55
Gas Pressure

Gas Pressure

  • Upload
    bin

  • View
    45

  • Download
    3

Embed Size (px)

DESCRIPTION

Gas Pressure. Air Pressure. Pressure Units. Units of pressure: atmosphere (atm) Pa (N/m 2 , 101,325 Pa = 1 atm)Torr (760 Torr = 1 atm) bar (1.01325 bar = 1 atm) mm Hg (760 mm Hg = 1 atm) lb/in 2 (14.696 lb/in 2 = 1 atm) in Hg (29.921 in Hg = 1 atm). - PowerPoint PPT Presentation

Citation preview

Page 1: Gas Pressure

Gas Pressure

Page 2: Gas Pressure

Air Pressure

Page 3: Gas Pressure

Pressure Units

• Units of pressure: atmosphere (atm)

Pa (N/m2, 101,325 Pa = 1 atm)Torr (760 Torr = 1 atm)

bar (1.01325 bar = 1 atm)

mm Hg (760 mm Hg = 1 atm)

lb/in2 (14.696 lb/in2 = 1 atm)

in Hg (29.921 in Hg = 1 atm)

Page 4: Gas Pressure

Universal Gas Behavior

• Unlike solids and liquids, gas behavior is generally independent of chemical identity.

• Depends on four things only:– Absolute temperature– Pressure– Volume– Amount (moles)

Page 5: Gas Pressure

Kinetic Molecular Theory

• This theory presents physical properties of gases in terms of the motion of individual molecules.

• Kinetic Theory (in this class) will be based upon six assumptions:

• Average Kinetic Energy Kelvin Temperature

• Gas molecules are points separated by a great distance

• Particle volume is negligible compared to gas volume

• Gas molecules are in rapid random motion

• Gas collisions are perfectly elastic

• Gas molecules experience no attraction or repulsion

Page 6: Gas Pressure

Gas Behavior:Gases in a Box

• Insert 1 mole of gas into a fixed volume container. Then:

1. Gas expands to fill the container. Why?

2. The pressure becomes whatever value the gas laws dictate for that volume, mole, and temperature combination.

Page 7: Gas Pressure

Gas Behavior:Gases in a Piston

• Insert 1 mole of gas into a piston. Then:

1.Gas fills the piston. Why?

2.The piston changes volume until the pressure inside is equal to the pressure outside. Why?

Page 8: Gas Pressure

Understanding the Gas Laws

• Two keys to understanding the gas laws:– Understand which parameters are changing– Understand which are NOT changing

Page 9: Gas Pressure

Boyle’s Law• Pressure–Volume Law (Boyle’s Law):

Page 10: Gas Pressure

Boyle’s Law• Pressure–Volume Law (Boyle’s Law):

• The volume of a fixed amount of gas maintained at constant temperature is inversely proportional to the gas pressure.

Pressure1

Volume

XPV 11

Page 11: Gas Pressure

Charles’ Law

• Temperature–Volume Law (Charles’ Law):

Page 12: Gas Pressure

Charles’ Law• Temperature–Volume Law (Charles’ Law):

• The volume of a fixed amount of gas at constant pressure is directly proportional to the Kelvin temperature of the gas.

V T

XT

V

1

1

Page 13: Gas Pressure

Avogadro’s Law

• The Volume–Amount Law (Avogadro’s Law):

Page 14: Gas Pressure

Avogadro’s Law• The Volume–Amount Law (Avogadro’s Law):

• At constant pressure and temperature, the volume of a gas is directly

proportional to the number of moles of the gas present.

nV

Xn

V

1

1

Page 15: Gas Pressure

Collecting the Gas Laws

• Mathematically one can combine all of the statements we’ve made about gases.

• Two equivalent equations come from this:– Combined gas law– Ideal gas law

Page 16: Gas Pressure

Combined Gas Law• Combining the law gives:

• But if it equals a constant, then after any change it will still be equal to the constant:

• We write it this way:

• Nothing needs to be held constant now• Remember that anything that does stay constant can be

cancelled.

XTn

VP

1

1

11

2

22

1

11 Tn

VP

Tn

VP

21

4

44

3

33

2

22

1

11 X Tn

VP

Tn

VP

Tn

VP

Tn

VP

4321

Page 17: Gas Pressure

Ideal Gas Law

• This constant “X” is just a number.

• Units of (pressure * volume) / (moles * temp)

• That is, L·atm·K–1·mol–1

• Numerically, this constant has a value of R = 0.08206 L·atm·K–1·mol–1

Page 18: Gas Pressure

Ideal Gas Law

• The equation then becomes

We usually write it this way instead:

PV = nRT

RTn

VP

Page 19: Gas Pressure

STP

• Standard temperature: 273.15 K

• Standard pressure: 1 atm

Page 20: Gas Pressure

Ideal gas law vs. combined gas law

• Ideal gas law– Under unchanging conditions

• Combined gas law– Under changing conditions

Page 21: Gas Pressure

What is the volume of one mole of helium gas at STP?

22.4 L

What is the volume of one mole of argon gas at STP?

22.4 L

What is the volume of one mole of radon gas at STP?

22.4 L

Page 22: Gas Pressure

What is the density of one mole of helium gas at STP?

4.003 g / 22.4 L = 0.179 g/L

What is the volume of one mole of argon gas at STP?

39.948 g / 22.4 L = 1.78 g/L

What is the volume of one mole of radon gas at STP?

222 g / 22.4 L = 9.91 g/L

Page 23: Gas Pressure

What information would you need to calculate the molar mass of a gas?

• Mass / moles (m / n)• Enough information to get mass• P,V,T to use ideal gas law to get n

• What is the molar mass of a gas with a density of

1.342 g/L–1 at STP?

mole

g

mole

STPatL

L

g06.30

1

4.22

1

342.1

Page 24: Gas Pressure

Funky questions

• At what temperature do you have 0.1 moles/atm of helium in a 1 L pure helium sample?

• In one mole of chlorine gas at STP, how many Kelvins are there per liter?

K

KmolatmL

moles

Latm

nR

PVT 9.121

08206.01.0

11

L

K

KmolatmL

mol

atm

nR

P

V

T2.12

08206.01

1

Page 25: Gas Pressure

Gas-phase stoichiometry

• We have a new route to moles PV=nRT

• But we need to know first how two different gases behave when in the same space

Page 26: Gas Pressure

Gas Mixtures

• Two gases in the same container have the same volume—whatever the volume of the container is.

• Two gases in the same container have the same temperature—whatever the temperature is inside the container.

Page 27: Gas Pressure

Gas Mixtures

• Two gases in the same container do NOT have the same pressure.

• They have whatever pressure they would have if they were in the container alone.

• That is, solve PV=nRT for each gas in the mixture separately.

Page 28: Gas Pressure

Gas Mixtures

• The total pressure inside the container is the sum of the pressures of the individual gases.

• Dalton’s Law of Partial Pressures

i

itotal PP

Page 29: Gas Pressure

New Density Unit: Mole Fraction

• For a two-component system, the moles of components A and B can be represented by the mole fractions (XA and XB).

1 BABA

BB

BA

AA

XX

nn

nX

nn

nX

Page 30: Gas Pressure

Gas Stoichiometry

• In gas stoichiometry, for a constant temperature and pressure, volume is proportional to moles.

• Assuming no change in temperature and pressure, calculate the volume of O2 (in liters) required for the complete

combustion of 14.9 L of butane (C4H10):

2 C4H10(g) + 13 O2(g) 8 CO2(g) + 10 H2O(l)

Page 31: Gas Pressure

Molecular Speed

• It can be shown that:

• So then for neon:

M

RTvrms

3

Molar mass

hr

milesm

molg

KmolKJ

M

RTvrms 3000sec136000

00.4

298314.833

Page 32: Gas Pressure

Mean Molecular Speeds

Page 33: Gas Pressure

Collisions

• It can be shown that:

• A room temp gas collides billions of times per second

• The mean free path is less than 100 nm.

kT

Pvz mean

P

kT

2

Collision frequency Mean free path

Page 34: Gas Pressure

Maxwell speed distribution curves.

Page 35: Gas Pressure

Same Behavior vs. Different Behavior

• Most gas behaviors are based upon comparisons of their relative energies (temperatures)– Same temperature = same behavior

• Some gas behaviors are based upon comparisons of their relative speeds– Same speed = same behavior

Page 36: Gas Pressure

• Diffusion is the mixing of different gases by random molecular motion and collision.

Graham’s Law

Page 37: Gas Pressure

Graham’s Law

• Effusion is when gas molecules escape without collision, through a tiny hole into a vacuum.

Page 38: Gas Pressure

Graham’s Law

• Graham’s Law: Rate of effusion is proportional to its rms speed, vrms.

• For two gases at same temperature and pressure:

M

RTRate rms

3 v

Rate1

Rate2

M2

M1

M2

M1

Page 39: Gas Pressure

Behavior of Real Gases

• Test of ideal gasbehavior.

• Z = PV/RT

Compressibility factor

This plot assumes room temperature.

Page 40: Gas Pressure

Real Gases

• All the assumptions of kinetic molecular theory break down when explored in sufficient detail.

• Two assumptions break down first:– The volume of gas molecules is negligible– There are no attractive or repulsive forces

between molecules

Page 41: Gas Pressure

Non-negligible volumes

• The volume of molecules affects pressure-volume behavior more than temperature-pressure behavior.

• For a given small volume, the pressure will be higher than the ideal gas suggests..

Page 42: Gas Pressure

Behavior of Real Gases

• Test of ideal gasbehavior.

Volume non-idealities seen here!

Page 43: Gas Pressure

Non-negligible interactions

• The long-range interactions of particles are attractions, not repulsions.

• Thus a real gas sample takes up less space than the ideal gas law suggests, when the molecules are not crowded together.

• This effect fades as molecules move faster.

Page 44: Gas Pressure

Behavior of Real Gases

• Test of ideal gasbehavior.

Attractive force non-idealities seen here!

Page 45: Gas Pressure

Behavior of Real Gases• Corrections for non-ideality require a non-ideal gas

law. The van der Waals equation is one of them:

nRTbnVV

naP –

2

2

IntermolecularAttractions

ExcludedVolume

Page 46: Gas Pressure

Van der Waals Constants

Gas a

(L2 atm / mole2)

b

(L / mole)

Helium (He) 0.03412 0.02370

Ammonia (NH3)

4.170 0.03707

Hydrogen (H2) 0.2444 0.02661

n-octane 37.32 0.2368

Water 5.464 0.03049

Carbon dioxide 3.592 0.04267

Page 47: Gas Pressure

Other gas laws

• van der Waals:

• Peng-Robinson:

• Redlich-Kwong:

B

nV

nV

T

A

BnVRT

P

nV

nV

nV

nVRT

P

nV

RT

a

bnVRT

P

Page 48: Gas Pressure

Unifying the Gas Laws

• Under normal temperatures you can liquefy a gas simply by raising the pressure

• Above a certain critical temperature (Tc) you cannot liquefy a gas under any pressure. The pressure and volume of that “last” liquid are Pc and Vc

Page 49: Gas Pressure

Critical Constants

Species Tc (K) Pc (atm) Vc (L)

Helium 5.195 2.2452 0.0578

Ammonia 405.3 109.84 0.0725

Water 647.126 217.66 0.05595

Page 50: Gas Pressure

“Critical” adjustments

• Now we stop using temperature (and pressure and volume) in the gas laws.

• Instead we write the reduced temperature (TR) as a fraction of the critical temperature (Tc).

• That is TR = T / Tc

Page 51: Gas Pressure

Compressibility factor plots redone

Page 52: Gas Pressure

Atmosphere

Page 53: Gas Pressure

Smog (Inversions)

32

2

OOO

ONOhNO

Brownish haze

Page 54: Gas Pressure

Acid Rain

4223

322

22

22

SOHOHSO

SOOSO

SOOS

Page 55: Gas Pressure

Global Warming