نتایج جستجو برای: s y directions in depth z
تعداد نتایج: 17476637 فیلتر نتایج به سال:
M. Ablikim, M. N. Achasov, X. C. Ai, O. Albayrak, M. Albrecht, D. J. Ambrose, A. Amoroso , F. F. An, Q. An, J. Z. Bai, R. Baldini Ferroli , Y. Ban, D. W. Bennett, J. V. Bennett, M. Bertani, D. Bettoni, J. M. Bian, F. Bianchi , E. Boger, O. Bondarenko, I. Boyko, R. A. Briere, H. Cai, X. Cai, O. Cakir, A. Calcaterra , G. F. Cao, S. A. Cetin , J. F. Chang, G. Chelkov, G. Chen, H. S. Chen, H. Y. Ch...
M. Ablikim, M. N. Achasov, X. C. Ai, O. Albayrak, M. Albrecht, D. J. Ambrose, A. Amoroso , F. F. An, Q. An, J. Z. Bai, R. Baldini Ferroli , Y. Ban, D. W. Bennett, J. V. Bennett, M. Bertani, D. Bettoni, J. M. Bian, F. Bianchi , E. Boger, O. Bondarenko, I. Boyko, R. A. Briere, H. Cai, X. Cai, O. Cakir, A. Calcaterra , G. F. Cao, S. A. Cetin , J. F. Chang, G. Chelkov, G. Chen, H. S. Chen, H. Y. Ch...
M. Ablikim, M. N. Achasov , X. C. Ai, O. Albayrak, M. Albrecht, D. J. Ambrose, A. Amoroso , F. F. An, Q. An, J. Z. Bai, R. Baldini Ferroli, Y. Ban, D. W. Bennett, J. V. Bennett, M. Bertani, D. Bettoni, J. M. Bian, F. Bianchi , E. Boger, I. Boyko, R. A. Briere, H. Cai, X. Cai, O. Cakir, A. Calcaterra , G. F. Cao, S. A. Cetin , J. F. Chang, G. Chelkov, G. Chen, H. S. Chen, H. Y. Chen, J. C. Chen,...
M. Ablikim, M. N. Achasov, X. C. Ai, O. Albayrak, M. Albrecht, D. J. Ambrose, A. Amoroso, F. F. An, Q. An, J. Z. Bai, R. Baldini Ferroli, Y. Ban, D. W. Bennett, J. V. Bennett, M. Bertani, D. Bettoni, J. M. Bian, F. Bianchi, E. Boger, I. Boyko, R. A. Briere, H. Cai, X. Cai, O. Cakir, A. Calcaterra, G. F. Cao, S. A. Cetin, J. F. Chang, G. Chelkov, G. Chen, H. S. Chen, H. Y. Chen, J. C. Chen, M. L...
T h e conceptual f ramework of a hybrid control s y s t e m architecture i s briefly motivated. It employs neural and f u z z y techniques on a side-by-side basis using each one for the task it i s best suited for. I n this paper, our m a i n interest i s with the adaptation of the f u z z y control knowledge. T h e adaptation algorithm i s based o n reinforcement signals and directly optimizes...
t(x · 1 + 0 · s) = t · x = 0. Therefore f ′ is injective. Now we need to show that im f ′ = ker g′. We have g′(f ′(x/s)) = g(f(x)/s) = (g ◦ f)(x)/s = 0, so im f ′ ⊂ ker g′. Conversely, if g′(y/s) = 0, then g(y)/s = 0, so there exists t ∈ S so that t · g(y) = g(t · y) = 0. Therefore t · y ∈ ker g, so t · y ∈ im f . Let x ∈ X so that f(x) = t · y. Then f ′(x/(st)) = f(x)/(st) = (t · y)/(st) = y/s...
F u z z y D C F : a c o n t r a d i c t i o n i n t e r m s , o r a w a y t o b e t t e r F u z z y D C F : a c o n t r a d i c t i o n i n t e r m s , o r a w a y t o b e t t e r F u z z y D C F : a c o n t r a d i c t i o n i n t e r m s , o r a w a y t o b e t t e r F u z z y D C F : a c o n t r a d i c t i o n i n t e r m s , o r a w a y t o b e t t e r F u z z y D C F : a c o n t r a d i c...
According to Ullman's Structure-from-Motion Theorem [U79], three orthogonal projections of four points in a rigid non-planar configuration uniquely determine their structure, and the relative orientations of the three views, up to a reflection in the image plane. It is here shown that a corresponding result holds for the more general "para-perspective" case, and leads to a rapidly convergent al...
SUMMARY Electromagnetic field theory is applied to the analysis of performance of an induction-motor rotor when it is exposed to a rotating magnetic field of constant amplitude. An idealized model of the rotor is taken and the analysis is simplified by the application of the concept of wave impedance. The model rotor is capable of simulating the effects of tooth-top and zigzag leakage fluxes, b...
testing plays a vital role in any language teaching program. it allows teachers and stakeholders, including program administrators, parents, admissions officers and prospective employers to be assured that the learners are progressing according to an accepted standard (douglas, 2010). the problems currently facing language testers have both practical and theoretical implications but the first i...
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