nuclear physics & radioactivity physics - unit one
TRANSCRIPT
NUCLEAR PHYSICS & RADIOACTIVITY
PHYSICS - UNIT ONE
ATOMIC STRUCTUREAtoms consist of:
Nucleus - The solid centre of the atom, containing protons and neutrons.
- Most of the mass of an atom is in the nucleus.
- The collective name for all particles found
in the nucleus is nucleons.
Protons are positively charged, with relative charge +1.
Neutrons are neutral and have no charge.
ATOMIC STRUCTUREAtoms consist of:
Electrons - Negatively charged particles, with relative charge of -1
- Found around the nucleus of an atom in ‘shells’ or ‘clouds’.
- These shells are arranged in energy levels – so the innermost
shell has the lowest energy level and is filled first.
ATOMIC STRUCTURE
The amount of protons, neutrons, electrons in an atom are represented as:
𝑋𝑍𝐴
Mass Number –The total number of
nucleons in the nucleus
(Neutrons + Protons)
Atomic Number –The total number of
protons in the nucleus
Chemical Symbol for the
element
The number of electrons in an
atom is equal to the number of
protons
ATOMIC STRUCTURE
𝐿𝑖36
𝐶612
𝑋𝑍𝐴
Mass Number –The total number of
nucleons in the nucleus
(Neutrons + Protons)
Atomic Number –The total number of
protons in the nucleus
Chemical Symbol for the
element
ISOTOPES
An atoms name is based on how many protons it has.
Not all atoms of the same name have the
same number of neutrons.
We call atoms with variations in number of
neutrons, isotopes of that element.
The isotopes therefore have the same Atomic Number
(number of protons), but different mass numbers.
ATOMIC STRUCTURE - QUESTIONS1. How many protons and neutrons are in the following atoms?
2. For the following elements, represent them in the form
a) 2 neutrons and 2 protons
b) 7 protons and 13 Nucleons
c) 91 Protons and 143 Neutrons
3. Explain why it is possible to have 2 atoms of different element with the
same number of nucleons
TYPES OF NUCLEAR RADIATION
Unstable isotopes can emit various types of radiation while striving to
become stable. The radiation that is emitted is ionising radiation, which
has the ability to knock electrons from atoms they come into contact with.
The 3 naturally occurring forms of nuclear radiation are:
Alpha Radiation α
Beta Radiation β
Gamma Radiation γ
ALPHA DECAY
An unstable nucleus ejects a relatively large particle known as an
α particle.
The α particle consists of 2 protons and 2 neutrons (a Helium
nucleus).
The remaining daughter nucleus is more stable & is now a
different element.
ALPHA DECAY
𝑈92238 → h𝑇90
234 + 𝐻𝑒24 +𝑒𝑛𝑒𝑟𝑔𝑦
𝑈92238 → h𝑇90
234 +𝛼+𝑒𝑛𝑒𝑟𝑔𝑦Or can be
written as…
BETA DECAY
Two types - β+ (produced under laboratory conditions only )
- β- (occurs naturally)
β- particle is a fast moving electron that is ejected from an unstable
nucleus.
In fact it’s true! The outer shell electrons don’t change, instead
other interesting changes take place in the nucleus……
Wait! An electron emitted from the
nucleus??? Nuclei doesn’t
contain electrons!
BETA DECAY One neutron transforms into a proton and an electron. The proton remains in the nucleus, the electron is emitted and is
called the β- particle.
The resulting daughter nucleus has the same number of nucleons as the parent, but one less neutron and one more proton.
𝑛01 → 𝑝1
1 + 𝑒− 10
h𝑇90234 → 𝑃𝑎91
234 + 𝑒−10 +𝑒𝑛𝑒𝑟𝑔𝑦
h𝑇90234 → 𝑃𝑎91
234 +𝛽−+𝑒𝑛𝑒𝑟𝑔𝑦Or can be
written
as…
GAMMA DECAY The nucleus is unstable after α or β decay and may need to
release energy.
Gamma emission occurs after another form of nuclear decay has
taken place, when the nucleus is ‘excited’.
A small packet of excess electromagnetic energy called a gamma
ray is emitted.
No mass, No charge, Travels at the speed of light.𝐵𝑖∗83
210 → 𝐵𝑖83210 +𝛾
PENETRATION POWERThe various forms of nuclear radiation are so different, so they of course react differently when coming into contact with matter after being ejected from the nucleus. They can each be absorbed by:α particles - a few centimetres of air
- a piece of paper
- a layer of dead skinβ particles - about 100 centimetres of air
- a few centimetres of Aluminiumγ rays - barely affected by air
- absorbed in many centimetres of Lead
IONISING POWER
An ion is an atom with an overall positive or negative charge.
Positive ions form when electrons are removed from a neutral atom.
Negative ions form when electrons are added to a neutral atom.
Alpha, Beta & Gamma radiation have the ability to ionise atoms they come into contact with.
IONISING POWER
α particles - Are slow-moving particles
- They have time to interact with most atoms in their path
- When they interact with an atom the α particles positive charge
attracts electrons from the atoms
- These atoms are ionised – they are no longer neutral
- With each ionisation, the α particle slows down and lose energy
- Poor penetrating power
- High ionising power
IONISING POWER
β- particles - Are repelled by the electrons in atoms
- The repulsion causes the β- particles to bounce between atoms.
- The collisions may cause some electrons to be ejected from the atom, ionising the atom
- Each β collision loses less energy than α collisions, so β particles have higher penetrating ability than α particles but less ionising power.
IONISING POWER
γ rays - May interact with electrons or nuclei they collide with as
they move through a substance.
- As γ rays have no charge, collisions are infrequent.
- Collisions occur only when a nucleus or electron is directly in the path of the γ ray (unlikely due to the large amount of empty space in an atom).
- Very low ionising power.
- Very high penetrating power.
HALF-LIFE
A half-life is the time taken for half a group of unstable nuclei to decay.
It’s impossible to know exactly when an unstable atom will decay.
We can however predict how many will decay in a period of time.
Half-lives vary according to the isotope that is decaying – these can range from microseconds, to thousands of millions of years.
HALF-LIFE
We will look at these in
greater detail later
in the course
HALF-LIFE
1st Half life –the time it takes for 50% of the nuclei to
decay
2nd Half life –the time it takes for
50% of the remaining nuclei to
decay
3rd Half life –the time it takes for
50% of the remaining nuclei to
decay4th Half life –
the time it takes for 50% of the
remaining nuclei to decay
The Half-life of an atom can be represented on a graph, known as a decay curve.
HALF-LIFE
The Half-life of an atom can be represented on a graph, known as a decay curve.
X
The y-axis shows the number of Californium-
252 atoms as a percentage
~2.645 yrs
To find the half-life, find 50% on the y-axis, ruling a line to the plot and match this up to the corresponding value
on the x-axis
HALF-LIFE
The Half-life of an atom can be represented on a graph, known as a decay curve.X
This tells us that the half-life of Californium-
252 is approx. 2.65 years
2.65
The second half-life (when only 25% remain un-
decayed – ie. Half of the remaining 50%) in this case, occurs in another
2.65 years, at approximately 5.3 years.
X
5.33
HALF-LIFE
X
2.65
The third half-life (when only 12.5% remain un-
decayed – ie. Half of the remaining 25%) in this case, occurs in another 2.65 years, at approximately
7.95 years.
X
5.33
7.95
X
The fourth half-life (when only 6.25% remain un-
decayed – ie. Half of the remaining 12.5%)
in this case, occurs in another 2.65 years, at approximately
10.6 years.
When does the fourth half-life occur?
X10.6
HALF-LIFE
HALF-LIFE
Use the decay curve to find:a) The Half-life of Uranium-235
b)The Second Half-life of Uranium-235
c) What fraction of the isotope will remain after 2840 million years?
d) What fraction of the isotope will remain after 4260 million years?
HALF-LIFE
Use the decay curve to find:a) The Half-life of Uranium-235
b)The Second Half-life of Uranium-235
c) What fraction of the isotope will remain after 2840 million years?
d) What fraction of the isotope will remain after 4260 million years?
710 million years
1420 million years
6.25%
1.5625%
NOW DO
HALF-LIFE ~ SIMULATION TASK
CHAPTER ONE - Q 17; 23-26
NOW TRY
HALF-LIFE
A half-life is the time taken for half a group of unstable nuclei to decay.
It’s impossible to know exactly when an unstable atom will decay.
We can however predict how many will decay in a period of time.
Half-lives vary according to the isotope that is decaying – these can range from microseconds, to thousands of millions of years.
HALF-LIFE
HALF-LIFE
1st Half life –the time it takes for 50% of the nuclei to
decay
2nd Half life –the time it takes for
50% of the remaining nuclei to
decay
3rd Half life –the time it takes for
50% of the remaining nuclei to
decay4th Half life –
the time it takes for 50% of the
remaining nuclei to decay
The Half-life of an atom can be represented on a graph, known as a decay curve.
HALF-LIFE
The Half-life of an atom can be represented on a graph, known as a decay curve.
X
The y-axis shows the number of Californium-
252 atoms as a percentage
~2.645 yrs
To find the half-life, find 50% on the y-axis, ruling a line to the plot and match this up to the corresponding value
on the x-axis
HALF-LIFE
The Half-life of an atom can be represented on a graph, known as a decay curve.X
This tells us that the half-life of Californium-
252 is approx. 2.65 years
2.65
The second half-life (when only 25% remain un-
decayed – ie. Half of the remaining 50%) in this case, occurs in another
2.65 years, at approximately 5.3 years.
X
5.33
HALF-LIFE
X
2.65
The third half-life (when only 12.5% remain un-
decayed – ie. Half of the remaining 25%) in this case, occurs in another 2.65 years, at approximately
7.95 years.
X
5.33
7.95
X
The fourth half-life (when only 6.25% remain un-
decayed – ie. Half of the remaining 12.5%)
in this case, occurs in another 2.65 years, at approximately
10.6 years.
When does the fourth half-life occur?
X10.6
HALF-LIFE
HALF-LIFE
Use the decay curve to find:a) The Half-life of Uranium-235
b)The Second Half-life of Uranium-235
c) What fraction of the isotope will remain after 2840 million years?
d) What fraction of the isotope will remain after 4260 million years?
HALF-LIFE
Use the decay curve to find:a) The Half-life of Uranium-235
b)The Second Half-life of Uranium-235
c) What fraction of the isotope will remain after 2840 million years?
d) What fraction of the isotope will remain after 4260 million years?
710 million years
1420 million years
6.25%
1.5625%
NOW DO
HALF-LIFE ~ SIMULATION TASK
CHAPTER ONE - Q 17; 23-29
NOW TRY
MEASURING DECAY
We can measure the ionising radiation of a
radioactive source using a Geiger counter.
• A Geiger counter detects Alpha, Beta and Gamma radiation.
• The common unit for measuring radioactive decay is Becquerel (Bq).
• Bq = number of decay’s per second.
http://atomic.lindahall.org/what-is-a-geiger-counter.html
MEASURING DECAY
Refer to the graph below, showing the decay curve of Thorium-234.
At the beginning when the decay is at large, the Geiger counter would of course be the most active, recording a
high count rate
Gradually decreasing over
time
So, if we measured the decay of a radioactive source as graphed it, it would be the same as
the decay curve
MEASURING DECAY
eg. A radioactive material is measured to have 600,000 decays per
second.
a) What is this equivalent to in Bq?
b) After 3 half-lives, what will the activity be in Bq?
600,000 Bq
One Half-life
Bq
Two Half-lifes
Bq
Three Half-lifes
Bq
RADIOACTIVE SERIES
We have been studying the decay (α, β, γ) of radioactive isotopes and
writing equations to represent the decay.
eg. α decay
The resulting daughter nucleus in this case is still not stable and as such
is still radioactive and will undergo additional decay in it’s pursuit to
reach stability.
The sequence of radioisotopes along this journey is called a decay chain. (Or decay series). Note: Not all radioactive isotopes go through a series of decay’s.
+
RADIOACTIVE SERIES
We can represent the decay graphically.
eg. α decay +
RADIOACTIVE SERIES
What happens to the daughter ?
β decay:
+
RADIOACTIVE SERIES
Lets look at what happens next...
β decay:
β decay:
α decay:
α decay:
α decay:
+
RADIOACTIVE SERIES
Which continues to decay to become Lead-206
RADIOACTIVE SERIES
Now you try:
For the radioisotope
• Write a series of equations to show it undergo the series of
decay: β, α, α, β.
• Represent the transformations using a Radioactive Series
graph
EFFECTS OF RADIATIONIONISING RADIATION
As covered previously, Alpha, Beta and Gamma radiation are Ionising
Radiation – high energy radiation that has the ability to change atom by
removing electrons and therefore giving the atom an overall charge (ions).
Overall positive charge - more protons than electrons. Can be represented as ,
Overall negative charge - more electrons than protons. Can be represented as
Recall – List the 3 types of decay in order of their ionising power……
Alpha, Beta, Gamma Do you remember why??
X-Rays are also a form of Ionising Radiation
EFFECTS OF RADIATIONNON-IONISING RADIATION
Other forms of electromagnetic
radiation, such as Radiowaves,
Microwaves & visible light,
have lower energies and don’t
interact with matter the same
way. These are Non-ionising
Radiation.
EFFECTS OF RADIATION
Sometimes when the electron that is knocked from the atom is part of a bond between one atom and another.
This causes the bond to be broken – this may result in a molecule being split in two. The two pieces have an overall charge and are known at free radicals.
Both ions and free radicals are very reactive – this may result in new chemical reactions taking place inside the substance that was exposed to the ionising radiation.
EFFECTS OF RADIATION
Video: The effects of radiation on our health
Source https://www.youtube.com/watch?v=tq6FDyFeCN0
more – textbook page 16
HOW MUCH RADIATION IS TOO MUCH?
Video: The most radioactive places on earth
Source https://www.youtube.com/watch?v=TRL7o2kPqw0
HOW MUCH RADIATION IS TOO MUCH?
The answer to this depends on many factors including:
• The type of radiation
• The part of the body exposed to the radiation
• The general health of the individual
ABSORBED DOSE
The amount of radiation received is called the Absorbed Dose.
This is the amount of energy absorbed by each kilogram of the tissue being exposed.
Absorbed Dose =
Units: Energy (Joules), Mass (kg), Absorbed Dose (Gray (Gy))
1 Gy = 1 joule per kilogram
ABSORBED DOSE
Absorbed Dose =
Example One: A 60kg person absorbs 0.06 Joules of energy due to ionising radiation.
Calculate the Absorbed Dose.
Absorbed Dose =
=
= 0.001 or Gy
ABSORBED DOSE
Unfortunately, the number of grays absorbed by a person does not provide much information about the extent of the damage to that person. We need to take into account the penetrating power of the type of radiation too. Why???
Alpha Particles are stopped in a short distance, passing on all energy in a short space. This causes much localised damage.Beta Particles are more penetrating, so the damage is less severe in any one area but is more widespread.Gamma rays (and X-rays) are far more penetrating than either α or β particles. They spread their energy over a large range.
DOSE EQUIVALENT
Units: Dose Equivalent (Sv), Absorbed Dose (Gy), Quality Factor (No units)
As this new equation takes into account the type of radiation, we can now make a true measure for comparision of the biological damage caused by
the radiation exposure.
DOSE EQUIVALENT
Source: From page 17 in your text book
DOSE EQUIVALENT
Eg1 (from before) : A 60kg person absorbs 0.06 Joules of energy due to ionising radiation.
Now calculate the Dose equivalent if the energy was delivered by Gamma Rays.
Absorbed Dose =
=
= 0.001 or Gy = 1 mGy
= 0.001 x 1= 0.001 Sv = 1 mSv
DOSE EQUIVALENT
Eg 2: An 80kg person absorbs 20 mJ of energy due to ionising radiation.
a) Calculate the Absorbed Dose.
b) Calculate the Dose equivalent if the energy was delivered by Alpha Particles (QF 20).
Absorbed Dose =
=
= 0.00025 or Gy = 250 Gy
= 0.00025 x 20= 0.005 Sv = 5 mSv
CHAPTER ONE - Q 30-43NOW TRY