


1. In 1896, Henri
Becquerel discovered that a photographic plate was darkened in the presence
of Uranium.
Marie and Pierre Curie isolated two radioactive substances, Polonium
and Radium.
In 1897, Thomson discovered that the atom was a ball of positive charge
filled with moving negatively charged electrons. This was termed the Plum
pudding model.
In 1899, Rutherford discovered that a Uranium compounds produced three
different kinds of radiation.
In 1911, Rutherford forwarded the idea of the atom being a dense positive
nucleus in the middle of the atom, with electrons moving around it. Most
of the mass resided in the nucleus. Also proposed that the nucleus consisted
of positively charged protons as well as negatively charged electrons.
In 1932, Chadwick proposed the presence of neutrons and that a nucleus
is made up of neutral neutrons and positively charged protons. Neutrons
are particles found in the nucleus that are electrically neutral and that
have a mass almost identical to the proton.
Bohr proposed that the atom had negatively charged electrons that were
orbiting the nucleus.
At a later time, the Quantum Mechanical Model was introduced. In this
model, the structure of the whole atom is described entirely by mathematical
equations.
In 1934, Enrico Fermi and Emilio Segré bombarded Uranium with
neutrons, producing new radioactive isotopes.
In 1939, German scientists Otto Hahn and Fritz Strassmann found that
Barium was produced by bombarding Uranium with neutrons. Lisa Meitner and
Otto Frisch proposed that the neutrons caused the uranium to divide into
two smaller nuclei, accompanied by a tremendous release of energy.
Physics Study Guide
pg 72
Physics Text Book pg
149
2. Atomic Number: The
number of protons in a nucleus (designated by the letter Z).
Atomic Mass Number: The total number of protons and neutrons (designated
by the letter A).
Stawa Set 15
Physics Study Guide
pg 73
Physics Text Book pg
151
3. Isotope: An isotope
is an atom that contain the same number of protons but a different numbers
of neutrons in the nucleus. The mass number changes but the atomic number
stays constant.



4. An atomic mass unit
is approximately 1.6606*10^-27 kg or approximately 1/12 the mass of a carbon-12
atom.
Stawa set 16
Physics Study Guide
pg 73
5. Protons and Neutrons
are held together by an attractive force termed the strong nuclear force.
This force is greater then the repulsion force that is present between
the positively charged protons. Since the strong nuclear force only acts
over a small distance, the very large distant nucleons are unable to attract
each other strongly enough thus fall apart as the protons repel.
The nuclei with Z=40 tend to be stable nuclei as they tend to have
equal numbers of protons and neutrons. For nuclei with Z greater
than 40, these are stable as they have more neutrons than protons. There
are no stable nuclei with Z greater than 82. They are all radioactive.
Due to their size, no number of neutrons can overcome the electric repulsion
between protons.
Physics Study Guide
pg 75-76
Physics Text Book pg
153
Physics Text Book pg
158-159
6. Alpha Particle: It
is essentially a helium nucleus. It contains two protons and two neutrons.
It has a charge of +2 and a mass of A=4. Alpha particles are positively
charged thus move towards the cathode when a potential difference is present.
When a nuclei decays by emitting an alpha particle, the number of protons
is reduced by two and its mass is reduced by four. Alpha particles are
emitted by very large nuclei where the strong nuclear force is insufficient
to hold the nuclei together. It is abbreviated to (a) or 4/2 He. Alpha
radiation is the least penetrating of the radiation types. It can be stopped
(or absorbed) by a few centimeters of air or just a sheet of paper. It
is a fairly large particle, which is one reason why alpha particles do
not penetrate things very well but are very good ionisers. These particles
have an emission velocity up to 10% the speed of light.
Beta Particle: Beta particles are a negatively charge electron emitted
by the nucleus. It is not an orbital electron, but one created in the nucleus
by the decay of a neutron into a proton and an electron. The electron then
shoots out at a high speed of about 30-90% the speed of light. It has a
charge of -1 and essentially has no mass. Since Beta particles are negatively
charged thus move towards the anode when a potential difference is present.
Weak nuclear forces are involved in the production of a beta particle in
the nucleus as Beta particles are emitted by nuclei that have too many
neutrons relative to the number of protons. It is abbreviated (B) or 0/-1
e. Beta radiation can penetrate air and paper but can be stopped by a thin
sheet of metal.
Gamma Radiation: Gamma radiation is composed of high-energy photons.
It is emitted by excited state nuclei. Gamma radiation has no charge and
no mass. It is abbreviated by (Y). Gamma radiation can penetrate air, paper
or thin metal. It can only be stopped by many centimeters of lead or by
many meters of concrete. Gamma radiation is uncharged so is unaffected
by electric fields. When a radioactive atom gives off gamma radiation it
will be emitted with a velocity of the speed of light. This is like other
types of electromagnetic radiation such as light and radio waves, which
can travel long distances.
| Property | Alpha Particle | Beta Particle | Gamma Particle |
| Description | Helium nucleus | High speed electron | High energy photon |
| Symbol | 4
He 2 |
0
e -1 |
0
y 0 |
| Charge | +2 | -1 | Neutral |
| Mass | 4u | 0.00055u | Nil |
| Emission Velocity | 10% speed of light | 30-90% speed of light | The speed of light |
| Penetration | Few cm air | 12 mm foil | 10 cm of lead or concrete |
| Ionizing Potential | Strong | Moderate | Little |
7. The strength
of a radioactive source is determined by the number of disintegrations
of its radioactivity per second. The unit for this is the becquerel (Bq).
One disintegration per second is equal to one Becquerel. This is a very
low rate and it is common for radioactive sources to be quoted in kilobecquerels
(kBq), megabecquerels (MBq) or gigabecquerels (GBq). The becquerel replaces
the curie. There are 37 thousand million becquerels in a curie.
Radioactivity dispersed in another material may be expressed as, megabecquerels
per kilogram for natural radioactivity of some rocks, or as becquerels
per cubic metre when describing the radioactive content of air. These units
do not describe your radiation dose but represent the strength of radioactivity
at a given place.
The measure of absorbed radiation dose is the gray (Gy) and it replaces the old unit, the Rad. The absorbed dosage is the energy absorbed per kilogram of tissue and calculated using the formula Absorbed Dose = Energy Absorbed/Mass of absorbing tissue.
However, while the energy delivered by different particles may be the
same, the effect on living cells can be quite different. Alpha particles
and neutrons are approximately ten times as damaging as beta particles
and gamma rays for the same amount of energy deposited. The dose equivalent,
the Sievert (Sv), is the important unit to assess the effects of ionizing
radiation on living cells, especially human beings. It does not measure
the same thing as the gray. The Sievert replaces the old unit, the Rem,
(the roentgen equivalent for man). Therefore One Sievert will have the
same effect no matter what type of radiation.
Dose Equivalent = Absorbed Dose * Quality Factor
Stawa Sets 17+18
Physics Study Guide
pg 77-78
Physics Text Book pg
170-172
8. In all radioactive
decay, the classical conservation laws hold. Energy, linear momentum, angular
momentum, and electric charge are conserved. Also, the nucleon number is
conserved. When balancing a nuclear reaction, mass and charge are conserved.
When a nucleus decays, it becomes the nucleus of another atom.
Original Nucleus = Parent Nucleus
Resultant Nucleus = Daughter Nucleus
Daughter Nucleus + emitted particle = decay produced
Stawa Set 15
Physics Study Guide
pg 74
Physics Text Book pg
162-163
9. The activity is proportional
to the number of nuclei not yet decayed.
Physics Text Book pg
166
10. Half-life (T1/2):
The time it takes for half the original amount of the substance to decay.
It is also the time it takes for the number of atoms you start with
to halve. If you were measuring the radioactivity with a Geiger Muller
detector, the count rate (e.g. the number of counts per second) would halve
in this time. The greater the time it takes for the number of decays to
halve, the greater its stability as its activity is low.
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11. Radioactive Decay
is a random process as you are unable to predict which actual nuclei will
decay next but rather you know only how many nuclei will decay in a period
of time.
Physics Study Guide
pg 78
Physics Text Book pg
165
12.
Calculate the half-life of this isotope from the graph
Model Answer. It is always better to give as much detail in your answer
as possible. Show your working For example: The start reading is 80 counts
Half this reading is 40 counts
It takes 6 days to reach 40 counts.
Stawa Set 17
Physics Study Guide
pg 79
Physics Text Book pg
165
13.
L=O/2^N where L = Left O = Original N = Number of Half-lives
N=T/H where N = Number of Half-lives T = Time H = Length of Half-life
Stawa Sets 17+18
Physics Study Guide
pg 79
Physics Text Book pg
169
14. Uses of radioactivity
1. Radioactive materials are used to measure the thickness of films
in, for example, a canning factory.
2. In hospitals they use radioactive materials to see what is happening
inside the body - they call these tracers.
3. Radioactive materials are used in smoke detectors and to check welds
in pipes.
4. Because they kill cells radioactive materials are used to kill germs.
We use them to irradiate food and to irradiate cancer cells.
5. Radioactive dating Radioactivity can also be used to work out how
old something is. When an unstable nucleus splits up (disintegrates) it
emits radiation and turns into a different atom. As something radioactive
gets older, it emits less radiation. Scientists measure radioactivity to
check the age of fossils and rocks -they call this radioactive dating.
6. Nuclear Bombs: the splitting of nucleons thus releasing energy.
Radioactive materials are used in different ways for different purposes.
For example, if it has a short half-life the radioactivity decays quickly.
This is good for when you use one as a body tracer, but bad when you use
one in a smoke alarm where you would have to keep changing it.
Similarly, the radioactive material needs to give off useful radiation.
For example: Gamma radiation is less useful for testing aluminum film
because it goes through the film with little change.
For a body tracer gamma radiation is safer and can be detected easily.
Physics Study Guide pg
81-84
Physics Text Book pg
167
Physics Text Book pg
174-176
Physics Text Book pg
184-189
15. Mass Defect: The
difference in the mass of a nucleus and the sum of the masses of its constituent
particles.
Nuclear Binding Energy: The amount of energy that must be put into
a nucleus to break it into its constituent particles. We can also look
at a nucleus in terms of the forces that hold it together. The electric
force described by Coulomb predicts that the nucleus should fly apart (since
positive charges repel other positive charges). Another short-range attractive
force must be acting within the nucleus.
Stawa Set 16
Physics Study Guide
pg 88-89
Physics Text Book pg
167
16. In the equation E
= mc^2
E stands for energy and m is mass. The letter c is the speed of light
(from the Latin word for speed, celeritas), which is 300,000,000 meters
per second. No one had thought of mass as a form of energy before. This
equation meant that it was possible for mass to be converted into energy.
People soon noticed that this is what was happening in nuclear reactions.
If you take the mass of a Uranium atom, and compare it with the masses
of the atoms and other particles that come out of a nuclear fission reaction
(when the Uranium nucleus breaks apart), you find that a little bit of
mass is missing. Einstein's law explains that the mass has become energy
- the kinetic energy (energy of movement) of the new particles speeding
away from the explosion. And because the speed of light is so high, a little
mass becomes a lot of energy. This energy becomes heat that can be used
in nuclear reactors to make electricity. One of the conclusions which Einstein
reached while working on his theory of relativity is that mass and energy
are different forms of the same entity. Since they are different
forms, you should be able to convert an amount of energy into an amount
of mass and vice versa. The equation which gives the correct conversion
is E = mc^2 which says that if you have a mass m, it is equivalent to c^2
time m amount of energy. Since c is the speed of light, you can see
that the amount of energy available from a small amount of mass is huge.
c^2 = (3 x 10^8)^2 = 9 x 10^16.
In theory, one kg of mass can be converted into 9 x 10^16 joules of
energy!
Einstein's equation is e = mc^2? Seriously, though, if you look at the
units in the equation, you will see that energy = mass * (distance/time)^2
= mass * (distance/time^2) * distance
= force * distance
which is one of the definitions of 'energy'.
Stawa Set 15
Physics Study Guide
pg 89
Physics Text Book pg
180-181
Physics Text Book pg
183
17. Fission: A division
of a nucleus into two or more smaller daughter nuclei.

eg. If the mass of a Uranium atom is 50 gm, and the masses of the atoms
and other particles that come out of a nuclear fission reaction (when the
Uranium nucleus breaks apart) is 45 gm, you find that a little bit of mass
is missing. Einstein's law explains that the mass has become energy.
Physics Study Guide pg
90
Physics Study Guide
pg 93
Physics Text Book pg
178-183
18. Chain Reaction: Neutrons
produced by the fission of one nucleus induces the fission of other nuclei.
The critical mass refers to the mass of fissile material required to sustain
un uncontrolled chain reaction such as the one that occurs in a bomb. When
an atom bomb is detonated, two separated masses of fissile material, each
less then critical mass, are forced together by a chemical explosive. The
two combined masses are then greater than the critical mass and an explosion
results.
Physics Study Guide
pg 91
Physics Text Book pg
185-186
19. The reaction
produces heat which is transferred to the water which is acting as a moderator
and coolant. This hot liquid is transported to the condenser where it turns
water into steam. The steam is ran through a turbine that is connected
to a generator. This is connected to wired which is connected to houses.

| Component | Material | Function |
| Fuel | Uranium-235 or Uranium Dioxide | Pprovides energy for the fission reaction to occur. |
| Moderator | Graphite or Heavy water | It slows down the neutrons to facilitate the fission process. |
| Control rods | Cadmium Steel | Absorbs neutrons to prevent uncontrolled chain reactions. |
| Coolant | Water, Liquid Sodium | Removes heat to prevent meltage. |
| Shield | Reinforced concrete or lead | Protects the workers and others from radioactive leakage. |
20. Some radiation comes
from rocks so expect to find it in the ground and the building materials
that make our houses. As a result the soil, the plants and our food can
be slightly radioactive too.
Some rocks actually give off radioactive Radon gas. All around us,
radiation called cosmic rays (cosmic means 'universal') reaches us from
space.
There's little we can do about natural radiation - but man has added
to it. We meet Ray machines when we travel by air, or have a chest X-Ray
in hospital. This exposes us to extra radiation. Man has also exploded
radioactive nuclear weapons and made nuclear power stations which add radiation
to the world.

21. When radiation collides
with neutral atoms or molecules they may become charged ions (ionized).
When this happens to molecules in living cells it can cause damage to the
genes called a mutation. This can make cells turn into cancer cells. The
cells go out of control, divide rapidly and cause serious problems. The
larger the dose of radiation a cell gets, the more chance the cell will
turn into a cancer cell. But, if the dose of radiation is very high it
can kill the cell completely. We use this idea to kill cancer cells.
Dangers of radiation (higher)
Different types of radioactivity present us with different dangers.
Beta and gamma radiation are the most dangerous because they can penetrate
our skin and damage the cells inside us.
Alpha radiation is less dangerous because it is unlikely to reach living
cells inside us.
But if we get radiation inside us - either by accident or because of
a hospital test - the story is very different. When it's inside us, alpha
radiation is the most dangerous because it is easily absorbed by cells.
Beta and gamma radiation are less dangerous because they are more likely
to pass right through a cell than to be absorbed.
The Dangers of Radiation:
| Type of radiation | Inside the body | Outside the body |
| Alpha | Most dangerous | Least dangerous |
| Beta | Less dangerous | More Dangerous |
| Gamma | Least dangerous | Most dangerous - although it's likely to pass straight through you. |
| Dosage | Effects |
| 0.25 Sv | Reduction in white blood cells |
| 1 Sv | Possible vomiting, Nausea |
| 4 Sv | Vomiting, diarrhea, drop in blood cell count, about 50 of exposed victims die within weeks from failure of blood forming organs |
| 5 Sv | Loss of hair, 50% die |
| 6 Sv | Damage to stomach and intestine walls with loss of fluids, immediate radiation sickness, bloody diarrhea, extreme thirst, death within 3 weeks |
| 10 Sv | Severe damage to central nervous system, death within days. |
Stawa set 18
Physics Study Guide
pg 85-87
Physics Text Book pg
170-174
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Created : 28 October 2000
Last modified : 26 November 2000
Author : Chad
Silver email:Chaddysi@start.com.au
Site maintained by : Chad
Silver
Copyright © MY ENTERPRISE,
PERTH, 2000.
URL : http://www.chaddysi.8m.com/nuclear/nuclear.htm