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Stratospheric carbon isotope fractionation and tropospheric histories of CFC-11, CFC-12, and CFC-113 isotopologues
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We present novel measurements of the carbon isotope composition of CFC-11 (CCl
3
F), CFC-12 (CCl
2
F
2
), and CFC-113 (CF
2
ClCFCl
2
), three atmospheric trace gases that are important for both stratospheric ozone depletion and global warming. These measurements were carried out on air samples collected in the stratosphere – the main sink region for these gases – and on air extracted from deep polar firn snow. We quantify, for the first time, the apparent isotopic fractionation,
ϵ
app
(
13
C), for these gases as they are destroyed in the high- and mid-latitude stratosphere:
ϵ
app
(CFC-12, high-latitude) =(-20.2±4.4) ‰, and
ϵ
app
(CFC-113, high-latitude) =(-9.4±4.4) ‰,
ϵ
app
(CFC-12, mid-latitude) =(-30.3±10.7) ‰, and
ϵ
app
(CFC-113, mid-latitude) =(-34.4±9.8) ‰. Our CFC-11 measurements were not sufficient to calculate
ϵ
app
(CFC-11), so we instead used previously reported photolytic fractionation for CFC-11 and CFC-12 to scale our
ϵ
app
(CFC-12), resulting in
ϵ
app
(CFC-11, high-latitude) =(-7.8±1.7) ‰ and
ϵ
app
(CFC-11, mid-latitude) =(-11.7±4.2) ‰. Measurements of firn air were used to construct histories of the tropospheric isotopic composition,
δ
T
(
13
C), for CFC-11 (1950s to 2009), CFC-12 (1950s to 2009), and CFC-113 (1970s to 2009), with
δ
T
(
13
C) increasing for each gas. We used
ϵ
app
(high-latitude), which was derived from more data, and a constant isotopic composition of emissions,
δ
E
(
13
C), to model
δ
T
(
13
C, CFC-11),
δ
T
(
13
C, CFC-12), and
δ
T
(
13
C, CFC-113). For CFC-11 and CFC-12, modelled
δ
T
(
13
C) was consistent with measured
δ
T
(
13
C) for the entire period covered by the measurements, suggesting that no dramatic change in
δ
E
(
13
C, CFC-11) or
δ
E
(
13
C, CFC-12) has occurred since the 1950s. For CFC-113, our modelled
δ
T
(
13
C, CFC-113) did not agree with our measurements earlier than 1980. This discrepancy may be indicative of a change in
δ
E
(
13
C, CFC-113). However, this conclusion is based largely on a single sample and only just significant outside the 95 % confidence interval. Therefore more work is needed to independently verify this temporal trend in the global tropospheric
13
C isotopic composition of CFC-113. Our modelling predicts increasing
δ
T
(
13
C, CFC-11),
δ
T
(
13
C, CFC-12), and
δ
T
(
13
C, CFC-113) into the future. We investigated the effect of recently reported new CFC-11 emissions on background
δ
T
(
13
C, CFC-11) by fixing model emissions after 2012 and comparing
δ
T
(
13
C, CFC-11) in this scenario to the model base case. The difference in
δ
T
(
13
C, CFC-11) between these scenarios was 1.4 ‰ in 2050. This difference is smaller than our model uncertainty envelope and would therefore require improved modelling and measurement precision as well as better quantified isotopic source compositions to detect.
Title: Stratospheric carbon isotope fractionation and tropospheric histories of CFC-11, CFC-12, and CFC-113 isotopologues
Description:
We present novel measurements of the carbon isotope composition of CFC-11 (CCl
3
F), CFC-12 (CCl
2
F
2
), and CFC-113 (CF
2
ClCFCl
2
), three atmospheric trace gases that are important for both stratospheric ozone depletion and global warming.
These measurements were carried out on air samples collected in the stratosphere – the main sink region for these gases – and on air extracted from deep polar firn snow.
We quantify, for the first time, the apparent isotopic fractionation,
ϵ
app
(
13
C), for these gases as they are destroyed in the high- and mid-latitude stratosphere:
ϵ
app
(CFC-12, high-latitude) =(-20.
2±4.
4) ‰, and
ϵ
app
(CFC-113, high-latitude) =(-9.
4±4.
4) ‰,
ϵ
app
(CFC-12, mid-latitude) =(-30.
3±10.
7) ‰, and
ϵ
app
(CFC-113, mid-latitude) =(-34.
4±9.
8) ‰.
Our CFC-11 measurements were not sufficient to calculate
ϵ
app
(CFC-11), so we instead used previously reported photolytic fractionation for CFC-11 and CFC-12 to scale our
ϵ
app
(CFC-12), resulting in
ϵ
app
(CFC-11, high-latitude) =(-7.
8±1.
7) ‰ and
ϵ
app
(CFC-11, mid-latitude) =(-11.
7±4.
2) ‰.
Measurements of firn air were used to construct histories of the tropospheric isotopic composition,
δ
T
(
13
C), for CFC-11 (1950s to 2009), CFC-12 (1950s to 2009), and CFC-113 (1970s to 2009), with
δ
T
(
13
C) increasing for each gas.
We used
ϵ
app
(high-latitude), which was derived from more data, and a constant isotopic composition of emissions,
δ
E
(
13
C), to model
δ
T
(
13
C, CFC-11),
δ
T
(
13
C, CFC-12), and
δ
T
(
13
C, CFC-113).
For CFC-11 and CFC-12, modelled
δ
T
(
13
C) was consistent with measured
δ
T
(
13
C) for the entire period covered by the measurements, suggesting that no dramatic change in
δ
E
(
13
C, CFC-11) or
δ
E
(
13
C, CFC-12) has occurred since the 1950s.
For CFC-113, our modelled
δ
T
(
13
C, CFC-113) did not agree with our measurements earlier than 1980.
This discrepancy may be indicative of a change in
δ
E
(
13
C, CFC-113).
However, this conclusion is based largely on a single sample and only just significant outside the 95 % confidence interval.
Therefore more work is needed to independently verify this temporal trend in the global tropospheric
13
C isotopic composition of CFC-113.
Our modelling predicts increasing
δ
T
(
13
C, CFC-11),
δ
T
(
13
C, CFC-12), and
δ
T
(
13
C, CFC-113) into the future.
We investigated the effect of recently reported new CFC-11 emissions on background
δ
T
(
13
C, CFC-11) by fixing model emissions after 2012 and comparing
δ
T
(
13
C, CFC-11) in this scenario to the model base case.
The difference in
δ
T
(
13
C, CFC-11) between these scenarios was 1.
4 ‰ in 2050.
This difference is smaller than our model uncertainty envelope and would therefore require improved modelling and measurement precision as well as better quantified isotopic source compositions to detect.
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