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The failure temperature is evaluated while respecting variable material characteristics in time of growing temperature.
The effect of the operating conditions, including current density, reactant concentration and temperature, is evaluated.
Fuel centerline temperature is evaluated to be 1853 °C and fission gas release fraction is about 45% including helium production.
Further, cup-mixing temperature is evaluated for various cases to establish optimal thermal mixing by distributed heating in comparison to conventional bottom wall heating.
The shift of critical temperature is evaluated as ΔT c /T c ≈ Δρ s /ρs 0.a We define the critical impurity concentration n imp c as a concentration at which Δρ s /ρs 0= 1.
In the mentioned terms, the magnetization of the ferrofluid which is dependent on temperature is evaluated as below [19]: M(T ={M}_{mathrm{ref}}left 1-{beta}_mleft T-{T}_{mathrm{ref}}right)right) (7)where β M}_{mathrm{ref}}left 1-{beta}_mleft T-{T}_{mathrm{ref}}rightwhich indicates the dependency of the M}_{mathrm{ref}}left 1-{beta}_mleft T-{T}_{mathrm{ref}}right
Similar(53)
The measurement offset and its dependence on temperature were evaluated in the same experimental test.
In addition, the structural effects associated with metal insertion at room temperature were evaluated.
Moreover, the dependence of distribution ratios on the temperature was evaluated.
Glass transition temperature and dilatometric softening temperature were evaluated by dilatometry.
The stresses at different temperature are evaluated with different loading conditions.
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