Proceedings, 1. bölüm |
Kitabın içinden
52 sonuçtan 1-3 arası sonuçlar
Sayfa 171
... Step 5 - 004 - S The final value theorem remains unchanged , f ( ∞ ) f ( x ) = lim SF ( s ) S + 0 ( 45 ) provided ... Step 1 - Laplace transform the original dE , of ( 46 ) , with X ( s ) in its functional form to obtain s2Y ( s ) y ( 0 ) ...
... Step 5 - 004 - S The final value theorem remains unchanged , f ( ∞ ) f ( x ) = lim SF ( s ) S + 0 ( 45 ) provided ... Step 1 - Laplace transform the original dE , of ( 46 ) , with X ( s ) in its functional form to obtain s2Y ( s ) y ( 0 ) ...
Sayfa 175
... step function Kô1 ( t ) . There- fore , upon comparing the two transforms , K Se- " dt L ( K ) = K = S K = ( 13 ) S whereas , L ( Ko1 ( t ) ) = K di ( t ) edt = k [ 82 ( t ) e = " d 00 Ko1 ( t ) e - st K + 0- S = -s K = -800 S * Jo ( t ) ...
... step function Kô1 ( t ) . There- fore , upon comparing the two transforms , K Se- " dt L ( K ) = K = S K = ( 13 ) S whereas , L ( Ko1 ( t ) ) = K di ( t ) edt = k [ 82 ( t ) e = " d 00 Ko1 ( t ) e - st K + 0- S = -s K = -800 S * Jo ( t ) ...
Sayfa 190
... STEP 1. Discretize the region into finite elements . STEP 2. Specify the approximate equation over each element in terms of unknown nodal values- Construct these equations in the form of local matrices . STEP 3. Construct the global ...
... STEP 1. Discretize the region into finite elements . STEP 2. Specify the approximate equation over each element in terms of unknown nodal values- Construct these equations in the form of local matrices . STEP 3. Construct the global ...
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