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tobojijo t1_itynwoe wrote
Over the course of say 4 billion years that adds up to a 20,000 year difference
MrMurchison t1_ityp99s wrote
Sure, but that only seems like a significant difference because of human time frames. Those 20,000 years describe the difference between being at exactly half of the original mass, and functionally half of the original mass.
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Implausibilibuddy t1_ityzueg wrote
What about gravity affecting ability for a particle to break the weak force, or is that negligible? Or pulling atoms closer together making them more likely to be hit by particle emissions from other atoms?
mfb- t1_itzenic wrote
Completely negligible unless you are well inside a black hole.
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pinocola t1_itzub5m wrote
Also the shell theorem shows that there is no net gravitational force at the center of a sphere. Lots of pressure down there, but the mass on all sides of the core cancels the gravity out.
fore4runner t1_iu1rs2f wrote
Does that cancel out the time dilation as well? (It seems like it should logically, but intuitively it 'feels' like the time dilation should be at a maximum at the very centre of the body).
pinocola t1_iu23ksq wrote
No, because light and information have to cross out of the gravity well to get to an observer, and time dilation is always measured in reference to some other point, in this case presumably outside of the core of the star.
fore4runner t1_iu2aue3 wrote
But, if a person, in the centre of the earth shout out a laser every 1ms to a relatively stationary observer in space they would get the pulse every 1ms? But if someone on the earths surface did that, they wouldn’t, right?
pinocola t1_iu2m0r6 wrote
The pulse from the surface would be a bit slower than once every ms due to time dilation, and the pulse from the center of the earth would be even more time dilated than that.
Time dilation comes from a speed difference or the gravity gradient you travel/observe across. The pulses of light don't observe any gravity at the core itself, but once they start traveling out from the earth, they feel the gravity from whatever portion of the earth they've traveled out from, and would appear proportionally time dilated.
If the earth were a big hollow shell like an inflated ball, two observers anywhere inside the shell would feel no gravity due to the mass of the earth, and would not observe any time dilation when observing one another (even if one was at the geometric center and another was hanging onto the inside of the shell). But an observer outside the shell would feel the entire gravity of the earth and would see both people inside the shell as time dilated by the same amount.
Emuuuuuuu t1_iu23luc wrote
Force can be applied in many directions such that the net is zero. The force is still being applied though. Time only changes in one direction (slows down) and can't be cancelled by other directions.
It could maybe be sped back up with a very dense clump of anti-matter? Can a general relativitist chime in here?
fore4runner t1_iu2b2mc wrote
I don’t think your right, isn’t the time dilation due to the curve of space time? So in the centre of a body of mass, space time is flat
Fogernaut t1_iu2cz1r wrote
Isn't anti matter just opposite of matter in terms of charge? I don't think anti matter has negative mass if that's what you are thinking of.
alien_from_earth_14 t1_iu08lvr wrote
So any element of really high atomic number can stay stable at the singularity theoretically? Also will it be just one atom?
8spd t1_iu0pfw6 wrote
I mostly like the term "well inside a black hole", because it implies the existence of "barely inside a black hole".
mfb- t1_iu2wbsw wrote
The event horizon is usually seen as boundary. You can be just behind the event horizon (you can't stay there, of course).
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Ituzzip t1_iu0dk7r wrote
Ok but what about the extreme pressure?
mfb- t1_iu2wlzo wrote
Also irrelevant for radioactivity. Electron degeneracy pressure can have an influence on electron capture and beta decays, neutron degeneracy pressure (neutron stars) can have an effect on the stability of nuclei.
vrnvorona t1_itzdqmn wrote
Isn't weak interaction only weak compared to strong interaction and is very small on atom scale?
nineinchgod t1_itzeuxd wrote
Yes, and at subatomic scales, gravity is by far the weakest of the fundamental forces in action.
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ackillesBAC t1_itzf5ny wrote
Doesnt every frame always observe thier time ticking at 1s/s?
So from the point of view of a particle in a star it lives a normal time span regardless.
However an outside observer would see thier time flowing at 1.000005s/s
mfb- t1_itzg0jb wrote
> Doesnt every frame always observe thier time ticking at 1s/s?
Sure. That's why I discussed "(as seen from far away)" in my comment.
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mfb- t1_itzgc2s wrote
Temperature in the Sun's core is just ~15 MK or ~1 keV, which leads to a typical gamma factor of ~1+10^(-6) for protons and ~1+5*10^(-9) for very heavy nuclei like uranium. That's a smaller effect, especially for heavy nuclei.
Flatworldnotearth t1_itzgu7f wrote
For extremely high temperatures in of over 2.7GK required for silicon fusion for example it could have been several orders of magnitudes greater.
mfb- t1_itzimnc wrote
2.7 GK / 15 MK = 200, so we get 1+10^(-6) for uranium. Still smaller than the gravitational effect, especially if we consider that we are now looking at the core of a far more massive star.
Flatworldnotearth t1_itzkpwd wrote
An uranium nucleus in solar core travels at around 36km/s and in a exploding star at 3GK is around 500km/s and the Lorentz factor is around 1.0000015. Reaching the effects of gravitational time dilation as you say but the heavier the star is the more gravitational time dilation it gets. Thanks for your explanation.
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mfb- t1_ityc918 wrote
Gravitational time dilation is based on the potential, not based on a force. The potential has its minimum (i.e. the largest time dilation) at the center.
DaRealKryall t1_itycuw0 wrote
Oh, I didn't know that, I stand corrected then!
Just graduated high school, but our last physics unit was special relativity; we were only taught it to be based on the velocity of an object relative to the stationary observer.
CrzySunshine t1_itzeop4 wrote
Gravitation is handled in General Relativity, of which Special Relativity is a much smaller (and much easier) part.
DaRealKryall t1_iu25haa wrote
Heh, easier by calculation, sure, but my classmates would disagree on the comprehension aspect of the questions.
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Phalcone42 t1_itxr3al wrote
Well, there are neutron stars that are functionally one giant unstable element held together by gravity instead of the strong force. The only reason they don't collapse further is because of neutron degeneracy pressure. Considering the relationship between half life and atomic size, coupled with the longevity of neutron stars, i'd say so, but it's a bit of a stretch.
Edit. For a less extreme condition where the nucleus is not so massive as to be stabilized by gravity, it seems that certain types of decay, like electron capture decay, vary with pressure, while others like ß emission does not.
ToolFO t1_itz8cb1 wrote
Are neutron stars functionally just one giant nucleus?
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RobusEtCeleritas t1_iu3t52l wrote
There's not really any meaningful sense in calling a neutron star a giant nucleus. A nucleus is bound by the residual strong force, and the heaviest nuclei have radii on the order of tens of femtometers or so.
A neutron star is bound by gravity, and has a radius of around a few kilometers.
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adm_akbar t1_itza9mb wrote
Not really
Ahandgesture t1_itzjl9d wrote
So the gravity prevents neutron decay after the 830 or so seconds we expect? Or at this point is the matter too exotic at that point to apply thinking like this?
noldig t1_itzm5gt wrote
Not completely, there is still neutron decay going on, but it is heavily surpressed because of electron degeneracy pressure, and balanced by electron capture
Ahandgesture t1_itzmhnb wrote
Interesting, thank you for the answer! I wonder what the neutron lifetime in this case is. There's already the discrepancy between beamline and "jar" lifetime experiments. If we could measure neutron decay in a neutron star, we'd probably have another point of discrepancy 😆
noldig t1_itzmxzz wrote
The lifetime will mostly depend on phase space and temperature, so two quantities a free neutron doesn't care about. But these processes are responsible for cooling neutron stars down so we try to measure it. I have computed the rate a few times but never converted the units haha I will check
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rootofallworlds t1_itzgwfj wrote
On the contrary, in a star undergoing fusion the conditions may well cause nuclear reactions such as induced fission, making the effective half-life of unstable nuclides shorter than their half-lives when isolated. In the same way that uranium and plutonium in a nuclear reactor are fissioned much faster than their natural half-lives of millions or billions of years. I predict that would mask the effect of gravitational time dilation which has been calculated to be tiny by other answers.
While it's not a heavy nuclide, Lithium-7 is destroyed in fusing stars, and its presence or absence helps distinguish red dwarfs from brown dwarfs.
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unkilbeeg t1_itzny0y wrote
At the core of the star there would be very little effect from gravity, because the gravity is close to zero there. The pressure from all the surrounding mass (which has gravity working on it), on the other hand, would be huge.
Inside a body, gravity decreases as you go towards the center. The maximum gravity is right at the surface.
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mfb- t1_ity0i9m wrote
Gravitational time dilation depends on the potential, not the gravitational force. It's maximal in the center of objects, including the Sun. But it's not a large effect overall.
autoposting_system t1_itz2p92 wrote
Thanks
west_of_everywhere t1_itxzn0i wrote
>However, at the center of the Sun, the gravitational force is close to zero. So I'm pretty sure there would be no effect.
Isn't time dilation a function of potential energy, not force? Thanks!
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mfb- t1_ity0qbe wrote
If you think of gravitational time dilation: No. It's a tiny effect for stars, just a few parts in a million. Instead of 1 second the lifetime (as seen from far away) is now 1.000005 seconds or something like that (with the exact number depending on the star) - not a big deal.