Digital signal processing technology was used to analyze daily carbon dioxide data from NOAA’s Global Monitoring Laboratory. The period surrounding the 1991 eruption of the Pinatubo volcano was rigorously analyzed for slope and acceleration of net global average atmospheric CO2 concentration and found to be consistent with the theory that Henry’s Law, the Law of Mass Action, and Le Chatelier’s principle control net global average atmospheric CO2 concentration rather than human-produced CO2 emissions. Background and theory are explained. A method of using common physics and math for a novel purpose is presented to compare natural CO2 emission or absorption with human-produced CO2 emission. The claim that human-produced CO2 emission is causing increasing global CO2 concentration and climate change is shown to be without scientific merit.
Key words: carbon, CO2, climate, warming, Impulse, Pinatubo, Henry’s Law, Mauna LoaGlossary
William Henry tested and documented his series of experiments on different gas and liquid combinations under various conditions which were published in 1803. (Henry, 1803) Today, the coefficients he developed are now available in tables in reference books and software which are used routinely by chemists and chemical engineers. This stable science is known today as Henry’s Law and is a foundation science for several large industries. Though it is not common knowledge among the public and only rarely found in climatology literature, Henry’s Law is the foundation science for the multi-billion dollar per year scientific instrumentation industry of gas chromatography, which is one of the methods used to measure atmospheric gases and most chemicals. It is also a foundation science underlying chemical engineering in gas, oil and coal refining and the beer and carbonated beverage industries. Also, it is one of the major variables in the absorption and emission exchanges of oxygen and carbon dioxide and other gases in the lungs and gills of all animals.
The event and its causes and effects are the subjects of many studies, for example, Stenchikov (2021).
An excerpt from Science News at the time from Hoppe (1992):
Ellsworth G. Dutton, a meteorologist with NOAA’s Climate Monitoring and Diagnostics Laboratory in Boulder, Colo., traced the effects of Pinatubo’s cloud with ground-based instruments that directly measure the strength of sunlight. Dutton says his results show a 20 to 30 percent decline in the amount of solar radiation that reaches the ground without being scattered or reflected, and a 2 to 4 percent decline in total solar radiation.
Temperatures have already started to drop, both at ground level and in the lower atmosphere, says James K. Angell of NOAA in Silver Spring, Md. Angell told Science News his analyses of weather balloon data show that the first half of 1992 was 0.4 [degrees] C cooler, overall, than the first half of 1991. He notes that the volcano’s effect may be greater than suggested by these observed temperature shifts, since this year’s El Nino warming would normally raise average temperatures by 0.2 [degrees] C (SN: 1/18/92, p.37).
Weather satellites confirm cooling in the lower atmosphere, recording a global drop of more than 0.5 [degrees[ C since last June, with this June being 0.2 [degrees] C cooler than average, according to John Christy of the University of Alabama at Huntsville and Roy Spencer of NASA’s Earth Science Lab at the Marshall Space Flight Center in Huntsville. Christy says their data indicate that the greatest cooling, 1.0 [degrees] C, occurred in the northern midlatitudes — an area that includes the continental United States — while temperatures in the southern hemisphere have dropped by only 0.3 [degrees] C.
Pinatubo was the largest or second largest volcanic explosion observed on Earth in the last 100 years. The explosion resulted in a belt of clouds, dust, various gases, and particles encircling and spreading in the atmosphere around Earth’s tropical zone, which is about 20 degrees latitude both north and south of the equator. In this large zone, ocean surface temperature averages 25 degrees C (77 degrees F) year-round, in contrast to average ocean temperature of 17 degrees C.
On average, ocean surface above 25 degrees C is a net emitter of CO2 gas, day and night, year-round. That is, more CO2 is being released from ocean surface than is absorbed from among the CO2 molecules which are continuously colliding with ocean surface. The belt of clouds, gases, and particles, etc., encircling the tropics is assumed by all known reports to have reduced short wave solar insolation reaching the surface; incoming sun light around 400 to 700 nanometer wavelength was shaded, blocked, absorbed, reflected, scattered, or otherwise obfuscated. Consequently, tropical ocean surface cooled. Higher latitude ocean surface cooled also.
Short wave infrared radiation from the sun is not absorbed by CO2. It is absorbed by ocean, soil, and biosphere.
Our theory is that Henry’s Law controls net global average atmospheric CO2 concentration and human CO2 emission from all sources only temporarily perturbs net global average atmospheric CO2 concentration and its rate of change. There are knowledgeable groups of scientists, such as chemists, analytical chemists, and chemical engineers, as well as individual scientists in other fields who support this theory. But this theory is rarely studied or found in climate literature and rarely funded in government environmental work. Generally, papers concerning Henry’s Law and climate are found only in less well-known journals.
Henry’s Law is a reproducible, well-documented law of chemistry and physics which defines the ratio of any gas in contact with any liquid. Each gas and liquid combination has a specific Henry’s Law coefficient, denoted kH. The coefficient is not a constant; kH varies with temperature at the gas – liquid interchange surface. The coefficient varies with (a) temperature of the surface (b) salinity of the liquid including certain minerals which are dissolved in the liquid not only sodium chloride, (c) alkalinity or pH or the liquid, (d) partial pressure of the gas in the space above the liquid and (e) partial pressure of the gas in the liquid. Concentration of CO2 gas in seawater is inversely proportional to sea surface temperature. High diligence is needed in sampling procedures to control (a), (b), (c), (d) and (e).
Henry’s Law has limitations on its application.
1. Henry’s Law only applies when the concentration of the unreacted gas in the liquid is minor and when the concentration of gas being measured in the gas volume above the liquid (i.e., its partial pressure) is minor relative to the other gases in the volume. An oversaturation condition is observed in chromatography by an abnormal, non-Gaussian peak shape. Henry’s Law is applicable to CO2 gas since it is a trace gas in both the atmosphere and in the ocean even at 10 times current concentrations.
2. Henry’s Law only applies to the gas in the liquid which has not reacted with the liquid; that is, Henry’s Law only applies to the reversible phase-state equilibrium reaction [CO2(gas)] <-> aqueous [CO2(gas)]. Henry’s Law does not apply to ionized CO2 gas, that is, hydrated CO2, nor to any of the carbonate or bicarbonate ions or un-ionized carbonic acid that are products of aqueous CO2 gas reacting with water known collectively as dissolved inorganic carbon (DIC).
The total concentration of dissolved inorganic carbon from Cohen and Happer (2021):
[C] = [CO2] + [HCO− 3] + [CO2− 3]
Most of the CO2 in seawater is in DIC form, which, according to most sources, is on the order of 38,000 gigatonnes (Gt) of DIC dissolved or reacted in deep seawater. Meanwhile 1000 Gt is in surface seawater and 850 Gt is in air (One Gt is 1000 billion kilograms, that is, 1 followed by 12 zeros). Figure 2 below (Cohen & Happer, 2021) illustrates the relative molar stoichiometric concentrations of the DIC species in ocean corresponding to atmospheric CO2 concentration. Barely visible, the fine dotted green line slightly above the horizontal axis is increasing. The concentration of the CO2 species of DIC in ocean and the concentration of the bicarbonate species in ocean are both increasing as atmospheric CO2 concentration increases. Simultaneously, the carbonate ion [CO2− 3] of carbonic acid is decreasing, along with alleged problems of so-called “ocean acidification”.
As we demonstrate in this paper, CO2 gas is rapidly absorbed into sea surface when the surface cools. Ocean surface demonstrates the capacity to rapidly absorb orders of magnitude more CO2 than humans produce, and then recover to trend. It is imperative to recognize that these reactions of ionized CO2 (DIC) are rapidly reversible reactions. We do not rely on estimates of models of CO2 in air and seawater to demonstrate this point.
Most CO2 in seawater is in the ionized form HCO3– known as bicarbonate as shown above in figure 2 (Cohen & Happer, 2021). Minor changes in ocean surface temperature reverse the CO2 hydration reaction and aqueous CO2 gas is formed. Aqueous CO2(gas) <-> H+ + HCO3–. Colder water pushes this reaction to the right, to products. Warmer water pushes the reaction to the left, to reactants. Once in its aqueous CO2 gas form, then Henry’s Law dynamic equilibrium applies: for a given seawater surface temperature, there is a fixed ratio of CO2 gas concentration in air versus CO2 gas concentration in seawater surface which is in contact with the air. Depending on changes in surface conditions, aqueous CO2 gas could react with H2O to become H2CO3 (carbonic acid), or it could react with H2O to become HCO3– (bicarbonate) plus hydrogen ion (hydronium), or it could remain in the water matrix as aqueous CO2 gas, or it could be emitted to the atmosphere as CO2 gas.
Cohen and Happer (2021) point out that transition of only a single proton (a hydrogen ion), determines bicarbonate versus carbonic acid species. The various DIC species are surrounded in the seawater matrix by hydrogen ions and hydroxide ions. CO2 gas molecules and DIC ions are not required to move in the seawater matrix. Both bicarbonate ion and carbonic acid are separate reaction products of the aqueous CO2 gas hydration reaction with H2O, as well as reversible with each other, as shown in the next graphic. In seawater surface these reactions can reverse in seconds due to changing surface temperature, or agitation by waves, buoys and moving ships, or a sampling procedure, or by an upwelling water current dense with DIC (e.g., an El Nino current). As upwelling seawater dense with DIC comes to the surface, it warms, and aqueous CO2 gas in the surface becomes oversaturated, out of balance with the Henry’s Law ratio for the temperature at the surface, resulting in CO2 gas being emitted to the air and a rebalancing the Henry’s Law dynamic equilibrium for that temperature.
Daniel Mazza explains Reversible Reactions of Higher Order (Mazza, 2020, pp16-17):
At any given temperature, the value of Keq remains constant no matter whether you start with A and B, or C and D, and regardless of the proportions in which they are mixed. Keq varies with temperature because k1, and k2 vary with temperature, but not by exactly the same amount.
… the general formulation of the law of mass action (Guldberg-Waage, 1864) that states: in a chemical system at equilibrium and constant temperature, the ratio between the product of the concentrations of chemicals formed (each elevated to its stoichiometric coefficient) and that of the reagents is a constant value.
The reactants and products of the carbonate chemistry in seawater are difficult to sample and quantify with precision because the reactions are so rapid and only very minor changes in surface conditions are required to change the dynamic equilibrium. Taking a sample affects the reactions. Special methods and systems must be used for these analyses at the thin layer at ocean surface. Journal and online articles report years or hundreds of years are required to move large amounts of CO2, allegedly because migration of CO2 vertically or horizontally in the water matrix is slow. There are such slow changes, with El Ninos and La Ninas being prime examples. However, simultaneously, second by second, bulk CO2 gas is continuously in flux into and out of millions of square kilometers of ocean surface, driven by SST change and CO2 is converting in seconds from one ionic species to another and aqueous CO2 gas is either released to air or hydrated to carbonic acid or bicarbonate. Slower or continuous changes such as human emissions are anomalous perturbations to the trend of the dynamic equilibrium for the local surface temperature. Adding or subtracting CO2 from any source or for any residence time or emission rate does not change the Henry’s ratio for a given temperature.
Demonstrating an example of this bulk sea surface reaction and its enormous quantity and rate in the natural environment as observed in the Mauna Loa data is a primary objective of this study.
The cyclical hydration reaction of aqueous CO2 gas with H2O is described in the following graphic:
Changes in kinetics force the reactions forward or backward, changes in kinetics are changes in motion of molecules. Those kinetic changes result from heating, cooling or agitation of the sea surface by waves, ships underway and buoy motion, currents, storms, gas and water sampling procedures, etc. For example, warm tropical sea surface that is normally continuously emitting CO2 gas can be depleted of CO2 gas by wind, storms, hurricanes, typhoons, etc. such that the undersaturated sea surface is absorbing CO2 from air instead of emitting. Significant sampling problems in actual sea water include CO2 gas added or subtracted by the biology – living and dead – in the sea, currents of CO2 dense seawater upwelling from deep ocean to the surface, and sampling sea surface when the necessary representative sample is only the top centimeter or less thin layer.
Simultaneously with the portion of the carbonate chemistry described above, calcium ions (Ca2+), which are readily available in seawater in great excess to carbon, react with bicarbonate ions (HCO3–) producing calcium carbonate (CaCO3). This reaction is not included in the Henry’s Law equilibrium, and not included in the estimated 38,000 Gt of DIC, and not included in the estimated 1000 Gt of DIC in sea surface, although it is accumulated inversely proportional to temperature into the largest CO2 sink by orders of magnitude. Richard E. Zeebe and Dieter A. Wolf-Gladrow remind us, aqueous CO2 gas as well as solid precipitant calcium carbonate are produced, “at surface water conditions… counterintuitively.. during CaCO3 precipitation CO2 is liberated…by only ~0.03 µmol per µmol CaCO3 precipitated.” (Zeebe & Wolf-Gladrow) The famous white cliffs of Dover and Sussex, England, limestone caves around the world, the famous marble quarries of Italy are examples of enormous CaCO3 deposits. Ultimately, when aqueous CO2 is oversaturated with respect to the Henry’s ratio, the Law of Mass Action requires the DIC and Ca2+ reactions to move to the right, towards products; thus excess CO2 is converted to one of the forms of calcium carbonate. The calcium carbonate precipitates as solid particles which sink in the ocean water column, removing it from the surface layer. The calcium reaction is another source of CO2 in sea water while at the same time it removes bicarbonate.
Ca2+ + 2HCO3– -> CaCO3 + CO2 + H2O
CO2 gas dissolved in ocean surface is estimated to be 30 to 40 times more concentrated than in air, results from multiple reactions, yet still a minor component of sea surface water. But, these estimates of CO2 in ocean surface include ocean surface that is many meters deep. In this report, we are concerned with the CO2 in the thin layer at the sea-air interface. This report and project do not rely on estimates of CO2 concentration. Demonstrating measurements of CO2 absorption and emission and their rates in comparison to human emissions is the purpose of this project.
Additional background on Henry’s Law and the carbonate chemistry is found in, for example, Cohen and Happer (2021), Stallinga and Khmelinskii (2018), Stallinga (2018), Harde (2019), Zeebe and Wolf-Gladrow, and Mazza (2020).
Our theory assumes net global atmospheric CO2 concentration is in a dynamic equilibrium that is constantly re-balancing CO2 concentration between atmosphere and ocean surface, a re-balancing based primarily on the change in relative surface area of Earth above or below 25 degrees C. Flux is not the same as flow or flow rate. Flux is the mass of material flowing through a surface per time interval. Sea surface temperature (SST) and surface area at SST must be used to calculate CO2 flux. Average ocean and or air temperatures and average SST result in incorrect Henry’s law equilibrium conditions. The Henry’s Law phase-state reaction is a two-phase dynamic equilibrium, it is never a static equilibrium.
CO2 gas is always being emitted from ocean surface and always being absorbed into ocean surface. Collision of CO2 gas molecules never stop colliding with ocean surface, resulting in increased kinetic energy in ocean surface followed by emission of CO2 gas from the surface. Many factors affect ocean surface temperature in addition to insolation; a topic well beyond the scope of this paper. In higher latitudes, millions of square kilometers of ocean surface are usually at 17 degrees C or less year round, and in this area of ocean surface net absorption of CO2 gas exceeds net emission year round. At the same time, millions of square kilometers of tropical ocean are generally above 25.6 degrees C year round, and in this area of ocean surface net emission of CO2 gas exceeds absorption year round. This clearly implies that the Henry’s Law dynamic equilibrium concentrations, rates and net flux are functions of surface area and surface temperature of those areas.
In the following graphic, we see that CO2 concentration changes rapidly follow changes in sea surface temperature. Changes up and down in the blue line (representing rate of change of sea surface temperature) are followed by changes in rate of CO2 change per month at the Earth Monitoring Laboratory, a joint operation of the U.S. government’s National Ocean and Atmospheric Administration and Scripps Oceanography Institute on Mauna Loa (MLO). CO2 concentration changes rapidly in response to changes in sea surface temperature. The response occurs in months.
The first phase of this study sought to determine if we could detect, in the “gold standard” data for global CO2 concentration, an inflection point in the slope of the daily CO2 concentration measurements before, during or after a single major climate event, the explosive volcanic eruption of Pinatubo on the island of Luzon in the Philippines in June 1991. Proprietary software for digital signal processing was used to analyze the publicly available daily CO2 concentration data reported by MLO. We defined an inflection point as a change in sign of the slope of CO2 concentration after the eruption of Pinatubo. Hypothetically, if we are able to detect these inflection points with statistical confidence, then, to support our theory, we can use the same data set and software to produce evidence from many different climate, weather and environmental events and a global CO2 calibration curve. We would be able to measure changes in CO2 concentration which resulted from other volcanoes, El Ninos, La Ninas, storms, human CO2 emissions, and other events which reportedly affect net global average atmospheric CO2 concentration. In a sense, we are iterating William Henry’s experiments for CO2 gas and water at the global scale with various climate and environmental conditions but using only measured global data. Instead of unreliable computer climate models with too many estimates and theories, we would have data experiments using empirical data from the natural environment to correct the pervasive misunderstanding of CO2 which is curated in popular culture and education.
The MLO data was selected because it is widely recognized and reported to be the gold standard reference measurement for net global average atmospheric CO2 gas concentration. The lab is located about 11,000 feet above sea level on the northwest facing flank of Mauna Loa volcano on Hawaii island, the Big Island of Hawaii. This data set was selected because it is accessible to the public and it has been diligently measured and curated since the 1970s. We selected their set of daily CO2 measurements. The data are reported in micromoles of CO2 gas per mole of dry air, which is equal to parts per million (ppm) CO2 in dry air. We are grateful to the MLO scientists, authors and administration for making these data available to the public (See acknowledgments and Thoning et al (2021) reference for details and access to the data).
The software toolset for this initial phase of the study was designed and operated by Shahar Ben-Menahem, PhD (physics, Stanford) and Abraham Ishihara, PhD (Aeronautics & Astronautics, Stanford) through their company Modoc Analytics LLC under contract with EnergyCite (https://energycite.com/) and its sister company ClimateCite (https://climatecite.com/)
Using these software tools, if these data were found to be responsive to a geographically remote event such as Pinatubo, then potentially it would not be necessary to examine many different CO2 data sets nor to employ laboratories to validate our theory. Instead of relying on theory, we would have measured, empirical evidence that CO2 concentration is controlled by nature. Our theory assumes sea surface temperature (SST) directly affects the ratio of atmospheric CO2 gas concentration versus CO2 gas concentration in sea surface, following Henry’s Law, while human CO2 has no effect on that ratio.
Care must be taken with Henry’s Law since it can be expressed in many forms for different uses. Here we use its dimensionless form. The Henry’s Law coefficient kH = c(aqueous)/c(gas) where c is concentration in moles. For example, 400 micromoles of CO2 per mole of air (which is 400 ppm CO2 concentration in air) is in equilibrium with 333 micromoles of CO2 per mole of seawater in sea surface at 298 K and a solution density of 997 kg/m3. Dimensionless kH = 0.8317 (Sander, 2015). Concentration of CO2 in seawater is directly proportion to depth due to higher density (kg/m3) and inversely proportional to temperature.
If this first phase data experiment worked, then the overall scientific complexity, effort, and expense of our project would be greatly reduced. The most difficult data experiment was done first: could we detect the Pinatubo perturbation in the MLO data?
We calculate a not-to-exceed amount of human-produced CO2 based on measured data rather than assuming estimates of human-produced CO2 based on estimates of fossil fuel production and cement production from spurious and dubious sources. This is not to doubt the diligent and careful curation of the data by Oakridge National Laboratories, for example. But the data they are handed comes from some sources which have been dubious over the years, for example Soviet Union, Nigeria, Iran, Venezuela, OPEC, to mention a few major oil producers.
This first phase of our project analyzed daily CO2 data from MLO to determine if the changes in CO2 due to the Pinatubo eruption were measurable in the data. Is the data set responsive to remote events? Could the software and skills of our scientists detect a reduction in the CO2 concentration and an inflection point in rate of change of concentration due to cooling of tropical ocean surface by the Pinatubo cloud belt. Velocity and acceleration of net global average CO2 concentration were calculated based on measurements.
The raw daily MLO data (as raw as available publicly) from the 1970s through 2020 was used as input for our sequence of algorithms. This “raw” time-series data set was only changed by us to fill in days with missing data.
Data for days for which no real CO2 data were available from MLO, marked as 999 in the MLO data file, but for which data were available for days both preceding and following the block of missing-data day(s), were interpolated accordingly.
Data for days (at the beginning of the recording period — early 1970s) for which no real data were available and no earlier data with valid data were available — were replaced by constant nominal values in the low 300s. This block of data is limited to the early 1970s and does not affect our Pinatubo results.
The following mathematical procedures (as summarized by boxes in the block diagram) are then applied to this “raw CO2 level data” time series wherein time is given in fractional Gregorian years and CO2 levels are given in ppm.
A JTFA (“Joint Time Frequency Analysis”) is performed. Those skilled in the art of time-series digital signal processing (DSP) will recognize that this term refers to a class of methods, wherein a quantity-vs-time series is analyzed for its frequency content (such as PSD = Power Spectrum Density) as a function of time. While there are many JTFA techniques, the simplest one is performing a Fast Fourier Transform analysis (FFT) in a moving (“swept”) time window and computing the complex FFT coefficients as a function of both window start-time and in-window frequency index. This type of JTFA transformation, however, is not easily invertible.
One of the simplest sub-classes of JTFA methods which is easily invertible, is the Gabor Transform. The Ben-Menahem- Ishihara proprietary analysis method used in this investigation was based on combining the Gabor Transform and FFT.
In the quantity-vs- time-frequency analyzes raw data result of our JTFA, we then remove the seasonal (1-year period) frequency-band peak via a notch filter, and also suppress the high-frequency band (“low-pass filtering”). Those skilled in the art of DSP or analog filtering in electrical engineering and other branches of physics-based engineering will readily recognize these terms and techniques.
After the notch- and low-pass filtering of the JTFA-produced data — represented by the relevant boxes in the Block Diagram — the filtered JTFA transform is then inverted. This computation yields the output (lower-left) box of the Block Diagram — the processed CO2 vs. time signal (and its time derivative).
Then with these data we introduce a proven and well-known math and physics calculation to compare natural CO2 absorption into the environment with human emissions. The calculation is used thousands of times each day to make decisions which mean life or death to a few million people each day.
The graph above is plotted over the entire Mauna Loa recording epoch (circa 5 decades) with both the “raw” (as defined above) and processed (as defined above) CO2 levels, vs. time. The graph appears very similar to the graphs typically produced by NOAA which appear frequently in media, education, politics and online.
The graph above is processed as in the previous graph and described in the method section above but simply zoomed in to cover only the Pinatubo decade: 1990-2000. The slope of the red line is visibly bending or flattening in July of 1991 into 1994, and then in 1995 the slope turns upward again.
The data in the graph above is again processed as the previous two graphs but here zoomed in to the year of Pinatubo plus the year before and after Pinatubo. The slope (grey line) is slightly bending or flattening after mid-year 1991 when the Pinatubo eruption occurred. Velocity of CO2 concentration is slowing after mid-year 1991.
No inflection point in the slope of CO2 concentration was found in the period following the Pinatubo eruption. Slope declined slightly from prior trend but did not turn negative. Large changes in acceleration were detected. In this case, acceleration is the rate of change of slope, or the time derivative of CO2 ppm per year.
The graph above plots the time derivative of the processed CO2 ppm/year.
The above plot is the time derivative of the processed CO2 ppm/year. The estimated “would-be inflection” times bracket the detected “Pinatubo Event” as indicated by arrows and DD/MM/YY date markers. The bracket dates are the points of fastest decline (deceleration) of slope and the fastest increase (acceleration) of slope. On this plot, the mean baseline pre- and post-Pinatubo CO2 slope are indicated as horizontal lines; the full time period of the Mauna Loa data before or after the “would-be inflection” times were used to calculate the means, 1970s to 2020. The points of minimum and maximum acceleration are used to determine respectively the end point of the pre-Pinatubo mean and the start point of the post-Pinatubo mean. These two points allow assignment of the points where offset is calculated. This offset (or over-recovery) is expected based on Le Chatelier’s Principle, basically stated, a perturbed trend will rapidly return to its equilibrium condition plus an offset amount or overcorrection.
Now we have a reliable method based on gold standard measurements of a single climate variable, i.e. CO2 concentration, which we can use to compare human-produced-CO2 emissions with changes in net global average atmospheric CO2 concentration.
The trace gas CO2 is produced, modified, and absorbed through many and varied natural processes in the environment. Documenting and quantifying all of these with accuracy and precision into a so-called carbon budget or energy balance is a quixotic task and approximate at best, yet that is what the public through their governments are paying for in elaborate projects, for example, annually documenting Earth’s carbon balance in over 100 pages by dozens of authors, e.g., Friedlingstein (2021), not to mention United Nations Intergovernmental Panel on Climate Change (IPCC) climate conferences around the world and their thick document and public relations campaigns. It is a climate modeler’s dream project with no end date and expanding budgets. These reports use too many estimates in too many models, not measurements of human-produced CO2.
Meanwhile, net global average atmospheric CO2 concentration is routinely and diligently measured in micromoles per mole (which is equal to parts per million or ppm) of atmosphere at Mauna Loa and a few other locations. It has been observed by many scientists that net global average atmospheric CO2 emissions vary with temperature. In contrast, the common misunderstanding is that temperature varies with CO2 concentration and global temperature is increasing because human-produced CO2 is increasing. While confirming that atmospheric CO2 gas contributes to Earth’s temperature, atmospheric physicist, Professor Murry Salby, PhD has educated us that CO2 varies coherently with temperature change, following temperature change.
“An increase of TS [surface temperature] introduced by a radiative perturbation dF [dF is the direct radiative forcing] thus leads to an increased emission rate of CO2, and, hence, cumulatively in CO2.” …”Increased temperature increases net emission of CO2. Decreased temperature has the reverse effect. It is noteworthy that the positive sensitivity to temperature, drCO2/dT is not restricted to small perturbations. As is evident in Fig. 1.43, the dependence on temperature applies to rCO2 as large as 100%. Also noteworthy is that the correspondence applies to changes of temperature that are clearly of different origin. Following the eruption of Pinatubo, when SW [shortwave radiation emitted by the sun] heating decreased, rCO2 decreased by more than 50%. During the 1997-1998 El Nino, when SST increased, rCO2 increased by more than 100%. To maintain stability, there must exist a negative feedback in CO2, one that is sufficiently strong to bridle the enhancement of CO2 emission by positive feedback from temperature. That negative feedback involves sinks of CO2 at Earth’s surface.”
Net emission rate of CO2, rCO2 = d/dt rCO2 (ppmv/yr)
As seen in the NOAA graph at the end of the introduction above, the time derivative of CO2 concentration follows quickly in months the time derivative of sea surface temperature (SST).
The link between sea surface temperature and CO2 concentration also has been noted by government scientists. For example: “At Mauna Loa the results implied that for the period 1970-1985, the season-to-season change would be about 0.2 ppm higher for a +1 degree C deviation in temperature of the eastern equatorial Pacific. A slightly lower figured 0.15 ppm/degree C was found at the south pole for the full record length and about 0.35 ppm/degree C at Barrow (Alaska) for the full record.”…“For the cumulative dCO2 we found a 1 degree C deviation would produce about 0.4 ppm change at Mauna Loa, 0.3 ppm change at the south pole, and 0.8 ppm at Barrow, Alaska.” (Elliott & Angell, 1986).
And “…we found as have others, that warming of this region is usually followed by an above average increase in CO2 concentration.” …” At Mauna Loa this increase follows SST by about one season and at the south pole by two seasons.” Unfortunately, these scientists usually do not pursue the linkage to its cause but instead, as these scientists did, the linkage or cause are dismissed. They concluded, “We take these results as further confirmation that the apparent effect of SST on the CO2 record comes less from changes in the equatorial eastern Pacific than from climate changes throughout the globe.” (Elliott et al., 1990).
Anthropogenic CO2 is widely believed to be responsible for the trend of increasing net global average atmospheric CO2 concentration, and from that belief it is inferred global temperature is increasing, some claim dangerously. Proponents of anthropogenic CO2-caused global warming (AGW) believe that reducing human CO2 emissions by stopping the use of fossil fuels will reduce net global average atmospheric CO2 concentration and thereby reduce global temperature. The need to reduce global temperature is an unproven assumption as is the need to reduce human-produced CO2. Those assumptions are based on computer models where only a few types of data are measurements. Comprehensive climate models have not been able to be validated against real world measured conditions. For example, “The inability of current models to estimate accurately oceanic uptake of CO2 creates one of the key uncertainties in predictions of atmospheric CO2 increases and climate responses over the next 100 to 200 years. 60 references.” (Peng, 1987).
Climate scientists who support alleged human-caused global warming, for example Ben Santer and Michael Mann with others, authored a peer reviewed paper in the journal Nature Geoscience which acknowledges that their climate models are wrong, although their admission is hidden in technical jargon. They say in the first sentence of their paper’s abstract, “In the early twenty-first century, satellite-derived tropospheric warming trends were generally smaller than trends estimated from a large multi-model ensemble.” (Santer, 2017). In other words, the actual temperature trends were less than their modeled trends. They continued, “Over most of the early twenty-first century, however, MODEL tropospheric warming is substantially larger than OBSERVED.” (Santer, 2017). (Capital letters are added for emphasis). In other words, their computer models substantially overestimate the global warming alleged to occur in the real world.
In contrast, the present study, based on measurements not models, simple in scope, analyzed a 2-year period where the rate of increase in slope of net global average atmospheric CO2 concentration slowed and then stopped momentarily. The acceleration of CO2 concentration was temporarily halted by the effects of the Pinatubo volcanic eruption. During those same months, CO2 emissions from human sources continued, CO2 emissions from natural sources continued (such as rotting soil and biosphere, etc.), the Pinatubo volcano itself added large amounts of CO2 gas to the atmosphere, and an El Nino event in 1991-1992 added CO2 to the atmosphere. According to the results of this study, the second derivative (i.e., the acceleration) of CO2 concentration dropped precipitously in the 2 years following Pinatubo to its lowest point in the pre-Pinatubo Mauna Loa record, despite the CO2 additions by humans, natural sources, a volcano and an El Nino. Nature rapidly absorbed the added CO2 and then more rapidly accelerated again to reset its CO2 concentration to trend.
The Law of Mass Action states that the rate of a chemical reaction is directly proportional to the concentrations of the reactants, applicable under any circumstances. In this case, the chemical reaction is the Henry’s Law phase-state equilibrium reaction of CO2 occurring in millions of square kilometers of tropical seawater surface cooled by the effects of the Pinatubo eruption.
To give the amounts of CO2 perspective, Earth’s “…forests provide a “carbon sink” that absorbs a net 7.6 billion metric tonnes of CO2 per year…” (World Resources Institute, 2021). Cooler surface in the two years following Pinatubo absorbed net 2778 billion metric tons of CO2, and then in the next two years emitted that amount plus an additional increment.
The rate of change of the slope of net global average atmospheric CO2 concentration in this analysis dropped momentarily below zero. CO2 concentration decelerated rapidly and briefly stopped growing. A large, global scale, decrease in CO2 emission is consistent with an oceanic source of CO2 and the rapid rate of change of slope is consistent with estimates of the size of absorption and emission fluxes of CO2 gas from ocean and no where else. By elimination, there is no other known, logical or physically possible sink for such a large amount of CO2 to be absorbed so rapidly other than ocean surface. The Henry’s global CO2 dynamic equilibrium ratio was abruptly perturbed by cooling SST. CO2 emissions decreased precipitously after millions of square kilometers of tropical ocean surface cooled. Millions of square kilometers of ocean and land surface in higher latitudes also cooled. For a period of about 2 years, the rate of CO2 absorptions into the environment greatly exceeded the rate of CO2 emissions from all sources. The rate of change of CO2 concentration (i.e., the slope of CO2 concentration) had been on average 1.4 ppm per year since mid-1970s. For a period of about 2 years, that slope decelerated and briefly reached below zero even though human emissions were continuing as usual, and the Pinatubo eruption had added large amounts of CO2 to the atmosphere, and Earth’s biosphere was continuing to emit CO2 as usual, and a El Nino event was adding CO2 to the air.
The decrease in CO2 slope after 1991 followed by its recovery are clearly seen in the graph above. This NOAA/Scripps graph is CO2 slope versus time, i.e. ppm per year or velocity of net global average CO2 atmospheric concentration. 1 ppm is 7.76 Gt of CO2.
Examining closely the NOAA/Scripps graph immediately above. A slight decrease or flattening is visible after 1991. This graph is CO2 concentration versus time.
In addition to the CO2 added to the atmosphere by Pinatubo, and the continuing CO2 emissions by humans from all sources, and the continuing natural emissions of CO2 by the biosphere, there was an El Nino event in 1991-1992. El Nino events add large amounts of CO2 to the atmosphere. “The equatorial Pacific is the largest oceanic source of carbon dioxide to the atmosphere and has been proposed to be a major site of organic carbon export to the deep sea… The data establish El Nino events as the main source of interannual variability.” (Murray, 1994). The historical series of El Nino and La Nina perturbations are beyond the scope of this document, but we hope these major CO2 and temperature perturbations can be examined in the next phases of this study.
During the period 1990 to 1995, as mentioned, there were major additions of CO2 to the atmosphere. We did not attempt to disentangle and quantify these additions. Yet our analysis revealed in MLO data a decrease in the slope of CO2 concentration and a sharp temporary deceleration in CO2 concentration. This begs the question: where did all of that CO2 go? After about 2 years of deceleration, and a temporary halt in CO2 growth concurrent with ongoing human and large unusual but natural CO2 additions, this rapid deceleration and halt was followed by an even more acceleration and recovery beyond the average rate of change of CO2 concentration for the pre-Pinatubo decades.
Where did that CO2 go? Where did that recovery CO2 come from? It was and is in the ocean. And it was there and is there in enormous quantity, as will be illustrated next.
We studied the period of the Pinatubo perturbation. A natural perturbation to the diligently measured approximate 20-year trend of CO2 concentration occurred. This Pinatubo perturbation period is an example, in both size and rates, of the capacity of the natural environment to emit and absorb CO2. Human-CO2 emissions are also a perturbation to the same net global average CO2 concentration trend, but tiny by comparison to Pinatubo’s perturbation.
The CO2 absorbed was over two orders of magnitude larger (over 100 times larger) than the perturbation due to human CO2 emissions in the same period, as we will now show. The rate of change (also known as slope, or velocity) of net global average CO2 concentration averaged 1.463 ppm per year prior to Pinatubo. After Pinatubo, the rate of change of concentration slowed. But the rate of change of the rate of change of CO2 concentration declined very sharply. In other words, CO2 slope decelerated to zero rate of change of slope. The growth of CO2 concentration stopped and declined momentarily. By analogy, you did only ease off the gas pedal on the car after previously you were previously pushing down on the gas, accelerating to increase velocity, you took your foot off the gas and stepped down hard on the brake. Then, after reaching zero, for the next 2 years Earth accelerated rapidly, more rapidly than it had decelerated, to an average rate of change of concentration (i.e., average slope for the post Pinatubo period from 1995 to 2020) of 2.087 ppm per year. This remarkable recovery to trend with an offset above previous trend, that is an over recovery, is expected from Le Chatelier’s principle.
Rather than estimate natural and human emissions based on computer modeling, carbon budgets and proxy data from pre-industrial times, and dubious fossil fuel data sources, we will compare CO2 measured diligently by the Mauna Loa laboratory.
On June 15, 1991, net global average CO2 atmospheric concentration (Mauna Loa data) was 358 ppm.
One ppm equals 7.76 gigatons (Gt) of CO2.
358 ppm times 7.76 = 2778 Gt CO2.
(1 ppm CO2 = 2.12 Gt carbon. 2.12 Gt carbon times 3.66 tonnes CO2 per tonne carbon = 7.7592 Gt CO2.)
The specific impulse calculation can be used to compare forces in the environment.
Imagine a fully loaded 747 airplane with a mass of 2778 Gt on the runway ready to depart. How did the jet engine and aircraft designers and later the pilots know that the engines could produce enough force to accelerate the airplane to sufficient velocity to become airborne before the end of the runway? This calculation is the impulse calculation. It gives us a reliable, well known and trusted calculation to compare human-produced CO2 with natural CO2. Assume our 747 is rolling along at velocity of 1.4 miles/year and accelerating by additional rate of 0.73 miles for each additional year. That is denoted as a velocity (or speed) of 1.4 miles per year accelerating at 0.73 miles per year, or 1.4 miles/year + 0.73 miles/year/year. Then our 747 hits a bump in the runway and our 747 slows rapidly. The pilots must decide instantly. Can this plane take off before reaching the end of the runway? Shortly later, our 747 accelerates very rapidly. Does our 747 have enough force to accelerate to take-off velocity? How do the pilots (and their flight computer) know?
The United Nations, leaders of over 100 nations through decades of government administrations in those nations, politicians and bureaucrats, judges, leaders of major industries, universities, mainstream media, the Pope in Rome, scientists and engineers who should know better, have been working vigorously for at least 40 years to convince you that the 747 must stop, turn around and go back to the gate. They have been telling us, attempting to scare us and scaring children worldwide, with practically non-stop, very expensive propaganda using our money, government policies and laws that the 747 will crash, that it does not have enough power to take off, that the 747 named Earth is in an existential crisis, life and death crisis, some alarmist claim the planet is beyond the point of no-return. They blame the trace gas CO2 generated as a by-product of humans using fossil fuels.
We will now use the same calculation that pilots use thousands of times everyday to make life and death decisions, such as: can our airplane loaded with passengers, crew, baggage and fuel take off in time before reaching the end of the runway. This is known as the specific impulse calculation. The same physics and math used in the specific impulse calculation demonstrates that humans can not be responsible for global warming.
This study provides the values measured by MLO for the critical variables in the specific impulse calculations for CO2. The important variables are the same for both airplane and for CO2 concentration. We have the mass of the airplane and the (measured, not estimated) mass of CO2 in the air. And, we have the speed or velocity (or its rate of change of position) of the airplane, and we have the rate of change of CO2 concentration in the air (aka the speed or velocity of the CO2 concentration). And, we have the acceleration of the airplane (aka the rate of change of speed or velocity). And, we have the acceleration of the concentration of CO2 in air (aka the rate of change of the velocity of CO2 concentration). We will use these variables for the mass, velocity and acceleration of CO2 concentration in atmosphere during the time period following the Pinatubo eruption to calculate the specific impulse of Earth’s environment. Does Earth’s environment have enough force to absorb human-produced CO2 ? The mass of CO2 is calculated from the MLO ppm concentration on the day of the Pinatubo main eruption.
m = mass of net global average CO2 concentration in air = 2778 Gt CO2 in air, which is equal to 358 ppm CO2 in air (measured by MLO June 15, 1991.) That is 2778 billion metric tons of CO2.
dt is change in time = 2 years following Pinatubo eruption
a = acceleration
a = dv/dt Acceleration a is the change in velocity divided by the change in time
a = 1.463 ppm/yr divided by 2 years = 0.73 ppm per year per year.
F is force. F = m times a
F = 2778 Gt CO2 times 0.73 ppm/yr/yr = 2027.94 Newton-years.
A Newton is the unit of force in the International system of units (SI). It is represented by the symbol N. Sir Isaac Newton devised the three Laws of Motion. The impulse-momentum theorem is logically equivalent to Newton’s second law of motion. Impulse is the measure of force applied over time. Impulse is denominated by the symbol J. J is always directional one-way (i.e. a vector).
J = F times dt. Impulse J = force times change in time
J = 2028 Newtons * 2 years
J = 4056 Newton-years.
4056 Newton-years is the specific impulse of total CO2 in the atmosphere on the day before the Pinatubo eruption. This is the fully loaded 747 airplane ready to take off before starting the engines.
For comparison, let’s assume human CO2 was equal to 100% of the CO2 that was added to the atmosphere between 1990 and 1991, the year preceding the Pinatubo eruption. Calculating from MLO data, the measured average rate of change (or velocity) of net global atmospheric CO2 concentration for 1990 to 1991 was about 1.5 ppm per year. How much CO2 is that? Thus 1.5 ppm/yr times 7.76 Gt/ppm = 11.64 Gt of CO2. 11.64 Gt is the total change in CO2 concentration in the year 1990 to 1991; this amount exceeds maximum possible human emission because it includes net CO2 emissions from all sources and sinks of CO2, not only human emission, all CO2 emitted from ocean, land, biosphere including CO2 from the El Nino of 1991-1992. But for the purpose of our comparison here, we will attribute 100% of the that increase in CO2 to humans. Next, let’s also assume that 100% of the average velocity of CO2 concentration measured by MLO from the 1970s to Pinatubo in 1991 was entirely due to humans. Our scientists calculated that average velocity in the pre-Pinatubo dataset period from 1970s to 1991 was 1.463 ppm/year.
Repeating the specific impulse J calculation for maximum possible “human” CO2:
F = mass times acceleration
J = F times dt. Impulse J = force times change in time
11.64 Gt of “human” CO2 times 0.73 ppm/year/year acceleration times 2 years = an impulse J of 16.99 Newton-years.
About 17 Newtons-years is J, the maximum possible specific impulse due to “human”-produced CO2 that was added to the atmosphere during the 2-year Pinatubo deceleration period. It is the maximum amount impulse because we assume (for the purpose of this comparison only) that all of the CO2 increase from all sources since the 1970s is due to humans.
The result of this comparison is exculpatory evidence. We have 4056 Newton-years versus 17 Newton-years.
The environment, mostly ocean surface (since ocean is about 71% of Earth’s surface), demonstrated rapid CO2 absorbance capacity which is 239 times larger than maximum possible amount of net human emissions. We conclude that net human emissions are trivially minor, negligible, and absorbed and re-emitted along with the 239 times larger change in natural CO2. One 747 airliner has 239 times the impulse to take off than another 747. Which would you fly?
Recall that deceleration of net global average CO2 concentration dropped to near zero ppm/yr/yr. CO2 concentration, both natural and human, is cumulative over time. Impulse is cumulative over time. Thus, the impulse is suitable and logical for this comparative analysis. Integration of cumulative CO2 concentrations would also be a correct method for comparison, but the math is less well known. Airliners would not be taking off without the impulse calculation. When we attribute 100% of the changes in CO2 concentration to humans, the impulse due to “humans” is negligible, not enough to stop CO2’s rapid deceleration. The human-produced-CO2 climate change story does not fly.
The environment demonstrated a measured impulse to absorb 239 times the human-produced CO2 impulse when very conservatively calculated. Simply said, the natural environment is controlling CO2 concentration. Human CO2 emissions are not causing the increase in atmospheric CO2. The amount of human CO2 emissions is negligible, less than a rounding error, in Earth’s specific impulse to absorb and emit CO2 perturbations. And we do not yet know how large is Earth’s overall capacity; so far we have only calculated based on MLO measurements for the Pinatubo event. Henry’s Law, the Law of Mass Action and le Chatelier’s principle strongly suggest that net global average CO2 concentration such as measured by MLO is controlled primarily by sea surface temperatures. These temperatures are controlled by various natural forces. Since an amount greatly exceeding all possible human CO2 emissions was absorbed rapidly by the environment, then no net warming or net cooling can be attributed to human CO2 emissions. Our result suggests human CO2 emissions are a minor perturbation which is rapidly returned to trend.
Scientist P. Stallinga, PhD concluded, “The correlation between temperature and [CO2] is readily explained by another phenomenon, called Henry’s Law: The capacity of liquids to hold gases in solution is depending on temperature. When oceans heat up, the capacity decreases and the oceans thus release CO2 (and other gases) into the atmosphere. When we quantitatively analyze this phenomenon, we see that it perfectly fits the observations, without the need of any feedback . We thus now have an alternative hypothesis for the explanation of the observations presented by Al Gore. The greenhouse effect can be as good as rejected and Henry’s Law stays firmly standing. We concluded that the effect of anthropogenic CO2 on the climate is negligible and the effect of the ocean temperature on atmospheric [CO2] is exactly, both sign and magnitude, equal to that as expected on basis of Henry’s Law.” (Stallinga, 2018, Stallinga, 2020).
Where did the CO2 go after Pinatubo? It was absorbed into the oceans primarily, and less into soils and the biosphere. Our results strongly support the theory that the Henry’s Law dynamic equilibrium was adjusted downward due to the lower sea surface temperature, resulting in much less CO2 being emitted from the cooled tropical ocean, soils and biosphere; meanwhile, normally colder water in higher latitudes was even colder due to the Pinatubo effects; net absorption increased in these higher latitudes. Thus the CO2 slope declined and acceleration rapidly declined post-Pinatubo. Then, about 2 years after Pinatubo, when the cloud belt had partially dissipated and insolation of tropical oceans increased, then the deceleration of net global average atmospheric CO2 concentration reversed sign and even more rapidly recovered. Average slope following the recovery was a step higher than the pre-Pinatubo average. Professor Murry Salby provides calculations and graphs showing that the observed long-term slope of CO2 concentration is explained by a series of offsets such as Pinatubo and El Ninos. “There is no evidence of a systematic trend in temperature.” [referring to the actual mean global University of Alabama Huntsville’s satellite records for global anomalous temperature.] (Salby, 2018, beginning about 16:30 time mark in the video).
Concerning the Pinatubo perturbation, Stallinga and Khmelinskii (2018) write, “In total, the natural contribution is negative 50% of the anthropogenic emissions (i.e., a sink; Sabine, C.L. et al. estimate 48% ( Sabine, C.L. et al., 2014), plus fluctuations, with these fluctuations being of the same order of magnitude as the anthropogenic emissions… We have thus direct proof of Henry’s Law that predicts such effects of temperature on the carbon-dioxide content in the atmosphere. Oceans undeniably outgas and absorb CO2 from the atmosphere and they govern the dynamics, the correlation of [CO2] with temperature.” (Stallinga & Khmelinskii, 2018). In other words, human emissions are absorbed by nature.
Kauppinen and Malmi (2019) explain, “Low cloud cover controls practically the global temperature.” “The IPCC climate sensitivity is about one order of magnitude too high, because a strong negative feedback of the clouds is missing in climate models. If we pay attention to the fact that only a small part of the increased CO2 concentration is anthropogenic, we have to recognize that the anthropogenic climate change does not exist in practice. The major part of the extra CO2 is emitted from oceans , according to Henry‘s law. The low clouds practically control the global average temperature. During the last hundred years the temperature is increased about 0.1°C because of CO2. The human contribution was about 0.01°C.” (Kauppinen & Malmi, 2019).
Since the Pinatubo cloud belt around Earth’s equator mostly obfuscated insolation of normally warm tropical ocean surface, and since CO2 gas solubility in sea surface is inversely proportion to SST, we confidently deduce that the measured, rapid deceleration of CO2 concentration was caused by cooling of millions of square kilometers of tropical ocean surface. Our result and the novel use of the standard specific impulse calculation reveal a MLO-measured net CO2 gas absorption impulse more than 230 times larger than the MLO-measured maximum possible net human emission impulse during the same time period. We expect that continuing this study into its next phases will yield a matrix of supporting evidence and, possibly, a calibration curve for human-CO2 emissions, based on measurements rather than estimates, so that the pernicious claims of global climate change due to human-produced CO2 can be summarily dismissed. The argument that human-CO2 emission is causing global climate change is shown to have no scientific merit.Credits and Acknowledgements
Thoning et al (2021). K.W. Thoning, A.M. Crotwell, and J.W. Mund (2021), Atmospheric Carbon Dioxide Dry Air Mole Fractions from continuous measurements at Mauna Loa, Hawaii, Barrow, Alaska, American Samoa and South Pole. 1973-2020, Version 2021-08-09 National Oceanic and Atmospheric Administration (NOAA), Global Monitoring Laboratory (GML), Boulder, Colorado, USA https://doi.org/10.15138/yaf1-bk21
FTP path: ftp://aftp.cmdl.noaa.gov/data/greenhouse_gases/co2/in-situ/surface/
The software toolset for this initial phase of the study was designed and operated by Shahar Ben-Menahem, PhD (physics, Stanford) and Abraham Ishihara, PhD (Aeronautics & Astronautics, Stanford) through their company Modoc Analytics LLC.
This study, referred to by the scientific team, management, and ClimateCite Corporation as the “Pinatubo Study – phase I”, was entirely funded by Tomer Tamarkin, Carmichael, CA with the generous help and support of Pat Boone, Beverly Hills, CA. No financial solicitations were made to any other corporations, companies, or individuals, nor funds received. Intellectual work product and copyright, 2022, ClimateCite Corp.
Bud Bromley has no conflicts of interests which might affect the direction of this study or authoring this report. This report is also available here: https://budbromley.blog/2022/05/20/correcting-misinformation-on-atmospheric-carbon-dioxide/
An extensive glossary of names, terms, & scientific principles used in this paper may be found online at: https://pinatubostudy.com/glossary.html
Cohen, R., & Happer, W., (2021, November 21). Fundamentals of Ocean pH. CO2 Coalition.org. https://co2coalition.org/publications/fundamentals-of-ocean-ph/
Elliott, W.P., & Angell, J.K., (1987). On the relation between atmospheric C02 and equatorial sea-surface temperature. Tellus B: Chemical and Physical Meteorology, 39B, 171-183. https://www.tandfonline.com/doi/pdf/10.3402/tellusb.v39i1-2.15335
Elliott, W.P., Angell, J.K., & Thoning, K.W. (1990). Relation of atmospheric CO2 to tropical sea and air
temperatures and precipitation. Tellus 43B: Chemical and Physical Meteorology, 43:2, 144-155, : https://doi.org/10.3402/tellusb.v43i2.15259
Friedlingstein, P., Jones, M. W., O’Sullivan, M., Andrew, R. M., Bakker, D. C. E., Hauck, J., Le Quéré, C., Peters, G. P., Peters, W., Pongratz, J., Sitch, S., Canadell, J. G., Ciais, P., Jackson, R. B., Alin, S. R., Anthoni, P., Bates, N. R., Becker, M., & Bellouin, N., (2021) Global Carbon Budget 2021, Earth Syst. Sci. Data Discuss. [preprint], https://doi.org/10.5194/essd-2021-386
Harde, H. (2019). What Humans Contribute to Atmospheric CO2: Comparison of Carbon Cycle Models with Observations. Earth Sciences. Vol. 8, No. 3, 2019, pp. 139-158. https://doi.org/doi: 10.11648/j.earth.20190803.13
Henry, W. (1803). Experiments on the quantity of gases absorbed by water, at different temperatures, and under different pressures. Phil. Trans. R. Soc. Lond. 93: 29–274. https://doi.org/doi:10.1098/rstl.1803.0004
Hoppe, K. (1992). Mt. Pinatubo’s cloud shades global climate. Science News. July 18, 1992. https://www.thefreelibrary.com/Mt.+Pinatubo’s+cloud+shades+global+climate.-a012467057
Kauppinen, J., & Malmi, P. (2019). No experimental evidence for the significant anthropogenic climate change. Cornell University. arXiv:1907.00165v1 [physics.gen-ph] 29 Jun 2019. https://arxiv.org/abs/1907.00165v1
Mazza, D. (accessed 2022, April 15) Academia.edu https://danielemazza.academia.edu/
Mazza, D. (2020). Algorithms in Ocean Chemistry. ISBN | 978-88-31688-62-8. https://www.academia.edu/attachments/64182996/download_file?s=portfolio
Murray J.W., Barber R.T., Roman, M.R., Bacon, M.P., & Feely, R.A. (1994) Physical and biological controls on carbon cycling in the equatorial pacific. Science. 1994 October 7;266(5182):58-65. https://www.science.org/doi/10.1126/science.266.5182.58
Onuki, Akira (2009). Henry’s Law, surface tension, and surface adsorption in dilute binary mixtures. J. Chem. Phys. 130, 124703. https://doi.org/10.1063/1.3089709
Peng, T-H, Post, W. M., DeAngelis, D. L., Dale, V. H., & Farrell, M. P. (1987) Atmospheric carbon dioxide and the global carbon cycle: The key uncertainties. United States. https://www.osti.gov/biblio/5473519-atmospheric-carbon-dioxide-global-carbon-cycle-key-uncertainties
Sabine, C.L., Feely, R.A., Gruber, N., Key, R.M., Lee, K., Bullister, J.L., Wanninkhof, R., Wong, C.S., Wallace, D.W.R., Tilbrook, B., Millero, F.J., Peng T-H, Kozyr, A., Ono, T., & Rios, A.F. (2004) The Oceanic Sink for Anthropogenic CO2. Science, 305, 367.
Salby, M.L. (2012). Physics of the Atmosphere and Climate. 2nd Edition. ISBN: 9780521767187. https://climatecite.com/physics-of-the-atmosphere-and-climate-pt-1/ and https://climatecite.com/physics-of-the-atmosphere-and-climate-pt-2/
Salby, M.L., & Helmut-Schmidt-University Hamburg. (2018, October 10). What is Really Behind the Increase of Atmospheric CO2 ? [Video]. YouTube. https://youtu.be/rohF6K2avtY
Sander, R. (2015). Compilation of Henry’s law constants (version 4.0) for water as solvent. Atmos. Chem. Phys., 15, 4399–4981, 2015. https://doi.org/10.5194/acp-15-4399-2015 and https://henry.mpch-mainz.gwdg.de/henry/
Santer, B.D., Fyfe, J.C., Pallotta, G., Flato, G.M., Meehl, G.A., England, M.H., Hawkins, E., Mann, M.E., Painter, J.F., Bonfils, C., Cvijanovic, I., Mears, C., Wentz, F.J., Po-Chedley, S., Fu, Q., & Zou, C-Z. 2017. Causes of differences in model and satellite tropospheric warming rates. Nature Geoscience. 19 June 2017. http://www.meteo.psu.edu/holocene/public_html/Mann/articles/articles/SanterEtAlNatureGeosci17.pdf
Stallinga, P. (2018). Carbon dioxide and ocean acidification. European Scientific Journal June 2018 edition Vol.14, No.18. https://doi.org/10.19044/esj. http://dx.doi.org/10.19044/esj.2018.v14n18p476
Stallinga, P. (2018). Signal analysis of the climate: correlation, delay and feedback. Journal of Data Analysis and Information Processing, 6, 30-45. https://doi.org/10.4236/jdaip.2018.62003
Stallinga, P. (2020). Comprehensive analytical study of the greenhouse effect of the atmosphere. Atmospheric and Climate Sciences, 10, 40-80. https://doi.org/10.4236/acs.2020.101003
Stallinga, P., & Khmelinskii, I. (2018). Analysis of temporal signals of climate, Natural Science, Vol.10 No.10, 2018. https://doi.org/10.4236/ns.2018.1010037
Stenchikov, G., Ukhov, A., Osipov, S., Ahmadov, R., Grell, G., Cady-Pereira, K., Mlawer, Mlawer, E., & Iacono, M. (2021). How does a Pinatubo-size volcanic cloud reach the middle stratosphere? JGR Atmospheres. 14 May 2021. https://doi.org/10.1029/2020JD033829
Stumm, W., & Morgan, J.J. (1996). Aquatic Chemistry: chemical equilibria and rates in natural waters. James J. Wiley Interscience.192. https://archive.org/details/aquaticchemistry0000stum/mode/2up
Tans, P.P. (2006). Acceleration of the rate of growth of atmospheric carbon dioxide. NOAA Earth System Research Laboratory. https://gml.noaa.gov/publications/annual_meetings/2006/abstracts/talks_2006_02.pdf
The Engineering Toolbox. (accessed 2022, April 15) The Solubility of Gases in Water vs Temperature. The Engineering Toolbox. https://www.engineeringtoolbox.com/gases-solubility-water-d_1148.html
Thoning, K.W., Crotwell, A.M., & Mund, J.W. (2021). Atmospheric carbon dioxide dry air mole fractions from continuous measurements at Mauna Loa, Hawaii, Barrow, Alaska, American Samoa and South Pole. 1973-2020, Version 2021-08-09. National Oceanic and Atmospheric Administration (NOAA), Global Monitoring Laboratory (GML), Boulder, Colorado, USA https://doi.org/10.15138/yaf1-bk21 Data Set Name: co2_mlo_surface-insitu_1_ccgg_DailyData. Description: Atmospheric carbon dioxide dry air mole fractions from quasi-continuous measurements at Mauna Loa, Hawaii.
Harris, N., & Gibbs, D. (2021, January 21). Forests absorb twice as much carbon as they emit each year. World Resources Institute. https://www.wri.org/insights/forests-absorb-twice-much-carbon-they-emit-each-year
Zeebe, R.E., & Wolf-Gladrow, D.A. Carbon dioxide, dissolved (ocean). University of Hawai’i at Manoa. https://www.soest.hawaii.edu/oceanography/faculty/zeebe_files/Publications/ZeebeWolfEnclp07.pdf
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