A Modified Block Diagram to Include Saturation of Synchronous Machines for Dynamic Analysis

1982 ◽  
Vol 2 (2) ◽  
pp. 119-122
Author(s):  
M.K. El-Sherbiny ◽  
A.M. EI-Serafi
1976 ◽  
Vol 22 (4) ◽  
pp. 193-193
Author(s):  
Gantiprasada Rao ◽  
K. R. Palanisamy

Author(s):  
H.T. Yu ◽  
W. Dai ◽  
S.L. Ho ◽  
M.Q. Hu ◽  
S.Y. Yang ◽  
...  

2020 ◽  
Vol 216 ◽  
pp. 01116
Author(s):  
Olimjon Toirov ◽  
Аllabergan Bekishev ◽  
Sardor Urakov ◽  
Utkir Mirkhonov

The article presents the differential equations of a synchronous generator in phase coordinates and in the coordinate system (d, q). In addition, differential equations of synchronous machines with longitudinal-transverse excitation and a block diagram based on these equations are given. The system of differential equations is solved by the operator method. On the basis of a system of differential equations using the Simulink Matlab program, a structural diagram was created and a graph of the self-swinging processes taking place in synchronous machines with conventional and longitudinal-transverse excitation was obtained. On the basis of the obtained graph, the processes of self-swinging of synchronous generators with traditional and longitudinal and transverse excitation are compared.


Author(s):  
D. E. Johnson

Increased specimen penetration; the principle advantage of high voltage microscopy, is accompanied by an increased need to utilize information on three dimensional specimen structure available in the form of two dimensional projections (i.e. micrographs). We are engaged in a program to develop methods which allow the maximum use of information contained in a through tilt series of micrographs to determine three dimensional speciman structure.In general, we are dealing with structures lacking in symmetry and with projections available from only a limited span of angles (±60°). For these reasons, we must make maximum use of any prior information available about the specimen. To do this in the most efficient manner, we have concentrated on iterative, real space methods rather than Fourier methods of reconstruction. The particular iterative algorithm we have developed is given in detail in ref. 3. A block diagram of the complete reconstruction system is shown in fig. 1.


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