There
are many places, e.g.,
https://en.wikipedia.org/wiki/Climate_sensitivity,
where you can read statements such as, "Without
any feedbacks, a doubling of CO2
(which amounts to a forcing of 3.7 W/m2)
would result in 1 °C global
warming, which is easy to calculate and is undisputed. The
remaining uncertainty is due entirely to feedbacks in the system,
namely, the
water vapor feedback, the ice-albedo
feedback, the cloud
feedback, and the lapse rate feedback"
(Rahmstorf, Stefan
(2008). "Anthropogenic Climate Change: Revisiting the Facts".
In Zedillo, E. Global
Warming: Looking Beyond Kyoto (PDF). Brookings Institution Press.
pp. 34–53.)
However,
finding the calculations by which this 1.0 - 1.2 °C is determined is
not easy
(https://judithcurry.com/2010/12/11/co2-no-feedback-sensitivity/).
In
fact, the no-feedback temperature increase from doubling CO2
is easy to calculate. Two
equations are needed to determine
the increase: the Arrhenius relationship which determines the
increase in radiative
forcing (∆RF)
due to a
CO2
increase:
∆RF
= α•ln((C0+∆C)/(C0))
(Eq. 1)
where
∆RF
is the change in radiative forcing, C0
is the initial concentration of CO2,
∆C
is the concentration change,
and
α
is generally accepted as 5.35, and the following arrangement
of the
Stephan-Boltzmann Law:
((RF0+∆RF)/RF0)1/4
=
((T0+∆T)/T0)
(Eq.
2)
where
RF0
is the initial radiative forcing for temperature T0,
∆RF
is defined above, and ∆T
is the temperature change.
For
a doubling of CO2
Arrhenius does
indeed
gives
5.35•ln(2)
=
3.7 W/m2
as
the
∆RF
mentioned
above. To use Equation 2, note that T0
is
the current temperature of Earth, 288K. To
determine the appropriate RF0 for this temperature
we can use the no-greenhouse model of the Earth which
is used to determine a 33° C
warming due to these gases. In
this model, the ~1360 W/m2
solar radiant flux when the sun is directly overhead is used to
calculate an average flux over the entire planet, after accounting
for an albedo of 0.3, of 240 W/m2.
The full Stephan-Boltzmann Law
(https://en.wikipedia.org/wiki/Stefan-Boltzmann_law)
is then used to calculate a surface temperature of 255K. Equation 2
can then be used to determine that an additional 150 W/m2,
or 390 W/m2
altogether, is needed to achieve T0.
We can now fill in
all the needed values in Equation 2, and solve for ∆T:
((390+3.7)/390)1/4
=
((288+∆T)/288),
∆T
=
0.68K
0.68K? What happened to the 1K rise that has been publicized so widely? Is there an error in my calculations, or the premises which set them up?
As noted above, "finding the calculations by which this 1.0 - 1.2 °C is determined is
not easy." A possibility does occur to me, however. If instead of using the current planetary values for T0 and RF0 we use the values calculated in the no-greenhouse model, the results of solving Equation 2 are somewhat different:
((240+3.7)/240)1/4
=
((255+∆T)/255),
∆T
=
0.98K
0.98K is remarkably close to the "undisputed" value for the no-feedback increase. To continue in this vein, if the actual current global temperature is used instead of the no-greenhouse value, the rise "rises" further, to 1.1K.
There are other possibilities. For example, the value of 5.35 used in Equation 1 is, I assume, a global average derived from various locations where the water vapor content of the air at those locations are significantly different -- which they can be by as much as 300 fold. This is important because, as water vapor absorbs most of the thermal IR given off from the ground, CO2's absorbance will be either greater or smaller as a consequence (this is why AGW should be stronger at the poles than the equator). Use of a single, global temperature, rather than summing results from regions colder or hotter, may have an effect as well.
There are other possibilities. For example, the value of 5.35 used in Equation 1 is, I assume, a global average derived from various locations where the water vapor content of the air at those locations are significantly different -- which they can be by as much as 300 fold. This is important because, as water vapor absorbs most of the thermal IR given off from the ground, CO2's absorbance will be either greater or smaller as a consequence (this is why AGW should be stronger at the poles than the equator). Use of a single, global temperature, rather than summing results from regions colder or hotter, may have an effect as well.
These complications can be explored in another post. For the moment, I will accept the 0.68K value calculated here as accurate, and ask the next logical question: how much of this no-feedback warming should we expect so far? By so far, I mean going back about 150 years when CO2 levels were 280 ppm and global temperature approximately 1K cooler. Since current (2017) CO2 levels are given as 405 ppm -- a 44.6% increase -- we can use Equation 1 to calculate a ∆RF of almost 2.0 W/m2. Equation 2 converts this into a ∆T of 0.37K, or only 37% of the full estimated temperature rise during the last century and a half.
I can't resist pushing this article beyond the scope of its title. What, for example, might be the total no-feedback temperature effect of all radiative forcings over the last century and a half taken together. To answer this I include the following chart:
I can't resist pushing this article beyond the scope of its title. What, for example, might be the total no-feedback temperature effect of all radiative forcings over the last century and a half taken together. To answer this I include the following chart:
There is considerable uncertainty in many of these measurements, but if the average values are reasonably correct, they appear to cancel each other out, leaving the CO2 forcing close to the average.
The remaining factor to be considered is the climate sensitivity factor. This is difficult to determine with confidence, and the literature shows a wide range of values, from below 1 to as much as 4 or 5. The IPCC offers a range of 1.5-4.0, but values lower than this are regularly reported. If we accept a value of around 1.4 however (https://judithcurry.com/2016/04/25/updated-climate-sensitivity-estimates/), an interesting suggestion emerges from the data. If the CSF is ~ 1.4, then the total anthropogenic warming since the 1860s is about a half of a kelvin, or about one half the total estimated warming since that time. This of course implies a natural warming over this period of about the same. Again, citing the IPCC, this fraction is at the lowest end of its estimate of 95% certainty that anthropogenic warming is greater than 50%.
It may be even lower than that, however. According to measurements of radiative forcing due to CO2 increase over the period of 2000-2010 (https://www.nature.chttps://www.nature.com/articles/nature14240om/articles/nature14240) the increase of CO2 concentration from 370 ppm to 392 ppm during this period was accompanied by a radiative forcing increase of 0.2 W m−2 per decade. Using this data Equation 1 can be rearranged to solve for α:
The remaining factor to be considered is the climate sensitivity factor. This is difficult to determine with confidence, and the literature shows a wide range of values, from below 1 to as much as 4 or 5. The IPCC offers a range of 1.5-4.0, but values lower than this are regularly reported. If we accept a value of around 1.4 however (https://judithcurry.com/2016/04/25/updated-climate-sensitivity-estimates/), an interesting suggestion emerges from the data. If the CSF is ~ 1.4, then the total anthropogenic warming since the 1860s is about a half of a kelvin, or about one half the total estimated warming since that time. This of course implies a natural warming over this period of about the same. Again, citing the IPCC, this fraction is at the lowest end of its estimate of 95% certainty that anthropogenic warming is greater than 50%.
It may be even lower than that, however. According to measurements of radiative forcing due to CO2 increase over the period of 2000-2010 (https://www.nature.chttps://www.nature.com/articles/nature14240om/articles/nature14240) the increase of CO2 concentration from 370 ppm to 392 ppm during this period was accompanied by a radiative forcing increase of 0.2 W m−2 per decade. Using this data Equation 1 can be rearranged to solve for α:
α = ∆RF / ln((C0+∆C)/(C0))
(Eq. 3)
to yield 3.46, or about 2/3'rds the standard accepted value. This in turn leads to a no feedback
∆T of 0.25K instead of 0.37K, implying (if we maintain the climate sensitivity of 1.4) a total anthropogenic warming of only 0.35K, or 35% of total warming over the last 150 years.
∆T of 0.25K instead of 0.37K, implying (if we maintain the climate sensitivity of 1.4) a total anthropogenic warming of only 0.35K, or 35% of total warming over the last 150 years.