Research Article

Numerical Study of Characteristic Equations of Thermoelastic Waves Propagating in a Uniaxial Prestressed Isotropic Plate

Table 1

Material properties of the copper foil under the natural state and two initial states with two uniaxial prestresses 0 . 0 2 𝑐 4 4 and 0 . 0 4 𝑐 4 4 applied in the 𝑋 1 -direction.

Natural statePrestress 𝑇 𝑖 1 1 = 0 . 0 2 𝑐 4 4 Prestress 𝑇 𝑖 1 1 = 0 . 0 4 𝑐 4 4

Thickness
(mm)
= 0 . 1 = 0 . 1 = 0 .1

Mass density
(mg/mm3)
𝜌 0 = 8 . 9 3 𝜌 𝑖 = 8 . 9 1 3 𝜌 𝑖 = 8 . 8 9 5

Elastic constants
(mg/mm μs2)
𝑐 1 1 = 1 8 8 . 1
𝑐 1 2 = 1 0 8 . 9
𝑐 4 4 = 3 9 . 6
𝑐 1 1 1 = 1 8 9 4 𝑐 1 1 2 = 7 5 4
𝑐 1 2 3 = 5 6 𝑐 1 4 4 = 4 0 1
𝑐 1 5 5 = 2 8 7 𝑐 4 5 6 = 5 7
𝑐 1 1 = 1 8 3 . 3 7 7
𝑐 2 2 = 𝑐 3 3 = 1 8 7 . 3 4 3
𝑐 2 3 = 1 1 1 . 9 2 6
𝑐 1 2 = 𝑐 1 3 = 1 0 6 . 0 9 4
𝑐 4 4 = 3 7 . 7 0 4
𝑐 5 5 = 𝑐 6 6 = 3 9 . 6 3 6
𝑐 1 1 = 1 7 8 . 6 5 5
𝑐 2 2 = 𝑐 3 3 = 1 8 6 . 5 8 7
𝑐 2 3 = 1 1 4 . 9 5 2
𝑐 1 2 = 𝑐 1 3 = 1 0 3 . 2 8 8
𝑐 4 4 = 3 5 . 8 0 7
𝑐 5 5 = 𝑐 6 6 = 3 9 . 6 7 1

Temperature
(k°K)
Θ 0 = 0 . 3 0 0 Θ 𝑖 = 0 . 3 0 0 Θ 𝑖 = 0 . 3 0 0

Thermal constant
(mg/mm 𝜇 s2 k°K2)
𝛼 = ( 𝜌 0 𝐶 E ) / Θ 0 = 1 1 . 1 2 9 𝛼 = 1 1 . 1 0 7 𝛼 = 1 1 . 0 8 5

Thermoelastic coupling coeff. (mg/mm 𝜇 s2 k°K) 𝜆 = ( 𝑐 1 1 + 2 𝑐 1 2 ) 𝛾 = 6 . 6 9 7 𝜆 1 = 6 . 7 8 2
𝜆 2 = 𝜆 3 = 6 . 6 4 8
𝜆 1 = 6 . 8 6 7
𝜆 2 = 𝜆 3 = 6 . 5 9 9

Thermal conductivity (mg/mm 𝜇 s2 k°K) 𝐤 = 0 . 3 9 8 × 1 0 3 𝐤 1 = 0 . 4 0 3 × 1 0 3
𝐤 2 = 𝐤 3 = 0 . 3 9 5 × 1 0 3
𝐤 1 = 0 . 4 0 8 × 1 0 3
𝐤 2 = 𝐤 3 = 0 . 3 9 2 × 1 0 3

𝐶 E = 3 . 7 4 is the heat capacity (mg/ 𝜇 s2 k°K), and 𝛾 = 0 . 0 1 6 5 is the thermal expansion coefficient (1/k°K).