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Phase Data from Millikan II Experiments

Dalam dokumen Energy Radiation from A Multi-Story Building (Halaman 102-111)

Chapter 1 Introduction

4.2 Phase Data from Millikan II Experiments

the frequency of excitation, the phase velocity is computed.

End End

As can be seen from Tables 4.19 to 4.36, the phase velocity values obtained are stable for similar experiments for a particular seismometer line. Furthermore, the difference for experiments with large variations in the values comes from competing local minima, similar to the ones shown in Figure 4.6. It should be noted that most of the plots have clear global minima, and that the case shown in Figure 4.6 is a worst-case scenario. Furthermore, for the particular case shown in this figure, the transverse component is located on a node for the EW shake, and the phase data could be unreliable. However, the scatter shown for the transverse component is consistent for similar experiments, and this further demonstrates the repeatability of the collected waveforms, as the data is also repeatable for instruments located on nodal lines. Therefore, it can be assumed that the observed waveforms are not dominated by noise, and that they are reliable (as are the measurements made from them).

The measured relative waveform phases lead to the supposition that there may be superimposed surface wave modes, or that 3-D effects are important for the problem being studied. The presence of multiple modes might also explain the large error between the measured and the best-fitting linear phases, as a constant phase velocity should not be expected to fit the data in this case. Furthermore, this could explain why the calculated phase velocities differ for different seismometer setups, as both the seismometer spacing and the distance between measurements have an influence on the linear fit.

Similarly to the previous section, the waveforms collected for stations at distances less than 150 meters from the building were removed (100 meters for instrument lines containing only 4 instruments), to minimize the near-field effects. The results of these linear fits are provided in Tables 4.28 through 4.36. The phase velocity values

Experiment A Experiment B Experiment C Experiment D

East line 1026 591 533 967

EN E line 824 836 836 832

North line 989 995 952 1069

NE line 691 683 683 683

NNE line 747 724 730 707

NNW line 622 626 630 633

Table 4.19 Phase velocities in meters/second computed for the radial component for an East-West Shake

Experiment A Experiment B Experiment C Experiment D

East line 1211 581 1704 1123

EN E line 725 723 731 731

North line 545 546 547 544

NE line 530 529 531 832

NN E line 548 547 553 555

NNW line 501 501 500 498

Table 4.20 Phase velocities in meters/second computed for the transverse component for an East-West Shake

Experiment A Experiment B Experiment C Experiment D

East line 1708 767 688 1549

EN E line 1128 1143 1171 1170

North line 1102 1114 1057 1240

NE line 1029 1039 1067 1069

NN E line 1186 1232 1312 1485

NNW line 910 940 967 1034

Table 4.21 Phase velocities in meters/second computed for the vertical component for an East-West Shake

Experiment A Experiment B Experiment C Experiment D

East line 567 513 560 493

EN E line 570 567 564 567

North line 565 566 565 565

NE line 794 309 308 310

NN E line 605 604 608 611

NNW line 477 476 480 482

Table 4.22 Phase velocities in meters/second computed for the radial component for a North-South Shake

Experiment A Experiment B Experiment C Experiment D

East line 510 474 505 448

EN E line 537 534 534 536

North line 512 512 512 511

NE line 578 269 271 270

NN E line 478 481 482 483

NNW line 492 497 492 493

Table 4.23 Phase velocities in meters/second computed for the transverse component for a North-South Shake

Experiment A Experiment B Experiment C Experiment D

East line 544 509 539 474

EN E line 719 716 716 718

North line 642 638 638 638

NE line 314 315 315 316

NN E line 648 647 648 651

NNW line 520 519 523 524

Table 4.24 Phase velocities in meters/second computed for the vertical component for a North-South Shake

Experiment A Experiment B Experiment C Experiment D

East line 540 458 535 572

EN E line 571 572 572 571

North line 490 516 482 517

NE line 286 290 250 289

NNE line 318 935 919 949

NNW line 566 575 573 572

Table 4.25 Phase velocities in meters/second computed for the radial component for a Torsional Shake

Experiment A Experiment B Experiment C Experiment D

East line 540 587 535 569

EN E line 527 526 528 527

North line 456 456 457 457

NE line 460 461 464 463

NN E line 460 466 466 465

NNW line 449 457 455 456

Table 4.26 Phase velocities in meters/second computed for the transverse component for a Torsional Shake

Experiment A Experiment B Experiment C Experiment D

East line 528 451 528 565

EN E line 755 765 767 779

North line 602 603 601 609

NE line 578 584 582 587

NN E line 596 605 606 611

NNW line 546 561 557 562

Table 4.27 Phase velocities in meters/second computed for the vertical component for a Torsional Shake

Experiment A Experiment B Experiment C Experiment D

East line 1567 523 466 1257

EN E line 809 817 809 806

North line 1066 1069 985 1103

NE line 694 681 678 684

NN E line 848 795 789 740

NNW line 661 660 665 671

Table 4.28 Phase velocities in meters/second computed for the radial component for an East-West Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 1503 512 432 1725

EN E line 695 687 699 700

North line 434 434 434 423

NE line 507 508 508 511

NN E line 515 517 524 521

NNW line 502 494 490 484

Table 4.29 Phase velocities in meters/second computed for the transverse component for an East-West Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 1708 633 560 1725

EN E line 1414 1426 1480 1474

North line 1664 1664 1667 1658

NE line 1057 1069 1054 1058

NN E line 1437 1617 1670 1663

NNW line 1102 1142 1197 1313

Table 4.30 Phase velocities in meters/second computed for the vertical component for an East-West Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 552 478 542 444

EN E line 580 567 551 551

North line 601 490 494 491

NE line 794 258 257 257

NNE line 587 588 598 600

NNW line 503 504 508 510

Table 4.31 Phase velocities in meters/second computed for the radial component for a North-South Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 534 471 524 427

EN E line 545 534 544 546

North line 527 523 524 523

NE line 578 238 238 239

NN E line 503 502 513 515

NNW line 528 525 546 549

Table 4.32 Phase velocities in meters/second computed for the transverse component for a North-South Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 699 601 681 521

EN E line 787 716 771 770

North line 689 676 669 669

NE line 314 271 272 272

NN E line 699 700 710 710

NNW line 549 548 554 557

Table 4.33 Phase velocities in meters/second computed for the vertical component for a North-South Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 540 413 526 588

EN E line 558 559 561 560

North line 243 399 240 397

NE line∗ 267 271 264 273

NN E line 361 714 710 741

NNW line 543 550 552 555

Table 4.34 Phase velocities in meters/second computed for the radial component for a Torsional Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 556 599 544 606

EN E line 527 528 528 530

North line 428 426 427 423

NE line 295 294 297 298

NN E line 481 489 490 488

NNW line 483 487 487 491

Table 4.35 Phase velocities in meters/second computed for the transverse component for a Torsional Shake with the data close to the building removed.

Experiment A Experiment B Experiment C Experiment D

East line 558 425 542 613

EN E line 839 858 855 865

North line 529 532 521 524

NE line 335 579 579 580

NN E line 580 585 585 583

NNW line 529 536 536 539

Table 4.36 Phase velocities in meters/second computed for the vertical component for a Torsional Shake with the data close to the building removed.

0 200 400 600 -4

-3 -2 -1 0 1

Distance (m)

0 200 400 600

-1 0 1

Distance (m)

0 500 1000 1500

0 0.2 0.4 0.6 0.8 1

Wavelength (m) Wavelength: 1064 m Velocity: 1211 m/s

0 200 400 600

-4 -3 -2 -1 0 1

Phase (rad)

Distance (m)

0 200 400 600

-2 -1 0 1 2

Distance (m)

Residual Error (rad)

0 500 1000 1500

0 0.2 0.4 0.6 0.8 1

Wavelength (m)

Avg. RMS Error (rad) Wavelength: 901 m

Velocity: 1026 m/s

0 200 400 600

-3 -2 -1 0

Distance (m)

0 200 400 600

-2 -1 0 1 2

Distance (m)

0 500 1000 1500

0 0.2 0.4 0.6 0.8 1

Wavelength (m) Wavelength: 1500 m Velocity: 1708 m/s

A) Radial component B) Transverse component C) Vertical component

Figure 4.6 Phase velocity minimization curves for an East-West shake recorded along the east line. The phase data shown are for the first shake (A). Shown are the radial, transverse, and vertical components. Sub-figures A and C show worst case scenarios for the linear fits, as there are outliers in the data.

calculated from the data of all of the seismometers and those obtained after removing the data for the closest instruments are very similar, which is incompatible with the observed displacements being due to the interference of multiple surface wave modes.

The good agreement between these results also supports that there is no interaction between near and far-field waves, as otherwise the measured phase velocities would be different for the two cases.

Dalam dokumen Energy Radiation from A Multi-Story Building (Halaman 102-111)