measures of radioactivity: a tool for understanding statistical data analysisa tool for...
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7/30/2019 Measures of radioactivity: a tool for understanding statistical data analysisa tool for understanding statistical data
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Measures of radioactivity:Measures of radioactivity:
a tool for understanding statistical data analysisa tool for understanding statistical data analysisVera Mont albanoVera Mont albano
Phys. Department, University of Siena
References
[1] A. Porri, R. Benedetti, E.Mariotti, V. Millucci, V. Montalbano, Esperienze significative del ProgettoLauree Scientifiche di Siena, Proceeding ComunicareFisica, Trieste 1 6 ottobre 2007
[2] A. Porri, R. Benedetti, E.Mariotti, V. Millucci, V. Montalbano, La Scuolaestiva del Pigelleto e I Giocattolial Liceo, in atti del XLVI National Congress AIF, Suppl. n. 3 La Fisicanella Scuola , 130, 2008
[3] R. Benedetti, S. DiRenzone, E.Mariotti, V. Montalbano, A. Porri, Un percorso di orientamento sulla fisica moderna, Comunicare Fisica 2010, in corso di stampa
[4] R. Benedetti, E. Mariotti, V. Montalbano, A.Porri, Active and cooperative learning paths in thePigelletos Summer School of Physics, Twelfth International Symposium Frontiers of Fondamental Physics (nearby poster ID 91)
[5] P. R. Bevington Data Reduction and Errors Analysis for Physical Science, McGraw-Hill Book Company, New York 1969
[6] http://stattrek.com/Lesson3/SamplingTheory.aspx?Tutorial=Stat
An early experience
The starting point was the Pigelletos Summer School of Physics [1-4] .
Forty students from high school are selected to attend a full immersion summer school of
physics in thePigelleto Natural Reserve, on the south east side of Mount Amiata in the
province of Siena.
In the 2009 school, titled The Achievements of Modern Physics, a learning path on
radioactivity was proposed to two small groups of students.
After a brief introduction to the nuclear phenomenology, they were involved
in measures of radioactivity from a weak source ofU in order
to characterize the emitted ionizing radiation by using a educational
device provided by a school.
A teacher was impressed by students involvement and suggested
of elaborating a learning path on Nuclear Physics in which
the students are active and perform directly measures of radioactivity.
Experiment al setup
The measures are realizedby using a commercialGeiger counter usuallyused for dosimetry.It can detect alpha, betaand gamma rays and it is
possible to collect datawithout any unit
conversion (counts) anddownload them into acomputer.
The detector and the sources are aligned by means of supportson an optical bench.
The sources are shown with theirsupports (from left):
a) small sheets of Uranium inplastic holder m1 = 0.152 g
b) sheets U in plastic holderm2 = 0.888 g
c) fluorescent marble
Our target
In order to integrate this learning path in
the ordinary school program, the activities
are planned for the last year of high school
(5a
Liceo Tecnologico) after the lessons onelectromagnetism.
Teachers make few lessons in class in which
present and discuss the phenomenology of
nuclear physics.
Afterward, the experimental setup is
presented in order to perform measure of
background radioactivity in the laboratory.
The next step is to divide students in small
groups that are involved in measures of,
and emission from weak sources ofU
and a very weak source with trace of
uranium ore.
During measurements, it rises soon the
necessity of performing many measures and
the problem of valuating uncertainties.
The students are ready to recall all their
knowledge on statistics for facing this
problem.
A brief intr oduction to n uclear phenomena
The lessons give an historical sight on the discovery of radioactivity, and connectthe previous knowledge of students to these phenomena so far from theirdaily experience.
The main topics are the following:- Discovery of radioactivity- Pierre e Marie Curie- Neutron discovery and atom structure- Dimensions of atom and its constituents- Natural radioactivity phenomenology (in particular , and rays)
- I sotopes- Forces into atoms and nuclei (how strong or weak with numerical examples)- Nuclei can die- Law of radioactive decay- Natural radioactive chains- Binding energy and mass of a bound state- Equivalence mass-energy- Binding energy per nucleon- Fission and related topics- Fusion and related topics
Related topics can be very stimulating for students, specially in these times forour society
An introduct ion to stati stical data analysis
Let us start from a question:
There are limits to the precision of a measurement?
By answering to this question, we can fix the cases in which the use of statistical data analysis
make sense.
The first step is to recall all previous knowledge of students on statistics (there are many but
almost never used in physics by teachers), such as [5,6]
- Distributions
- Representation of casual phenomena
- Mean, median, variance and standard deviation
- Bernoulli, Poisson and Gauss distributions and examples
At this point, it is possible to introduce the pupils to some elements of sampling theory, such
as
- The existence of a parent distribution- What is a good statistical sample
- Mean and variance of a sample
Now we are ready to deal with the statistical data analysis of our measures.
The data are collected in the meantime by the Geiger detector and can be downloaded in a
computer. The teacher can divide the data in sets in order of giving different tasks to any
group of students.
Some examples:
- testing samples by giving 10, 20, 30, 50 data from the background and compare means
and standard deviations of these samples with the mean and standard deviation of much
more measures (e.g. more then 1000)
- Perform measures for short period in order to verify that radioactive decay follows
Poissons distributions
- Verify that for mean values greater than the Poissons distribution become
indistinguishable from the normal one
In particular, can be very interesting to show that in case of very weak source it is possible to
quantify differences from background smaller than the uncertainties related to the physics
of radioactive decay by performing many measurements and by using statistical data
analysis.
interessante stimare qual la varianza della media m
Si pu far vedere che
n
i
mmx
nn
s
1
22 )()1(
1
Quindi nel caso in cui si hanno misure i cui risultati fluttuano,
una volta verificato che non ci sono errori sistematici, il risultato
della misura si scrive:
msm
2039
4925143
597054
326
248541
275337
d1=d0 d1=d0+4.25 d3=d0+26.4
m1= 0.152 g
24821 244
2108 286
213 215
184855 714
157134 608
685 227
Fondo =18.08 0.05
Prime misure in classe
N=25