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2/3/2003 OFB Chapter 5 1
When you can measure what you are speaking about and express it in numbers, you know something about it; but when you cannot measure it, when you cannot express it in numbers, you knowledge is of a meager and unsatisfactory kind; it may be the beginning of knowledge but you have scarcely, in your thoughts advanced to the stage of science, whatever the matter may be.
--Lord Kelvin, May 3rd, 1883
2/3/2003 OFB Chapter 5 2
OFB Chapter 5
The Gaseous State
5-1 The Chemistry of Gases
5-2 Pressure and Boyle’s Law
5-3 Temperature and Charles’s Law
5-4 The Ideal Gas Law
5-5 Chemical Calculations for Gases
5-6 Mixtures of Gases
5-7 Real Gases
2/3/2003 OFB Chapter 5 3
2/3/2003 OFB Chapter 5 4
OFB Chapter 5
The Gaseous StateEarly discoveries of gases formed by chemical reactions:
2 HgO(s) → 2 Hg(l) + O2(g)
Lavoisier used this to establish the conservation of mass theory
heat
Marble: CaCO3(s) → CaO(s) + CO2(g)heat
NH4Cl(s) → HCl(g) + NH3(g)heat
Nitroglycerin: 4 C3H5(NO3)3(l) →
6 N2(g) + 12 CO2(g) + O2(g) + 10 H2O(g)
CaCO3(s) + HCl(aq) →
CaCl2(aq) + H2O(g) + CO2(g)
2/3/2003 OFB Chapter 5 5
Pressure and Boyle’s Law• In physics, a force (F) is a simple push
exerted by one object on another.
• Applying a force to a stationary object sets it in motion, unless the object pushes back with an equal force.
• Applying a force to an object that pushes back creates a pressure (P) on the object.
• Applying a force to an object that pushes back creates a pressure (P) on the object.
• The pressure equals the force divided by the area (A) over which the force is applied:
2/3/2003 OFB Chapter 5 6
Pressure and Boyle’s Law
force (F) = mass * acceleration = Newton (N) = kg m s-2
area (A) = m2
acceleration (a) = velocity per unit of time [m s-2]
mass (m) = quantity of matter [kg]
2/3/2003 OFB Chapter 5 7
Pressure and Boyle’s Law
2/3/2003 OFB Chapter 5 8
Pressure and Boyle’s Law
P = gdh
g = acceleration of gravity at the surface of the Earth
= 9.80665 m s-2
d = density of the liquid = for Hg at 0ºC
= 13.5951 g cm-3 = 13.5951 kg m-3
h = height of mercury in the column
= 76 cm = 760 mm = 0.76 m
P = gdh = (9.80665 m s-2)(13.5951 kg m-3)
(0.76 m)
2/3/2003 OFB Chapter 5 9
A pressure of 101.325 kPa is need to raise the column of
Hg 760 mm or 76 cm
Called standard pressure
2/3/2003 OFB Chapter 5 10
Boyle’s Law: The Effect of Pressure on Gas Volume
The product of the pressure and volume, PV, of a sample of gas is a constant at a constant temperature:
2/3/2003 OFB Chapter 5 11
Boyle’s Law: The Effect of Pressure on Gas Volume
STP
For 1 mole of any gas
(i.e., 32.0 g of O2; 28.0 g N2; 2.02 g H2),
STP = standard temperature and pressure= 0oC and 1 atm
2/3/2003 OFB Chapter 5 12
Boyle’s Law: The Effect of Pressure on Gas VolumeExercise 5-3The long cylinder of a bicycle pump has a volume of 1131 cm3 and is filled with air at a pressure of 1.02 atm. The outlet valve is sealed shut, and the pump handle is pushed down until the volume of the air is 517 cm3. The temperature of the air trapped inside does not change. Compute the pressure inside the pump.
2/3/2003 OFB Chapter 5 13
Charles’ Law: The Effect of Temperature on Gas Volume
Temperature and Charles’ Law
−°=
°1)
VV C273.15t
2/3/2003 OFB Chapter 5 14
Charles’ Law: The Effect of Temperature on Gas Volume
Absolute Temperature
V = Vo ( 1 + )t273.15oC
Kelvin temperature scale
2/3/2003 OFB Chapter 5 15
Charles’ Law: The Effect of Temperature on Gas Volume
2/3/2003 OFB Chapter 5 16
Exercise 5-4
The gas in a gas thermometer that has been placed in a furnace has a volume that is 2.56 times larger than the volume that it occupies at 100oC. Determine the temperature in the furnace (in degrees Celsius).
2/3/2003 OFB Chapter 5 17
V1 / V2 = T1 / T2(at a fixed pressure)
P1V1 = P2V2(at a fixed
temperature)
Boyle’s Law
Charles’ Law
(at a fixed pressure and temperature)Avogadro
2/3/2003 OFB Chapter 5 18
The Ideal Gas Law
V ∝ nTP-1
2/3/2003 OFB Chapter 5 19
The Ideal Gas Law
11
11
TnVPR =
22
22
TnVPR =
2/3/2003 OFB Chapter 5 20
Exercise 5-5At one point during its ascent, a weather balloon filled with helium at a volume of 1.0 × 104 L at 1.00 atm and 30oC reaches an altitude at which the temperature is -10oC yet the volume is unchanged. Compare the pressure at that point.
2/3/2003 OFB Chapter 5 21
The Ideal Gas Law
R universal gas constant ?for fixed V, P, and T, the number of n is fixed as well, and independent of the particular gas studied
nTPVR =
5K)mol)(273.1 (1.00)m N 10)(101.325xm 10 x (22.414 R
-233-3
=
K) 5mol)(273.1 (1.001atm)(22.414L)(
=
2/3/2003 OFB Chapter 5 22
Exercise 5-6
What mass of Hydrogen gas is needed to fill a weather balloon to a volume of 10,000 L at 1.00 atm and 30°C?
2/3/2003 OFB Chapter 5 23
Exercise 5-6
What mass of Hydrogen gas is needed to fill a weather balloon to a volume of 10,000 L at 1.00 atm and 30°C?
2/3/2003 OFB Chapter 5 24
Gas Density and Molar Mass
RTMmPV
nRTPV
=
=
2/3/2003 OFB Chapter 5 25
Gas Density and Molar Mass
Exercise 5-7Calculate the density of gaseous hydrogen at a pressure of 1.32 atm and a temperature of -45oC.
2/3/2003 OFB Chapter 5 26
Molar Mass
RTMmPV
nRTPV
=
=
2/3/2003 OFB Chapter 5 27
Exercise 5-8Fluorocarbons are compounds of fluorine and carbon. A 45.60 g sample of a gaseous fluorocarbon contains 7.94 g of carbon and 37.66 g of fluorine and occupies 7.40 L at STP (P = 1.00 atm and T = 273.15 K). Determine the approximate molar mass of the fluorocarbon and give its molecular formula.
2/3/2003 OFB Chapter 5 28
Exercise 5-8Fluorocarbons are compounds of fluorine and carbon. A 45.60 g sample of a gaseous fluorocarbon contains 7.94 g of carbon and 37.66 g of fluorine and occupies 7.40 L at STP (P = 1.00 atm and T = 273.15 K). Determine the approximate molar mass of the fluorocarbon and give its molecular formula.
1
11
mol g 138M
1atm273K x Kmol atm L 0.082
7.40L45.60g
−
−−
=
PRTdM =
F mol 1.982F g 19F 1mol x F g 37.66n
C mol 0.661C g 12C 1mol x C g 7.94n
F
C
=
=
=
=
Cpart 1mol 0.661 =÷
F parts 3mol 0.661 =÷
2/3/2003 OFB Chapter 5 29
Why use Volume for gases in chemical reaction calculations?The volume of a gas is easier to
measure than the mass of a gas.Exercise 5-9
Ethylene burns in oxygen:
C2H4(g) + 3 O2(g) → 2 CO2(g) + 2H2O(g)
A volume of 3.51 L of C2H4(g) at a temperature of 25oC and a pressure of 4.63 atm reacts completely with O2(g). The water vapor is collected at a temperature of 130oC and a pressure of 0.955 atm. Calculate the volume of the water vapor.
Chemical Calculations for Gases
2/3/2003 OFB Chapter 5 30
Exercise 5-9
Ethylene burns in oxygen:
C2H4(g) + 3 O2(g) → 2 CO2(g) + 2H2O(g)
A volume of 3.51 L of C2H4(g) at a temperature of 25oC and a pressure of 4.63 atm reacts completely with O2(g). The water vapor is collected at a temperature of 130oC and a pressure of 0.955 atm. Calculate the volume of the water vapor.
22
22
11
11
TnVP
TnVP
=
xV
403KT
atm 0.955P
298KT
3.51LV
4.63atmP
n 2nOH parts 2for HC1part
OH is 2Conditon andHC is 1Condition
OH
OH
OH
HC
HC
HC
0HHC
242
2
42
2
2
2
42
42
42
242
=
=
=
=
=
=
= L 46.0V OH2=
OHOH
OHOH
HCHC
HCHC
TnVP
TnVP
22
22
4242
4242 =
2/3/2003 OFB Chapter 5 31
Exercise 5-10
Hydrazine (N2H4), a rocket fuel, is prepared by the reaction of ammonia with a solution of sodium hypochlorite:
2 NH3(g) + NaOCl(aq) →
N2H4(aq) + NaCl(aq) + H2O(g)
What volume of gaseous ammonia at a temperature of 10oC and a pressure of 3.63 atm is required to produce 15.0 kg of hydrazine according to this equation.
2/3/2003 OFB Chapter 5 32
Exercise 5-10Hydrazine (N2H4), a rocket fuel, is prepared by the reaction of ammonia with a solution of sodium hypochlorite:
2 NH3(g) + NaOCl(aq) →
N2H4(aq) + NaCl(aq) + H2O(g)
What volume of gaseous ammonia at a temperature of 10oC and a pressure of 3.63 atm is required to produce 15.0 kg of hydrazineaccording to this equation.
342 NH mol 2HN mol 1nRTPV
==
( )
L 10 x 6.4V
3.63atm283K x 0.082
HN mol g 30.04HN g 10 x 152V
PTR
Mm
2V
PTR2n
PTRn
V
3NH
421-
423
NH
NH
NHNH
HN
HNNH
NH
NHNHHN
NH
NHNHNHNH
3
3
3
33
42
42
3
3
3342
3
333
3
=
=
=
==
PRT
Mm
PnRTV
==
2/3/2003 OFB Chapter 5 33
Mixtures of Gases
Dalton’s Law of Partial Pressures
The total pressure of a mixture of gases equals the sum of the partial pressures of the individual gases.
2/3/2003 OFB Chapter 5 34
Mole Fractions and Partial PressuresThe mole faction of a component in a mixture is define as the number of moles of the components that are in the mixture divided by the total number of moles present.
NBA
A
tot
AA
A
n...nnn
nnX
X A ofFraction Mole
+++==
=
totAA
tottot
AA
tot
A
tot
A
tottot
AA
tottot
AA
PXP
PnnPor
nn
PPor
RTnVPRTnVP
equations divideRTnVP
RTnVP
=
====
==
2/3/2003 OFB Chapter 5 35
Exercise 5-11
A solid hydrocarbon is burned in air in a closed container, producing a mixture of gases having a total pressure of 3.34 atm. Analysis of the mixture shows it to contain 0.340 g of water vapor, 0.792 g of carbon dioxide, 0.288 g of oxygen, 3.790 g of nitrogen, and no other gases. Calculate the mole fraction and partial pressure of carbon dioxide in this mixture.
2/3/2003 OFB Chapter 5 36
The Kinetic Theory of Gases
1. A pure gas consists of a large number of identical molecules separated by distances that are large compared with their size.2. The molecules of a gas are constantly moving in random directions with a distribution of speeds.
3. The molecules of a gas exert no forces on one another except during collisions, so that between collisions they move in straight lines with constant velocities.4. The collisions of the molecules with each other and with the walls of the container are elastic; no energy is lost during a collision.
2/3/2003 OFB Chapter 5 37
Temperature and Molecular Motion
Pressure ∝ (impulse per collision) x (rate of collisions with the walls)
•impulse pre collision
∝ momentum (m × u)•rate of collisions
∝ number of molecules per unit volume (N/V)•rate of collisions
∝ speed of molecules (u)
P ∝ (m × u) × [(N/V) × u]
2/3/2003 OFB Chapter 5 38
The Kinetic Theory of Gases
PV ∝ Nmu2
mean-square speed
M3RTu
mNM
RTumN31
NnNnumber sAvogadro'N if
nRTuNm31
nRTPV
uNm31PV
2
2
2
2
=
=
=∴
==
=∴
=
=
o
o
o
o
2/3/2003 OFB Chapter 5 39
Distribution of Molecular Speeds
M3RTu2 =
2/3/2003 OFB Chapter 5 40
Exercise 5-12
At a certain speed, the root-mean-square-speed of the molecules of hydrogen in a sample of gas is 1055 ms-1. Compute the root-mean square speed of molecules of oxygen at the same temperature.
2/3/2003 OFB Chapter 5 41
Exercise 5-12
At a certain speed, the root-mean-square-speed of the molecules of hydrogen in a sample of gas is 1055 ms-1. Compute the root-mean square speed of molecules of oxygen at the same temperature.
2/3/2003 OFB Chapter 5 42
Exercise 5-12
At a certain speed, the root-mean-square-speed of the molecules of hydrogen in a sample of gas is 1055 ms-1. Compute the root-mean square speed of molecules of oxygen at the same temperature.
Strategy
1. Find T for the H2 gas with a urms =1055 ms-1
2. Find urms of O2 at the same temperature
( )RMu
T HHrms
32
22
=
12
Orms
O
H2HO
rms
O
H2H
Orms
O
Orms
264.8ms32
(2)(1005)u
MMu
u
M3RMu
3Ru
M3RTu
2
2
222
2
22
2
2
2
−==
=
=
=
2/3/2003 OFB Chapter 5 43
Speed Distribution Curves
Maxwell-Boltzmann speed distribution
Temperature is a measure of the average kinetic energy of molecules when their speeds have Maxwell Boltzmann distribution. I.e., the molecules come to thermal equilibrium.
2/3/2003 OFB Chapter 5 44
Gaseous DiffusionRate of effusion of A ∝ uA
rms
factor enrichmentMM
M3RTM3RT
uu
B Eff of RateA Eff of Rate
A
B
B
A
Brms
Arms
==
=
=
Rate of effusion of B ∝ uBrms
2/3/2003 OFB Chapter 5 45
Exercise 5-13
A gas mixture contains equal numbers of molecules of N2and SF6. A small portion of it is passed through a gaseous diffusion apparatus. Calculate how many molecules of N2are present in the product of gas for every 100 molecules of SF6.
2/3/2003 OFB Chapter 5 46
Exercise 5-13
A gas mixture contains equal numbers of molecules of N2 and SF6. A small portion of it is passed through a gaseous diffusion apparatus. Calculate how many molecules of N2 are present in the product of gas for every 100 molecules of SF6.
A
B
MMfactor enrichment =
2.2814 x 2
19) x (632=
+=
2
6
N of molecules 2282.28 x SF molecules 100 =
2/3/2003 OFB Chapter 5 47
SkipSection 5-8Real Gases
2/3/2003 OFB Chapter 5 48
2/3/2003 OFB Chapter 5 49
Chapter 5The Gaseous State
Examples / Exercises– 5-1 thru 5-13
Problems– 34, 38, 48, 62, 70, 81