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Chemical Bonding & Molecular Structure

1. Kössel-Lewis Approach & Octet Rule

Core Concept

Lewis Octet Rule: Atoms combine either by transfer of valence electrons (gaining or losing) or by sharing valence electrons in order to attain a stable octet ($8\mathrm{e^-}$) in their outermost shell (duplet $2\mathrm{e^-}$ for Hydrogen).

Lewis Dot Structures and Covalent Bonds
Fig. 4.1 Covalent sharing and Lewis dot representations of $\mathrm{Cl_2}$, $\mathrm{H_2O}$, and $\mathrm{CCl_4}$.

1.1 Formal Charge Calculation (100% Board Exam Guaranteed)

The formal charge ($FC$) of an atom in a polyatomic ion or molecule is defined as:

Formula $$\text{Formal Charge } (FC) = V - L - \frac{1}{2}S$$

Where: $V = \text{Valence } \mathrm{e^-}$ of isolated atom, $L = \text{Lone pair (non-bonding) } \mathrm{e^-}$, $S = \text{Shared (bonding) } \mathrm{e^-}$.

✍ SCHOOL EXAM CLASSIC — Formal Charge of Ozone ($\mathrm{O_3}$)

Q. Calculate formal charge on each oxygen atom in Ozone ($\mathrm{O_3}$): $\mathrm{O_{(1)} = O_{(2)} - O_{(3)}}$.

Atom 1 (Central $\mathrm{O}$): $V = 6$, $L = 2$, $S = 6 \implies FC = 6 - 2 - \frac{1}{2}(6) = \mathbf{+1}$.
Atom 2 (Double-bonded $\mathrm{O}$): $V = 6$, $L = 4$, $S = 4 \implies FC = 6 - 4 - \frac{1}{2}(4) = \mathbf{0}$.
Atom 3 (Single-bonded $\mathrm{O}$): $V = 6$, $L = 6$, $S = 2 \implies FC = 6 - 6 - \frac{1}{2}(2) = \mathbf{-1}$.

1.2 Limitations of the Octet Rule (3-Mark Board Favorite)

Limitation Explanation Key Standard Examples
1. Incomplete Octet Central atom has fewer than 8 valence electrons. $\mathrm{LiCl}$ ($2\mathrm{e^-}$), $\mathrm{BeH_2}$ ($4\mathrm{e^-}$), $\mathrm{BF_3, BCl_3}$ ($6\mathrm{e^-}$)
2. Odd-Electron Molecules Total valence electrons is odd, so octet cannot be satisfied for all atoms. Nitric oxide ($\mathrm{NO}$), Nitrogen dioxide ($\mathrm{NO_2}$)
3. Expanded Octet Central atom (Period 3+) uses vacant $d$-orbitals, accommodating $> 8$ electrons. $\mathrm{PF_5}$ ($10\mathrm{e^-}$), $\mathrm{SF_6}$ ($12\mathrm{e^-}$), $\mathrm{H_2SO_4}$ ($12\mathrm{e^-}$)

2. Ionic Bond, Lattice Enthalpy & Fajans' Rules

Conditions Favoring Ionic Bond Formation
  1. Low Ionization Enthalpy of the metal atom (easier cation formation).
  2. High Negative Electron Gain Enthalpy of the non-metal atom (easier anion formation).
  3. High Lattice Enthalpy of the resulting ionic crystal lattice.

2.1 Lattice Enthalpy & Born-Haber Cycle

Lattice Enthalpy ($\Delta_{\text{lattice}}H^\circ$): Energy required to completely separate 1 mole of a solid ionic compound into gaseous constituent ions (or energy released when 1 mole ionic solid forms from gaseous ions).

Born-Haber Cycle for NaCl
Fig. 4.2 Born-Haber Cycle for Solid Sodium Chloride ($\mathrm{NaCl}$). $\Delta_f H^\circ = \Delta_{\text{sub}}H + \frac{1}{2}\Delta_{\text{bond}}H + \Delta_i H + \Delta_{eg}H + U_L$.

2.2 Fajans' Rules (Covalent Character in Ionic Bonds)

No bond is 100% ionic. Cation distorts electron cloud of anion — a phenomenon called Polarization.

Fajans' Rules Summary
✍ REASONING DRILL — Fajans' Rules

Q. Why is $\mathrm{LiI}$ more covalent than $\mathrm{LiF}$? Why is $\mathrm{CuCl}$ more covalent than $\mathrm{NaCl}$?

Ans 1: $\mathrm{I^-}$ is much larger than $\mathrm{F^-}$, making it more easily polarized by $\mathrm{Li^+}$, giving $\mathrm{LiI}$ greater covalent character.
Ans 2: $\mathrm{Cu^+}$ ($3d^{10}$) has a $18\mathrm{e^-}$ pseudo-noble shell which shields nuclear charge less effectively than $\mathrm{Na^+}$ ($2p^6$, $8\mathrm{e^-}$), exerting greater polarizing power.

3. Covalent Bond Parameters & Dipole Moment

3.1 Dipole Moment ($\mu$) & Molecular Geometry

Dipole Moment ($\mu$): $\mu = Q \times r$ (Unit: Debye, $1\text{ D} = 3.3356 \times 10^{-30}\text{ C m}$). It is a vector quantity pointing from $\delta+$ to $\delta-$.

Molecule Geometry Dipole Moment ($\mu$) Exam Reason / Explanation
$\mathrm{CO_2}$ Linear $\mu = 0$ Two equal bond dipoles ($\mathrm{C=O}$) point in opposite directions ($180^\circ$) and cancel.
$\mathrm{BF_3}$ Trigonal Planar $\mu = 0$ Resultant of two $\mathrm{B-F}$ dipoles equals and opposes the third $\mathrm{B-F}$ dipole ($120^\circ$).
$\mathrm{NH_3}$ vs $\mathrm{NF_3}$ Pyramidal $\mathrm{NH_3} (1.47\text{D}) > \mathrm{NF_3} (0.23\text{D})$ In $\mathrm{NH_3}$, orbital dipole of lone pair & $\mathrm{N-H}$ bond dipoles reinforce; in $\mathrm{NF_3}$, $\mathrm{N-F}$ dipoles oppose lone pair dipole.
✍ SCHOOL EXAM CLASSIC — Dipole Moment ($\mathrm{CCl_4}$ vs $\mathrm{CHCl_3}$)

Q. Why is dipole moment ($\mu$) of $\mathrm{CCl_4}$ zero, whereas that of $\mathrm{CHCl_3}$ is non-zero ($1.04\text{ D}$)? How is % ionic character calculated?

Ans 1: $\mathrm{CCl_4}$ is symmetrical tetrahedral; the vector sum of 4 equal $\mathrm{C-Cl}$ bond dipoles cancels out ($\mu = 0$). In $\mathrm{CHCl_3}$, replacement of one $\mathrm{Cl}$ by $\mathrm{H}$ breaks symmetry, producing a net dipole moment ($\mu = 1.04\text{ D}$).
Ans 2 (% Ionic Character Formula): $$\% \text{Ionic Character} = \left(\frac{\mu_{\text{observed}}}{\mu_{\text{theoretical ionic}}}\right) \times 100$$

3.2 Resonance & Resonance Hybrid

Core Concept

Resonance: When a single Lewis structure cannot accurately describe a molecule, two or more canonical structures with identical atomic positions but different electron distributions are drawn. The actual molecule is a resonance hybrid of all canonical forms.

Resonance Bond Order Formula: $\text{Bond Order} = \frac{\text{Total number of bonds between two atoms in all canonical forms}}{\text{Total number of canonical forms}}$.
Example ($\mathrm{CO_3^{2-}}$): $\mathrm{C-O}$ Bond Order = $\frac{4}{3} = \mathbf{1.33}$.

4. VSEPR Theory (Shape of Molecules)

Postulates of VSEPR Theory
  1. The shape of a molecule depends on the total number of valence shell electron pairs (bonded and lone pairs) around the central atom.
  2. Electron pairs repel each other and stay as far apart as possible to minimize repulsion.
  3. Order of Repulsive Force: $\mathbf{\text{Lone Pair - Lone Pair (lp-lp) > Lone Pair - Bond Pair (lp-bp) > Bond Pair - Bond Pair (bp-bp)}}$.

4.1 The Master VSEPR Shape Table (Must-Memorize for Exams)

Type bp lp Electron Geometry Molecular Shape Bond Angle Standard Examples
$\mathrm{AB_2}$ 2 0 Linear Linear $180^\circ$ $\mathrm{BeCl_2, CO_2, HgCl_2}$
$\mathrm{AB_3}$ 3 0 Trigonal Planar Trigonal Planar $120^\circ$ $\mathrm{BF_3, BCl_3}$
$\mathrm{AB_2E}$ 2 1 Trigonal Planar Bent / V-shaped $< 120^\circ$ ($119.5^\circ$) $\mathrm{SO_2, O_3}$
$\mathrm{AB_4}$ 4 0 Tetrahedral Tetrahedral $109.5^\circ$ $\mathrm{CH_4, NH_4^+}$
$\mathrm{AB_3E}$ 3 1 Tetrahedral Trigonal Pyramidal $107^\circ$ $\mathrm{NH_3, H_3O^+}$
$\mathrm{AB_2E_2}$ 2 2 Tetrahedral Bent / V-shaped $104.5^\circ$ $\mathrm{H_2O, H_2S}$
$\mathrm{AB_5}$ 5 0 Trigonal Bipyramidal Trigonal Bipyramidal $120^\circ, 90^\circ$ $\mathrm{PCl_5}$
$\mathrm{AB_4E}$ 4 1 Trigonal Bipyramidal See-Saw $< 120^\circ, < 90^\circ$ $\mathrm{SF_4}$
$\mathrm{AB_3E_2}$ 3 2 Trigonal Bipyramidal T-Shaped $< 90^\circ$ ($87.5^\circ$) $\mathrm{ClF_3, BrF_3}$
$\mathrm{AB_2E_3}$ 2 3 Trigonal Bipyramidal Linear $180^\circ$ $\mathrm{XeF_2, I_3^-}$
$\mathrm{AB_6}$ 6 0 Octahedral Octahedral $90^\circ$ $\mathrm{SF_6}$
$\mathrm{AB_5E}$ 5 1 Octahedral Square Pyramidal $< 90^\circ$ $\mathrm{BrF_5, IF_5}$
$\mathrm{AB_4E_2}$ 4 2 Octahedral Square Planar $90^\circ$ $\mathrm{XeF_4}$
✍ SCHOOL EXAM FAVORITE — $\mathrm{PCl_5}$ Axial vs Equatorial Bonds

Q. Why are axial $\mathrm{P-Cl}$ bonds in $\mathrm{PCl_5}$ longer and weaker than equatorial bonds?

Ans: In $\mathrm{PCl_5}$ (Trigonal Bipyramidal), 3 equatorial bonds lie in one plane ($120^\circ$ apart), while 2 axial bonds lie perpendicular ($90^\circ$).
The 2 axial bond pairs experience greater repulsion from 3 equatorial bond pairs at $90^\circ$ compared to equatorial pairs which experience repulsion from only 2 pairs at $90^\circ$. To minimize repulsion, axial bonds stretch, becoming longer and weaker.
Trigonal Bipyramidal Geometry of PCl5
Fig. 4.17 Trigonal bipyramidal geometry of $\mathrm{PCl_5}$ showing axial ($90^\circ$, $240\text{ pm}$) and equatorial ($120^\circ$, $202\text{ pm}$) bonds.
✍ 3-MARK BOARD REASONING — Bond Angle Trend ($\mathrm{CH_4 > NH_3 > H_2O}$)

Q. Explain why $\mathrm{CH_4, NH_3}$, and $\mathrm{H_2O}$ all have $sp^3$ central atoms, but their bond angles decrease: $\mathrm{CH_4} (109.5^\circ) > \mathrm{NH_3} (107^\circ) > \mathrm{H_2O} (104.5^\circ)$.

Ans: According to VSEPR theory, electron pair repulsion order is $\mathbf{\text{lp-lp > lp-bp > bp-bp}}$.
1. $\mathrm{CH_4}$ has 0 lone pairs: regular tetrahedral angle ($109.5^\circ$).
2. $\mathrm{NH_3}$ has 1 lone pair: $\text{lp-bp}$ repulsion pushes $\mathrm{N-H}$ bond pairs closer, reducing angle to $107^\circ$.
3. $\mathrm{H_2O}$ has 2 lone pairs: strong $\text{lp-lp}$ repulsion compresses $\mathrm{O-H}$ bond pairs even further, reducing angle to $104.5^\circ$.

5. Valence Bond Theory (VBT) & Orbital Overlap

PE Curve for H2
Fig. 4.7 Potential energy curve for the formation of gaseous $\mathrm{H_2}$ molecule. Minimum energy corresponds to 74 pm bond length and $-435.8\text{ kJ/mol}$ bond enthalpy.

5.1 Comparison: $\sigma$ (Sigma) Bond vs $\pi$ (Pi) Bond

Feature $\sigma$ (Sigma) Bond $\pi$ (Pi) Bond
Type of Overlap Head-on / End-to-end (axial) overlap along internuclear axis ($s-s, s-p_z, p_z-p_z$). Sideways / Lateral (parallel) overlap perpendicular to axis ($p_x-p_x, p_y-p_y$).
Extent of Overlap Greater overlap $\implies$ Strong bond. Smaller overlap $\implies$ Weaker bond.
Electron Density Cylindrically symmetrical around internuclear axis. Two saucer-like clouds above and below the nodal plane.
Rotation Free rotation about $\sigma$-axis is possible. Free rotation is restricted.
Existence Can exist independently as a single bond. Always formed alongside a $\sigma$ bond in multiple bonds ($\mathrm{C=C}$ has $1\sigma + 1\pi$; $\mathrm{C\equiv C}$ has $1\sigma + 2\pi$).
Types of Orbital Overlaps
Fig. 4.9 Positive (bonding), Negative (antibonding), and Zero (non-bonding) orbital overlaps.

6. Hybridisation

Definition & Rules

Hybridisation: The process of intermixing of atomic orbitals of slightly different energies of an atom to form a new set of equivalent orbitals of identical shape and energy called hybrid orbitals.

6.1 Summary of Hybridisation Types

Hybridisation Orbitals Mixed Geometry Bond Angle Examples
$sp$ $1s + 1p_z$ Linear $180^\circ$ $\mathrm{BeCl_2, C_2H_2, CO_2}$
$sp^2$ $1s + 2p$ ($p_x, p_y$) Trigonal Planar $120^\circ$ $\mathrm{BCl_3, C_2H_4, BF_3}$
$sp^3$ $1s + 3p$ Tetrahedral $109.5^\circ$ $\mathrm{CH_4, C_2H_6, NH_3, H_2O}$
$sp^3d$ $1s + 3p + 1d_{z^2}$ Trigonal Bipyramidal $120^\circ, 90^\circ$ $\mathrm{PCl_5, SF_4, ClF_3}$
$sp^3d^2$ $1s + 3p + 2d$ ($d_{z^2}, d_{x^2-y^2}$) Octahedral $90^\circ$ $\mathrm{SF_6, XeF_4}$
Formation of BeCl2 sp Hybrid Orbitals
Fig. 4.10 Formation of $sp$ hybrid orbitals in $\mathrm{BeCl_2}$ molecule ($180^\circ$ linear geometry).
✍ GUARANTEED 2-MARK DRILL — Counting $\sigma$ & $\pi$ Bonds

Q. Find the total number of $\sigma$ and $\pi$ bonds in: (a) Ethene ($\mathrm{C_2H_4}$), (b) Ethyne ($\mathrm{C_2H_2}$), (c) Benzene ($\mathrm{C_6H_6}$), and (d) Propadiene ($\mathrm{CH_2=C=CH_2}$).

(a) Ethene ($\mathrm{H_2C=CH_2}$): $5\sigma$ bonds ($4\text{ C-H} + 1\text{ C-C}$) and $1\pi$ bond.
(b) Ethyne ($\mathrm{HC\equiv CH}$): $3\sigma$ bonds ($2\text{ C-H} + 1\text{ C-C}$) and $2\pi$ bonds.
(c) Benzene ($\mathrm{C_6H_6}$): $12\sigma$ bonds ($6\text{ C-H} + 6\text{ C-C}$) and $3\pi$ bonds.
(d) Propadiene ($\mathrm{H_2C=C=CH_2}$): $6\sigma$ bonds and $2\pi$ bonds. Central carbon is $\mathbf{sp}$ hybridised; terminal carbons are $\mathbf{sp^2}$.

7. Molecular Orbital Theory (MOT)

Salient Features of MOT
Feature Bonding Molecular Orbital (BMO) Antibonding Molecular Orbital (ABMO)
Wave Function Formed by constructive interference ($\psi = \psi_A + \psi_B$). Formed by destructive interference ($\psi^* = \psi_A - \psi_B$).
Energy & Stability Lower energy than parent AOs $\implies$ High stability. Higher energy than parent AOs $\implies$ Lower stability.
Electron Density High electron density concentrated between the nuclei. Zero electron density between nuclei (possesses a Nodal Plane).
Molecular Orbital Energy Level Diagram
Fig. 4.19 LCAO combination of two $1s$ atomic orbitals forming $\sigma 1s$ bonding MO and $\sigma^* 1s$ antibonding MO.
Shapes of Bonding and Antibonding MOs
Fig. 4.20 Shapes of bonding ($\sigma 2p_z, \pi 2p_x, \pi 2p_y$) and antibonding ($\sigma^* 2p_z, \pi^* 2p_x, \pi^* 2p_y$) molecular orbitals.

7.1 Two Energy Level Sequences & $2s-2p$ Orbital Mixing

Physical Reason for Energy Sequence Shift ($2s-2p$ Mixing)

In lighter homonuclear diatomics ($Z \le 7$: $\mathrm{Li_2, Be_2, B_2, C_2, N_2}$), the energy gap between $2s$ and $2p$ atomic orbitals is small, leading to significant $2s-2p$ orbital mixing. This pushes the $\sigma 2p_z$ MO higher in energy than the degenerate $\pi 2p_x = \pi 2p_y$ pair. In heavier diatomics ($Z > 7$: $\mathrm{O_2, F_2}$), the $2s-2p$ energy gap is large $\implies$ negligible mixing $\implies \sigma 2p_z$ remains lower in energy than $\pi 2p$.

Energy Order Rule

1. For $Z \le 7$ ($14\mathrm{e^-}$ or fewer: $\mathrm{Li_2, Be_2, B_2, C_2, N_2}$):

$$\sigma 1s < \sigma^* 1s < \sigma 2s < \sigma^* 2s < (\pi 2p_x = \pi 2p_y) < \sigma 2p_z < (\pi^* 2p_x = \pi^* 2p_y) < \sigma^* 2p_z$$

2. For $Z > 7$ (More than $14\mathrm{e^-}$: $\mathrm{O_2, F_2, Ne_2}$):

$$\sigma 1s < \sigma^* 1s < \sigma 2s < \sigma^* 2s < \sigma 2p_z < (\pi 2p_x = \pi 2p_y) < (\pi^* 2p_x = \pi^* 2p_y) < \sigma^* 2p_z$$

7.2 Homonuclear Diatomic Series

Species Total $\mathrm{e^-}$ MO Electronic Configuration $N_b$ $N_a$ Bond Order Magnetic Character & Notes
$\mathrm{H_2}$ 2 $\sigma 1s^2$ 2 0 1 Diamagnetic
$\mathrm{He_2}$ 4 $\sigma 1s^2 \, \sigma^* 1s^2$ 2 2 0 Does not exist ($BO=0$)
$\mathrm{Li_2}$ 6 $\sigma 1s^2 \, \sigma^* 1s^2 \, \sigma 2s^2$ 4 2 1 Diamagnetic (Stable in gas phase)
$\mathrm{Be_2}$ 8 $\sigma 1s^2 \, \sigma^* 1s^2 \, \sigma 2s^2 \, \sigma^* 2s^2$ 4 4 0 Does not exist ($BO=0$)
$\mathrm{B_2}$ 10 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2$ $(\pi 2p_x^1 = \pi 2p_y^1)$ 6 4 1 Paramagnetic (2 unpaired $\mathrm{e^-}$)
$\mathrm{C_2}$ 12 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2$ $(\pi 2p_x^2 = \pi 2p_y^2)$ 8 4 2 Diamagnetic (Both bonds are $\pi$ bonds!)
$\mathrm{N_2}$ 14 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2$ $(\pi 2p_x^2 = \pi 2p_y^2) \, \sigma 2p_z^2$ 10 4 3 Diamagnetic ($1\sigma + 2\pi$, highest $BO$)
$\mathrm{O_2}$ 16 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2 \, \sigma 2p_z^2$ $(\pi 2p_x^2 = \pi 2p_y^2)$ $(\pi^* 2p_x^1 = \pi^* 2p_y^1)$ 10 6 2 Paramagnetic (2 unpaired $\mathrm{e^-}$)
$\mathrm{F_2}$ 18 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2 \, \sigma 2p_z^2$ $(\pi 2p_x^2 = \pi 2p_y^2)$ $(\pi^* 2p_x^2 = \pi^* 2p_y^2)$ 10 8 1 Diamagnetic
$\mathrm{Ne_2}$ 20 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2 \, \sigma 2p_z^2$ $(\pi 2p_x^2 = \pi 2p_y^2)$ $(\pi^* 2p_x^2 = \pi^* 2p_y^2) \, \sigma^* 2p_z^2$ 10 10 0 Does not exist ($BO=0$)
MO Energy and Bond Properties
Fig. 4.21 MO energy level occupancy chart and bond properties ($\mathrm{B_2}$ to $\mathrm{Ne_2}$).

7.3 Heteronuclear Diatomic Species ($\mathrm{CO, NO, NO^+}$)

Species Total $\mathrm{e^-}$ MO Electronic Configuration $N_b$ $N_a$ Bond Order Magnetic Character & Notes
$\mathrm{CO}$ 14 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2$ $(\pi 2p_x^2 = \pi 2p_y^2) \, \sigma 2p_z^2$ 10 4 3 Diamagnetic (Isoelectronic with $\mathrm{N_2}$)
$\mathrm{NO}$ 15 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2 \, \sigma 2p_z^2$ $(\pi 2p_x^2 = \pi 2p_y^2) \, (\pi^* 2p_x^1)$ 10 5 2.5 Paramagnetic (1 unpaired $\mathrm{e^-}$ in $\pi^* 2p$)
$\mathrm{NO^+}$ 14 $\mathrm{KK} \, \sigma 2s^2 \, \sigma^* 2s^2$ $(\pi 2p_x^2 = \pi 2p_y^2) \, \sigma 2p_z^2$ 10 4 3 Diamagnetic (More stable than $\mathrm{NO}$)
✍ MOST FAMOUS BOARD QUESTION — Paramagnetism of Oxygen

Q. Why is $\mathrm{O_2}$ paramagnetic according to MOT while VBT predicts it to be diamagnetic?

Ans: VBT assumes all electrons in $\mathrm{O_2}$ are paired in double bonds ($\mathrm{:O=O:}$), wrongly predicting diamagnetism.
MOT gives electronic configuration: $\sigma 1s^2 \, \sigma^* 1s^2 \, \sigma 2s^2 \, \sigma^* 2s^2 \, \sigma 2p_z^2 \, (\pi 2p_x^2 = \pi 2p_y^2) \, (\pi^* 2p_x^1 = \pi^* 2p_y^1)$. Due to Hund's rule, the 2 highest energy electrons enter degenerate antibonding orbitals $\pi^* 2p_x$ and $\pi^* 2p_y$ singly, proving $\mathrm{O_2}$ has 2 unpaired electrons and is paramagnetic.
✍ HIGH-YIELD BOARD DRILL — Oxygen Series ($\mathrm{O_2^+, O_2, O_2^-, O_2^{2-}}$)

Q. Arrange $\mathrm{O_2, O_2^+, O_2^-, O_2^{2-}}$ in increasing order of bond length and stability.

Bond Orders: $\mathrm{O_2^+} (2.5) > \mathrm{O_2} (2.0) > \mathrm{O_2^-} (1.5) > \mathrm{O_2^{2-}} (1.0)$.
Stability Order ($\propto \text{Bond Order}$): $\mathbf{\mathrm{O_2^{2-}} < \mathrm{O_2^-} < \mathrm{O_2} < \mathrm{O_2^+}}$.
Bond Length Order ($\propto 1/\text{Bond Order}$): $\mathbf{\mathrm{O_2^+} < \mathrm{O_2} < \mathrm{O_2^-} < \mathrm{O_2^{2-}}}$.
✍ HIGH-YIELD BOARD DRILL — Nitrogen Series ($\mathrm{N_2, N_2^+, N_2^-}$)

Q. Calculate bond order of $\mathrm{N_2, N_2^+}$, and $\mathrm{N_2^-}$. Compare their stabilities and magnetic behaviors.

$\mathrm{N_2}$ ($14e^-$): $BO = \frac{10 - 4}{2} = \mathbf{3.0}$. Diamagnetic. Highest stability.
$\mathrm{N_2^+}$ ($13e^-$): Electron removed from bonding $\sigma 2p_z \implies BO = \frac{9 - 4}{2} = \mathbf{2.5}$. Paramagnetic.
$\mathrm{N_2^-}$ ($15e^-$): Electron added to antibonding $\pi^* 2p_x \implies BO = \frac{10 - 5}{2} = \mathbf{2.5}$. Paramagnetic.
Stability Order: $\mathbf{\mathrm{N_2} > \mathrm{N_2^+} > \mathrm{N_2^-}}$. Note: $\mathrm{N_2^+}$ is slightly more stable than $\mathrm{N_2^-}$ despite equal bond order because $\mathrm{N_2^-}$ contains 5 antibonding electrons versus 4 in $\mathrm{N_2^+}$.

8. Hydrogen Bonding

Definition & Conditions

Hydrogen Bond: Electrostatic attraction between hydrogen atom covalently bonded to a highly electronegative atom ($\mathrm{F, O, N}$) and another electronegative atom with a lone pair. Energy $\approx 10 - 40\text{ kJ/mol}$.

Type Description & Mechanism Examples & Physical Effect
Intermolecular H-Bond Occurs between different molecules of same or different compounds. $\mathrm{H_2O, HF, NH_3}$, alcohols.
Effect: Raises b.p. ($\mathrm{H_2O}$ liquid while $\mathrm{H_2S}$ gas).
Intramolecular H-Bond Occurs within the same molecule forming a 5/6-membered chelate ring. $o$-nitrophenol, salicylaldehyde.
Effect: Lowers b.p., makes $o$-nitrophenol steam volatile.
Intermolecular Hydrogen Bonding Diagram
Fig. 4.23 Intermolecular H-bonding in $\mathrm{HF}$ chain and $\mathrm{H_2O}$ open tetrahedral network.
Fig 4.22 Intramolecular vs Intermolecular H-bonding
Fig. 4.22 Intramolecular H-bonding in $o$-nitrophenol vs Intermolecular H-bonding in $p$-nitrophenol.
✍ BOARD REASONING — $o$-Nitrophenol vs $p$-Nitrophenol

Q. Why does $o$-nitrophenol have a lower boiling point and higher steam volatility than $p$-nitrophenol?

Ans: In $o$-nitrophenol, $\mathrm{-OH}$ and $\mathrm{-NO_2}$ groups are adjacent, forming intramolecular H-bonding (chelate ring within molecule). It does not associate with neighboring molecules.
In $p$-nitrophenol, groups are far apart, forming extensive intermolecular H-bonding (chains between molecules). Thus, $p$-nitrophenol requires more energy to separate molecules $\implies$ higher b.p. and non-volatile in steam.
✍ CLASSIC SCHOOL EXAM QUESTIONS — H-Bonding Anomalies

Q1. Why is $\mathrm{H_2O}$ a liquid while $\mathrm{H_2S}$ is a gas at room temperature?
Q2. Why does ice float on water and why is water's density maximum at $4^\circ\text{C}$?

Ans 1: Oxygen has high electronegativity and small size, forming strong intermolecular hydrogen bonds in $\mathrm{H_2O}$ that associate molecules into liquid state. Sulfur is larger with lower electronegativity, so $\mathrm{H_2S}$ has no H-bonding and remains a gas.
Ans 2: Ice forms a 3D open cage-like structure held by 4 hydrogen bonds per $\mathrm{H_2O}$ molecule, trapping empty space $\implies$ lower density than liquid water (ice floats). At $4^\circ\text{C}$, cage partially collapses, giving maximum density.

9. Rapid Exam Formula & Fact Summary

Concept High-Yield Exam Formula / Key Result Exam Tip
Formal Charge $FC = V - L - \frac{1}{2}S$ Sum of FCs equals total charge on ion.
Dipole Moment $\mu = q \times r$ (Debye, D) $\mu = 0$ for symmetrical molecules ($\mathrm{CO_2, BF_3, CCCl_4}$).
VSEPR Repulsion $\text{lp-lp} > \text{lp-bp} > \text{bp-bp}$ Lone pairs squeeze bond angles ($\mathrm{CH_4} 109.5^\circ \to \mathrm{NH_3} 107^\circ \to \mathrm{H_2O} 104.5^\circ$).
Bond Order (MOT) $BO = \frac{N_b - N_a}{2}$ $BO \propto \text{Bond Enthalpy} \propto \frac{1}{\text{Bond Length}}$.
Steric Number $SN = \frac{1}{2}[V + M - C + A]$ $SN = 2(sp), 3(sp^2), 4(sp^3), 5(sp^3d), 6(sp^3d^2)$.
⚠️ Top 5 Common School Exam Pitfalls & Mistakes