What is the heat released from the decay of 1 kg of 40K atoms?

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Discussion Overview

The discussion revolves around the heat released from the decay of 1 kg of the radioisotope 40K, focusing on the calculations and assumptions involved in determining the energy output from its decay processes. Participants explore the theoretical and practical implications of the decay modes, energy release, and discrepancies in calculated values.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant calculates the mean heat released per decay of 40K to be about 1.33 MeV, leading to an estimated total energy release of 3.2x10^12 Joules from 1 kg of 40K.
  • Another participant notes that a significant fraction of the energy from decay is released as neutrinos, which do not contribute to heating the material under normal conditions.
  • A participant provides the decay equations for 40K, questioning how to calculate the heat if the indicated energy does not account for all forms of energy release.
  • It is mentioned that for electron capture, nearly all energy is released as neutrinos, while in beta decay, the energy is shared between the electron and neutrino, with the kinetic energy of the nucleus being negligible.
  • There is a reference to the positron annihilation producing additional gamma rays, which could contribute to heating if absorbed.

Areas of Agreement / Disagreement

Participants express differing views on the calculation of heat released from 40K decay, particularly regarding the role of neutrinos and the energy distribution in decay processes. There is no consensus on the correct value for the heat produced per kilogram of 40K.

Contextual Notes

Participants highlight the importance of considering the fraction of energy released as neutrinos and the implications for heat calculation. There are unresolved aspects regarding the exact contributions of different decay modes and energy forms.

Hypatio
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The radioisotope 40K decays either by electron capture (~10% of the time), releasing about 1.31 MeV, or by beta decay (90% of the time), releasing about 1.51 MeV. Thus the mean heat released is about 1.33 MeV per decay.

There are 1.5x10^25 40K atoms in 1 kilogram. Therefore the energy which could be released from complete decay of 1 kg is \phi=3.2x10^12 Joules.

The half-life of 40K is T=1.277x10^9 years, or 4.027x10^16 sec.

Therefore, we can calculate the heat produced (W/kg) from the decay of 1 kg of 40K atoms as:

=\phi\exp(-tln(2)/T)\frac{ln(2)}{T}=\phi\frac{ln(2)}{T}

I calculate 5.53x10^-5 W/kg, but numerous sources which I would otherwise consider authoritative give values which are closer to 3x10^-5 W/kg. I don't understand why our values are so different. I have calculated the heat released from many other radioisotopes (e.g. 235U, 232Th, etc.) without problems.

Am I correct, or where have I gone wrong?
 
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Thus the mean heat released is about 1.33 MeV per decay.
This looks like the mean energy released. A significant fraction is released as neutrinos, which do not heat the material unless you happen to be in a neutron star or similar environments.
 
ok well the equations for 40K decay are

40K ---> 40Ca + e- + n + 1.31 MeV
40K+ e- ---> 40Ar + v + 1.51 MeV

where e- is an electron, n is an electron anti-neutrino, and v is an electron neutrino.

So if the energy indicated doesn't give you the heat, how do you calculate it?
 
You need the fraction of the energy which is released as neutrinos. For electron capture, this is nearly the whole energy. In the beta decay, electron and neutrino (not a neutron) share the released energy. The kinetic energy of the nucleus should be negligible here.
The positron annihilates afterwards, producing two gamma rays. If they get absorbed, they give additional 1.022 MeV.
 

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