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Historical Seismograms - Evidence from the AD 2000 Izu Islands ...

Historical Seismograms - Evidence from the AD 2000 Izu Islands ...

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394 R. Inoue and T. Matsumoto3. Digitization and Correction ProceduresTo obtain <strong>the</strong> corrected data with equal time intervals, <strong>the</strong> following steps wereperformed on <strong>the</strong> original data: (1) The original seismogram was enlarged andprinted on a polyester base. (2) The co-ordinates of peaks, troughs and points ofinflection of <strong>the</strong> enlarged record were read by a digitizer. (3) Baseline correctionswere performed on <strong>the</strong> data by <strong>the</strong> least squares method. (4) The effects of finitearm length and inclination of <strong>the</strong> arm were eliminated <strong>from</strong> <strong>the</strong> data. (5) The datawere interpolated by a cosine curve and equally spaced data were produced. Thetime interval At was chosen as 0.25 sec in this analysis. (6) The corrections forinstrumental characteristics on <strong>the</strong> data were performed. (7) A bandpass filter wasapplied to <strong>the</strong> data to remove <strong>the</strong> high and low frequency noise. As shown inFigure 3, <strong>the</strong> upper cut-off frequency is 0.5 Hz (2 sec), and <strong>the</strong> lower is 0.05 Ha(20 sec).These correction procedures of <strong>the</strong> digitized data are similar to those outlinedin Skoko and Sat0 (1973). The records of <strong>the</strong> J.M.A. strong motion seismometerswere corrected by <strong>the</strong> above procedures.However, in <strong>the</strong> case of <strong>the</strong> records by <strong>the</strong> old type seismographs, <strong>the</strong>re aretwo additional problems to be solved. First, <strong>the</strong> mechanical arm length of <strong>the</strong>seismographs cannot be found in any of <strong>the</strong> documents now available. Second,<strong>the</strong>re are a few records in which <strong>the</strong> apparent zero-line varies while <strong>the</strong> earthquakeis being recorded (Figure 5). We solved <strong>the</strong>se problems by <strong>the</strong> following procedures.First, <strong>the</strong> procedures for estimating <strong>the</strong> arm length R are as follows (Figure 4):(1) A portion where <strong>the</strong> amplitude of <strong>the</strong> time history is very large was chosen.(2) An iso-time circle (Figure 4) which passes through <strong>the</strong> peak or trough of <strong>the</strong>large amplitude was constructed, and three points, P1, P2 and P3, on <strong>the</strong> iso-timecircle were read by a digitizer. (3) The perpendicular bisectors of <strong>the</strong> line P1 . P2and <strong>the</strong> line P2. P3 were drawn, and <strong>the</strong> co-ordinates of <strong>the</strong> point C which is <strong>the</strong>intersection of <strong>the</strong> two bisectors was calculated. That point is <strong>the</strong> position of <strong>the</strong>pivot of arm. (4) The length of <strong>the</strong> line segment P1. C (= P2 . C = p3c) wasmeasured. That is <strong>the</strong> arm length of <strong>the</strong> seismograph.The values of <strong>the</strong> arm length for <strong>the</strong> old type seismographs in Table 2 wereestimated by <strong>the</strong> above procedures.Second, <strong>the</strong> procedures for <strong>the</strong> arm-correction of <strong>the</strong> above mentioned record areas follows (Figure 5): (1) For <strong>the</strong> given time history where <strong>the</strong> apparent zero-linevaries in many stages (Figure 5a), <strong>the</strong> baseline correction in each section corre-F1 = 0.035 Hz (T = 28.6 sec); F2 = 0.05 Hz (T = 20.0 sec);F3 = 0.5 Hz (T = 2.0 sec); F4 =0.7 Hz (T = 1.4 sec).Figure 3. Characteristics of <strong>the</strong> bandpass filter.

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