gases dr. ron rusay fall 2007 © copyright 2007 r.j. rusay

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Gases Gases Dr. Ron Rusay Dr. Ron Rusay Fall 2007 Fall 2007 © Copyright 2007 R.J. Rusay © Copyright 2007 R.J. Rusay

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Page 1: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

GasesGases

Dr. Ron RusayDr. Ron Rusay

Fall 2007Fall 2007

© Copyright 2007 R.J. Rusay© Copyright 2007 R.J. Rusay

Page 2: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

GasesGases

Uniformly fill any container.Uniformly fill any container. Exert pressure on its surroundings. Exert pressure on its surroundings. Mix completely with other gasesMix completely with other gases

Page 3: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Gases: Gases: Pressure, Mass, Volume, TemperaturePressure, Mass, Volume, Temperature

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Page 4: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

PressurePressure

is equal to force/unit areais equal to force/unit area SI units = Newton/meterSI units = Newton/meter22 = 1 Pascal = 1 Pascal

(Pa)(Pa) 1 standard atmosphere = 101,325 Pa1 standard atmosphere = 101,325 Pa 1 standard atmosphere = 1 atm =1 standard atmosphere = 1 atm =

760 mm Hg = 760 torr760 mm Hg = 760 torr

Page 5: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONFour bicycle tires are inflated to the following pressures. Which one has the highest pressure? Tire A 3.42 atm; Tire B 48 lbs/sq in; Tire C 305 kPa; Tire D 1520 mmHg. (Recall; 1.00 atm = 760 mmHg = 14.7 lb/sq in = 101.3 kPa)

1. Tire A2. Tire B3. Tire C4. Tire D

Page 6: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 7: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Toricellian BarometerToricellian Barometer05_47

h = 760mm Hgfor standardatmosphere Vacuum

Page 8: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 9: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Pressure & VolumePressure & VolumeBoyle’s LawBoyle’s Law**

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Page 10: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Boyle’s LawBoyle’s Law**

Pressure Pressure Volume = Constant Volume = Constant (T = constant)(T = constant)

PP11VV11 = P = P22VV22 (T = constant) (T = constant) V V 1/ P (T = constant) 1/ P (T = constant)

((**Holds Holds preciselyprecisely only at very low only at very low pressures.)pressures.)

Page 11: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Changing VolumeChanging Volume

A) 4.0 LA) 4.0 LB) 0.57 LB) 0.57 LC) 5.7 LC) 5.7 LD) 0.4 LD) 0.4 L

Page 12: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Pressure vs. VolumePressure vs. Volume

05_50

0V(in3)20406050100PP2V2V(a)

00 1/P (in Hg)0.010.020.032040slope = k

(b)

Page 13: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Definition: A gas that Definition: A gas that strictly obeys strictly obeys Boyle’s Boyle’s Law is called an Law is called an ideal gasideal gas..

Ideal GasesIdeal GasesReal vs. “Ideal”Real vs. “Ideal”

Page 14: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Temperature & Volume Temperature & Volume

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Page 15: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Temperature & VolumeTemperature & Volume

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Page 16: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Charles’s LawCharles’s Law

The volume of a gas is directly The volume of a gas is directly proportional to temperature, and proportional to temperature, and extrapolates to zero at zero Kelvin.extrapolates to zero at zero Kelvin.

V = V = T (P = constant)T (P = constant)

= a proportionality constant= a proportionality constant

Page 17: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Temperature and VolumeTemperature and Volume (@ constant P)(@ constant P)

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Page 18: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Charles’s LawCharles’s LawVTVTP1122==(constant)

Page 19: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Pressure vs. TemperaturePressure vs. Temperature (@ constant V)(@ constant V)

05_1542Pext Pext

Temperature is increasedChanging VolumeChanging Volume

Page 20: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

The Meaning of TemperatureThe Meaning of Temperature

Kelvin temperature is an index of the random Kelvin temperature is an index of the random motions of gas particles (higher T means greater motions of gas particles (higher T means greater motion.)motion.)

(KE)32avg=RT

Page 21: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONKinetic molecular theory helps explain the definition of temperature based on molecular motion. Which statement describes an important aspect of this connection?

1. Temperature is inversely related to the kinetic energy of thegas particles.

2. At the same temperature, more massive gas particles will bemoving faster than less massive gas particles.

3. As the temperature of a gas sample increases, the average velocity of the gas particles increases.

4. Kinetic energy is directly related to temperature. This is validfor any units of temperature.

Page 22: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Kinetic Molecular TheoryKinetic Molecular Theory

1.1. Volume of individual particles is Volume of individual particles is zero.zero.

2.2. Collisions of particles with container Collisions of particles with container walls cause pressure exerted by gas.walls cause pressure exerted by gas.

3.3. Particles exert no forces on each Particles exert no forces on each other.other.

4.4. Average kinetic energy Average kinetic energy Kelvin Kelvin temperature of a gas.temperature of a gas.

Page 23: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Molecular Motion / TheoryMolecular Motion / TheoryThe Meaning of TemperatureThe Meaning of Temperature

Temperature (Kelvin) is an index of the random motions of gas particles (higher T means greater motion.)(KE)32avg=RT

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Page 24: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Velocity & TemperatureVelocity & Temperature

Page 25: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONWhy is it critical that the temperature be held constant when applying Boyle’s law to changing the pressure of a trapped gas?

1. Gas molecules may expand at higher temperatures; this wouldchange the volume.

2. Changing the temperature causes the gas to behave in non-idealfashion.

3. Changing the temperature affects the average particle speed,which could affect the pressure.

4. Allowing the temperature to drop below 0°C would cause thetrapped gas to no longer follow Boyle’s Law.

Page 26: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 27: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONAs the temperature of a gas increases, which statement best correlates to information about molecular velocity?

1. The average molecular velocity will increase, but thedistribution of molecular velocities will stay the same.

2. The average molecular velocity will stay the same, but themolecular velocity distribution will spread.

3. The average molecular velocity will increase, and thedistribution of the molecular velocities will spread.

4. The average molecular velocity will stay the same, and thedistribution of the molecular velocities will stay the same.

Page 28: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

View Gas Molecules AppletView Gas Molecules Applethttp://chemconnections.llnl.govJava/molecules/index.html

View Molecular Vibrations: IRGasTutorhttp://chemistry.beloit.edu/Warming/pages/infrared.html

Page 29: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Changes in Temperature Changes in Temperature ((PV&T)PV&T)05_1543

PextPext

Energy (heat) added

Page 30: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Pressure, Volume & TemperaturePressure, Volume & Temperature

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Page 31: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

An empty one gallon can An empty one gallon can is hooked to a vacuum is hooked to a vacuum

pump. pump.

What do you expect to What do you expect to happen? happen?

Page 32: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Explain why the Explain why the can collapsed. can collapsed.

Page 33: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

V1

An Ideal gasin a cylinder

V2 = 1/ 2 V1

Something(s) happen(s)

What can be going on?

Provide 3 different sets of conditions Provide 3 different sets of conditions (Pressure and Temperature) which can (Pressure and Temperature) which can

account for the volume of the gas account for the volume of the gas decreasing by 1/2.decreasing by 1/2.

Cases 1-3 in the handout.Cases 1-3 in the handout.

Applying a Gas LawApplying a Gas Law

Page 34: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Avogadro’s LawAvogadro’s Law

For a gas at constant temperature For a gas at constant temperature and pressure, the volume is directly and pressure, the volume is directly proportional to the number of moles of proportional to the number of moles of gas (at low pressures).gas (at low pressures).

VV = = nn

= proportionality constant= proportionality constant V = volume of the gasV = volume of the gas n = number of moles of gasn = number of moles of gas

Page 35: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Volume vs. n (moles of a gas)Volume vs. n (moles of a gas)

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Page 36: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 37: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONEach of the balloons hold 1.0 L of different gases. All four are at 25°C and each contains the same number of molecules. Of the following which would also have to be the same for each balloon? (obviously not their color)

1. Their density2. Their mass3. Their atomic numbers4. Their pressure

Page 38: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Ideal Gas LawIdeal Gas Law

An An equation of state equation of state for a gas.for a gas. ““state” is the condition of the gas at a given state” is the condition of the gas at a given

time.time. PV = nRTPV = nRT

[Consider] If the moles remain constant and [Consider] If the moles remain constant and conditions change then:conditions change then:

PP11VV11/ T/ T11 = P = P22VV22/ T/ T22

Page 39: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONIf a person exhaled 125 mL of CO2 gas at 37.0°C and 0.950 atm of pressure, what would this volume be at a colder temperature of 10.0°C and 0.900 atm of pressure?

1. 3.12 mL2. 0.130 L3. 0.120 L4. 22.4 L

Page 40: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Ideal Gas LawIdeal Gas Law

PPVV = n = nRRTT R = proportionality constant R = proportionality constant

= 0.08206 L atm = 0.08206 L atm mol mol

P = pressure in atmP = pressure in atm V = volume in litersV = volume in liters n = molesn = moles T = temperature in KelvinsT = temperature in Kelvins Holds closely at P < 1 atmHolds closely at P < 1 atm

Page 41: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Standard Temperature Standard Temperature and Pressureand Pressure

““STP”STP” For 1 mole of a gas at STP:For 1 mole of a gas at STP: P = P = 1 atmosphere1 atmosphere T = T = CC The molar volume of an ideal gas The molar volume of an ideal gas

is is 22.4222.42 liters liters at STP at STP

Page 42: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONIf a 10.0 L sample of a gas at 25°C suddenly had its volume doubled, without changing its temperature what would happen to its pressure? What could be done to keep the pressure constant without changing the temperature?

1. The pressure would double; nothing else could be done toprevent this.

2. The pressure would double; the moles of gas could be doubled.3. The pressure would decrease by a factor of two; the moles of gas

could be halved.4. The pressure would decrease by a factor of two; the moles could

be doubled.

Page 43: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 44: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONThe typical capacity for human lungs is approximately 5,800 mL. At a temperature of 37°C (average body temperature) and pressure of 0.98 atm, how many moles of air do we carry inside our lungs? (R = 0.08206 L atm/ K mol)

1. 1.9 mol2. 0.22 mol3. 230 mol4. No one wants moles in their lungs.

Page 45: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

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Do you have enough oxygen to climb Mt. Everest?http://ir.chem.cmu.edu/irproject/applets/everest/Applet.asp

Actually, an average pair of human lungs contains about 3.5 L of air after inhalation and about 3.0 L after exhalation. Assuming that air in your lungs is at 37°C and 1.0 atma) How many moles of air are in a typical breath?.b) What is the mass of air in a typical breath?.c) How much of the mass is essential biochemically?

Page 46: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONThe primary way your body produces exhaled CO2 is by the

combustion of glucose, C6H12O6 (molar mass = 180. g/mol.). The

balanced equation is shown here:

C6H12O6 (aq) + 6 O2 (g) 6 CO2 (g) + 6 H2O (l)

If you oxidized 5.42 grams of C6H12O6 while tying your boots to

climb Mt. Everest, how many liters of O2 did you use (assume STP

conditions)?

1. 0.737 L2. 0.672 L3. 4.05 L4. 22.4 L

Page 47: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Applying the Ideal Gas LawApplying the Ideal Gas Law

PV = PV = n n RTRT n n = g of gas/ = g of gas/ MM MM gasgas [ [MM MM gasgas =g/mol] =g/mol] PV = (g of gas/ PV = (g of gas/ MM MM gasgas )RT )RT MM MM gasgas = g of gas(RT)/PV = g of gas(RT)/PV MM MM gasgas = g of gas/V (RT/P) = g of gas/V (RT/P) MM MM gasgas = density of gas (RT/P) = density of gas (RT/P)

Page 48: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Applying the Ideal Gas LawApplying the Ideal Gas Law

The density of an unknown The density of an unknown atmospheric gas pollutant was atmospheric gas pollutant was experimentally determined to be experimentally determined to be 2.144 g/ L @ 0 2.144 g/ L @ 0 ooC and 760 torr. C and 760 torr.

•What is the molar mass of the What is the molar mass of the gas? gas?

•What might the gas be?What might the gas be?

Page 49: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Applying the Ideal Gas LawApplying the Ideal Gas Law

MM MM gas gas = density of gas (= density of gas (RRT/P)T/P)

MM MM gas gas = 1.964 g/ L x = 1.964 g/ L x 0.08206 L atm 0.08206 L atm mol mol

x 273K/ 760 torr x 760 torr/ 1atmx 273K/ 760 torr x 760 torr/ 1atm

1.964 g/ L @ 0 1.964 g/ L @ 0 ooC and 760 torr. C and 760 torr. R = 0.08206 L atm R = 0.08206 L atm mol molooC C K Ktorr torr atm atm

MM MM gas gas ==MM MM gas gas = 44.0 g/mol= 44.0 g/mol

Page 50: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONUnder STP conditions what is the density of O2 gas?

1. Not enough information is given to solve this.2. 1.31 g/L3. 1.43 g/L4. 0.999 g/L

Page 51: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONThe aroma of fresh raspberries can be attributed, at least in part, to 3-(para-hydroxyphenyl)-2-butanone. What is the molar mass of this pleasant smelling compound if at 1.00 atmosphere of pressure and 25.0°C, 0.0820 grams has a volume of 12.2 mL?

1. 13.8 g/mol2. 164 g/mol3. 40.9 g/mol4. 224 g/mol

Page 52: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Dalton’s Law of Dalton’s Law of Partial PressuresPartial Pressures

For a mixture of gases, the total pressure is the For a mixture of gases, the total pressure is the sum of the pressures of each gas in the mixture.sum of the pressures of each gas in the mixture.

PPTotalTotal = P = P11 + P + P22 + P + P33 + . . . + . . .

PPTotalTotal n n TotalTotal

nnTotalTotal = n = n11 + n + n22 + n + n33 + . . . + . . .

Page 53: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONIf the mole fraction of O2 in our atmosphere at standard conditions is approximately 0.209, what is the partial pressure of the oxygen in every breath you take?

1. 1.00 atm2. 4.78 atm3. 159 torr4. 3640 mmHg

Page 54: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Dalton’s Law of Dalton’s Law of Partial PressuresPartial Pressures

For a mixture of gases, the partial gas pressurFor a mixture of gases, the partial gas pressure and total pressure equal the mole fraction of e and total pressure equal the mole fraction of each gas in the mixture.each gas in the mixture.

PP11 / / PPTotalTotal = n= n11 / / n nTotalTotal

Page 55: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONFreon-12 had been widely used as a refrigerant in air conditioning systems. However, it has been shown to be related to destroying Earth’s important ozone layer. What is the molar mass of Freon-12 if 9.27 grams was collected by water displacement, in a 2.00 liter volume at 30.0°C and 764 mmHg. Water’s vapor pressure at this temperature is approximately 31.8 mmHg.

1. 120. g/mol2. 12.0 g/mol3. 115 g/mol4. 92.7 g/mol

Page 56: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Effusion: describes the passage of gas into an evacuated chamber.

Diffusion: describes the mixing of gases. The rate of diffusion is the rate of gas mixing.

Diffusion and EffusionDiffusion and Effusion

Page 57: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

EffusionEffusion05_60

GasVacuum

Pinhole

Page 58: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Rate of effusion for gas 1Rate of effusion for gas 221=MMDistance traveled by gas 1Distance traveled by gas 221=MMEffusion:Effusion:

Diffusion:Diffusion:

Effusion and DiffusionEffusion and Diffusion

Page 59: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Applying Gas BehaviorApplying Gas BehaviorPreparation of Preparation of 235235UU

235235UOUO3 (s) 3 (s) + + 238238UOUO3 (s) 3 (s) 235235UFUF6 (g) 6 (g) + + 238238UFUF6 (g)6 (g)

235235U is the unstable isotope that is used in U is the unstable isotope that is used in nuclear fission. Which isoptope is the most nuclear fission. Which isoptope is the most abundant? abundant?

Design a method to separate the isomers.Design a method to separate the isomers. Be very carefulBe very careful

Page 60: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Real GasesReal Gases

Must correct ideal gas behavior when at Must correct ideal gas behavior when at high high pressure pressure (smaller volume) and (smaller volume) and low temperature low temperature (attractive forces become important).(attractive forces become important).

Page 61: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Real GasesReal Gases[]PaVnbnRTobs2(/)+↔−()=nV

corrected pressurecorrected pressure corrected volumecorrected volume

PPidealideal VVidealideal

Page 62: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 63: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Real GasesReal GasesVolume vs. Temperature @ constant PVolume vs. Temperature @ constant P

Page 64: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONAfter examining the figure, which statement is accurate, and consistent about the real gases shown at constant pressure?

1. At –273°C all gases occupy nearly the same volume; the different slopes are because of differences in molar masses.

2. At zero Celsius the gases have different volumes because the larger the molecule, the larger the volume.

3. Since the pressure is constant, the only difference in volume that could cause the different slopes is in the attractive forces (Van der Waal’s forces).

4. Although it does appear to do so, the volumes do not reach zero but if the graph used K instead of °C the volume would reach zero for all the gases.

Page 65: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 66: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

QUESTIONQUESTIONReal gases exhibit their most “ideal” behavior at which relative conditions?

1. Low temperatures and low pressures2. High temperatures and high pressures3. High temperatures and low pressures4. Low temperatures and high pressures

Page 67: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Atmospheric PollutantsAtmospheric Pollutants

Page 68: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Atmospheric PollutantsAtmospheric Pollutants

Page 69: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay
Page 70: Gases Dr. Ron Rusay Fall 2007 © Copyright 2007 R.J. Rusay

Gases & AirbagsGases & AirbagsUse of Chemical Reactions and Physical PropertiesUse of Chemical Reactions and Physical Properties

Workshop: Gases IIWorkshop: Gases II

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