SlideShare ist ein Scribd-Unternehmen logo
1 von 86
Chapter 7

Gases, Liquids,
  and Solids
Chapter 7
      Table of Contents
      7.1The Kinetic Molecular Theory of Matter
      7.2Kinetic Molecular Theory and Physical States
      7.3Gas Law Variables
      7.4Boyle’s Law: A Pressure-Volume Relationship
      7.5 Charles’s Law: A Temperature-Volume Relationship
      7.6The Combined Gas Law
      7.7The Ideal Gas Law
      7.8Dalton’s Law of Partial Pressures
      7.9Changes of State
      7.10Evaporation of Liquids
      7.11Vapor Pressure of Liquids
      7.12Boiling and Boiling Point
      7.13Intermolecular Forces in Liquids
Copyright © Cengage Learning. All rights reserved            2
Section 7.1
      The Kinetic Molecular Theory of Matter

      Common Physical Properties of Matter
       •     Volume and Shape
       •     Density
       •     Compressibility
       •     Thermal Expansion




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved           3
Section 7.1
      The Kinetic Molecular Theory of Matter

      Compressibility
       • A measure of the change in volume of a
         sample of matter resulting from a pressure
         change.




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved             4
Section 7.1
      The Kinetic Molecular Theory of Matter

      Thermal Expansion
       • A measure of the change in volume of a
         sample of matter resulting from a
         temperature change.




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved           5
Section 7.1
      The Kinetic Molecular Theory of Matter
      Distinguishing Properties of Solids, Liquids, and
      Gases




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                 6
Section 7.1
      The Kinetic Molecular Theory of Matter

      Kinetic Molecular Theory of Matter
       1. Matter is composed of tiny particles
          (atoms, molecules, or ions) that have
          definite and characteristic sizes that do
          not change.




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved             7
Section 7.1
      The Kinetic Molecular Theory of Matter

      Kinetic Molecular Theory of Matter
       1. The particles are in constant random
          motion and therefore possess kinetic
          energy.
            Kinetic energy – energy that matter
             possesses because of particle motion.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved            8
Section 7.1
      The Kinetic Molecular Theory of Matter

      Kinetic Molecular Theory of Matter
       1. The particles interact with one another
          through attractions and repulsions and
          therefore possess potential energy.
            Potential energy – stored energy that
             matter possesses as a result of its
             position, condition, and/or composition.




                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved               9
Section 7.1
      The Kinetic Molecular Theory of Matter

      Kinetic Molecular Theory of Matter

       1. The kinetic energy (velocity) of the
          particles increases as the temperature is
          increased.




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            10
Section 7.1
      The Kinetic Molecular Theory of Matter

      Kinetic Molecular Theory of Matter

       1. The particles in a system transfer energy
          to each other through elastic collisions.




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            11
Section 7.1
      The Kinetic Molecular Theory of Matter

      Differences Among Solids, Liquids, and Gases
       • Explained by the relative magnitudes of
         kinetic energy and potential energy
         (electrostatic attractions).
       • Kinetic energy is a disruptive force that
         tends to make the particles of a system
         increasingly independent of one another.
       • Potential energy is a cohesive force that
         tends to cause order and stability among
         the particles of a system.

                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           12
Section 7.2
      Kinetic Molecular Theory and Physical States

      Solid
       • The physical state characterized by a
         dominance of potential energy (cohesive
         forces) over kinetic energy (disruptive
         forces).
       • Particles in a solid are drawn close
         together in a regular pattern by the strong
         cohesive forces present.
       • Each particle occupies a fixed position,
         about which it vibrates because of
         disruptive kinetic energy.
                                                       Return to TOC


Copyright © Cengage Learning. All rights reserved             13
Section 7.2
      Kinetic Molecular Theory and Physical States

      Solid




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           14
Section 7.2
      Kinetic Molecular Theory and Physical States

      Definite Volume and Definite Shape
       • The strong, cohesive forces hold the
         particles in essentially fixed positions,
         resulting in definite volume and definite
         shape.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           15
Section 7.2
      Kinetic Molecular Theory and Physical States

      High Density
       • The constituent particles of solids are
         located as close together as possible
         (touching each other). Therefore, a given
         volume contains large numbers of
         particles, resulting in a high density.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           16
Section 7.2
      Kinetic Molecular Theory and Physical States

      Small Compressibility
       • Because there is very little space between
         particles, increased pressure cannot push
         the particles any closer together;
         therefore, it has little effect on the solid’s
         volume.




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                17
Section 7.2
      Kinetic Molecular Theory and Physical States

      Very Small Thermal Expansion
       • An increased temperature increases the
         kinetic energy (disruptive forces), thereby
         causing more vibrational motion of the
         particles. Each particle occupies a slightly
         larger volume, and the result is a slight
         expansion of the solid. The strong,
         cohesive forces prevent this effect from
         becoming very large.



                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              18
Section 7.2
      Kinetic Molecular Theory and Physical States

      Liquid
       • The physical state characterized by
         potential energy (cohesive forces) and
         kinetic energy (disruptive forces) of about
         the same magnitude.
       • Particles that are randomly packed but
         relatively near one another.
       • The molecules are in constant, random
         motion; they slide freely over one another
         but do not move with enough energy to
         separate.
                                                       Return to TOC


Copyright © Cengage Learning. All rights reserved             19
Section 7.2
      Kinetic Molecular Theory and Physical States

      Liquid




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           20
Section 7.2
      Kinetic Molecular Theory and Physical States

      Definite Volume and Indefinite Shape
       • The attractive forces are strong enough to
         restrict particles to movement within a
         definite volume. They are not strong
         enough to prevent the particles from
         moving over each other in a random
         manner that is limited only by the
         container walls.




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            21
Section 7.2
      Kinetic Molecular Theory and Physical States

      High Density
       • The particles in a liquid are not widely
         separated; they are still touching one
         another. Therefore, there will be a large
         number of particles in a given volume – a
         high density.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           22
Section 7.2
      Kinetic Molecular Theory and Physical States

      Small Compressibility
       • Because the particles in a liquid are still
         touching each other, there is very little
         empty space. Therefore, an increase in
         pressure cannot squeeze the particles
         much closer together.




                                                       Return to TOC


Copyright © Cengage Learning. All rights reserved             23
Section 7.2
      Kinetic Molecular Theory and Physical States

      Small Thermal Expansion
       • Most of the particle movement in a liquid
         is vibrational because a particle can move
         only a short distance before colliding with
         a neighbor. The increased particle velocity
         that accompanies a temperature increase
         results only in increased vibrational
         amplitudes. The net effect is an increase
         in the effective volume a particle occupies,
         which causes a slight volume increase in
         the liquid.
                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              24
Section 7.2
      Kinetic Molecular Theory and Physical States

      Gas
       • The physical state characterized by a
         complete dominance of kinetic energy
         (disruptive forces) over potential energy
         (cohesive forces).
       • Attractive forces among particles are very
         weak and are considered to be zero.
       • The particles move essentially
         independently of one another in a totally
         random manner.

                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            25
Section 7.2
      Kinetic Molecular Theory and Physical States

      Gas




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           26
Section 7.2
      Kinetic Molecular Theory and Physical States

      Indefinite Volume and Indefinite Shape
       • The attractive (cohesive) forces between
         particles have been overcome by high
         kinetic energy, and the particles are free
         to travel in all directions.
       • Particles completely fill their container and
         the shape of the gas is that of the
         container.




                                                         Return to TOC


Copyright © Cengage Learning. All rights reserved               27
Section 7.2
      Kinetic Molecular Theory and Physical States

      Low Density
       • The particles are widely separated. There
         are relatively few particles in a given
         volume, which means little mass per
         volume.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           28
Section 7.2
      Kinetic Molecular Theory and Physical States

      Large Compressibility
       • A gas is mostly empty space. When
         pressure is applied, the particles are
         easily pushed closer together, decreasing
         the amount of empty space and the
         volume of the gas.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           29
Section 7.2
      Kinetic Molecular Theory and Physical States

      Moderate Thermal Expansion
       • An increase in temperature means an
         increase in particle velocity. The increased
         KE enables the particles to push back
         whatever barrier is confining them, and
         the volume increases. It is the space
         between the particles that changes.




                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              30
Section 7.3
      Gas Law Variables

      Gas Law
       • A generalization that describes in
         mathematical terms the relationships
         among the amount, pressure,
         temperature, and volume of a gas.




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          31
Section 7.3
      Gas Law Variables

      Pressure

                                                     force
                                         Pr essure =
                                                     area


              • 1 atm = 760 mm Hg = 760 torr
              • 1 atm = 14.7 psi




                                                             Return to TOC


Copyright © Cengage Learning. All rights reserved                   32
Section 7.3
      Gas Law Variables

      Pressure of a Gas
       • The force that creates pressure is that
         which is exerted by the gas molecules or
         atoms as they constantly collide with the
         walls of their container.




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           33
Section 7.3
      Gas Law Variables

      Barometer
       • A device used to measure atmospheric
         pressure.




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          34
Section 7.3
      Gas Law Variables



      Barometer




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          35
Section 7.4
      Boyle’s Law: A Pressure-Volume Relationship

      Boyle’s Law
       • Pressure and volume are inversely related
         (constant T, temperature, and n, # of
         moles).

                                                    P1 × V1 = P2 × V2




                                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved                              36
Section 7.4
      Boyle’s Law: A Pressure-Volume Relationship

      Boyle’s Law




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          37
Section 7.4
      Boyle’s Law: A Pressure-Volume Relationship

                        Exercise


           A sample of helium gas occupies 12.4 L at
           23°C and 0.956 atm. What volume will it
           occupy at 1.20 atm assuming that the
           temperature stays constant?

                                                    P1 × V1 = P2 × V2
                            (0.956 atm)(12.4 L) = (1.20 atm)(V2 )
                                                        V2 = 9.88 L

                                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved                              38
Section 7.5
      Charles’s Law: A Temperature-Volume Relationship

      Charles’s Law
              • Volume and temperature (in Kelvin) are
                directly related (constant P and n).
              • K = °C + 273


                                                    V1 V2
                                                      =
                                                    T1 T2




                                                            Return to TOC


Copyright © Cengage Learning. All rights reserved                  39
Section 7.5
      Charles’s Law: A Temperature-Volume Relationship

      Charles’s Law




                                                         Return to TOC


Copyright © Cengage Learning. All rights reserved               40
Section 7.5
      Charles’s Law: A Temperature-Volume Relationship

                        Exercise

           Suppose a balloon containing 1.30 L of air at
           24.7°C is placed into a beaker containing liquid
           nitrogen at –78.5°C. What will the volume of
           the sample of air become (at constant
           pressure)?
                                 V1 V2
                                    =
                                 T1 T2
                                                  1.30 L           V2
                                                            =
                                              ( 24.7 + 273 ) ( −78.5 + 273 )
                                                        V2 = 0.849 L
                                                                               Return to TOC


Copyright © Cengage Learning. All rights reserved                                     41
Section 7.6
      The Combined Gas Law


              • The product of the pressure and volume of a
                fixed amount of gas is directly proportional
                to its Kelvin temperature.


                                                    P1V1 P2 V2
                                                        =
                                                     T1   T2




                                                                 Return to TOC


Copyright © Cengage Learning. All rights reserved                       42
Section 7.6
      The Combined Gas Law

                        Exercise

                   At what temperature (in °C) does 121 mL of
                   CO2 at 27°C and 1.05 atm occupy a volume
                   of 293 mL at a pressure of 1.40 atm?
                                  P1V1 P2 V2
                                      =
                                   T1     T2
                         ( 1.05 atm ) ( 121 mL )      =
                                                          ( 1.40 atm ) ( 293 mL )
                               ( 27+273 )                       ( T2 + 273 )
                                                    T2 = 969 K − 273
                                                    T2 = 696°C
                                                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved                                          43
Section 7.7
      The Ideal Gas Law



      • We can bring all of these laws together
        into one comprehensive law:


                                PV = nRT
                                (where R = 0.0821 L·atm/mol·K`




                                                                 Return to TOC


Copyright © Cengage Learning. All rights reserved                       44
Section 7.7
      The Ideal Gas Law

                        Exercise


                   An automobile tire at 23°C with an internal
                   volume of 25.0 L is filled with air to a total
                   pressure of 2.18 atm (32 pounds per square
                   inch). Determine the number of moles of air
                   in the tire.

                             PV = nRT
              (2.18 atm)(25.0 L) = n(0.0821 L ⋅ atm/mol ⋅ K)(23+273 K)
                               n = 2.24 mol
                                                                         Return to TOC


Copyright © Cengage Learning. All rights reserved                               45
Section 7.7
      The Ideal Gas Law

                        Exercise


                   What is the pressure in a 304.0 L tank that
                   contains 5.670 kg of helium at 25°C?


                         PV = nRT
                    5.670 × 1000 
    (P)(304.0 L) =                (0.0821 L ⋅ atm/mol ⋅ K)(25+273)
                       4.003     
               n = 114 atm


                                                                  Return to TOC


Copyright © Cengage Learning. All rights reserved                        46
Section 7.8
      Dalton’s Law of Partial Pressures


       • For a mixture of gases in a container,
                       PTotal = P1 + P2 + P3 + . . .
       • The total pressure exerted by a mixture of
         gases is the sum of the partial pressures of
         the individual gases present.




                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              47
Section 7.8
      Dalton’s Law of Partial Pressures




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          48
Section 7.8
      Dalton’s Law of Partial Pressures

                        Exercise


           Consider the following container of helium at 45°C.
           Initially the valve is closed.
            – After the valve is opened, what is the pressure of
                the helium gas?


                                       2.00 atm
                                                         3.00 atm
                                        9.00 L
                                                          3.00 L


                                              2.25 atm
                                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved                          49
Section 7.9
      Changes of State



       • A process in which a substance is
         transformed from one physical state to
         another physical state.
       • Usually accomplished by heating or cooling
         a substance, but pressure can also be a
         factor.
       • Changes of state are examples of physical
         changes.


                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            50
Section 7.9
      Changes of State

      Six Possible Changes of State
       •     Freezing
       •     Melting
       •     Evaporation
       •     Condensation
       •     Sublimation
       •     Deposition




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          51
Section 7.9
      Changes of State

      Six Possible Changes of State




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          52
Section 7.9
      Changes of State

      Two Categories

       1. Endothermic change of state – change of
          state in which heat energy is absorbed.
           – Melting
           – Sublimation
           – Evaporation




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          53
Section 7.9
      Changes of State

      Two Categories

       1. Exothermic change of state – change of
          state in which heat energy is given off.
           – Freezing
           – Condensation
           – Deposition




                                                     Return to TOC


Copyright © Cengage Learning. All rights reserved           54
Section 7.10
      Evaporation of Liquids



       • Process by which molecules escape from
         the liquid phase to the gas phase.
       • For a liquid to evaporate, its molecules must
         gain enough kinetic energy to overcome the
         attractive forces among them.




                                                         Return to TOC


Copyright © Cengage Learning. All rights reserved               55
Section 7.10
      Evaporation of Liquids

      Rate of Evaporation
       • Increased surface area results in an
         increased evaporation rate because a
         greater fraction of the total molecules are on
         the surface (so they are not completely
         surrounded by other molecules with
         attractive forces).




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                56
Section 7.10
      Evaporation of Liquids

      Rate of Evaporation
       • Always increases as liquid temperature
         increases.
       • A cooling effect is produced in the liquid
         when evaporation occurs.
       • Vapor – A gas that exists at a temperature
         and pressure at which it ordinarily would be
         thought of as a liquid or solid.



                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              57
Section 7.11
      Vapor Pressure of Liquids

      Evaporation of a Liquid in a Closed Container




      g) The liquid level drops for a time.
      h) Then becomes constant (ceases to drop).
      i) Rate of evaporation equals the rate of condensation.
                                                                Return to TOC


Copyright © Cengage Learning. All rights reserved                      58
Section 7.11
      Vapor Pressure of Liquids

      Equilibrium
      • A condition in which two opposite processes
        take place at the same rate.
      • No net macroscopic changes can be detected,
        but the system is dynamic.
      • Forward and reverse processes are occurring at
        equal rates.




                                                         Return to TOC


Copyright © Cengage Learning. All rights reserved               59
Section 7.11
      Vapor Pressure of Liquids

      Vapor Pressure
      • Pressure exerted by a vapor above a liquid
        when the liquid and vapor are in equilibrium with
        each other.
      • Magnitude of vapor pressure depends on the
        nature and temperature of the liquid.




                                                            Return to TOC


Copyright © Cengage Learning. All rights reserved                  60
Section 7.11
      Vapor Pressure of Liquids

      Vapor Pressure
      • Liquids that have strong attractive forces
        between molecules have lower vapor pressures
        than liquids that have weak attractive forces
        between particles.




                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              61
Section 7.11
      Vapor Pressure of Liquids

      Vapor Pressure
      • Substances that have high vapor pressures
        evaporate readily – they are volatile.
          Volatile substance – a substance that readily
           evaporates at room temperature because of a
           high vapor pressure.




                                                           Return to TOC


Copyright © Cengage Learning. All rights reserved                 62
Section 7.12
      Boiling and Boiling Point

      Boiling
      • A form of evaporation where conversion from the
        liquid state to the vapor state occurs within the
        body of the liquid through bubble formation.
      • Occurs when the vapor pressure of the liquid
        reaches a value equal to that of the prevailing
        external pressure on the liquid (for an open
        container it’s atmospheric pressure).



                                                            Return to TOC


Copyright © Cengage Learning. All rights reserved                  63
Section 7.12
      Boiling and Boiling Point

      Boiling




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          64
Section 7.12
      Boiling and Boiling Point

      Boiling Point
      • The temperature at which the vapor pressure of
        a liquid becomes equal to the external
        (atmospheric) pressure exerted on the liquid.
      • Normal boiling point – the temperature at which
        a liquid boils under a pressure of 760 mm Hg.
      • Boiling point changes with elevation.




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                65
Section 7.12
      Boiling and Boiling Point

      BP of Water at Various Locations That Differ in Elevation




                                                                  Return to TOC


Copyright © Cengage Learning. All rights reserved                        66
Section 7.12
      Boiling and Boiling Point

                        Concept Check


        What is the vapor pressure of water at 100°C?
        How do you know?

                                                    1 atm




                                                            Return to TOC


Copyright © Cengage Learning. All rights reserved                  67
Section 7.13
      Intermolecular Forces in Liquids

      Intramolecular Forces
      • Forces “Within” molecules.




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          68
Section 7.13
      Intermolecular Forces in Liquids

      Intermolecular Force
      • An attractive force that acts between a molecule
        and another molecule.
      • Intermolecular forces are weak compared to
        intramolecular forces.




                                                           Return to TOC


Copyright © Cengage Learning. All rights reserved                 69
Section 7.13
      Intermolecular Forces in Liquids

      Three Main Types of Intermolecular Forces
      • Dipole-dipole interactions
      • Hydrogen bonds
      • London forces




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          70
Section 7.13
      Intermolecular Forces in Liquids

      Dipole-Dipole Interactions
      • An IMF that occurs between polar molecules.
      • Molecules with dipole moments can attract each
        other electrostatically by lining up so that the
        positive and negative ends are close to each
        other.
      • The greater the polarity of the molecules, the
        greater the strength of the dipole-dipole
        interactions.


                                                           Return to TOC


Copyright © Cengage Learning. All rights reserved                 71
Section 7.13
      Intermolecular Forces in Liquids


      Dipole-Dipole Interactions
      Between ClF Molecules




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          72
Section 7.13
      Intermolecular Forces in Liquids

      Dipole-Dipole Interactions




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          73
Section 7.13
      Intermolecular Forces in Liquids

      Hydrogen Bonds
      • Unusually strong dipole-dipole interactions are
        observed among hydrogen-containing molecules
        in which hydrogen is covalently bonded to a
        highly electronegative element of small atomic
        size (fluorine, oxygen, and nitrogen).




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                74
Section 7.13
      Intermolecular Forces in Liquids

      Two Factors

      1. The highly electronegative element to which
         hydrogen is covalently bonded attracts the
         bonding electrons to such a degree that the
         hydrogen atom is left with a significant δ+charge.
      2. The small size of the “bare” hydrogen nucleus
         allows it to approach closely, and be strongly
         attracted to a lone pair of electrons on the
         electronegative atom of another molecule.


                                                              Return to TOC


Copyright © Cengage Learning. All rights reserved                    75
Section 7.13
      Intermolecular Forces in Liquids

      Hydrogen Bonding in Water




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          76
Section 7.13
      Intermolecular Forces in Liquids

      Hydrogen Bonding




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          77
Section 7.13
      Intermolecular Forces in Liquids



      • The vapor pressures of liquids that have
        significant hydrogen bonding are much lower
        than those of similar liquids wherein little or no
        hydrogen bonding occurs.




                                                             Return to TOC


Copyright © Cengage Learning. All rights reserved                   78
Section 7.13
      Intermolecular Forces in Liquids




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          79
Section 7.13
      Intermolecular Forces in Liquids

      London Forces




                                                    Return to TOC


Copyright © Cengage Learning. All rights reserved          80
Section 7.13
      Intermolecular Forces in Liquids

      London Forces
      • A weak temporary intermolecular force that
        occurs between an atom or molecule (polar or
        nonpolar) and another atom or molecule (polar
        or nonpolar).
      • Results from momentary uneven electron
        distributions in molecules.
      • Significant in large atoms/molecules.
      • Occurs in all molecules, including nonpolar
        ones.
                                                        Return to TOC


Copyright © Cengage Learning. All rights reserved              81
Section 7.13
      Intermolecular Forces in Liquids

      Boiling Point Trends for Related Series of Nonpolar Molecules




                                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved                            82
Section 7.13
      Intermolecular Forces in Liquids

                        Concept Check


        Which are stronger, intramolecular bonds or
        intermolecular forces?

  How do you know?




                                                      Return to TOC


Copyright © Cengage Learning. All rights reserved            83
Section 7.13
      Intermolecular Forces in Liquids

                        Concept Check


  Which has the stronger intermolecular forces?

                                                    N2   H2O


  Explain.




                                                               Return to TOC


Copyright © Cengage Learning. All rights reserved                     84
Section 7.13
      Intermolecular Forces in Liquids

                        Concept Check


        Draw two Lewis structures for the formula C2H6O
        and compare the boiling points of the two
        molecules.




                                                          Return to TOC


Copyright © Cengage Learning. All rights reserved                85
Section 7.13
      Intermolecular Forces in Liquids

                        Concept Check


        Which gas would behave more ideally at the
        same conditions of P and T?

                                                CO   or   N2


        Why?



                                                               Return to TOC


Copyright © Cengage Learning. All rights reserved                     86

Weitere ähnliche Inhalte

Was ist angesagt?

Chemical Bonding
Chemical BondingChemical Bonding
Chemical BondingDavid Genis
 
Intermolecular Forces
Intermolecular ForcesIntermolecular Forces
Intermolecular Forcesglenn adams
 
Molecular polarity
Molecular polarityMolecular polarity
Molecular polarityPeggyGeiger
 
Chem 2 - Analyzing Strengths of Intermolecular Forces III
Chem 2 - Analyzing Strengths of Intermolecular Forces IIIChem 2 - Analyzing Strengths of Intermolecular Forces III
Chem 2 - Analyzing Strengths of Intermolecular Forces IIILumen Learning
 
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole Attractions
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole AttractionsIntermolecular Forces: London Dispersion Forces and Dipole-Dipole Attractions
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole AttractionsShaina Mavreen Villaroza
 
INTERMOLECULAR FORCES
INTERMOLECULAR FORCESINTERMOLECULAR FORCES
INTERMOLECULAR FORCESEuniceGianna
 
Physical Science Week 2.1.pptx
Physical Science Week 2.1.pptxPhysical Science Week 2.1.pptx
Physical Science Week 2.1.pptxKipAizaFernandez
 
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEET
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEETSolid State & Solution_Unit 1-2_Class-12_Board-JEE-NEET
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEETSupratim Das
 
Covalent bonds
Covalent bondsCovalent bonds
Covalent bondsMrsKendall
 
Polar Bonds and Polar Molecules.pptx
Polar Bonds and Polar Molecules.pptxPolar Bonds and Polar Molecules.pptx
Polar Bonds and Polar Molecules.pptxLiezlValiente1
 
47 intermolecularforces
47 intermolecularforces47 intermolecularforces
47 intermolecularforcesclwatson12
 
Molecular geometry
Molecular geometryMolecular geometry
Molecular geometrychan_sicat14
 
Chapter4 120319075415-phpapp02
Chapter4 120319075415-phpapp02Chapter4 120319075415-phpapp02
Chapter4 120319075415-phpapp02Cleophas Rwemera
 
Chemical bonds- Properties of Ionic and Covalent compounds
Chemical bonds- Properties of Ionic and Covalent compoundsChemical bonds- Properties of Ionic and Covalent compounds
Chemical bonds- Properties of Ionic and Covalent compoundsSyed Amirul Aiman
 
Covalent Bonds
Covalent BondsCovalent Bonds
Covalent Bondsmreve
 
Chemical bonding cheat sheet
Chemical bonding cheat sheetChemical bonding cheat sheet
Chemical bonding cheat sheetTimothy Welsh
 

Was ist angesagt? (20)

Chemical Bonding
Chemical BondingChemical Bonding
Chemical Bonding
 
Intermolecular Forces
Intermolecular ForcesIntermolecular Forces
Intermolecular Forces
 
Molecular polarity
Molecular polarityMolecular polarity
Molecular polarity
 
Metallic bonding
Metallic bondingMetallic bonding
Metallic bonding
 
Chem 2 - Analyzing Strengths of Intermolecular Forces III
Chem 2 - Analyzing Strengths of Intermolecular Forces IIIChem 2 - Analyzing Strengths of Intermolecular Forces III
Chem 2 - Analyzing Strengths of Intermolecular Forces III
 
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole Attractions
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole AttractionsIntermolecular Forces: London Dispersion Forces and Dipole-Dipole Attractions
Intermolecular Forces: London Dispersion Forces and Dipole-Dipole Attractions
 
INTERMOLECULAR FORCES
INTERMOLECULAR FORCESINTERMOLECULAR FORCES
INTERMOLECULAR FORCES
 
Intermolecular forces
Intermolecular forcesIntermolecular forces
Intermolecular forces
 
Physical Science Week 2.1.pptx
Physical Science Week 2.1.pptxPhysical Science Week 2.1.pptx
Physical Science Week 2.1.pptx
 
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEET
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEETSolid State & Solution_Unit 1-2_Class-12_Board-JEE-NEET
Solid State & Solution_Unit 1-2_Class-12_Board-JEE-NEET
 
Covalent bonds
Covalent bondsCovalent bonds
Covalent bonds
 
Covalent bond
Covalent bond Covalent bond
Covalent bond
 
Polar Bonds and Polar Molecules.pptx
Polar Bonds and Polar Molecules.pptxPolar Bonds and Polar Molecules.pptx
Polar Bonds and Polar Molecules.pptx
 
47 intermolecularforces
47 intermolecularforces47 intermolecularforces
47 intermolecularforces
 
UCSD NANO106 - 02 - 3D Bravis Lattices and Lattice Computations
UCSD NANO106 - 02 - 3D Bravis Lattices and Lattice ComputationsUCSD NANO106 - 02 - 3D Bravis Lattices and Lattice Computations
UCSD NANO106 - 02 - 3D Bravis Lattices and Lattice Computations
 
Molecular geometry
Molecular geometryMolecular geometry
Molecular geometry
 
Chapter4 120319075415-phpapp02
Chapter4 120319075415-phpapp02Chapter4 120319075415-phpapp02
Chapter4 120319075415-phpapp02
 
Chemical bonds- Properties of Ionic and Covalent compounds
Chemical bonds- Properties of Ionic and Covalent compoundsChemical bonds- Properties of Ionic and Covalent compounds
Chemical bonds- Properties of Ionic and Covalent compounds
 
Covalent Bonds
Covalent BondsCovalent Bonds
Covalent Bonds
 
Chemical bonding cheat sheet
Chemical bonding cheat sheetChemical bonding cheat sheet
Chemical bonding cheat sheet
 

Ähnlich wie Chapter7

Chapter7 120319075433-phpapp02
Chapter7 120319075433-phpapp02Chapter7 120319075433-phpapp02
Chapter7 120319075433-phpapp02Cleophas Rwemera
 
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptx
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptxLesson 1_Kinetic Molecular Theory of Solids and Liquids.pptx
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptxKimberlyAnnePagdanga1
 
08 an introduction to metabolism
08 an introduction to metabolism08 an introduction to metabolism
08 an introduction to metabolismkindarspirit
 
Kmt, intermolecular forces, intro energy
Kmt, intermolecular forces, intro energyKmt, intermolecular forces, intro energy
Kmt, intermolecular forces, intro energyFelipe De la Garza
 
Need of a new approach to Atomic structure
Need of a new approach to Atomic structureNeed of a new approach to Atomic structure
Need of a new approach to Atomic structureMithil Fal Desai
 
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptx
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptxKMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptx
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptxaminaviadohael
 
1-Kinetic-Molecular-Theory.pdf
1-Kinetic-Molecular-Theory.pdf1-Kinetic-Molecular-Theory.pdf
1-Kinetic-Molecular-Theory.pdfSamNisperos
 
Kinetic Particle Theory (Slg Introduction)
Kinetic Particle Theory (Slg Introduction)Kinetic Particle Theory (Slg Introduction)
Kinetic Particle Theory (Slg Introduction)sYhira
 
Phy exppp chap08
Phy exppp chap08Phy exppp chap08
Phy exppp chap08hmsoh
 
Intermolecular forces
Intermolecular forcesIntermolecular forces
Intermolecular forcesSiyavula
 
Intermolecular forces, 12(1)
Intermolecular forces, 12(1)Intermolecular forces, 12(1)
Intermolecular forces, 12(1)K. Shahzad Baig
 
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th edition
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th editionLecture 1 Introduction to statics Engineering Mechanics hibbeler 14th edition
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th editionaxmedbaasaay
 
M3 explaining and applying chemical kinetics
M3 explaining and applying chemical kineticsM3 explaining and applying chemical kinetics
M3 explaining and applying chemical kineticsRz Ame
 
Chapter 2 - Basic Chemistry
Chapter 2 - Basic ChemistryChapter 2 - Basic Chemistry
Chapter 2 - Basic Chemistrycavalierem
 

Ähnlich wie Chapter7 (20)

Chapter7 120319075433-phpapp02
Chapter7 120319075433-phpapp02Chapter7 120319075433-phpapp02
Chapter7 120319075433-phpapp02
 
thermodynamics
thermodynamicsthermodynamics
thermodynamics
 
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptx
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptxLesson 1_Kinetic Molecular Theory of Solids and Liquids.pptx
Lesson 1_Kinetic Molecular Theory of Solids and Liquids.pptx
 
Physics and Matter
Physics and Matter Physics and Matter
Physics and Matter
 
08 an introduction to metabolism
08 an introduction to metabolism08 an introduction to metabolism
08 an introduction to metabolism
 
steric effect.pptx
steric effect.pptxsteric effect.pptx
steric effect.pptx
 
Kmt, intermolecular forces, intro energy
Kmt, intermolecular forces, intro energyKmt, intermolecular forces, intro energy
Kmt, intermolecular forces, intro energy
 
Need of a new approach to Atomic structure
Need of a new approach to Atomic structureNeed of a new approach to Atomic structure
Need of a new approach to Atomic structure
 
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptx
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptxKMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptx
KMT-PROPERTIES-OF-LIQUIDS-AND-SOLIDS.pptx
 
1-Kinetic-Molecular-Theory.pdf
1-Kinetic-Molecular-Theory.pdf1-Kinetic-Molecular-Theory.pdf
1-Kinetic-Molecular-Theory.pdf
 
Kinetic Particle Theory (Slg Introduction)
Kinetic Particle Theory (Slg Introduction)Kinetic Particle Theory (Slg Introduction)
Kinetic Particle Theory (Slg Introduction)
 
Phy exppp chap08
Phy exppp chap08Phy exppp chap08
Phy exppp chap08
 
KINETIC MOLECULAR.pptx
KINETIC MOLECULAR.pptxKINETIC MOLECULAR.pptx
KINETIC MOLECULAR.pptx
 
Intermolecular forces
Intermolecular forcesIntermolecular forces
Intermolecular forces
 
Intermolecular forces, 12(1)
Intermolecular forces, 12(1)Intermolecular forces, 12(1)
Intermolecular forces, 12(1)
 
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th edition
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th editionLecture 1 Introduction to statics Engineering Mechanics hibbeler 14th edition
Lecture 1 Introduction to statics Engineering Mechanics hibbeler 14th edition
 
M3 explaining and applying chemical kinetics
M3 explaining and applying chemical kineticsM3 explaining and applying chemical kinetics
M3 explaining and applying chemical kinetics
 
KMT.pptx
KMT.pptxKMT.pptx
KMT.pptx
 
Chapter 2 - Basic Chemistry
Chapter 2 - Basic ChemistryChapter 2 - Basic Chemistry
Chapter 2 - Basic Chemistry
 
10+2 physics
10+2 physics10+2 physics
10+2 physics
 

Kürzlich hochgeladen

Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024
Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024
Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024Victor Rentea
 
DBX First Quarter 2024 Investor Presentation
DBX First Quarter 2024 Investor PresentationDBX First Quarter 2024 Investor Presentation
DBX First Quarter 2024 Investor PresentationDropbox
 
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ..."I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...Zilliz
 
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...apidays
 
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost SavingRepurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost SavingEdi Saputra
 
MS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectorsMS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectorsNanddeep Nachan
 
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemke
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemkeProductAnonymous-April2024-WinProductDiscovery-MelissaKlemke
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemkeProduct Anonymous
 
ICT role in 21st century education and its challenges
ICT role in 21st century education and its challengesICT role in 21st century education and its challenges
ICT role in 21st century education and its challengesrafiqahmad00786416
 
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data DiscoveryTrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data DiscoveryTrustArc
 
WSO2's API Vision: Unifying Control, Empowering Developers
WSO2's API Vision: Unifying Control, Empowering DevelopersWSO2's API Vision: Unifying Control, Empowering Developers
WSO2's API Vision: Unifying Control, Empowering DevelopersWSO2
 
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...Jeffrey Haguewood
 
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, AdobeApidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobeapidays
 
Architecting Cloud Native Applications
Architecting Cloud Native ApplicationsArchitecting Cloud Native Applications
Architecting Cloud Native ApplicationsWSO2
 
DEV meet-up UiPath Document Understanding May 7 2024 Amsterdam
DEV meet-up UiPath Document Understanding May 7 2024 AmsterdamDEV meet-up UiPath Document Understanding May 7 2024 Amsterdam
DEV meet-up UiPath Document Understanding May 7 2024 AmsterdamUiPathCommunity
 
Introduction to Multilingual Retrieval Augmented Generation (RAG)
Introduction to Multilingual Retrieval Augmented Generation (RAG)Introduction to Multilingual Retrieval Augmented Generation (RAG)
Introduction to Multilingual Retrieval Augmented Generation (RAG)Zilliz
 
FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024The Digital Insurer
 
CNIC Information System with Pakdata Cf In Pakistan
CNIC Information System with Pakdata Cf In PakistanCNIC Information System with Pakdata Cf In Pakistan
CNIC Information System with Pakdata Cf In Pakistandanishmna97
 
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...Zilliz
 

Kürzlich hochgeladen (20)

Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024
Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024
Modular Monolith - a Practical Alternative to Microservices @ Devoxx UK 2024
 
Understanding the FAA Part 107 License ..
Understanding the FAA Part 107 License ..Understanding the FAA Part 107 License ..
Understanding the FAA Part 107 License ..
 
DBX First Quarter 2024 Investor Presentation
DBX First Quarter 2024 Investor PresentationDBX First Quarter 2024 Investor Presentation
DBX First Quarter 2024 Investor Presentation
 
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ..."I see eyes in my soup": How Delivery Hero implemented the safety system for ...
"I see eyes in my soup": How Delivery Hero implemented the safety system for ...
 
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
Apidays New York 2024 - APIs in 2030: The Risk of Technological Sleepwalk by ...
 
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost SavingRepurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
Repurposing LNG terminals for Hydrogen Ammonia: Feasibility and Cost Saving
 
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
+971581248768>> SAFE AND ORIGINAL ABORTION PILLS FOR SALE IN DUBAI AND ABUDHA...
 
MS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectorsMS Copilot expands with MS Graph connectors
MS Copilot expands with MS Graph connectors
 
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemke
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemkeProductAnonymous-April2024-WinProductDiscovery-MelissaKlemke
ProductAnonymous-April2024-WinProductDiscovery-MelissaKlemke
 
ICT role in 21st century education and its challenges
ICT role in 21st century education and its challengesICT role in 21st century education and its challenges
ICT role in 21st century education and its challenges
 
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data DiscoveryTrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
TrustArc Webinar - Unlock the Power of AI-Driven Data Discovery
 
WSO2's API Vision: Unifying Control, Empowering Developers
WSO2's API Vision: Unifying Control, Empowering DevelopersWSO2's API Vision: Unifying Control, Empowering Developers
WSO2's API Vision: Unifying Control, Empowering Developers
 
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
Web Form Automation for Bonterra Impact Management (fka Social Solutions Apri...
 
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, AdobeApidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
Apidays New York 2024 - Scaling API-first by Ian Reasor and Radu Cotescu, Adobe
 
Architecting Cloud Native Applications
Architecting Cloud Native ApplicationsArchitecting Cloud Native Applications
Architecting Cloud Native Applications
 
DEV meet-up UiPath Document Understanding May 7 2024 Amsterdam
DEV meet-up UiPath Document Understanding May 7 2024 AmsterdamDEV meet-up UiPath Document Understanding May 7 2024 Amsterdam
DEV meet-up UiPath Document Understanding May 7 2024 Amsterdam
 
Introduction to Multilingual Retrieval Augmented Generation (RAG)
Introduction to Multilingual Retrieval Augmented Generation (RAG)Introduction to Multilingual Retrieval Augmented Generation (RAG)
Introduction to Multilingual Retrieval Augmented Generation (RAG)
 
FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024FWD Group - Insurer Innovation Award 2024
FWD Group - Insurer Innovation Award 2024
 
CNIC Information System with Pakdata Cf In Pakistan
CNIC Information System with Pakdata Cf In PakistanCNIC Information System with Pakdata Cf In Pakistan
CNIC Information System with Pakdata Cf In Pakistan
 
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...
Emergent Methods: Multi-lingual narrative tracking in the news - real-time ex...
 

Chapter7

  • 2. Chapter 7 Table of Contents 7.1The Kinetic Molecular Theory of Matter 7.2Kinetic Molecular Theory and Physical States 7.3Gas Law Variables 7.4Boyle’s Law: A Pressure-Volume Relationship 7.5 Charles’s Law: A Temperature-Volume Relationship 7.6The Combined Gas Law 7.7The Ideal Gas Law 7.8Dalton’s Law of Partial Pressures 7.9Changes of State 7.10Evaporation of Liquids 7.11Vapor Pressure of Liquids 7.12Boiling and Boiling Point 7.13Intermolecular Forces in Liquids Copyright © Cengage Learning. All rights reserved 2
  • 3. Section 7.1 The Kinetic Molecular Theory of Matter Common Physical Properties of Matter • Volume and Shape • Density • Compressibility • Thermal Expansion Return to TOC Copyright © Cengage Learning. All rights reserved 3
  • 4. Section 7.1 The Kinetic Molecular Theory of Matter Compressibility • A measure of the change in volume of a sample of matter resulting from a pressure change. Return to TOC Copyright © Cengage Learning. All rights reserved 4
  • 5. Section 7.1 The Kinetic Molecular Theory of Matter Thermal Expansion • A measure of the change in volume of a sample of matter resulting from a temperature change. Return to TOC Copyright © Cengage Learning. All rights reserved 5
  • 6. Section 7.1 The Kinetic Molecular Theory of Matter Distinguishing Properties of Solids, Liquids, and Gases Return to TOC Copyright © Cengage Learning. All rights reserved 6
  • 7. Section 7.1 The Kinetic Molecular Theory of Matter Kinetic Molecular Theory of Matter 1. Matter is composed of tiny particles (atoms, molecules, or ions) that have definite and characteristic sizes that do not change. Return to TOC Copyright © Cengage Learning. All rights reserved 7
  • 8. Section 7.1 The Kinetic Molecular Theory of Matter Kinetic Molecular Theory of Matter 1. The particles are in constant random motion and therefore possess kinetic energy.  Kinetic energy – energy that matter possesses because of particle motion. Return to TOC Copyright © Cengage Learning. All rights reserved 8
  • 9. Section 7.1 The Kinetic Molecular Theory of Matter Kinetic Molecular Theory of Matter 1. The particles interact with one another through attractions and repulsions and therefore possess potential energy.  Potential energy – stored energy that matter possesses as a result of its position, condition, and/or composition. Return to TOC Copyright © Cengage Learning. All rights reserved 9
  • 10. Section 7.1 The Kinetic Molecular Theory of Matter Kinetic Molecular Theory of Matter 1. The kinetic energy (velocity) of the particles increases as the temperature is increased. Return to TOC Copyright © Cengage Learning. All rights reserved 10
  • 11. Section 7.1 The Kinetic Molecular Theory of Matter Kinetic Molecular Theory of Matter 1. The particles in a system transfer energy to each other through elastic collisions. Return to TOC Copyright © Cengage Learning. All rights reserved 11
  • 12. Section 7.1 The Kinetic Molecular Theory of Matter Differences Among Solids, Liquids, and Gases • Explained by the relative magnitudes of kinetic energy and potential energy (electrostatic attractions). • Kinetic energy is a disruptive force that tends to make the particles of a system increasingly independent of one another. • Potential energy is a cohesive force that tends to cause order and stability among the particles of a system. Return to TOC Copyright © Cengage Learning. All rights reserved 12
  • 13. Section 7.2 Kinetic Molecular Theory and Physical States Solid • The physical state characterized by a dominance of potential energy (cohesive forces) over kinetic energy (disruptive forces). • Particles in a solid are drawn close together in a regular pattern by the strong cohesive forces present. • Each particle occupies a fixed position, about which it vibrates because of disruptive kinetic energy. Return to TOC Copyright © Cengage Learning. All rights reserved 13
  • 14. Section 7.2 Kinetic Molecular Theory and Physical States Solid Return to TOC Copyright © Cengage Learning. All rights reserved 14
  • 15. Section 7.2 Kinetic Molecular Theory and Physical States Definite Volume and Definite Shape • The strong, cohesive forces hold the particles in essentially fixed positions, resulting in definite volume and definite shape. Return to TOC Copyright © Cengage Learning. All rights reserved 15
  • 16. Section 7.2 Kinetic Molecular Theory and Physical States High Density • The constituent particles of solids are located as close together as possible (touching each other). Therefore, a given volume contains large numbers of particles, resulting in a high density. Return to TOC Copyright © Cengage Learning. All rights reserved 16
  • 17. Section 7.2 Kinetic Molecular Theory and Physical States Small Compressibility • Because there is very little space between particles, increased pressure cannot push the particles any closer together; therefore, it has little effect on the solid’s volume. Return to TOC Copyright © Cengage Learning. All rights reserved 17
  • 18. Section 7.2 Kinetic Molecular Theory and Physical States Very Small Thermal Expansion • An increased temperature increases the kinetic energy (disruptive forces), thereby causing more vibrational motion of the particles. Each particle occupies a slightly larger volume, and the result is a slight expansion of the solid. The strong, cohesive forces prevent this effect from becoming very large. Return to TOC Copyright © Cengage Learning. All rights reserved 18
  • 19. Section 7.2 Kinetic Molecular Theory and Physical States Liquid • The physical state characterized by potential energy (cohesive forces) and kinetic energy (disruptive forces) of about the same magnitude. • Particles that are randomly packed but relatively near one another. • The molecules are in constant, random motion; they slide freely over one another but do not move with enough energy to separate. Return to TOC Copyright © Cengage Learning. All rights reserved 19
  • 20. Section 7.2 Kinetic Molecular Theory and Physical States Liquid Return to TOC Copyright © Cengage Learning. All rights reserved 20
  • 21. Section 7.2 Kinetic Molecular Theory and Physical States Definite Volume and Indefinite Shape • The attractive forces are strong enough to restrict particles to movement within a definite volume. They are not strong enough to prevent the particles from moving over each other in a random manner that is limited only by the container walls. Return to TOC Copyright © Cengage Learning. All rights reserved 21
  • 22. Section 7.2 Kinetic Molecular Theory and Physical States High Density • The particles in a liquid are not widely separated; they are still touching one another. Therefore, there will be a large number of particles in a given volume – a high density. Return to TOC Copyright © Cengage Learning. All rights reserved 22
  • 23. Section 7.2 Kinetic Molecular Theory and Physical States Small Compressibility • Because the particles in a liquid are still touching each other, there is very little empty space. Therefore, an increase in pressure cannot squeeze the particles much closer together. Return to TOC Copyright © Cengage Learning. All rights reserved 23
  • 24. Section 7.2 Kinetic Molecular Theory and Physical States Small Thermal Expansion • Most of the particle movement in a liquid is vibrational because a particle can move only a short distance before colliding with a neighbor. The increased particle velocity that accompanies a temperature increase results only in increased vibrational amplitudes. The net effect is an increase in the effective volume a particle occupies, which causes a slight volume increase in the liquid. Return to TOC Copyright © Cengage Learning. All rights reserved 24
  • 25. Section 7.2 Kinetic Molecular Theory and Physical States Gas • The physical state characterized by a complete dominance of kinetic energy (disruptive forces) over potential energy (cohesive forces). • Attractive forces among particles are very weak and are considered to be zero. • The particles move essentially independently of one another in a totally random manner. Return to TOC Copyright © Cengage Learning. All rights reserved 25
  • 26. Section 7.2 Kinetic Molecular Theory and Physical States Gas Return to TOC Copyright © Cengage Learning. All rights reserved 26
  • 27. Section 7.2 Kinetic Molecular Theory and Physical States Indefinite Volume and Indefinite Shape • The attractive (cohesive) forces between particles have been overcome by high kinetic energy, and the particles are free to travel in all directions. • Particles completely fill their container and the shape of the gas is that of the container. Return to TOC Copyright © Cengage Learning. All rights reserved 27
  • 28. Section 7.2 Kinetic Molecular Theory and Physical States Low Density • The particles are widely separated. There are relatively few particles in a given volume, which means little mass per volume. Return to TOC Copyright © Cengage Learning. All rights reserved 28
  • 29. Section 7.2 Kinetic Molecular Theory and Physical States Large Compressibility • A gas is mostly empty space. When pressure is applied, the particles are easily pushed closer together, decreasing the amount of empty space and the volume of the gas. Return to TOC Copyright © Cengage Learning. All rights reserved 29
  • 30. Section 7.2 Kinetic Molecular Theory and Physical States Moderate Thermal Expansion • An increase in temperature means an increase in particle velocity. The increased KE enables the particles to push back whatever barrier is confining them, and the volume increases. It is the space between the particles that changes. Return to TOC Copyright © Cengage Learning. All rights reserved 30
  • 31. Section 7.3 Gas Law Variables Gas Law • A generalization that describes in mathematical terms the relationships among the amount, pressure, temperature, and volume of a gas. Return to TOC Copyright © Cengage Learning. All rights reserved 31
  • 32. Section 7.3 Gas Law Variables Pressure force Pr essure = area • 1 atm = 760 mm Hg = 760 torr • 1 atm = 14.7 psi Return to TOC Copyright © Cengage Learning. All rights reserved 32
  • 33. Section 7.3 Gas Law Variables Pressure of a Gas • The force that creates pressure is that which is exerted by the gas molecules or atoms as they constantly collide with the walls of their container. Return to TOC Copyright © Cengage Learning. All rights reserved 33
  • 34. Section 7.3 Gas Law Variables Barometer • A device used to measure atmospheric pressure. Return to TOC Copyright © Cengage Learning. All rights reserved 34
  • 35. Section 7.3 Gas Law Variables Barometer Return to TOC Copyright © Cengage Learning. All rights reserved 35
  • 36. Section 7.4 Boyle’s Law: A Pressure-Volume Relationship Boyle’s Law • Pressure and volume are inversely related (constant T, temperature, and n, # of moles). P1 × V1 = P2 × V2 Return to TOC Copyright © Cengage Learning. All rights reserved 36
  • 37. Section 7.4 Boyle’s Law: A Pressure-Volume Relationship Boyle’s Law Return to TOC Copyright © Cengage Learning. All rights reserved 37
  • 38. Section 7.4 Boyle’s Law: A Pressure-Volume Relationship Exercise A sample of helium gas occupies 12.4 L at 23°C and 0.956 atm. What volume will it occupy at 1.20 atm assuming that the temperature stays constant? P1 × V1 = P2 × V2 (0.956 atm)(12.4 L) = (1.20 atm)(V2 ) V2 = 9.88 L Return to TOC Copyright © Cengage Learning. All rights reserved 38
  • 39. Section 7.5 Charles’s Law: A Temperature-Volume Relationship Charles’s Law • Volume and temperature (in Kelvin) are directly related (constant P and n). • K = °C + 273 V1 V2 = T1 T2 Return to TOC Copyright © Cengage Learning. All rights reserved 39
  • 40. Section 7.5 Charles’s Law: A Temperature-Volume Relationship Charles’s Law Return to TOC Copyright © Cengage Learning. All rights reserved 40
  • 41. Section 7.5 Charles’s Law: A Temperature-Volume Relationship Exercise Suppose a balloon containing 1.30 L of air at 24.7°C is placed into a beaker containing liquid nitrogen at –78.5°C. What will the volume of the sample of air become (at constant pressure)? V1 V2 = T1 T2 1.30 L V2 = ( 24.7 + 273 ) ( −78.5 + 273 ) V2 = 0.849 L Return to TOC Copyright © Cengage Learning. All rights reserved 41
  • 42. Section 7.6 The Combined Gas Law • The product of the pressure and volume of a fixed amount of gas is directly proportional to its Kelvin temperature. P1V1 P2 V2 = T1 T2 Return to TOC Copyright © Cengage Learning. All rights reserved 42
  • 43. Section 7.6 The Combined Gas Law Exercise At what temperature (in °C) does 121 mL of CO2 at 27°C and 1.05 atm occupy a volume of 293 mL at a pressure of 1.40 atm? P1V1 P2 V2 = T1 T2 ( 1.05 atm ) ( 121 mL ) = ( 1.40 atm ) ( 293 mL ) ( 27+273 ) ( T2 + 273 ) T2 = 969 K − 273 T2 = 696°C Return to TOC Copyright © Cengage Learning. All rights reserved 43
  • 44. Section 7.7 The Ideal Gas Law • We can bring all of these laws together into one comprehensive law: PV = nRT (where R = 0.0821 L·atm/mol·K` Return to TOC Copyright © Cengage Learning. All rights reserved 44
  • 45. Section 7.7 The Ideal Gas Law Exercise An automobile tire at 23°C with an internal volume of 25.0 L is filled with air to a total pressure of 2.18 atm (32 pounds per square inch). Determine the number of moles of air in the tire. PV = nRT (2.18 atm)(25.0 L) = n(0.0821 L ⋅ atm/mol ⋅ K)(23+273 K) n = 2.24 mol Return to TOC Copyright © Cengage Learning. All rights reserved 45
  • 46. Section 7.7 The Ideal Gas Law Exercise What is the pressure in a 304.0 L tank that contains 5.670 kg of helium at 25°C? PV = nRT  5.670 × 1000  (P)(304.0 L) =   (0.0821 L ⋅ atm/mol ⋅ K)(25+273)  4.003  n = 114 atm Return to TOC Copyright © Cengage Learning. All rights reserved 46
  • 47. Section 7.8 Dalton’s Law of Partial Pressures • For a mixture of gases in a container, PTotal = P1 + P2 + P3 + . . . • The total pressure exerted by a mixture of gases is the sum of the partial pressures of the individual gases present. Return to TOC Copyright © Cengage Learning. All rights reserved 47
  • 48. Section 7.8 Dalton’s Law of Partial Pressures Return to TOC Copyright © Cengage Learning. All rights reserved 48
  • 49. Section 7.8 Dalton’s Law of Partial Pressures Exercise Consider the following container of helium at 45°C. Initially the valve is closed. – After the valve is opened, what is the pressure of the helium gas? 2.00 atm 3.00 atm 9.00 L 3.00 L 2.25 atm Return to TOC Copyright © Cengage Learning. All rights reserved 49
  • 50. Section 7.9 Changes of State • A process in which a substance is transformed from one physical state to another physical state. • Usually accomplished by heating or cooling a substance, but pressure can also be a factor. • Changes of state are examples of physical changes. Return to TOC Copyright © Cengage Learning. All rights reserved 50
  • 51. Section 7.9 Changes of State Six Possible Changes of State • Freezing • Melting • Evaporation • Condensation • Sublimation • Deposition Return to TOC Copyright © Cengage Learning. All rights reserved 51
  • 52. Section 7.9 Changes of State Six Possible Changes of State Return to TOC Copyright © Cengage Learning. All rights reserved 52
  • 53. Section 7.9 Changes of State Two Categories 1. Endothermic change of state – change of state in which heat energy is absorbed. – Melting – Sublimation – Evaporation Return to TOC Copyright © Cengage Learning. All rights reserved 53
  • 54. Section 7.9 Changes of State Two Categories 1. Exothermic change of state – change of state in which heat energy is given off. – Freezing – Condensation – Deposition Return to TOC Copyright © Cengage Learning. All rights reserved 54
  • 55. Section 7.10 Evaporation of Liquids • Process by which molecules escape from the liquid phase to the gas phase. • For a liquid to evaporate, its molecules must gain enough kinetic energy to overcome the attractive forces among them. Return to TOC Copyright © Cengage Learning. All rights reserved 55
  • 56. Section 7.10 Evaporation of Liquids Rate of Evaporation • Increased surface area results in an increased evaporation rate because a greater fraction of the total molecules are on the surface (so they are not completely surrounded by other molecules with attractive forces). Return to TOC Copyright © Cengage Learning. All rights reserved 56
  • 57. Section 7.10 Evaporation of Liquids Rate of Evaporation • Always increases as liquid temperature increases. • A cooling effect is produced in the liquid when evaporation occurs. • Vapor – A gas that exists at a temperature and pressure at which it ordinarily would be thought of as a liquid or solid. Return to TOC Copyright © Cengage Learning. All rights reserved 57
  • 58. Section 7.11 Vapor Pressure of Liquids Evaporation of a Liquid in a Closed Container g) The liquid level drops for a time. h) Then becomes constant (ceases to drop). i) Rate of evaporation equals the rate of condensation. Return to TOC Copyright © Cengage Learning. All rights reserved 58
  • 59. Section 7.11 Vapor Pressure of Liquids Equilibrium • A condition in which two opposite processes take place at the same rate. • No net macroscopic changes can be detected, but the system is dynamic. • Forward and reverse processes are occurring at equal rates. Return to TOC Copyright © Cengage Learning. All rights reserved 59
  • 60. Section 7.11 Vapor Pressure of Liquids Vapor Pressure • Pressure exerted by a vapor above a liquid when the liquid and vapor are in equilibrium with each other. • Magnitude of vapor pressure depends on the nature and temperature of the liquid. Return to TOC Copyright © Cengage Learning. All rights reserved 60
  • 61. Section 7.11 Vapor Pressure of Liquids Vapor Pressure • Liquids that have strong attractive forces between molecules have lower vapor pressures than liquids that have weak attractive forces between particles. Return to TOC Copyright © Cengage Learning. All rights reserved 61
  • 62. Section 7.11 Vapor Pressure of Liquids Vapor Pressure • Substances that have high vapor pressures evaporate readily – they are volatile.  Volatile substance – a substance that readily evaporates at room temperature because of a high vapor pressure. Return to TOC Copyright © Cengage Learning. All rights reserved 62
  • 63. Section 7.12 Boiling and Boiling Point Boiling • A form of evaporation where conversion from the liquid state to the vapor state occurs within the body of the liquid through bubble formation. • Occurs when the vapor pressure of the liquid reaches a value equal to that of the prevailing external pressure on the liquid (for an open container it’s atmospheric pressure). Return to TOC Copyright © Cengage Learning. All rights reserved 63
  • 64. Section 7.12 Boiling and Boiling Point Boiling Return to TOC Copyright © Cengage Learning. All rights reserved 64
  • 65. Section 7.12 Boiling and Boiling Point Boiling Point • The temperature at which the vapor pressure of a liquid becomes equal to the external (atmospheric) pressure exerted on the liquid. • Normal boiling point – the temperature at which a liquid boils under a pressure of 760 mm Hg. • Boiling point changes with elevation. Return to TOC Copyright © Cengage Learning. All rights reserved 65
  • 66. Section 7.12 Boiling and Boiling Point BP of Water at Various Locations That Differ in Elevation Return to TOC Copyright © Cengage Learning. All rights reserved 66
  • 67. Section 7.12 Boiling and Boiling Point Concept Check What is the vapor pressure of water at 100°C? How do you know? 1 atm Return to TOC Copyright © Cengage Learning. All rights reserved 67
  • 68. Section 7.13 Intermolecular Forces in Liquids Intramolecular Forces • Forces “Within” molecules. Return to TOC Copyright © Cengage Learning. All rights reserved 68
  • 69. Section 7.13 Intermolecular Forces in Liquids Intermolecular Force • An attractive force that acts between a molecule and another molecule. • Intermolecular forces are weak compared to intramolecular forces. Return to TOC Copyright © Cengage Learning. All rights reserved 69
  • 70. Section 7.13 Intermolecular Forces in Liquids Three Main Types of Intermolecular Forces • Dipole-dipole interactions • Hydrogen bonds • London forces Return to TOC Copyright © Cengage Learning. All rights reserved 70
  • 71. Section 7.13 Intermolecular Forces in Liquids Dipole-Dipole Interactions • An IMF that occurs between polar molecules. • Molecules with dipole moments can attract each other electrostatically by lining up so that the positive and negative ends are close to each other. • The greater the polarity of the molecules, the greater the strength of the dipole-dipole interactions. Return to TOC Copyright © Cengage Learning. All rights reserved 71
  • 72. Section 7.13 Intermolecular Forces in Liquids Dipole-Dipole Interactions Between ClF Molecules Return to TOC Copyright © Cengage Learning. All rights reserved 72
  • 73. Section 7.13 Intermolecular Forces in Liquids Dipole-Dipole Interactions Return to TOC Copyright © Cengage Learning. All rights reserved 73
  • 74. Section 7.13 Intermolecular Forces in Liquids Hydrogen Bonds • Unusually strong dipole-dipole interactions are observed among hydrogen-containing molecules in which hydrogen is covalently bonded to a highly electronegative element of small atomic size (fluorine, oxygen, and nitrogen). Return to TOC Copyright © Cengage Learning. All rights reserved 74
  • 75. Section 7.13 Intermolecular Forces in Liquids Two Factors 1. The highly electronegative element to which hydrogen is covalently bonded attracts the bonding electrons to such a degree that the hydrogen atom is left with a significant δ+charge. 2. The small size of the “bare” hydrogen nucleus allows it to approach closely, and be strongly attracted to a lone pair of electrons on the electronegative atom of another molecule. Return to TOC Copyright © Cengage Learning. All rights reserved 75
  • 76. Section 7.13 Intermolecular Forces in Liquids Hydrogen Bonding in Water Return to TOC Copyright © Cengage Learning. All rights reserved 76
  • 77. Section 7.13 Intermolecular Forces in Liquids Hydrogen Bonding Return to TOC Copyright © Cengage Learning. All rights reserved 77
  • 78. Section 7.13 Intermolecular Forces in Liquids • The vapor pressures of liquids that have significant hydrogen bonding are much lower than those of similar liquids wherein little or no hydrogen bonding occurs. Return to TOC Copyright © Cengage Learning. All rights reserved 78
  • 79. Section 7.13 Intermolecular Forces in Liquids Return to TOC Copyright © Cengage Learning. All rights reserved 79
  • 80. Section 7.13 Intermolecular Forces in Liquids London Forces Return to TOC Copyright © Cengage Learning. All rights reserved 80
  • 81. Section 7.13 Intermolecular Forces in Liquids London Forces • A weak temporary intermolecular force that occurs between an atom or molecule (polar or nonpolar) and another atom or molecule (polar or nonpolar). • Results from momentary uneven electron distributions in molecules. • Significant in large atoms/molecules. • Occurs in all molecules, including nonpolar ones. Return to TOC Copyright © Cengage Learning. All rights reserved 81
  • 82. Section 7.13 Intermolecular Forces in Liquids Boiling Point Trends for Related Series of Nonpolar Molecules Return to TOC Copyright © Cengage Learning. All rights reserved 82
  • 83. Section 7.13 Intermolecular Forces in Liquids Concept Check Which are stronger, intramolecular bonds or intermolecular forces? How do you know? Return to TOC Copyright © Cengage Learning. All rights reserved 83
  • 84. Section 7.13 Intermolecular Forces in Liquids Concept Check Which has the stronger intermolecular forces? N2 H2O Explain. Return to TOC Copyright © Cengage Learning. All rights reserved 84
  • 85. Section 7.13 Intermolecular Forces in Liquids Concept Check Draw two Lewis structures for the formula C2H6O and compare the boiling points of the two molecules. Return to TOC Copyright © Cengage Learning. All rights reserved 85
  • 86. Section 7.13 Intermolecular Forces in Liquids Concept Check Which gas would behave more ideally at the same conditions of P and T? CO or N2 Why? Return to TOC Copyright © Cengage Learning. All rights reserved 86

Hinweis der Redaktion

  1. (0.956 atm)(12.4 L) = (1.20 atm)(V 2 ) The new volume is 9.88 L.
  2. The new volume will become 0.849 L. Remember to convert the temperatures to Kelvin. (1.30 L) / (24.7+273) = V 2 / (-78.5 + 273)
  3. The new temperature is 696°C. (1.05 atm)(121 mL) / (27+273) = (1.40 atm)(293 mL) / (T 2 + 273)
  4. The number of moles of air is 2.24 mol. (2.18 atm)(25.0 L) = n(0.0821)(23+273)
  5. The pressure is 114 atm. Remember to convert kg of helium into moles of helium before using the ideal gas law. (P)(304.0) = ([5.670×1000]/4.003)(0.0821)(25+273)
  6. The pressure is 2.25 atm. There are two ways to solve the problem: 1) Find the new pressure of the gas on the left side after the valve is opened (P 1 V 1 =P 2 V 2 ). The pressure becomes 1.50 atm. Find the new pressure of the gas on the right side after the valve is opened (P 1 V 1 =P 2 V 2 ). The pressure becomes 0.75 atm. The total pressure is therefore 1.50 + 0.75 = 2.25 atm. 2) Find the number of moles in each chamber separately (using PV = nRT), add the number of moles and volumes on each side, then use PV = nRT to solve for the new pressure.
  7. The vapor pressure of water at 100 o C is 1 atm. You know this because atmospheric pressure is 1 atm and this is the temperature at which we observe water to boil.
  8. Intramolecular bonds are stronger because it would take a lot more energy to overcome covalent bonds and break apart the molecule than to overcome intermolecular forces in between the atoms (to make it become a liquid or gas).
  9. H 2 O has the stronger intermolecular forces because it exhibits hydrogen bonding, whereas N 2 only exhibits London dispersion forces.
  10. One Lewis structure could be ethanol and one Lewis structure could be dimethyl ether. Ethanol will have a higher boiling point than dimethyl ether because ethanol exhibits hydrogen bonding and dimethyl ether exhibits dipole-dipole interactions. Hydrogen bonding is an especially strong type of dipole-dipole interaction and will thus raise the boiling point of ethanol.
  11. N 2 would behave more ideally because it is nonpolar and only exhibits London dispersion forces, therefore the intermolecular forces between N 2 molecules are weak (and thus the collisions will be more “elastic”). CO also exhibits dipole-dipole interactions.