Wood Pole Strength and Loading-Key to Resiliency, Require Programs

2017 ◽  
Vol 34 (3) ◽  
pp. 12-15
Author(s):  
Nelson G. Bingel
Keyword(s):  

1989 ◽  
Vol 65 (9) ◽  
pp. 3583-3585 ◽  
Author(s):  
Richard Williams ◽  
J. R. Matey ◽  
Y. Arie ◽  
J. Rathee
Keyword(s):  


1993 ◽  
Vol 119 (7) ◽  
pp. 2199-2214 ◽  
Author(s):  
Nilson Franco ◽  
Patrick J. Pellicane


1944 ◽  
Vol 66 (3-4) ◽  
pp. 94-94 ◽  
Author(s):  
J. E. Goldman


2009 ◽  
Vol 24 (35n37) ◽  
pp. 2984-2994 ◽  
Author(s):  
PHILIP G. RATCLIFFE ◽  
OLEG TERYAEV

We examine the large-x QCD evolution of the twist-three gluonic-pole strength defining an effective T -odd Sivers function, where evolution of the T -even transverse-spin DIS structure function g2 is multiplicative. The result corresponds to a colour-factor modified spin-averaged twist-two evolution.



1962 ◽  
Vol 58 (2) ◽  
pp. 401-404 ◽  
Author(s):  
C. J. Eliezer ◽  
S. K. Roy

The possible existence of a magnetic pole has been under discussion for many years. Dirac worked out in detail an electro-dynamics in which a single magnetic pole is assumed to exist (1,2). He has shown that the existence of such a pole leads naturally to the quantization of charge, the magnetic pole strength g and the electric charge e being related by the equation where p is an integer, h is Planck's constant divided by 2π, and c is the velocity of light.



Author(s):  
E. Bauer

AbstractDirac has shown that in quantum theory free magnetic poles are possible only if their pole strength g is an integral multiple of ℏc/(2e) = 137e/2. The ionization produced by such particles is calculated by the classical impact parameter method and also by quantal perturbation theory; at sufficiently large velocities the rate of loss of energy of poles of unit strength is g2/e2 ≑ 5000 times as large as that of an electron of the same velocity; at low velocities the energy loss of a monopole decreases steadily without rising to a maximum as in the case of electric particles.



We have measured the drift velocity, v, of negative ions in He II at a temperature of 0.34 K and a pressure of 25 bar¶ for electric fields, E , in the range 5 x 10 3 < E < 6 x 10 6 V m -1 . For v <70 m s -1 , the results are in good agreement with the predictions of the roton pair-emission theory of Bowley & Sheard. Even better agreement is obtained by extending the theory to take explicit account of departures from parabolicity of the real dispersion curve at large momenta, variations in the pole strength of high momentum excitations, and the slight increase in the average momentum of excitations emitted at large values of v. For v> 70 m s -1 , however, experiment and theory are in clear disagreement: by v = 80 m s -1 , the measured drag on the ion has become about 100 % larger than the theoretical prediction. We tentatively attribute this discrepancy to the onset at v« 70 m s -1 of a new and, so far, unidentified dissipation mechanism.



1982 ◽  
Vol 9 (4) ◽  
pp. 258-261 ◽  
Author(s):  
Coerte V. Voorhies ◽  
Edward R. Benton
Keyword(s):  
The Core ◽  


NDT World ◽  
2017 ◽  
pp. 46-49
Author(s):  
Кугушев ◽  
Vladimir Kugushev


1975 ◽  
Vol 35 (18) ◽  
pp. 1211-1213 ◽  
Author(s):  
R. S. Poggioli ◽  
A. D. Jackson
Keyword(s):  


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