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Publication Number:  FHWA-HRT-14-067    Date:  September 2014
Publication Number: FHWA-HRT-14-067
Date: September 2014

 

Dynamic Properties of Stay Cables on The Penobscot Narrows Bridge

CHAPTER 6. SUMMARY OF COMPARISONS

FREQUENCY

The frequencies obtained from phase 1 and phase 2 testing for the cables in fans A and C were nearly equivalent, confirming that damper installation did not affect frequency. Phase 2 testing also showed that frequencies compared well between similar cables from the symmetrically matching fans. The graphs comparing the first two modes between the two phases are shown in figure 51 and figure 52. The remaining graphs for modes 3 through 7 can be found in appendix B. On average, the frequencies match within 3 percent, although the frequencies on some of the shorter cables in the higher modes differed as much as 8 percent.

This graph compares the first mode frequencies from both phase 1 and phase 2 testing. The x-axis represents the cable number, and ranges from 20 to 12. The y-axis represents frequency, and ranges from 0.6 to 1.2 Hertz. Fan A is represented by red triangles for phase 1 and red squares for phase 2 and its values range from 0.8 to 1.2 Hertz. Fan B is represented by green squares for phase 2 and its values range from 0.7 to 0.9 Hertz. Fan C is represented by purple triangles for phase 1 and purple squares for phase 2 and its values range from 0.7 to 0.9 Hertz. Fan D is represented by blue squares for phase 2 and its values range from 0.8 to 1.1 Hertz. Fans A and D are the side span fans and their frequencies match closely, while fans C and B are the main span fans and their frequencies also match. The respective fans also match closely across both phases.
Figure 51. Graph. First mode frequencies.

This graph compares the second mode frequencies from both phase 1 and phase 2 testing. The x-axis represents the cable number, and ranges from 20 to 12. The y-axis represents frequency, and ranges from 1.2 to 2.4 Hertz. Fan A is represented by red triangles for phase 1 and red squares for phase 2 and its values range from 1.5 to 2.3 Hertz. Fan B is represented by green squares for phase 2 and its values range from 1.4 to 1.7 Hertz. Fan C is represented by purple triangles for phase 1 and purple squares for phase 2 and its values range from 1.4 to 1.8 Hertz. Fan D is represented by blue squares for phase 2 and its values range from 1.5 to 2.2 Hertz. Fans A and D are the side span fans and their frequencies match closely, while fans C and B are the main span fans and their frequencies also match. The respective fans also match closely across both phases.
Figure 52. Graph. Second mode frequencies.

First mode theoretical frequencies were calculated for each cable using the string theory equation whose solution is shown in figure 4. These frequencies were then plotted against the field data and the results are shown in figure 53 and figure 54, from phase 1 and phase 2 testing, respectively. Results compared favorably between field and theory, however the longest cables found in fans B and C varied by a small percentage. Complete tables of the numerical values of the first mode theoretical frequencies are presented in appendix A.

These two graphs compare first mode theoretical frequency values to the actual values obtained during phase 1 testing. The left graph shows the data from fan A and the right graph shows the data from fan C. The x-axis on both graphs represents the cable number, and ranges from 20 to 1. The y-axis on both graphs represents the frequency, and ranges from 0 to 3.5 Hertz. In both graphs the theoretical data is marked by blue diamonds, and ranges from cables 20 to 1. The actual data is marked by red squares and is only plotted for the cables that were tested. For both plots, the theoretical frequencies start off between 0.5 and 1.0 Hertz for the longest cable, cable 20, and proceed to increase in value to around 3.0 to 3.5 Hertz for the shortest cable, cable 1. The measured data points match favorably to the theoretical data in both plots.
Figure 53. Graph. First mode theoretical frequencies versus phase 1 field data.

These four graphs compare first mode theoretical frequency values to the actual values obtained during phase 2 testing. The top-left graph shows the data from fan A, the top-right graph shows the data from fan B, the bottom-left graph shows the data from fan C, and the bottom-right graph shows the data from fan D. The x-axis on all graphs represents the cable number, and ranges from 20 to 1. The y-axis on all graphs represents the frequency, and ranges from 0 to 3.5 Hertz. In all graphs the theoretical data is marked by blue diamonds, and ranges from cables 20 to 1. The actual data is marked by red squares and is only plotted for the cables that were tested. For all plots, the theoretical frequencies start off between 0.5 and 1.0 Hertz for the longest cable, cable 20, and proceed to increase in value to around 3.0 to 3.5 Hertz for the shortest cable, cable 1. The measured data points match favorably to the theoretical data in all plots.
Figure 54. Graph. First mode theoretical frequencies versus phase 2 field data.

DAMPING

Differences in damping between phase 1 and phase 2 data were readily apparent. Cable vibrations comparatively lasted only a fraction of the time after damper installation, which was clearly evident in the damping curves. Figure 55 shows a comparison of the decay curves before and after damper installation.

This graph from the program Matlab compares the decay curves for cable 19A before and after the installation of dampers. The x-axis represents time, and ranges from 0 to 200 seconds. The y-axis represents acceleration, and ranges from -0.2 to 0.2 gravitational constant. The two decay curves are plotted on top of each other, marked by a sinusoidal decay curve with the peaks outlined by a bold line. The phase 1 curve decays from 0.2 g to about 0.02 g in the full 200 seconds of the plot, while the phase 2 curve decays from 0.2 to about 0.02 g in roughly 25 seconds, indicating the effects of the damper on the cable.
Figure 55. Graph. Comparison of the decay curves between phase 1 and phase 2 for
cable 19A.

The installation of dampers on the cable-stays had a tremendous impact on the damping ratio values, causing the damping ratios to increase by at least a factor of 5, and sometimes as high as 15. In general, first mode damping ratios for phase 1 testing were between 0.10 and 0.39 percent, where in phase 2 they ranged from 1.22 to 2.21 percent. Second mode damping ratios increased from 0.17 to 0.46 percent in phase 1 to 1.41 to 2.48 percent in phase 2. Figure 56 and figure 57 show the comparison of the damping ratios obtained from the cables tested in fan A between the two phases.

This graph compares the first mode damping ratios of the cables from fan A between phase 1 and phase 2 testing. The x-axis represents the cable number, and ranges from 20 to 12. The y-axis represents the damping ratio, and ranges from 0 to 2.5 percent. The data points from phase 1 all range between 0 and 0.5 percent while the data points from phase 2 all range from around 1.5 to 2.5 percent.
Figure 56. Graph. Comparison of first mode damping ratios.

This graph compares the second mode damping ratios of the cables from fan A between phase 1 and phase 2 testing. The x-axis represents the cable number, and ranges from 20 to 12. The y-axis represents the damping ratio, and ranges from 0 to 2.5 percent. The data points from phase 1 all range between 0 and 0.5 percent while the data points from phase 2 all range from 1.5 to 2.5 percent.
Figure 57. Graph. Comparison of second mode damping ratios.

SCRUTON NUMBER

Before the installation of dampers, Scruton numbers for the cable stays were much lower than the recommended minimum value of 10 for controlling rain/wind-induced vibrations, even falling below the reduced value of 5 allowed for cables with an aerodynamic surface treatment. Phase 1 testing produced Scruton numbers ranging between 0.6 and 2.0. In phase 2 testing, the Scruton numbers climbed to acceptable levels, ranging between 7 and 12. A comparison of the values for the two phases of testing in fan A is shown in figure 58.

This graph compares the Scruton numbers of the cables from fan A between phase 1 and phase 2 testing and also compares these numbers to the target value of five. The x-axis represents the cable number, and ranges from 20 to 12. The y-axis represents the Scruton number, and ranges from 0 to 14. The data points from phase 1 all range between 0 and 2 while the data points from phase 2 all range from 8 to 12. The target value of five for cables with an aerodynamic surface treatment is plotted as a red line. The data points from phase 1 all fall below this target value, while the data points from phase 2 all sit above it.
Figure 58. Graph. Comparison of Scruton numbers.

 

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