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Show that the net result of the proton-proton fusion chain that occurs inside our sun can be summarized as $$6 \mathrm{p}^{+} \rightarrow_{2}^{4} \mathrm{He}+2 \mathrm{p}^{+}+2 \beta^{+}+2 \gamma+2 \nu_{\mathrm{e}}$$

Short Answer

Expert verified
The proton-proton chain converts 6 protons to helium-4 plus 2 protons, 2 positrons, 2 gamma rays, and 2 neutrinos.

Step by step solution

01

Understanding Proton-Proton Chain

The proton-proton chain is a series of nuclear reactions that occur in stars like the Sun. It primarily starts with the fusion of two protons to form a deuterium nucleus. Our objective is to show how six protons produce helium and other byproducts.
02

Basic Proton-Proton Reaction

In the first step of the proton-proton chain, two protons ( p^+ p^+ ) fuse together to form deuterium ( p + p ightarrow ext{D} + eta^+ + u_e"). This occurs twice to produce two deuterium nuclei.
03

Formation of Helium-3

Next, deuterium reacts with another proton to form helium-3 ( D + p ightarrow {^3 ext{He}} + ext{energy}"). This reaction also occurs twice, resulting in two helium-3 nuclei.
04

Formation of Helium-4

Two helium-3 nuclei then collide and fuse to form one helium-4 nucleus and release two protons ( {^3 ext{He}} + {^3 ext{He}} ightarrow {^4 ext{He}} + 2p").
05

Net Reaction Formation

Putting all the steps together: starting with six protons, two protons return in the final step, leading to a net input of four protons. The emissions, such as positrons ( eta^+ ), neutrinos ( u_e ), and gamma rays ( ext{gamma} ), are produced during intermediate reactions, typically two of each.
06

Conclusion

The entire chain results in the transformation of six protons into one helium-4 nucleus, accompanied by the byproducts of 2 protons, 2 positrons, 2 neutrinos, and 2 gamma rays. Thus, the existing summarized equation is verified: 6 ext{p}^{+} ightarrow {^4} ext{He} + 2 ext{p}^{+} + 2eta^{+} + 2 ext{gamma} + 2 u_e.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Nuclear Reactions
Nuclear reactions are processes that involve changes in an atom's nucleus and result in the transformation of elements. This is different from chemical reactions, where electrons participate and the nucleus remains unchanged. In stars like the Sun, nuclear reactions are responsible for producing energy. These reactions often happen under extreme conditions of temperature and pressure found in stellar cores.

A key aspect of nuclear reactions in stars is fusion, where lighter nuclei come together to form a heavier nucleus. The proton-proton fusion chain is a series of such reactions that occurs in stars. Fusion reactions release enormous amounts of energy, which powers the stars and provides the light and heat we receive on Earth. During these processes, byproducts such as positrons (\( \beta^+ \)), neutrinos (\( u_e \)), and gamma rays are also emitted as particles and energy are conserved.
Helium Nuclei
Helium nuclei, often referred to as alpha particles, consist of two protons and two neutrons \( ({}^{4} \text{He}) \). In the context of the proton-proton fusion chain in the Sun, helium nuclei are the end product of a sequence of nuclear reactions.

When hydrogen nuclei (protons) undergo fusion, they eventually form helium through intermediate steps involving deuterium and helium-3. The formation of helium-4 from these processes stabilizes the chain of reactions, as helium-4 is a stable nucleus.

Helium nucleus formation is crucial as it signifies the net conversion of mass into energy, validating the famous equation \( E=mc^2 \). This energy radiates from the star's surface, providing the light and warmth essential for life on Earth.
Stellar Energy Production
Stars produce energy through nuclear fusion occurring in their cores. This energy is essential for their existence and the energy they emit into the universe. In stars like the Sun, the main sequence of energy production is through the proton-proton chain, a series of reactions converting hydrogen into helium.

During these reactions, mass is converted into energy as postulated by Einstein's formula \( E=mc^2 \). This released energy is primarily in the form of light and heat. It travels from the star's core to its surface and ultimately radiates into space.
  • The energy sustains the star's structural integrity, counteracting gravitational collapse.
  • It influences stellar evolution, as stars transition different stages based on their ability to sustain fusion.
  • Accounts for stellar luminosity, determining how bright a star appears from Earth.
Stellar energy production through nuclear reactions is fundamental to the life cycle of stars and, by extension, the development of the universe as a whole.
Proton Fusion
Proton fusion is the initial step in many nuclear reactions in stars, including the proton-proton chain in the Sun. It involves the combining of two protons to form a heavier nucleus. In the Sun, this first step results in the formation of deuterium, an isotope of hydrogen composed of one proton and one neutron.

The conditions necessary for proton fusion require immense pressure and temperature, such as those found in stellar cores. The high energy environment overcomes the repulsive electromagnetic force between the positively charged protons.

Proton fusion releases energy due to the change in nuclear binding energy and contributes to the star's energy output. It is a vital mechanism in nuclear astrophysics, explaining the energy generation in many stars across the galaxy.
Deuterium Formation
Deuterium, a stable isotope of hydrogen, forms when two protons undergo fusion, with one proton converting to a neutron via weak nuclear interaction. This process is significant in the proton-proton chain.

The formation of deuterium is accompanied by the emission of a positron (\( \beta^+ \)) and a neutrino (\( u_e \)). This conversion is crucial as it provides the necessary stepping stone for the synthesis of heavier elements and facilitates the continuation of the fusion process in stars.
  • Represents the first change from hydrogen to helium intermediary components in stellar nucleosynthesis.
  • A necessary precursor for the formation of helium-3 in subsequent fusion reactions.
  • Although a relatively small mass component in the universe, it is crucial for the fusion cycles powering stars.
Understanding deuterium formation helps in explaining broader astrophysical phenomena and the evolutionary dynamics of stars.

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Most popular questions from this chapter

Given that each particle contains only combinations of \(u, d,\) \(s, \overline{u}, \overline{d},\) and \(\overline{s},\) deduce the quark content of (a) a particle with charge \(+e,\) baryon number \(0,\) and strangeness \(+1 ;\) (b) a particle with charge \(+e,\) baryon number \(-1,\) and strangeness \(+1 ;\) (c) a particle with charge \(0,\) baryon number \(+1,\) and strangeness \(-2 .\)

An unstable isotope of cobalt, \(^{60} \mathrm{Co}\) , has one more neutron in its nucleus than the stable \(^{59}\mathrm{Co}\) and is a beta emitter with a half-life of 5.3 years. This isotope is widely used in medicine. A certain radiation source in a hospital contains 0.0400 \(\mathrm{g}\) of \(^{60} \mathrm{Co.}\) (a) What is the decay constant for that iso- tope? (b) How many atoms are in the source? (c) How many decays occur per second? (d) What is the activity of the source, in curies?

(a) If a chest \(x\) ray delivers 0.25 \(\mathrm{mSv}\) to 5.0 \(\mathrm{kg}\) of tissue, how many total joules of energy does this tissue receive? (b) Natural radiation and cosmic rays deliver about 0.10 \(\mathrm{mSv}\) per year at sea level. Assuming an RBE of \(1,\) how many rem and rads is this dose, and how many joules of energy does a 75 kg person receive in a year? (c) How many chest x rays like the one in part (a) would it take to deliver the same total amount of energy to a 75 kg person as she receives from natural radiation in a year at sea level, as described in part (b)?

Comparison of energy released per gram of fuel. (a) When gasoline is burned, it releases \(1.3 \times 10^{8}\) J per gallon \((3.788\) L) of energy. Given that the density of gasoline is \(737 \mathrm{kg} / \mathrm{m}^{3},\) express the quantity of energy released in \(\mathrm{J} / \mathrm{g}\) of fuel. (b) During fission, when a neutron is absorbed by a \(^{235} \mathrm{U}\) nucleus, about 200 \(\mathrm{MeV}\) of energy is released for each nucleus that undergoes fission. Express this quantity in \(\mathrm{J} / \mathrm{g}\) of fuel. (c) In the proton-proton chain that takes place in stars like our sun, the overall fusion reaction can be summarized as six protons fusing to form one 4 He nucleus with two leftover protons and the liberation of 26.7 \(\mathrm{MeV}\) of energy. The fuel is the six protons. Express the energy produced here in units of J/g of fuel. Notice the huge difference between the two forms of nuclear energy, on the one hand, and the chemical energy from gasoline, on the other. (d) Our sun produces energy at a meas- ured rate of \(3.92 \times 10^{26} \mathrm{W}\) . If its mass of \(1.99 \times 10^{30} \mathrm{kg}\) were all gasoline, how long could it last before consuming all its fuel? (Historical note: Before the discovery of nuclear fusion and the vast amounts of energy it releases, scientists were confused. They knew that the earth was at least many millions of years old, but could not explain how the sun could survive that long if its energy came from chemical burning.)

To scan or not to scan? It has become popular for some people to have yearly whole-body scans (CT scans, formerly called CAT scans), using x rays, just to see if they detect anything suspicious. A number of medical people have recently questioned the advisability of such scans, due in part to the radiation they impart. Typically, one such scan gives a dose of 12 \(\mathrm{mSv}\) , applied to the whole body. By contrast, a chest \(x\) ray typically administers 0.20 \(\mathrm{mSv}\) to only 5.0 \(\mathrm{kg}\) of tissue. How many chest \(\mathrm{x}\) rays would deliver the same total amount of energy to the body of a 75 \(\mathrm{kg}\) person as one whole-body scan?

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