13 Properties of Liquids Liquid water provides the basis for our bodies as well as recreational sports like windsurfing. Foundations of College Chemistry, 14th Ed. Morris Hein and Susan Arena Copyright © 2014 John Wiley & Sons, Inc. All rights reserved. Chapter Outline 13.1 States of Matter: A Review 13.2 Properties of Liquids A. Evaporation B. Vapor Pressure C. Surface Tension 13.3 Boiling Point and Melting Point 13.4 Changes of State 13.5 Intermolecular Forces 13.6 Hydrates 13.7 Water, a Unique Liquid © 2014 John Wiley & Sons, Inc. All rights reserved. States of Matter: A Review Gases: contain particles that are far apart, in random motion, and independent of one another. Little contact No attractive forces Random motion Solids: contain particles very close in space and maintain a rigid shape. Significant attractive forces exist between particles. Close contact Strong attractive forces Rigid shape © 2014 John Wiley & Sons, Inc. All rights reserved. States of Matter: A Review Liquids: intermediate between gases and solids. Contain particles close to one another but have fluidity (can assume the shape of a container). Significant attractive forces exist between particles in a liquid. Close contact Some attractive forces Fluid shape © 2014 John Wiley & Sons, Inc. All rights reserved. Evaporation Evaporation or Vaporization: Escape of molecules from the liquid to the gas phase. Liquid Vapor Molecules in the liquid state have different kinetic energies (KEs). Those with higher KEs can overcome attractive forces between particles and escape to the gas phase. © 2014 John Wiley & Sons, Inc. All rights reserved. Sublimation Phase change from the solid to gas phase that bypasses the liquid state. Solid Vapor Examples CO2 (s) I2 (s) CO2 (g) I2 (g) © 2014 John Wiley & Sons, Inc. All rights reserved. Vapor Pressure Molecules from the liquid phase can escape to the vapor phase through evaporation. Molecules in the gas phase can strike the surface of the liquid and return to the liquid phase. This process is called condensation. In a closed container, an equilibrium develops between molecules evaporating and condensing. liquid evaporation condensation vapor © 2014 John Wiley & Sons, Inc. All rights reserved. Vapor Pressure Vapor pressure: pressure exerted by a vapor in equilibrium with its liquid phase. © 2014 John Wiley & Sons, Inc. All rights reserved. Vapor Pressure Vapor pressure: pressure exerted by a vapor in equilibrium with its liquid phase. Independent of the quantity of liquid or its surface area. Increases with increasing temperature. Depends on the strength of attraction between molecules in the liquid state. Volatile liquids: very weak attractive forces between molecules. Evaporate very rapidly at ambient temperature. Have high vapor pressures as a result. © 2014 John Wiley & Sons, Inc. All rights reserved. Vapor Pressure Measuring Vapor Pressure of a Liquid Measure using a barometer. Vapor from the liquid exerts a force on the Hg and pushes the column downward. The difference in height relative to vacuum provides the vapor pressure for the liquid. © 2014 John Wiley & Sons, Inc. All rights reserved. Surface Tension Resistance of a liquid to an increase in surface area. Molecules on a liquid surface are strongly attracted by molecules within the liquid. Surface tension increases with increasing attractive interactions between molecules. Mercury droplets form spheres due to surface tension. © 2014 John Wiley & Sons, Inc. All rights reserved. Capillary Action Spontaneous rise of a liquid in a narrow tube. Cohesive forces exist between water molecules in a liquid. Adhesive forces exist between water molecules and the walls of the container. When the cohesive forces between molecules are less than the adhesive forces between liquid and container, the liquid will move up the walls of the container. © 2014 John Wiley & Sons, Inc. All rights reserved. Capillary Action Capillary Action in Action Shape of the meniscus reflects the relative strength of cohesive forces within the liquid and adhesive forces between the liquid and the tube. If convex: adhesive forces < cohesive forces If concave: adhesive forces > cohesive forces Hg H2 O © 2014 John Wiley & Sons, Inc. All rights reserved. Boiling Point Temperature at which the vapor pressure of a liquid is equal to the external pressure above the liquid. Where is the boiling point of a liquid higher, at or above sea level? At sea level. The atmospheric pressure is higher. © 2014 John Wiley & Sons, Inc. All rights reserved. Boiling Point Normal boiling point: temperature when the vapor pressure is 1 atm Vapor Pressure Curve Normal boiling points: Water: 100 ºC Ether: 35 ºC Ethyl Alcohol: 78 ºC © 2014 John Wiley & Sons, Inc. All rights reserved. Boiling Point Practice The vapor pressure curve for water is given below. What is the boiling point of water at 300 mmHg? a. 100 ºC b. 86 ºC c. 76 ºC d. 30 ºC © 2014 John Wiley & Sons, Inc. All rights reserved. Freezing Point or Melting Point Freezing/melting point: the temperature at which the solid phase of a substance is in equilibrium with its liquid phase. solid melting freezing liquid While both phases are present, the temperature remains constant. The energy is used to change the solid to the liquid phase. © 2014 John Wiley & Sons, Inc. All rights reserved. Changes of State Heat of fusion: energy required to change 1 g of a solid at its melting point to a liquid. Heat of vaporization Boiling Melting Heat of fusion Heat of vaporization: energy required to change 1 g of a liquid to vapor at its normal boiling point. © 2014 John Wiley & Sons, Inc. All rights reserved. Energy and Phase Changes Heat of fusion: energy required to change 1 g of a solid at its melting point to a liquid. The heat of fusion for water is 335 J/g. Calculate the amount of heat needed to melt 25.0 g of water. Use the heat of fusion as a conversion factor! 25.0 g × 335 J 1g = 8380 J © 2014 John Wiley & Sons, Inc. All rights reserved. Energy and Phase Changes Heat of vaporization: energy required to change 1 g of a liquid to vapor at its normal boiling point. The heat of vaporization for water is 2259 J/g. Calculate the amount of heat needed to vaporize 25.0 g of water at 100 ºC. Use the heat of vaporization as a conversion factor! 25.0 g × 2259 J 1g = 56,500 J © 2014 John Wiley & Sons, Inc. All rights reserved. Phase Change Practice Calculate the energy needed to convert 25.0 g of ice at 0 ºC to steam at 100 ºC? Given: heat of fusion = 335 J/g heat of vaporization = 2259 J/g specific heat of liquid water = 4.184 J/gºC Plan The conversion of ice to steam is a three step process: 1. ice melts (total energy = mass x heat of fusion) 2. liquid water is warmed from 0° to 100°C (energy = mass x specific heat x ΔT) 3. water evaporates (energy = mass x heat of vaporization) The overall energy required for the process is the sum of the 3 steps. © 2014 John Wiley & Sons, Inc. All rights reserved. Phase Change Practice Calculate the energy needed to convert 25.0 g of ice at 0 ºC to steam at 100 ºC? Calculate 1. ice melts 2. warm water 25.0 g × 335 J 1g = 8375 J 25.0 g × 4.184 J 1 g ºC × 100 ºC 3. evaporate water 25.0 g × Total energy required: 2259 J 1g = 10,460 J = 56,475 J E = Step 1 + Step 2 + Step 3 = 8375 J + 10,460 J + 56475 J = 75,300 J © 2014 John Wiley & Sons, Inc. All rights reserved. Phase Change Practice How many joules of energy are needed to change 10.0 g of ice at 0.00 ºC to water at 20.0 ºC? Given: heat of fusion = 335 J/g specific heat of liquid water = 4.184 J/gºC a. 4.19 x 103 J b. 478 J c. 3.35 x 103 J d. 2.51 x 103 J Plan The conversion of ice to liquid water is a two step process. 1. ice melts (total energy = mass x heat of fusion) 2. liquid water is warmed from 0° to 20 °C (energy = mass x specific heat x ΔT) © 2014 John Wiley & Sons, Inc. All rights reserved. Phase Change Practice How many joules of energy are needed to change 10.0 g of ice at 0.00 ºC to water at 20.0 ºC? Calculate 1. ice melts 2. warm water 10.0 g 335 J × 10.0 g 1g × 4.184 J 1 g ºC = 3350 J × 20 ºC = 837 J Total energy required: Energy = Step 1 + Step 2 = 3350 J + 837 J = 4.19 x 103 J © 2014 John Wiley & Sons, Inc. All rights reserved. Intermolecular Forces Attractive forces between molecules. These forces allow for formation of liquids and solids. The degree of intermolecular forces correlates with a compound’s physical properties. Example: The stronger the interaction between molecules in a liquid, the higher the boiling point and the lower the vapor pressure. © 2014 John Wiley & Sons, Inc. All rights reserved. Types of Intermolecular Forces Dipole-Dipole Attractions In covalent molecules, due to different atoms having different electronegativities, molecules are polar. When polar molecules are put together, they will align to permit interaction between oppositely polarized portions of the molecules. The interaction of two polar H2O molecules. These interactions between dipoles in different molecules are called dipole-dipole forces. © 2014 John Wiley & Sons, Inc. All rights reserved. The Hydrogen Bond Water has very high melting and boiling points, and heats of fusion and vaporization. These anomalous properties are due to strong attraction between water molecules due to hydrogen bonding, a special type of dipole-dipole attraction. © 2014 John Wiley & Sons, Inc. All rights reserved. The Hydrogen Bond Hydrogen bonds: one type of strong intermolecular force/attraction between molecules. Hydrogen bonds are much weaker than ionic or covalent bonds which are intramolecular forces. Hydrogen Bonding between H2O molecules. © 2014 John Wiley & Sons, Inc. All rights reserved. The Hydrogen Bond To form hydrogen bonds, a compound must have covalent bonds between hydrogen and F, O or N (a very electronegative element). Can hydrogen bond. Cannot hydrogen bond. (No H attached to oxygen). © 2014 John Wiley & Sons, Inc. All rights reserved. The Hydrogen Bond Practice Which of the following molecules would be expected to participate in hydrogen bonding? © 2014 John Wiley & Sons, Inc. All rights reserved. London Dispersion Forces Molecules without dipoles can also interact with one another. These interactions between nonpolar molecules and noble gases are called London dispersion forces. London forces arise from uneven, instantaneous charge distributions due to electron movement in nonpolar molecules. © 2014 John Wiley & Sons, Inc. All rights reserved. London Dispersion Forces This instantaneous dipole can then induce a dipole in a neighboring nonpolar molecule, resulting in a small attraction between particles. London forces are very weak forces. Generally become more important as the size of the molecule increases. Larger sizes provide more possible electrons to provide dipoles. © 2014 John Wiley & Sons, Inc. All rights reserved. London Dispersion Forces Which of the following molecules would have the largest London dispersion forces? a. CH4 b. C4H10 c. C15H32 d. C8H18 The largest hydrocarbon (i.e., having the largest molar mass) will have the strongest London forces. © 2014 John Wiley & Sons, Inc. All rights reserved. Hydrates Hydrates are solids that contain water molecules as part of their crystalline structure. The formula lists the anhydrous (without water) formula of the compound. The number of waters present per structural unit (water of hydration) are then given. CaCl2∙2H2O Hydrates are named by placing a prefix corresponding to the number of water molecules, followed by hydrate CaCl2∙2H2O FeCl3∙6H2O calcium chloride dihydrate iron(III) chloride hexahydrate © 2014 John Wiley & Sons, Inc. All rights reserved. Hydrates Hydrates will often decompose by losing water upon heating. CuSO4∙5 H2O (s) 250°C CuSO4 (s) + 5 H2O (g) © 2014 John Wiley & Sons, Inc. All rights reserved. Hydrates Practice Calculate the percent water in Epsom salts MgSO4∙7H2O (s). 1. Calculate the molar mass of the compound. Molar Mass MgSO4∙7H2O (s) = 120.4 + 7(18.02) = 246.5 g 2. Calculate the % water of the compound. Mass water x 100 = % water = Molar mass 126.1 g 246.5 g © 2014 John Wiley & Sons, Inc. All rights reserved. x 100 = 51.16 % Hydrates Practice What is the percent water in CuSO4∙5H2O (s)? a. 56.46% 1. Calculate the molar mass of the compound. b. 36.08% c. 63.92% Molar Mass CuSO4∙5H2O (s) = 159.6 + 5(18.02) = 249.2 g d. 61.57% 2. Calculate the % water of the compound. Mass water x 100 = % water = Molar mass 90.10 g 259.2 g © 2014 John Wiley & Sons, Inc. All rights reserved. x 100 = 36.08 % Water: A Unique Liquid Water covers 75% of the Earth’s surface; 97% of all water resides in the oceans. Water constitutes 70% of a human body by mass. Physical Properties of Water Colorless, odorless, tasteless liquid. More dense in liquid than solid phase (why ice floats). High boiling point, high heat of fusion/vaporization due to hydrogen bonding. © 2014 John Wiley & Sons, Inc. All rights reserved. Water: A Unique Liquid Structure of Water Molecules Two OH bonds are formed by the overlap of 1s orbitals on H with orbitals on the O. The molecular geometry of water is bent, due to the two lone pairs on oxygen. Water has a permanent dipole due to the molecules’ shape and the polar O-H bonds. © 2014 John Wiley & Sons, Inc. All rights reserved. Water: A Unique Liquid Sources of Water for Human Consumption Climate change and increased demand for fresh water make finding and sustaining sources of potable water critical for future generations. Strategies to Sustain Water Supplies 1. Reclamation of wastewater Currently used in agriculture and industry 2. Desalination of seawater Expensive, but useful for countries near the ocean. 3. Low temperature distillation At low pressure, water’s boiling point is reduced. Less energy is required to separate the salts by boiling. 4. Combustion of H2 H2 and O2 react very exothermically to produce water. © 2014 John Wiley & Sons, Inc. All rights reserved. Chemistry in Action: Osmosis Osmosis: process by which water flows through a membrane from a region of more pure water to a region of less pure water. Water flows into the raisin to dilute the sugar. The size of the raisin expands. © 2014 John Wiley & Sons, Inc. All rights reserved. Chemistry in Action: Reverse Osmosis Reverse Osmosis: process by which water flows through a membrane from a region of less pure water to a region of more pure water, due to the presence of an external stimulus (typically pressure) Process often used in water purification. A semipermeable membrane is used and only water can pass through. By applying pressure, only water passes through the membrane. The water is now pure! © 2014 John Wiley & Sons, Inc. All rights reserved. Learning Objectives 13.1 States of Matter: A Review Review the states of matter and their properties. 13.2 Properties of Liquids Explain why liquids tend to form drops and the process of evaporation and its relationship to vapor pressure. 13.3 Boiling Point and Melting Point Define boiling and melting points and determine the boiling point of a liquid from a graph of temperature and vapor pressure. © 2014 John Wiley & Sons, Inc. All rights reserved. Learning Objectives 13.4 Changes of State Calculate the amount of energy involved in a change of state. 13.5 Intermolecular Forces Describe the three types of intermolecular forces and explain their significance in liquids. 13.6 Hydrates Explain what hydrates are, write formulas for hydrates and calculate the percent water in a hydrate. 13.7 Water, A Unique Liquid Describe the characteristics of water in terms of its structure and list the sources of drinking water. © 2014 John Wiley & Sons, Inc. All rights reserved.