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Experimental and Modelling Studies on the Reactions of the Sulfate Ion Radical

Abstract

Ez az értekezés közvetlen folytatása és kiegészítése a kutatócsoportunkban korábban lezajlott vizsgálatoknak a kén(IV) autooxidációjának kinetikájával és mechanizmusával kapcsolatosan. Tanulmányoztuk a S(IV) és a peroxodiszulfát-ion (S2O82-) közötti redoxireakciót, mint az autooxidáció mechanizmusának egyik alrendszerét. Az ezüstionok a peroxodiszulfát-ion oxidációs reakcióinak jól ismert katalizátorai, vizsgálataink során ezért ezüst-nitrátot adtunk a S(IV)–oxigén–peroxodiszulfát reakcióelegyekhez, erősen savas közegben. Részletes kinetikai vizsgálatok alapján javaslatot tettünk a S(IV) autooxidációjának mechanizmusára ezüst(I)- és peroxodiszulfát-ionok jelenlétében, valamint meghatároztuk a reakció sebességi egyenletét. Az autooxidációs folyamatok mechanizmusa gyökös láncreakció, amelyben szulfit-, szulfát- és peroxomonoszulfát-iongyökök (rendre SO3•-, SO4•- és SO5•-) a láncvivő részecskék. A szulfátiongyök (SO4•-) kiemelt szerepet tölt be a katalízisben, mivel reakciója a katalizátorral fontos láncvivő lépés, valamint a peroxodiszulfát ionokat termelő másodrendű rekombinációja többnyire az egyetlen jelentős lánclezáró lépés. A szulfátiongyök reakcióit független kísérletekben, lézeres villanófény-fotolízis segítségével vizsgáltuk, és meghatároztuk a SO4•- és számos kis szervetlen részecske, valamint néhány biomolekula között lejátszódó másodrendű reakciók sebességi állandóját. A szulfátiongyök–jodidion rendszerben pszeudo-elsőrendű viselkedést tapasztaltunk, noha ennek feltétele, a jodidionok nagy feleslege lokálisan nem teljesül a reakcióelegyben. Matematikai modellt vezettünk be annak vizsgálatára, hogy van-e mód a jodidionok diffúzió általi pótlására a reakciótéren kívüli térrészből és ezáltal a pszeudo-elsőrendű kinetikához szükséges koncentrációarány visszaállítására. A szulfátiongyök inhomogén térbeli koncentráció-eloszlásának modellezése megmutatta, hogy a diffúzió nem befolyásolja a jodidionnal való másodrendű sebességi állandó meghatározását pszeudo-elsőrendű körülmények között.

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Experimental and Modelling Studies on the Reactions of the Sulfate Ion Radical

Author: Dóka, Éva
Year: 2016
Source: https://dea.lib.unideb.hu/bitstreams/fbce0f50-2b99-403c-8d97-d8375a13ca4d/download
DE TTK
1949
Expe imen al and Modelling S udies on he Reac ions o he Sul a e
Ion Radical
Ph.D. hesis
Dóka É a
Supe iso : D . Gábo Len e
UNIVERSITY OF DEBRECEN
Chemis y G adua e School
Deb ecen, 2016
DE TTK
1949
Expe imen al and Modelling S udies on he Reac ions o he Sul a e
Ion Radical
Ph.D. hesis
Dóka É a
Supe iso : D . Gábo Len e
UNIVERSITY OF DEBRECEN
Chemis y G adua e School
Deb ecen, 2016
II
III
Ezen é ekezés a Deb eceni Egye em Te mésze udományi Dok o i
Tanács Kémiai Dok o i Iskola K/2 Koo dinációs és Anali ikai Kémia
p og amja ke e ében készí e em a Deb eceni Egye em
e mésze udományi dok o i (Ph.D.) okoza ának elnye ése céljából.
Deb ecen, 2016. május 27.
Dóka É a
Tanúsí om, hogy Dóka É a dok o jelöl 2012 - 2015 közö a en
megne eze Dok o i Iskola K/2 Koo dinációs és Anali ikai Kémia
p og amjának ke e ében i ányí ásommal égez e munkájá . Az
é ekezésben oglal e edményekhez és az ezekből szüle e
publikációkhoz a jelöl önálló alko ó e ékenységé el megha á ozóan
hozzájá ul . Az é ekezés el ogadásá ja asolom.
Deb ecen, 2016. május 27.
D . Len e Gábo

IV
V
EXPERIMENTAL AND MODELLING STUDIES ON THE REACTIONS OF THE
SULFATE ION RADICAL
É ekezés a dok o i (Ph.D.) okoza megsze zése é dekében
a Kémia udományágban
Í a: Dóka É a okle eles egyész és alapokle eles ma ema ikus
Készül a Deb eceni Egye em Kémiai Dok o i Iskolája
(Koo dinációs és anali ikai kémiai p og amja) ke e ében
Téma eze ő: D . Len e Gábo egye emi aná
A dok o i szigo la i bizo ság:
elnök: D . Kö é Ka alin egye emi aná (DE)
agok: D . Tó h Ágo a egye emi aná (SZTE)
D . Só ágó Im e p o esso eme i us (DE)
A dok o i szigo la időpon ja: 2016. má cius 8.
Az é ekezés bí álói:
D . ...........................................
D . ...........................................
D . ...........................................
A bí álóbizo ság:
elnök: D . ...........................................
agok: D . ...........................................
D . ...........................................
D . ...........................................
D . ...........................................
Az é ekezés édésének időpon ja: 2016. ..............................................
VI
VII
"In he end, e e y hing will be OK. I i 's no OK,
i 's no ye he end."
/Fe nando Sabino/
XIV

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
1
1. In oduc ion
Sul u (S) is a nonme allic elemen in he 16 h g oup o he pe iodic able, a membe o he
oxygen amily o chalcogens. The la e name is a hyb id o he G eek wo d  (khalkos,
meaning o e) and he La inized su ix ‘-gen’, meaning bo n o p oduced. This name implies
ha he i s wo elemen s o he g oup, oxygen and sul u a e highly equen componen s o
o es and mine als, oxygen being he mos abundan elemen in he Ea h’s c us .1 The
chalcophile g oup wi hin he Goldschmid classi ica ion comp ises he elemen s which a e
likely o o m compounds wi h sul u , mainly p and d block me als o so cha ac e .2,3 Sul u
is ubiqui ous in Na u e, i occu s mos ly in he ollowing o ms:
 elemen al sul u in he cap ocks o sal domes o in olcanic e up ions
 H2S in na u al gas and sul u o ganic subs ances in pe oleum
 sul ide o es o me als (PbS, FeS2, CuS, ZnS, HgS e c.).1
Owing o he high abundance o he elemen , sul u has been known since he ancien imes.
I is men ioned se e al imes in he Bible as ‘ i e and b ims one’,
*
in he con ex o hell i e and
e e nal mise y. Maybe i is he malodo ous smell and oxic na u e o many sul u compounds
ha ea ned he elemen such a nega i e epu a ion (al hough pu e sul u does no smell a all).
Fi e and b ims one also appea s in he G eek classics Iliad and Odyssey, al hough Home migh
ha e mis akenly e e o he smell o sul u ins ead o he unpleasan odo o ligh ning-gene a ed
ozone.4,5 The odo o skunk sp ay is also due o low molecula weigh hiol compounds o
me cap ans.
The o igin o he name sul u is obscu e, he ea lies appea ances da e back o ea ly La in
cul u e o he i s cen u ies BC. I is known no o be a G eek loan wo d, since G eek au ho s
called he elemen θεῖον ( heion, ances o o he p e ix hio- o sul u con aining compounds).
Concei ably, he wo d de eloped om sulpu o sulphu and inally o sul u . The spelling
‘sulphu ’ pe sis ed, especially in B i ish linguis ic en i onmen , e en hough IUPAC
s anda dized he ‘ ’ spelling a ew decades ago, wi hou espec o geog aphical di e ences.6,7
Owing o i s alence elec on composi ion and ca ena ion p ope y, sul u ea u es e sa ile
edox beha io wi h signi ican en i onmen al aspec s, biological ele ance as well as indus ial
applica ions.
*
The Lo d es s he igh eous and he wicked, And he one who lo es iolence His soul ha es. Upon
he wicked He will ain sna es; Fi e and b ims one and bu ning wind will be he po ion o hei cup.
/Psalms 11:5-6/
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
2
Sul u dioxide (SO2) is one o he so-called c i e ia ai pollu an s. De imen al e ec s o
SO2 gas necessi a ed he admission o uppe limi s o daily exposu e, se by EPA (U. S.
En i onmen al P o ec ion Agency), o a oid po en ial human heal h and p ope y damage.8
SO2 is a gaseous compound ha accumula es in he a mosphe e by olcanic ac i i y and
om an h opogenic sou ces such as combus ion o ossil ene gy ca ie s (due o sul u
con amina ions in coal, pe oleum and na u al gas) and me allu gy.
Upon di ec exposu e, highe le els o sul u dioxide cause espi a o y i i a ion, induce
b onchocons ic ion9 (sho ness o b ea h due o he cons ic ion o pulmona y ai ways) and
inc ease he symp oms o as hma ic pa ien s.10 A slow- eleasing SO2 dono molecule,
benzo hiazole-sul ina e has ecen ly been disco e ed, which acili a es he examina ion o he
biological e ec o inhaled and endogenously gene a ed SO2.11
On a global le el, he majo consequence o a mosphe ic SO2 is he o ma ion o acid ain
o acid deposi ion.12-17 Acid ain is ainwa e wi h a pH below he na u al alue o 5.6, which is
a esul o he dissolu ion o a mosphe ic CO2. Acidi ica ion o ain all is a ela i ely mode n
phenomenon, he consequence o hea y indus ializa ion o he las wo cen u ies. G eenland
ice laye s om he 1800s ha e nea ly neu al pH alues. The pH dec ease is agg a a ed by he
o ma ion o sul u ic acid om SO2 acco ding o eq. (1), he au oxida ion o hyd a ed SO2.
Au oxida ion is a gene ic e m o he eac ions whe e he educ an is oxidized by elemen a y
oxygen om ai . The p e ix ‘au o’ e e s o he ac ha he oxidan is seldom added delibe a ely
in hese p ocesses bu is simply aken up om he en i onmen .
2 H2O·SO2 + O2 = 2 HSO4− + 2 H+ (1)
The lowes pH alue measu ed in ainwa e was 1.5, de ec ed in Wheeling, Wes Vi ginia,
in 1979.18 Hea y acid ains lead o ex ended de o es a ion, des uc ion o limes one moun ains
and man-made objec s and buildings, such as he Taj Mahal in India, buil en i ely om ma ble.
A e y in e es ing and scien i ically challenging aspec o he s epwise o ma ion o H2SO4
om sul u and oxygen is he es o a ion o he Swedish wa ship Vasa, which sank on he
maiden jou ney in 1628 and was conse ed unde wa e un il 1961, when he w eckage was
sal aged om S ockholm ha bo . Today he emains o he ship a e exhibi ed in he Vasa
Musee in S ockholm. The wa e which Vasa sank in was ich in sul a e educing bac e ia.
Elemen a y sul u , as well as sul u compounds o in e media e oxida ion s a es accumula ed in
he oak beams o he ship du ing he 333 yea s she spen subme ged. E e since he Vasa was
b ough o he su ace, scien is s s uggle wi h he massi e acidi ica ion o he skele on because
he i on in he bol s ca alyzes he o e all oxida ion o sul u o sul u ic acid.19
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
3
An ini ia i e eme ged in he ield o geoenginee ing o coun e ac global wa ming based on
he global dimming e ec o s a osphe ic sul a e ae osols by he e lec ion o sola adia ion.
The concep would endo se he applica ion o missiles and ai c a o deli e sul u dioxide and
o he sul u gases in he s a osphe e, o ac as sul a e p ecu so s and hus inc ease he albedo
( e lec i i y) o he plane . Howe e , he ecep ion o such echnological measu es has been
con o e sial because hey do no eplace consis en poli ical and social engagemen o he
educ ion o o al g eenhouse gas emission. In addi ion, he long- e m ha m ul consequences o
he ex a sul u bu den a e unp edic able.20-22
A mosphe ic au oxida ion o SO2 d ew conside able a en ion om ino ganic chemis s, and
de ailed mechanis ic s udies e ealed ha he in e media es o he au oxida ion p ocess a e o
adical na u e (mainly SO3, SO4, SO5).
In gene al, sul a e ion adical (SO4) is one o he mos b oadly s udied ee adical in he
li e a u e, along wi h hyd oxyl adical (OH).23-25 SO4 is a highly eac i e ansien species
wi h s ong oxidizing powe Eº(SO4/SO42V
Recen ly, he ole o sul a e ion adical in a mosphe ic aqueous phase chemis y has been
in es iga ed by He mann and co-wo ke s.23,26-29 SO4 is conside ed as an oxidan in so-called
ad anced oxida ion p ocesses (AOPs) in wa e and was ewa e ea men , in o de o elimina e
o ganic and ino ganic con aminan s.30-35 Simul aneously, ad anced educ ion p ocesses (ARPs)
in ol e UV o ul asound p oduced sul i e ion adical (SO3) o he educ i e deg ada ion o
ha m ul oxidized pollu an s.36 Sul a e ion adical de i ed oxida ion also has biochemical
applica ions. An e icien , unable oo p in ing me hod was de eloped o moni o ing global
p o ein oxida ion s a us. O iginal FPOP (Fas Pho ochemical Oxida ion o P o eins) u ilized
OH as oxidan . The in oduc ion o SO4 as a oo p in ing agen is an imp o emen due o he
sligh ly lowe eac i i y and highe a ge speci ici y compa ed o hyd oxyl adical.37
The p esen hesis is dedica ed o shed u he ligh on he ole o sul a e ion adical in he
ansi ion me al ca alyzed and he iodide ion ca alyzed, pho oini ia ed au oxida ion o hyd a ed
SO2, and mo e gene ally, he au oxida ion o S(IV). T adi ional me hods o aqueous solu ion
kine ics a e employed, as well as lase lash pho olysis o he di ec obse a ion o SO4.
Compu a ional simula ions a e ca ied ou o s udy he po en ial e ec o di usion and spa ial
inhomogenei ies du ing lase lash pho olysis expe imen s.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
4
2. Li e a u e o e iew
2.1. Redox chemis y o sul u
Sul u has a alence elec on con igu a ion o 3s23p4. The e o e, i can occu in compounds
in (2)  (+6) oxida ion s a es (e en numbe s a e p e e ed). Due o he wide ange o a ailable
oxida ion numbe s, sul u exhibi s e sa ile edox chemis y. This sec ion will ocus on he
edox cha ac e is ics o sul u oxyacids and anions along wi h he de i ed sul u oxy adicals.
Table 1. Sul u oxyacids, conjuga e oxyanions and he ela ed ee adicals.
Fo mula
Name o
oxyacid
Oxida ion
s a e(s)
Conjuga e
anion
Rela ed
adical
H2SO4
sul u ic acid
VI
sul a e, SO42
hyd ogen
sul a e, HSO4
sul a e ion
adical,a SO4
H2S2O7
disul u ic acid
VI
disul a e,
S2O72
H2SO5
pe oxomono-
sul u ic acid
VI
pe oxomono-
sul a e, SO52
pe oxomono-
sul a e ion
adical, SO5
H2S2O8
pe oxodi-
sul u ic acid
VI
pe oxodisul-
a e, S2O82
H2S2O6
di hionic acid
V
di hiona e,
S2O62
H2Sn+2O6
poly hionic
acid
V, 0
poly hiona e,
Sn+2O62
H2S2O3
hiosul u ic
acid
IV, 0,
(o II, II)
hiosul a e,
S2O32
(H2SO3)
H2O∙SO2
(sul u ous
acid) hyd a ed
sul u -dioxide
IV
sul i e, SO32
hyd ogen-
sul i e, HSO3
sul i e ion
adical, SO3
H2S2O5
disul u ous
acid o
py osul u ous
acid
V, III
Disul i e;
commonly
known as
me abisul i e
o py osul i e,
S2O52
H2S2O4
di hionous acid
III
di hioni e,
S2O42
aal e na i e names: sul a e adical anion, sul a e adical
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
5
Table 1 gi es a b ie summa y o hese kinds o species in he o de o dec easing oxida ion
numbe .1 The s abili ies o hese acids and sal s a y on a b oad scale, e.g. ee acid o ms o
di hionic, ‘sul u ous’ and di hionous acids a e i ually nonexis en , hey a e mos ly ound in
solu ions and in sal s as he conjuga e oxyanions.
H2O∙SO2 and SO4 a e o u mos impo ance in he p esen hesis, hei spec al and
chemical ea u es will be discussed in u he de ail in Sec ions 2.2 and 2.3. Py osul a e sal s
will be p esen ed he ein as a sou ce o S(IV) species and o he sul u oxy adicals (SO3, SO5)
as congene s o sul a e ion adical.
The sul u oxy species p esen ed in Table 1 pa icipa e in a ious edox equilib ia. S anda d
elec ode po en ials o a ew edox pai s a e collec ed in Table 2.
Table 2. S anda d elec ode po en ials o sul u oxy ions and adicals
Redox couplea
E° (V)
Redox coupleb,c
E° (V)
S/S2
-0.476
SO2/SO2
-0.17
S/H2Saq
0.142
-0.262
S2O62/S2O3
0.564
-0.288
S2O82/SO42
2.010
-0.31
S2O82/HSO4
2.123
SO3/SO32
0.63
S4O62/S2O32
0.080
0.72
H2SO3/HS2O4
-0.056
0.76
H2SO3/S
0.449
0.89
SO32/S2O42
-1.120
0.73±0.01b
SO32/S2O32
-0.571
SO3/HSO3
0.84
SO42H2SO3
0.172
SO4/SO42
2.43
SO42/S2O62
-0.220
2.52-3.08
SO42SO32
-0.930
2.6
SO5/HSO5
1.1
SO5/SO52
0.81±0.02b
S2O62/SO3SO32
-0.49
S2O82/SO4SO42
1.39
S4O63/2S2O32
1.07±0.03b
a: e .38; b: e .39 ; c: e .40 and e e ences he ein

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
6
SO42 and HSO4 a e he mos equen sul u oxyanions in Na u e. These a e bo h e y
s able species, hey a e o med as oxida ion p oduc s o sul u compounds and du ing he
decomposi ion o pe oxodisul a e ions. Sul a e sal s ake pa in he composi ion o pa icula e
ma e in he a mosphe e. Howe e , sul u ic acid, especially in i s concen a ed o m, is a highly
eac i e, s ong oxidizing agen , which is able o dissol e elec oposi i e me als. Disul u ic o
py osul u ic acid is ound in uming sul u ic acid (also known as oleum, oil o i iol, o spi i
o i iol), i is o med by he dissolu ion o SO3 in H2SO4.
Anhyd ous pe oxomonosul a e ion (H2SO5) is also called Ca o’s acid, i is one o he
s onges oxidan s known (E°(HSO5/HSO4) = 1.84 V)40. I s conjuga e anion, SO52 is
a ailable as he composi e sal Oxone® ( egis e ed adema k o DuPon ), which has been
ecognized as a ‘g een’ oxidizing agen as i s educ ion p oduc is sul a e ion and wi h he
possible by-p oduc elemen a y oxygen.41,42
Pe oxodisul a e ion (S2O82) is gene ally used in he o m o i s wa e -soluble ammonium
o po assium sal s. Pe oxodisul a e sal s a e u ilized as oxidizing and bleaching agen s and o
ini ia e adical polyme iza ion p ocesses. Ammonium pe sul a e (APS) is he mos common
ini ia o in polyac ylamide gel elec opho esis.
S2O82 has e y high elec ode po en ials (see Table 2), hus i is expec ed o be a s ong
oxidizing agen , bu i s edox eac ions a e qui e sluggish due o a kine ic ba ie . Sil e (I) ion
has been p o ed o be a powe ul ca alys o hese eac ions. They usually ake place as chain
eac ions and hei a e de e mining s ep is eq. (2), which is a one-elec on ans e ha p oduces
highly eac i e sul a e ion adical.43-45
Ag+ + S2O82 = Ag2+ + SO42 + SO4 (2)
Di hiona e ion (S2O62) exhibi s qui e poo edox chemis y, i is highly ine unde common
ci cums ances. I canno be p o ona ed in he usual pH ange, and i eac s e en wi h s ong
oxidizing agen s only a ele a ed empe a u es. I i pa icipa es in a edox eac ion, he i s
s ep is disp opo iona ion in mos cases, whe e sul u (VI) and sul u (IV) a e he di ec p oduc s
and he la e can be oxidized apidly by he oxidizing agen .46
Poly hiona es (O3S-(S)n-SO32 o Sn+2O62) a e ela i ely s able sul u oxyanions,
con aining a chain o ze o- alen sul u a oms as a linke be ween wo SO3 g oups.
Poly hiona es a e equen ly ound in c a e lakes, and hey we e sugges ed o se e as e icien
ma ke s o o hcoming olcanic e up ions.47
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
7
Thiosul u ic acid has no been isola ed so a , i is only known o exis in hiosul a e sal s.
S2O32ion is a medium s ong educing agen . I is ex ensi ely used in iodome ic
measu emen s in he labo a o y p ac ice and as dechlo ina ing agen in he ex ile indus y.48
Di hionous acid is uns able bo h in i s pu e o m and in aqueous solu ion, di hioni es
(S2O42) can be isola ed as anhyd ous sal s. In he p esence o wa e , hey disp opo iona e in o
sul i e and hiosul a e anions (especially in acidic medium). Sodium di hioni e is used as a
educing agen in indus ial dyeing p ocedu es and o labo a o y pu poses as well.49,50
2.2. Au oxida ion s udies o sul u (IV)
Table 1 and Table 2 in he p e ious sec ion show ha +4 is an in e media e oxida ion
s a e o sul u . SO2 is gene ally conside ed o be a mode a e educing agen , al hough depending
on he eac ion pa ne , i can be an oxidizing agen as well. A well-known example o he la e
is he eac ion be ween SO2 and hyd ogen sul ide, which is an impo an s ep o he Claus
p ocess (pa en ed in 1883), used simul aneously o he desul u iza ion o c ude oils and he
p oduc ion o elemen a y sul u .51
The majo occu ences o S(IV) a oms a e sul u dioxide (SO2), hyd a ed sul u dioxide,
H2O∙SO2 and i s dep o ona ed o ms: HSO3 and SO32 ions. S(IV) is also ound in sul u o ganic
molecules, such as sul onic acids, sul ona es and sul i e es e s.52,53 The o mula H2OSO2 is
gene ally used o deno e dissol ed sul u dioxide because he e is no expe imen al e idence o
he exis ence o he ully p o ona ed H2SO3 molecule. The acid dissocia ion cons an alues o
he subsequen dep o ona ion s eps o H2O∙SO2 a e pKa,1 = 1.86 and pKa,2 = 6.34.
The dime iza ion o sul i e ions in o py osul i e o me abisul i e ions (S2O52) a highe
concen a ions is a well-known phenomenon.54 In aqueous medium, he dime ic anion is in
equilib ium wi h he hyd ogen sul i e ion, he S2O52 o m only occu s in concen a ed solu ions
( 0.1 M). The e o e, i is con enien o p epa e solu ions o sul i e ions by dissol ing
py osul i e sal s, e.g. Na2S2O5.55 In he subsequen sec ions o he hesis, he di e en
dep o ona ed o ms o H2O∙SO2 will be collec i ely e e ed o as ‘sul i e ion’ o simply S(IV).
The a mosphe ic au oxida ion o S(IV), depic ed in eac ion (1) is he majo sou ce o acid
ain o ma ion. SO2 can easily accumula e in ain d ople s, as i s wa e solubili y is much highe
compa ed o o he a mosphe ic gases (Table 3).38 Mole ac ions a e compa ed ins ead o he
co esponding Hen y’s cons an s because he concen a ion o SO2 passes h ough he limi o
alidi y o Hen y’s law.56 The solubili y o sul u dioxide is lowe in acidic medium, which
p o ides he basis o he iden i ica ion o sul i e ions wi hin he F esenius sys em.57
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
8
Table 3. Mole ac ions (X) o a mosphe ic gases in aqueous solu ions. p = 1 a m, T = 25 °C38
X
SO2
2.9102
CO2
7.1104
O2
2.5105
N2
1.3105
The kine ics and mechanism o he p ocess ep esen ed by he o e all equa ion shown in eq.
(1) d ew conside able a en ion om ino ganic chemis s, a signi ican amoun o expe imen al
indings ha e been published on his subjec . Ca aly ic aspec s, pho ochemical phenomena o
he ole o ee adicals in he sys em ha e been discussed.
2.2.1. T ansi ion me al ion ca alysis in he au oxida ion o sul u (IV)
Nume ous s udies ha e e ealed he ole o ansi ion me al ion ca alysis in he oxida ion o
sul u (IV) species. K a and an Eldik in es iga ed he i on(III) ca alyzed au oxida ion o
sul u (IV) oxides and conside ed he possible ole o me al-sul i o complexes in he
mechanism.58-61 A de ailed kine ic and mechanis ic analysis o he Fe(III)S(IV)O2 sys em
was published la e on and p o ed he ca aly ic e ec o i on(III).62 B and and an Eldik
examined he in luence o pH, he medium and aging in independen expe imen s.63 These
au ho s also p esen ed a comp ehensi e o e iew o he subjec , ocusing on a mosphe ic-
ele an p ocesses and mechanisms.40 Acco ding o his summa y, he majo i y o he published
eac ion mechanisms o he homogeneous ansi ion me al ca alyzed au oxida ion o sul u (IV)
oxides sugges adical mechanisms ha in ol e s eps om he scheme gi en by Bäcks öm,
who was he i s o publish mechanis ic obse a ions on eac ion (1).55 He p oposed a adical
chain mechanism in ol ing sul oxy adical in e media es, which was suppo ed by he ac ha
common adical sca enge s inhibi he eac ion. Fábián and Cso dás e iewed he ole o me al
ions in au oxida ion p ocesses om kine ic and mechanis ic poin s o iew.64
Elding and co-wo ke s examined he ca aly ic e ec o manganese, ch omium and
anadium ions, and hey obse ed he eme gence o i on-manganese syne gism. They e en
conside ed gold(III) as a ca alys in S(IV) au oxida ion based on a educ ion s udy o Au(III)
complexes by sul i e and hyd ogen sul i e ions.65-68 Alexande e al. epo ed ha 9-17% o o al
sul a e p oduc ion on Ea h can be assigned o oxida ion o S(IV) by O2 ca alyzed by Fe(III)
and Mn(II).69
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
9
Coiche and co-wo ke s s udied he adical in e media es ha a e gene a ed in he
au oxida ion p ocess ca alyzed by Co(II) and Cu(II) complexes, and hei po en ial de imen al
e ec s on DNA chains.70,71 The ca aly ic e ec o Cu(III) e aglycine complexes on he
au oxida ion was ound and s udied by Anas and Ma ge um.72 DNA damage examina ions
we e also ca ied ou by Bu ows’s eam wi h Ni(II) and Mn(II) complexes.73-75 Pionee ing
wo k on ee adical induced DNA damage was p esen ed by Clemens on Sonn ag.76
2.2.2. Pho ochemical phenomena in he au oxida ion o sul u (IV)
Pho oini ia ed au oxida ion in he p esence o i on(II)
The au oxida ion p ocesses o sul u (IV) in acidic aqueous solu ion ha e been ex ensi ely
s udied by Ke ezsi e al.55,77-79 They obse ed ha he unca alyzed o da k eac ion is e y slow.
In he p esence o Fe(II), he a e o he eac ion inc eases, bu i ac s as an auxilia y educing
agen a he han a ca alys . The expe imen s ha e been ca ied ou in a diode a ay
spec opho ome e , which is a con enien ool o he simul aneous ini ia ion and de ec ion o
he eac ion. Acco ding o hei esul s, he unca alyzed au oxida ion akes place h ough exci ed
H2OSO2 and HSO5 in e media es and ollows he s oichiome y indica ed in eq. (1).78
The eac ion a e is independen o he concen a ion o dissol ed oxygen in he pH- ange
0.0  1.67, bu shows a well-de ined dependence on ligh in ensi y and sul u (IV) concen a ion.
In he p esence o i on(II), he o ma ion o i on(III) ions was de ec ed, which may be
in e p e ed by he simul aneous p esence o wo addi ional pa hways. Bo h pa hways con ain
he oxida ion o i on(II) in o i on(III) by one o he eac ion in e media es. Figu e 2.1 p esen s
he sugges ed scheme o he eac ion.
Figu e 2.1. Pho oini ia ed au oxida ion o sul u (IV) in he absence and p esence o i on(II)
ions in acidic aqueous phase.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
16
A de ailed kine ic and spec oscopic analysis o sul i e anion adical and i s decay
mechanisms was gi en by Waygood and McEl oy.135 Lase lash pho olysis o sodium
di hiona e (S2O62)solu ions a 193 nm led o he o ma ion o SO3 and SO32. They epo ed
ha he decay o sul i e ion adical is second o de wi h a limi a e cons an o (4.0 ± 0.3)  l08
M1 s1 and akes place by he simul aneous ecombina ion in o di hiona e ion and sel - eac ion
in o sul i e ion and SO3. The ela i e a e cons an o eac ion () compa ed o (7) was ound o
be 0.8 ± 0.2.
SO3 + SO3S2O62 
SO3 + SO3SO32 + SO3 (7)
Wa neck and colleagues s udied he s eady s a e pho olysis o SO32and HSO3a 254 nm
and analyzed he possible ee adical eac ions, a e cons an s and p oduc dis ibu ion in he
p esence and absence o dissol ed oxygen.136,137
The li e a u e o pe oxomonosul a e adical (SO5) is limi ed compa ed o he p e iously
discussed congene s, al hough due o apid in e con e sion eac ions, he sepa a e in es iga ion
o hese adicals is ba ely easible. P ac ically all ee adical s udies connec ed o S(IV)
au oxida ion men ioned ea lie deal wi h he pa allel occu ence o SO3, SO4 and
SO5 adicals, some o hem wi h SO2 as well. The adical is mos likely gene a ed by he
oxygen addi ion o sul i e ion adical and decays by se e al adical- adical and adical-s able
species eac ions. A pape om T. N. Das ocuses mainly on SO5 adical, e-e alua ing i s
ole in sul i e au oxida ion chains in liquid hyd ome eo s.138 SO5 adical shows a weak
abso p ion band be ween 260-265 nm wi h a mola abso p ion coe icien o 1065 ± 80 M1
cm1.
2.4. E ec o inhomogenei ies in as eac ion kine ics
As men ioned in he p e ious sec ion o his hesis, he inhomogeneous dis ibu ion o he
ansien abso bing species in he sample is a ypical cha ac e is ic o lase lash pho olysis
expe imen s. This ac should be aken in o accoun du ing he acquisi ion and p ocessing o
ansien abso p ion da a. Sample inhomogenei ies can lead o dis o ed conclusions, especially
when he kine ic ace de ec ed is no an exponen ial cu e. Whene e possible, se ing pseudo-
i s o de condi ions is desi able in o de o a oid he usage o ac ual ansien concen a ions.
Only a hand ul o pape s deal wi h he expe imen al and/o ma hema ical ea men o
po en ial inhomogenei y issues and he esul ing e o s in kine ic conclusions.

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
17
A he dawn o he lash pho olysis echnique, J. W. Boag analyzed he e ec o non-uni o m
dis ibu ion o ini ial ansien concen a ion along and ac oss he analyzing ligh beam.139 He
conside ed i s and second o de eac ions and made an e o o gi e analy ical exp essions
o he di e ence be ween he ac ual and he expe imen ally de e mined a e cons an s. He
assumed ce ain shapes o he ini ial dis ibu ion (see Figu e 2.4) and used p ac ically
concei able pa ame e s, such as o al abso bance be ween 0 and 2 ( ypically 0.4-0.6), h > 0.5,
expe imen al ime leng h a leas 4-5 hal -li e o he obse ed species. He concluded ha i s
o de eac ions a e less in luenced by ini ial dis ibu ions, and wi h he abo e pa ame e alues,
he di e ence be ween 𝑘
 (as he assigned he obse ed a e cons an ) and k ( he ac ual alue) is
less han 1%. I is wo h no ing ha he used he linea ized e sions o he in eg a ed a e laws
(which is a sou ce a s a is ical dis o ions i sel ) in his deduc ions and igno ed di usi e mo ion
o he pa icles wi hin he expe imen al ime.
A) B)
Figu e 2.4. Ini ial dis ibu ion o ansien concen a ion along he analyzing ligh beam in lash
pho olysis expe imen s. A) Ex eme cases. a = (sine)2, b = iangula , c = sine dis ibu ion; I0 =
inciden ligh in ensi y; I( ) = exi ligh in ensi y a ime . B) Expec ed p ac ical dis ibu ions.
(a) iangula cap; (b) sine cap; (c) pa abolic cap. The pa ame e h is he a io be ween he
minimum and maximum o ini ial concen a ion (0  h  1). Figu es adap ed om Boag, T ans.
Fa aday Soc. 1968, Figs. 1 and 4.139
Bazin and Ebbesen s udied he e o o igina ing om a poo o e lap be ween he lase beam
and he analyzing (o p obe) beam in gi en expe imen al a angemen s o lase lash pho olysis.
They in oduced wo kinds o co ec ion ac o s o such bad o e laps in he lase and p obe
di ec ions, and p o ided echnical ad ice on how o de ec hem.140
Ins ead o conside ing ac ual kine ic measu emen s, hey ocused on he de ia ion o he
measu ed abso bance (ODexp) om he eal alue (OD ue). Figu e 2.5 shows he possible
sou ces o insu icien o e lap be ween he wo ligh beams.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
18
Figu e 2.5. Examples o bad o e lap si ua ions in lase lash pho olysis expe imen s. The solid
line ep esen s he analyzed space, he dashed line delinea es he lase beam. The ha ched a ea
shows he o e lap. (a) and (b): pe pendicula , (c) pseudo on ace, (d) collinea a angemen .
( he eade migh no ice ha he panels a e labelled clockwise ins ead o ow-con inuously).
Figu e adap ed om Bazin and Ebbesen Pho ochem. Pho obiol. 1983, Fig. 1.140
The au ho s assigned x and y o he ac ions no co e ed by he complemen a y beams o
cases (a) and (b) in Figu e 2.5. Wi h he no a ions o he igu e,
l
'll
y

and
s
'ss
x

; 0  x, y < 1,
and he ela ion be ween OD ue and ODexp is gi en in eq. (8).
OD ue = ODexp  SF(x,y)  DF(x) (8)
SF alues a e he scale ac o s 1/(1  x) and 1/(1  y), he p opo ionali y ac o s o bad
o e lap ac oss and along he analyzing di ec ion, espec i ely. An impo an ou come o hei
calcula ions is ha he a io OD ue/ODexp inc eases wi h ODexp, and hey de ined a dis o ion
ac o (DF) as he a io o he ela i e e o s a high and low expe imen al alue.
DF = (
exp
ue
OD
OD
)/(
exp
ue
OD
OD
)ODexp  0 (9)
DF is only a unc ion o x and no y, in he case o bad o e lap along he ligh pa h, OD ue
is always linea ly dependen on ODexp. They sugges ha DF ends o cause mo e ouble in
da a p ocessing, which con i ms ha i is p e e able o wo k wi h low abso bance alues, as
long as he signal- o-noise a io is accep able.
Cassidy and Long c ea ed a ma hema ical model o es he alidi y o expe imen al a e
cons an s de e mined unde pu a i e pseudo- i s o de condi ions.141 The unde lying chemical
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
19
sys ems we e lase lash pho olysis s udies o CO pho odissocia ion eac ions om ansi ion
me al ca bonyl complexes and he subsequen coupling o he ML6 and ML5 o ms.
CO(CO)M(CO)M 56 hν
(10)
11256 (CO)M(CO)M(CO)M  hν
(11)
Thei model implies ha M(CO)5 is gene a ed by a lase beam o ci cula c oss sec ion and
moni o ed by a second beam in collinea a angemen , in a cylind ical olume. M(CO)5
concen a ion decays eaching ze o a he a ace o he cu e e, and he abso bance can be
calcula ed om Bee ’s law. They also conside ed he di usion o M(CO)5 molecules ou side
o he moni o ed olume in he case whe e eac ion (11) is su icien ly slow. Ma hema ically,
his sys em could be desc ibed by wo-dimensional di usion equa ions coupled o a second
o de eac ion. All di usion coe icien s we e supposed o be equal.
I was assumed ha M(CO)6 is in high excess compa ed o M(CO)5 and he second o de
a e cons an o eq. (11) was calcula ed by he adi ional pseudo- i s o de me hod (plo ing
kobs as a unc ion o [M(CO)6], he ob ained slope is k). The pe cen age di e ences we e gi en
be ween log(kcalc) and log(kinpu ) alues, whe e k we e used as an inpu pa ame e in he model.
Upon conside ing di e en kinds o concen a ion inhomogenei ies and pa ame e se s, he
ollowing conclusions we e d awn om hei esul s:
i. when he ela i e concen a ion o M(CO)5 was high ( iola ing pseudo- i s
o de condi ions), he di usion ou side he cylinde s a ed o in e e e below
kinpu = 107 M1 s1, causing up o 14% dec ease
ii. inhomogeneous dis ibu ion along he ligh pa h (due o Bee ’s law) did no
cause any dis o ion, as long as he high excess o M(CO)6 was main ained
iii. when a Gaussian beam p o ile was used o he exci a ion pulse, di usion caused
e o s below 107 M1s1, a low ela i e concen a ion o M(CO)6;
i . as an in e es ing complemen a y in o ma ion, he pseudo- i s o de plo o he
de e mina ion o kcalc was always pe ec ly linea , e en i high e o s we e ound
be ween log(kcalc) and log(kinpu ). The e o e, he co ela ion coe icien in his
case was no a good indica o o es ing pseudo- i s o de beha io .
The esul s o he abo e desc ibed model calcula ions we e no compa ed o expe imen al
da a because LFP measu emen s we e ca ied ou wi h pe pendicula a angemen .
Sample inhomogenei y issues can be assessed by expe imen al app oaches as well. Bonneau
and co-wo ke s published a de ailed manual o he collec ion and analysis o ansien
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
20
abso p ion da a and emphasized he impo ance o co ec ins umen geome y and
inhomogeneous ansien dis ibu ions. They sugges ed ha a mi o should be placed a he
side o he sample opposi e o he lase exci a ion spo in o de o e lec he pumping ligh back
and hus inc ease he abso bed ac ion o ligh and o se inhomogenei ies a he same ime.142
Goez e al. ealized he idea abo e, al hough hey used a solid co ne - ube e o e lec o
ins ead o a mi o , in o de o educe Bee inhomogenei y (caused by abso p ion along he ligh
pa h o he lase ).143 Re o e lec o s a e less sensi i e o alignmen impe ec ions han mi o s
and make i possible o ca y ou measu emen s a di e en wa eleng hs wi hou changing he
mi o . The inciden and he e lec ed beams we e mixed wi h he aid o he e o e lec o which
had double bene icial e ec : he o al abso bed in ensi y inc eased and he Bee inhomogenei y
dec eased ( he o me by a ac o o 1.45-1.65, he la e 2.6-4.8- old). They ound a e y simple
ela ion be ween hese wo e ec s. Acco ding o hei calcula ions and measu emen s, in he
p esence o he e o e lec o , he abso bed in ensi y inc eased by a ac o o 𝜃, hen he o al
dec ease o inhomogenei y equals 2/𝜃-1. Dis o ions a ising om he Gaussian beam p o ile
also imp o ed a li le by his me hod, bu he au ho s poin ed ou ha beam shape s o easie
expe imen al se ings could co ec o he non-uni o mi y o he beam.
Solu ion inhomogenei ies end o cause dis o ions in s opped low (SF) measu emen s as
well, al hough he sou ce i he non-uni o m dis ibu ion o concen a ions is concep ually
di e en han he ones connec ed o lash pho olysis expe imen s. In he case o he s opped
low echnique, he inhomogenei y a ises om he ac ha he mix u e o he eac ing
componen s needs a ce ain ime o ill he obse a ion cell ( illing ime). Fo e y apid
eac ions, whose hal -li e is compa able o he illing ime o he ins umen , a signi ican
di e ence can be o med be ween he on and he a ace o he obse a ion cell (see Figu e
2.6). Ro abache and colleagues de eloped ma hema ical models o esol e second o de a e
cons an s o such apid eac ions, aking in o accoun he concen a ion g adien unde
app op ia e condi ions. Fi s , hey ea ed i e e sible second o de eac ions, choosing an
a bi a y ‘ze o ime’ o he measu emen s. They managed o de e mine a a e cons an o 7 
106 M1 s1 his way.144 Thei model was la e imp o ed o emo e he e e sibili y and s a ing
ime es ic ions and he a e cons an limi shi ed up by an o de o magni ude.145 Finally, hey
comple ed hei esul s by ano he g adien -co ec ed app oach, whe e hey used he s eady s a e
abso bance o ming in he low cell be o e he cessa ion o he low.146 The esol ed a e
cons an s o bo h me hods, as well as a non-co ec ed second o de ea men o he sake o
compa ison, we e ca e ully analyzed using as eac ions o ansi ion me al complexes as an
expe imen al model. The a e cons an s o he la e we e p edic ed om he Ma cus heo y.147
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
21
As a conclusion, second o de a e cons an s o magni ude up o 108 M1 s1 became a ailable
om s opped low measu emen s o eac ions whose hal -li es a e less han one hal o he
ins umen dead ime ( he ime equi ed o he solu ion o a el he dis ance x + l in Figu e
2.6).
Figu e 2.6. Scheme o sample concen a ion g adien in a s opped low expe imen . Figu e
adap ed om Dunn e al. J. Phys. Chem. 1996, Fig. 1.146
Conside ing he sub-nanosecond o millisecond ime esolu ion o he lase lash pho olysis
echnique, i has impo an o e lap wi h he s opped low me hod om he poin o iew o he
o de o magni ude o he accessible a e cons an s. Howe e , he majo di e ences be ween
hese echniques s ill hold, i.e. s opped low deals wi h g ound s a e species (e en i e y sho
li ed), whe eas LFP ope a es wi h ansien species gene a ed by he high ene gy lase pulse.
The lase gene a ion me hod elimina es he need o manual o ins umen al mixing. On he
o he hand, he ‘ba ch’ cha ac e is ic o LFP measu emen s is a echnical limi a ion. The poin
is ha all g ound s a e molecules a e loca ed in he cu e e a he momen o he lase pulse.
The e o e, he e ec o he lase on all componen s has o be es ed indi idually be o e
obse ing a adical eac ion and some imes i is impossible o isola e a ce ain componen o
abso b he o al amoun o lase ene gy.

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
22
3. Resea ch objec i es
The p esen hesis is dedica ed o shed u he ligh on he ole o sul a e ion adical in he
ansi ion me al ca alyzed au oxida ion o hyd a ed SO2, mo e gene ally, au oxida ion o S(IV).
The ca aly ic e ec o sil e (I) ions in he p esence o pe oxodisul a e (S2O82) ions is
in es iga ed. T adi ional me hods o aqueous solu ion kine ics a e employed, as well as lase
lash pho olysis echnique o he di ec obse a ion o SO4. Compu a ional simula ions a e
ca ied ou o s udy he po en ial e ec o di usion and spa ial inhomogenei ies du ing lase
lash pho olysis expe imen s.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
23
4. Expe imen al me hods
4.1. Ma e ials
All chemicals used in his s udy we e o analy ical eagen g ade and we e pu chased om
comme cial sou ces. Sodium sul i e s ock solu ions we e p epa ed eshly om Na2S2O5
(Reanal) e e y day. Whene e necessa y, py osul i e solu ions we e deae a ed by bubbling A
(pu i y > 99.95%) o a leas 15 min in o de o inc ease he ep oducibili y o measu emen s
unde anae obic condi ions.
Po assium pe oxodisul a e s ock solu ions we e p epa ed om K2S2O8 (Reanal). This
solu ion was oxygena ed du ing he O2-dependen expe imen s. Sil e (I) ca alys solu ions we e
p epa ed by dissol ing a weighed amoun o AgNO3 (Reanal) o a known inal olume. Doubly
deionized and ul a il e ed wa e om a Millipo e Q sys em was used in he en i e wo k. Mos
o he expe imen s we e ca ied ou a high and cons an acid concen a ion (0.10 o 0.33 M
sul u ic acid). The e o e, addi ional sal was no used o adjus he ionic s eng h.
4.2. Ins umen a ion and so wa es
4.2.1. UV- is spec opho ome ic expe imen s ela ed o S(IV) au oxida ion
UV- is spec a we e eco ded on a Pe kin Elme Lambda 2S o a Pe kin Elme Lambda 25
scanning spec opho ome e . Kine ic expe imen s we e ca ied ou in s anda d qua z cu e es
(op ical pa h leng h = 1.000 cm). The o e all sample olume was 3.00 cm3 in each case.
Cons an empe a u e (25.0  0.1 C) was main ained wi h an ex e nal he mos a and
ci cula ing he mal ba h.
Samples we e p epa ed by he ollowing me hod. Requi ed aliquo s o py osul i e,
pe oxodisul a e and sul u ic acid solu ions we e mixed wi h wa e and he mos a ed o 3-4
min. The p ocess was s a ed by adding he ca alys immedia ely p io o commencing he
de ec ion in he spec opho ome e .
Reac ion a es we e de e mined by linea i ing o da a cu es. One can calcula e he ac ual
a e om he slopes o abso bance e sus ime unc ions by using he mola abso p ion
coe icien o sul u (IV), known om independen expe imen s. F om a ma hema ical poin o
iew, he a e de e mina ion equi es nume ical di e en ia ion. Unde he usual condi ions, he
accu acy o eac ion a es a e 10%, indica ed by he e o ba s in Figu e 5.3-Figu e 5.7Figu e
5.9. In he sil e (I) ca alysis s udy, ano he me hod was applied o compu e he eac ion a es
(which we e ai ly cons an wi hin a single expe imen ) and compa e hem wi h he esul s o
nume ical de i a ion. The slopes o he sec ions p eceding he b eak poin we e calcula ed (see
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
24
Figu e 5.2) The abso bance change can be ans e ed in o concen a ion change by di iding i
wi h he (appa en ) mola abso p ion coe icien alid a he pH o he eac ion sys em. The
main ad an age o he la e me hod is ha i a oids he possible p oblems a ising om
impe ec he mos a ing, which may occu a he beginning o expe imen s.
Reac ion a es de e mined wi h he wo di e en me hods we e in e y good ag eemen , and
we used he esul s o he me hod o ini ial a es in he inal calcula ions.
4.2.2. Lase lash pho olysis measu emen s
Lase lash pho olysis (he ea e e e ed o as LFP) expe imen s ha e been ca ied ou in
an LKS.60 nanosecond ansien abso p ion spec ome e , shown in Figu e 4.1.
Figu e 4.1. Applied Pho ophysics LKS.60 nanosecond lase lash pho olysis ins umen
The ins umen is equipped wi h a Quan el B illian Nd:YAG lase along wi h i s second,
hi d, ou h and i h ha monic gene a o s ( e e ed as SHG, THG, FoHG, FiHG). Nd:YAG
(Neodymium doped y ium aluminum ga ne ) is a common solid-s a e lase ype, whe e he
lasing medium is a Y3Al5O12 c ys al doped wi h 0.1-1% Nd3+. The p ima y wa eleng h o an
Nd:YAG lase ligh is 1064 nm, i s ha monics emi a 532 (2nd), 355 (3 d), 266 (4 h) and 213
nm (5 h). Ha monics a e gene a ed by speci ic c ys als ha exhibi non-linea op ical e ec s.
Common non-linea c ys als a e KDP, DKDP, LaTiO3, BaTiO3 e c.
Table 4. Speci ica ion o he ou h ha monic o Quan el B illan Nd:YAG lase
Wa eleng h
266 nm
Pulse leng h ( ull wid h a hal maximum)
6 ns
Repe i ion a e
10 Hz
Ene gy pe pulse (max.)
40 mJ
Beam diame e
6 mm
Q-swi ch
ON
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
25
In he p esen hesis, he ou h ha monic o he Nd:YAG lase was used o gene a e sul a e
ion adicals and o he ansien species. Table 4 con ains he cha ac e is ic ea u es o he lase
beam. Un o una ely, he i h ha monic gene a o educed he ene gy o he lase pulse oo
much and i could no be employed o any p ac ical pu poses in his s udy.
Q-swi ching is a equen echnique applied o inc ease lase powe by sho ening he lase
pulse. O iginally, he Q- ac o (o quali y ac o ) is a e m o elec onics, i desc ibes he
goodness o an RLC ci cui . Q-swi ching is ealized by a Pockels-cell in he LKS.60 ins umen .
The analyzing ligh sou ce was a 150 W ozone ee xenon a c lamp (OSRAM 150W/CR
OFR) and i s ligh beam en e ed a 1.00  1.00 cm luo escence qua z cu e e. We ha e implied
c oss-beam exci a ion, he p obe beam and he lase beam we e in oduced in o he sample in a
pe pendicula a angemen . The cu e e was placed in an adjus able sample holde , which was
posi ioned ho izon ally so ha he analyzing ligh beam hi close o he on ace o he cu e e
whe e lase beam en e ed. This is an impo an se ing as he concen a ion o ansien species
gene a ed by he lase exci a ion ypically dec eases apidly wi h he dis ance om he on
window (see also Sec ion 5.3.7.).
A p og ammable /3.4 g a ing monoch oma o wi h a symme ical Cze ny-Tu ne op ical
con igu a ion was combined wi h a R928 pho omul iplie o he ansien signal de ec ion a
di e en wa eleng hs. Da a poin s we e collec ed by an Agilen In iniium digi al s o age
oscilloscope (model numbe DSO8064A, maximum sampling speed 4 GSa/s (0.25 ns be ween
da a poin s), bandwid h 600 MHz, ou pu impedance 50 Ω).
The exci a ion o is(bipy idine) u henium(II) chlo ide (Ru(bpy)3Cl2) by he hi d ha monic
o he lase (355 nm) was used as a es eac ion (Figu e 4.2).148
Figu e 4.2. A) T ansien abso p ion spec a o is(bipy idine) u henium(II) chlo ide a e 355
nm lase pulse. The signals we e eco ded a he indica ed ime poin s a e he lase pulse. B)
Fi s o de decay o iple Ru(bpy)32+. The solid line ep esen s he non-linea leas squa e i
o he obse ed da a poin s. [Ru(bpy)32+] = 31 μM,

ex = 355 nm
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
32
Figu e 5.6. Reac ion a es as a unc ion o he pe oxodisul a e ion concen a ion in he
au oxida ion o sul u (IV). The solid line ep esen s he bes i o he p oposed mechanism
shown in Scheme 1. [S(IV)] = 3.0 mM; [H2SO4] = 0.103 M; [Ag+] = 0.167 mM; pa h leng h =
1.000 cm; [O2] = 0.130 mM; V = 3.00 cm3; T = 25.0 C.
Dependence o he eac ion a e on pH
Finally, he e ec o pH on he a e o he ze o h o de p ocess is shown in Figu e 5.7. The
pH was calcula ed om he concen a ion o added sul u ic acid conside ing he ac ha
hyd ogen sul a e ion is no a s ong acid (pKa2 = 1.06 a 25 °C)
Figu e 5.7. Reac ion a es as a unc ion o he pH in he au oxida ion o sul u (IV). [S(IV)] =
3.0 mM; [S2O82] = 0.0284 M; [Ag+] = 0.167 mM; [O2] = 0.130 mM; pa h leng h = 1.000 cm;
V = 3.00 cm3; T = 25.0 C.

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
33
5.1.3. Sugges ed mechanism
Ou kine ic obse a ions, in acco dance wi h ea lie esul s o in es iga ions77,79 abou he
au oxida ion o S(IV), con i m ha a chain eac ion akes place in he s udied sys em.
The ini ia ion s ep is e y likely o be he well-known eac ion be ween sil e (I) and
pe oxodisul a e ions (2), which p oduces wo eac i e chain ca ie s, sil e (II) and sul a e ion
adicals. Ano he ini ia ion s ep will be men ioned la e , as he e e se di ec ion o a chain
e mina ion s ep.



 2
44
2
18
2
82 SOSOAgOSAg k
(18)
Among he p opaga ion s eps, he eac ion o Ag(I) and SO4 p oducing sil e (II) and
HSO4 ce ainly occu s (19).



 2
4
2
19
4SOAgSOAg k
(19)
P e ious s udies e ealed ha he possible di ec eac ion be ween sul a e ion adical and
sul u (IV) does no play a ole in he au oxida ion p ocess.62,77,79 The e o e, i is easonable o
assume ha sil e (II) eac s wi h sul u (IV) in he chain eac ion. Ag(II) is a s ong oxidizing
species, which can easily be educed by S(IV) in a one-elec on s ep (20).

  3
20
2SOAg(IV)SAg k
(20)
I is also known om he li e a u e ha sul i e ion adical eac s e y quickly wi h dissol ed
oxygen124 and i is likely ha he p oduc o his eac ion, pe oxomonosul a e ion adical
(SO5), oxidizes sul u (IV) (21, 22).
  5
21
23 SOOSO k
(21)
  4
2
4
22
5SOSO(IV)SSO k
(22)
A his poin , one can see ha s eps (19 – 22) compose a chain in which one cycle leads o
he o ma ion o wo sul a e ions by he eac ion o one oxygen and wo sul u (IV).
Wi h ega d o chain e mina ion, one can conside he disp opo ion o sil e (II) in o
sil e (I) and sil e (III) which is also a p e iously published assump ion.43,45
(III)AgAgAg223
2  k
(23)
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
34
  2
24 Ag2(III)AgAg k
(24)
Eqs. (23) and (24) desc ibe a e e sible p ocess in which he e e se s ep ac s as ini ia ion,
as i p oduces a chain ca ie . This should be aken in o accoun in he de i a ion o he a e law.
Sil e (III) is a e y eac i e species and i eac wi h sul u (IV) in a wo-elec on p ocess
(25), whe e sil e (I) is ep oduced, eady o join he ca aly ic cycle again.

 2
4
52 SOAg(IV)S(III)Ag k
(25)
Sil e (III) is supposed o occu as he AgO+ oxoca ion in aqueous solu ion, which means
ha eac ion (25) possibly occu s as oxygen a om ans e .45
The ecombina ion o sul a e ion adicals o pe oxodisul a e ion (26) has always appea ed
in he chain mechanisms o he au oxida ion p ocesses o sul u (IV) examined be o e.77,79 Fo
his eason, i seems app op ia e o conside i in he scheme as a possible e mina ion s ep.
   2
82
26
4OSSO2k
(26)
Scheme 1.
The sugges ed mechanism o he au oxida ion o sul u (IV) in he p esence o sil e (I) and
pe oxodisul a e ions.



 2
44
2
18
2
82 SOSOAgOSAg k
1=k18[Ag+][S2O82−]
(R1)



 2
4
2
19
4SOAgSOAg k
2=k19[Ag+][SO4•−]
(R2)

   3
obs
20
2SOAg(IV)SAg k
3= 𝑘20
obs[Ag2+][S(IV)]
(R3)
  5
21
23 SOOSO k
4=k21[SO3•−][O2]
(R4)
   4
2
4
obs
22
5SOSO(IV)SSO k
5= 𝑘22
obs[SO3•−][S(IV)]
(R5)
(III)AgAgAg223
2  k
6=k23[Ag2+]2
(R6)
  2
24 Ag2(III)AgAg k
7=k24[Ag+][Ag(III)]
(R7)

  2
4
obs
25 SOAg(IV)S(III)Ag k
8= 𝑘25
obs[Ag(III)][S(IV)]
(R8)
   2
82
26
4OSSO2k
9=k26[SO4•−]2
(R9)
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
35
Figu e 5.8. The sugges ed mechanism o he au oxida ion o sul u (IV) in he p esence o
sil e (I) and pe oxodisul a e ions.
5.1.4. De i a ion o he a e law
The egula ma hema ical ea men o chain eac ions is he long-chain app oach.91
Essen ially, i is buil on wo main pilla s:
 he s eady-s a e app oxima ion can be applied o e e y eac i e in e media es (Ag(II),
Ag(III), SO3, SO4, SO5 in he p esen s udy)
 he a e o chain ini ia ion o e mina ion is lowe han hose o he p opaga ion s eps.
Two gene ally applied conclusions can be d awn om he assump ions abo e:
i. Each p opaga ion s ep has he same a e as he a e o he ne eac ion.
ii. The a e o ini ia ion and e mina ion s eps a e equal. I mo e han one ini ia ion o
p opaga ion s eps occu , hen equali y e e s o he sum o he a es o a ce ain ype:
 
kkT,
jjI,
He e j is he numbe o ini ia ion s eps (I), k is he numbe o e mina ion s eps (T).
The a e o eac ion (1) may be desc ibed by eq. (27).
   
d
Od
d
SOOHd
2
1222 


(27)
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
36
The a e is equal o he a e o any p opaga ion s eps, so i can be de i ed om eqs. (19)-
(22). I is con enien o use eq. (20) o his pu pose, in o de o simpli y subsequen
calcula ions.
= 3 = 𝑘20
obs[Ag2+]ss[S(IV)] (28)
he e subsc ip ss indica e s eady-s a e concen a ions
All eac ions discussed a e supposed o be second o de , and hese a e elemen a y s eps
excep o eac ions (20), (22) and (25). In he la e cases, he dep o ona ion o H2OSO2 should
be aken in o accoun in he pH- ange o he s udy. H2OSO2 and HSO3 o ms a e ela ed by a
as p e-equilib ium. Consequen ly, he a e o s ep (20) is gi en in eq. (29)
= [Ag2+]ss(k20[H2O∙SO2] + k20′[HSO3]) (29)
Conside ing he equilib ium o he wo S(IV) o ms, he o mula akes he ollowing o m:
)][H(
][H
[S(IV)]][Ag
a2020
a
ss
2K'kk
K





(30)
Implying he long-chain assump ion (ii), one can ob ain eq. (31):
2
ss426
2
ss
2
23ss24
2
8218 ][SO][Ag][Ag(III)][Ag]O][S[Ag 


 kkkk
(31)
The s eady-s a e concen a ion o sil e (III) can be exp essed om eq. (32) as ollows:
2
ss
2
23ss24
a
a2525
ss ][Ag][Ag[Ag(III)]
][H
][H
[S(IV)][Ag(III)] 




kk
K
K'kk
(32)
][Ag
][H
][H
[S(IV)]
][Ag
[Ag(III)]
24
a
a2525
2
ss
2
23
ss








k
K
K'kk
k
(33)
The s eady-s a e concen a ion o sul a e ion adicals can be gi en om he ac ha he
a es o p opaga ion s eps a e equal ( 2 = 3):
a
a2020
ss
2
ss419 ][H
][H
[S(IV)]][Ag][Ag][SO K
K'kk
k





(34)
)]([H
][H
][Ag
[S(IV)]][Ag
][SO
a19
a2020ss
2
ss4Kk
K'kk


 




(35)
Subs i u ing he s eady-s a e concen a ions in eqs. (33) and (35) in o eq. (31) yields:
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
37
2
a19
a2020
2
2
2
ss
2
26
2
ss
2
23
24
a
a2525
2
ss
2
23
24
2
8218
)]([H
][H
][Ag
[S(IV)]][Ag
][Ag
][Ag
][H
][H
[S(IV)]
][Ag
][Ag]O][S[Ag




























Kk
K'kk
kk
k
K
K'kk
k
kk
(36)
F om eq. (36), he s eady-s a e concen a ion o sil e (II) can be exp essed:
 
][Ag
][H
][H
S(IV)
][Ag
)]([H
][H
][Ag
[S(IV)]
1
]O][S[Ag
][Ag
24
a
a2525
24
2
a19
a2020
2
2
23
26
2
82
23
18
2
ss
2


























k
K
K'kk
k
Kk
K'kk
k
k
k
k
(37)
The combina ion o eqs. (30) and (37) leads o he inal a e law:
 
][Ag
][H
][H
S(IV)
][Ag
)]([H
][H
][Ag
[S(IV)]
1
]O][S[Ag
][H
)][H[S(IV)](
24
a
a2525
24
2
a19
a2020
2
2
23
26
2
82
23
18
a
a2020































k
K
K'kk
k
Kk
K'kk
k
k
k
k
K
K'kk
(38)

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
38
The sugges ed model i s he obse ed kine ic da a e y well. Solid lines in Figu e 5.3-
Figu e 5.6 ep esen he bes i o he p oposed mechanism. Figu e 5.9 shows he co ela ion
be ween all eac ion a es measu ed a one gi en pH ([H2SO4] = 0.103 M). The ho izon al axis
con ains he measu ed a es, while da a on he e ical axis a e he a es calcula ed wi h he
pa ame e s om he bes i . The co ela ion plo also con i ms ha he model p o ides excellen
quan i a i e in e p e a ion o he kine ic esul s.
Figu e 5.9. Co ela ion be ween measu ed and calcula ed a es.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
39
5.2. Lase lash pho olysis s udies on he eac ions o sul a e ion adical
5.2.1. Gene a ion and ecombina ion o he sul a e ion adical (SO4)
P e iously published gene a ion me hods and cha ac e iza ion o he sul a e ion adical,
SO4, a e ex ensi ely discussed in Sec ion 2.3. In ou expe imen s, SO4 was gene a ed by he
pho olysis o an aqueous solu ion o K2S2O8 (3). The adicals a e he p oduc o he homoly ic
scission o he pe oxy bond in S2O82– ion.
  4
2
82 SOOS hν
(39)
Whene e equi ed o he calcula ions,

(SO4)450 nm = 1600 dm3 mol–1 cm–1 was used,
based on he s udies o McEl oy.118
Following he pho olysis o a 0.0967 M K2S2O8 solu ion a 266 nm, kine ic aces simila
o he one in Figu e 5.10 we e de ec ed. The eco ded kine ic aces in he absence o any o he
eac an s we e i ed wi h second o de cu es, and hey all ga e a e y good i . The e o e, i
is easonable o assume ha he ecombina ion o sul a e ion adicals in o he p ecu so
pe oxodisul a e ions akes place unde hese condi ions (40), which is he same p ocess as he
las chain e mina ion s ep in Scheme 1. (R9).
   2
82
40
4OSSO2k
(40)
Figu e 5.10. T ansien abso p ion signal o he sul a e ion adical. [K2S2O8] = 0.0967 M, T =
25 °C, V = 3.00 cm3. The solid line ep esen s he i ed second o de cu e (k = 3.91  108 M1
s1).
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
40
The second o de a e cons an o he eac ion, deno ed he e by k40, was de e mined om
he i ed pa ame e s conside ing he mola abso p ion coe icien men ioned abo e. The alue
o he calcula ed second o de a e cons an was (4.1  0.2)  108 M–1s–1.
The ecombina ion p ocess occu s on he millisecond imescale, which equi es special
ea men , as he basic se ings o he ins umen a e con igu ed o nanosecond measu emen s.
In o de o measu e on longe imescales, he impedance o he oscilloscope has o be inc eased
om 50 Ω in o he kΩ ange, up o 1 MΩ, by he ins alla ion o a a iable esis ance box be ween
he signal cable om he pho omul iplie ube and p ope oscilloscope channel. Fu he mo e, a
longe imescales, he Xe a c lamp has o be ope a ed in con inuous mode ins ead o pulsed
mode, o he wise he lamp lashes would be oo sho o he de ec ion o he ansien species.
Theo e ically, he LKS.60 ins umen wi h i s ac ual equipmen is able o ollow chemical
eac ions on he imescales be ween 1 ns o a ew seconds wi h he con enien ins umen
se ings and da a e alua ion me hods implied.
In o de o e eal a possible pH-dependence o he a e cons an , k40 was measu ed o e
he acidic ange. Figu e 5.11 shows ha he a e cons an o he ecombina ion p ocess is
independen o pH in he implied ange.
Figu e 5.11. The e ec o pH on he ecombina ion a e o sul a e ion adicals. [K2S2O8] =
0.0967 M, T = 25 °C, V = 3.00 cm3.
5.2.2. Reac ion o sul a e ion adical and sil e (I)-ion
In he subsequen s age o ou kine ic in es iga ion, he main ocus was he ole o sul a e
ion adical in he au oxida ion p ocess o sul u (IV). One can see om Scheme 1 ha SO4 is
a chain ca ie in e media e, i is p oduced in he ini ial s ep (2) and in a p opaga ion s ep by he
educ ion o pe oxomonosul a e ion adical.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
41
Figu e 5.12. Abso p ion a 450 nm ollowing he pho olysis o K2S2O8 (0.100 M) solu ion,
con aining AgNO3 (6.12 mM). The solid line ep esen s he i ed single exponen ial cu e (kobs
= 3.8  107 s1).
The eac ion be ween sul a e ion adical and sil e (I) ion is o high impo ance in chain
p opaga ion, because i is he p ocess h ough which he ca alys en e s he cycle. The e o e, we
in ended o de e mine he a e cons an o eac ion (19) by means o lase lash pho olysis.
An aqueous solu ion o AgNO3 was pho olyzed a 266 nm as a blank expe imen in o de o
measu e i s con ibu ion o he o e all abso p ion in he eac ion. I was ound ha sil e ni a e
does no show any ansien abso p ion a 450 nm, hus he abso p ion can be a ibu ed solely
o sul a e ion adical. Figu e 5.12 shows a ep esen a i e ansien abso p ion cu e.
The eac ion akes place on he nanosecond imescale, and can be i ed wi h a single
exponen ial cu e, hus e e ing o a i s o de p ocess. Concen a ions o he eac an we e se
in a way ha pseudo- i s o de condi ions would be ul illed o Ag+ ions o e sul a e ion
adicals.
A su p ising obse a ion was made ollowing he pho olysis o K2S2O8–AgNO3 aqueous
solu ion. A e a ew lase sho s (3-10 depending on he concen a ion a io), da k g ey cloudy
p ecipi a ion was seen in he cu e e, i s a he spo o lase exci a ion. Ag2O o ma ion was
excluded upon he ac s ha he colo o he p ecipi a e is di e en om b ownish Ag2O, i does
no dissol e in sul u ic acid and i appea s e en a e y low pH. The da k g ey p ecipi a ion is
hus assumed o be elemen a y sil e , he sou ce o which is unknown so a . I was hough o
be p oduced in he pho odecomposi ion o AgNO3, bu in he absence o K2S2O8, he
p ecipi a ion did no occu .
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
48
Figu e 5.21. Ra io o second o de a e cons an o he decomposi ion and he mola abso p ion
coe icien o chlo ine molecule anion. [K2S2O8] = 0.100 M, () [H2SO4] = 0 M, (▼) [H2SO4]
= 0.0049 M, T = 25 °C, V = 3.00 cm3.
On he longe ime scale, he second o de decomposi ion o chlo ine molecule anion was
de ec ed (see Figu e 5.21). The second o de a e cons an o he decay o Cl2 is (1.4 ± 0.04) 
105 s1 cm 

(Cl2−) a ei he pH = 2.03 o in unbu e ed aqueous solu ion.
5.2.6. Reac ion o sul a e ion adical wi h b omide ion
In he eac ion o sul a e ion adical wi h b omide ion, b omide molecule anion is p oduced
in eac ions (47) and (48). Kine ic da a we e collec ed a 360 nm (see spec a in Figu e 5.22).157
B  + SO4 = B + SO42 (47)
B  + B ⇌ B 2 (48)
Figu e 5.22. Time esol ed ansien abso p ion spec a o he b omine molecule anion.
[K2S2O8] = 0.100 M, [KB ] = 0.010 M, V = 3.00 cm3, T = 25 °C, pH = 7 (unbu e ed). Spec a
we e eco ded a he indica ed ime poin s a e he lase pulse. Nega i e ime on panel A (-0.1
μs) e e s o he p e-pulse sec ion o he cu es (panel B, < 0).

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
49
Figu e 5.23. Pseudo- i s o de a e cons an s as a unc ion o b omide ion concen a ion in he
eac ion o sul a e ion adical and b omide ion. [K2S2O8] = 0.100 M, () [H2SO4] = 0 M, (▼)
[H2SO4] = 0.0049 M, T = 25 °C, V = 3.00 cm3.
The eac ion was ollowed on sho e and longe imescales, unde pseudo- i s o de
condi ions. The second o de a e cons an was ound o be (1.51 ± 0.02)  109 M1 s1 in
unbu e ed aqueous solu ion and (1.59 ± 0.03)  109 M1 s1 a pH 2.03 (Figu e 5.23).
On he longe ime scale, he second o de decomposi ion o b omine molecule anion was
de ec ed, which was ound o be independen om he b omide ion concen a ion (see Figu e
5.24). The second o de a e cons an o he decay o B 2 is (1.8 ± 0.1)  105 s1 cm 

(B 2−)
in unbu e ed aqueous solu ion and a pH = 2.03.
Figu e 5.24. Ra io o second o de a e cons an and mola abso p ion coe icien o he
decomposi ion o b omine molecule anion. [K2S2O8] = 0.100 M, [H2SO4] = 0.0049 M, V = 3.00
cm3, T = 25 °C.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
50
5.2.7. Reac ion o sul a e ion adical wi h yp ophan
The kine ics and mechanism o he oxida ion o yp ophan (T p) and i s de i a i es by
pe oxomonosul a e ions ha e been ecen ly s udied in ou labo a o y.158 Since yp ophan is an
a oma ic amino acid wi h nume ous po en ial oxida ion si es (Figu e 5.25), he de ailed
cha ac e iza ion o i s oxida ion eac ions is a a he challenging ask ha needs o be
app oached by a combina ion o expe imen al echniques.
The lase lash pho olysis me hod p o ides an e icien ool o s udy he one elec on
oxida ion eac ions o T p ha in ol e sho li ed eac i e in e media es. The one elec on
oxida ion o a oma ic amino acids such as yp ophan and y osine plays an impo an ole in
he o ma ion o p o ein adicals,159-163 hus pa icipa ing in elec on anspo and edox
egula ion.
Figu e 5.25. S uc u e o L- yp ophan and L- yp ophanamide.
The pho olysis o yp ophan a 266 nm on a mic osecond ime scale led o kine ic cu es
con aining a posi i e and a nega i e peak (see ep esen a i e cu e in Figu e 5.26). The posi i e
peak could be assigned o he ansien abso p ion o he in e media e p oduc o he pho olysis
o T p, whe eas he nega i e peak p esumably co esponds o he lase induced luo escence o
T p. Nega i e peaks a e comple ely in e p e able in he con ex o lash pho olysis cu es, since
he measu ed alue is in ac he di e ence be ween he abso bance o he g ound s a e species
and he exci ed species. Figu e 5.26A shows ha he in ensi y o he nega i e peak exceeds ha
o he posi i e one. The a io o hese alues (in a o o he abso p ion peak) could be op imized
by he al e a ion o he wa eleng h o he analyzing beam (Figu e 5.26B).
The emission- o-abso p ion a io was ound o be op imal a 580 nm, u he kine ic
expe imen s we e ca ied ou a his wa eleng h. The 580 nm peak in he ansien spec um o
exci ed yp ophan was p e iously assigned o be he pho oioniza ion p oduc o T p, a adical
ca ion (T p+).164
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
51
Figu e 5.26. A) Rep esen a i e kine ic cu e o he 266 nm pho olysis o aqueous solu ion o
yp ophan. B) In ensi y o ligh abso p ion and emission in he 266 nm pho olysis o aqueous
solu ion o yp ophan, based on kine ic cu es as in panel A. The peak in ensi y co esponds
o he absolu e alue o he maxima o he posi i e and nega i e peaks, in abso bance uni s.
Condi ions o bo h panels: [T p] = 0.5 mM, unbu e ed, V = 3.00 cm3, T = 25 °C, l = 1.000 cm.
The plo s ep esen A) he a e age B) he a e age and s anda d de ia ion o 5 pa allel
measu emen s, whe e esh sample was applied o each lase sho .
Figu e 5.27 shows he linea dependence o he obse ed pseudo- i s o de a e cons an s
on he concen a ion o yp ophan. 580 nm was no sui able o ollow he eac ion a pH 7.21
due o poo signal o noise a io. 520 nm was ound o be op imal wi h ega ds o emission o
abso p ion a io. 520 nm is he epo ed abso p ion maximum o T pN adical.162,165-167
Figu e 5.27. Pseudo- i s o de a e cons an s in he eac ion o sul a e ion adical and
yp ophan. The da a poin s and e o ba s ep esen he a e age and s anda d de ia ion o 5
pa allel measu emen s, whe e esh sample was applied o each lase sho . The measu ed
second o de a e cons an s we e (7.4 ± 0.1) × 109 M1 s1 in unbu e ed solu ion and (8.7 ± 0.4)
109 M1 s1 close o physiological pH (7.21). [K2S2O8] = 0.100 M, unbu e ed (■), pH = 7.21
(20 mM phospha e bu e , ▼), V = 3.00 cm3, T = 25 °C, l = 1.000 cm.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
52
Figu e 5.28. Pseudo- i s o de a e cons an s in he eac ion o sul a e ion adical and L-
yp ophanamide. The da a poin s and e o ba s ep esen he a e age and s anda d de ia ion
o 5 pa allel measu emen s, whe e a esh sample was applied o each lase sho . The solid line
ep esen s he linea leas squa e i o he measu ed poin s. The slope o he line is (8.8 ± 0.2)
109 M1 s1 and he in e cep is (0.8 ± 0.2) 106 s1. [K2S2O8] = 0.100 M, pH = 7.21
(phospha e bu e ), V = 3.00 cm3, T = 25°C, l = 1.000 cm,

= 520 nm.
L-T yp ophanamide (T pA) was es ed in expe imen s simila o hose wi h T p, he aqueous
solu ion o T pA and K2S2O8 was pho olyzed a 266 nm and he abso bance was ollowed a
520 nm. The obse ed a e cons an depends linea ly on he concen a ion o T pA, wi h a
posi i e in e cep on he e ical axis (Figu e 5.28).
E ec o dissol ed oxygen concen a ion in he eac ion o sul a e ion adical and
yp ophan
We al e ed he concen a ion o oxygen in he sul a e ion adical– yp ophan adical sys em
in o de o e eal any po en ial in luence o dissol ed oxygen on he obse ed a e cons an s.
When a gon o ni ogen was igo ously bubbled in o he eagen solu ions o 15-20 minu es
be o e he exci a ion, i had no obse able e ec on he pho olysis o yp ophan solu ion. On
he o he hand, upon he applica ion o a lase sho on he de-ae a ed samples, a p e iously
unobse ed yellow p oduc appea ed in he solu ions. The cha ac e iza ion o he na u e o his
p oduc would equi e de ailed spec oscopic and kine ic s udies.
F om a kine ic poin o iew, he inc ease o dec ease o oxygen concen a ion in he
solu ions caused only sligh di e ences in he measu ed a e cons an s. The measu ed second
o de a e cons an s we e (9.4 ± 0.5) × 109 M1 s1 in ai sa u a ed solu ion and (9.0 ± 0.3) 109
M1 s1 in de-ae a ed samples. Da a poin s ob ained upon oxygena ion o he solu ions s ill show
linea dependence, al hough he unc ion has a posi i e in e cep on he e ical axis.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
53
Figu e 5.29. A) Rep esen a i e kine ic cu es in he eac ion o sul a e ion adical wi h L-
yp ophan wi h di e en oxygen concen a ions. Oxygen was emo ed by igo ously bubbling
a gon in he eagen solu ions o 20 min, whe eas oxygena ion was achie ed by in oducing
ex a oxygen in he samples om a gas bo le o 15-20 min. B) Pseudo- i s o de a e cons an s
in he eac ion o sul a e ion adical wi h L- yp ophan om kine ic cu es as shown in A). The
da a poin s and e o ba s ep esen he a e age and s anda d de ia ion o 5 pa allel
measu emen s, whe e esh sample was applied o each lase sho . The solid line ep esen s he
linea leas squa e i o he measu ed poin s. The slope o he blue line is (8.4 ± 0.8) 109 M1
s1 and he in e cep is (1.4 ± 0.4) 106 s1. [K2S2O8] = 0.100 M, pH = 7.21 (phospha e bu e ),
V = 3.00 cm3, T = 25 °C, l = 1.000 cm,

= 520 nm.
Figu e 5.29A shows h ee ep esen a i e kine ic cu es eco ded a 520 nm in ai sa u a ed,
de-ae a ed and oxygena ed solu ions, espec i ely. Figu e 5.29B shows he obse ed pseudo-
i s o de a e cons an s as a unc ion o he applied yp ophan concen a ion wi h di e en
oxygen sa u a ion in he samples. The measu ed second o de a e cons an s we e (9.4 ± 0.5) ×
109 M1 s1 in ai sa u a ed solu ion and (9.0 ± 0.3) 109 M1 s1 in de-ae a ed samples. Da a
poin s ob ained upon oxygena ion o he solu ions s ill show linea dependence, al hough he
unc ion has a posi i e in e cep on he e ical axis.

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
54
Al e na i e gene a ion o yp ophanyl adical
The li e a u e claims ha yp ophanyl adical can be gene a ed by he oxida ion o aqueous
yp ophan by b omine molecule anion (B 2).165,168 The expe imen al cons ain is ha we we e
no able o de ec B 2di ec ly upon he pho olysis o b omide solu ion, bu only by he
oxida ion o b omide wi h sul a e ion adical (see Figu e 5.23). I is s ill easible o oxidize T p
by b omine molecule anion in he p esence o K2S2O8. Howe e , one should ake he oxida ion
o T p by sul a e ion adical in o accoun as well acco ding o he abo e men ioned a es.
The e o e, in he SO4–T p–b omide sys em, we should conside eq. (47) as well. The
in oduc ion o T p inc eases he obse ed a e cons an o he eac ion in such a mix u e (Figu e
5.30). The eac ion was ollowed a 360 nm, he abso p ion maximum o b omine molecule
anion, on a mic osecond ime scale. The decay cu es did no i nicely o a single exponen ial
cu e. A second o de i was much be e cu es in ag eemen wi h he second o de decay o
B 2.
Figu e 5.30. Second o de decay o b omine molecule anion in he absence and p esence o L-
yp ophan. [K2S2O8] = 0.100 M, unbu e ed solu ion, V = 3.00 cm3, T = 25 °C, l = 1.000 cm.
The in oduc ion o 0.3 mM T p led o a 3- old inc ease in he obse ed a e cons an .
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
55
5.2.8. Reac ion o sul a e ion adical wi h y osine
Simila ly o he s udy ca ied ou wi h yp ophan, ano he a oma ic amino acid, y osine
(Ty ) was also eac ed wi h sul a e ion adical, in o de o measu e he second o de a e cons an
o eac ion (49).
Ty + SO4  Ty  + SO42 (49)
The eac ion was ollowed a 450 nm, because in he applied concen a ion ange, he
concen a ion o Ty adical ha is gene a ed is insu icien o p oduce decen abso p ion signal.
Unde pseudo- i s o de condi ions, he obse ed a e cons an s showed linea dependence on
he concen a ion o y osine, as indica ed in Figu e 5.31. The da a poin s measu ed in acidic
solu ions i e y well o linea unc ions going h ough he o igin. The ob ained second o de
a e cons an s we e (6.1 ± 0.1)  109 M1 s1 in acidic medium (black line – he pH is no cons an
in his case, concen a ion o added sul u ic acid is inc easing) and (5.1 ± 0.1)  109 M1 s1 a
pH 2.72. Close o neu al pH, he dependence emains linea , al hough he linea unc ion has a
small posi i e in e cep .
The second o de ecombina ion o he y osyl adical leads o he o ma ion o di y osine,
which is known o ha e an emission peak a 405 nm and o ms he basis o se e al luo escen
assays in he biochemical labo a o y p ac ice.169,170
Figu e 5.31. Obse ed a e cons an s in he eac ion o sul a e ion adical and y osine as a
unc ion o y osine concen a ions a di e en pH alues. [K2S2O8] = 0.100 M, ■: changing pH
([H2SO4] om 1.5 o 15 mM), ●: pH = 2.72 (measu ed); ▲: pH = 7.14 (0.1 M phospha e bu e ),
V = 3.00 cm3, T = 25 °C,

= 450 nm. Solid lines ep esen he linea i o he measu ed da a
poin s. The blue line has a slope o (1.4 ± 0.1)  109 M1 s1 and an in e cep o (0.4 ± 0.3) 
106 s1.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
56
5.2.9. Reac ion o sul a e ion adical wi h S(IV)
In he nex phase o ou s udies, we in ended o examine he eac ion o sul a e ion adical
wi h sul u oxy anions (SxOyz-), p e e ably wi h he ones con aining sul u in he oxida ion s a e
o +4. Du ing he au oxida ion cycles o S(IV) (see Figu e 5.8), SO3 and SO5 a e p oduced
as chain ca ie s along wi h he sul a e ion adical. We sough independen me hods o s udy
he eac ions o hese species. We pos ula ed he exis ence o eac ion ():
SO4 + SO32SO42 + SO3 
To check his possible p ocess, we eac ed sul a e ion adical wi h sul i e solu ions. The
echnique was simila o he one applied p e iously: sul a e ion adical was gene a ed by he
pho olysis o po assium pe sul a e.
Sul u (IV) has an abso p ion peak a 275 nm (see Figu e 5.1) in acidic medium. The e o e,
K2S2O8 has o be in high excess in o de o abso b he majo i y o ligh om he inciden (lase )
pulse. In ou sys ems, K2S2O8 is usually p esen in 0.1 M concen a ion in he samples, whe eas
he eac an species a e applied in he millimola concen a ion ange, K2S2O8 is in 10-100- old
excess. On he o he hand, he eac an species has o be in excess o e he gene a ed sul a e ion
adical, because pseudo- i s o de app oach is applied in he da a p ocessing. The pseudo- i s
o de condi ions a e a o able in ee adical eac ions because he ac ual concen a ions o he
ansien species a e no equi ed. The hi d equi emen is ha he eac an has o be applied in
an app op ia e amoun in o de o each decen signal- o-noise a io in he obse ed kine ic
cu es. Some imes o he ac o s a e o be conside ed as well, such as he solubili y o he
compound, possible ligh sensi i i y, he mal eac ion wi h K2S2O8, e c. Because o he abo e
men ioned ac o s, he op imal concen a ion ange should be he subjec o ca e ul
conside a ion.
Sodium py osul i e o me abisul i e (Na2S2O5) was used as a sou ce o sul i e ions, simila ly
o he au oxida ion s udies o S(IV) p esen ed in he Sec ion 5.1. The e ec o pH along wi h
dissol ed oxygen concen a ion was examined on he a e cons an o () and he eac ion was
ollowed a 450 nm. Signi ican di e ence was obse ed when he medium was changed om
neu al o s ongly acidic (Figu e 5.32).
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
57
Figu e 5.32. Pseudo- i s o de a e cons an s as a unc ion o S(IV) concen a ion in he
eac ion o sul a e ion adical and S(IV). [K2S2O8] = 0.100 M, pH = 6.98 (0.1 M phospha e
bu e , ■) o 1.16 (0.045 M H2SO4, ●), V = 3.00 cm3, T = 25 °C,

= 450 nm. The solid lines
ep esen he linea i o he measu ed da a poin s. The black line has a slope o (1.3 ± 0.01) 
109 M1s1 and i s in e cep wi h he e ical axis is a (0.8 ± 0.1) s1whe eas he slope
o he ed line, hus he espec ing second o de a e cons an is (0.4 ± 0.01)  109 M1s1.
The nega i e in e cep a neu al pH shown in Figu e 5.32 implies ha he dissol ed oxygen
p esen in he samples migh oxidize a po ion o he S(IV), hus he indica ed alues a e
o e es ima ions o he ac ual concen a ions ha pa icipa e in eac ion (). The e o e, he
e ec o dissol ed oxygen was es ed by bubbling a gon in he solu ions and epea ing he
expe imen s wi h de-ae a ed samples, in neu al and acidic medium as well (Figu e 5.33 and
Figu e 5.34). The nega i e in e cep becomes insigni ican when a gon is in oduced,
con i ming he con ibu ion o dissol ed oxygen o he oxida ion p ocess.
Figu e 5.34 would also sugges ha he concen a ion o dissol ed oxygen ac ually has an
in luence on he a e cons an unde acidic condi ions, i only he ed and he blue da a se ies
we e aken in o accoun (since he pH alues a e e y close). Howe e , conside ing he black
poin s as well, measu ed in ai sa u a ed solu ions such as he ed one, he mo e p obable
explana ion is ha he a e cons an is highly sensi i e o pH, and dissol ed oxygen has li le
e ec compa ed o he acidi y o he medium. The pH dependence can be obse ed in de-ae a ed
samples, oo (Figu e 5.35).
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
64
abso p ion coe icien s a e mo e di icul o de e mine, which leads o a high le el
o unce ain y in he

alues106 (see Sec ion 2.3).
S ill, we can make a ough es ima ion o [SO4]0, whe e = 0 ep esen s he ime poin o
he lase exci a ion (no e ha he exci a ion also pulse has a non-ze o leng h in ime, ~20 ns bu
o ou pu poses i can be handled as a poin ). A second o de i o he ecombina ion cu es
gi es an idea o he ini ial concen a ion, using

= 1600 M1 cm1 published by McEl oy118 and
l = 0.5 cm as an op ical pa h leng h. Fi ing o pu e second o de ecombina ion cu es o sul a e
ion adical ga e a alue o 2 104 M, which is compa able o he applied concen a ion o
iodide ion. This ac aised some ques ions: why a e he de ec ed cu es exponen ial and why
does he dependence on he concen a ion o iodide ion gi e a easonably good s aigh line?
Re u ning o he abo e men ioned conside a ions (i-i ), he concen a ion o SO4 is a local
alue, i applies o he loca ion o he de ec ion ha is limi ed o a ac ional olume in he
cu e e. The o al olume is 3.00 cm3, so i he a e age concen a ion o SO4 is calcula ed
o e he o al olume, a much lowe alue is ob ained. Addi ionally, while SO4 goes h ough
a apid decay, iodide ion can be pe manen ly eplenished by di usion om ou side o he
eac ion space, hus main aining he high excess o iodide o e sul a e ion adical. In he
ollowing pa ag aphs, an a emp will be made o analyze he e ec o di usion in he sul a e
ion adical–iodide ion sys em and o explo e he e ec o spa ial inhomogenei y on he obse ed
a e cons an s.
5.3.2. Reac ion-di usion equa ion using cylind ical coo dina es
A gene al eac ion-di usion (he eina e e e ed o as: RD) equa ion has a closed o m
shown in (51):
)(
cRcD
c


(51)
He e, c is he ec o o concen a ions, D is he ma ix o he di usion coe icien s,  is he
Laplace ope a o o Laplacian and R is a complex ope a o embedding all o he ongoing
eac ions in he sys em. Dc is called he di usion e m, R(c) o ms he eac ion e m.
Inspi ed by he seminal wo k o Alan Tu ing on mo phogenesis (shape o ma ion in
biological sys ems),182 eac ion-di usion sys ems s and in he main ocus o esea ch on
chemical and biological pa e n o ma ion183-185 as well as o he nonlinea dynamic phenomena
such as oscilla ion, chaos o sel -o ganizing sys ems.186,187

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
65
Eq. (51) is a second o de , semilinea , pa abolic pa ial di e en ial equa ion (PDE) sys em,
in which each chemical en i ies is ep esen ed by a ime-dependen a iable.149,188 The solu ion
o eq. (51) is a ec o o c( ) unc ions, whe e each concen a ion is explici ly exp essed as a
unc ion o ime.
The Laplacian () is a di e en ial ope a o wi h a scala alue ha gi es he di e gence o
he g adien o a eal alued unc ion. Fo an (x,y,z) unc ion in he h ee-dimensional Euclidean
space,
2
2
2
2
2
2
2
zyx









(52)
whe e  is he g adien o ,














 z
,
y
,
x
(53)
Eq. (52) desc ibes he Laplacian in Ca esian coo dina es, bu i is a o able o ou pu poses
o ans o m he p oblem in o a cylind ical coo dina e sys em, since he eac ion space is a
ci cula cylinde (see Sec ion 5.3.4). Figu e 5.38 shows he ans o ma ion om Ca esian o
cylind ical coo dina es, and eq. (54) is he o m o Laplacian in he new coo dina e sys em.
2
2
22
2
2
211












x
(54)
The angula ( ou h) e m in eq. (54) can be neglec ed in ou model because o he cylind ical
symme y. Thus, applying eq. (54) in eq. (51) yields:
)(
1
2
2
2
2cR
ccc
D
c



















x
(55)
Figu e 5.38. T ans o ma ion om Ca esian o cylind ical coo dina es. x = x, y = ∙ cos(

) and
z = ∙ sin(

).
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
66
In he p esen case, wo concen a ion unc ions a e o be calcula ed,
)(
4
SO x, , c 
and
)(
Ix, , c 
, he objec i e is o ga he an insigh o he spa ial dis ibu ion o he eac an s a each
pa icula ime poin .
5.3.3. App oxima ion o he pa ial de i a i es
In ini esimal quan i ies canno be handled compu a ionally, pa ial de i a i es in ol ed in
eq. (55) need o be app oxima ed. T adi ionally, de i a i es a e app oxima ed by ini e
di e ences, ha is, he slope o he angen a a ce ain poin on he g aph is close o he slope
o a secan lying on wo nea by g aph poin s (Figu e 5.39).189,190
Figu e 5.39. Geome ic in e p e a ion o he ini e di e ences app oxima ion.
Gi en wi h o mulae:
 
Δx
ΔxxuΔxxu
Δx
Δxxuxu
Δx
xuΔxxu
xu' iiiiii
i2
)()()()()()( 





(56)
The le side is he de i a i e o he u(x) unc ion a poin xi,

x is a small a bi a y dis ance on
he x axis and he e ms a e called o wa d, backwa d and cen al di e ences, espec i ely (i is
easy o see ha he cen al di e ence is he a e age o he o wa d and he backwa d ones). I
is e y common in nume ical p oblems (e.g. in eg a ion o unc ions o sea ching o oo s o
polynomials) ha an app op ia e g id (also called mesh) is de ined on he domain o he
unc ion, alues o he unc ion a e known a he g id poin s and u he alues a e calcula ed
using hese p e iously known alues. Equidis an g ids (whe e

x is cons an ) a e use ul and
p ac ical o many cases, bu he g id poin s ha e o be chosen cau iously a o he imes o
minimize he e o o he app oxima ion ( he di e ence be ween he eal and he calcula ed
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
67
alues). Using such a me hod, complica ed di e en ial and in eg al issues can be disc e ized
and ende ed compu a ionally sol able.
Highe o de de i a i es can be simila ly es ima ed by ini e di e ences, e.g. second o de
cen al di e ence is gi en in eq. (57):
 
2
)()(2)(
Δx
ΔxxuxuΔxxu
xu" iii
i


(57)
I is con enien o ew i e eqs. (56) and (57) in o a closed o m using ma ix mul iplica ion.
Assuming an equidis an one-dimensional g id wi h an in e al leng h o h, he cen al
di e ence in eq. (56) akes he ollowing o m:
   













1
1
101
2
1
xi
xi
xi
i
u
u
u
h
xu'
(58)
He e, uxi deno es he alue o u a g id poin xi, and xi+1 = xi + h, xi1 = xi  h.
The second o de di e ence can be simila ly ep esen ed wi h ma ix mul iplica ion, by
   













1
1
121
1
xi
xi
xi
i
u
u
u
h
xu"
(59)
Eqs. (58) and (59) a e easily applicable o mul i a ia e unc ions. Ou model equi es a wo
dimensional g id o esol e he x and ex en s o he eac ion space. Acco ding o eq. (55),
2
2c
x

,

c
and
2
2c


need o be app oxima ed. Applying eqs. (56) and (57) in eq. (55) gi es:
2
11
11
2
11
2
2
2
2
)()(2)(
)()(
1
)()(2)(
1
Δ
, xc, xc, xc
Δ
, xc, xc
Δx
, xc, xc, xc
c
c
x
c
jijiji
jijijijiji
i,j

























(60)
He e i and j a e he indices o he g id ep esen ing x and , axes and c can ei he be c(SO4)
o c(I). The sum o eqs. (61)-(63) yields eq. (60) i eqs. (58) and (59) a e used in a wo-
dimensional a angemen .
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
68
2
1
1
2
21
)(
)(
)(
2100
1
121
1
0012
x
, xc
, xc
, xc
x
c
ji
ji
ji
i
j,i 



























































(61)
, xc, xc, xc
c
i
jijiji
j,i
11
010
11
0
11
010
)()()(
111 
























































(62)
2
11
2
21
210
11
2
11
012
)()()(
, xc, xc, xc
ci
jijiji
j,i 

























































(63)
The limi a ion o his me hod (i.e. he p oduc ion o he di e ences by ma ix mul iplica ion
using coe icien ma ices) a ises om he = 0 case (eq. (62) con ains in he denomina o ),
which is one o he bounda y condi ions o sol ing eq. (55). Physically, = 0 is a he cen al
axis o he cylinde , no di usion occu s along his axis as a consequence o he cylind ical
symme y. This condi ion canno be handled in he ame o he o mula ion abo e, an
al e na i e ea men o he di usion e m is gi en in he ollowing sec ions.
5.3.4. Model o he eac ion space
Ou desc ip ion o he eac ion space is a modi ied e sion o a model p o ided by Cassidy
and Long (see Sec ion 2.4).141 These au ho s published a wo-dimensional model o measu ing
pseudo- i s o de a e cons an s in lase lash pho olysis expe imen s in collinea a angemen ,
whe e he lase beam and he analyzing beam a e pa allel o each o he . In ou calcula ions, we
assumed c ossed o pe pendicula a angemen in acco dance based on he expe imen al se up.
Figu e 5.40 shows he geome ic model applied o ep esen he physical eac ion space.
j

j

j

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
69
Figu e 5.40. Model geome y o modelling he ole o di usion in lase lash pho olysis
expe imen s. See explana ion o he labels in he ex below.
The a ow labelled ‘hν’ ep esen s he lase beam and he blue a ow is he analyzing beam
ha is used o ollow he concen a ion o he ansien species. Adap ing he common no a ions
o Bee ’s law, I0 is he in ensi y o he en e ing ligh beam and I is he in ensi y o he lea ing
beam. x and a e he labels o he spa ial axes, L is he pa h leng h o he cu e e in he di ec ion
o he lase beam. The c oss sec ion o he lase beam is conside ed o be ci cula wi h 0 adius,
and he o igin is ixed o he cen e o his ci cle a he en e ing poin o he lase . The shading
e e s o he dec easing concen a ion o he ansien species along he lase beam.
Sul a e ion adical is gene a ed by he lase pulse along he x axis, adially om he o igin
wi hin 0, hus o ming a cylinde -shaped olume. An ex e nal adius is de ined ( ex, Figu e
5.41) a ound his objec , di usion o bo h sul a e ion adical and iodide ions is allowed om
his ou e shell o he in e nal cylinde and ice e sa.
Figu e 5.41. C oss sec ion o he eac ion space, app oxima ed by he uni y o an inne ( 0) and
ou e ( ex) cylinde .

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
70
5.3.5. Disc e e andom walk model o di usion
Acco ding o Sec ion 5.3.4., he eac ion o sul a e ion adical and iodide ion akes place in
a cylind ical space, su ounded by an ex e nal ube which is accessible o he di usi e mo ion
o he pa icles. In o de o calcula e he spa ial dis ibu ion o each eac an , he eac ion space
(including he ou e shell) is di ided in o small olume uni s ha a e shaped like cylinde ings
(Figu e 5.42.).
Figu e 5.42. Shape o he olume uni s.
This kind o esolu ion in o elemen a y olumes o cells eplaces he in e p e a ion in 5.3.3,
whe e a wo dimensional g id was in oduced on he x and axes. This model is concep ually
di e en , in a sense ha ins ead o app oxima ing each pa ial de i a i es in eq. (55)
indi idually, di usion in each olume uni is ea ed as a ma e exchange wi h he neighbo ing
cells.
The numbe o pa icles in a ce ain cell in a gi en ime in e al changes ia wo ways:
species can a i e om he nea by cells and o he s can lea e he uni o en e hose adjacen
cells. The e o e, he change o concen a ion in he cell will be he esul an o he ou low and
he in low ia di usion. I is impo an o no e ha only he di usion e m is conside ed a his
poin , he eac ion e m is in oduced a a la e s age.
An a bi a y olume uni is in jux aposi ion wi h ou o he ones, wo in axial, wo in adial
di ec ions. In he x di ec ion, hey o m a shape like a longe ube, whe eas in he adial
dimension, he smalle ones a e embedded in o he bigge ones.
The nea by olume uni s ha e common ‘walls’, h ough which di usion akes place. In
acco dance wi h Fick’s 1s law, he low a e o he componen s be ween wo chosen uni s is
p opo ional o he common su ace and he concen a ion g adien .56 Reac an s a e only
allowed o mo e un il hey each he bo de s o he eac ion space (0   ex and 0  x  L),
he e is no lux o ma e on he bounda ies.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
71
Le ’s ake a cylinde ing wi h an inne adius o , an ou e adius o + d and a heigh o
dx. Fo he sake o simplici y, we can assume ha d = dx = 1.
The su ace o such an objec consis s o ou pa s (see Table 7), wo ci cle ings o annulus
o equal a ea, an ou e side and an inne side, bo h o which ha e he shape o a cu ed
ec angula .
Table 7. Su ace a ea o he pa s o a cylinde ing wi h a g id size o d = dx =1
ou e adius =
Su ace a ea
F ac ion o he o al a ea
Uppe annulus
   
π π π 121 2
2
4
1
48
12 


Lowe annulus
   
π π π 121 2
2
4
1
48
12 


Ou e su ace
π2
48
2

Inne su ace
π )12( 
48
22


To al
π )48( 
1
Clea ly, he inne su ace o his uni is he ou e su ace o he one inside i and e e sely,
i s ou e su ace is equal o he inne su ace o he nex one wi h inc eased adius.
The olume o he desc ibed objec is:
V = 2

 ( 1)2

= (2 1)

(64)
The olumes o i s neighbo ing cells a e (2 1)

(uppe and lowe ; x±1, ), (2 +1)

(ou side;
x, +1) and (2 3)

(inside; x, 1).
As s a ed be o e, he di usion e m can be decomposed in o ou low and in low om and
in o each pa icula ly olume uni . The ou low e m is qui e s aigh o wa d o demons a e. I
is assumed ha all pa icles lea e he cell, a each su ace pa acco ding o i s a io o he o al
su ace (Table 7, column 3). In a gene al olume uni , whe e he ac ual concen a ion is c(x, ),
he scheme o he di usion is shown in Figu e 5.43.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
72
Figu e 5.43. Exchange o ma e in a olume uni o gene al posi ion. The uni shown has an
inne adius o  1 and an ou e adius o , ha ing an index o n in he adial di ec ion ( = 0
is he i s one, whe e n = 1). The a ios gi en in he igu e ha e o be mul iplied by he di usion
coe icien . Blue a ows ep esen he ou low om he cell, igh a ows co espond o he
in low om he neighbo ing uni s.
Figu e 5.43 e e s o a cell in gene al posi ion, i.e. i is loca ed inside he eac ion space, i
does no each any o he bounda ies (  0;  ex; x  0; x  L). When he cell has one o wo
bo de su aces, hen i is assumed ha he ac ion o he pa icles co esponding o ha su ace
a ea do no lea e he cell.
The in low pa is u he di ided in o he in low om he x and neighbo s. In he x
di ec ion, cells ha e he same olume (since is cons an ). The e o e, he numbe o esiding
pa icles has he same a io as hei concen a ions. Eq. (65) gi es he x in low in o he c(x, )
uni .



















,x
,x
,x
c
c
c
, xc, xc
1
1
4
1
0
4
1
)1(
4
1
)1(
4
1
(65)
In he case o he adial in low, no only he common su ace, bu he a io o he olumes is
conside ed in he ollowing mul iplica ion:
adial in low =
n
n
n, o
n,ou
n
n
n, o
n,in
V
V
A
A
x, c
V
V
A
A
x, c 1
1
1
1
1
1)1()1( 





(66)
Subs i u ing he known olumes and su aces in o eq. (66) gi es:
12
32
128
22
)1(
12
12
48
2
)1( 







n
n
n
n
x, c
n
n
n
n
x, c
(67)
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
73
Upon simpli ica ion, he ollowing equa ion is ob ained:
 
















)(
0
)(
48
22
)1(
48
2
)1( 11
u
ccc
n
n
x, c
n
n
x, c ,x ,x ,x
(68)
He e ( ) and u( ) a e he coe icien s desc ibing he in low om he inne and he ou e cells,
espec i ely.
Sepa a e ma ices we e de ined o coe icien s con aining he x in low (DX), he in low
(DR) and he ou low as well (DE). Using hese ma ices, he igh hand side o eq. (55), s ill
wi hou he eac ion e m, can be econs i u ed as eq. (69)
D∙(DXc + cDR + DE.c) (69)
He e, ∙ is he egula mul iplica ion sign,  is he ma ix mul iplica ion and . is he elemen -
wise mul iplica ion o ma ices. Ma ix mul iplica ion is sensi i e o he o de o he ac o s,
and he ma ix dimensions ha e o ma ch o a alid ope a ion.
5.3.6. Nume ical in eg a ion
Acco ding o he New on-Leibniz o mula, one o he undamen al heo ems o calculus,
he de ini e in eg al o an u(x) uni a ia e unc ion be ween xi and xi+1 poin is gi en as

 1
1)()()( i
i
ii
x
xdssu'xuxu
(70)
Eq. (70) is in he backg ound in he nume ical solu ions o kine ic di e en ial equa ions,
whe e he independen a iable is ime and he dependen a iables a e concen a ions. Ou
p e ious e o s we e a ge ed o gi e a easonable app oxima ion o he igh hand side o (55),
i.e. he de i a i e o concen a ions wi h espec o ime. The nex s ep is o de ine how o ob ain
he c( + h) concen a ions in he possession o he c( ) alues.
De ini e in eg a ion is ano he ope a ion ha compu e s canno handle di ec ly (al hough
symbolic so wa es such as Ma hema ica con ain nume ous p imi i e unc ions). A ple ho a o
algo i hms exis o nume ical in eg a ion, he app oxima ion o de ini e in eg als be ween wo
ime poin s (o wha e e is he independen a iable).191
The mos widely used algo i hm in chemical kine ics is he ou h-o de Runge-Ku a
me hod (RK4),91 because i is ela i ely easy o code and i has high accu acy, gi en ha ime
s ep leng h (h) is chosen co ec ly. Adap i e ime s epping is p ac ical in mos cases, whe e he
s ep size g adually changes as he i e a ion p oceeds.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
80
o he apid na u e o he eac ion o sil e (I) and sul a e ion adical became a ailable by he
applica ion o he lase lash pho olysis echnique. A newly acqui ed Applied Pho ophysics
lase lash pho olysis (LFP) ins umen o nanosecond ime esolu ion allowed us o s udy he
eac ions o he sul a e ion adical in a di ec manne . SO4 was gene a ed by he pho olysis o
K2S2O8 by a 266 nm pulse and ollowed by i s abso p ion a 450 nm. The second o de a e
cons an o i s eac ion wi h sil e (I) ion was de e mined unde pseudo- i s o de condi ions,
he measu ed alue is (7.7 ± 0.5)  109 M1 s1 in s ongly acidic medium. This alue app oaches
he di usion con olled limi , a i ming he ole o eac ion (19) in chain p opaga ion.
Simila ly o he case o sil e (I), he second o de eac ions o sul a e ion adical wi h
p e iously ecognized ca alys s o he au oxida ion o S(IV) we e s udied. Ra e cons an s o
Ce(III) and iodide ions we e de e mined, as well as u he a e cons an s wi h halide ions, a
ew biomolecules and S(IV).
In he sul a e ion adicaliodide ion sys em, in e es ing kine ic beha io was obse ed. The
eco ded kine ic cu es i ed o double exponen ial kine ics, and bo h i ed pa ame e s showed
linea dependence on he concen a ion o iodide ion. One o he wo dependence unc ions
wen h ough he o igin. The e o e, he espec i e a e cons an was assigned o eac ion (42).
The o he line had a signi ican in e cep wi h he e ical axis, i was hus concluded o belong
o he e e sible eac ion o iodide ion and iodine a om, p oducing iodide molecule anion (I2).
This was sugges ed as a no el me hod o gene a ion iodine a oms and he equilib ium cons an
o (43) was de e mined.
Pseudo- i s o de beha io was obse ed in he sul a e ion adicaliodide ion sys em, e en
hough he p e equisi e o pseudo- i s o de kine ics, he high excess o iodide ions, was no
eached locally a he si e o obse a ion. The po en ial eplenishmen o iodide ions by
di usion om ou side he eac ion space was examined by a nume ical model. The eac ion
space was di ided in o uni olumes and an ou e adius was de ined inside which di usion o
pa icles was allowed. The andom walk model o di usion was applied o simpli y he solu ion
o he ope a i e pa ial di e en ial equa ion (PDE) sys em. Using a chemically concei able
pa ame e se , i was shown ha o a a e cons an in he 109 M1 s1 o de o magni ude,
di usion does no in luence he de e mina ion o he a e cons an wi hin he ime ame o he
eac ion.

É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
81
7. Össze oglalás
Ez az é ekezés köz e len oly a ása és kiegészí ése a ku a ócsopo unkban ko ábban
lezajlo izsgála oknak a kén(IV) au ooxidációjának kine ikájá al és mechanizmusá al
kapcsola osan. Ezek a ko ábbi munkák el á ák a Ce(III) és I ionok ka ali ikus sze epé
alamin a Fe(II) ionok lehe séges ész é elé a o oiniciál au ooxidációs mechanizmusban. A
kísé le ek so án diódaso os spek o o omé e alkalmaz ak a eakciók indí ásá a és kö e ésé e
egya án .54,75-77
Az au ooxidációs olyama ok mechanizmusa gyökös lánc eakció, amelyben szul i -,
szul á - és pe oxomonoszul á -iongyökök ( end e SO3, SO4 és SO5 a közös lánc i ők. Az
e edmények az mu a ják, hogy a szul á iongyök (SO4) kiemel sze epe öl be a ka alízisben,
ké éle okból. A szul á iongyök eakciója a ka alizá o al on os lánc i ő lépés alamin a
pe oxodiszul á ionoka e melő másod endű ekombinációja öbbnyi e az egye len jelen ős
lánclezá ó lépés.
Az au ooxidáció mechanizmusának mélyebb megé ése é dekében célul űz ük ki a
mechanizmus elépí ő ész endsze ek ügge len izsgála á . Egy ilyen ész endsze a S(IV)
eakciója a lánczá ó lépésben képződő pe oxodiszul á -ionnal, amely élhe ően szinp opo ciós
olyama ban szul á iongyökö e mel. Ko ábbi e edmények alapján az emlí e eakció sa as
közegben, ka alizá o á ollé ében endkí ül lassú. Az S2O82 ionok edoxi eakciói kine ikai
gá lás mia öbbnyi e igen lassúak a nagy edoxipo enciál ellené e is. Az ezüs ionok a
pe oxodiszul á ion oxidációs eakcióinak jól isme ka alizá o ai, mi el az iniciáló lépés
e mékei a szul á ion melle igen eak í észecskék, Ag(II) és szul á iongyök.43-45
Vizsgála aink so án ezé ezüs -ni á o ad unk a S(IV)–oxigén–pe oxodiszul á
eakcióelegyekhez, e ősen sa as közegben. Előkísé le ek alapján a S(IV) au ooxidációja ily
módon ha ékonyan iniciálha ó. A o okémiai mellék eakció kizá ása é dekében a diódaso os
spek o o omé e alkalmazásá kísé le eink so án kizá uk, no mál spek o o omé e
segí ségé el kö e ük a eakció .
Ez a dolgoza észle esen isme e i a S(IV) ezüs ionok ál al ka alizál au ooxidációjának
kine ikai izsgála á , pe oxodiszul á -ion, min ko-ka alizá o jelenlé ében. A kísé le ekből
le on mechanisz ikus kö e kez e ések ugyancsak a dolgoza á gyá képezik. Kilenc lépésből
álló mechanizmus ja asol unk (Scheme 1), alamin egy némileg össze e , ugyanakko
kine ikailag megalapozo sebességi egyenle e eze ünk le (38) a kine ikai ada ok
é elmezésé e.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
82
A szul á iongyök és az ezüs ionok közö i másod endű eakció (Scheme 1; R2) az
ezüs ionok ál al ka alizál au ooxidáció ál alunk ja asol mechanizmusának egyik lánc i ő
lépése. A sebességi egyenle le eze ése so án a hosszú lánco el é elező megközelí és
alkalmaz uk, amely el é elezi, hogy a lánc i ő lépések sebessége nagyobb, min a láncindí ó
és a lánclezá ó lépéseké (mi el másképp a lánc eakció nem udna lezajlani), ille e az is, hogy
a lánc i ő lépések sebessége megegyezik. Annak igazolásá , hogy a szul á iongyök (SO4) és
az Ag+ ionok közö igen gyo s eakció já szódik le, léze es illanó ény- o olízis módsze
alkalmazása e e lehe ő é. A anszékünkön nem égiben meg ásá ol Applied Pho ophysics
nanoszekundum idő elbon ású illanó ény- o olízis készülék segí ségé el köz e lenül ud uk
anulmányozni a szul á iongyök eakcióinak kine ikájá . Az SO4 gyököke K2S2O8 olda
o olízisé el állí o uk elő 266 nm hullámhosszúságú léze impulzus segí ségé el. A eakcióka
450 nm-en, a szul á iongyök elnyelési maximumán kö e ük. Az ezüs ionnal aló eakció
pszeudo-első endű kö ülmények közö izsgál uk, és a másod endű sebességi állandó mé
é éke (7.7 ± 0.5)  109 M1s1 ol , e ősen sa as kö ülmények közö . Ez az é ék megközelí i
a di úzió kon ollál eakciók sebességi állandójának maximális é éké , mege ősí e a (19)
eakció lánc i ő lépéskén aló ész é elé a mechanizmusban.
Az ezüs ionokhoz hasonlóan anulmányoz uk a szul á iongyök másod endű eakciói az
au ooxidáció ko ábban megisme ka alizá o ai al is. Megha á oz uk a másod endű sebességi
állandók é ékei Ce(III) ionokkal és I ionokkal, alamin egyéb halogenidionokkal, néhány
biomolekulá al és S(IV) a almú észecskékkel.
A szul á iongyök–jodidion endsze ben é dekes kine ikai iselkedés igyelhe ünk meg. A
eakció 340 nm-en, a jód molekulaion (I2) elnyelési maximumán kö e ük és a el e kine ikai
gö béke ké exponenciális gö be összegé el illesz e ük. Mindké illesz e sebességi állandó
ípusú pa amé e lineá is üggés mu a o a jodidionok koncen ációjá ól. Az egyik lineá is
ügg ény á men az o igón, így ez az állandó hozzá endel ük a (42) eakcióhoz. A másik
ügg énynek jelen ős üggőleges engelyme sze e ol , így ebből a ügg ényből megha á oz uk
a (43) eakció oda- és isszai ányú sebességi állandójá , alamin a olyama o jellemző
egyensúlyi állandó . Ezzel új módsze alál unk a jóda omok előállí ásá a.
A szul á iongyök–jodidion endsze ben pszeudo-első endű iselkedés apasz al unk, noha
ennek el é ele, a jodidionok nagy eleslege lokálisan nem eljesül a eakcióelegyben, mi el a
szul á iongyök egy kis é oga észben képződik a léze sugá haladási i ánya ál al
megha á ozo módon. Ma ema ikai modell eze ünk be annak izsgála á a, hogy an-e mód
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
83
a jodidionok di úzió ál ali pó lásá a a eakció é en kí üli é észből és ezál al a pszeudo-
első endű kine ikához szükséges koncen ációa ány isszaállí ásá a.
A henge alakú eakció e e kis é oga elemek e bon o uk és megha á oz unk egy külső
suga a , amelyen belül ől megengede a észecskék di úziója a eakció é be és onnan ki elé.
A di úzió éle len bolyongás modelljé alkalmaz uk a endsze leí ó pa ciális di e enciál
egyenle endsze megoldásának egysze űsí ésé e. Egy kémiailag eális pa amé e készle
használa á al az alál uk, hogy 109 M1 s1 nagyság endű másod endű sebességi állandó ese én
a di úzió nem be olyásolja a pszeudo-első endű sebességi állandó megha á ozásá , a eakció
időskáláján nincs megha á ozó sze epe.
É a Dóka: PhD Thesis – Reac ions o he sul a e ion adical
84
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