When does the formula for radioactive decay become invalid?

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Discussion Overview

The discussion revolves around the validity of the radioactive decay formula N(t)=N_0e^{-\lambda t}, specifically questioning the conditions under which it remains applicable. Participants explore the implications of the number of atoms considered, the density of radioactive materials, and the statistical nature of decay processes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how to determine the number of atoms (N_0) to use in the decay formula when considering multiple sources of radioactive material, such as two separate balls of plutonium.
  • Another participant argues that the number of decays over time does not depend on the total number of atoms present, emphasizing that the formula represents a statistical probability rather than a deterministic outcome.
  • Some participants suggest that as long as there are enough atoms for statistical reasoning to apply, the formula remains valid, regardless of whether the atoms are grouped or separated.
  • One participant clarifies that the formula can be applied to either one or both balls of material, indicating that the decay rate is independent of the interaction between the two groups.
  • There is a discussion about the interpretation of decay rates and how they relate to the concept of probability, with some participants expressing confusion about the implications of grouping atoms.

Areas of Agreement / Disagreement

Participants express varying views on the applicability of the decay formula in different scenarios, with some agreeing that it can be applied to individual or combined groups of atoms, while others emphasize the statistical nature of decay processes. The discussion remains unresolved regarding the specific conditions that might invalidate the formula.

Contextual Notes

Participants highlight the potential limitations of the formula when dealing with very small numbers of atoms, suggesting that the average rate of decay may not hold in such cases. There is also mention of the need for a minimum density of radioactive elements for accurate application of the formula.

fluidistic
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Hello,
I'd like to know when the formula N(t)=N_0e^{-\lambda t} is not valid anymore. By that I mean... since N_0 is the number of atoms at time t=0 and N(t) is the number of atoms at time "t", we see that N(t) depends of N_0. Now my question is : how do you know how many atoms should we take in count? Say we have 2 balls of plutonium, separated by 3 meters. How do you apply the formula given above? Is it still valid? Do you have to take N_0 as the number of atoms in the 2 balls, or you can apply the formula for each ball?
To be more precise, what is the minimum density of radioactive elements we can consider to have a decent approximation using the formula?
What is the "error" of the formula?
I'm sorry if this makes a lot of questions and if they're not precise enough.
 
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It doesn't matter.
The number of decays in a period of time doesn't depend physically on the number of atoms present - it's really just another way of writing the probability of a given atom decaying within a certain time.

Obviously it breaks down when there are only a few atomspresent since it is only an average rate.
 
I'd generally agree with mgb's post...radioactive decay is a quantum tunneling statistical phenom so if you've got a glob of matter big enough to see likely there are enough atoms in it for statistical reasoning to apply...
 
I think you guys are making this harder than the original question. The answer is, you apply the equation to either or both balls of decaying material. If you apply it to both, you get the "N" vs time that is the total number in both balls. If you apply it to one ball, N is the number in that ball. The two balls don't have to know anything about each other... and ultimately, there is a probability of each individual atom decaying (thats what the lambda is in the equation)

Sorry I don't know how to write equations here, but think about this:

N = No exp(-lambda t)

so the time derivative of N (the rate of decay) is

N-dot = (-lambda)No exp(-lambda t)

then N-dot divided by N(t) (or the probability of decay) is

((-lambda)No exp(-lambda t))/(No exp(-lambda t))
=-lambda

see, the "No" drops out

Have I done that right? Does it help??

Now, can someone point me to the instructions for entering equations here?
 
Radioactive decay is often described in terms of the 'number of atoms present' this makes it sound like there is some hidden/quantum communication between the atoms as they decide how many are going to decay in the next second. From this explanation it's resonable to ask how you define a group of atoms - does the rate change if you split the group in two etc.

The important thing is that the half life and decay laws have nothing to do with radioactivity - they work for any process where a large number of things have the same probability of doing some event within a certain time frame.

ps. Click the 'go advanced' button in the reply - then the Sigma sign for help with latex.
 
I think I got it. It means that it doesn't matter if I take into consideration one ball or 2 balls, the formula would work in either cases. Nice to know.
 

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