André
Koch Torres Assis* & Marcos Cesar Danhoni Neves**
To infinity and
beyond...
A little-known developmant in the history of cosmology
*Instituto de Física "Gleb Wataghin",
Universidade Estadual de Campinas, 13083-970, Campinas-SP, Brasil, e-mail: assis@ifi.unicamp.br
** Departamento de Física, Universidade Estadual de
Maringá, Av. Colombo, 5790, 87020-900, Maringá-PR, Brasil, e-mail: macedane@yahoo.com
Abstract. We
present the history of estimates of the temperature of intergalactic space. We
begin with the works of Guillaume and Eddington on
the temperature of interstellar space due to starlight belonging to our Milky
Way galaxy. Then we discuss works relating to cosmic radiation, concentrating
on Regener and Nernst. We
also discuss Finlay-Freundlich’s and Max Born’s important research on this topic. Finally, we
present the work of Gamow and collaborators. We show
that the models based on an Universe in dynamical
equilibrium without expansion predicted the 2.7 K temperature prior to and
better than models based on the Big Bang.
Key Words: Cosmic background
radiation, temperature of intergalactic space, blackblody
radiation
Introduction
In 1965 Penzias
and Wilson discovered the Cosmic Background Radiation (CBR) utilizing a horn
reflector antenna built to study radio astronomy (Penzias
and Wilson 1965). They found a temperature of 3.5± 1.0 K observing background
radiation at 7.3 cm wavelength. This was soon interpreted as a relic of the hot
Big Bang with a blackbody spectrum (Dicke et al. 1965).
The finding was considered a proof of the standard cosmological model of the
Universe based on the expansion on the Universe (the Big Bang), which had
predicted this temperature with the works of Gamow
and collaborators.
In this paper we show that
other models of a Universe in dynamical equilibrium without expansion had
predicted this temperature prior to Gamow. Moreover,
we show that Gamow’s own predictions were worse than
these previous ones.
Before begining
let us list briefly some important historical information which help to
understand the findings. Stefan found experimentally in 1879 that the total
bolometric flux of radiation F emitted by a blackbody at a temperature T
is given by F=s T4, where s is now
called Stefan-Boltzmann’s constant (5.67 x 10-8
Wm-2K-4). The theoretical derivation of this expression
was obtained by Boltzmann in 1884. In 1924 Hubble
established that the nebulae are stellar systems outside the Milky Way. In 1929
he obtained the famous redshift-distance law.
Guillaume and Eddington
The earliest estimation of
a temperature of "space" known to us is that of Guillaume (1896). It
was published in 1896, prior to Gamow’s birth (1904).
Here we quote from this paper (English translation by C. Roy Keys):
Captain
Abney has recently determined the ratio of the light from the starry sky to
that of the full Moon. It turns out to be 1/44, after reductions for the
obliqueness of the rays relative to the surface, and for atmospheric
absorption. Doubling this for both hemispheres, and adopting 1/600000 as the
ration of the light intensity of the Moon to that of the Sun (a rough average
of the measurements by Wollaston, Douguer
and Zöllner), we find that the Sun showers us with
15,200,000 time more vibratory energy than all the stars combined. The increase
in temperature of an isolated body in space subject only to the action of the
stars will be equal to the quotient of the increase of temperature due to the
Sun on the Earth’s orbit divided by the fourth root of 15,200,000, or about 60.
Moreover, this number should be regarded as a minimum, as the measurements of
Captain Abney taken in
Of course, Guillaume’s
estimation of a 5-6 K blackbody temperature may not have been the earliest one,
as Stefan’s law had been known since 1879. Moreover, it is restricted to the
effect due to the stars belonging to our own galaxy.
We now quote from Eddington’s book, The Internal Constitution of the Stars
(1988), published in 1926. The last chapter of this book is called
"Diffuse Matter in Space" and begins discussing "The Temperature
of Space":
Chapter XIII
DIFFUSE MATTER IN SPACE
The Temperature of Space.
256.
The total light received by us from the stars is estimated to be equivalent to
about 1000 stars of the first magnitude. Allowing an average correction to
reduce visual to bolometric magnitude for stars of types other than F and G,
the heat received from the stars may be taken to correspond to 2000 stars of
apparent bolometric magnitude 1.0. We shall first calculate the energy-density
of this radiation.
A
star of absolute bolometric magnitude 1.0 radiates 36.3 times
as much energy as the sun or 1.37 x 1035 ergs per sec. This
gives 1.15 x 10-5 ergs per sq. cm. per sec. over a sphere of 10
parsecs (3.08 x 1019 cm.) radius. The corresponding energy-density
is obtained by dividing by the velocity of propagation and amounts to 3.83 x 10-16
ergs per cu. cm. At 10 parsecs distance the apparent magnitude is equal to the
absolute magnitude; hence the energy-density 3.83 x 10-16
corresponds to apparent bolometric magnitude 1.0.
Accordingly
the total radiation of the stars has an energy-density
2000
x 3.83 x 10-16 = 7.67 x 10-13 ergs / cm3.
By
the formula E=s
T4 the effective temperature corresponding to this density is
3°
18 absolute
In
a region of space not in the neighbourhood of any
star this constitutes the whole field of radiation, and a black body, e.g., a black
bulb thermometer, will there take up a temperature of 3° 18 so that its
emission may balance the radiation falling on it and absorbed by it. This is
sometimes called ‘temperature of interstellar space.’
One important aspect to
emphasize here is that Eddington’s estimation of a
temperature of 3.18 K was not the first one, as Guillaume had obtained a
similar figure by 30 years earlier. Although Eddington
did not quote Guillaume or any other author, it is clear that he was here
following someone’s else derivation. This is indicated
by the sentences «The total light received by us from the stars is estimated
[by whom?] to be ...» and «This is sometimes called
[by whom?] the ‘temperature of interstellar space».
These sentences show that others had also arrived at this result. It is very
probable that in the fifty years between Stefan’s law (1879) and Eddington’s book (1926) others arrived at the same
conclusion independent of Guillaume’s work (1896).
Another point to bear in
mind is that Eddington and Guillaume were discussing
the temperature of interstellar space due to fixed stars belonging to our own
galaxy, and not of intergalactic space. Remember that Hubble only established
the existence of external galaxies beyond doubt in 1924.
Aside
Wright (2006) said that
the Eddington prediction of 3.18 K of the temperature
of space is not an anticipation of CMB or interstellar dust (ISB). He stated
that the equality of the energy densities of starlight and the CMB is (believe it or not) «just a coincidence». According to Lerner (2007):
Tegmark et al
[arXiv:astro-ph/0302496] have shown that the quadruple and octopole component
of the CBR are not random, but have a strong preferred orientation in the sky.
The quadruple and octopole power is concentrated on a ring around the sky and
are essentially zero along a preferred axis. The direction of this axis is
identical with the direction toward the Virgo cluster and lies exactly along
the axis of the Local Supercluster filament of which our Galaxy is a part. This
observation completely contradicts the BB [Big Bang] assumption that the CBR originated far from the
local Supercluster and is, on the largest scale,
isotropic without a preferred direction in space. Big Bang theorists have
implausibly labeled the coincidence of the preferred CBR direction and the
direction to Virgo to be mere accident and have scrambled to produce new ad-hoc
assumptions, including that the universe is finite only in one spatial
direction, an assumption that entirely contradicts the assumptions of the
inflationary model of the Big Bang, the only model generally accepted by the
Big Bang supporters.
Lerner concludes that
«Wright is Wrong». So, the meaning of «temperature of
space» used by Eddignton is the same meaning of CMB.
Regener
Cosmic rays were discovered
in 1912 by V.F. Hess (Rossi 1964). He made a balloon flight and observed that a
charged electroscope would discharge faster at high altitudes than at the sea
level, contrary to expectations. This discharge is due to the ionization of the
air, which was shown to increase with altitude. It was known that radiation
emitted by radioactive substances ionized the air, and Hess’s measurements
showed that the radiation responsible for the natural ionization of air entered
the atmosphere from above, and not from the ground.
In 1928 R.A. Millikan and Cameron (1928) found that the total energy of
cosmic rays at the top of the atmosphere was one-tenth of that due to starlight
and heat. In 1933 E. Regener (1933) concluded that
both energy fluxes should have essentially the same value. This is a very
important result with far reaching cosmological implications: It indicates that
the energy density of starlight due to our own galaxy is in equilibrium with
the cosmic radiation, which for the most part is of extragalactic origin. It
has always been difficult to know exactly the origin of the cosmic rays, but
the fact that a major part of its components originated outside our galaxy was
inferred from another measurement of Millikan and
Cameron (1928). In this work they showed that the intensity of the radiation
coming from the plane of the Milky Way was the same as that coming from a plane
normal to it. This isotropy clearly indicated an extragalactic origin.
Regener’s work in
general has been described briefly by Rossi (1964) as follows:
In
the late 1920s and early 1930s the technique of self-recording electroscopes
carried by balloons into the highest layers of the atmosphere or sunk to great
depths under water was brought to an unprecedented degree of perfection by the
German physicist Erich Regener and his group. To
these scientists we owe some of the most accurate measurements ever made of
cosmic-ray ionization as a function of altitude and depth.
In his work of 1933, Regener says the following (we are here replacing the term Ultrastrahlung – ultraradiation
– which Regener and others utilized at that time by
the expression "cosmic radiation", as this radiation is called
nowadays):
However,
the density of energy produced by cosmic rays, which is nearly equal to the
density of light and heat emitted by the fixed stars, is very interesting from
an astrophysical point of view. A celestial body with the necessary dimensions
to absorb the cosmic rays – in case of a density of 1, a body with a diameter
of several meters (5 meters of water absorb 9/10 of the cosmic rays) – will be
heated by cosmic rays. The increase in temperature will be proportional to the
energy of absorbed cosmic rays (SU) and the surface (O). The
temperature of the body will increase until the heat it emits – in case of
black body radiation s .
T4 . O – reaches
the same value. We then obtain a final temperature of
T
= .
Substituting
numerical values we obtain 2.8 K.
This, according to Regener (1933), would be the temperature characteristic of
intergalactic space, since in this region the light and heat from any galaxy
would be negligible.
Nernst
The work of Regener was discussed by the famous physicist Walther Nernst (1864-1941) who received the Nobel prize for chemistry in 1920 for his third law of
thermodynamics (1906). By 1912 Nernst had developed
the idea of an Universe in a stationary state. He
expressed this idea in simple terms in 1928: «The Universe is in a stationary
condition, that is, the present fixed stars cool continually and new ones are
being formed» (Nernst 1928). In 1937 he developed
this model and proposed a tired light explanation of the cosmological redshift, namely, the absorption of radiation by the luminiferous ether, decreasing the energy and frequency of
galactic light (Nernst 1937). This would not be due
to a Doppler effect according to Nernst. In this work
Nernst also mentions Regener’s
important paper discussed above.
The following year Nernst (1938) published another paper discussing the
radiation temperature in the Universe. Here he arrived at a temperature in
intergalactic space as 0.75 K. Once more he discusses Regener’s
work and asserts that the cosmological redshift is
not due to a Doppler effect.
In the works of Eddington, Regener, Nernst and others to follow, it is important to stress the
utilization of Stefan-Boltzmann’s law, which is
characteristic of a black body radiation. Another point to be noted is that the
energy densities of these radiations (due to star light and cosmic rays, for
instance) have been measured to have the same value, indicating a situation of
dynamical equilibrium. Sciama describes this
situation as follows (Sciama 1971):
The
cosmic ray flux almost certainly fills the Milky Way, and corresponds to an
energy density in interstellar space of about 1 eVcm-3 (10-12ergcm-3).
This is comparable with the energy of starlight, the turbulent kinetic energy
density of the interstellar gas and, as we shall see later, the energy density
of the interstellar magnetic field. This is the basis of our statement that the
cosmic rays are dynamically important. They constitute a relativistic gas whose
energy and pressure cannot be ignored. The near-equality of the various energy
densities is probably no accident, but despite many attempts a full
understanding of it has not yet been achieved.
And again on p. 185, after
mentioning Penzias and
From
a laboratory point of view 3 °K is a very low temperature. Indeed to
measure it the microwave observers had to use a reference terminal immersed in
liquid helium. Nevertheless from an astrophysical point of view 3 °K
is a very high temperature. An universal black body
radiation field at this temperature would contribute an energy density
everywhere of 1 eVcm-3. As we saw in chapter 2 [p.25] this is just
the energy density in our Galaxy of the various modes of interstellar
excitation – starlight, cosmic rays, magnetic fields and turbulent gas clouds.
So even in our Galaxy the cosmological background radiation would be for many
purposes as important as the well-known energy modes of local origin.
We would like to make two
remarks here. The first is that the main part of the cosmic radiation may have
an extragalactic origin (see the comment on the work of Millikan
and Cameron above), as may the magnetic fields which fill all space. If this is
the case, then three extragalactic modes of excitation (the cosmic ray flux,
magnetic fields and the CBR) would be in thermal equilibrium with one another
and with energy fields generated inside our own galaxy, such as starlight and
turbulent gas clouds. The easiest way to understand this fact is to conclude
that the Universe as a whole is in a state of dynamical equilibrium.
McKellar and Herzberg
Here we would like to
mention briefly the work of Herzberg in 1941 (based
on observations made by A. McKellar) discussing cyanogen measurements in interstellar space. Herzberg found a temperature of 2.3 K characterizing the
observed degree of excitation of the CN molecules if they were in equilibrium
in a heat bath (Herzberg):
The
observation that in interstellar space only the very lowest rotational levels
of CH, CH+, and CN are populated is readily explained by
depopulation of the higher levels by emission of the far infrared rotation
spectrum (see p. 43) and by the lack of excitation to these levels by
collisions or radiation. The intensity of the rotation spectrum of CN is much
smaller than that of CH or CH+ on account of the smaller dipole
moment as well as the smaller frequency [due to the factor v4 in (I, 48)]. That is why lines from the second lowest level (K =
1) have been observed for CN. From the intensity ratio of the lines with K = 0
and K = 1, a rotational temperature of 2.3 K follows, which has of course only
a very restricted meaning.
Obviously there is a great
meaning in this result, although it was not recognized by Herzberg.
This is discussed by Sciama (1971). It should only be
stressed that once more, this result was not obtained utilizing the Big Bang
cosmology.
Finlay-Freundlich and Max
Born
In 1953–4 Finlay-Freundlich (1953, 1954a,b)
proposed a tired light model to explain the redshift
of solar lines and some anomalous redshifts of
several stars, as well as the cosmological redshift.
He proposed a redshift proportional to the fourth
power of the temperature, and his work was further analysed
by max Born (1953, 1954). His formula is as follows: D n = - A T 4l, where D n is the
change in frequency of the line, n is the original frequency, A is a constant, T the temperature of the
radiation field and l the length of path traversed through the radiation field.
What matters to us here is his discussion (1954b) of the cosmological redshift:
§
6. The Cosmological Red Shift
The
fundamental character of the effect under consideration raises, necessarily,
the question whether it might not also be the cause of the cosmological red
shift which hitherto has been interpreted as a Doppler effect. In this case,
the influence of the factor l in formula (1) is given explicitly from
observations. The observed red shift D l ¤ l increases for every million parsec (= 3 x 1024
cm) by 0.8 x 10-3 which corresponds to a velocity increase of 500 km/sec
when interpreted as a Doppler effect. An increase by 10 km/sec – corresponding
to the red shift in a B2 star with TB = 20000 K – would correspond
to a path ls = 1.2 x 1023 cm.
As
far as the mean temperature TS of intergalactic space is concerned, apart
from the knowledge that it must be near the absolute zero, no reliable
information is available. If we may interpret the cosmological red shift in the
same way as the stellar red shifts, the following equation should hold:
TS4lS
= T4BlB , or TS
= TB (lB/lS)1/4
. (3)
"Equation
(3) shows that the value TS obtained in this way does not depend
strongly on the choice of lB. Taking for lB the two extremes values 107 cm and
109 cm, we get the following two reasonable
values
TS
= 1.9 K and TS = 6.0 K
In a recent paper Gamow
(1953) [Gamow, G., 1953, Dan. Acad.-Phys. Section, 27, No. 10] derives a value for TS of 7 K from thermodynamical considerations assuming a mean density of
matter in space of 10-30 g/cm3.
One
may have, therefore, to envisage that the cosmological red shifts is not due to
an expanding Universe, but to a loss of energy which light suffers in the
immense lengths of space it has to traverse coming from the most distant star
systems. That intergalactic space is not completely empty is indicated by Stebbins and Whitford’s discovery
(1948) [Stebbins, J., and Whitford,
A.E., 1948, Ap. J., 108, 413] that the cosmological
red shift is accompanied by a parallel unaccountable excess reddening. Thus the
light must be exposed to some kind of interaction with matter and radiation in
intergalactic space.
The main points to
emphasize here are that Finlay-Freundlich proposed an
alternative to the Doppler interpretation of the cosmological redshift and arrived at 1.9 K < T < 6.0 K for the temperature of
intergalactic space. This is quite remarkable.
It is important to quote
here Max Born (1954) when discussing Finlay-Freundlich’s
proposal that this new effect might be due to a photon-photon interaction,
namely
An
effect like this is of course not in agreement with current theory. It has,
however, an attractive consequence. A simple application of the conservation laws of energy and momentum shows that a collision of this kind is only
possible if a pair of particles with opposite momenta
is created. The energy of one of these is hn
’ = - h d n
/ 2, where d
n
is given by (6) [d
n
= - Cn
/
n
o]. If the
secondary particles are photons their frequency is of the order of radar waves
(for the sun v’~ 2 x 109 sec-1, l
’ ~ 15 cm). Thus the red-shift is linked to
radio-astronomy.
We need only remember here
the work of Penzias and Wilson 11 years later with a
horn antenna built to study radio waves which found the CBR with a
characteristic wavelength of 7 cm ... This must be considered a highly
successful prediction by Max Born!
Gamow and
Collaborators
As we have seen, Finlay-Freundlich (1954b) mentioned that Gamow had derived the value of 7 K for intergalactic space
in 1953. Prior to this work we could only find two other papers where there was
a prediction of this temperature by Gamow’s
collaborators Alpher and Herman (1948, 1949). In the
first of these works they said: «The temperature of the gas at the time of
condensation was 600 K, and the temperature in the Universe at the present time
is found to be about 5 K. We hope to publish the details of these calculations
in the near future».
In the second of these
works, where the present the details of these calculations, they said the
following (our emphasis in bold):
In
accordance with eq. (4) [r rr
m-4/3
= constant], the specification of r m’’
, r m’,
and r
r’, fixes the
present density of radiation, r r’’.
In fact, we find that the value of r r’’
consistent with eq. (4) is
r
r’’ @
10-22 g/cm3, (12d)
which
corresponds to a temperature now of the order 5 K. This
mean temperature for the Universe is to be interpreted as the background
temperature which would result from the universal expansion alone. However,
the thermal energy resulting from the nuclear energy production in stars would
increase this value.
From this it is evident
that their prediction in 1948 was T » 5 K and in 1949 they obtained a temperature greater than 5 K, although
close to this value.
The only other prediction
of this temperature by Gamow known to us prior to Penzias and Wilson discovery (beyond that of 7 K in 1953)
was published by Gamow (1961) in his book The
Creation of the Universe. The first edition of this book is from 1952, and
here we quote from the revised edition of 1961, only four years before Penzias and Wilson. In this book there is only one place
where he discusses the temperature of the Universe, namely [21, p.42, our
emphasis in bold]:
The
relation previously stated between the value of Hubble’s constant and the mean
density of the Universe permits us to derive a simple expression giving us the
temperature during the early stages of expansion as the function of the time
counted from the moment of maximum compression. Expressing that time in seconds
and the temperature in degrees (see Appendix, pages 142-143), we have:
Temperature
=
Thus
when the Universe was 1 year old, and 1 million year old, its temperatures were
15 billion, 3 million, and 3 thousand degrees absolute, respectively. Inserting
the present age of the universe (t = 1017 sec) into that
formula, we find
Tpresent
= 50 degrees absolute
Which is in reasonable agreement with the actual
temperature of interstellar space.
Yes, our Universe took some time to cool from the blistering heat of its early
days to the freezing cold of today!
We discuss these
predictions by Gamow and collaborators below.
Discussion and Conclusion
In most textbooks nowadays
we see the statement that Gamow and collaborators
predicted the 2.7 K temperature prior to Penzias and Wilson,
while the steady-state theory of Hoyle, Narlikar and
Gold did not predict this temperature. Therefore the correct prediction of the
2.7 K is hailed as one of the strongest arguments in favour
of the Big Bang. However, these two models have one very important aspect in
common: both accept the interpretation of the cosmological redshift
as being due to a Doppler effect, which means that both models accept the
expansion of the Universe.
But there is a third model
of the Universe which has been developed in this century by several scientists
including Nernst, Finlay-Freundlich,
Max Born and Louis de Broglie (1966). It is based on
a Universe in dynamical equilibrium without expansion and without continuous
creation of matter. We reviewed this subject in earlier papers (Assis 1992, 1993). Although it is not considered by almost
any textbook dealing with cosmology nowadays, this third model proves to be the
most important one of all of them.
In order to understand how the
textbooks could neglect equilibrium cosmology so completely, it is worthwhile
to quote a letter sent by Gamow to Arno Penzias, in 1965 after Penzias and Wilson’s discovery (curiously the letter was
dated 1963 ...). This letter was reproduced in Penzias’s
article (1972), from which we quote:
Thank
you for sending me your paper on 3 K radiation. It is very nicely written
except that "early history" is not "quite complete". The
theory of, what is now known, as, "primeval fireball", was first
developed by me in 1946 (Phys. Ver. 70, 572, 1946;
74, 505, 1948; Nature 162, 680, 1948). The prediction of the numerical value of
the present (residual) temperature could be found in Alpher
& Hermann’s paper (Phys. Ver. 75, 1093, 1949) who
estimate it as 5 K, and my paper (KongDansk.
Ved.
Sels 27
no. 10, 1953) with the estimate of 7 K. Even in my popular book Creation of the Universe (Viking 1952) you can find on p. 42) the
formula T = 1.5 x 1010 / t1/2 K, and the upper limit of
50 K. Thus, you see the world did not start with almighty Dicke.
Sincerely,
G.
Gamow
This letter, as we have
seen, does not correspond to the true facts. Gamow,
in the revised edition of his book of 1952, published in 1961, calculated a
temperature. Thus, in this work Gamow did not
estimate an upper limit of 50 K. The need for Gamow
to convince everybody that he had predicted correctly, and before everyone
else, the temperature of the cosmic background radiation is evident from
another part of Penzias’s paper (1972):
It
is beyond the scope of this contribution to weigh the various theoretical
explanations of the 3 K. Still the unique claim of the hot evolving Universe
theory is that it predicted the background radiation before the fact. At the 4th
"
As we have seen in this
paper, Gamow and collaborators obtained from T » 5 K to T
= 50 K in monotonic order (5 K, ³ 5 K, 7 K and 50 K)... These are quite poor predictions compared with
Guillaume, Eddington, Regener
and Nernst, McKellar and Herzberg, Finlay-Freundlich and
Max Born, who arrived at, respectively: 5 K < T < 6 K, T = 3.1 K, T = 2.8 K,
1.9 K < T < 6.0 K!
All of these authors obtained these values from measurements and or theoretical
calculations, but none of them utilized the Big Bang. This means that the
discovery of Penzias and Wilson cannot be considered
decisive evidence in favour of the Big Bang. Quite
the contrary, as the models of a Universe in dynamical equilibrium predicted
its value before Gamow and with better accuracy. And
not only this, Max Born also predicted that the cosmological redshift and the cosmic background radiation should be
related with radio astronomy eleven years before the discovery of the CBR by Penzias and Wilson utilizing a horn reflector antenna built
to study radio emissions!
Our conclusion is that the
discovery of the CBR by Penzias and Wilson is a
decisive fact in favour of a Universe in dynamical
equilibrium, and against models of an expanding Universe, such as the Big Bang
and the steady-state.
Acknowledgments
The
authors with to thank Dr. Anthony Peratt for bringing
Guillaume’s paper to their attention. A.K.T.A.
wishes to thank CNPq, FAPESP and FAEP for financial
support in the past few years. M.C.D.N. wishes to thank CNPq,
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Posted: April 30,
2008; last revision: May 12, 2008
Scienza e
Democrazia/Science and Democracy