Liquids and Intermolecular Forces

A Molecular Comparison of Gases, Liquids, and Solids

  • The three states of matter represent a balance (or competition) between two opposing factors:     * Kinetic energy of individual particles: Keeps particles in motion.     * Attractive forces between particles (intermolecular forces): Tends to draw particles together.
  • Gaseous State:     * Kinetic energy is the dominant factor.     * Particle motion greatly exceeds the strength of intermolecular attractions.     * Intermolecular forces are very weak or negligible.     * Particles are far apart, leading to no definite shape or volume and a high degree of compressibility.
  • Liquid State:     * There is a balanced relationship between kinetic energy and attractive forces.     * Particles possess enough kinetic energy to move past one another (allowing flow).     * Intermolecular forces are strong enough to keep particles close together.     * Liquids have a definite volume but no definite shape.
  • Solid State:     * Attractive forces are dominant.     * Strong interactions hold particles in fixed positions relative to each other.     * Kinetic energy is low; particles only vibrate about equilibrium positions.     * Solids possess both a definite shape and a definite volume.

Intermolecular Forces (IMF’s\text{IMF's})

  • Definition: Attractions among molecules.
  • Comparison: IMFs are significantly weaker than intramolecular attractions (atomic bonds) that hold individual molecules together.     * Metaphor: IMFs are described as a "gentle handshake" in the microscopic world.
  • Role: IMFs determine physical properties, including:     * Boiling points     * Melting points     * Vapor pressure     * Viscosity

Types of Intermolecular Forces (IMFs\text{IMFs})

  • In pure liquids or solids, interactions typically occur between identical molecules.
  • Ordered list from weakest to strongest:     1. London dispersion forces (LDFs\text{LDFs})     2. Dipole–dipole interactions     3. Hydrogen bonding

London Dispersion Forces (LDFs\text{LDFs})

  • Origin: Arise from the constant, random motion of electrons within atoms and molecules. All substances with electrons exhibit LDFs.
  • Mechanism:     * Motion of electrons can momentarily create an instantaneous dipole due to uneven electron density distribution.     * One region becomes slightly negative; another becomes slightly positive.     * This temporary dipole induces a dipole in a neighboring particle, resulting in a weak, short-lived attraction.
  • Characteristics: The weakest IMF due to its transitory nature.
  • Factors influencing strength:     * Number of electrons (molar mass): More electrons result in electron clouds that are held less tightly and are more polarizable (often described as "squishier"), leading to stronger LDFs.     * Molecular shape:         * Elongated or flat molecules: Large surface area for contact with neighbors, allowing more dispersion interactions.         * Compact or spherical molecules: Fewer contact points, resulting in weaker dispersion forces.
  • Importance: Particularly critical for neutral atoms and nonpolar molecules where LDFs are the only forces present.     * Explains why noble gases can form liquids/solids under low temperature and/or high pressure.
Table 11.1: Normal Melting and Boiling Points of Selected Substances
SubstanceMolar Mass (g/molg/mol)Melting Point (extC^∘ ext{C})Boiling Point (extC^∘ ext{C})
Ar\text{Ar}4040189.4-189.4185.9-185.9
Xe\text{Xe}131131111.8-111.8108.1-108.1
N2\text{N}_22828210-210195.8-195.8
O2\text{O}_23232218.8-218.8183.0-183.0
F2\text{F}_23838219.7-219.7188.1-188.1
I2\text{I}_2254254113.7113.7184.4184.4
CH4\text{CH}_41616182.5-182.5161.5-161.5
  • Observations from Table 11.1: As molar mass and polarizability increase, LDFs strengthen, requiring more kinetic energy to separate molecules, thus increasing melting and boiling points.
Shape Case Study: Alkanes
  • n-pentane: Elongated shape, greater surface contact; liquid at room temperature.
  • neopentane: Compact, nearly spherical shape; gas at room temperature.
  • Note: Both are structural isomers with the same molar mass.

Dipole-Dipole Interactions

  • Definition: Attractions between permanent dipoles in polar molecules.
  • Nature: Molecules in liquids experience both attractive and repulsive dipole-dipole interactions simultaneously. They orient to maximize attraction and minimize repulsion.
  • Range: Only significant when molecules are very close; strength decreases rapidly with distance.
  • Factors influencing strength:     * Electronegativity difference: Larger differences produce more polar bonds and larger dipole moments (μ\mu), resulting in stronger attractions.     * Distance: Forces strengthen as distance between molecules decreases.     * Molecular orientation: Head-to-tail and anti-parallel orientations are the strongest.     * Molecular size and shape: Smaller molecules can approach more closely; more surface contact allows better dipole alignment.
  • Independence from mass: Unlike LDFs, dipole-dipole strength does not explicitly depend on molar mass.
Table 11.2: Dipole Moment and Boiling Point for Organic Compounds (Similar Molar Mass)
SubstanceFormulaMolar Mass (g/molg/mol)Dipole Moment (DD)Boiling Point (KK)
CyclopentaneC3extH6\text{C}_3 ext{H}_6404000240240
Dimethyl etherCH3extOCH3\text{CH}_3 ext{OCH}_346461.301.30248248
AcetonitrileCH3extCN\text{CH}_3 ext{CN}41413.93.9355355

Hydrogen Bonding

  • Definition: A particularly strong form of dipole-dipole interaction, often called the "strongest of the weak."
  • Requirement: Hydrogen must be covalently bonded to a highly electronegative atom (N\text{N}, O\text{O}, or F\text{F}) and be attracted to a lone pair on a neighboring N\text{N}, O\text{O}, or F\text{F} atom.
  • Mechanism: The highly electronegative atoms draw electron density away from hydrogen, leaving its proton weakly shielded. This exposed positive charge is strongly attracted to lone pairs (regions of high electron density).
  • Terminology:     * Hydrogen bond donor: The H atom bonded to N\text{N}, O\text{O}, or F\text{F}.     * Hydrogen bond acceptor: The lone pair on a neighboring N\text{N}, O\text{O}, or F\text{F}.
  • Geometry: Strongest when the three involved atoms are colinear (approx. 180180^∘). Bent bonds can occur in strained environments (down to 120120^∘).
  • Physical Effects: Leads to anomalously high boiling points for compounds like HF\text{HF}, NH3\text{NH}_3, and H2extO\text{H}_2 ext{O} compared to other members of their groups with higher molar masses.
The Unique Properties of Water
  • Density: Water's solid state (ice) is less dense than its liquid state.
  • Structure of Ice: Each water molecule forms up to four hydrogen bonds. This favors a nearly linear, open, cage-like structure with significant empty space.
  • Liquid Phase: Hydrogen bonds constantly form and break, allowing molecules to pack more closely in a disordered arrangement, increasing density.
  • Biological Importance: Ice floats, insulating liquid water below and allowing aquatic life to survive in winter.
  • Practical Consequence: Water expands upon freezing, which can cause household pipes to burst.

Comparing Relative Strengths of IMFs

  • Analogy (Household Fasteners):     * LDFs: A small square of Velcro (weak individually, but numerous).     * Dipole–dipole: A refrigerator magnet strip.     * Hydrogen bonding: A neodymium magnet (very strong for its size).
  • Impact of Molar Mass: Though typically weak, the cumulative effect of many LDFs can dominate. A long strip of Velcro (high molar mass) is harder to separate than a single neodymium magnet.
  • Guidelines for Comparison:     1. Similar Molar Masses: The substance with the stronger type of IMF (H-bond > Dip-Dip > LDF) has higher melting/boiling points.     2. Large Molar Mass Differences (60100g/mol≈ 60\text{--}100\,g/mol): The higher molar mass substance typically has higher points, even if it is nonpolar.     3. Nonpolar Substances: Elongated > compact/branched due to surface contact.
  • Organic Molecules Notes:     * C–H\text{C--H} bonds are effectively nonpolar.     * Hydrocarbons (only C\text{C} and H\text{H}) are nonpolar; show only LDFs.     * Presence of F\text{F}, O\text{O}, or N\text{N} can introduce polarity (Dip-Dip) and H-bonding if H is bonded directly to N\text{N} or O\text{O}.

Example 11.1: IMF Determination and Ranking

SetSubstancesApprox MMDominant IMFsBP Ranking (High to Low)
Aa. CH3extCH2extCH2extOH\text{CH}_3 ext{CH}_2 ext{CH}_2 ext{OH} / b. CO2\text{CO}_2 / c. SO2\text{SO}_2a: 60, b: 44, c: 64a: LDF, H-bond; b: LDF; c: LDF, Dip-Dipa > c > b
Ba. C<em>9extH</em>10\text{C}<em>9 ext{H}</em>{10} / b. C3extH8\text{C}_3 ext{H}_8a: 118, b: 44a: LDF (many); b: LDF (few)a > b
Ca. CH3extCl\text{CH}_3 ext{Cl} / b. CH3extCH2extOH\text{CH}_3 ext{CH}_2 ext{OH}a: 50, b: 46a: LDF, Dip-Dip; b: LDF, H-bondb > a

Select Properties of Liquids

Surface Tension

  • Definition: The property of a liquid surface enabling it to resist external forces; behaves like a thin elastic film.
  • Origin: Cohesive IMFs.     * Interior molecules: Experience attractive forces in every direction; net force is zero.     * Surface molecules: Lack neighbors above, experiencing a net inward force toward the bulk.
  • Effect: Inward pull minimizes surface area, creating spherical droplets.
  • Quantitative Definition: Force per unit length (N/mN/m) needed to increase surface area.
  • Example: Mosquito reproduction is supported by surface tension on undisturbed water.

Capillary Action

  • Definition: Ability of a liquid to rise against gravity in a narrow space.
  • Factors:     * Adhesive forces: Attraction between liquid and the surface (e.g., water and polar SiO2\text{SiO}_2 in glass).     * Cohesive forces: Attractions within the liquid (e.g., H-bonds in water).
  • Equilibrium: Liquid rises until its weight balances the IMFs. Narrower tubes produce higher columns. Denser liquids produce shorter columns.
  • Meniscus Shape:     * Concave (Water): Adhesive forces > Cohesive forces. Water "wets" the glass.     * Convex (Mercury): Cohesive forces > Adhesive forces. Mercury does not wet the glass.
  • Biological/Practical Roles: Xylem in plants, cellulose fibers in paper towels, tear ducts in eyes.

Viscosity

  • Definition: Measure of a fluid’s resistance to flow; reflects internal friction.
  • Measurement: Time for a liquid to flow through a tube or metal sphere fall rate.
  • Factors influencing viscosity:     * Temperature (most important):         * Liquids: T,extViscosityT ↑, ext{Viscosity} ↓ (Thermal energy overcomes IMFs).         * Gases: T,extViscosityT ↑, ext{Viscosity} ↑ (More molecular collisions).     * Intermolecular Forces: Stronger IMFs result in higher viscosity.     * Molecular Structure: Large/complex/irregular shapes become entangled, increasing viscosity.
  • Unit: Measured in poise (mPasmPa ⋅ s).
Table 11.4: Viscosities at 25extC25^∘ ext{C}
SubstanceFormulaViscosity (poise)
WaterH2extO\text{H}_2 ext{O}0.8900.890
EthanolCH3extCH2extOH\text{CH}_3 ext{CH}_2 ext{OH}1.0741.074
Ethylene glycolCH2(extOH)extCH2(extOH)\text{CH}_2( ext{OH}) ext{CH}_2( ext{OH})16.116.1
Motor OilLong hydrocarbons50500\approx 50\text{--}500
HoneyVariable, high OH groups2,00010,000\approx 2,000\text{--}10,000

Phase Changes

  • Phase transitions occur when energy (heat) is added or removed, establishing or breaking IMFs.
  • Temperature: Remains constant during a phase change because energy is used for state change, not kinetic energy increase.

Types of Phase Transitions

  • Endothermic (+ΔH+ΔH) (Require energy input to weaken IMFs):     * Melting (Fusion): Solid to liquid.     * Vaporization (Boiling): Liquid to gas.     * Sublimation: Solid to gas (e.g., dry ice).
  • Exothermic (ΔH-ΔH) (Release energy as particles slow):     * Freezing: Liquid to solid.     * Condensation: Gas to liquid.     * Deposition: Gas to solid (e.g., frost).

Heating and Cooling Curves

  • Diagonal Segments: Substance warming/cooling within one phase. Calculated by:     Q=mCsΔTQ = mC_sΔT     * QQ: Heat (JJ or kJkJ)     * mm: Mass (gg)     * CsC_s: Specific heat capacity (Jg1K1J ⋅ g^{-1} ⋅ K^{-1})     * ΔTΔT: Temperature change.
  • Horizontal Plateaus: Phase changes. Calculated by latent heat:     Q=mΔHQ = mΔH or Q=nΔHQ = nΔH     * ΔHΔH: Latent heat (kJ/gkJ/g or kJ/molkJ/mol).
  • Types of Latent Heat:     * Heat of Fusion (ΔHfusΔH_{\text{fus}}): Solid to liquid at melting point.     * Heat of Vaporization (ΔHvapΔH_{\text{vap}}): Liquid to gas at boiling point.     * Comparison: 0˘394Hvap\u0394H_{\text{vap}} is generally much larger than 0˘394Hfus\u0394H_{\text{fus}} because separating molecules into a gas requires more energy than loosening them into a liquid.

Example 11.2: Total Energy Calculation for Water

  • Mass: 137.1mol×18.01528g/mol=2,469.89g137.1\,mol × 18.01528\,g/mol = 2,469.89\,g
  • Stages from 22.0extC-22.0^∘ ext{C} to 137.0extC137.0^∘ ext{C}:     1. Heating Solid (22.0-22.0 to 0extC0^∘ ext{C}): QI=(2469.89g)(2.05J/gK)(22.0K)=111,392JQ_I = (2469.89\,g)(2.05\,J/gK)(22.0\,K) = 111,392\,J     2. Melting: QII=(2.46989kg)(334kJ/kg)=824.94kJQ_{II} = (2.46989\,kg)(334\,kJ/kg) = 824.94\,kJ     3. Heating Liquid (00 to 100extC100^∘ ext{C}): QIII=(2469.89g)(4.1813J/gK)(100.0K)=1,032,735JQ_{III} = (2469.89\,g)(4.1813\,J/gK)(100.0\,K) = 1,032,735\,J     4. Vaporizing: QIV=(2.46989kg)(2264.76kJ/kg)=5,593.708kJQ_{IV} = (2.46989\,kg)(2264.76\,kJ/kg) = 5,593.708\,kJ     5. Heating Gas (100.0100.0 to 137.0extC137.0^∘ ext{C}): QV=(2469.89g)(2.080J/gK)(37.0K)=190,082JQ_V = (2469.89\,g)(2.080\,J/gK)(37.0\,K) = 190,082\,J
  • Total Energy (QTQ_T): QI+QII+QIII+QIV+QV=7,750.85kJ7.751×103kJQ_I + Q_{II} + Q_{III} + Q_{IV} + Q_V = 7,750.85\,kJ ≈ 7.751 × 10^3\,kJ.

Example 11.3: Final State Problem for Benzene

  • Given: 12.00g12.00\,g Benzene, Ti=10.0extCT_i = -10.0^∘ ext{C}, Heat Added = 2.10kJ2.10\,kJ.     1. Heat solid to 5.5extC5.5^∘ ext{C}: Q=(12.00g)(1.25J/gextC)(15.5extC)=0.2325kJQ = (12.00\,g)(1.25\,J/g^∘ ext{C})(15.5^∘ ext{C}) = 0.2325\,kJ. Energy left: 1.86kJ1.86\,kJ.     2. Melting process: n=12.00g/78.11g/mol=0.1536moln = 12.00\,g / 78.11\,g/mol = 0.1536\,mol. Q=(9.8kJ/mol)(0.1536mol)=1.505kJQ = (9.8\,kJ/mol)(0.1536\,mol) = 1.505\,kJ. Energy left: 0.3625kJ0.3625\,kJ.     3. Remaining energy (362.5J362.5\,J) used to heat liquid: 362.5=(12.00g)(1.70J/gextC)(Tf5.5)362.5 = (12.00\,g)(1.70\,J/g^∘ ext{C})(T_f - 5.5).
  • Result: Tf=23.26extCT_f = 23.26^∘ ext{C} (Rounded to 20extC20^∘ ext{C} based on sig figs); Benzene is liquid.

Vapor Pressure

  • Definition: Pressure exerted by a vapor in equilibrium with its liquid in a closed system.
  • Maxwell–Boltzmann Distribution: Particles in a liquid have a range of kinetic energies. Higher temperature leads to a larger fraction of particles at higher energies.
  • Escape Energy (E0E_0): Threshold energy needed for a particle at the surface to overcome IMFs and evaporate.
  • Dynamic Equilibrium: Occurs when rate of evaporation = rate of condensation. At this point, vapor pressure is measured.
  • Factors influencing Vapor Pressure:     * Temperature: Higher TT increases the number of particles with energy > E0E_0, increasing vapor pressure.     * Intermolecular Forces: Stronger IMFs increase E0E_0, resulting in lower vapor pressure.
  • Volatility:     * Volatile: Liquids with weak IMFs and high vapor pressure; evaporate readily.     * Nonvolatile: Liquids with strong IMFs and low vapor pressure.

Boiling Point (BPBP)

  • Definition: Temperature where vapor pressure equals external atmospheric pressure.
  • Bubble Formation: Boiling occurs throughout the bulk of the liquid. Bubbles collapse if vapor pressure < atmospheric pressure.
  • Normal Boiling Point: Boiling point at a standard pressure of 1atm1\,atm.
  • Pressure Effect: Boiling point varies with external pressure. Lower pressure results in lower boiling points.

Phase Diagrams

  • Map showing the stable physical state at various temperatures (xx-axis) and pressures (yy-axis).
  • Components:     * Regions: Temperature/pressure ranges for solid, liquid, or gas.     * Phase Boundaries: Lines where two phases coexist in equilibrium.     * Triple Point (Ttp,PtpT_{\text{tp}}, P_{\text{tp}}): Only condition where solid, liquid, and gas coexist.     * Critical Point (Tc,PcT_c, P_c): End of the liquid-gas boundary. beyond this, a supercritical fluid exists (gas-like mobility, liquid-like density).

Comparing Substances

  • Carbon Dioxide (CO2\text{CO}_2):     * Weak LDFs result in low critical parameters.     * Triple point pressure > 1atm1\,atm (5.11atm5.11\,atm). Therefore, liquid CO2\text{CO}_2 cannot exist under normal atmospheric conditions; it sublimes.
  • Water (H2extO\text{H}_2 ext{O}):     * Strong H-bonding causes a left-sloping solid-liquid boundary.     * This unique slope indicates that increasing pressure can melt ice (due to liquid water's higher density).     * Triple point is well below 1atm1\,atm, allowing liquid water to exist at Earth's surface.
Problem 11.2
  • Estimation from water phase diagram at 150atm150\,atm: Both the melting and boiling points change relative to normal values (0extC0^∘ ext{C} and 100extC100^∘ ext{C}), with the boiling point increasing significantly and the melting point decreasing slightly.