Proceedings of the Annual Meeting, 1. ciltSociety for the Promotion of Engineering Education., 1987 |
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67 sonuçtan 1-3 arası sonuçlar
Sayfa 174
Session 1266 Using Impulse and Higher - Order Singularity Functions to Simplify
Laplace Transforms Richard D . Morris Assistant Dean School of Engineering
and Applied Science Portland State University Portland , Oregon Go ( t ) = 0 , 160
...
Session 1266 Using Impulse and Higher - Order Singularity Functions to Simplify
Laplace Transforms Richard D . Morris Assistant Dean School of Engineering
and Applied Science Portland State University Portland , Oregon Go ( t ) = 0 , 160
...
Sayfa 175
The tag on indicates that the quantity Keo is the result of taking the Laplace
transform of a singularity function . ... L { K On ( t o ) } = Ken - 80 , to 20 and finite (
20 ) ( 13 ) Thus , the Laplace transform of all singularity functions that occur when
t 20 ...
The tag on indicates that the quantity Keo is the result of taking the Laplace
transform of a singularity function . ... L { K On ( t o ) } = Ken - 80 , to 20 and finite (
20 ) ( 13 ) Thus , the Laplace transform of all singularity functions that occur when
t 20 ...
Sayfa 176
2 still contains two step functions . y ( t ) = L - ' ( Y ( s ) } = L - ' ( H ( s ) F ( s ) } , t > 0
( 25 ) By using the tag , the effect of the initial condition at t = 0would be included
in the response . f ( t ) We now consider the Laplace transform of piecewise ...
2 still contains two step functions . y ( t ) = L - ' ( Y ( s ) } = L - ' ( H ( s ) F ( s ) } , t > 0
( 25 ) By using the tag , the effect of the initial condition at t = 0would be included
in the response . f ( t ) We now consider the Laplace transform of piecewise ...
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