Lower calcification rates would reduce the alkalinity pump, reduce surface CO2 and increase the buffering
capacity of surface waters.
Cooling temperatures would still cause atmospheric CO2 to decline over time, since
the capacity of surface water to «hold» CO2 is an inverse function of temperature.
Not exact matches
The loss
of fertile top soil by erosion results in a lower yield
capacity on the onehand and in a undesired transfer
of nutrients, pesticides and sediments in
surface water on the other.
But then the effective heat
capacity, the
surface temperature, depends on the rate
of mixing
of the ocean
water and I have presented evidence from a number
of different ways that models tend to be too diffusive because
of numerical reasons and coarse resolution and wave parameter rise, motions in the ocean.
The
surface heat
capacity C (j = 0) was set to the equivalent
of a global layer
of water 50 m deep (which would be a layer ~ 70 m thick over the oceans) plus 70 %
of the atmosphere, the latent heat
of vaporization corresponding to a 20 % increase in
water vapor per 3 K warming (linearized for current conditions), and a little land
surface; expressed as W * yr per m ^ 2 * K (a convenient unit), I got about 7.093.
Corresponding time for
surface + tropospheric equilibration: given 3 K warming (including feedbacks) per ~ 3.7 W / m2 forcing (this includes the effects
of feedbacks): 10 years per heat
capacity of ~ 130 m layer
of ocean (~ heat
capacity of 92 or 93 m
of liquid
water spread over the whole globe)
Re 9 wili — I know
of a paper suggesting, as I recall, that enhanced «backradiation» (downward radiation reaching the
surface emitted by the air / clouds) contributed more to Arctic amplification specifically in the cold part
of the year (just to be clear, backradiation should generally increase with any warming (aside from greenhouse feedbacks) and more so with a warming due to an increase in the greenhouse effect (including feedbacks like
water vapor and, if positive, clouds, though regional changes in
water vapor and clouds can go against the global trend); otherwise it was always my understanding that the albedo feedback was key (while sea ice decreases so far have been more a summer phenomenon (when it would be warmer to begin with), the heat
capacity of the sea prevents much temperature response, but there is a greater build up
of heat from the albedo feedback, and this is released in the cold part
of the year when ice forms later or would have formed or would have been thicker; the seasonal effect
of reduced winter snow cover decreasing at those latitudes which still recieve sunlight in the winter would not be so delayed).
Model simulations for the North Atlantic Ocean and thermodynamic principles reveal that this feedback should be stronger, at present, in colder midlatitude and subpolar
waters because
of the lower present - day buffer
capacity and elevated DIC levels driven either by northward advected
surface water and / or excess local air - sea CO2 uptake.
This makes sense since warming the
surfaces of the world's oceans would tend to decrease their CO2 - carrying -
capacity, and this would be a slow process due to the buffering effects
of the specific heat
capacity of these large bodies
of water.
More than 109 cubic km (26 cubic miles)
of groundwater disappeared between 2002 and 2008 — double the
capacity of India's largest
surface water reservoir, the Upper Wainganga, and triple that
of Lake Mead, the largest man - made reservoir in the United States...
That has the amount
of land and
water per 5 degree latitude band with a rough estimate
of the
surface ocean heat
capacity.
A mere 16,400 hectares
of land will be irrigated, while
water storage
capacity will increase from 3 to 24 %
of the annual
surface water availability.
The main difference between H2O and CO2 (apart from the numerical differences
of their specific physical properites such as degree
of freedom, thermal
capacity, physical mass, etc) in terms
of their effects on the atmosphere is that
water is capable
of condensing into liquid to form clouds and readily and rapidly moves between
surface and atmosphere, daily, seasonally, annually and on even greater time scales, but CO2 does not liquify in the biosphere and transfers over mostly long time periods between
surface (primarily oceans, seas, etc) and the atmosphere.
As carbon dioxide is acidic, the
surface waters of the oceans could become more acidic than ever before in five million years, reducing the
capacity of shell - forming species to form shells and affecting the marine food chain.
In contrast, the oceans lose heat less rapidly, because
of the large heat
capacity of water, their ability to overturn as the
surfaces cool and become negatively buoyant, and the movement
of ocean currents such as the Gulf Stream and the Kuroshio current.
With a heat
capacity for the total atmosphere equal to ~ 3 meter
of water and an average temperature far below the average
surface temperature there is no way you can warm Earth's
surface and oceans from the atmosphere.
So if on shined that laser on a square meter for say 10 mins then the 1 mm depth
of square meter could warm by about 1 C. Rather than
water one could also heat up anything with a thin
surface [and assuming one reduces the heat loss] So thin sheet
of paper which absorbs [has heat
capacity of whatever wavelength one is using could heated within mins
of exposure.
Differences in available energy, canopy roughness, the timing
of physiological functioning,
water holding
capacity of the soil and rooting depth
of the vegetation explained the observed differences in sensible and latent heat exchange
of the contrasting vegetation
surfaces.
Of course, this may only happen mostly on the 30 % land surfaces, predominantly at lower elevations, I would think — not on water covered surfaces where the heat capacity of water would limit the cooling or heating of the crust, although any part of the affected plate that is land bound would still lever the whole plate to or fr
Of course, this may only happen mostly on the 30 % land
surfaces, predominantly at lower elevations, I would think — not on
water covered
surfaces where the heat
capacity of water would limit the cooling or heating of the crust, although any part of the affected plate that is land bound would still lever the whole plate to or fr
of water would limit the cooling or heating
of the crust, although any part of the affected plate that is land bound would still lever the whole plate to or fr
of the crust, although any part
of the affected plate that is land bound would still lever the whole plate to or fr
of the affected plate that is land bound would still lever the whole plate to or fro.
Note: LOTI provides a more realistic representation
of the global mean trends than dTs below; it slightly underestimates warming or cooling trends, since the much larger heat
capacity of water compared to air causes a slower and diminished reaction to changes; dTs on the other hand overestimates trends, since it disregards most
of the dampening effects
of the oceans that cover about two thirds
of the Earth's
surface.
The mass
of the
water and the mass
of the cookie are supposed to represent the relative thermal
capacities of the earth's
surface and rarefied CO2.
Yes, it is not a simple problem considering about 70 %
of the earth's
surface is covered by
water and the heat
capacity of the oceans is several orders
of magnitude greater than the atmosphere.
The «note» you refer to goes: «Note: LOTI provides a more realistic representation
of the global mean trends than dTs below; it slightly underestimates warming or cooling trends, since the much larger heat
capacity of water compared to air causes a slower and diminished reaction to changes; dTs on the other hand overestimates trends, since it disregards most
of the dampening effects
of the oceans that cover about two thirds
of the earth's
surface.»
We also know that a purely radiative response is not the way our climate reacts, mainly because
of the presence
of liquid
water on the
surface and its
capacity to vaporize, and also because
of instabilities that can lead to convective adjustments.