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Published: 01 August 2005
Fig. 1.17 Effect of contact angle on fillet formation and joint filling. Low contact angles tend to be preferred when external fillets can form. In other geometries, higher contact angles result in lower stress concentrations. More
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Published: 01 April 2004
Fig. 1.12 Effect of contact angle on fillet formation and joint filling. Low contact angles tend to be preferred when external fillets can form. In other geometries, higher contact angles result in lower stress concentrations. More
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Published: 01 August 2005
Fig. 1.16 Contact angle of copper-silicon brazes of different composition on vitreous carbon substrates demonstrating the effect of driving force of alloying on wetting rate and the dependence of the equilibrium wetting angle on the reaction product, which is the same in the three cases More
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Published: 01 August 2005
Fig. 1.18 Wettability index (defined as the product of the contact angle and spread area [ Feduska 1959 ]) of silver-base brazes on 316L stainless steel, heated in vacuum for 5 min. Palladium additions clearly have a beneficial effect on wetting and spreading by the braze, despite widening More
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Published: 01 August 2005
Fig. 4.34 A lap joint showing step height, H , fillet radius, R , and contact angle, θ More
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Published: 01 August 2005
Fig. 7.6 Variation of contact angle for gold-silicon alloys on silicon carbide at 1200 °C (2190 °F) as a function of alloy composition in relatively high- and low-oxygen partial pressure atmospheres (the silicon-rich end of the curve is derived by extrapolation because silicon is not molten More
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Published: 01 August 2005
Fig. 7.7 The dependence of the equilibrium contact angle of selected molten metals on titanium carbide as a function of the carbon content of the substrate. In all cases, the contact angle decreases as the carbon deficiency in the titanium carbide, with respect to its stoichiometric value More
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Published: 01 August 2005
Fig. 7.8 The equilibrium contact angle, measured by the sessile drop technique, for molten metals on titanium carbide as a function of the titanium content of the braze. Test temperatures used were 1150 °C (2100 °F) for gold-, copper-, and tin-base alloys and 1050 °C, or 1920 °F for silver More
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Published: 01 August 2005
Fig. 7.14 Wettability (contact angle) and room temperature strength of alumina brazed with copper containing varying amounts of titanium, prepared by brazing in vacuum at 1150 °C (2100 °F) for 15 min More
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Published: 01 August 2005
Fig. 7.23 Variation in contact angle with brazing time for Ag-27Cu-2Ti on Si 3 N 4 . Adapted from Loehman [1988] More
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Published: 01 November 2019
Figure 18 Comparison of 3-axis vs. 5-axis grinding. (Top) In 3-axis the contact angle is invariant and cannot follow the shape of a curved die, producing “saw teeth” that are several microns in size. (Bottom) 5-axis control changes the contact angle to follow the curved shape and yields a well More
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Published: 01 November 2011
Fig. 7.3 Contact angle θ for a liquid droplet on a solid surface: (a) θ > 90°, (b) θ < 90 °, and (c) θ = 0°. γ SL is the solid-liquid surface energy, γ SV is the solid-vapor surface energy, and γ LV is the liquid-vapor surface energy. Source: Ref 7.3 , p 4 More
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Published: 30 April 2020
Fig. 3.30 The contact angle is illustrated for a classic horizontal sessile drop of liquid resting on the solid. The contact angle, θ, represents the balance of the surface energy vectors as illustrated, leading to a mathematical relation between surface energies. More
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Published: 30 April 2020
Fig. 3.33 Contact angle relation to droplet diameter for a constant droplet volume of 0.01 mL. Measuring the droplet diameter is often more accurate than measuring the contact angle. More
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Published: 01 April 2004
Fig. 1.11 Contact angle of copper-silicon brazes of different composition on vitreous carbon substrates demonstrating the effect of driving force of alloying on wetting rate and the dependence of the equilibrium wetting angle on the reaction product. Adapted from Landry, Rado More
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Published: 01 April 2004
Fig. 1.13 Effect of nonwettable surface features on the contact angle of solder on copper. Data of Yost, Hosking, and Frear [1993] augmented by the authors. Lead-tin solder wetted onto a copper surface containing embedded nonwettable particles 10–20 μm (400–800 μin.) in diameter (RMA flux More
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Published: 01 April 2004
Fig. 1.15 Contact angle of lead-tin solder on copper as a function of wetting time, using an inert flux and low superheat. There are four distinct stages of wetting, the last being the equilibrium contact angle that is obtained using more typical process parameters. More
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Published: 01 April 2004
Fig. 3.16 Contact angle for In-48Sn solder on four metal substrates, after heating for 5 min at 250 °C (482 °F), as a function of oxygen partial pressure. Adapted from Preuss, Adolphi, and Werner [1994 ] More
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Published: 01 April 2004
Fig. 4.35 A lap joint showing step height, H , fillet radius, R , and contact angle, θ More
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Published: 01 April 2004
Fig. 5.20 Relationships among spread ratio, spread factor, and contact angle More