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zero-phase fraction line

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Published: 01 August 2018
line is where the solid phase fraction is zero, that is, the line that defines the temperatures and compositions where the solid phase starts to appear in equilibrium. As solidification progresses, solute has no time to diffuse into the previously formed solid and the solid average composition (dashed More
Book Chapter

Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2012
DOI: 10.31399/asm.tb.pdub.t53420191
EISBN: 978-1-62708-310-2
... changes occur. Fig. 10.5 Isopleth through hypothetical ternary phase diagram at a constant 40% C . Adapted from Ref 10.1 Single-Phase Boundary and Zero-Phase Fraction Lines Two-dimensional (2-D) sections of any multicomponent phase diagram, whether it is an isotherm or an isopleth, can...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 July 2009
DOI: 10.31399/asm.tb.fdmht.t52060111
EISBN: 978-1-62708-343-0
... 1.25 971/1724 179 89.7 (483⇔871) (141/250) CCOP 900⇔1600 0.90 0.32 1.22 729/1441 220 28.3 (483⇔871) (106/209) (a) HROP, high-rate out-of-phase; CCOP, compressive creep out-of-phase. (b) Includes time at zero load during temperature changes between maximum. and minimum...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 August 1999
DOI: 10.31399/asm.tb.lmcs.t66560029
EISBN: 978-1-62708-291-4
... isothermal transformation and continuous-cooling diagrams and how to recognize the effect of various alloying elements. alloying elements constitutional diagram continuous-cooling diagram isothermal transformation diagram phase transformations It has been established that a microscopical...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2007
DOI: 10.31399/asm.tb.smnm.t52140055
EISBN: 978-1-62708-264-8
... not elongate at the hot working temperature. Unless their volume fraction becomes excessive, they do not lead to dramatic reductions of toughness. Effect of Alloying Elements on the Iron-Carbon Phase Diagram The phase diagrams for steel presented in Chapter 3, such as Fig. 3.5 , are all pure iron...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2019
DOI: 10.31399/asm.tb.mfadr7.t91110461
EISBN: 978-1-62708-247-1
... of semiconductor devices and identify defects that introduce crystallographic phase variations of the transmitted electron waves. An example of a diffraction contrast image of poly silicon lines is shown in Figure 11 . The contrast variation in the polysilicon lines is a result of scattering incident electrons...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2012
DOI: 10.31399/asm.tb.pdub.t53420041
EISBN: 978-1-62708-310-2
... Ref 3.1 If a pure component is heated from absolute zero, the heat supplied will raise the enthalpy at a rate determined by C p (solid) along line ab in Fig. 3.4 . Meanwhile, the free energy will decrease along line ae . At T m , the heat supplied to the system will not raise its...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 June 2008
DOI: 10.31399/asm.tb.emea.t52240053
EISBN: 978-1-62708-251-8
... energy for the liquid rises at a faster rate than that of the solid, as illustrated in Fig. 4.3 . At T m , the equilibrium melting point, the free energies of both phases are equal. However, solidification does not occur, because the free-energy change is zero (Δ G = 0) and it must be negative. Below...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2006
DOI: 10.31399/asm.tb.fdsm.t69870123
EISBN: 978-1-62708-344-7
... and damage levels. Ref 6.17 (1981) DLDR, Manson and Halford’s (double linear damage rule) Simplifies DLDC concept with break points forced along a line of constant damage separating phase I and II damage. Each phase has a fatigue curve that adds to become the total fatigue life curve. Failure occurs...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2012
DOI: 10.31399/asm.tb.pdub.t53420015
EISBN: 978-1-62708-310-2
..., can be independently changed at point 2 if two phases are to remain. A similar analysis shows that there are zero degrees of freedom at point 3, the triple point, in Fig. 2.4 . The triple point is also called an invariant point because, at that location on the diagram, all externally controllable...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 December 1984
DOI: 10.31399/asm.tb.mpp.t67850410
EISBN: 978-1-62708-260-0
... length of randomly placed lines within the phase of interest Σ L α is divided by the total line length L T to obtain the lineal fraction: (6-2) L L = Σ L α L T = V V A number of devices have been developed to facilitate the analysis. One...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2007
DOI: 10.31399/asm.tb.smnm.t52140021
EISBN: 978-1-62708-264-8
.... The phase diagram provides information about the volume fraction of the proeutectoid phase that will be present between the pearlite grains. Suppose the steel were a 1075 steel. The 0.75% C composition is very close to the pearlite composition of 0.77, and so, this steel must be nearly 100% pearlite...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2012
DOI: 10.31399/asm.tb.pdub.t53420263
EISBN: 978-1-62708-310-2
... Plot of the phase fraction of α as a function of temperature for one Ti-64 alloy. The line was calculated by PanTi and experimental data. Source: Ref 13.7 and 13.9 as published in Ref 13.2 Fig. 13.12 Plot of the phase fraction of β as a function of temperature for one Ti-6242 alloy...
Book Chapter

Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2007
DOI: 10.31399/asm.tb.smnm.t52140133
EISBN: 978-1-62708-264-8
... were discussed briefly in Chapter 6, “The Low-Alloy AISI Steels.” By drawing a vertical section through the Cr-Fe-C ternary diagram at a fixed %C, a diagram is obtained that approximates the pure chromium-iron phase diagram as the %C approaches zero. Figure 13.4(a) shows a vertical section through...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 June 2008
DOI: 10.31399/asm.tb.emea.t52240017
EISBN: 978-1-62708-251-8
... of vibration is almost independent of temperature, but the amplitude increases with increasing temperature. For copper, the amplitude near room temperature is approximately one-half its value near the melting point and approximately twice its value near absolute zero. As the temperature is increased...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 March 2012
DOI: 10.31399/asm.tb.pdub.t53420363
EISBN: 978-1-62708-310-2
... of the electrons. At some equilibrium distance, the attractive and repulsive forces balance each other and the net force is zero. At this equilibrium distance, the potential energy is at a minimum, as shown in Fig. A.2 . The magnitude of this energy is known as the bond energy, usually expressed in kJ/mol...
Series: ASM Technical Books
Publisher: ASM International
Published: 31 December 2020
DOI: 10.31399/asm.tb.phtbp.t59310001
EISBN: 978-1-62708-326-3
... classified under four main divisions: point defects, line defects, planar defects, and volume defects. Point Defects Point defects (also known as zero-dimensional defects) occur at any lattice node with a vacancy (missing atom), an extra (interstitial) atom, or an impurity (substitutional) atom ( Fig...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 October 2011
DOI: 10.31399/asm.tb.mnm2.t53060013
EISBN: 978-1-62708-261-7
... of equilibrium phase diagrams, the role of enthalpy and Gibb’s free energy in chemical reactions, and a method for determining phase compositions along the solidus and liquidus lines. atomic diffusion body-centered cubic systems crystal defects equilibrium phase diagram face-centered cubic systems...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.tb.msisep.t59220129
EISBN: 978-1-62708-259-4
.... Solidification starts at T liquidus (T l ) with the appearance of a solid with kC 0 composition. The “liquidus” line is where the solid phase fraction is zero, that is, the line that defines the temperatures and compositions where the solid phase starts to appear in equilibrium. As solidification progresses...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 June 2008
DOI: 10.31399/asm.tb.emea.t52240303
EISBN: 978-1-62708-251-8
... , in terms of the atom fraction (at.%/100) as follows: (Eq 17.17) ρ i = A c i ( 1 − c i ) where A is a composition-independent constant that is a function of both the impurity and host metals. For a two-phase alloy consisting of α and β phases, a rule-of-mixtures expression may...