liquids

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properties & structure

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Liquids. properties & structure. Surface Tension. surface tension is a property of liquids that results from the tendency of liquids to minimize their surface area in order to minimize their surface area, liquids form drops that are spherical as long as there is no gravity - PowerPoint PPT Presentation

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Page 1: Liquids

properties &structure

Page 2: Liquids

Surface Tensionsurface tension is a property of liquids that results from the tendency of liquids to minimize their surface area

in order to minimize their surface area, liquids form drops that are sphericalas long as there is no gravity

the layer of molecules on the surface behave differently than the interior because the cohesive forces on the surface

molecules have a net pull into the liquid interiorthe surface layer acts like an elastic skin

2

Page 3: Liquids

Surface Tensionbecause they have fewer

neighbors to attract them, the surface molecules are less stable than those in the interiorhave a higher potential energy

the surface tension of a liquid is the energy required to increase the surface area a given amountat room temp, surface tension of

H2O = 72.8 mJ/m2

Tro, Chemistry: A Molecular Approach 3

Page 4: Liquids

Factors Affecting Surface Tensionthe stronger the intermolecular attractive

forces, the higher the surface tension will beraising the temperature of a liquid reduces

its surface tensionraising the temperature of the liquid increases

the average kinetic energy of the moleculesthe increased molecular motion makes it easier

to stretch the surface

Tro, Chemistry: A Molecular Approach 4

Page 5: Liquids

Tro, Chemistry: A Molecular Approach 5

Surface Tension of Water vs. Temperature

50

55

60

65

70

75

80

-20 0 20 40 60 80 100 120

Temperature, °C

Surf

ace

Ten

sion,

mJ/

m2

Page 6: Liquids

Viscosityviscosity is the resistance of a liquid to flow

1 poise = 1 P = 1 g/cm∙soften given in centipoise, cP

larger intermolecular attractions = larger viscosity

higher temperature = lower viscosity

Tro, Chemistry: A Molecular Approach 6

Page 7: Liquids

Tro, Chemistry: A Molecular Approach 7

Viscosity of Water vs. Temperature

0

0.2

0.4

0.6

0.8

1

1.2

0 20 40 60 80 100 120

Temperature, deg C

Visc

osity

, cP

Page 8: Liquids

Capillary Actioncapillary action is the ability of a liquid to

flow up a thin tube against the influence of gravitythe narrower the tube, the higher the liquid

risescapillary action is the result of the two forces

working in conjunction, the cohesive and adhesive forces cohesive forces attract the molecules togetheradhesive forces attract the molecules on the

edge to the tube’s surface

Tro, Chemistry: A Molecular Approach 8

Page 9: Liquids

Capillary Actionthe adhesive forces pull the surface liquid up

the side of the tube, while the cohesive forces pull the interior liquid with it

the liquid rises up the tube until the force of gravity counteracts the capillary action forces

Tro, Chemistry: A Molecular Approach 9

Page 10: Liquids

Vaporizationmolecules in the liquid are constantly in motion

the average kinetic energy is proportional to the temperature

however, some molecules have more kinetic energy than the average

if these molecules are at the surface, they may have enough energy to overcome the attractive forcestherefore – the larger the surface

area, the faster the rate of evaporation

this will allow them to escape the liquid and become a vapor

Tro, Chemistry: A Molecular Approach 10

Page 11: Liquids

Distribution of Thermal Energyonly a small fraction of the molecules in a liquid have enough

energy to escapebut, as the temperature increases, the fraction of the

molecules with “escape energy” increasesthe higher the temperature, the faster the rate of

evaporation

Tro, Chemistry: A Molecular Approach 11

Page 12: Liquids

Condensationsome molecules of the vapor will lose energy

through molecular collisionsthe result will be that some of the molecules

will get captured back into the liquid when they collide with it

also some may stick and gather together to form droplets of liquidparticularly on surrounding surfaces

we call this process condensation

Tro, Chemistry: A Molecular Approach 12

Page 13: Liquids

Evaporation vs. Condensationvaporization and condensation are opposite processes

in an open container, the vapor molecules generally spread out faster than they can condense

the net result is that the rate of vaporization is greater than the rate of condensation, and there is a net loss of liquid

however, in a closed container, the vapor is not allowed to spread out indefinitely

the net result in a closed container is that at some time the rates of vaporization and condensation will be equal

Tro, Chemistry: A Molecular Approach 13

Page 14: Liquids

Effect of Intermolecular Attraction on Evaporation and Condensationthe weaker the attractive forces between

molecules, the less energy they will need to vaporize

also, weaker attractive forces means that more energy will need to be removed from the vapor molecules before they can condense

the net result will be more molecules in the vapor phase, and a liquid that evaporates faster – the weaker the attractive forces, the faster the rate of evaporation

liquids that evaporate easily are said to be volatilee.g., gasoline, fingernail polish removerliquids that do not evaporate easily are called

nonvolatile e.g., motor oil

Tro, Chemistry: A Molecular Approach 14

Page 15: Liquids

Energetics of Vaporizationwhen the high energy molecules are lost from

the liquid, it lowers the average kinetic energyif energy is not drawn back into the liquid, its

temperature will decrease – therefore, vaporization is an endothermic processand condensation is an exothermic process

vaporization requires input of energy to overcome the attractions between molecules

Tro, Chemistry: A Molecular Approach 15

Page 16: Liquids

Heat of Vaporizationthe amount of heat energy required to vaporize one

mole of the liquid is called the Heat of Vaporization, Hvapsometimes called the enthalpy of vaporization

always endothermic, therefore Hvap is +somewhat temperature dependent Hcondensation = -Hvaporization

Tro, Chemistry: A Molecular Approach 16

Page 17: Liquids

Example 11.3 – Calculate the mass of water that can be vaporized with 155 kJ of heat at 100°C

since the given amount of heat is almost 4x the Hvap, the amount of water makes sense

1 mol H2O = 40.7 kJ, 1 mol = 18.02 g

155 kJg H2O

Check:

Solution:

Concept Plan:

Relationships:

Given:Find:

kJ 40.7mol 1

OH g 8.66 mol 1

g 8.021kJ 40.7

OH mol 1 kJ 551 22

kJ mol H2O g H2O

mol 1g 02.18

Page 18: Liquids

Tro, Chemistry: A Molecular Approach 18

Page 19: Liquids

Vapor Pressurethe pressure exerted by the vapor when it is in dynamic equilibrium with its liquid is called the vapor pressureremember using Dalton’s Law of Partial Pressures to

account for the pressure of the water vapor when collecting gases by water displacement?

the weaker the attractive forces between the molecules, the more molecules will be in the vapor

therefore, the weaker the attractive forces, the higher the vapor pressurethe higher the vapor pressure, the more volatile the liquid

Tro, Chemistry: A Molecular Approach 19

Page 20: Liquids

Vapor-Liquid Dynamic Equilibriumif the volume of the chamber is increased, that will

decrease the pressure of the vapor insideat that point, there are fewer vapor molecules in a given volume,

causing the rate of condensation to sloweventually enough liquid evaporates so that the rates of

the condensation increases to the point where it is once again as fast as evaporation equilibrium is reestablished

at this point, the vapor pressure will be the same as it was before

Tro, Chemistry: A Molecular Approach 20

Page 21: Liquids

Dynamic Equilibriuma system in dynamic equilibrium can respond

to changes in the conditionswhen conditions change, the system

shifts its position to relieve or reduce the effects of the change

Tro, Chemistry: A Molecular Approach 21

Page 22: Liquids

Vapor Pressure vs. Temperatureincreasing the temperature increases the

number of molecules able to escape the liquidthe net result is that as the temperature

increases, the vapor pressure increasessmall changes in temperature can make big

changes in vapor pressurethe rate of growth depends on strength of the

intermolecular forces

Tro, Chemistry: A Molecular Approach 22

Page 23: Liquids

Boiling Pointwhen the temperature of a liquid reaches a

point where its vapor pressure is the same as the external pressure, vapor bubbles can form anywhere in the liquidnot just on the surface

this phenomenon is what is called boiling and the temperature required to have the vapor pressure = external pressure is the boiling point

Tro, Chemistry: A Molecular Approach 23

Page 24: Liquids

Boiling Pointthe normal boiling point is the

temperature at which the vapor pressure of the liquid = 1 atm

the lower the external pressure, the lower the boiling point of the liquid

Tro, Chemistry: A Molecular Approach 24

Page 25: Liquids

Heating Curve of a Liquidas you heat a liquid, its

temperature increases linearly until it reaches the boiling pointq = mass x Cs x T

once the temperature reaches the boiling point, all the added heat goes into boiling the liquid – the temperature stays constant

once all the liquid has been turned into gas, the temperature can again start to rise

Tro, Chemistry: A Molecular Approach 25

Page 26: Liquids

Clausius-Clapeyron Equation2-Point Formthe equation below can be used with just two

measurements of vapor pressure and temperaturehowever, it generally gives less accurate results

fewer data points will not give as accurate an average because there is less averaging out of the errors as with any other sets of measurements

can also be used to predict the vapor pressure if you know the heat of vaporization and the normal boiling pointremember: the vapor pressure at the normal boiling point is 760

torr

Tro, Chemistry: A Molecular Approach 26

12

vap

1

2

T1

T1

RH

PPln