|Taken from Jacob 1999, Chapter 7, page 121|
Note that CO2 absorbs strongest right where Earth's infrared spectrum would peak and also has the deepest valley. Water vapor has the broadest portion of the spectrum it absorbs. As a result, CO2 is directly responsible for about 1/3 of the greenhouse effect, the rest is due mostly to water vapor. (Kiehl and Trenberth 1997; Pierrehumbert 2011).
Only 35 years after Tyndall identified the first greenhouse gases, the absorptive properties of carbon dioxide were known well enough for Svante Arrhenius to propose the theory of anthropogenic climate change (Arrhenius 1896). Arrhenius calculated that a doubling of CO2 would raise global temperatures by 3 to 4ºC, which is within the range for the best estimate of climate sensitivity today (2.5 to 4ºC, Knutti and Hegerl 2008; Paleosens 2013).
Beyond Arrhenius' calculations and laboratory measurements of absorptive properties, we have direct satellite measurements showing that increasing levels of CO2 and CH4 are the primary gases trapping more heat in the atmosphere, with minor contributions from other greenhouse gases such as CFCs, ozone, and N2O (Harries et al. 2001; Anderson et al. 2004; Griggs and Harries 2007; Chapman et al. 2013, Gastineau et al. 2014). Gastineau et al. (2014) also found that the total greenhouse effect had increased by 0.80 ± 0.13 W/m2 per decade between 1982 and 2004.
So if CH4 is also rising and most of the greenhouse effect is due to water vapor, why the focus on CO2? There are two reasons.
First, water vapor cannot cause a warming trend by itself. The amount of water vapor in the atmosphere is controlled by air temperature, not the other way around. The relationship between water vapor and air temperature is given by the Clausius-Clapeyron relation:
es = saturation water vapor pressure
T = Temperature
Rv = water vapor gas constant and
Lv = Latent heat of evaporation
Since Lv is also dependent on temperature, the August-Roche-Magnus formula is often used to approximate the relationship:
T = Temperature (ºC)
The August-Roche-Magnus formula shows that the amount of water vapor in the atmosphere rises exponentially with temperature.
|Relationship between water vapor pressure and air temperture|
So what is the role of water vapor? Positive feedback. As air temperature rises, the amount of water vapor also rises, reinforcing and magnifying that rise in air temperature. The converse is also true: As air temperature falls, water vapor precipitates out of the atmosphere, magnifying the drop in air temperature. Without the backstop provided by CO2, once temperature started falling, water vapor would magnify that drop until there was no more water vapor left to precipitate out, lowering global average temperature by 21ºC to an average surface temperature of -6ºC (21.2ºF) (Lacis et al. 2010).
The water vapor positive feedback effect has already been measured in the atmosphere. In the wake of Mount Pinatubo's 1991 eruption, a drop in water vapor magnified the cooling effect from sulfate aerosols temporarily increasing Earth's albedo (Soden et al. 2002). The long-term trend, however, is for water vapor to increase as the atmosphere warms. For instance, water vapor increased over the oceans at an average rate of 0.41 kg/m2 per decade between 1988 and 2006 (Santer et al. 2007) as the atmospheric temperature increased by 0.206ºC per decade during that time period (rate calculated using UAH temperature data).
As for methane, while it is a powerful greenhouse gas with a global warming potential 25x greater than CO2, its current concentration is 1.874 ppmv (CDIAC 2013). The average concentration for carbon dioxide for the last 12 months is 393.82 ppmv, more than 210x greater. We can also calculate the amount of warming expected from changes in each gas once equilibrium is reached using the Equilibrium Climate Sensitivity equation:
ΔT = λΔF
ΔT = change in global temperature (ºC)
λ = Climate sensitivity (best current estimate: 0.809ºC/W/m2) and
ΔF = change in radiative forcing (W/m2).
According to Myhre et al. (1998), for CO2, ΔF can be calculated as
C = target CO2 concentration (ppmv) and
C0 = reference CO2 concentration (ppmv), usually set at the pre-industrial value of 280 ppmv.
The corresponding equation for CH4 is
M = target CH4 concentration (ppbv) and
M0 = reference CH4 concentration (ppbv), usually set at the pre-industrial value of 700 ppbv.
Plugging in the current concentration of CO2 and CH4 into their respective formulas gives us
ΔT (CO2) = 0.809ºC/W/m2 * [5.35 W/m2 * ln(393.82 ppmv / 280 ppmv)]
= 0.809ºC/W/m2 * 1.82 W/m2
ΔT (CH4) = 0.809ºC/W/m2 * [0.036 W/m2 * (√- √ )
= 0.809ºC/W/m2 * 0.606 W/m2
While CH4 may be the more potent gas on a molecule by molecule basis, changes in CO2 concentrations are currently causing 3x the amount of temperature change.
So why the focus on CO2? Simple. It's currently the main gas behind the increase in global temperatures.