Bonding, Structure, and Gases

Lattice Structures

  • Most ionic, metallic, and covalent compounds form crystalline lattices.
  • Ions, atoms, or molecules are arranged in a regular, repeating pattern within these lattices.

Giant Ionic Lattices

  • An ionic bond is the electrostatic force of attraction between a positively charged metal ion (cation) and a negatively charged non-metal ion (anion).
  • Metals become positively charged by transferring electrons to non-metals, which then become negatively charged.
  • Ionic compounds arrange themselves into giant ionic lattices (also called giant ionic structures).
  • The specific type of lattice structure depends on the relative sizes of the positive and negative ions, which are arranged in an alternating pattern.
  • Examples of ionic lattices with a cubic structure include Magnesium Oxide (MgOMgO) and Sodium Chloride (NaClNaCl).
  • In general ionic lattices, negative ions (anions) are typically larger than the positive ions (cations).
  • The ionic lattices for NaClNaCl and MgOMgO are similar due to the 1:1 ratio of cations to anions.

Covalent Lattices

  • Covalent bonds involve the sharing of electrons between non-metal atoms.
  • Covalent compounds can form simple molecular lattices or giant molecular lattices.
    • Simple molecular lattices: Examples include iodine (I<em>2I<em>2), buckminsterfullerene (C</em>60C</em>{60}), and ice (H2OH_2O).
    • Giant molecular lattices: Examples include silicon(IV) oxide (SiO2SiO_2), graphite, and diamond.
  • Different simple molecular lattices (e.g., ice, buckminsterfullerene, iodine) exhibit different structures and intermolecular forces.
  • Giant molecular lattices generally have higher melting and boiling points due to the significant energy needed to overcome intramolecular and/or intermolecular forces.

Metallic Lattices

  • Metals form giant metallic lattices where metal ions are surrounded by a 'sea' of delocalized electrons.
  • Metal ions are often arranged in hexagonal layers or cubic arrangements.
  • In copper (CuCu), the cations are arranged in regular layers.

Allotropes of Carbon

  • Graphite, diamond, and buckminsterfullerene are allotropes of carbon.
  • Allotropes are different structural forms of the same element.

Bonding & Structure and Physical Properties

  • Different types of bonding and structure influence physical properties like melting and boiling points, electrical conductivity, and solubility.

Ionic Bonding & Giant Ionic Lattice Structures

  • Ionic compounds are strong due to strong electrostatic forces that hold the ions together.
  • They tend to be brittle because ionic crystals can easily split apart under stress.
  • Ionic compounds have high melting and boiling points because strong electrostatic forces between ions act in all directions, maintaining a strong lattice.
  • Melting and boiling points increase with the charge density of the ions due to greater electrostatic attraction. For example, Mg2+O2Mg^{2+}O^{2-} has a higher melting point than Na+ClNa^+Cl^-.
  • Ionic compounds are often soluble in water because they can form ion-dipole bonds.
  • Ionic compounds conduct electricity only when molten or in solution, as ions can move freely. In the solid state, ions are fixed in position.

Metallic Bonding & Giant Metallic Lattice Structures

  • Metallic compounds are malleable; metal layers can slide when a force is applied, and metallic bonds reform.
  • The attractive forces between metal ions and delocalized electrons act in all directions.
  • Metallic compounds are strong and hard due to strong attractive forces between metal ions and delocalized electrons.
  • Metals have high melting and boiling points because of these strong attractive forces.
  • A greater number of delocalized electrons and smaller cation size result in greater attractive force and higher melting/boiling points.
  • Pure metals are insoluble in water.
  • Metals conduct electricity in solid and liquid states because mobile electrons can move freely.

Covalent Bonding & Simple Covalent Lattice Structures

  • Simple covalent lattices have low melting and boiling points because of weak intermolecular forces.
    • Little energy is needed to break the lattice.
  • Most compounds are insoluble in water unless they are polar (like HClHCl) or can form hydrogen bonds (like NH3NH_3).
  • They do not conduct electricity in solid or liquid states due to the absence of charged particles.
  • Some simple covalent compounds conduct electricity in solution (e.g., HClHCl forms H+H^+ and ClCl^- ions).

Covalent Bonding & Giant Covalent Lattice Structures

  • Giant covalent lattices have high melting and boiling points because of a large number of covalent bonds linking the entire structure.
  • A lot of energy is required to break the lattice.
  • The compounds can vary in hardness.
    • Graphite is soft due to weak forces between carbon layers.
    • Diamond and silicon(IV) oxide are hard due to their 3D network of strong covalent bonds.
  • Most compounds are insoluble in water.
  • Most compounds do not conduct electricity, but some exceptions exist.
    • Graphite has delocalized electrons between carbon layers that can move when a voltage is applied.
    • Diamond and silicon(IV) oxide do not conduct electricity because all outer electrons are involved in covalent bonds.

Characteristics Comparison Table

CharacteristicGiant IonicGiant MetallicSimple CovalentGiant Covalent
Melting/Boiling PointsHighModerately high to highLowVery high
Electrical ConductivityOnly when molten/solutionWhen solid or liquidDo not conduct electricityDo not conduct electricity (except graphite)
SolubilitySolubleInsoluble (some may react)Usually insoluble unless they are polarInsoluble
HardnessHard, brittleHard, malleableSoftVery hard (diamond/SiO2) or soft (graphite)
Physical StateSolidSolidSolid, liquid, gasSolid
ForcesElectrostatic attractionDelocalised sea of electrons attracting positive ionsWeak intermolecular forces between moleculesElectrons in covalent bonds between atoms
ParticlesIonsPositive ions in a sea of electronsSmall moleculesAtoms
ExampleNaClNaClCopperBr2Br_2Graphite, silicon(IV) oxide

Example Problem

  • Problem: Given the physical properties of substances X, Y, and Z, identify their structure.
  • Solution:
    • X (Melting Point: 839°C, Conductivity: Good when molten, Solubility: Soluble) - likely a giant ionic structure.
    • Y (Melting Point: 95°C, Conductivity: Very poor, Solubility: Almost insoluble) - likely a simple molecular structure.
    • Z (Melting Point: 1389°C, Conductivity: Good, Solubility: Insoluble) - likely a giant metallic structure.

Gas Pressure

  • Gases exert pressure due to gas molecules colliding with the container walls.

Changing Gas Volume:

  • Decreasing volume (at constant temperature) increases pressure due to more frequent collisions.
  • Volume is inversely proportional to pressure at constant temperature.

Changing Gas Temperature:

  • Increasing temperature (at constant volume) increases pressure as molecules gain kinetic energy and collide more frequently.
  • Temperature is directly proportional to pressure at constant volume.

Ideal Gases

Kinetic Theory of Gases:

  • Gas molecules are constantly moving randomly.
  • Molecules have negligible volume.
  • No intermolecular forces exist.
  • Collisions are elastic (no kinetic energy loss).
  • Temperature is related to average kinetic energy.
  • Gases following these rules are called ideal gases; real gases approximate this.

Ideal Gas Law:

  • Volume depends on pressure and temperature.
  • Heating a gas (at constant pressure) increases volume as particles gain kinetic energy and collide more frequently.
  • Volume is directly proportional to temperature.

Limitations of the Ideal Gas Law:

  • Real gases deviate at high pressures and low temperatures because:
    • Molecules are closer together.
    • Intermolecular forces become significant.
    • Molecular volume is no longer negligible.
  • Assumptions of no intermolecular forces and negligible volume break down.
  • Attractive forces reduce impact force, lowering measured pressure.

Equations

  • pV=nRTpV = nRT