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Book Chapter

Series: ASM Desk Editions
Publisher: ASM International
Published: 01 November 1995
DOI: 10.31399/asm.hb.emde.a0003024
EISBN: 978-1-62708-200-6
... employed for analytical prediction of deformation characteristics of polymers. Boltzmann superposition principle creep experiments deformation characteristics dynamic mechanical experiments plastics polymers prediction of deformation time-temperature superposition viscoelastic characteristics...
Book Chapter

By Scott M. Olig
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
... often cannot be considered to behave, even at room temperature, as purely elastic materials. Several superposition principles can be used to extrapolate short-term test data to a longer period of material property behavior. These include the Boltzmann superposition principle, the time-temperature...
Series: ASM Handbook
Volume: 11B
Publisher: ASM International
Published: 15 May 2022
DOI: 10.31399/asm.hb.v11B.a0006909
EISBN: 978-1-62708-395-9
... activated process strongly dependent on temperature, diffusivity ( D ) can, in principle, be expressed as a function of absolute temperature, T , according to the Arrhenius expression: (Eq 6) D ( T ) = D 0 e − ( E a / kT ) In this expression, k is the Boltzmann’s...
Book Chapter

By Michelle Brown
Series: ASM Handbook
Volume: 11B
Publisher: ASM International
Published: 15 May 2022
DOI: 10.31399/asm.hb.v11B.a0006929
EISBN: 978-1-62708-395-9
... temperatures. Source: Ref 14 There are precautions for using time-temperature superposition for the prediction of long-term behavior. The time-temperature superposition is valid only if linear viscoelastic equations are applicable, which is referred to as the Boltzmann linearity. The application limits...
Book Chapter

By Charles P. Poole, Jr., Horatio A. Farach
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001750
EISBN: 978-1-62708-178-8
...) n 1 n 2 = e − h ν / k T where h is Planck's constant, ν is frequency, k is the Boltzmann constant, and T is temperature. Therefore, use of a high applied frequency improves the sensitivity of this technique. In practice, the frequencies in the well-developed radar...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006954
EISBN: 978-1-62708-439-0
... convenient to use c 1 L = 1.191,042,972 × 10 8 W · μm 4 · m −2 · sr −1 and c 2 = 1.438,776,877 × 10 4 μm · K ( Ref 34 ). These constants are based on c 1 L = 2 hc 2 and c 2 = hc / k B , where h is the Planck’s constant, c is the speed of light, and k B is the Boltzmann constant...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005413
EISBN: 978-1-62708-196-2
... temperature changes). As a consequence, the activation enthalpy, Q = kTm / m *, is constant as well during a stress-strain test, where k is the Boltzmann factor. The usual interpretation of these interdependencies is that the thermal and the athermal parts of the flow stress stay in a fixed relation...
Book Chapter

By Chon L. Tsai, Chin M. Tso
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001333
EISBN: 978-1-62708-173-3
... where ∈ is emissivity, σ is the Stefan-Boltzmann constant, θ w is the surface temperature, θ ∞ , is the environmental temperature, and B is the characteristic surface dimension. Natural convection is dominant at a temperature below 550 °C (1020 °F), whereas radiation becomes more important...
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006667
EISBN: 978-1-62708-213-6
... energy ( E , in meV) and a temperature ( T , in Kelvin), associated with the corresponding Maxwell-Boltzmann distribution (because moderated neutron beams can be approximated as ideal gases) . Such characteristics can be inferred from knowledge of the neutron velocity (υ, in m/s) obtained from...
Book Chapter

By Chon L. Tsai
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005588
EISBN: 978-1-62708-174-0
... for an oxidized steel surface), σ is the Stefan-Boltzmann constant (5.6704 × 10 −14 J/s · mm 2 · K 4 , where K is the absolute temperature in °C), θ w is the surface temperature (°C), and θ ∞ is the environmental temperature (°C). The natural convection heat-loss coefficient in air is in the range...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006458
EISBN: 978-1-62708-190-0
... in nonmagnetic and magnetic metals using inductive coupling and, specifically, without the use of a mechanical coupling medium between the transducer and the adjacent metal. The most common coupling mechanisms are the Lorentz force on induced currents (various first-principle methods of deriving Lorentz force...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005421
EISBN: 978-1-62708-196-2
... , individual cavity-growth rate parameter in complex stress state η i , cavity-growth rate along principal direction “ i ” k , Boltzmann constant K , strength coefficient k D, constant dependent on the geometry of the deformation L i , cavity length along principal direction “ i ” λ, cavity spacing...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.9781627084390
EISBN: 978-1-62708-439-0
Book

Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.9781627081788
EISBN: 978-1-62708-178-8
Book

Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.9781627082136
EISBN: 978-1-62708-213-6