V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
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V.E.5 Analysis and Simulation <strong>of</strong> Electrochemical Energy Systems (LBNL)<br />
Newman – LBNL<br />
V.E.5 Analysis and Simulation <strong>of</strong> Electrochemical Energy Systems (LBNL) <br />
John Newman<br />
Lawrence Berkeley National Laboratory<br />
306 Gilman Hall<br />
University <strong>of</strong> California, Berkeley<br />
Berkeley, CA 94720<br />
Phone: (510) 642-4063; Fax: (510) 642-4778<br />
E-mail: newman@newman.cchem.berkeley.edu<br />
Start Date: October 1, 2010<br />
Projected End Date: September 30, 2011<br />
Objectives<br />
· Develop experimental methods for measuring<br />
transport, thermodynamic, and kinetic properties.<br />
· Model electrochemical systems to optimize<br />
performance, identify limiting factors, and mitigate<br />
failure mechanisms.<br />
Technical Barriers<br />
This project addresses the following technical barriers<br />
from the USABC:<br />
(A) Capacity and power fade<br />
(B) Safety and overcharge protection<br />
Technical Targets<br />
This project contributes to the USABC Requirements<br />
<strong>of</strong> End <strong>of</strong> Life Energy Storage Systems for PHEVs and<br />
EVs:<br />
· 300,000 shallow discharge cycles<br />
· 15 year calendar life<br />
Accomplishments<br />
· Developed both steady-state and transient methods to<br />
characterize the SEI using through-film reduction<br />
kinetics <strong>of</strong> ferrocene<br />
· Expanded ferrocene characterization method from<br />
model surface (glassy carbon) to highly-oriented<br />
pyrolytic graphite, a more realistic battery material<br />
(collaboration with Takeshi Abe, Kyoto University)<br />
Introduction<br />
<br />
Our main project in FY10 was the experimental study<br />
<strong>of</strong> SEI formation reactions and the interaction <strong>of</strong> the SEI<br />
with redox shuttles. Our novel method <strong>of</strong> SEI<br />
characterization contributes to understanding <strong>of</strong><br />
passivation in nonaqueous electrolytes, which is in turn<br />
critical to battery performance and lifetime. While FY09<br />
was spent primarily on the development <strong>of</strong> reproducible<br />
experimental methods, FY10 saw both experimental<br />
refinement and the development <strong>of</strong> theoretical tools for<br />
data analysis. Additionally, we began to expand our<br />
studies from glassy carbon, a model surface, to highlyoriented<br />
pyrolytic graphite (HOPG), which more<br />
accurately resembles the carbon found in a lithium-ion<br />
battery.<br />
Approach<br />
· Utilize classical electrochemistry experiments to<br />
understand the fundamental growth kinetics <strong>of</strong> the<br />
SEI, as well as how it interacts with a redox shuttle.<br />
· Measure shuttle reduction kinetics in the presence and<br />
absence <strong>of</strong> passivating films to determine the relative<br />
transport and kinetic inhibitions to reaction.<br />
· Use a rotating-disk electrode (RDE) to measure the<br />
steady-state through-film reduction current, and<br />
electrochemical impedance spectroscopy (EIS) to<br />
measure the frequency response <strong>of</strong> the ferrocene<br />
reaction in the presence and absence <strong>of</strong> the SEI.<br />
Results<br />
1. Steady-state characterization. Steady-state<br />
measurements and model fits are shown in Figure V - 201.<br />
The markers show the current measured at 900 rpm after<br />
films were built on the electrode for 30 seconds, 6, 30, and<br />
60 minute holds at 0.6 V. Dashed lines are model fits to<br />
the passivated current, and the dotted line is the reversible<br />
current, which is seen on the clean electrode. Current<br />
decreases with passivation time because the electrode has<br />
had longer to grow a “thicker” film. The model includes<br />
only three adjustable parameters: a transfer coefficient α,<br />
an exchange current density i 0 , and a through-film<br />
ferrocene limiting current i lim , given below.<br />
i lim<br />
<br />
FD<br />
εC bulk<br />
O, f O<br />
L<br />
bulk c bulk a<br />
i 0<br />
k (C O<br />
) (C R<br />
)<br />
Energy Storage R &D 644 FY 2011 Annual Progress Report