Natural Climate Change has been Hiding in Plain Sight
See refined assessment with evidence (thermalization) that CO2 has no significant effect on climate at http://globalclimatedrivers2.blogspot.com (rev 10/23/16)
About 41.8% of reported average global temperature change
results from natural ocean surface temperature oscillation and 58.2% results
from change in the rate that the planet radiates energy to outer space and/or reflects it, as
calculated using a proxy, which is the time-integral of sunspot numbers. Using
just these two factors explains average global temperatures (least biased
values based on HadCRUT4 and other credible measurements) since before 1900 with
89.82% accuracy (R2=0.8982). [See revised attributions] (rev 8/3/19)
If atmospheric carbon dioxide (CO2) is included
in the calculation, it might account for as much as 17.6% of reported average global
temperature (AGT) change during the period 1909-2005. If CO2 has that much influence, then the calculated
ocean surface temperature effect decreases to about 37.8% and sunspot influence
decreases to about 44.6%, but accuracy increases an insignificant amount to
90.06%. This miniscule increase in accuracy indicates that CO2
change probably has substantially less than 17.6% influence on average
global temperature change.
Ocean oscillations
Some ocean cycles have been named according to the
particular area of the oceans where they occur. Names such as PDO (Pacific
Decadal Oscillation), ENSO (el Nino Southern Oscillation), and AMO (Atlantic
Multidecadal Oscillation) might be familiar. They report the temperature of the
water surface while the average temperature of the bulk water that is participating
in the oscillation can not significantly change so quickly because of its high
thermal capacitance 5.
This high thermal capacitance absolutely prohibits the
reported rapid (year-to-year) AGT fluctuations as a result of any credible forcing. According to one assessment 5,
the time constant is about 5 years. A possible explanation is that the reported
rapid fluctuations may be stochastic artifacts of the process that has been
used to determine AGT. A simple calculation shows the standard deviation of the
reported annual average measurements to be about ±0.1 °K with respect to the trend. The
temperature fluctuations of the bulk volume near the surface of the planet are
more closely represented by the fluctuations in the trend. The trend is a
better indicator of the change in global energy; which is the difference
between energy received that is above or below break-even and energy radiated above or below break-even.
There is some average surface temperature oscillation that
accounts for all of the oceans considered together of which the named
oscillations are participants. Studies 1,2,3,4 of the primary
contributor (the PDO) to this planet-wide oscillation have been done which
identify the period of this oscillation to be in the range of 50-70 years. One
of these studies considered data from as far back as 1000 years.
Complex phase relations between the various local cycles cause
the effective over-all oscillation to vary in magnitude and period over the centuries. In
the present assessment, the period of the planet-wide oscillation, since before
1900, has been found to be about 64 years with a magnitude of about ± 1/5 °K.
The most recent calculated trend peak was in 2005.
Sunspot number
time-integral
Sunspots have been suspected as being associated with
climate change for a long time. Sunspot numbers are recorded as solar cycles
which have been considered by others for magnitude or for time factors with
poor success when trying to correlate with AGT trends.
A
low but broad solar cycle may have just as much cumulative influence on AGT as
a high but brief one. Both magnitude and duration are accounted for by using
the time-integral of sunspot numbers. The temperature trend rise from the
Little Ice Age and over half of the AGT rise of the 20th century are
accounted for by the time-integral of sunspot numbers with an appropriate proxy
factor. Of course, the time-integral of increase above or below
break-even must be reduced by the time-integral of energy radiated from
the planet above or below break-even; which varies with the fourth power of its
absolute temperature.
The
first law of thermodynamics, conservation of energy, is applied to evaluate the
hypothesis that the temperature trend is influenced by sunspot numbers. Average
global temperature has not changed much over the centuries so on average, over
the centuries, energy-in equals energy-out. In any one year, the energy-in is
given by
Ein = B * S(i) (a)
where
‘B’ is the proxy factor. If the AGT never changed, the energy-out is given by
Econst AGT = B * Savg
To
account for the yearly variation in energy-out it is multiplied by the fourth
power of the temperature ratio which gives
Ei out = B * Savg * [T(i)/Tavg]4 (b)
Subtracting
(b) from (a) results in the energy change for any year. Also, factor out B
Echg = B * {S(i) – Savg *
[T(i)/Tavg]4} (c)
Dividing
the energy change by the thermal capacitance gives the temperature change from
the previous year. Summation of changes for previous years obtains the total
change from the start of the summation.
Tchng = B/Ceffective * Σyinitial {S(i) – Savg
* [T(i)/Tavg]4} (d)
With
appropriate offset this becomes the sunspot number contribution to the temperature
anomaly. The high coefficient of correlation demonstrates that the hypothesis is
true.
Atmospheric carbon
dioxide
Atmospheric CO2 is called a greenhouse gas (ghg)
because it absorbs electromagnetic radiation (EMR) within the range of
significant Stephan-Boltzmann (black body) radiation from the planet. The EMR
that CO2 absorbs (and emits) is only over a very narrow
band of the over-all radiation spectrum from the planet (never mind that the ghg effect is an insignificant factor in how greenhouses work). Most of the EMR that
is absorbed is emitted (nearly all of the absorption and emission is actually
by water vapor) but about 11.59% is thermalized 8 and appears as
sensible heat which warms the atmosphere.
Added increments of CO2 and other ghgs exhibit a
logarithmic decline in their influence on AGT. This is accounted for
mathematically for each year by taking the logarithm of the ratio of the average
CO2 level for the year to the CO2 level in 1895, which
was 294.8 ppmv (Law Dome 7). The cumulative effect to a year of
interest is the summation of the effects for prior years plus the effect for the current year. The best current
source for atmospheric carbon dioxide level 6 is Mauna Loa, Hawaii.
Combined equation
The net effect on AGT of the combination of the above three
contributing factors is obtained by their sum. The word equation is: anomaly = ocean oscillation effect + net sunspot & thermal radiation effect + CO2 effect + offset. This is expressed in the following physics-based
equation.
(1)
Where:
anom(y) =
calculated average global temperature anomaly in year y, in K degrees.
(A,y)
= Effective Sea Surface Temperature Anomaly (ESSTA) in year y calculated using
a range (peak-to-peak magnitude) of A, °K, and the number of years since the
last maximum or minimum. ESSTA is a simple (saw-tooth) surface temperature
approximation of the net effect of the Pacific Decadal Oscillation (PDO) and
all of the other natural ocean oscillations, named or not. It has a maximum
amplitude of about ± 1/5 °K with no intrinsic energy change for the bulk volume
at any time between the beginning value and the end value of its estimated 64
year period. The most recent peak was in 2005.
s(i) = average daily Brussels International sunspot number
in year i
17 = effective
thermal capacitance 5, W Yr m-2 K-1
43.97 = average
sunspot number for 1850-1940.
286.8 = global mean surface temperature for 1850-1940, °K.
T(i) = average global absolute temperature of year i, °K,
ppm co2(i) = ppmv CO2 in year i
294.8 = ppmv atmospheric CO2 in 1895
B is a proxy
factor in the function that accounts for the solar radiation, W yr m-2.
C is a multiplier
in the function that accounts for the influence of atmospheric CO2, W
yr m-2
D is merely an
offset that shifts the calculated trajectory vertically, without changing its
shape, to center it over the measurements, K degrees. This offset is equivalent to having selected slightly different reference temperatures for the measured anomalies.
A, B,
C, and D are calibration
coefficients which have been determined to maximize the coefficient of
determination, R2 (which makes the least biased fit of the trajectory,
that is calculated using the physics-based equation, to measurements). Some have
mistakenly interpreted these coefficients to indicate mathematical curve
fitting, which is something that is entirely different. Instead, the
coefficients allow the rational estimation of the amount that each of the two
or three major contributors has made to the total temperature change.
It is worth emphasizing that equation (1) provides for a
test to determine the influence, or lack thereof, of CO2 to the
total contributions to global anomalies by forcing the coefficient, C, to zero
and adjusting the other coefficients to maximize R2.
In Figure 1, the anomaly trajectory calculated using
Equation (1) is co-plotted with measurements. The excellent match of the up and
down trends since before 1900 is displayed and corroborates the usefulness and
validity of Equation (1).
Figure 1: Measured average global temperature anomalies with calculated prior and projected trends.
Figure 1: Measured average global temperature anomalies with calculated prior and projected trends.
Projections until 2020 use the expected sunspot number trend
for the remainder of solar cycle 24 as provided 9 by NASA. After
2020 the limiting cases are either assuming sunspots like from 1925 to 1941 or
for the case of no sunspots which is similar to the Maunder Minimum.
The influence of CO2 can be removed from the
equation by setting C to zero. Doing
so results in an insignificantly lower coefficient of determination (R2).
The coefficients in Equation (1) and resulting R2 are presented in
Table 1.
Ocean oscillation, A
|
Sunspot integral, B
|
Carbon dioxide influence, C
|
Offset, D
|
Accuracy, R2
|
0.3593
|
0.003731
|
0.3112
|
–0.3903
|
0.900641
|
0.400
|
0.004894
|
0.0
|
–0.3892
|
0.898220
|
Table 1. Coefficients in Equation (1) and resulting
accuracy.
Complementary theories as to why this calculation works have
been described previously10. The most significant theory appears to
be: Fewer sunspots; reduced solar magnetic shielding; increased galactic cosmic
rays penetrating the atmosphere; increased low-level clouds; lower average
cloud altitude; higher average cloud temperature; increased cloud-to-space
radiation; declining AGT.
It is easy to show that an increase in average cloud
altitude of about 100 meters would account for half of the AGT increase in the
20th century that some have referred to as ‘Global Warming’. Increased low level clouds also means increased over-all cloud cover with attendant increased albedo. This also leads to declining AGT 11.
Without human caused Global Warming there can be no human
caused climate change.
Climate science appears to have missed the above and other factors 12.
Climate science appears to have missed the above and other factors 12.
Corroboration that CO2 is not
a significant forcing (added 2/10/15)
It is trivially
easy for anyone with access to existing CO2 and temperature
measurement data-sets to falsify the statement that CO2 (at any
level that ever existed) causes significant warming.
If CO2
is a forcing, a scale factor times average CO2 level times the
duration divided by the effective thermal capacitance (consistent units) equals
the temperature change of the duration. Thus the temperature responds gradually
to a forcing. During previous glaciations and interglacials (as so dramatically
displayed in An Inconvenient Truth) CO2
and temperature went up and down nearly together. This is impossible if CO2 is
a significant forcing so this actually proves CO2 CHANGE DOES NOT
CAUSE SIGNIFICANT CLIMATE CHANGE.
See more on
this and discover the two factors that do cause climate change (95% correlation
since before 1900) at http://agwunveiled.blogspot.com . The two
factors which explain the last 300+ years of climate change are also identified
in a peer reviewed paper published in Energy and Environment, vol. 25, No. 8,
1455-1471.
Conclusions
This assessment demonstrates that the annual average
temperatures of the planet, for at least as far back in time as accurate
temperatures have been measured world wide, are accurately calculated by
considering only natural ocean oscillations and the sunspot numbers, and that
credible changes to the levels of non-condensing greenhouse gases have no significant
influence on average global temperature.
Equation (1) explains approximately 90% of the AGT trajectory since
before 1900. All factors that were not explicitly considered must find room in
the unexplained 10%.
References:
- MacDonald, Glen M. and
Roslyn A. Case (2005), Variations in the Pacific Decadal Oscillation over
the past millennium, Geophysical
Research Letters, 32, L08703
- Mantua, N. J., S. R. Hare,
Y. Zhang, J. M. Wallace, and R. C. Francis, A Pacific interdecadal climate
oscillation with impacts on salmon production. Bull. Am. Met. Soc. 76, 1069-1079, 1997
- Minobe, S., (1999),
Resonance in bidecadal and pentadecadal climate oscillations over the
North Pacific: Role in climatic regime shifts, Geophys. Res. Lett., 26, 855–858.
- Minobe S., (1997) A 50–70
year climatic oscillation over the North Pacific and North America. Geophs. Res. Lett., 24, 683–686.
- Schwartz, Stephen E.,
(2007) Heat capacity, time constant, and sensitivity of earth’s climate
system, J. Geophys. Res., vol. 113,
Issue D15102, doi:10.1029/2007JD009373
- Annual average atmospheric
carbon dioxide level at Mauna Loa ftp://ftp.cmdl.noaa.gov/ccg/co2/trends/co2_annmean_mlo.txt
- http://climaterealists.com/attachments/ftp/Cloudaltitudevsglobaltemperature.pdf
- Graphical sunspot number
prediction for the remainder of solar cycle 24 http://solarscience.msfc.nasa.gov/predict.shtml
- http://climaterealists.com/attachments/ftp/Verification%20Dan%20P.pdf
- http://endofgw.blogspot.com/
-
Obsolete graph