chapter 7 states of matter (gases, liquids and solids)
DESCRIPTION
Chapter 7 States of Matter (gases, liquids and solids). A solid has a definite shape and a definite volume A liquid has no definite shape (it takes the shape of its container) but a definite volume A gas has no definite shape or volume. - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/1.jpg)
Chapter 7 States of Matter (gases, liquids and solids)
Copyright © Houghton Mifflin Company. All rights reserved. 1–2
Figure 1.2 (a) A solid has a definite shape and a definite volume. (b) A liquid has an indefinite shape -it takes the shape of its container - a definite volume. (c) A gas has an indefinite shape and an indefinite
volume.
solid liquid gas
• A solid has a definite shape and a definite volume• A liquid has no definite shape (it takes the shape of its container) but a definite volume• A gas has no definite shape or volume
1
![Page 2: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/2.jpg)
• In a gas, the particles are in constant random motion, each particle being independent of the others present.
• The particles in a liquid, though still close together, freely slide over one another.
• In a solid, the particles (atoms, molecules, or ions) are close together and vibrate about fixed sites.
2
![Page 3: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/3.jpg)
1. Matter is composed of tiny particles (atoms, molecules, or ions) that have definite and characteristic sizes that do not change.
Kinetic Molecular Theory of Matter
2. The particles are in constant random motion and therefore possess kinetic energy. Kinetic energy – energy that matter
possesses because of particle motion.
3
![Page 4: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/4.jpg)
3. 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.
4. The kinetic energy (velocity) of the particles increases as the temperature is increased.
5. The particles in a system transfer energy to each other through elastic collisions.
4
![Page 5: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/5.jpg)
Solid: High densitySmall compressibilityVery small thermal expansion
Liquid:High densitySmall compressibilitySmall thermal expansion
Gas: Low densityLarge compressibilityModerate thermal expansion
Fig. 7.5
Pages 165 - 166
5
![Page 6: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/6.jpg)
I. Properties of gases A. Pressure
P = force/areaUsually measured by height of Hg
(mercury)
1 atmosphere pressure = 1 atm = 760 mm Hg
=760 torr
6
![Page 7: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/7.jpg)
Figure 6.3
7
![Page 8: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/8.jpg)
Page 178 Chemical Connections
Systolic pressure Diastolic pressureMeasure of bloodpressure
8
![Page 9: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/9.jpg)
Systole is the contraction of heart chambers, driving blood out of the chambers.
Diastole is the period of time when the heart relaxes after contraction.
Systolic pressure - the highest arterial pressure during each heart beat.
Diastolic pressure - the lowest arterial pressure between heart beats
Normal range:
Normal range:
9
![Page 10: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/10.jpg)
B. Volume, L C. Temperature, K 273K = 0oC K = oC + 273
10
![Page 11: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/11.jpg)
D. The Gas Laws
a) Boyle’s law
or PV = constant or P1V1 = P2V2
Constant temperature
pV
1
11
![Page 12: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/12.jpg)
b) Charles law
Copyright © Houghton Mifflin Company. All rights reserved. 7–6
Figure 7.12 Data illustrating the direct proportionality associated with Charles's law.
2
2
1
1
T
V
T
V
Constant pressure
T
Vconstant oror
TV
12
![Page 13: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/13.jpg)
c) The Combined Gas Law
Boyle's law: P1V1 = P2V2 pV
1
Charles law: TVT
V
T
V
2
2
1
1
Combined gas law:
P
TV or
T
PVconstant
2
22
1
11
T
VP
T
VP Combined gas law
13
![Page 14: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/14.jpg)
Example (1) A gas occupies 3L at 2 atm. What would be the pressure if the volume was 6L at the same temperature?
Example (2) A gas occupies 2.0 L at 200K and 1.0 atm pressure. What temperature would it be if the volume was 3.0L and the pressure was 380 torr?
2
22
1
11
T
VP
T
VP
14
![Page 15: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/15.jpg)
nVP
TV ,
(n = number of moles)
P
nTRV
P
nTV
PV = nRT Ideal gas law
R = gas constant = 0.0821 Kmol
Latm
Example 2.00 mol of CH4 occupies 16.4 L at 200K. What is the pressure?
d) The ideal Gas law
15
![Page 16: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/16.jpg)
g) Dalton's law of partial pressure Consider a mixture of two gases A and B at V, T.
V
RTn
V
RTn
V
RTnnP BABA
T
)(
= PA + PB
Example: A 10 L container contains 2.0 mol O2 and 4.0 N2 at 300K. Find PO2, PN2 and PT.
Total pressure
partial pressure of A partial pressure of B
PV = nRTV
nRTP
16
![Page 17: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/17.jpg)
PT = P1 + P2 + P3 + . . .In general
Example:Example: to a tank containing N2 at 2.5 atm and O2 at 1.5 atm
we add an unknown quantity of CO2 until the total pressure
in the tank is 5.2 atm. What is the partial pressure of CO2?
http://highered.mcgraw-hill.com/olcweb/cgi/pluginpop.cgi?it=swf::525::530::/sites/dl/free/0072828471/291136/movement_oxygen_carbon_dioxide.swf::Movement%20of%20Oxygen%20and%20Carbon%20Dioxide
17
![Page 18: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/18.jpg)
Figure 7.15 There are six changes of state possible for substances.
E. Changes of state
18
![Page 19: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/19.jpg)
1. Evaporation and condensation
H2O
evaporation
H2O
condensation
19
![Page 20: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/20.jpg)
H2O
2. Vapor pressure (v.p.) of liquids
evaporation
condensation
rate (evaporation) = rate (condensation)
liquid vapor
State of equilibrium (Saturation)
Vapor pressure = partial pressure exerted by the vapor above the liquid at saturation at a given temperature
20
![Page 21: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/21.jpg)
Evaporation of a Liquid in a Closed Container
Figure 7.17
21
![Page 22: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/22.jpg)
Vapor pressure increases with temperatureV
apor
pre
ssur
e
Temperature
22
![Page 23: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/23.jpg)
3. Boiling – evaporation occurs anywhere in the liquid
Normal boiling point – T at which v.p. of the liquid = 1 atm.
or boiling T under 1 atm
atmAt 100oC, v.p. of water = 1 atm
v.p.
(w
ater
)
T 100oC
1 atm
23
![Page 24: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/24.jpg)
T
Heating time
100oC
24
![Page 25: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/25.jpg)
25
![Page 26: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/26.jpg)
4. Conditions that affect boiling pointa) External Pressure:
Boiling point increasesas Pext increases
b) Attractive forces between molecules:
The stronger the attractive forces, the higher the
boiling point
26
![Page 27: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/27.jpg)
G. Intermolecular forcesa) Dipole-dipole interaction H Cl H Cl
+ - + -
H Cl H Cl H Cl H Cl
Cl H Cl H Cl H Cl H
27
![Page 28: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/28.jpg)
b) London dispersion forces
Nonpolar molecules such as H2 can develop instantaneous dipoles and induced dipoles. The attractions between such dipoles, even though they are transitory, create London forces.
Induced-induced dipole forces
London force increases with size of the molecule
28
![Page 29: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/29.jpg)
CH3CH2CH2CH3 CH3-C-CH3
O-
+Butane
(bp 0.5°C)Acetone(bp 58°C)
Consider
29
![Page 30: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/30.jpg)
b) Hydrogen bonds
H F H O H N
Example: H2O
H O
H
H
O
H
- +
hydrogenbond
hydrogenbond
- +
(a) (b) (c)
figure 6.9
Structuralformulas
ball and stickmodels
electron densitymodels
30
![Page 31: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/31.jpg)
H2OH O
H
H
OH
H O
HH
O H
H
O H
H
OH
H C
H
H
O H
31
![Page 32: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/32.jpg)
If there were no hydrogen bonding between water molecules, the boiling point of water would be approximately - 80C.
oC
oC
oC
oC
oC
32
![Page 33: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/33.jpg)
cannot H-bond with another
33
![Page 34: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/34.jpg)
For compounds of similar dipole moment, the larger the MW, the higher the boiling point.
For compounds of similar MW, the larger the dipole moment, the higher the boiling point.
In general
34
![Page 35: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/35.jpg)
Boiling point of compounds that can form H-bonds are relatively high.
H-bond > dipole-dipole forces > London forces
35
![Page 36: Chapter 7 States of Matter (gases, liquids and solids)](https://reader036.vdocuments.us/reader036/viewer/2022062314/56813931550346895da0da1c/html5/thumbnails/36.jpg)
Circle those compounds below in which the molecules are capable of forming hydrogen bonds between themselves.
NH3 NF3 HF
CO2 H C
H
O H C
H
O
H
H
In each pair below, circle the compound with the higher boiling point:
(1) O2 or Cl2 (2) H2O or H2S
(3) HBr or CF436