Calculating disintegration energies of alpha emmision.

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Homework Help Overview

The discussion revolves around calculating disintegration energies associated with alpha emission, specifically focusing on the decay of 232/92U into 228/90Th. Participants are examining the mass differences and energy transformations involved in this nuclear process.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the calculation of mass differences and the application of energy equations. Questions arise regarding the interpretation of energy distribution between the alpha particle and the resulting nucleus, as well as the conservation of momentum in the decay process.

Discussion Status

The discussion is active, with participants providing insights and guidance on the calculations. There is an exploration of how energy is divided between the alpha particle and the remaining nucleus, with some participants confirming the reasoning behind the calculations presented.

Contextual Notes

Participants are working within the constraints of provided atomic masses and the requirement to apply the mass-energy equivalence principle. There is an emphasis on maintaining precision in calculations and understanding the implications of momentum conservation during the decay process.

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Homework Statement



(a) Calculate the disintegration energy when 232/92U decays by alpha emission
into 228/90Th. Atomic masses of 232/92U and 228/90Th are 232.037156u and 228.028741u, respectively.

(b) For the 232/92U decay in part (a), how much of the disintegration energy will be carried off by the alpha particle?

Given: Mass of 4/2He = 4.002603u
c^2 = 931.5MeV

Homework Equations



E=mc^2

The Attempt at a Solution



Well for part (a), first I found the difference in the starting masses and the end masses ie,
232.037156u - (228.028741u + 4.002603u) = 0.005812u
I then put this into the equation and got 5.413878MeV.
I thought this was right until I read part (b) and now I'm starting to think this might be how I'm meant to do that part, not part (a). Could anyone tell me if I'm even on the right track with this question or should I be using different equations?
 
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I see nothing wrong in a). In b), consider what happens when U-232 disintegrates, if you look at it in the frame of reference of that isotope. What happens to the nuclei? And assuming no energy loss, where does that energy go?
 
Does most or all of the energy get carried off by the alpha particle then?
 
Not all of it, no. Think of the U-232 nucleus as a group of particles bundled together. In their frame of reference, they aren't moving. Then the nucleus gets split into two different nuclei, but they can't share the same space. So what happens then to rectify this?
 
Last edited:
Well the alpha particle and the Th-228 have to move away from each other so the energy turns into kinetic energy. So if it isn't moving in the beginning, and momentum has to be conserved, then they move in opposite directions. So then since K = (p^2)/2m, the energy is divided according to their masses? So, 228/(228+4) = 0.9827. Then (0.9827)(5.413878MeV) = 5.3202179MeV goes to the alpha particle. Is that right?
 
Yes. Just remember to use all of those decimals. :smile:
 
Ok, thanks so much for the help!
 

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