Sections
It's big, it's complex, it's a morass.
We try to find a path through without sinking into the mire.
First let's look at the galaxies in Seyfert's Sextet in the figure above (local link / general link: seyfert_sextet.html) and the figure below (local link / general link: seyfert_sextet.html) to get a preview.
php require("/home/jeffery/public_html/astro/galaxies/seyfert_sextet_2.html");?>
Let's have a look at the man himself.
See the figure below
(local link /
general link: carl_seyfert.html)
A general remark, NOT to be forgotten, is that stars, dust, gas,
and, we believe,
dark matter
essentially orbit the
centers of mass
of
galaxies.
The orbits are, however, constantly being perturbed by interactions
with other stars, dust, gas, and, perhaps,
dark matter, and
so are non-repeating and somewhat chaotic.
After all it is very slow on the human time scale.
Typically, orbital periods
are of order 100 million years.
Of course, only matter with line spectra
show the Doppler effect.
So for dark matter and other matter
without line spectra, the motion is
only inferred.
php require("/home/jeffery/public_html/astro/astronomer/carl_seyfert.html");?>
Dark matter (NOT including
baryonic (i.e., ordinary-matter) dark matter)
is peculiar case.
Recall that dark matter is a gas of
particles that interact with other matter and each other only very weakly (except through
gravity).
It interacts so weakly that it has virtually zero pressure force.
As result I think that the
dark matter particles
must individually follow chaotic
orbits and NOT move as clumps of matter
the way an ordinary gas with
pressure would.
Question:
How do we know observationally
about the motion of matter in galaxies?
Note also the disk orbital motion is
differential---disks do NOT
rotate like rigid bodies.
Answer 3 is right. However, answer 1 would be partially right too without the first sentence.
There are some units and distance scales that it is convenient to note or recapitulate for a start. See the listing in the insert below (local link / general link: astronomical_distances_larger.html).
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Now what we can see of the
observable universe
(whose radius is given in the table above)
is a sphere centered on us.
To explicate, see the artist's conception of the observable universe in the figure below (local link / general link: cosmos_artist_conception.html).
To further explicate the observable universe, consider the 2 diagrams in the figure below (local link / general link: observable_universe_cartoon.html).
php require("/home/jeffery/public_html/astro/cosmol/observable_universe_cartoon.html");?>
What is the observable universe
made of? See the figure below
(local link /
general link: pie_chart_cosmic_energy.html).
php require("/home/jeffery/public_html/astro/cosmol/pie_chart_cosmic_energy.html");?>
Edwin Hubble (1889--1953) beginning in the 1920s developed the first galaxy morphological classification (see Wikipedia: Hubble sequence; No-508--510). It is is still in use today
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Hubble's classification scheme is called the
Hubble sequence---Hubble
probably didn't call it that himself---there's
Hubble this and Hubble that nowadays.
See figure below
(local link /
general link: alien_hubble.html).
php require("/home/jeffery/public_html/astro/alien_images/alien_hubble.html");?>
The main galaxy types in the Hubble sequence
are
spiral (S),
barred spiral (SB),
elliptical (E),
lenticular (S0 and SB0),
and
irregular galaxy (Irr).
These galaxy types are divided into
subtypes which we discuss below
in subsection The Hubble Sequence Explicated.
If one says spirals without qualification, one often means both spirals and barred spirals, unless one doesn't---context must decide.
Ellipticals and lenticulars are often called early-type galaxies and spirals, late-type galaxies.
This is astro-jargon has NO physical meaning: early-type galaxies are NOT early and late-type galaxies are NOT late. Hubble himself emphasized that the Hubble sequence originated as a purely empirical galaxy morphological classification without theoretical understanding or bias (see Wikipedia: Hubble seqence: Physical significance).
In fact, the main channel for creating ellipticals is galaxy mergers of spirals. This process is enhanced in rich galaxy clusters where galaxy collisions are enhanced (FK-602).
We take up the subject of galaxy evolution in IAL 29: The Large-Scale Structure of the Universe.
Answer 2 is right. See No-510.
Also note Hubble announced the discovery of the expansion of the universe in 1929 (see Wikipedia: Edwin Hubble: Redshift increases with distance; No-523). It was the observational discovery. The expansion of the universe had been theoretically predicted from general relativity earlier in the 1920s by Alexander Alexandrovich Friedmann (1888--1925) and Georges Lemaitre (1894--1966).
Einstein completed general relativity by 1915 (see Wikipedia: History of general relativity; St. Andrews Mathematics Archives: Einstein biography).
The Hubble sequence is best illustrated by a
Hubble tuning-fork diagram such
as the one shown in
the figure below
(local link /
general link: galaxy_hubble_sequence.html).
The Hubble sequence was
extended by
Gerard de Vaucouleurs (1918--1995)
in the
de Vaucouleurs system as we call it now.
The figure below
(local link /
general link: galaxy_vaucouleurs.html)
illustrates the
de Vaucouleurs system
php require("/home/jeffery/public_html/astro/galaxies/galaxy_hubble_sequence.html");?>
Table:
Some Galaxy Properties for the Local Universe
below gives some of the properties of
galaxies classified by the
Hubble sequence types
for the
local universe
(which is also the modern universe as you
recall from IAL 26: The Discovery of Galaxies).
Table: Some Galaxy Properties for the Local Universe
Property S and SB galaxies E galaxies Irr galaxies
Mass 10**9 -- 4*10**11 10**5 -- 10**13 10**8 -- 3*10**10
(M_sun) baryonic matter only all matter baryonic matter only
baryonic matter
about 1/6
to 1/30
of all matter
Luminosity 10**8 -- 2*10**10 3*10**5 --10**11 10**7 -- 10**9
(L_☉)
Diameter 5 -- 250 1 -- 200 1 -- 10
(kpc)
Stellar arms: young Pop I; Pop II and mostly Pop I
population bulge and disk: old Pop I
old Pop I and Pop II
halo: Pop II
Percentage 77 20 3
observed
NOT counting numbers of ordinary
many dwarf spirals and barred
ellipticals? spirals are comparable.
Color blue/pink/dark yellow blue/pink mostly?
depends yellow in bulge
mainly
star ages
Gas and Dust thick in arms very little generally rich
and throughout disk obvious matter
but probably
significant
very hot, nearly
invisible hot gas
seen in X-ray band
References:
CK-393,
Dekel et al. (2019)
(for the baryonic to total matter ratio),
FK-565,582,583,585,
Wikipedia:
Elliptical galaxy: Sizes and shapes.
Notes:
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Form groups of 2 or 3---NOT more---and tackle Homework 28 problems 2--5 on galaxies and galaxy types.
Discuss each problem and come to a group answer.
Let's work for 5 or so minutes.
The winners get chocolates.
See Solutions 28.
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php require("/home/jeffery/public_html/astro/videos/ial_028_galaxies.html");?>
php require("/home/jeffery/public_html/astro/art/art_c/chocolate_easter_bunny_2.html");?>
They are a bland boring white/yellow in true color. NOT nearly as interesting to look at as spiral galaxies.
Ellipticals have a tremendous range in mass from ∼ 10**5 M_☉ (smallest dwarf ellipticals) to 10**13 M_☉ (the largest giant ellipticals which are called cD elliptical galaxies).
The stars in ellipticals orbit in all random orientations (FK-585).
Answer 1 is right.
Each star in an elliptical has its own angular momentum that keeps it from falling to the center. But the summing the random angular momentum components, there is a great deal of cancellation and the net angular momentum will be relatively small compared to spirals where the disk stars rotate in one direction.
Angular momentum is actually a vector quantity, but we will say no more on that topic.
Nowadays, we know that at least large-mass ellipticals probably have significant ionized gas (i.e., hydrogen ion (H**(+) gas), but it is kept very hot by outflows from the central supermassive black hole (which in turn is fed by inflows from the intergalactic medium (IGM)), and is so nearly invisible, except in the X-ray band. The fact that the gas is very hot gives it high pressure, and so keeps it from undergoing gravitational collapse leading to star formation or the outflows push out the cold gas. The overall process can be called AGN feedback (see Wikipedia: Galaxy quenching).
What of low-mass ellipticals (which in many cases are dwarf ellipticals)? Interaction with their environments seems to remove low-temperature gas by processes that could be galaxy ram-pressure stripping, galaxy strangulation, or galaxy virial shock heating (see Wikipedia: Galaxy quenching).
It also seems to yours truly's that once a galaxy has lost its interstellar dust (by e.g., galaxy ram-pressure stripping or "evaporation" by electromagnetic radiation (EMR)), it is hard to get star formation going again since star formation occurs in molecular clouds that form in thick nebulae of interstellar dust. To oversimplify the hypothesis is that lack of interstellar dust leads to lack of star formation that leads to lack of interstellar dust that comes from mainly from post-main-sequence stars (which become very spread out in cosmic time because the slow stellar evolution of low-mass stars) and supernovae.
So ellipticals usually have very little
star formation.
They are, in modern jargon, usually
quenched galaxies
or
red sequence galaxies.
Q&A:
The
OB stars
and A stars
have masses greater than about 1.4 M_☉
(see Wikipedia: A-type main-sequence star),
and thus have lifetimes shorter than about 3 Gyr
(see Wikipedia:
File:Representative lifetimes of stars as a function of their masses).
Answer 2 is right.
There are actually supposed to have been
Population III stars:
these were the first stars and they were extremely metal-poor.
They must have had a little lithium
from the Big Bang.
They were probably all massive and exploded early on.
None survive that we know of.
Answer 1 is a standard definition of a
metal.
Answer 2 is the astro jargon
definition of metals.
First, the morphology: the subtypes of ellipticals
range from E0 (most round on the sky) to E7 (to most elongated on the sky).
These subtypes are NOT completely intrinsic characterizations of
the true 3-dimensional shapes
of the ellipticals.
The subtypes also depend on the
on the orientation of the ellipticals
on the sky.
This is unlike the situation with
spirals
(the term here includes barred spirals)
(see below), where we usually can determine the subtype
independent of
orientation on the sky (see below).
Second the color.
Without many blue
stars
and much interstellar medium (ISM),
all that is left are yellow and red
stars to give color to
ellipticals.
Thus,
ellipticals
look bland yellow in color.
On most images, they
are over-exposed bright near their centers where the stars
are dense and then decrease in brightness as you move away from the center
and the density of stars falls.
The figure below
(local link /
general link: galaxy_cluster_abell_s740.html)
shows a typical elliptical
located in a rich galaxy cluster.
There are a lot of them, but they are small and NOT so obvious as large
ellipticals.
The smallest
dwarf ellipticals
are comparable to globular clusters in mass,
but are less compact I think????.
Recall the distinction between
dwarf ellipticals and
globular clusters.
Since they are galaxies,
dwarf ellipticals underwent
generations of star formation
before
galaxy quenching.
Since they are star clusters,
globular clusters formed
their stars all in one episode or nearly of
star formation.
The dwarf ellipticals
are quite transparent due their few
stars (less than a few times 10**6) and lack of obvious
interstellar medium
(i.e., dust and gas): you can see right through them
(FK-584).
This is provided that their
point spread functions
don't overlap in an image.
The galaxy group
in the figure below
(local link /
general link: galaxy_hcg_87.html)
shows
unquenched
spiral galaxies
and a
quenched
elliptical galaxy.
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Question: What stars are metal-poor and formed in the
early universe?
Question: Metals are:
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Answers 1 and 2 are right. Answer 3 is close.
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The figure below
(local link /
general link: m87_virgo.html)
shows another
elliptical:
M87 (NGC 4486) in
the Virgo Cluster
in Virgo.
php require("/home/jeffery/public_html/astro/galaxies/m87_virgo.html");?>
M87 (NGC 4486)
in its region of the Virgo Cluster
is shown in the figure below
(local link /
general link: galaxy_cluster_virgo.html).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_cluster_virgo.html");?>
The locations of M87
in constellation
Virgo
and the Virgo Cluster
in constellations
Virgo and
Coma Berenices
are shown in the figure below
(local link /
general link: iau_virgo.html).
php require("/home/jeffery/public_html/astro/constellation/iau_virgo.html");?>
A point spread function (PSF)
if the response of an imaging system to a point source.
Frequently, a PSF
is also used to mean the finite blob in an image
which is recorded for an unresolved point object.
The blob being the result of the PSF.
See the figure below
(local link /
general link: galaxy_fornax_dwarf.html)
of a nearby
dwarf spheriodal galaxy (dSph)
(which is much like a
dwarf elliptical).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_fornax_dwarf.html");?>
The SO (unbarred) and SBO (barred) lenticular galaxies have a bulge and a disk, but NO or ILL-DEFINED spiral arms (FK-584). They can have significant interstellar dust in their galactic disks.
Lenticular galaxies are sort of middle case between ellipticals and spirals.
They are usually galaxy quenched.
An example lenticular galaxy is shown in the figure below (local link / general link: galaxy_lenticular_ngc_2787.html).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_lenticular_ngc_2787.html");?>
Lenticular galaxy formation
is uncertain.
There are several theories all of which may be right in some cases since there may be multiple formation channels which may also overlap.
Yours truly thinks the two most likely theories currently are:
But why isn't the gas replaced by inflows of intergalactic medium (IGM)? Maybe the lenticulars are just in a low density region of IGM. Or maybe the lenticulars have fallen into galaxy clusters and had their interstellar gas stripped by galactic ram pressure stripping.
Another possibility is that there may be a lack of galaxy interaction to excite spiral density waves.
More extreme galaxy merger are probably the main channel for creating ellipticals other than dwarf ellipticals???.
Typically, spirals typically 2 major ones ??? plus maybe smaller or fragmentary ones: e.g., the Milky Way: see figure below (local link / general link: milky_way_map.html).
php require("/home/jeffery/public_html/astro/galaxies/milky_way_map.html");?>
There may also be isolated arm segments: e.g., the Orion arm
segment in the
Milky Way
which the Sun is just outside of
(FK-563).
The spiral arms rotate in the direction you would think: i.e., the spiral arms are trailing with the ends pointing opposite to the direction of orbital rotation.
There is one exception: NGC 4622 has leading spiral arms. See the figure below (local link / general link: galaxy_spiral_ngc_4622.html).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_spiral_ngc_4622.html");?>
We know the direction of rotation of the arms, stars, and gas
from spectroscopy of the
spirals
and the
Doppler effect.
See
IAL 7: Spectra
for more on the
Doppler effect.
Spirals probably mostly have luminous halos and dark matter halos like the Milky Way.
The extents of the luminous halos are harder to see for remote galaxies, of course.
Galaxy rotation curves (see the section Galaxy Rotation Curves below) indicate massive dark matter halos just as they do for the Milky Way (FK-600).
The closest spiral to the Milky Way (NOT counting itself, of course) is the Andromeda Galaxy (M31). See the collage figure below (local link / general link: m31_002_noao_moon.html).
php require("/home/jeffery/public_html/astro/galaxies/m31_002_noao_moon.html");?>
The Hubble types are:
References: CK-388; FK-583; Wikipedia: Spiral galaxy.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_hubble_sequence.html");?>
Note that spirals
can be at any orientation to the Earth
observer from face-on to edge-on.
The arms of edge-on spirals are hard to see, but the shape of the bulge (which is correlated with the arms) permits the Hubble type to be distinguished.
Except, it is sometimes hard to tell if there is a bar or NOT.
In the figure below (local link / general link: galaxy_sombrero.html) is a famous example of an Sa spiral galaxy.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_sombrero.html");?>
The figure below
(local link /
general link: galaxy_whirlpool.html)
shows a famous
Sc spiral galaxy.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_whirlpool.html");?>
The Hubble types are:
References: CK-392; FK-583; Wikipedia: Barred spiral galaxy.
See the Hubble tuning fork diagram in the figure below (local link / general link: galaxy_hubble_sequence.html).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_hubble_sequence.html");?>
Note the
barred spirals (like ordinary spirals) can be
at any orientation to the Earth observer from face-on to
edge-on.
The arms of edge-on barred spirals are hard to see, but the shape of the bulge (which is correlated with the arms) permits the spiral type to be distinguished.
The figure below (local link / general link: galaxy_spiral_m83.html) shows an example of SABc (i.e., intermediate spiral galaxy which is a barred spiral with a small bar) seen face-on.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_spiral_m83.html");?>
The Milky Way
is a barred spiral:
an SBb or SBc or somewhere in between
(see
Milky Way: Composition and structure).
It's hard to classify Milky Way exactly because we don't have a good overall view---"can't see the forest for the trees."
A real image of a galaxy that resembles the Milky Way (i.e., the Milky Way twin) is shown in the figure below (local link / general link: milky_way_ngc_6744.html).
php require("/home/jeffery/public_html/astro/galaxies/milky_way_ngc_6744.html");?>
Actually, there are two subtypes: Irr I's with some of ordered structure and Irr II's which are badly disordered and may often have resulted from violent collisions with other galaxies (FK-585--586).
Irregulars are generally smaller than the large spirals and ellipticals.
They are typically rich in dust and gas, and have young and old stars and STAR FORMATION. The Large Magellanic Cloud (LMC) is the nearest (at about 50 kps) and most famous irregular: an Irr I (FK-500, 585). See figure below (local link / general link: galaxy_lmc.html).
php require("/home/jeffery/public_html/astro/galaxies/galaxy_lmc.html");?>
Question: Amerigo Vespucci (1454--1512)
is most famous for:
I have no idea, but see the figure below
(local link /
general link: amerigo_vespucci.html).
php require("/home/jeffery/public_html/astro/art/art_a/amerigo_vespucci.html");?>
Of order 5 % of the
emitted photons
will at least
be scattered by
free electrons
by Thomson scattering on a time scale equal to the
age of the observable universe = 13.797(23) Gyr (Planck 2018)
(see
NASA: Optical depth
τ
since reionization) on a time scale equal to the
age of the observable universe = 13.797(23) Gyr (Planck 2018).
php require("/home/jeffery/public_html/astro/galaxies/spiral_arms_bars.html");?>
Question: By the by, what ultimately probably happens to most of
the light energy from
stars,
galaxies,
etc.?
What happens to the
energy of the
photons when they
cosmological redshift
if we have
conservation of energy?
Answer 3 is right.
Yours truly is embarrased to admit that energy conservation as a simple scalar quantity is NOT maintained in contexts of general relativity with expanding space. The Einstein field equations embody energy conservation in a general relativity sense and that is all one can say (see Sean Carroll, 2003, Spacetime and Geometry: An Introduction to General Relativity, p. 120).
The photon energy just vanishes with the cosmological redshift.
We take up the expansion of the universe in IAL 30: Cosmology: The Expansion of the Universe.
Form groups of 2 or 3---NOT more---and tackle
Homework 28
problems 6--15 on
galaxies
and galaxy types.
Discuss each problem and come to a group answer.
Let's work for 5 or so minutes.
The winners get chocolates.
See Solutions 28.
php require("/home/jeffery/public_html/astro/art/art_c/chocolate_fountain_3.html");?>
Group Activity:
php require("/home/jeffery/public_html/astro/videos/ial_0000_standards.html");?>
php require("/home/jeffery/public_html/astro/videos/ial_028_galaxies.html");?>
php require("/home/jeffery/public_html/astro/art/art_c/chocolate_fountain_2.html");?>
What the rotation curves should be for the observed visible baryonic matter (mainly stars) can be predicted using classical physics (i.e., Newtonian physics and Newton's law of universal gravitation).
But the predictions are almost always too low.
The rotation curves show that there is several times more dark matter than visible baryonic matter (mainly stars). The ratio of visible baryonic matter (mainly stars) to dark matter in galaxies is quite various it seems and ranges from ∼ 1/30 to ∼ 1/10.????
The animation in the figue below (local link / general link: galaxy_rotation.html) shows how a spiral galaxy rotates without and with dark matter.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_rotation.html");?>
The figure below
(local link /
general link: galaxy_rotation_cartoon.html)
gives a cartoon
galaxy rotation curve plot.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_rotation_curve_cartoon.html");?>
The motions of
galaxy clusters
and
galaxy superclusters
also show evidence for
dark matter.
The first evidence of dark matter was found by Fritz Zwicky (1898--1974) in 1933 from studying the motions of the galaxy cluster the Coma Cluster (see English and Spanish Translation of Zwicky's (1933) The Redshift of Extragalactic Nebulae (Die Rotverschiebung von extragalaktischen Nebeln)). Zwicky coined the term for dark matter for dark matter. More precisely he said dunkle materie, but that translates from German to dark matter.
However, it wasn't until circa 1980 that dark matter became a widely accepted theory.
What is dark matter?
Some of it is hot intergalactic hydrogen and helium gas which is usually called intergalactic medium (IGM).
Some of it is probably unseen neutron stars and black holes.
But these contributions must be minor if Big Bang cosmology is correct---and Big Bang cosmology is a very solidly established theory these days.
Big Bang cosmology dictates how much ordinary matter (i.e., matter made up principally of protons, neutrons, and electrons) there is. (Black holes whatever they are now, were ordinary matter before becoming what they are.)
And the dark matter weighs in at several times this amount.
So it is believed that dark matter is some sort of exotic particle that we have NOT detected---except through its gravitational effects.
It is very weakly interacting, except through its gravity.
The dark matter paticles are thought to be clumped into clouds that are gravitational potential wells.
The biggest potential wells are where galaxies, galaxy cluster, and galaxy superclusters formed.
These structures are, in fact, largely held together by their dark matter.
What is the dark matter particle?
There are many theoretical candidates and there are experimental searches for them but at present we've had to no luck.
A second idea about dark matter is that it is NOT an exotic particle, but that it is primordial black holes (PBHs). PBHs formed in the Big Bang, but before Big Bang nucleosynthesis (BBN, cosmic time ∼ 10--1200 s ≅ 0.17--20 m)---and so they do NOT spoil the good results of BBN. For some explication of primordial black holes (PBHs), see the figure below (local link / general link: black_hole_primordial.html).
php require("/home/jeffery/public_html/astro/black_hole/black_hole_primordial.html");?>
There is an alternative theory
to dark matter:
MOND (MOdified Newtonian Dynamics)---see the
explication of
MOND,
the Devil,
Dracula,
and the
worst of all possible worlds
in the figure below
(local link /
general link: gravity_mond.html).
php require("/home/jeffery/public_html/astro/gravity/gravity_mond.html");?>
For a slightly long answer, see the figure below (local link / general link: galaxy_quenching.html) for more on galaxy quenching.
Who knows? There are a lot of them.
In the
observable universe there are
estimated to be at least ∼ 2*10**12
galaxies
(see Wikipedia: Observable universe).
But since galaxies get more abundant
as one goes down in mass coordinate, where is the cut-off?
Also, we don't know how far galaxies
extend beyond the observable universe.
Well beyond certainly since we see no boundary effects in the
observable universe, but to infinity?
For an example of the plethora of
galaxies, see
the Hubble Ultra-Deep Field (HUDF, 2003--2004)
in the figure below
(local link /
general link: hubble_ultra_deep_field.html).
Form groups of 2 or 3---NOT more---and tackle
Homework 28
problems 6--15 on
galaxies
and galaxy types.
Discuss each problem and come to a group answer.
Let's work for 5 or so minutes.
The winners get chocolates.
See Solutions 28.
php require("/home/jeffery/public_html/astro/galaxies/galaxy_quenching.html");?>
Are there galaxies without end?
php require("/home/jeffery/public_html/astro/galaxies/hubble_ultra_deep_field.html");?>
php require("/home/jeffery/public_html/astro/art/art_c/chocolate_hot_3.html");?>
Group Activity:
php require("/home/jeffery/public_html/astro/videos/ial_0000_standards.html");?>
php require("/home/jeffery/public_html/astro/videos/ial_028_galaxies.html");?>
php require("/home/jeffery/public_html/astro/art/art_c/chocolate_hot_2.html");?>