Global Warming Temperatures and Projections: As Related to CO2 and H2O Absorptions, H2O Evaporation, and Post-Condensation Convection
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About this ebook
The author earned an PhD from Princeton, is a Bell Laboratories retiree with multiple patents and scientific papers and is a Fellow in the IEEE Technical Society.
The analysis provides verification that with no other background changes, the concentration of CO2 in the atmosphere would have to increase beyond 4,000 parts per million in order to have a surface temperature increase of 2 degrees Celsius. With step-ups in the background, the concentration of CO2 would need to rise to 2,500 parts per million to have the same effect.
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Global Warming Temperatures and Projections - William T. Lynch, PhD
Global Warming Temperatures and Projections
As Related to CO2 and H2O Absorptions, H2O Evaporation, and Post-Condensation Convection
William T. Lynch, PhD
Copyright © 2017 William T. Lynch PhD
All rights reserved.
ISBN 978-1-387-25332-6
All rights reserved. This book or any portion thereof may not be reproduced or used in any manner whatsoever without the express written permission of the publisher except for the use of brief quotations in a book review or scholarly journal.
First Edition: 2017
Contact the author at globalwarming.lynch@gmail.com.
Contents
About this book
Acknowledgments
Preface
Abstract (extended)
Preliminary ‘peeks’
Section One: Modeling the atmosphere
Introduction
Definitions
A very brief summary of the spreadsheet model
Normalization of altitude
Basic BBR, power and Planck expressions
Calculations within each slice
A second representation of the notch
The overall picture of atmospheric interactions
Molecular density and altitude
Soft entry to the calibration tables
Calibration
Continuation of the (1-TOth) & (1-Tcomb) analysis
Doubling plots: ΔK(0) vs. LOG2(CO2/380)
Comparisons with the calibration plot
Additional details on absorption
How much additional absorption does CO2 provide?
Progression of atmospheric parameters as CO2 is increased
Section One summary
Section One references
Section Two: H2O and its phases
H2O water vapor influence on global warming vis a vis CO2
The adiabatic lapse rate
Specific comparisons of atmospheric water and CO2
Average water vapor content in the atmosphere
Published distributions of water vapor
Heat convection from the Tropics
Water as a ‘climate changer,’ with replacement of the Tropical heat bus by circulation cells
Section Two summary
Section Two references
Appendicies
Appendix A: Correlations with total absorption
Appendix B: Normalized altitude Z’
Appendix C: Organization of the spreadsheet and of the individual slices
Appendix D: Absorption ‘notches’
Appendix E: Final sets of data and their interpretation
Quick references (5 tables)
About the author
About this book
Global Warming Temperatures and Projections clarifies the roles of both CO 2 and H 2 O in global warming and climate change. In particular, it addresses the fear- cum -belief claims that further CO 2 increases threaten to create runaway climate effects. The examination is devoid of politics and rhetoric and relies on a mathematical and scientific analysis of a slice-by-slice modeling of the atmosphere.
William T. Lynch (M.S. from MIT, PhD from Princeton) is a retired Department Head (Very Large Scale Integration) from Bell Laboratories, with multiple scientific papers and patents, and is a Fellow in the IEEE Technical Society.
Several distinguishing features of this book are:
A 50-slice model of the atmosphere in which the altitude of 0 to infinity is normalized to a range of 0 to 1.0;
Calculations within each slice of absorptions of upwardly directed infrared emissions from the earth and the tracking of the evolution of the thermal blanket from higher to lower altitudes;
A generic calibration plot for correlating equilibrium surface temperature with net absorption for whatever mix of absorbers are present;
Verification that the only distinguishing (and important) feature of CO2 is that its concentration in the atmosphere may increase since it is not fully flushable, but that, with no change in background, CO2 would have to increase beyond 4,000 ppm in order to have a surface temperature increase of 2 degrees Celsius, or 2,500 ppm with step-ups in the background;
Verification that H2O is the dominating influence, both by means of its water vapor absorption, but also by the heat transfer associated with evaporation from the earth and condensation at upper altitudes, and the convection of that heat to provide blanket contributions at upper Latitudes;
Realization that nature’s available energies dwarf any capabilities of human-created energies; nature always seeks a resolution of a non-equilibrium situation and is not concerned about damages to human stuff. The day after any distempered resolution is not a runaway but a very peaceful day.
Acknowledgments
William T. Lynch acknowledges the early guidance and comments by Professors Hugo Fritz Franzen (Iowa State) and Will Happer (Princeton). He also acknowledges the book compilation and editing by Anthony Lynch, the helpful commentaries by Kevin Johnson, Edward Stubenrauch and Joseph Kneuer, and the continuing support of this project by his wife, Gerry Lynch.
Preface
The analyses of this document were initiated neither as a polemic against nor an apologia for existing opinions about CO 2 and its role in global warming.
Its primary purpose is to quantify convincingly the limiting effects of increases in CO2 on the earth’s temperature and to do so independently of any possible linkages to secondary enhancements. In particular, any propensities for CO2 to produce runaway effects had to be resolved.
A secondary purpose is to assess why official projections for global warming have been in disagreement with the official measurements, and to produce a model that can adjust parameters so as to, forcibly if necessary, cause official CO2 and temperature values to be in agreement.
There has been no verification that official average (as opposed to peak) daily temperatures have been uniformly and properly calculated and integrated over many years of increasing data points with new technologies and new locations. Official records of past averages have been accepted, but official projections have not been employed.
A truly successful goal would be a calibration plot that aligns average surface temperature K(0) with whatever absorbing molecules are present in the atmosphere. Any additions in surface temperatures should more likely be self-limiting rather than runaway scenarios.
These goals have been achieved, but all CO2 and H2O increases in absorption are, by themselves, insufficient to provide the necessary increases in the Blanket to support the K(0) values of the calibration plots.
Section One incorporates all the arguments associated with CO2 and H2O absorption.
Section Two incorporates the additional, and significant, effects associated with evapotranspiration, surface cooling, upper atmosphere condensation, and the lateral convection of the heats of condensation from the Tropics latitudes towards the Poles.
This convection provides almost half the Blanket in the Temperate zones, reduces temperature in the Tropics, and has little to nothing to do with CO2 or other human influences.
The calibration plots of Section One are made whole again, without absolute proof, by the realization that the unspecified background
absorptions are directly replaceable with the justifiable convection contributions to the blanket.
The document is organized as a sequence of learning elements. The ultimate conclusions are firmly based in physics and mathematical constructs.
The openness of the analysis has been rewarded by proofs that the effects of CO2 have been overstated, that increases in global warming are limited, and that nature does not support a runaway.
The style of this book intentionally avoids having hundreds of references. References with direct application are acknowledged. References are not sought for knowledge that is believed to be well-accepted.
Abstract (extended)
Section One concentrates on CO 2 and on physics- and mathematics-based models. The emphasis is on calculating absorptions by CO 2 molecules of Black Body Radiation (BBR) from the surface and in the return of nearly one half of that absorbed energy in the form of a blanket. Section Two emphasizes H 2 O and its phases. H 2 O not only has an atmospheric molecular phase (vapor) but also an atmospheric liquid phase, which is, of course, critical for rainfalls. Section Two also emphasizes the crown of atmospheric heat in the Tropics that spills towards the Poles and contributes significantly to local blankets.
Section One presents an unbiased mathematical confirmation of a general model that states that any absorbing molecules in the atmosphere will interrupt surface heat from escaping directly. The returning blanket
raises the surface temperature K(0) and the surface BBR emission until a level is reached at which the unabsorbed portion plus the half that is not returned as a blanket is sufficient to satisfy the demand for K(0) equilibrium. In all of these calculations thermodynamic adiabatic effects must be considered. Energies are never lost, but adiabatic work is always taking place. (See illustration: Cross section parameters for the earth and atmosphere.)
Absorptions by present CO2 levels are far from sufficient to match the levels of the actual BBR, and Section One determines the level of additional absorptions that must be present in order to match present reality. H2O concentrations are also introduced in Section One; direct H2O absorptions are equivalent to CO2 but the combined CO2 and H2O absorptions are still insufficient to satisfy present reality. There is a residual background
of apparent absorption that has to be explained. (Figure A1.)
Section One deals only with a vertical modeling of the atmosphere, with an average surface temperature K(0). All net directions are up and down, because the model block has an undefined surface area that extends to left and right and encompasses the world. Its ultimate conclusions are, in fact, accurate, except that the residual background tentatively incorporated as an unknown absorption does not have to be totally ascribed to absorptions. Section Two shows that the unknown absorption
is primarily a blanket supplement dominated by upper atmosphere heat convection emanating from the Tropics. (See Figures A2, A3, A4.)
Although both H2O and CO2 are necessary inputs for plant growth, CO2 never appears in the liquid or solid phases, and so does not make its presence in the atmosphere known by means of evaporation, but H2O does. Furthermore, the evaporation of water from the surface significantly cools the surface. The required heat of evaporation of water is very high; it takes more than 500 times as much heat to vaporize one gram of water as to raise its liquid temperature by 1.0C. Cooling takes place upon evaporation of liquid water but heating occurs higher in the atmosphere when the vapor is condensed.
Besides any long-term increase in atmospheric CO2 from carbon burning, atmospheric CO2 does demonstrate cyclic shifts when temperatures change from any cause (such as El Niño and La Niña effects). The oceans are a large reservoir of CO2 and release CO2 when warmed and collect CO2 when cooled. (The daily net releases and collections can at times be greater than the human production of new CO2.) CO2 has no direct linkage to produce unusual weather effects but the multiple effects for creating a constantly varying H2O atmospheric distribution — pressure, temperature, surface water, Coriolis effect, convection — absolutely disrupt weather uniformity. Nature does not adjust uniformly and temporally towards a global average, but adjusts locally and instantaneously to disruptions caused by sun changes, wind changes, and the 23 degree offset of the earth’s rotational axis relative to the earth’s axis of rotation around the sun. The offset does more than just cause seasonal opposites between the northern and southern hemispheres; for latitudes beyond the range of the 46 degree Tropical band the winters are colder and the summers are warmer than they otherwise would be.
All in all, this may be considered as a fortunate result, but it produces more weather disruption at all latitudes. Weather disruption is greatest at latitudes where the earth’s rotational speeds are large and, simultaneously, where the rotational speeds vary significantly with latitude. The mid-latitudes, therefore, are the optimum latitudes for hurricanes and tornados. (They are optimum for nature, not necessarily so for humans.) Nature’s power and