Energy released when 238U is divided into two 119Pd.

In summary: MeVIn summary, the energy released in the nuclear fission reaction of 238_U (B/A = 7.6 MeV/n) into two 119_Pd (B/A = 8.5 MeV/n) is 214 MeV. This is because the binding energy per nucleon is smaller for 119_Pd, meaning that more energy is released when the nucleus is assembled from its constituents. The negative binding energy is subtracted from the total mass-energy of the nuclei to get the total energy released in the reaction.
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Ulrik Nordin
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Hi! I have a question about nuclear fission. Here is the problem:

238_U (B/A = 7.6 MeV/n) is divided into two 119_Pd ( B/A = 8.5 MeV/n). How much energy will be released?

I was thinking since the 119_Pd has larger B/A (binding energy per nucleus), energy is needed for this reaction to happen. But in my notes, the teacher has made this calculation 238*(8.5-7.6) = 214 MeV and states that this is released from the reaction. I do not undertand.

Best regards
ulrik
 
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Binding energy is actually negative. That is, you must subtract it from the sum of the mass-energies of the individual nucleons, in order to get the total mass-energy of a nucleus. So if you think in terms of "average mass-energy per nucleon", this is smaller for 119Pd than for 238U.
 
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Although binding energy is defined in such a way that the numbers come out positive, it is actually a negative energy, since it represents how much energy is released when the nucleus is assembled from its constituents. so we can write:

E(U238) = E(238 separate nuclei) - 238 * B/A(U238); E(Pd119) = E(119 separate nuclei) - 119 * B/A(Pd119)

So if you subtract the final energy from the initial energy, you get:

E(238 separate nucleu) - 238 * 7.6 - 2*(E(119 separate nuclei) - 119 * 8.5) = 238*(8.5 - 7.6)
 
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1. What is the process of dividing 238U into two 119Pd and why does energy get released?

The process of dividing 238U into two 119Pd is called nuclear fission. This is a process in which the nucleus of an atom splits into smaller nuclei, releasing a large amount of energy. This energy is released because the total mass of the smaller nuclei is less than the original nucleus, and according to Einstein's famous equation E=mc^2, this mass difference is converted into energy.

2. How is the energy released when 238U is divided into two 119Pd measured?

The energy released in a nuclear fission reaction is measured using the unit of electron volts (eV). This unit represents the amount of energy gained by an electron when it is accelerated through an electric potential difference of one volt. In the case of dividing 238U into two 119Pd, the energy released is typically measured in millions or billions of electron volts (MeV or GeV).

3. What factors affect the amount of energy released when 238U is divided into two 119Pd?

The amount of energy released in a nuclear fission reaction depends on several factors, including the mass of the original nucleus, the mass of the resulting nuclei, and the binding energy of the particles involved. Additionally, the speed and direction of the particles can also affect the amount of energy released.

4. Is the energy released when 238U is divided into two 119Pd always the same?

No, the amount of energy released in a nuclear fission reaction can vary depending on the specific atoms involved and the conditions of the reaction. For example, the amount of energy released in a controlled nuclear power plant reaction may be different from the amount released in an uncontrolled nuclear explosion. However, the total amount of energy released in any nuclear fission reaction will always follow the law of conservation of energy.

5. What are the potential uses of the energy released when 238U is divided into two 119Pd?

The energy released in a nuclear fission reaction has many potential uses, including electricity generation in nuclear power plants, propulsion for spacecraft, and medical treatments such as cancer therapy. However, it also has the potential for destructive uses, such as nuclear weapons, which is why it is crucial to carefully control and monitor nuclear reactions.

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