By C. Christopoulos, P. Sewell, J. Paul (auth.), İzzet Cem Göknar, Levent Sevgi (eds.)
This publication uniquely combines new advances within the electromagnetic and the circuits&systems idea. It integrates either fields concerning computational facets of universal curiosity. emphasised topics are these equipment which mimic brain-like and electrodynamic behaviour; between those are mobile neural networks, chaos and chaotic dynamics, attractor-based computation and movement ciphers.
The e-book comprises rigorously chosen contributions from the Symposium CCN2005. photos from the bestowal of Honorary Doctorate levels to Leon O. Chua and Leopold B. Felsen are included.
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Additional resources for Complex Computing-Networks: Brain-like and Wave-oriented Electrodynamic Algorithms
Thus, for higher frequencies a significant difference is observed between the values of the induced load current predicted by the three models. 9 1 Fig. 10. Magnitude of the induced load current due to an incident plane wave with a linei i arly-polarized, x-directed electric field, propagating in +y-direction. E = E x xˆ , k = k y yˆ , ZL1 = ZL2 =Z0 As a second example we consider the case where the electric field of the incii i dent wave is E = E x xˆ , with propagation vector k = k y yˆ . The line terminations are assigned the values ZL1 = ZL2 = Z0, where Z0 is the characteristic impedance of the transmission line.
Combining this result with (9), allows us to cast (7) in the form i ³ S xt r ˆ = ( E × H ) ⋅ nds − ³ l/2 i D E x ( x , s /2, 0) I t ( x ) dx. −l / 2 (10) A similar development for the x-directed section of the bottom wire yields i ³ S xb r ˆ =− ( E × H ) ⋅ nds ³ l/2 i −l / 2 D E x ( x , − s / 2, 0) I b ( x ) dx. (11) Following an identical process as above it is straightforward to show that the remaining integral on the right-hand side of (4) may be cast in the form − ³ Sy i r ³ ˆ = ( E × H ) ⋅ nds s/2 −s / 2 i D E y ( −l / 2, y , 0) I l ( y ) dy + ³ s/2 −s / 2 i D (12) E y (l / 2, y , 0) I r ( y ) dy.
Magnitude of induced load current due to an incident plane wave with a linearly-polarized, y-directed electric field, propagating in the +x-direction. i i E = E y yˆ , k = k x xˆ , ZL1 = 0, ZL2 = Z0 Numerical Examples The response of the terminated transmission line excited by an incident electromagnetic field is obtained from (13–15). The line is terminated as shown in Fig. 1 with the source V01 shorted. The output of interest is the load current IL2 at the terminating impedance ZL2, computed as a function of frequency for different polarizations and propagation directions of the incident field.