physics 12 mr. jean may 23 rd, 2014 the plan: video clip of the day radio activity decay models half...
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Physics 12
Mr. JeanMay 23rd, 2014
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The plan:
• Video clip of the day• Radio Activity• Decay models• Half Life modeling• Text book questions• Visiting the Relatives
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RadioactivityAs the heavier atoms become more unstable, particles and photons are emitted from the nucleus and it is said to be radioactive. All elements with A > 82 are radioactive.
As the heavier atoms become more unstable, particles and photons are emitted from the nucleus and it is said to be radioactive. All elements with A > 82 are radioactive. Examples
are:Alpha particles a b- particles
(electrons)b+ particles (positrons)
Gamma rays g
b-
g
b+
a
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The Alpha Particle
An alpha particle a is the nucleus of a helium atom consisting of two protons and two neutrons tightly bound.
Charge = +2e- = 3.2 x 10-
19 C Mass = 4.001506 u
Relatively low speeds ( 0.1c ) Not very penetrating
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The Beta-minus Particle
A beta-minus particle b- is simply an electron that has been expelled from the nucleus.
Charge = e- = -1.6 x 10-19 C-
High speeds (near c)-
Mass = 0.00055 u-
Very penetrating-
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The Positron
A beta positive particle b+ is essentially an electron with positive charge. The mass and speeds are similar.
Charge = +e- = 1.6 x 10-19 C
+
High speeds (near c)+
Mass = 0.00055 u+
Very penetrating+
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The Gamma Photon
A gamma ray g has very high electromagnetic radiation carrying energy away from the nucleus.
Charge = Zero (0)
g
Mass = zero (0)g
Speed = c (3 x 108 m/s)g
Most penetrating radiation
g
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Radioactive DecayAs discussed, when the ratio of N/Z gets very large, the nucleus becomes unstable and often particles and/or photons are emitted.Alpha decay results in the loss of two protons and two neutrons from the nucleus.
42
4 42 2
A AZ ZX Y energy
X is parent atom and Y is daughter atomThe energy is carried away
primarily by the K.E. of the alpha particle.
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Example: Write the reaction that occurs when radium-226 decays by alpha emission.
4 42 2
A AZ ZX Y energy
226 226 4 488 88 2 2Ra Y energy
From tables, we find Z and A for nuclides. The daughter atom: Z = 86,
A = 222226 222 488 86 2Ra Rn energy
Radium-226 decays into radon-222.
Radium-226 decays into radon-222.
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Beta-minus Decay
Beta-minus b- decay results when a neutron decays into a proton and an electron. Thus, the Z-number increases by one.
01 1
A AZ ZX Y energy
X is parent atom and Y is daughter atom
The energy is carried away primarily by the K.E. of the electron.
-
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Beta-plus Decay
Beta-plus b+ decay results when a proton decays into a neutron and a positron. Thus, the Z-number decreases by one.
01 1
A AZ ZX Y energy
X is parent atom and Y is daughter atom
The energy is carried away primarily by the K.E. of the positron.
+
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Radioactive MaterialsThe rate of decay for radioactive
substances is expressed in terms of the activity R, given by:
NR
t
Activit
y
N = Number of undecayed nuclei
One curie (Ci) is the activity of a radioactive material that decays at the rate of 3.7 x 1010 Bq or 3.7 x 1010 disintegrations per second.
One curie (Ci) is the activity of a radioactive material that decays at the rate of 3.7 x 1010 Bq or 3.7 x 1010 disintegrations per second.
One becquerel (Bq) is an activity equal to one disintegration per second (1 s-1).One becquerel (Bq) is an activity equal to one disintegration per second (1 s-1).
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The Half-LifeThe half-life T1/2
of an isotope is the time in which one-half of its unstable nuclei will decay.
No
0
2
N
0
4
N
Number of Half-lives
Nu
mb
er
Und
eca
yed
N
ucl
ei
1 432
0
1
2
n
N N
Where n is number of half-
lives
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Half-Life (Cont.)The same reasoning will apply to activity R or to amount of material. In general,
the following three equations can be applied to radioactivity:Nuclei
Remaining
0
1
2
n
N N
Activity R
0
1
2
n
R R
Mass Remaining
0
1
2
n
m m
Number of Half-lives:
12
tnT
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To do: p.915 (4-6)
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Please keep in mind:
• Visiting the relatives due on Monday – May 26th , 2014
• Chapter 20 & 21 assignment due next Friday– May 31st, 2014
• Final assessment on Chapter 17, 18 to 21 on Wednesday June 11th, 2014