 0.98
Ent
halp
y, k
J/m
ol
Number of carbons
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ConclusionsConclusions
Silver thiolates and zeolites both explore spatial confinement
The former show much stronger “tethering”
Both show enthalpy-entropy compensation