(i) Sine sweep (ii) Sine beat (iii) Time history (iv) Continuous sine

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A description is given of one way to implement an earthquake test where the test severities are specified by the sine-beat method. The test is done by using a biaxial computer aided servohydraulic test rig. The test rig, excitation signal generation, measurement, analyses and presentation of results are described. There exist many standards for such tests. For example IEC 68-2-59: Test Fe: Vibration - Sine-beat method and IEEE Std. 693: Recommended Practice for Seismic Design of Substations. In power plants and other processing industries ensuring safe shutdowns is necessary in case of a serious disturbance, as an earthquake. It is also important that vital parts of the community are intact after such an event. This implies that equipment such as control consoles, battery racks, high voltage equipment and telecommunication equipment must have a granted function for ground vibrations corresponding to the "worst possible" earthquake. The ground motion of an earthquake can be amplified or attenuated in foundation mounted equipment. For a given ground motion, the alteration depends on the system s natural frequencies and the damping mechanism. For equipment mounted on structures the ground motion is filtered by the building and the secondary structures. The dynamic response of equipment mounted on structures may be amplified or attenuated to an acceleration level many times more or less than the maximum ground acceleration. It is well known that earthquakes are random events and cannot be predicted in detail. Often is a general seismic qualification commonly wanted, when no information is none of the characteristic of the geographic location, the supporting structure or the building. When simulating seismic loads by general seismic classification, there are several wave forms that can be used: (i) Sine sweep (ii) Sine beat (iii) Time history (iv) Continuous sine From now only the sine beat method will be considered. A seismic motion is often characterized by one specific value which is the peak acceleration at the ground level precede by several minor increasing seismic motions. If there is no significant coupling between the orthogonal test axes of the specimen single axes testing with sine beat is preferred, shown in. This due to horizontal earthquake wave at floor levels in simple structure presenting one mode of resonance is similar as its form to sine beat. If a significant coupling yet exist biaxial or triaxial testing, multiaxis testing, can be used. When multiaxis sine beat testing is chosen, caution must be taken to the peak seismic acceleration for the different axes not usually are in phase. If so, other wave forms should be taken into account such as time-history.

2 Sine Beat Amplitud [g] 1.5 1.5 -.5-1 -1.5-2 1 2 3 4 5 Time [s] Besides the qualification test with multiple frequency motion a seismic test often contains a Vibration Response Investigation, VRI. In some standards this test is called a resonance search or exploratory test. The aim of the test is to determine if the test object has any resonance frequencies in the earthquake frequency range. The test should be run at such low level that the test object suffers no mechanical damage. As excitation either noise or sine sweep signals can be used. Often the VRI is repeated after the qualification test. If the test object has suffered global mechanical damage, its resonance frequencies will be lower. The principle of the two-axis vibration table at the Swedish National Testing and Research Institute is illustrated in. The table is supported on three vertical actuators and the horizontal thrust is provided by a single horizontal actuator arranged as shown in the figure. The dimension of the table is 1.2 1.2 m. Due to the three vertical actuators the table is capable of reacting large bending moments.

The table can be used for tests with simultaneous vertical, horizontal and rotational motion. The dynamic capacity of the table is shown in. 1 The performance in the horizontal direction 1.7 m/s Velocity [m/s] 1.1 2 mm.9 g 9 g 1 kg 5 kg.1.1 1 1 1 Frequency [Hz]

1 The performance in the vertical direction 1.5 m/s Velocity [m/s] 1.1 2 mm 1.5 g 15 g 1 kg 5 kg.1.1 1 1 1 Frequency [Hz] Each actuator is servo controlled with acceleration and displacement feedback by a digital control system, INSTRON 858. Transfer functions of servohydraulic equipment are always non flat, i.e., high frequencies are damped more than low. Before using a wave form as a drive signal it must therefore be adjusted. This is done by a special software package, called PROFILE CORRECTION, supplied by INSTRON. Before the testing the adjustment is done. The transfer function of the rig is determined when the table is run without any test object mounted on it. This software can also compensate for unwanted geometric displacement caused by angular movement of the actuators. The general mathematical expression for generating one beat of the whole excitation signal, sine-beat, is given in where ρ 2 2π () = sin2π sin ρ (1) ρ is the test level is the fixed test frequency is the ratio between the fixed test frequency and the modulating frequency, P, in the general case. A number of preset beats generated with the equation above and a pause provided between the beats in order to allow decay of the response of the specimen are generated. The time between the beats shall be long enough so that no significant superposition of

response motion of the specimen occur. The fixed test frequency is the predetermined natural frequency identified in the vibration response investigation. The modulating frequency is proportional to the number of cycles,, in a beat and determined by P = 2 (2) If no vibration response investigation is made or no frequency is specified other test methods should be considered. This due to the accumulated fatigue damage caused by the number of increased critical frequencies. If a sine beat test still is actual the test is carried out in steps of usually one-half octave over the full frequency range of interest or at a frequency of 33 Hz. Servo accelerometers are used for measuring the acceleration of the vibrator table. The measurement chain, for one accelerometer, is shown in. A D 1 2 3 4 5 During an earthquake test of a structure it is often required to monitor the dynamic behavior of the test object. For this purpose accelerometers, strain gauges and displacement transducers are mounted on the test object. The control console of the vibrator table contains a data acquisition system for sampling of up to eight external channels. shows a schematic sketch of the data acquisition system.

. 2 3 4 A D. 6 7 1 5 By the data acquisition system the analogue signals are low pass filtered for frequencies below 1 khz and sampled at 5 khz. As the frequency contents of the signals is less than 5 Hz, the data are by software programs resampled at 2 Hz before long time storage on the disk. The number of data is then reduced without losing any information. The vibrator table excitation and the responses at the test object are sampled by the data acquisition system. The transfer functions are obtained by Fast Fourier Transform, FFT, technique. The signals are then broken into overlapping sections and estimates of the transfer functions are obtained as averages of periodograms of these sections modified by a Hanning window. This is a good overall purpose weighting function for continuous signals. The section length is typically 124 points and the overlap 2/3. With this overlap an effective flat time weighting is achieved. When the transfer function has been calculated, see the modal parameters can be determined by a curve fitting procedure. The theoretic amplitude transfer function for a Single Degree of Freedom Systems is given by ( ) N L = = 1 L + 1 2ςL 2 L L + 1 2ς L L 2 2 2, (3)

where Amplitude transfer function Frequency [Hz] ζ L Relative damping L Resonance frequency [Hz] L Modal constant The values of the modal constant, the resonance frequency and the relative damping giving the best curve fits are obtained by the least square method. This adaptation is done in a frequency range around the resonance frequency. The size of this range has to be chosen manually. Different ranges can give somewhat different values of the modal parameters. However, if the measured transfer function and the theoretic transfer function are plotted in the same graph it is fairly simple to see if the curve fit is good. It is easy to see if the agreement is improved if another frequency range is used. As mentioned in many standards for vibration testing the estimation of damping requires engineering judgment," the presented damping values should therefore be used with care. Normally =1 is used but if there is a double peak, =2 is used. The result presentation of a sine beat excitation is the recorded acceleration time history, shown in. In a zoomed beat of the time history is shown, where the decay of the response motion after the excitation from one beat is distinguish. Example of a time history plot 15 Used File: test15 Channel: AccTop Vibration amplitud [g] 1 5-5 -1-15 1 2 3 4 5 6 Time [s]

A zoomed time history plot 1 Vibration amplitud [g] 5-5 -1 1 11 12 13 Time [s] The determined amplitude transfer function is plotted. An example of such a plot is given in Results from the estimation of the modal parameters are given in plots like that in. Example of presentation of a measured transfer function 25 2 test25 FB Amplification [db] 15 1 5 5 1 15 1 2 3 4 5 Frequency [Hz]

Estimated modal parameters Amplification [db] 3 test25 FB 2 1 4 5 6 7 8 Frequency [Hz] Curve fitting between 4. Hz and 8. Hz gives: Modal constant 1.3 Resonance frequency 5.8 Hz Relative damping 6.4 %