Chemistry 119 - Chapter 2: Orbital Shapes, Energies, Electron Spin, and Pauli Principle

Fundamentals of Atomic Models and Quantum Mechanics

  • Bohr Model vs. Quantum Mechanical Model:

    • The Bohr model depicts electrons orbiting the nucleus in fixed, quantized circular shells.
    • The Bohr model is limited and only works accurately for the hydrogen atom (single-electron system).
    • Quantum mechanics provides a comprehensive, mathematically complete description of multi-electron atoms.
  • Wavefunctions and Probability Distributions:

    • The square of the wavefunction (ψ2\psi^2) represents the probability density or probability distribution of finding an electron in a specific region of space around the nucleus.
    • This three-dimensional probability distribution defines the spatial volume known as an atomic orbital shape.
  • Electronic State Assignment:

    • Electronic states within an atom are uniquely specified and assigned using a set of quantum numbers.

Quantum Numbers and Orbital Structure

  • Summary of Quantum Numbers and Interrelationships:

    • Principal Quantum Number (nn):
    • Values: n=1,2,3,4,…n = 1, 2, 3, 4, \dots
    • Indicates the main energy level or principal shell.
    • Number of subshells in shell nn equals nn.
    • Total number of orbitals in shell nn equals n2n^2.
    • Angular Momentum Quantum Number (ll):
    • Values: l=0,1,2,…,n−1l = 0, 1, 2, \dots, n - 1
    • Defines the subshell type and three-dimensional shape of the orbital.
    • Subshell designations: l=0l = 0 (ss), l=1l = 1 (pp), l=2l = 2 (dd), l=3l = 3 (ff).
    • Magnetic Quantum Number (mlm_l):
    • Values: ml=+l,…,0,…,−lm_l = +l, \dots, 0, \dots, -l
    • Specifies the spatial orientation of an orbital within a given subshell.
    • Total number of orbitals in a subshell equals 2l+12l + 1.
    • Spin Quantum Number (msm_s):
    • Values: ms=±12m_s = \pm \frac{1}{2}
    • Describes the intrinsic spin orientation of an individual electron (+12+\frac{1}{2} for spin-up ↑\uparrow, −12-\frac{1}{2} for spin-down ↓\downarrow).
  • Shell and Subshell Breakdown:

    • n=1n = 1 Shell:
    • Subshell: l=0l = 0 (1s1s)
    • Magnetic quantum number: ml=0m_l = 0
    • Total orbitals: 1 orbital (1s1s) of 1 type; holds up to 2 electrons.
    • n=2n = 2 Shell:
    • Subshell l=0l = 0 (2s2s): ml=0m_l = 0 (one 2s2s orbital, 2 electrons).
    • Subshell l=1l = 1 (2p2p): ml=+1,0,−1m_l = +1, 0, -1 (three 2p2p orbitals, 6 electrons).
    • Total orbitals: 4 orbitals (n2=22=4n^2 = 2^2 = 4) of 2 types; holds up to 8 electrons.
    • n=3n = 3 Shell:
    • Subshell l=0l = 0 (3s3s): ml=0m_l = 0 (one 3s3s orbital).
    • Subshell l=1l = 1 (3p3p): ml=+1,0,−1m_l = +1, 0, -1 (three 3p3p orbitals).
    • Subshell l=2l = 2 (3d3d): ml=+2,+1,0,−1,−2m_l = +2, +1, 0, -1, -2 (five 3d3d orbitals).
    • Total orbitals: 9 orbitals (n2=32=9n^2 = 3^2 = 9) of 3 types; holds up to 18 electrons.
    • n=4n = 4 Shell:
    • Subshell l=0l = 0 (4s4s): ml=0m_l = 0 (one 4s4s orbital).
    • Subshell l=1l = 1 (4p4p): ml=+1,0,−1m_l = +1, 0, -1 (three 4p4p orbitals).
    • Subshell l=2l = 2 (4d4d): ml=+2,+1,0,−1,−2m_l = +2, +1, 0, -1, -2 (five 4d4d orbitals).
    • Subshell l=3l = 3 (4f4f): ml=+3,+2,+1,0,−1,−2,−3m_l = +3, +2, +1, 0, -1, -2, -3 (seven 4f4f orbitals).
    • Total orbitals: 16 orbitals (n2=42=16n^2 = 4^2 = 16) of 4 types; holds up to 32 electrons.

Characteristics and Shapes of Atomic Orbitals

  • ss Orbitals (l=0,ml=0l = 0, m_l = 0):

    • Subshell orbital count: 2l+1=2(0)+1=12l + 1 = 2(0) + 1 = 1 orbital.
    • Extends radially from the nucleus to form a spherical shape.
    • Spherical Nodes:
    • All ss orbitals possess n−1n - 1 spherical radial nodes.
    • A 1s1s orbital has 1−1=01 - 1 = 0 nodes.
    • A 2s2s orbital has 2−1=12 - 1 = 1 node.
    • A 3s3s orbital has 3−1=23 - 1 = 2 nodes, and so forth.
    • A spherical node is a concentric surface of zero probability for finding an electron.
  • pp Orbitals (l=1l = 1):

    • Subshell orbital count: 2l+1=2(1)+1=32l + 1 = 2(1) + 1 = 3 degenerate orbitals (px,py,pzp_x, p_y, p_z).
    • Dumbbell-shaped, oriented mutually perpendicular along the xx, yy, and zz axes at 90∘90^\circ relative to one another.
    • Each pp orbital contains 1 nodal plane (l=1l = 1) passing through the nucleus.
  • dd Orbitals (l=2l = 2):

    • Subshell orbital count: 2l+1=2(2)+1=52l + 1 = 2(2) + 1 = 5 degenerate orbitals.
    • Orbitals possess 2 nodal planes (l=2l = 2).
    • The five dd orbital orientations are dxyd_{xy}, dxzd_{xz}, dyzd_{yz}, dx2−y2d_{x^2-y^2}, and dz2d_{z^2}.
    • The dz2d_{z^2} orbital exhibits a unique shape consisting of two lobes along the zz-axis with a donut-shaped ring (torus) in the xyxy-plane, and is noted for being one of the most reactive orbital configurations.

Quantum orbital spatial structures across n=1 to 7

Electron Spin, Magnetism, and the Pauli Exclusion Principle

  • The Stern-Gerlach Experiment:
    • Conducted by passing a beam of neutral silver atoms from a furnace through an inhomogeneous magnetic field toward a detector screen.
    • Classical Physics Prediction: Predicted a continuous vertical spread/smear of atoms based on classical magnetic moment continuum.
    • Experimental Observation: The atomic beam split into two discrete pathways (two distinct spots).
    • Conclusion: Proved quantization of intrinsic electron angular momentum (electron spin). The two deflection paths demonstrate two distinct spin states affected by the magnetic field (one spinning to the right/clockwise, one to the left/counterclockwise).

Stern-Gerlach Experiment setup showing splitting of silver atom beam

  • Spin Quantum Number (msm_s):

    • Assigned values: ms=±12m_s = \pm \frac{1}{2}.
    • ms=+12m_s = +\frac{1}{2} designates spin-up (↑\uparrow).
    • ms=−12m_s = -\frac{1}{2} designates spin-down (↓\downarrow).
  • Magnetic Properties of Matter:

    • Diamagnetic Substances: Contain no unpaired electrons (all electrons paired). They are NOT attracted to a magnetic field and are weakly repelled.
    • Paramagnetic Substances: Contain one or more unpaired electrons. They ARE attracted into a magnetic field.
  • Pauli Exclusion Principle:

    • Formulated by Wolfgang Pauli in 1925.
    • Definition: No two electrons in the same atom can possess identical sets of all four quantum numbers (n,l,ml,msn, l, m_l, m_s).
    • Consequence: An individual orbital defined by (n,l,ml)(n, l, m_l) can accommodate a maximum of 2 electrons, and they must have opposite spins (+12+\frac{1}{2} and −12-\frac{1}{2}).

Polyelectronic Atoms, Penetration Effect, and Effective Nuclear Charge

  • Polyelectronic Atoms:

    • Refers to any atom possessing more than one electron.
    • Electron Correlation Problem: Because exact electron trajectories cannot be known in quantum mechanics, inter-electronic repulsions cannot be calculated with absolute precision.
  • Subshell Energy Splitting in Multi-Electron Systems:

    • Unlike hydrogen (where subshells in the same principal energy level are degenerate), multi-electron atoms experience energy splitting among subshells within a principal quantum level nn:      Ens<Enp<End<EnfE_{ns} < E_{np} < E_{nd} < E_{nf}
  • The Penetration Effect:

    • An electron in a 2s2s orbital penetrates closer to the nucleus than an electron in a 2p2p orbital.
    • Higher nuclear penetration causes the 2s2s electron to experience a stronger nuclear electrostatic attraction.
    • Consequently, the 2s2s orbital is lower in energy than 2p2p orbitals in a multi-electron atom. The same penetration phenomenon applies across higher quantum levels (e.g., 3s<3p<3d3s < 3p < 3d).
  • Effective Nuclear Charge (Z∗Z^*):

    • Definition: The net positive nuclear charge experienced by a specific electron in a multi-electron atom, reflecting a balance between attraction to the nucleus and repulsions from other (shielding) electrons.
    • Formula: Z∗=Z−SZ^* = Z - S
    • ZZ = atomic number (total proton charge of nucleus).
    • SS = screening/shielding constant (approximated by the number of inner core electrons).
    • Trend across a period: Z∗Z^* increases progressively across a period from left to right due to incomplete shielding of nuclear charge by valence electrons.
    • Examples for 2s electron nuclear charge experience:
    • Lithium (Li\text{Li}, Z=3Z = 3): Z∗≈3−2=1Z^* \approx 3 - 2 = 1
    • Beryllium (Be\text{Be}, Z=4Z = 4): Z∗≈4−2=2Z^* \approx 4 - 2 = 2
    • Boron (B\text{B}, Z=5Z = 5): Z∗≈5−2=3Z^* \approx 5 - 2 = 3
  • Single-Electron vs. Multi-Electron Energy Level Hierarchy:

    • Single-Electron Atom (Hydrogen): Energy depends solely on nn. Orbitals within the same shell are degenerate:          1s<2s=2p<3s=3p=3d<4s=4p=4d=4f1s < 2s = 2p < 3s = 3p = 3d < 4s = 4p = 4d = 4f
    • Multi-Electron Atom: Screening and penetration cause orbital energies to depend on both nn and ll. The energy order follows the n+ln + l rule:
    • 4s4s vs. 3d3d:
      • For 4s4s: n+l=4+0=4n + l = 4 + 0 = 4
      • For 3d3d: n+l=3+2=5n + l = 3 + 2 = 5
      • Because 4+0<3+24 + 0 < 3 + 2, the 4s4s orbital is lower in energy than the 3d3d orbital during ground-state electron filling.

History and Organization of the Periodic Table

  • Historical Development:
    • The periodic table was originally constructed empirically to categorize patterns in observed chemical properties of elements.
    • Mendeleev's Periodic Table:
    • Emphasized using elemental periodic patterns to predict the existence and properties of undiscovered elements.
    • Corrected accepted values for several atomic masses.
    • Modern Periodic Table:
    • Organizes elements sequentially by atomic number (ZZ) rather than atomic mass.

The Aufbau Principle and Electron Configurations

  • **The Aufbau Principle (