New distance between the Geiger counter and the source

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Homework Help Overview

The discussion revolves around a problem involving a point source of γ-radiation, its half-life, and the relationship between count rates recorded by a Geiger counter at different distances from the source. Participants explore how to determine the new distance between the counter and the source after a specified time period, given initial and final count rates.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the inverse square law and its implications for the count rate as distance changes. There are attempts to relate count rates to distance through various formulas, including exponential decay and ratios. Some participants express uncertainty about how to connect different equations and concepts.

Discussion Status

Several participants have offered insights into the relationship between count rates and distance, suggesting the use of ratios and the inverse square law. There is ongoing exploration of how to apply these concepts to find the new distance, with no clear consensus reached yet.

Contextual Notes

Participants note the constraints of the problem, including the half-life of the radiation source and the specific count rates at two different times. There is also mention of the need for a constant of proportionality in the equations discussed, which remains undefined in the context of the problem.

moenste
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Homework Statement


A point source of γ-radiation has a half-life of 30 minutes. The initial count rate, recorded by a Geiger counter placed 2.0 m from the source, is 360 s-1. The distance between the counter and the source is altered. After 1.5 hour the count rate recorded is 5 s-1. What is the new distance between the counter and the source?

Answer: 6 m.

2. The attempt at a solution
We have:
T1 / 2 = 1800 s.
d = 2 m
R = 360 s-1

t = 5400 s
d = ?
R = 5 s-1

No idea what to do here. R = R0 e- λ t, but I don't see a way to find distance from this formula. There is also a formula from the experimental verification of the inverse square law for γ-rays: x = k R- 1 / 2 - c, where d = x + c (distance between actual position of source and effective point of detection), k = constant of proportionality. But I still see not much connection between these two formulas.

Maybe I'm looking in the wrong direction?
 
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The inverse square law applies. First determine the new count rate that would be detected at the original distance (if the counter were not moved). Any difference of the actual measured rate from that rate must be due to the change in distance from the source.
 
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We seem number of photons will be distributed onto a sphere, If N is number of photons that appears at time t, ##\frac{N}{4\pi r^2}## will be the number of photons that the count rate recorded.
 
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gneill said:
First determine the new count rate that would be detected at the original distance (if the counter were not moved).
R = R0 e- λ t = 360 * e- (ln 2 / 1800) * 5400 = 45 s-1?

gneill said:
Any difference of the actual measured rate from that rate must be due to the change in distance from the source.
It looks like the difference is 45 - 5 = 40 s-1.

I also simplified the formula d = k / √ R. Though I've no idea what is k.
 
moenste said:
R = R0 e- λ t = 360 * e- (ln 2 / 1800) * 5400 = 45 s-1?
Good.
It looks like the difference is 45 - 5 = 40 s-1.

I also simplified the formula d = k / √ R. Though I've no idea what is k.

Differences won't help. Use ratios to scale the rate with distance. It's an inverse square law so rate ∝ 1/d2.
 
gneill said:
Differences won't help. Use ratios to scale the rate with distance. It's an inverse square law so rate ∝ 1/d2.
I ∝ 1 / d2
I ∝ 1 / 22
I ∝ 0.25

I still don't the use of it. Maybe you mean 45 s-1 / 2 m = 5 s-1 / d → d = 0.22 m?
 
At intial time, the count rate recorded is R. It means:
$$R=\frac{N_0}{4\pi d^2}$$
The distane d will change into d'. After 1,5h and ##N_0## will change into N. Find the ratio d'/d. You will have the answer
 
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Suppose you have a quantity A that varies as the inverse square of the distance d. Then inserting a constant of proportionality k you can write:

##A = \frac{k}{d^2}##

Now if you have two pairs of data, ##(A_1,d_1)## and ##(A_2,d_2)##, then you can write:

##A_1 = \frac{k}{d_1^2}## and ##A_2 = \frac{k}{d_2^2}##

You can then form the ratios:

##\frac{A_2}{A_1} = \frac{\frac{k}{d_2^2}}{\frac{k}{d_2^2}} = \frac{d_1^2}{d_2^2}##

Or, extracting the important relationship:

##\frac{A_2}{A_1} = \frac{d_1^2}{d_2^2}##

If you have a known data pair and one half of another data pair, you can find the "missing" value.
 
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Hamal_Arietis said:
$$R=\frac{N_0}{4\pi d^2}$$
Sorry my equation is incorrect.
R is the number of photon that the count rate recorded in 1s. So at the time A point source of γ-radiation has ##N_0## photons. Number of photons that count rate recorded in 1s is:
$$R=\frac{N_0(1-e^{-1.\lambda })}{4\pi d^2}$$
After 1,5h and d change into d'
$$R'=\frac{N(1-e^{-1.\lambda })}{4\pi d'^2}=\frac{N_0.e^{-\lambda t}.(1-e^{-1.\lambda })}{4\pi d'^2}$$

Find the ratio.
 
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gneill said:
Suppose you have a quantity A that varies as the inverse square of the distance d. Then inserting a constant of proportionality k you can write:

##A = \frac{k}{d^2}##

Now if you have two pairs of data, ##(A_1,d_1)## and ##(A_2,d_2)##, then you can write:

##A_1 = \frac{k}{d_1^2}## and ##A_2 = \frac{k}{d_2^2}##

You can then form the ratios:

##\frac{A_2}{A_1} = \frac{\frac{k}{d_2^2}}{\frac{k}{d_2^2}} = \frac{d_1^2}{d_2^2}##

Or, extracting the important relationship:

##\frac{A_2}{A_1} = \frac{d_1^2}{d_2^2}##

If you have a known data pair and one half of another data pair, you can find the "missing" value.
Get it, just rearrange the equation for k and then substitute in the first equation parts of the second instead of k.

R1 d12 = R2 d22
45 * 22 = 5 * d22
d2 = 6 m.

Thank you!
 

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