A. Rutherford\'s Alpha-Scattering Experiment (1911):
- Observation 1: Most $\\alpha$-particles passed through undeflected $\\implies$ Most of the space inside an atom is completely empty.
- Observation 2: A few particles deflected at large angles $\\implies$ Positive charge is concentrated in a tiny central region called the Nucleus.
- Observation 3: Extremely rare particles ($1$ in $20,000$) rebounded at $180^\\circ$ $\\implies$ The nucleus is incredibly dense, massive, and rigid.
B. Atomic Number ($Z$) and Mass Number ($A$):
$$\\mathbf{Z = \\text{Number of Protons} = \\text{Number of Electrons (in neutral atom)}}$$ $$\\mathbf{A = \\text{Number of Protons } (Z) + \\text{Number of Neutrons } (n) \\implies n = A - Z}$$Standard notation: $\\mathbf{^A_Z\\text{X}}$, e.g., $^{23}_{11}\\text{Na} \\implies Z = 11, A = 23, n = 23 - 11 = 12$.
C. Bohr-Bury Rules of Electron Distribution:
- Maximum electrons in $n^{\\text{th}}$ shell $= \\mathbf{2n^2}$: $$K\\text{ shell } (n=1) = 2, \\quad L\\text{ shell } (n=2) = 8, \\quad M\\text{ shell } (n=3) = 18, \\quad N\\text{ shell } (n=4) = 32$$
- The outermost (valence) shell can never hold more than $8$ electrons (Octet Rule; $2$ for helium, Duplet).
- Electrons do not enter a new shell until the inner shell is step-wise filled.