Atomic structure and periodicity are like a lock and key, electron configuration determines where elements fit in the periodic table: Electron shell filling follows the Aufbau principle, explaining why the periodic table has its characteristic shape
Why it matters: Connecting atomic structure to periodicity enables prediction of chemical behavior across the entire table
The key insight: Electron shell filling follows the Aufbau principle, explaining why the periodic table has its characteristic shape
Atoms consist of three subatomic particles. Their properties define the behaviour of every element:
Property Proton Neutron Electron Symbol p + p^+ p + n 0 n^0 n 0 e − e^- e − Relative mass 1 1 1 1 1 1 ≈ 1 / 1836 \approx 1/1836 ≈ 1/1836 Actual mass (u) 1.00728 1.00728 1.00728 1.00867 1.00867 1.00867 0.00055 0.00055 0.00055 Charge + 1 +1 + 1 0 0 0 − 1 -1 − 1 Location Nucleus Nucleus Electron shells
Definition. The atomic number (Z Z Z ) is the number of protons in the nucleus. It uniquely Identifies an element.
Definition. The mass number (A A A ) is the total number of protons and neutrons in the Nucleus:
A = Z + N A = Z + N A = Z + N Where N N N is the neutron number.
Definition. A nuclide is a specific atom characterised by its atomic number, mass number, And energy state, denoted as \prescript A Z X \prescript{A}{Z}\mathrm{X} \prescript A Z X .
Definition. Isotopes are atoms of the same element (same Z Z Z ) with different numbers of Neutrons (different A A A ).
Isotopes have identical chemical properties (same electron configuration) but different physical Properties (different mass, different nuclear stability).
Element Isotope Z Z Z A A A N N N Natural Abundance Hydrogen H \mathrm{H} H (protium)1 1 1 1 1 1 0 0 0 99.985 % 99.985\% 99.985% Hydrogen D \mathrm{D} D (deuterium)1 1 1 2 2 2 1 1 1 0.015 % 0.015\% 0.015% Hydrogen T \mathrm{T} T (tritium)1 1 1 3 3 3 2 2 2 Trace (radioactive) Carbon C \mathrm{C} C -126 6 6 12 12 12 6 6 6 98.89 % 98.89\% 98.89% Carbon C \mathrm{C} C -136 6 6 13 13 13 7 7 7 1.11 % 1.11\% 1.11% Carbon C \mathrm{C} C -146 6 6 14 14 14 8 8 8 Trace (radioactive) Chlorine C l \mathrm{Cl} Cl -3517 17 17 35 35 35 18 18 18 75.77 % 75.77\% 75.77% Chlorine C l \mathrm{Cl} Cl -3717 17 17 37 37 37 20 20 20 24.23 % 24.23\% 24.23%
Definition. The relative atomic mass (A r A_r A r ) is the weighted average mass of an atom of an Element relative to 1 / 12 1/12 1/12 the mass of a carbon-12 atom, taking into account the natural abundances of all isotopes.
A r = ∑ i ( i s o t o p e m a s s ) i × ( f r a c t i o n a l a b u n d a n c e ) i A_r = \sum_{i} (\mathrm{isotope mass})_i \times (\mathrm{fractional abundance})_i A r = i ∑ ( isotopemass ) i × ( fractionalabundance ) i Example, Chlorine
Chlorine has two occurring isotopes: C l \mathrm{Cl} Cl -35 (75.77 % 75.77\% 75.77% mass ≈ 34.97 u \approx 34.97\mathrm{ u} ≈ 34.97 u ) and C l \mathrm{Cl} Cl -37 (24.23 % 24.23\% 24.23% mass ≈ 36.97 u \approx 36.97\mathrm{ u} ≈ 36.97 u ).
A r = ( 34.97 × 0.7577 ) + ( 36.97 × 0.2423 ) = 26.50 + 8.96 = 35.46 A_r = (34.97 \times 0.7577) + (36.97 \times 0.2423) = 26.50 + 8.96 = 35.46 A r = ( 34.97 × 0.7577 ) + ( 36.97 × 0.2423 ) = 26.50 + 8.96 = 35.46 The nucleus is extremely small relative to the atom (≈ 10 − 15 m \approx 10^{-15}\mathrm{ m} ≈ 1 0 − 15 m diameter vs ≈ 10 − 10 m \approx 10^{-10}\mathrm{ m} ≈ 1 0 − 10 m for the atom). It contains over 99.9 % 99.9\% 99.9% of the atom”s mass. Nuclear Stability depends on the neutron-to-proton ratio:
Light elements (Z < 20 Z \lt 20 Z < 20 ): stable when N ≈ Z N \approx Z N ≈ Z Heavier elements: stable when N > Z N \gt Z N > Z (neutrons provide additional strong nuclear force to counteract electrostatic repulsion between protons) The classical Rutherford-Bohr model failed to explain several observations:
Discrete emission line spectra (not continuous) The stability of atoms (classically, orbiting electrons should radiate energy and spiral in) The photoelectric effect These required a quantum mechanical treatment where electron energy is quantised.
Electrons occupy shells (principal energy levels) labelled n = 1 , 2 , 3 , … n = 1, 2, 3, \ldots n = 1 , 2 , 3 , …
Each shell contains subshells, designated by the azimuthal quantum number l l l :
n n n Subshells (l l l values) Maximum electrons 1 1 1 1 s 1s 1 s 2 2 2 2 2 2 2 s 2s 2 s , 2 p 2p 2 p 8 8 8 3 3 3 3 s 3s 3 s , 3 p 3p 3 p , 3 d 3d 3 d 18 18 18 4 4 4 4 s 4s 4 s , 4 p 4p 4 p , 4 d 4d 4 d , 4 f 4f 4 f 32 32 32
The maximum number of electrons in shell n n n is 2 n 2 2n^2 2 n 2 .
Definition. An orbital is a region of space where there is a high probability (≥ 90 % \ge 90\% ≥ 90% ) Of finding an electron. Each orbital holds a maximum of two electrons with opposite spins.
Subshell Number of orbitals Max electrons Orbital shape s s s 1 1 1 2 2 2 Spherical p p p 3 3 3 6 6 6 Dumbbell d d d 5 5 5 10 10 10 Cloverleaf f f f 7 7 7 14 14 14 Complex (multi-lobed)
Each electron in an atom is described by four quantum numbers:
Quantum Number Symbol What it specifies Allowed values Principal n n n Energy level (shell) 1 , 2 , 3 , … 1, 2, 3, \ldots 1 , 2 , 3 , … Azimuthal l l l Subshell shape 0 , 1 , 2 , … , n − 1 0, 1, 2, \ldots, n-1 0 , 1 , 2 , … , n − 1 Magnetic m l m_l m l Orbital orientation in space − l , − l + 1 , … , 0 , … , l − 1 , l -l, -l+1, \ldots, 0, \ldots, l-1, l − l , − l + 1 , … , 0 , … , l − 1 , l Spin m s m_s m s Electron spin direction + 1 2 +\frac{1}{2} + 2 1 or − 1 2 -\frac{1}{2} − 2 1
The number of orbitals in a subshell is 2 l + 1 2l + 1 2 l + 1 .
Example: Quantum numbers for a 3 p 3p 3 p electron
For the 3 p 3p 3 p subshell: n = 3 n = 3 n = 3 , l = 1 l = 1 l = 1 , m l = − 1 , 0 , + 1 m_l = -1, 0, +1 m l = − 1 , 0 , + 1 , m s = ± 1 2 m_s = \pm\frac{1}{2} m s = ± 2 1 .
This gives three p p p -orbitals (p x p_x p x , p y p_y p y , p z p_z p z ), each holding two electrons, for a total of six 3 p 3p 3 p electrons.
Three rules govern how electrons fill orbitals:
Aufbau principle : Electrons fill orbitals starting from the lowest energy level upwards.Pauli exclusion principle : No two electrons in the same atom can have identical sets of four quantum numbers. Each orbital holds a maximum of two electrons with opposite spins.Hund’s rule : Within a subshell, electrons occupy degenerate orbitals singly first, with parallel spins, before pairing up.The filling order follows the ( n + l ) (n + l) ( n + l ) rule: orbitals with a lower ( n + l ) (n + l) ( n + l ) value fill first. When ( n + l ) (n + l) ( n + l ) values are equal, the orbital with lower n n n fills first.
1 s < 2 s < 2 p < 3 s < 3 p < 4 s < 3 d < 4 p < 5 s < 4 d < 5 p < 6 s < 4 f < 5 d < 6 p < 7 s < 5 f < 6 d < 7 p 1s \lt 2s \lt 2p \lt 3s \lt 3p \lt 4s \lt 3d \lt 4p \lt 5s \lt 4d \lt 5p \lt 6s \lt 4f \lt 5d \lt 6p \lt 7s \lt 5f \lt 6d \lt 7p 1 s < 2 s < 2 p < 3 s < 3 p < 4 s < 3 d < 4 p < 5 s < 4 d < 5 p < 6 s < 4 f < 5 d < 6 p < 7 s < 5 f < 6 d < 7 p Full notation , write every subshell explicitly:
F e : 1 s 2 2 s 2 2 p 6 3 s 2 3 p 6 4 s 2 3 d 6 \mathrm{Fe}: 1s^2\, 2s^2\, 2p^6\, 3s^2\, 3p^6\, 4s^2\, 3d^6 Fe : 1 s 2 2 s 2 2 p 6 3 s 2 3 p 6 4 s 2 3 d 6 Noble gas core notation , replace the inner-shell electrons with the preceding noble gas symbol In brackets:
F e : [ A r ] 4 s 2 3 d 6 \mathrm{Fe}: [\mathrm{Ar}]\, 4s^2\, 3d^6 Fe : [ Ar ] 4 s 2 3 d 6 Caution
3 d 6 4 s 2 3d^6\, 4s^2 3 d 6 4 s 2 ). When writing configurations for ions, remove electrons from the highest n n n value First: F e 2 + \mathrm{Fe}^{2+} Fe 2 + is [ A r ] 3 d 6 [\mathrm{Ar}]\, 3d^6 [ Ar ] 3 d 6 Not [ A r ] 4 s 2 3 d 4 [\mathrm{Ar}]\, 4s^2\, 3d^4 [ Ar ] 4 s 2 3 d 4 .
Half-filled and fully-filled d d d -subshells are more stable due to symmetry and exchange energy. This causes exceptions in chromium, copper, molybdenum, silver, and gold:
Element Expected configuration Actual configuration Reason C r \mathrm{Cr} Cr [ A r ] 4 s 2 3 d 4 [\mathrm{Ar}]\, 4s^2\, 3d^4 [ Ar ] 4 s 2 3 d 4 [ A r ] 4 s 1 3 d 5 [\mathrm{Ar}]\, 4s^1\, 3d^5 [ Ar ] 4 s 1 3 d 5 Half-filled d d d -subshell C u \mathrm{Cu} Cu [ A r ] 4 s 2 3 d 9 [\mathrm{Ar}]\, 4s^2\, 3d^9 [ Ar ] 4 s 2 3 d 9 [ A r ] 4 s 1 3 d 10 [\mathrm{Ar}]\, 4s^1\, 3d^{10} [ Ar ] 4 s 1 3 d 10 Fully-filled d d d -subshell M o \mathrm{Mo} Mo [ K r ] 5 s 2 4 d 4 [\mathrm{Kr}]\, 5s^2\, 4d^4 [ Kr ] 5 s 2 4 d 4 [ K r ] 5 s 1 4 d 5 [\mathrm{Kr}]\, 5s^1\, 4d^5 [ Kr ] 5 s 1 4 d 5 Half-filled d d d -subshell A g \mathrm{Ag} Ag [ K r ] 5 s 2 4 d 9 [\mathrm{Kr}]\, 5s^2\, 4d^9 [ Kr ] 5 s 2 4 d 9 [ K r ] 5 s 1 4 d 10 [\mathrm{Kr}]\, 5s^1\, 4d^{10} [ Kr ] 5 s 1 4 d 10 Fully-filled d d d -subshell A u \mathrm{Au} Au [ X e ] 6 s 2 4 f 14 5 d 9 [\mathrm{Xe}]\, 6s^2\, 4f^{14}\, 5d^9 [ Xe ] 6 s 2 4 f 14 5 d 9 [ X e ] 6 s 1 4 f 14 5 d 10 [\mathrm{Xe}]\, 6s^1\, 4f^{14}\, 5d^{10} [ Xe ] 6 s 1 4 f 14 5 d 10 Fully-filled d d d -subshell
Orbital diagrams represent electrons as arrows in boxes (one box per orbital). Up and down arrows Represent m s = + 1 2 m_s = +\frac{1}{2} m s = + 2 1 and m s = − 1 2 m_s = -\frac{1}{2} m s = − 2 1 .
For nitrogen (1 s 2 2 s 2 2 p 3 1s^2\, 2s^2\, 2p^3 1 s 2 2 s 2 2 p 3 ):
\begin`\{array}`{c} 1s\quad \boxed{\uparrow\downarrow} \\ 2s\quad \boxed{\uparrow\downarrow} \\ 2p\quad \boxed{\uparrow}\quad\boxed{\uparrow}\quad\boxed{\uparrow} \end`\{array}` All three 2 p 2p 2 p electrons are unpaired with parallel spins, following Hund’s rule.
The periodic table arranges elements in order of increasing atomic number. The layout reflects the electron configurations of the elements.
Feature Description Periods Horizontal rows; number = principal quantum number n n n of the valence shell Groups Vertical columns; elements share similar valence electron configurations Blocks Regions corresponding to the subshell being filled
Block Subshell being filled Groups Examples s s s n s 1 ns^1 n s 1 to n s 2 ns^2 n s 2 1$$2 H, He, Li, Na, Mg, Ca p p p n p 1 np^1 n p 1 to n p 6 np^6 n p 6 13 13 13 —18 18 18 B, C, N, O, F, Ne, Cl, Ar d d d ( n − 1 ) d 1 (n-1)d^1 ( n − 1 ) d 1 to ( n − 1 ) d 10 (n-1)d^{10} ( n − 1 ) d 10 3 3 3 —12 12 12 Sc, Ti, Fe, Cu, Zn f f f ( n − 2 ) f 1 (n-2)f^1 ( n − 2 ) f 1 to ( n − 2 ) f 14 (n-2)f^{14} ( n − 2 ) f 14 Lanthanides/Actinides Ce, Th, U
The IB uses IUPAC group numbers 1 1 1 —18 18 18 :
IUPAC Group Common Name Valence electrons 1 1 1 Alkali metals n s 1 ns^1 n s 1 2 2 2 Alkaline earth metals n s 2 ns^2 n s 2 13 13 13 Boron group n s 2 n p 1 ns^2\, np^1 n s 2 n p 1 14 14 14 Carbon group n s 2 n p 2 ns^2\, np^2 n s 2 n p 2 15 15 15 Nitrogen group n s 2 n p 3 ns^2\, np^3 n s 2 n p 3 16 16 16 Oxygen group n s 2 n p 4 ns^2\, np^4 n s 2 n p 4 17 17 17 Halogens n s 2 n p 5 ns^2\, np^5 n s 2 n p 5 18 18 18 Noble gases n s 2 n p 6 ns^2\, np^6 n s 2 n p 6 (except He: 1 s 2 1s^2 1 s 2 )
Definition. The effective nuclear charge (Z e f f Z_{\mathrm{eff}} Z eff ) is the net positive charge Experienced by an electron, after accounting for shielding by other electrons:
Z e f f = Z − S Z_{\mathrm{eff}} = Z - S Z eff = Z − S Where Z Z Z is the actual nuclear charge and S S S is the shielding constant.
Shielding is the reduction in the attractive force between the nucleus and an electron due to Repulsion by other electrons. Inner-shell electrons shield outer-shell electrons far more effectively than electrons in the same shell.
Trend Explanation Decreases across a period Z e f f Z_{\mathrm{eff}} Z eff increases; electrons are pulled closer to the nucleusIncreases down a group Additional electron shells increase the average distance from the nucleus
Definition. Atomic radius is half the distance between the nuclei of two bonded atoms of the Same element.
For noble gases, atomic radius is taken as the van der Waals radius (half the distance between nuclei of adjacent atoms in the solid or liquid), which is significantly larger than covalent radii.
Trend Explanation Cations are smaller than their parent atoms Fewer electron-electron repulsions; same Z Z Z pulling fewer electrons Anions are larger than their parent atoms Increased electron-electron repulsion with the same Z Z Z Ionic radius increases down a group Additional shells Across a period, ions decrease in size Isoelectronic series: same number of electrons, increasing Z Z Z
Example, Isoelectronic series
O 2 − > F − > N a + > M g 2 + > A l 3 + \mathrm{O}^{2-} \gt \mathrm{F}^- \gt \mathrm{Na}^+ \gt \mathrm{Mg}^{2+} \gt \mathrm{Al}^{3+} O 2 − > F − > Na + > Mg 2 + > Al 3 +
All have the neon configuration (1s^2\, 2s^2\, 2p^6$$10 electrons). The nuclear charge increases from Z = 8 Z = 8 Z = 8 to Z = 13 Z = 13 Z = 13 So the radius decreases.
Definition. The first ionization energy (I E 1 IE_1 I E 1 ) is the minimum energy required to remove One mole of electrons from one mole of gaseous atoms:
X ( g ) → X + ( g ) + e − Δ H = I E 1 \mathrm{X}(g) \to \mathrm{X}^+(g) + e^- \qquad \Delta H = IE_1 X ( g ) → X + ( g ) + e − Δ H = I E 1 Trend Explanation Increases across a period Z e f f Z_{\mathrm{eff}} Z eff increases; electrons held more tightlyDecreases down a group Electrons are farther from the nucleus and more shielded
Deviations from the general trend across a period:
Deviation Element pair Explanation Drop from Group 2 2 2 to 13 13 13 Be → \to → B Be: 2 s 2 2s^2 2 s 2 (stable filled subshell); B: 2 p 1 2p^1 2 p 1 (easier to remove) Drop from Group 15 15 15 to 16 16 16 N → \to → O N: 2 p 3 2p^3 2 p 3 (half-filled, stable); O: 2 p 4 2p^4 2 p 4 (paired electron in 2 p 2p 2 p experiences repulsion)
Each subsequent ionization energy is larger than the previous one because the remaining electrons Experience less shielding from a shrinking electron cloud and are held by a constant Z Z Z :
I E 1 < I E 2 < I E 3 < ⋯ IE_1 \lt IE_2 \lt IE_3 \lt \cdots I E 1 < I E 2 < I E 3 < ⋯ A large jump in successive ionization energies indicates the removal of an electron from a new inner Shell. This reveals the electron configuration.
Example, Aluminium
For aluminium (1 s 2 2 s 2 2 p 6 3 s 2 3 p 1 1s^2\, 2s^2\, 2p^6\, 3s^2\, 3p^1 1 s 2 2 s 2 2 p 6 3 s 2 3 p 1 ):
I E 1 = 578 k J / m o l IE_1 = 578\mathrm{ kJ/mol} I E 1 = 578 kJ/mol (removes 3 p 3p 3 p electron)I E 2 = 1817 k J / m o l IE_2 = 1817\mathrm{ kJ/mol} I E 2 = 1817 kJ/mol (removes 3 s 3s 3 s electron)I E 3 = 2745 k J / m o l IE_3 = 2745\mathrm{ kJ/mol} I E 3 = 2745 kJ/mol (removes 3 s 3s 3 s electron)I E 4 = 11577 k J / m o l IE_4 = 11577\mathrm{ kJ/mol} I E 4 = 11577 kJ/mol (removes 2 p 2p 2 p electron, large jump!)The jump from I E 3 IE_3 I E 3 to I E 4 IE_4 I E 4 confirms that aluminium has three valence electrons.
Definition. Electron affinity (E A EA E A ) is the enthalpy change when one mole of electrons is Added to one mole of gaseous atoms:
X ( g ) + e − → X − ( g ) Δ H = E A \mathrm{X}(g) + e^- \to \mathrm{X}^-(g) \qquad \Delta H = EA X ( g ) + e − → X − ( g ) Δ H = E A A more negative E A EA E A indicates a greater tendency to accept an electron.
Trend Explanation Generally becomes more negative across a period Increasing Z e f f Z_{\mathrm{eff}} Z eff attracts electrons more strongly Generally becomes less negative down a group Increased distance and shielding reduce the nuclear pull
Noble gases have positive (endothermic) electron affinities because the added electron enters a new, Higher-energy subshell.
Definition. Electronegativity is the ability of an atom to attract the shared pair of Electrons in a covalent bond. The Pauling scale is the most common.
Trend Explanation Increases across a period Increasing Z e f f Z_{\mathrm{eff}} Z eff Decreases down a group Increased distance and shielding
Scale Most electronegative Least electronegative Pauling F (3.98 3.98 3.98 ) Fr (0.7 0.7 0.7 )
Trend Metallic character Non-metallic character Across a period Decreases Increases Down a group Increases Decreases
Metallic character correlates with low ionization energy, low electronegativity, and large atomic Radius. Non-metallic character correlates with high ionization energy, high electronegativity, and small atomic radius.
Property Across a period (left to right) Down a group (top to bottom) Atomic radius Decreases Increases Ionic radius Decreases (isoelectronic) Increases Ionization energy Increases Decreases Electron affinity More negative Less negative Electronegativity Increases Decreases Metallic character Decreases Increases Non-metallic character Increases Decreases
Property Trend down the group Melting point Decreases (Cs is below room temp in some conditions) Boiling point Decreases Density Generally increases (Li, K anomalies) Atomic radius Increases Softness Increases (softer metals)
All alkali metals have the outer electron configuration n s 1 ns^1 n s 1 . The single valence electron is lost, forming M + \mathrm{M}^+ M + ions.
2 M ( s ) + 2 H 2 O ( l ) → 2 M O H ( a q ) + H 2 ( g ) 2\mathrm{M}(s) + 2\mathrm{H}_2\mathrm{O}(l) \to 2\mathrm{MOH}(aq) + \mathrm{H}_2(g) 2 M ( s ) + 2 H 2 O ( l ) → 2 MOH ( a q ) + H 2 ( g ) Reactivity increases down the group:
Metal Observation Li Steady fizzing; moves on surface Na Rapid fizzing; melts into a ball; may ignite H2 _2 2 K Ignites immediately with a lilac flame Rb, Cs Explosive reaction; often thrown from the water
Explanation of trend : Ionization energy decreases down the group. The valence electron is Farther from the nucleus and more shielded, so less energy is required to remove it.
Alkali metals burn in oxygen to form oxides:
Metal Product with limited O2 _2 2 Product with excess O2 _2 2 Li L i 2 O \mathrm{Li}_2\mathrm{O} Li 2 O (oxide)L i 2 O \mathrm{Li}_2\mathrm{O} Li 2 O Na N a 2 O \mathrm{Na}_2\mathrm{O} Na 2 O (oxide)N a 2 O 2 \mathrm{Na}_2\mathrm{O}_2 Na 2 O 2 (peroxide)K K 2 O 2 \mathrm{K}_2\mathrm{O}_2 K 2 O 2 (peroxide)K O 2 \mathrm{KO}_2 KO 2 (superoxide)Rb, Cs Superoxides form readily Superoxides
All Group 1 hydroxides (M O H \mathrm{MOH} MOH ) are strong bases and highly soluble in water:
M O H ( s ) → M + ( a q ) + O H − ( a q ) \mathrm{MOH}(s) \to \mathrm{M}^+(aq) + \mathrm{OH}^-(aq) MOH ( s ) → M + ( a q ) + OH − ( a q ) Basicity increases down the group (solubility increases, so [ O H − ] [\mathrm{OH}^-] [ OH − ] is higher).
Alkali metal ions produce characteristic flame colours due to electron transitions:
Ion Flame colour L i + \mathrm{Li}^+ Li + Crimson red N a + \mathrm{Na}^+ Na + Yellow K + \mathrm{K}^+ K + Lilac (viewed through cobalt glass to filter Na) R b + \mathrm{Rb}^+ Rb + Red-violet C s + \mathrm{Cs}^+ Cs + Blue
Metal Use Li Batteries, psychiatric medication (lithium carbonate) Na Street lamps (Na vapour), NaK coolant K Fertilisers (K N O 3 \mathrm{KNO}_3 KNO 3 ), potash
Property Trend down the group Melting point Increases Boiling point Increases Atomic radius Increases State at RT F2 _2 2 Cl2 _2 2 (gas); Br2 _2 2 (liquid); I2 _2 2 (solid) Colour Pale yellow → \to → yellow-green → \to → red-brown → \to → dark grey Volatility Decreases
The increase in melting and boiling points down the group is due to increasing London dispersion Forces as the number of electrons (and therefore polarizability) increases.
All halogens have the outer electron configuration n s 2 n p 5 ns^2\, np^5 n s 2 n p 5 . They gain one electron to form X − \mathrm{X}^- X − ions, achieving a noble gas configuration.
Reactivity decreases down the group. This is because atomic radius increases and Z e f f Z_{\mathrm{eff}} Z eff on the incoming electron decreases, so electron affinity becomes less favourable.
F 2 > C l 2 > B r 2 > I 2 \mathrm{F}_2 \gt \mathrm{Cl}_2 \gt \mathrm{Br}_2 \gt \mathrm{I}_2 F 2 > Cl 2 > Br 2 > I 2 A more reactive halogen displaces a less reactive halogen from its halide solution:
C l 2 ( a q ) + 2 K B r ( a q ) → 2 K C l ( a q ) + B r 2 ( a q ) \mathrm{Cl}_2(aq) + 2\mathrm{KBr}(aq) \to 2\mathrm{KCl}(aq) + \mathrm{Br}_2(aq) Cl 2 ( a q ) + 2 KBr ( a q ) → 2 KCl ( a q ) + Br 2 ( a q ) B r 2 ( a q ) + 2 K I ( a q ) → 2 K B r ( a q ) + I 2 ( a q ) \mathrm{Br}_2(aq) + 2\mathrm{KI}(aq) \to 2\mathrm{KBr}(aq) + \mathrm{I}_2(aq) Br 2 ( a q ) + 2 KI ( a q ) → 2 KBr ( a q ) + I 2 ( a q ) C l 2 ( a q ) + 2 K I ( a q ) → 2 K C l ( a q ) + I 2 ( a q ) \mathrm{Cl}_2(aq) + 2\mathrm{KI}(aq) \to 2\mathrm{KCl}(aq) + \mathrm{I}_2(aq) Cl 2 ( a q ) + 2 KI ( a q ) → 2 KCl ( a q ) + I 2 ( a q ) But: B r 2 \mathrm{Br}_2 Br 2 cannot displace C l − \mathrm{Cl}^- Cl − and I 2 \mathrm{I}_2 I 2 cannot displace B r − \mathrm{Br}^- Br − or C l − \mathrm{Cl}^- Cl − .
2 M ( s ) + X 2 ( g ) → 2 M X ( s ) 2\mathrm{M}(s) + \mathrm{X}_2(g) \to 2\mathrm{MX}(s) 2 M ( s ) + X 2 ( g ) → 2 MX ( s ) These are vigorous, exothermic reactions forming ionic halides.
Halide Reagent Observation C l − \mathrm{Cl}^- Cl − A g N O 3 \mathrm{AgNO}_3 AgNO 3 (aq) + dilute HNO3 _3 3 White precipitate (A g C l \mathrm{AgCl} AgCl ), soluble in dilute NH3 _3 3 B r − \mathrm{Br}^- Br − A g N O 3 \mathrm{AgNO}_3 AgNO 3 (aq) + dilute HNO3 _3 3 Cream precipitate (A g B r \mathrm{AgBr} AgBr ), partially soluble in NH3 _3 3 I − \mathrm{I}^- I − A g N O 3 \mathrm{AgNO}_3 AgNO 3 (aq) + dilute HNO3 _3 3 Yellow precipitate (A g I \mathrm{AgI} AgI ), insoluble in NH3 _3 3
Dilute HNO3 _3 3 is added first to remove any carbonate or hydroxide ions that would also form Precipitates with A g + \mathrm{Ag}^+ Ag + .
Halogen Use F 2 \mathrm{F}_2 F 2 Fluoridation of water, Teflon (PTFE) production C l 2 \mathrm{Cl}_2 Cl 2 Water purification, PVC, bleach (N a C l O \mathrm{NaClO} NaClO ) B r 2 \mathrm{Br}_2 Br 2 Flame retardants, brominated compounds, photography I 2 \mathrm{I}_2 I 2 Antiseptics, iodised salt, thyroid hormone synthesis
Definition. Interhalogens are compounds formed between two different halogen atoms. The more Electronegative halogen is the negative end of the molecule.
General formula: X X n ′ \mathrm{XX}'_n XX n ′ where n = 1 , 3 , 5 , 7 n = 1, 3, 5, 7 n = 1 , 3 , 5 , 7 (depending on the size of the central Halogen).
Example Type Structure C l F \mathrm{ClF} ClF Diatomic Linear B r F 3 \mathrm{BrF}_3 BrF 3 Triatomic T-shaped I F 5 \mathrm{IF}_5 IF 5 Pentaatomic Square pyramidal I F 7 \mathrm{IF}_7 IF 7 Heptaatomic Pentagonal bipyramidal
Interhalogens are generally more reactive than the parent halogens because the bonds are polar.
Noble gases have complete valence shells (n s 2 n p 6 ns^2\, np^6 n s 2 n p 6 Except He which is 1 s 2 1s^2 1 s 2 ), making them Chemically inert under standard conditions. They exist as monatomic gases.
Element Configuration Boiling point (K) First IE (kJ/mol) He 1 s 2 1s^2 1 s 2 4.2 4.2 4.2 2372 2372 2372 Ne [ H e ] 2 s 2 2 p 6 [\mathrm{He}]\, 2s^2\, 2p^6 [ He ] 2 s 2 2 p 6 27.1 27.1 27.1 2081 2081 2081 Ar [ N e ] 3 s 2 3 p 6 [\mathrm{Ne}]\, 3s^2\, 3p^6 [ Ne ] 3 s 2 3 p 6 87.3 87.3 87.3 1521 1521 1521 Kr [ A r ] 4 s 2 4 p 6 [\mathrm{Ar}]\, 4s^2\, 4p^6 [ Ar ] 4 s 2 4 p 6 119.8 119.8 119.8 1351 1351 1351 Xe [ K r ] 5 s 2 5 p 6 [\mathrm{Kr}]\, 5s^2\, 5p^6 [ Kr ] 5 s 2 5 p 6 165.0 165.0 165.0 1170 1170 1170 Rn [ X e ] 6 s 2 6 p 6 [\mathrm{Xe}]\, 6s^2\, 6p^6 [ Xe ] 6 s 2 6 p 6 211.0 211.0 211.0 1037 1037 1037
Boiling points increase down the group because the number of electrons increases, leading to stronger London dispersion forces between atoms. The only intermolecular force in noble gases is London dispersion.
Under extreme conditions, the heavier noble gases can form compounds:
Xenon forms \mathrm{XeF}_2$$\mathrm{XeF}_4$$\mathrm{XeF}_6$$\mathrm{XeO}_3 X e O 4 \mathrm{XeO}_4 XeO 4 Krypton forms K r F 2 \mathrm{KrF}_2 KrF 2 (extremely reactive)Argon forms very unstable compounds under extreme conditionsXenon compounds exist because its ionization energy is low enough that highly electronegative Fluorine and oxygen can remove or share electrons.
Noble Gas Use He Balloons, cryogenics, helium-neon lasers, deep-sea diving gas mix Ne Neon signs (orange-red glow) Ar Inert atmosphere for welding, light bulbs Kr High-performance lighting, photography flash lamps Xe Xenon lamps (used in IMAX projectors, car headlights), ion propulsion
Definition. A transition metal is an element that has a partially filled d d d -subshell in Either its atom or any of its common oxidation states.
This definition excludes scandium (S c 3 + \mathrm{Sc}^{3+} Sc 3 + : [ A r ] [\mathrm{Ar}] [ Ar ] ) and zinc (Z n 2 + \mathrm{Zn}^{2+} Zn 2 + : [ A r ] 3 d 10 [\mathrm{Ar}]\, 3d^{10} [ Ar ] 3 d 10 ) as transition metals in their common oxidation States, though they are in the d d d -block.
Property Typical behaviour of transition metals Melting/boiling points High (strong metallic bonding from d d d -electrons) Density High Hardness Hard Electrical conductivity Good conductors Malleability Malleable and ductile
Transition metals can lose different numbers of d d d -electrons to form ions with different charges. This is because the 3 d 3d 3 d and 4 s 4s 4 s energy levels are close in energy.
Element Common oxidation states Ti + 2 , + 3 , + 4 +2, +3, +4 + 2 , + 3 , + 4 V + 2 , + 3 , + 4 , + 5 +2, +3, +4, +5 + 2 , + 3 , + 4 , + 5 Cr + 2 , + 3 , + 6 +2, +3, +6 + 2 , + 3 , + 6 Mn + 2 , + 3 , + 4 , + 6 , + 7 +2, +3, +4, +6, +7 + 2 , + 3 , + 4 , + 6 , + 7 Fe + 2 , + 3 +2, +3 + 2 , + 3 Co + 2 , + 3 +2, +3 + 2 , + 3 Cu + 1 , + 2 +1, +2 + 1 , + 2
Trend : The maximum oxidation state increases across the period to manganese (+ 7 +7 + 7 ) then Decreases. Higher oxidation states become more stable with oxygen (oxoanions) than with water.
Definition. A complex ion consists of a central metal ion surrounded by ligands coordinated Via coordinate (dative covalent) bonds.
[ C u ( H 2 O ) 6 ] 2 + , [ A g ( N H 3 ) 2 ] + , [ F e ( C N ) 6 ] 4 − [\mathrm{Cu}(\mathrm{H}_2\mathrm{O})_6]^{2+}, \quad [\mathrm{Ag}(\mathrm{NH}_3)_2]^+, \quad [\mathrm{Fe}(\mathrm{CN})_6]^{4-} [ Cu ( H 2 O ) 6 ] 2 + , [ Ag ( NH 3 ) 2 ] + , [ Fe ( CN ) 6 ] 4 − Definition. A ligand is a molecule or ion that can donate a lone pair of electrons to a Central metal ion to form a coordinate bond.
Type of ligand Examples Denticity Bonds donated Monodentate \mathrm{H}_2\mathrm{O}$$\mathrm{NH}_3$$\mathrm{Cl}^-$$\mathrm{CN}^- 1 1 1 1 1 1 Bidentate Ethylenediamine (en), oxalate (C 2 O 4 2 − \mathrm{C}_2\mathrm{O}_4^{2-} C 2 O 4 2 − ) 2 2 2 2 2 2 Hexadentate EDTA (E D T A 4 − \mathrm{EDTA}^{4-} EDTA 4 − ) 6 6 6 6 6 6
Definition. The coordination number is the total number of coordinate bonds from ligands to The central metal ion.
Coordination number Geometry Example 4 4 4 Tetrahedral [ C o C l 4 ] 2 − [\mathrm{CoCl}_4]^{2-} [ CoCl 4 ] 2 − 4 4 4 Square planar [ C u ( N H 3 ) 4 ] 2 + [\mathrm{Cu(NH}_3)_4]^{2+} [ Cu ( NH 3 ) 4 ] 2 + (sometimes), [ N i ( C N ) 4 ] 2 − [\mathrm{Ni(CN)}_4]^{2-} [ Ni ( CN ) 4 ] 2 − 6 6 6 Octahedral [\mathrm{Cu}(\mathrm{H}_2\mathrm{O})_6]^{2+}$$[\mathrm{Fe(CN)}_6]^{4-}
Transition metal complexes are coloured because of d d d -d d d electron transitions:
In an isolated atom/ion, all five d d d -orbitals are degenerate (same energy). In a complex, ligands split the d d d -orbitals into groups of different energies (d d d -orbital splitting). When white light passes through the complex, photons with energy matching the Δ E \Delta E Δ E between split d d d -levels are absorbed. The remaining light is transmitted, giving the complex its complementary colour. \Delta E = hf = \frac`\{hc}`{\lambda} Spectrochemical series (increasing Δ \Delta Δ ):
I − < B r − < C l − < F − < H 2 O < N H 3 < e n < C N − < C O \mathrm{I}^- \lt \mathrm{Br}^- \lt \mathrm{Cl}^- \lt \mathrm{F}^- \lt \mathrm{H}_2\mathrm{O} \lt \mathrm{NH}_3 \lt \mathrm{en} \lt \mathrm{CN}^- \lt \mathrm{CO} I − < Br − < Cl − < F − < H 2 O < NH 3 < en < CN − < CO Ligands that produce larger splitting are called strong-field ligands ; those producing smaller Splitting are weak-field ligands .
Complex ion Colour observed Colour absorbed [ C u ( H 2 O ) 6 ] 2 + [\mathrm{Cu}(\mathrm{H}_2\mathrm{O})_6]^{2+} [ Cu ( H 2 O ) 6 ] 2 + Blue Orange/red [ C u ( N H 3 ) 4 ( H 2 O ) 2 ] 2 + [\mathrm{Cu}(\mathrm{NH}_3)_4(\mathrm{H}_2\mathrm{O})_2]^{2+} [ Cu ( NH 3 ) 4 ( H 2 O ) 2 ] 2 + Deep blue Yellow/orange [ C o ( H 2 O ) 6 ] 2 + [\mathrm{Co}(\mathrm{H}_2\mathrm{O})_6]^{2+} [ Co ( H 2 O ) 6 ] 2 + Pink Green [ C o C l 4 ] 2 − [\mathrm{CoCl}_4]^{2-} [ CoCl 4 ] 2 − Blue Yellow/orange
::: :::caution $[\mathrm{Ti}(\mathrm{H}_2\mathrm{O})_6]^{4+}$ has $d^0$), or (b) it has a full $d$-subshell (e.g., $\mathrm{Zn}^{2+}$$[\mathrm{Cu}(\mathrm{NH}_3)_4]^+$ has $d^{10}$). In both cases, there are no $d$-$d$ transitions possible.
Transition metals are effective catalysts because they can adopt variable oxidation states and form Intermediate complexes, providing alternative reaction pathways with lower activation energies.
Heterogeneous catalysis (catalyst in a different phase):
Catalyst Reaction Fe Haber process: N 2 + 3 H 2 ⇌ 2 N H 3 \mathrm{N}_2 + 3\mathrm{H}_2 \rightleftharpoons 2\mathrm{NH}_3 N 2 + 3 H 2 ⇌ 2 NH 3 V2 _2 2 O5 _5 5 Contact process: 2 S O 2 + O 2 → 2 S O 3 2\mathrm{SO}_2 + \mathrm{O}_2 \to 2\mathrm{SO}_3 2 SO 2 + O 2 → 2 SO 3 Ni Hydrogenation of alkenes Pt/Pd Catalytic converters (oxidation of CO and hydrocarbons, reduction of NOx _x x )
Homogeneous catalysis (catalyst in the same phase):
Catalyst Reaction F e 2 + / F e 3 + \mathrm{Fe}^{2+}/\mathrm{Fe}^{3+} Fe 2 + / Fe 3 + Fenton’s reagent (oxidation of organic pollutants) M n 2 + \mathrm{Mn}^{2+} Mn 2 + Decomposition of H 2 O 2 \mathrm{H}_2\mathrm{O}_2 H 2 O 2
Transition metals and their complexes can be paramagnetic (attracted to a magnetic field) or diamagnetic (weakly repelled).
Property Condition Example Paramagnetic Unpaired d d d -electrons present [ F e ( H 2 O ) 6 ] 3 + [\mathrm{Fe}(\mathrm{H}_2\mathrm{O})_6]^{3+} [ Fe ( H 2 O ) 6 ] 3 + (d 5 d^5 d 5 )Diamagnetic All d d d -electrons paired [ Z n ( H 2 O ) 6 ] 2 + [\mathrm{Zn}(\mathrm{H}_2\mathrm{O})_6]^{2+} [ Zn ( H 2 O ) 6 ] 2 + (d 10 d^{10} d 10 )
The number of unpaired electrons determines the magnetic moment (measured in Bohr magnetons, μ B \mu_B μ B ):
μ ≈ n ( n + 2 ) μ B \mu \approx \sqrt{n(n + 2)}\ \mu_B μ ≈ n ( n + 2 ) μ B Where n n n is the number of unpaired electrons.
When atoms absorb energy (e.g., from heat or electricity), electrons are excited to higher energy Levels. When they fall back to lower levels, they emit photons with energies corresponding to the energy differences:
\Delta E = E_{\mathrm{higher}} - E_{\mathrm{lower}} = h\nu = \frac`\{hc}`{\lambda} Where:
h = 6.626 × 10 − 34 J ⋅ s h = 6.626 \times 10^{-34}\mathrm{ J}\cdot\mathrm{s} h = 6.626 × 1 0 − 34 J ⋅ s (Planck’s constant)c = 3.00 × 10 8 m / s c = 3.00 \times 10^8\mathrm{ m/s} c = 3.00 × 1 0 8 m/s (speed of light)λ \lambda λ = wavelength of emitted lightν \nu ν = frequencyEach element produces a unique line emission spectrum , a series of discrete lines at specific Wavelengths. This is the basis of flame tests and spectroscopic analysis.
When white light passes through a cool gas, the gas absorbs photons at wavelengths corresponding to the energy differences between its electron levels. The transmitted light shows dark lines at these wavelengths on a continuous spectrum.
The hydrogen emission spectrum shows several series, each corresponding to transitions to a specific Lower energy level:
Series Final n n n Spectral region Wavelength range Lyman 1 1 1 Ultraviolet < 400 n m < 400\mathrm{ nm} < 400 nm Balmer 2 2 2 Visible 400 400 400 —700 n m 700\mathrm{ nm} 700 nm Paschen 3 3 3 Infrared > 700 n m > 700\mathrm{ nm} > 700 nm Brackett 4 4 4 Infrared > 700 n m > 700\mathrm{ nm} > 700 nm
The energy levels of hydrogen are given by:
E n = − 13.6 e V n 2 = − 2.18 × 10 − 18 J n 2 E_n = -\frac{13.6\mathrm{ eV}}{n^2} = -\frac{2.18 \times 10^{-18}\mathrm{ J}}{n^2} E n = − n 2 13.6 eV = − n 2 2.18 × 1 0 − 18 J For the Balmer series (transitions to n = 2 n = 2 n = 2 ), the first four lines correspond to:
Transition λ \lambda λ (nm)Colour 3 → 2 3 \to 2 3 → 2 656 656 656 Red 4 → 2 4 \to 2 4 → 2 486 486 486 Cyan 5 → 2 5 \to 2 5 → 2 434 434 434 Blue 6 → 2 6 \to 2 6 → 2 410 410 410 Violet
Lines in each series converge at the series limit (the ionization energy). As n n n increases, the energy levels get closer together and transitions approach a continuum:
E ∞ = 0 J ( i o n i z a t i o n t h r e s h o l d ) E_{\infty} = 0\mathrm{ J} \quad (\mathrm{ionization threshold}) E ∞ = 0 J ( ionizationthreshold ) The existence of discrete spectral lines is direct evidence that electron energy is quantised. The classical model predicted a continuous spectrum, which is never observed for individual atoms.
Mass spectrometry measures the mass-to-charge ratio (m / z m/z m / z ) of ions. The general process:
Ionization : Atoms or molecules are ionized ( by electron impact. High-energy electrons knock an electron off the sample, forming positive ions).Acceleration : Ions are accelerated by an electric field. All ions receive the same kinetic energy: $$ \frac{1}{2}mv^2 = zVwhere $V$ is the accelerating voltage and $z$ is the charge on the ion. 3. **Deflection**: Ions pass through a magnetic field and are deflected. Lighter ions (or more highly charged ions) are deflected more: $$ r = \frac{\sqrt{2mV}}{zB} where r r r is the radius of curvature and B B B is the magnetic field strength. 4. Detection : A detector records the abundance of ions at each m / z m/z m / z value, producing a mass spectrum.
A mass spectrum plots relative abundance (y-axis) against m / z m/z m / z (x-axis).
For a single element, the mass spectrum shows peaks at each isotope’s mass, with heights Proportional to natural abundance. :::
Example, Boron
Boron has two isotopes: B \mathrm{B} B -10 (19.9 % 19.9\% 19.9% ) and B \mathrm{B} B -11 (80.1 % 80.1\% 80.1% ).
The mass spectrum shows peaks at m / z = 10 m/z = 10 m / z = 10 and m / z = 11 m/z = 11 m / z = 11 with relative heights in the ratio 19.9 : 80.1 19.9 : 80.1 19.9 : 80.1 Approximately 1 : 4 1 : 4 1 : 4 .
A r = ( 10 × 0.199 ) + ( 11 × 0.801 ) = 1.99 + 8.81 = 10.81 A_r = (10 \times 0.199) + (11 \times 0.801) = 1.99 + 8.81 = 10.81 A r = ( 10 × 0.199 ) + ( 11 × 0.801 ) = 1.99 + 8.81 = 10.81 The molecular ion peak (M + \mathrm{M}^+ M + ) corresponds to the intact molecule with one electron Removed. Its m / z m/z m / z value gives the molecular mass.
C H 4 + e − → C H 4 + ∙ + 2 e − \mathrm{CH}_4 + e^- \to \mathrm{CH}_4^{+\bullet} + 2e^- CH 4 + e − → CH 4 +∙ + 2 e − The molecular ion peak for C H 4 \mathrm{CH}_4 CH 4 appears at m / z = 16 m/z = 16 m / z = 16 .
After ionization, the molecular ion often breaks apart into smaller fragments. The fragmentation Pattern is characteristic of the molecule and can be used to identify it.
Fragment m / z m/z m / z Likely species Common origin 15 15 15 C H 3 + \mathrm{CH}_3^+ CH 3 + Loss of H from C H 4 + ∙ \mathrm{CH}_4^{+\bullet} CH 4 +∙ 29 29 29 C 2 H 5 + \mathrm{C}_2\mathrm{H}_5^+ C 2 H 5 + or C H O + \mathrm{CHO}^+ CHO + Ethanol, aldehydes 43 43 43 C 3 H 7 + \mathrm{C}_3\mathrm{H}_7^+ C 3 H 7 + or C H 3 C O + \mathrm{CH}_3\mathrm{CO}^+ CH 3 CO + Ketones, propanol 77 77 77 C 6 H 5 + \mathrm{C}_6\mathrm{H}_5^+ C 6 H 5 + Benzene ring
For molecules containing chlorine or bromine, the isotope patterns are distinctive:
Element Isotopes Approximate ratio Cl C l \mathrm{Cl} Cl -35, C l \mathrm{Cl} Cl -373 : 1 3 : 1 3 : 1 Br B r \mathrm{Br} Br -79, B r \mathrm{Br} Br -811 : 1 1 : 1 1 : 1
A molecule with one chlorine atom shows an M \mathrm{M} M and M + 2 \mathrm{M}+2 M + 2 peak in a 3 : 1 3:1 3 : 1 ratio. A molecule with one bromine atom shows an M \mathrm{M} M and M + 2 \mathrm{M}+2 M + 2 peak in a 1 : 1 1:1 1 : 1 ratio.
Example, Chlorobenzene
Chlorobenzene (C 6 H 5 C l \mathrm{C}_6\mathrm{H}_5\mathrm{Cl} C 6 H 5 Cl ) shows:
M + \mathrm{M}^+ M + at m / z = 112 m/z = 112 m / z = 112 (C 6 H 5 35 C l \mathrm{C}_6\mathrm{H}_5^{35}\mathrm{Cl} C 6 H 5 35 Cl )M + 2 \mathrm{M}+2 M + 2 at m / z = 114 m/z = 114 m / z = 114 (C 6 H 5 37 C l \mathrm{C}_6\mathrm{H}_5^{37}\mathrm{Cl} C 6 H 5 37 Cl )Ratio of peak heights: approximately 3 : 1 3:1 3 : 1 High-resolution MS can determine exact masses to several decimal places, distinguishing between molecules with the same nominal mass but different molecular formulas:
Species Exact mass (u) C 2 H 4 O \mathrm{C}_2\mathrm{H}_4\mathrm{O} C 2 H 4 O 44.0262 44.0262 44.0262 C O 2 \mathrm{CO}_2 CO 2 43.9898 43.9898 43.9898 N 2 O \mathrm{N}_2\mathrm{O} N 2 O 44.0011 44.0011 44.0011
Slater’s rules provide a systematic way to estimate the shielding constant S S S for an electron in a many-electron atom.
Write the electron configuration in groups: ( 1 s ) ( 2 s , 2 p ) ( 3 s , 3 p ) ( 3 d ) ( 4 s , 4 p ) ( 4 d ) ( 4 f ) ( 5 s , 5 p ) … (1s)(2s, 2p)(3s, 3p)(3d)(4s, 4p)(4d)(4f)(5s, 5p) \ldots ( 1 s ) ( 2 s , 2 p ) ( 3 s , 3 p ) ( 3 d ) ( 4 s , 4 p ) ( 4 d ) ( 4 f ) ( 5 s , 5 p ) …
Electrons in groups to the right of the electron of interest contribute 0 0 0 to S S S .
Other electrons in the same group contribute:
For n s ns n s or n p np n p electrons: each other electron contributes 0.35 0.35 0.35 (except 1 s 1s 1 s Where the other electron contributes 0.30 0.30 0.30 ) For n d nd n d or n f nf n f electrons: each other electron contributes 0.35 0.35 0.35 Electrons in the n − 1 n-1 n − 1 shell contribute: 0.85 0.85 0.85 each (for s s s and p p p electrons in the n n n shell)1.00 1.00 1.00 each (for d d d and f f f electrons in the n n n shell)Electrons in shells n − 2 n-2 n − 2 or lower contribute 1.00 1.00 1.00 each. Note
Example, Z e f f Z_{\mathrm{eff}} Z eff for a 3 p 3p 3 p electron in chlorine (Z = 17 Z = 17 Z = 17 ) Configuration: ( 1 s ) 2 ( 2 s , 2 p ) 8 ( 3 s , 3 p ) 7 (1s)^2(2s, 2p)^8(3s, 3p)^7 ( 1 s ) 2 ( 2 s , 2 p ) 8 ( 3 s , 3 p ) 7
For a 3 p 3p 3 p electron:
Same ( 3 s , 3 p ) (3s, 3p) ( 3 s , 3 p ) group: 6 6 6 other electrons × 0.35 = 2.10 \times 0.35 = 2.10 × 0.35 = 2.10 n − 1 n - 1 n − 1 shell ( 2 s , 2 p ) 8 (2s, 2p)^8 ( 2 s , 2 p ) 8 : 8 × 0.85 = 6.80 8 \times 0.85 = 6.80 8 × 0.85 = 6.80 n − 2 n - 2 n − 2 shell ( 1 s ) 2 (1s)^2 ( 1 s ) 2 : 2 × 1.00 = 2.00 2 \times 1.00 = 2.00 2 × 1.00 = 2.00 S = 2.10 + 6.80 + 2.00 = 10.90 S = 2.10 + 6.80 + 2.00 = 10.90 S = 2.10 + 6.80 + 2.00 = 10.90 Z _ e f f = 17 − 10.90 = 6.10 Z\_{\mathrm{eff}} = 17 - 10.90 = 6.10 Z _ eff = 17 − 10.90 = 6.10 Note
Example, Z e f f Z_{\mathrm{eff}} Z eff for a 3 d 3d 3 d electron in scandium (Z = 21 Z = 21 Z = 21 ) Configuration: ( 1 s ) 2 ( 2 s , 2 p ) 8 ( 3 s , 3 p ) 8 ( 3 d ) 1 ( 4 s ) 2 (1s)^2(2s, 2p)^8(3s, 3p)^8(3d)^1(4s)^2 ( 1 s ) 2 ( 2 s , 2 p ) 8 ( 3 s , 3 p ) 8 ( 3 d ) 1 ( 4 s ) 2
For the 3 d 3d 3 d electron:
Same ( 3 d ) (3d) ( 3 d ) group: 0 0 0 other electrons × 0.35 = 0 \times 0.35 = 0 × 0.35 = 0 n − 1 n - 1 n − 1 shell: ( 3 s , 3 p ) 8 (3s, 3p)^8 ( 3 s , 3 p ) 8 each contributes 1.00 1.00 1.00 (for d d d electrons, the rule is different) = 8 × 1.00 = 8.00 8 \times 1.00 = 8.00 8 × 1.00 = 8.00 Shells n − 2 n - 2 n − 2 and lower: ( 2 s , 2 p ) 8 ( 1 s ) 2 (2s, 2p)^8(1s)^2 ( 2 s , 2 p ) 8 ( 1 s ) 2 = 10 × 1.00 = 10.00 10 \times 1.00 = 10.00 10 × 1.00 = 10.00 S = 0 + 8.00 + 10.00 = 18.00 S = 0 + 8.00 + 10.00 = 18.00 S = 0 + 8.00 + 10.00 = 18.00 Z _ e f f = 21 − 18.00 = 3.00 Z\_{\mathrm{eff}} = 21 - 18.00 = 3.00 Z _ eff = 21 − 18.00 = 3.00 The low Z e f f Z_{\mathrm{eff}} Z eff on the 3 d 3d 3 d electron explains why the 4 s 4s 4 s orbital fills before 3 d 3d 3 d , The 4 s 4s 4 s electron experiences a higher effective nuclear charge.
Plotting log ( I E ) \log(IE) log ( I E ) against ionization number reveals jumps that correspond to the removal of electrons from inner shells.
For aluminium (Z = 13 Z = 13 Z = 13 ):
I E 1 , I E 2 , I E 3 ⏟ v a l e n c e 3 s 2 3 p 1 ≪ I E 4 , I E 5 , … , I E 11 ≪ I E 12 , I E 13 \underbrace{IE_1, IE_2, IE_3}_{\mathrm{valence } 3s^2\, 3p^1} \ll IE_4, IE_5, \ldots, IE_{11} \ll IE_{12}, IE_{13} valence 3 s 2 3 p 1 I E 1 , I E 2 , I E 3 ≪ I E 4 , I E 5 , … , I E 11 ≪ I E 12 , I E 13 Ionization number Electron removed Approximate IE (kJ/mol) Shell 1 1 1 3 p 1 3p^1 3 p 1 578 578 578 n = 3 n = 3 n = 3 2 2 2 3 s 1 3s^1 3 s 1 1817 1817 1817 n = 3 n = 3 n = 3 3 3 3 3 s 1 3s^1 3 s 1 2745 2745 2745 n = 3 n = 3 n = 3 4 4 4 2 p 1 2p^1 2 p 1 11577 11577 11577 n = 2 n = 2 n = 2 (jump!)… \ldots … 11 11 11 2 s 1 2s^1 2 s 1 6521 6521 6521 n = 2 n = 2 n = 2 12 12 12 1 s 1 1s^1 1 s 1 18560 18560 18560 n = 1 n = 1 n = 1 (jump!)13 13 13 1 s 1 1s^1 1 s 1 21600 21600 21600 n = 1 n = 1 n = 1
The jumps reveal:
3 3 3 valence electrons (n = 3 n = 3 n = 3 )8 8 8 electrons in n = 2 n = 2 n = 2 2 2 2 electrons in n = 1 n = 1 n = 1 The Rydberg equation for hydrogen gives the wavelength of any spectral line:
1 λ = R H ( 1 n f 2 − 1 n i 2 ) \frac{1}{\lambda} = R_H \left(\frac{1}{n_f^2} - \frac{1}{n_i^2}\right) λ 1 = R H ( n f 2 1 − n i 2 1 ) Where R H = 1.097 × 10 7 m − 1 R_H = 1.097 \times 10^7\mathrm{ m}^{-1} R H = 1.097 × 1 0 7 m − 1 is the Rydberg constant, n i n_i n i is the initial energy Level, and n f n_f n f is the final energy level (n i > n f n_i \gt n_f n i > n f for emission).
Note
Example, Wavelength of the first Balmer line for the transition n = 3 → n = 2 n = 3 \to n = 2 n = 3 → n = 2 :
1 λ = 1.097 × 10 7 ( 1 4 − 1 9 ) = 1.097 × 10 7 × 0.1389 = 1.524 × 10 6 m − 1 \frac{1}{\lambda} = 1.097 \times 10^7 \left(\frac{1}{4} - \frac{1}{9}\right) = 1.097 \times 10^7 \times 0.1389 = 1.524 \times 10^6\mathrm{ m}^{-1} λ 1 = 1.097 × 1 0 7 ( 4 1 − 9 1 ) = 1.097 × 1 0 7 × 0.1389 = 1.524 × 1 0 6 m − 1 λ = 1 1.524 × 10 6 = 6.56 × 10 − 7 m = 656 n m \lambda = \frac{1}{1.524 \times 10^6} = 6.56 \times 10^{-7}\mathrm{ m} = 656\mathrm{ nm} λ = 1.524 × 1 0 6 1 = 6.56 × 1 0 − 7 m = 656 nm This corresponds to the red line in the Balmer series (Hα \alpha α ).
E = h\nu = \frac`\{hc}`{\lambda} For the n = 3 → n = 2 n = 3 \to n = 2 n = 3 → n = 2 transition:
E = ( 6.626 × 10 − 34 ) ( 3.00 × 10 8 ) 6.56 × 10 − 7 = 3.03 × 10 − 19 J E = \frac{(6.626 \times 10^{-34})(3.00 \times 10^8)}{6.56 \times 10^{-7}} = 3.03 \times 10^{-19}\mathrm{ J} E = 6.56 × 1 0 − 7 ( 6.626 × 1 0 − 34 ) ( 3.00 × 1 0 8 ) = 3.03 × 1 0 − 19 J Converting to electron-volts:
E = 3.03 × 10 − 19 1.602 × 10 − 19 = 1.89 e V E = \frac{3.03 \times 10^{-19}}{1.602 \times 10^{-19}} = 1.89\mathrm{ eV} E = 1.602 × 1 0 − 19 3.03 × 1 0 − 19 = 1.89 eV The number of possible spectral lines from energy level n n n down to the ground state is:
N = n ( n − 1 ) 2 N = \frac{n(n - 1)}{2} N = 2 n ( n − 1 ) For n = 4 n = 4 n = 4 : N = 6 N = 6 N = 6 spectral lines.
(a) Define the term relative atomic mass . (2 marks)
(b) occurring boron consists of two isotopes, B \mathrm{B} B -10 and B \mathrm{B} B -11. The Relative atomic mass of boron is 10.81 10.81 10.81 . Calculate the percentage abundance of B \mathrm{B} B -10. (2 Marks)
Markscheme:
(a) The weighted mean mass of an atom of an element relative to 1 / 12 1/12 1/12 the mass of an atom of carbon-12, based on the abundance of isotopes in a occurring sample. (2 marks)
(b) Let x x x = fractional abundance of B \mathrm{B} B -10, so ( 1 − x ) (1 - x) ( 1 − x ) = fractional abundance of B \mathrm{B} B -11.
10.81 = 10 x + 11 ( 1 − x ) 10.81 = 10x + 11(1 - x) 10.81 = 10 x + 11 ( 1 − x ) 10.81 = 10 x + 11 − 11 x 10.81 = 10x + 11 - 11x 10.81 = 10 x + 11 − 11 x 10.81 = 11 − x 10.81 = 11 - x 10.81 = 11 − x X = 0.19 X = 0.19 X = 0.19 Percentage abundance of B \mathrm{B} B -10 = 19 % 19\% 19% . (1 mark for setup, 1 mark for answer)
Explain why the first ionization energy of sodium is lower than that of magnesium, but the first ionization energy of magnesium is lower than that of aluminium.
Markscheme:
Na (1 s 2 2 s 2 2 p 6 3 s 1 1s^2\, 2s^2\, 2p^6\, 3s^1 1 s 2 2 s 2 2 p 6 3 s 1 ) to Mg (1 s 2 2 s 2 2 p 6 3 s 2 1s^2\, 2s^2\, 2p^6\, 3s^2 1 s 2 2 s 2 2 p 6 3 s 2 ): Z e f f Z_{\mathrm{eff}} Z eff increases across the period, so the 3 s 3s 3 s electrons in Mg are held more tightly. (1 mark)
Mg (3 s 2 3s^2 3 s 2 ) to Al (3 s 2 3 p 1 3s^2\, 3p^1 3 s 2 3 p 1 ): the electron removed from Al is a 3 p 3p 3 p electron, which is at a higher energy level than the 3 s 3s 3 s electrons of Mg and is partially shielded by the 3 s 3s 3 s electrons. (1 mark)
Also: Mg has a stable filled 3 s 3s 3 s subshell configuration. (1 mark)
(a) State the electron configuration of F e 2 + \mathrm{Fe}^{2+} Fe 2 + using noble gas notation. (1 mark)
(b) Describe the trend in atomic radius across Period 3 and explain this trend in terms of effective Nuclear charge. (3 marks)
Markscheme:
(a) [ A r ] 3 d 6 [\mathrm{Ar}]\, 3d^6 [ Ar ] 3 d 6 (1 mark; note: electrons are removed from 4 s 4s 4 s before 3 d 3d 3 d )
(b) Atomic radius decreases from Na to Ar. (1 mark)
Across a period, the nuclear charge (Z Z Z ) increases by one proton per element, but the additional Electrons enter the same shell and provide only partial shielding. (1 mark)
Therefore Z e f f Z_{\mathrm{eff}} Z eff increases across the period, pulling the electron cloud closer to the nucleus and decreasing the atomic radius. (1 mark)
A sample of chlorine gas is analysed by mass spectrometry. Describe and explain the appearance of the mass spectrum.
Markscheme:
Two peaks are observed at m / z = 35 m/z = 35 m / z = 35 and m / z = 37 m/z = 37 m / z = 37 . (1 mark)
The heights of the peaks are in the approximate ratio 3 : 1 3:1 3 : 1 Reflecting the natural abundances of C l \mathrm{Cl} Cl -35 (75.77 % 75.77\% 75.77% ) and C l \mathrm{Cl} Cl -37 (24.23 % 24.23\% 24.23% ). (1 mark)
The sample is diatomic (C l 2 \mathrm{Cl}_2 Cl 2 ), so additional peaks appear at m / z = 70 m/z = 70 m / z = 70 (35 C l ^{35}\mathrm{Cl} 35 Cl —35 C l ^{35}\mathrm{Cl} 35 Cl ), m / z = 72 m/z = 72 m / z = 72 (35 C l ^{35}\mathrm{Cl} 35 Cl —37 C l ^{37}\mathrm{Cl} 37 Cl ), and m / z = 74 m/z = 74 m / z = 74 (37 C l ^{37}\mathrm{Cl} 37 Cl —37 C l ^{37}\mathrm{Cl} 37 Cl ) in the ratio 9 : 6 : 1 9:6:1 9 : 6 : 1 . (1 mark)
(a) State the four quantum numbers for each of the valence electrons in a ground-state oxygen atom. (3 marks)
(b) Explain why the fourth ionization energy of beryllium is much larger than the third. (2 marks)
Markscheme:
(a) Oxygen: 1 s 2 2 s 2 2 p 4 1s^2\, 2s^2\, 2p^4 1 s 2 2 s 2 2 p 4 . The six valence electrons (in n = 2 n = 2 n = 2 ):
2 s 2s 2 s electrons: ( 2 , 0 , 0 , + 1 2 ) (2, 0, 0, +\frac{1}{2}) ( 2 , 0 , 0 , + 2 1 ) and ( 2 , 0 , 0 , − 1 2 ) (2, 0, 0, -\frac{1}{2}) ( 2 , 0 , 0 , − 2 1 )
2 p 2p 2 p electrons: (2, 1, -1, +\frac{1}{2})$$(2, 1, 0, +\frac{1}{2})$$(2, 1, +1, +\frac{1}{2}) ( 2 , 1 , − 1 , − 1 2 ) (2, 1, -1, -\frac{1}{2}) ( 2 , 1 , − 1 , − 2 1 ) (1 mark for n , l , m l n, l, m_l n , l , m l ; 1 mark for m s m_s m s showing Hund’s rule with first Three 2 p 2p 2 p electrons having parallel spins; 1 mark for the fourth being paired)
(b) Beryllium: 1 s 2 2 s 2 1s^2\, 2s^2 1 s 2 2 s 2 . IE_1$$IE_2$$IE_3 remove the two 2 s 2s 2 s electrons and one 1 s 1s 1 s Electron. I E 4 IE_4 I E 4 removes the remaining 1 s 1s 1 s electron. (1 mark)
The 1 s 1s 1 s electron is much closer to the nucleus and experiences far less shielding, so it requires much more energy to remove. This is an inner shell electron. (1 mark)
(a) Explain what is meant by the term ligand and give one example of a bidentate ligand. (2 Marks)
(b) The complex [ C o ( N H 3 ) 6 ] 3 + [\mathrm{Co}(\mathrm{NH}_3)_6]^{3+} [ Co ( NH 3 ) 6 ] 3 + is yellow but [ C o ( H 2 O ) 6 ] 3 + [\mathrm{Co}(\mathrm{H}_2\mathrm{O})_6]^{3+} [ Co ( H 2 O ) 6 ] 3 + is blue. Explain this difference. (2 marks)
(c) Explain why transition metals often show catalytic activity, using the Haber process as an example. (2 marks)
Markscheme:
(a) A ligand is a molecule or ion that can donate a lone pair of electrons to a central metal ion via a coordinate bond. (1 mark) Example of bidentate ligand: ethylenediamine (en) or oxalate ion (C 2 O 4 2 − \mathrm{C}_2\mathrm{O}_4^{2-} C 2 O 4 2 − ). (1 mark)
(b) N H 3 \mathrm{NH}_3 NH 3 is a stronger-field ligand than H 2 O \mathrm{H}_2\mathrm{O} H 2 O on the spectrochemical Series, so it causes greater d d d -orbital splitting (Δ \Delta Δ ) in [ C o ( N H 3 ) 6 ] 3 + [\mathrm{Co}(\mathrm{NH}_3)_6]^{3+} [ Co ( NH 3 ) 6 ] 3 + . (1 mark) A larger Δ \Delta Δ means higher-energy photons are Absorbed, so the complementary colour transmitted is different (yellow vs blue). (1 mark)
(c) Transition metals have variable oxidation states, allowing them to form intermediate compounds with reactants. This provides an alternative reaction pathway with a lower activation energy. (1 Mark) In the Haber process, iron catalyses the reaction by adsorbing N 2 \mathrm{N}_2 N 2 and H 2 \mathrm{H}_2 H 2 onto its surface, weakening the N ≡ N \mathrm{N}\equiv\mathrm{N} N ≡ N triple bond and Facilitating the formation of N H 3 \mathrm{NH}_3 NH 3 . (1 mark)
The successive ionization energies of an element X are shown below (in kJ/mol):
IE_1 = 577$$IE_2 = 1816$$IE_3 = 2744$$IE_4 = 11577$$IE_5 = 14842$$IE_6 = 18376
(a) Identify element X and explain your reasoning. (2 marks)
(b) Write the electron configuration of X2 + ^{2+} 2 + . (1 mark)
(c) Explain why I E 4 IE_4 I E 4 is significantly larger than I E 3 IE_3 I E 3 . (1 mark)
Markscheme:
(a) The element is aluminium. (1 mark) There is a large jump between I E 3 IE_3 I E 3 and I E 4 IE_4 I E 4 Indicating that the first three electrons are removed from the valence shell and the fourth electron is from an inner shell. This is consistent with Group 13, and aluminium is the element in Period 3, Group 13. (1 mark)
(b) [ N e ] 3 s 1 [\mathrm{Ne}]\, 3s^1 [ Ne ] 3 s 1 (1 mark; removing two electrons from the 3 s 2 3 p 1 3s^2\, 3p^1 3 s 2 3 p 1 configuration)
(c) I E 4 IE_4 I E 4 removes an electron from the n = 2 n = 2 n = 2 shell, which is closer to the nucleus and experiences much less shielding. The effective nuclear charge on inner-shell electrons is much Higher. (1 mark)
Calculate the wavelength of radiation emitted when an electron in a hydrogen atom transitions from n = 5 n = 5 n = 5 to n = 2 n = 2 n = 2 . Identify the spectral series and the region of the electromagnetic spectrum.
Markscheme:
1 λ = R H ( 1 n f 2 − 1 n i 2 ) = 1.097 × 10 7 ( 1 4 − 1 25 ) \frac{1}{\lambda} = R_H \left(\frac{1}{n_f^2} - \frac{1}{n_i^2}\right) = 1.097 \times 10^7 \left(\frac{1}{4} - \frac{1}{25}\right) λ 1 = R H ( n f 2 1 − n i 2 1 ) = 1.097 × 1 0 7 ( 4 1 − 25 1 ) = 1.097 × 10 7 × 21 100 = 2.304 × 10 6 m − 1 = 1.097 \times 10^7 \times \frac{21}{100} = 2.304 \times 10^6\mathrm{ m}^{-1} = 1.097 × 1 0 7 × 100 21 = 2.304 × 1 0 6 m − 1 λ = 1 2.304 × 10 6 = 4.34 × 10 − 7 m = 434 n m \lambda = \frac{1}{2.304 \times 10^6} = 4.34 \times 10^{-7}\mathrm{ m} = 434\mathrm{ nm} λ = 2.304 × 1 0 6 1 = 4.34 × 1 0 − 7 m = 434 nm (2 marks for correct substitution and calculation)
This is part of the Balmer series (transitions to n = 2 n = 2 n = 2 ) and falls in the visible region of the electromagnetic spectrum (blue-violet). (2 marks)
Common Mistake
When writing electron configurations for transition metal ions, always remove electrons from the n s ns n s orbital first (highest principal quantum number), NOT from the ( n − 1 ) d (n-1)d ( n − 1 ) d orbital. So F e 3 + \mathrm{Fe}^{3+} Fe 3 + is [ A r ] 3 d 5 [\mathrm{Ar}]\, 3d^5 [ Ar ] 3 d 5 Not [ A r ] 4 s 2 3 d 3 [\mathrm{Ar}]\, 4s^2\, 3d^3 [ Ar ] 4 s 2 3 d 3 .
Common Mistake
Do not confuse atomic radius trends with ionic radius trends. When comparing ionic radii within an isoelectronic series, the ion with the largest nuclear charge has the smallest radius. For example, N a + \mathrm{Na}^+ Na + is smaller than F − \mathrm{F}^- F − even though N a \mathrm{Na} Na has a larger atomic radius than F \mathrm{F} F .
Common confusions
Confusing first ionisation energy with electronegativity: First ionisation energy is the energy required to REMOVE the outermost electron from a gaseous atom. Electronegativity is the ability of an atom to ATTRACT electrons in a covalent bond. Both generally increase across a period, but they measure fundamentally different properties and have different periodic trends down a group.
Misunderstanding why ionisation energy decreases down a group: Ionisation energy decreases down a group because the outermost electron is in a higher energy shell, FURTHER from the nucleus and more shielded by inner electrons. The increased distance and shielding outweigh the increased nuclear charge. Students often mention only one factor when both are needed.
Confusing periodic trends across a period: Across a period, atomic radius DECREASES (increasing nuclear charge pulls electrons closer), first ionisation energy generally INCREASES, electronegativity INCREASES, and metallic character DECREASES. Students frequently get one or more of these trends backwards.
Misidentifying exceptions in ionisation energy trends: The general increase in first ionisation energy across a period has dips at Group 13 (e.g., boron) and Group 16 (e.g., oxygen). Group 13 dips because the p1 electron is in a higher energy p-subshell. Group 16 dips because the p4 electron is paired with another electron in the same orbital, creating repulsion. These exceptions are frequently tested in IB exams. ::: :::
Question 1: Calculating Relative Atomic Mass occurring boron consists of two isotopes: B \mathrm{B} B -10 (19.9 % 19.9\% 19.9% abundance, mass 10.01 u 10.01\mathrm{ u} 10.01 u ) and B \mathrm{B} B -11 (80.1 % 80.1\% 80.1% abundance, mass 11.01 u 11.01\mathrm{ u} 11.01 u ). Calculate the Relative atomic mass of boron.
Answer A r = ( 10.01 × 0.199 ) + ( 11.01 × 0.801 ) = 1.992 + 8.819 = 10.81 A_r = (10.01 \times 0.199) + (11.01 \times 0.801) = 1.992 + 8.819 = 10.81 A r = ( 10.01 × 0.199 ) + ( 11.01 × 0.801 ) = 1.992 + 8.819 = 10.81 The relative atomic mass of boron is 10.81 u 10.81\mathrm{ u} 10.81 u .
Question 2: Electron Configuration and Quantum Numbers (a) Write the electron configuration of C r \mathrm{Cr} Cr (Z = 24 Z = 24 Z = 24 ) using noble gas notation.
(b) State the four quantum numbers for the last electron added to chromium.
Answer (a) Chromium is an exception to the Aufbau principle. A half-filled d d d -subshell is more stable:
C r : [ A r ] 4 s 1 3 d 5 \mathrm{Cr}: [\mathrm{Ar}]\, 4s^1\, 3d^5 Cr : [ Ar ] 4 s 1 3 d 5 (b) The last electron enters the 3 d 3d 3 d subshell:
Principal quantum number: n = 3 n = 3 n = 3 Azimuthal quantum number: l = 2 l = 2 l = 2 (for d d d -orbital) Magnetic quantum number: m l = + 2 m_l = +2 m l = + 2 (one of − 2 , − 1 , 0 , + 1 , + 2 -2, -1, 0, +1, +2 − 2 , − 1 , 0 , + 1 , + 2 ) Spin quantum number: m s = + 1 2 m_s = +\frac{1}{2} m s = + 2 1 (Hund’s rule: first five electrons have parallel spins) Question 3: Periodic Trends Explain why the first ionization energy of aluminium is lower than that of magnesium, but the first ionization energy of sulfur is lower than that of phosphorus.
Answer Aluminium vs Magnesium: Mg has the electron configuration [ N e ] 3 s 2 [\mathrm{Ne}]\, 3s^2 [ Ne ] 3 s 2 with a stable, Filled 3 s 3s 3 s subshell. Al has [ N e ] 3 s 2 3 p 1 [\mathrm{Ne}]\, 3s^2\, 3p^1 [ Ne ] 3 s 2 3 p 1 . The 3 p 3p 3 p electron in Al is at a higher Energy level than the 3 s 3s 3 s electrons of Mg and is partially shielded by the 3 s 3s 3 s electrons, so it requires less energy to remove.
Sulfur vs Phosphorus: P has the configuration [ N e ] 3 s 2 3 p 3 [\mathrm{Ne}]\, 3s^2\, 3p^3 [ Ne ] 3 s 2 3 p 3 with a stable Half-filled 3 p 3p 3 p subshell. S has [ N e ] 3 s 2 3 p 4 [\mathrm{Ne}]\, 3s^2\, 3p^4 [ Ne ] 3 s 2 3 p 4 Where the fourth 3 p 3p 3 p electron is paired with another electron in the same orbital. The paired electrons experience mutual repulsion, Making the paired electron easier to remove.
Question 4: Isoelectronic Series Arrange the following ions in order of increasing ionic radius and explain your reasoning: \mathrm{O}^{2-}$$\mathrm{F}^-$$\mathrm{Na}^+$$\mathrm{Mg}^{2+}$$\mathrm{Al}^{3+} .
Answer All five species are isoelectronic with the neon configuration (1 s 2 2 s 2 2 p 6 1s^2\, 2s^2\, 2p^6 1 s 2 2 s 2 2 p 6 10 electrons).
A l 3 + < M g 2 + < N a + < F − < O 2 − \mathrm{Al}^{3+} \lt \mathrm{Mg}^{2+} \lt \mathrm{Na}^+ \lt \mathrm{F}^- \lt \mathrm{O}^{2-} Al 3 + < Mg 2 + < Na + < F − < O 2 − All have the same number of electrons, but the nuclear charge increases from O \mathrm{O} O (Z = 8 Z = 8 Z = 8 ) To A l \mathrm{Al} Al (Z = 13 Z = 13 Z = 13 ). A higher nuclear charge pulls the electron cloud closer to the nucleus, Resulting in a smaller ionic radius.
Question 5: Spectral Line Calculation Calculate the wavelength of the photon emitted when an electron in a hydrogen atom transitions from n = 4 n = 4 n = 4 to n = 2 n = 2 n = 2 . Use the Rydberg equation with R H = 1.097 × 10 7 m − 1 R_H = 1.097 \times 10^7\mathrm{ m}^{-1} R H = 1.097 × 1 0 7 m − 1 .
Answer 1 λ = R H ( 1 n f 2 − 1 n i 2 ) = 1.097 × 10 7 ( 1 4 − 1 16 ) \frac{1}{\lambda} = R_H \left(\frac{1}{n_f^2} - \frac{1}{n_i^2}\right) = 1.097 \times 10^7 \left(\frac{1}{4} - \frac{1}{16}\right) λ 1 = R H ( n f 2 1 − n i 2 1 ) = 1.097 × 1 0 7 ( 4 1 − 16 1 ) 1 λ = 1.097 × 10 7 × ( 4 − 1 16 ) = 1.097 × 10 7 × 0.1875 = 2.057 × 10 6 m − 1 \frac{1}{\lambda} = 1.097 \times 10^7 \times \left(\frac{4 - 1}{16}\right) = 1.097 \times 10^7 \times 0.1875 = 2.057 \times 10^6\mathrm{ m}^{-1} λ 1 = 1.097 × 1 0 7 × ( 16 4 − 1 ) = 1.097 × 1 0 7 × 0.1875 = 2.057 × 1 0 6 m − 1 λ = 1 2.057 × 10 6 = 4.86 × 10 − 7 m = 486 n m \lambda = \frac{1}{2.057 \times 10^6} = 4.86 \times 10^{-7}\mathrm{ m} = 486\mathrm{ nm} λ = 2.057 × 1 0 6 1 = 4.86 × 1 0 − 7 m = 486 nm This corresponds to the cyan line in the Balmer series (visible region).
For the A-Level treatment of this topic, see Atomic Structure & Periodicity .
Writing half-equations without balancing charges or atoms. Always check electrons, hydrogen ions, and water molecules.
Forgetting to convert between units (e.g., cm 3 \text{cm}^3 cm 3 to dm 3 \text{dm}^3 dm 3 ) when calculating concentrations.
Assuming that a strong acid always has a lower pH than a weak acid without considering concentration.
Confusing the terms ‘molar’ and ‘molecular’. Molar refers to per mole (mol − 1 \text{mol}^{-1} mol − 1 ), while molecular refers to individual molecules.
Stoichiometric Relationships — Mole concept and Avogadro’s number are foundational for understanding atomic structure calculations.Chemical Bonding — Electron configuration determines bonding behaviour, linking atomic structure to chemical properties.Periodicity — Trends in ionisation energy and electronegativity arise directly from the atomic structure covered here.Thermochemistry — Enthalpy changes in reactions depend on bond energies derived from atomic and molecular structure.