Compared to their high operating temperature counterparts such as high temperature
protonic ceramic fuel cells or
solid oxide fuel cells, solid acid fuel cells benefit from operating at low temperatures where
plastic deformation and
creep mechanisms are less likely to cause permanent damage to the cell materials. Permanent deformation occurs more readily at elevated temperatures because
defects present within the material have sufficient energy to move and disrupt the original structure. Lower temperature operation also allows for the use of non-
refractory materials which tends to decrease the cost of the SAFC. However, solid acid fuel cell electrolyte materials are still susceptible to mechanical degradation under normal operating conditions above their superprotonic phase transition temperatures due to the
superplasticity enabled by this transition. For instance in the case of CsHSO4, a study has shown that the material can undergo strain rates as high as 10^{-2} s^{-1} for an applied compressive stress in the range of several MPa. Since fuel cells often require pressures in this range to properly seal the device and prevent leaks,
creep is likely to degrade the cells by creating a short circuiting path. The same study showed that the strain rate, as modeled using the standard steady-state creep equation \overset{\cdot}{\epsilon} = A \sigma^n e^{\frac{-Q}{kT}}, has a stress exponent of n = 3.6 typically associated with a
dislocation glide mechanism, and an
activation energy of 1.02 eV. n is the stress exponent, Q is the creep activation energy, and A is a constant that depends on the creep mechanism. Another study focused on thin CsH2PO4 membranes emphasized that while thinner membranes are preferred for promoting conductivity, they can be more susceptible to mechanical degradation and physical leaks, leading to a loss of cell stability. Creep resistance can be obtained by
precipitate strengthening using a composite electrolyte whereby ceramic particles are introduced to prevent dislocation motion. For example, the strain rate of CsH2PO4 was reduced by a factor of 5 by mixing in
SiO2 particles with a size of 2 microns, however resulting in a 20% decrease in protonic conductivity. Other studies have looked at CsH2PO4/
epoxy resin composites where micron size particles of CsH2PO4 are embedded in a cross-linked polymer matrix. A comparison between the
flexural strength of an SiO2 composite versus an epoxy composite demonstrated that while the strengths themselves are similar, the flexibility of the epoxy composite is superior, a property which is essential in preventing electrolyte
fracture during operation. The epoxy composite also shows comparable but slightly lower conductivities than the SiO2 composite when operating at temperatures below 200 °C. == Applications ==