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Chapter 11: Liquids & Solids The molecular compounds like water, ammonia, and carbon dioxide have different physical properties because of the intermolecular forces. Comparison of all three phases:

Chapter 11: Liquids & Solids The molecular compounds like water, ammonia, and carbon dioxide have different physical properties because of the intermolecular

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Chapter 11: Liquids & Solids The molecular compounds like water, ammonia, and carbon dioxide have different physical properties because of the intermolecular forces. Comparison of all three phases: Slide 2 Liquids & Solids Slide 3 Slide 4 Compressibility Slide 5 Changes of State Changes in state can be induced by a change in temperature or pressure. Slide 6 Intermolecular Forces Forces between molecules. Always LESS in energy than actual bond. The attractive force between two HCl molecules is about 16 kJ/mol. The bond dissociation energy of the HCl bond is about 431 kJ/mol. Slide 7 Intermolecular Forces One method to compare the strength of intermolecular forces is to examine the substances boiling point. When the forces are relatively weak, then the boiling point is small. Ex) HCl, bp = -85 o C. There are three main types of intermolecular forces between neutral substances. Slide 8 Intermolecular Forces In the LS packet, we identified molecules as being polar or non-polar based on shape, types of atoms, etc. Polar molecules have a dipole that is a positive and negative end. Slide 9 Intermolecular Forces Thus, the first type of force is called Dipole-Dipole (or DD) forces and occurs for any polar molecule. The larger the dipole moment, the more DD forces. Slide 10 Intermolecular Forces If you cool any non-polar molecule or atom to a low enough temperature, then it will liquefy. Yet, these have no reason to be attractive to each other. Fritz London first proposed a theory in 1930. On average, electrons in an atom like He are evenly distributed. But, in one INSTANT, the two electrons may both be on the same side. Slide 11 Intermolecular Forces Thus, in that one INSTANT, a He atom would have an instantaneous dipole. This is called the London Dispersion (or LD) force. Slide 12 Intermolecular Forces Since all molecules have electrons, they all have a LD force. The polarizability of an atom or molecules electrons depends on two factors. 1. The number of electrons. More electrons = More LD forces. 2. The shape of molecule. More spread out = more LD forces. Slide 13 Intermolecular Forces Slide 14 Non-polar Alkanes Slide 15 Intermolecular Forces The formula C 5 H 12 has three structural isomers. CH 3 CH 2 CH 2 CH 2 CH 3 CH 3 CH 3 CH 3 CH 2 CH CH 3 CH 3 C CH 3 CH 3 Slide 16 Non-polar Branched Alkanes NameMolar MassBoiling Point Pentane72.15 g/mol36.1 o C Methylbutane72.15 g/mol27.7 o C Dimethylpropane72.15 g/mol10 o c Butane58.12 g/mol-0.5 o C Methylpropane58.12 g/mol-11.7 o C Slide 17 Comparison of the group 4A, 5A, 6A, and 7A hydrides shows an interesting result. What type of forces do the group 4A have? Group 6A? What is the notable exception? Slide 18 Intermolecular Forces The third type of force is a special case of DD force and is called Hydrogen Bonding (or HB). The name Hydrogen Bonding is a misnomer! HB can only occur when: H is bonded to either N, O, or F. The N, O, or F atom has at least one lone pair. Slide 19 Intermolecular Forces The strength of Hydrogen Bonding varies from 5 kJ to 40 kJ, which is still much weaker than a covalent bond (200 1000 kJ). However, it is MUCH stronger than DD or LD forces. Thus, it can greatly increase the boiling point temperatures of molecules. Slide 20 Intermolecular Forces HB forces are very important in biochemistry. Proteins are made from the twenty amino acids. The structure of the amino acid has both an OH group and an NH 2 group that can HB. R O H N C C O H H H Slide 21 Intermolecular Forces Predicting relative boiling points. 1. Determine the molecular weight. 2. Determine the type(s) of intermolecular forces present. If weights are similar, then LD < DD < HB If weights are very dissimilar, then #2 probably does not matter. However, HB can really distort the bps! Ex) H 2 O, bp = 100 o C, MW = 18 g/mol versus CCl 4, bp = 76 o C, MW = 154 g/mol. Slide 22 Intermolecular Forces The strengths of attractions between the molecules may affect a liquids properties. Viscosity Surface Tension Slide 23 Intermolecular Forces Viscosity is the resistance of a liquid to flow. Liquids with low viscosity, like water, will produce a splash whereas liquids with high viscosity, like corn syrup or ketchup, will not. Slide 24 Intermolecular Forces Viscosity tends to increase with more intermolecular forces and molecular weight. Many liquids, like water, have a consistent viscosity over a wide range of temperatures. Some liquids, like corn syrup, will decrease in viscosity as the temperature increases. Multi-weight motor oil actually increases with an increase in temperature (ie. 5W 30). Non-Newtonian liquids (ie. Slime) have a variable viscosity at the same temperature. Slide 25 Surface Tension Surface Tension is the skin-like appearance of the surface. Results from surface molecules seeking six nearest neighbors like interior molecules. Slide 26 Surface Tension Slide 27 Phase Changes Slide 28 Energy when changing between solid and liquid phase is called the Heat of Fusion and denoted as H fus. H fus for water is 6.01 kJ/mol or 334 J/g. Energy when changing between liquid and gas is called the Heat of Vaporization and denoted as H vap. H vap for water is 40.67 kJ.mol or 2,260 J/g. Slide 29 Heating Curve Slide 30 Refrigeration The basics of refrigeration. First law of thermodynamics at work again! Coolant is CF 2 Cl 2 (old) or CF 3 CH 2 F (new). Slide 31 Vapor Pressure Above the surface of any liquid, some liquid molecules will have enough energy to escape and become gas molecules. In a closed system, an equilibrium will be achieved between the gas molecules and the liquid. This is the vapor pressure. Slide 32 Vapor Pressure As the temperature of the liquid increases, its vapor pressure will increase. Slide 33 Vapor Pressure When the vapor pressure equals 1 atmosphere, then the liquid spontaneously becomes a gas. You would call this the boiling point. Does pure water always boil at 100 o C? Slide 34 Clausius-Clapeyron Equation The graphs of vapor pressure versus temperature are approximately an exponential function. Mathematically, if you take the natural logarithm (ln key on calculator) of the vapor press versus 1/T, then you get a linear relationship. Slide 35 Clausius-Clapeyron Equation R is molar gas constant = 8.314 J/K mol and the T is the temperature in Kelvin Heat of vaporization must be in J/mol. Pressures can be in either atm or mmHg (must agree). Slide 36 Phase Diagrams Display a singles substances states of matter over a wide range of P and T. Slide 37 Carbon Dioxide The phase diagram of CO2 shows that the liquid phase can only be found above a pressure of 5.11 atm. As the temperature of solid CO2 increases, it undergoes sublimation. Slide 38 Water The phase diagram of water has one very important difference. What is it? Slide 39 Solids Solids can be either amorphous (random) or crystalline (repeating pattern). Unit cell is the smallest repeating pattern for the crystalline structure. Analogy: a hotel with many floors. Structure of unit cell can have various lengths and angles. Slide 40 Solids While many types of unit cells are possible, a few are seen many times in structures of metals, molecular, and ionic compounds. Cubic unit cells two main versions. Body-centered cubic (BCC) has atoms at each corner and an atom in the body-center. Face-centered cubic (FCC) has atoms at each corner and an atom on each face. Important just like a hotel room shares walls, floors, and ceilings with other rooms, so does a unit cell share atoms with other unit cells. Slide 41 Solids Slide 42 Slide 43 Can also have atoms on edges in larger unit cells namely for ionic compounds. Thus, the following are the contributions for locations on or in a unit cell: Slide 44 Solids Unit cell calculations will follow the formula: Where V c is the volume of the cubic unit cell, MW is the molar mass, C is the number of atoms per unit cell, D is the density (m/V), and N a is Avogadros Number. Slide 45 Solids Another view Closest Packing Model. Assumes that atoms are hard spheres. Maximize the density, minimize the empty spaces. Slide 46 Solids First layer what is the most efficient method of arrangement? Slide 47 Solids Second layer is placed so that spheres sit in gaps from previous row. Third layer can either repeat first layer yielding an ABABAB pattern. OR, the third layer is offset from the first two producing an ABCABCABC pattern. Slide 48 Solids The ABABAB pattern produces a unit cell called hexagonal closest packing or HCP. This is NOT a cubic unit cell! Slide 49 Solids The ABCABCABC pattern produces a unit cell called cubic closest packing or CCP. However, CCP is the same as FCC! Slide 50 Solids HHe Hcp Li Bcc Be Hcp BCNOFNe Fcc Na Bcc Mg Hcp Al Fcc SiPSClAr Fcc K Bcc Ca Fcc Sc Hcp Ti Hcp V Bcc Cr Bcc Mn Bcc Fe Bcc Co Hcp Ni Fcc Cu Fcc Zn Hcp GaGeAsSeBrKr Fcc Rb Bcc Sr Fcc Y Hcp Zr Hcp Nb Bcc Mo Bcc Tc Hcp Ru Hcp Rh Fcc Pd Fcc Ag Fcc Cd Hcp InSnSbTeIXe Fcc Cs Bcc Ba Bcc Hf Hcp Ta Bcc W Bcc Re Hcp Os Hcp Ir Fcc Pt Fcc Au Fcc HgTl Hcp Pb Fcc BiPoAtRn Slide 51 Solids All crystalline solids can be catagerized into one of four types. Type 1: Molecular Solids Consist of atoms or molecules like Ne, CH 4, and H 2 O. Are held together by relatively weak intermolecular forces. Are soft and have low melting points (unless they have a high MW). Poor conductors of heat and electricity. Slide 52 Solids Type 2: Ionic Solids Consist of ions held together by their electrostatic attractions. Unit cells are always larger since the smallest repeating pattern must include two ions. When cation and anion are of similar sizes, get BCC type arrangement. When anion is much larger, get a CCP arrangement of anions with cations stuck in the holes. Hard and brittle and have high melting points. Poor electrical conductors as solids, but excellent when melted. Slide 53 Solids (a) CsCl (b) ZnS (c) CaF2 Slide 54 Solids View of NaCl Slide 55 Solids Type 3: Metallic Solids Atoms are held together by a sea of valence electrons. Can be soft (Na, Au) or very hard (Fe, Co) with low to very high melting points. Excellent conductors of both heat and electricity. Malleable and ductile. Slide 56 Solids Type 4: Covalent Network Solids Consist of atoms held together in large networks of covalent bonds. There are not many of these C(diamond), SiO2, quartz, SiC, and BN. Very hard with very high melting points. Poor conductors. Slide 57 Solids Two forms of carbon, diamond and graphite. Slide 58 Solids Comparing metal points of solids. First determine the type of solid. Molecular is always the lowest of the four types. Second if both are the same type of solid, then: Molecular is like bps. LD < DD < HB. Ex) CH4 (-182 C) < COCl2 (-118 C) < H2O (0 C) Ionic depends on lattice energy the larger the lattice energy, the higher the mp. Ex) NaCl (801 C) < MgO (2852 C) Slide 59 Solids Metallic depends on the number of unpaired electrons. More unpaired electrons = higher melting point. K, 1 unpaired electron, mp = 64 C Ti, 2 unpaired electrons, mp = 1668 C Cr, 6 unpaired electrons, mp = 1907 C Cu, 1 unpaired electron, mp = 1065 C Covalent network are always very high. Quartz, mp = 1670 to 1710 C Diamond, mp = 3550 C (highest of any naturally occurring substance)