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Atoms, Subatomic Particles, Isotopes & Atomic Mass

The Atom: Fundamental Overview

  • Atoms are the smallest particles of an element that retain that element’s chemical identity.
    • Example: Every sheet of aluminum foil is an immense collection of individual aluminum atoms.
  • All elements on the periodic table are built from atoms; each element’s atoms have unique properties.

Dalton’s Atomic Theory (1808)

  • Formulated by John Dalton (1766–1844) to explain fixed composition in compounds.
  • Core postulates (modern wording):
    • All matter consists of tiny, indivisible particles called atoms.
    • Atoms of a given element are identical (same mass & properties) and differ from atoms of other elements.
    • Chemical compounds form when atoms of two or more elements combine in simple, fixed whole-number ratios.
    • Chemical reactions involve rearrangement, separation, or combination of atoms; atoms are neither created nor destroyed (law of conservation of mass).
  • Significance: Provided the first coherent, testable framework for describing matter on the atomic scale and predicting stoichiometric relationships.

Discovery of Subatomic Particles

  • By the late 1800s, experiments showed atoms are divisible and contain smaller constituents (subatomic particles):
    • Protons (p^+) – positive charge
    • Neutrons (n^0) – neutral
    • Electrons (e^-) – negative charge
  • Charged-particle interaction rules:
    • Like charges ( (+,+) or (-,-) ) repel.
    • Unlike charges ( + and - ) attract.

J. J. Thomson’s Cathode-Ray Experiment (1897)

  • Observed cathode rays deflected by electric & magnetic fields, concluding they are streams of negatively charged electrons.
  • Proposed “plum-pudding” model: electrons embedded in a diffuse, positively charged cloud (analogous to plums in pudding).
  • Philosophical import: Demonstrated atoms were not indivisible, contradicting Dalton’s first postulate.

Rutherford’s Gold-Foil Experiment (1911)

  • Fired α-particles at thin gold foil.
    • Most particles passed straight through (empty space).
    • Some deflected at large angles; a few rebounded.
  • Conclusions:
    • Atom contains a dense, small, positively charged nucleus.
    • Electrons occupy the spacious region surrounding the nucleus.
  • Led to planetary/nuclear model of the atom, superseding Thomson’s view.

Present-Day Atomic Structure

  • Components & locations:
    • Nucleus – houses protons (+) and neutrons (0).
    • Electron cloud – vast, mostly empty space containing electrons (–).
  • Approximate sizes: nucleus diameter \sim10^{-15}\text{ m} vs. whole atom \sim10^{-10}\text{ m} (factor of 10^5 difference).

Atomic Mass Unit (amu) & Particle Masses

  • 1 amu is defined as \frac{1}{12} the mass of a ^{12}\text{C} atom (6 p, 6 n).
  • Typical masses:
    • Proton: 1.007\text{ amu} (≈1 amu)
    • Neutron: 1.008\text{ amu} (≈1 amu)
    • Electron: 0.00055\text{ amu} (≈1/1836 of a proton)
  • Practical consequence: Nearly all atomic mass resides in the nucleus; electrons dominate volume but not mass.

Tabulated Summary of Subatomic Particles

  • Proton (symbol p\text{ or }p^+) – charge +1, mass 1.007\text{ amu}, in nucleus.
  • Neutron (symbol n\text{ or }n^0) – charge 0, mass 1.008\text{ amu}, in nucleus.
  • Electron (symbol e^-) – charge -1, mass 0.00055\text{ amu}, outside nucleus.

Electrical Neutrality of Atoms

  • Any isolated atom has zero net charge.
    • Number of electrons = number of protons.
    • Example: Calcium (Z=20) contains 20 protons and 20 electrons.

Atomic Number (Z)

  • Definition: Whole number unique to each element, equal to the number of protons.
  • Placement: Shown above element symbol on periodic table.
  • Examples:
    • Z=1 – Hydrogen (1 p)
    • Z=6 – Carbon (6 p)
    • Z=29 – Copper (29 p)
    • Z=79 – Gold (79 p)
  • Critical outcome: Identifies an element; changing Z changes the element.

Mass Number (A)

  • Definition: Total particles in nucleus:
    A = \text{protons} + \text{neutrons}
  • Does not appear on the periodic table because each single atom may have a distinct A (isotopes).
  • Determining neutrons:
    \text{Neutrons} = A - Z
    • Example: Potassium with A=39 and Z=19 → 20 neutrons.

Quick Reference / Study Tip

  • Z = \text{number of protons}
  • A = \text{protons} + \text{neutrons}
  • \text{Neutrons} = A - Z
  • Applies to individual atoms, not necessarily the bulk element.

Practice Highlights (from Exercises)

  • Identifying particles:
    • Outside nucleus → electron.
    • Positive charge → proton.
    • Mass but no charge → neutron.
  • True/False checkpoints:
    • Electron mass > proton mass? → False.
    • Proton (+) and electron (-) charges? → True.
    • Nucleus contains only protons & neutrons? → True.
  • Sample proton counts:
    • F atom → 9 p.
    • K atom → 19 p.
    • Ba atom → 56 p.
  • Filling atomic-number tables (Na, Zn, S): each property equals Z because atoms are neutral.
  • Lead-207 example: 82 p, 125 n, 82 e.
  • Zinc-65 example: 30 p, 35 n; alt. isotope with 37 n has A=67.
  • Unknown element with 14 p and 20 n → Z=14, A=34, element = silicon (Si).

Isotopes

  • Definition: Atoms of the same element (same Z) with different A due to varying neutron counts.
  • Atomic symbol (nuclide notation):
    ^{A}_{Z}\text{X} where X = element symbol.
  • Example isotopes & particle counts:
    • ^{16}{8}\text{O} – 8 p, 8 n, 8 e. • ^{31}{15}\text{P} – 15 p, 16 n, 15 e.
    • ^{65}_{30}\text{Zn} – 30 p, 35 n, 30 e.

Carbon Isotopes (Exercise 13)

  • ^{12}_{6}\text{C} → 6 p, 6 n, 6 e.
  • ^{13}_{6}\text{C} → 6 p, 7 n, 6 e.
  • ^{14}_{6}\text{C} → 6 p, 8 n, 6 e.
  • Importance: ^{14}\text{C} is radioactive and useful for radiocarbon dating.

Additional Symbol Practice (Exercise 14)

  • 8 p, 8 n, 8 e → ^{16}_{8}\text{O}.
  • 17 p, 20 n, 17 e → ^{37}_{17}\text{Cl}.
  • 47 p, 60 n, 47 e → ^{107}_{47}\text{Ag}.

Isotope Comparison (Exercise 15)

  • Pair B with 6 p each are isotopes of carbon.
  • Pair C are the atoms that both contain 8 n.

Atomic Mass (Weighted Average)

  • Listed beneath each element symbol on periodic table (units: amu).
  • Represents weighted average of all naturally occurring isotopes, not a single atom’s mass.
  • Calculated relative to ^{12}\text{C} standard.
  • Contrast: A is an integer for an individual atom; atomic mass is often fractional.

Examples from Periodic Table

  • Ca → 40.08\text{ amu}
  • Al → 26.98\text{ amu}
  • Pb → 207.2\text{ amu}
  • Ba → 137.3\text{ amu}
  • Fe → 55.85\text{ amu}

Majority Isotope & Abundance Logic

  • The isotope whose mass is closest to the average atomic mass is the most abundant.
    • Lithium: 6.941 amu → ^{7}\text{Li} predominates.
    • Potassium: 39.10 amu → ^{39}\text{K} predominates.

Formal Calculation of Atomic Mass

  1. Obtain each isotope’s percent abundance and its individual atomic mass (A in amu).
  2. Convert percent → decimal fraction.
  3. Multiply: (\text{fraction})(\text{isotope mass}) for each isotope.
  4. Sum contributions: \Sigma\,[(\text{fraction})(\text{mass})] = \text{average atomic mass}.
Chlorine Example (conceptual)
  • Given atomic mass 35.45\text{ amu}.
  • Chlorine has isotopes ^{35}\text{Cl} and ^{37}\text{Cl}.
  • Cl-35 must have the larger percent abundance because 35.45 is nearer to 35 than 37.

Magnesium Isotopes Table (Key Data)

IsotopepeAn% Abundance
^{24}_{12}\text{Mg}1212241278.70\%
^{25}_{12}\text{Mg}1212251310.13\%
^{26}_{12}\text{Mg}1212261411.17\%
  • Weighted average → 24.31\text{ amu} (agrees with periodic table value).

Practical & Conceptual Implications

  • Understanding subatomic make-up enables:
    • Prediction of chemical behavior (valence depends on electrons).
    • Computation of molar masses (link macroscopic grams to microscopic atoms).
    • Use of isotopic signatures in geochemistry, medicine (PET scans), archeology (radiocarbon dating).
  • Philosophically, atomic theory bridges empirical observations with an unseen microscopic world, embodying the reductionist approach in science.

Quick Reference Equation Set

  • Atomic number: Z = #\text{protons}
  • Mass number: A = Z + #\text{neutrons}
  • Neutrons: #n = A - Z
  • Atomic mass (average): \bar{m} = \sumi \left( \text{fraction}i \times A_i \right)