Gases Kinetic Theory of Gases, Gas Laws, Ideal Gases, Partial Pressures, Graham’s Law of Effusion.
Chapter 14 The Ideal Gas Law and Kinetic Theorysites.millersville.edu/tgilani/pdf/PHYS...
Transcript of Chapter 14 The Ideal Gas Law and Kinetic Theorysites.millersville.edu/tgilani/pdf/PHYS...
Chapter 14
The Ideal Gas Law and Kinetic Theory
14.1 Molecular Mass, the Mole, and Avogadro’s Number
To facilitate comparison of the mass of one atom with another, a mass scaleknow as the atomic mass scale has been established.
kg106605.1u 1 27−×=
The atomic mass is given in atomicmass units. For example, a Li atom has a mass of 6.941u.
The unit is called the atomic mass unit (symbol u). The reference element is chosen to be the most abundant isotope of carbon, which is called carbon-12. Carbon-12 has exactly 12 atomic mass units.
14.1 Molecular Mass, the Mole, and Avogadro’s Number
One gram-mole of a substance contains as many particles as there are atoms in 12 grams of the isotope carbon-12.
123 mol10022.6 −×=AN
ANNn =
number ofmoles
number ofatoms
The number of atoms per mole is known as Avogadro’s number, NA.
14.1 Molecular Mass, the Mole, and Avogadro’s Number
ANmNm
nparticle
particle=
The mass per mole (in g/mol) of a substancehas the same numerical value as the atomic or molecular mass of the substance (in atomicmass units).
ANNn =
moleper Massmn =
For example Hydrogen has an atomic mass of 1.00794 g/mol, while the mass of a single hydrogen atom is 1.00794 u.
14.1 Molecular Mass, the Mole, and Avogadro’s Number
Example: The Hope Diamond and the Rosser Reeves RubyThe Hope diamond (44.5 carats) is almost pure carbon. The RosserReeves ruby (138 carats) is primarily aluminum oxide (Al2O3). Onecarat is equivalent to a mass of 0.200 g. Determine (a) the number of carbon atoms in the Hope diamond and
(b) the number of Al2O3 molecules in the ruby.
(a)
AnNN =
( ) ( ) ( )[ ]molg12
carat 1g 200.0carats 5.44=
moleper Massmn =
0.74 moles
( )( )123 mol10022.6mol 74.0 −×=N
atoms1046.4 23×=N
14.1 Molecular Mass, the Mole, and Avogadro’s Number
(b)
moles 271.0=n
atoms1063.1 23×
moleper Massmn =
AnNN =
( ) ( ) ( )[ ]
( ) ( )molg96.101
carat 1g 200.0carats 138
99.15398.262
+
=
the number of Al2O3 molecules in the ruby.
( )( )123 mol10022.6mol 271.0 −×== AnNN
14.2 The Ideal Gas Law
The condition of low density means that the molecules are so far apart that they do not interact except during collisions, which are effectively elastic.
TP ∝
At constant volume the pressureis proportional to the temperature.
An ideal gas is an idealized model for real gases that have sufficiently low densities.
• No interactions• All collisions are elastic
14.2 The Ideal Gas Law
At constant temperature, the pressure is inversely proportional to the volume.
VP 1∝
The pressure is also proportionalto the amount of gas.
nP ∝
VnTP ∝
14.2 The Ideal Gas Law
The absolute pressure of an ideal gas is directly proportional to the Kelvintemperature and the number of moles of the gas and is inversely proportionalto the volume of the gas.
VnRTP =
nRTPV =
( )KmolJ31.8 ⋅=R
THE IDEAL GAS LAW
VnTP ∝
14.2 The Ideal Gas Law
nRTPV =
ANNn =
( ) KJ1038.1mol106.022
KmolJ31.8 23123
−− ×=
×⋅
==AN
Rk
TNRNPV
A
=
NkTPV =Boltzmann Constant
nRTPV = NkTPV =OR
No. of moles No. of particles
14.2 The Ideal Gas Law
Example: Oxygen in the LungsIn the lungs, the respiratory membrane separates tiny sacs of air(pressure 1.00x105Pa) from the blood in the capillaries. These sacsare called alveoli. The average radius of the alveoli is 0.125 mm, andthe air inside contains 14% oxygen. Assuming that the air behaves asan ideal gas at 310 K (body temperature), find the number of oxygen molecules in one ofthese sacs.
NkTPV =
air of molecules109.1 14×
kTPVN =
( ) ( )[ ]( )( )K 310KJ1038.1
m10125.0Pa1000.123
33345
−
−
×××
=πN
? sac onein oxygen of molecules ofNumber =
( ) ( )14.0109.1 14 ×× molecules107.2 13×
14.2 The Ideal Gas Law
Consider a sample of an ideal gas that is taken from an initial to a finalstate, with the amount of the gas remaining constant.
nRTPV =
i
ii
f
ff
TVP
TVP
=
constant == nRT
PV
Constant T, constant n: iiff VPVP = Boyle’s law
Constant P, constant n:i
i
f
f
TV
TV
= Charles’ law
14.3 Kinetic Theory of Gases
• As a result, the atoms and molecules have different speeds.
• The particles are in constant, random motion, colliding with each other and with the walls of the container.
• Each collision changes the particle’s speed.
14.3 Kinetic Theory of Gases
KINETIC THEORY
( ) ( )Lmv
vLmvmv 2
2 force Average −
=+−−
=
∑ = maF
( )t
mvtvmF
∆∆
=∆∆
=∑
𝑎𝑎 =∆𝑣𝑣∆𝑡𝑡
collisions successivebetween Timemomentum Initial-momentum Final force Average =
=∆𝑝𝑝∆𝑡𝑡
14.3 Kinetic Theory of Gases
LmvF
2
=
For a single molecule, the magnitude of average force is:
For N molecules, the average force is:
=
LvmNF
2
3 root-mean-squarespeed
=== 3
2
2 3 LvmN
LF
AFP
volume
Since 𝑃𝑃 = 𝐹𝐹𝐴𝐴
and A = L2
14.3 Kinetic Theory of Gases
=
VvmNP
2
3
( ) ( )221
322
31
rmsrms mvNmvNPV ==
NkT KE
kTmvrms 232
21KE ==
= 3
2
3 LvmNP
𝑁𝑁𝑁𝑁𝑁𝑁 =23𝑁𝑁(𝐾𝐾𝐾𝐾) 𝐾𝐾𝐾𝐾 =
32𝑁𝑁𝑁𝑁
14.3 Kinetic Theory of Gases
kTmvrms 232
21KE ==
THE INTERNAL ENERGY OF A MONATOMIC IDEAL GAS
nRTkTNU 23
23 ==
14.3 Kinetic Theory of Gases
Example: The Speed of Molecules in AirAir is primarily a mixture of nitrogen N2 molecules (molecular mass 28.0 u) and oxygen O2 molecules (molecular mass 32.0 u). Assumethat each behaves as an ideal gas and determine the rms speedsof the nitrogen and oxygen molecules when the temperature of the airis 293 K.
kTmvrms 232
21 = m
kTvrms3
=
For Nitrogen
123 mol106.022molg0.28
−×=m
sm511=rmsv
kg1065.4g1065.4 2623 −− ×=×=
mkTvrms
3= ( )( )
kg1065.4K293KJ1038.13
26
23
−
−
××
=
For Oxygen sm478=rmsv
Problem: 3
Since the sample has a mass of 135 g, the mass per mole is
135 g5.00 mol
= 27.0 g/mol
The periodic table of the elements
. A mass of 135 g of an element is known to contain 30.1 x 1023 atoms. What is the unknown element?
Aluminum
𝑛𝑛 =𝑁𝑁𝑁𝑁𝐴𝐴
=30.1 × 1023
6.022 × 10235 moles
Atomic mass of the substance is 27.0 u
Problem: 16
Therefore, the mass m of helium in the blimp is,
A Goodyear blimp typically contains 5400 m3 of helium (He) at an absolute pressure of 1.10 x 105 Pa. The temperature of the helium is 280 K. What is the mass (in kg) of the helium in the blimp?
𝑛𝑛 =𝑃𝑃𝑃𝑃𝑅𝑅𝑁𝑁
PV = nRT
=(1.1 × 105𝑃𝑃𝑎𝑎)(5400 𝑚𝑚3)8.31 𝐽𝐽/(𝑚𝑚𝑚𝑚𝑚𝑚.𝐾𝐾)(280 𝐾𝐾) 2.55 × 105 𝑚𝑚𝑚𝑚𝑚𝑚𝑚𝑚𝑚𝑚
From Periodic table 1 mole of Helium is 4.0026 g
𝑚𝑚 = (2.55 × 105𝑚𝑚𝑚𝑚𝑚𝑚)(4.0026𝑔𝑔𝑚𝑚𝑚𝑚𝑚𝑚
)
= 1.0 × 106𝑔𝑔
1.0 × 103 𝑁𝑁𝑔𝑔
Problem: 39
ionosphere earth's surface3T T=
( )( )
ionosphererms ionosphere ionosphere
earth's surfaceearth's surfacerms earth's surface
3
3 1.733
kTv Tm
TkTvm
= = = =
Dividing the first equation by the second and using the fact that
An oxygen molecule is moving near the earth's surface. Another oxygen molecule is moving in the ionosphere (the uppermost part of the earth's atmosphere) where the Kelvin temperature is 3.00 times greater. Determine the ratio of the translational rmsspeed in the ionosphere to that near the earth's surface.
kTmvrms 232
21 =
mkT
v ionosphereionosphererms
3)( =
and
mkTv earth
earthrms3)( =
Reading For Next ClassCh. 16 & Ch 17
HWAssignment#4 on WileyPlus is due by Thursday, June 8th
For PracticeCh. 14
FOC: 1, 3, 6, 7 & 8. Problems 13, 16, & 58.