Transient β, or Andrade, creep occurs when magnesia‐partially‐stabilized zirconia is loaded in tension at room temperature. The equation relating the longitudinal or tensile creep strain, ε c ℓ to the tensile stress, σ, and to the time, t , has been determined to be ε c ℓ = A σ m t n in which the constants A , m , and n depend on the phase content of the zirconia. Observations are reported of the tetragonal‐to‐monoclinic and tetragonal‐to‐orthorhombic phase transformations which occur during creep: there is also a progressive development of microcracking. It is shown that a combination of these phenomena can account for the observed creep behavior.
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Finlayson et al. (1994) studied this question.
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