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Published byMarilynn Boyd Modified over 9 years ago
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Nuclear Radiation Natural Radioactivity Nuclear Equations
Producing Radioactive Isotopes Half-Life Nuclear Fission and Fusion
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Subatomic Particles Protons- plus charge In the nucleus
Neutrons- neutral Electrons - negative charge Outside the nucleus
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Nuclear Symbols Mass number (p+ + no) Element symbol Atomic number
(number of p+)
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RADIOACTIVITY Nuclei of unstable isotopes called radioisotopes gain stability by undergoing changes These changes are always accompanied by large amounts of energy Discovery of radioactivity dealt a blow to Dalton’s theory that atoms are indivisible
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Radiation Radiation comes from the nucleus of an atom.
Unstable nucleus emits a particle or energy alpha beta gamma
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Same as a helium nucleus
Alpha Particle Same as a helium nucleus (He) 4 2 He or Two protons Two neutrons
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Beta Particle e or 1 An electron emitted from the nucleus
e or 1 A neutron in the nucleus breaks down n H + e
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Gamma Radiation Pure radiation
Like an X-ray but comes from the nucleus
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Radiation Protection Shielding alpha – paper, clothing
beta – lab coat, gloves gamma- lead, thick concrete Limit time exposed Keep distance from source
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Radiation Protection
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Balancing Nuclear Equations
In the reactants and products Atomic numbers must balance and Mass numbers must balance
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Alpha decay
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Beta decay 234Th ® 234Pa e 1 beta particle
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No change in atomic or mass number
Gamma radiation No change in atomic or mass number 11B 11B boron atom in a high-energy state
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Types of Radioactive Decay
gamma ray production (g): positron production : electron capture: (inner-orbital electron is captured by the nucleus) e 1
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Types of Radiation
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Learning Check NR1 Write the nuclear equation for the beta emitter Co-60.
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Solution NR1 Write the nuclear equation for the Beta emitter Co-60. 60Co Ni e
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Half-Life of a Radioisotope
The time for the radiation level to fall (decay) to one-half its initial value decay curve 8 mg 4 mg 2 mg mg initial 1 half-life 2 3
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Examples of Half-Life Isotope Half life C-15 2.4 sec Ra-224 3.6 days
I days C years U years
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Learning Check NR3 The half life of I-123 is 13 hr. How much of a 64 mg sample of I-123 is left after 26 hours?
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Solution NR3 t1/2 = 13 hrs 26 hours = 2 x t1/2 Amount initial = 64mg
Amount remaining = 64 mg x ½ x ½ = 16 mg
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Nuclear Fission Fission large nuclei break up
235U n Ba Kr + 3 1n + Energy
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Fission
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Nuclear Fusion Fusion small nuclei combine 2H + 3H 4He + 1n + 1 1 2 0
Occurs in the sun and other stars Energy
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Learning Check NR4 Indicate if each of the following are
Fission (2) fusion Nucleus splits Large amounts of energy released Small nuclei form larger nuclei Hydrogen nuclei react Energy
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Solution NR4 Indicate if each of the following are Fission (2) fusion
Nucleus splits Large amounts of energy released Small nuclei form larger nuclei Hydrogen nuclei react
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Energy and Mass Nuclear changes occur with small but measurable losses of mass. The lost mass is called the mass defect, and is converted to energy according to Einstein’s equation: DE = Dmc2 Dm = mass defect DE = change in energy c = speed of light Because c2 is so large, even small amounts of mass are converted to enormous amount of energy.
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