“…To the best knowledge of the authors, dislocation structures originating from non-isothermal cyclic creep have to date only been studied by Viguier and Hantcherli et al [7,41] Their test series on the superalloy MC2 exposed the material to a peak temperature of 1150°C for 30 minutes and cooled the sample down to room temperature in 25 minutes. In other studies of high-temperature (heating to 1050°C and more) thermal creep cycling, [2,22,41] the c¢-dissolution was equally large, resulting in a much larger movement of the interface between its peak and base temperature position than in the current study. This greater disruption to the interface is thought to be the reason why paired dislocation networks have not been observed in the cited studies.…”
Section: A the Effect Of Interfacial Dislocation Network During Cyccontrasting
confidence: 50%
“…Le Graverend et al showed that similarly high misfit magnitudes could be achieved during short high-temperature excursions. [22,44] The same study verified in-situ that an increase in misfit magnitude was directly related to an addition in strain accumulation from added dislocation motion. The high-temperature excursions thus require additional interfacial dislocations, while simultaneously decreasing the Orowan glide resistance in the c-matrix (see Figure 6(c)) thereby allowing the dislocations to reach their required target quicker.…”
Section: A the Effect Of Interfacial Dislocation Network During Cycmentioning
confidence: 68%
“…The primary driving forces for the added dislocation activity during thermal cycling are the continuously changing misfit stresses. [22,42]…”
Section: Discussionmentioning
confidence: 99%
“…The phase fraction variation does not precisely track the temperature profile due to the different diffusivities of the alloying elements. [20,21] Instead, as seen in-situ using synchrotron X-ray radiation, [22] the c¢-dissolution lags behind the temperature profiles depending on exposed temperature and thermal gradient.…”
The creep responses of the superalloy CMSX-4 under thermal cycling conditions (900°C to 1050°C) and constant load (r 0 ¼ 200MPa) were analyzed using TEM dislocation analysis and compared to the modeled evolution of key creep parameters. By studying tests interrupted at different stages of creep, it is argued that the thermal cycling creep rate under these conditions depends on the creation of interfacial dislocation networks and their disintegration by the c¢-shear of dissimilar Burgers vector pairs.
“…To the best knowledge of the authors, dislocation structures originating from non-isothermal cyclic creep have to date only been studied by Viguier and Hantcherli et al [7,41] Their test series on the superalloy MC2 exposed the material to a peak temperature of 1150°C for 30 minutes and cooled the sample down to room temperature in 25 minutes. In other studies of high-temperature (heating to 1050°C and more) thermal creep cycling, [2,22,41] the c¢-dissolution was equally large, resulting in a much larger movement of the interface between its peak and base temperature position than in the current study. This greater disruption to the interface is thought to be the reason why paired dislocation networks have not been observed in the cited studies.…”
Section: A the Effect Of Interfacial Dislocation Network During Cyccontrasting
confidence: 50%
“…Le Graverend et al showed that similarly high misfit magnitudes could be achieved during short high-temperature excursions. [22,44] The same study verified in-situ that an increase in misfit magnitude was directly related to an addition in strain accumulation from added dislocation motion. The high-temperature excursions thus require additional interfacial dislocations, while simultaneously decreasing the Orowan glide resistance in the c-matrix (see Figure 6(c)) thereby allowing the dislocations to reach their required target quicker.…”
Section: A the Effect Of Interfacial Dislocation Network During Cycmentioning
confidence: 68%
“…The primary driving forces for the added dislocation activity during thermal cycling are the continuously changing misfit stresses. [22,42]…”
Section: Discussionmentioning
confidence: 99%
“…The phase fraction variation does not precisely track the temperature profile due to the different diffusivities of the alloying elements. [20,21] Instead, as seen in-situ using synchrotron X-ray radiation, [22] the c¢-dissolution lags behind the temperature profiles depending on exposed temperature and thermal gradient.…”
The creep responses of the superalloy CMSX-4 under thermal cycling conditions (900°C to 1050°C) and constant load (r 0 ¼ 200MPa) were analyzed using TEM dislocation analysis and compared to the modeled evolution of key creep parameters. By studying tests interrupted at different stages of creep, it is argued that the thermal cycling creep rate under these conditions depends on the creation of interfacial dislocation networks and their disintegration by the c¢-shear of dissimilar Burgers vector pairs.
“…As shown in [3], while the plastic strain of the γ channels stops immediately, it carries on for a while at a reduced rate within the γ' rafts in direction As pointed in [25], the density of dislocations climbing within a raft before the jump move afterwards on an average distance 2 ⁄ before reaching its end and annihilating. The residual plastic strain for population 2 is then also:…”
Section: Mobile Dislocation Densities In Domain 2: Load Dropsmentioning
The good mechanical resistance to high temperature creep of [001] oriented single crystal superalloys is due to the properties of the rafts, i.e. platelets of the L12 γ' phase embedded in a γ matrix. At temperatures higher than 900°C, the plastic strain of the rafts results from the climb of dislocation pairs with a total. < 100 > Burgers vector and/or from the climb at the γ/γ' interfaces of 2 ⁄. < 110 > dislocation segments. This climb motion involves the exchange of vacancies between these dislocations and vacancy sinks such as pores and the specimens' surfaces. In this paper we suggest that the entry of. < 100 > into the rafts requires the overcoming of a threshold stress and show that this hypothesis gives a natural explanation to some of the most salient aspects of their mechanical behavior.
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