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Detection of halogen radicals by millimetre – wave spectroscopy

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<strong>Detection</strong> <strong>of</strong> <strong>of</strong> <strong>halogen</strong> <strong>radicals</strong> <strong>by</strong> <strong>by</strong><br />

<strong>millimetre</strong> <strong>–</strong><strong>–</strong> <strong>wave</strong> <strong>wave</strong> <strong>spectroscopy</strong><br />

Presented Presented <strong>by</strong>: <strong>by</strong>: Eva Grigorová Grigorov<br />

Supervisor: Supervisor: Stephane Bailleux<br />

Georges Wlodarczak<br />

Zdeněk Zelinger


VŠB- Technical University <strong>of</strong><br />

Ostrava, faculty <strong>of</strong> Safety<br />

engineering<br />

eng neering<br />

Branch <strong>of</strong> Study <strong>of</strong> Fire<br />

Protection and Industrial<br />

Safety<br />

Cooperate with J.Heyrovský<br />

J.Heyrovsk<br />

Institute <strong>of</strong> Physical<br />

Chemistry, Academy <strong>of</strong><br />

Sciences <strong>of</strong> Czech Republic<br />

Where Where I I am am from? from?


From October 2006 in Lille 1<br />

University in France<br />

Laboratoire de Physique des<br />

Lasers, Atomes et Molécules Mol cules<br />

(PHLAM)<br />

Study <strong>halogen</strong> <strong>radicals</strong> <strong>radicals</strong><br />

(CH2I) (CH I) <strong>by</strong> mmw<br />

<strong>spectroscopy</strong> and analysis ana ysis <strong>of</strong><br />

ν4 band <strong>of</strong> FCO2 FCO measured<br />

<strong>by</strong> FTIR<br />

Present


Study theoretical<br />

background <strong>of</strong><br />

<strong>spectroscopy</strong><br />

1. 1. Part Part <strong>of</strong> <strong>of</strong> my my work work<br />

How to operate the<br />

spectrometer


2. 2. Part Part <strong>of</strong> <strong>of</strong> my my work work<br />

High igh resolution <strong>spectroscopy</strong> <strong>of</strong> <strong>halogen</strong><br />

Difficult to prepare<br />

short life time - (few ms)<br />

have to choose suitable<br />

<strong>radicals</strong> radical<br />

precursor<br />

preparative process, reaction<br />

physical conditions (pressures,<br />

temperature)<br />

Difficult to detect them<br />

few weak transitions <strong>of</strong> reactive species<br />

many strong lines <strong>of</strong> stable species


Halogen <strong>radicals</strong>s radical CH22XX CH<br />

[ [ X X = = Cl, Cl, F, F, Br, Br, I I ] ]<br />

1) 1) Atmospheric interest<br />

• Reaction: Reaction:<br />

CH 3X X + OH or Cl → CH 2X • Subsequent reactions involving CH 2X X<br />

produce <strong>halogen</strong> atoms atom<br />

• Destr estroying oying stratospheric ozone


2) 2) Spectroscopic interest<br />

• CH 2F F and CH 2Cl Cl: : micro <strong>wave</strong> spectra<br />

published more than 2 decades<br />

ago(Y.Endo et al,1983,1984)<br />

• CH2Br CH Br rotational otational spectrum analyzed<br />

(Bailleux Bailleux et t al, al 2OO5)<br />

• CH2I CH no high resolution spectroscopic<br />

data availa available<br />

ble<br />

• All these <strong>radicals</strong> have planar structure


CH CH22Br<br />

Br radical radical<br />

Come Come<br />

from CH3Br CH Br<br />

natural and anthropogenic source<br />

• In the Atmosphere:<br />

CH 3Br Br + OH → CH 2Br Br + H O 2<br />

• In Laboratory:<br />

CH 3Br Br + Cl → CH 2Br Br + HCl


What What about about CH CH22I<br />

I ??? ???<br />

Difficultiies<br />

Difficult es with with producing and and<br />

detecting<br />

No experimental data <strong>of</strong> rotational rotational<br />

constants constant<br />

How ow to produce ?<br />

CH3Br CH Br + Cl → CH2Br CH Br ...exotherm<br />

... exothermic ic reaction<br />

CH3I CH I + Cl → CH2I CH I ...exo ... exo, , endo... endo...<br />

Not clear<br />

according to papers<br />

Fine and hyperfine splitting: splitting:<br />

II I (5/2)>IBr (5/2)>IBr(3/2)<br />

(3/2)<br />

Lines ines <strong>of</strong> CH 2I I are expected weaker than lines<br />

<strong>of</strong> CH2Br CH Br:<br />

= 0,8 < µ (CH2Br ) = 1<br />

: µ( ( CH2I ) =<br />

< µ(CH2Br )


CH22I CH I radical radical<br />

CH 3I most most<br />

abundant abun ant iodo compound in the<br />

atmosphere<br />

Natural atural source : pelagic ocean,<br />

ocean surface waters, volcanic production<br />

Previous studies studies<br />

Only nly low resolution studies studies<br />

Photoelectron spectra pectra<br />

(L.Adrews L.Adrews et t al,1984 al,1984)<br />

Matrix infrared spectrum<br />

(D.W.Smith D.W.Smith and L.Adrews,1973<br />

L.Adrews,1973)


How How to to detect detect CH22I? CH I?<br />

Based on high level ab initio calculations<br />

calculation<br />

A = 279413,0 MHz B = 8806,1 MHz C = 8537,1 MHz<br />

→ calculated spectrum → graph


Use Use glow glow elecctric ele tric ddiischarge scharge<br />

...easer to use it at first<br />

C-I I chemical bond weaker than C-Br C Br bond<br />

Test on CH2Br CH Br radical - We produced CH2Br CH Br!


CH2I CH I in glow el. discharge ?<br />

• many vibrationally<br />

vibrationally<br />

excited states <strong>of</strong> CH3I CH<br />

Intensity<br />

8<br />

3<br />

-2<br />

-7<br />

-12<br />

Congested spectrum <strong>of</strong> CH3I<br />

450000 450050 450100 450150 450200<br />

Frequency<br />

CH3I


Change to to hydrogen<br />

abstraction with with fluorine<br />

• Atomic tomic fluorine produced in micro<strong>wave</strong> discharge:<br />

Primary reaction:<br />

CH3I CH I + F → CH2I+ CH I+ HF ???<br />

• Test at first on CH2Br CH Br radical<br />

CH2Br CH Br only observed using F 2 !!!


• Secondary reaction:<br />

F + CH 2I I → [CH CH2FI FI] * → CH 2F F + I ???<br />

• Test to detect CH 2F F → Detected !!!<br />

CH 3I I + F → CH 3F F + I → CH 2F F + HI<br />

• Test to detect CH 3F F → Detected!!!


• Searching for lines is still in progress... progress...<br />

• At least observed spectra are not congested...<br />

Intensity<br />

8<br />

3<br />

-2<br />

-7<br />

-12<br />

450080 450085 450090 450095 450100<br />

Frequency<br />

Congested spectrum <strong>of</strong> CH3I<br />

Nocongested spectrum <strong>of</strong><br />

CH3I


Wish Wish<br />

We have seen few paramagnetic lines<br />

(probably probably from CH 2I???) I???) and therefore is<br />

important to continuous in measurement...<br />

measurement...


3. 3. Analysis <strong>of</strong> <strong>of</strong> νν band band <strong>of</strong> <strong>of</strong> FCO<br />

44 FCO2 2<br />

obtained <strong>by</strong> <strong>by</strong> FTIR FTIR<br />

A, B, C rotational constant, centriftugal distortion constants, co stants, fine constants ???


FCO 2<br />

Probably produced during the stratospheric<br />

degradation <strong>of</strong> HFCs<br />

Most stable member amongst carboxy<br />

<strong>radicals</strong> <strong>of</strong> the type XCO 2<br />

[X = H, F,Cl, Br, I, CF 3 , OCF 3 ]<br />

Rotational spectrum in its ground vibrational<br />

state in the range 240-380 GHz (Z. Zelinger<br />

et al,2003) and 210-245 GHz (Z.Zelinger et<br />

al, 2007)


Conclusion<br />

Spectroscopy <strong>of</strong> radical has essential importance importance<br />

for obtaining the information about chemistry in<br />

the atmosphere<br />

We will continuous in measurement...<br />

Long Long time time prospect<br />

After stay in France, France work with Zdeněk Zden k Zelinger<br />

group in J.Heyrovský J.Heyrovsk Institute <strong>of</strong> Physical<br />

Chemistry Academy <strong>of</strong> Sciences <strong>of</strong> Czech Republic<br />

Finish inish my postgraduate study in<br />

VŠB- Technical University <strong>of</strong> Ostrava


Thanks Thanks to to my my supervisors for for<br />

expert expert advice advice and and patience<br />

leading<br />

leading


Thank Thank you you for for your your<br />

attention

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