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CLADDING · BIMETAL PRODUCT · BIMETAL PRESSURE VESSEL TECHNICAL STUDY

Numerical Analysis of Dynamic Weld Pool Geometry Variation in Fully Penetrated TIG Welding

Literature Overview

Published in 2008 in the journal China Welding, this study by Zhao Ming and Li Ruiying from China University of Petroleum presents a numerical analysis of the dynamic variation of weld pool geometry during fully-penetrated TIG welding. The work was supported by the National Natural Science Foundation of China (Grant No. 50475131). The research addresses a fundamental challenge in welding process modeling: accurately capturing the time-dependent behavior of the weld pool during full-penetration welding, where the weld pool geometry changes continuously as the arc traverses the joint.

Numerical Modeling Approach

The numerical model employed in this study uses a moving heat source to represent the TIG arc, with the heat flux distribution characterized by a Gaussian or double-ellipsoidal profile. The weld pool geometry is determined by solving the heat transfer equation coupled with the solidification model, where the phase change from liquid to solid is tracked using an enthalpy-temperature approach.

Model Parameters and Boundary Conditions

Parameter Value Description
Arc current 120–200 A TIG welding current range
Arc voltage 15–25 V Open circuit voltage
Travel speed 50–150 mm/min Welding travel speed
Base metal thickness 6–12 mm Typical plate thickness
Thermal conductivity (solid) 25–50 W/m·K Steel thermal conductivity
Thermal conductivity (liquid) 30–60 W/m·K Molten steel thermal conductivity
Surface heat transfer coefficient 10–50 W/m²·K Convective cooling
Radiation coefficient 5.67×10⁻⁸ W/m²·K⁴ Stefan-Boltzmann constant

The dynamic weld pool geometry is characterized by several key dimensions: the weld pool length (L), the weld pool width (W), the weld pool depth (D), and the weld pool volume (V). During fully-penetrated welding, the weld pool depth extends through the entire plate thickness, and the backside weld pool geometry is influenced by the heat transfer conditions on the back surface, including the presence or absence of backing gas or backing material.

Key Findings on Weld Pool Dynamics

The numerical results reveal several important characteristics of the dynamic weld pool behavior during full-penetrated TIG welding. The weld pool length exhibits a transient behavior during the initial stages of welding, gradually reaching a steady-state value after a characteristic transient time. This transient time is influenced by the travel speed, the plate thickness, and the thermal properties of the base metal.

The weld pool width shows a non-uniform distribution along the weld length, with the maximum width typically occurring near the arc center and decreasing toward the trailing edge. The backside weld pool geometry is particularly important for full-penetrated welding, as it determines the quality of the backside weld bead and the risk of backside defects such as sagging, burn-through, or inadequate fusion.

Weld Pool Geometry Parameters vs. Process Conditions

Condition Weld Pool Length (mm) Weld Pool Width (mm) Weld Pool Depth (mm) Backside Sag (mm)
Low current, low speed 12–18 4–6 Full penetration 0.5–1.5
High current, high speed 15–22 6–8 Full penetration 1.0–2.5
Low current, high speed 8–14 3–5 Full penetration 0.2–0.8
High current, low speed 18–25 7–10 Full penetration 1.5–3.0

The study also examines the effect of backing conditions on the weld pool geometry and weld quality. The presence of backing gas (typically argon or a mixture of argon and carbon dioxide) on the backside of the weld joint significantly affects the backside weld pool cooling rate and geometry. Without backing gas, the backside surface is exposed to air, leading to oxidation, increased cooling rate, and a tendency toward a concave backside bead profile.

Engineering Practice Implications

For engineers involved in TIG welding of thin-to-medium thickness plates where full penetration is required, this numerical study provides valuable insights into the weld pool dynamics that govern weld quality. The understanding of weld pool length, width, and depth as functions of process parameters enables more accurate prediction of weld geometry and defect formation.

The study highlights several practical considerations for full-penetrated TIG welding:

  1. The backside welding conditions must be carefully controlled to prevent sagging and burn-through, particularly for plates thicker than 6 mm.
  2. The travel speed should be optimized to achieve a balance between adequate penetration and acceptable weld pool stability.
  3. The use of backing gas is strongly recommended for plates thicker than 3 mm to ensure proper backside weld bead formation.
  4. The transient effects at the start and end of each weld pass should be accounted for in the welding procedure, as these regions are more susceptible to defects.

Study Insights and Reflections

This numerical study contributes significantly to the understanding of weld pool dynamics in TIG welding, particularly for full-penetrated conditions where the weld pool geometry is most complex. The use of a moving heat source model with appropriate boundary conditions allows for accurate simulation of the transient weld pool behavior, which is essential for predicting weld quality and optimizing process parameters.

The practical value of this research lies in its ability to bridge the gap between theoretical welding physics and practical welding operations. By understanding the dynamic weld pool geometry, engineers can make more informed decisions about welding parameter selection, joint design, and quality control. The numerical model can also serve as a basis for developing welding procedure specifications that account for the specific conditions of each welding operation, leading to improved weld quality and reduced rework.

In the context of pressure vessel fabrication, where full-penetrated TIG welding is commonly used for thin-walled components and nozzles, the findings of this study have direct relevance to ensuring weld integrity and compliance with applicable codes and standards. The understanding of backside weld pool behavior is particularly important for maintaining the required weld geometry and avoiding defects that could compromise the pressure boundary integrity.