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Abundances, emissions, and loss processes of the long-lived and potent greenhouse gas octafluorooxolane (octafluorotetrahydrofuran, <i>c</i>-C<sub>4</sub>F<sub>8</sub>O) in the atmosphere
oleh: M. K. Vollmer, F. Bernard, F. Bernard, F. Bernard, B. Mitrevski, L. P. Steele, C. M. Trudinger, S. Reimann, R. L. Langenfelds, P. B. Krummel, P. J. Fraser, D. M. Etheridge, M. A. J. Curran, M. A. J. Curran, J. B. Burkholder
Format: | Article |
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Diterbitkan: | Copernicus Publications 2019-03-01 |
Deskripsi
<p>The first atmospheric observations of octafluorooxolane (octafluorotetrahydrofuran, <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span>), a persistent greenhouse gas, are reported. In addition, a complementary laboratory study of its most likely atmospheric loss processes, its infrared absorption spectrum, and global warming potential (GWP) are reported. First atmospheric measurements of <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> are provided from the Cape Grim Air Archive (41<span class="inline-formula"><sup>∘</sup></span> S, Tasmania, Australia, 1978–present), supplemented by two firn air samples from Antarctica, in situ measurements of ambient air at Aspendale, Victoria (38<span class="inline-formula"><sup>∘</sup></span> S), and a few archived air samples from the Northern Hemisphere. The atmospheric abundance in the Southern Hemisphere has monotonically grown over the past decades and leveled at 74 ppq (parts per quadrillion, femtomole per mole in dry air) by 2015–2018. The growth rate of <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> has decreased from a maximum in 2004 of 4.0 to <span class="inline-formula"><0.25</span> ppq yr<span class="inline-formula"><sup>−1</sup></span> in 2017 and 2018. Using a 12-box atmospheric transport model, globally averaged yearly emissions and abundances of <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> are calculated for 1951–2018. Emissions, which we speculate to derive predominantly from usage of <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> as a solvent in the semiconductor industry, peaked at 0.15 (<span class="inline-formula">±0.04</span>, 2<span class="inline-formula"><i>σ</i></span>) kt yr<span class="inline-formula"><sup>−1</sup></span> in 2004 and have since declined to <span class="inline-formula"><0.015</span> kt yr<span class="inline-formula"><sup>−1</sup></span> in 2017 and 2018. Cumulative emissions over the full range of our record amount to 2.8 (2.4–3.3) kt, which correspond to 34 Mt of <span class="inline-formula">CO<sub>2</sub></span>-equivalent emissions. Infrared and ultraviolet absorption spectra for <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> as well as the reactive channel rate coefficient for the <span class="inline-formula">O(<sup>1</sup>D)</span> <span class="inline-formula">+</span> <span class="inline-formula"><i>c</i></span>-<span class="inline-formula">C<sub>4</sub>F<sub>8</sub>O</span> reaction were determined from laboratory studies. On the basis of these experiments, a radiative efficiency of 0.430 W m<span class="inline-formula"><sup>−2</sup></span> ppb<span class="inline-formula"><sup>−1</sup></span> (parts per billion, nanomol mol<span class="inline-formula"><sup>−1</sup></span>) was determined, which is one of the largest found for synthetic greenhouse gases. The global annually averaged atmospheric lifetime, including mesospheric loss, is estimated to be <span class="inline-formula">>3</span>000 years. GWPs of 8975, 12 000, and 16 000 are estimated for the 20-, 100-, and 500-year time horizons, respectively.</p>