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Transcript
1
Topic 14 – Nuclear Chemistry
RADIOACTIVITY
A. The first three types of radiation discovered
1. Alpha radiation
a. Positive charge
b. Helium-4 nucleus
2. Beta radiation
a. Negative charge
b. High speed electron
3. Gamma radiation
a. No charge
b. High energy quantum of electromagnetic radiation
B. Nuclear Equations
1. Nuclide symbol
a. “A” is the mass number, the number of protons plus
the number of neutrons in the nucleus.
b. “Z” is the atomic number, the number of protons in
the nucleus.
c. The nuclide symbol has the form
A
ZX
2. Isotope name
a. Gives the value of the mass number of that isotope
b. Takes the form “name-A”
3. Reactants and products
a. Nuclides
b. Other particles
(1) Alpha particle or helium nucleus
4
4
2  or 2 He
(2) Proton
1
1
1 p or 1 H
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
2
(3) Neutron
1
0n
(4) Beta particle or electron
0
or 10 e
1 
(5) Positron
0
1  or
0
1
e
(6) Gamma photon
0
0

4. Conservation rules for nuclear reactions
a. Total charge is conserved  conservation of atomic
number
(1) The sum of the charges of the products must
equal the sum of the charges of the reactants.
(2) The sum of the subscripts of the products must
equal the sum of the subscripts of the reactants.
b. Total number of nucleons is conserved  conservation
of mass number
(1) The sum of the nucleons of the products must
equal the sum of the nucleons of the reactants.
(2) The sum of the superscripts of the products
must equal the sum of the superscripts of the
reactants.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
3
5. Comparison of chemical reactions and
nuclear reactions
Chemical Reactions
Nuclear Reactions
Atoms are rearranged by the
breaking and forming of chemical
bonds.
Only electrons in atomic orbitals are
involved in the breaking and
forming of bonds
Reactions are accompanied by
absorption or release of relatively
small amounts of energy.
Rates of reaction are influenced by
temperature, pressure,
concentration, and catalysts.
Elements or isotopes of the of the
same elements are converted from
one to another.
Protons, neutrons, electrons, and
other elementary particles may be
involved.
Reactions are accompanied by
absorption or release of tremendous
amounts of energy.
Rates of reaction normally are not
affected by temperature, pressure,
and catalysts.
6. Writing nuclear equations
a. Procedure
(1) Using a periodic table, determine the value of
“Z” (atomic number), or the symbol.
(2) Determine the missing value of “A”
(mass number).
(3) Determine the missing value of “Z”.
(4) Determine the identity of the missing nuclide
or particle.
(5) Write the complete reaction.
b. Examples
(1) Write the equation for the following reaction,
oxygen-20 emits a beta particle producing
fluorine-20.
Using a periodic table, determine the value
of “Z” (atomic number), or the symbol.
Oxygen is O.
Fluorine is F.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
4
Determine the missing value of “A”
(mass number).
The mass numbers are given in the
name of the isotope.
Determine the missing value of “Z”.
The atomic numbers are determined
from the periodic table.
Oxygen is 8.
Fluorine is 9.
Write the complete reaction.
20
8
O 
0
1
 +
20
9
F
(2) Write the equation for the following reaction,
radium-226 emits an alpha particle producing
radon-222.
Using a periodic table, determine the value
of “Z” (atomic number), or the symbol.
Radium is Ra.
Radon is Rn.
Determine the missing value of “A”
(mass number).
The mass numbers are given in the
name of the isotope.
Determine the missing value of “Z”.
The atomic numbers are determined
from the periodic table.
Radium is 88.
Radon is 86.
Write the complete reaction.
226
88
Ra  42  +
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
222
86
Rn
5
(3)
212
84
Po 
208
82
Pb + X
Determine the missing value of “A”.
212 = 208 + A
A=4
Determine the missing value of “Z”.
84 = 82 + Z
Z=2
Determine the identity of the missing
nuclide or particle.
A = 4 and Z = 2,
therefore this is an alpha particle.
Write the complete reaction.
212
84
(4)
137
55
Cs 
137
56
Po 
208
82
Pb + 42 
Ba + X
Determine the missing value of “A”.
137 = 137 + A
A=0
Determine the missing value of “Z”.
55 = 56 + Z
Z = 1
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
6
Determine the identity of the
missing nuclide or particle.
A = 0 and Z = 1,
therefore this is a beta particle.
Write the complete reaction.
137
55
(5)
78
33
As 
0
1
Cs 
137
56
Ba +
0
1

 +X
Determine the missing value of “A”.
78 = 0 + A
A = 78
Determine the missing value of “Z”.
33 = 1 + Z
Z = 34
Determine the identity of the missing
nuclide or particle.
A = 78 and Z = 34,
since Z = 34, therefore this is
Se, and the missing nuclide is
78
34
Se
Write the complete reaction.
78
33
As 
0
1
78
Se
 + 34
C. Nuclear Stability
1. The strong nuclear force holds the nucleus together.
a. It is very strong compared to the other three fundamental
forces.
b. It acts over a distance of only 1015 m.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
7
2. Predicting nuclear stability
a. “Magic numbers”
(1) Nuclei that contain 2, 8, 20, 50, 82, or 114
protons are generally more stable than those
that do not possess these numbers.
(2) Nuclei that contain 2, 8, 20, 50, 82, or 126
neutrons are generally more stable than those
that do not possess these numbers.
b. Nuclei with even numbers of both protons and neutrons
are generally more stable than those with odd numbers
of one or the other.
c. Nuclei with an even number of either protons or neutrons
and an odd number of the other are generally more stable
than those with odd numbers of both.
d. All nuclei with atomic numbers higher than 83 are
unstable and are radioactive.
e. All isotopes of technetium (Tc, Z = 43) and promethium
(Pm, Z = 61) are unstable and radioactive.
3. There is a “band of stability” in a plot of number of protons
versus number of neutrons.
a. Up to Z = 20 this ratio of neutrons to protons ranges
from 1 up to about 1.1 near Z = 20.
b. At increasingly higher Z the band of stability falls in
ratios of neutrons to protons which are continually
increasing (up to 1.5 at the highest values of Z).
4. Example
38
K or 38
Which is radioactive: 19
18 Ar ?
Argon-38 is doubly even, and potassium-38 is
doubly odd, so the radioactive nuclide would have
to be potassium-38.
D. Types of radioactive decay
1. 5 common types
a. Alpha emission
(1) Description
The emission of a 42 He nucleus, or alpha
particle
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
8
(2) Symbol

(3) Effect on Z (atomic number)
2
(4) Effect on A (mass number)
4
(5) Usual nuclear condition
Z > 83
(6) Radiation
4
4
2  or 2 He
b. Beta emission
(1) Description
The emission of a high-speed electron
(2) Symbol

(3) Effect on Z (atomic number)
+1
(4) Effect on A (mass number)
0
(5) Usual nuclear condition
Neutron/proton ratio is too high
(6) Radiation
0
1

or
0
1
e
c. Positron emission
(1) Description
The emission of a positron
(2) Symbol
+
(3) Effect on Z (atomic number)
1
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
9
(4) Effect on A (mass number)
0
(5) Usual nuclear condition
Neutron/proton ratio is too low
(6) Radiation
0
1  or
0
1
e
d. Electron capture
(1) Description
The capture of an electron from the
innermost orbital of an atom, made possible
by quantum mechanical effects
(2) Symbol
EC
(3) Effect on Z (atomic number)
1
(4) Effect on A (mass number)
0
(5) Usual nuclear condition
Neutron/proton ratio is too low
(6) Radiation
x rays
e. Gamma emission
(1) Description
The emission of a gamma photon from an
excited nucleus
(2) Symbol

(3) Effect on Z (atomic number)
0
(4) Effect on A (mass number)
0
(5) Usual nuclear condition
Excited nucleus
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
10
(6) Radiation
0
0

2. Predicting types of radioactive decay
a. Procedure
(1) Determine whether Z > 83.
Alpha emission
(2) Determine neutron/proton ratio.
(a) Z  20
Neutron/proton ratio less than 1.0
+ or EC
Neutron/proton ratio greater than 1.1

(b) Z  20
Neutron/proton ratio less than
“stable band”
+ or EC
Neutron/proton ratio greater than
“stable band”

b. Examples
(1) Predict the type of decay for
Z=7
13
7
N
Z  20?
YES
Neutron/proton ratio = 6/7 = 0.86
Neutron/proton ratio less than 1.1?
YES
+ or EC
(2) Predict the type of decay for
Z = 11
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
26
11
Na
11
Z  20?
YES
Neutron/proton ratio =15/11 = 1.36
Neutron/proton ratio greater than 1.1?
YES

NUCLEAR BOMBARDMENT REACTIONS
A. Transmutation
Is the changing of one element into another by bombarding the
target nucleus with nuclear particles or nuclei
B. Particle accelerator
Is the device used to accelerate electrons, protons, alpha particles,
or other ions to the very high speeds needed to cause transmutation
reactions through nuclear bombardment
C. Transuranium elements
Are elements with atomic numbers higher than uranium (Z = 92)
All of these are man-made through various transmutation reactions
D. Bombardment reactions
1. Rules for writing the abbreviated notation for bombardment
reactions
a. Write the nuclide symbol for the target nucleus.
b. Write an open parenthesis, then the symbol for the
projectile particle and a comma.
c. After the comma, write the symbol for the ejected
particle and a closed parenthesis.
d. After the closed parenthesis, write the nuclide symbol
for the product nucleus.
2. Examples of writing the abbreviated notation for bombardment
reactions
a. 147 N + 11 p  116 C + 42 He
14
7
N (p, )
11
6
C
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
12
b.
63
29
Cu + 42 He 
63
29
Cu (, n)
66
31
Ga + 01 n
66
33
Ga
3. Examples of writing the nuclear equations from abbreviated
notation for bombardment reactions
42
a. 45
21Sc (n, ) 19 K
45
21
Sc + 01 n 
b. 2963 Cu (p, n)
63
29
63
30
42
19
K + 42 He
Zn
Cu + 11 p 
63
30
Zn + 01 n
BIOLOGICAL EFFECTS OF RADIATION
A. Two types of biological damage from radiation
1. Somatic
a. Somatic injuries affect the organism during its lifetime.
b. Examples of somatic injuries:
sunburn
skin rash
cancer
cataracts
2. Genetic
Genetic injuries cause inheritable gene changes
(gene mutations)
B. Chemical basis for radiation damage
1. Due to the ionizing ability of these types of radiation
2. Alpha and beta particles, as well as gamma photons, can cause
ionization, and are therefore called “ionizing radiation”.
3. These can directly ionize biological and organic molecules.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
13
4. In addition, these can and do form radicals (also called
“free radicals”).
a. Definition
A radical is a molecular fragment having one
or more unpaired electrons
b. Radicals are highly reactive and are usually short-lived.
5. Formation of radicals
H2O radiation

 H2O+ + e
a. H2O+ + H2O  H3O+ +  OH
(hydroxyl radical)
b. e + O2   O2
(superoxide ion,
which is also a radical)
C. Factors that affect the amount of damage caused by radiation
1. The intensity of the radiation – the number of particles or
quanta absorbed
2. The energy of the radiation absorbed
3. The type of radiation absorbed
D. Units of radiation
1. Curie – disintegrations
a. Symbol – Ci
b. Is exactly 3.70 x 1010 nuclear disintegrations per second.
c. This is the same rate of decay as that of 1 gram of
pure radium.
2. Roentgen – output
a. symbol – R
b. The amount of x-rays or gamma rays that produce ions
carrying 2.1 x 109 units of electrical charge in 1 cm3 of
dry air at 0 C and 1 atm pressure
c. The amount of ionization of body tissue is proportional
to the radiation exposure measured in roentgens.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
14
3. rad – absorbed
a. The name is an acronym: radiation absorbed dose
b. Is the dosage of radiation that deposits 1 x 102 J of
energy per kilogram of tissue
c. Is a way of measuring the intensity and energy of
radiation absorbed
d. With soft body tissue the “rad” and the “roentgen”
are equivalent.
4. rem – damage
a. The name is an acronym: roentgen equivalent for man
b. 1 rem = 1 rad x 1 RBE
c. RBE is from Relative Biological Effectiveness.
d. The RBE factor depends on how destructive to biological
tissues a type of radiation happens to be for the same
amount of energy delivered to the tissue
e. RBEs for selected radiation
(1) X-rays: RBE = 0.7
(2) beta:
RBE = 1
(3) gamma: RBE = 1
(4) neutron: RBE = 5
(5) alpha:
RBE = 10
E. Duration of exposure is critical for determining the effects
1. The body can repair damage from ionizing radiation at only
a certain rate.
2. The shorter the period of time over which the same dose of
radiation is received, the more harmful it is.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
15
KINETICS OF RADIOACTIVE DECAY
A. All radioactive decays obey first-order kinetics.
B. The mathematics of radioactive decay
1. The rate law for radioactive decay is rate = Nt
a.  is the nuclear physics equivalent of “k” in chemical
rate expressions
b. Nt is the number of radioactive nuclei present at time “ t ”
2. The integrated rate law is ln
N0
= t
Nt
3. The expression for the half-life is
0.693147
t =
½

4. The expression for the rate constant is
0.693147
=
t1
2
C. Calculations involving radioactive decay
1. Calculating the decay constant from a measure of the activity
of a substance
A 2.8 x 106 g sample of plutonium-238 decays at a rate of
1.8 x 106 disintegrations per second. Calculate the decay
constant of plutonium-238 in s1.
mass of
238
94
GIVEN
Pu = 2.8 x 106 g
disintegrations
rate = 1.8 x 10
s
FIND
Nt = ?
6
MM
238
94
2.8 x 106 g
Nt
=
=?
Pu = 238 g/mol
238
94
Pu
6.022 x 1023 nuclei
1 mol
238 g
238
94
Pu
Nt = 7.08 x 1015 nuclei
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
1 mol
16
rate = 1.8 x 106
nuclei
s
(the number of nuclei that
disintegrate per second)
rate = Nt
=
rate
Nt
nuclei
s
=
15
7.08 x 10 nuclei
1.8 x 106
= 2.54 x 1010 s1
= 2.5 x 1010 s1
2. Calculating the half-life from the decay constant
Neptunium-237 has a decay constant of 1.03 x 1014 s1.
Calculate its half-life in years.
GIVEN
FIND
t =?
½
 = 1.03 x 1014 s1
t1 =
2
t
½
=
0.693147

0.693147
1.03 x 1014 s1
1 hr
3600 s
1 da
24 hr
1 yr
365.24 da
= 2.132 x 106 yr
= 2.13 x 106 yr
3. Calculating the half-life from activity measurements
A 0.01746 g sample of potassium-40 K-40 decays at a rate
of 4.5 x 103 disintegrations per second. Calculate the halflife of potassium-40 in years.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
17
mass of
GIVEN
K = 0.01746 g
40
19
rate = 4.5 x 103
MM
40
19
0.01746 g
Nt
=
FIND
Nt = ?
disintegra tions
s
t =?
½
K = 40.00 g/mol
40
19
K
=?
6.022 x 1023 nuclei
1 mol
40.00 g
40
19
K
1 mol
Nt = 2.6286 x 1020
=
rate
Nt
nuclei
s
=
20
2.6286 x 10 nuclei
4.5 x 103
 = 1.71 x 1017 s1
t =
½
t
½
=
0.693147

0.693147
1.71 x 1017 s1
1 hr
3600 s
1 da
24 hr
1 yr
365.24 da
t = 1.3 x 109 yr
½
4. Calculating the decay constant from the half-life
Promethium-147 has a half-life of 2.5 yr. Calculate its
decay constant in s1.
=
0.693147
t1
2

=
0.693147
2.5 yr
1 yr
365.24 da
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
1 da
24 hr
1 hr
3600 s
18
 = 8.786 x 109 s1
= 8.8 x 109 s1
5. Using radioisotopes for dating samples
a. Deriving the radiodating equation
N
ln 0 = t
Nt
=
0.693147
t1
2


0.693147 
N0

ln
=
 (t)
Nt
 t1
2


ln
N0
= 0.693147
Nt

 t
 t
 12




b. Approach to radiodating
(1) Determine the decay constant from a measure
of the activity of a substance.
(2) Calculate the half-life from the decay constant.
(3) For rocks, determine the amounts of the
daughter products and the amounts of the parent
isotopes in the sample.
(a) This uses the radioactive decay series of
various radioisotopes found in the
minerals of which igneous rocks are
formed.
(b) A radioactive decay series is a sequence
of steps in which one radioactive nucleus
decays to a second, and then to a third,
and so on, until a stable nucleus is
formed.
(4) For carbon containing substances, convert all
of the carbon to CO2, trap it, and then measure
the level of activity per gram of total carbon.
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby
19
c. Example
Carbon from the Dead Sea scrolls gave 12.1
disintegrations of carbon-14 per minute per gram of
carbon. Carbon from today’s living material gives
15.3 disintegrations of carbon-14 per minute per
gram of carbon. Calculate the age of the scrolls.
GIVEN
dis
N0  15.3
min  g
Nt  12.1
FIND
dis
min  g
t=?
t = 5730 yr
½
ln

t
N0
= 0.693147 
Nt
 t1
 2




ln


t
15.3

= 0.693147 
12.1
 5730 yr 


t

0.2346 = 0.693147 
 5730 yr 
t
0.3385 =
5730 yr
t = 1.94 x 103 yr
Topic 14 – Nuclear Chemistry
© 2006 Lloyd Crosby