Probability of 1st Arrival From Poisson Process of Rate $\lambda$

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Discussion Overview

The discussion centers around calculating the probability that the first arrival from a combined Poisson process of rates $\lambda$ and $\mu$ comes from the process with rate $\lambda$. Participants explore various methods of integration and probability calculations related to Poisson processes, with a focus on understanding the underlying reasoning and assumptions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents an initial solution involving integration but expresses uncertainty about the reasoning behind it, arriving at the result $1/\lambda - 1/(\lambda + \mu)$.
  • Another participant challenges the initial result, noting that it does not behave correctly under certain limits (e.g., as $\mu \to 0$), suggesting a different approach that leads to a result of $1$ in that limit.
  • A participant reflects on their previous summation method and acknowledges the need for conditioning on no events occurring before time $t$, leading to a revised result of $\lambda/(\lambda + \mu)$.
  • Further elaboration on the conditional probabilities is provided, with one participant detailing their calculations using specific probabilities for the Poisson processes and arriving at the same result as the previous participant.
  • There is a request for an alternative method that does not rely on infinitesimals, indicating a desire for clarity using the standard definition of the Poisson process.

Areas of Agreement / Disagreement

Participants express differing views on the correct approach to the problem, with multiple methods proposed and no consensus reached on a single solution. Some results align, but the reasoning and methods vary significantly.

Contextual Notes

Participants note limitations in their approaches, including assumptions about independence and the treatment of events over time. There are unresolved questions regarding the use of infinitesimals and the equivalence of different definitions of the Poisson process.

Who May Find This Useful

This discussion may be useful for individuals interested in probability theory, particularly those studying Poisson processes and their applications in various fields of mathematics and engineering.

rsq_a
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I did this question, but I'm unsure of my reasons behind it. I was hoping someone here could go through the problem for me.

Consider the sum of two independent Poisson processes of rates [itex]\lambda[/itex] and [itex]\mu[/itex]. Find the probability that the first arrival of the combined [itex](\lambda + \mu)[/itex] process comes from the process of rate [itex]\lambda[/itex]

I got the answer [tex]1/\lambda - 1/(\lambda + \mu)[/tex]. I did so by integrating,

[tex]\int_0^\infty P(\text{one event from } \lambda \text{ in }(0, t]) \times P(\text{zero event from } \mu \text{ in }(0, t]) \ dt[/tex]

Except I didn't have any good reason for integrating the whole thing except for the idea that I want to add up all the probabilities. Is this the way it's supposed to be done?
 
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If you look at your result, and consider mu -> 0, your result approaches 0, which is not correct. It should approach 1 in that case. When lambda -> 0 in your formula, the probability diverges towards infinity...

You can use the first formula here for all probabilities below:
http://en.wikipedia.org/wiki/Poisson_process

I would calculate it like this:

[tex] P = \int_0^\infty dP(t)[/tex]

where dP(t) = P1*P2*P2 is a conditional probability:

P1 = prob. that the lambda-process increases by one in the interval [t,t+dt]
P2 = prob. that the lambda process is 0 at time t
P3 = prob. that mu-process is zero at time t+dt.

The three contributions are independent, so their probabilities can simply be multiplied. The contribution to the total probability represent different events, so they can be summed.

The end result I get I get is different from your, and in the limit lambda -> infty or mu->0 I get 1. In the limit lambda -> 0 (where mu \neq 0) I get 0. These limits are quite sensible. Also, my result is always in [0,1] independent of the values of lambda and mu, as long as they are bth positive.

I first started to fool around with a stopping time, but it seems to be unnecessary.

Torquil
 
Last edited:
Torquil,

I believed I did it correctly this time. It would be very helpful if you could write out for me your solution method. I'm a bit new to probability, so little differences in notation and approaches are confusing to me.

The problem with what I did before was that I was summing,

[tex]\sum_t P(N_\lambda(0,t+\Delta t] = 1, N_\mu(0,t+\Delta t] = 0)[/tex]

where N denotes the number of arrivals from each distribution. This is incorrect because the different events (over all t) are not disjoint. The correct way to proceed is to make things conditional on no events occurring from 0 to t. Like so...

[tex]\sum_t P(N_\lambda(0,t] = 0, N_\lambda(t,t+\dDelta t] = 1, N_\mu(0,t+\Delta t] = 0)[/tex]

After this, taking [itex]\Delta t \to 0[/itex] and integrating gives me [itex]\lambda/(\lambda + \mu)[/itex], which seems to make more sense.

Even if your solution is similar, it would help me a lot if you could post it. Thanks!
 
rsq_a said:
Torquil,

I believed I did it correctly this time. It would be very helpful if you could write out for me your solution method. I'm a bit new to probability, so little differences in notation and approaches are confusing to me.

The problem with what I did before was that I was summing,

[tex]\sum_t P(N_\lambda(0,t+\Delta t] = 1, N_\mu(0,t+\Delta t] = 0)[/tex]

where N denotes the number of arrivals from each distribution. This is incorrect because the different events (over all t) are not disjoint. The correct way to proceed is to make things conditional on no events occurring from 0 to t. Like so...

[tex]\sum_t P(N_\lambda(0,t] = 0, N_\lambda(t,t+\dDelta t] = 1, N_\mu(0,t+\Delta t] = 0)[/tex]

After this, taking [itex]\Delta t \to 0[/itex] and integrating gives me [itex]\lambda/(\lambda + \mu)[/itex], which seems to make more sense.

That is the same result that I got.

Even if your solution is similar, it would help me a lot if you could post it. Thanks!

For my P1, P2, P3 above, I used (from the wikipedia formula):

P1 = lambda*dt*exp(-lambda*dt)
P2 = exp(-lambda*t)
P3 = exp(-mu*(t+dt))

Multiplying them together, expanding to first order in dt, then putting it into the integral, I get

\int_0^infinity exp(-(lambda+mu)t) lambda dt = lambda/(lambda+mu)

Torquil
 
torquil said:
That is the same result that I got.
For my P1, P2, P3 above, I used (from the wikipedia formula):

P1 = lambda*dt*exp(-lambda*dt)
P2 = exp(-lambda*t)
P3 = exp(-mu*(t+dt))

Multiplying them together, expanding to first order in dt, then putting it into the integral, I get

\int_0^infinity exp(-(lambda+mu)t) lambda dt = lambda/(lambda+mu)

Torquil

Yes, this was exactly what I had done.

Is there a way to do this without the use of infinitesimals? That is, is there a way to do the problem, only using the fact that we know,

[tex]P(N_\lambda(0,t] = k) = \frac{e^{-\lambda t} (\lambda t)^k}{k!}[/tex]

I realize the two definitions of the Poisson Process are equivalent, but an alternative route using this definition would clear things up for me.
 

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