Can ozone be used to calibrate aerosol photoacoustic spectrometers?
<p>Photoacoustic spectroscopy (PAS) has become a popular technique for measuring absorption of light by atmospheric aerosols in both the laboratory and field campaigns. It has low detection limits, measures suspended aerosols, and is insensitive to scattering. But PAS requires rigorous calibra...
| Main Authors: | , |
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| Format: | Article |
| Language: | English |
| Published: |
Copernicus Publications
2018-12-01
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| Series: | Atmospheric Measurement Techniques |
| Online Access: | https://www.atmos-meas-tech.net/11/6419/2018/amt-11-6419-2018.pdf |
| Summary: | <p>Photoacoustic spectroscopy (PAS) has become a popular technique for measuring
absorption of light by atmospheric aerosols in both the laboratory and
field campaigns. It has low detection limits, measures suspended aerosols,
and is insensitive to scattering. But PAS requires rigorous calibration to be
applied quantitatively. Often, a PAS instrument is either filled with a gas
of known concentration and absorption cross section, such that the absorption
in the cell can be calculated from the product of the two, or the absorption
is measured independently with a technique such as cavity ring-down
spectroscopy. Then, the PAS signal can be regressed upon the known absorption
to determine a calibration slope that reflects the sensitivity constant of
the cell and microphone. Ozone has been used for calibrating PAS instruments
due to its well-known UV–visible absorption spectrum and the ease with which
it can be generated. However, it is known to photodissociate up to
approximately 1120 nm via the <span class="inline-formula">O<sub>3</sub></span> <span class="inline-formula">+</span> <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M3" display="inline" overflow="scroll" dspmath="mathml"><mrow><mi>h</mi><mi mathvariant="italic">ν</mi><mspace linebreak="nobreak" width="0.25em"/><mo>(</mo><mo>></mo><mn mathvariant="normal">1.1</mn><mi mathvariant="normal">eV</mi><mo>)</mo><mo>→</mo><mrow class="chem"><msub><mi mathvariant="normal">O</mi><mn mathvariant="normal">2</mn></msub></mrow><msup><mo>(</mo><mn mathvariant="normal">3</mn></msup><msubsup><mi mathvariant="normal">Σ</mi><mi>g</mi><mo>-</mo></msubsup><mo>)</mo></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="117pt" height="17pt" class="svg-formula" dspmath="mathimg" md5hash="2540a17128385cdeb672d3ea6820a4f8"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="amt-11-6419-2018-ie00001.svg" width="117pt" height="17pt" src="amt-11-6419-2018-ie00001.png"/></svg:svg></span></span> <span class="inline-formula">+</span> <span class="inline-formula">O(<sup>3</sup>P)</span> pathway, which is likely to
lead to inaccuracies in aerosol measurements. Two recent studies have
investigated the use of <span class="inline-formula">O<sub>3</sub></span> for PAS calibration but have reached
seemingly contradictory conclusions with one finding that it results in a
sensitivity that is a factor of 2 low and the other concluding that it is
accurate. The present work is meant to add to this discussion by exploring
the extent to which <span class="inline-formula">O<sub>3</sub></span> photodissociates in the PAS cell and the role
that the identity of the bath gas plays in determining the PAS sensitivity.
We find a 5 % loss in PAS signal attributable to photodissociation at 532 nm
in <span class="inline-formula">N<sub>2</sub></span> but no loss in a 5 % mixture of <span class="inline-formula">O<sub>2</sub></span> in <span class="inline-formula">N<sub>2</sub></span>.
Furthermore, we discovered a dramatic increase of more than a factor of 2
in the PAS sensitivity as we increased the <span class="inline-formula">O<sub>2</sub></span> fraction in the bath
gas, which reached an asymptote near 100 % <span class="inline-formula">O<sub>2</sub></span> that nearly matched the
sensitivity measured with both <span class="inline-formula">NO<sub>2</sub></span> and nigrosin particles. We
interpret this dependence with a kinetic model that suggests the reason for
the observed results is a more efficient transfer of energy from excited
<span class="inline-formula">O<sub>3</sub></span> to <span class="inline-formula">O<sub>2</sub></span> than to <span class="inline-formula">N<sub>2</sub></span> by a factor of 22–55 depending on
excitation wavelength. Notably, the two prior studies on this topic used
different bath gas compositions, and although the results presented here do
not fully resolve the differences in their results, they may at least
partially explain them.</p> |
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| ISSN: | 1867-1381 1867-8548 |