Time dependent probabilities












0














I have a problem understanding how probabilities develop over time. An example:




A radioactive element has a half life $t_{1/2}$.




That must mean that for an individual atom the probability that it has decayed at $t_{1/2}$ is $0.5$. (Sorry about the ugly notation $t_{1/2}$ means half life, I change to $k$ henceforth to make it look a bit cleaner)




After two half lives only a quarter of the original population remains.




I interpret this as the cumulative probability $P(t)$ of an atom having decayed after a time $t$ should look like $P(t)=1-0.5^{frac{t}{k}}$. This makes sense with $P(0)=0$ and $P(inf)=1$.



Now for the part where I get confused: There must be such a thing as an instantaneous probability at every moment that integrates to $P(t)$. You'd guess that this should be the derivative $frac{dP}{dt}=frac{ln(2) cdot 0.5^{t/k}}{k}$. However, this probability is time dependent and that is unphysical. The atom must have a constant probability of decay at any given moment. It doesn't know how I set up the experiment. I understand that there is something about probabilities that I don't understand. Any insight would be appreciated.










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  • Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
    – Oskar
    2 days ago










  • You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
    – Did
    2 days ago










  • But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
    – Oskar
    2 days ago










  • No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
    – Did
    2 days ago










  • integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
    – Oskar
    yesterday
















0














I have a problem understanding how probabilities develop over time. An example:




A radioactive element has a half life $t_{1/2}$.




That must mean that for an individual atom the probability that it has decayed at $t_{1/2}$ is $0.5$. (Sorry about the ugly notation $t_{1/2}$ means half life, I change to $k$ henceforth to make it look a bit cleaner)




After two half lives only a quarter of the original population remains.




I interpret this as the cumulative probability $P(t)$ of an atom having decayed after a time $t$ should look like $P(t)=1-0.5^{frac{t}{k}}$. This makes sense with $P(0)=0$ and $P(inf)=1$.



Now for the part where I get confused: There must be such a thing as an instantaneous probability at every moment that integrates to $P(t)$. You'd guess that this should be the derivative $frac{dP}{dt}=frac{ln(2) cdot 0.5^{t/k}}{k}$. However, this probability is time dependent and that is unphysical. The atom must have a constant probability of decay at any given moment. It doesn't know how I set up the experiment. I understand that there is something about probabilities that I don't understand. Any insight would be appreciated.










share|cite|improve this question









New contributor




Oskar is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
Check out our Code of Conduct.




















  • Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
    – Oskar
    2 days ago










  • You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
    – Did
    2 days ago










  • But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
    – Oskar
    2 days ago










  • No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
    – Did
    2 days ago










  • integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
    – Oskar
    yesterday














0












0








0







I have a problem understanding how probabilities develop over time. An example:




A radioactive element has a half life $t_{1/2}$.




That must mean that for an individual atom the probability that it has decayed at $t_{1/2}$ is $0.5$. (Sorry about the ugly notation $t_{1/2}$ means half life, I change to $k$ henceforth to make it look a bit cleaner)




After two half lives only a quarter of the original population remains.




I interpret this as the cumulative probability $P(t)$ of an atom having decayed after a time $t$ should look like $P(t)=1-0.5^{frac{t}{k}}$. This makes sense with $P(0)=0$ and $P(inf)=1$.



Now for the part where I get confused: There must be such a thing as an instantaneous probability at every moment that integrates to $P(t)$. You'd guess that this should be the derivative $frac{dP}{dt}=frac{ln(2) cdot 0.5^{t/k}}{k}$. However, this probability is time dependent and that is unphysical. The atom must have a constant probability of decay at any given moment. It doesn't know how I set up the experiment. I understand that there is something about probabilities that I don't understand. Any insight would be appreciated.










share|cite|improve this question









New contributor




Oskar is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
Check out our Code of Conduct.











I have a problem understanding how probabilities develop over time. An example:




A radioactive element has a half life $t_{1/2}$.




That must mean that for an individual atom the probability that it has decayed at $t_{1/2}$ is $0.5$. (Sorry about the ugly notation $t_{1/2}$ means half life, I change to $k$ henceforth to make it look a bit cleaner)




After two half lives only a quarter of the original population remains.




I interpret this as the cumulative probability $P(t)$ of an atom having decayed after a time $t$ should look like $P(t)=1-0.5^{frac{t}{k}}$. This makes sense with $P(0)=0$ and $P(inf)=1$.



Now for the part where I get confused: There must be such a thing as an instantaneous probability at every moment that integrates to $P(t)$. You'd guess that this should be the derivative $frac{dP}{dt}=frac{ln(2) cdot 0.5^{t/k}}{k}$. However, this probability is time dependent and that is unphysical. The atom must have a constant probability of decay at any given moment. It doesn't know how I set up the experiment. I understand that there is something about probabilities that I don't understand. Any insight would be appreciated.







probability






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Check out our Code of Conduct.









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edited 2 days ago









amWhy

192k28225439




192k28225439






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asked 2 days ago









OskarOskar

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1




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Oskar is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
Check out our Code of Conduct.






Oskar is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
Check out our Code of Conduct.












  • Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
    – Oskar
    2 days ago










  • You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
    – Did
    2 days ago










  • But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
    – Oskar
    2 days ago










  • No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
    – Did
    2 days ago










  • integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
    – Oskar
    yesterday


















  • Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
    – Oskar
    2 days ago










  • You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
    – Did
    2 days ago










  • But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
    – Oskar
    2 days ago










  • No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
    – Did
    2 days ago










  • integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
    – Oskar
    yesterday
















Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
– Oskar
2 days ago




Thanks for the clean-up of the formulas but it should be ln2 x 0.5^(t/k).
– Oskar
2 days ago












You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
– Did
2 days ago




You missed that $P'(t)=ae^{-at}$ is the variation of the total proportion of decayed atoms at time $t$. The probability of a single non decayed atom at time $t$ to decay between times $t$ and $t+dt$ is $acdot dt$.
– Did
2 days ago












But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
– Oskar
2 days ago




But then the cumulative probability will increase linearly with time and soon be >1. Or am I missing something?
– Oskar
2 days ago












No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
– Did
2 days ago




No, the cumulative probability increases nonlinearly up to $1$. What makes you think otherwise?
– Did
2 days ago












integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
– Oskar
yesterday




integration of dP=(a x dt) from 0 to t gives P(t)=at, right?
– Oskar
yesterday










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