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The effect of air-fuel equivalence ratio change on the vibration components of an internal-combustion engine

Manhertz, Gábor; Antal, Ákos

Abstract

Nowadays the automotive industry and the motor development are one of the most dynamically developing industries. One solution to the diagnostic systems providing reliability is the acoustic and vibration measurement system, which can indicate and predict a variety of malfunctions after signal processing. The purpose of this experiment is to analyze the effect of the air-fuel equivalence ratio on the vibration components of an internal-combustion engine (ICE) which is a part of the in question measurement system. In the focus of the experiments are the analysis of the time signal, its spectra, and the power content of the signal. With the increment of the air-fuel ratio the amplitudes of the measured signal and its spectral amplitudes showed a downward trend as the RMS values. In addition, certain frequency components disappeared during the actuation of the ICE with an electromotor, so the characterization of the combustion could be come to the front.

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Recen Inno a ions in Mecha onics (RIiM) Vol. 2. (2015). No. 1-2. DOI: 10.17667/ iim.2015.1-2/13. 1 The e ec o ai - uel equi alence a io change on he ib a ion componen s o an in e nal-combus ion engine Gabo Manhe z Depa men o Mecha onics, Op ics and Mechanical Enginee ing In o ma ics Budapes Uni e si y o Technology and Economics Budapes , Hunga y Co esponding au ho ’s e-mail: [email p o ec ed]me.hu Akos An al Depa men o Mecha onics, Op ics and Mechanical Enginee ing In o ma ics Budapes Uni e si y o Technology and Economics Budapes , Hunga y Abs ac — Nowadays he au omo i e indus y and he mo o de elopmen a e one o he mos dynamically de eloping indus ies. One solu ion o he diagnos ic sys ems p o iding eliabili y is he acous ic and ib a ion measu emen sys em, which can indica e and p edic a a ie y o mal unc ions a e signal p ocessing. The pu pose o his expe imen is o analyze he e ec o he ai - uel equi alence a io on he ib a ion componen s o an in e nal-combus ion engine (ICE) which is a pa o he in ques ion measu emen sys em. In he ocus o he expe imen s a e he analysis o he ime signal, i s spec a, and he powe con en o he signal. Wi h he inc emen o he ai - uel a io he ampli udes o he measu ed signal and i s spec al ampli udes showed a downwa d end as he RMS alues. In addi ion, ce ain equency componen s disappea ed du ing he ac ua ion o he ICE wi h an elec omo o , so he cha ac e iza ion o he combus ion could be come o he on . Keywo ds— ib a ion diagnos ics; in e nal-combus ion engine; ai - uel equi alence a io, spec a, RMS I. INTRODUCTION The au omo i e manu ac u e s a e ying o adap mo e om he di ec i es o he compe i ion on he ma ke . To mee hese equi emen s he bes , hey need o ind he bes comp omise be ween he p ice, he ope a ional sa e y, he uel consump ion, he emission limi s and he pe o mance. The pe o mance can be in luenced by he ai - uel equi alence a io which can be esul ed in he examina ion o he pollu an emission o he alida ion o ma hema ical models. Se e al e e ences desc ibe his kind o esea ch wo ks based on ICEs [1]-[3]. Besides o he ai - uel a io, he engine cha ac e is ics and ope a ion can be in luenced wi h a ious ypes o uel as well [4]. Nowadays, because o he en i onmen al awa eness, expe imen ally iendly uels a e used also. In [5] an expe imen al s udy can be seen on a di ec injec ion diesel engine ope a ed wi h Kapok me hyl. An in e nal-combus ion engine has se e al physical alues which can be measu ed and he esul s cha ac e ize he s a e o he engine. Vib a ion analysis is applied equen ly as he basis o expe sys ems. Some o hese sys ems a e used o condi ion moni o ing and aul diagnosis [6]-[8]. A e y in e es ing esea ch can be seen in e e ence [9] whe e he combina ion o he ib a ion and acous ic emission was applied. F equency-based analysis is o en used in he ib a ion diagnos ics o ICEs. Lin e . al [10] ep esen s a ib a ion diagnos ic echnique based on he co ela ion o disc e e spec um. In e e ence [11] he combina ion o he ime and equency domain analysis can be seen. I can be concluded om he li e a u e ha he ib a ion analysis o he ICEs is qui e common and he esea ch ends a e e y di e se o e and abo e he ela ion be ween he ib a ion and he ai - uel a io is no a equen ly discussed opic. Howe e , he applied diagnos ic me hods a e becoming mo e complex and he simple ones being o go en o will be no applied anywhe e. This esea ch wo k will go back o he basic ib a ion diagnos ic me hods which made us also possible o de e mine co ela ion be ween he nume ical esul s and he ac ual ai - uel equi alence a io. A. The Ai - uel Equi alence Ra io The ai - uel equi alence a io gi es he a io o he in ake ai -amoun and he heo e ically equi ed ai -amoun o he combus ion. This a io a ec s he engines e iciency, pe o mance and he pollu an emission. Du ing he combus ion, because i is a chemical p ocess, he co ec a io o he p esen uel and oxygen is a e y impo an ac o . I he amoun o he ai and he uel is no close o equilib ium du ing he eac ion, he combina ion o he inpu and ou pu ma e ials will no be ully. The ai - uel equi alence a io a he ideal – heo e ic – ai - uel a io is 1, i.e. he mix u e is s oichiome ic. The combus ion equi es ha he mix u e need o be be ween he lowe and he uppe lammabili y limi . Wi hin his ange, i he ai - uel equi alence a io is less han 1 (i.e. he mix u e is uel- ich) he chemically bounded ene gy canno ully be con e ed in o hea – a signi ican amoun o CO emission occu s. I he mix u e is uel-poo , he ai - uel equi alence Recen Inno a ions in Mecha onics (RIiM) Vol. 2. (2015). No. 1-2. DOI: 10.17667/ iim.2015.1-2/13. 2 a io will be g ea e han 1; he mix u e con ains mo e oxygen han i is necessa y o he combus ion. The ai - uel equi alence a io is he a io o he in ake ai - amoun and he heo e ically equi ed ai -amoun , so i s alue can be de e mined om oxygen concen a ion o he lue gas: measu ed OL V O O L L ,20 0 2 2 09,20 9,20 21 1             whe e: L is he ac ual ai -amoun , L0 is he heo e ic ai - amoun , V0 is he heo e ic lue gas-amoun . The main ask is o analyze he e ec o change o he ai - uel equi alence a io on he ib a ion componen s o an in e nal-combus ion engine. II. EXPERIMENTAL SETUP Today’s mode n ehicle engines a e equipped wi h many senso s and con ol uni s which de e mine he equi ed mix u e o he ac ual ope a ing s a e. The inadequa e ai - uel equi alence a io can a ec o he pa ame e s analyzed by he ECM so he con inuous moni o ing o hese pa ame e s is he base o he diagnos ics. The ib a ion measu emen s based on a gas-powe ed ICE. The main pa o he uni is a BAG-20 ype de ice manu ac u ed by Ganz-Se L d. which consis s o he ollowing componen s  Wiscon To al TM27 ype gas-engine  Ma elli CX IM B3 180M ype asynch onous gene a o Fo he measu emen s a single-axis knock senso used in au omo i e indus y manu ac u ed by Siemens was applied. I s signal was eco ded by a USB-6008 DAQ de ice p oduced by Na ional Ins umen s. The da a acquisi ion de ice had 12bi esolu ion and 10000samples/sec maximum sampling equency. Wi h hese de ices he lowe equency ib a ion o he engine we e measu ed well bu o u he esea ches i is essen ial o examine he highe equency anges. The uel- ai mix u e o he engine was con olled wi h a al e and i was de e mined om he oxygen concen a ion o he exhaus gas. To measu e he O2 concen a ion du ing he es a Se omex 570A ype pa amagne ic de ice was used. In o de o moun he knock senso wo moun ing place we e possible. The i s was a he join o he c ank-case and he cylinde -head, he second was on he c ack-case (Fig. 1). F om he measu emen s o he i s moun ing place, a numbe o ac o s seemed o a ec nega i ely he esul s. Fig. 1. The moun ing o he accele ome e on he i s (le ) and on he second ( igh ) moun ing place One o he p oblems was he moun ing place i sel , since he c ank-case and he cylinde -head was no lush so he senso could no abu on comple ely on he su ace. A space was needed o be equipped which wo ked as a sp ing and caused up o 100 m/s2 (hence o wa d [g]) accele a ion alues in he ime signal (Fig. 2). Ano he p oblem was he hickness o he space because he base o he accele ome e could no s ill abu comple ely on he cas o he c ank-case. The hi d p oblem was he bad ib a ion ansmission o he pain ing o he engine o he senso . On he housing was app ox. a 0,3mm hink laye o pain which was no conduci e o he measu emen as well. These ac o s men ioned abo e b ough majo noise in o he sys em, as well as hey occu ed non- eal equencies in he spec um and he eal ones ha e been blu ed. A he second moun ing place, aking in o accoun he expe ienced de ec s p e iously, he pain has been emo ed om he engine and he accele ome e could be able o be moun ed comple ely on he su ace wi hou a space . The esul s ob ained wi h his se -up ca ied much mo e p ocessable in o ma ion. The maximum accele a ion alue o he measu emen s pe o med a he second moun ing place nea ly wi h he same ai - uel equi alence a io was less han hal o he p e ious. Fig. 2. The eco ded ime signals o senso a he i s (abo e) and he second (bo om) moun ing place – he ime [s] unc ion o he accele a ion [g] Recen Inno a ions in Mecha onics (RIiM) Vol. 2. (2015). No. 1-2. DOI: 10.17667/ iim.2015.1-2/13. 3 Du ing he measu emen he engine’s speed was 1500 RPM ( o a ion pe minu e) which was equal o 25Hz. Due o he p ope ies o he da a acquisi ion ca d, he maximum compu able 5000 Hz was su ice o he analysis o he lowe equencies. The ca d ecei ed ol age signal wi h mV magni udes he e o e o de e mine he accele a ion alues a con e sion had o be applied. The sensi i i y o he senso was 30mV/g which needed o be co ec ed by -8,1mV/g p o me e . The a ached cable leng h was 0,74m which dec eased he o iginal sensi i i y wi h 6mV so he esul ing sensi i i y o he senso was 24mV/g. Du ing he esea ch h ee ime signals we e measu ed a wa m engine unde di e en ai - uel equi alence a ios (Table I.) as well as ano he signal which was eco ded when he e was no combus ion in he engine only he asynch onous machine ac ua ed i . TABLE I. THE THREE PRESET AIR-FUEL EQUIVALENCE RATIO VALUES DURING THE MEASUREMENTS O2 con en o he exhaus gas [%] Ai - uel equi alence a io [-] 1,3 1,063 3,9 1,214 7,6 1,515 III. THE EVALUATION OF THE MEASUREMENT RESULTS The measu emen s we e ca ied ou on cons an pm, so as a consequence he equency componen s o he signal should ha e changed only a li le. This can be e i ied i he ime signal was subjec o he STFT1 ans o ma ion [12] wi h which he ime- equency-ampli ude unc ion, he so-called Wa e all-diag am could be plo ed. The STFT p inciples a e he same as he as Fou ie ans o m bu in his case he ans o m is execu ed a speci ic ime s eps and i s equency esolu ion is much less. I du ing he measu emen he spec a would ha e changed, i would be clea ly isible on he diag am. On he signal measu ed a he lowes ai - uel equi alence a io such ans o ma ion has been execu ed on which i is clea ly isible ha he spec um does no change in ime signi ican ly as i was expec ed. On he h ee-dimensional 1 Sho -Time Fou ie T ans o m diag am he spec a can be seen be ween 20 and 32,6 seconds wi h a s ep size o 0,7seconds. The illus a ed equency ange is he 0-700Hz in e al. To e alua e he measu emen s a he gi en ai - uel equi alence a ios he ampli udes o he ime signals, he spec al ampli udes and componen s, and he powe con en (RMS2 alue) o he signal should be analyzed. Fig. 3. STFT ans o m pe o med a he lowes ai - uel equi alence a io ( he ime [s] unc ion o he ampli ude [g] and he equency [Hz]) A. The Analysis O The Time Signals In he able below he maximum and minimum ampli ude alues o he en i e ime signals a e shown. TABLE II. THE MAXIMUM AND MINIMUM AMPLITUDE VALUES OF THE FOUR MEASUREMENT SETUP AS A FUNCTION OF THE AIR-FUEL EQUIVALENCE RATIO Ai - uel equi alence a io [-] Maximum accele a ion [s] Minimum accele a ion [s] 1,063 46,57 -54,645 1,214 36,81 -38,306 1,515 31,51 -32,491  29,38 -28,97 The able shows ha he maximum and minimum ampli udes o he ime signals ha e a dec easing as unc ion o he ai - uel equi alence a io. This means ha he deg ada ion o he ai - uel mix u e, i.e. he s ep-by-s ep ga bling o he pe ec ion o he combus ion, he ib a ion componen s we e dec easing. In he case o no combus ion (ac ua ion wi h he asynch onous machine) we e he ib a ion componen s he lowes . This led o he conclusion ha he combus ion i sel could a ec he ib a ion o he engine. B. The Analysis O The Spec a Based on he esul s o he STFT analysis, he Fou ie ans o ma ion could be used o de e mine he spec al componen s. Figu e 4 shows he spec a o a ime signal 2 Roo Mean Squa e Recen Inno a ions in Mecha onics (RIiM) Vol. 2. (2015). No. 1-2. DOI: 10.17667/ iim.2015.1-2/13. 4 belongs o =1,063 ai - uel equi alence a io. Fo he aceabili y o he la e analysis ha equency componen was ma ked which belongs o he e o he engine (25Hz). In addi ion, his equencies mul iplies could be ound which could be a esul o he ope a ion o he a ious engine componen s. Se e al componen s o he engine depend on he e o he c anksha hus ha could be iden i ied which componen belongs o which ha monic o spec al componen . The e o he camsha is he hal o he e o he c anksha so he ela ed equency componen is 12,5Hz. The 50Hz componen may be in connec ion wi h he combus ion p ocess bu he elec ical 50Hz was also p esen ing signi ican . Due o he ou cylinde s he combus ion occu ed in wo cylinde s p o a o a ion and he equency o he asynch onous machine changed his componen as well. On he spec a o he measu emen s a h ee di e en ai - uel equi alence a ios i could be seen ha he ampli udes o he componen s we e p og essi ely dec easing (Fig. 8) o e en disappea ed in he backg ound noise. As ega ds o he analysis o he ha monic componen s, ha signal eco ded a ac ua ion o he engine wi h asynch onous machine was also analyzed (Fig. 7). On his i could be seen ha he 48,5Hz componen is much highe han he 25Hz componen . A his case wo p ominen equencies should be highligh ed. The i s one is he 48,5Hz componen which de i ed om he 50Hz o he gene a o as well as om i s cha ac e is ic 3% slip. The o o o he gene a o has ou poles so i s o h ha monic equency is 194Hz (4x48,5=194Hz). Compa ing he spec a wi h each o he , i can be concluded ha in he case o he disappea ance o he equency componen s a asynch onous machine ac ua ion, and he dec easing o he ampli udes ( he combus ion equencies we e no supe pona ed on o he o he componen s) we e esul ed om he cha ac e (o he exis ence) o he combus ion. The equencies which comple ely disappea ed a he low- equency ange: 75Hz, 100Hz, 112,5Hz, 125Hz, 150Hz. Fig. 4. Spec a a =1,063 ai - uel equi alence a io ( he equency [Hz] unc ion o he accele a ion [g]) Fig. 5. Spec a a =1,214 ai - uel equi alence a io ( he equency [Hz] unc ion o he accele a ion [g]) Fig. 6. Spec a a =1,515 ai - uel equi alence a io ( he equency [Hz] unc ion o he accele a ion [g]) Fig. 7. Spec a a he ac ua ion wi h he asynch onous machine ( he equency [Hz] unc ion o he accele a ion [g]) Recen Inno a ions in Mecha onics (RIiM) Vol. 2. (2015). No. 1-2. DOI: 10.17667/ iim.2015.1-2/13. 5 Fig. 8. The changes o he ampli udes o some equency componen as a unc ion o he ai - uel equi alence a io Powe Con en In ib a ion diagnos ics and analysis, a gene ally accep ed measu e is he RMS alue o he signal which ep esen s he powe con en o he s udied signal sec ion in a nume ical o m. This powe con en is de i ed om he selec ed a iable in eg al o he analyzed sec ion. Du ing he pos -p ocessing, he ime signal and he spec a RMS alue was calcula ed wi h he ollowing o mulas [12]: In case o ime signal:    In case o spec a:   As he e he powe con en was he main poin o he analysis ha cases was needed o be s udied when he e was combus ion in he engine, i.e. he asynch onous machine ac ua ion was i ele an in his case. Be o e p ocessing he measu emen esul s he dec easing o he RMS alues we e expec ed as he unc ion o he ai - uel equi alence a io. The heo e ical explana ion o his is (as be o e) because o he deg ada ion o he mix u e he combus ion will be shi ed om he =1 alue equi ed o he pe ec combus ion, so he e ec i e medium p essu e and he eby he o que will be educed. The esul s (Table III.) we e as expec ed. This means ha all o he RMS alues o he ime signals and he spec um showed a dec easing end do o he inc ease o he ai - uel equi alence a io. TABLE III. THE RMS VALUES OF THE TIME SIGNAL AND THE SPECTRA AS FUNCTION OF THE AIR-FUEL EQUIVALENCE RATIO Ai - uel equi alence a io [-] Time signal RMS [g RMS] FFT ampli ude RMS [g RMS] (0-300Hz) 1,063 2,57438 0,01080030 1,214 2,11306 0,00814465 1,515 2,06645 0,00659716 C. Fu he esea ch oppo uni ies To imp o e and suppo he esea ch esul s u he measu emen s a e necessa y e.g. wi h less han one ai - uel equi alence a io, a iable e and load, adial ib a ion measu emen s and wi h he use o a da a acquisi ion ca d ha ing highe esolu ion and sampling equency. Wi h hese esul s a complex engine cha ac e is ic will be able o ob ained. IV. CONCLUSION The expe imen al esul s showed ha wi h he inc ease o he ai - uel equi alence a io o a gas engine ope a ing a a cons an speed, he ampli udes o he measu ed signals and spec um dec eased as well as hei RMS alues – he powe con en . This means ha nume ical esul s o he basis ib a ion diagnos ic me hods a e able o show co ela ions and ends be ween he ai uel a ion and he ib a ion o a gas engine. Du ing he measu emen s he engine was ac ua ed wi h an asynch onous machine as well – he e was no combus ion in he combus ion chambe . 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