Electrolytes for lithium batteries and fuel cells · Polymer Battery at NASA Glenn Research Center....
Transcript of Electrolytes for lithium batteries and fuel cells · Polymer Battery at NASA Glenn Research Center....
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Electrolytes for lithium batteries and fuel cells
http://www.pa.msu.edu/~duxbury/CND/CND.html
January 24th : Jim McCusker (Chemistry - MSU), "Photochemical control of charge transfer complexes for improved solar cells"
January 31st : Keith Promislow (Mathematics - MSU), "The role of nanomorphology in proton conduction through polymer electrolytes"
February 7th : Greg Baker (Chemistry - MSU), "Materials for Fuel Cells"
February 14th : Don Morelli (Materials Science - MSU), "Introduction to high ZT thermoelectric materials and their applications"
February 21st : Special Energy Seminar : Wolfgang Bauer (Physics, MSU) Is bio-gas generation a cost-effective option for the Michigan energy economy?
February 28th : Phillip Duxbury (Physics - MSU) "Theoretical and practical limits on solar conversion efficiency : Why use nanostructured materials?"
Center for Nanomaterials Design and Assembly
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Organic (ion-conducting) membranes in energy applications
Li ion batteriessolar cells
supercapacitors
CO2 sequestration
CO2CH4
Fuel cells
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Rechargeable Batteries
High reactivity with solvents used for electrolytes -only polyethersare compatible with Li metal
Tarascon, J. M.; Armand, M., 2001, 414, (6861), 359-367
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"Rocking Chair" batteries (Lithium Ion Cells)
applications: laptops, cell phones, power tools,
Tarascon, J. M.; Armand, M., 2001, 414, (6861), 359-367
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Making batteries is as simple as baking ...
Tarascon, J. M.; Armand, M., 2001, 414, (6861), 359-367
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Properties of real lithium batteries
DOE Workshop on Basic Research Needs For Electrical Energy Storage, 2007, http://www.sc.doe.gov/bes/reports/abstracts.html
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Advanced batteries
A prototype Lithium-Ion Polymer Battery at NASA Glenn Research Center.
LiCoO2 (Sony)
C-Li(x)
Anode Cathode
Li+
Li+
LiMn2O4 (Bellcore/Telcordia)
Current technology:•liquid electrolyte or gel electrolyte (liquid dispersed in a PVDF gel, allows flat packaging, rather than metal cans).•Li+PF6 or similar salt•mixtures (usually) of ethylene carbonate, dimethylcarbonate, diethyl carbonate
O O
O
H3CO OCH3
O
OO
O
ethylene carbonate
diethyl carbonate
dimethyl carbonate
LiFePO4 (A123 systems)
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Flambeau de laptop ...
X-W Zhang, Y. Li, S. A. Khan, P. S. Fedkiw, J. Electrochem. Soc., 2004, 151, A1257-A1263.
Lithium dendrites
Li(1-x)CoO2C-Li(x)
Anode Cathode
LiMn2O4
liquid or polymer electrolyte(flammable! organic )
•over charging leads to dendrite formation
•excessive dendrite growth leads to a short
•a short leads to heat, venting, fire, .......
http://www.theinquirer.net/en/inquirer/news/2006/06/21/dell-laptop-explodes-at-japanese-conference
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The moral of the story ....
"....... the theoretical specific energy of a lithium thionyl chloride battery is on the order of 1420 Wh/L, which is comparable to the theoretical specific energy of TNT at 1922 Wh/L."
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The moral of the story ....
"....... the theoretical specific energy of a lithium thionyl chloride battery is on the order of 1420 Wh/L, which is comparable to the theoretical specific energy of TNT at 1922 Wh/L."
Li(1-x)CoO2C-Li(x)
Anode Cathode
Li+
Li+
passivating layers (SEI)
Solvent Electrode Interface:•ionic conductor, electrical insulator•mechanically robust through repeated cycling•inhibit dendrite formation
most organic solvents are inherently unstable to high oxidation and reduction potentials at cathode and anode, small molecule easily transported to electrodes
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BASIC RESEARCH NEEDS FOR ELECTRICAL ENERGY STORAGE(DOE Workshop, 2007, http://www.sc.doe.gov/bes/reports/abstracts.html)
suggests polymer-based, ionic liquid, or other solutions
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BASIC RESEARCH NEEDS FOR ELECTRICAL ENERGY STORAGE(DOE Workshop, 2007, http://www.sc.doe.gov/bes/reports/abstracts.html)
suggests polymer-based, ionic liquid, or other solutions
a partial wish list ...inherent safetystable, reproducible passivating layersinfinite cyclinghigh capacitylow temperature performance
could be solved via immobile (polymer) electrolytesinherent kinetic stability
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1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
2.4 2.6 2.8 3.0 3.2 3.4
1000/T (1/K)
σ (S
/cm
)
Tm
σ = n • q • µ
Ion-conduction in polyethers
•dissolves Li salts well
•ion mobility correlated with segmental motion of the PEO chain
•crystallinity limits the conductivity below 60 °C
CH2CH2On
# of charge carriers
charge/carrier
mobility
O
OO O
O
O
OO O
O
OO
O
O
Li+
τ
O O
OO
O
O
O
O O
O
OO
O
OLi+
O
OO
O
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Structures designed to limit crystallinity
•“blocky” polymers
•branched copolymers
•network polymers
Additives designed to limit crystallinity
•polymer blends
•polymer-filler composites
Limited success (10-4-10-5 S/cm @ room temperature, vs. 10-1 -10-5S/cm for liquids
Typical Approaches to Enhance Conductivity
1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
2.4 2.6 2.8 3.0 3.2 3.4
1000/T (1/K)σ
(S/c
m)
Tm
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V
s
V
s
M+
ions diffusing in a uniform potential - weak coupling limit
ion hopping: - strong coupling
highest mobility
M+chaperone approach
(a compromise)
screening layer
Idealized ion transport
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"coupled" systems
σ and E derived from a single material
"de-coupled" systems
σ and E derived from separate components
composite systems -inert fillers + electrolyte
bicontinuous block copolymers
low molar mass electrolytes + inert separator
PEO/salt complexes
inorganic oxides and glasses
classifying electrolytes systems by function (mechanical, σ)
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"coupled" systems
σ and E derived from a single material
"de-coupled" systems
σ and E derived from separate components
composite systems -inert fillers + electrolyte
bicontinuous block copolymers
low molar mass electrolytes + inert separator
PEO/salt complexes
inorganic oxides and glasses
vacancy-based diffusion, thermally activated (high T)
transport coupled to chain mobility
classifying electrolytes systems by function (mechanical, σ)
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"coupled" systems
σ and E derived from a single material
"de-coupled" systems
σ and E derived from separate components
composite systems -inert fillers + electrolyte
bicontinuous block copolymers
low molar mass electrolytes + inert separator
PEO/salt complexes
inorganic oxides and glasses
current technology has safety issues, stuck with "canned" batteriesto be displaced by ionic liquids?
advantages for manufacture providing the morphology can be controlled. - but will the electrolyte be a liquid (high σ, but safety issues) or a polymer (low σ)
*high molecular weight and cross-linked polymers are kinetically stable - no transport to the electrode surface
classifying electrolytes systems by function (mechanical, σ
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Bicontinuous phase approach to electrolytes
hydrophobic
Ion conducting matrix (hydrophilic)
• conducting phase, high σ
• network structure, mechanical stability
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Si ClClCl
Cl
flame
(H2O)SiO2 n
•irregularly shaped particles
•20-100 nm in diameter
•SiOH surface groups
•aggregate in liquids and form gels
Applications:
•thickening agents for paints, coatings, cosmetics, ...
•moisture control in powders
Bicontinuous phase approach to electrolytes
hydrophobic Ion conducting matrix (hydrophilic)
• conducting phase, high σ
• network structure, mechanical stability
250 nm
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V is c
o si ty
Staticperiod Shearing Static
period
Time
Driving force:
aggregates
3-D aggregates
rest
shear
primary particles
agglomerated network
phase separationH-bonding (SiOH surfaces)van der Waals (alkyl-terminated)
Thickening & Thixotropy
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•fumed silica provides reversible structure formation
•low molecular weight PEO/Li salt provides good conductivity
•both properties can be optimized independently to give highly conductive electrolytes that can easily be processed.
Strategy:
CH3O CH2CH2O CH3
PEGDME 500
n
LiClO4 or Li imide
hydrophobic fumedsilica (R805)
Particle-based Li+ conductors
PEGDME-500LiClO4
temporary silica network
PEGDME-500LiClO4
cross-linked silica network
Fumed Silica (R805) weight %
0 5 10 15 20 25
RT C
onductivity σ298Κ (S
/cm)
10-4
10-3
Ela
stic
Mod
ulus
, G' (
Pa)
103
104
105
106
G'
PEG-DM, Li Imide
σ298K
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+OH
OH
OH
OHOH
OH
OH
OH
4:1silica
1:1
OH
O
O
SiOOH
O
O
SiO
OC
O
C
CH2
CH3
+
OSiRO
ORRO
O
SiRO
ORRO
Preparation of Modified Silicas
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0
10
20
30
40
50
60
70
80
90
100
110
0 5 10 15 20 25 30
Irradiation Time, (min)
Con
vers
ion,
%
C=C
C=O
•Irradiate with medium pressure Hg lamp at 30 °C
•Follow loss of C=C and shift of C=O
conductivity cell cross-section
electrolyte
SS electrode
Teflon
Hg lamp
Photocuring of Composites
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1.0E-04
1.0E-03
1.0E-02
2.75 2.95 3.15 3.35
1000/T (K)
Con
duct
ivity
(S/c
m)
BMA before UV
OMA before UV
MMA before UV
PEO-500
1.0E-04
1.0E-03
1.0E-02
2.75 2.95 3.15 3.35
1000/T (K)
Con
duct
ivity
(S/c
m)
BMA after UV
OMA after UV
MMA after UV
Conductivities Before and After Curing
•Difference in initial conductivities reflect solubility of monomer•Same final σ implies no polymer in electrolyte phase
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1.00E-04
1.00E-03
0.5 1 1.5solubility parameter (δPEO - δmethacrylate)
σ (S
/cm
)
before UVafter UV
methylbutyl
octyl
Conductivity of composites related to mis-match in solubility parameters.
Supports phase separation model.
PEGDME-500, cross-linkable fumed silica LiClO4
Effect of Added Monomer: a viscosity effect
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solution: immobilize anions
Transference number
( ) 1
iti i
t t
++
+ −
+ −
=+
+ =∑
t+ = the fraction of current carried by a charge species
Single-ion Conductors Prepared from SulfonimidesImmobilized on Fumed Silica Nanoparticles
For common binary salts:LiClO4,LiN(SO2CF3)2 (LiTFSI), ..t+ ~0.2-0.4
X-
X-
X-X-
X-
X-
X-X-X-
X-
X- X-
X-
X-X-
X-
X-X-
Li+
Li+
Li+
Li+
anions part of a rigid solid (low σ)
Design issues: single component, but must
optimize transport and tether ions at the
same time
Polarization – decreased cell performance
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Composite electrolytes: 2-component solutions to electrolyte design
X XX X XX
XXXXX3-d network structure, high tLi
+
Ion-exchanged clays
low molecular weight PEO
Li+X-
Network formation
Improved mechanical properties
σ unchangedhydrophobic particles
X
XX
XX
X
“massive” relative to Li+, µ ~ 0 hydrophilic particles
dispersed in PEO
For an overview see: Electrochimica Acta 2003 48, 2071-2077
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Approaches
Particles with a monolayer of anions tethered to the surface
Particles with polymer tethers decorated with multiple anions/chain
(increased carrier concentration, easily 10X)
monolayer of anions
anions bound to polymers grown from the surface
σ = n • q • µ
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OHtriethyl amine
CHCl3, TsClOTs
1) potassium phtalimide, DMF, 80%
2) H2NNH2.H2O, EtOH, 60°C3) HCl, EtOH, reflux, 52%
NH2
(CF3SO2)2O
Et3N, CH2Cl2NH
Tf (EtO)3SiH
Pt(0), benzeneNH
Tf(EtO)3Si
OHOHOH
HN S
CF3O
O(EtO)3Si
1) diethyl amine
2) nBuLi, toluene
OOO
Si N-S
CF3O
OLi+
Fumed Silica
Ts = p-toluene sulfonyl
Tf = trifluoromethane sulfonyl
98%
58%
Synthetic route to tethered Li imides
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•Li+ concentrations:–40 wt% ≈ O:Li = 250–35 wt% ≈ O:Li = 310–30 wt% ≈ O:Li = 390–19 wt% ≈ O:Li = 710
Conductivity data
At 40 and 50 wt% - poor ionic conductivity discontinuous polymer matrix
At 10 & 15 wt % - σ<10-8 S/cm(few charge carriers)
Data for PEO/LiClO4/hydrophobic fumed silica
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Li+
Li+Li+
Li+Li+
Li+
Li+
Li+
Li+
Li+Li+
High weight loading
Low weight loading
nanoparticles PEO
15 20 25 30 35 401E-9
1E-8
1E-7
1E-6
1E-5
1E-4
σ (S
/cm
)
A200-C5NTfLi weight fraction (%)
Connectivity issues
Poor connectivity
non-continuous conducting phase
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• σ < 10-8 S/cm for 10, 15 and 50 wt% particles in PEGDME500/.– For 10, and 15 wt%, low lithium concentrations.
(O/Li > 1000)– For 50 wt%, discontinuity of the polymer phase.
• Weak dependence on temperature
Interim conclusions
Need more charge carriers!
monolayer of anions anions bound to
polymers grown from the surface
Particles with polymer tethers decorated with multiple anions/chain have increased carrier concentrations, easily a 10X increase.
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• Increase number of anions on silica nano-particles
OH
OH
OH
O
OH
Cl
Si
OCl
Si CuCl2, dNbipy
2. MeLi
ClCl
Si
O
OH
Si
OSi
Cln
SO3- Li+
Cln
SO3- Li+
O
OH
Si
OSi
Cln
Cl
n
1. SO3
Growth of polymer tethers from particle surfaces
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0
20
40
60
80
100
100 200 300 400 500 600 700
temperature ( 0C )
wei
ght %
particles after sulfonationparticles after surface initiated polymerizationparticles with initiator monolayer
Thermal gravimetric analysis of modified nanoparticles
Weight loss data can be analyzed to estimate the number of functional groups on the surface.
Cleaving chains from surface with HF would give molecular weight.
2.3 mmol/g (titration)
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-7
-6
-5
-4
2.8 2.9 3.0 3.1 3.2 3.3 3.4
1000/T
log
σ
20 wt% particles (2.3 mmol/g)
10 wt% particles (2.3 mmol/g)26 wt% A200 (0.23 mmol/g)
Li+ conductivity of nanoparticles in PEG-DME 350
10 fold increase in conductivity
>10-5 even for aryl sulfonates
single layer of immobilized anions
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BASIC RESEARCH NEEDS FOR ELECTRICAL ENERGY STORAGE(DOE Workshop, 2007, http://www.sc.doe.gov/bes/reports/abstracts.html)
Cross-Cutting Science: technology challenges
Liquid electrolytes• Provide the needed high conductivity for electrochemical capacitors
but can have safety and containment issues.• Have voltage windows that limit the device performance range.• Contain electrolyte impurities that lead to degradation in performance.Electrolytes can be the weak link limiting innovations in electrode
materials, and associated power and power density.
Need new electrolytes with high ionic conductivity, low fluidity, easily purified.
Low nucleophilicity and electrophilicity - unreactive in both electron transfer and acid-base chemistry.
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BASIC RESEARCH NEEDS FOR ELECTRICAL ENERGY STORAGE(DOE Workshop, 2007, http://www.sc.doe.gov/bes/reports/abstracts.html)
Cross-Cutting Science: technology challenges
"Solid" electrolytes• Difficult to combine the electrolyte and electrode separator functions in
a single material. • Modeling provides a recipe for high conductivity - polymers with low
glass transition temperatures - but low Tg polymers have poor mechanical properties.
• Two-phase materials provide a partial solution - favorable mechanical properties, but with the electrochemical characteristics and problems of low molecular weight liquid electrolytes ( electrolyte decomposition, flammability, ...).
New approaches to electrolyte design are needed that go beyond incremental improvements.
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• Establish design rules that define the relationship between electrolyte structure and performance, including ion mobility, electrochemical stability new concepts for electrolytes.
• Precisely define the double layer and interaction of electrolyte and solvent at electrode surfaces. Create self healing/self regulating electrolytes for the electrode/electrolyte interface.
• Expand the range of weakly coordinating anions (BARF, carboranes, dicationic ionic liquids, ions linked by electronically conducting segments ) to broaden the spectrum of electrolytes available forbatteries and capacitors.
• Investigate electrochemical phenomena in molten salts establish electrolytes with high conductivities, stabilities, and wide potential windows.
• Establish the thermodynamic properties of electrolytes.
Cross-Cutting Science: Electrolytes for Energy Storage
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Solid electrolytes• Nanoparticle composites that exploit the interstitial
space in ensembles of high surface area nanoparticles and provide conductive channels for ion transport.
• Design smart materials that respond that moderate temperature excursions within batteries, polymer layers that selectively remove lithium dendrites, or restore conductive pathways in composite electrode structures - potentially dramatic improvement in device reliability, lifetime, and safety.
Cross-Cutting Science: basic-science challenges, opportunities
M+
anode
cathode
"dendrite mower"
V
M+
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Fuel Cells
http://www.epa.gov
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Fuel cell issues
Costs. Platinum (1 mg/cm²) and membrane costs. Nafion®membranes are ~$400/m²!
Water management (in PEMFCs).
too little water: dry membranes, increased resistance, failure by cracking, creating a gas "short circuit" where hydrogen and oxygen combine directly, generating heat that damages the fuel cell.
too much water: electrodes flood, preventing the reactants from reaching the catalyst.
Fuel and oxygen flow control.
Temperature management.
Limited carbon monoxide tolerance of the anode.
Advantages of high temperature operation:
• Reduce CO poisoning effect on electrode catalyst.
• Enhance reaction kinetic at higher temperature.
• Simplify water management.
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Nafion, the prototype PEM
Perfluorinated polyethylene backbone affords chemical and mechanical stability; sulfonic groups attached on side chains provides mobile protons when hydrated.
Hickner, M. A.; Pivoar, B. S.; Fuel Cells, 2005, 5, 213-229Hickner, M. A.; Pivoar, B. S.; Fuel Cells 2005, 5, 213. Hsu, W. Y.; Gierke, T. D.; J. Membr. Sci. 1983, 13, 307. Mauritz, K. A.; Moore, R. B.; Chem. Rev. 2004, 104, 4535.
Limitations:
•Cost. ~$400/m2
•Poor high temperature performance (80-90 °C)
•Low conductivity at low humidity or high temperature
•CH3OH permeability
CF2 CF2 CF2CFa b
OCF2 CF
CF3
O(CF2)2 SO3H
n
Ionic clusterchannel
• Chemically stable• Mechanically stable• High conductivity
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"Diat tubes"
Rubatat, L.; Gebel, G.; Diat, O., Macromolecules 2004, 37, (20), 7772-7783.
1 µm x 1µm
AFM image of Nafion at RT, 30% relative humidity
Nafion "tube" structure inferred from scattering data
SO3H
SO3H
SO3H HO3S
HO3S
HO3S
HO3SSO3H
SO3H
H OH
HOH
HO H
end view
CF2 CF2 CF2CFa b
OCF2 CF
CF3
O(CF2)2 SO3H
n
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Commercial alternatives to NafionSulfonated ESI (Dais-Analytic)
Commercial Dow Insight product, 30-60% sulfonation
85 °C max temp (Tm of polyethylene crystallites)
Polybenzimidazole (Celanese Ventures) with Honda, PlugPower
Sulfonated PEEK (Vitrex/Ballard)
N
HN
NH
N
n
Polybenzimidazole ( PBI )
PBI soaked with 11M H3PO4 showed conductivity of 0.02 S/cm at 130 °C, 0.3 atmosphere water vapor pressure.
150-190 °C maximum, CO tolerant
* CH2 CH CH2 CH2 *
SO3H
x 1-x n
O
OO*
*
n
HO3S
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The bicontinuous phase structure is an analog of the cluster-network model (Nafion)
Hydrophobic polymer
Hydrophilic network
Schmidt-Rohr, K.; Chen, Q., Nat. Mater. 2008, 7, 75-83.
Nafion model from neutron scattering
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More Nafion alternatives
Nafion’s bicontinuous structureYang, Y. S.; Shi, Z. Q.; Holdcroft, S., Macromolecules 2004, 37, (5), 1678-1681.
Faure S, Cornet N, Gebel G, Mercier R, Pineri M, Silicon B. Proceedings of Second International Symposium on New Materials for Fuel Cell and Modern Battery Systems, Montreal, Canada, July 6-10, 1997. P. 818.
NN O
O
O O
O
NO
N O
O
OO
O
x y
SO3H
HO3S
Random incorporation of sulfonic acid groups causes uncontrolled swelling in H2O
Distribution as blocks (a la Nafion) controls swelling
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Khan, A. S.; Baker, G. L.; Colson, S.; Chem. Mater, 1994, 6, 2359-2363
hydrophobic silicahydrophobic matrix (mechanical stability)
invert
Hydrophobic particles (alkyl terminated) dispersed in a hydrophilic ion-conducting electrolyte.
Network formation enhances mechanical properties with insignificant effects on conductivity
Hydrophilic particles (sulfonic acid terminated) dispersed in a hydrophobic matrix (PVDF).
Dimensionally stable hydrophobic polymer provides mechanical stability and is uninvolved in transport
hydrophilic silica(ion conducting)
Ion conducting matrix
Particle in polymer approach
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Particles with polystyrene brushes
OSi
Cln
SO3H
SiO2
Composite membranes made from poly(styrene sulfonic acid) grown from nano-sized silica surface and PVDF:
+ PVDF
Nano sized particle provides high surface areaHomogeneous membranes, comparable conductivity compared to Nafion. de-coupled mechanical properties from proton transportEasy solution to swelling issues.
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+
PVDF in DMFParticles in DMF Combined mixture, stirred overnight at room temperature
Mixtures were cast on glass slide and dried at ~50 oC Cast membrane
Membrane fabrication
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Particle content vs conductivity
Measurements taken at room temperature, 100% relative humidity
The conductivity data suggest a percolation threshold at ~20% particle content.
0.00001
0.0001
0.001
0.01
0.1
1
0 10 20 30 40 50 60
Particle content ( wt%)
Con
duct
ivity
(S/c
m)
Nafion 117 measured under the same conditions: 0.08 S/cm
Need to push the particle content to lower loadings while maintaining conductivity.
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Membrane conductivity vs. temperature
Membranes were soaked with 8M H3PO4,
measurements were taken under 0.3 atmosphere pressure humidity
0
0.2
0.4
0.6
0.8
1
1.2
1.4
80 90 100 110 120 130 140
Temperature 0C
σ (S
/cm
)
50%40%30%
30% particles
40% particles
50% particles
Compatible with high temperatures
Still need to push the particle content to lower loadings
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Qin YuanFadi AsfourPing LiuMica StoweJun HouSaad Khan & Peter Fedkiw (NC State)
Financial SupportDepartment of Energy, Basic Energy SciencesMSU IRGP (Keith Promislow)
Acknowledgements