Atomic Structure_01.10.2024
Hydrogen Spectrum
Understanding Hydrogen Spectrum
High voltage discharge in hydrogen gas produces a line spectrum
Diffraction grating creates distinct atomic spectral series
Principal quantum numbers denoted as n:
Lyman series (n = 1)
Balmer series (n = 2)
Paschen series (n = 3)
Various wavelengths associated with transitions:
Wavelength values expressed as ( \lambda ) in nm
Example: 820 nm (n=4), 364.56 nm (n=6)
Balmer Series
Characteristics and Measurements
Electric discharge in hydrogen yields 4 intense visible lines and 5 ultraviolet lines
Measured by Huggins with observed wavelengths:
656.28 nm, 486.13 nm, 434.05 nm, 410.17 nm, 364.56 nm
Includes a converging limit in the ultraviolet region
Balmer empirical relation describes the wavelength of spectral lines
Rydberg Formula (1888)
Foundational Concepts
Proposed by Swedish physicist Johannes Rydberg
Generalizes Balmer series relations for other elements
Expressed in terms of series terms and quantum numbers
Five Series of Hydrogen Spectrum
Details of Each Spectrum Series
Lyman:
Series Term: 1, n (2,3,4,5…)
1st line: 122 nm, Converging line: 91 nm
Balmer:
Series Term: 2, n (3,4,5,6…)
1st line: 656 nm, Converging line: 365 nm
Paschen:
Series Term: 3, n (4,5,6,7…)
1st line: 1875 nm, Converging line: 826 nm
Brackett:
Series Term: 4, n (5,6,7…)
1st line: 4050 nm, Converging line: 1458 nm
Pfund:
Series Term: 5, n (6,7,8…)
1st line: 7400 nm, Converging line: 2280 nm
Rydberg Constant Values
Calculations and Discrepancies
Rydberg constant (R): ( R = 1.0973731 \times 10^7 , m^{-1} )
Experimental value: ( 1.0967758 \times 10^7 , m^{-1} )
Discrepancy of ~60 cm^-1 explained by considering electron and nucleus motion about their center of mass
Bohr Model (1911)
Foundations of the Model
Addressed failures of Rutherford model leading to instability of atoms
Based on quantum conditions for the electron's movement in defined orbits
Stability provided by stationary (non-radiating) orbits which do not emit radiation
Angular momentum quantization given by ( mvr = n \frac{h}{2\pi} )
Bohr’s Atomic Model Postulates
Key Postulates
Nucleus at the center with positive charge
Electrons occupy discrete energy levels (not continuous)
Motion controlled by Newtonian principles, leading to stationary orbits
Electrons can emit or absorb radiation during transitions
Energy Relationships in Bohr’s Model
Kinetic and Potential Energy
Total energy of the electron system is given via kinetic and potential energy relations
Energy levels quantized and derived for hydrogen as function of principal quantum numbers
Rydberg Equation & Energies
Link to Electron Energies
Rydberg equation reveals quantized energies for hydrogen’s electron
Energy transitions relate directly to emitted photon frequencies, establishing quantization of electron energies
Bohr Model Merits
Advantages of Bohr’s Model
Explains stability of atoms and origins of spectral lines
Predicts resonant and ionization potentials which align with experimental data
Incorporates isotopic shifts demonstrating robustness in calculations
Aids in understanding electron-proton mass ratio
Evidence Supporting Bohr’s Theory
Observational Facts
Empirical relations confirmed through experimental data
Discovery of heavy hydrogen (deuterium) supported predictions of spectral lines
Quantized energy levels show consistency across various hydrogen lines
Shortcomings of Bohr’s Theory
Limitations Encountered
Fine structure of spectral lines not explained
No information on electron distribution in multi-electron systems
Dual reliance on classical and quantum theories leads to conceptual inconsistencies
Franck & Hertz Experiment
Quantum Nature of Atomic Energy Levels
Experiment involved electric interactions in evacuated and gas-filled tubes
Observed current variations as function of accelerating voltage (Va)
Findings confirmed quantized energy states through specific excitation potentials
Wave Mechanics Overview
Historical Context
The transition from classical to wave-particle duality concepts in physics
Key contributions from Planck, Einstein, de Broglie, Schrödinger leading to quantum mechanics
Wave Packet Concept
Understanding Particles as Waves
Defined through wave functions representing probabilities in space
Represents electron behavior as a quantifiable disturbance in defined regions
Heisenberg uncertainty principle expressed through wave packets ( ext{ΔxΔp} ext{≥} h/2 )
Group vs Phase Velocity
Distinction of Waves
Group velocity relates to a moving particle, while phase velocity pertains to individual wave properties
Wave packets can exhibit varying velocities based on constituent wave frequencies
Conclusion
Synthesis of Quantum Mechanics
Integration of particle and wave theories establishes a robust framework for understanding atomic structures and behavior
Ongoing experimentation and theoretical development continues to validate and expand upon these foundational principles.