140912 elbc entek low erstatic.entek.com/140912-elbc_entek-low-er.pdf · 2014. 9. 24. · diffusion...
TRANSCRIPT
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A Continuum of Separator Options for Next Generation Lead‐Acid BatteriesR. Waterhouse, C. La, L. Keith, K. Hanawalt, D. Merritt, D. Walker, J. Moore, C. Rogers, J. Kim, J. Frenzel, M. Warren, J. Norris, D. Trueba, and R.W. Pekala
September 12 , 2014
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Background
ENTEK focused on providing new low resistance separator to EFB/ECL market (start‐stop) without compromising mechanical properties
Explored key characteristics that influence electrical resistance % porosity Wettability Tortuosity
Improvements achieved through modifications to formulation and process conditions
Worked with customers and verified improved battery performance
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Separator ER
Separator resistance is a function of electrolyte resistivity (acid) plus the design, pore structure, and composition of the separator.
Resistance of electrolyte within a porous structure (Ω): R = pLτ2 / P A
Where p = resistivity of the electrolyte, f ([C], T)L = thickness of the separator (design)τ = tortuosity of the pore path (structure)P = porosity filled with acid (structure and composition)A = cross‐sectional area through which ions flow
New product attributes Higher porosity Lower tortuosity Sustained wettability through interface modification(s)
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Electrical resistance ‐‐‐ PALICO measurement
Electrical resistance of a PE separator is traditionally measured using the Palico Low Resistance Measuring System: RSES: the areal resistance of the Separator‐Electrolyte System RPalico: The resistance value in milliohms measured by the Palico instrument
times the area of the aperture (32.26 cm²) RE: The areal resistance of the electrolyte that would occupy the same
volume as the SES 4
V’1 V’2
I
V1 V2
I
R’ = (V’ 1-V’2)/I = R1 + RSES + R2With Separator
R = (V 1-V2)/I = R1 + RE +R2Without Separator
RPalico = (R’ – R) = (RSES – RE)
R1 RSES R2 R1 RE R2
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Separator ER Model
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V2
R SES
The resistivity of the electrolyte‐filled separator can be calculated for various separators from the ER measurement data and the geometry of the rib profile.
Separator schematic with major and minor ribs.The space filled by the acid‐containing separator and the space filled with acid comprise the separator‐electrolyte system (SES).
Rmajor
Relyte,bw
Rbw
Relyte,minor
V1
Rminor
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Pore Structure
The pore structure of PE/silica separator is characterized by its heterogeneity: Hydrophilic silica aggregates of different sizes Hydrophobic polyethylene fibrils Differences in structure between surface (polymer‐rich) and bulk
(silica‐rich) Not all pore volume is filled with electrolyte or stays filled with
electrolyte Total pore volume ≠ acid accessible pore volume
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Constricted Pore
BlindPore
Variety of pores
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SEM ‐‐‐ Bulk Structure
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UHMWPE
Silica Aggregates
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SEM: Surface Structure ‐ Rib Side
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SEM: Surface Structure ‐ Flat Side
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Tortuosity – Electrical Resistance Measurement
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1.00
1.50
2.00
2.0 2.2 2.4 2.6 2.8 3.0
Tort
uosi
ty
SiO2/PE Ratio
Tortuosity vs. SiO2/PE Ratio - 0.25mm BW: Determined from ER Measurement
SiO2/PE Water Porosity Tortuosity2.3 57 1.372.75 60 1.312.9 60 1.28
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Tortuosity – Diffusional Resistance Measurement
Separator samples were boiled in DI water for 10 minutes, and equilibrated at room temperature prior to measurement: Conductivity of the solution in the diffusate compartment was
measured with time for 1 hour
Tortuosity was determined from the measured diffusional resistance.
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Conductivity Probe
Separator
KCl Feed Compartment: C0 = 1.0M
D = 1.9 X 10‐9 m2/sec
Diffusate Compartment
Reference: C. Labbez, et al., Desalination, 141 (2001) p. 291
Cf(t) Cd(t)
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Tortuosity Measurement – Diffusional Resistance
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Diffusion through a membrane separating two compartments:
Slope of the left‐hand‐side of eq. (2) vs. time can be used to calculate the diffusional resistance
C0: initial concentration in the feed compartmentCf(t): concentration of electrolyte in the feed compartment at time tCd(t): concentration of electrolyte in the diffusate compartment at time tA: Separator area exposed to the solutionsV: volume of solution in one compartmentRd: Diffusional resistance of separator
εDτtR
2
d
t: separator thicknessτ : tortuosityD: Diffusivity of soluteε : porosity
ln[(C0-2Cd(t))/C0] vs. Time
-0.06
-0.05
-0.04
-0.03
-0.02
-0.01
0.00
0 500 1000 1500 2000 2500 3000 3500 4000Time (sec.)
ln[(C
0-2C
d(t))
/C0]
Slope = -(2*A)/(V*Rd)
Diffusional resistance is related to tortuosity by:
(1)
ln (2)
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Tortuosity Comparison
Difference between the two methods is 12‐15%: Electrolyte: H2SO4 vs. KCl Concentration: ~ 5M for H2SO4 vs. 1M for KCl
Increasing SiO2/PE ratio from 2.3 to 2.9 only results in a small increase in water porosity and a small decrease in tortuosity.
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1.00
1.50
2.00
2.0 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 3.0
Tort
uosi
ty
SiO2/PE Ratio
Tortuosity vs. SiO2/PE Ratio - 0.25mm BW: Determined from Diffusional and Electrical Resistance Measurement
Diffusional Resistance Electrical Resistance
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How does the new Low Resistance Separator differ from a traditional PE/SiO2 Separator?
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New 2.6
New 2.3
New 2.1
New 1.8
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Low ER separator ‐ Tortuosity
Change in % porosity and pore size distribution leads to lower tortuosity.
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1.00
1.50
2.00
1.7 1.8 1.9 2.0 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 3.0
Tort
uosi
ty
SiO2/PE Ratio
Tortuosity vs. SiO2/PE Ratio: Determined from Diffusional and Electrical Resistance Measurement
Determined from Diffusional Resistance
Determined from Electrical Resistance
Standard Separator
LER SeparatorProduct SiO2/PE
Water Porosity (%)
Tortuosity - Diffusion
Standard Separator 2.3 57 1.63Standard Separator 2.75 60 1.49Standard Separator 2.9 60 1.51
LER Separator 1.8 60 1.30LER Separator 2.6 64 1.35
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Electrical Resistance
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New
New
New
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Initial product Launch ‐ 162‐0.8‐0.25 GE_LR
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‐ 34%
+ 22%+ 21%
+ 13%
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Battery Performance Results
Lower internal resistance: Rbatt decreased by 0.07‐0.16 mΩ
Better Cold Cranking Performance EN U10: increased by 100 to 300mv. EN U30: increased by 60 to 140mv.
Excellent cycle life 50% DOD cycles 17.5% DOD cycles
Low water consumption
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Advanced Development Activities
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MOTIVATION
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1. Low Resistance Separator2. Melt blown polymer fiber mats3. High porosity silica‐filled sheets4. Crosslinked polymer gels
Porosity Range
55%PE/SiO2
Separators
93%AGM
How can we create separators with 60‐90% porosity ?
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Melt‐blown Fiber Technology
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Air In
Polymer Melt In
Attenuated Fiber
Air
Spinning Nozzles
Spinning Nozzles
Air Gap
Bottom View
Sectional View
Air Gap
Orifice
Polymer Melt In
Bottom View Sectional View
1. AGM Substitute2. Extraction‐Free SLI separators
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AGM – BGO Grade
SEM Comparison
Fiber size comparable to AGM can be achieved. Polymer fiber mats exhibit sustained wettability
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Polymer Melt Blown Fiber Mat
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Porosity and Wicking Behavior
Wicking height was determined after 2 minutes in H2SO4, 1.28 SG.
Wicking height varied between 62mm to 72mm: Comparable to the H&V AGM sample –
65mm 23
50
55
60
65
70
75
80
85
90
95
100
1 2 3 4 5
Percen
t Porosity
Lane Number
Run #1 Run #3 Run #4 Run #9
Porosity between 86% and 89% was achieved.0
10
20
30
40
50
60
70
80
1 2 3 4 5Wicking
Height (mm)
Lane Number
Run #1 Run #3 Run #4 Run #9
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Compressibility Behavior
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Melt blown fiber mat and AGM samples had the same initial thickness –about 1.7mm measured at 10kPa, dry.
Melt blown polymer fiber mat demonstrates minimal shrinkage upon wetting, and more compression resistance under stress.
1.00
1.10
1.20
1.30
1.40
1.50
1.60
1.70
1.80
1.90
2.00
0 10 20 30 40 50 60
Fibe
r She
et T
hick
ness
(mm
)
Compressive Stress (KPa)
Melt Blown Fiber Mat: Sheet Thickness vs. Compressive Stress
MBFM, Dry State MBFM, Wet StateAGM, Dry State AGM, Wet State
AGM
Melt Blown Polymer Fiber Mat
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Calendered Sheet
The fiber mats were calendered using one groove roll and one flat roll: Longitudinal rib profile was introduced on the calendered fiber mats Precusor fiber mats were densified more aggressively
75%‐80% densification Final backweb thickness ~ 0.4mm
Preferred thickness is 0.15‐0.25mm
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Rib profile
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Electrical Resistivity
Samples were soaked in H2SO4, 1.28 SG, at room temperature for 20 minutes prior to ER measurement.
Electrical resistance depends on the extent of calendering and the final porosity. The instantaneous wettability in H2SO4 allows the calendered polymer fiber mats to
achieve soaked electrical resistivity that is better than the boiled electrical resistivity of a standard PE/SiO2 separator.
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0
1000
2000
3000
4000
5000
6000
MBFM140407.4
MBFM140421.1
MBFM140421.3
MBFM140421.4
MBFM140421.9
0.25mmStandard PE
Separator
Elec
tric
al R
esis
tivity
(mΩ
-cm
) Boiled ER Value
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Mechanical Properties – BW Puncture
When normalized for backweb thickness, the calendered polymer fiber mats exhibit puncture strength comparable to a PE/SiO2separator
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0
10
20
30
40
50
60
0
5
10
15
20
25
MBFM140407.4
MBFM140421.1
MBFM140421.3
MBFM140421.4
MBFM140421.9
0.25mmStandard PE
Separator
Nor
mal
ized
Pun
ctur
e St
reng
th (N
/mm
)
Punc
ture
Str
engt
h (N
)Puncture Strength Normalized Puncture Strength
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SEM: High OA Silica‐filled Sheets
FG silica‐filled sheet at SiO2/PE=5 has similar porosity with larger amount of PE fibrils that enhance mechanical properties
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TX; SiO2/PE = 10FG; SiO2/PE =5
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0
0.5
1
1.5
2
2.5
3
3.5
4
0.0010.010.1110
Log diffe
rential intrusion
(mL/g)
Pore size diameter (μm)
FG/PE=5
AB/PE=5
TX/PE=10
UK 0.15 mm 2.6 control
Hg Porosimetry ‐ Pore Size Distribution
Highly filled silica sheets show larger pore size distribution and higher tortuosity compared with standard separator 29
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Crosslinked Polymer Gel Formation in Sulfuric Acid
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O
NH2
acrylamideHN
HN
O
H2N
O O
H2N
O
HN
C OC O
H2NO
NH
O
NH
N,N'-methylene-bis-acrylamide
C O
H2N
C O
HN
(NH4)2S2O8+
Lead
10% PA gel in H2SO4
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SEM: Polyacrylamide Gel (Supercritical Drying)
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Cycle Performance
Test conditionCharge rate=1CCut-off voltage in charge= 2.45 VCut-off voltage in discharge= 1.3 V
Cell performance is similar to controls with AGM separator
320
0.02
0.04
0.06
0.08
0.1
0.12
0 10 20 30 40 50 60
Resistance (Ω)
Cycle
0
0.2
0.4
0.6
0.8
1
1.2
1.4
0 10 20 30 40 50 60
Discharge capacity (A
h)
Cycle
PAM009 (10% polymer in prismatic cell )
Prismatic cell assembly
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Summary
Value creation through product and manufacturing innovation is the foundation of ENTEK
ENTEK is working on next generation separators for deep cycle, start‐stop, and high power battery applications
ENTEK would like to work with battery manufacturers on new growth opportunities that could change the way that separators are integrated into Pb‐acid cell designs
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