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1 Topic 11 Liquids and Solids. 2 States of Matter Comparison of gases, liquids, and solids. –Gases are compressible fluids. Their molecules are widely.

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Presentation on theme: "1 Topic 11 Liquids and Solids. 2 States of Matter Comparison of gases, liquids, and solids. –Gases are compressible fluids. Their molecules are widely."— Presentation transcript:

1 1 Topic 11 Liquids and Solids

2 2 States of Matter Comparison of gases, liquids, and solids. –Gases are compressible fluids. Their molecules are widely separated with no volume or shape. –Liquids are relatively incompressible fluids. Their molecules are more tightly packed and touching with volume but no shape. –Solids are nearly incompressible and rigid. Their molecules or ions are in close contact and do not move with volume and shape.

3 3 Changes of State A change of state or phase transition is a change of a substance from one state to another. The energy associated with changing states is equal for both directions but opposite in sign meaning exothermic vs endothermic. solid liquid gas melting or fusion freezing or crystallization condensationboiling or vaporization sublimation condensation or deposition exo endo

4 4 Vapor Pressure Liquids are continuously vaporizing even if their not at their boiling point. –If a liquid is in a closed vessel with space above it, a partial pressure of the vapor state builds up in this space. –The vapor pressure of a liquid is the partial pressure of the vapor over the liquid, measured at equilibrium at a given temperature. –The more gas molecules (vapor), the higher the vapor pressure.

5 5 Vapor Pressure The vapor pressure of a liquid depends on its temperature. –Liquids with relatively high vapor pressures at normal temperatures are said to be volatile. The higher the vapor pressure, the easier it goes from a liquid to a gas. –i.e. acetone has a high vapor pressure. –As the temperature increases, the kinetic energy of the molecular motion becomes greater, and vapor pressure increases. More energy available to convert liquid molecules to gas; hence, more gas molecules and higher vapor pressure.

6 6 Boiling Point The temperature at which the vapor pressure of a liquid equals the pressure exerted on the liquid is called the boiling point. –As the temperature of a liquid increases, the vapor pressure increases (more gas molecules formed) until it reaches atmospheric pressure and begins to boil. –At this point, stable bubbles of vapor (same species) form within the liquid. This is called boiling. –The normal boiling point is the boiling point at 1 atm. –Because atmospheric pressure varies with altitude and weather conditions, the boiling point of a liquid does as well. –Boiling point of water at 1 atm is 100 o C but approximately 71 o C on Mount Everest at 8850m elevation (0.33 atm). as atm pressure decreases, boiling point decreases

7 7 Clausius-Clapeyron Equation We noted that vapor pressure was a function of temperature. –It has been demonstrated that the logarithm of the vapor pressure of a liquid varies linearly with absolute temperature, K. –Consequently, the vapor pressure of a liquid at two different temperatures is described by: –Equation allows you to determine the vapor pressure of substance at any temperature if you know the vapor pressure at the normal boiling point.

8 8 Carbon disulfide, CS 2, has a normal boiling point of 46 ° C (vapor pressure = 760 mmHg) and a heat of vaporization of 26.8 kJ/mol. What is the vapor pressure of carbon disulfide at 35 ° C? Substituting into the Clausius-Clapeyron equation, we obtain: Taking the antiln we obtain: 319 K 308 K Note: Temp decreased and VP decreased

9 9 Freezing Point The temperature at which a pure liquid changes to a crystalline solid, or freezes, is called the freezing point. –The melting point is identical to the freezing point and is defined as the temperature at which a solid becomes a liquid. –Unlike boiling points, melting points are not affected significantly by pressure changes; however, large pressure changes may have some affect. S L melting, +  H endothermic freezing, -  H exothermic

10 10 Heat of Phase Transition To melt a pure substance at its melting point requires an extra boost of energy to overcome lattice energies. –The heat needed to melt 1 mol of a pure substance is called the heat of fusion and denoted  H fus. –For ice, the heat of fusion is 6.01 kJ/mol.  

11 11 Heat of Phase Transition To boil a pure substance at its boiling point requires an extra boost of energy to overcome intermolecular forces. –The heat needed to boil 1 mol of a pure substance is called the heat of vaporization and denoted  H vap. –For liquid water, the heat of vaporization is 40.66 kJ/mol.  

12 12 Figure : Heating curve for water. Note: Temp does not change while changing states; heat is used to overcome forces of attraction  H fus = 6.01 kJ   H crystal = -6.01 kJ   H vap = 40.66 kJ   H cond = -40.66 kJ 

13 13 Phase Diagrams A phase diagram is a graphical way to summarize the conditions under which the different states of a substance are stable for different temperatures and pressures. –The diagram is divided into three areas representing each state of the substance. –The curves separating each area represent the boundaries of phase changes.

14 14 Phase Diagrams Below is a typical phase diagram. It consists of three curves that divide the diagram into regions labeled “solid, liquid, and gas”. B temperature pressure A C D solidliquid gas..

15 15 Phase Diagrams Curve AB, dividing the solid region from the liquid region, represents the conditions under which the solid and liquid are in equilibrium. B temperature pressure A C D solidliquid gas..

16 16 Phase Diagrams Usually, the melting point is only slightly affected by pressure. For this reason, the melting point curve, AB, is nearly vertical. B temperature pressure A C D solidliquid gas..

17 17 Phase Diagrams If a liquid is more dense than its solid (i.e. water), the curve leans slightly to the left (points toward less dense state), causing the melting point to decrease with pressure. B temperature pressure A C D solid less dense liquid more dense gas..

18 18 Phase Diagrams If a liquid is less dense than its solid, the curve leans slightly to the right, causing the melting point to increase with pressure. Most solids are more dense than liquids. B temperature pressure A C D liquid less dense gas.. solid more dense

19 19 Phase Diagrams Curve AC, which divides the liquid region from the gaseous region, represents the boiling points of the liquid for various pressures. Note that pressure has a major affect on curve and the boiling point. B temperature pressure A C D solidliquid gas..

20 20 Phase Diagrams Curve AD, which divides the solid region from the gaseous region, represents the vapor pressures of the solid at various temperatures. An example of a solid that goes directly to a gas is dry ice, CO 2. B temperature pressure A C D solidliquid gas..

21 21 Phase Diagrams The curves intersect at A, the triple point, which is the temperature and pressure where three phases (solid, liquid, gas) of a substance exist in equilibrium (i.e. water occurs at 273.15K and 4.58 Torr). B temperature pressure A C D solidliquid gas.. L solid less dense g s

22 22 Phase Diagrams The temperature above which the liquid state of a substance no longer exists regardless of pressure is called the critical temperature. B temperature pressure A C D solidliquid gas.. T crit

23 23 Phase Diagrams The vapor pressure at the critical temperature is called the critical pressure. Note that curve AC ends at the critical point, C. No liquefaction is observed above the critical temperature. When the pressure of the gas above the critical temperature is increased beyond the critical pressure, we have what is called a supercritical fluid, SCF. B temperature pressure A C D solidliquid gas.. T crit P crit SCF

24 24 Intermolecular Forces In general, properties like boiling point, melting point, viscosity, vapor pressure, and surface tension depend on the strength of the attractive forces among the molecules. The stronger the attractive forces, the higher the boiling point, viscosity and surface tension of a liquid; the higher the melting point of a solid; and the lower the vapor pressure of a liquid. Molecules gain more freedom of movement as a solid melts or as a liquid vaporizes. The amount of energy that they need to overcome the forces of attraction among them increases the stronger the forces are.

25 25 Surface Tension Surface tension is the energy required to increase the surface area of a liquid by a unit amount. A molecule within a liquid is pulled in all directions, whereas a molecule on the surface is only pulled to the interior. As a result, there is a tendency for the surface area of the liquid to be minimized. To increase the surface area of a liquid requires movement of molecules within the interior, where they experience stronger attractions, to the surface. This requires energy. The stronger the intermolecular (attractive) forces between molecules, the higher the surface tension.

26 26 Viscosity Viscosity is the resistance to flow exhibited by all liquids and gases. Viscosity can be illustrated by measuring the time required for a steel ball to fall through a column of the liquid. Even without such measurements, you know that syrup has a greater viscosity than water (thicker the fluid, the more resistant to flow). The stronger the intermolecular (attractive) forces among the molecules of the gas or liquid, the more resistant they would be to flow, the higher the viscosity. You can lower the viscosity of a substance by increasing the temperature giving the system more energy to overcome the attractive forces thereby increasing flow.

27 27 Intermolecular Forces The attractive forces between two molecules can be classified into two major types: 1.) van der Waals forces which are the weak attractive forces in a large number of substances (all covalent bonded). 2.) hydrogen bonding interactions which occurs in substances containing hydrogen atoms bonded to certain very electronegative atoms (O, N, & F).

28 28 Van der Waals Forces Van der Waals forces can be further classified into: 1.) London dispersion forces (occurs between any pair of molecules) 2.) dipole-induced dipole interaction (occurs between a nonpolar molecule and a polar molecule) 3.) dipole-dipole interaction (occurs between two polar molecules)

29 29 London Dispersion Forces London forces refers to the force of attraction that exists between any pair of molecules and is the predominant interaction among most molecules. It is due to temporary molecular polarizations, which occur because electrons are always moving causing a distortion of the electron cloud surrounding a molecule. The larger the molecule, the more frequently the polarization occur. Therefore, we expect attractions to be stronger among larger molecules. This means London forces increase with molecular weight. The larger a molecule, the more easily the electron cloud can be distorted.

30 30 London Dispersion Forces Let’s look at N 2 and O 2 as pure substances. Both are nonpolar molecules that only have London dispersion forces of attraction. Since they only have London forces, the molecule with the larger molar mass will have more polarization and a higher boiling point, viscosity, and surface tension as well as a lower vapor pressure. N2O2N2O2 M m 28g/mol32g/mol BP-196 o C-183 o C Since O 2 has a higher molar mass, we expect it to have a higher boiling point than N 2.

31 31 Dipole-Dipole Interactions Dipole-dipole interactions refers to the force of attraction that exists between polar molecules. The dipole-dipole interaction is an attractive intermolecular force resulting from the tendency of polar molecules to align themselves positive end to negative end. There is a higher electron density in the Cl end of the polar molecule; this end, we say, is partially negative. The H end of the polar molecule is partially positive and is attracted to the partially negative end of a nearby HCl molecule which is a dipole-dipole interaction. H Cl   H  

32 32 Dipole-Dipole Interactions N 2 NOO 2 M m 28g/mol30g/mol32g/mol BP-196 o C-152 o C-183 o C Let’s look at N 2, NO, and O 2 pure substances. Both N 2 and O 2 are nonpolar molecules that only have London dispersion forces of attraction. However, NO is a polar molecule which has dipole-dipole interactions in addition to London forces to overcome which affects its boiling point, viscosity, surface tension, and vapor pressure. The boiling point of NO will be the highest among these substances because of the additional dipole-dipole interactions in the polar molecule.

33 33 Dipole-induced Dipole Interactions Dipole-induced dipole interaction refers to the force of attraction that exists between a polar molecule and a nonpolar molecule. When a nonpolar molecule comes close to the positive end of a polar molecule, its electrons would be attracted toward the polar molecule causing temporary (or induced) polarization. Similarly, when a molecule comes close to the negative end of a polar molecule, its electrons would be repelled, again causing temporary (or induced) polarization.

34 34 Hydrogen Bonding Hydrogen bonding is a force that exists between a hydrogen atom covalently bonded to a very electronegative atom (O, N, F). –To exhibit hydrogen bonding, one of the following three structures must be present. H NOHFH ::: –Only N, O, and F are electronegative enough to leave the hydrogen nucleus almost stripped bare of electrons making it strongly attracted to a lone pair of a highly electronegative atom (O, N, F) in a nearby molecule.

35 35 Hydrogen Bonding in H 2 O H H O : : H H O : : H H O : : H H O : : The H atoms in water are bonded to a highly electronegative O atom. Because H is almost stripped bare of electrons, it is strongly attracted to the lone pair of the O atom in the neighboring water molecule

36 36 Hydrogen Bonding Hydrogen bonding interaction is much stronger than dipole- dipole interaction and for small molecules stronger than London forces. Hydrogen bonding accounts for the unusually high boiling point of water. Water molecules are small and a liquid at room temperature; substances made of molecules of comparable size are gaseous at room temperature. O 2 is a gas at room temperature, while H 2 O is a liquid even though H 2 O molecules are smaller than O 2 molecules. Water is a polar molecule and capable of extensive hydrogen bonding thereby raising its boiling point considerably.

37 37 Hydrogen Bonding Molecules exhibiting hydrogen bonding have abnormally high boiling points compared to molecules with similar van der Waals forces. Which of the following are capable of exhibiting hydrogen bonding? N 2 HIHF(CH 3 ) 2 OCH 3 OHNH 3 CH 4 C 6 H 5 OHH 2 S Within the Lewis structure of the molecule, H must be attached to O, N, or F for hydrogen bonded to occur.

38 -68 o C 38 H 2 O H 2 SH 2 Se H 2 Te M m 18.02 34.08 80.98 129.63g/mol BP -60.33 o C -41.3 o C -2 o C 100 o C Let’s look at H 2 O, H 2 S, H 2 Se, and H 2 Te as pure substances. If you draw the Lewis structures and examine the VSEPR geometry of these molecules, you would determine that all of these molecules are polar with a same bent geometry. This means that all of the molecules have London dispersion and dipole-dipole interactions. Since they are all polar molecules, their London dispersion forces will dictate their boiling points which will vary based on their molar mass (larger molar mass, stronger London forces). Based on molar mass, we would predict H 2 Te to have the highest boiling point because it has the largest molar mass. If we extrapolate the boiling point of H 2 O based on the other actual boiling points, the boiling point of H 2 O should be -68 o C. However, since H 2 O has very strong hydrogen bonding to overcome as well, it’s boiling point is actually extremely high, 100 o C, as compared to the other substances despite it’s low molar mass. due to hydrogen bonding

39 39 For which of the following pairs of molecules do we expect London dispersion forces, dipole-dipole, dipole-induced, and hydrogen bonding? First, we must realize through Lewis structures and VSEPR that CO 2, CH 4 are nonpolar while H 2 O, HCl, NH 3 are polar. CH 4 and CH 4 H 2 O and H 2 O H 2 O and CO 2 NH 3 and NH 3 HCl and HCl London dipole-dipole dipole-induced hydrogen bonding London dipole-dipole all have polar-polarpolar-nonpolar hydrogen bonding H–O, N, F dipole-dipole

40 40 Which species has the higher boiling point CS 2 or CCl 4 ? If you draw the Lewis structures and examine the VSEPR geometry of these molecules, you would determine that both of these molecules are nonpolar with CS 2 having a linear geometry and CCl 4 having a tetrahedral geometry. Since both are nonpolar molecules, they only have London dispersion forces of attraction which means the molecule with the larger molar mass (CCl 4 ) will have more polarization and a higher boiling point.

41 41 Which species has the higher boiling point H 2 O or CO? If you draw the Lewis structures and examine the VSEPR geometry of these molecules, you would determine that H 2 O is a polar molecule with a bent geometry and CO is a polar molecule with a linear geometry. Since both are polar molecules, they have London dispersion and dipole-dipole interactions. Usually in this instance, the species with the larger molar mass would have the stronger London forces and higher boiling point; however, H 2 O also has hydrogen bonding causing the boiling point to be much higher despite the lower molar mass.

42 42 Intermolecular Forces In summary, intermolecular forces play a large role in many of the physical properties of liquids and gases. These include: –vapor pressure as intermolecular forces increase, vapor pressure decreases –boiling point as intermolecular forces increase, boiling point increases –surface tension as intermolecular forces increase, surface tension increases –viscosity as intermolecular forces increase, viscosity decreases

43 43 Crystalline Solids The regular arrangement of particles in a crystalline solid leads to the minimization of total potential energy of interactions of the particles and the most stable arrangement. A crystalline structure is said to have a long-range order. The overall structure can be thought of in terms of a repeating pattern, called a unit cell. The unit cells making up the solid are in close contact and in fixed positions. Solids are characterized by the type of force holding the structural units together. In some cases, these forces are intermolecular, but in others they are chemical bonds (metallic, ionic, or covalent).

44 44 Crystalline Solid Properties of crystals depend on the type of particles in the lattice. Crystals can be classified as ionic, molecular, or atomic. –Ionic crystals tend to have very high melting points due to strong attractions among ions. They are brittle due to the strong repulsions that result when ions of like charges are momentarily brought closer together as ions are slightly displaced from their locations when the crystal is, say, hit by a hammer. –Molecular crystals tend to have low melting or sublimation points. The attractive forces among the molecules are relatively weak (mainly van der Waals forces).

45 45 Crystalline Solid Atomic crystals can be classified as nonbonding, metallic, or covalent network. –Nonbonding atomic crystals are formed when noble gases are frozen to very low temperatures. These atoms are held together by very weak London dispersion forces. –Metallic crystals are made up of atoms of metallic elements. If more than one element is present, the solid is a solution and is called an alloy. A strong metallic bond is the reason metals have high melting points and boiling points; most metals are solids at room temperature. Because metal atoms can readily slip and roll over each other without breaking the metallic bond, metals are malleable and ductile. –Covalent network crystal can be thought of as one giant molecule; the atoms are held together by very strong covalent bonds. Thus, a network covalent crystal like diamond has a very high melting point and is among the hardest material known.

46 46 Physical Properties Many physical properties of a solid can be attributed to its structure and forces of attraction called crystal lattice energy or ion-ion intermolecular forces. –For a solid to melt, the forces holding the structural units together must be overcome. –For a molecular solid, these are weak intermolecular attractions. –Thus, molecular solids tend to have low melting points (below 300 o C).

47 47 Physical Properties –For ionic solids and covalent network solids to melt, chemical bonds must be broken. –For that reason, their melting points are relatively high. –Note that for ionic solids, melting points increase with the strength of the ionic bond while solubility decreases. –Ionic bonds are stronger when: 1.The magnitude of charge is high. Higher the charge, the stronger the attraction, the more energy needed to overcome attraction; therefore, MP increases and solubility decreases. 2.The ions are small (higher charge density). Smaller the radius, the closer the opposite charges and larger attraction, the more energy needed to overcome attraction; therefore, MP increases and solubility decreases.

48 48 Summary: The attractive forces (crystal lattice energy) between a pair of oppositely charged ions increases (stronger bond) as the charges on the ions increases and as ionic size decreases; hence higher MP and lower solubility. Which of the following has the higher melting point and lower solubility? MgO vs. NaCl CaBr 2 vs. CaCl 2 HW 69 Since magnesium oxide involves higher charges (+2, -2) than sodium chloride (+1, -1), MgO will have the higher MP and lower solubility. Since both species have the same charges (+2, -1), the size of the ions (anion in this case) will affect the properties. Calcium chloride has the smaller anion; therefore, it will have the stronger attraction to calcium and have the higher MP and lower solubility. code: liquids


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