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Search Results for kinetic energy
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Published: 31 December 2017
Fig. 8 Relationship between the kinetic energy of the particles and the erosion mass loss for AISI 316L (UNS S31603) and LDX 2101 (UNS S32101) stainless steels and various types of erodents and for certain erodents with a different size in 10 wt% slurries. Source: Ref 69
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Published: 31 December 2017
Fig. 22 Erosion parameter (excluding the initial kinetic energy term) calculated from Eq 1 is plotted against the experimentally determined volumetric erosion rate. Good correlation is observed for the range of materials studied here. Adapted from Ref 34
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Published: 01 January 1996
Fig. 7 Impact force versus impacter kinetic energy for [45/0/−45/90] 6s IM7/8551-7 and AS4/3501-6 laminates and a 12.7 mm diam tup
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Published: 01 January 1996
Fig. 11 Impact force versus impacter kinetic energy for [45/0/−45/90] ns AS4/3501-6 uniweave (RFI) and a 12.7 mm diam tup
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Published: 01 January 1996
Fig. 12 Damage diameter versus impacter kinetic energy for [45/0/−45/90] ns AS4/3501-6 uniweave (RFI) and a 12.7 mm diam tup
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Published: 01 January 1996
Fig. 19 Impact force versus impacter kinetic energy for [45/0/−45/90] 6s AS4/3501-6 laminates of various sizes
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Published: 01 January 1996
Fig. 20 Minimum impacter kinetic energy to reduce burst pressure of small and large pressure vessels.
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Published: 01 January 1996
Fig. 21 Postimpact compressive strength versus impacter kinetic energy for 6.3 mm thick AS4/3501-6 coupons and panels with three bolted spars
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Published: 01 January 1996
Fig. 22 Damage diameter versus impacter kinetic energy for falling-weight impact tests and gas-gun tests conducted on [45/0/−45/90] 6s AS4/3501-6 laminates
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Published: 15 December 2019
Fig. 5 Dependence of escape depth, λ, on kinetic energy of electrons. Data points are experimental measurements for various elements; full curve is an empirical least-squares fit. Source: Ref 27 (adapted from Ref 14 )
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Series: ASM Handbook
Volume: 14A
Publisher: ASM International
Published: 01 January 2005
DOI: 10.31399/asm.hb.v14a.a0003973
EISBN: 978-1-62708-185-6
... Abstract Hammers and high-energy-rate forging machines are classified as energy-restricted machines as they deform the workpiece by the kinetic energy of the hammer ram. This article provides information on gravity-drop hammers, power-drop hammers, die forger hammers, counterblow hammers...
Abstract
Hammers and high-energy-rate forging machines are classified as energy-restricted machines as they deform the workpiece by the kinetic energy of the hammer ram. This article provides information on gravity-drop hammers, power-drop hammers, die forger hammers, counterblow hammers, and computer-controlled hammers. It describes the three basic designs of high-energy-rate forging (HERF) machines: the ram and inner frame, two-ram, and controlled energy flow. The article reviews forging mechanical presses, hydraulic presses, drive presses, screw presses, and multiple-ram presses.
Series: ASM Handbook
Volume: 18
Publisher: ASM International
Published: 31 December 2017
DOI: 10.31399/asm.hb.v18.a0006374
EISBN: 978-1-62708-192-4
... and the classifications of brake lining materials. It discusses the effect of formulation compositions and manufacturing processes and the effect of braking operation conditions. The article provides information on aircraft brake linings, which operate under a wide range of kinetic energy conditions. The morphology...
Abstract
This article focuses on friction and wear of automotive and aircraft brakes. It provides a comparison of friction and wear behaviors, frictional characteristics, and frictional performance of the friction materials. The article describes the components of brake friction materials and the classifications of brake lining materials. It discusses the effect of formulation compositions and manufacturing processes and the effect of braking operation conditions. The article provides information on aircraft brake linings, which operate under a wide range of kinetic energy conditions. The morphology effect of graphite on automotive brake drum and disk is explained. The article also describes the characteristics of specific wear rates for both normal and local cast iron in automotive brake drums and disk rotors. It provides information on noises, vibrations, and harshness caused by brake pads. The article concludes with information on physical and chemical testing of brakes and toxicity of brake formulation and regulations.
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Published: 31 October 2011
Fig. 5 Schematic illustrations of the three basic ways in which electrical energy, supplied by a power source, can be used to heat and fusion weld a metal, including (a) use of the kinetic energy of electrons and positive ions in an arc to bombard the workpiece and produce heat (in arc welding
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Published: 31 October 2011
Fig. 10 Distribution of turbulent variables in the weld pool. (a) Dimensionless viscosity, μ t /μ. (b) Dimensionless thermal conductivity, k t / k . (c) Turbulent kinetic energy, m 2 /s 2 × 10 −4 . (d) Dissipation rate of turbulent kinetic energy, m 2 /s 3 × 10 −4 . Adapted from Ref 15
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Published: 15 December 2019
Fig. 10 Mean free path for inelastic scattering of electrons as a function of kinetic energy of electrons travelling in a solid. Electrons in the low-energy electron diffraction energy range travel only of the order of 0.4 to 2 nm in the crystal before losing energy and thus becoming lost
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in Introduction and Fundamental Principles of Induction Melting
> Induction Heating and Heat Treatment
Published: 09 June 2014
Fig. 8 Measured distribution of the time averaged flow velocity and specific turbulent kinetic energy in an experimental induction crucible furnace
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Published: 01 January 1996
Fig. 18 Calculated impact force versus natural frequency ratio squared for AS4/3501-6 [45/0/−45/90] 6s and an impacter kinetic energy = 13.5J
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Published: 01 January 1986
. The kinetic energy left in a projectile of mass m after an elastic backscattering collision with an atom of mass m is a fraction k m of the incident energy ( Eq 1 and 2 ). The abscissa yields K m for a selection of elements, assuming that the projectiles are helium ions ( m = 4). Source: Ref
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Published: 30 September 2014
Fig. 27 Schematic showing basic elements of an ion-nitriding system. High-kinetic-energy nitrogen-ion bombardment on the workpiece surface is indicated by blue-white glow discharge around the components.
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Published: 15 December 2019
for a selection of elements. The kinetic energy left in a projectile of mass m after an elastic backscattering collision with an atom of mass m is a fraction k m of the incident energy ( Eq 1 and 2 ). The abscissa yields K m for a selection of elements, assuming that the projectiles are helium
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