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15. Energy Applications I: Batteries
What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and
Ralph J. Brodd
Battery types:
Primary Battery: Non reversible chemical reactions (no recharge)
Secondary Battery: Rechargeable
Common characteristics
Electrode
complex coposite of powders of active material and conductive
diluent, polymer matrix to bind the mix
typically 30% porosity, with complex surface throughout the material
allows current production to be uniform in the structure
Current distribution
primary – cell geometry
secondary – production sites within the porous electrode
parameters affecting the secondarycurrent distribution are
conductivity of diluent (matrix)
electrolyte conductivity,
exchange current
diffusion characteristics of reactants and products
total current flow
porosity, pore size, and tortuosisity
What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and
Ralph J. Brodd
We will briefly look at: Lead and Lithium insertion
What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and
Ralph J. Brodd
What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and
Ralph J. Brodd
Require very good conductivity
Throughout the system
Which tends to lower the energy
Content of the system
In the lead acid system a significant amount
Of the weight Is in the grids required
To hold the paste
Equivalent Circuit for a Battery
Terminals, Resistance
To current flow of, RM
External Resistance, Rext
Internal Discharge
Rate (e.t.)
Capacitance of
electrode
Resistance of
electrolyte
ad Acid Battery
Basic requirements for a battery
1. chemical energy stored near the electrode ( if too far away current will
be controlled by time to get to electrode)
2. The chemical form coating the electrode must allow ion transport, or
better yet, electronic conduction
3. The chemical form of the energy must be mechanically robust
4. The chemical form of the energy should generate a large voltage
Fitch lead book Support grids
The capacity of the battery depends on
The type of material present.
PbO e H SO PbSO H
s aq s
2 2 4
2 2
, ,
  



One possible mechanism:. simultaneous dissolution of PbO2 and introduction of 2e
Requires electronic conductivity of PbO2 and pore space for motion of wat
1. Add e, H+ and OH- to PbO2
2. Add 2nd e to reduce valence of Pb
3. Add 3rd e to reduce valence while r
4. PbO is more soluble than PbO2 so
5. Initiate formation of PbSO4, nuclea
6. PbSO4 structure is rhombic which
7. Therefore need to control the alletr
Beta PbO2 is formed under acid and can be compressed to shorten bonds
overlap induces semiconductor behavior which increases the performance
Of the battery
Alpha forms when Pb metal
Corrodes – reduces lifetime of
Battery, is more compressible.
Add antiomony
To drive reaction
To beta phase
Lead Acid battery
a.What is the potential associated with a lead
acid battery with the overall reaction:
at the following concentration:
[H2SO4] = 4.5 M
Pb PbO H HSO PbSO H O
s s aq aq s
   
  

2 4 2
2 2 2 2
, , 
-0.35
Vo
1.69
-(-0.35)
2.04
1.69
PbO H e SO PbSO H O
s aq aq s
2
2
4 2
4 2 2
, ,
   
  
 
PbSO e Pb SO
s s aq
4
2
2
,  



PbO H e SO PbSO H O
s aq aq s
2
2
4 2
4 2 2
, ,
   
  
 
Pb SO PbSO e
s aq s
 
 

2
4 2
,
Pb PbO H HSO PbSO H O
s s aq aq s
   
  

2 4 2
2 2 2 2
, , 
V V
n
Q Q
o
   
00592
2 04
00592
2
.
log .
.
log
Lead Acid battery energy
Pb PbO H HSO PbSO H O
s s aq aq s
   
  

2 4 2
2 2 2 2
, , 
   
     
V Q
PbSO H O
Pb PbO HSO H O
s
s s aq
   




  
2 04
00592
2
2 04
00592
2
4
2
2
2
3
2
.
.
log .
.
log
,
   
V Q
HSO H O
aq
   










 
2 04
0 0592
2
2 04
0 0592
2
1
2
3
2
.
.
log .
.
log
   
V  






2 04
00592
2
1
45 45
2 2
.
.
log
. .
 
V     
2 04 00296 2 6 211
. . . .
c. What is the free energy associated with the
lead acid battery?
   
nFV G RT K
o
 ln
  
G  2 96 485 2 04
, .
G kJ
 3936
.
PbO H SO e PbSO H O
solid aqueous aqueous solid
2 4
2
4 2
4 2 2
, , ,
   
  

Dendrites are
Good: porous (makes more
Of possible energy available)
Bad: fragile, break and fall
from underlying
electrode
= NO CURRENT
e
No e
The type of structure that forms depends upon the rate of crystallization which
Depends upon rate of reaction which depends upon:
Loss/production of products (current)
Which depends also upon the rate constant (potential dependent)
One way to “image” the various processes described above is by an
Equivalent Circuit
In a simplified system
IDisch e
arg
Rext
Rapparent ernal resis ce
int tan IDisch e
arg
 
V I R R
t d ext app
  
0
  
V I R
Disch e D ext
arg 
  
V I R
remaining D app

As the battery is discharged the discharge voltage is the
Difference between what we started with and the remaining
Voltage in the battery
V V I R
Disch e t D App
arg  
0
Lead acid batteries can be valve regulated to control the pressure associated
With
1.29 V
1.38 V
No pressure
pressurized
Lower CT resistance
Under pressure
Suggests higher
Degree of interparticle
Contact under pressure
Insulating layer which can conduct only protons and lead
Solubility
Diffusion
Et at conducting PbO2
Solubility
Diffusion
Et at conducting PbO2
Modeled effect of diffusion
Solubility
Diffusion
Et at conducting PbO2
Modeled effect of proton conc
Solubility
Diffusion
Et at conducting PbO2
Different magnitude of discharge
Changes the solubility and proton conc
As well as the conductivity of the film
IDisch e
arg
Rext
Rapparent ernal resis ce
int tan IDisch e
arg
 
V I R R
t d ext app
  
0
  
V I R
Disch e D ext
arg 
  
V I R
remaining D app

P V I
D D

   
P I R I I R
D ext D D ext
 
2
 
 
P
V R
R R
ext
app ext


0
2
2
 
V
R R
I
t
ext app
d



0
Based on V. S. Bagotsky text, Fundamentals of Electrochemistry
V V I R
Disch e t D App
arg  
0
 
 
P
V R
R R
ext
app ext


0
2
2
0
0.5
1
1.5
2
2.5
0 0.5 1 1.5 2 2.5
Current Density
V
0
0.2
0.4
0.6
0.8
1
1.2
P
For the simplified model
Monitor structural changes at electrode as a function of the discharge power
High charge transfer
Resistance due to insulating
PbSO4 layer
Charge transfer resistance
Decreases due formation of more porous PbO2
Small diameter
Of impedance
Circle here indic
The fast et kine
O2 reaction.
Increasing
Charge transfer
Resistance due
To layer of PbSO4
Reaction Vo
Li++e Li -3.0
K+ + e K -2.95
Na+ + e Na -2.71
NCl3_4H+ + 6e 3Cl- + NH4
+ -1.37
2H2O + 2e H2 + 2OH- -0.828
Fe2+ + 2e Fe -0.44
Pb2+ + 2e Pb -0.13
2H+ + 2e H2(gas) 0
N2(g) + 8H+ + 6e 2NH4
+ 0.275
Cu2+ + 2e Cu 0.34
O2 + 2H2O + 4e 4OH- 0.40
O2 + 2H+ + 2e H2O2 0.68
Ag+ + e Ag 0.799
NO3
- + 4H+ + 3e NO(g) +2H2O 0.957
Br2 + 2e 2Br- 1.09
2NO3
- + 12H+ + 10e N2(g) +6H2O 1.246
Cl2
+ 2e 2Cl- 1.36
Au+ + e Au 1.83
F2 + 2e 2F- 2.87
7g/mol
207g/mol
Lithium oxidation proceeds a little too
uncontrollably
Lithium reduction does not not result
in good attachment back to the lithium
metal
Forms dendrites which can grow to
Short circuit
C e Li LiC
6 6
1
  

Lithium intercalated in graphite is close
to metallic, formal potential differs by
only 0.1 to .3 V = -2.7 to -2.9V
Anode –
Solid electroactive metal salt
(Can change overall charge so that it can electrostatically stabilize & localize Li+
Potential should be very positive (far from -2.5 V for Li/C reaction
Solid should conduct charge throughout
Solid should allow ion motion
Should have fast kinetics (open and porous)
Should be stable (does not convert to alleotropes)
Low cost
Environmentally benign
   
M X M X e
x
m
z
x
x
m
z
x
  


 

1
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
   
 
M X Li M X Li
x
m
z
x
x
m
z
x
fast
     



   

 
   
M X Li M X Li e
x
m
z
x
x
m
z
x
fast
     



  
 
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
LiTiS2 LiVSe2 LiCoO2
LiNiO2
Group I
Group II
V O
2 5 MoO3
Group III
Spinels
Mn O
2 4
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
LiTiS2
Smooth galvanostatic curve indicates
That there are no sites nucleating
Alleotropes of the compound.
Allotropes would alter the structure,
Porosity, and the ease of intercalation,
Potential, and conductivity
Went to market
In the late 1970s
Single phase
Light weight
Conducting, but not
Reactive (oxidised or reduced)
Li ion intercalates in response to double layer charging
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
LiVSe2
Indicates various crystal forms
V Se xLi xe Li V Se
IV
x
IV x
2 2
  
 
   
Li V Se x Li x e LiV Se
x
IV x III
 
    
2 2
1 1
LiV Se Li e Li V Se
III II
2 2 2
  

Lithium ion inserts in response
To reduction of vanadium
Different phases of VSe2 have similar structures
So the distortion is not great
octahedral
2nd is tetrahedral
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
Group II
V O
2 5 MoO3
Major phase changes in LixV2O5
 (x<0.01) is well ordered
Є ( 0.35<x<0.7)is more puckered
 (x=1) shifting of layers
 (x>1) results in permanent structural change
ω (x>>1) is a rock salt form
Sol gel processes of the V2O5 materials
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301
Group III
Spinels
Mn O
2 4
These materials have a major change in
Unit cell dimensions when Mn changes
Oxidation state (see B). Need to keep the
Lattice parameter less than 8.23 A for good
Cycling, which
1. Keeps Mn in higher oxidation state,
therefore
less soluble
2. Prevents distortion in the coordination of
oxygen (Jahn-Teller)
around the manganese. These distortions
will alter the oxidation and
reduction potential as seen in the next slide
M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301

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15. Energy Applications II. Batteries.ppt

  • 1. 15. Energy Applications I: Batteries
  • 2. What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and Ralph J. Brodd Battery types: Primary Battery: Non reversible chemical reactions (no recharge) Secondary Battery: Rechargeable Common characteristics Electrode complex coposite of powders of active material and conductive diluent, polymer matrix to bind the mix typically 30% porosity, with complex surface throughout the material allows current production to be uniform in the structure Current distribution primary – cell geometry secondary – production sites within the porous electrode parameters affecting the secondarycurrent distribution are conductivity of diluent (matrix) electrolyte conductivity, exchange current diffusion characteristics of reactants and products total current flow porosity, pore size, and tortuosisity
  • 3. What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and Ralph J. Brodd We will briefly look at: Lead and Lithium insertion
  • 4. What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and Ralph J. Brodd
  • 5. What are Batteries, Fuel Cells, and Supercapacitors, Chem Rev, 2004, 104, 4245, Martin Winter and Ralph J. Brodd Require very good conductivity Throughout the system Which tends to lower the energy Content of the system In the lead acid system a significant amount Of the weight Is in the grids required To hold the paste
  • 6. Equivalent Circuit for a Battery Terminals, Resistance To current flow of, RM External Resistance, Rext Internal Discharge Rate (e.t.) Capacitance of electrode Resistance of electrolyte
  • 7.
  • 8. ad Acid Battery Basic requirements for a battery 1. chemical energy stored near the electrode ( if too far away current will be controlled by time to get to electrode) 2. The chemical form coating the electrode must allow ion transport, or better yet, electronic conduction 3. The chemical form of the energy must be mechanically robust 4. The chemical form of the energy should generate a large voltage
  • 9. Fitch lead book Support grids The capacity of the battery depends on The type of material present.
  • 10. PbO e H SO PbSO H s aq s 2 2 4 2 2 , ,       One possible mechanism:. simultaneous dissolution of PbO2 and introduction of 2e Requires electronic conductivity of PbO2 and pore space for motion of wat 1. Add e, H+ and OH- to PbO2 2. Add 2nd e to reduce valence of Pb 3. Add 3rd e to reduce valence while r 4. PbO is more soluble than PbO2 so 5. Initiate formation of PbSO4, nuclea 6. PbSO4 structure is rhombic which 7. Therefore need to control the alletr
  • 11. Beta PbO2 is formed under acid and can be compressed to shorten bonds overlap induces semiconductor behavior which increases the performance Of the battery Alpha forms when Pb metal Corrodes – reduces lifetime of Battery, is more compressible. Add antiomony To drive reaction To beta phase
  • 12. Lead Acid battery a.What is the potential associated with a lead acid battery with the overall reaction: at the following concentration: [H2SO4] = 4.5 M Pb PbO H HSO PbSO H O s s aq aq s         2 4 2 2 2 2 2 , , 
  • 13. -0.35 Vo 1.69 -(-0.35) 2.04 1.69 PbO H e SO PbSO H O s aq aq s 2 2 4 2 4 2 2 , ,          PbSO e Pb SO s s aq 4 2 2 ,      PbO H e SO PbSO H O s aq aq s 2 2 4 2 4 2 2 , ,          Pb SO PbSO e s aq s      2 4 2 , Pb PbO H HSO PbSO H O s s aq aq s         2 4 2 2 2 2 2 , ,  V V n Q Q o     00592 2 04 00592 2 . log . . log
  • 14. Lead Acid battery energy Pb PbO H HSO PbSO H O s s aq aq s         2 4 2 2 2 2 2 , ,            V Q PbSO H O Pb PbO HSO H O s s s aq            2 04 00592 2 2 04 00592 2 4 2 2 2 3 2 . . log . . log ,     V Q HSO H O aq                 2 04 0 0592 2 2 04 0 0592 2 1 2 3 2 . . log . . log     V         2 04 00592 2 1 45 45 2 2 . . log . .   V      2 04 00296 2 6 211 . . . .
  • 15. c. What is the free energy associated with the lead acid battery?     nFV G RT K o  ln    G  2 96 485 2 04 , . G kJ  3936 .
  • 16. PbO H SO e PbSO H O solid aqueous aqueous solid 2 4 2 4 2 4 2 2 , , ,         Dendrites are Good: porous (makes more Of possible energy available) Bad: fragile, break and fall from underlying electrode = NO CURRENT e No e
  • 17. The type of structure that forms depends upon the rate of crystallization which Depends upon rate of reaction which depends upon: Loss/production of products (current) Which depends also upon the rate constant (potential dependent)
  • 18. One way to “image” the various processes described above is by an Equivalent Circuit
  • 19. In a simplified system IDisch e arg Rext Rapparent ernal resis ce int tan IDisch e arg   V I R R t d ext app    0    V I R Disch e D ext arg     V I R remaining D app  As the battery is discharged the discharge voltage is the Difference between what we started with and the remaining Voltage in the battery V V I R Disch e t D App arg   0
  • 20. Lead acid batteries can be valve regulated to control the pressure associated With 1.29 V 1.38 V No pressure pressurized Lower CT resistance Under pressure Suggests higher Degree of interparticle Contact under pressure
  • 21. Insulating layer which can conduct only protons and lead Solubility Diffusion Et at conducting PbO2
  • 22. Solubility Diffusion Et at conducting PbO2 Modeled effect of diffusion
  • 23. Solubility Diffusion Et at conducting PbO2 Modeled effect of proton conc
  • 24. Solubility Diffusion Et at conducting PbO2 Different magnitude of discharge Changes the solubility and proton conc As well as the conductivity of the film
  • 25.
  • 26.
  • 27. IDisch e arg Rext Rapparent ernal resis ce int tan IDisch e arg   V I R R t d ext app    0    V I R Disch e D ext arg     V I R remaining D app  P V I D D      P I R I I R D ext D D ext   2     P V R R R ext app ext   0 2 2   V R R I t ext app d    0 Based on V. S. Bagotsky text, Fundamentals of Electrochemistry
  • 28. V V I R Disch e t D App arg   0     P V R R R ext app ext   0 2 2 0 0.5 1 1.5 2 2.5 0 0.5 1 1.5 2 2.5 Current Density V 0 0.2 0.4 0.6 0.8 1 1.2 P For the simplified model
  • 29. Monitor structural changes at electrode as a function of the discharge power
  • 30. High charge transfer Resistance due to insulating PbSO4 layer Charge transfer resistance Decreases due formation of more porous PbO2 Small diameter Of impedance Circle here indic The fast et kine O2 reaction. Increasing Charge transfer Resistance due To layer of PbSO4
  • 31. Reaction Vo Li++e Li -3.0 K+ + e K -2.95 Na+ + e Na -2.71 NCl3_4H+ + 6e 3Cl- + NH4 + -1.37 2H2O + 2e H2 + 2OH- -0.828 Fe2+ + 2e Fe -0.44 Pb2+ + 2e Pb -0.13 2H+ + 2e H2(gas) 0 N2(g) + 8H+ + 6e 2NH4 + 0.275 Cu2+ + 2e Cu 0.34 O2 + 2H2O + 4e 4OH- 0.40 O2 + 2H+ + 2e H2O2 0.68 Ag+ + e Ag 0.799 NO3 - + 4H+ + 3e NO(g) +2H2O 0.957 Br2 + 2e 2Br- 1.09 2NO3 - + 12H+ + 10e N2(g) +6H2O 1.246 Cl2 + 2e 2Cl- 1.36 Au+ + e Au 1.83 F2 + 2e 2F- 2.87 7g/mol 207g/mol
  • 32.
  • 33. Lithium oxidation proceeds a little too uncontrollably Lithium reduction does not not result in good attachment back to the lithium metal Forms dendrites which can grow to Short circuit C e Li LiC 6 6 1     Lithium intercalated in graphite is close to metallic, formal potential differs by only 0.1 to .3 V = -2.7 to -2.9V
  • 34. Anode – Solid electroactive metal salt (Can change overall charge so that it can electrostatically stabilize & localize Li+ Potential should be very positive (far from -2.5 V for Li/C reaction Solid should conduct charge throughout Solid should allow ion motion Should have fast kinetics (open and porous) Should be stable (does not convert to alleotropes) Low cost Environmentally benign     M X M X e x m z x x m z x         1 M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301       M X Li M X Li x m z x x m z x fast                     M X Li M X Li e x m z x x m z x fast              
  • 35. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301 LiTiS2 LiVSe2 LiCoO2 LiNiO2 Group I Group II V O 2 5 MoO3 Group III Spinels Mn O 2 4
  • 36. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301 LiTiS2 Smooth galvanostatic curve indicates That there are no sites nucleating Alleotropes of the compound. Allotropes would alter the structure, Porosity, and the ease of intercalation, Potential, and conductivity Went to market In the late 1970s Single phase Light weight Conducting, but not Reactive (oxidised or reduced) Li ion intercalates in response to double layer charging
  • 37. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301 LiVSe2 Indicates various crystal forms V Se xLi xe Li V Se IV x IV x 2 2          Li V Se x Li x e LiV Se x IV x III        2 2 1 1 LiV Se Li e Li V Se III II 2 2 2     Lithium ion inserts in response To reduction of vanadium Different phases of VSe2 have similar structures So the distortion is not great octahedral 2nd is tetrahedral
  • 38. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301 Group II V O 2 5 MoO3
  • 39. Major phase changes in LixV2O5  (x<0.01) is well ordered Є ( 0.35<x<0.7)is more puckered  (x=1) shifting of layers  (x>1) results in permanent structural change ω (x>>1) is a rock salt form
  • 40. Sol gel processes of the V2O5 materials
  • 41. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301 Group III Spinels Mn O 2 4 These materials have a major change in Unit cell dimensions when Mn changes Oxidation state (see B). Need to keep the Lattice parameter less than 8.23 A for good Cycling, which 1. Keeps Mn in higher oxidation state, therefore less soluble 2. Prevents distortion in the coordination of oxygen (Jahn-Teller) around the manganese. These distortions will alter the oxidation and reduction potential as seen in the next slide
  • 42. M. Stanley Whittingham, Lithium Batteries and Cathode Materials, Chem. Rev. 2004, 104, 4271-4301