DSP APPLICATION TO THE PORTABLE VIBRATION EXCITER

Transcription

1 DSP PPLICTION TO THE PORTBLE VIBRTION EXCITER W. Barwicz 1, P. Panas 1 and. Podgórski 2 1 Svantek Ltd., Warsaw, Poland Institute o Radioelectronics, Faculty o Electronics and Inormation Technology 2 Warsaw University o Technology, Warsaw, Poland bstract: In the paper a new portable battery operated exciter dedicated or the calibration o the mechanical vibration sensors (transducers) is presented. This instrument is based on the Motorola s digital signal processor DSP [1] which is quite new approach to the construction o such instrument. The DSP with the reerence sensor [2] used as an inormation source about the generated vibration signals constitutes the measurement system. This system is used or the generation o the reerence mechanical vibrations. The digital approach to the calibration ensures the new level o the perormances. Programmability o the generated vibration, requency accuracy and the level o total harmonic distortions (THD) overcomes all other designs available on the market. Keywords: DSP, vibration exciter, calibration o vibration sensors 1 INTRODUCTION The parameters o the existing analogue portable vibration exciters (calibrators) [3], [4] are not satisactory. The maximum load or the classic analogue handheld exciters is not so high and can not be changed in the wide range. The requency accuracy o the generated sinusoidal signal is also not good enough. Finally, these units can not be programmed in order to generate the dierent signals in. The requency inaccuracy results in additional velocity and displacement errors. This is the reason or the investigations with the application o the digital technology [5], namely digital signal processor (DSP), or the improvement o these parameters. The introduction o the DSP to the mechanical construction o the exciter enables one to generate the vibration signal with the very good compensation o the harmonic components. The usage o the DSP ensures the compact, lexible construction which is not possible to obtain on the analogue way. In the exciter taken under consideration there exists the non-linear mechanical system which parameters are unknown and highly dependent rom the environmental conditions. The main source o the undetermined transer unction are the vibration sensors with the dierent masses and the base the instrument is placed on (the stable table, hand etc.). The aim o the DSP is to ind out the transer unction o the mechanical system in the current conditions and the syntheses o the sinusoidal vibration signal. The DSP has to realise the negative eedback circuit in which the o the generated vibrations is stabilised with the high precision and the harmonic components o the signal are negligible thanks to the compensation procedure. The implemented algorithm has to be adapted to the changing external situation. 2 BLOCK DIGRMME OF THE DEVELOPPED LGORITHM The block diagram o the developed algorithm or the stabilisation and the compensation o the harmonic components o the generated signal in the vibration exciter is presented in Fig. 1. The digital processor introduced in the construction o the vibration exciter has to: generate the signal stimulating the mechanical system; analyse the spectrum o the signal coming rom the reerence transducer; stabilise the o the mechanical vibrations on the required level; search the compensation signal or the harmonic components. The tasks which DSP has to ulil are shortly presented in the ollowing parts o the paper. 3 THE TSKS OF THE DIGITL SIGNL PROCESSOR 3.1 The generation o the signal exciting the mechanical system The system o the signal generation works in the real time. The parameters which are necessary or the signal generation are taken rom the searching module and rom the stabilisation module. These

2 parameters are as ollows: the s o the harmonic components and their phases related to the base harmonic component. On the base o these data the DSP calculates and syntheses the components o the inal output exciting vibration signal. U out =U 1 cos(ωt)+u 2 cos(2ωt+ϕ 2 )+... Nonlinear mechanics Linear transducer Disturbances U 1 cos(ωt) U 2 cos(2ωt+ϕ 2 ) U 3 cos(3ωt+ϕ 3 ) U in =U 1 cos(ωt+ϕ 1 )+U 2 cos(2ωt+ϕ 2 )+... G1 G2 G3 Generator (U 1 ) (U 2, ϕ 2 ) (U 3, ϕ 3 ) nalyser Figure 1. The block diagram o the algorithm or the stabilisation and the compensation o the harmonic components o the generated signal in the proposed realisation o vibration exciter. 3.2 The stabilisation o the mechanical system vibration on a required level The aim o the vibration exciter is the generation o the highly stable vibration signal with the deined by the standards. In the eedback circuit the measurement o the generated signal is perormed and the comparison with the reerence level deined in the programme is done. Too high o the generated signal orces the decrease o this parameter in the DSP programme and too small - the increase. The stabilisation o the is perormed on-line with the high precision. The inormation about the o the vibration signal are taken rom the module o the spectrum analysis. 3.3 The measurement o the coeicient o the mechanical system attenuation The mechanical system o the exciter is described by the certain resonance characteristic (the dierent requencies are attenuated dierently). For the practical reasons the resonance requency o the mechanic part o the instrument is closed to the working requency o the instrument. Such solution ensures the small attenuation o the required requency and the big attenuation or the harmonic components ar rom the resonance requency. The additional eature o such solution is its power saving very important in the portable instrument (in the resonance the amount o the energy required or the vibration signal with the desired is relatively low). The measurement o the coeicient o the harmonic requency attenuation is important. This parameter is used by the module which searches the compensation signal or the exact determination o the parasitic harmonic s to be compensated. 3.4 The spectrum analysis o the signal rom the reerence sensor Non-linearity o the mechanical system causes the appearance o the harmonic components in the spectrum [6] o the vibration signal. The spectrum o the eedback signal rom the reerence transducer built-in in the exemplary analogue calibrator and the spectrum rom the standard transducer mounted

3 on the exciter are presented in Fig. 2a and Fig. 2b respectively. The observed value o the THD coeicient or the transducer mounted on the exciter is usually on the level 2 3 % (c. Fig. 2b). a) b) Figure 2. The spectrum o the eedback signal rom the reerence transducer built-in in the exemplary analogue calibrator (a) and the spectrum rom the standard transducer mounted on the exciter (b). The module o the spectral analysis built-in the exciter searches the harmonic components, determines their and the phase related to the main harmonic. These data are transerred to the module which searches the compensation signal. 3.5 The searching o the compensation signal In the real systems the excitation o the non-linear mechanical system with the sinusoidal signal leads to the complex vibration signal which is composed by the multiple requencies components. In order to excite the sinusoidal vibration in the non-linear mechanical instrument the generated signal must be complex. In the practice such signal can be built rom the ew sinusoidal signals with the requencies equal to the main harmonic component and its multiplies. The knowledge o the phases and the s o the components is also very important. The harmonic components should be generated with the opposite phase and the s proportional to those obtained rom the mechanical system. This module on the base o the data obtained rom the spectrum analysis and the previous state o the system calculates the parameters and applies them to the module which generates the output signal. 4 RESULTS The results obtained ater the implementation o the stabilisation and compensation algorithm in the DSP introduced in the analogue vibration exciter are shown in Fig. 3. a) b) Figure 3. The spectrum o the eedback signal rom the reerence transducer built-in in the exemplary analogue calibrator (a) and the spectrum rom the standard transducer mounted on the exciter (b) ater compensation algorithm implementation in the DSP.

4 In the spectrum o the signal rom the reerence transducer the second harmonic component is on the level o the internal noise (c. Fig. 3a). The spectrum rom the standard transducer is ree rom this noise (c. Fig.3b). The dierent values on both igures comes rom the dierent reactions o these two transducers on the same signal. The reerence transducer returns the value o the voltage corresponding to the given o the vibration, while the standard transducer returns the value o the electrical charge proportional to this signal. The time required or the digital compensation o the harmonic components is usually equal to s. The observed value o the THD coeicient or the calibrated sensor is on the level o % and is not bigger than 0.5 %. The ull description o the perormed investigations and obtained results are presented in [7]. The data speciication o the vibration exciter, which model is now under tests going beore the introduction the unit on the market, with the comparison to the classic analogue instruments manuactured by world well-known producers (RION [8], PCB PIEZOTRONICS [9] and BRUEL & KJER [10]) is presented in the Table 1. Table 1. The data speciication o the dierent vibration calibrators. Producer RION PCB BRUEL & KJER SVNTEK PIEZOTRONICS Model VE C SV10 Frequency Hz ±1% (-10 C +55 C) Hz (±1%) Hz Hz ±0.01 Hz cceleration Velocity Displacement ±3% (10 C 40 C) ±5% (-10 C 55 C) 10 mm/s (RMS) ±4% (10 C 40 C) ±6% (-10 C 55 C) 10 µm (RMS) ±5% (10 C 40 C) ±7% (-10 C 55 C) 1.00 g (RMS) (9.81 ms -2 ) 0.39 in/s (RMS) (9.81 mm/s) 0.39 mil (RMS) (9.81µm) ±3% 10 mm/s (RMS) ±4% 10 µm (RMS) ±5% 10 ms -2 (PEK) 1.00 g (RMS) 1.00 g (PEK) or up to 220 grams: 1 ms -2 (RMS) 1 ms -2 (PEK) 0.10 g (RMS) 0.10 g (PEK) 10 mm/s (RMS), etc or up to 220 grams: 1 mm/s (RMS), etc. 10 µm (RMS), etc or up to 220 grams: 1 µm (RMS), etc. Maximum Load 70 grams 210 grams 70 grams 120 grams 220 grams Transverse mplitude <5% o main axis <3% o main axis <5% o main axis <7% o main axis Total Harm. <3% (20 g 60 g) <2% (0 g 100 g) <3% (20 g 60 g) <0.5% Distortion <5% (10 g 70 g) <3% (100 g 200 g) <5% (10 g 70 g) Temperature range -10 C +55 C -10 C +55 C 10 C +55 C ±3% -10 C +55 C ±5% -10 C to +55 C Power Supply IEC 6LR61 9V battery 4 alkaline 6LF22 9V alkaline 2 NiMH recharg. battery Dimensions 51 mm (diameter) x 56 mm (diameter) x 52 mm (diameter) x 64 x 64 x 130 mm 134 mm 200 mm 150 mm Weight 600 g with battery 900 g 500 g with battery 600 g with battery Mounting thread UNF UNF UNF

5 5 CONCLUSIONS The application o the DSP to the mechanical system o the vibration exciter seems to be successul. It ensures the miniaturisation and the energy saving so important or the portable instruments. The construction is lexible and enables one to work in many modes. The number o external elements o adjustment is minimised. The good reerence sensor ensures very good accuracy o the measurements. The system can adapt itsel to the new external working conditions. The instrument is nearly independent rom the strain ageing o the elements and can be easily recalibrated in the digital way. The presented vibration exciter can work with the wide range o the masses o the calibrated vibration sensors in the comparison to the analogue solution. It has the best relation between the mass o the calibrated transducer to its own mass. The THD coeicient is signiicantly lower in relation to the analogue instruments. The requency accuracy is extremely good in comparison to the other market existing exciters. This accuracy ensures that the error in the case o the calibration o the velocity and displacement transducers rests on the same level as or the acceleration sensors. REFERENCES [1] DSP Product Inormation and Manual; Motorola. [2] Wilcoxon, Research Industrial Vibration Sensors, Product Catalogue. [3] PCB PIEZOTRONICS, Calibration Equipment, Product Catalogue, [4] M. Serridge, T. O. Licht, Piezoelectric ccelerometers and Vibration Preampliiers, Theory and pplication Handbook, Bruel & Kjaer Rev. Nov [5].V. Oppenheim, R. Schaer, Digital Signal Processing, Prentice-Hall, Englewood Clis, NJ, [6] E.Oran Bringham, The Fast Fourier Transorm and its pplications, Prentice-Hall, En. Clis [7] P. Panas, Digital Handheld Calibration Exciter Supported by DSP56167, Master Thesis, WTU, Faculty o Electronics and Inormation Technology, Warsaw, [8] RION VE-10 Speciications: [9] PCB PIEZOTRONICS: Vibration Calibrators: [10] BRUEL & KJER Vibration Transducer Calibration Equipment: UTHORS: ssist. Pro. Ph.D. ndrzej PODGÓRSKI, Institute o Radioelectronics, Faculty o Electronics and Inormation Technology, Warsaw University o Technology, Warsaw, ul. Nowowiejska 15/19, Poland, Phone Int , Fax Int , a.podgorski@ire.pw.edu.pl M.Sc. Wies³aw BRWICZ and M.Sc. Piotr PNS Svantek Ltd, Warsaw, ul. ks. Jana Sitnika 1 m. 68, Poland, Phone/Fax Int wbarwicz@svantek.com.pl and oice@svantek.com.pl