syllll_213 said:
Homework Statement: Which would halve Sarah's dose rate? Not Doubling the thickness of Perspex.
Relevant Equations: I = I0e(-x/lamdax)
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Hi, I wonder how C should be calculated. I tried finding the ratio of new intensity to the original intensity, which gives the exponential chunck, and I wonder if that is enough to show that doubling the shield thickness would not halve the dose? Is there a clearer and more numerical representation?
For monochromatic gamma radiation and X-rays (but not ##\alpha## or ##\beta## radiation):
##I(d) = I_0 e^{-\mu d}##
where ##\mu## is the linear absorption coefficient and ##d## is the absorber thickness.
If ##d## is the ‘half-thickness’ then ##I(d) = \frac 12 I_0##. That means ##e^{-\mu d} = \frac 12##
If we have two half-thicknesses then:
##I(2d) = I_0 e^{-\mu 2d} = I_0( e^{-\mu d})^2 = I_0 \times (\frac 12)^2 = \frac 14 I_0##
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The above shows that if the original shield thickness is the half-thickness, then doubling it does indeed halve the dose-rate (reducing it from ##\frac 12 I_0## to ##\frac 14 I_0##).
But in this question we are give no information about the value of ##d##. It may not be the half-thickness. If the original thickness, ##d##, is some arbitrary value that reduces the intensity by a factor ##f## then a thickness of ##2d## reduces the intensity by a factor ##f^2## (e.g. from ##0.60 I_0## to ##0.36 I_0## which is not halving).
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The exponential relationship is applicable to gamma/X-rays. It is
not applicable to ##\alpha## or ##\beta## radiation (because ##\alpha## and ##\beta## patticles have finite ranges in matter). P-32 is a ##\beta## emitter so the above equations can’t be used. This may be an unintended error by the author of the question.
So (IMO) there is only one correct answer on the answer-list (not C).
Minor edit.