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: T1/2=5730extyearsT_{1/2} = 5730 ext{ years}

  • 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: t=4imesT1/2=4imes5730extyr=22,920extyrt = 4 imes T_{1/2} = 4 imes 5730 ext{ yr} = 22{,}920 ext{ yr}

  • Conceptual takeaway: fraction remaining after n half-lives is rac12nrac{1}{2^n}; 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 11extamu11 ext{ amu} for that nuclide)

  • Periodic table mass: a weighted average reflecting natural abundances of all isotopes of the element (e.g., boron average ≈ 10.81extamu10.81 ext{ amu}, 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:
    extAvgmass=(63imes0.69)+(65imes0.31)=63.62extamuext{Avg mass} = (63 imes 0.69) + (65 imes 0.31) = 63.62 ext{ amu}

Nuclear Emission Processes (Overview)

  • Alpha emission (α): a helium nucleus is emitted

    • Example form (common representation):
      A<em>ZXightarrowA4</em>Z2Y+24extHe^{A}<em>{Z}X ightarrow ^{A-4}</em>{Z-2}Y + ^{4}_{2} ext{He}

  • 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: A<em>ZXightarrowA</em>ZX+<br>obreakextγ^{A}<em>{Z}X^{*} ightarrow ^{A}</em>{Z}X + <br>obreak ext{γ}

  • Electron capture (EC): a proton captures an inner-shell electron to become a neutron, nucleus shifts to a lower Z

    • Form: A<em>ZX+eightarrowA</em>Z1Y+<br>ue^{A}<em>{Z}X + e^{-} ightarrow ^{A}</em>{Z-1}Y + <br>u_e

  • 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 t=nimesT1/2t = n imes T_{1/2}

  • 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

    • T1/2=ractn=rac903=30extyearsT_{1/2} = rac{t}{n} = rac{90}{3} = 30 ext{ years}

    • 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}_e

  • Half-life concept: t=nimesT1/2t = n imes T_{1/2} where n is the number of half-lives

  • Fraction remaining after n half-lives: extFraction=rac12next{Fraction} = rac{1}{2^n}

  • Average mass with isotopic abundances: $$ ext{Avg mass} =

ight( ext{mass}1 imes ext{abundance}1
ight) + ext{mass}2 imes ext{abundance}2 + \