Masterclass: 25 Ultra-Challenging JEE Advanced Problems on Chemical Bonding
From the orbital overlaps of Molecular Orbital Theory to the electronegativity dictates of Bent's Rule. Master the quantum mechanics of molecular structure.
Chemical Bonding is the heart of inorganic chemistry. At the JEE Advanced level, you cannot rely merely on octet rules. You must deploy advanced concepts like Bent's Rule for trigonal bipyramidal geometries, Fajan's Rules for polarization, and Molecular Orbital Theory (MOT) for fractional bond orders and magnetic properties.
View Solution
Step 1: Apply Bent's Rule
Bent's rule states that more electronegative atoms prefer hybrid orbitals having less s-character, and more electropositive atoms (or lone pairs) prefer hybrid orbitals having more s-character.
Step 2: Assign Positions
Fluorine is more electronegative than Chlorine. The axial bonds in a trigonal bipyramidal ($sp^3d$) structure are formed from $p_z$ and $d_{z^2}$ orbitals, meaning they have $0\%$ s-character. The equatorial bonds ($sp^2$) have $33.3\%$ s-character.
Therefore, the two highly electronegative Fluorine atoms will strictly occupy the two axial positions. The three less electronegative Chlorine atoms will occupy the three equatorial positions.
Step 3: Evaluate Dipole Moment
The molecule is highly symmetrical. The two axial $P-F$ bond dipoles are exactly $180^{\circ}$ apart and perfectly cancel each other. The three equatorial $P-Cl$ bond dipoles are exactly $120^{\circ}$ apart in a plane, so their vector sum is exactly zero.
View Solution
Step 1: Calculate Bond Orders
The electronic configuration of $O_2$ ($16$ electrons) ends with $2$ unpaired electrons in the degenerate $\pi^*_{2px}$ and $\pi^*_{2py}$ antibonding orbitals.
Bond Order (B.O.) $= \frac{N_b - N_a}{2}$.
- $O_2$ ($16e^-$): B.O. $= \frac{10 - 6}{2} = 2.0$
- $O_2^+$ ($15e^-$, loses one antibonding $e^-$): B.O. $= \frac{10 - 5}{2} = 2.5$
- $O_2^-$ ($17e^-$, gains one antibonding $e^-$): B.O. $= \frac{10 - 7}{2} = 1.5$
- $O_2^{2-}$ ($18e^-$, gains two antibonding $e^-$): B.O. $= \frac{10 - 8}{2} = 1.0$
Step 2: Relate to Bond Length
Higher bond order means a stronger, shorter bond.
Bond length order: $O_2^+ < O_2 < O_2^- < O_2^{2-}$.
Step 3: Determine Magnetic Properties
- $O_2$: 2 unpaired $e^-$ (Paramagnetic)
- $O_2^+$: 1 unpaired $e^-$ (Paramagnetic)
- $O_2^-$: 1 unpaired $e^-$ (Paramagnetic)
- $O_2^{2-}$: 0 unpaired $e^-$ (Diamagnetic, fully paired $\pi^*$ orbitals).
View Solution
Step 1: Analyze ortho-dichlorobenzene
The two $C-Cl$ bonds are at an angle $\theta = 60^{\circ}$.
$\mu_{ortho} = \sqrt{\mu^2 + \mu^2 + 2\mu^2\cos(60^{\circ})} = \sqrt{2\mu^2 + 2\mu^2(0.5)} = \sqrt{3\mu^2} = \mathbf{1.732\mu}$.
Step 2: Analyze meta-dichlorobenzene
The two $C-Cl$ bonds are at an angle $\theta = 120^{\circ}$.
$\mu_{meta} = \sqrt{\mu^2 + \mu^2 + 2\mu^2\cos(120^{\circ})} = \sqrt{2\mu^2 + 2\mu^2(-0.5)} = \sqrt{\mu^2} = \mathbf{1.0\mu}$.
Step 3: Analyze para-dichlorobenzene
The two $C-Cl$ bonds are at an angle $\theta = 180^{\circ}$.
$\mu_{para} = \sqrt{\mu^2 + \mu^2 + 2\mu^2\cos(180^{\circ})} = \sqrt{2\mu^2 - 2\mu^2} = \mathbf{0}$.
View Solution
Step 1: Apply Fajan's Rules
Fajan's rules state that polarizing power of a cation increases with an increase in charge density (i.e., smaller size and higher charge). All cations here are $+2$. Therefore, polarizing power depends entirely on ionic radius.
Step 2: Analyze Cation Sizes
Ionic radius increases down the group: $Be^{2+} < Mg^{2+} < Ca^{2+} < Sr^{2+} < Ba^{2+}$.
$Be^{2+}$ is extremely small and possesses a colossal charge density. It fiercely polarizes the electron cloud of the $CO_3^{2-}$ anion, pulling an oxygen atom towards itself. This heavily weakens the internal $C-O$ bond of the carbonate, causing $BeCO_3$ to decompose at near room temperatures.
Step 3: Determine Stability Trend
As we move down the group, the cation becomes larger, its polarizing power decreases, and the carbonate anion suffers less distortion. The salt becomes significantly more thermally stable.
View Solution
Step 1: Analyze Trimethylamine ($N(CH_3)_3$)
Nitrogen is $sp^3$ hybridized, giving a pyramidal shape. Carbon is in the second period and has no empty d-orbitals. The lone pair remains entirely localized on the Nitrogen, causing lone-pair/bond-pair repulsion (pyramidal shape) and making the molecule highly basic.
Step 2: Analyze Trisilylamine ($N(SiH_3)_3$)
Silicon is in the third period and possesses empty $3d$ orbitals. The lone pair on Nitrogen resides in a $2p$ orbital. Because these orbitals are adjacent, the Nitrogen lone pair delocalizes and donates electron density into the empty $3d$ orbitals of the three Silicon atoms. This is called $p\pi-d\pi$ back bonding.
Step 3: Geometric Consequence
To maximize this orbital overlap, the Nitrogen atom rehybridizes from $sp^3$ to $sp^2$. The three $N-Si$ sigma bonds form a perfect trigonal planar geometry, and the unhybridized p-orbital (now shared via $\pi$-bonding) lies perpendicular to the plane. Because the lone pair is completely delocalized into the Silicon atoms, it is unavailable for protonation, rendering the molecule completely non-basic.
View Solution
1. $XeF_2$:
Valence $e^-$ on Xe = 8. Uses 2 for bonding with F. Leaves 6 $e^-$ = 3 lone pairs.
Steric Number = 2 B.P. + 3 L.P. = 5 $\rightarrow$ $sp^3d$ hybridization.
To minimize $90^{\circ}$ L.P.-L.P. repulsions, the 3 lone pairs occupy the equatorial positions. The 2 Fluorines occupy axial positions. Shape: Linear.
2. $XeF_4$:
Valence $e^-$ on Xe = 8. Uses 4 for bonding. Leaves 4 $e^-$ = 2 lone pairs.
Steric Number = 4 B.P. + 2 L.P. = 6 $\rightarrow$ $sp^3d^2$ hybridization.
The 2 lone pairs locate $180^{\circ}$ apart on the axial positions to minimize repulsion. The 4 Fluorines form a flat plane. Shape: Square Planar.
3. $XeF_6$:
Valence $e^-$ on Xe = 8. Uses 6 for bonding. Leaves 2 $e^-$ = 1 lone pair.
Steric Number = 6 B.P. + 1 L.P. = 7 $\rightarrow$ $sp^3d^3$ hybridization.
The presence of 1 lone pair distorts the perfect octahedral geometry. Due to the stereochemically active lone pair moving rapidly through the faces of the octahedron, the molecule is highly fluxional. Shape: Distorted Octahedral (or capped octahedral).
View Solution
Step 1: Write Configuration
$CO$ has 14 electrons (isoelectronic with $N_2$). However, due to the electronegativity difference, the $s-p$ mixing is extreme.
Configuration: $\sigma_{1s}^2 \sigma^*_{1s}^2 \sigma_{2s}^2 \sigma^*_{2s}^2 \pi_{2px}^2 = \pi_{2py}^2 \sigma_{2pz}^2$
Bond Order = $\frac{10 - 4}{2} = 3.0$. (Triple bond explains the high dissociation energy).
Step 2: HOMO Analysis
The Highest Occupied Molecular Orbital (HOMO) is the $\sigma_{2pz}$ orbital (often designated as a slightly antibonding $\sigma^*_{2s}$ in more complex MO diagrams due to heavy $s-p$ mixing, making it effectively a lone pair localized on Carbon).
Because Carbon is less electronegative than Oxygen, its atomic orbitals are higher in energy, placing them closer in energy to the HOMO.
Step 3: Coordination Chemistry
Therefore, the HOMO has significantly more Carbon character. When $CO$ acts as a ligand in metal carbonyls, it is the Carbon atom that donates this lone pair to the transition metal, not the Oxygen.
View Solution
Step 1: Analyze Hydrogen Fluoride ($HF$)
Each $HF$ molecule has 3 lone pairs on Fluorine but only 1 Hydrogen atom. Therefore, each $HF$ molecule can only participate in an average of two hydrogen bonds (one donating, one accepting). They form zig-zag linear chains.
Step 2: Analyze Ammonia ($NH_3$)
Each $NH_3$ molecule has 3 Hydrogen atoms but only 1 lone pair on Nitrogen. The lack of lone pairs restricts the network. It also averages only two hydrogen bonds per molecule. Furthermore, Nitrogen is less electronegative than Fluorine, making these bonds relatively weak, resulting in the lowest boiling point.
Step 3: Analyze Water ($H_2O$)
Each $H_2O$ molecule perfectly possesses 2 Hydrogen atoms AND 2 lone pairs on Oxygen. This precise 1:1 ratio allows every single water molecule to participate in four continuous hydrogen bonds (acting as a donor twice and an acceptor twice). This creates an immense, highly interlocked 3D tetrahedral network in the liquid state.
Conclusion: While an individual $H-F$ bond is stronger than an $O-H \cdots O$ bond, the sheer quantity of bonds (4 per molecule in water vs 2 per molecule in HF) makes the entire water network thermodynamically much harder to break apart.
View Solution
Step 1: Analyze $NO_2$
In $NO_2$, the central Nitrogen atom is $sp^2$ hybridized with a bond angle of $134^{\circ}$. The odd, unpaired electron resides in an $sp^2$ orbital directly on the Nitrogen atom. Because Nitrogen is small and highly electron-deficient in this state, two $NO_2$ molecules easily bring their Nitrogen atoms together, pairing the odd electrons to form a stable $N-N$ sigma bond in $N_2O_4$.
Step 2: Analyze $ClO_2$
In $ClO_2$, Chlorine is a larger, 3rd-period element. It has expanded octet capabilities. The odd electron does not sit localized on the Chlorine atom. Instead, it is heavily delocalized over the entire molecule, specifically residing in an extensive three-center delocalized $\pi^*$ antibonding orbital spread largely over the highly electronegative oxygen atoms.
Step 3: The Barrier to Dimerization
Because the odd electron is heavily delocalized over the oxygen atoms rather than localized on the central Chlorine atom, there is no concentrated radical center available for a second molecule to effectively bond with. The highly diffuse nature of this radical completely suppresses the thermodynamic driving force for dimerization.
View Solution
Step 1: Analyze $I_3^-$ (Triiodide anion)
Central atom: Iodine. Valence $e^-$ = $7$. Add 1 for the negative charge = $8 e^-$.
It forms 2 single bonds with the other two Iodine atoms, using 2 $e^-$.
Remaining $e^-$ = 6, which equals 3 Lone Pairs.
Steric Number = 2 B.P. + 3 L.P. = 5 $\rightarrow$ $sp^3d$ hybridization.
To minimize $90^{\circ}$ repulsions, the 3 lone pairs occupy the equatorial plane. The two iodine atoms are forced into the axial positions.
Shape: Perfectly Linear ($180^{\circ}$).
Step 2: Analyze $I_3^+$ cation
Central atom: Iodine. Valence $e^-$ = $7$. Subtract 1 for the positive charge = $6 e^-$.
It forms 2 single bonds with the other two Iodine atoms, using 2 $e^-$.
Remaining $e^-$ = 4, which equals 2 Lone Pairs.
Steric Number = 2 B.P. + 2 L.P. = 4 $\rightarrow$ $sp^3$ hybridization.
The two lone pairs compress the bond angle slightly from the ideal tetrahedral angle.
Shape: Bent / V-shaped.
View Solution
Step 1: The Terminal Bonds
There are four terminal $B-H$ bonds. These are standard, coplanar, localized single bonds. Each uses 2 electrons.
Number of $2\text{c}-2\text{e}$ bonds = 4 (consuming 8 electrons total).
Step 2: The Bridge Bonds (Banana Bonds)
We have 4 electrons left to hold the two central Boron atoms and the two bridging Hydrogen atoms together. Standard bonding is impossible.
Instead, an $sp^3$ hybrid orbital from Boron-1, the 1s orbital of the bridging Hydrogen, and an empty $sp^3$ hybrid orbital from Boron-2 overlap to form a single, continuous, banana-shaped molecular orbital spanning three atoms.
Step 3: The 3c-2e classification
Two electrons drop into this massive orbital, binding all three atoms simultaneously. This is a three-center, two-electron ($3\text{c}-2\text{e}$) bond. There is one bridge above the plane and one below it.
View Solution
Step 1: Analyze $CO$ (Carbon Monoxide)
Structure: $:C \equiv O:$. It features a full triple bond (one sigma, two pi bonds, including one dative bond from oxygen).
Bond Order = 3.0.
Step 2: Analyze $CO_2$ (Carbon Dioxide)
Structure: $\ddot{O}=C=\ddot{O}$. It features two standard double bonds.
Bond Order = 2.0.
Step 3: Analyze $CO_3^{2-}$ (Carbonate Ion)
Structure: It has three equivalent resonance structures. A central Carbon is bonded to three Oxygens. The single double bond delocalizes equally across all three positions.
Fractional Bond Order = $\frac{\text{Total number of bonds}}{\text{Number of bonding positions}} = \frac{4}{3} = \mathbf{1.33}$.
Step 4: Conclusion
Higher bond order pulls the atoms closer together (shorter bond).
B.O. Sequence: $CO$ ($3.0$) > $CO_2$ ($2.0$) > $CO_3^{2-}$ ($1.33$).
Therefore, Bond Length Sequence is exactly the reverse.
View Solution
Step 1: Size Mismatch Rule
Lattice energy is highest when the cation and anion are of similar size. A large mismatch in size leads to poor packing and lower lattice energy.
Step 2: Analyze Hydroxides (Small Anion)
The $OH^-$ ion is very small. Down the group, the cation gets larger ($Mg^{2+} \rightarrow Ba^{2+}$). The mismatch increases, causing Lattice Energy to drop rapidly. Hydration energy also drops as cation size increases, but not as fast as the lattice energy plummets. Since breaking the lattice becomes increasingly easy, solubility increases down the group.
Step 3: Analyze Sulfates (Massive Anion)
The $SO_4^{2-}$ ion is massive. $Mg^{2+}$ is small, so there is a massive mismatch, meaning $MgSO_4$ has weak lattice energy and dissolves easily (assisted by high hydration energy of $Mg^{2+}$). As we move down to $Ba^{2+}$, the massive cation perfectly matches the massive sulfate anion. The Lattice Energy remains exceptionally strong and high due to perfect packing. However, the hydration energy drops rapidly because $Ba^{2+}$ is too large to attract water effectively. Because Hydration energy drops much faster than Lattice energy, solubility decreases heavily down the group.
View Solution
Step 1: Valence Electrons
Nitrogen has 5 valence electrons. Total = $3(5) + 1(\text{anion}) = 16 e^-$.
Step 2: The Best Resonance Structure
To satisfy octets with 16 electrons, we need a central Nitrogen double-bonded to two terminal Nitrogens: $[:\ddot{N}=N=\ddot{N}:]^-$.
Step 3: Calculate Formal Charges
- Terminal N 1: Valence = $5$. Non-bonding = $4$. Bonding = $4$ (2 bonds). F.C. = $5 - 4 - 2 = \mathbf{-1}$.
- Central N 2: Valence = $5$. Non-bonding = $0$. Bonding = $8$ (4 bonds). F.C. = $5 - 0 - 4 = \mathbf{+1}$.
- Terminal N 3: Symmetrical to N 1. F.C. = $\mathbf{-1}$.
Net charge = $(-1) + (+1) + (-1) = -1$ (Matches the ion's charge).
Step 4: Explosive Nature
Heavy separation of charge (adjacent positive and negative formal charges) makes the molecule thermodynamically highly unstable. It violently wants to rearrange to form the incredibly stable, neutral, triple-bonded $N_2$ gas. This massive release of energy and gas volume makes azides (like heavy metal azides) primary explosives.
View Solution
Step 1: Apply Fajan's Rules
Fajan's rule states that covalent character (polarization) increases with the size of the anion. The $Ag^+$ cation has a pseudo-noble gas configuration ($d^{10}$), giving it exceptionally high polarizing power.
Step 2: Analyze the Anions
The anion size increases dramatically: $Cl^- < Br^- < I^-$.
The massive $I^-$ ion holds its outer electrons very loosely. The $Ag^+$ ion violently distorts (polarizes) the electron cloud of the $I^-$ ion, pulling it deeply into the space between the two nuclei. This introduces massive covalent character to $AgI$.
Step 3: The Energy Gap (Color)
In a purely ionic lattice, transferring an electron from the anion back to the cation (Charge Transfer) requires massive energy (UV light, hence $AgCl$ is white/colorless). However, as polarization increases, the electron cloud is already physically pulled closer to the cation. The energy gap for this charge-transfer plummets into the visible light region.
$AgBr$ absorbs violet/blue light (appearing pale yellow). $AgI$ has such extreme polarization that the gap drops further, heavily absorbing blue/green light and appearing intensely yellow/orange.
View Solution
Step 1: Define Drago's Rule
Drago's rule states that if the central atom belongs to Group 15 or 16, is in the 3rd period or below, and the attached terminal atoms have an electronegativity of 2.5 or less (like Hydrogen), then hybridization does not occur.
Step 2: Analyze Phosphine ($PH_3$)
Phosphorus is in period 3. Hydrogen's electronegativity is 2.1. The energy gap between the 3s and 3p orbitals is large, and the weak electronegativity of H doesn't provide enough energy payoff to force hybridization. Therefore, Phosphorus simply uses its pure, unhybridized $3p_x$, $3p_y$, and $3p_z$ orbitals to bond with the Hydrogen 1s orbitals.
Step 3: The Geometric Outcome
Pure p-orbitals are exactly $90^{\circ}$ apart. Because $PH_3$, $AsH_3$, and $SbH_3$ use pure p-orbitals for bonding, their bond angles collapse to roughly $90^{\circ}$ (slightly widened by minor steric repulsion between the large hydrogens). The lone pair safely resides in the lower-energy, spherical pure s-orbital (making them very weak Lewis bases compared to $NH_3$).
View Solution
(a) Methane ($CH_4$): Tetrahedral. A plane can pass through the central Carbon and any two Hydrogen atoms. The other two Hydrogens will be above and below the plane. Maximum = 3 atoms.
(b) Ethene ($C_2H_4$): Both carbons are $sp^2$ hybridized. The entire molecule is perfectly flat. All atoms lie in the same plane. Maximum = 6 atoms.
(c) Allene ($C_3H_4$, $CH_2=C=CH_2$): The central carbon is $sp$ hybridized. The two double bonds are formed by mutually perpendicular p-orbitals. Therefore, the terminal $CH_2$ groups lie in planes that are exactly $90^{\circ}$ perpendicular to each other. A plane can pass through the 3 Carbons and the 2 Hydrogens of one end. Maximum = 5 atoms.
(d) Sulfur Hexafluoride ($SF_6$): Perfect Octahedral ($sp^3d^2$). A square plane passes through the central Sulfur and the 4 equatorial Fluorines. Maximum = 5 atoms.
View Solution
Step 1: Analyze Boron ($B_2$)
Boron has 10 total electrons. The configuration includes significant $s-p$ mixing, pushing the $\sigma_{2pz}$ orbital higher in energy than the degenerate $\pi_{2px}$ and $\pi_{2py}$ orbitals.
Configuration: $\sigma_{1s}^2 \sigma^*_{1s}^2 \sigma_{2s}^2 \sigma^*_{2s}^2 \pi_{2px}^1 \pi_{2py}^1$
The last 2 electrons enter the degenerate $\pi$ orbitals singly (parallel spins) following Hund's Rule. It has exactly 2 unpaired electrons. It is paramagnetic.
Step 2: Analyze Sulfur ($S_2$)
Sulfur exists as $S_2$ in the vapor phase at high temperatures. It is completely analogous to Oxygen ($O_2$), just utilizing $3s$ and $3p$ orbitals instead of $2s$ and $2p$.
Like $O_2$, its HOMO consists of the degenerate $\pi^*_{3px}$ and $\pi^*_{3py}$ antibonding orbitals. The final two electrons drop into these orbitals singly.
It has exactly 2 unpaired electrons. It is highly paramagnetic.
View Solution
Step 1: The Inert Pair Effect
Lead is at the very bottom of Group 14. Its valence shell is $6s^2 6p^2$. The inner $4f$ and $5d$ subshells shield the nucleus extremely poorly. Thus, the effective nuclear charge ($Z_{eff}$) heavily pulls on the penetrating $6s^2$ electrons, binding them tightly to the nucleus and making them reluctant to participate in bonding (they become "inert").
Step 2: The Energy Debt
To form $PbCl_4$, Lead must exhibit a $+4$ oxidation state. It must absorb a massive amount of promotional energy to unpair the tightly bound $6s^2$ electrons and excite one into the $6p$ subshell.
Step 3: Bond Energy Failure
Normally, forming two extra bonds releases enough energy to "pay back" this promotional energy debt. However, Lead is a massive atom. The $Pb-Cl$ bonds it forms are long and incredibly weak. The energy released by forming these weak bonds is insufficient to pay back the huge promotion energy. Thus, $PbCl_4$ is highly unstable and spontaneously drops back to the $+2$ state ($PbCl_2$).
Step 4: The Heavier Halogens
Bromine and Iodine are even larger. The $Pb-Br$ and $Pb-I$ bonds are so pathetically weak that the energy released doesn't even come close to covering the promotion energy. Thus, $PbBr_4$ and $PbI_4$ cannot even form in the first place.
View Solution
Step 1: Phosphate Ion ($PO_4^{3-}$)
Phosphorus is the central atom bonded to 4 Oxygens. To minimize formal charge, the best Lewis structure features one $P=O$ double bond and three $P-O^-$ single bonds. (Total 5 bonds shared across 4 positions).
Bond Order = $\frac{5 \text{ bonds}}{4 \text{ positions}} = \mathbf{1.25}$.
Step 2: Perchlorate Ion ($ClO_4^-$)
Chlorine is the central atom bonded to 4 Oxygens. To minimize formal charge, the best Lewis structure features three $Cl=O$ double bonds and one $Cl-O^-$ single bond. (Total 7 bonds shared across 4 positions).
Bond Order = $\frac{7 \text{ bonds}}{4 \text{ positions}} = \mathbf{1.75}$.
Step 3: Compare Bond Lengths
Higher bond order correlates with a stronger, shorter bond. The $Cl-O$ bond order is $1.75$ (closer to a double bond), while the $P-O$ bond order is $1.25$ (closer to a single bond).
View Solution
Step 1: Analyze o-Nitrophenol
In the ortho-isomer, the $-OH$ group and the $-NO_2$ group are perfectly adjacent to each other. The hydrogen of the hydroxyl group falls completely into the electrostatic trap of the nitro oxygen, forming a tight, 6-membered chelate ring via Intramolecular Hydrogen Bonding. Because the molecule "satisfies itself" internally, it ignores neighboring molecules. This lack of intermolecular stickiness results in low boiling points and high volatility (steam volatile).
Step 2: Analyze p-Nitrophenol
In the para-isomer, the $-OH$ and $-NO_2$ groups are on opposite ends of the benzene ring. They are too far apart to interact internally. Consequently, the $-OH$ of one molecule must hydrogen bond with the $-NO_2$ of a different molecule. This Intermolecular Hydrogen Bonding creates a massive, infinitely repeating polymeric chain in the solid state. This immense intermolecular network requires huge amounts of thermal energy to break, making it a high-melting, non-volatile solid.
View Solution
Step 1: The Ideal Benchmark ($CH_4$)
Methane has 4 Bonding Pairs (B.P.) and 0 Lone Pairs (L.P.). The 4 bonding pairs repel each other equally in 3D space, resulting in the mathematically perfect tetrahedral angle of $109.5^{\circ}$.
Step 2: The First Compression ($NH_3$)
Ammonia has 3 B.P. and 1 L.P. A lone pair is attracted to only one nucleus (Nitrogen), causing its electron cloud to mushroom outward, occupying significantly more physical space near the central atom than a bonding pair (which is stretched tight between two nuclei). According to VSEPR, repulsion follows the order: $L.P.-B.P. > B.P.-B.P.$. The bulky lone pair physically pushes the three bonding pairs closer together, compressing the angle from $109.5^{\circ}$ down to $107^{\circ}$.
Step 3: The Second Compression ($H_2O$)
Water has 2 B.P. and 2 L.P. Now, the dominant repulsion is $L.P.-L.P.$, which is the strongest repulsion force of all. The two massive lone pairs aggressively push each other apart, and in doing so, crush the two remaining bonding pairs even closer together, compressing the angle further down to $104.5^{\circ}$.
View Solution
Step 1: Static Shape of $SF_4$
Steric number = 5 (4 B.P., 1 L.P.). The bulky lone pair must occupy an equatorial position to minimize $90^{\circ}$ repulsions. This leaves 2 axial and 2 equatorial Fluorines, creating a See-Saw (or Teeter-Totter) shape.
Step 2: Static Shape of $ClF_3$
Steric number = 5 (3 B.P., 2 L.P.). Both bulky lone pairs occupy equatorial positions. This leaves 2 axial and 1 equatorial Fluorine, creating a bent T-Shape.
Step 3: The Berry Pseudorotation Mechanism
Molecules with 5-coordinate $sp^3d$ geometries are often highly fluxional. They undergo an internal molecular dance called Berry Pseudorotation. In this rapid process, the two axial bonds bend inward to become equatorial, while simultaneously, two of the equatorial bonds stretch outward to become axial. The transition state temporarily mimics a Square Pyramidal geometry.
Because this swapping occurs millions of times per second at room temperature, slow analytical techniques like NMR cannot "freeze" the frame, observing only a blurred time-average where all Fluorines appear identical. Cooling the sample to extreme sub-zero temperatures slows the dance, resolving the distinct axial and equatorial signals.
View Solution
Step 1: Analyze $Al_2Cl_6$ (Dative Bonding)
Aluminum has an empty orbital (electron deficient). Chlorine, however, has three full, non-bonding lone pairs. To dimerize, a Chlorine atom from one $AlCl_3$ molecule simply takes one of its lone pairs and donates it entirely into the empty orbital of the Aluminum atom on the other molecule. This forms a classic Coordinate Covalent (Dative) Bond. It is a standard $2\text{c}-2\text{e}$ bond, just formed by one atom donating both electrons.
Step 2: Analyze $B_2H_6$ (Banana Bonding)
Boron has an empty orbital. Hydrogen, however, has ONLY one electron, which is already used in the single $B-H$ bond. There are strictly zero lone pairs anywhere in the molecule. It is physically impossible to form a dative bond.
To dimerize, the two electrons already making up the $B-H$ bond must delocalize and stretch to cover a second Boron atom simultaneously. This creates a highly unusual $3\text{c}-2\text{e}$ (Three-center, two-electron) Banana bond.
View Solution
Step 1: Identify the Halogens
The central atom $X$ is a Period 4 halogen, which must be Bromine (Br). The surrounding atoms $Y$ must be a more electronegative halogen to force Bromine into a positive oxidation state. Thus, $Y$ must be Fluorine (F). The compound is $BrF_3$.
Step 2: Determine Shape of $BrF_3$
Bromine has 7 valence electrons. It forms 3 bonds with Fluorine, leaving 4 electrons = 2 Lone Pairs.
Steric Number = 3 B.P. + 2 L.P. = 5 $\rightarrow$ $sp^3d$ hybridization.
The two massive lone pairs occupy equatorial positions, pushing the axial fluorines slightly inward. The shape is a Bent T-Shape.
Step 3: Justify Dipole Moment
Because it is a Bent T-shape, the highly polar $Br-F$ bonds do not cancel each other out symmetrically (unlike a trigonal planar or linear molecule). The vector sum of the dipoles points away from the lone pairs, giving the molecule a strong, permanent non-zero dipole moment.
Step 4: Verify the Anion
Reaction with $F^-$ yields $BrF_4^-$. (Valence = $7 + 4(1) + 1 = 12 e^-$ = 4 B.P. and 2 L.P.). Steric number 6 ($sp^3d^2$). The lone pairs go trans to each other, forming a perfectly Square Planar (octahedral derivative) anion. The clues match perfectly.
Mastering the Architecture of Molecules
Congratulations on conquering these 25 ultra-challenging problems on Chemical Bonding! You have successfully navigated the advanced quantum nuances of Molecular Orbital Theory, the geometric fluxionality of Berry Pseudorotations, and the stark contrast between dative and electron-deficient multi-center bonds. Remember, in JEE Advanced, exceptions to the octet rule are not anomalies; they are the standard. Always evaluate steric numbers, back-bonding possibilities, and electronegativity differentials before assigning a final structure. Keep honing your spatial intuition, and visit Chemca.in for more elite masterclasses!
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