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3-D solid elements

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Published: 01 January 2001
Fig. 1 An I-beam discretized with 3-D solid elements More
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003389
EISBN: 978-1-62708-195-5
... on micromechanics and macromechanics. The article describes the FEA of 3-D solid elements, 2-D cylindrical shell elements, and 1-D beam elements. It contains a table that lists the commercially available finite element codes related to the analysis of fibrous composite materials. The article presents classical...
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
... a differential volume element of the solidifying alloy and assume no diffusion in the solid. Mass conservation of any solute element in the alloy, in the absence of transport across the volume element, is: (Eq 1) ( C L − C S * ) d f S = ( 1 − f S ) d C L where C L...
Book Chapter

Series: ASM Handbook
Volume: 13B
Publisher: ASM International
Published: 01 January 2005
DOI: 10.31399/asm.hb.v13b.a0006544
EISBN: 978-1-62708-183-2
... unit cell is given in Fig. 3(a) 3(b) , 3(c) , and 3(d) and is identified next to it. To assist in classification and identification, each crystal structure type is assigned a representative substance (element or phase) having that structure. The substance selected is called the structure...
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001726
EISBN: 978-1-62708-178-8
... or † = limited number of elements or groups; S or * = under special conditions; D = after dissolution/extraction; V = volatile solids or components (can also be analyzed by GC/MS), pyrolyzed solids; C = crystalline solids Method Elem Speciation Compound Iso/Mass Qual Semiquant Quant Macro/Bulk...
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001059
EISBN: 978-1-62708-162-7
...- corrosion cracking (b) Gas Arc Resistance spot and seam 1050 O A A A E A A B A A Chemical equipment, railroad tank cars  H12 A A A E A A A A A  H14 A A A D A A A A A  H16 A A B D A A A A A  H18 A A B D A A A A A 1060 O A A A E...
Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003085
EISBN: 978-1-62708-199-3
... freezing, and (d) heating of a homogenized sample. Source: Ref 1 At the left end of the line between α 1 and L 1 , the bulk composition is Y % component B and 100 - Y % component A, and consists of 100% α solid solution. As the percentage of component B in the bulk composition moves...
Series: ASM Handbook
Volume: 4E
Publisher: ASM International
Published: 01 June 2016
DOI: 10.31399/asm.hb.v04e.a0006257
EISBN: 978-1-62708-169-6
... of the liquid at a given temperature (as in, e.g., Fig. 2 ). When an incremental amount of solid ( df s ) forms, C s df s solute transfers from the liquid to the solid. As a result, the incremental change in the liquid composition is given by: (Eq 3) d C l = ( C l − C s ) d f...
Series: ASM Handbook
Volume: 11B
Publisher: ASM International
Published: 15 May 2022
DOI: 10.31399/asm.hb.v11B.a0006941
EISBN: 978-1-62708-395-9
..., on the elastic solid element, Fig. 4(c) the resultant stress, σ (t), on the nearly purely viscous fluid element, and Fig. 4(d) the resultant stress, E(t)* ε 0 , on the viscoelastic material. Viscoelastic materials therefore have finite, non-zero relaxation times ( Ref 4 , 17 ). This generalized description...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005592
EISBN: 978-1-62708-174-0
... by longitudinal stress, they mapped only the longitudinal plastic strain component. The plastic strain field was computed by a 2-D generalized plane-strain thermoelastoplastic welding simulation and was applied as a thermal load in a structural 3-D analysis. Solid elements were used in the structural analysis...
Series: ASM Handbook
Volume: 5
Publisher: ASM International
Published: 01 January 1994
DOI: 10.31399/asm.hb.v05.a0001301
EISBN: 978-1-62708-170-2
... A. , in Thin Solid Films , No. 31 , 1976 , p 3 10.1016/0040-6090(76)90620-9 2. Hofmann S. and Zalar A. , in Thin Solid Films , No. 39 , 1976 , p 219 10.1016/0040-6090(76)90639-8 3. Briggs D. and Seah M.P. , Ed., Practical Surface Analysis, Vol 1: Auger- and X-ray...
Book: Casting
Series: ASM Handbook
Volume: 15
Publisher: ASM International
Published: 01 December 2008
DOI: 10.31399/asm.hb.v15.a0005209
EISBN: 978-1-62708-187-0
... % C s Solid composition % D Diffusion coefficient in liquid m 2 /s D i Diffusion coefficient across interface m 2 /s D s Diffusion coefficient in solid m 2 /s d Diameter m f s Solid fraction … G Temperature gradient K/m G c Concentration gradient %/m...
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006652
EISBN: 978-1-62708-213-6
... number of elements or functional groups; S = under special conditions (i.e., with tandem mass spectrometer detection); D = after dissolution/extraction; V = volatile solids or components, pyrolyzed solids; C = crystalline solids. (a) AES, Auger electron spectroscopy; AFM, atomic force microscopy; COMB...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005609
EISBN: 978-1-62708-174-0
... of radius r , the free-energy change for homogeneous nucleation is given by: (Eq 5) Δ G hom = − 4 3 π r 3 Δ G v + 4 π r 2 γ SL Fig. 6 Schematic illustrations of homogeneous (a and b) and heterogeneous (c and d) nucleation. Figures on the left...
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001115
EISBN: 978-1-62708-162-7
...-temperature measurement was made at liquid helium temperature (4.2 K). The electrical resistivity of a metal can be conveniently divided into three parts: (Eq 4) ρ T = ρ th + ρ d + ρ i where ρ T is total resistivity, ρ th is resistivity due to thermal vibrations...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005431
EISBN: 978-1-62708-196-2
.... As computing power increased, so did the complexity of finite-element modeling and analysis techniques. The first analyses and elements available were limited to 2-D beams and spars. The progression was then toward three-dimensional (3-D) spars and beams, 2-D solid and axisymmetric elements, and the full 3-D...
Series: ASM Handbook
Volume: 1A
Publisher: ASM International
Published: 31 August 2017
DOI: 10.31399/asm.hb.v01a.a0006299
EISBN: 978-1-62708-179-5
... ( − d f s d t ) where f s and df s / dt are given by the extraction of the heat from the sample ( Eq 3 ). By combining these two relations, one finds the growth rate as a function of fraction solid. If this expression is combined with a kinetic law, the growth temperature can...
Series: ASM Handbook
Volume: 22B
Publisher: ASM International
Published: 01 November 2010
DOI: 10.31399/asm.hb.v22b.a0005521
EISBN: 978-1-62708-197-9
..., or 65.61 °F) and 0.15 wt% and 268.52 K (−4.63 °C, or 23.67 °F) and 5.146 wt%, respectively, in the solid and in the liquid. Symmetry conditions are applied at the left and bottom boundaries of the simulation domain in Fig. 3(a) , explaining the arrangement of the four representations (a) to (d) in Fig. 3...
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001089
EISBN: 978-1-62708-162-7
... elements in various states of matter Table 1 The electronic structures of the rare earth elements in various states of matter Element Neutral atom configuration 4 f configuration of known oxidation states Metallic state number of electrons M 2+ M 3+ M 4+ Valence 4 f Sc 3 d 4...
Book: Casting
Series: ASM Handbook
Volume: 15
Publisher: ASM International
Published: 01 December 2008
DOI: 10.31399/asm.hb.v15.a0005214
EISBN: 978-1-62708-187-0
... ) where ℓ β is the thickness of the β-phase, t is the time, and D β is the diffusion coefficient in the β-phase. All other terms are concentrations that are defined in Fig. 10 : (Eq 3) d ℓ β d t = d ℓ β / α d t + d ℓ β / L d t = D β...