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handle: 10261/307903
ThermalZeroField_T-M-DataSet_RFvariance_000000_1.ascii ThermalZeroField_T-M-DataSet_RFvariance_000000_5.ascii ThermalZeroField_T-M-DataSet_RFvariance_000001_0.ascii ThermalZeroField_T-M-DataSet_RFvariance_000001_5.ascii ThermalZeroField_T-M-DataSet_RFvariance_000002_0.ascii AthermalField_sigma-M-DataSet_RFvariance_000000_1.ascii AthermalField_sigma-M-DataSet_RFvariance_000000_5.ascii AthermalField_sigma-M-DataSet_RFvariance_000001_0.ascii AthermalField_sigma-M-DataSet_RFvariance_000001_5.ascii AthermalField_sigma-M-DataSet_RFvariance_000000_1.ascii strain_rate-vs-temp-pureAl-11MPa.ascii strain_rate-vs-temp-pureAl-17MPa.ascii strain_rate-vs-temp-pureAl-32MPa.ascii strain_rate-vs-temp-AA6061-17MPa.ascii strain_rate-vs-temp-AA6061-32MPa.ascii strain_rate-vs-temp-AA6061-38MPa.ascii strain_rate-vs-temp-AA6061-45MPa.ascii
Experimental tests have been carried out by applying a constant stress to the materials under study (Al-99.8% as well as AA6061alloy) and increasing the temperature from room temperature to 800K. The heating rate used was 2K/min. We implemented the three-dimensional random-field Ising model, both as function of stress and as a function of temperature for cubic supercells of 16×16×16 sites. We also investigated the behavior of the secondary creep strain rate ε ˙_SS as a function of temperature at different disorder strength ∆ = 0, 0.5, 1, 1.5, 2, i.e. different applied stress.
This work was funded by Ministerio de Asuntos Económicos y Transformación Digital (TED2021-129580B-100 (ECOAUTO) and MAT2017-83825-C4-1-R ().
Peer reviewed
Temperature, Strain rate, Stress
Temperature, Strain rate, Stress
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