SLIDE 1
Henriett Daróczi
Doctoral School of Environmental Sciences PhD student Northern Building 0.123A daroczi.henriett@gmail.com
SLIDE 2 History
- 1895. Wilhelm Conrad Röntgen discovers a type
- f electromagnetic radiation which he calls X-rays
- 1896. Henri Becquerel discovers the principle
- f radioactive decay when he
exposes photographic plates to uranium
- 1897. Sir Joseph John Thomson first describes his
discovery of the electron
SLIDE 3 History
- 1898. Marie and Pierre Curie announce
discovery of two substances they call polonium and radium.
- 1899. Ernest Rutherford classifies two types
- f radiation, alpha rays and beta rays.
- Henri Becquerel discovers that radiation
from uranium consists of charged particles and can be deflected by magnetic fields.
SLIDE 4
Marie Curie coined the term radioactivity Radiation Activity
SLIDE 5 Marie Curie coined the term radioactivity Radiation
- Ionizing radiation
- Non-ionizing radiation
Activity
SLIDE 6 Marie Curie coined the term radioactivity Radiation
- Electromagnetic radiation
- Particle radiation
- Acoustic radiation
- Gravitational radiation
Activity
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SLIDE 10
Types of decays:
SLIDE 11 Types of decays:
- Alpha decay
- Beta decay
- Gamma decay
- Neutron emission
- Electron capture
- Proton emission
- Spontaneous fission
- Cluster decay
- Internal conversion
SLIDE 12
SLIDE 13
Negative Beta Decay Positive Beta Decay Electron Capture
SLIDE 14
Negative Beta Decay Positive Beta Decay Electron Capture
SLIDE 15
Negative Beta Decay Positive Beta Decay Electron Capture
SLIDE 16
Negative Beta Decay
Nucleus level Nucleon level Quark level
SLIDE 17
Negative Beta Decay
Nucleus level Nucleon level Quark level
SLIDE 18
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SLIDE 20
Negative Beta Decay Positive Beta Decay Electron Capture
SLIDE 21
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SLIDE 24 Marie Curie coined the term radioactivity Radiation Activity
desintergration per second
SLIDE 25
In a simple decay, if the number of decaying nucleus is N(t)
SLIDE 26
In a simple decay, if the number of decaying nucleus is N(t) In a general case, the activity is proportional to the number of decaying atoms
SLIDE 27
In a simple decay, if the number of decaying nucleus is N(t) In a general case, the activity is proportional to the number of decaying atoms
SLIDE 28
In a simple decay, if the number of decaying nucleus is N(t) In a general case, the activity is proportional to the number of decaying atoms the solution of this differential equation
Exponential Decay Law
SLIDE 29
Exponential Decay Law Decay constant λ
SLIDE 30
Exponential Decay Law Decay constant λ Half-life time T1/2
SLIDE 31
Exponential Decay Law Decay constant λ Half-life time T1/2
SLIDE 32
Exponential Decay Law Decay constant λ Half-life time T1/2
SLIDE 33
Half-life time
SLIDE 34
Half-life time
SLIDE 35
Decay chain if λ1<<λ2<<λ3 … <<λi
SLIDE 36
Decay chain if λ1<<λ2<<λ3 … <<λi
SLIDE 37
Decay chain if λ1<<λ2<<λ3 … <<λi
SLIDE 38
Decay chain if λ1<<λ2<<λ3 … <<λi
SLIDE 39
Decay chain if λ1<<λ2<<λ3 … <<λi Secular equilibrium
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sheet of paper very thick layer of lead Al shielding light elements (hydrogen)
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Stochastic vs Deterministic effects Justification Limitation ALARA Time Distance Shielding
SLIDE 44 Stochastic vs Deterministic effects Justification: no unnecessary use of radiation is
permitted, which means that the advantages must
- utweigh the disadvantages
Limitation: each individual must be protected
against risks that are too great, through the application of individual radiation dose limits
ALARA - "As Low As Reasonably Achievable" Time: Reducing the time of an exposure reduces
the effective dose proportionally
Distance: Increasing distance reduces dose due
to the inverse square law
Shielding: absorbing the energy of the radiation
SLIDE 45
Primordial Radionuclides Secondary Radionuclides Cosmogenic Radionuclides Artifical Radionuclides
SLIDE 46
Primordial Radionuclides are produced
in stellar nucleosynthesis and supernova explosions, their half-lives are so long (>100 million years)
Secondary Radionuclides derived from the
decay of primordial radionuclides
Cosmogenic Radionuclides are continually
being formed in the atmosphere due to cosmic rays.
SLIDE 47
IAEA (2013)
SLIDE 48
SLIDE 49
IAEA (2013)
SLIDE 50
IAEA (2013)
SLIDE 52 Isotope sign Name First member of decay series Mother element Half-life time
222Rn
Radon
238U 226Ra
3.8 d
220Rn
Toron
232Th 224Ra
55 s
219Rn
Aktinon
235U 223Ra
4 s
SLIDE 53
IAEA (2013)
SLIDE 54
IAEA (2013)
SLIDE 55 IAEA (2013)
Recoil ranges depending on media:
- solid 20-70 nm
- air ~60m
- liquid100 nm
SLIDE 58
International Atomic Energy Agency (2013):
Measurement and calculation of radon releases from NORM residues. ISBN 978–92–0–142610–9
Horváth, Á. et al. (2012): Environmental Physics Methods
Laboratory Pracitces
Encyclopædia Britannica
https://www.britannica.com/science/neptunium-series
J. Porstendörfer (1994): Properties and behaviour of
radon and thoron and their decay products in the air. Journal of Aerosol Science, Vol. 25, p 219-263.
Khan et al., J Phys Chem Biophys 2017, 7:3 DOI:
10.4172/2161-0398.1000254
nuclear-power.net wikipedia.org