Chapter 11 Intermolecular Forces, Liquids, and Solids. Intermolecular Forces

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Chapter 11, Liquids, and Solids

States of Matter The fundamental difference between states of matter is the distance between particles.

States of Matter Because in the solid and liquid states particles are closer together, we refer to them as condensed phases.

The States of Matter The state a substance is in at a particular temperature and pressure depends on two antagonistic entities: The kinetic energy of the particles The strength of the attractions between the particles

The attractions between molecules are not nearly as strong as the intramolecular attractions that hold compounds together.

They are, however, strong enough to control physical properties such as boiling and melting points, vapor pressures, and viscosities.

These intermolecular forces as a group are referred to as van der Waals forces.

van der Waals Dipole-dipole interactions Hydrogen bonding London dispersion forces

Ion-Dipole Interactions A fourth type of force, ion-dipole interactions are an important force in solutions of ions. The strength of these forces are what make it possible for ionic substances to dissolve in polar solvents.

Dipole-Dipole Interactions Molecules that have permanent dipoles are attracted to each other. The positive end of one is attracted to the negative end of the other and viceversa. These forces are only important when the molecules are close to each other.

Dipole-Dipole Interactions The more polar the molecule, the higher is its boiling point.

London Dispersion While the electrons in the 1s orbital of helium would repel each other (and, therefore, tend to stay far away from each other), it does happen that they occasionally wind up on the same side of the atom.

London Dispersion At that instant, then, the helium atom is polar, with an excess of electrons on the left side and a shortage on the right side.

London Dispersion Another helium nearby, then, would have a dipole induced in it, as the electrons on the left side of helium atom 2 repel the electrons in the cloud on helium atom 1.

London Dispersion London dispersion forces, or dispersion forces, are attractions between an instantaneous dipole and an induced dipole.

London Dispersion These forces are present in all molecules, whether they are polar or nonpolar. The tendency of an electron cloud to distort in this way is called polarizability.

Factors Affecting London The shape of the molecule affects the strength of dispersion forces: long, skinny molecules (like n-pentane tend to have stronger dispersion forces than short, fat ones (like neopentane). This is due to the increased surface area in n-pentane.

Factors Affecting London The strength of dispersion forces tends to increase with increased molecular weight. Larger atoms have larger electron clouds, which are easier to polarize.

Which Have a Greater Effect: Dipole-Dipole Interactions or Dispersion? If two molecules are of comparable size and shape, dipole-dipole interactions will likely be the dominating force. If one molecule is much larger than another, dispersion forces will likely determine its physical properties.

Boiling Points as a Function of Molecular Weight The BP of the group 4A (bottom) and 6A (top) hydrides are shown as a function of molecular weight. In general, the BP increase with increasing molecular weight because of the increasing strength of dispersion forces.

How Do We Explain This? The nonpolar series (SnH 4 to CH 4 ) follow the expected trend. The polar series follows the trend from H 2 Te through H 2 S, but water is quite an anomaly.

Hydrogen Bonding The dipole-dipole interactions experienced when H is bonded to N, O, or F are unusually strong. We call these interactions hydrogen bonds.

Hydrogen Bonding Hydrogen bonding arises in part from the high electronegativity of nitrogen, oxygen, and fluorine. Also, when hydrogen is bonded to one of those very electronegative elements, the hydrogen nucleus is exposed.

Summarizing

Predicting the Types and Relative Strengths of List the substances Barium Chloride Hydrogen molecule Carbon Monoxide Hydrogen fluoride Neon In order of increasing boiling points.

Solution H2<Ne<CO<HF<BaCl2 Attractive forces are stronger for ionic substances than molecular. BaCl2 should be highest The intermolecular forces of the remaining substances depend on molecular weight, polarity, and hydrogen bonding. H2 lowest nonpolar and lowest molecular weight CO, HF, Ne molecular weights are roughly the same. HF has hydrogen bonding = highest of the 3 CO, slightly polar and higher molecular weight compared to Ne.

Practice Exercise A. Identify the intermolecular forces present in the following substances, and B. Select the substance with the highest boiling point: CH3CH3 CH3OH CH3CH2OH

CH3CH3 Solution Has only dispersion forces it is nonpolar and contains no ions. CH3OH Dispersion forces and hydrogen bonds CH3CH2OH Dispersion forces and hydrogen bonds Highest boiling point: CH3CH2OH

Affect Many Physical Properties The strength of the attractions between particles can greatly affect the properties of a substance or solution.

Viscosity Resistance of a liquid to flow is called viscosity. It is related to the ease with which molecules can move past each other. Viscosity increases with stronger intermolecular forces and decreases with higher temperature.

Surface Tension Surface tension results from the net inward force experienced by the molecules on the surface of a liquid. These are COHESIVE.

Phase Changes

Energy Changes Associated with Changes of State Heat of Fusion: Energy required to change a solid at its melting point to a liquid. DHfus

Energy Changes Associated with Changes of State Heat of Vaporization: Energy required to change a liquid at its boiling point to a gas. DHvap Notice that the heat of vaporization is always larger than its heat of fusion.

Water The heat of fusion, or enthalpy of fusion, for ice is 6.01 kj/mol. The heat of vaporization, or enthalpy of vaporization, for water is 40.7 kj/mol. The heat of sublimation is the sum of heats of vaporization and fusion. For water = approx 47 kj/mol

Energy Changes Associated with Changes of State The heat added to the system at the melting and boiling points goes into pulling the molecules farther apart from each other. The temperature of the substance does not rise during the phase change.

Calculating DH for Temperature and Phase Changes Calculate the enthalpy change upon converting 1 mol of ice at -25 o C to water vapor (steam) at 125 o C under a constant pressure of 1 atm. The specific heats of ice, water, and steam are 2.09 J/g-K, 4.18 J/g-K, and 1.84 J/g-K respectively. For H2O, DHfus = 6.01 kj/mol and DHvap = 40.67 kj/mol.

Practice Exercise What is the enthalpy change during the process in which 100 g of water at 50.0 o C is cooled to ice at -30 o C?

Critical Temperature and Pressure A gas normally liquefies at some point when pressure is applied to it. The highest temperature at which a distinct liquid phase can form is referred to as the critical temperature. The critical pressure is the pressure required to bring about liquefaction at this critical temperature.

Vapor Pressure At any temperature, some molecules in a liquid have enough energy to escape. As the temperature rises, the fraction of molecules that have enough energy to escape increases.

Vapor Pressure As more molecules escape the liquid, the pressure they exert increases.

Vapor Pressure The liquid and vapor reach a state of dynamic equilibrium: liquid molecules evaporate and vapor molecules condense at the same rate.

Vapor Pressure The boiling point of a liquid is the temperature at which its vapor pressure equals atmospheric pressure. The normal boiling point is the temperature at which its vapor pressure is 760 torr.

Examples Use Figure 11.24 to estimate the boiling point of diethyl ether under an external pressure of 0.80 atm. At what external pressure will ethanol have a boiling point of 60 o C?

Phase Diagrams Phase diagrams display the state of a substance at various pressures and temperatures and the places where equilibria exist between phases.

Phase Diagrams The AB line is the liquid-vapor interface. It starts at the triple point (A), the point at which all three states are in equilibrium.

Phase Diagrams It ends at the critical point (B); above this critical temperature and critical pressure the liquid and vapor are indistinguishable from each other.

Phase Diagrams Each point along this line is the boiling point of the substance at that pressure.

Phase Diagrams The AD line is the interface between liquid and solid. The melting point at each pressure can be found along this line.

Phase Diagrams Below A the substance cannot exist in the liquid state. Along the AC line the solid and gas phases are in equilibrium; the sublimation point at each pressure is along this line.

Phase Diagram of Water Note the high critical temperature and critical pressure: These are due to the strong van der Waals forces between water molecules.

Phase Diagram of Water The slope of the solid liquid line is negative. This means that as the pressure is increased at a temperature just below the melting point, water goes from a solid to a liquid.

Phase Diagram of Carbon Dioxide Carbon dioxide cannot exist in the liquid state at pressures below 5.11 atm; CO 2 sublimes at normal pressures.

Phase Diagram of Carbon Dioxide The low critical temperature and critical pressure for CO 2 make supercritical CO 2 a good solvent for extracting nonpolar substances (such as caffeine).

Solids We can think of solids as falling into two groups: Crystalline particles are in highly ordered arrangement.

Solids Amorphous no particular order in the arrangement of particles.

Attractions in Ionic Crystals In ionic crystals, ions pack themselves so as to maximize the attractions and minimize repulsions between the ions.

Crystalline Solids Because of the order in a crystal, we can focus on the repeating pattern of arrangement called the unit cell.

Crystalline Solids There are several types of basic arrangements in crystals, such as the ones shown above.

Crystalline Solids We can determine the empirical formula of an ionic solid by determining how many ions of each element fall within the unit cell.

Types of Bonding in Crystalline Solids

Covalent-Network and Molecular Solids Diamonds are an example of a covalentnetwork solid in which atoms are covalently bonded to each other. They tend to be hard and have high melting points.

Covalent-Network and Molecular Solids Graphite is an example of a molecular solid in which atoms are held together with van der Waals forces. They tend to be softer and have lower melting points.

Metallic Solids Metals are not covalently bonded, but the attractions between atoms are too strong to be van der Waals forces. In metals, valence electrons are delocalized throughout the solid.