15. Atoms have an approximately spherical shape (on average). It is impossible to pack spheres together without some empty space among the spheres.

Size: px
Start display at page:

Download "15. Atoms have an approximately spherical shape (on average). It is impossible to pack spheres together without some empty space among the spheres."

Transcription

1 CAPTER 0 LIQUIDS AND SOLIDS Questions. Chalk is composed of the ionic compound calcium carbonate (CaCO ). The electrostatic forces in ionic compounds are much stronger than the intermolecular forces in covalent compounds. Therefore, CaCO should have a much higher boiling point than the covalent compounds found in motor oil and in O. Motor oil is composed of nonpolar C C and C! bonds. The intermolecular forces in motor oil are therefore London dispersion forces. We generally consider these forces to be weak. owever, with compounds that have large molar masses, these London dispersion forces add up significantly and can overtake the relatively strong hydrogen-bonding interactions in water.. In the vapor phase, gas molecules are relatively far apart from each other, so far apart that gas molecules are assumed to exhibit no intermolecular forces. 4. ydrogen bonding occurs when hydrogen atoms are covalently bonded to highly electronegative atoms such as oxygen, nitrogen, or fluorine. Because the electronegativity difference between hydrogen and these highly electronegative atoms is relatively large, the N, O, and F bonds are very polar covalent bonds. This leads to strong dipole forces. Also, the small size of the hydrogen atom allows the dipoles to approach each other more closely than can occur between most polar molecules. Both of these factors make hydrogen bonding a special type of dipole interaction. 5. Atoms have an approximately spherical shape (on average). It is impossible to pack spheres together without some empty space among the spheres. 6. Critical temperature: The temperature above which a liquid cannot exist; i.e., the gas cannot be liquified by increased pressure. Critical pressure: The pressure that must be applied to a substance at its critical temperature to produce a liquid. 6

2 CAPTER 0 LIQUIDS AND SOLIDS 7 The kinetic energy distribution changes as one raises the temperature (T 4 > T c > T > T > T ). At the critical temperature T c, all molecules have kinetic energies greater than the intermolecular forces F, and a liquid can't form. Note: The various temperature distributions shown in the plot are not to scale. The area under each temperature distribution should be equal to each other (area total number of molecules). 7. Evaporation takes place when some molecules at the surface of a liquid have enough energy to break the intermolecular forces holding them in the liquid phase. When a liquid evaporates, the molecules that escape have high kinetic energies. The average kinetic energy of the remaining molecules is lower; thus the temperature of the liquid is lower.. A crystalline solid will have the simpler diffraction pattern because a regular, repeating arrangement is necessary to produce planes of atoms that will diffract the X rays in regular patterns. An amorphous solid does not have a regular repeating arrangement and will produce a complicated diffraction pattern. 9. An alloy is a substance that contains a mixture of elements and has metallic properties. In a substitutional alloy, some of the host metal atoms are replaced by other metal atoms of similar size, e.g., brass, pewter, plumber s solder. An interstitial alloy is formed when some of the interstices (holes) in the closest packed metal structure are occupied by smaller atoms, e.g., carbon steels. 0. Equilibrium: There is no change in composition; the vapor pressure is constant. Dynamic: Two processes, vapor liquid and liquid vapor, are both occurring but with equal rates, so the composition of the vapor is constant.. a. As the strength of the intermolecular forces increase, the rate of evaporation decreases. b. As temperature increases, the rate of evaporation increases. c. As surface area increases, the rate of evaporation increases.. O(l) O(g) 44 kj/mol; heat must be absorbed by water in order to evaporate. This heat comes from the surroundings. ence, as water evaporates, the surroundings (which includes earth) get cooler.. Sublimation will occur, allowing water to escape as O(g). 4. Water boils when the vapor pressure equals the external pressure. Because the external pressure is significantly lower at high altitudes, a lower temperature is required to equalize the vapor pressure of water to the external pressure. Thus food cooked in boiling water at high elevations cooks at a lower temperature, so it takes longer. 5. The strength of intermolecular forces determines relative boiling points. The types of intermolecular forces for covalent compounds are London dispersion forces, dipole forces, and hydrogen bonding. Because the three compounds are assumed to have similar molar mass and shape, the strength of the London dispersion forces will be about equal among the three compounds. One of the compounds will be nonpolar, so it only has London dispersion forces. The other two compounds will be polar, so they have additional dipole forces and will boil at

3 CAPTER 0 LIQUIDS AND SOLIDS a higher temperature than the nonpolar compound. One of the polar compounds will have an covalently bonded to either N, O, or F. This gives rise to the strongest type of covalent intermolecular forces, hydrogen bonding. The compound that hydrogen bonds will have the highest boiling point, whereas the polar compound with no hydrogen bonding will boil at a temperature in the middle of the other compounds. 6. a. Both forms of carbon are network solids. In diamond, each carbon atom is surrounded by a tetrahedral arrangement of other carbon atoms to form a huge molecule. Each carbon atom is covalently bonded to four other carbon atoms. The structure of graphite is based on layers of carbon atoms arranged in fused sixmembered rings. Each carbon atom in a particular layer of graphite is surrounded by three other carbons in a trigonal planar arrangement. This requires sp hybridization. Each carbon has an unhybridized p atomic orbital; all of these p orbitals in each sixmembered ring overlap with each other to form a delocalized π electron system. b. Silica is a network solid having an empirical formula of SiO. The silicon atoms are singly bonded to four oxygens. Each silicon atom is at the center of a tetrahedral arrangement of oxygen atoms that are shared with other silicon atoms. The structure of silica is based on a network of SiO 4 tetrahedra with shared oxygen atoms rather than discrete SiO molecules. Silicates closely resemble silica. The structure is based on interconnected SiO 4 tetrahedra. owever, in contrast to silica, where the O/Si ratio is :, silicates have O/Si ratios greater than : and contain silicon-oxygen anions. To form a neutral solid silicate, metal cations are needed to balance the charge. In other words, silicates are salts containing metal cations and polyatomic silicon-oxygen anions. When silica is heated above its melting point and cooled rapidly, an amorphous (disordered) solid called glass results. Glass more closely resembles a very viscous solution than it does a crystalline solid. To affect the properties of glass, several different additives are thrown into the mixture. Some of these additives are Na CO, B O, and K O, with each compound serving a specific purpose relating to the properties of glass. 7. a. Both CO and O are molecular solids. Both have an ordered array of the individual molecules, with the molecular units occupying the lattice points. A difference within each solid lattice is the strength of the intermolecular forces. CO is nonpolar and only exhibits London dispersion forces. O exhibits the relatively strong hydrogen-bonding interactions. The differences in strength is evidenced by the solid-phase changes that occur at atm. CO (s) sublimes at a relatively low temperature of!7ec. In sublimation, all of the intermolecular forces are broken. owever, O(s) doesn t have a phase change until 0EC, and in this phase change from ice to water, only a fraction of the intermolecular forces are broken. The higher temperature and the fact that only a portion of the intermolecular forces are broken are attributed to the strength of the intermolecular forces in O(s) as compared to CO (s). Related to the intermolecular forces are the relative densities of the solid and liquid phases for these two compounds. CO (s) is denser than CO (l), whereas O(s) is less dense than O(l). For CO (s) and for most solids, the molecules pack together as close as possible; hence solids are usually more dense than the liquid phase. O is an

4 CAPTER 0 LIQUIDS AND SOLIDS 9 exception to this. Water molecules are particularly well suited for hydrogen bonding interaction with each other because each molecule has two polar O bonds and two lone pairs on the oxygen. This can lead to the association of four hydrogen atoms with each oxygen atom: two by covalent bonds and two by dipoles. To keep this arrangement (which maximizes the hydrogen-bonding interactions), the O(s) molecules occupy positions that create empty space in the lattice. This translates into a smaller density for O(s) as compared to O(l). b. Both NaCl and CsCl are ionic compounds with the anions at the lattice points of the unit cells and the cations occupying the empty spaces created by anions (called holes). In NaCl, the Cl anions occupy the lattice points of a face-centered unit cell, with the Na + cations occupying the octahedral holes. Octahedral holes are the empty spaces created by six Cl ions. CsCl has the Cl ions at the lattice points of a simple cubic unit cell, with the Cs + cations occupying the middle of the cube.. Because silicon carbide is made from Group 4A elements, and because it is extremely hard, one would expect SiC to form a covalent network structure similar to diamond. 9. If TiO conducts electricity as a liquid, then it is an ionic solid; if not, then TiO is a network solid. 0. The interparticle forces in ionic solids (the ionic bonds) are much stronger than the interparticle forces in molecular solids (dipole forces, London forces, etc.). The difference in intermolecular forces is most clearly shown in the huge difference in melting points between ionic and molecular solids. Table salt and ordinary sugar are both crystalline solids at room temperature that look very similar to each other. owever, sugar can be melted easily in a saucepan during the making of candy, whereas the full heat of a stove will not melt salt. When a substance melts, some interparticle forces must be broken. Ionic solids (salt) require a much larger amount of energy to break the interparticle forces as compared to the relatively weak forces in molecular solids (sugar).. The mathematical equation that relates the vapor pressure of a substance to temperature is: vap ln P vap! + C R T y m x + b As shown above, this equation is in the form of the straight-line equation. If one plots ln P vap versus /T with temperature in Kelvin, the slope of the straight line is! vap /R. Because vap is always positive, the slope of the straight line will be negative.. The typical phase diagram for a substance shows three phases and has a positive-sloping solid-liquid equilibrium line (water is atypical). A sketch of the phase diagram for I would look like this:

5 40 CAPTER 0 LIQUIDS AND SOLIDS P 90 torr s l g Exercises 5 o C T Statements a and e are true. For statement a, the liquid phase is always more dense than the gaseous phase (gases are mostly empty space). For statement e, because the triple point is at 90 torr, the liquid phase cannot exist at any pressure less than 90 torr, no matter what the temperature. For statements b, c, and d, examine the phase diagram to prove to yourself that they are false. Intermolecular Forces and Physical Properties. Ionic compounds have ionic forces. Covalent compounds all have London dispersion (LD) forces, whereas polar covalent compounds have dipole forces and/or hydrogen bonding forces. For hydrogen-bonding (-bonding) forces, the covalent compound must have either a N, O, or F bond in the molecule. a. LD only b. dipole, LD c. -bonding, LD d. ionic e. LD only (C 4 is a nonpolar covalent compound.) f. dipole, LD g. ionic 4. a. ionic b. dipole, LD (LD London dispersion) c. LD only d. LD only (For all practical purposes, a C bond can be considered as a nonpolar bond.) e. ionic f. LD only g. -bonding, LD 5. a. OCS; OCS is polar and has dipole-dipole forces in addition to London dispersion (LD) forces. All polar molecules have dipole forces. CO is nonpolar and only has LD forces. To predict polarity, draw the Lewis structure and deduce whether the individual bond dipoles cancel. b. SeO ; both SeO and SO are polar compounds, so they both have dipole forces as well as LD forces. owever, SeO is a larger molecule, so it would have stronger LD forces. c. NC C N ; more extensive hydrogen bonding (-bonding) is possible because two N groups are present.

6 CAPTER 0 LIQUIDS AND SOLIDS 4 d. CO; CO is polar, whereas C C is nonpolar. CO has dipole forces in addition to LD forces. C C only has LD forces. e. C O; C O can form relatively strong -bonding interactions, unlike CO. 6. Ar exists as individual atoms that are held together in the condensed phases by London dispersion forces. The molecule that will have a boiling point closest to Ar will be a nonpolar substance with about the same molar mass as Ar (9.95 g/mol); this same size nonpolar substance will have about equivalent strength of London dispersion forces. Of the choices, only Cl (70.90 g/mol) and F (.00 g/mol) are nonpolar. Because F has a molar mass closest to that of Ar, one would expect the boiling point of F to be close to that of Ar. 7. a. Neopentane is more compact than n-pentane. There is less surface-area contact among neopentane molecules. This leads to weaker LD forces and a lower boiling point. b. F is capable of -bonding; Cl is not. c. LiCl is ionic, and Cl is a molecular solid with only dipole forces and LD forces. Ionic forces are much stronger than the forces for molecular solids. d. n-exane is a larger molecule, so it has stronger LD forces.. Ethanol, C 6 O, has (4) + 6() valence electrons. C C O Exhibits -bonding and London dispersion forces. Dimethyl ether, C 6 O, also has 0 valence electrons. It has a Lewis structure of: C O C Exhibits dipole and London dispersion forces but no hydrogen bonding since it has no covalently bonded to the O. Propane, C, has (4) + () 0 valence electrons. C C C Propane only has relatively nonpolar bonds, so it is nonpolar. Propane exhibits only London dispersion forces. The three compounds have similar molar mass, so the strength of the London dispersion forces will be approximately equivalent. Because dimethyl ether has additional dipole forces,

7 4 CAPTER 0 LIQUIDS AND SOLIDS it will boil at a higher temperature than propane. The compound with the highest boiling point is ethanol since it exhibits relatively strong hydrogen-bonding forces. The correct matching of boiling points is: ethanol, 7.5EC; dimethyl ether,!ec; propane,!4.ec 9. Boiling points and freezing points are assumed directly related to the strength of the intermolecular forces, whereas vapor pressure is inversely related to the strength of the intermolecular forces. a. Br; Br is polar, whereas Kr and Cl are nonpolar. Br has dipole forces unlike Kr and Cl. b. NaCl; ionic forces are much stronger than the intermolecular forces for molecular substances. c. I ; all are nonpolar, so the largest molecule (I ) will have the strongest LD forces and the lowest vapor pressure. d. N ; nonpolar and smallest, so it has the weakest intermolecular forces. e. C 4 ; smallest, nonpolar molecule, so it has the weakest LD forces. f. F; F can form relatively strong -bonding interactions, unlike the others. g. C C C O; -bonding, unlike the others, so it has strongest intermolecular forces. 40. a. CBr 4 ; largest of these nonpolar molecules, so it has strongest LD forces. b. F ; ionic forces in LiF are much stronger than the molecular forces in F and Cl. Cl has dipole forces, whereas the nonpolar F does not exhibit these. So F has the weakest intermolecular forces and the lowest freezing point. c. C C O; can form -bonding interactions, unlike the other covalent compounds. d. O ; O-O structure produces stronger -bonding interactions than F, so it has the greatest viscosity. e. CO; CO is polar, so it has dipole forces, unlike the other nonpolar covalent compounds. f. I ; I has only LD forces, whereas CsBr and CaO have much stronger ionic forces. I has the weakest intermolecular forces, so it has smallest fusion. Properties of Liquids 4. The attraction of O for glass is stronger than the O O attraction. The miniscus is concave to increase the area of contact between glass and O. The g g attraction is greater than the g glass attraction. The miniscus is convex to minimize the g glass contact.

8 CAPTER 0 LIQUIDS AND SOLIDS 4 4. Water is a polar substance, and wax is a nonpolar substance; they are not attracted to each other. A molecule at the surface of a drop of water is subject to attractions only by water molecules below it and to each side. The effect of this uneven pull on the surface water molecules tends to draw them into the body of the water and causes the droplet to assume the shape that has the minimum surface area, a sphere. 4. The structure of O is O O, which produces greater hydrogen bonding than in water. Thus the intermolecular forces are stronger in O than in O, resulting in a higher normal boiling point for O and a lower vapor pressure. 44. CO is a gas at room temperature. As melting point and boiling point increase, the strength of the intermolecular forces also increases. Therefore, the strength of forces is CO < CS < CSe. From a structural standpoint, this is expected. All three are linear, nonpolar molecules. Thus only London dispersion forces are present. Because the molecules increase in size from CO < CS < CSe, the strength of the intermolecular forces will increase in the same order. Structures and Properties of Solids 45. nλ d sin θ, d nλ sin θ 54 pm sin 4. pm. 0 0 m 46. d nλ sin θ 54 pm sin.0 40 pm m 47. λ dsin θ n m sin 5.0 o m D 4. nλ d sin θ, d nλ sin θ.6 D 4.9 D m 49 pm sin 5.55 sin θ n λ.6 D d 4.9D 0.56, θ A cubic closest packed structure has a face-centered cubic unit cell. In a face-centered cubic unit, there are: corners / atom corner / atom + 6 faces 4 atoms face The atoms in a face-centered cubic unit cell touch along the face diagonal of the cubic unit cell. Using the Pythagorean formula, where l length of the face diagonal and r radius of the atom:

9 44 CAPTER 0 LIQUIDS AND SOLIDS 4r l l + l (4r) l 6r l r l l r 97 0 m 5.57 Volume of a unit cell l ( m cm 0 cm).7 0 cm Mass of a unit cell 4 Ca atoms mol Ca atoms 40.0 g Ca mol Ca.66 0 g Ca Density mass volume.66 0 g.54 g/cm.7 0 cm 50. There are four Ni atoms in each unit cell. For a unit cell: mass density volume Solving: l g/cm 4 Ni atoms 0 cm cube edge length mol Ni atoms l 5.69 g Ni mol Ni 4r l For a face-centered cube: (4r) l + l l r l, r l / r.5 0 cm / r.6 0 cm 6 pm l 5. The unit cell for cubic closest packing is the face-centered unit cell. The volume of a unit cell is: V l 0 (49 0 cm).9 0 cm There are four Pb atoms in the unit cell, as is the case for all face-centered cubic unit cells. The mass of atoms in a unit cell is:

10 CAPTER 0 LIQUIDS AND SOLIDS 45 mass 4 Pb atoms mol Pb atoms 07. g Pb mol Pb. 0 g Density mass volume. 0 g.6 g/cm.9 0 cm From Exercise 49, the relationship between the cube edge length l and the radius r of an atom in a face-centered unit cell is l r. r l 49 pm 74 pm m 5. The volume of a unit cell is: V l (. 0 0 cm) cm There are four Ir atoms in the unit cell, as is the case for all face-centered cubic unit cells. The mass of atoms in a unit cell is: mol Ir 9. g Ir mass 4 Ir atoms.77 0 g atoms mol Ir Density mass volume.77 0 g.6 g/cm cm 5. A face-centered cubic unit cell contains four atoms. For a unit cell: mass of X volume density ( cm) 0.5 g/cm 7. 0 g mol X 4 atoms X mol X atoms mol X Molar mass g X mol X 0 g/mol; the metal is silver (Ag). 54. For a face-centered unit cell, the radius r of an atom is related to the length of a cube edge l by the equation l r (see Exercise 49). Radius r l / 9 0 m / m.9 0 cm The volume of a unit cell is l, so the mass of the unknown metal (X) in a unit cell is: volume density (.9 0 cm).45 g X cm.9 0 g X

11 46 CAPTER 0 LIQUIDS AND SOLIDS Because each face-centered unit cell contains four atoms of X: mol X in unit cell 4 atoms X mol X atoms X mol X Therefore, each unit cell contains.9 0 g X, which is equal to mol X. The molar mass of X is: g X mol X 94 g/mol From the periodic table, the best choice for the metal is platinum. / Ti 55. For a body-centered unit cell, corners corner + Ti at body center Ti atoms. All body-centered unit cells have two atoms per unit cell. For a unit cell where l cube edge length: mol Ti 47. g Ti atoms Ti density 4.50 g/cm atoms mol Ti l Solving: l edge length of unit cell. 0 cm pm Assume Ti atoms just touch along the body diagonal of the cube, so body diagonal 4 radius of atoms 4r. The triangle we need to solve is: l 4r -. x 0 cm l - (. x 0 cm) (4r) (. 0 cm) + [(. 0 cm) ], r.4 0 cm 4 pm For a body-centered unit cell (bcc), the radius of the atom is related to the cube edge length by: 4r l or l 4r/. 56. From Exercise 55:

12 CAPTER 0 LIQUIDS AND SOLIDS 47 4r l l 6r l + l l 4r/ (.09)r l.09( pm) 5 pm 5. 0 cm In a body-centered cubit unit cell, there are two atoms per unit cell. For a unit cell: density mass volume atoms Ba mol Ba (5. 0 atoms cm) 7. g Ba mol Ba. g cm 57. If gold has a face-centered cubic structure, then there are four atoms per unit cell, and from Exercise 49: l 6r 4r l l r (44 pm) 407 pm l m cm l mol Au 4 atoms Au atoms Density ( cm) 97.0 g Au mol Au 9.4 g/cm If gold has a body-centered cubic structure, then there are two atoms per unit cell, and from Exercise 55: 6r l + l 4r l l l 4r/ pm 0 m l 0 0 cm. 0 cm Density atoms Au mol Au atoms (. 0 cm) 97.0 g Au mol Au 7.7 g/cm The measured density of gold is consistent with a face-centered cubic unit cell.

13 4 CAPTER 0 LIQUIDS AND SOLIDS 5. If face-centered cubic: l r (7 pm) 7 pm.7 0 cm density 4 atomsw mol (.7 0 atoms cm).9 g W mol. g/cm If body-centered cubic: l 4r 4 7 pm 6 pm.6 0 cm density atoms W mol.9 g W atoms mol (.6 0 cm) 9.4 g/cm The measured density of tungsten is consistent with a body-centered unit cell. 59. In a face-centered unit cell (ccp structure), the atoms touch along the face diagonal: 4r l (4r) l + l l r V cube l (r ) (.6)r There are four atoms in a face-centered cubic cell (see Exercise 49). Each atom has a volume of (4/)πr volume of a sphere. V atoms 4 4 πr (6.76)r So V V atoms. atoms cube (6.76)r , or 74.06% of the volume of each unit cell is occupied by (.6)r In a simple cubic unit cell, the atoms touch along the cube edge l: (radius) r l r l V cube l (r) r

14 CAPTER 0 LIQUIDS AND SOLIDS 49 There is one atom per simple cubic cell ( corner atoms / atom per corner atom/unit cell). Each atom has an assumed volume of (4/)πr volume of a sphere. 4 V atom πr (4.9)r Vatom (4.9)r So 0.56, or 5.6% of the volume of each unit cell is occupied by V cube r atoms. A cubic closest packed structure (face-centered cubic unit cell) packs the atoms much more efficiently than a simple cubic structure. 60. From Exercise 55, a body-centered unit cell contains two net atoms, and the length of a cube edge l is related to the radius of the atom r by the equation l 4r/. Volume of unit cell l (4r/ ) (.)r Volume of atoms in unit cell 4 πr (.7)r So V V atoms cube (.7)r % occupied (.)r To determine the radius of the Fe atoms, we need to determine the cube edge length l. Volume of unit cell Fe atoms Volume l.6 mol Fe atoms 0 cm, l.7 0 cm 55.5 g Fe cm mol Fe 7.6 g.6 0 cm l 4r/, r l / cm / cm 6. Doping silicon with phosphorus produces an n-type semiconductor. The phosphorus adds electrons at energies near the conduction band of silicon. Electrons do not need as much energy to move from filled to unfilled energy levels, so conduction increases. Doping silicon with gallium produces a p-type semiconductor. Because gallium has fewer valence electrons than silicon, holes (unfilled energy levels) at energies in the previously filled molecular orbitals are created, which induces greater electron movement (greater conductivity). 6. A rectifier is a device that produces a current that flows in one direction from an alternating current that flows in both directions. In a p-n junction, a p-type and an n-type semiconductor are connected. The natural flow of electrons in a p-n junction is for the excess electrons in the n-type semiconductor to move to the empty energy levels (holes) of the p-type semiconductor. Only when an external electric potential is connected so that electrons flow in this natural direction will the current flow easily (forward bias). If the external electric potential is connected in reverse of the natural flow of electrons, no current flows through the system (reverse bias). A p-n junction only transmits a current under forward bias, thus converting the alternating current to direct current.

15 50 CAPTER 0 LIQUIDS AND SOLIDS 6. In has fewer valence electrons than Se. Thus Se doped with In would be a p-type semiconductor. 64. To make a p-type semiconductor, we need to dope the material with atoms that have fewer valence electrons. The average number of valence electrons is four when mixtures of Group A and Group 5A elements are considered. We could dope with more of the Group A element or with atoms of Zn or Cd. Cadmium is the most common impurity used to produce p-type GaAs semiconductors. To make an n-type GaAs semiconductor, dope with an excess Group 5A element or dope with a Group 6A element such as sulfur. 65. E gap.5 ev J/eV J; we want E gap E light hc/λ, so: hc λ E ( J s)( J m / s) m nm 66. E hc λ ( J s)( m m / s) J energy of band gap / Cl 67. Sodium chloride structure: corners corner + 6 faces / Cl face 4 Cl ions / 4 Na edges + Na at body center 4 Na ions; NaCl is the formula. edge / Cl Cesium chloride structure: Cs ion at body center; corners Cl ion; CsCl is the formula. corner Zinc sulfide structure: There are four Zn ions inside the cube. / S corners corner / S + 6 faces face 4 S ions; ZnS is the formula. Titanium oxide structure: / Ti corners corner + Ti at body center Ti ions 4 faces / O face + O inside cube 4 O ions; TiO is the formula. / Ni 6. Both As ions are inside the unit cell. corners corner + 4 edges / 4 Ni Ni ions edge The unit cell contains ions of Ni and ions of As, which gives a formula of NiAs. 69. There is one octahedral hole per closest packed anion in a closest packed structure. If onehalf of the octahedral holes are filled, then there is a : ratio of fluoride ions to cobalt ions in the crystal. The formula is CoF.

16 CAPTER 0 LIQUIDS AND SOLIDS There are two tetrahedral holes per closest packed anion. Let f fraction of tetrahedral holes filled by the cations. f Na O: Cation-to-anion ratio, f ; all the tetrahedral holes are filled by Na + cations. f CdS: Cation-to-anion ratio, f ; one-half the tetrahedral holes are filled by Cd + cations. f ZrI 4 : Cation-to-anion ratio, f ; one-eighth the tetrahedral holes are filled 4 by Zr 4+ cations. 7. In a cubic closest packed array of anions, there are twice the number of tetrahedral holes as anions present, and an equal number of octahedral holes as anions present. A cubic closest packed array of sulfide ions will have four S ions, eight tetrahedral holes, and four octahedral holes. In this structure we have /() Zn + ion and /(4) Al + ions present, along with the 4 S ions. The formula is ZnAl S A repeating pattern in the two-dimensional structure is: Assuming the anions A are the larger circles, there are four anions completely in this repeating square. The corner cations (smaller circles) are shared by four different repeating squares. Therefore, there is one cation in the middle of the square plus /4 (4) net cation from the corners. Each repeating square has two cations and four anions. The empirical formula is MA. 7. F ions at corners / F /corner F ion per unit cell; Because there is one cubic hole per cubic unit cell, there is a : ratio of F ions to metal ions in the crystal if only half of the body centers are filled with the metal ions. The formula is MF, where M + is the metal ion. 74. Mn ions at corners: (/) Mn ion; F ions at edges: (/4) F ions; the formula is MnF. Assuming fluoride is charged, then the charge on Mn is From Figure 0.7, MgO has the NaCl structure containing 4 Mg + ions and 4 O ions per face-centered unit cell. 4 MgO formula units mol MgO atoms 40.g MgO mol MgO.67 0 g MgO

17 5 CAPTER 0 LIQUIDS AND SOLIDS 76. Volume of unit cell.67 0 g MgO cm.5 g Volume of unit cell l, l cube edge length; l ( cm For a face-centered unit cell, the O ions touch along the face diagonal: 4. 0 cm l 4r, r.49 O O 4 0 cm ) / 4. 0 cm 0 cm The cube edge length goes through two radii of the O anions and the diameter of the Mg + cation, so: l r + +, 4. 0 cm (.49 0 cm) + r, r 6.5 O r Mg Mg + Mg cm Assuming K + and Cl just touch along the cube edge l: l (4 pm) 6 pm 6. 0 cm Volume of unit cell l The unit cell contains four K + and four Cl ions. For a unit cell: density 4 KCl formula units mol KCl formula units (6. 0 cm) g KCl mol KCl.00 g/cm 77. CsCl is a simple cubic array of Cl ions with Cs + in the middle of each unit cell. There is one Cs + and one Cl ion in each unit cell. Cs + and Cl ions touch along the body diagonal. Body diagonal r + + r l, l length of cube edge Cs Cl In each unit cell: mol CsCl mass CsCl formula unit formula units volume l.796 l g CsCl cm.97 g CsCl g CsCl mol CsCl 0 cm 0 cm, l 4. 0 cm 4 pm length of cube edge g

18 CAPTER 0 LIQUIDS AND SOLIDS 5 r + + r l (4 pm) 75 pm Cs Cl The distance between ion centers r r 75 pm/ 5 pm Cs + + Cl From ionic radius: r + 69 pm and r pm; r + + Cs Cl Cs r Cl pm The distance calculated from the density is pm (.%) greater than that calculated from tables of ionic radii. 7. a. The NaCl unit cell has a face-centered cubic arrangement of the anions with cations in the octahedral holes. There are four NaCl formula units per unit cell, and since there is a : ratio of cations to anions in MnO, then there would be four MnO formula units per unit cell, assuming an NaCl-type structure. The CsCl unit cell has a simple cubic structure of anions with the cations in the cubic holes. There is one CsCl formula unit per unit cell, so there would be one MnO formula unit per unit cell if a CsCl structure is observed. Formula units of MnO Unit cell ( cm) 5. g MnO cm mol MnO g MnO formula units MnO 4.00 formula units MnO mol MnO From the calculation, MnO crystallizes in the NaCl type structure. b. From the NaCl structure and assuming the ions touch each other, then l cube edge length r. + + r Mn O l cm + (.40 0 cm), + r.5 0 cm 4 pm + r Mn 79. a. CO : molecular b. SiO : network c. Si: atomic, network d. C 4 : molecular e. Ru: atomic, metallic f. I : molecular g. KBr: ionic h. O: molecular i. NaO: ionic j. U: atomic, metallic k. CaCO : ionic l. P : molecular 0. a. diamond: atomic, network b. P : molecular c. : molecular d. Mg: atomic, metallic e. KCl: ionic f. quartz: network g. N 4 NO : ionic h. SF : molecular i. Ar: atomic, group A j. Cu: atomic, metallic k. C 6 O 6 : molecular. a. The unit cell consists of Ni at the cube corners and Ti at the body center or Ti at the cube corners and Ni at the body center. 4 Mn

19 54 CAPTER 0 LIQUIDS AND SOLIDS b. / atom from corners + atom at body center; empirical formula NiTi c. Both have a coordination number of (both are surrounded by atoms). / Al. Al: corners corner Al; Ni: 6 face centers / Ni face center Ni The composition of the specific phase of the superalloy is AlNi.. Structure Structure / Ca / Ti corners Ca atom corners Ti atom corner corner 6 faces / O face / 4 O O atoms edges corner O atoms Ti at body center. Formula CaTiO Ca at body center. Formula CaTiO In the extended lattice of both structures, each Ti atom is surrounded by six O atoms. 4. With a cubic closest packed array of oxygen ions, we have 4 O ions per unit cell. We need to balance the total! charge of the anions with a + charge from the Al + and Mg + cations. The only combination of ions that gives a + charge is Al + ions and Mg + ion. The formula is Al MgO 4. There are an equal number of octahedral holes as anions (4) in a cubic closest packed array and twice the number of tetrahedral holes as anions in a cubic closest packed array. For the stoichiometry to work out, we need Al + and Mg + per unit cell. ence one-half of the octahedral holes are filled with Al + ions, and one-eighth of the tetrahedral holes are filled with Mg + ions. 5. a. Y: Y in center; Ba: Ba in center / Cu Cu: corners corner Cu, edges / 4 Cu edge Cu, total Cu atoms / 4 O O: 0 edges edge 5 oxygen, faces / O face 4 oxygen, total 9 O atoms Formula: YBa Cu O 9 b. The structure of this superconductor material follows the second perovskite structure described in Exercise. The YBa Cu O 9 structure is three of these cubic perovskite unit cells stacked on top of each other. The oxygen atoms are in the same places, Cu takes the place of Ti, two of the calcium atoms are replaced by two barium atoms, and one Ca is replaced by Y. c. Y, Ba, and Cu are the same. Some oxygen atoms are missing.

20 CAPTER 0 LIQUIDS AND SOLIDS 55 / 4 O edges edge O, faces / O face 4 O, total 7 O atoms Superconductor formula is YBa Cu O a. Structure (a): / Tl Ba: Ba inside unit cell; Tl: corners corner Tl Cu: 4 edges O: 6 faces Structure (b): / 4 Cu edge / O face Cu / 4 O + edges edge 5 O; Formula TlBa CuO 5. Tl and Ba are the same as in structure (a). / 4 Cu Ca: Ca inside unit cell; Cu: edges Cu edge O: 0 faces Structure (c): / O face / 4 O + edges edge 7 O; Formula TlBa CaCu O 7. Tl and Ba are the same, and two Ca are located inside the unit cell. Cu: edges / 4 Cu edge Cu; O: 4 faces / O face / 4 O + edges edge 9 O Formula TlBa Ca Cu O 9. Structure (d): Following similar calculations, formula TlBa Ca Cu 4 O. b. Structure (a) has one planar sheet of Cu and O atoms, and the number increases by one for each of the remaining structures. The order of superconductivity temperature from lowest to highest temperature is (a) < (b) < (c) < (d). c. TlBa CuO 5 : + () + x + 5( ) 0, x + Only Cu + is present in each formula unit. TlBa CaCu O 7 : + () + + (x) + 7( ) 0, x +5/ Each formula unit contains Cu + and Cu +. TlBa Ca Cu O 9 : + () + () + (x) + 9( ) 0, x +7/ Each formula unit contains Cu + and Cu +. TlBa Ca Cu 4 O : + () + () + 4(x) + ( ) 0, x +9/4 Each formula unit contains Cu + and Cu +.

21 56 CAPTER 0 LIQUIDS AND SOLIDS d. This superconductor material achieves variable copper oxidation states by varying the numbers of Ca, Cu, and O in each unit cell. The mixtures of copper oxidation states are discussed in part c. The superconductor material in Exercise 5 achieves variable copper oxidation states by omitting oxygen at various sites in the lattice. Phase Changes and Phase Diagrams 7. If we graph ln P vap versus /T with temperature in Kelvin, the slope of the resulting straight line will be vap /R. P vap ln P vap T (Li) /T T (Mg) /T torr 0 0 K K 9 K. 0 4 K For Li: We get the slope by taking two points (x, y) that are on the line we draw. For a line, slope y/ x, or we can determine the straight-line equation using a calculator. The general straight-line equation is y mx + b, where m slope and b y intercept. The equation of the Li line is: ln P vap (/T) +.6, slope K Slope vap /R, vap slope R K.45 J/K mol vap J/mol 5 kj/mol

22 CAPTER 0 LIQUIDS AND SOLIDS 57 For Mg: The equation of the line is: ln P vap (/T) +.7, slope K vap slope R K.45 J/K mol vap J/mol 9 kj/mol The bonding is stronger in Li because vap is larger for Li.. We graph ln P vap vs /T. The slope of the line equals! vap /R. T(K) 0 /T (K ) P vap (torr) ln P vap Slope ( ) K!4600 K K R vap vap, vap,000 J/mol kj/mol.45 J/K mol To determine the normal boiling point, we can use the following formula: P vap ln P R T T At the normal boiling point, the vapor pressure equals.00 atm or 760. torr. At 7 K, the vapor pressure is 4.4. torr (from data in the problem). 4.4,000 J/mol ln, J/K mol T 7 K! (/T!.66 0 )! /T.0 0, T 57 K normal boiling point 9. At 00. C (7 K), the vapor pressure of O is.00 atm 760. torr. For water, vap 40.7 kj/mol. P ln P R vap T T or P ln P R vap T T

23 5 CAPTER 0 LIQUIDS AND SOLIDS 50. torr J/mol ln, 760. torr.45 J/K mol 7 K T! K! ! T, T.76 0, T.76 0 T 6 K or 9 C 90. At 00. C (7 K), the vapor pressure of O is.00 atm. For water, vap 40.7 kj/mol. P ln P R vap T T or P ln P R vap T T P ln.00 atm J/mol,.45 J/K mol 7 K K ln P 0.5, P e atm.50 ln J/mol.45 J/K mol 7 K T, K T T, T.4 0, T K or 40. C 9. P vap 6 torr vap ln, ln P R T T torr.45 J/K mol K 5 K Solving: vap. 0 4 J/mol; for the normal boiling point, P.00 atm 760. torr torr ln torr 4. 0 J/mol.45 J/K mol K T, T T 50. K 77EC; the normal boiling point of CCl 4 is 77EC. 9. P ln P R vap T T P 760. torr, T 56.5 C K; P 60. torr, T? J/mol ln, J/K mol T T , T.0 0, T 4.5 K 5. C T

24 CAPTER 0 LIQUIDS AND SOLIDS torr.0 0 J/mol ln, P.45 J/K mol ln 60.! ln P.05 ln P 5.40, P e 5.40 torr X(g, 00. C) X(g, 75 C), T -5 C.0 J q s gas m T 50. g (!5 C)!600 J 6. kj g C X(g, 75 C) X(l, 75 C), q 50. g mol 0. kj!67 kj 75.0 g mol.5 J X(l, 75 C) X(l, 5 C), q 50. g ( 90. C) 56,000 J 56 kj g C X(l, 5 C) X(s,!5 C), q g mol 5.0 kj!7 kj 75.0 g mol.0 J X(s, 5 C) X(s,!50. C), q g (!5 C)!6,000 J!6 kj g C q total q + q + q + q 4 + q kj 95. a. Many more intermolecular forces must be broken to convert a liquid to a gas as compared with converting a solid to a liquid. Because more intermolecular forces must be broken, much more energy is required to vaporize a liquid than is required to melt a solid. Therefore, vap is much larger than fus. b..00 g Na mol Na.60 kj 0. kj J to melt.00 g Na.99 g mol Na

25 60 CAPTER 0 LIQUIDS AND SOLIDS c..00 g Na mol Na.99 g 97.0 kj 4. kj 40 J to vaporize.00 g Na mol Na d. This is the reverse process of that described in part c, so the energy change is the same quantity but opposite in sign. Therefore, q 40 J; i.e., 40 of heat will be released. 96. Melt:.5 g C 6 6 mol C6 7. g kj.05 kj mol C 6 6 Vaporize:.5 g C 6 6 mol C6 7. g kj.4 kj mol C 6 6 As is typical, the energy required to vaporize a certain quantity of substance is much larger than the energy required to melt the same quantity of substance. A lot more intermolecular forces must be broken to vaporize a substance as compared to melting a substance. 97. To calculate q total, break up the heating process into five steps. O(s, 0. C) O(s, 0 C), T 0. C.0 J q s ice m T g 0. C J 0. kj o g C O(s, 0 C) O(l, 0 C), q mol 6.0 kj g O 67 kj.0 g mol O(l, 0 C) O(l, 00. C), q 4. J g 00. C. 0 5 J 0 kj o g C O(l, 00. C) O(g, 00. C), q g mol.0 g 40.7 kj 0 kj mol.0 J O(g, 00. C) O(g, 50. C), q g 50. C J o g C 50 kj q total q + q + q + q 4 + q kj 9. O(g, 5 C) O(g, 00. C), q.0 J/g C C 75.0 g (!5 C) 00 J!. kj O(g, 00. C) O(l, 00. C), q 75.0 g mol 40.7 kj 69 kj.0 g mol O(l, 00. C) O(l, 0 C), q 4. J/g C C 75.0 g ( 00. C),000 J kj To convert O(g) at 5 C to O(l) at 0 C requires (!. kj! 69 kj! kj )!05 kj of heat removed. To convert from O(l) at 0 C to O(s) at 0 C requires:

26 CAPTER 0 LIQUIDS AND SOLIDS 6 q g mol 6.0 kj!5. kj.0 g mol This amount of energy puts us over the!5 kj limit (!05 kj! 5. kj!0. kj). Therefore, a mixture of O(s) and O(l) will be present at 0 C when 5 kj of heat is removed from the gas sample. 99. Total mass O cubes 0.0 g cube eat removed to produce ice at -5.0 C: mol O 540. g; 540. g O 0.0 mol O.0 g. J g C 4 o 540. g.0 C mol J 0.0 mol.0 J o g 5.0 C g C J J J J J g CF Cl.49 0 g CF Cl must be vaporized. 5 J 00. eat released 0.50 g Na mol.99 g 6 kj.00 kj mol To melt 50.0 g of ice requires: 50.0 g ice mol O 6.0 kj 6.7 kj.0 g mol The reaction doesn't release enough heat to melt all of the ice. The temperature will remain at 0 C. 0. A: solid B: liquid C: vapor D: solid + vapor E: solid + liquid + vapor F: liquid + vapor G: liquid + vapor : vapor triple point: E critical point: G Normal freezing point: Temperature at which solid-liquid line is at.0 atm (see following plot). Normal boiling point: Temperature at which liquid-vapor line is at.0 atm (see following plot )..0 atm nfp Because the solid-liquid line equilibrium has a positive slope, the solid phase is denser than the liquid phase. nbp

27 6 CAPTER 0 LIQUIDS AND SOLIDS 0. a. b. Triple point at 95. C: rhombic, monoclinic, gas Triple point at 5. C: monoclinic, liquid, gas Triple point at 5 C: rhombic, monoclinic, liquid c. From the phase diagram, the monoclinic solid phase is stable at T 00. C and P atm. d. Normal melting point 5. C; normal boiling point C; the normal melting and boiling points occur at P.0 atm. e. Rhombic is the densest phase because the rhombic-monoclinic equilibrium line has a positive slope, and because the solid-liquid equilibrium lines also have positive slopes. 5 f. No; P.0 0 atm is at a pressure somewhere between the 95. and 5. C triple points. At this pressure, the rhombic and gas phases are never in equilibrium with each 5 other, so rhombic sulfur cannot sublime at P.0 0 atm. owever, monoclinic sulfur can sublime at this pressure. 0. a. two g. From the phase diagram, we would start off with gaseous sulfur. At 00. C and ~ 0 5 atm, S(g) would convert to the solid monoclinic form of sulfur. Finally at 00. C and some large pressure less than 40 atm, S(s, monoclinic) would convert to the solid rhombic form of sulfur. Summarizing, the phase changes are S(g) S(monoclinic) S(rhombic). b. igher-pressure triple point: graphite, diamond and liquid; lower-pressure triple point: graphite, liquid and vapor c. It is converted to diamond (the more dense solid form). d. Diamond is more dense, which is why graphite can be converted to diamond by applying pressure. 04. The following sketch of the Br phase diagram is not to scale. Because the triple point of Br is at a temperature below the freezing point of Br, the slope of the solid-liquid line is positive. 00 Pressure (atm) 0.05 Solid Liquid Gas Temperature ( o C)

28 CAPTER 0 LIQUIDS AND SOLIDS 6 The positive slopes of all the lines indicate that Br (s) is more dense than Br (l), which is more dense than Br (g). At room temperature (~ C) and atm, Br (l) is the stable phase. Br (l) cannot exist at a temperature below the triple-point temperature of!7. C or at a temperature above the critical-point temperature of 0 C. The phase changes that occur as temperature is increased at 0.0 atm are solid liquid gas. 05. Because the density of the liquid phase is greater than the density of the solid phase, the slope of the solid-liquid boundary line is negative (as in O). With a negative slope, the melting points increase with a decrease in pressure, so the normal melting point of X should be greater than 5EC. 06. P (torr) 760 s l 0 g T( C) From the three points given, the slope of the solid-liquid boundary line is positive, so Xe(s) is more dense than Xe(l). Also, the positive slope of this line tells us that the melting point of Xe increases as pressure increases. The same direct relationship exists for the boiling point of Xe because the liquid-gas boundary line also has a positive slope. Connecting to Biochemistry 07. The structures of the two C 6 O compounds (0 valence e ) are:

29 64 CAPTER 0 LIQUIDS AND SOLIDS C C O exhibits relatively strong hydrogen bonding C O C does not exhibit hydrogen bonding The liquid will have the stronger intermolecular forces. Therefore, the first compound above (ethanol) is the liquid, whereas the second compound (dimethyl ether) with the weaker intermolecular forces is the gas. 0. Benzene Naphthalene LD forces only LD forces only Note: London dispersion forces in molecules such as benzene and naphthalene are fairly large. The molecules are flat, and there is efficient surface-area contact between molecules. Large surface-area contact leads to stronger London dispersion forces. Cl Carbon tetrachloride (CCl 4 ) has polar bonds but is a nonpolar molecule. CCl 4 only has LD forces. Cl C Cl Cl In terms of size and shape CCl 4 < C 6 6 < C 0. The strengths of the LD forces are proportional to size and are related to shape. Although the size of CCl 4 is fairly large, the overall spherical shape gives rise to relatively weak LD forces as compared to flat molecules such as benzene and naphthalene. The physical properties given in the problem are consistent with the order listed above. Each of the physical properties will increase with an increase in intermolecular forces.

30 CAPTER 0 LIQUIDS AND SOLIDS 65 Acetone Acetic acid O C C C O C C O LD, dipole LD, dipole, -bonding Benzoic acid O C O LD, dipole, -bonding We would predict the strength of interparticle forces of the last three molecules to be: acetone < acetic acid < benzoic acid polar -bonding -bonding, but large LD forces because of greater size and shape This ordering is consistent with the values given for boiling point, melting point, and vap. The overall order of the strengths of intermolecular forces based on physical properties are: acetone < CCl 4 < C 6 6 < acetic acid < naphthalene < benzoic acid The order seems reasonable except for acetone and naphthalene. Because acetone is polar, we would not expect it to boil at the lowest temperature. owever, in terms of size and shape, acetone is the smallest molecule, and the LD forces in acetone must be very small compared to the other molecules. Naphthalene must have very strong LD forces because of its size and flat shape. 09. Both molecules are capable of -bonding. owever, in oil of wintergreen the hydrogen bonding is intramolecular (within each molecule): O C O C O In methyl-4-hydroxybenzoate, the -bonding is intermolecular (between molecules), resulting in stronger forces between molecules and a higher melting point. 0. With the charged ends, this tripeptide exhibits ionic forces. Between the charged ends, there are nonpolar C groups, polar CO groups, and polar N groups. The nonpolar C groups will interact with C groups on other tripeptides through London dispersion forces. The polar CO group allows the tripeptides to interact with each other through dipole forces. And finally, the N bonds allow for hydrogen-bonding interactions with other tripeptides.

31 66 CAPTER 0 LIQUIDS AND SOLIDS. C 5 O(l) C 5 O(g) is an endothermic process. eat is absorbed when liquid ethanol vaporizes; the internal heat from the body provides this heat, which results in the cooling of the body.. O(l) O(g) 44 kj/mol; the vaporization of water is an endothermic process. In order to evaporate, water must absorb heat from the surroundings. In this case, part of the surroundings is our body. So, as water evaporates, our body supplies heat, and as a result, our body temperature can cool down. From Le Chatelier s principle, the less water vapor in the air, the more favorable the evaporation process. Thus the less humid the surroundings, the more favorably water converts into vapor, and the more heat that is lost by our bodies.. The phase change O(g) O(l) releases heat that can cause additional damage. Also, steam can be at a temperature greater than 00 C. 4. P vap 760 torr vap ln, ln P R T T 400. torr.45 J/K mol 9. K 07. K Solving: vap. 0 4 J/mol. kj/mol Additional Exercises 5. As the physical properties indicate, the intermolecular forces are slightly stronger in D O than in O. 6. C CO : -bonding + dipole forces + LD forces C ClCO : C CO C : -bonding + larger electronegative atom replacing (greater dipole) + LD forces Dipole forces (no -bonding) + LD forces From the intermolecular forces listed above, we predict C CO C to have the weakest intermolecular forces and C ClCO to have the strongest. The boiling points are consistent with this view. 7. At any temperature, the plot tells us that substance A has a higher vapor pressure than substance B, with substance C having the lowest vapor pressure. Therefore, the substance with the weakest intermolecular forces is A, and the substance with the strongest intermolecular forces is C. N can form hydrogen-bonding interactions, whereas the others cannot. Substance C is N. The other two are nonpolar compounds with only London dispersion forces. Because C 4 is smaller than Si 4, C 4 will have weaker LD forces and is substance A. Therefore, substance B is Si 4.

32 CAPTER 0 LIQUIDS AND SOLIDS 67. As the electronegativity of the atoms covalently bonded to increases, the strength of the hydrogen-bonding interaction increases. N N < N O < O O < O F < F F weakest / Xe 9. corners corner / 4 F + Xe inside cell Xe; edges edge strongest + F inside cell 4 F Empirical formula is XeF. This is also the molecular formula. 0. One B atom and one N atom together have the same number of electrons as two C atoms. The description of physical properties sounds a lot like the properties of graphite and diamond, the two solid forms of carbon. The two forms of BN have structures similar to graphite and diamond.. B 6 : This compound contains only nonmetals, so it is probably a molecular solid with covalent bonding. The low boiling point confirms this. SiO : This is the empirical formula for quartz, which is a network solid. CsI: This is a metal bonded to a nonmetal, which generally form ionic solids. The electrical conductivity in aqueous solution confirms this. W: Tungsten is a metallic solid as the conductivity data confirm.. Ar is cubic closest packed. There are four Ar atoms per unit cell, and with a face-centered unit cell, the atoms touch along the face diagonal. Let l length of cube edge. Face diagonal 4r l, l 4(90. pm)/ 57 pm cm mol 9.95 g 4 atoms mass atoms mol Density.7 g/cm volume (5.7 0 cm). 4.7 g C 6 6 P C 6 6 mol 7. g 0.6 mol C L atm 0.6 mol 9. K nrt K mol atm, or 57. torr V 00.0 L 4. In order to set up an equation, we need to know what phase exists at the final temperature. To heat 0.0 g of ice from!0.0 to 0.0 C requires: q.0 J g C 0.0 g 0.0EC 406 J

London dispersion (LD) < dipole-dipole < H bonding < metallic bonding, covalent network, ionic.

London dispersion (LD) < dipole-dipole < H bonding < metallic bonding, covalent network, ionic. CAPTER TEN LIQUIDS AND SOLIDS For Review. Intermolecular forces are the relatively weak forces between molecules that hold the molecules together in the solid and liquid phases. Intramolecular forces are

More information

CHAPTER 10 LIQUIDS AND SOLIDS. Questions

CHAPTER 10 LIQUIDS AND SOLIDS. Questions CHAPTER 0 LIQUIDS AND SOLIDS Questions 2. Chalk is composed of the ionic compound calcium carbonate (CaCO ). The electrostatic forces in ionic compounds are much stronger than the intermolecular forces

More information

13. London dispersion (LD) < dipole-dipole < H bonding < metallic bonding, covalent network, ionic.

13. London dispersion (LD) < dipole-dipole < H bonding < metallic bonding, covalent network, ionic. CHAPTER TEN LIQUIDS AND SOLIDS Questions 12. Dipole forces are the forces that act between polar molecules. The electrostatic attraction between the positive end of one polar molecule and the negative

More information

Chapter 10. Liquids and Solids

Chapter 10. Liquids and Solids Chapter 10 Liquids and Solids Section 10.1 Intermolecular Forces Section 10.1 Intermolecular Forces Section 10.1 Intermolecular Forces Section 10.1 Intermolecular Forces Metallic bonds Covalent bonds Ionic

More information

London Dispersion Forces (LDFs) Intermolecular Forces Attractions BETWEEN molecules. London Dispersion Forces (LDFs) London Dispersion Forces (LDFs)

London Dispersion Forces (LDFs) Intermolecular Forces Attractions BETWEEN molecules. London Dispersion Forces (LDFs) London Dispersion Forces (LDFs) LIQUIDS / SOLIDS / IMFs Intermolecular Forces (IMFs) Attractions BETWEEN molecules NOT within molecules NOT true bonds weaker attractions Represented by dashed lines Physical properties (melting points,

More information

Chapter 10. Liquids and Solids

Chapter 10. Liquids and Solids Chapter 10 Liquids and Solids Chapter 10 Table of Contents 10.1 Intermolecular Forces 10.2 The Liquid State 10.3 An Introduction to Structures and Types of Solids 10.4 Structure and Bonding in Metals 10.5

More information

Liquids and Solids. H fus (Heat of fusion) H vap (Heat of vaporization) H sub (Heat of sublimation)

Liquids and Solids. H fus (Heat of fusion) H vap (Heat of vaporization) H sub (Heat of sublimation) Liquids and Solids Phase Transitions All elements and compounds undergo some sort of phase transition as their temperature is increase from 0 K. The points at which these phase transitions occur depend

More information

Metallic & Ionic Solids. Crystal Lattices. Properties of Solids. Network Solids. Types of Solids. Chapter 13 Solids. Chapter 13

Metallic & Ionic Solids. Crystal Lattices. Properties of Solids. Network Solids. Types of Solids. Chapter 13 Solids. Chapter 13 1 Metallic & Ionic Solids Chapter 13 The Chemistry of Solids Jeffrey Mack California State University, Sacramento Crystal Lattices Properties of Solids Regular 3-D arrangements of equivalent LATTICE POINTS

More information

Chapter 10: Liquids and Solids

Chapter 10: Liquids and Solids Chapter 10: Liquids and Solids Chapter 10: Liquids and Solids *Liquids and solids show many similarities and are strikingly different from their gaseous state. 10.1 Intermolecular Forces Intermolecular

More information

- intermolecular forces forces that exist between molecules

- intermolecular forces forces that exist between molecules Chapter 11: Intermolecular Forces, Liquids, and Solids - intermolecular forces forces that exist between molecules 11.1 A Molecular Comparison of Liquids and Solids - gases - average kinetic energy of

More information

Chapter 11 Intermolecular Forces, Liquids, and Solids

Chapter 11 Intermolecular Forces, Liquids, and Solids Chapter 11 Intermolecular Forces, Liquids, and Solids Dissolution of an ionic compound States of Matter The fundamental difference between states of matter is the distance between particles. States of

More information

Chapter 11. Intermolecular Forces and Liquids & Solids

Chapter 11. Intermolecular Forces and Liquids & Solids Chapter 11 Intermolecular Forces and Liquids & Solids The Kinetic Molecular Theory of Liquids & Solids Gases vs. Liquids & Solids difference is distance between molecules Liquids Molecules close together;

More information

They are similar to each other. Intermolecular forces

They are similar to each other. Intermolecular forces s and solids They are similar to each other Different than gases. They are incompressible. Their density doesn t change much with temperature. These similarities are due to the molecules staying close

More information

They are similar to each other

They are similar to each other They are similar to each other Different than gases. They are incompressible. Their density doesn t change much with temperature. These similarities are due to the molecules staying close together in solids

More information

Intermolecular forces (IMFs) CONDENSED STATES OF MATTER

Intermolecular forces (IMFs) CONDENSED STATES OF MATTER Intermolecular forces (IMFs) CONDENSED STATES OF MATTER States of Matter: - composed of particles packed closely together with little space between them. Solids maintain a. - any substance that flows.

More information

CHAPTER 11 INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS

CHAPTER 11 INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS CAPTER 11 INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS 11.7 ICl has a dipole moment and Br 2 does not. The dipole moment increases the intermolecular attractions between ICl molecules and causes that substance

More information

What determines the phase of a substance? Temperature Pressure Interparticle Forces of Attraction

What determines the phase of a substance? Temperature Pressure Interparticle Forces of Attraction Liquids and Solids What determines the phase of a substance? Temperature Pressure Interparticle Forces of Attraction Types of Interparticle Forces Ionic Bonding Occurs between cations and anions Metallic

More information

Chapter 10 Liquids and Solids. Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, , 113

Chapter 10 Liquids and Solids. Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, , 113 Chapter 10 Liquids and Solids Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, 104-106, 113 Recall: Intermolecular vs. Intramolecular Forces Intramolecular: bonds between

More information

compared to gases. They are incompressible. Their density doesn t change with temperature. These similarities are due

compared to gases. They are incompressible. Their density doesn t change with temperature. These similarities are due Liquids and solids They are similar compared to gases. They are incompressible. Their density doesn t change with temperature. These similarities are due to the molecules being close together in solids

More information

Liquids, Solids and Phase Changes

Liquids, Solids and Phase Changes Chapter 10 Liquids, Solids and Phase Changes Chapter 10 1 KMT of Liquids and Solids Gas molecules have little or no interactions. Molecules in the Liquid or solid state have significant interactions. Liquids

More information

Exercises 491. Phase Changes and Phase Diagrams

Exercises 491. Phase Changes and Phase Diagrams Exercises 491 above that of liquid nitrogen were recently discovered. The structures of these materials are based on the perovskite structure. Were they to have the ideal perovskite structure, the superconductor

More information

Chapter 12. Insert picture from First page of chapter. Intermolecular Forces and the Physical Properties of Liquids and Solids

Chapter 12. Insert picture from First page of chapter. Intermolecular Forces and the Physical Properties of Liquids and Solids Chapter 12 Insert picture from First page of chapter Intermolecular Forces and the Physical Properties of Liquids and Solids Copyright McGraw-Hill 2009 1 12.1 Intermolecular Forces Intermolecular forces

More information

AP* Chapter 10. Liquids and Solids. Friday, November 22, 13

AP* Chapter 10. Liquids and Solids. Friday, November 22, 13 AP* Chapter 10 Liquids and Solids AP Learning Objectives LO 1.11 The student can analyze data, based on periodicity and the properties of binary compounds, to identify patterns and generate hypotheses

More information

Chapter 11: Intermolecular Forces. Lecture Outline

Chapter 11: Intermolecular Forces. Lecture Outline Intermolecular Forces, Liquids, and Solids 1 Chapter 11: Intermolecular Forces Lecture Outline 11.1 A Molecular Comparison of Gases, Liquids and Solids Physical properties of substances are understood

More information

Solids. properties & structure

Solids. properties & structure Solids properties & structure Determining Crystal Structure crystalline solids have a very regular geometric arrangement of their particles the arrangement of the particles and distances between them is

More information

Chapter 9. Liquids and Solids

Chapter 9. Liquids and Solids Chapter 9 Liquids and Solids Chapter 9 Table of Contents (9.1) (9.2) (9.3) (9.4) (9.5) (9.6) (9.7) (9.8) (9.9) (9.10) Intermolecular forces The liquid state An introduction to structures and types of solids

More information

Liquids and Solids Chapter 10

Liquids and Solids Chapter 10 Liquids and Solids Chapter 10 Nov 15 9:56 AM Types of Solids Crystalline solids: Solids with highly regular arrangement of their components Amorphous solids: Solids with considerable disorder in their

More information

Chapter 10: Liquids, Solids, and Phase Changes

Chapter 10: Liquids, Solids, and Phase Changes Chapter 10: Liquids, Solids, and Phase Changes In-chapter exercises: 10.1 10.6, 10.11; End-of-chapter Problems: 10.26, 10.31, 10.32, 10.33, 10.34, 10.35, 10.36, 10.39, 10.40, 10.42, 10.44, 10.45, 10.66,

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 A phase is a homogeneous part of the system in contact

More information

Chapter 10 Review Packet

Chapter 10 Review Packet Chapter 10 Review Packet Name 1. If water and carbon dioxide molecules did interact, what major intermolecular force will exist between these molecules? a) Hydrogen bonding b) London dispersion c) Dipole-dipole

More information

ก ก ก Intermolecular Forces: Liquids, Solids, and Phase Changes

ก ก ก Intermolecular Forces: Liquids, Solids, and Phase Changes ก ก ก Intermolecular Forces: Liquids, Solids, and Phase Changes ก ก ก ก Mc-Graw Hill 1 Intermolecular Forces: Liquids, Solids, and Phase Changes 12.1 An Overview of Physical States and Phase Changes 12.2

More information

Intermolecular Forces and Liquids and Solids. Chapter 11. Copyright The McGraw Hill Companies, Inc. Permission required for

Intermolecular Forces and Liquids and Solids. Chapter 11. Copyright The McGraw Hill Companies, Inc. Permission required for Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw Hill Companies, Inc. Permission required for 1 A phase is a homogeneous part of the system in contact with other parts of the

More information

Name: Class: Date: ID: A

Name: Class: Date: ID: A Name: Class: _ Date: _ CH11 1. Order the intermolecular forces (dipole-dipole, London dispersion, ionic, and hydrogen-bonding) from weakest to strongest. A) dipole-dipole, London dispersion, ionic, and

More information

The Liquid and Solid States

The Liquid and Solid States : The Liquid and Solid States 10-1 10.1 Changes of State How do solids, liquids and gases differ? Figure 10.4 10-2 1 10.1 Changes of State : transitions between physical states Vaporization/Condensation

More information

CHEM Principles of Chemistry II Chapter 10 - Liquids and Solids

CHEM Principles of Chemistry II Chapter 10 - Liquids and Solids CHEM 1212 - Principles of Chemistry II Chapter 10 - Liquids and Solids 10.1 Intermolecular Forces recall intramolecular (within the molecule) bonding whereby atoms can form stable units called molecules

More information

Chap. 12 INTERMOLECULAR FORCES

Chap. 12 INTERMOLECULAR FORCES Chap. 12 INTERMOLECULAR FORCES Know how energy determines physical properties and how phase changes occur as a result of heat flow. Distinguish between bonding (intermolecular) and nonbonding (intermolecular)

More information

Forces, Liquids, and Solids

Forces, Liquids, and Solids 11 Intermolecular Forces, Liquids, and Solids Visualizing Concepts 11.1 The diagram best describes a liquid. In the diagram, the particles are close together, mostly touching but there is no regular arrangement

More information

Ch 11: Intermolecular Forces, Liquids, and Solids

Ch 11: Intermolecular Forces, Liquids, and Solids AP Chemistry: Intermolecular Forces, Liquids, and Solids Lecture Outline 11.1 A Molecular Comparison of Liquids and Solids Physical properties of liquids and solids are due to intermolecular forces. These

More information

Diamond. There are four types of solid: -Hard Structure - Tetrahedral atomic arrangement. What hybrid state do you think the carbon has?

Diamond. There are four types of solid: -Hard Structure - Tetrahedral atomic arrangement. What hybrid state do you think the carbon has? Bonding in Solids Bonding in Solids There are four types of solid: 1. Molecular (formed from molecules) - usually soft with low melting points and poor conductivity. 2. Covalent network - very hard with

More information

Chapter 12 INTERMOLECULAR FORCES. Covalent Radius and van der Waals Radius. Intraand. Intermolecular Forces. ½ the distance of non-bonded

Chapter 12 INTERMOLECULAR FORCES. Covalent Radius and van der Waals Radius. Intraand. Intermolecular Forces. ½ the distance of non-bonded Chapter 2 INTERMOLECULAR FORCES Intraand Intermolecular Forces Covalent Radius and van der Waals Radius ½ the distance of bonded ½ the distance of non-bonded Dipole Dipole Interactions Covalent and van

More information

Some Properties of Solids, Liquids, and Gases

Some Properties of Solids, Liquids, and Gases AP Chemistry: Intermolecular Forces, Liquids, and Solids Lecture Outline 11.1 A Molecular Comparison of Liquids and Solids Physical properties of liquids and solids are due to intermolecular forces. These

More information

There are four types of solid:

There are four types of solid: Bonding in Solids There are four types of solid: 1. Molecular (formed from molecules) - usually soft with low melting points and poor conductivity. 2. Covalent network - very hard with very high melting

More information

CHEMISTRY The Molecular Nature of Matter and Change

CHEMISTRY The Molecular Nature of Matter and Change CHEMISTRY The Molecular Nature of Matter and Change Third Edition Chapter 12 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Chapter 11 INTERMOLECULAR FORCES

More information

Intermolecular Forces. Chapter 16 Liquids and Solids. Intermolecular Forces. Intermolecular Forces. Intermolecular Forces. Intermolecular Forces

Intermolecular Forces. Chapter 16 Liquids and Solids. Intermolecular Forces. Intermolecular Forces. Intermolecular Forces. Intermolecular Forces Big Idea: Systems that form macromolecules (ionic, metallic, and covalent network) have the strongest interactions between formula units. Systems that cannot form macro molecules still contain intermolecular

More information

INTERMOLECULAR FORCES: LIQUIDS, SOLIDS & PHASE CHANGES (Silberberg, Chapter 12)

INTERMOLECULAR FORCES: LIQUIDS, SOLIDS & PHASE CHANGES (Silberberg, Chapter 12) INTERMOLECULAR FORCES: LIQUIDS, SOLIDS & PASE CANGES (Silberberg, Chapter 12) Intermolecular interactions Ideal gas molecules act independently PV=nRT Real gas molecules attract/repulse one another 2 n

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. A phase is a homogeneous part of the system in contact

More information

Chem 1A Dr. White Fall 2015 Exam 3 Practice Problems

Chem 1A Dr. White Fall 2015 Exam 3 Practice Problems Exam 3 Practice Problems 1. The face centered cubic cell of copper has an edge length of 0.362 nm. Calculate the density of copper (g/cm 3 ). 2. Consider the following ionic substances and arrange them

More information

Chemistry 101 Chapter 14 Liquids & Solids

Chemistry 101 Chapter 14 Liquids & Solids Chemistry 101 Chapter 14 Liquids & Solids States of matter: the physical state of matter depends on a balance between the kinetic energy of particles, which tends to keep them apart, and the attractive

More information

2. As gas P increases and/or T is lowered, intermolecular forces become significant, and deviations from ideal gas laws occur (van der Waal equation).

2. As gas P increases and/or T is lowered, intermolecular forces become significant, and deviations from ideal gas laws occur (van der Waal equation). A. Introduction. (Section 11.1) CHAPTER 11: STATES OF MATTER, LIQUIDS AND SOLIDS 1. Gases are easily treated mathematically because molecules behave independently. 2. As gas P increases and/or T is lowered,

More information

Chapters 11 and 12: Intermolecular Forces of Liquids and Solids

Chapters 11 and 12: Intermolecular Forces of Liquids and Solids 1 Chapters 11 and 12: Intermolecular Forces of Liquids and Solids 11.1 A Molecular Comparison of Liquids and Solids The state of matter (Gas, liquid or solid) at a particular temperature and pressure depends

More information

Some Properties of Solids, Liquids, and Gases

Some Properties of Solids, Liquids, and Gases AP Chemistry: Intermolecular Forces, Liquids, and Solids Sec 1. A Molecular Comparison of Liquids and Solids Physical properties of liquids and solids are due to intermolecular forces. These are forces

More information

Properties of Liquids and Solids. Vaporization of Liquids. Vaporization of Liquids. Aims:

Properties of Liquids and Solids. Vaporization of Liquids. Vaporization of Liquids. Aims: Properties of Liquids and Solids Petrucci, Harwood and Herring: Chapter 13 Aims: To use the ideas of intermolecular forces to: Explain the properties of liquids using intermolecular forces Understand the

More information

Properties of Liquids and Solids. Vaporization of Liquids

Properties of Liquids and Solids. Vaporization of Liquids Properties of Liquids and Solids Petrucci, Harwood and Herring: Chapter 13 Aims: To use the ideas of intermolecular forces to: Explain the properties of liquids using intermolecular forces Understand the

More information

Chapter 7. Ionic & Covalent Bonds

Chapter 7. Ionic & Covalent Bonds Chapter 7 Ionic & Covalent Bonds Ionic Compounds Covalent Compounds 7.1 EN difference and bond character >1.7 = ionic 0.4 1.7 = polar covalent 1.7 Electrons not shared at

More information

Ch 9 Liquids & Solids (IMF) Masterson & Hurley

Ch 9 Liquids & Solids (IMF) Masterson & Hurley Ch 9 Liquids & Solids (IMF) Masterson & Hurley Intra- and Intermolecular AP Questions: 2005 Q. 7, 2005 (Form B) Q. 8, 2006 Q. 6, 2007 Q. 2 (d) and (c), Periodic Trends AP Questions: 2001 Q. 8, 2002 Q.

More information

AP Chemistry: Liquids and Solids Practice Problems

AP Chemistry: Liquids and Solids Practice Problems AP Chemistry: Liquids and Solids Practice Problems Directions: Write your answers to the following questions in the space provided. or problem solving, show all of your work. Make sure that your answers

More information

PROPERTIES OF SOLIDS SCH4U1

PROPERTIES OF SOLIDS SCH4U1 PROPERTIES OF SOLIDS SCH4U1 Intra vs. Intermolecular Bonds The properties of a substance are influenced by the force of attraction within and between the molecules. Intra vs. Intermolecular Bonds Intramolecular

More information

Chapter 11 SOLIDS, LIQUIDS AND GASES Pearson Education, Inc.

Chapter 11 SOLIDS, LIQUIDS AND GASES Pearson Education, Inc. Chapter 11 SOLIDS, LIQUIDS AND GASES States of Matter Because in the solid and liquid states particles are closer together, we refer to them as. The States of Matter The state of matter a substance is

More information

The Liquid and Solid States

The Liquid and Solid States : The Liquid and Solid States 10-1 10.1 Changes of State How do solids, liquids and gases differ? Figure 10.4 10-2 10.1 Changes of State : transitions between physical states Vaporization/Condensation

More information

CHEM 172 EXAMINATION 2. February 12, Dr. Kimberly M. Broekemeier NAME: l = 2r l = 8 1/2 r l = (4/3 1/2 )r. h = 6.

CHEM 172 EXAMINATION 2. February 12, Dr. Kimberly M. Broekemeier NAME: l = 2r l = 8 1/2 r l = (4/3 1/2 )r. h = 6. EM 17 EXAMINATION February 1, 009 Dr. Kimberly M. Broekemeier NAME: P 1 1 P1 R T T1 ln = - ( - ) l = r l = 8 1/ r l = (4/3 1/ )r onstants: c = 3.00 X 10 8 m/s h = 6.63 X 10-34 J x s R = 0.0806 L x atm/mol

More information

Chapter 14. Liquids and Solids

Chapter 14. Liquids and Solids Chapter 14 Liquids and Solids Section 14.1 Water and Its Phase Changes Reviewing What We Know Gases Low density Highly compressible Fill container Solids High density Slightly compressible Rigid (keeps

More information

Properties of Liquids and Solids

Properties of Liquids and Solids Properties of Liquids and Solids World of Chemistry Chapter 14 14.1 Intermolecular Forces Most substances made of small molecules are gases at normal temperature and pressure. ex: oxygen gas, O 2 ; nitrogen

More information

States of matter. Chapter 11. Kinetic Molecular Theory of Liquids and Solids. Kinetic Molecular Theory of Solids Intermolecular Forces

States of matter. Chapter 11. Kinetic Molecular Theory of Liquids and Solids. Kinetic Molecular Theory of Solids Intermolecular Forces States of matter Chapter 11 Intermolecular Forces Liquids and Solids By changing the T and P, any matter can exist as solid, liquid or gas. Forces of attraction determine physical state Phase homogeneous

More information

States of Matter; Liquids and Solids. Condensation - change of a gas to either the solid or liquid state

States of Matter; Liquids and Solids. Condensation - change of a gas to either the solid or liquid state States of Matter; Liquids and Solids Phase transitions - a change in substance from one state to another Melting - change from a solid to a liquid state Freezing - change of a liquid to the solid state

More information

Unit Six --- Ionic and Covalent Bonds

Unit Six --- Ionic and Covalent Bonds Unit Six --- Ionic and Covalent Bonds Electron Configuration in Ionic Bonding Ionic Bonds Bonding in Metals Valence Electrons Electrons in the highest occupied energy level of an element s atoms Examples

More information

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS Chemistry 1411 Joanna Sabey Forces Phase: homogeneous part of the system in contact with other parts of the system but separated from them by a

More information

General Chemistry 202 CHM202 General Information. General Chemistry 202 CHM202 Policies. General Chemistry 202 CHM202 Laboratory Guidelines

General Chemistry 202 CHM202 General Information. General Chemistry 202 CHM202 Policies. General Chemistry 202 CHM202 Laboratory Guidelines General Chemistry 202 CHM202 General Information Instructor Meeting times and places Text and recommended materials Website Email Grading Schedule 1 General Chemistry 202 CHM202 Policies Equipment Instruction

More information

Chapter 11/12: Liquids, Solids and Phase Changes Homework: Read Chapter 11 and 12 Keep up with assignments

Chapter 11/12: Liquids, Solids and Phase Changes Homework: Read Chapter 11 and 12 Keep up with assignments P a g e 1 Unit 3: Chapter 11/12: Liquids, Solids and Phase Changes Homework: Read Chapter 11 and 12 Keep up with assignments Liquids and solids are quite different from gases due to their attractive forces

More information

CH116 - General Chemistry 2 - Solutions to HW Problems - Chapter 10

CH116 - General Chemistry 2 - Solutions to HW Problems - Chapter 10 CH116 - General Chemistry 2 - Solutions to HW Problems - Chapter 10 HW: Chapter 10: Problems 36, 38, 40, 42, 44, 46, 50, 58, 66, 68, 74, 76, 82, 84, 86, 88, 90 The IMFs (intermolecular forces) to consider

More information

Unit Five: Intermolecular Forces MC Question Practice April 14, 2017

Unit Five: Intermolecular Forces MC Question Practice April 14, 2017 Unit Five: Intermolecular Forces Name MC Question Practice April 14, 2017 1. Which of the following should have the highest surface tension at a given temperature? 2. The triple point of compound X occurs

More information

Bonding. Polar Vs. Nonpolar Covalent Bonds. Ionic or Covalent? Identifying Bond Types. Solutions + -

Bonding. Polar Vs. Nonpolar Covalent Bonds. Ionic or Covalent? Identifying Bond Types. Solutions + - Chemical Bond Mutual attraction between the nuclei and valence electrons of different atoms that binds them together. Bonding onors Chemistry 412 Chapter 6 Types of Bonds Ionic Bonds Force of attraction

More information

Lesson 1: Stability and Energy in Bonding Introduction

Lesson 1: Stability and Energy in Bonding Introduction Lesson 1: Stability and Energy in Bonding Introduction Chemical bonding is the simultaneous attraction of two positive nuclei to negative electrons. Chemical bonding is said to be the glue that holds particles

More information

Chem 112 Dr. Kevin Moore

Chem 112 Dr. Kevin Moore Chem 112 Dr. Kevin Moore Gas Liquid Solid Polar Covalent Bond Partial Separation of Charge Electronegativity: H 2.1 Cl 3.0 H Cl δ + δ - Dipole Moment measure of the net polarity in a molecule Q Q magnitude

More information

Honors Chemistry Dr. Kevin D. Moore

Honors Chemistry Dr. Kevin D. Moore Honors Chemistry Dr. Kevin D. Moore Key Properties: Solid is less dense than liquid Water reaches maximum density at 4 C Very high specific heat Dissolves many substances Normal Boiling Point: 100 C Normal

More information

Chapter 16: Phenomena. Chapter 16 Liquids and Solids. intermolecular forces? Intermolecular Forces. Intermolecular Forces. Intermolecular Forces

Chapter 16: Phenomena. Chapter 16 Liquids and Solids. intermolecular forces? Intermolecular Forces. Intermolecular Forces. Intermolecular Forces Chapter 16: Phenomena Phenomena: The tables below show melting points and boiling points of substances. What patterns do you notice from the data? Melting Boiling Substance Point Point CaO 2886 K 4123

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids PowerPoint Lecture Presentation by J. David Robertson University of Missouri Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction

More information

Notes on Solids and Liquids

Notes on Solids and Liquids THE LIQUID STATE Notes on Solids and Liquids Why do liquids tend to bead up when on a solid surface? The effect of uneven pull on surface molecules draws them into the body of the liquid causing droplet

More information

16. NO 3, 5 + 3(6) + 1 = 24 e. 22. HCN, = 10 valence electrons

16. NO 3, 5 + 3(6) + 1 = 24 e. 22. HCN, = 10 valence electrons Solution to Chapts 9 & 10 Problems: 16. N 3, 5 + 3(6) + 1 = 24 e 22. HCN, 1 + 4 + 5 = 10 valence electrons Assuming N is hybridized, both C and N atoms are sp hybridized. The C H bond is formed from overlap

More information

CHAPTER 8 BONDING: GENERAL CONCEPTS Ionic solids are held together by strong electrostatic forces that are omnidirectional.

CHAPTER 8 BONDING: GENERAL CONCEPTS Ionic solids are held together by strong electrostatic forces that are omnidirectional. CAPTER 8 BDIG: GEERAL CCEPTS 1 CAPTER 8 BDIG: GEERAL CCEPTS Questions 15. a. This diagram represents a polar covalent bond as in. In a polar covalent bond, there is an electron rich region (indicated by

More information

Bonding. Honors Chemistry 412 Chapter 6

Bonding. Honors Chemistry 412 Chapter 6 Bonding Honors Chemistry 412 Chapter 6 Chemical Bond Mutual attraction between the nuclei and valence electrons of different atoms that binds them together. Types of Bonds Ionic Bonds Force of attraction

More information

INTERMOLECULAR FORCES AND CONDENSED STATES

INTERMOLECULAR FORCES AND CONDENSED STATES INTERMOLECULAR FORCES AND CONDENSED STATES I. Intermolecular Forces A. Types of Intermolecular Forces. 1. Van der Waals forces = attractive forces that exist between neutral molecules. a. Are much weaker

More information

Chapter 11. Intermolecular Forces, Liquids, and Solids

Chapter 11. Intermolecular Forces, Liquids, and Solids 11.2 Intermolecular Forces Intermolecular forces are much weaker than ionic or covalent bonds (e.g., 16 kj/mol versus 431 kj/mol for HCl). Melting or boiling = broken intermolecular forces Intermolecular

More information

Questions 1 to 58 must be answered on the Scantron sheets.

Questions 1 to 58 must be answered on the Scantron sheets. Questions 1 to 58 must be answered on the Scantron sheets. Base your answers to questions 1 to 5 on the heating curve for a pure substance that is shown below. 1. The freezing point of the substance is

More information

Multiple Choice. Multiple Choice

Multiple Choice. Multiple Choice 1. At what temperature in degree Celcius is the value in degree Fahrenheit twice of that in degree Celcius? A) 160 o C B) -24.6 o C C) 6.4 o C D) 22.2 o C E) 32 o C 2. The correct name for NaOCl is, A)

More information

Chapter 11. Liquids and Intermolecular Forces

Chapter 11. Liquids and Intermolecular Forces Chapter 11 Liquids and Intermolecular Forces States of Matter The three states of matter are 1) Solid Definite shape Definite volume 2) Liquid Indefinite shape Definite volume 3) Gas Indefinite shape Indefinite

More information

SOLID STATE CHEMISTRY

SOLID STATE CHEMISTRY SOLID STATE CHEMISTRY Crystal Structure Solids are divided into 2 categories: I. Crystalline possesses rigid and long-range order; its atoms, molecules or ions occupy specific positions, e.g. ice II. Amorphous

More information

Chapter 10: Liquids and Solids

Chapter 10: Liquids and Solids Chapter 10: Liquids and Solids STATES OF MATTER: At any temperature above absolute zero, the atoms, molecules, or ions that make up a substance are moving. In the kinetic theory of gases, this motion is

More information

Liquids & Solids. For the condensed states the ave KE is less than the attraction between molecules so they are held together.

Liquids & Solids. For the condensed states the ave KE is less than the attraction between molecules so they are held together. Liquids & Solids Intermolecular Forces Matter exists in 3 states. The state of matter is influenced by the physical properties of a substance. For liquids & solids, the condensed states, many of the physical

More information

The exam time is 1hr45 minutes. Try to finish this practice exam in the same time.

The exam time is 1hr45 minutes. Try to finish this practice exam in the same time. Practice exam for final exam, Chem 1210, Dr. Wu Note: The exam time is 1hr45 minutes. Try to finish this practice exam in the same time. 1. Which of the following gases will exhibit the least ideal behavior?

More information

Sample Exercise 11.1 Identifying Substances That Can Form Hydrogen Bonds

Sample Exercise 11.1 Identifying Substances That Can Form Hydrogen Bonds Sample Exercise 11.1 Identifying Substances That Can Form Hydrogen Bonds In which of these substances is hydrogen bonding likely to play an important role in determining physical properties: methane (CH

More information

Chapter 10. The Liquid and Solid States. Introduction. Chapter 10 Topics. Liquid-Gas Phase Changes. Physical State of a Substance

Chapter 10. The Liquid and Solid States. Introduction. Chapter 10 Topics. Liquid-Gas Phase Changes. Physical State of a Substance Introduction Chapter 10 The Liquid and Solid States How do the properties of liquid and solid substances differ? How can we predict properties based on molecular- level structure? Glasses Wires Reshaping

More information

Chapter 6. Chemical Bonding

Chapter 6. Chemical Bonding Chapter 6 Chemical Bonding Section 6.1 Intro to Chemical Bonding 6.1 Objectives Define chemical bond. Explain why most atoms form chemical bonds. Describe ionic and covalent bonding. Explain why most chemical

More information

CHM 151 Practice Final Exam

CHM 151 Practice Final Exam CM 151 Practice Final Exam 1. ow many significant figures are there in the result of 5.52 divided by 3.745? (a) 1 (b) 2 (c) 3 (d) 4 (e) 5 2. ow many significant figures are there in the answer when 9.021

More information

1051-3rd Chem Exam_ (A)

1051-3rd Chem Exam_ (A) 1051-3rd Chem Exam_1060111(A) MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) The molecular-orbital model for Ge shows it to be A) a conductor,

More information

1051-3rd Chem Exam_ (B)

1051-3rd Chem Exam_ (B) 1051-3rd Chem Exam_1060111(B) MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) In liquids, the attractive intermolecular forces are. A) strong enough

More information

1051-3rd Chem Exam_ (C)

1051-3rd Chem Exam_ (C) 1051-3rd Chem Exam_1060111(C) MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) The hybridizations of iodine in IF3 and IF5 are and, respectively.

More information

Remember the purpose of this reading assignment is to prepare you for class. Reading for familiarity not mastery is expected.

Remember the purpose of this reading assignment is to prepare you for class. Reading for familiarity not mastery is expected. Remember the purpose of this reading assignment is to prepare you for class. Reading for familiarity not mastery is expected. After completing this reading assignment and reviewing the intro video you

More information

Chapter 10. Liquids and Solids. Copyright 2017 Cengage Learning. All Rights Reserved.

Chapter 10. Liquids and Solids. Copyright 2017 Cengage Learning. All Rights Reserved. Chapter 10 Liquids and Solids Chapter 10 Table of Contents (10.1) (10.2) (10.3) (10.4) (10.5) Intermolecular forces The liquid state An introduction to structures and types of solids Structure and bonding

More information

Intermolecular Forces, Liquids, & Solids

Intermolecular Forces, Liquids, & Solids , Liquids, & Solids Mr. Matthew Totaro Legacy High School AP Chemistry States of Matter The fundamental difference between states of matter is the distance between particles. States of Matter Because in

More information

Ch 6 Chemical Bonding

Ch 6 Chemical Bonding Ch 6 Chemical Bonding What you should learn in this section (objectives): Define chemical bond Explain why most atoms form chemical bonds Describe ionic and covalent bonding Explain why most chemical bonding

More information