Proceedings of the Annual Meeting, 1. ciltSociety for the Promotion of Engineering Education., 1987 |
Kitabın içinden
82 sonuçtan 1-3 arası sonuçlar
Sayfa 88
The second formulation is the electric vector potential , - 100 Ēz = V xk az vxq = 0
VO , = 0 Figure 3 : Current Ummiting Fun ( acalod ) And the solutions to the
above systems of equation renders E , and E , . Then the error can be computed
as ...
The second formulation is the electric vector potential , - 100 Ēz = V xk az vxq = 0
VO , = 0 Figure 3 : Current Ummiting Fun ( acalod ) And the solutions to the
above systems of equation renders E , and E , . Then the error can be computed
as ...
Sayfa 268
561 I 1867 3850 P - V Diagram 1062 1 - V Diagran TO BEGIN PRESS - ' Fl ' FOR
EXPERIMENT ' TS ' POR COMPLETE P - T DIAGRAM ' F ' FOR
DEMONSTRATION AROUND CRITICAL POINT ' T18 TO END Figure 3 . Program
Menu - 14 .
561 I 1867 3850 P - V Diagram 1062 1 - V Diagran TO BEGIN PRESS - ' Fl ' FOR
EXPERIMENT ' TS ' POR COMPLETE P - T DIAGRAM ' F ' FOR
DEMONSTRATION AROUND CRITICAL POINT ' T18 TO END Figure 3 . Program
Menu - 14 .
Sayfa 466
Figure 4 ( a ) shows the loopclosure equation graphically . Now consider the
triangle formed by A , B , 04 . For side 04A , the magnitude and direction is known
because of the previous step . For sides OB and AB the magnitudes are known
but ...
Figure 4 ( a ) shows the loopclosure equation graphically . Now consider the
triangle formed by A , B , 04 . For side 04A , the magnitude and direction is known
because of the previous step . For sides OB and AB the magnitudes are known
but ...
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