What Will Happen To The Universe In The Future – Lambda-CDM, fast growing edge. The timeline in this diagram extends from the Big Bang / Era of Inflation 13.8 billion years ago to the previous cosmological epoch.
The observations show that the expansion of the universe is rapid, so the speed of the galaxy far from the observer increases with time.
- 1 What Will Happen To The Universe In The Future
- 2 The Black Hole At The Birth Of The Universe
What Will Happen To The Universe In The Future
The speed of the planet was discovered in 1998 by two independent projects, the Supernova Cosmology Project and the High-Z Supernova Research Group, which used distant Type Ia supernovae to measure the speed.
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The idea is that Type Ia supernovae have nearly the same luminosity (standard candle), and since the objects appear ever dimmer, the observed luminosity of the supernovae can be used to measure their distance. The distance can be compared to the cosmological redshift of supernovae, which measures how much the universe has expanded since the supernova occurred; Hubble’s law states that the farther away an object is, the faster it recedes. The unexpected result is that the objects in the universe are moving away from each other at a rapid rate. Cosmologists at the time thought that the rate of economic growth would slow down due to the absorption of matter into the world. Three members of these two groups later won Nobel Prizes for their discoveries.
The acceleration of the universe is believed to have started since the universe ended its dark energy about 5 billion years ago.
In the framework of the general theory of relativity, the rapid expansion can be explained by the positive value of the cosmological constant Λ, equal to the prior of the positive absorption archy, called “dark archy”. While there are other explanations, the explanation for example is the dark argya (positive Λ) used in the standard model of cosmology, which also includes cold dark matter (CDM) and is called the Lambda -CDM model.
The Big Bang model has become the most accepted model that explains the evolution of our universe. The Friedman equation defines how the forces in the world drive its expansion.
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Where κ denotes the curvature of the universe, a(t) is the measurement parameter, ρ is the total erd density of the universe, and H is the Hubble parameter.
The four current phenomena for Earth’s energy are curvature, matter, radiation and dark energy.
All the objects decrease with the expansion of the world (increase the index), with the possibility of special time of darkness. The results of these cosmological measurements are what physicists use to determine the speed of the universe.
At the time, physicists were so sure that the world’s expansion was slowing down that they introduced the so-called delay parameter q0.
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According to the theory of cosmic inflation, the early universe went through a period of very rapid, quasi-exponential expansion. While the duration of this period of expansion is shorter than that of Expansion, it is a time of rapid expansion with some similarities to the modern era.
The definition of “accelerated expansion” is that the second derivative of the cosmic scale factor, a ¨ }} , is positive, which equals the delay parameter, q, becomes negative. However, note that this does not mean that the Hubble index increases with time. Since the Hubble parameter is defined as H (t) ≡ a ˙ (t) / a (t) }(t) / a (t)} , it follows that the derivative of the Hubble parameter is derived from
Hubble’s parameter therefore decreases with time, except for q < − 1. Observations agree q ≈ − 0.55 , which means that a ¨ }} is positive, but d H/d t is negative. Essentially, this means that the cosmic recession velocity of a particular galaxy increases with time, but its speed/distance ratio continues to decrease; Therefore, different galaxies expanding around a constant radius cross the sphere more slowly over time.
It is seen from above that the “zero acceleration / deceleration” data corresponding to a (t) is a function of t, q = 0, a ˙ = co o n s t } = const}, and H (t) = 1 / t .
The Black Hole At The Birth Of The Universe
The expansion rate of the planet can be determined using the mass-redshift relation of the stellar material using candles, or the distance-redshift relation using the ruler model. Another important factor is the growth of sample size, which shows that the cosmological consensus is not best explained by models that include expansion.
In 1998, the first evidence of acceleration came from the observation of Type Ia supernovae, which explode white stars that have exceeded their stability. Since they all have the same mass, their internal brightness can be adjusted. Repeated images of regions of the sky are used to detect supernovae, the observations after they give off their peak brightness, which are converted to a quantity called luminosity distance (see distance measurement in cosmology for sure).
For supernovae with redshift less than 0.1 per centimeter, or light traveling less than 10 percent of the age of Earth, this results in an almost linear distance-to-redshift due to Hubble’s law. At greater distances, because the expansion of the Universe changes over time, the distance-redshift relationship deviates from linearity, and this deviation depends on the expansion how far it has changed. The complete calculation requires a computer integration of the Friedman equation, but a simple derivation can be given as follows: the redshift z directly gives the cosmic scale value during the time of supernova explosion.
Such a supernova with measured redshift z = 0.5 means the universe is 1/1 + 0.5 =
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2/3 of its original size when the supernova exploded. In the case of rapid expansion, ¨ }} good; Therefore, ˙ }} was smaller in the past than today. Thus, an accelerating Earth took longer to expand from 2/3 to 1 times its original size, compared to a slow Earth with a constant ˙ }} and the same solar action first value of Hubble’s constant. Therefore, the light travels more, the distance is greater and supernovae are weaker, which is according to actual observations. Adam Rees et al. found that “the distance of high-redshift SNe Ia is on average 10% to 15% further than expected in a low-mass universe ΩM = 0.2 without the cosmological constant”.
This means that the high-redshift distance measurements are too large, compared to the nearby ones, for a matte Earth.
Some scientists have questioned the common view of acceleration or the theory of “cosmological principles” (that the universe is homogeneous and isotropic).
For example, a 2019 paper analyzed the light-corrected analysis of Type Ia supernovae, which contained t times more supernovae than used in the 1998 analysis, and concluded that there is little evidence for “business “, that is, for isotropic acceleration. in all directions.
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In the early universe before recombination and decay occurred, photons and matter existed in a primordial plasma. The elements of dsity higher in the photon-brion plasma will contract, will be compressed by gravity until the pressure becomes more and more interesting.
This contraction and expansion creates vibrations in the blood similar to sound waves. Since dark matter has only gravitational interaction, it remains at the height of the sound wave, the source of the hyperbolic effect. The Wh burst occurred approximately 380,000 years after the Big Bang,
Photons separate from matter and can flow into the universe, creating the cosmic microwave background as we know it. This left a shell of baryonic matter at a constant radius of the dark matter abundance, the distance called the sonic horizon. As time passes and the universe expands, it is in these disparate pieces of material that galaxies begin to form. Thus, by looking at the distance between galaxies at different redshifts td for a cluster, the standard angular diameter can be determined and used to compare the distance predicted by various cosmological models.
Peaks are observed in the correlation function (the probability that two galaxies will be at a distance from each other) at 100 h-1 Mpc,
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(where h is the dimensionless Hubble constant) shows that this is the size of the sweet sound today, and by comparing it with the sound horizon at the time of the explosion (with the CMB), we can clearly know the speed of the world . .
Measuring the mass function of galaxy clusters, which describes the number of superclusters, also provides evidence for dark energy.
By comparing the mass functions at high and low redshifts with those predicted by various cosmological models, values for w and Ωm are obtained that confirm the low density problem and non-zero value of the dark argya.
Given a cosmological model with some value of the cosmological density parameter, one can combine the Friedman equations and derive the age of the universe.
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