Phase Diagrams, Structures of Solids, Bonding in Solids

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Presentation transcript:

Phase Diagrams, Structures of Solids, Bonding in Solids Sections 11.6-11.8 Phase Diagrams, Structures of Solids, Bonding in Solids

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; CO2 sublimes at normal pressures.

Solids We can think of solids as falling into two groups: 1) Crystalline—particles are in highly ordered arrangement. Have “faces” : flat surfaces and definite angles Melt at specific temp

Solids 2) Amorphous—no particular order in the arrangement of particles. Intermolecular forces vary throughout Do not melt at specific temperatures Soften over a temp range

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.

Ionic Solids What are the empirical formulas for these compounds? (a) Green: chlorine; Gray: cesium (b) Yellow: sulfur; Gray: zinc (c) Green: calcium; Gray: fluorine (a) (b) (c) CsCl ZnS CaF2

SAMPLE EXERCISE 11.7 Determining the Contents of a Unit Cell Determine the net number of Na+ and Cl– ions in the NaCl unit cell (Figure 11.36). Solution Analyze: We must sum the various contributing elements to determine the number of Na+ and Cl– ions within the unit cell. Plan: To find the total number of ions of each type, we must identify the different locations within the unit cell and determine the fraction of the ion that lies within the unit cell boundaries. Solve: There is one-fourth of an Na+ on each edge, a whole Na+ in the center of the cube (refer also to Figure 11.35), one-eighth of a Cl– on each corner, and one-half of a Cl– on each face. Thus, we have the following: Thus, the unit cell contains Check: This result agrees with the compound’s stoichiometry: PRACTICE EXERCISE The element iron crystallizes in a form called -iron which has a body-centered cubic unit cell. How many iron atoms are in the unit cell? Answer: two

SAMPLE EXERCISE 11.8 Using the Contents and Dimensions of a Unit Cell to Calculate Density The geometric arrangement of ions in crystals of LiF is the same as that in NaCl. The unit cell of LiF is 4.02 Å on an edge. Calculate the density of LiF. Solution Analyze: We are asked to calculate the density of LiF from the size of the unit cell. Plan: We need to determine the number of formula units of LiF within the unit cell. From that, we can calculate the total mass within the unit cell. Because we know the mass and can calculate the volume of the unit cell, we can then calculate density. Solve: The arrangement of ions in LiF is the same as that in NaCl (Sample Exercise 11.7), so a unit cell of LiF contains 4 Li+ ions and 4 F– ions. Density measures mass per unit volume. Thus, we can calculate the density of LiF from the mass contained in a unit cell and the volume of the unit cell. The mass contained in one unit cell is 4(6.94 amu) + 4(19.0 amu) = 103.8 amu The volume of a cube of length a on an edge is a3, so the volume of the unit cell is (4.02 Å)3. We can now calculate the density, converting to the common units of g/cm3.

Types of Bonding in Crystalline Solids