Physical Chemistry I(TKK-2246)
13/14 Semester 2
Instructor: Rama OktavianEmail: [email protected] Hr.: M.13-15, Tu. 13-15, W. 13-15, Th. 13-15, F. 09-11
Outlines
1. Gas structure
2. Kinetic theory of gas
3. Calculation of the gas pressure
4. Dalton’s law in kinetic theory of gas
Learning check
Molar mass of gas
In an experiment to measure the molar mass of a gas, 250 cm3
of the gas was confined in a glass vessel. The pressure was 152
Torr at 298 K and, after correcting for buoyancy effects, the mass
of the gas was 33.5 mg. What is the molar mass of the gas?
Learning check
Dalton’s partial pressure
A gas mixture consists of 320 mg of methane, 175 mg of argon,
and 225 mg of neon. The partial pressure of neon at 300 K is 8.87
kPa. Calculate
(a) the volume and (b) the total pressure of the mixture.
Learning check
Dalton’s partial pressure
A vessel of volume 22.4 dm3 contains 2.0 mol H2and 1.0 mol N2 at 273.15 K
initially. All the H2 reacted with sufficient N2 to form NH3. Calculate
the partial pressures and the total pressure of the final mixture.
Gas structure
1. In gases, the particles are very spread out
2. They are moving very quickly in different directions
3. They are not arranged in any pattern
4. They are changing places all of the time.
Gas structure
1. A gas will fill the whole volume of its container.
2. A gas is easily compressed.
3. The speed of the particles in a gas increases as the temperature increases
Kinetic theory of gases
• Kinetic theory of gas observes molecular motion in gases
• In the kinetic model of gases we assume that the only contribution to the energy of
the gas is from the kinetic energies of the molecules
The pressure that a gas exerts is caused by the collisions of its molecules with the walls of the container.
Kinetic theory of gases1. Gases are made of tiny particles far apart relative to their size:
Volume occupied by the molecules is inconsequential
Volume is mostly space
Explains why gases are compressible
Kinetic theory of gases
2. Gas particles are in continuous, rapid, random motion
As a result there are collisions with other molecules or with the wall of the container
Creates pressure
Increase in temperature increases the movement of the molecules and thus the pressure exerted by the gas
Kinetic theory of gases
3. There are no attractive forces between molecules under normal conditions of temperature and pressure
Gas molecules are moving too fastGas molecules are too far apartIntermolecular forces are too weak
Kinetic theory of gases
4. Collisions between gas particles and between particles and container walls are elastic collisions.
Collisions in which there is no net loss of total kinetic energy
Kinetic energy can be transferred between two particles during collisions
Total kinetic energy remains the same as long as temperature remains the same
Kinetic theory of gases
5. All gases at the same temperature have the same average kinetic energy. The energy is proportional to the absolute temperature.
Absolute temperature = Kelvin temp scale
Ke = ½ mv2
Ke = the kinetic energy m = mass v = the velocity
Kinetic theory of gasesPressure and molecular speed relation
2
31 nMcpV (1)
Where M = mNA, the molar mass of the molecules, and c is the root mean square speed of the molecules, the square root of the mean of the squares of the speeds, v, of the molecules:
212vc (2)
Kinetic theory of gasesPressure and molecular speed relation
Justification
Consider the movement of gas
the momentum before collision isxmv
the momentum after collision isxmv
the change in momentum is the difference between final and initial momentum
xmv2
Kinetic theory of gasesPressure and molecular speed relation
JustificationThe distance that molecule can travel along the x-axis in an interval ∆t is written as
if the wall has area A, then all the particles in a volume
tvx
tAv x will reach the wall
Kinetic theory of gasesPressure and molecular speed relation
JustificationThe number density of particles is
where n is the total amount of molecules in the container of volume V and NA is Avogadro’s constant
VnN A
The number of molecules in the volume tAv x
VnN A x tAv x
Kinetic theory of gasesPressure and molecular speed relation
JustificationAt any instant, half the particles are moving to the right and half are moving to the left
Therefore the number of molecules will become
VtAvnN xA 21
The total momentum change within interval Δt is
VtAvnN xA
2
x xmv2
Kinetic theory of gasesPressure and molecular speed relation
JustificationThe total momentum change within interval Δt is
VtAvnN xA
2
x xmv2
VtnMAv
VtvnmAN xxA
22
Where M = mNA
Kinetic theory of gasesPressure and molecular speed relation
JustificationRate of change of momentum can be written as total momentum divided by time interval
VnMAv x
2
rate of change of momentum is equal to the force (by Newton’s second law of motion)
Kinetic theory of gasesPressure and molecular speed relation
Justificationthe pressure, the force divided by the area, is
rate of change of momentum is equal to the force (by Newton’s second law of motion)
Not all the molecules travel with the same velocity, so the detected pressure, p, is the average (denoted ) of the quantity just calculated
...
Kinetic theory of gasesPressure and molecular speed relation
JustificationTo write an expression of the pressure in terms of the root mean square speed, c, we begin by writing the speed of a single molecule, v, as
2222zyx vvvv
212vc 22222zyx vvvvc
because the molecules are moving randomly, all three averages are the same, it follows
22 3 xvc
Kinetic theory of gasesPressure and molecular speed relation
Justification 22 3 xvc
22
31 cvx
2
31 nMcpV
Kinetic theory of gasesPressure and molecular speed relation
2
31 nMcnRT
Using Boyle’s Law and ideal gas Law
the root mean square speed of the molecules in a gas at a temperature T must be
the higher the temperature, the higher the root mean square speed of the molecules, and, at a given temperature, heavy molecules travel more slowly than light molecules
Kinetic theory of gasesPressure and kinetic energy relation
2
21 mc
Kinetic energy of molecule is defined as
2
31 nMcpV M = mNA
AnNpV32
N = nNA
NpV32
Kinetic theory of gasesPressure and kinetic energy relation
NnRT32
Using Boyle’s Law and ideal gas Law
ANRT
23
kT23
k is Boltzmann constant
k = 1.3806488 × 10-23 m2 kg s-2 K-1
Kinetic theory of gasesThe Speed of Molecules in Air
Air is primarily a mixture of nitrogen N2 (molecular mass = 28.0 g/mol) and oxygen O2 (molecular mass = 32.0 g/mol). Assume that each behaves as an ideal gas and determine the speeds of the nitrogen and oxygen molecules when the temperature of the air is 293 K and determine the kinetic energy contained in that molecule
kT23
Kinetic theory of gasesDalton’s law of partial pressure
In a mixture of gases the total pressure is the sum of the forces per unit area produced by the impacts of each kind of molecule on a wall of a container