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CLADDING TECHNOLOGY SHANXI CO., LTD
CLADDING · BIMETAL PRODUCT · BIMETAL PRESSURE VESSEL TECHNICAL STUDY

Numerical Simulation of TIG Welding Arc Protected by Argon and Helium Shielding Gas

Literature Overview and Research Background

This study presents a numerical simulation investigation into the behavior of the gas tungsten arc welding (GTAW/TIG) arc under two different shielding gas environments: argon (Ar) and helium (He). The work addresses a fundamental question in welding engineering — how the choice of shielding gas influences arc geometry, heat flux distribution, and ultimately the weld pool characteristics. For cladding and weld overlay applications, where precise control of dilution and penetration is critical, understanding the thermal and fluid dynamics of the arc is essential. The simulation employs computational fluid dynamics (CFD) coupled with electromagnetic field modeling to capture the full physics of the arc plasma column, including Joule heating, radiation, and convection effects.

Core Technical Content and Arc Physics

The numerical model solves the coupled Navier-Stokes equations for momentum, energy, and mass conservation within the arc plasma, alongside Maxwell's equations for the electromagnetic field. The arc is treated as a magnetohydrodynamic (MHD) fluid, where the Lorentz force drives the plasma flow and shapes the arc column. Key assumptions include local thermodynamic equilibrium (LTE) for the plasma and a two-temperature model accounting for the difference between electron and heavy-particle temperatures.

The comparison between argon and helium shielding reveals significant differences in arc behavior:

Parameter Argon Shielding Helium Shielding
Arc column radius Larger Narrower
Arc voltage (at same current) Lower Higher
Heat flux concentration More diffuse More concentrated
Penetration depth Shallower Deeper
Arc stability Higher Slightly lower
Typical current range 20-300 A 20-400 A
Arc temperature (K) ~14,000-16,000 ~15,000-18,000
Heat input efficiency Moderate Higher

The helium arc exhibits a more constricted, higher-temperature plasma column due to helium's higher ionization energy and thermal conductivity. This results in a more concentrated heat flux at the workpiece surface, producing deeper penetration at equivalent welding currents. Argon, being heavier and with lower thermal conductivity, produces a broader, more stable arc with shallower penetration but better shielding coverage.

Implications for Cladding and Weld Overlay Applications

For weld overlay and cladding operations, the choice of shielding gas has direct consequences on dilution control, overlay layer composition, and bond line integrity. When overlaying nickel-based alloys (such as Inconel 625 or Hastelloy C276) onto carbon steel substrates, dilution from the base metal is a primary concern. The concentrated heat flux of helium shielding produces deeper penetration and consequently higher dilution, which may be undesirable when maintaining a pure overlay composition is required.

In practice, for overlay welding of stainless steel (304/316/321/347) onto carbon steel, argon shielding is generally preferred because it provides a more controlled, shallower heat input that limits dilution to the base metal. However, when higher deposition rates and deeper bond lines are needed — such as in GTAW overlay of thick cladding layers — helium or helium-argon mixtures (typically 75% He / 25% Ar) can be advantageous.

The simulation results also inform travel speed optimization. The numerical heat flux profiles show that helium arcs maintain a higher heat flux over a shorter distance, meaning that for the same welding speed, the linear heat input (q = VI/ν) is effectively concentrated in a narrower zone. This has implications for residual stress distribution and distortion in large clad plate assemblies.

Key Technical Insights and Engineering Reflections

The numerical model validates several empirical observations made in shop practice. First, the arc constriction observed with helium shielding correlates with the higher arc voltage and the need for greater electrode-to-workpiece distance to avoid arc blow-off. Second, the simulation confirms that argon's higher atomic mass contributes to better shielding gas coverage, particularly in outdoor or drafty conditions, which is a practical advantage for field overlay welding operations.

For bimetal pressure vessel fabrication, where weld overlay is applied to the interior of vessels to provide corrosion resistance, the shielding gas choice must account for the confined geometry. Argon's superior shielding characteristics make it more reliable in tight internal weld positions where gas backflow is difficult to manage.

The study also highlights the importance of electrode composition and arc force. The numerical results suggest that the interaction between electrode material (thoriated tungsten vs. ceriated tungsten) and shielding gas affects arc stability and spot size, which in turn influences the surface quality and porosity susceptibility of the overlay weld.

Summary and Practical Recommendations

This numerical simulation study provides a rigorous theoretical foundation for understanding how shielding gas selection governs TIG arc behavior. The key takeaway for cladding and weld overlay engineers is that argon shielding offers superior stability and dilution control, making it the default choice for most overlay applications on bimetal products and pressure vessels. Helium shielding, while offering deeper penetration and higher thermal efficiency, must be used judiciously where dilution is acceptable or even desirable for achieving metallurgical bonding. The simulation results should be treated as a design tool — when specifying welding procedures for critical overlay applications, the predicted heat flux profiles and arc geometry from such models can guide the selection of welding parameters, travel speeds, and shielding gas compositions to achieve the required overlay quality and bond strength.