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Series: ASM Handbook
Volume: 4C
Publisher: ASM International
Published: 09 June 2014
DOI: 10.31399/asm.hb.v04c.a0005898
EISBN: 978-1-62708-167-2
... Abstract This article focuses on the basic turbulent flow, and the thermal, mass-transfer, and hydrodynamic phenomena for use in modeling physical processes during induction melting. It provides a discussion on transport phenomena equations that includes the approximation of convective terms...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005437
EISBN: 978-1-62708-196-2
... Abstract This article presents the governing equations for moving a solidification front, based on the balance of mass, momentum, energy, and solute. It reviews how material properties and geometry can be analyzed in the context of the governing equations. The article provides several example...
Series: ASM Handbook
Volume: 22B
Publisher: ASM International
Published: 01 November 2010
DOI: 10.31399/asm.hb.v22b.a0005525
EISBN: 978-1-62708-197-9
... Abstract This article presents conservation equations for heat, species, mass, and momentum to predict transport phenomena during solidification processing. It presents transport equations and several examples of their applications to illustrate the physics present in alloy solidification...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005636
EISBN: 978-1-62708-174-0
... welding. The article presents the mathematical equations of mass, momentum, energy, and species conservation. It reviews the applications of heat transfer and fluid flow models for different welding processes. Finally, the article discusses the approaches to improve reliability of, and reduce uncertainty...
Series: ASM Handbook
Volume: 4A
Publisher: ASM International
Published: 01 August 2013
DOI: 10.31399/asm.hb.v04a.a0005824
EISBN: 978-1-62708-165-8
... Abstract This article provides an overview of common quenching media, the factors involved in the mechanism of quenching, and process variables, namely, surface condition, mass and section size of the workpiece, and flow rate of the quenching liquid. It describes the methods of quenchant...
Book: Casting
Series: ASM Handbook
Volume: 15
Publisher: ASM International
Published: 01 December 2008
DOI: 10.31399/asm.hb.v15.a0005208
EISBN: 978-1-62708-187-0
... Abstract This article begins with balance equations for mass, momentum, energy, and solute and the necessary boundary conditions for solving problems of interest in casting and solidification. The transport phenomena cover a vast range of length and time scales, from atomic dimensions up...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005579
EISBN: 978-1-62708-174-0
... through 3 are the continuity, moment conservation, and energy conservation equations, respectively. Detailed discussion on the solution of the transport equations and associated boundary conditions to calculate heat and mass transfer in the weld pool is provided elsewhere in this Volume (see...
Series: ASM Handbook
Volume: 13A
Publisher: ASM International
Published: 01 January 2003
DOI: 10.31399/asm.hb.v13a.a0003587
EISBN: 978-1-62708-182-5
.... On the other hand, the reaction involving UF 4 ( Eq 12 ) may have an equilibrium constant that is strongly temperature dependent; therefore, when the salt is forced to circulate through a temperature gradient, a possible mechanism exists for mass transfer and continued attack. Equation 12 is of significance...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005426
EISBN: 978-1-62708-196-2
... to the following three equations of motion: the mass, or continuity, equation: (Eq 1) ∂ ρ ∂ t + ∂ ρ u i ∂ x i = 0 the momentum equation: (Eq 2) ∂ ρ u i ∂ t + ∂ ( ρ u i u j ) ∂ x j = ∂ Σ i j ∂ x j + ρ F i...
Book Chapter

Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005448
EISBN: 978-1-62708-196-2
..., for example, from potential to kinetic energy, heat to work, internal energy to kinetic energy, or transferred from one mass to another as heat or work. First Law of Thermodynamics— Conservation of Energy Closed-System Formulation The general energy equation is Q − W = E f = E i , where...
Book: Casting
Series: ASM Handbook
Volume: 15
Publisher: ASM International
Published: 01 December 2008
DOI: 10.31399/asm.hb.v15.a0005234
EISBN: 978-1-62708-187-0
... A COMPLETE MODEL of the solidification of a metal alloy involves coupling of energy, species, mass, and momentum conservation equations ( Ref 1 , 2 , 3 , 4 , 5 , 6 , 7 ). This article examines critical features of four key areas of modeling transport phenomena associated with casting processes...
Series: ASM Handbook
Volume: 20
Publisher: ASM International
Published: 01 January 1997
DOI: 10.31399/asm.hb.v20.a0002444
EISBN: 978-1-62708-194-8
... lead to the following three equations of motion: the mass, or continuity, equation: (Eq 1) ∂ ρ ∂ t + ∂ ρ u i ∂ x i = 0 the momentum equation: (Eq 2) ∂ ρ u i ∂ t + ∂ ( ρ u i u j ) ∂ x j = ∂ Σ i j ∂ x j...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005450
EISBN: 978-1-62708-196-2
... . For the rate of flow of an extensive property, B , out of the control volume, the mass rate is multiplied by the intensive property, β: (Eq 52) B ˙ = ∑ c s β ρ V ⋅ A Generally, this equation is used in integral form: (Eq 53) B ˙ = ∫ c s β ρ V...
Image
Published: 01 February 2024
Fig. 85 Schematic representation of a quenching system showing boundary conditions for momentum, mass, and energy equations. 1, inlet flow; 2, outlet flow; 3, nonslip wall conditions; 4, free surface; 5, internal mass and momentum source More
Image
Published: 01 February 2024
Fig. 4 Schematic representation of a quenching system showing boundary conditions for momentum, mass, and energy equations. 1, inlet flow; 2, outlet flow; 3, nonslip wall condition; 4, free surface; 5, internal mass and momentum source More
Series: ASM Handbook
Volume: 4F
Publisher: ASM International
Published: 01 February 2024
DOI: 10.31399/asm.hb.v4F.a0007008
EISBN: 978-1-62708-450-5
... on phenomenological and thermofluid equations, which are well-understood engineering principles. However, there are many model parameters, such as heat- or mass-transfer coefficients; solid-state transformation kinetic coefficients; and parameters appearing from the numerical solution, such as mesh characteristics...
Book: Casting
Series: ASM Handbook
Volume: 15
Publisher: ASM International
Published: 01 December 2008
DOI: 10.31399/asm.hb.v15.a0005237
EISBN: 978-1-62708-187-0
... of solidification. As solidification proceeds, eventually C L = C E and the amount of the liquid is (1 − f S ) = f E , so the mass fraction of eutectic in the as-cast microstructure can be calculated. Equations 1 and 2 are best applied to substitutional alloy elements with attendant low mass...
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003402
EISBN: 978-1-62708-195-5
... respectively. V barrel = π DN , where D is the diameter of the screw and N is the speed in revolutions per second. Physical Laws Once the system is identified, one would express conservation of mass, momentum, and energy within the system boundaries ( Ref 21 , 22 ). The conservation equations...
Series: ASM Handbook
Volume: 13A
Publisher: ASM International
Published: 01 January 2003
DOI: 10.31399/asm.hb.v13a.a0003589
EISBN: 978-1-62708-182-5
...-Vink notation and must obey the usual rules of electrochemical equations (mass and charge conservancy). The key difference is an additional conservation law, the “rule of the lattice conservancy,” which states that only a stoichiometric number of the cationic and anionic lattice elements can be formed...
Series: ASM Handbook
Volume: 1A
Publisher: ASM International
Published: 31 August 2017
DOI: 10.31399/asm.hb.v01a.a0006295
EISBN: 978-1-62708-179-5
..., the following equations are used to describe the maximum solubility of carbon (mass%) in various phases as a function of temperature (in °C unless otherwise specified): For the liquid in the interval eutectic temperature, 1600 °C: (Eq 1a) % C max L / Gr = 2.11 + 1.213...