Posted on June 26th, 2014
The change in near surface relative humidity averaged over CMIP5 models over the 21st century in the RCP4.5 scenario. Dec-Jan-Feb is on the left and June-July-Aug on the right. From Laine et al, 2014.
We expect the amount of water vapor in the atmosphere to increase as the atmosphere warms. The physical constraints that lead us to expect this are particularly strong in the atmospheric boundary layer over the oceans. The relative humidity (RH — the ratio of the actual vapor pressure to the saturation value) at the standard height of 2 meters is roughly 0.80 over the oceans. At typical temperatures near the surface, the fractional increase in the saturation vapor pressure per degree C warming is about 7%. So RH would decrease by about the same fraction, amounting to roughly 0.06 per degree C of warming if the water vapor near the surface did not increase at all. Why isn’t it possible for RH to decrease by this seemingly modest amount?
The figure shows what CMIP5 models predict will happen to RH near the surface by the end of the present century in the RCP4.5 scenario. In this scenario, which requires major mitigation efforts by mid-century, these models warm the tropics by about 1.6C on average, so fixed vapor concentrations would result in a decrease in RH of about 0.10. (I am avoiding expressing RH as a percentage to avoid having to talk about percentages of percentages.) The figure, from Laine et al 2014, shows RH over the oceans increasing by a modest amount, something like 0.01. (Over most land surfaces, RH is predicted to decrease — this is important, but I am going to focus on the oceans here since this is where most evaporation occurs.) So, to first order we can say that RH over the oceans does not change much in these simulations, relative to the decrease that would occur at fixed vapor concentrations. To second order RH near the surface over the oceans actually increases modestly.
To understand the first order picture, we need two pieces of information, one regarding the global energy balance of the troposphere and other regarding how the strength of the global hydrological cycle is related to near-surface RH.
The tropospheric energy balance to first order is a balance between radiative cooling and the release of latent heat when water vapor condenses. In the global mean there is roughly 80 W/m2 of latent heating. The change in this number in global climate models is typically only 1 or maybe 1.5 W/m2 increase per degree C warming in 1%/yr transient CO2 simulations (Pendergrass and Hartmann 2014), or at most 2% per degree C warming. Pendergrass and Hartmann provide a nice deconstruction of this number. Prevedi 2010 is very useful as well. There is a lot of literature on this energetic constraint on the strength of the hydrological cycle, starting, I think, with Betts and Ridgeway 1988. Aerosols — especially absorbing aerosols — can change things quantitatively quite a bit. But for our first order picture we only need to know not to expect large fractional changes in global mean evaporation or precipitation given the modest fractional changes in atmospheric radiative cooling involved.
The second point to appreciate is that the evaporation is controlled by the degree of sub-saturation of the air near the surface — roughly speaking by (1-RH) rather than RH itself. The air in contact with the ocean surface is saturated and it is the gradient in the concentration of water vapor between this surface air and the air near the surface that drives evaporation. If the relative humidity at the reference level is 0.80, the sub-saturation, 1-RH, is 0.20 and a reduction in relative humidity from 0.8 to 0.7 (as would be consistent with fixed vapor concentration in the warming simulation pictured above) would result in a 50%(!) increase in (1-RH). A 50% increase in evaporation is obviously ruled out by energy balance requirements. So we expect small changes in RH near the surface as the climate warms.
More precisely, evaporation over the oceans can be approximated by the “bulk formula”
Here and are the saturation humidities at the ocean surface and reference level temperatures respectively, and are the relative humidity and wind speed at this reference level, the atmospheric density and a non-dimensional constant. A lot of physics and a lot of empirical evidence has been stuffed into the constant , guided by what is affectionately known as Monin-Obukhov similarity theory. (All global climate models compute surface fluxes using Monin-Obukhov scaling as the starting point.) depends on the height of the reference level, some properties of the surface (specifically surface “roughnesses”), and the gravitational stability of the atmosphere near the surface, which in turn is strongly coupled to the air-sea temperature difference.
If we ignore the air sea temperature difference as well as changes in wind speed and , then we just have . If the specific humidity does not change, then the large fractional reduction in results in a huge increase in evaporation, as discussed above. But it even worse than that, because will also increase by about 7%/C on top of the effect of the change in .
Can the other factors in the expression for evaporation compensate somehow? The changes in tropical weather would have to be profound to produce reductions in average wind speed large enough to compensate for a such a large increase in . Fortunately, no models even hint at such profound changes. We can rewrite the expression for the evaporation as
For the term proportional to to compensate for the large reduction in RH this air-sea temperature difference would have to change sign, since the temperature difference is small — only +1 to +2C over the tropical oceans. But this temperature difference is itself constrained by an energy balance argument, as discussed by Betts and Ridgeway. [Due to mixing of water vapor in the turbulent boundary layer, the specific humidity is relatively homogeneous with height in this layer while temperatures decrease with height, so we often reach a point at which saturation occurs within the boundary layer, the cloud base. Latent heat release comes into play only above this level; something has to balance the radiative cooling below cloud base and it is the sensible heat transfer from the surface, proportional to the air-sea temperature difference, which has to pick up the slack.] And it is also extremely implausible that the value of C could cause this magnitude of an adjustment in evaporation (the easiest way of changing C is to change the air-sea temperature difference a lot). Something very dramatic would have to happen in the tropical atmosphere to avoid the constraint that near surface water vapor over the ocean must increase as the surface warms to maintain nearly constant relative humidity.
As for the second order picture, the small increase in RH over the oceans, note that the term would result in an increase in evaporation of 7% per degree C warming even if the relative humidity were fixed, and that this increase is already too large to be consistent with the energy constraint. An increase in RH of about 0.01, that is, a decrease in 1-RH of about 5%, is about the right order of magnitude to restore consistency. This seems to be part of what is going on in the CMIP5 composite at the top of the post. But now the changes are small enough that reduction in average wind speed and modest change in air-sea temperature difference could also play a role, as they seem to do in models. However, the models do seem to take advantage of the simplest way of throttling back the evaporation — a small increase in RH.
This near surface relative humidity is not just relevant for the lowest few meters of the atmosphere, since these near surface values are coherent with the humidity of the entire planetary boundary layer — the lowest 1-2 kms of the troposphere — because of the strong turbulent mixing throughout this layer. While the boundary layer is not where most water vapor feedback originates, it does contain a large fraction of the mass of water vapor. The increase in total mass of water vapor with warming has lots of consequences — for example, for the increase in the amplitude of the pattern of evaporation minus precipitation discussed in Posts #13 and #14.
[The views expressed on this blog are in no sense official positions of the Geophysical Fluid Dynamics Laboratory, the National Oceanic and Atmospheric Administration, or the Department of Commerce.]