. Bohr’s theory and its limitations ii. Dual behavior of matter and radiation iii. De Broglie’s relation iv. Heisenberg’s Uncertainty Principle v. Hydrogen atom spectra vi. Need for a new approach to Atomic Structure (2L) 2 i. Time independent Schrodinger’s Equation; meaning of various terms involved ii. Significance of ψ and ψ² iii. Schrödinger’s equation for hydrogen atom (derivation not required) iv. Radial and angular parts of the hydrogenic wave function (atomic orbital) and their variations for 1s, 2s, 2p, 3s, 3p and 3d orbital (Graphical representation only) v. Radial and angular nodes and their significance. vi. Radial distribution functions and concept of the most Probable distance (special reference to 1s and 2s atomic orbital) vii. Significance of quantum numbers viii. Shapes of s, p and d atomic orbital, ix. Calculation of nodes (angular & radial) for the orbitals. (6L) 3 Aufbau and Pauli exclusion principles, Hund’s multiplicity Rule. (3L) 4 Electronic configurations of the elements, effective nuclear charge. (2L) 5 Modern Periodic Table: General trends in the modern periodic table
Here’s a clean study-outline version of the topics you pasted, organized the way they usually appear in atomic structure / periodicity units.
If you want, I can turn this into any of these next:
2
Bohr’s model explained the spectrum of hydrogen fairly well, but it failed for:
So a new model was needed, based on quantum mechanics.
Radiation sometimes behaves like a wave and sometimes like particles (photons).
Matter also shows both wave and particle behavior.
For light:
E = h\nu
p = \frac{h}{\lambda}
For matter, moving particles also have wave nature.
De Broglie proposed that every moving particle has an associated wavelength:
\lambda = \frac{h}{mv}
where:
This means electrons in atoms can behave like standing waves.
It is impossible to measure both position and momentum of a particle exactly at the same time.
\Delta x \cdot \Delta p \ge \frac{h}{4\pi}
So an electron cannot be said to move in a fixed circular orbit as Bohr assumed. We can only talk about the probability of finding it in a region.
When electrons in hydrogen move between energy levels, they emit or absorb light of specific wavelengths.
This gives line spectra rather than continuous spectra.
Main series:
The spectral lines show that electron energy is quantized.
Bohr’s model could not explain:
Hence the quantum mechanical model was developed, where the electron is described by a wave function \psi, not a definite path.
For a particle in a potential field:
-\frac{h^2}{8\pi^2 m}\nabla^2 \psi + V\psi = E\psi
where:
This equation is used to find allowed energy states and wave functions of electrons.
So orbitals are regions of high probability, not fixed paths.
For hydrogen, the electron moves under attraction of the nucleus, and solving Schrödinger’s equation gives:
The exact derivation is not required here, only the result and significance.
The wave function can be separated into:
This gives the shape of orbitals.
For orbitals:
A node is a region where probability of finding the electron is zero.
For an orbital:
where:
Examples:
The radial distribution function tells the probability of finding an electron at a certain distance from the nucleus.
It is important because electron density is spread over space, not at one point.
For hydrogen:
This helps explain why electrons in s-orbitals are often found close to the nucleus.
Quantum numbers describe the state of an electron.
Electrons fill orbitals starting from lower energy to higher energy.
Order of filling:
1s < 2s < 2p < 3s < 3p < 4s < 3d < 4p < 5s \dots
No two electrons in an atom can have the same set of four quantum numbers.
So one orbital can hold a maximum of 2 electrons with opposite spins.
In orbitals of equal energy, electrons occupy them singly first with parallel spins before pairing up.
This gives maximum stability.
Electronic configuration tells how electrons are distributed among orbitals.
Example:
In multi-electron atoms, outer electrons do not feel the full nuclear charge because inner electrons shield them.
Effective nuclear charge:
Z_{eff} = Z - S
where:
This affects atomic size, ionization energy, and electronegativity.
Across a period:
Down a group:
These trends are due to changes in shell number and shielding.
If you want, I can turn this into a 1-page revision sheet or 10-mark answer format next.
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