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Fig. 4 Time variation for the first two mode coefficients from the three GNSS stations data sets.
By considering the first two mode shapes, it can be noted that closure of midspan crack, affects the 1(mathrm{st}) mode of vibration while leaving the 2(mathrm{nd}) one practically unaffected for the point of contraflexure at midspan in the second flexural mode shape.
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Numerical results are presented for the first two modes.
The first two modes are named the SAW mode and the SEZAWA mode.
The non-dimensional static buckling load almost remains constant for the first two modes.
The first two modes do lose some of their IMF properties in the process.
Note that the first two modes are not separated by 2-D Fourier transform.
Numerical results are presented for different flexural stiffness values and for the first two modes.
The natural frequency results showed that the adjustable ranges for the first two modes could all reach more than 30%.
Even when the first two modes are measured under the 5percentt corruption level, the added mass could be estimated properly.
The significance that the first two modes of vibration and damping play in the force response is also addressed.
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CEO of Professional Science Editing for Scientists @ prosciediting.com