PSI - Issue 42
A. Sulamanidze et al. / Procedia Structural Integrity 42 (2022) 412–419 Author name / Structural Integrity Procedia 00 (2019) 000 – 000
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3
3. Algorithm for TMF IP and OOP multi-physics computations In order to determination a local thermo-mechanical stress-strain rate and displacement fields a new algorithm for the multi-physics numerical calculations developed and implemented incorporates Maxwell 3D, Fluent and Transient Structural modules of ANSYS 2021R1. The algorithm builds upon a coupled heat loss from eddy currents of magnetic induction and force convective cooling accounting for by k-omega SST turbulence model response, which cause gradients of mechanical elastic-plastic deformations (Fig. 2a).
Fig. 2. (a) Algorithm and (b) FE model for TMF multi-physics computations.
The Maxwell 3D solver computes the values by Maxwell's curl equation (Eq. 1) to solve for the magnetic field H (ANSYS, 2021):
1
(1)
H j = −
H
k j +
where j - current density A/m2; - magnetic permeability; - imaginary component of permittivity; - is the angular frequency of the wave rad/s ; k – bulk conductivity S/m. At the stage of computational fluid dynamics (CFD) analysis, a two-equation eddy-viscosity Shear-stress transport (SST) k- ω turbulence model was used to close unsteady Reynolds averaged Navier – Stokes (URANS) equations. The pressure-based coupled algorithm was used to solve a coupled system of equations comprising the momentum equations and the pressure-based continuity equation. The total strain as a result of thermomechanical loading is equal to:
el pl th = + +
(2)
where el th ref t t = − thermal expansion; th - linear thermal expansion; ref t - reference temperature. The elastic-plastic material behavior is set by Power law nonlinear isotropic hardening model E = elastic strain according to Hooke's law; ( ) th
N
3
G = +
(3)
pl
0
0
0
where N = 1/n is strain hardening exponent. The main electromagnetic, fluid dynamics and mechanical properties used in the numerical study for SENT specimen configuration produced from a high-temperature nickel-based alloy ХН73М are listed in Tables 1 and 2. In our computations, a sequence of thermomechanical loading was simulated, which was implemented in experiments using an inductor coil and nozzles, as shown in Fig.2b.
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