Atomic Physics Atomic Notation A X Z X – symbol of the atom Z – atomic number (no of protons) A – mass number 14 C 6 C – carbon Z = 6 , the number of protons in the nucleus A = 14, the number or protons plus the number of neutrons in the nucleus A is also known as the nucleon number , the number of particles in the nucleus
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Atomic Physics Atomic Notation A X Z X – symbol of the atom Z – atomic number (no of protons) A – mass number 14 C 6 C – carbon Z = 6, the number of protons.
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Atomic Physics
Atomic Notation
A
X
Z
X – symbol of the atomZ – atomic number (no of protons)A – mass number
14
C
6
C – carbonZ = 6 , the number of protons in the nucleusA = 14, the number or protons plus the number of neutrons in the nucleus
A is also known as the nucleon number, the number of particles in the nucleus
Atomic Physics
Atomic Notation
56
Fe
26
Fe - ironthe number of protons = 26the number of neutrons = 30the number of electrons = 26
1.00794
H
1
H - hydrogenthe number of protons = 1the number of electrons = 1the number of neutrons = 0.00794 ??
Atomic Physics
Isotopes
Isotopes are variations of the same elements. Their nuclei contain the same number of protons but a different number of neutrons
12
C
6
13
C
6
14
C
6
Isotopes of carbon
Atomic Physics
Nuclear Reactions
4 Al + 3 O2 2 Al203
Al3+ loses 3 electronsO2- gains 2 electrons
In a chemical reaction it is the movement of electrons that brings about the formation of compounds
Atomic Physics
Nuclear Reactions
2
H +
1
3
H
1
4
He +
2
1
n
0
+ energy
A nuclear reaction involves nuclei only. Electrons don’t play a significant part
Atomic Physics
Atomic Notation
+ energy
Two small nuclei have collided to form a larger nuclei plus a neutron with the release of energy (fusion)
Atomic Physics
Radioactivity:
238
U +
1
n144
Ba 92
Kr
31
n + + 92 0 56 36 0
A large nuclei is broken up into 2 smaller nuclei with the release of energy (fission)
Before AfterNo of protons Nucleon number
This demonstrates two conservation laws:1. Conservation of charge: No. of protons before = no. protons
afterwards2. Conservation of nucleon number: total number of protons and
neutrons stays the same
Atomic Physics
Example
235
U +
1
na
Xe 94
Sr
21
n + + 92 0 54 b 0
Find the values of a and b.
Atomic Physics
Examples:
226
Ra222
Rn 4
He1. + 88 86 2
Radium 226 Radon 222 + α particle
Radium Radonα -
particleprotons 88 86 2
neutrons 138 136 2
The radium nucleus emits an α particle (a helium nucleus) and changes into a radon nucleus.
Atomic Physics
14
C14
N 0
e2. + 6 7 -1
Carbon 14 Nitrogen 14 + β particle
Carbon Nitrogenβ -
particleprotons 6 7 0
neutrons 8 7 01
n1
p 0
e + 0 1 -1
A carbon nucleus emits an electron as a neutron is converted into a proton
Atomic Physics
60
Co60
Ni * 0
e3. + 27 28 -1
60
Ni*60
Ni
γ + 28 28
60
Ni* is a Ni nucleus in an excited state. It returns to ground state by emitting a photon
28
Atomic Physics
Radioactivity: The spontaneous and random emission of particles from the nucleus of an atom.
There are 3 types
α 2 protons and 2 neutronsβ 1 electronγ photon
217
At213
Bi
?1. +
85 83
234
Pa234
Bi
?2. +
91 92
Atomic Physics
In a nuclear reactor, is broken
down by a chain of α and β particles
238
U234
Th 92 90
α particle
238
U92
Atomic Physics
234
Th234
Pa 90 91
β particle
Atomic Physics
234
Pa234
U 91 92
β particle
Atomic Physics
234
U230
Th 92 90
α particle
Atomic Physics
230
Th226
Ra 90 88
α particle
Atomic Physics
226
Ra222
Rn 88 86
α particle
Atomic Physics
218
Po 84
then loses an α particle, then β, α, β, β, β then α
What does it end up as?
206
Pb 82
Atomic Physics
Deflection by a Magnetic Field
α – particle deflected slightly because it has the greatest mass
β – particle deflected more because it has less mass and in the opposite direction as it has the opposite charge
γ – radiation, no deflection because it has no charge and no mass
Atomic Physics
The radio active source is not a health risk as α – particles can travel only a short distance in air. As they are placed on the ceiling, they are well away from people.
Smoke Detector
The radioactive source emits α – particles that ionise the air, ie, they remove electrons forming positive and negative ions. This allows the current to flow. Smoke particles absorb the α – particles so the ionisation stops. The current stops that triggers the alarm
Atomic Physics
Calculating the Energy Released in a Nuclear Reaction
2
H +
1
3
H
1
4
He +
2
1
n
0
+ energy
The amount of energy released is given by the formulaE = mc2
Where mass is the mass that has been “lost”, and c is the speed of light, 3.00 x 108 ms-1
The mass of the nucleus of:Deuterium is 3.34330 x 10-27 kgTritium is 5.00784 x 10-27 kgHelium is 6.64591 x 10-27 kgA neutron has a mass of 1.67483 x 10-27 kgFind the energy released in this reaction
Deuterium 3.3433 x 10-27 Helium 6.64591 x 10-27
Tritium 5.00784 x 10-27 Neutron 1.67483 x 10-27
Total 8.35114 x 10-27 Total 8.32074 x 10-27
8.35114 x 10-27
8.32074 x 10-27
Difference 0.0304 x 10-27
Atomic Physics
Energy released = 0.0304 x 10-27 kg x (3.00 x 108 ms-1)2
= 2.736 x 10-12 J
Atomic Physics
+ β particle228
Ra228
Ac 88 89
The mass of the Radon nucleus is 3.81743 x 10-27 kgThe mass of the Actium nucleus is 3.68334 x 10-27 kgThe mass of a β particle is 0.00091 x 10-27 kg