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Geometry of laser spot welds from dimensionless numbers

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Abstract

Recent computer calculations of heat transfer and fluid flow in welding were intended to provide useful insight about weldment geometry for certain specific welding conditions and alloys joined. However, no generally applicable correlation for the joining of all materials under various welding conditions was sought in previous work. To address this difficulty, computer models of fluid flow and heat transfer were used for the prediction of weld pool geometry in materials with diverse properties, such as gallium, pure aluminum, aluminum alloy 5182, pure iron, steel, titanium, and sodium nitrate under various welding conditions. From the results, a generally applicable relationship was developed between Peclet (Pe) and Marangoni (Ma) numbers. For a given material, Ma and Pe increased with the increase in laser power and decrease in beam radius. For materials with high Prandtl number (Pr), such as sodium nitrate, the Pe and Ma were high, and heat was transported primarily by convection within the weld pool. The resulting welds were shallow and wide. For low Pr number materials, like aluminum, the Pe and Ma were low in most cases, and low Pe made the weld pool deep and narrow. The cross-sectional areas of stationary and low speed welds could be correlated with welding conditions and material properties using dimensionless numbers proposed in this article.

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Abbreviations

A :

cross-sectional area of the weld pool (m2)

C ps :

specific heat of solid (J/kg K, which may also be written as m2/s2 K)

C pl :

specific heat of liquid (J/kg K, which may also be written as m2/s2 K)

D :

depth of the weld pool (m)

DA:

dimensionless cross-sectional area

DH:

dimensionless heat input

dγ/dT :

temperature coefficient of the surface tension (N/m K, which may also be written as kg/s2 K)

D s :

diameter of disc-shaped specimen (m)

H f :

enthalpy of fusion (J/kg, which may also be written as m2/s2)

H m :

enthalpy of liquid at melting point (J/kg, which may also be written as m2/s2)

H s :

specimen thickness (m)

K s :

thermal conductivity of solid (J/m s K, which may also be written as kg m/s3 K)

K l :

thermal conductivity of liquid (J/m s K, which may also be written as kg m/s3 K)

L s :

length of specimen (m)

Ma:

Marangoni number

Pe:

Peclet number

Pr:

Prandtl number

Q :

rate of heat absorption (J/s, which may also be expressed as kg/m2 s3)

t :

irradiation time or the time necessary to reach quasi-steady-state size of the weld pool (s)

T m :

melting point (K)

V max :

calculated maximum surface velocity (m/s)

W :

width of the weld pool (m)

W s :

width of the specimen (m)

α s :

thermal diffusivity of solid (m2/s)

α l :

thermal diffusivity of liquid (m2/s)

ΔT :

temperature drop from the center to the edge of the weld pool (K)

μ :

viscosity (kg/m s)

v :

kinematic viscosity (m2/s)

ϱ :

density (kg/m3)

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Robert, A., Debroy, T. Geometry of laser spot welds from dimensionless numbers. Metall Mater Trans B 32, 941–947 (2001). https://doi.org/10.1007/s11663-001-0080-0

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