Characterization of SOFC Electrolytes for Improved...
Transcript of Characterization of SOFC Electrolytes for Improved...
Characterization of SOFC Electrolytes for Improved Mechanical RobustnessCharacterization of SOFC Electrolytes for Improved Mechanical RobustnessRyan Berke, Bodhayan Dev, Mark Walter, The Ohio State UniversityRyan Berke, Bodhayan Dev, Mark Walter, The Ohio State University
Mick Day, Michael Jansen, Scott Swartz, NexTech Materials LtdMick Day, Michael Jansen, Scott Swartz, NexTech Materials Ltd
Elastic properties are obtained using
ASTM 1875-08, a sonic resonance technique.
Rectangular bar specimens are suspended in a furnace,
and excited over a range of frequencies.
Certain frequencies exhibit resonance.
The resonant modes are reproduced via FEA.
The frequencies are used to calculate
Temperature-dependent elastic properties
GOALActuator
240
3% mol YSZ
ASTM 1875-08, a sonic resonance technique. and excited over a range of frequencies. The resonant modes are reproduced via FEA. Temperature-dependent elastic properties
for 3-YSZ and 6-ScSZ.
Configuration of
Optimize FlexCellTM geometry
GOALActuator & Sensor
200
220
Ela
stic
Mod
ulus
, E
(G
Pa)
6% mol ScSZ
Photo of
resonance
� First flexural
mode (FE)
Configuration of
bar specimens
used in the Optimize FlexCellTM geometry
to improve mechanical robustness
without sacrificing electrochemical
Electrolyte Hanging Specimen
180
Ela
stic
Mod
ulus
, E
(G
Pa)resonance
apparatus.
used in the
experiments.
without sacrificing electrochemical
efficiency.
Electrolyte
Material0.035
0.04
f4= 1884 Hz,
140
160
Ela
stic
Mod
ulus
, E
(G
Pa)
3 22
0.9465 1 6.585Emf L tE
b t L
= +
� First torsional
mode (FG)
efficiency.Material
0.02
0.025
0.03
0.035
f1 = 633 Hz
(fE)
f2= 944
Hz
f3= 1752
Hz
f4= 1884 Hz,
(fG)0 100 200 300 400 500 600 700 800
120
Temperature, T (oC)
Where
E = Young’s Modulus (GPa)
0.9465 1 6.585b t L
Typical amplitude
versus frequency
data obtained via
0
0.005
0.01
0.015
E = Young’s Modulus (GPa)
m= Mass of specimen (g)
L, b, t = Geometry of specimen (mm)
f = Fundamental frequency in flexure (Hz)
data obtained via
resonance.
First 5 resonant modes obtained using ANSYS.
The elastic properties are used as inputs for the
structural and thermal models below.
INTRODUCTION
300 800 1300 1800 2300fE = Fundamental frequency in flexure (Hz) First 5 resonant modes obtained using ANSYS. structural and thermal models below.
A small-scale repeating geometry models the support Each small-scale geometry is modeled under uniaxial “Effective” properties are computed relative to those of “Effective” properties are validated with 4-point INTRODUCTION100
Total Equivalent Stiffness δ
A small-scale repeating geometry models the support
structure.
Each small-scale geometry is modeled under uniaxial
tension using FEA.
“Effective” properties are computed relative to those of
a uniformly thick solid:
“Effective” properties are validated with 4-point
bending of representative samples.
The FlexCellTM is the latest generation electrolyte-
supported planar SOFC from NexTech Materials Ltd. 60
70
80
90
Per
cent
Equ
ival
ent
Stif
fnes
s (%
)
All Points
Points having shared thicknessδ
Tensile
displacement
Reduction in
stiffness with
increased active supported planar SOFC from NexTech Materials Ltd.
Support 20
30
40
50
60
Per
cent
Equ
ival
ent
Stif
fnes
s (%
)
displacement
applied to the
model.
increased active
area.
Support
Structure0 10 20 30 40 50 60 70 80 90 100
0
10
20
Percent Active Area (%)
Specimen Geometry %AA %Eeq
Predicted Modulus
(GPa)
Experimental Modulus
(GPa)
model.
% Active Area:
Structure (GPa) (GPa)
Large Hexes 57 39 79.6 73.3
Small Hexes 39 52 106.4 108.678 small-scale geometries were selected by varying: Principal stress
distribution
SOFC Construction and Operation
Small Hexes 39 52 106.4 108.6
Small Circles 36 55 111.7 112.1
No Hexes 0 100 204.6 202.2
1. Width of each hex, w (mm)
2. Space between hexes, b (mm)
3. Radius of corner fillets, r (mm)
distribution
resulting from
edge
Magnification of
membrane stress
with increased SOFC Construction and Operation 3. Radius of corner fillets, r (mm)
4. Thickness of membrane, tm (mm)
5. Thickness of support mesh, ts (mm)
edge
displacement.with increased
active area. The “effective” properties can be used for larger
scale modeling.
FlexCellTM Innovation: A honeycomb-type structure
provides a thicker support mesh with thin active area.
5. Thickness of support mesh, ts (mm) scale modeling.
Large-scale geometries are modeled using “effective” Large-scale geometry is modeled with shell elements The relatively stiffer ribs appear to carry more stress, Based on initial findings, recommendations are made provides a thicker support mesh with thin active area. Large-scale geometries are modeled using “effective”
mechanical properties in active regions.
Large-scale geometry is modeled with shell elements
under structural and thermal loading using FEA.
The relatively stiffer ribs appear to carry more stress,
but unlike the active area the stresses are unmagnified.
Based on initial findings, recommendations are made
for the development of even larger cells.
Rounded fillet to
Stress response
to out-of-plane
Wider vertical rib
Rounded fillet to
reduce stress
Narrow frame
WholeElectrolyte
color-coded to
show “effective”
to out-of-plane
pressure loading.
Whole
Electrolyte
show “effective”
material types.The ribs also reduce out-of-plane displacements.
Honeycomb structure in a FlexCellTM
Electrolyte
Stress response
The ribs also reduce out-of-plane displacements.
Narrow side rib
Rounded fillet to
reduce thermal
Thin regions are more electro-chemically efficient for
Honeycomb structure in a FlexCellTM
1st principal stress contour plot of ultra large FlexCell
with widened rib
Each large-scale geometry was selected by varying:
1. Stiffness applied to active regions, Eeq (GPa)
Stress response
to horizontal
temperature
Narrow side ribreduce thermal
stress
Thin regions are more electro-chemically efficient for
improved performance.
1. Stiffness applied to active regions, Eeq (GPa)
2. Support rib and frame dimensions, (mm)
3. Radius of corner fillets, (mm)
temperature
gradient. Large cells which are mechanically robust have a
higher power density..improved performance.
An individual cell model is used to evaluate the Current-collecting, corrugated foams in the cell transfer Foam properties in the model are changed over several Cell models consider variations in foam geometry to
3. Radius of corner fillets, (mm) higher power density..
An individual cell model is used to evaluate the
electrolyte within the context of a stack.
Current-collecting, corrugated foams in the cell transfer
loads onto the electrolyte.
Foam properties in the model are changed over several
iterations until the load-displacement behavior
matches the experimental data.
Cell models consider variations in foam geometry to
characterize stress distributions in electrolytes.
matches the experimental data.
Mechanical
properties of an
Brittle electrolytes can withstand considerable bendingLoad
The load-displacement behavior of foam compressed in
properties of an
ideal foam.
Thick regions support against mechanical damage
Brittle electrolytes can withstand considerable bendingLoad
TransferThe load-displacement behavior of foam compressed in
a load frame is reproduced in a contact model.
Thick regions support against mechanical damage
during manufacturing, assembly, and operation.
Transfer
Changes in foam geometry may reduce loads
Load frame data. Contact simulation.Schematic of a planar SOFC stack assembly. Material property inputs. Load-displacement results.
Changes in foam geometry may reduce loads
(and therefore stresses) imposed on electrolyte.