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V.B.12 Developing Materials for Lithium-Sulfur Batteries (ORNL)<br />

Liang – ORNL<br />

Capacity (mAh g -1 )<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

Charge, pore volume 2.35<br />

Discharge, pore volume 2.35<br />

Charge, pore volume 1.12<br />

Discharge, pore volume 1.12<br />

Pore volume 2.35<br />

0<br />

5 10 15<br />

0<br />

20<br />

Cycle Number<br />

Figure V - 65: Cycling performance <strong>of</strong> S/C composites with 50% sulfur<br />

loading. Carbon hosts have pore volumes <strong>of</strong> 2.35 and 1.12 cm 3 /g. Surface<br />

areas are ~ 800 m 2 /g for both materials. Capacity is normalized by the sulfur<br />

alone.<br />

Electrolyte Additives. To overcome the corrosion<br />

problem associated with the LiBr additive, a number <strong>of</strong><br />

alternative compounds have been investigated. Organic<br />

alternatives include benzoquinone,<br />

Tetracyanoquinodimethane (TCNQ), and 2,3-Dichloro­<br />

5,6-dicyano-1,4-benzoquinone (DDQ). These compounds<br />

have electrochemical redox potentials between 2.5 and 3.9<br />

V. However, the chemical compatibility <strong>of</strong> benzoquinone<br />

and TCNQ with bare lithium anode is a problem. DDQ has<br />

better chemical stability with lithium metal. It was found<br />

that using DDQ as the additive [5% in tetraglyme] reduces<br />

the capacity <strong>of</strong> S by half. The possible reason for this<br />

unexpected capacity loss could be the polymerization <strong>of</strong><br />

DDQ at high concentration. The resulting polymer coats<br />

the carbon electrode surface and compromises the<br />

electrochemical performance <strong>of</strong> the cathode. When the<br />

concentration <strong>of</strong> DDQ was reduced to 1%, the<br />

electrochemical performance was improved comparing<br />

with the 5% DDQ in tetraglyme. Inorganic alternatives to<br />

LiBr were also investigated. Promising results were<br />

obtained when a phosphorous sulfide additive was used in<br />

the cell. As shown in Figure V - 66a, the charge/discharge<br />

curves have plateaus close to the ideal curves. The cell has<br />

a good retention <strong>of</strong> capacity at 0.1 C rate. The cut-<strong>of</strong>f cell<br />

voltage has been set to 1.9 V because the additive can be<br />

reduced at the cathode when the discharge voltage is below<br />

1.9 V. The stability <strong>of</strong> this phosphorous sulfide additive is<br />

still under investigation. The mechanism <strong>of</strong> how the<br />

additive works will be studied in future experiments.<br />

Protection <strong>of</strong> Lithium Anode. To protect lithium<br />

from reacting with the sulfur species, a novel anode made<br />

<strong>of</strong> metal lithium with a pre-formed solid electrolyte<br />

interphase (SEI) on its surface was designed and<br />

implemented in the Li-S batteries. The tenet <strong>of</strong> the design<br />

is to have an ionic conductor covering the surface <strong>of</strong><br />

lithium metal, thereby impeding surface reaction <strong>of</strong> lithium<br />

with polysulfide.<br />

Lithium thiophosphate salts were chosen to form the<br />

100 SEI. Lithium thiophosphates are fast Li ion conductors.<br />

Their ionic conductivity ranges from 10 -6 to 10 -3 S/cm<br />

80<br />

depending on the composition. It was found that Li 2 S x ­<br />

60<br />

P 2 S 5 can react with lithium metal to form a solid<br />

electrolyte <strong>of</strong> lithium thiophosphate at the surface <strong>of</strong><br />

40 lithium metal. This solid electrolyte conducts lithium ions<br />

while it blocks the access <strong>of</strong> polysulfide to the lithium.<br />

20 Because the polysulfide shuttle phenomenon is more<br />

Coulombic Efficiency (%)<br />

severe at low cycling rates than at high rates, the cell was<br />

intentionally cycled at a low rate <strong>of</strong> 0.1 C to demonstrate<br />

the protection <strong>of</strong> lithium metal through this solid<br />

electrolyte coating. Shown in Figure V - 67a is the voltage<br />

pr<strong>of</strong>ile <strong>of</strong> the first cycle. The discharge curve has two<br />

plateaus at 2.4 and 2.0 V, corresponding to the reduction <strong>of</strong><br />

long chain polysulfides (sulfur atoms greater than 4) and<br />

short chain polysulfides (sulfur atoms less than 4),<br />

respectively. The ratio <strong>of</strong> the first plateau to the second<br />

plateau is exactly 1:3. The same ratio <strong>of</strong> the high to low<br />

plateaus was found in the charging curve. The constant<br />

ratio <strong>of</strong> 1:3 <strong>of</strong> these plateaus at both charging and<br />

discharge cycles proves that the polysulfide shuttle has<br />

been completely blocked by this solid electrolyte coating<br />

on the surface <strong>of</strong> lithium metal. The coulombic efficiency<br />

shown in Figure V - 67b is above 98% for all cycles. The<br />

energy efficiency is about 90% at 0.1 C. Capacity decay<br />

during cycling was still present. It is known that the<br />

capacity decay is caused by the precipitation <strong>of</strong> Li 2 S in the<br />

liquid electrolyte.<br />

Sample Transfer Stage. A new sample transfer stage<br />

has been developed for taking samples from a glove box to<br />

a scanning electron microscope (SEM) without exposure to<br />

air and moisture. The transfer stage operates by the<br />

difference <strong>of</strong> pressure inside and outside the SEM<br />

chamber: when a sample is loaded in a glove box and<br />

exposed to a slight vacuum, the atmospheric pressure<br />

pushes the lid against the o-ring seal. The sample is<br />

protected by the transfer stage as it is moved from the<br />

glove box to the SEM. After the sample stage is loaded<br />

inside the SEM chamber, the higher vacuum causes the lid<br />

to pop open, thus exposing the sample for imaging. This<br />

sample stage enables the analysis <strong>of</strong> lithium anodes after<br />

battery cycling.<br />

Conclusions and Future Directions<br />

Because <strong>of</strong> the poor electronic conductivity <strong>of</strong> sulfur,<br />

the high surface area carbon is the enabler <strong>of</strong> achieving the<br />

maximum utilization <strong>of</strong> sulfur under electrochemical<br />

cycling. The porosity is important for the retention <strong>of</strong><br />

capacity. With the same sulfur loading, excess pore<br />

volume accommodates liquid electrolyte and facilitates the<br />

mass transport <strong>of</strong> lithium ions. Physical adsorption by<br />

porous carbon is insufficient to completely eliminate the<br />

polysulfide shuttle.<br />

Energy Storage R &D 526 FY 2011 Annual Progress Report

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