Does Space Expand? What Do You Think?

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In summary: In this theory, distance is not absolute, but rather depends on the curvature of spacetime and the observer's frame of reference. The proper distance, as mentioned before, is the length between two events in a frame of reference where they occur simultaneously. However, in GR, this distance can change over time as the curvature of spacetime changes. This allows for the possibility of objects to move away from each other at a rate faster than the speed of light, as long as they are not in the same inertial frame of reference. This is why, in an expanding universe, distant galaxies can appear to be moving away from each other at speeds greater than the speed of light
  • #141
steve watson said:
My problem is with the nature of "space" and what it is or rather what it is not. Nobody seems to be able to give me a straight answer. But everyone seems to think "space" is a "thing" rather than "nothing". If "space" were "nothing" wouldn't that turn a lot of these theories upside down?

It's not a trivial question. For example, if space is the absence of anything, how can it have a permitivity and permeability? What about the Casimir Effect, is that caused by "stuff in space" or is it a property of the vacuum itself? Space may not be a "thing" but it definitely seems to have measurable properties. You might also like to do a search for the term "substantivalism" (be careful with the spelling) and look at the Hole Argument just to get a flavour of this topic:

http://plato.stanford.edu/entries/spacetime-holearg/

Note that the Hole Argument is a problem for manifold substantivalism but perhaps not for metric substantivalism (which the SEP barely mentions).

You should also consider what gravitational waves (as indirectly measured by Hulse and Taylor) and "gravitational wave recoil" imply for the existence of the metric.

http://www.black-holes.org/explore2.html
 
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  • #142
No, it's not a trivial question .. tks for your response and the website info .. it's not easy to understand ...
 
  • #143

Cosmology scale factor equation:
[tex]\frac{\lambda_0}{\lambda_t} = \frac{T_t}{T_0} = \frac{a(t_0)}{a(t)} = 1 + z[/tex]
λCDM redshift at decoupling:
[tex]z = 1090.89[/tex]
CMBR temperature at present:
[tex]T_0 = 2.72548 \; \text{K}[/tex]
[tex]T_t = T_0 (1 + z) = 2.72548 \; \text{K} \times (1 + 1090.89) = 2975.92 \; \text{K}[/tex]
Universe temperature at photon decoupling time t:
[tex]\boxed{T_t = 2975.92 \; \text{K}}[/tex]

However, does the Cosmology scale factor equation also work this way?

Universe total observable radius:
[tex]R_u(t_0) = 4.399 \cdot 10^{26} \; \text{m}[/tex]
[tex]\frac{R_u(t_0)}{R_u(t)} = \frac{a(t_0)}{a(t)} = \frac{T_t}{T_0} = 1 + z[/tex]
[tex]\boxed{a(t_0) = 1}[/tex]
[tex]R_u(t) = a(t) R_u(t_0) = 9.158 \cdot 10^{-4} \times 4.399 \cdot 10^{26} \; \text{m} = 4.028 \cdot 10^{23} \; \text{m}[/tex]
Universe total observable radius at photon decoupling time t:
[tex]\boxed{R_u(t) = 4.028 \cdot 10^{23} \; \text{m}}[/tex]

Reference:
Total amount of energy in the Universe - Orion1 #13
Lambda-CDM model - Parameters - Wikipedia
Scale_factor - Cosmology - Wikipedia
Redshift formulae - Wikipedia
Cosmic microwave background radiation - Features - Wikipedia
Recombination - Cosmology - Wikipedia
Timeline of the Big Bang - Photon epoch
 
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  • #144
Orion1 said:
However, does the Cosmology scale factor equation also work this way?

Universe total observable radius:
[tex]\frac{R_u(t_0)}{R_u(t)} = \frac{a(t_0)}{a(t)} = 1 + z[/tex]
[tex]\boxed{a(t_0) = 1}[/tex]

Yes, in fact that is the definition of a(t). However, that only gives you the ratio of the present size to that at the time of emission. The values you quote of roughly 42 million and 46 billion light years respectively are correct but to get those, you need to find the lookback time first.
 
  • #145

Cosmology scale factor equation:
[tex]\frac{R_u(t_0)}{R_u(t)} = \frac{a(t_0)}{a(t)} = \frac{T_t}{T_0} = 1 + z[/tex]

Universe total observable radius:
[tex]R_u(t_0) = 4.399 \cdot 10^{26} \; \text{m}[/tex]

Cosmic neutrino background radiation temperature at present:
[tex]T_0 = 1.95 \; \text{K}[/tex]

Cosmic neutrino background radiation temperature at neutrino decoupling time t:
[tex]T_t = 1 \cdot 10^{10} \; \text{K}[/tex]

[tex]R_u(t) = R_u(t_0) \left( \frac{T_0}{T_t} \right) = 4.399 \cdot 10^{26} \; \text{m} \times \left( \frac{1.95 \; \text{K}}{1 \cdot 10^{10} \; \text{K}} \right) = 8.578 \cdot 10^{16} \; \text{m}[/tex]

Universe total observable radius at neutrino decoupling time t:
[tex]\boxed{R_u(t) = 8.578 \cdot 10^{16} \; \text{m}}[/tex]

Reference:
Total amount of energy in the Universe - Orion1 #13
Timeline of the Big Bang - Hadron epoch - Wikipedia
Neutrino_decoupling - Wikipedia
Cosmic neutrino background - Wikipedia
Red shift - Highest redshifts
 
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  • #146
Orion1 said:
Universe total observable radius:
[tex]R_u(t_0) = 4.399 \cdot 10^{26} \; \text{m}[/tex]

That figure is for what is observable optically, i.e. the CMBR. We can't observe primordial neutrinos. However, your end result will still be a reasonable rough estimate.
 
  • #147
The rate of expansion (hubble constant) of the universe is equivalent to the sun moving 3/4 of a mile farther away in 100 years. Do the math. The solar wind adds solar particles to the solar system and universe. This causes distant objects to appear ever more distant as space becomes more opague. Space is not empty as recent articles have stated.
 
  • #148
dtyarbrough said:
This causes distant objects to appear ever more distant as space becomes more opague.

That makes no sense, you need to explain why space becoming opaque would change the wavelength of a spectral line.
 
  • #149
dtyarbrough said:
The rate of expansion (hubble constant) of the universe is equivalent to the sun moving 3/4 of a mile farther away in 100 years. Do the math. The solar wind adds solar particles to the solar system and universe. This causes distant objects to appear ever more distant as space becomes more opague. Space is not empty as recent articles have stated.

This is so wrong, I have to question if you have a clue about what you're talking about.

First of all, recessional velocity on large scales requires a frame of reference. The distance from this FoR is then multiplied by a scale factor, Hubble's constant. This is shown by Hubble's law:

[tex]V=H_{0}D[/tex]

Also, expansion only effects very large objects, such as galaxies or super clusters, not the Sun.

Second, Hubble's constant is estimated by WMAP to be 70.8 ± 1.6 (km/s)/Mpc.

So, an object that is very far away will appear to have an extremely high recessional velocity, your calculation was completely made up, and had no basis whatsoever.

Also, the cosmic microwave background provides conclusive evidence the universe is expanding and cooling.
 
  • #150
Mark M said:
This is so wrong, I have to question if you have a clue about what you're talking about.

He doesn't, he is confusing reddening with redshift.

.. Hubble's law:

[tex]V=H_{0}D[/tex]

Use 1AU for D to get V then multiply by a century and you might get the figure he quoted. Of course that ignores all orbital mechanics and doesn't seem to have any rational connection to the solar wind anyway.
 
  • #151
GeorgeDishman said:
He doesn't, he is confusing reddening with redshift.



Use 1AU for D to get V then multiply by a century and you might get the figure he quoted. Of course that ignores all orbital mechanics and doesn't seem to have any rational connection to the solar wind anyway.

I just did the calculation, I doesn't come out to exactly what he said, but it is still very low.

Obviously, someone forgot to tell him that Hubble's law is only used for objects affected by the expansion of space.
 
  • #152
Mark M said:
Obviously, someone forgot to tell him that Hubble's law is only used for objects affected by the expansion of space.

Actually it can be used even for gravitationally bound objects. For example we can measure the motion of the Earth relative to the "fixed stars" so we know its angular velocity and we can estimate the mass of the Sun ignoring Hubble expansion. If we then include expansion, over a short period the Earth would accelerate away from the Sun so to keep the same orbit, we would need to very slightly increase the mass of the Sun. Of course the difference is orders of magnitude less than could be measured but it would be possible to calculate the difference (if I could be bothered).

On a more practical note, I did some work on the Pioneer Anomaly many years ago and although the sign was obviously wrong, I calculated the effect of the Hubble flow when they were proposing a follow-up mission. It turns out to be only about an order of magnitude less than the anomaly so it might be possible to measure it with a carefully designed mission.
 
  • #153

Cosmology scale factor equation:
[tex]\frac{R_u(t_0)}{R_u(t)} = \frac{a(t_0)}{a(t)} = \frac{T_t}{T_0} = 1 + z[/tex]

Universe total observable radius:
[tex]R_u(t_0) = 4.399 \cdot 10^{26} \; \text{m}[/tex]

Cosmic gravitational wave background redshift at present:
[tex]z \geq 10^{25}[/tex]

[tex]R_u(t) \leq \frac{R_u(t_0)}{1 + z} = \frac{4.399 \cdot 10^{26} \; \text{m}}{1 + 10^{25}} = 43.99 \; \text{m}[/tex]

Universe total observable radius at gravitational wave decoupling time t:
[tex]\boxed{R_u(t) \leq 43.99 \; \text{m}}[/tex]

Reference:
Cosmic microwave background radiation - Wikipedia
Cosmic inflation - Wikipedia
Timeline of the Big Bang - Inflationary epoch - Wikipedia
Cosmic gravitational wave background - Wikipedia
Red shift - Highest redshifts
 
  • #154

The the LCDM model scale factor is defined as:
[tex]a(t) = \left[ \frac{\Omega_m}{\Omega_v} \sinh^2 \left( \frac{3}{2} \sqrt{\Omega_v} H_0 t \right) \right]^{\frac{1}{3}}[/tex]

Differentiating the scale factor function with respect to t:
[tex]\frac{d a(t)}{dt} = \frac{d}{dt} \left[ \frac{\Omega_m}{\Omega_v} \sinh^2 \left( \frac{3}{2} \sqrt{\Omega_v} H_0 t \right) \right]^{\frac{1}{3}} = \frac{ \Omega_m H_0 \cosh \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right) \sinh \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right)}{\sqrt{\Omega_v} \left(\frac{\Omega_m \sinh^2 \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right)}{\Omega_v} \right)^{2/3}}[/tex]

The scale factor derivative function:
[tex]\boxed{\frac{d a(t)}{dt} = \frac{ \Omega_m H_0 \cosh \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right) \sinh \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right)}{\sqrt{\Omega_v} \left(\frac{\Omega_m \sinh^2 \left(\frac{3}{2} \sqrt{\Omega_v} H_0 t \right)}{\Omega_v} \right)^{2/3}}}[/tex]

Is this equation correct?

Attachments: plot a(t), plot a'(t)

Reference:
LambdaCDM geometry - mathematical details - Wikipedia
 

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  • #155
I'm not good enough at the math to quickly check your solution but I believe there is no analytic solution when there is more than one phase involved. The graph is initially matter dominated but becomes energy dominated so I think you have to perform an integration to get the curve.

However, the section "mixtures" here suggests it can be solved:

http://en.wikipedia.org/wiki/Friedmann_equations#Useful_solutions

The "Lecture notes on Astrophysics" looks comprehensive too, though beyond my level.
 
  • #156
i was thinking about light.
a particle and/or a wave ?
but what about darkness.?
does darkness move at the speed of light?
does light move at the speed of darkness?
does light really bend around corners or is it pulled around by darkness?
in a dark universe, does the universe expand when light appears?
does light "push" darkness away ?

but what if the universe is in a "bubble"?
would the darkness get squashed?
is light a constant in the universe.?
does the universe expand at different speeds at different times depending on how much is being added at that particular time?
 
  • #157
lostprophets said:
i was thinking about light.
a particle and/or a wave ?

The best description I've heard is that light is an electromagnetic wave that transfers energy only in packets we call photons.

but what about darkness.?
does darkness move at the speed of light?
does light move at the speed of darkness?

Darkness is nothing but the absence of light, similar to how a vacuum is the absence of matter in a volume of space.

does light really bend around corners or is it pulled around by darkness?
in a dark universe, does the universe expand when light appears?
does light "push" darkness away ?

Light really does diffract (bend if you want to call it that) around corners to a certain extent that depends on the wavelength. The rest of the quote doesn't make any sense.

but what if the universe is in a "bubble"?
would the darkness get squashed?
is light a constant in the universe.?
does the universe expand at different speeds at different times depending on how much is being added at that particular time?

I think you have a misunderstanding on how we view the universe. I cannot answer these questions because they don't even make sense with current cosmological models. My suggestion is to read up on the subject. There are plenty of websites including wikipedia that will help you understand. Here's two articles that will greatly help you if you read them and follow all the links around. Don't be surprised if it doesn't make much sense first, as unless you understand the basics of light and matter the terms won't mean much.

http://en.wikipedia.org/wiki/Universe
http://en.wikipedia.org/wiki/Physical_cosmology
 
  • #158
Drakkith said:
Darkness is nothing but the absence of light, similar to how a vacuum is the absence of matter in a volume of space.
Light really does diffract (bend if you want to call it that) around corners to a certain extent that depends on the wavelength. The rest of the quote doesn't make any sense.
http://en.wikipedia.org/wiki/Universe
http://en.wikipedia.org/wiki/Physical_cosmology

:eek: are you serious?
darkness is nothing but the absence of light... ooosh
so what came first, the darkness or the light?
but i thought we knew or at least thought ,that there is no such thing as nothing
 
  • #159
lostprophets said:
:eek: are you serious?
darkness is nothing but the absence of light... ooosh
so what came first, the darkness or the light?

Light has been around since the earliest moment of the universe. So I would say light. What happened "before" the universe is pure speculation and doesn't belong here. (Just in case you were going to bring that up)

but i thought we knew or at least thought ,that there is no such thing as nothing

That is more philosophy than science. We have defined darkness to be the absence of visible light, just as we have defined a vacuum to be the absence of matter.
 
  • #160

These are the scale factor equations that I reviewed from reference 1 and 2.

Inflation Hubble parameter (end of inflationary epoch): 'ref. 1 p. 34 (167)'
[tex]H_i = \frac{1}{t_{i}} = \frac{1}{10^{-32} \; \text{s}} = 10^{32} \; \text{s}^{-1}[/tex]
[tex]\boxed{H_i = 10^{32} \; \text{s}^{-1}}[/tex]

Inflation scale factor: 'ref. 1 p.35 (165)'
[tex]a(t) \propto e^{H_i t} \tag{1}[/tex]

Radiation scale factor: 'ref. 1 p. 22 (119)'
[tex]a(t) = (2 H_0)^{\frac{1}{2}} \cdot t^{\frac{1}{2}} \tag{2}[/tex]

Matter scale factor: 'ref. 1 p. 21 (115)'
[tex]a(t) = \left( \frac{4 H_0}{2} \right)^{\frac{2}{3}} \cdot t^{\frac{2}{3}} \tag{3}[/tex]

LCDM matter scale factor: 'ref. 2'
[tex]a(t) = \left[ \frac{\Omega_m}{\Omega_v} \sinh^2 \left( \frac{3}{2} \sqrt{\Omega_v} H_0 t \right) \right]^{\frac{1}{3}} \tag{4}[/tex]

Equations 2 and 3 appear to be describing a universe that is much younger.

Attachments: plot 1, plot 2,3,4

Reference:
Friedmann equations - useful solutions - Wikipedia
http://nicadd.niu.edu/~bterzic/PHYS652/PHYS652_notes.pdf
LambdaCDM - geometry - mathematical details - Wikipedia
 

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  • #161
Drakkith said:
Light has been around since the earliest moment of the universe. So I would say light. .

i respect your guess.
if light was more abundant than darkness at the start where as the reverse is true now, am i to believe then that the universe is getting smaller?
what if it was expanding and contracting
i ask about light "pushing" darkness (light pressure) clearing a path .
so if we had darkness first with energy, then light energy appears,room has to be made for this light.
could light then clear this "room" creating a vacuum redundant of energy once this light has lost its energy and gone..this then takes time to rebuild itself with dark energy matter, un til it over crowds sparking another light source and repeats the process.

this would mean light energy is finite but that does not mean the universe cannot expand..

i could be way off and have no idea what I am on about.but I've read some say that the universe is expanding fast than light... how do we measure this.do we measure it with light?
if light is "pushing" then light will always be behind therefore it could be seen that anything infront of it is moving fast when really its not
 
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  • #162
lostprophets said:
i respect your guess.
if light was more abundant than darkness at the start where as the reverse is true now, am i to believe then that the universe is getting smaller?

As has been said, darkness is only the absence of light, so in the presence of a single particle of light, the universe is not dark.

what if it was expanding

It is expanding, and the rate at which it does so is increasing.

i ask about light "pushing" darkness (light pressure) clearing a path.

That is poetic licence, it has no physical meaning. Light pressure can push a sail around (look up the Ikaros project) but darkness isn't a substance, just the absence of light.

so if we had darkness first with energy, then light energy appears,

For the first 378,000 years, the whole universe looked like the interior of the Sun, the farther back in time you go, the brighter it was.

room has to be made for this light.

Space, time and light possibly arose together but we don't know, that is presently beyond our understanding.

this would mean light energy is finite but that does not mean the universe cannot expand..

It is definitely expanding, it may be finite or infinite, we cannot tell which.

i could be way off and have no idea what I am on about.but I've read some say that the universe is expanding fast than light... how do we measure this.do we measure it with light?

Yes. Surprisingly, the light can still reach us, but I'd need to go into maths to explain why.

if light is "pushing" then light will always be behind therefore it could be seen that anything infront of it is moving fast when really its not

Light was created everywhere equally and moved in all directions. There was no "in front" or "behind", it always surrounded.
 
  • #163
lostprophets said:
i respect your guess.
if light was more abundant than darkness at the start where as the reverse is true now, am i to believe then that the universe is getting smaller?

No, as has been repeatedly said, the universe is expanding.

what if it was expanding and contracting

There's no need to ask "what ifs" that aren't real. The universe is expanding, not contracting.

i ask about light "pushing" darkness (light pressure) clearing a path .

I don't know what you don't understand about darkness simply being the absence of light. Darkness is an abstract concept linked to vision. If a volume of space is completely devoid of EM radiation (light) we do not call it dark, we call it empty of radiation. Light propagates through space and interacts with matter. It cannot interact with empty space as there is nothing to interact with!
so if we had darkness first with energy

We did not have darkness first. As I said light has existed since the earliest moments of the universe when the density and temperature of the universe was so high that matter and antimatter was continually being created from EM radiation and annihilated, converting back to EM radiation.

then light energy appears,room has to be made for this light.

It did not "appear". The energy already existed. Furthermore you keep suggesting that "darkness" is something physical and tangible. It is not. Does a vacuum have to make room for particles to exist in it? No!

could light then clear this "room" creating a vacuum redundant of energy once this light has lost its energy and gone..this then takes time to rebuild itself with dark energy matter, un til it over crowds sparking another light source and repeats the process.

Absolutely not. The earliest moments of the universe was full of interacting particles and radiation. As George said above, imagine being inside the core of the Sun, but a billion billion trillion times denser and hotter. Then go another quadrillion above that. Then you will be getting close to the state of the early universe.

i could be way off and have no idea what I am on about.but I've read some say that the universe is expanding fast than light... how do we measure this.do we measure it with light?
if light is "pushing" then light will always be behind therefore it could be seen that anything infront of it is moving fast when really its not

We measure it by looking at the amount of redshift an object presents to us. The further away an object such as a galaxy is, the more its light is redshifted. This is due to the expansion of the universe causing it to recede from us and stretching out the light as it travels over billions of years.

Also, the expansion of the universe is a "rate", not a measurement of velocity. What this means is that objects further away will accelerate away from us quicker than objects closer to us will. The speed at which objects move away from us is called the recession velocity. Currently our measurements show that this recession velocity increases by about 70 km/s per megaparsec (3.26 million light-years) in distance that an object is from us. So a galaxy at 2 megaparsecs in distance from us would be receding at about 140 km/s, while a galaxy at 20 megaparsecs would recede at 1400 km/s. If the rate of expansion were higher, the recession velocity would increase by a larger amount per distance, such as being 100 km/s per megaparsec.
 
  • #164
sorry . i did mean to use the word "front" lightly .ooosh pun ,not so poetic...
yes there's no front, back, middle, only edges,curves,surrounding, enclosed ,in a tomb of darkness..
the further we look back the brighter it gets. its logic for it to be so. but is it logic to think that what one is looking at is not the beginning but a random?

thanks for the reply ...

also how far can my eyes see. meaning
when i see light that has come from a far distance.at what distance am i seeing it.?
am i seeing the light from the distance of my eye or am i seeing the light light years away. my eyes can see distances.so i ask is it possible to travel down the light to the source and bring it nearer?
i no i may like a fruit loop hope you don't mind..
my question is this.
is the light seeing me or am i seeing it?

also i went to the optitions today.he put a light in my eye .when this light was taken away i had a dark line of vision.i asked why.
he said its because the light removes something or other ,sorry can't remember exactly,so there was an empty space .but
over time the energy recovers and bring the light back to this dark spot...can space work the same?
meaning does light remove matter then once the light has gone this matter returns over a time period...
 
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  • #165
lostprophets said:
the further we look back the brighter it gets. its logic for it to be so. but is it logic to think that what one is looking at is not the beginning but a random?

Well, your first sentence is incorrect. It is not brighter the further we look back. After the universe formed it cooled and expanded over millions of years. Finally after the temperature and density dropped beyond a critical point, protons could combine with electrons, forming neutral atoms that are mostly transparent to light. Before this point in time light could not travel more than mere nanometers before interacting with protons or electrons. After this point in time the universe became "transparent", and the radiation that was released from electrons combining with protons could suddenly travel over light-years and is currently seen as the Cosmic Microwave Background. The CMB is literally the furthest back we can see using light. It is not physically possible to see beyond this point unless we can somehow invent a neutrino detector in the future that is a few trillion times more sensitive than current ones.

After this recombination, atoms could finally start to collapse under gravitational attraction to form the first stars and galaxies. Whether the universe is "brighter" now or then is unknown to me.

I don't know what your asking with the 3rd sentence.

also how far can my eyes see. meaning
when i see light that has come from a far distance.at what distance am i seeing it.?
am i seeing the light from the distance of my eye or am i seeing the light light years away. my eyes can see distances.so i ask is it possible to travel down the light to the source and bring it nearer?
i no i may like a fruit loop hope you don't mind..
my question is this.
is the light seeing me or am i seeing it?

I don't really know what you are asking. Since photons can travel through space for billions of years, if your eye detects one then you are seeing something billions of lightyears away. The only limit to how far an object can be seen is simply that the universe is only a finite age. The CMB was released over 13 billion years ago, so as time passes the area of space that those photons we see were released from is getting further away.
 
  • #166
im now confused. one of you is saying the further you go back the brighter it gets,and the other is saying not so...
the problem may stem from the "no matter which direction we look ,it all looks the same" on a large scale not small...
so how do we get around this.?
its like looking at a field full of sheep and guessing which one came first.
neutrinos collide with things at random points at random times...this to me is very important.
 
  • #167
lostprophets said:
im now confused. one of you is saying the further you go back the brighter it gets,and the other is saying not so...

Sorry. Before the CMB was emitted you did in fact get "brighter" the further back you go, but that is kind of inaccurate as the state of the universe was very different from what it is today. I prefer the terms "hotter" and "denser".

the problem may stem from the "no matter which direction we look ,it all looks the same" on a large scale not small...
so how do we get around this.?
its like looking at a field full of sheep and guessing which one came first.
neutrinos collide with things at random points at random times...this to me is very important.

Get around what? The universe is very homogenous on the large scale.

And may I request that you make specific questions. Much of your posts seem to be ramblings that don't make any sense and don't seem to be asking anything. It would help both us and yourself if you could trim your posts down to clear, concise questions.
 
  • #168
lostprophets said:
also i went to the optitions today.he put a light in my eye .when this light was taken away i had a dark line of vision.i asked why.
he said its because the light removes something or other ,sorry can't remember exactly,so there was an empty space .but
over time the energy recovers and bring the light back to this dark spot...can space work the same?
meaning does light remove matter then once the light has gone this matter returns over a time period...

The bright light uses up the chemicals in your eye that respond to light, allowing you to see. These chemicals require time to be replaced in your cells, so it takes a little bit for your vision to return to normal. The light isn't pushing anything out of the way and the chemicals are still there, they are just used up in a reaction that turns them into something else.
 
  • #169
Drakkith said:
The bright light uses up the chemicals in your eye that respond to light, allowing you to see. These chemicals require time to be replaced in your cells, so it takes a little bit for your vision to return to normal. The light isn't pushing anything out of the way and the chemicals are still there, they are just used up in a reaction that turns them into something else.
yes..
i see. thank you. the light turns them into something else...1+1 = 3
 
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  • #170
lostprophets said:
im now confused. one of you is saying the further you go back the brighter it gets,and the other is saying not so...
the problem may stem from the "no matter which direction we look ,it all looks the same" on a large scale not small...
so how do we get around this.?
its like looking at a field full of sheep and guessing which one came first.
neutrinos collide with things at random points at random times...this to me is very important.

It is summer and you are in a field of sheep, all born in the same week in the spring. If light travels slowly, you see old sheep near you but lambs far off. When we look far away, we see the universe as it was earlier. It was brighter earlier.
 
  • #171
lostprophets said:
yes..
i see. thank you. the light turns them into something else...1+1 = 3

What's up with your equation? Is something confusing or are you joking?

GeorgeDishman said:
It is summer and you are in a field of sheep, all born in the same week in the spring. If light travels slowly, you see old sheep near you but lambs far off. When we look far away, we see the universe as it was earlier. It was brighter earlier.

I am uncertain if you can say that the universe was brighter earlier. I think that depends on the amount of light being output by stars at various times in the universe. If there are more stars now than in the past, today may be "brighter". Either way it's a confusing issue that doesn't really say much.
 
  • #172
Some context might help:

OP:
so if we had darkness first with energy, then light energy appears,

Me:
For the first 378,000 years, the whole universe looked like the interior of the Sun, the farther back in time you go, the brighter it was.

Drakkith said:
I am uncertain if you can say that the universe was brighter earlier. I think that depends on the amount of light being output by stars at various times in the universe. If there are more stars now than in the past, today may be "brighter". Either way it's a confusing issue that doesn't really say much.

A small black body at a "typical" location in the universe now (i.e. probably in intergalactic space) would be at equilibrium somewhere near 3K, at the time of last scattering what we see as the CMBR was at 2975K and our test body would also have had that temperature. If that applied today, the Earth could be no cooler. Before 48,000 years, the universe was the "radiation dominated" era so I think my statement is valid.

If the OP is curious what the sky would have looked like back then, he can put 2975 into the box at the bottom right of this applet:

http://webphysics.davidson.edu/alumni/milee/java/bb_mjl.htm

The colour is the circle marked "composite" in the left panel.
 
Last edited:
  • #173
GeorgeDishman said:
A small black body at a "typical" location in the universe now (i.e. probably in intergalactic space) would be at equilibrium somewhere near 3K, at the time of last scattering what we see as the CMBR was at 2975K and our test body would also have had that temperature. If that applied today, the Earth could be no cooler. Before 48,000 years, the universe was the "radiation dominated" era so I think my statement is valid.

While all true, what I mean is that saying the universe is brighter in the past may only be correct when you look back to a certain point in time. My question is if there are more stars now than in the past, and if those stars are outputting more total light than they were in the past. That combined with the density of the universe could mean it is definitely brighter in the past, or not. I have no idea if it was brighter, nor do I know how to find out.
 
  • #174
Drakkith said:
While all true, what I mean is that saying the universe is brighter in the past may only be correct when you look back to a certain point in time. My question is if there are more stars now than in the past, and if those stars are outputting more total light than they were in the past. That combined with the density of the universe could mean it is definitely brighter in the past, or not. I have no idea if it was brighter, nor do I know how to find out.

The OP was talking about the first instants of the universe and prior to the release of the CMBR, it was brighter earlier. After that is more complex ;-)

Once the plasma combined into neutral hydrogen, there was the period called the "dark ages" because there were no stars at all. Then the first Pop III stars formed perhaps after around 100 million years. They were probably very large and short lived and put a lot of "metals" (elements beyond helium) into the mix when they ended as supernovae. As the proportion of heavy elements increased, stars could be smaller and new star production peaked then fell. All that time the universe was expanding so the density was falling too. Overall, there would have been a peak in stellar brightness when the universe was perhaps 1 to 3 billion years old. The rate of new star production now is conventionally thought to be perhaps one tenth of the peak but that is a point of current debate.
 
  • #175
Hmmm. I have a few ideas/questions but I'll save that for another thread.
 
<h2>1. Does space really expand?</h2><p>Yes, according to current scientific theories and observations, space does expand. This expansion is known as the expansion of the universe.</p><h2>2. How does space expand?</h2><p>Space expands through a process known as cosmic inflation, which is believed to have occurred shortly after the Big Bang. This inflationary period caused the rapid expansion of the universe and continues to this day, although at a much slower rate.</p><h2>3. What evidence supports the idea of space expanding?</h2><p>There are several pieces of evidence that support the idea of space expanding. One of the most notable is the observation of galaxies moving away from each other, which is known as the Hubble's law. Additionally, the cosmic microwave background radiation, leftover radiation from the Big Bang, also supports the idea of cosmic inflation and the expansion of space.</p><h2>4. Is there a limit to how much space can expand?</h2><p>The current understanding is that space does not have a limit to how much it can expand. However, the expansion rate may change over time, and there are theories that suggest that the expansion may eventually slow down or even reverse.</p><h2>5. How does the expansion of space affect objects within it?</h2><p>The expansion of space does not directly affect objects within it. This is because the expansion happens at a much larger scale than the objects in our everyday lives. However, the expansion does have an impact on the distance between objects, causing them to move further apart over time.</p>

1. Does space really expand?

Yes, according to current scientific theories and observations, space does expand. This expansion is known as the expansion of the universe.

2. How does space expand?

Space expands through a process known as cosmic inflation, which is believed to have occurred shortly after the Big Bang. This inflationary period caused the rapid expansion of the universe and continues to this day, although at a much slower rate.

3. What evidence supports the idea of space expanding?

There are several pieces of evidence that support the idea of space expanding. One of the most notable is the observation of galaxies moving away from each other, which is known as the Hubble's law. Additionally, the cosmic microwave background radiation, leftover radiation from the Big Bang, also supports the idea of cosmic inflation and the expansion of space.

4. Is there a limit to how much space can expand?

The current understanding is that space does not have a limit to how much it can expand. However, the expansion rate may change over time, and there are theories that suggest that the expansion may eventually slow down or even reverse.

5. How does the expansion of space affect objects within it?

The expansion of space does not directly affect objects within it. This is because the expansion happens at a much larger scale than the objects in our everyday lives. However, the expansion does have an impact on the distance between objects, causing them to move further apart over time.

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