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Coal to gas: The influence of methane leakage

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Carbon dioxide (CO2) emissions from fossil fuel combustion may be reduced by using natural gas rather than coal to produce energy. Gas produces approximately half the amount of CO2 per unit of primary energy compared with coal. Here we consider a scenario where a fraction of coal usage is replaced by natural gas (i.e., methane, CH4) over a given time period, and where a percentage of the gas production is assumed to leak into the atmosphere. The additional CH4 from leakage adds to the radiative forcing of the climate system, offsetting the reduction in CO2 forcing that accompanies the transition from coal to gas. We also consider the effects of: methane leakage from coal mining; changes in radiative forcing due to changes in the emissions of sulfur dioxide and carbonaceous aerosols; and differences in the efficiency of electricity production between coal- and gas-fired power generation. On balance, these factors more than offset the reduction in warming due to reduced CO2 emissions. When gas replaces coal there is additional warming out to 2,050 with an assumed leakage rate of 0%, and out to 2,140 if the leakage rate is as high as 10%. The overall effects on global-mean temperature over the 21st century, however, are small.
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LETTER
Coal to gas: the influence of methane leakage
Tom M. L. Wigley
Received: 19 May 2011 / Accepted: 10 August 2011
#
Springer Science+Business Media B.V. 2011
Abstract Carbon dioxide (CO
2
) emissions from fossil fuel combustion may be reduced by
using natural gas rather than coal to produce energy. Gas produces approximately half the
amount of CO
2
per unit of primary energy compared with coal. Here we consider a scenario
where a fraction of coal usage is replaced by natural gas (i.e., methane, CH
4
) over a given
time period, and where a percentage of the gas production is assumed to leak into the
atmosphere. The additional CH
4
from leakage adds to the radiative forcing of the climate
system, offsetting the reduction in CO
2
forcing that accompanies the transition from coal to
gas. We also consider the effects of: methane leakage from coal mining; changes in radiative
forcing due to changes in the emissions of sulfur dioxide and carbonaceous aerosols; and
differences in the efficiency of electricity production between coal- and gas-fired power
generation. On balance, these factors more than offset the reduction in warming due to
reduced CO
2
emissions. When gas replaces coal there is additional warming out to 2,050 with
an assumed leakage rate of 0%, and out to 2,140 if the leakage rate is as high as 10%. The
overall effects on global-mean temperature over the 21st century, however, are small.
Hayhoe et al. (2002) have comprehensively assessed the coal-to-gas issue. What has changed
since then is the possibility of substantial methane production by high volume hydraulic
fracturing of shale beds (fracking) and/or exploitation of methane reservoirs in near-shore
ocean sediments. Fracking, in particular, may be associated with an increase in the amount of
attendant gas leakage compared with other means of gas production (Howarth et al. 2011). In
Hayhoe et al., the direct effects on global-mean temperature of differential gas leakage
between coal and gas production are very small (see their Fig. 4). Their estimates of gas
Climatic Change
DOI 10.1007/s10584-011-0217-3
Electronic supplementary material The online version of this article (doi:10.1007/s10584-011-0217-3)
contains supplementary material, which is available to authorized users.
T. M. L. Wigley (*)
National Center for Atmospheric Research, Post Office Box 3000, Boulder, CO 80307-3000, USA
e-mail: wigley@ucar.edu
T. M. L. Wigley
University of Adelaide, Adelaide, South Australia, Australia
leakage, however, are less than more recent estimates. Here, we extend and update the
analysis of Hayhoe et al. to examine the potential effects of gas leakage on the climate, and on
uncertainties arising from uncertainties in leakage percentages.
We begin with a standard no-climate-policy baseline emissions scenario, viz. the
MiniCAM Reference scenario (MINREF below) from the CCSP2.1a r eport (Clarke et
al. 2007). (Hayhoe et al. used the MiniCAM A1B scenario, Nakićenović and Swart
2000.) We chose MINREF partly because it is a more recent no-policy scenario, but
also because there is an extended version of MINREF that runs beyond 2,100 out to 2,300
(Wigley et al. 2009). The l onger time horizon is important because of the long timescales
involved in t he carbon cycle where changes to CO
2
emissions made in the 21st century
can have effects extending well into the 22nd century. (A second baseline scenario, the
MERGE Reference scenario from the CCSP2.1a report, is considered in the Electronic
Supplementary Material).
In MINREF, coal combustion provides from 38% (in 2010) to 51% (in 2100) of the
emissions of CO
2
from fossil fuels. (The corresponding percentages for gas are 19 to 21%,
and for oil are 43 to 28%.) For our coal-to-gas scenario we start with their contributions to
energy. It is important here to distinguish between primary energy (i.e., the energy content
of the resource) and final energy (the amount of energy delivered to the user at the point of
production). For a transition from coal to gas, we assume that there is no change in final
energy. As electricity generation from gas is more efficient than coal-fired generation, the
increase in primary energy from gas will be less than the decrease in primary energy from
coal the differential depends on the relative efficiencies with which energy is produced.
To calculate the change in fossil CO
2
emissions for any transition scenario we use the
following relationship relating CO
2
emissions to primary energy (P)
ECO2 ¼ A Pcoal þ B Poil þ C Pgas ð1Þ
where A, B and C are representative emissions factors (emissions per unit of primary
energy) for coal, oil and gas. The emissions factors relative to coal that we use are 0.75 for
oil and 0.56 for gas, based on information in EPAs AP-42 Report (EPA 2005). Using the
MINREF emissions for CO
2
and the published primary energy data give a best fit emissions
factor for coal of 0.027 GtC/exajoule, well within the uncertainty range for this term.
To determine the change in CO
2
emissions in moving from coal to gas under the
constraint of no change in final energy we use the equivalent of Eq. (1) expressed in terms
of final energy (F). This requires knowing the efficiencies for energy production from coal,
oil and gas (i.e., final energy/primary energy). If F=P×(efficiency), then we have
ECO2 ¼ A=aðÞFcoal þ B=bðÞFoil þ C=cðÞFgas ð2Þ
where a, b and c are the efficiencies for energy production from coal, oil and gas. For
changes in final energy (ΔF) in the coal-to-gas case, ΔFoil is necessarily zero. To keep
final energy unchanged, therefore, we must have ΔFgas = ΔFcoal. Hence, from Eq. (2)
ΔECO2 ¼ ΔFcoalðÞA=a C=cðÞ ð3Þ
or
ΔECO2 ¼ A ΔPcoal 1 C=AðÞ= c=aðÞ½ ð4Þ
As ΔPcoal is negative, the first term here is the reduction in CO
2
emissions from the
reduction in coal use, while the second term is the partially compensating increase in CO
2
Climatic Change
emissions from the increase in gas use. Our best-fit value for A is 0.027 GtC/exajoule, and
C/A=0.56. To apply Eq. (4) we need to determine a reasonable value for the relative gas-to-
coal efficiency ratio (c/a), which we assume does not change appreciably over time. For
electricity generation, the primary sector for coal-to-gas substitution, Hayhoe et al. (2002,
Table 2) give representative efficiencies of 32% for coal and 60% for gas. Using these
values, Eq. (4) becomes
ΔECO2 ¼ 0:027 ΔPcoal 1 0:299½ ð5Þ
for ΔECO2 in GtC and ΔP in exajoules. Thus, for a unit reduction in coal emissions, there
is an increase in emissions from gas combustion of about 0.3 units.
To complete our calculations, we need to estimate the changes in methane, sulfur dioxide
and black carbon emissions that would follow the coal-to-gas conversion. Consider
methane first. Methane is emitted to the atmosphere as a by-product of coal mining and gas
production. Although these fugitive emissions are relatively small, they are important
because methane is a far more powerful forcing agent per unit mass than CO
2
.
For coal mining we use information from Spath et al. (1999 ; Figs. C1 and C4). A typical
US coal-fired power plant emits 1,100 gCO2/kWh, with an attendant release of methane of
2.18 gCH4/kWh, almost entirely from mining. Thus, for each GtC of CO
2
emitted from a
coal-fired power plant, 7.27 TgCH4 are emitted from mining. Spath et al. give other
information that can used to check the above result. They give values of 1.91 gCH4
released per ton of coal mined from surface mines, and 4.23 gCH4 per ton from deep
mines. As 65% of coal comes from deep mines, the weighted average release is 3.42 gCH4/
ton. Since 1 ton of coal, when burned, typically produces 1.83 kgCO2, the amount of
fugitive methane per GtC of CO
2
emissions from coal-fired power plants is 6.85 TgCH4/
GtC, consistent with the previous result. For our calculations we use the average of these
two results, 7.06 TgCH4/GtC; i.e., if CO
2
emissions from coal-fired power generation are
reduced by 1 GtC, we assume a concomitant decrease in CH
4
emissions of 7.06 TgCH4.
We assume that this value for the USA is applicable for other countries.
For leakage associated with gas extraction and transport we note that every kg of gas
burned produces 12/16 kgC of CO
2
. If the leakage rate is p percent, then, for any given
increase in CO
2
emissions from gas combustion, the amount of fugitive methane released is
(p/100) (16/12) 1000=13.33 (p) TgCH4/GtC. For a leakage rate of 2.5%, for example
(roughly the present leakage rate for conventional gas extraction), this is 33.3 TgCH4/GtC.
Because the CO
2
emissions change from gas combustion is much less than that for coal
(about 30%; see Eq. (5)), for the 2.5% leakage case this would make the coal mining and
gas leakage effects on CH
4
quite similar (but of opposite sign), in accord with Hayhoe et al.
(2002, Table 1).
SO
2
emissions are important because coal combustion produces substantial SO
2
,
whereas SO
2
emissions from gas combustion are negligible. Reducing energy production
from coal has compensating effects reduced CO
2
emissions leads to reduced warming in
the long term, but this is offset by the effects of reduced SO
2
emissions which lead to lower
aerosol loadings in the atmosphere and an attendant warming (Wigley 1991). For CO
2
and
SO
2
, emissions factors for coal (from Hayhoe et al. 2002, Table 1) are 25 kgC/GJ and
0.24 kgS/GJ
.
For each GtC of CO
2
produced from coal combustion, therefore, there will be
19.2 TgS of SO
2
emitted. We can check this using emissions factors from Spath et al.
(1999, Figs. C1 and C2). For a typical coal-fired power plant these are 7.3 gSO2/kWh and
1,100 gCO2/kWh. Hence, for each GtC of CO
2
produced from coal combustion, SO
2
emissions will be 12.17 TgS. Effective global emissions factors can also be obtained from
Climatic Change
published emissions scenarios. For example, for changes over 2000 to 2010 in the MINREF
scenario, the emissions factor for coal combustion is approximately 11.6 TgS/GtC.
From these different estimates it is clear that there is considerable uncertainty in the SO
2
emissions factor, echoing in part the widely varying sulfur contents in coal. Furthermore,
for future emissions from coal combustion the SO
2
emissions factor is likely to decrease
markedly due to the imposition of SO
2
pollution controls (as explained, for example, in
Nakićenović and Swart 2000). It is difficult to quantify this effect, a difficulty highlighted,
for example, by the fact that, in the second half of the 21st century, many published
scenarios show increasing CO
2
emissions, but decreasing SO
2
emissions with large
differences between scenarios in the relative changes.
For the coal-to-gas transition, it is not at all clear how to account for the effects that SO
2
pollution controls, that will likely go on in parallel with any transition from coal to gas, will
have on the SO
2
emissions factor. However, future coal-fired plants will certainly employ
such controls, so emissions factors for SO
2
will decrease over time. To account for this we
assume a value of 12 TgS/GtC for the present (2010) declining linearly to 2 TgS/GtC by
2,060 and remaining at this level thereafter. This limit and the attainment date are consistent
with the fact that many of the SRES scenarios tend to stabilize SO
2
emissions at a finite,
non-zero value at around this time.
For black carbon (BC) aerosol emissions we use the relationship between BC and SO
2
emissions noted by Hayhoe et al. (2002, p. 125) and make BC forcing proportional to SO
2
emissions. Using best-estimate forcings from the IPCC Fourth Assessment Report, this
means that the increase in sulfate aerosol forcing changes due to SO
2
emissions reductions
are reduced by approximately 30% by the attendant changes in BC emissions. This is a
larger BC effect than in Hayhoe et al. However, compared with the large overall uncertainty
in aerosol forcing, the difference between what we obtain here and the results of Hayhoe et
al. are relatively small.
For our coal-to-gas emissions scenario we assume that primary energy from coal is
reduced linearly (in percentage terms) by 50% over 2010 to 2050 (1.25%/yr), and that the
reduction in final energy is made up by extra energy from gas combustion. (A second, more
extreme scenario is considered in the Electronic Supplementary Material). In this way, there
are no differences in final energy between the MINREF baseline scenario and the coal-to-
gas perturbation scenario. Hayhoe et al. consider scenarios where coal production reduces
by 0.4, 1.0 and 2.0%/yr over 2000 to 2025. After 2050 we assume no further percentage
reduction in coal-based energy (i.e., the reduction in emissions from coal relative to the
baseline scenario remains at 50%). This is an idealized scenario, but it is sufficiently
realistic to be able to assess the relative importance of different gas leakage rates. We
consider leakage rates of zero to 10%,
Baseline and perturbed (coal to gas) primary energy scenarios for coal and gas are shown
in Fig. 1, together with the corresponding fossil-fuel CO
2
emissions. The changes in
primary energy breakdown are large: e.g., in 2100, primary energy from coal is 37% more
than from gas in the baseline case, but 50% less than gas in the perturbed case. The
corresponding reduction in emissions is less striking. In the perturbed case, 2100 emissions
are reduced only by 19%. (Cases where there are larger emissions reductions are considered
in the Electronic Supplementary Material).
To determine the consequences of the coal-to-gas scenario we use the MAGICC coupled
gas-cycle/upwelling-diffusion climate model (Wigley et al. 2009 ; Meinshausen et al. 2011).
These are full calculations from emissions through concentrations and radiative forcing to
global-mean temperature consequences. We do not make use of Global Warming Potentials
(as in Howarth et al. 2011, for example), which are a poor substitute for a full calculation
Climatic Change
(see, e,g., Smith and Wigley 2000a, b). MAGICC considers all important radiative forcing
factors, and has a carbon cycle model that includes climate feedbacks on the carbon cycle.
Methane lifetime is affected by atmospheric loadings on methane, carbon monoxide,
nitrogen oxides (NOx) and volatile organic compounds. The effects of methane on
tropospheric ozone and stratospheric water vapor are considered directly. For component
forcing values we use central estimates as given in the IPCC Fourth Assessment Report
(IPCC 2007, p.4). We also assume a central value for the climate sensitivity of 3°C
equilibrium warming for a CO
2
doubling. (A second case using a higher sensitivity is
considered in the Electronic Supplementary Material).
Figure 2 shows the relative and total effects of the coal-to-gas transition for a leakage
rate of 5%. This is within the estimated leakage rate range (1.76.0%; Howarth et al. 2011)
for conventional methane production (the effects of well site leakage, liquid uploading and
gas processing, and transport, storage and processing). For methane from shale, Howarth et
al. estimate an additional leakage of 1.9% (their Table 2) with a range of 0.63.2% (their
Table 1). The zero to 10.0% leakage rate range considered here spans these estimates
although we note that the high estimates of Howarth et al. have been criticized (Ridley
2011, p. 30).
The top panel of Fig. 2 shows that the effects of CH
4
leakage and reduced aerosol
loadings that go with the transition f rom coal to gas can appreciably offset the effect of
reduced CO
2
concentrations, potenti ally (see Fig. 3) until well into the 22nd century.
For the leakage rate ranges considered here, however, the overall effects of the coal to
(a)
(b)
Fig. 1 a Primary energy
scenarios. Baseline data to 2100
are from the CCSP2.1a
MiniCAM Reference scenario.
After 2100, baseline primary
energy data have been
constructed to be consistent with
emissions data in the extended
MiniCAM Reference scenario
(Wigley et al. 2009 REFEXT).
Full lines are for coal, dotted
lines are for gas. NEW data
correspond to the coal-to-gas
scenario. Under the final energy
constraint that ΔFgas = ΔFcoal,
ΔPgas = (a/c) ΔPcoal = 0.533
ΔPcoal. b Corresponding fossil
CO
2
emissions data
Climatic Change
gas transition on global-mean temperatur e are very small throughout the 21st c entury,
both in absolute and relative terms (see F ig. 2a). This is primarily due to the relatively
small reduction in CO
2
emissions that is effected by the transi tion a way from coal (see
Fig. 1b). Cases where the CO
2
emissions reductions ar e larger ( due to a more extr eme
substitution scenario, or a different baseline) are considered in the Electronic
Supplementary Material. The relative contributions to temperature change are similar,
but the magnitudes of temperature change scale roughly with the overall reduction in
CO
2
emissions.
Figure 3 shows the sensitivity of the temperature differential to the assumed leakage
rate. The CO
2
and aerosol terms are independent of the assumed leakage rate, so we only
show the methane and total-effect r esults. These results are qualitatively similar to those
of Hayhoe et al. who considered only a single leakage rate case (corresponding
approximately to our 2.5% leakage case). For leakage rates of more than 2%, the methane
leakage contribution is positive (i.e., replacing coal by gas produces higher methane
concentrations) see the CH4 COMPONENT curves in Fig. 3. Depending on leakage
rate, replacing coal by gas leads, not to cooling, but to additional w arming out to between
2,050 and 2,140. Initially, this is due mainly to the influence of SO
2
emissions changes,
with the effects of CH
4
leakage becoming more important over time. Even with zero
leakage from gas production, however, the cooling that eventually arises from the coal-to-
gas transition is only a few tenths of a degC (greater for g reater climate sensitivity see
Electronic Supplementary Material). Using climate amelioration as an argument for the
(a)
(b)
Fig. 2 a Baseline global-mean
warming (solid bold line) from
the extended CCSP2.1a Mini-
CAM reference scenario together
with the individual and total
contributions due to reduced CO
2
concentrations, reduced aerosol
loadings and increased methane
emissions for the case of 5%
methane leakage. The bold
dashed line gives the result for all
three components, the dotted line
shows the effect of CO
2
alone.
The top two thin lines show the
CH
4
and aerosol components. b
Detail showing differences from
the baseline
Climatic Change
transition is, at best, a very weak argument, as noted by Hayhoe et al. (2002), Howarth et
al. (2011) and others .
In summary, our results show that the substitution of gas for coal as an energy
source results in increased rather than decreased global warming for m any decades
out to the mid 22nd century for the 10% leakage case. This is in accord with Hayhoe
et al. (2002) and with the less well established claims of Howarth et al. (2011) who base
their analysis on Global Warming Potentials rather than direct modeling of the climate.
Our r esults are critically sensitive to the assumed leakage rate. In our analysis, the
warming results from two effects: the reduction in SO
2
emissions that occurs due to
reduced coa l combustion; and t he pot entially great er leakage of methane that
accompanies new gas production relative to coal. The first effect is in accord with
Hayhoe e t al. In Hayhoe et al., however, the methane effect is in the opposite direction to
our result (albeit very small). This is because our analyses use more recent information on
gas leakage from coal mines and gas production, with greater leakage from the latter. The
effect of methane leakage from gas production in our analyses is, nevertheless, small and
less than implied by Howarth et al.
Our coal-to-gas scenario assumes a linear decrease in coal use from zero in 2010 to 50%
reduction in 2050, continuing at 50% after that. Hayhoe et al. consider linear decreases
from zero in 2000 to 10, 25 and 50% reductions in 2025. If these authors assumed constant
reduction percentages after 2025, then their high scenario is very similar to our scenario.
In our analyses, the temperature differences between the baseline and coal-to-gas
scenarios are small (less than 0.1°C) out to at least 2100. The most important result,
however, in accord with the above authors, is that, unless leakage rates for new
methane can be kept below 2%, substituting gas for c oal is not an effective means for
reducing the magnitude of future climate change. This is contrary to claims such as
that by Ridley (20 11) who states (p. 5), with regard to the exploitation of shale gas, that
it will accelerate the decarbonisation of the world economy. The key point here is that it
is not decarbonisation per se that is the goal, but the attendant reduction of climate
change. Indeed, the shorter-term effects are in the opposite direction. Given the small
climate differences between the baseline and the coal-to-gas scenarios, decisions
regarding further exploitation of gas reserves should be based on resource availability
(both gas and water), the economics of extraction, and environmental impacts u nrelated
to climate change.
Fig. 3 The effects of different
methane leakage rates on global-
mean temperature. The top four
curves (CH4 COMPONENT)
show the effects of methane con-
centration changes, while the
bottom four curves (TOTAL)
show the total effects of methane
changes, aerosol changes and
CO
2
concentration changes. The
latter two effects are independent
of the leakage rate, and are shown
in Fig. 2. Results here are for a
climate sensitivity of 3.0°C
Climatic Change
Acknowledgments Comments from Chris Green and the external reviewers helped improve the original
version of this manuscript. The National Center for Atmospheric Research is supported by the National
Science Foundation.
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Object detection, a fundamental and challenging problem in computer vision, has experienced rapid development due to the effectiveness of deep learning. The current objects to be detected are mostly rigid solid substances with apparent and distinct visual characteristics. In this paper, we endeavor on a scarcely explored task named Gaseous Object Detection (GOD), which is undertaken to explore whether the object detection techniques can be extended from solid substances to gaseous substances. Nevertheless, the gas exhibits significantly different visual characteristics: 1) saliency deficiency, 2) arbitrary and ever-changing shapes, 3) lack of distinct boundaries. To facilitate the study on this challenging task, we construct a GOD-Video dataset comprising 600 videos (141,017 frames) that cover various attributes with multiple types of gases. A comprehensive benchmark is established based on this dataset, allowing for a rigorous evaluation of frame-level and video-level detectors. Deduced from the Gaussian dispersion model, the physics-inspired Voxel Shift Field (VSF) is designed to model geometric irregularities and ever-changing shapes in potential 3D space. By integrating VSF into Faster RCNN, the VSF RCNN serves as a simple but strong baseline for gaseous object detection. Our work aims to attract further research into this valuable albeit challenging area.
... Fossil fuels, such as oil and natural gas, form the foundation of social development and technological advancement. Unfortunately, accidental gas leaks frequently occur during the extraction process, leading to industrial explosions, fires, and air pollution, which have raised serious social concerns [1][2][3][4][5]. Consequently, real-time diffusion alerts of gas leaks are vital for effective emergency response and safeguarding public safety and property. ...
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