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Frequency Dependent Alterations of S. Cerevisiae Proliferation Due to LF EMF Exposure

Radil, Roman

Abstract

The presented paper deals with low frequency electromagnetic field application on Saccharomyces cerevisiae cells. Experiments performed through wide frequency range have shown selective frequency dependent biological response, which could be successfully predicted by ion parametric resonance theory proposed by V. V. Lednev. Although observed results give satisfying answer to questions whether or not electromagnetic fields could affect cell cultures even at non-thermal levels, the research presented herein opens a multitude of questions about the exact physical mechanisms underlying the observed microorganism behavior, as the theory discussed within the scope of this article is still not completely unambiguous.

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BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE F equency Dependen Al e a ions o S. Ce e isiae P oli e a ion Due o LF EMF Exposu e Roman RADIL1, Jan BARABAS 1, Ladisla JANOUSEK 1, Ma in BERETA2,3 1Depa men o Elec omagne ic and Biomedical Enginee ing, Facul y o Elec ical Enginee ing and In o ma ion Technology, Uni e si y o Zilina, Uni e zi na 1, 010 26 Zilina, Slo ak Republic 2Ins i u e o Measu emen Science, Slo ak Academy o Sciences, Dub a ska ces a 9, 841 04 B a isla a, Slo ak Republic 3Depa men o Radiologic Technology, Facul y o Heal h, Ca holic Uni e si y in Ruzombe ok, Names ie And eja Hlinku 1159, 034 01 Ruzombe ok, Slo ak Republic [email p o ec ed], [email p o ec ed], ladisla[email p o ec ed], ume be e@sa ba.sk DOI: 10.15598/aeee. 18i2.3461 Abs ac . The p esen ed pape deals wi h low e- quency elec omagne ic ield applica ion on Saccha- omyces ce e isiae cells. Expe imen s pe o med h ough wide equency ange ha e shown selec i e e- quency dependen biological esponse, which could be success ully p edic ed by ion pa ame ic esonance he- o y p oposed by V. V. Ledne . Al hough obse ed e- sul s gi e sa is ying answe o ques ions whe he o no elec omagne ic ields could a ec cell cul u es e en a non- he mal le els, he esea ch p esen ed he ein opens a mul i ude o ques ions abou he exac physical mech- anisms unde lying he obse ed mic oo ganism beha - io , as he heo y discussed wi hin he scope o his a - icle is s ill no comple ely unambiguous. Keywo ds Elec omagne ism, low equency elec omag- ne ic ields, p oli e a ion, cell memb ane, ion pa ame ic esonance. 1. In oduc ion I is well known ha he elec omagne ic condi ions in which we li e nowadays a e di e en om hose in which people used o li e in he pas . The majo i y o li ing beings a e con on ed wi h a i icial Elec o- Magne ic Fields (EMFs), which complemen he na u- ally occu ing EMF o he Ea h, and ques ions pe - aining o in luence he eo on biological sys ems a e mo e equen han e e . The numbe o expe imen al s udies in es iga ing EMF e ec s on li ing cells, issues o on human heal h in gene al, has g own apidly o e he las ew decades. Much a en ion is cu en ly being paid o esea ch e- ga ding po en ial connec ion be ween EMF exposu e and cance o o he diseases, which has been dis- cussed in a ious s udies [1], [2], [3], [4], [5], [6] and [7]. Nume ous wo ks ocusing on expe imen s wi h li ing cells ha e shown di e ences in he p oli e a ion p o- cess be ween cells exposed o EMF and con ol (non- exposed) cells [8], [9], [10], [11], [12], [13] and [14]. O he wo ks in es iga e animal beha iou when ex- posed o EMF [15] and [16] o possible genomic ins a- bili ies due o EMF exposu e [17], [18], [19] and [20]. The esul s o hese wo ks a e o en inconsis en and, as s a ed in Buchachenko [21], he biological elec o- magne ic e ec s some imes seem o be i ep oducible and con adic o y. As poin ed ou in Ma ko [22], he p oblem is o en discussed wi hin he scope o he mal e ec s wi h mi- no in e es on possible non- he mal mechanisms, e en when conside ing cu en ly accep ed s anda ds and ecommenda ions (e.g. om In e na ional Commi ee o Nonionizing Radia ion P o ec ion - ICNIRP, 1998). Ac ually, he e alua ion o EMF e ec s on biological objec s is much mo e complica ed due o p incipal di - e ences in each app oach, and no pa o he p ob- lem should be neglec ed, especially when Low F e- quency EMF (LF EMF) and weak signals, ha a e a below he ICNIRP ecommenda ions, a e conside ed. The complexi y o his p oblem is documen ed by many au ho s [23], [24], [25] and [26], who ied o p opose physical mechanism o biological LF EMF impac , bu he e is s ill lack o gene al accep ance o any p oposed heo y ac oss he scien i ic communi y. This ac is a c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 99 BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE he same ime a s ong mo i a ional ac o o u he in es iga ion in his ield o esea ch. The Ion Pa ame ic Resonance (IPR) heo y, p o- posed by Ledne [25], [26] and [27], is one o he mos discussed models o LF EMF in e ac ion wi h bi- ological objec s. The assump ions o his heo y a e based on he Ion Cyclo on Resonance heo y (ICR), i s desc ibed by Libo [24], specula ing ha he physiological ac i i y o ce ain impo an ions can be al e ed when he equency o applied ime- a ying magne ic ield is equal o he equency o ion mo ion in a s a ic magne ic ield. Ions in IPR model a e ep esen ed by a ha monic oscilla o , bound o a speci ic loca ion a he su ace o he cell mem- b ane, and applica ion o combined magne ic ield should al e i s oscilla ions. The men ioned physical model included se e al impe ec ions, pa icula ly due o he p oblem o he mal noise, and was c i icized by Adai [28] and [29]. The heo y was de ended by Engs om [30] and men ioned impe ec ions we e ad- d essed by Ledne [26] and [31]. Despi e c i icism, he e emains an imp essi e body o expe imen al e i- dence ha can be aken as an empi ical basis o ICR and IPR hypo heses [8], [9], [10], [11], [12] and [13]. In gene al, as Halgamuge e al. concluded [33]: “. . . models based on elec ic in e ac ions ha e di icul- ies o ob ain a high enough signal- o-noise a io a low ield s eng hs. The ields ha a e needed o explain he opening o a memb ane channel p o ein a e un e- alis ically high. On he o he hand, models based on magne ic in e ac ions can easily ob ain a la ge enough signal- o-noise a io, because he le el o magne ic he - mal noise in issue is low. The eason ha hese models wo k, is he same eason ha makes he MRI echnique possible.” Ano he a emp o shed mo e ligh in o his e- sea ch a ea is p esen ed wi hin his a icle. The au- ho s op ed o expe imen ally in es iga e non- he mal e ec s o LF EMF on Saccha omyces Ce e isiae cells, a a ious uncommon equencies, o en neglec ed in o he esea ch wo ks. To gain be e ep oducibili y o conduc ed expe imen s, au ho s used hei inno a- i e exposi ion sys em desc ibed in [33], p oposed wi h he aim o achie ing he highes possible homogene- i y o magne ic lux densi y wi hin he exposed ol- ume, aking in o accoun sample dimensions and in- cuba o p opo ions. This sys em enables expe imen s wi h 3 pe i dishes (diame e o 9 cm, heigh o 2 cm - each), each i adia ed by a homogeneous magne ic ield. Ob ained esul s and obse ed biological eac- ions a e hen discussed wi hin he scope o he IPR heo y. 2. Ma e ials and Me hods Saccha omyces ce e isiae cells (b and VIVO – com- me cially a ailable om Lesa e Slo akia, Inc.) we e selec ed as he a ge biological objec o i adia ion by LF EMF. The eason o his choice is he g ow h analogy wi h cance cells [34], as well as p e iously published wo ks ega ding LF EMF e ec s on yeas cells [35] and [36]. 2.1. Expe imen al P o ocol Chemical labo a o y es ing p o ocol o he men ioned VIVO s and o S. Ce e isiae is publicly a ailable om company Mik olab, LLC. This means ha he mic obi- ological, physical and chemical p ope ies and pa am- e e s o in es iga ed mic oo ganisms we e known p io o he expe imen s. Cells we e cul i a ed on GKCH aga , in acco - dance wi h STN EN ISO 7218 (560104) and STN ISO 7954 (560087) s anda ds and speci ica ions. Cul i- a ion was pe o med unde iden ical ambien condi- ions o 72 hou s, wi h empe a u e o bo h exposed and con ol samples se sligh ly abo e oom empe - a u e, speci ically o 27 ◦C. Con inuous empe a u e moni o ing was pe o med using h ee Nega i e Tem- pe a u e Coe icien (NTC) he mis o s and p ocessed and logged in eal- ime. Two o he NTC he mis o s we e placed wi hin he incuba o chambe s o moni o he empe a u e o bo h exposed and con ol samples, and he hi d he mis o was placed ou side he in- cuba o as a e e ence senso . To a oid any e ec s om ai low, humidi y, o changes o ligh condi ions, he exposed samples we e held in a solid plas ic holde , ma ching he diame e o he coil ca i y. 2.2. Expe imen al Se up and E alua ion Me hods The expe imen al se up, used o all o he p esen ed expe imen s and de ailed in [37], is schema ically shown in Fig. 1. The se up was speci ically designed o pai ed sample expe imen s, conduc ed on wo se s o h ee Pe i dishes inocula ed by S. Ce e isiae. One se was placed wi hin one chambe o incu- ba o , housing he mu-me al magne ic shielding box. This se was he con ol, o e e ence sample - being shielded om he gene a ed LF EMF. The second se o samples, ep esen ing he exposed cells, was placed a speci ic posi ion wi hin he al eady men ioned de- eloped coil sys em, depic ed wi hin he eal scheme o expe imen al se up on Fig. 2. The coil sys em was d i en by ha monic cu en (gene a ed by he Agilen 33220A signal gene a o , manu ac u e Agilen Tech- c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 100 BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE nologies, Inc.), and ampli ied using a linea ampli ie (Hube A1110-05, manu ac u e D . Hube GmbH) - he esul ing ampli ude Imbeing in he 0.96–1.09 A ange. The exac alue o exci a ion cu en depended on he impedance ma ching and equency used, so as o achie e he equi ed magni ude o magne ic lux den- si y. The expe imen was epea ed o 5 imes a said equency. PC NI El is AmG MS CS ES Incuba o A Fig. 1: Expe imen al se up: G - signal gene a o Agilen 33220A; Am - ampli ie ; A - ampe e me e ; Incuba o wi h wo chambe s: ES - exposed samples placed wi hin he exci a ion coil, CS - con ol samples placed wi hin he MS - magne ic shielding box; NI El is II - de el- opmen boa d o empe a u e da a acquisi ion; PC - empe a u e moni o ing and isualiza ion. Fig. 2: P opopsed and cons uc ed expe imen al se up show- ing he applica o used in p elimina y expe imen s and he newly designed applica o . F om he a o e men ioned i is e iden ha samples we e i adia ed by LF EMF wi h magne ic lux densi y ~ B, which a ies spa ially wi hin he exposed olume. The exac alue o ~ B- ield p oduced by he coil sys em was alida ed by measu emen s, using sensi i e lux- ga e senso s. Since his me hod is desc ibed in mo e de ail in [33] and [38], o he pu pose o his a icle, i is su icien o men ion he conclusion ha eal-li e measu emen s e-con i med alues ob ained om nu- me ical simula ions, documen ing minimum magne ic lux a ia ions (max. 5 %) wi hin he i adia ed ol- ume, when using he p oposed exci a ion coil sys em. The alue o magne ic lux densi y a ied be ween ~ B=2.33–2.45 mT, and was equency independen . A e con inuous i adia ion, he g ow h dynam- ics pa ame e o bo h con ol and exposed samples was quan i ied. Speci ically, g ow h dynamics we e compu ed ia semi-au oma ed so wa e called Pe i- Coun e , which was de eloped as a eplacemen o comme cially a ailable coun e s. Algo i hm he eo is de ailed in [39]. P incipally, i allows de ec ion and coun ing o yeas g ow h a eas, using me hods o im- age p ocessing, analysis, and ea u e ex ac ion, o en- able expe imen al esul s quan i ica ion and compa i- son o obse ed e ec s. S a is ical signi icance o ob- se ed esul s was inally e alua ed using S uden ’s T- es o pai ed samples, wi h signi icance le el α= 0.05. 3. Resul s and Discussion As was men ioned in p e ious sec ion o his a icle, expe imen s we e ocused on he beha iou o Sac- cha omyces ce e isiae cells in luenced by exogenous LF EMF o di e en equencies p oduced by he de- signed coil sys em. Ou wo k ollows p e iously con- duc ed expe imen s published in [40], [41] and [42], bu he equency ange di e s, and is wide in compa - ison wi h p elimina y expe imen s. A i s , we e- e alua ed he base equency o 1.6 kHz, which was ex- pe imen ally p o en as s a is ically ele an o he in- hibi o y e ec on S. Ce e isiae p oli e a ion. The i s se o expe imen s was hen conduc ed wi h equen- cies o 1.6, 0.8, and 0.4 kHz o e i y hypo hesis ega d- ing e ec s o subha monic equencies and co ela ion he eo wi h IPR heo y, p esen ed in [30]. Resul s o hese expe imen s a e shown in Tab. 1. Tab. 1: Compa ison be ween expe imen al esul s obse ed a i adia ion signal equencies and IPR p edic ed e- quencies a speci ied magne ic lux densi y a ge ing Ca2+ ion. Magne ic lux 2.39 2.39 2.39 2.39 densi y (mT) F equency 1.600 0.800 0.400 0.200 gene a ed (kHz) F equency 1.596 0.798 0.398 0.204 p edic ed (kHz) G ow h a ea a io 0.59 0.54 0.64 0.80 (exposed/con ol) F om he expe imen al esul s i is clea ha all sub- ha monic equencies ha e shown inhibi o y e ec s and s a is ically signi ican biological esponses a e p esen a equencies 0.8 and 0.4 kHz, as well as he base e- quency. These equencies co espond o he ion pa a- me ic esonance equency o Ca2+ ions, and ha monic componen s he eo in acco dance wi h Ledne ’s IPR heo y om [25], [26] and [31] and he Eq. (1): = c n=1 n · q 2πm ·Bgen,(1) whe e c ep esen s he cyclo on esonance equency o he ion, qis he elemen a y cha ge o he ion, mis c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 101 BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE 0.850 0.800 0.890 0.640 0.899 0.690 0.540 0.750 0.864 0.590 0.720 0.650 0.100 0.200 0.300 0.400 0.700 0.750 0.800 0.850 0.900 1.600 1.800 2.000 F equency (kHz) 0 0.2 0.4 0.6 0.8 1 1.2 G ow h a ea a io (exposed/con ol) Fig. 3: G aphical in e p e a ion o p oli e a ion esponse o i adia ed samples wi hin he in es iga ed equency ange o applied ime- a ying LF EMF. mass o he ion and ndeno es he co esponding ha - monic componen . Bgen is he mean alue o gene a ed magne ic lux densi y, which in ou case was 2.39 mT. P edic ed equencies o he biological esponse based on his model a e also shown in Tab. 1. I is e iden ha expe imen al equencies a which s a is- ically signi ican biological e ec s we e obse ed a e closely ela ed o hei heo e ically p edic ed coun e - pa s. Also appa en om he p esen ed se o expe i- men s is ha he biological e ec ends o disappea a lowe equencies, as was he case in expe imen s using 0.4 kHz. To e i y his obse a ion, we op ed o in es- iga e a wide equency ange, wi h ocus on low e- quencies and also on equencies a ound he expe imen- ally p o en biologically ac i e equency o 0.8 kHz. This se o expe imen s is p esen ed g aphically in Fig. 3, o be e illus a ion and in e p e a ion he eo . Obse ed esul s once again show inhibi o y e ec s. Mo e in e es ingly, he e a e signs o pe iodici y wi hin he expe imen al da a, wi h s ong peaks a p e iously desc ibed esonance equencies o Ca2+ ha could be p edic ed by IPR model. Fu he mo e, he p e ious as- sump ion, ega ding he biological e ec ex inc ion a lowe equencies, seemed o occu a equencies below 0.4 kHz. Ano he in e es ing obse a ion conce ns he neigh- bou hood o he equency 0.8 kHz, whe e he p oli e a- i e esponse is weak in compa ison wi h he esonance (base) equency, albei s ill p esen . This obse a ion poin s o he window heo y, men ioned by Ma ko in [22], bu could be also explained as a cumula i e e - ec o o he ions, which play an impo an pa in cell p oli e a ion p ocesses. Since equency dependen biological esponse is e - iden om he p esen ed esul s, we op ed o also in es iga e he in luence o magne ic lux densi y ~ B o he gene a ed LF EMF. Fo his pu pose, we chose he equency o 0.8 kHz, whe e he biological esponse seemed o be mos signi ican , and al e ed he alue o ~ B o 50 %, 25 % and 10 % o i s o iginal alue. These al e a ions we e echnically pe o med by am- pli ude changes o e ec i e alue o d i ing cu en , which di ec ly in luences he ampli ude o ~ Bin he coil ca i y and hus he exposed olume. Resul s p esen ed in Fig. 4 show ha signi ican ly s ong p oli e a i e esponse is p esen only wi h o igi- nal magne ic lux densi y o 2.39 mT. The biological e- sponse is weak o no longe obse ed a gi en equency due o modi ied magne ic lux densi y o he applied LF EMF. F equency 800 Hz 2.39 1.195 0.5975 0.239 Bgen (mT) 0 0.2 0.4 0.6 0.8 1 1.2 G ow h a ea a io (exposed/con ol) 0.56 0.79 0.94 0.90 Fig. 4: G aph o p oli e a ion dependence o S. Ce e isiae on Bgen, a he equency o 800 Hz. c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 102 BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE 4. Conclusion The p esen ed a icle discusses chosen heo ies ela ed o LF EMF mechanisms o in e ac ion wi h biologi- cal objec s, ep esen ed he ein by Saccha omyces ce e- isiae cells. Repe i ion o p e iously conduc ed expe - imen s published in [8], [38], [40], [41] and [42] con- i med inhibi o y e ec on he p oli e a ion esponse a he equency o 1.6 kHz. Fu he mo e, he expe - imen al esul s clea ly demons a ed non- he mal e - ec s o ex e nally applied ime- a ying LF EMF on he p oli e a ion p ocess o cul i a ed cells. Ou ind- ings ega ding he Ca2+ a e also in co ela ion wi h esea ch p esen ed in [43]. The obse ed biological e- sponses could be e e ed o as equency selec i e be- cause s a is ically signi ican e ec s occu only a spe- ci ic equencies, which poin s o he esonance cha ac- e o he obse ed bio-e ec s. The mechanism o ac ion in luencing he beha iou o he i adia ed biological samples could be heo e i- cally explained by he IPR heo y. This model success- ully p edic s obse ed biologically ac i e equencies, conside ed esonance equencies o Ca2+ ions and ha - monic componen s he eo . F om his poin o iew, we can d aw he conclusion ha Ca2+ ions play an im- po an ole in cellula p oli e a ion p ocesses, and could be exploi ed as a ge s o i adia ion by ex e - nal LF EMF uned o pa ame ic esonance equency he eo , which co esponds wi h indings p esen ed by Belo a [27]. The ele ance o V. V. Ledne ’s heo y can be also con i med by esul s o ou in es iga ion o magne ic lux densi y changes wi h espec o p oli - e a ion esponse a unchanged equency. This means ha when expec ing biological esponse in acco dance wi h he IPR heo y and Eq. (1), any change o ~ Bnec- essa ily leads o change o he ion pa ame ic esonance equency, bu no e e y change o equency mus lead o change o magne ic lux densi y. Despi e he indings p esen ed wi hin his a icle, an unambiguous explana ion o EMF in luence on li - ing s uc u es is s ill lacking. 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DOI: 10.1007/s10867-018-9500-0. c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 105 BIOMEDICAL ENGINEERING VOLUME: 18 |NUMBER: 2 |2020 |JUNE Abou Au ho s Roman RADIL was bo n in T encin, Slo ak Republic, in 1984. G adua ed om he Facul y o Elec ical Enginee ing, Uni e si y o Zilina, in 2008 om Biomedical Enginee ing and ecei ed he Ph.D. deg ee in Theo e ical Elec omagne ics a he same uni e si y, in 2012. A p esen he wo ks as assis an p o esso a he Dep . o Elec omagne ic and Biomedical Enginee ing, Facul y o Elec ical Enginee ing and In o ma ion Technology, Uni e si y o Zilina. His esea ch ac i i ies a e ocused on in es- iga ion o LF EMF e ec s on biological samples and biomedical image p ocessing. Resul s o his esea ch ha e been published in se e al jou nals and p esen ed in na ional and in e na ional con e ences. Jan BARABAS was bo n in Ba dejo , Slo ak Republic, in 1982. G adua ed om he Facul y o Elec ical Enginee ing, Uni e si y o Zilina, in 2008 om Biomedical Enginee ing and ecei ed he Ph.D. deg ee in Theo e ical Elec omagne ics a he same uni e si y, in 2011. A p esen he wo ks as esea che a he Depa men o Elec omagne ic and Biomedical Enginee ing, Facul y o Elec ical Enginee ing and In o ma ion Technology, Uni e si y o Zilina. His cu en esea ch endea ou s include ongoing in es- iga ion o elec omagne ic ields and in e ac ion he eo wi h biological objec s, he indings o which ha e been published in se e al jou nals and in e na- ional con e ences. O he ac i i ies include biomedical image p ocessing, signal p ocessing and p og amming. Ladisla JANOUSEK was bo n in Michalo ce, Slo ak Republic, in 1974. G adua ed om he Facul y o Elec ical Enginee ing, Uni e si y o Zilina, in 1997 om Elec ic Powe Sys ems and ecei ed he Ph.D. deg ee in Elec ic Machines and Appa a uses a he same uni e si y, in 2002. A p esen he is head o he Depa men o Elec omagne ic and Biomedical Enginee ing, Facul y o Elec ical Enginee ing and In- o ma ion Technology, Uni e si y o Zilina. The main ields o his esea ch ac i i ies a e elec omagne ic me hods o ma e ials’ non-des uc i e e alua ion and non- he mal e ec s o EMF on li ing o ganisms. His achie emen s ha e been acknowledged by se e al p es igious awa ds. Ma in BERETA was bo n in Ruzombe ok, Slo ak Republic, in 1990. G adua ed om he Facul y o Elec ical Enginee ing, Uni e si y o Zilina, in 2014 om Biomedical Enginee ing and ecei ed he Ph.D. deg ee in Theo e ical Elec omagne ics a he same uni e si y, in 2017. A p esen he wo ks as esea che a he Ins i u e o Measu emen Science, Slo ak Academy o Sciences in B a isla a. His esea ch ac i i ies a e ocused on LF EMF biological e ec s and moni o ing o ul a-weak pho on emission om biological samples. Resul s o his esea ch ha e been published in se e al jou nals and p esen ed in na ional and in e na ional con e ences. c 2020 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 106