Download presentation
1
Nuclear Chemistry
2
Outline Background/Introduction Spontaneous Nuclear Reactions
Types of Radioactive Decay Radioactive Half-Life Stimulated Nuclear Reactions Nuclear Fission Nuclear Fusion
3
Nuclear Chemistry - Background
Traditional Chemistry Reactions occur due to interactions between valence electrons (surrounding nucleus) Late 1800s – Early 1900s New Developments Discovery that Uranium emits radiation (Henry Becquerel) Amount of radiation emitted is proportional to amount of element present (Marie Curie) “Radioactive” substances = radiation-emitting (Curie) Radioactivity = a inherent property of certain ATOMS, as opposed to a chemical property of compounds (Curie) Birth of nuclear chemistry
4
Video: Early (Mis)uses of Radium
A radioactive element discovered in 1898 by Curie Found to glow in the dark! Many (at the time) thought it had health benefits Radium Toothpaste For video, see below URL: For more complete list of “quack” cures, see below URL:
5
Chemical vs. Nuclear Reactions
Chemical Reactions Nuclear Reactions Loss, gain, sharing of valence electrons Formation of compounds (Recall the different reaction types) Affected by temperature, pressure, presence of other atoms Changes in nucleus Transformation of one element into a different isotope or a different element altogether Unaffected by temperature, pressure, presence of other atoms
6
Atomic Structure Review
Isotopes: variants of atoms of a particular chemical element, which have differing numbers of neutrons (e.g. Carbon-12, Carbon-13, Carbon-14, etc.)
7
Nuclear Stability How can a stable nucleus exist? Nuclear Force (1934)
Net positive charge in nucleus surrounded by negative charges (electrons) Electrostatic force Opposite charges attract Like charges repel Why doesn’t the nucleus break apart? Nuclear Force (1934) Force between protons and neutrons than binds nucleus together within atom Very strong (must be!)
8
Which Elements/Isotopes Are Radioactive?
Based on the nuclear force and nuclear stability More protons in nucleus more neutrons needed to bind nucleus together Critical Factor = Neutral-to-Proton Ratio Neutron-to-Proton ratios of stable nuclei increase with increasing atomic number Unstable neutron-to-proton ratio = RADIOACTIVE Nuclei with atomic numbers ≥ 84 = ALWAYS Radioactive Very large nuclei! Neutron-to-proton ratio always unstable
10
Spontaneous Nuclear Reactions
11
Radiation and Radioactive Decay
Unstable (radioactive) nuclei emit radiation (energy) in order to become more stable Radioactive Decay – occurs when a nucleus spontaneously decomposes in this way 3 Common Types of Nuclear Reactions Alpha Radiation Beta Radiation Gamma Radiation
12
Alpha (α) Radiation
13
Alpha Radiation: Nuclear Equation
Emission of 2 protons and 2 neutrons (as an alpha particle, ) from radioactive atom’s nucleus Atom’s atomic mass decreases by 4 units Atom’s atomic number decreases by 2 units (a different element!)
14
Beta (β) Radiation
15
Beta Radiation: Nuclear Equation
Conversion of a neutron into a proton and an electron, followed by the emission of the electron (beta particle) from the nucleus Atom’s atomic mass does NOT change Atom’s atomic number increases by 1 units (a different element!)
16
Gamma (ϒ) Radiation Emission of electromagnetic energy from an atom’s nucleus No particles emitted Often occurs during α and/or β decay Example: X-rays emitted during β-decay of cobalt-60 (above)
17
Uranium-238: Radioactive Decay Chain
18
Practice: WE DO Write a nuclear equation for the β-decay of francium-234 Write a nuclear equation for the α-decay of radium-235 Write a nuclear equation for the ϒ-decay of uranium-239
19
Practice: YOU DO What isotope is present after Po-210 undergoes 2 consecutive alpha decays, followed by a beta decay, followed by another alpha decay.
20
Half-Life (T1/2) = The amount of time necessary for one-half of a particular radioactive sample to decay
21
Different Elements Different Half-Lives
Data for most stable isotope of element
22
Half-Life Problems Half-Life Formulas
Can be completed without the below formulas! Conceptual knowledge of half-life is sufficient Half-Life Formulas Fraction remaining = (n = # of half-lives elapsed) Amount remaining = Original Amount * Fraction Remaining
23
Practice: WE DO The half-life of radium-226 is 1600 years. How many grams of a 0.25 gram sample will remain after 4800 years?
24
Practice: YOU DO How many days does it take for 16 g of palladium-103 to decay to 1.0 g? The half-life of palladium-103 is 17 days. The half-life of thorium-227 is days. How many days are required for 75% of a given amount to decay?
25
Stimulated Nuclear Reactions
26
Nuclear Fission Neutron fired at atom’s nucleus
Energy of neutron “bullet” causes target element to split into two (or more) elements that are lighter than the parent atom Unpredictable composition of products Energy released! More neutrons released! RESULT? SEE NEXT SLIDE
28
Nuclear Fission Chain Reactions
Nuclear Fission Power (Controlled Nuclear Fission) Nuclear Fission (Atomic) Bomb (Uncontrolled Nuclear Fission)
29
Nuclear Fission (Atomic) Bombs
Fuel Core (B) Two subcritical masses of plutonium Each contains not enough fissionable material to sustain nuclear fission Neutron source (radioactive isotope) in separate compartment Detonation of outer casing of TNT (A) Two plutonium masses brought together to form supercritical mass Mass now contains enough fissionable material to sustain nuclear fission! Neutrons brought to speed necessary to initiate nuclear fission
30
Nuclear Fusion Reactions in which two or more elements “fuse” together to form one larger element (heaver isotope formed from lighter isotopes) Requires extremely high heat (lots of energy!) and pressure Analogy: trying to squeeze an unopened can of Coke into a little ball without spilling any Coke Lots of energy is released! Example: Fusion of 2 hydrogen isotopes (deuterium and tritium) into helium
31
Nuclear Fusion (Hydrogen) Bombs
Central core (B) of trillions of deuterium and tritium isotopes Surrounded by small atomic (fission) bombs (A) Detonation of atomic bombs provides energy and pressure for fusion of hydrogen isotopes into helium LOTS of energy released in this process! Atomic bombs (nuclear fission) used to initiate nuclear fusion Fusion itself energy release Release of neutrons accompanying fusion triggers fission of bomb casing (C), which is made of Uranium!
32
Nuclear Fusion (Hydrogen) Bombs
Energy released = over 10 times greater than fission (atomic) bomb Has never been used in warfare Neutron bomb = Hydrogen bomb without uranium casing Less explosion, due to lack of fission of casing Large quantity of neutrons propelled outward (neutron radiation) and captured by nuclei of substances they encounter Results: * Neutron radiation induces radioactivity in most substances it encounters * Massive radiation without massive blast Targets: * Potential H-bomb survivors (e.g. tank drivers, stronghold inhabitants, etc.) * Ballistic missiles (intense neutron flux damages electron components)
33
Nuclear Fusion in the Sun
Energy is released from these fusion reactions that we receive as LIGHT and HEAT! NOTE: 3 hydrogen-1 atoms required (total), yet only 2 produced The Sun is running out of fuel (hydrogen-1 atoms)!
34
Controlled Nuclear Fusion on Earth?
Advantages over nuclear fission More energy created Very little dangerous radiation released Potential Source = Water (and not much of it)!! Main Challenge Need to find way to bring small sample of deuterium and tritium to very high temperature and pressure WITHOUT detonating atomic bombs Subject of much current research in physics and chemistry
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.