Poster Session May,2015
Battery Section
Sn/C composite anode material for lithium ion batteries
M. Sivarajakumar, N.H. Kwon, K.M. Fromm
M. Sivarajakumar, N.H. Kwon, K.M. Fromm
Much interest has been flowing towards the trending high energy density batteries for wide
applications including the most vital grid storage, electric vehicles and portable electronics.
Alloy-type anodes (Si, Ge, Sn, Al, Sb, etc.) have much higher Li storage capacity than the
intercalation-type graphite anode that is currently commercially used in Li-ion batteries.
The theoretical capacities of alloy anodes are 2- 10 times higher than that of graphite and
4-20 times higher than that of the lithium titanate anode. Also, these alloy based anode
materials have a moderate onset potential ranging between 0.3-0.4 V above Li/Li+, gaining
safety advantages over low potential graphite anode and avoiding energy penalty over LTO anode.
Na-ion Batteries: New Challenges
C. Marino, L.O. Vogt, M. Kovalenko, K.M. Fromm, P. Novák, C. Villevieille
C. Marino, L.O. Vogt, M. Kovalenko, K.M. Fromm, P. Novák, C. Villevieille
In the last few years, research to determine the most suitable anode and cathode materials for Na-ion
batteries has gained an increased attention. It was a great surprise to discover that pure commercially
available elements such as Sb, Sn, or P1-3 can react electrochemically with Na, leading to sustainable
reversible capacities as high as 500 mAh/g over more than 100 cycles when carboxymethyl cellulose
(CMC) binder is used. These results were unexpected, especially if we compare them to the Li-ion
systems. The most commonly used Li-ion binder, polyvinylidene difluoride (PVDF), was reported to not
work in the sodium system but no further investigation was done to understand the chemical reasons.
Recently, Dahbi et al.4 reported on Na-CMC binder for hard carbon electrodes in Na-ion batteries.
They demonstrated better electrochemical results with CMC binder than with PVDF. They also
reported that fluoroethylene carbonate (FEC) was essential as an electrolyte additive to improve the
cyclability of the PVDF-based electrode.
Thermal Energy Section
High-Temperature Combined Sensible/Latent-Heat Storage for AA-CAES
L. Geissbühler, M. Kolman, G. Zanganeh, A. Haselbacher, A. Steinfeld
L. Geissbühler, M. Kolman, G. Zanganeh, A. Haselbacher, A. Steinfeld
At present, electricity storage with advanced adiabatic compressed air energy storage (AA-CAES) is
considered to the only large-scale alternative to pumped hydro storage. Thermocline storage has gained
increasing interest as a solution for thermal energy storage with potentially high efficiency and low costs. The
present research aims at enhancing the concept using an experimental-numerical approach to study
combined sensible/latent heat storage, which is based on placing a limited amount of steel-encapsulated
AlSi12 on top of a packed bed of rocks. The primary motivation for combining sensible and latent heat
storage is to reduce the decrease in outflow temperature during discharging of sensible heat storage, which
is favorable for downstream applications such as chemical reactions or thermodynamic power cycles. Air is
used as heat transfer fluid and the storage may be operated at ambient pressure or at high pressure for the
use in AA-CAES.
CFD Modeling and Experimental Validation of a High-temperature Pilot-scale
Combined Sensible/Latent Thermal Energy Storage
S. Zavattoni, M. Barbato, L. Geissbühler, A. Haselbacher, G. Zanganeh, A. Steinfeld
S. Zavattoni, M. Barbato, L. Geissbühler, A. Haselbacher, G. Zanganeh, A. Steinfeld
Single-tank, or thermocline, thermal energy storage (TES) systems, with a packed bed of low cost filler
material, represent a valuable alternative to the commonly exploited two-tank solution in nowadays
conventional concentrating solar power (CSP) plants. However, an intrinsic drawback of this solution is
the decrease of the heat transfer fluid (HTF) outlet temperature, towards the end of the discharge
phase, leading to a detrimental effect on the power block efficiency. To avoid the HTF temperature
decrease during discharging, a latent heat TES, based on phase change material (PCM), might be
exploited instead. However, the high cost of the PCM, along with the relatively low efficiency for large
temperature ranges1, are strong limiting factors on the integration of a latent TES into a CSP plant. For
this reason, the idea of adding a small amount of encapsulated PCM on top of the packed bed was
proposed with the aim of mitigating the HTF temperature decrease during discharging limiting, at the
same time, the increment of the overall TES system cost.
Hydrogen Section
Catalytic chemical discharge of an all-vanadium redox flow battery to generate hydrogen from
renewable energy sources.
V. Amstutz, H. Vrubel, C.R. Dennison, P. Peljo, K.E. Toghill, H.H. Girault
V. Amstutz, H. Vrubel, C.R. Dennison, P. Peljo, K.E. Toghill, H.H. Girault
Recently, our laboratory has developed the concept of a dual-circuit redox flow battery
in order to improve the energy density of conventional redox flow batteries (RFBs)1.
The battery is adapted with an external circuit that enables chemical discharge of the
electrolytes on demand. This chemical discharge is a fast alternative to electrochemical
discharge and enables the production of useful products simultaneously to the regeneration
of the discharged electrolyte. On the negative side of the all-vanadium RFB the V(II) electrolyte
is discharged to V(III) when passed over a Mo2C catalytic bed: this reaction generates hydrogen
from the protons present in the solution.
Synthetic Fuel Section
ECSA determination of Cu electrodes by Pb under potential deposition.
Application for CO2 Reduction.
Y. Paratcha, J. Herranz, A. Permyakova, J. Durst, T.J. Schmidt
Y. Paratcha, J. Herranz, A. Permyakova, J. Durst, T.J. Schmidt
Carbon dioxide is a major contributor to global warming and, beyond the mandatory reduction of our
emissions, the possibility of recycling this greenhouse gas is becoming increasingly attractive. The
electrochemical reduction of CO2 is an interesting pathway, since a broad range of useful products can be
formed such as methanol and formic acid (fuels for PEFC), methane and ethylene (reactants for synthesis
or combustion process), CO and H2 (syngas), etc. [1]. Nevertheless, on top of the high overpotential
required to drive this reaction, the electrochemical reduction of CO2 suffers from a poor yield/selectivity of
valuable products [2, 3].Copper-based electrocatalysts seem to be the most efficient to overcome these
kinetic and barriers [3], but it has been shown that the size of the Cu (nano)particles envisaged for
practical applications can influence the reaction selectivity [4]. In order to clarify this particle size effect,
one needs to determine the electrochemically active surface area (ECSA) of the catalysts of interest that,
for Cu, can be derived in-situ by lead underpotential deposition (Pb-UPD) [5]. Additionally, the selectivity
of the CO2-reduction reaction on these well-characterized materials needs to be determined with an
appropriate technique