chapter 5 the gas laws. pressure force per unit area. gas molecules fill container. molecules...

41
Chapter 5 The Gas Laws

Upload: cornelius-king

Post on 11-Jan-2016

218 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Chapter 5Chapter 5

The Gas LawsThe Gas Laws

Page 2: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

PressurePressure

Force per unit area. Gas molecules fill container. Molecules move around and hit

sides. Collisions are the force. Container has the area. Measured with a barometer.

Force per unit area. Gas molecules fill container. Molecules move around and hit

sides. Collisions are the force. Container has the area. Measured with a barometer.

Page 3: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

BarometerBarometer The pressure of

the atmosphere at sea level will hold a column of mercury 760 mm Hg.

1 atm = 760 mm Hg

The pressure of the atmosphere at sea level will hold a column of mercury 760 mm Hg.

1 atm = 760 mm Hg

1 atm Pressure

760 mm Hg

Vacuum

Page 4: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ManometerManometer

Gas

h

Column of mercury to measure pressure.

h is how much lower the pressure is than outside.

Column of mercury to measure pressure.

h is how much lower the pressure is than outside.

Page 5: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ManometerManometer

h is how much higher the gas pressure is than the atmosphere.

h is how much higher the gas pressure is than the atmosphere.

h

Gas

Page 6: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Units of pressureUnits of pressure 1 atmosphere = 760 mm Hg 1 mm Hg = 1 torr 1 atm = 101,235 Pascals = 101.325

kPa Can make conversion factors from

these.

1 atmosphere = 760 mm Hg 1 mm Hg = 1 torr 1 atm = 101,235 Pascals = 101.325

kPa Can make conversion factors from

these.

Page 7: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

The Gas LawsThe Gas Laws

Boyle’s Law Pressure and volume are inversely

related at constant temperature. PV= k As one goes up, the other goes down. P1V1 = P2 V2

Boyle’s Law Pressure and volume are inversely

related at constant temperature. PV= k As one goes up, the other goes down. P1V1 = P2 V2

Page 8: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Charles’s LawCharles’s Law

Volume of a gas varies directly with the absolute temperature at constant pressure.

V = kT (if T is in Kelvin)

V1 = V2

T1 = T2

Volume of a gas varies directly with the absolute temperature at constant pressure.

V = kT (if T is in Kelvin)

V1 = V2

T1 = T2

Page 9: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Avogadro's LawAvogadro's Law

At constant temperature and pressure, the volume of gas is directly related to the number of moles.

V = k n (n is the number of moles)

V1 = V2

n1 n2

At constant temperature and pressure, the volume of gas is directly related to the number of moles.

V = k n (n is the number of moles)

V1 = V2

n1 n2

Page 10: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Gay- Lussac LawGay- Lussac Law

At constant volume, pressure and absolute temperature are directly related.

P = k T

P1 = P2

T1 = T2

At constant volume, pressure and absolute temperature are directly related.

P = k T

P1 = P2

T1 = T2

Page 11: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Combined Gas LawCombined Gas Law If the moles of gas remains

constant, use this formula and cancel out the other things that don’t change.

P1 V1 = P2 V2

. T1 T2

If the moles of gas remains constant, use this formula and cancel out the other things that don’t change.

P1 V1 = P2 V2

. T1 T2

Page 12: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Ideal Gas LawIdeal Gas Law

PV = nRT V = 22.41 L at 1 atm, 0ºC, n = 1

mole, what is R? R is the ideal gas constant. R = 0.08206 L atm/ mol K Tells you about a gas is NOW. The other laws tell you about a gas

when it changes.

PV = nRT V = 22.41 L at 1 atm, 0ºC, n = 1

mole, what is R? R is the ideal gas constant. R = 0.08206 L atm/ mol K Tells you about a gas is NOW. The other laws tell you about a gas

when it changes.

Page 13: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Ideal Gas LawIdeal Gas Law

An equation of state. Independent of how you end up

where you are at. Does not depend on the path.

Given 3 you can determine the fourth.

An equation of state. Independent of how you end up

where you are at. Does not depend on the path.

Given 3 you can determine the fourth.

Page 14: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Ideal Gas LawIdeal Gas Law

An ideal gas is a hypothetical substance

Think of it as a limit. Gases only approach ideal behavior at

low pressure (< 1 atm) and high temperature.

Use the laws anyway, unless told to do otherwise. They give good estimates.

An ideal gas is a hypothetical substance

Think of it as a limit. Gases only approach ideal behavior at

low pressure (< 1 atm) and high temperature.

Use the laws anyway, unless told to do otherwise. They give good estimates.

Page 15: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Gas Density and Molar Mass

Gas Density and Molar Mass

D = m/V Let M stand for molar mass M = m/n n= PV/RT M = m

PV/RT M = mRT = m RT = DRT

PV V P P

D = m/V Let M stand for molar mass M = m/n n= PV/RT M = m

PV/RT M = mRT = m RT = DRT

PV V P P

Page 16: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Gases and StoichiometryGases and Stoichiometry

Reactions happen in moles At Standard Temperature and

Pressure (STP, 0ºC and 1 atm) 1 mole of gas occuppies 22.42 L.

If not at STP, use the ideal gas law to calculate moles of reactant or volume of product.

Reactions happen in moles At Standard Temperature and

Pressure (STP, 0ºC and 1 atm) 1 mole of gas occuppies 22.42 L.

If not at STP, use the ideal gas law to calculate moles of reactant or volume of product.

Page 17: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ExamplesExamples

Mercury can be achieved by the following reaction

What volume of oxygen gas can be produced from 4.10 g of mercury (II) oxide at STP?

At 400.ºC and 740 torr?

Mercury can be achieved by the following reaction

What volume of oxygen gas can be produced from 4.10 g of mercury (II) oxide at STP?

At 400.ºC and 740 torr?

→HgO Hg(l) + O (g) heat

2

Page 18: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Dalton’s LawDalton’s Law

The total pressure in a container is the sum of the pressure each gas would exert if it were alone in the container.

The total pressure is the sum of the partial pressures.

PTotal = P1 + P2 + P3 + P4 + P5 ...

For each P = nRT/V

The total pressure in a container is the sum of the pressure each gas would exert if it were alone in the container.

The total pressure is the sum of the partial pressures.

PTotal = P1 + P2 + P3 + P4 + P5 ...

For each P = nRT/V

Page 19: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Dalton's LawDalton's Law

PTotal = n1RT + n2RT + n3RT +...

V V V In the same container R, T and V are the

same.

PTotal = (n1+ n2 + n3+...)RT

V

PTotal = (nTotal)RT

V

PTotal = n1RT + n2RT + n3RT +...

V V V In the same container R, T and V are the

same.

PTotal = (n1+ n2 + n3+...)RT

V

PTotal = (nTotal)RT

V

Page 20: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

The mole fractionThe mole fraction

Ratio of moles of the substance to the total moles.

symbol is Greek letter chi

= n1 = P1

nTotal PTotal

Ratio of moles of the substance to the total moles.

symbol is Greek letter chi

= n1 = P1

nTotal PTotal

Page 21: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ExamplesExamples

3.50 L

O2

1.50 L

N2

2.70 atm When these valves are opened, what is

each partial pressure and the total pressure?

When these valves are opened, what is each partial pressure and the total pressure?

4.00 L

CH4

4.58 atm 0.752 atm

Page 22: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Vapor PressureVapor Pressure

Water evaporates! When that water evaporates, the

vapor has a pressure. Gases are often collected over

water so the vapor. pressure of water must be subtracted from the total pressure.

It must be given.

Water evaporates! When that water evaporates, the

vapor has a pressure. Gases are often collected over

water so the vapor. pressure of water must be subtracted from the total pressure.

It must be given.

Page 23: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ExampleExample

N2O can be produced by the following

reaction

what volume of N2O collected over

water at a total pressure of 94 kPa and 22ºC can be produced from 2.6 g of NH4NO3? ( the vapor pressure of

water at 22ºC is 21 torr)

N2O can be produced by the following

reaction

what volume of N2O collected over

water at a total pressure of 94 kPa and 22ºC can be produced from 2.6 g of NH4NO3? ( the vapor pressure of

water at 22ºC is 21 torr)

NH NO NO (g) + 2H O4 heat

23 2( ) ( )s l⏐ →⏐

Page 24: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Kinetic Molecular TheoryKinetic Molecular Theory

Theory tells why the things happen. explains why ideal gases behave the

way they do. Assumptions that simplify the theory,

but don’t work in real gases. The particles are so small we can ignore

their volume. The particles are in constant motion and

their collisions cause pressure.

Theory tells why the things happen. explains why ideal gases behave the

way they do. Assumptions that simplify the theory,

but don’t work in real gases. The particles are so small we can ignore

their volume. The particles are in constant motion and

their collisions cause pressure.

Page 25: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Kinetic Molecular TheoryKinetic Molecular Theory

The particles do not affect each other, neither attracting or repelling.

The average kinetic energy is proportional to the Kelvin temperature.

Appendix 2 shows the derivation of the ideal gas law and the definition of temperature.

We need the formula KE = 1/2 mv2

The particles do not affect each other, neither attracting or repelling.

The average kinetic energy is proportional to the Kelvin temperature.

Appendix 2 shows the derivation of the ideal gas law and the definition of temperature.

We need the formula KE = 1/2 mv2

Page 26: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

What it tells usWhat it tells us

(KE)avg = 3/2 RT This the meaning of temperature. u is the particle velocity. u is the average particle velocity. u 2 is the average particle velocity

squared. the root mean square velocity is

u 2 = urms

(KE)avg = 3/2 RT This the meaning of temperature. u is the particle velocity. u is the average particle velocity. u 2 is the average particle velocity

squared. the root mean square velocity is

u 2 = urms

Page 27: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Combine these two equations

Combine these two equations

(KE)avg = NA(1/2 mu 2 )

(KE)avg = 3/2 RT

(KE)avg = NA(1/2 mu 2 )

(KE)avg = 3/2 RT

Page 28: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Combine these two equations

Combine these two equations

(KE)avg = NA(1/2 mu 2 ) (KE)avg = 3/2 RT Where M is

the molar mass in kg/mole, and R has the units 8.3145 J/Kmol.

The velocity will be in m/s

(KE)avg = NA(1/2 mu 2 ) (KE)avg = 3/2 RT Where M is

the molar mass in kg/mole, and R has the units 8.3145 J/Kmol.

The velocity will be in m/s

u = 3RT

Mrms

Page 29: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Range of velocitiesRange of velocities

The average distance a molecule travels before colliding with another is called the mean free path and is small (near 10-7)

Temperature is an average. There are molecules of many speeds in the average.

Shown on a graph called a velocity distribution

The average distance a molecule travels before colliding with another is called the mean free path and is small (near 10-7)

Temperature is an average. There are molecules of many speeds in the average.

Shown on a graph called a velocity distribution

Page 30: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

num

ber

of p

arti

cles

Molecular Velocity

273 K

Page 31: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

num

ber

of p

arti

cles

Molecular Velocity

273 K

1273 K

Page 32: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

num

ber

of p

arti

cles

Molecular Velocity

273 K

1273 K

1273 K

Page 33: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

VelocityVelocity

Average increases as temperature increases.

Spread increases as temperature increases.

Average increases as temperature increases.

Spread increases as temperature increases.

Page 34: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

EffusionEffusion

Passage of gas through a small hole, into a vacuum.

The effusion rate measures how fast this happens.

Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.

Passage of gas through a small hole, into a vacuum.

The effusion rate measures how fast this happens.

Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.

Page 35: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

EffusionEffusion Passage of gas through a small

hole, into a vacuum. The effusion rate measures how

fast this happens. Graham’s Law the rate of effusion

is inversely proportional to the square root of the mass of its particles.

Passage of gas through a small hole, into a vacuum.

The effusion rate measures how fast this happens.

Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.

Rate of effusion for gas 1

Rate of effusion for gas 2=

MM

Page 36: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

DerivingDeriving

The rate of effusion should be proportional to urms

Effusion Rate 1 = urms 1

Effusion Rate 2 = urms 2

The rate of effusion should be proportional to urms

Effusion Rate 1 = urms 1

Effusion Rate 2 = urms 2effusion rate 1

effusion rate 2

u 1

u 2

3RT

M

3RT

M2

M

Mrms

rms

1= = =

Page 37: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

DiffusionDiffusion

The spreading of a gas through a room.

Slow considering molecules move at 100’s of meters per second.

Collisions with other molecules slow down diffusions.

Best estimate is Graham’s Law.

The spreading of a gas through a room.

Slow considering molecules move at 100’s of meters per second.

Collisions with other molecules slow down diffusions.

Best estimate is Graham’s Law.

Page 38: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

ExamplesExamples A compound effuses through a porous cylinder 3.20 time faster than helium. What is it’s molar mass?

If 0.00251 mol of NH3 effuse through a

hole in 2.47 min, how much HCl would effuse in the same time?

A sample of N2 effuses through a hole in

38 seconds. what must be the molecular weight of gas that effuses in 55 seconds under identical conditions?

A compound effuses through a porous cylinder 3.20 time faster than helium. What is it’s molar mass?

If 0.00251 mol of NH3 effuse through a

hole in 2.47 min, how much HCl would effuse in the same time?

A sample of N2 effuses through a hole in

38 seconds. what must be the molecular weight of gas that effuses in 55 seconds under identical conditions?

Page 39: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

DiffusionDiffusion

The spreading of a gas through a room.

Slow considering molecules move at 100’s of meters per second.

Collisions with other molecules slow down diffusions.

Best estimate is Graham’s Law.

The spreading of a gas through a room.

Slow considering molecules move at 100’s of meters per second.

Collisions with other molecules slow down diffusions.

Best estimate is Graham’s Law.

Page 40: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Real GasesReal Gases

Real molecules do take up space and they do interact with each other (especially polar molecules).

Need to add correction factors to the ideal gas law to account for these.

Real molecules do take up space and they do interact with each other (especially polar molecules).

Need to add correction factors to the ideal gas law to account for these.

Page 41: Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force

Volume CorrectionVolume Correction

The actual volume free to move in is less because of particle size.

More molecules will have more effect.

Pressure Correction Because the molecules are attracted to each

other, the pressure on the container will be less than ideal

depends on the number of molecules per liter.

The actual volume free to move in is less because of particle size.

More molecules will have more effect.

Pressure Correction Because the molecules are attracted to each

other, the pressure on the container will be less than ideal

depends on the number of molecules per liter.