AP CHEMISTRY • PROPERTIES OF SUBSTANCES AND MIXTURES

Properties of Solids

Understanding how atomic-level bonding and structure determine the macroscopic properties of crystalline and amorphous solids.

Historical Context & Motivation

Humanity's understanding of the solid state has evolved dramatically over millennia, from the empirical metallurgy of ancient civilizations to the precise crystal-structure determinations made possible by modern diffraction techniques. Early natural philosophers categorized matter by observable properties—hardness, luster, and cleavage—but lacked the conceptual tools to explain why certain solids conducted electricity while others did not, or why some shattered along planar surfaces while others deformed plastically. The quest to connect microscopic structure with macroscopic behavior has driven some of chemistry's and physics's most consequential breakthroughs, from the discovery of X-ray diffraction to the band theory of electronic structure.

1669
Steno's Law of Constancy of Angles
Nicolaus Steno observed that the angles between corresponding faces of quartz crystals are constant regardless of crystal size, hinting at an internal periodic arrangement of matter long before atomic theory was formalized.
1848
Bravais Lattices
Auguste Bravais mathematically proved that only 14 distinct three-dimensional lattice types exist, providing the foundational framework for classifying crystalline solids that persists in modern crystallography.
1912
X-Ray Diffraction by Crystals
Max von Laue demonstrated that crystals diffract X-rays, confirming the periodic atomic arrangement of crystalline solids. This technique became the gold standard for structure determination.
1913
Bragg's Law
William Henry and William Lawrence Bragg derived the relationship nλ = 2d sin θ, enabling precise measurement of interplanar spacing in crystals and ushering in quantitative solid-state chemistry.
1984
Discovery of Quasicrystals
Dan Shechtman observed a diffraction pattern with five-fold symmetry in a rapidly cooled Al–Mn alloy, revealing a new class of ordered but non-periodic solids that expanded the definition of crystallinity.

These milestones collectively shaped a central question that still drives AP Chemistry and materials science: How do the type and strength of interparticle forces within a solid determine its melting point, hardness, electrical conductivity, and other macroscopic properties? Answering this question requires classifying solids by their bonding type—ionic, metallic, covalent-network, and molecular—and understanding how the resulting structures manifest in measurable physical behavior.

Core Principles & Definitions

A solid is a phase of matter in which constituent particles—atoms, ions, or molecules—occupy fixed positions and resist both changes in shape and volume. Unlike gases and liquids, solids exhibit long-range structural order (in crystalline solids) or only short-range order (in amorphous solids). The properties a solid displays at the macroscopic level—melting point, hardness, electrical and thermal conductivity, malleability, and solubility—are direct consequences of the type and strength of interparticle forces holding its constituents in place. In AP Chemistry, four principal categories of crystalline solids are recognized, each defined by a distinct bonding model.

1

Ionic Solids

Composed of cations and anions held in a lattice by strong electrostatic (Coulombic) attractions. High melting points, brittle, conduct electricity only when dissolved or molten. Example: NaCl.
2

Metallic Solids

Metal cations arranged in a lattice surrounded by a delocalized sea of electrons. Good thermal and electrical conductors, malleable, ductile, with variable melting points. Example: Cu.
3

Covalent-Network Solids

Atoms connected by an extended three-dimensional network of strong covalent bonds. Extremely high melting points, very hard, generally poor electrical conductors (graphite is an exception). Example: SiO₂ (quartz), diamond.
4

Molecular Solids

Discrete molecules held together by relatively weak intermolecular forces (London dispersion, dipole–dipole, or hydrogen bonding). Low melting points, soft, poor conductors. Example: ice (H₂O), sucrose (C₁₂H₂₂O₁₁).
KEY TAKEAWAY
Think of the four solid types as buildings constructed with different fasteners. Ionic solids use bolts (strong but brittle under lateral stress). Metallic solids use rivets in sliding tracks (strong yet deformable). Covalent-network solids are welded steel frameworks (incredibly rigid). Molecular solids are assembled with Velcro (easy to pull apart). The nature of the fastener dictates the building's strength, just as the type of interparticle force dictates the solid's macroscopic properties.

Visual Explanation — Solid Types at the Particle Level

Top row: particle-level depictions of the four crystalline solid types. Ionic shows alternating cations/anions; metallic shows cations in a delocalized electron sea (small cyan dots); covalent-network shows continuous covalent bonds between atoms; molecular shows discrete H₂O molecules connected by dashed lines representing hydrogen bonds. Bottom bar: general trend of increasing melting points across the four types.

The diagram above illustrates the fundamental structural differences among the four categories of crystalline solids. In the ionic panel, note the alternating arrangement of differently sized and oppositely charged ions—there are no discrete "NaCl molecules" in the solid. The metallic panel emphasizes the small, mobile electrons (cyan dots) delocalized throughout the lattice, which accounts for both electrical conductivity and malleability. The covalent-network panel shows every atom covalently bonded to its neighbors in a continuous framework; breaking such a solid requires cleaving actual covalent bonds, explaining its extreme hardness and melting point. Finally, the molecular panel shows intact H₂O molecules connected only by dashed intermolecular forces—comparatively weak, which is why molecular solids have the lowest melting points. The bottom bar summarizes the general trend: melting point increases as the interparticle forces transition from intermolecular forces to full covalent-network bonds.

Mathematical Framework — Coulomb's Law & Lattice Energy

The measurable properties of ionic solids can be rationalized quantitatively through Coulomb's law and the concept of lattice energy. Although the AP Chemistry exam does not require detailed Born–Haber cycle calculations, understanding how ionic charge magnitude and ionic radius influence the strength of ionic interactions—and therefore melting point and hardness—is essential. The same Coulombic reasoning extends qualitatively to the relative strengths of metallic bonds (higher charge density → stronger metallic bonding) and to comparing London dispersion forces among molecular solids (more electrons → greater polarizability → stronger LDFs).

COULOMB'S LAW (ELECTROSTATIC FORCE)
F = k × (q₁ × q₂) / d²
F = electrostatic force between two ions; k = Coulomb's constant (8.99 × 10⁹ N·m²/C²); q₁, q₂ = charges on the ions; d = distance between ion centers (sum of ionic radii). Greater charges and smaller interionic distances produce stronger attractive forces and higher melting points.
LATTICE ENERGY (MAGNITUDE TREND)
U_lattice ∝ (|q₊| × |q₋|) / (r₊ + r₋)
Lattice energy is the energy required to completely separate one mole of a solid ionic compound into gaseous ions. It is directly proportional to the product of ionic charge magnitudes and inversely proportional to the sum of the ionic radii. Larger lattice energies correspond to higher melting points, greater hardness, and lower solubility (in general).
LONDON DISPERSION FORCES (QUALITATIVE TREND)
Strength of LDF ∝ molar mass ∝ number of electrons ∝ polarizability
For nonpolar molecular solids, the primary intermolecular force is London dispersion. Larger, more electron-rich molecules have greater polarizability and thus stronger temporary dipole attractions, leading to higher melting and boiling points. This explains why I₂ (s) melts at 114 °C while F₂ (g) boils at −188 °C.
💡 AP Exam Tip
On the AP Chemistry exam, you will frequently be asked to rank substances by melting point. The key strategy is: (1) identify the solid type for each substance, (2) if they are the same type, compare the strength of the specific forces (e.g., charge and size for ionic, molar mass and IMF type for molecular). Never compare across categories using a single metric—e.g., molar mass alone does not predict that NaCl melts higher than glucose.

Detailed Classification — Properties by Solid Type

Comprehensive comparison of properties for the four types of crystalline solids.
PropertyIonicMetallicCovalent-NetworkMolecular
ParticlesCations & anionsCations & delocalized e⁻Atoms (covalently bonded)Discrete molecules
Force holding latticeCoulombic (ion–ion)Metallic bondingCovalent bondsIMFs (LDF, dipole–dipole, H-bonding)
Melting pointHigh (e.g., NaCl: 801 °C)Variable (Hg: −39 °C; W: 3422 °C)Very high (diamond: ~3550 °C)Low (ice: 0 °C; CO₂: −78 °C sub.)
HardnessHard but brittleVariable; often malleable/ductileVery hardSoft
Electrical conductivity (solid)No (ions fixed)Yes (mobile e⁻)No (exception: graphite)No
Electrical conductivity (molten/dissolved)Yes (mobile ions)Yes (liquid metal)N/A (decomposes)No
Solubility in waterOften soluble (polar solvent)InsolubleInsolublePolar in polar; nonpolar in nonpolar
ExamplesNaCl, MgO, CaF₂Cu, Fe, Au, NaDiamond, SiO₂, SiCIce, I₂, sucrose, CO₂
A decision flowchart for classifying a crystalline solid. Begin by asking whether the substance is a metal, then whether it is composed of metal and nonmetal ions, then whether it forms an extended covalent network. If the answer to all prior questions is no, the solid is molecular.

The flowchart provides a systematic decision pathway that mirrors common AP Chemistry exam questions. When confronted with an unfamiliar substance, begin with composition: if the substance is a pure metal or an alloy, it is a metallic solid. If it combines a metal cation with a nonmetal anion (or polyatomic ions), classify it as ionic. For solids composed entirely of nonmetals, the distinguishing criterion is whether the substance forms a continuous covalent-bond network (like SiO₂ or diamond) or consists of distinct molecular units (like CO₂ or naphthalene). Covalent-network solids will have characteristically extremely high melting points and exceptional hardness, whereas molecular solids will melt and boil at much lower temperatures. Remember that graphite is a special case: it is a covalent-network solid with delocalized π-electrons in its planar layers, giving it electrical conductivity parallel to its planes.

Worked Example — Ranking Melting Points

Rank the following solids from lowest to highest melting point: NaCl, SiO₂, CO₂, and Fe.
1
Step 1 — Classify Each SolidIdentify the type of solid each substance forms. NaCl is composed of Na⁺ and Cl⁻ ions → ionic solid. SiO₂ (quartz) is a nonmetal network where each Si atom is covalently bonded to four O atoms in an extended 3D lattice → covalent-network solid. CO₂ in the solid state (dry ice) consists of discrete, nonpolar CO₂ molecules → molecular solid. Fe is a transition metal → metallic solid.
CO₂ = molecular; NaCl = ionic; Fe = metallic; SiO₂ = covalent-network
2
Step 2 — Apply the General Melting-Point TrendThe general trend is: molecular < metallic (variable) < ionic < covalent-network. Molecular solids have the weakest interparticle forces (only IMFs), so CO₂ will have the lowest melting point. Covalent-network solids require breaking strong covalent bonds to melt, so SiO₂ will have the highest. The metallic solid (Fe) and ionic solid (NaCl) fall between these extremes.
3
Step 3 — Compare Fe and NaCl More CarefullyIron is a transition metal with strong metallic bonding due to partially filled d-orbitals contributing to the metallic bond. Its melting point is 1538 °C. NaCl has singly charged ions (Na⁺ and Cl⁻), giving a melting point of 801 °C. Here, the metallic bonding in Fe is stronger than the Coulombic interactions in NaCl. Note that this order can vary—for example, MgO (mp ≈ 2852 °C) would rank above Fe because of its doubly charged ions and small ionic radii.
4
Step 4 — Confirm with Known Data and State Final RankingCO₂ sublimes at −78 °C (does not melt under 1 atm), NaCl melts at 801 °C, Fe melts at 1538 °C, and SiO₂ melts at approximately 1713 °C. These values confirm our reasoning based on interparticle forces.
Lowest → Highest: CO₂ (−78 °C) < NaCl (801 °C) < Fe (1538 °C) < SiO₂ (~1713 °C)
⚠️ Common Pitfall
Students often mistakenly rank all ionic solids above all metallic solids. In reality, metallic bonding strength varies enormously—mercury is liquid at room temperature, while tungsten melts at 3422 °C. Always consider the specific identity of the substance and the strength of its particular interparticle forces before applying the general trend.

Crystalline vs. Amorphous Solids

Not all solids fall neatly into the four crystalline categories. Amorphous solids lack the long-range periodic order that defines crystals; their atoms or molecules are arranged irregularly, much like a liquid that has been frozen in place without the time to organize. Common examples include glass (SiO₂ with disordered bonding), many polymers (e.g., polyethylene, rubber), and rapidly cooled metals (metallic glasses). The distinction between crystalline and amorphous solids has important practical and conceptual consequences that occasionally appear on the AP exam.

Comparison of crystalline and amorphous solids.
FeatureCrystalline SolidAmorphous Solid
Long-range orderYes — repeating unit cellNo — only short-range order
Melting behaviorSharp melting pointSoftens over a range (glass transition)
CleavageBreaks along defined planesFractures irregularly (conchoidal)
X-ray diffractionSharp, well-defined peaksBroad, diffuse bands
ExamplesQuartz, NaCl, diamond, iceWindow glass, rubber, plastics
KEY TAKEAWAY
The defining characteristic of a crystalline solid is its sharp melting point—the temperature at which the lattice's long-range order collapses simultaneously. An amorphous solid, by contrast, softens gradually because there is no uniform lattice to disassemble. Think of it like a neatly stacked wall of identical bricks (crystalline) versus a pile of irregularly shaped stones cemented together (amorphous): the brick wall collapses cleanly under stress at a defined threshold, while the stone pile crumbles unpredictably over a range of applied forces.

Connection to Advanced Theory — Band Theory & Materials Science

The AP Chemistry classification of solids by bonding type provides a powerful predictive framework, but advanced materials science goes further by invoking band theory to explain electrical and optical properties. In a solid composed of N atoms, atomic orbitals combine to form N molecular orbitals that are so closely spaced in energy that they merge into continuous energy bands. The gap between the highest occupied band (valence band) and the lowest unoccupied band (conduction band) determines whether a solid behaves as a conductor, semiconductor, or insulator—a direct consequence of the same bonding ideas you study in AP Chemistry.

Bridging AP Chemistry bonding models to band theory.
ConceptAP Chemistry LevelAdvanced (Band Theory)
Why metals conductDelocalized sea of electrons moves freelyValence and conduction bands overlap; electrons move into empty states with no energy gap
Why ionic solids insulateIons are fixed; no mobile charge carriers in solidLarge band gap (~6–12 eV) prevents electron promotion
Why diamond insulates but graphite conductsDiamond: all valence electrons in covalent bonds; Graphite: delocalized π electronsDiamond: 5.5 eV band gap; Graphite: zero band gap in the plane (semimetal)
Silicon behaviorCovalent-network solid, low conductivityModerate band gap (1.1 eV): semiconductor; conductivity increases with temperature or doping

While band theory goes beyond the AP exam, recognizing that the macroscopic properties of solids emerge from electronic structure provides a satisfying conceptual closure. The leap from "metallic bonding involves a sea of electrons" to "overlapping bands permit electron mobility" is a natural extension that you may encounter in college-level general chemistry or introductory materials science courses. For the AP exam, the essential takeaway remains: the type and strength of interparticle forces in a solid determine every measurable physical property.

Practice Problems

1
A solid substance has a very high melting point, is extremely hard, does not conduct electricity in either the solid or liquid phase, and is insoluble in water. Which type of solid is this substance most likely?
2
Which of the following ionic compounds is predicted to have the highest melting point based on Coulomb's law considerations?
3
Solid iodine (I₂) and solid sodium chloride (NaCl) are both crystalline, yet I₂ sublimes at 184 °C while NaCl melts at 801 °C. Which of the following best explains this difference?
PROBLEM 4APPLIED
A student is given three unknown solids and the following experimental data: Solid X: melting point 2072 °C, very hard, does not conduct electricity as a solid, does not dissolve in water. Solid Y: melting point 660 °C, malleable, conducts electricity as a solid, does not dissolve in water. Solid Z: melting point 80 °C, soft and waxy, does not conduct electricity as a solid or in the liquid state, dissolves in hexane but not in water. (a) Classify each solid (X, Y, Z) by type. Justify each classification by citing at least two properties from the data. (b) For Solid Z, identify the dominant intermolecular force responsible for holding the solid together and explain how the solubility data supports your classification.
PROBLEM 5CRITICAL THINKING
The table below shows the melting points of four Group 14 (IVA) solids. | Substance | Formula | Melting Point (°C) | |-----------|---------|--------------------| | Carbon (diamond) | C | ~3550 | | Silicon | Si | 1414 | | Germanium | Ge | 938 | | Tin (gray) | Sn | 232 | All four substances adopt a diamond-cubic crystal structure in which each atom is tetrahedrally bonded to four neighbors. (a) All four solids are covalent-network solids. Using the data, identify the trend in melting points going down Group 14 and explain this trend in terms of bond strength and atomic radius. (b) Tin also has a metallic allotrope (white tin, mp 232 °C) that conducts electricity. Gray tin does not conduct electricity. Using your understanding of solid types, explain why the two allotropes of tin exhibit different electrical conductivities. (c) A student claims that because germanium has a lower melting point than silicon, germanium must have weaker intermolecular forces. Evaluate this claim. Is the student's reasoning correct? Explain.

Summary — Properties of Solids

The macroscopic properties of solids—melting point, hardness, electrical conductivity, and solubility—are direct consequences of the type and strength of interparticle forces within the solid. Ionic solids are held together by Coulombic attractions between cations and anions, making them hard, brittle, and high-melting, with conductivity only when molten or dissolved. Metallic solids feature delocalized electrons that enable conductivity and malleability. Covalent-network solids derive extraordinary hardness and melting points from an extended lattice of strong covalent bonds. Molecular solids are held together only by weak intermolecular forces—London dispersion, dipole–dipole, or hydrogen bonding—giving them the lowest melting points and softest textures.

For quantitative ranking within the ionic category, Coulomb's law predicts that higher ion charges and smaller ionic radii produce greater lattice energies and higher melting points. Among molecular solids, greater molar mass and polarizability strengthen London dispersion forces, while permanent dipoles and hydrogen bonding further raise melting and boiling points. Finally, always distinguish crystalline solids (long-range order, sharp melting point) from amorphous solids (short-range order only, gradual softening). Mastering these structure–property relationships is the key to predicting and explaining the physical behavior of any solid on the AP Chemistry exam.

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