PHY563 – 10/02/2021
PHY 563 – Tutorial on Batteries
Jean-François Guillemoles
Nathanaelle Schneider
UMR-IPVF 9006 - CNRS
PHY563 – 10/02/2021
Publication
2
General questions:
- Which type of publication is it?
- How important/relevant is the journal? the article?
Specific questions:
- What is the field?
- What are the main claims of the paper?
- Which methods and materials? Preparation (principle, pro/cons)
and Characterization (principle, ex-/in-situ, what is observed)
- What is new since the publication of the article?
PHY563 – 10/02/2021
Publication
Impact factor = 41,845 (2019)
cited 8135 times (Google scholar on 08/02/2021)
22
General questions:
PHY563 – 10/02/2021
Publication
22
Specific questions:
- What is the field?
PHY563 – 10/02/2021
Outline
What is the field? What are the main claims of the paper?
Main tackled issue
New electrode material
New mechanism (nano effect), what are the classical mechanism?
Which methods and materials? Preparation (principle, pro/cons) and
Characterization (principle, ex-/in-situ, what is observed)
Setups Voltage-composition profiles In-situ XRD TEM/SAED XANES
•Back-up slides
5PHY563 – 10/02/2021
Setups
• Give and explain a schematic representation of classical
mecanisms « Li insertion/desinsertion » and « Li-alloiyng
process »
•Reported mechanism
PHY563 – 10/02/2021
Li-metal
Tarascon, cours Collège de France (2011)
Li-metal > negative electrode = metal Li
J. Rouxel
Reactions during discharge:
Cathode / Reduction : TiS2 + e- + Li+ TiLiS 2
e-PHY563 – 10/02/2021
20 µm
Cu
Electrolyte
M. Dolle, L. Sannier, B. Beaudoin, M. Trentin, J.-M. Tarascon, Electrochem. Solid State Lett., 5 (12), A286, (2002)
PHY563 – 10/02/2021 Tarascon, cours Collège de France (2011)
Li-ion: electrodes = Li
+intercalation compounds
anode
cathode
PHY563 – 10/02/2021
+
LiC6 C6 Li+ LiCoO2 Li1-xCoO2 LiC6 C6 Li P F6 EC -DMC e -Li+ e -Graphite Li1-xCoO2 Carbone SP Liant-From P. Poizot, LRCS
Li-ion
PHY563 – 10/02/2021 Tarascon, cours Collège de France (2011)
Li-ion: which electrode materials?
PHY563 – 10/02/2021
Li-ion : exploration of electrode materials
PHY563 – 10/02/2021
13
Conclusions
NATURE | VOL 407 | 28 SEPTEMBER 2000 | www.nature.com
Impact?
Critics?
PHY563 – 10/02/2021
EC methods
14
Principle?
In-situ? Ex situ?
What is observed? What is evidenced?
NATURE | VOL 407 | 28 SEPTEMBER 2000 | www.nature.com
Mesure voltage– composition:
Experimental method Evaluation of curves Specific capacity
PHY563 – 10/02/2021
XRD= X-Ray Diffraction
15
Diffraction – Braggs’s law
d = spacing between diffracting planes
Θ = incident angle n = integer
λ = beam wavelength (1,54A)
Peak height : proportional to the number of incident electron, to the size and number of crystallites
Peak position: depends on the type and the parameter of the primitive cell ( + constraints in the material) Peak width : depends on internal micro-constraints and the size of the crystalline coherence
Principle?
In-situ? Ex situ?
PHY563 – 10/02/2021
Structure identification: XRD
16 (200) (220) (111) (311)Exemple: XRD zinc-blende structure
- Cubic face-centered- Two atoms per primitive cell A (0,0,0) B (¼, ¼, ¼)
PHY563 – 10/02/2021
XRD
172Θ
Θ
Bragg-BrentanoCubic: (1/d
hkl)² = (h²+k²+l²)/a²
Preferential orientation: (111)
d
111= λ/(2 sinθ) = a√3 = 3.12 Å
a = 1.80 Å
samplePHY563 – 10/02/2021 Secondary electrons: Low energy Superficial layers > Topology Back-scattered electrons: High energy Atomic number sensitive > Chemical homogeneity Auger electrons: Very low energy
> Surface, Chemical bounds X-rays Low energy Superficial layers > Atomic composition, (EDX analysis)
PHY563 – 10/02/2021
TEM/SAED
19
Electronic Microscopy:
TEM (Transmission Electron Microscopy)
and SEAD (Selected Area Electron Diffraction)
NATURE | VOL 407 | 28 SEPTEMBER 2000 | www.nature.com
Principle
PHY563 – 10/02/2021
TEM
20
Electronic Microscopy:
TEM (Transmission Electron Microscopy)
and SEAD (Selected Area Electron Diffraction)
TEM
• Transmitted electrons
• High vacuum system (10-4 Pa) to increase electron mean free path
SAED
• Crystallographic technique that can be performed inside TEM
• Atoms act as diffraction grating to the electrons
• Similar to XRD but smaller samples can be analysed (100 nm vs. cm)
PHY563 – 10/02/2021
SEM
21
Scanning Electron Microscopy: SEM
• Resolution : nm scale
• Conditions: vacuum, ambient T, pre-treatments
• Ex: insulating part (charged) appears bright and conducting part appears dark
PHY563 – 10/02/2021
XANES/EXAFS
XANES (X-ray Absorption Near-Edge Spectroscopy) and EXAFS
(Extended X-ray Absorption Fine Structure)
• Source = synchrotron light
• XANES : electronic state, oxidation state
• EXAFS = oscillations : chemical environment, neighboring atoms (nature, number)
PHY563 – 10/02/2021
Synchrotron tools
• Powerful tunable
light source
From IR to hard X
Rays
•Based on accelerated
charged particles
23 Soleil@SaclayPHY563 – 10/02/2021
24
XANES, EXAFS
XANES (X-ray Absorption Near-Edge Spectroscopy) and EXAFS
(Extended X-ray Absorption Fine Structure)
• Excitation source = synchrotron light
• XANES (or NEXAFS) : sensitive to electronic transitions within atoms => electronic state, oxidation state
• EXAFS = oscillations due to interferences with neighboring atoms (of a given atom)=> chemical environment, neighboring atoms (nature, number). Distribution of neighbors requires mathematical fitting
PHY563 – 10/02/2021
25
Size effect
NATURE | VOL 407 | 28 SEPTEMBER 2000 | www.nature.com
IPVF Academic joint Lab UMR
IPVF Academic joint Lab UMR
Lithium batteries
Tarascon, cours Collège de France (2011)
>
Small ionic radius
rapid diffusion >> Power
>
Works in aqueous medium
>> Thermodynamic limit at
1.2 V
>
Lightest metal (6.9g), d= 0.53g.cm
-3>
Most electropositive element
>> ΔE 3 – 4V
>
High chemical reactivity (water)
>> Organic electrolytes (non aqueous)
Highest
energy mass
density
IPVF Academic joint Lab UMR
Lithium batteries
IPVF Academic joint Lab UMR
Li-metal
Tarascon, cours Collège de France (2011)
Li-metal > negative electrode = metal Li
J. Rouxel
Décharge:
TiS2 + e- + Li+ TiLiS 2
e-IPVF Academic joint Lab UMR
Li-polymer
Tarascon, cours Collège de France (2011)
Li-polymer: Li-metal + polymer electrolyte
(flexibilité polymère)
IPVF Academic joint Lab UMR
Li-polymer: Electrolytes
(+) non volatils, Li-metal compatible, low cost, reinforced cells (-) low ionic conductivity (working T 70-80°C)
Polymère gélifié à ilots d’électrolyte liquide
HPE = Hybrid Polymer Electrolyte cryst.: Mechanical stability amorph.: Liquid electrolyte Structured polymer membrane SPE =
Solid Polymer Electrolyte
P(VDF-HFP)- based membrane
IPVF Academic joint Lab UMR Tarascon, cours Collège de France (2011)
Li-ion: electrodes = Li
+intercalation compounds
anode
cathode
IPVF Academic joint Lab UMR
Li-ion
IPVF Academic joint Lab UMR Tarascon, cours Collège de France (2011)
Li-ion: which electrode materials?
No elements being:
Dangerous
Expensive
Heavy
Rare earth
Noble
gases
IPVF Academic joint Lab UMR
IPVF Academic joint Lab UMR
LiMnO2/LiCoO2 : 10% less capacity
advantage : cost & green
to achieve higher capacities : design materials in which the metal-redox oxidation state can change reversibly by 2 units :
Mn+2/Mn
Preserving frame work structure
Molecular masses similar to 3d metal-layer oxides (ex : LiMnO2 or LiCoO2)
Not W, Mo ou Nb : heavy
V-based oxides L3V2O5-Li3V3O8
Cr6+/Cr3+
LiMnO2 : structural instability upon cycling : substitution by Cr : Li1+X Mn0.5Cr0,5O2
Capacity : 190 mAhg-1
Mn : stabilize the layered structure
Cr : large capacity due to oxidation state that changes from +3 to +6 But Cr : presents major toxicity & pricing issues
IPVF Academic joint Lab UMR
Li2MnO3
LiCoO2 LiNi1/2Mn1/2O2
LiNi1/3Mn1/3Co1/3O2 Chosen to be the next generation of + electrode material in lithium-ion batteries
Li(
Co
1-xLi
x/3Mn
2x/3)O
2 (5)Li(
Ni
x/2Li
(1/3 -x/3 )Mn
(2 /3 -x/6))O
2 (4 )Li(Co
1-xNi
x/2Mn
x/2)O
2 (1,2,3)(4) Z.H. Lu, D.D. MacNeil, and J.R. Dahn, ESSL., 4(11), A191 (2001)
(5) K. Numata, C. Sakaki and S. Yamanaka, Solid State Ionics, 117, 257 (1999) (1) Y. Makimura and T. Ohzuku, J. Power Sources, 119, 156 (2003)
(2) N. Yabuuchi and T. Ohzuku, J. Power Sources, 119, 171 (2003) (3) Z.H. Lu, D.D. MacNeil, and J.R. Dahn, ESSL., 4(12), A200 (2001)
The Li(Co1-xNix/2Mnx/2)O2 systems :
High capacity
High cycleability
Larger safety (vs. LiCoO2)
Lower cost (vs. LiCoO2)
The Li(Co1-xNix/2Mnx/2)O2 systems :
High capacity
High cycleability
Larger safety (vs. LiCoO2)
Lower cost (vs. LiCoO2)
IPVF Academic joint Lab UMR 50 75 100 125 150 175 200 0 10 20 30 40 50 Cycle Number Q (mAh/g) LiCoO2 3.5-4.25V, 0.5C, 25°C LiNi1/3Co1/3Mn1/3O2 3.0-4.3V, 0.5C, 25°C LiNi1/3Co1/3Mn1/3O2 3.0-4.5V, 0.5C, 25°C LiNi1/3Co1/3Mn1/3O2 3.0-4.7V, 0.5C, 25°C
Q
(mA h/ g) LiCoO2 - 4.3 V Li (Co.33Ni.33Mn.33)O2 – 4.3 V Li (Co.33Ni.33Mn.33) O2 – 4.5 V 4. 7 VDischarge capacity (mAh)
0.2 C
2 C
Li (Co.33Ni.33Mn.33) O2
94% retained capacity at 2C
(design not optimized for high power applications)
Excellent capacity retention up to 4.5-4.6V
Reversible capacity of 170mAh/g at 4.5V
Technical Data Cellcore® MX- Kindly provide by UMICORE
IPVF Academic joint Lab UMR
a
b
(001)
Structure olivine
J. Goodenough and K. Padhi, 1996
Cheap, safe
FeO6 LiOPO64 FeO6Triphylite
Low electronic and ionic conductivitiesFrom P. Poizot, LRCS
Li-ion: LiFePO
4
Coating + nanostructuration : cœur-courrone
strategy
IPVF Academic joint Lab UMR
Li-ion: LiFePO
4
– carbon coating
C. Wurm; C. Masquelier – LRCS, Amiens
15% de carbone
C coating LiFePO4 0,1 1 10 0 20 40 60 80 100 120 140 160 0.04 0.2 0.4 2 4 20 RT 55 C Capaci ty (m A h /g) Rate (C) 40IPVF Academic joint Lab UMR
Li-ion: LiFePO
4
– nanstructuration
500 nm
50 nm 0 10 20 30 40 50 60 70 80 90 100 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 0 2 4 6 8 10 12 14 16 18 nm % %Taille des particules (nm)
0 20 40 60 80 100 120 140 160 1.8 2.0 2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8 4.0 4.2 4.4 4.6 4.8 1-10 1 2-10
Capacité Spécifique mAhg
- 1Poten
ti
el
Li
+vs.
Li (V)
C. Delacourt, P. Poizot et al. , Electrochem Solid State Lett 9(7) A352-55(2006).
LRCS-Umicore Patent (2006)
IPVF Academic joint Lab UMR
Li-ion: Nanostructuration
IPVF Academic joint Lab UMR