nuclear chemistry powerpoint
DESCRIPTION
From Sir PazTRANSCRIPT
Nuclear Chemistry
Radioactivity – spontaneous emission of particles and or radiation
(proposed by Marie Curie)
• Three types of ray are produced by the decay, or breakdown, of radioactive
substances
A. Alpha rays ( α ) – consist of positively charged particles called alpha particles and therefore are
deflected by the positively charged plate.B. Beta rays ( β ) – or beta particles – are
electrons and deflected by negatively charged plateC. Gamma rays ( γ ) – have no charged and are
not affected by an external electric field or magnetic field
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Radioactive substance
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Radioactive substance
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XAZ
Mass Number
Atomic NumberElement Symbol
Atomic number (Z) = number of protons in nucleus
Mass number (A) = number of protons + number of neutrons
= atomic number (Z) + number of neutrons
A
Z
1p11H1or
proton1n0
neutron0e-1
0b-1or
electron0e+1
0b+1or
positron4He2
4a2or
a particle
1
1
1
0
0
-1
0
+1
4
2
23.1
Balancing Nuclear Equations
1. Conserve mass number (A).
The sum of protons plus neutrons in the products must equal the sum of protons plus neutrons in the reactants.
1n0U23592 + Cs138
55 Rb9637
1n0+ + 2
235 + 1 = 138 + 96 + 2x1
2. Conserve atomic number (Z) or nuclear charge.
The sum of nuclear charges in the products must equal the sum of nuclear charges in the reactants.
1n0U23592 + Cs138
55 Rb9637
1n0+ + 2
92 + 0 = 55 + 37 + 2x023.1
212Po decays by alpha emission. Write the balanced nuclear equation for the decay of 212Po.
4He24a2oralpha particle -
212Po 4He + AX84 2 Z
212 = 4 + A A = 208
84 = 2 + Z Z = 82
212Po 4He + 208Pb84 2 82
23.1
23.1
I. Nuclear Stability and Radioactive Decay
n/p too large
beta decay
X
n/p too small
positron decay or electron capture
Y
23.2
Predicting the mode of decay
1. High n/p ratio (too many neutrons; lie above band of stability) --- undergoes beta decay
2. Low n/p ratio (neutron poor; lie below band of stability) --- positron decay or electron capture
3. Heavy nuclides ( Z > 83) --- alpha decay
II. Nuclear Transmutations
• Nuclear reactions that are induced in a way that nucleus is struck by a neutron or by another nucleus (nuclear bombardment)
a. Positive ion bombardment- alpha particle is the most commonly used positive ion- uses acceleratorsExamples:14
7 N + 42 He → 17
8 O + 11 H
94 Be + 4
2 He → 126 C + 1
0n
b. Neutron bombardment- neutron is bombarded to a nucleus to form a new nucleus- most commonly used in the transmutation to form synthetic isotopes because neutron are neutral, they are not repelled by nucleusExample: 58
26 Fe + 10 n → 59
26 Fe → 5927 Co + 0
-1 e
Transuranium elements
- Element with atomic numbers above 92- Produced using artificial transmutations, either
by:a. alpha bombardmentb. neutron bombardmentc. bombardment from other nucleiExamples:
a.
b.
4He2Pu23994 + Cm242
961n0 +
1n0U23892 + U239
92
0 e-1Pu23994 + Np239
93 + 0-1 e
14N7U23892 + Es247
991n0+ 5c.
III. Nuclear Energy
Recall:Nucleus is composed of proton and neutronThen, is the mass of an atom equal to the total mass of all the proton plus the total mass of all the neutron?
Example for a He atom:Total mass of the subatomic particles= mass of 2 p+ + mass of 2n0
= 2 ( 1.00728 amu ) + 2 (1.00867 amu)= 4.03190 amuAnd atomic weight of He-4 is 4.00150
Why does the mass differ if the atomic mass = number of protons + number of neutrons?
Mass defect
-mass difference due to the release of energy-this mass can be calculated using Einstein’s equation E =mc2
2 11 H + 2 2
0 H → 42 He + energy
Therefore:-energy is released upon the formation of a nucleus from the constituent protons and neutrons-the nucleus is lower in energy than the component parts.-The energy released is a measure of the stability of the nucleus. Taking the reverse of the equation:
42 He + energy → 2 1
1 H + 2 20 n
Therefore,-energy is released to break up the nucleus into its component parts. This is called the nuclear binding energy.-the higher the binding energy, the stable the nuclei.-isotopes with high binding energy and most stable are those in the mass range 50-60.
Nuclear binding energy per nucleon vs Mass number
nuclear binding energynucleon
nuclear stability
23.2
-The plot shows the use of nuclear reactions as source of energy.-energy is released in a process which goes from a higher energy state (less stable, low binding energy) to a low energy state (more stable, high binding energy).-Using the plot, there are two ways in which energy can be released in nuclear reactions:
a. Fission – splitting of a heavy nucleus into smaller nuclei
b. Fusion – combining of two light nuclei to form a heavier, more stable nucleus.
Nuclear binding energy (BE) is the energy required to break up a nucleus into its component protons and neutrons.
BE + 19F 91p + 101n9 1 0
BE = 9 x (p mass) + 10 x (n mass) – 19F mass
E = mc2
BE (amu) = 9 x 1.007825 + 10 x 1.008665 – 18.9984
BE = 0.1587 amu 1 amu = 1.49 x 10-10 J
BE = 2.37 x 10-11J
binding energy per nucleon = binding energy
number of nucleons
= 2.37 x 10-11 J19 nucleons
= 1.25 x 10-12 J
23.2
23.3
Radiocarbon Dating
14N + 1n 14C + 1H7 160
14C 14N + 0b + n6 7 -1 t½ = 5730 years
Uranium-238 Dating
238U 206Pb + 8 4a + 6 0b92 -182 2 t½ = 4.51 x 109 years
23.3
Nuclear Transmutation
Cyclotron Particle Accelerator
14N + 4a 17O + 1p7 2 8 1
27Al + 4a 30P + 1n13 2 15 0
14N + 1p 11C + 4a7 1 6 2
23.4
Nuclear Transmutation
23.4
Nuclear Fission
23.5
235U + 1n 90Sr + 143Xe + 31n + Energy92 54380 0
Energy = [mass 235U + mass n – (mass 90Sr + mass 143Xe + 3 x mass n )] x c2
Energy = 3.3 x 10-11J per 235U
= 2.0 x 1013 J per mole 235U
Combustion of 1 ton of coal = 5 x 107 J
Nuclear Fission
23.5
235U + 1n 90Sr + 143Xe + 31n + Energy92 54380 0
Representative fission reaction
Nuclear Fission
23.5
Nuclear chain reaction is a self-sustaining sequence of nuclear fission reactions.The minimum mass of fissionable material required to generate a self-sustaining nuclear chain reaction is the critical mass.
Non-critical
Critical
Nuclear Fission
23.5
Schematic diagram of a
nuclear fission reactor
Annual Waste Production
23.5
35,000 tons SO2
4.5 x 106 tons CO2
1,000 MW coal-firedpower plant
3.5 x 106
ft3 ash
1,000 MW nuclearpower plant
70 ft3 vitrified waste
Nuclear Fission
23.5
Nuclear Fission
Hazards of the radioactivities in spent
fuel compared to uranium ore
From “Science, Society and America’s Nuclear Waste,” DOE/RW-0361 TG
23.6
Nuclear Fusion
2H + 2H 3H + 1H1 1 1 1
Fusion Reaction Energy Released
2H + 3H 4He + 1n1 1 2 0
6Li + 2H 2 4He3 1 2
6.3 x 10-13 J
2.8 x 10-12 J
3.6 x 10-12 J
Tokamak magnetic plasma
confinement
23.7
Radioisotopes in Medicine• 1 out of every 3 hospital patients will undergo a nuclear
medicine procedure
• 24Na, t½ = 14.8 hr, b emitter, blood-flow tracer
• 131I, t½ = 14.8 hr, b emitter, thyroid gland activity
• 123I, t½ = 13.3 hr, -g ray emitter, brain imaging
• 18F, t½ = 1.8 hr, b+ emitter, positron emission tomography
• 99mTc, t½ = 6 hr, -g ray emitter, imaging agent
Brain images with 123I-labeled compound
Geiger-Müller Counter
23.7
23.8
Biological Effects of RadiationRadiation absorbed dose (rad)
1 rad = 1 x 10-5 J/g of material
Roentgen equivalent for man (rem)
1 rem = 1 rad x Q Quality Factorg-ray = 1b = 1a = 20
Chemistry In Action: Food Irradiation
Dosage Effect
Up to 100 kiloradInhibits sprouting of potatoes, onions, garlics. Inactivates trichinae in pork. Kills or prevents insects from reproducing in grains, fruits, and vegetables.
100 – 1000 kilorads Delays spoilage of meat poultry and fish. Reduces salmonella. Extends shelf life of some fruit.
1000 to 10,000 kiloradsSterilizes meat, poultry and fish. Kills insects and microorganisms in spices and seasoning.