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1ST SEM MT CHAP 22 REVIEW
1ST SEM MT CHAP 22 REVIEW

Chapter 4 and 5
Chapter 4 and 5

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An Unifying Basis for all the Nuclear Reactions Karunakar
An Unifying Basis for all the Nuclear Reactions Karunakar

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... Beta particles are identical to electrons and thus have a charge of (1). This type of decay process leaves the mass number of the nuclei unchanged. A beta particle is minute in comparison to that of an alpha particle and has about one hundred times the penetrating ability. Where an alpha particle ca ...
An Unifying Basis for all the Nuclear Reactions
An Unifying Basis for all the Nuclear Reactions

... already in an expanded form as a gas at the room temperature. They can't release any more energy when they are subjected to any kind of nuclear reactions. To make the hydrogen atoms to release energy, first we need to compress the atoms to the state of plasma and then that plasma should be subjected ...
Chapter 16 Atomic Energy
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... nucleus of an atom. It differs from a chemical reaction in several ways. • One difference is that chemical reactions do not change the mass of atoms, but nuclear reactions do so by a very small amount. • A small amount of mass can change into a large amount of energy, because energy is equal to mass ...
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... the heavy nuclei like uranium. This corresponds to the mass difference that accounts for an energy release of about 1 MeV for each nucleon involved in the process. The fission reactions that were studied first involved the use of the neutron bombardment of the fissionable material. The theoretical e ...
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... be exerted upon them to cause such large deflections. Rutherford found that the only way to explain the deflections was to picture an atom with a tiny nucleus in which positive charge existed and nearly all the mass existed; And the electrons were some distance away from the nucleus. In other words, ...
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7.2- Nuclear reactions (PPT)

... Returning to the BE / A graph we see that iron (Fe) is the most stable of the nuclei. Nuclear fusion will occur with the elements below Fe because joining smaller nuclei forms bigger ones, which are higher on the graph (and thus more stable). Nuclear fission will occur with the elements above Fe ...
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Fusion Video Workbook.Final - General Atomics Fusion Education

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7.3 – Nuclear Reactions, Fission and Fusion 7.3.1 – Describe and

1 2 3 4 >

Muon-catalyzed fusion

Muon-catalyzed fusion (μCF) is a process allowing nuclear fusion to take place at temperatures significantly lower than the temperatures required for thermonuclear fusion, even at room temperature or lower. It is one of the few known ways of catalyzing nuclear fusion reactions.Muons are unstable subatomic particles. They are similar to electrons, but are about 207 times more massive. If a muon replaces one of the electrons in a hydrogen molecule, the nuclei are consequently drawn 207 times closer together than in a normal molecule. When the nuclei are this close together, the probability of nuclear fusion is greatly increased, to the point where a significant number of fusion events can happen at room temperature.Current techniques for creating large numbers of muons require large amounts of energy, larger than the amounts produced by the catalyzed nuclear fusion reactions. This prevents it from becoming a practical power source. Moreover, each muon has about a 1% chance of ""sticking"" to the alpha particle produced by the nuclear fusion of a deuterium with a tritium, removing the ""stuck"" muon from the catalytic cycle, meaning that each muon can only catalyze at most a few hundred deuterium tritium nuclear fusion reactions. So, these two factors, of muons being too expensive to make and then sticking too easily to alpha particles, limit muon-catalyzed fusion to a laboratory curiosity. To create useful room-temperature muon-catalyzed fusion reactors would need a cheaper, more efficient muon source and/or a way for each individual muon to catalyze many more fusion reactions.
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