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Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

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4.3 The discharge flow (DF) technique 78<br />

4.3 The discharge flow (DF) technique<br />

DF technique is used for gas phase reactions on ms timescale:<br />

• laminar flow along tubular reactor:<br />

∆ = ∆<br />

<br />

with =meanflow speed, ∆ = distance along the flow tube.<br />

(4.1)<br />

• y first-order reaction gives exponential decay of concentration along ∆.<br />

• in reality ⇒ Hagen-Poisseuille flow (parabolic flow profile),<br />

• but fast radial diffusion of reactants (at pressures of 1 to 10 mbar) gives “plug<br />

shaped” radial concentration profiles despite parabolic flow profile.<br />

• more complicated, when “back diffusion” and radial diffusionhavetobetaken<br />

into account (at higher pressures).<br />

• problem: heterogeneous reactions lead to first-order decay of reactive radicals<br />

even in the absence of a reactant.<br />

Combinations with numerous highly sensitive detection techniques, for instance:<br />

• mass spectrometry (MS): universal, but often low sensitivity; problems with fragmentationofmoleculesintheionsource,<br />

• laser induced fluorescence (LIF): excitation to electronically excited state followed<br />

by relaxation by spontaneous emission. very sensitive (e.g., for OH ( 2 Σ ← 2 Π)<br />

detection limit below 10 6 molecules cm 3 ),<br />

• electron spin resonance (ESR): for paramagnetic atoms by exploiting the Zeeman<br />

effect depending on magnetic field <br />

= 0 + (4.2)<br />

∆ =1y ∆ = (4.3)<br />

ESR transitions are in the microwave region (X band: 9GHz).<br />

• laser magnetic resonance (LMR): very sensitive; based on observation of rotational<br />

transitions between Zeeman-shifted rotational levels of paramagnetic radicals<br />

( rot = rotational constant).<br />

00 = rot ( +1)+ 00<br />

00 (4.4)<br />

0 = rot ( +1)+ 0 0 (4.5)<br />

∆ = ±1 ∆ =0 ±1 : (4.6)<br />

y 0 = rot ( 00 +1)( 00 +2)+ 0 0 (4.7)<br />

y ∆ = =2 rot ( 00 +1)+ ( 0 0 − 00<br />

00 ) (4.8)<br />

LMR transitions are in the FIR region (100 m ≤ ≤ 2000 m).

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