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Additional info for ASM Handbook: Volume 6: Welding, Brazing, and Soldering (Asm Handbook)
0044 ( 550 − T0 ) 2πλ max 804 (EQ 69) resulting in a value for T0 of 354 °C (670 °F). 75, the use of the thin-plate equation is inadequate. 2 = 2 (EQ 71) 804 resulting in a value for T0 of 389 °C (730 °F). 75, using the thin-plate equation is adequate. 3 °F). ), but there is the same level of energy input, then the thick-plate equation (Eq 49) applies and, again, the value for T0 is 389 °C (730 °F). 75, the use of the thick-plate equation is adequate. (EQ 73) Under some welding conditions, it is not necessary to reduce the cooling rate by using a preheat.
Cooling rate is inversely (that is, Q /V) and is proportional to thermal conductivity and the critical temperature at which the cooling rate needs to be evaluated. On the basis of experimental results, a cooling-rate equation was developed for the HAZ of low-carbon steel weldments (Ref 25). 8 (EQ 32) The variables α and H0 depend on the critical temperature of interest. Several values are given in Table 1. 8 in. 9 in. 39 The units used in Eq 32 are important, because the same units that were used in developing the equation must be employed in its application.
9). For a sufficiently strong pressure gradient, pB, the liquid level under the arc may be pushed down to the bottom of the pool, as shown in Fig. 9(c). High-speed motion pictures of the effect of sulfur additions on weld pool fluid flow in 21-6-9 stainless steel showed behavior similar to that in Fig. 9(c) after large sulfur additions. Sulfur additions substantially reduce the weld pool surface tension and thereby increase the effect of the plasma jet. FIG. 9 EFFECT OF ARC PRESSURE ON THE WELD POOL FOR STATIONARY AND TRAVELING WELDS.