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The three-dimensional structure of humic substances and soil ...

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Table 2 (continued)<br />

o<br />

CH2-CH2-C~H<br />

0H<br />

CH2-CH:-CHO<br />

H3C0 OCH 3<br />

OCH3 OH<br />

(210)<br />

CH=CH2 (180) 22--(CH2) s-CH3<br />

H3CO~0CH 3 ~ (218)<br />

OKcI{2__CH3(180) ~ ~CH2) 7-cn3<br />

/ ~ 0H (220)<br />

H3CO OCH 3<br />

OH ~H2--( CH2 ) 9-CH3<br />

1182)<br />

©<br />

(232)<br />

CH2--( CH 2 ) io-CH3<br />

OH OK (186) ~--~H3<br />

--( CH 2 ) ~-CH3<br />

(246 )<br />

(1901 ~ -(CH2) II--CH3<br />

H O ~ 12601<br />

1194) ~C6H14<br />

CH2-CHO<br />

TC6HI4<br />

H3C0 0CH 3 (264)<br />

OH<br />

(196) ~--(CH2) 12-CH3<br />

.~--( CH2 ) 7 -CH3<br />

(204)<br />

(274)<br />

¢<br />

CH2--(CH2) 13-CH3<br />

12881<br />

-4CH 2114-CH3<br />

(302)<br />

-qCH 2 ) 15-CH3<br />

1316)<br />

-~CH 2 ) 16-CH3<br />

(330)<br />

romolecules be simulated at atomic <strong>and</strong> molecular<br />

level?<br />

Experimental<br />

Pyrolysis-fieM ionization mass spectrometry (Py-FIMS)<br />

For temperature-resolved Py-FIMS, about 100~tg <strong>of</strong><br />

<strong>humic</strong> <strong>substances</strong> such as <strong>humic</strong> acid (HA), fulvic acid<br />

(FA), humin or 5 mg <strong>of</strong> whole <strong>soil</strong> samples, respectively,<br />

were thermally degraded in the ion source <strong>of</strong> a MAT 731<br />

(Finnigan, 28127 Bremen, Germany) modified high-per-<br />

formance (AMD Intectra GmbH, 27243 Harpstedt, Ger-<br />

many) mass spectrometer. <strong>The</strong> samples were weighed be-<br />

Table 3. Aliphatic compounds characteristic for <strong>soil</strong> organic matter<br />

(see Table i) [11<br />

CH2=CHCHO<br />

CH3-C0--CH 3<br />

CH3-C00H<br />

CHa--CO--CHO<br />

CH2-C--CO--CH 3<br />

CN3-CH--CH--CH--CH--CH 3<br />

3 H C ~ CH3<br />

65<br />

(56)<br />

(58)<br />

(601<br />

(72)<br />

(84)<br />

(96)<br />

0<br />

(i12)<br />

Qo 1114)<br />

3HC-~ OH<br />

11281<br />

0 0 0<br />

II II II<br />

CH3-C--CH2-C--CH2-C--CH 3<br />

11421<br />

~H3 ?H3 ~H3<br />

CH3-CH--(CH2) 3--CH--(CH2) 3-CH--CH2=CH--CH2 (224)<br />

CH CH 3 CH 3<br />

3 i i<br />

CH3--CH--~CH2)3--CH---~CH 2 3~CH~--~CH2 2-C~3<br />

CH3--~ CH 2 )IT"CH20H<br />

CH 3 CH 3 CH 3 CH 3<br />

I I I<br />

CH3-CK--~CH 2 3-CN--CH 2 3-CH--CN 2 3-C=CH2<br />

n=2-30 series<br />

CH3-~ CH 2 )~--CH3<br />

n=i-28 series<br />

CH2=CH--( CH 2 )~--CH 3<br />

CH3--( CH 2 )~4 COOH<br />

(226)<br />

12281<br />

(266)<br />

(58-450)<br />

(56-4341<br />

(256)<br />

14101<br />

fore <strong>and</strong> after Py-FIMS (error + 0.01 mg) to determine the<br />

pyrolysis residue <strong>and</strong> the produced volatile matter. <strong>The</strong><br />

heatable/coolable direct introduction system with elec-<br />

tronic temperature-programming, adjusted at the + 8 kV<br />

potential <strong>of</strong> the ion source <strong>and</strong> the field ionization emit-<br />

ter, was used. <strong>The</strong> slotted cathode plate serving as count-<br />

er electrode was on - 6 kV potential. Thus, at 2 mm dis-<br />

tance between the emitter tips <strong>and</strong> the cathode, in total a<br />

potential difference <strong>of</strong> 14 kV is applied resulting in an ex-<br />

tremely high electric field strength which is the essential<br />

basis for s<strong>of</strong>t ionization. All samples were heated in high<br />

vacuum (1.3 × 10 -4 Pa) from 323 K to 973 K at a heating<br />

rate <strong>of</strong> approximately 0.5Ks -1. About 60magnetic

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