Exam Review Notes: Nuclear Chemistry and Radioisotopes
Protons, Neutrons, and Electrons
Subatomic particles and basic properties
Proton: charge +1; mass ≈ 1 amu; located in the nucleus
Neutron: charge 0; mass ≈ 1 amu; located in the nucleus
Electron: charge −1; mass ≈ 0 amu; located outside the nucleus (electron cloud)
Rationale: nucleus contains protons and neutrons (nucleons); electrons occupy orbitals around the nucleus and determine chemical behavior
Isotopes, Atomic Mass, and Mass Number
Definitions
Isotope: atoms of the same element with different numbers of neutrons
Mass number (A): A = Z + N, where Z = number of protons, N = number of neutrons
Atomic (decimal) mass on the periodic table is a weighted average of all isotopes of the element, reflecting natural abundances
Interpretation of a given isotope table (conceptual):
Mass number applies to the specific isotope (not to all isotopes of the element)
Protons determine the element; neutrons contribute to mass and stability; electrons balance charge in neutral atoms
Carbon Isotopes and Radioactivity
Carbon has three stable/radioactive isotopes commonly discussed:
Carbon-12: Protons = 6; Neutrons = 6
Carbon-13: Protons = 6; Neutrons = 7
Carbon-14: Protons = 6; Neutrons = 8
Carbon-14 is radioactive due to an unstable nucleus (excess neutrons relative to stability for this nuclide)
Note: mass numbers are 12, 13, 14, with identical proton count (6) but different neutron counts
Nuclear Decay of Carbon-14
Decay mode: beta emission (β−)
Balanced reaction (beta decay):
^{14}{6}C ightarrow ^{14}{7}N + e^{-} + ar{
u}_e
Half-life of Carbon-14:
Example problem: a fossilized tree shows 6.25% of Carbon-14 remaining
6.25% = 1/16 ≈ (1/2)^4, so 4 half-lives have passed
Time elapsed:
Conceptual takeaway: fraction remaining after n half-lives is ; elapsed time scales with the half-life
Atomic Mass vs. Isotope Mass and Average Atomic Mass
Isotope mass: exact mass of a specific isotope (e.g., boron-11 has a mass of exactly for that nuclide)
Periodic table mass: a weighted average reflecting natural abundances of all isotopes of the element (e.g., boron average ≈ , not equal to any single isotope mass)
Important distinction: use exact isotope mass for a single nuclide; use average mass for elemental properties and comparisons
Copper Isotopes and Average Atomic Mass
Naturally occurring copper isotopes and abundances:
Cu-63: abundance ≈ 69%
Cu-65: abundance ≈ 31%
Average atomic mass calculation:
Nuclear Emission Processes (Overview)
Alpha emission (α): a helium nucleus is emitted
Example form (common representation):
Beta emission (β−): a neutron converts to a proton with emission of an electron and an antineutrino
Form: ^{A}{Z}X ightarrow ^{A}{Z+1}Y + e^{-} + ar{
u}_e
Gamma emission (γ): emission of high-energy photons from a excited nucleus, no change in Z or A
Form:
Electron capture (EC): a proton captures an inner-shell electron to become a neutron, nucleus shifts to a lower Z
Form:
General notes from the slide set include example reactions: Ra-222 → Rn-218 + He-4 (alpha decay), Co-59 + n → … (beta pathways), Mo + e− (electron capture) and pathways involving gamma emission
Radiation Health Effects and Shielding (External vs Internal)
External exposure (radiation source outside the body): ranking from least to most harmful based on penetrating power
Alpha particles: least penetrating; stopped by skin or a sheet of paper
Beta particles: moderate penetrating; can be stopped by plastic, clothing, or light shielding
Gamma rays: highly penetrating; require dense shielding (lead or concrete, roughly 10 cm or more depending on energy)
Key principle: more penetrating radiation is generally more harmful externally
Shielding guidelines (external protection):
Alpha: paper or thin clothing is typically sufficient
Beta: plastic, glass, or lightweight metal shielding
Gamma: thick shielding such as lead or concrete (≈ 10 cm or more as a general guideline)
Internal exposure (emissions inside the body, e.g., via inhalation, ingestion, implantation): ranking is opposite
Inside the body, high-LET (often more localized) alpha radiation can cause significant damage despite being less penetrating externally
In this context, alpha particles are most harmful internally; beta particles are intermediate; gamma rays are least harmful internally (though they still pose risk)
Half-Life Calculation Guidelines and Key Formulas
Core formula: Total time = (number of half-lives) × (half-life time) or
Key relationships:
Final amount = Initial amount ÷ 2^n
Initial amount = Final amount × 2^n
Always compare total time with the half-life time to determine n when given t
Total time is always larger than or equal to the half-life time for at least one half-life to pass; initial amount > final amount for decay scenarios
Example: solve half-life from a pair of amounts and time
If 1.0 g decays to 0.125 g in 90 years:
0.125 = 1.0 ÷ 2^n ⇒ 2^n = 8 ⇒ n = 3
If final amount is achieved after a given time with a known starting amount, use the same multiplication/division by powers of 2
Medical Radioisotopes: Diagnosis vs. Treatment
Medical applications of radioisotopes
Diagnosis (imaging): trace amounts are used to image organs; short half-lives are preferred to minimize radiation exposure
Treatment: higher doses aimed at destroying diseased or cancerous tissue; targeted to specific organs or tissues; often longer half-lives (days to weeks) to sustain dose
Brachytherapy (internal radiotherapy) specifics
Permanent (low dose-rate) brachytherapy implant: radioactive seeds implanted into a target area (e.g., prostate) with ultrasound guidance
Typical seed count: about 40 to 100 seeds implanted depending on treatment plan
Seeds remain in place permanently and become biologically inert after months, providing localized high-dose radiation with limited damage to surrounding tissues
Pd-103 brachytherapy components
Pd-103 seeds or sources are often delivered on ion-exchange beads placed into Ti capsules and can be part of Au/Cu alloy carriers
Pd-103 half-life ≈ 17 days
Pd-103: Case Study, Timing, and Safety Considerations
What does Pd-103 mean?
Pd-103 is one isotope of palladium with mass number 103
Why is Pd-103 radioactive?
It has an unstable nucleus, leading to radioactive decay (emitting gamma radiation and/or particles over time)
Key timing for safety and patient family exposure
After about 3–5 half-lives, most radioactivity decays away
For Pd-103 (half-life ≈ 17 days), 5 half-lives ≈ 85 days ≈ ~3 months; this is why patients are advised about exposure to others (especially children) for several months after implantation
Specific calculation example: 3 months corresponds to roughly 5 half-lives
Amount remaining ≈ Initial × (1/2)^5 ≈ Initial × 1/32 ≈ 3.125%
Electron capture recap (for context):
Electron capture is a mode of decay where a nucleus captures an inner-shell electron, converting a proton to a neutron in the process
Practical takeaway: long-term radiation safety in brachytherapy hinges on knowing half-lives, dose delivery, and decay timelines to minimize risk to others while delivering effective treatment
Valence Electrons, Ion Formation, and the Octet Rule
Valence electron concept: electrons in the outermost shell determine chemical properties
Common-group rule: number of valence electrons typically equals the group number for main-group elements (exceptions for transition metals)
Examples of valence electrons (per page):
Calcium: 2 valence electrons
Oxygen: 6 valence electrons
Chlorine (Chloride): 7 valence electrons
Krypton: 8 valence electrons
Arsenic: 5 valence electrons
Aluminum: 3 valence electrons
Charge on ions via the octet rule (stability when an atom attains 8 valence electrons):
Calcium → Ca^{2+} (loses 2 electrons)
Oxygen → O^{2-} (gains 2 electrons)
Chlorine → Cl^{-} (gains 1 electron)
Krypton → does not form a typical ion (noble gas, stable with full octet)
Arsenic → As^{3-} (gains 3 electrons) or forms other ionic states depending on context
Aluminum → Al^{3+} (loses 3 electrons)
Summary of the octet rule: main-group atoms are most stable with 8 electrons in their valence shell; transition metals may deviate from this rule
Medical Applications for Radioisotopes: Diagnosis and Therapeutic Use
Diagnosis:
Radioisotopes concentrate in specific organs, enabling imaging of diseased states
Administered in trace amounts; very short half-lives reduce long-term exposure
Treatment:
Higher doses are used to destroy diseased or cancerous tissue
Targeted to affected organ; tissues that divide rapidly (e.g., cancer cells) are more affected
Often employ slightly longer half-lives (days to weeks) to sustain therapeutic dose
Brachytherapy: Seeds, Capsule, and Materials
Seed construction and materials
Pd-103 seeds may be embedded on ion-exchange beads
Seed components can include Ti capsules and Au/Cu alloy constructions for shielding and structural integrity
Practical aspects
Implantation guided by imaging (e.g., ultrasound)
Number of seeds and placement are customized per patient
Seeds become biologically inert after months while delivering a high, localized dose during that period
Quick Reference Formulas and Facts (Summary)
Beta decay balance (example): ^{14}{6}C ightarrow ^{14}{7}N + e^{-} + ar{
u}_eHalf-life concept: where n is the number of half-lives
Fraction remaining after n half-lives:
Average mass with isotopic abundances: $$ ext{Avg mass} =
ight( ext{mass}1 imes ext{abundance}1
ight) + ext{mass}2 imes ext{abundance}2 + \