Liquids and Solids — Comprehensive Notes (Sections 12.1, 12.3–12.5)
Section 12.1 Intermolecular Forces
Condensed states are held together by forces called intermolecular forces (IMFs).
IMFs are weaker than intramolecular (chemical) bonds but govern physical properties (melting/boiling points, solubility, etc.).
Four types of intermolecular forces:
Ion–dipole attractions
Electrostatic interactions between ions and polar molecules.
Hydrated ions form by ion–dipole attractions.
Strongest type of IMF.
Example: salt water where ionic compounds dissolve in water.
Hydrogen bonds
Require two components:
A molecule with a partially positive hydrogen atom (a hydrogen donor).
A molecule with a partially negative N, O, or F atom (a hydrogen acceptor).
An attraction between the partially positive H in one molecule and the lone pair on N, O, or F in another molecule.
Dipole–dipole interactions (permanent dipole–dipole)
Polar molecules interact with other polar molecules via electrostatic attractions between oppositely charged ends.
London dispersion forces (dispersion forces)
Result from instantaneous dipoles due to random electron motion.
Induced dipoles in neighboring molecules lead to short-lived attractions.
Intramolecular vs Intermolecular Forces
Intramolecular forces occur within a molecule (covalent or ionic bonds); relatively strong and remain after physical processes.
Intermolecular forces occur between molecules; relatively weaker and are affected by physical processes (e.g., heating, phase changes).
Polar vs. non-polar molecules
Polar molecules have a permanent dipole moment (uneven charge distribution).
Non-polar molecules have no permanent dipole moment (even charge distribution).
Halogen size and polarizability (data related to IMFs)
Atomic Radius (pm) and Boiling Point (K) for halogens:
Fluorine:
Chlorine:
Bromine:
Iodine:
Types of Intermolecular Forces (Summary)
Strongest → Weakest order (conceptual):
Ion–dipole attractions (present in mixtures of ionic and polar compounds, e.g., NaCl dissolved in water).
Hydrogen bonding (between molecules containing H–donor and H–acceptor N, O, or F).
Dipole–dipole attractions (polar molecules, e.g., H2O, HCl).
London dispersion forces (all molecular substances and inert gases; e.g., H2O, HCl, Cl2, He, Ne).
Section 12.3 Phase Changes and Heating Curves
Phase changes and related terms:
Melting (fusion): solid → liquid
Freezing (solidification): liquid → solid
Vaporization (evaporation): liquid → gas
Condensation: gas → liquid
Sublimation: solid → gas
Deposition: gas → solid
Enthalpies associated with phase changes (per mole):
Heating curve (for a pure substance)
Temperature versus time as a substance is heated.
Plateaus occur at phase changes due to latent heat (no temperature change while changing phase).
Examples and calculations:
Problem: Identify the phase change for each equation:
(a) \ce{C{18}H{38}(s) -> C{18}H{38}(l)}
Melting (fusion).
(b) \ce{CO2(g) -> CO2(s)}
Deposition.
(c) \ce{NH3(l) -> NH3(g)}
Vaporization (boiling/evaporation).
Example: Energy required to melt 16.4 g of ice at 0°C with
Molar mass of water: M_{\ce{H2O}} = 18.015\ \text{g}\,\text{mol}^{-1}
Moles melted:
Energy:
Section 12.4 Vapor Pressure, Boiling Point, and the Clausius–Clapeyron Equation
Vapor pressure ( Pvap )
The equilibrium pressure of a vapor above its liquid or solid in a closed container.
At equilibrium, rate of evaporation equals rate of condensation.
Pvap increases with temperature; it is a function of intermolecular forces.
Boiling point (BP)
The temperature at which Pvap equals the ambient atmospheric pressure (P_{ ext{atm}}).
Example reference points for water at various elevations:
Sea level: BP =
Everest: BP ≈
Relationship among Pvap, BP, and IMFs
Substances with stronger IMFs tend to have lower Pvap at a given temperature and higher BP.
The Pvap–T curves differ for substances (e.g., diethyl ether, ethanol, water) due to IMF strength.
Clausius–Clapeyron equation (to relate Pvap at two temperatures)
General form (two states):
Alternative linear form: where C is a constant.
Universal gas constant:
In practice, use Pvap data at known temperatures to solve for or to predict Pvap at another temperature.
Example: Methanol
Given: Normal boiling point ; ; Measured vapor pressure at ; Assume .
Calculation steps:
Compute:
Product:
Result: The vapor pressure of methanol at is approximately .
Applications and notes
The Clausius–Clapeyron equation enables extraction of enthalpies from Pvap data and vice versa.
Pvap data and BP are practical indicators of how substances will behave under heating, cooling, or reduced/augmented pressure conditions.
Section 12.5 Phase Diagrams
Phase diagrams show the phase (solid, liquid, gas) of a substance under all possible pressure–temperature (P–T) combinations.
Key features of a generic phase diagram:
Regions corresponding to solid, liquid, and gas phases.
Lines separating phases depict equilibria between phases (fusion/melting line, vaporization/condensation line, sublimation/deposition line).
Points of interest:
Triple point: the single point where all three phases are in equilibrium; lines intersect there.
Critical point: above this P–T location, the substance no longer exists as a distinct liquid; liquid and gas become indistinguishable (supercritical fluid).
Normal melting point: the temperature at which the solid melts at 1 atm.
Normal boiling point: the temperature at which the vapor pressure equals 1 atm.
Reading and interpreting phase diagrams
Identify phase in each region (solid, liquid, gas).
Determine the phase boundary for solid–gas equilibrium (sublimation/deposition line).
Locate the normal boiling point on the temperature axis by finding the point where Pvap equals 1 atm.
Conceptual use
Phase diagrams predict phase changes when changing temperature or pressure (
e.g., heating/cooling at constant pressure or compression/expansion at constant temperature).
Example interpretation task (from slides)
a) Identify the phase(s) in regions A, B, and C.
b) Identify the line where the solid and gas phases are in equilibrium (sublimation line).
c) Identify the point indicating the normal boiling point (where Pvap = 1 atm).
Note: The exact labels A, B, C depend on the specific diagram provided, but the concepts remain the same.