2022
DOI: 10.1177/03093247221119303
|View full text |Cite
|
Sign up to set email alerts
|

The vibration of viscothermoelastic static pre-stress nanobeam based on two-temperature dual-phase-lag heat conduction and subjected to ramp-type heat

Abstract: In this work, the two-temperature dual-phase-lag theorem has been used to present an analytical mathematical model for calculating the vibration in a viscothermoelastic nano-resonator. The governing equations have been derived when a simply supported nano-resonator is exposed to a ramp-type thermal load and static pre-stress. The governing equations have been solved by using a direct method and obtained the solution in the Laplace transform domain where the inversions of the Laplace transform have been calcula… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2023
2023
2023
2023

Publication Types

Select...
3

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(2 citation statements)
references
References 43 publications
(52 reference statements)
0
2
0
Order By: Relevance
“…In the case of a semi-infinite conductor [50], the temperature peak diffuses with time progress, leaving the boundary surface. Here, in the finite domain setting, because of the presence of the reflecting boundary condition on the lower boundary (36) and the acute heat flux precedence, τ θ τ q , the heat flux vector reverses its direction between the dimensionless instants t = 0.08 and t = 0.09, so that the upper surface always has the highest temperature though the overall dissipation of heat (i.e., the decrease in temperature value with time). This behavior is also attributed to the immobilization characteristic of the Jeffreys "DPL" equation referred to in the literature; see [2,21,62].…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…In the case of a semi-infinite conductor [50], the temperature peak diffuses with time progress, leaving the boundary surface. Here, in the finite domain setting, because of the presence of the reflecting boundary condition on the lower boundary (36) and the acute heat flux precedence, τ θ τ q , the heat flux vector reverses its direction between the dimensionless instants t = 0.08 and t = 0.09, so that the upper surface always has the highest temperature though the overall dissipation of heat (i.e., the decrease in temperature value with time). This behavior is also attributed to the immobilization characteristic of the Jeffreys "DPL" equation referred to in the literature; see [2,21,62].…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…When τ ε → 0 , the Hookean response is recovered, i.e., σ = Eε. The Kelvin-Voigt thermoelasticity has been considered in a variety of viscoelastic applications, e.g., unbounded thermoviscoelastic domain with spherical cavity [35], vibration of an Euler Bernoulli beam [36,37], and micropolar thermoelasticity [38], and has been extended to the second-gradient media [39].…”
Section: Introductionmentioning
confidence: 99%