Showing posts with label Celestial mechanics. Show all posts
Showing posts with label Celestial mechanics. Show all posts

Friday, June 26, 2020

Is The Milankovitch Hypothesis Really Based On Celestial Mechanics - Or Sea Floor Geology?



In 1976 three scientists (James Hays, John Imbrie,  Nicholas Shackleton)  published a seminal paper. In it they presented a deep sea "climate record"  which they claimed contained the same temporal cycles as three parameters shown in Fig. 1 below, from a recent paper appearing in Physics Today (May, p. 48) by Mark Maslin.  
figure
Their technique basically entailed using deep sea sediment cores to extract marine micro-fossils, to then estimate past sea surface temperatures.  The claim then was made that this geological proxy climate record revealed the same temporal cycles manifested in the three orbital parameters: eccentricity, obliquity, and precession.  All this is to substantiate the so-called Milankovitch theory which asserts these three distinct cycles are applicable to Earth's orbital motion.

The eccentricity (a) describes the shape of Earth's orbit around the Sun,  said to vary from near circular (as it is now) to more elliptical, with a period of 96,000 years.  The obliquity (b) is the tilt of the Earth's axis of rotation with respect to the orbital plane, and oscillates with a period of 41,000 years. The precession (c) combines the spin of Earth's orbital axis and its orbital path over time, producing a 21,000 year cycle.

Let me now back up to say I do not regard this as a "theory" but rather a hypothesis.  A theory, as I (and most physicists) define it, refers to a hypothesis which actually has made predictions that have been verified.  To my knowledge no such predictions have been made by Milankovitch's acolytes.   To be consistent, one would also expect such predictions to come out of a pure model from celestial mechanics - not one dependent on sea floor topography or geology.  These are two distinct sciences after all. (Paleo-climatology, i.e. based  on marine mciro-fossils,  is also distinct from celestial mechanics.)

Start with its contention that the obliquity of the ecliptic (inclination of Earth to its orbital axis) varies from 21 to 24 degrees over a 41,000 period in a process called ‘nutation’. This is certainly a magnitude in excess of a half degree (1800”) on either side of its current 23.5 deg.

Astronomers-astrometrists recognize no such period or differential of axial tilt. The following is from the book, Astronomy- Principles and Practice by A.E. Roy and D. Clarke, 1978, Adam Hilger Books, p. 118:

Because of the nutational wobble in the Earth’s axis of rotation, the obliquity of the ecliptic (KP in Fig. 10.32) varies about its mean value. The magnitude on either side is about 9.”2.”

For the benefit of non-astronomers, the magnitude cited (9.”2) isn’t even one hundredth of a degree! Indeed it is nearly a factor 4 LESS than a hundredth of a degree! (which translates to 36”- there are 3600” = 1 degree))

Going now to Eichhorn and Mueller’s standard text in astrometry and geodesy, 

 p. 69, “astronomic nutation’:

"The main term of astronomic nutation is produced by the non-coincidence of the Moon's orbit with the ecliptic in conjunction with the retrograde motion of the lunar nodes. This results in a periodic change in the obliquity of the ecliptic termed nutation in obliquity, denoted by d  e

The astronomic nutation, from now on called simply ‘nutation’ is not to be confused with the true nutation appearing as a force-free precession (Eulerian motion) of the Earth’s rotation axis about its principal moment of inertia axis, which is part of the polar motion

The first six terms of the expression for nutation in obliquity are:

(9.”2100 + 0.”00091t) cos W - (0.”0904 - 0.”0004t) cos 2W – (0.”0024 cos (2 w m W) + 0.”0002 cos (2 s  – W) + 0.”0002cos 2 ( w m  + W) + (0.”5522 – 0.”00029) cos 2W  

Where t denotes the time interval measured from 1900 January 0.5 d ET in Julian centuries (1 JC = 36525 mean solar days), W is the longitude of the mean ascending node of the lunar orbit on the ecliptic measured from the mean equinox of date, w m  is the ‘argument’ of the point where the Moon is nearest the Earth (i.e. from the lunar perigee),   is the mean longitude of the solar perigee measured from the mean equinox of date, and  W  is the geometric mean longitude of the Sun measured from the mean equinox of date.

We can then examine the putative change in the eccentricity e, which is currently at 0.0167 but which Milankovitch adherents claim can reach e = 0.07. (Elongating the orbit so as to influence climatic factors, e.g. see this video demonstration:

eccentricity with border


But what would it take to change the shape of the Earth's current orbit, to the one proposed by Milankovitch supporters?  How much energy would be required?  We can use the equation for the total energy of the orbit, in terms of the eccentricity, e, and the dimension of orbit known as the semilatus rectum,  r o   (=   b 2 /a)  and the other familiar parameters for Newtonian orbit computations, e.g.


The objective is to find the change in energy E, i.e. when e is altered from 0.0167 to 0.07.  This turns out to be approximately:

D E   »  1.9  x 10   42 J


This is an enormous amount of energy input.  WHERE does it come from? HOW is it produced?  What is the time evolution - in energy increments- leading to the final more eccentric orbit?  The Milankovitch adherents who adopt the work of a Serbian civil engineer, provide no answers.  How can they when they are working from reconstructed sea floor geology  findings and not celestial mechanics per se?

Given the preceding we should acknowledge that  there are significant problems with that Serbian civil engineer's hypothesis that bid us to exercise much more caution, i.e. before adopting it without qualification.  Especially given its reversed engineered construction from geological data, to arrive at a celestial mechanics format requiring new orbital elements.   Or conferring the benediction of an origin in celestial mechanics, as opposed to geology. One major issue was raised in a paper by Daniel B. Karner and Richard A. Muller 2 which pointed out a number of serious problems, inconsistencies associated with the Milankovitch hypothesis. 

Specifically the authors – after  assessing the  data from numerous sources (e.g. U-Th dating from the Devil’s Hole cave in Nevada) found that:

-         

       the Devil’s Hole data indicated a shift in d 18 O  to interglacial values and was “essentially complete by 135 ka but the Northern Hemisphere summer insolation hadn’t yet warmed to the point when it would have triggered anything extraordinary, let alone a glacial termination  Adding: “We call this discrepancy the causality problem



-         Most of the sea level rise took place prior to the expected insolation warming



The authors conclude (op. cit.):



The standard Milankovitch insolation theory does not account for the termination of the Ice Ages.”



Adding that:



We can conclude that models that attribute the terminations to large insolation peaks (or equivalently to peaks in the precession parameter)…are incompatible with the observations.”



Equally significant, perhaps, Richard A. Muller  has pointed out in a separate paper 3 that “the spectral shapes predicted by the Milankovitch theory do not match those in the spectrum and bispectrum of the data..”



In addition, Muller notes that the net forcing associated with clouds, i.e. about 30 W/m 2  is substantially greater than the rms variations in insolation.   This leads him to conclude:  The changes in cloud cover could be more important than the changes in Milankovitch parameters. 



Finally, Puetz et al4,  employed a “universal cycle model” – using a Universal Wave Series (UWS) with cycles in the kyr range -  to show that  orbital tuning limits independent and objective testing of an empirical hypothesis like that of Milankovitch. In effect, while Milankovitch offers a “seductively elegant solution to the problem of age-stratum mapping”, its template remains a trap for selection effects (and data bias) to enter. This results in a condition, as it pertains to the Milankovitch hypothesis,  whereby:



 ”Reporting bias occurs when articles mention favorable results from orbitally tuned records, which are supportive of the Milankovitch theory, while failing to mention unfavorable results from un-tuned versions of the same records.”


The reason is clear given that (ibid.): “Statistically significant positive results that support a desired outcome are more likely to be published in high impact journals.”

Thus, while one can certainly appreciate Prof. Maslin’s article, it is also worthwhile to be aware of the problems to do with the underlying hypothesis, most of which I suspect were engendered by the origins in sea floor geologic data.. 

My primary gripe, then,  is there is no independent confirmation of the Milankovitch hypothesis from celestial mechanics proper. That is, where is the model, or even numerical simulation,  actually showing how the three orbital parameters evolve over time t to yield  the temporal cycles suggested by the  marine microfossil studies?  Granted Hays et al's paper is ingenious - even somewhat convincing - but when you strip away all the ersatz arguments it is still reverse engineered geology, from which the changing orbital elements must be indirectly  inferred.

Where is the direct connection to orbital parameter development in a celestial mechanics context?  In particular, leave out the geological data, where is the theory based on celestial mechanics showing how Earth's orbit changes its parameters to yield the temporal cycles claimed by Maslin, as well as Hays et al, and oh yes, Milankovitch.

References:


1. J.D. Hays, J. Imbrie, N.J. Shackleton, Science 194, 1121 (1976)

2.Daniel B. Karner, Richard A. Muller, A Causality Problem for Milankovitch, Science, 288, 2143 (2000)

3. Richard A. Muller, Limitations and Failures of the Milankovitch Theory, poster paper, American Geophysical Union Fall Meeting (2001)

4. Stephen J. Puetz, Andreas Prokoph, Glenn Borchardt, Evaluating Alternatives To The Milankovitch Theory, Journal of Statistical Planning and Inference, 170,  158 (2016)




Thursday, May 17, 2018

Selected Questions- Answers From All Experts Astronomy Forum (General Astronomy Information)

Question: i need information on astronomy, anything...what it is, it's history,
etc... thank you. Wolfie, Tacoma Park, Md


Answer:   'Astronomy' is actually quite a vast area to try to explain at one time
because it includes a number of large sub-disciplines:

astrometry - the study of star positions and how these change over time
with celestial coordinates

celestial mechanics - the prediction of the future positions of the
planets, Moon, etc. using orbital elements

 stellar astrophysics - the study of the physics of the stars, and their
evolution, changing properties

 solar physics - the study of the Sun, its physics and properties, as well
as terrestrial effects


radio astronomy - the study of celestial objects using sensitive antennas designed
 to receive signals  in the radio spectrum

galactic dynamics  - the study of the dynamics and physics of the galaxies, galaxy 

clusters, and their origin, evolution, 

cosmology - the study of the large scale structure, origin and evolution of the universe.

Each one of these - particularly the respective history of each sub discipline - 
would probably take several large books to even survey, far less 'explain'. 
What this shows is that like many other scientific disciplines, astronomy has grown
and developed beyond simple description or being one simple science. When
people become astronomers today, in fact, they have to specialize in one
area, say solar physics - they can't just do astronomy. It's too much!

As for the history, or any one part of it, as you can gather from the
above it's far beyond the scope of any practical (and even partially
complete) response here.  Hence, rather than expect a concise set of 
information it is better to go out and get basic books to learn the 
knowledge and master the principles on your own.


Many of the basic books are somewhat dated, but the essential (foundational)
 knowledge  and physical principles remain intact. One of the best is Sir Fred
 Hoyle's 'Frontiers of Astronomy' which  is  available online:

His textbook, 'Astronomy and Cosmology - A Modern Course' is also excellent
and very readable.  Both of these books provide astronomy insights across a wide
spectrum of subjects. 

As for a concise history of astronomy as an overall subject, an excellent book
 to read - which should be available at any public library- is:

'A Short History of Astronomy: From Earliest Times Through the Nineteenth
Century
' by Arthur Berry, Dover Publications, 1961.


If you are serious about garnering more information about astronomy and its
 many facets, the  approach I've outlined here will be a major help - as well as
 the books cited.  You can, of course, also find numerous other good texts on
your own simply by use of appropriate Google inputs.

Wednesday, January 24, 2018

Selected Questions - Answers From All Experts Astronomy Forum (Celestial Mechanics)

Question -

How do they find the positions of planets  (mathematically)?


Answer:

Determining the position of any planet in the orbital plane is not trivial
at all, nor can it be answered in a simple response format. The reason is
that whole courses in what is called celestial mechanics are devoted to
it.

Students cannot take this course without first having studied (or taken
courses in) calculus, advanced calculus and differential equations, as
well as advanced computer programming. Hence, if you haven't taken or been
exposed to such - it is impossible to convey what is necessary to compute
orbit positions!

Basically, position determination entails identifying - calculating the
seven elements that make up a given planetary orbit, including: the
eccentricity of orbit (how much it deviates from circularity); the
semi-major axes (or mean distance from the Sun); the longitude of the
ascending node, the inclination (i) of the orbit, the true anomaly, and
the mean anomaly, and the time of perihelion passage (T) or alternately
the 'mean motion' n = M/ (t - T).



Getting more specific, the diagram  below shows assorted orbital elements
for a planet of mass m2 (the Sun is m1) .














In the diagram, w   is the argument of the perihelion, W is the
longitude of the ascending node, f is the true anomaly and i is the
inclination of the orbit. The critical or key parameter
here is h, the angular momentum vector for the orbiting system. 

The true anomaly is perhaps most difficult to obtain since it requires one
take a Fourier expansion (again, this is taught in advanced calculus!) of
the difference (w - M), e.g. the mean anomaly (M) from the true anomaly.

The student must be  able to ascertain that  W  = M - w  (difference
between mean anomaly and argument of the perihelion) where M can
be obtained from a table based on observations, and w can be obtained
using a Fourier expansion of the mean anomaly, M:

w  = M + (2e – e3 / 4) sin M + 5 e2/4 sin 2M + ... etc.

One then needs to obtain the energy constants C1, C2, C3.
Where:

C1/ h = sin W sin (i)
C2/ h = - cos W sin (i)
C3/h = cos(i)

The magnitude h, of the angular momentum vector is:

h = r x r’ =

(y z’ - z y’)

(z x’ - x z’) = (C1 C2 C3)

(x y’ - y z’)

so (r x r’) = (C1/ h, C2/ h, C3/h)

Since the inclination of Earth's orbit to the ecliptic  (i) is known
(23.5 deg) and therefore cos(i) can be determined, then sin(i) can be
found as well.  Also h can be determined, since: h = C3 / cos(i) =
(GMm a (1 – e2)12 where all the constants are known (a = semi-major axis
of orbit, e = eccentricity of orbit)


(The energy equation is: ½V 2 - u/r = C, and the C's - energy integration
constants- are  found from this.)

Once W is known, C1 and C2 and C3 are known, and the student can
compute the position of a planet, say Jupiter, forty or so years in the future.

If you would like to find out more details of planetary position computation
and exactly how it's done - there is an excellent and detailed site (with tutorials)