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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

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