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The nuclide B58 decays by positron emission to B58 . What is the energy released (in MeV).

Short Answer

Expert verified

The energy released is 21.40MeV.

Step by step solution

01

Positron Emission

For a nucleus having NZ<1 , positron decay takes place to stabilize the nucleus. When a positron emission takes place, a proton is transformed to a neutron. Positron emission is also accompanied by a neutrino emission. The mass number of the daughter nuclei remains same as that of the parent nucleus, but the atomic umber of the daughter nuclei is one less than that of the parent nuclei.

B58Be +48e++ 10+ν

02

  Energy released

To calculate the kinetic energy involved in the positron decay we have to calculate the mass difference.

Δm=mB410+2me+10-mB510=8.000530u+2×0.00054858u-8.024607u=-0.022981u

ΔE=-0.022981×931.5MeV=-21.40MeV

Therefore, the energy released is 21.40MeV.

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Most popular questions from this chapter

Plutonium-239 is the fissionable isotope produced in breeder reactors; it is also produced in ordinary nuclear plants and in weapon tests. It is an extremely poisonous substance with a half-life of 24,100 years.

  1. Write an equation for the decay Pu239of via alpha emission.
  2. The atomic mass of Pu239is 239.05216 u and that of U235is 235.04393 u. Calculate the energy released per Pu239atom , in MeV, in decaying via alpha emission.
  3. What will be the initial activity, in disintegrations per second of 1.00 g of Pu239buried in a disposal site for radioactive wastes?
  4. What activity will the material from part c show after 100,000 years.

Calculate the total binding energy, in both kJ per mole and MeV per atom, and the binding energy per nucleon of the following nuclides using the data from Table 19.1.

(a) Ca2040


(b) Rb3787

(c) U92238

The nuclide U92231converts spontaneously to Pa91231.

1. Write two balanced nuclear equations for this conversion, one if it proceeds by electron capture and the other if it proceeds by positron emission.

2. Using the nuclidic masses in Table 19.1, calculate the change in mass for each process. Explain why electron capture can occur spontaneously in this case but positron emission cannot.

The nuclidePu239 undergoes alpha decay with a half-life of2.411×104years. An atomic energy worker breathes in5.0×10-6g5.0mg of role="math" localid="1663337289506" Pu239, which lodged permanently in a lung.

  1. Compute the activity in becquerels, of the Pu239 ingested, taking the atomic mass of the nuclide to be 239g/mol.
  2. Determine the radiation absorbed dose in milligrays, during the first year after its ingestion. Assume that alpha particles emitted by have an average kinetic energy of 5.24MeV, that all of this energy is deposited within the worker’s body, and the worker weighs 60 kg.
  3. Is this dose likely to be lethal?

Use the data from Table 19.1 to predict which is more stable: 16 protons, 16 neutrons and 16 electrons organized as two O16 or one S32. What is the mass difference?

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