Why Half life radiation is constant

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Discussion Overview

The discussion centers around the concept of half-life in radioactive decay, specifically addressing why half-life is independent of the quantity of radioactive substance present. Participants explore definitions, implications, and alternative concepts related to half-life.

Discussion Character

  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants define half-life as the time it takes for half of a radioactive sample to decay, asserting that the decay of individual nuclei is independent of the sample size.
  • Others question the terminology of "half-life," suggesting that a "full life" might be more intuitive, although they acknowledge that full life depends on quantity.
  • Several participants emphasize that there is no defined time for all nuclei to decay, leading to the conclusion that "full life" is a meaningless concept in practical terms.
  • Some argue that half-life is a preferred fraction due to its simplicity in calculations, while others propose the idea of defining other fractional lives, such as third or quarter life.
  • A few participants note that half-life is primarily used in the context of radioactive decay, contrasting it with other exponential decay situations that utilize decay constants.
  • One participant mentions the biological half-life, which differs from radioactive half-life, as an example of half-life's application in other fields.
  • There is a discussion about the historical context of the term "half-life" and its mathematical implications, with some participants expressing curiosity about its origins.

Areas of Agreement / Disagreement

Participants express a mix of agreement and disagreement regarding the terminology and implications of half-life. While there is a shared understanding of the definition of half-life, the discussion reveals competing views on the relevance and utility of the concept of "full life" and alternative fractional lives.

Contextual Notes

Some statements reflect uncertainty regarding the definitions and implications of half-life, particularly in relation to individual atoms and the mathematical modeling of decay. The discussion also touches on the limitations of applying the concept of half-life outside of radioactive decay.

  • #61
One cannot establish "half' unless one knows the "whole"
Else there is no half.

How is it that nuclear decay "knows" this?
Some type of entanglement?
 
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  • #62
pallidin said:
One cannot establish "half' unless one knows the "whole"
Else there is no half.

How is it that nuclear decay "knows" this?
Some type of entanglement?

The half is as compared to the total number of atoms. No entanglement needed. If it would make you happier, another way to look at the half life is that it is the time in which any given atom has a 50% probability of decaying. No connection to any other atoms (or knowledge of them) is needed.
 
  • #63
pallidin said:
One cannot establish "half' unless one knows the "whole"
Else there is no half.
I thought you said above you were onboard with exponential decay and just wanted to know why? You even gave an example of radioactive decay you accepted. Now you're not accepting it anymore? Did you read the above posts regarding stability?
 
Last edited:
  • #64
pallidin said:
One cannot establish "half' unless one knows the "whole"
Else there is no half.

How is it that nuclear decay "knows" this?
Some type of entanglement?

No. You are thinking of the semantics of the phrase "half-life" incorrectly. The half-life is NOT the time it takes a particular sample to decay by half. There is no difference between the sample you started with, and half of that sample. It is the time it takes ANY AMOUNT to decay by half. The half-life is completely independent of how much material you have. The half-life is defined as:

t_{1/2}=\frac{ln \: 2}{\lambda}

Lambda is the decay constant, which is a particular value for each isotope. The half-life is just a different mathematical representation of this decay constant. Another way of expressing half-life is the mean lifetime, tau:

t_{1/2}=\tau \: ln \: 2

The mean lifetime is the average time it takes for any atom of a particular isotope to decay, even if it is just a single atom by itself.

The nuclear decay of an atom does not know about any other atoms around it. There is no entanglement. This is precisely the point.
 
  • #65
pallidin said:
One cannot establish "half' unless one knows the "whole"
Else there is no half.

How is it that nuclear decay "knows" this?
Some type of entanglement?
Exactly the same exponential decrease happens with charge stored on a capacitor or water draining from a small hole in the bottom of a cylindrical tank. In all cases, the rate of decrease is proportional to the level at any given time.
Why introduce "entanglement" when it's not necessary. You seem to be introducing it as just a buzzword, for no reason.
 
  • #66
pallidin said:
One cannot establish "half' unless one knows the "whole"
Else there is no half.

How is it that nuclear decay "knows" this?
Some type of entanglement?

The "whole" is the initial quantity. "Half" does not refer to "half of the whole life" but to "half of the initial quantity", which is well established.
 
  • #67
QuantumPion said:
No. You are thinking of the semantics of the phrase "half-life" incorrectly. The half-life is NOT the time it takes a particular sample to decay by half. There is no difference between the sample you started with, and half of that sample. It is the time it takes ANY AMOUNT to decay by half. The half-life is completely independent of how much material you have. The half-life is defined as:

t_{1/2}=\frac{ln \: 2}{\lambda}

Lambda is the decay constant, which is a particular value for each isotope. The half-life is just a different mathematical representation of this decay constant. Another way of expressing half-life is the mean lifetime, tau:

t_{1/2}=\tau \: ln \: 2

The mean lifetime is the average time it takes for any atom of a particular isotope to decay, even if it is just a single atom by itself.

The nuclear decay of an atom does not know about any other atoms around it. There is no entanglement. This is precisely the point.

Ah, yes, I think I'm beginning to understand. Thank you.
 

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