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By the end of this section, you will be able to:
  • Describe the evolution of the early universe in terms of the four fundamental forces
  • Use the concept of gravitational lensing to explain astronomical phenomena
  • Provide evidence of the Big Bang in terms of cosmic background radiation
  • Distinguish between dark matter and dark energy

In the previous section, we discussed the structure and dynamics of universe. In particular, the universe appears to be expanding and even accelerating. But what was the universe like at the beginning of time? In this section, we discuss what evidence scientists have been able to gather about the early universe and its evolution to present time.

The early universe

Before the short period of cosmic inflation, cosmologists believe that all matter in the universe was squeezed into a space much smaller than an atom. Cosmologists further believe that the universe was extremely dense and hot, and interactions between particles were governed by a single force. In other words, the four fundamental forces (strong nuclear, electromagnetic, weak nuclear, and gravitational) merge into one at these energies ( [link] ). How and why this “unity” breaks down at lower energies is an important unsolved problem in physics.

Figure shows a timeline. At 10 to the power minus 43 seconds after big bang, the line splits into two. One branch is gravitational force. The other moves ahead and further splits into two at 10 to the power minus 35 seconds. From here, one branch is strong nuclear force. The other splits into two at 10 to the power minus 12 seconds. The two branches are labeled electromagnetic force and weak nuclear force. The particle energy and the temperature of the universe at the time of the first split are: 10 to the power 19 GeV and 10 to the power 32 K respectively. At the second split, they are: 10 to the power 14 GeV and 10 to the power 27 K respectively. At the third split, they are 100 GeV and 10 to the power 15 K respectively. All four lines continue till they reach the values: 5 into 10 to the power 17 seconds, 10 to the power minus 4 eV and 3 K.
The separation of the four fundamental forces in the early universe.

Scientific models of the early universe are highly speculative. [link] shows a sketch of one possible timeline of events.

Figure shows a timeline. Inflation starts at 10 to the power minus 43 seconds after big bang, at a temperature of 10 to the power  32 K and an energy of 10 to the power 19 GeV. Inflation ends at 10 to the power minus 35s, 10 to the power 27 K and 10 to the power 15 GeV. This is followed by Age of leptons: quarks, muons, taus, gluons and photons. Protons are formed at 10 to the power minus 6 s, 10 to the power 13 K and 0.1 GeV. This is followed by the age of nucleons: quarks, protons, muons, neutrons, taus, electrons, mesons, photons. Nuclear fusion begins at 225 s, 10 to the power 11 K and 10 to the power minus 4 GeV. This is followed by the age of nucleo synthesis: protons, He, electrons, photons. Nuclear fusion ends at 1000 years, 100,000 K and 10 to the power minus 8 GeV. This is followed by the age of ions: protons, positrons, He, electrons, photons. Cosmic microwave background is at 3000 years, 60,000 K and 5 into 10 to the power minus 9 GeV. This is followed by age of atoms. First stars and galaxies are formed at 300,000 years, 3000 K and 3 into 10 to the power minus 10 GeV. This is followed by the age of stars and galaxies. Today the temperature is 2.7 K and the energy is 2.3 into 10 to the power minus 13 GeV.
An approximate timeline for the evolution of the universe from the Big Bang to the present.
  1. Big Bang ( t < 1 0 43 s ) : The current laws of physics break down. At the end of the initial Big Bang event, the temperature of the universe is approximately T = 1 0 32 K .
  2. Inflationary phase ( t = 1 0 43 to 1 0 35 s ) : The universe expands exponentially, and gravity separates from the other forces. The universe cools to approximately T = 1 0 27 K .
  3. Age of leptons ( t = 1 0 35 to 1 0 6 s ) : As the universe continues to expand, the strong nuclear force separates from the electromagnetic and weak nuclear forces (or electroweak force). Soon after, the weak nuclear force separates from the electromagnetic force. The universe is a hot soup of quarks, leptons, photons, and other particles.
  4. Age of nucleons ( t = 1 0 6 to 225 s ) : The universe consists of leptons and hadrons (such as protons, neutrons, and mesons) in thermal equilibrium. Pair production and pair annihilation occurs with equal ease, so photons remain in thermal equilibrium:
    γ + γ e + e + γ + γ p + p γ + γ n + n .

    The number of protons is approximately equal to the number of neutrons through interactions with neutrinos:
    ν e + n e + p ν e + p e + + n.

    The temperature of the universe settles to approximately 1 0 11 K —much too cool for the continued production of nucleon-antinucleon pairs. The numbers of protons and neutrons begin to dominate over their anti-particles, so proton-antiproton ( p p ) and neutron-antineutron ( n n ) annihilations decline. Deuterons (proton-neutron pairs) begin to form.
  5. Age of nucleosynthesis ( t = 225 s to 1000 years): As the universe continues to expand, deuterons react with protons and neutrons to form larger nuclei; these larger nuclei react with protons and neutrons to form still larger nuclei. At the end of this period, about 1/4 of the mass of the universe is helium. (This explains the current amount of helium in the universe.) Photons lack the energy to continue electron-positron production, so electrons and positrons annihilate each other to photons only.
  6. Age of ions ( t = 1000 to 3000 years): The universe is hot enough to ionize any atoms formed. The universe consists of electrons, positrons, protons, light nuclei, and photons.
  7. Age of atoms ( t = 3000 to 300,000 years): The universe cools below 10 5 K and atoms form. Photons do not interact strongly with neutral atoms, so they “decouple” (separate) from atoms. These photons constitute the cosmic microwave background radiation to be discussed later.
  8. Age of stars and galaxies ( t = 300,000 years to present): The atoms and particles are pulled together by gravity and form large lumps. The atoms and particles in stars undergo nuclear fusion reaction.

Questions & Answers

it is the relatively stable flow of income
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what is circular flow of income
Divine Reply
branches of macroeconomics
SHEDRACK Reply
what is Flexible exchang rate?
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is gdp a reliable measurement of wealth
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introduction to econometrics
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Tom
Why is unemployment rate never zero at full employment?
Priyanka Reply
bcoz of existence of frictional unemployment in our economy.
Umashankar
what is flexible exchang rate?
poudel
due to existence of the pple with disabilities
Abdulraufu
the demand of a good rises, causing the demand for another good to fall
Rushawn Reply
is it possible to leave every good at the same level
Joseph
I don't think so. because check it, if the demand for chicken increases, people will no longer consume fish like they used to causing a fall in the demand for fish
Anuolu
is not really possible to let the value of a goods to be same at the same time.....
Salome
Suppose the inflation rate is 6%, does it mean that all the goods you purchase will cost 6% more than previous year? Provide with reasoning.
Geetha Reply
Not necessarily. To measure the inflation rate economists normally use an averaged price index of a basket of certain goods. So if you purchase goods included in the basket, you will notice that you pay 6% more, otherwise not necessarily.
Waeth
discus major problems of macroeconomics
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what is the problem of macroeconomics
Yoal
Economic growth Stable prices and low unemployment
Ephraim
explain inflationcause and itis degre
Miresa Reply
what is inflation
Getu
increase in general price levels
WEETO
Good day How do I calculate this question: C= 100+5yd G= 2000 T= 2000 I(planned)=200. Suppose the actual output is 3000. What is the level of planned expenditures at this level of output?
Chisomo Reply
how to calculate actual output?
Chisomo
how to calculate the equilibrium income
Beshir
Criteria for determining money supply
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who we can define macroeconomics in one line
Muhammad
Aggregate demand
Mohammed
C=k100 +9y and i=k50.calculate the equilibrium level of output
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I want to know how can we define macroeconomics in one line
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it must be .9 or 0.9 no Mpc is greater than 1 Y=100+.9Y+50 Y-.9Y=150 0.1Y/0.1=150/0.1 Y=1500
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hi can someone help me on this question If a negative shocks shifts the IS curve to the left, what type of policy do you suggest so as to stabilize the level of output? discuss your answer using appropriate graph.
Galge Reply
if interest rate is increased this will will reduce the level of income shifting the curve to the left ◀️
Kalombe
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Source:  OpenStax, University physics volume 3. OpenStax CNX. Nov 04, 2016 Download for free at http://cnx.org/content/col12067/1.4
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