Electron scattering anisotropy and the electrical resistivity of dislocations in aluminium and aluminium alloys

1986 ◽  
Vol 16 (2) ◽  
pp. 203-208 ◽  
Author(s):  
R D Barnard
Keyword(s):  
Electrical Resistivity ◽  
Electron Scattering ◽  
Aluminium Alloys ◽  
Scattering Anisotropy

scholarly journals Electrical Resistivity of Ni–Fe Wires Coated with Sn Using low-Pressure Chemical Vapor Deposition

Coatings ◽  
2020 ◽  
Vol 10 (4) ◽  
pp. 317
Author(s):  
Jun-Hyun Kim ◽  
Jeong Geun Bak ◽  
Chang-Koo Kim
Keyword(s):  
Electrical Resistivity ◽  
Chemical Vapor Deposition ◽  
Electron Scattering ◽  
Vapor Deposition ◽  
Deposition Temperature ◽  
Chemical Vapor ◽  
Low Pressure ◽  
Reaction Products ◽  
Irregular Shapes ◽  
Pressure Chemical

In this study, we demonstrated that the deposition of Sn on Ni–Fe wires using low-pressure chemical vapor deposition (LPCVD) can be used to control the electrical resistivity of the wires. Furthermore, the effect of the deposition temperature on the resistivity of the Ni–Fe wires was investigated. The resistivity of the Sn-deposited Ni–Fe wires was found to increase monotonically with the deposition temperature from 550 to 850 °C. Structural and morphological analyses revealed that electron scattering by Ni3Sn2 and Fe3Sn particulates, which were the reaction products of LPCVD of Sn on the surface of the Ni–Fe wires, was the cause of the resistivity increase. These coalesced particulates displayed irregular shapes with an increase in the deposition temperature, and their size increased with the deposition temperature. Owing to these particulate characteristics, the Sn content increased with the deposition temperature. Furthermore, the temperature dependency of the Sn content followed a pattern very similar to that of the resistivity, indicating that the atomic content of Sn directly affected the resistivity of the Ni–Fe wires.

On the evidence for electron-electron scattering in the electrical resistivity of In

1970 ◽  
Vol 8 (24) ◽  
pp. 2129-2133 ◽  
Author(s):  
O.J. Bressan ◽  
A.E. Ridner ◽  
C.A. Luengo ◽  
B. Alascio
Keyword(s):  
Electrical Resistivity ◽  
Electron Scattering

Is potassium a simple metal?

1982 ◽  
Vol 60 (5) ◽  
pp. 693-702 ◽  
Author(s):  
Nathan Wisbr
Keyword(s):  
Electrical Resistivity ◽  
Electron Scattering ◽  
Phonon Scattering ◽  
Measured Data ◽  
The Other ◽  
Simple Metal ◽  
Temperature Dependent ◽  
Dependent Part ◽  
Simple Behavior ◽  
Electron Phonon Scattering

The temperature-dependent part of the electrical resistivity ρ(T) of a metal consists of the sum of two terms, one term being due to electron–phonon scattering ρcp(T) and the other term being due to electron–electron scattering ρcc(T). One may write[Formula: see text]where θD, is the Debye temperature of the metal and the coefficients C and A give the magnitudes of ρcp(T) and ρcc(T), respectively. For a metal whose electrical resistivity exhibits "simple" behavior, it had been expected that the measured data for ρ(T) would have the following properties. (i) The function f(T/θD) should approach (T/θD) for [Formula: see text]. (ii) The magnitude of the coefficient C should be the same, or nearly so, for all measured samples. (iii) The magnitude of the coefficient A should be the same, or nearly so, for all measured samples.The low-temperature ρexpt(T) data for potassium, which has by now been measured for many samples, exhibit none of these three properties. A discussion will be presented of the reasons for this "non-simple" behavior of ρexpt(T) for potassium.

scholarly journals Electron scattering processes in Ho5(SixGe1−x)4compounds: Electrical resistivity studies

2011 ◽  
Vol 83 (14) ◽  
Author(s):  
A. M. Pereira ◽  
J. P. Araújo ◽  
J. R. Peixoto ◽  
M. E. Braga ◽  
P. A. Algarabel ◽  
...  
Keyword(s):  
Electrical Resistivity ◽  
Electron Scattering

THE LOW-TEMPERATURE THERMAL CONDUCTIVITY, ELECTRICAL RESISTIVITY, AND THERMOELECTRIC POWER OF DILUTE SILVER ALLOYS WITH MANGANESE

1966 ◽  
Vol 44 (10) ◽  
pp. 2293-2302 ◽  
Author(s):  
H. L. Malm ◽  
S. B. Woods
Keyword(s):  
Thermal Conductivity ◽  
Electrical Resistivity ◽  
Low Temperature ◽  
Thermoelectric Power ◽  
Electron Scattering ◽  
The Other ◽  
Temperature Measurements ◽  
Silver Alloys ◽  
Temperature Range ◽  
Dilute Alloy

Low-temperature measurements of electrical resistivity, thermal conductivity, and thermoelectric power on silver alloys containing 0.005, 0.067, 0.11, and 0.31 at.% of manganese are reported. The same specimens were used for the measurement of all properties over the temperature range from 2 to 25 °K. The well-known minimum and maximum are observed in the electrical resistivity of the three more concentrated alloys and the minimum is visible in the most dilute alloy near the lowest temperatures of measurement. Associated effects are observed in the other properties and their possible relationship to theoretical electron scattering mechanisms, particularly that of Kondo, is discussed.

Electrical Resistivity Measurements: A Sensitive Tool for Studying Aluminium Alloys

2006 ◽  
Vol 519-521 ◽  
pp. 1391-1396 ◽  
Author(s):  
B. Raeisinia ◽  
Warren J. Poole
Keyword(s):  
Electrical Resistivity ◽  
Aluminum Alloys ◽  
Aluminium Alloys ◽  
Room Temperature ◽  
Pure Aluminum ◽  
Cold Work ◽  
Resistivity Measurements ◽  
Sensitive Tool ◽  
Solute Atoms

This paper examines the challenges which are encountered when using electrical resistivity measurements for characterization of microstructures in aluminum alloys. Experimental examples are provided of electrical resistivity studies conducted on two aluminum alloys, a heattreatable alloy (AA6111) and a non-heat-treatable alloy (AA5754), which demonstrate how the technique can be used to characterize changes in the microstructure. Results on AA6111 show that the dependence of the measurement on solute atoms and fine scale precipitates makes deconvolution of the resistivity signal non-trivial and therefore, utilization of supplementary technique(s) in conjunction with electrical resistivity measurements is essential. In the next example, room temperature electrical resistivity measurements as a function of cold work for AA5754 illustrate a larger resistivity contribution from dislocations in this alloy as compared to that reported for pure aluminum. The interaction of solutes and dislocations is cited as the possible source for the increased dislocation contribution.

The transport properties of rubidium, and electron–electron scattering

1979 ◽  
Vol 57 (6) ◽  
pp. 871-883 ◽  
Author(s):  
J.G. Cook
Keyword(s):  
Thermal Conductivity ◽  
Electrical Resistivity ◽  
Transport Properties ◽  
Thermoelectric Power ◽  
Electron Scattering ◽  
Strong Evidence ◽  
Freezing Point ◽  
Thermal Contraction ◽  
Thomas Fermi

The electrical resistivity, thermal conductivity, and thermoelectric power of Rb have been measured between 40 and 300 K. Two of the samples were bare, to avoid thermal contraction difficulties; the softness of these samples necessitated further, calibration, measurements on a third sample in glass, just below the freezing point. The electrical resistivity values agree well with published values of Dugdale and Phillips. The Lorenz function, not previously examined in detail above 25 K, shows strong evidence of electron–electron scattering, of a strength intermediate to that calculated by Kukkonen for Thomas–Fermi screening, and for Geldart–Taylor screening. Such scattering appears to have affected the thermoelectric power as well.

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