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| Displacement: | |||||
| k i | 1 | 2 | 3 | 4 | 5 |
| 1 | 0 | ||||
| 2 | -.020154 | 0.020154 | |||
| 3 | -.024759 | 0 | 0.024759 | ||
| 4 | -.023445 | -.019519 | 0.019519 | 0.023445 | |
| 5 | -.021226 | -.028299 | 0 | 0.028299 | 0.021226 |
| Compression: | |||||
| k i | 1 | 2 | 3 | 4 | 5 |
| 1 | 0 | ||||
| 2 | -.0764 | 0.0764 | |||
| 3 | -.0554 | 0 | 0.0554 | ||
| 4 | -.0418 | -.0271 | 0.0271 | 0.0418 | |
| 5 | -.0334 | -.0358 | 0 | 0.0358 | 0.0334 |
The numbers are the coefficients of 
in the expansion. Note the number of digits in the table for the compression. The terms in summation (33) decay rather slowly with j and although 200 terms were used to compute the above values, they are only valid up to the third significant digit. For the displacement the contributions decay much faster
with j and are almost entirely determined by the (k+2)th contribution.
|
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