6,476 research outputs found
A table of the integrals <for the bessel, hankel, and neumann functions of order zero<
Tabulations of Bessel, Hankel, and Neumann functions of order zer
Error analysis of a weighted least squares process to determine the lunar gravitational field
Error analysis of weighted least squares method to determine lunar gravitational fiel
An adaptive array for interference rejection
Adaptive array based on feedback system for rejection of interfering signal
Recombination lifetimes in gamma-irradiated P-type float zone silicon
Electron decay rate and absorption cross sections for electron holes and recombination in gamma irradiated n-type silico
Recombination luminescence in N-type Czochralski silicon
Recombination luminescence in Czochralski silico
Radiation effects on lasers Technical report, Jul. 1, 1965 - May 31, 1966
Effects of space radiation on laser
The dyadic green's function for an infinite moving medium
Derivation of dyadic Green function for electromagnetic field in moving medium using Minkowski theory and method of Fourier analysi
Defeating the Agricultural Exemption: The Norris LaGuardia Act as a Means for Collective Action for Agricultural Labor
Double potential step chronoamperometry at a microband electrode: Theory and experiment
Numerical simulation is used to characterise double potential step
chronoamperometry at a microband electrode for a simple redox process A + e-
goes to B, under conditions of full support such that diffusion is the only
active form of mass transport. The method is shown to be highly sensitive for
the measurement of the diffusion coefficient of both A and B, and is applied to
the one electron reduction of decamethylferrocene (DMFc), DMFc - e- goes to
DMFc+, in the room temperature ionic liquid 1-propyl-3-methylimidazolium
bistrifluoromethylsulfonylimide. Theory and experiment are seen to be in
excellent agreement and the following values of the diffusion coefficients were
measured at 298 K: D_(DMFc) = 2.50 x 10^(-7) cm^(2) s^(-1) and D_(DMFc+) = 9.50
x 10^(-8) cm^(2) s^(-1)
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