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Properties of Gases Properties of Gases Chpt. 10 Chpt. 10

Properties of Gases Chpt. 10

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Properties of Gases Chpt. 10. A Quick Review Matter is anything that occupies space and has mass There are three states of matter. Particles slide over each other. Particles vibrate about a fixed position. Particles have almost complete freedom of movement. - PowerPoint PPT Presentation

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Page 1: Properties of Gases Chpt. 10

Properties of GasesProperties of GasesChpt. 10Chpt. 10

Page 2: Properties of Gases Chpt. 10

A Quick Review • Matter is anything that occupies space and has mass• There are three states of matter

Particles vibrate about a fixed position

Particles slide over each other Particles have

almost complete freedom of movement

Page 3: Properties of Gases Chpt. 10

In this chapter we will be looking at the third state of matter - GAS.

Gases have distinct properties that distinguish them from solids and liquids. These properties may be explained in terms of the particles (atoms, molecules, ions) of a gas having more freedom of movement than the particles of a solid or liquid.

Page 4: Properties of Gases Chpt. 10

Some Properties of Gases:

1.Gases DO NOT have a definite shape or size and will spread throughout any container they are placed in – DIFFUSION

Diffusion: is the movement of particles from an area of high concentration to an area of low concentration.

Example: NH3 and HCl Ammonium Chloride

Smoke particles travelling throughout the air

Example liquids (much slower):Spreading of ink throughout a beaker of water

Page 5: Properties of Gases Chpt. 10

A gas is defined as a substance that has no well-defined boundaries but diffuses rapidly to fill any container in which it is placed.

Page 6: Properties of Gases Chpt. 10

2. Gases do not have a fixed volume – they fill any space into which they are put, therefore the volume of the gas is the volume of the container in which they are placed.

The volume of a gas is influenced by two factors: - temperature - pressure

Increasing Temperature – gas expands and occupies greater volume

Increasing Pressure – gas becomes compressed and occupies a smaller volume

Page 7: Properties of Gases Chpt. 10

Jacques Charles and Robert Boyle were two scientists who investigated how the volume of a gas changes with temperature and how the volume of a gas changes with pressure respectively.

Charles (volume & temperature)

Boyle (volume & pressure)

Page 8: Properties of Gases Chpt. 10

In this chapter we shall be studying the laws that gases obey

and why they obey these laws. This also involves a study of the

work of Charles and Boyle

Page 9: Properties of Gases Chpt. 10

3 Main properties of a fixed amount of gas

TemperaturePressureVolume

Note: Before studying the laws that gases obey we must first understand how to measure the above three properties

Page 10: Properties of Gases Chpt. 10

Temperature:Temperature is a measure of the degree of hotness of an object.

Two Scales

Celsius (centigrade) scale Kelvin (absolute) scale

Two fixed points: - 0oC – freezing point of water- 100OC – boiling point of water

- 0 K – absolute zero (temperature at which a gas would occupy no volume)

Page 11: Properties of Gases Chpt. 10

Relationship between Celsius Scale and Kelvin Scale

O0C 10O0C-273O C

0 K 273 K 373 KAbsolute

Zero

Page 12: Properties of Gases Chpt. 10

Celsius Kelvin

*0oC = 0 + 273 = 273 K30oC = 30 + 273 = 303 K50oC =80oC =100oC =273oC =

Temperature can be converted from the Celsius scale to the Kelvin scale by adding 273

Page 13: Properties of Gases Chpt. 10

*Note:

- size of a degree on the Celsius scale is the same as that on the Kelvin scale i.e. rise in temperature of 10oC is same as rise in temperature of 10 K

- SI unit of temperature – Kelvin*

Page 14: Properties of Gases Chpt. 10

Pressure:Pressure of a gas is the force it exerts on each unit area of its container

• SI unit of pressure is N/m2 (Nm-2) or *Pascal (Pa)

• We will be dealing with pressure in terms of atmospheric pressure:

Normal atmospheric pressure:1.013 x 105 N/m2

1.013 x 105 Pa101,325 Pa101kPa (*1kPa – 1000 Pa)

Page 15: Properties of Gases Chpt. 10

Note:Old method of expressing pressure of gases used millimetres of mercury or atmospheres:

Normal Atmospheric Pressure:

760 mm Hg = 1 atm = 1.013 x 105Pa

Page 16: Properties of Gases Chpt. 10

Volume:The volume of a sample of gas is the same as the volume of the container in which the sample is held

• SI unit of volume is m3

• Laboratory units:cm3

Litres (L)

A litre is also called a cubic decimetre (dm3= 1/10 of

metre)

1L = 1000cm3 = 1dm3

Page 17: Properties of Gases Chpt. 10

Relationship between m3, cm3 and Litres

1m3 = 1 x 106 cm3

*N.B.To change cm3 to m3 multiply by 10-6

To change litres to m3 multiply by 10-3

Page 18: Properties of Gases Chpt. 10

Summary of measuring three main properties of gases

Temperature – unit Kelvin ( convert from celsius)

Pressure – unit Pascal

Volume – unit cubic metre (convert from cm3 and litres)

Page 19: Properties of Gases Chpt. 10

Standard Temperature and Pressure (s.t.p.)

As previously noted the volume of a gas varies with temperature and pressure. Thus in order to compare volumes occupied by gases, it is necessary to measure all volumes at the same temperature and pressure:

Standard Temperature = 273 K (0OC)Standard Pressure = 1.013 x 105 Pa

or 101,325 Pa or 101kPa

Page 20: Properties of Gases Chpt. 10

Five Main Gas Laws

• Boyles Law

• Charles Law

• The Combined Gas Law

• Gay-Lussac’s Law of combing Volumes

• Avogadro’s Law

Page 21: Properties of Gases Chpt. 10

Boyles LawIrish scientist Robert Boyle experimented with the relationship between pressure and volume of gases.

He set up a J-shaped tube and added mercury to see what it did to the volume of a trapped gas, kept at a constant temperature

Page 22: Properties of Gases Chpt. 10

As pressure increases, volume decreases

Page 23: Properties of Gases Chpt. 10

Boyles Experimental Results

*This relationship is inversely proportional, when one increases the other decreases.

Page 24: Properties of Gases Chpt. 10

The volume is inversely proportional to the pressure

*Note: see fig. 10.5(a) and fig. 10.5(b) pg. 110

Page 25: Properties of Gases Chpt. 10

Boyles Law:At a constant temperature , the volume of a fixed mass of gas is inversely proportional to its pressure

V α 1 P

The proportionality symbol can be replaced by a constant k which gives us a mathematical equation:

V = k1 pV = k P

p = pressureV = volumek = proportionality constant

Page 26: Properties of Gases Chpt. 10

Knowing that the pressure of a gas multiplied by its volume is always a constant value gives another way of expressing Boyle’s Law:

p1V1 = p2V2

Thus, it is possible to calculate the volume of a gas at one pressure when its volume at another pressure is known.

*Note: see pg. 111 table 10.1 and fig. 10.7 for further explanation

Page 27: Properties of Gases Chpt. 10

Boyle’s Air Pump

Page 28: Properties of Gases Chpt. 10

Boyles Law Summary

V α 1 P

pV = k

p1V1 = p2V2

Must also be familiar with associated graphs (3)!!!!!

Page 29: Properties of Gases Chpt. 10

Charles Law

French scientist, Jacques Charles, investigated the relationship between the volume and temperature of a fixed mass of gas at constant pressure

Page 30: Properties of Gases Chpt. 10

Charles Law

French physicist Jacques Charles was the first to fill a balloon with hydrogen gas and make a solo flight.

He showed that the volume of a gas increases when the temperature increases (at a constant pressure)

Page 31: Properties of Gases Chpt. 10

Charles Law Experiment

Page 32: Properties of Gases Chpt. 10

Charles Law Experimental results

*Note: see figure 10.10 pg. 112

Page 33: Properties of Gases Chpt. 10

In previous graph straight line does not go through the origin therefore one cannot say that the volume of the gas is directly proportional to the temperature measured in O C.

However, if the line is continued backwards, it cuts the x-axis at -273oC i.e. absolute zero in terms of the Kelvin Scale

Page 34: Properties of Gases Chpt. 10

Using the Kelvin scale of temperature a direct relationship between volume and

temperature can be seen i.e. volume is directly proportional to temperature

-273oC O K

*Note: see figure 10.11 pg. 112

Page 35: Properties of Gases Chpt. 10
Page 36: Properties of Gases Chpt. 10

Charles Law:At constant pressure , the volume of a fixed mass of gas is directly proportional to its temperature measured on the Kelvin scale

V α T

V = kt V = k T

The proportionality symbol can be replaced by a constant k which gives us a mathematical equation:

V = volumek = proportionality constantT = temperature (Kelvin)

Page 37: Properties of Gases Chpt. 10

Knowing that volume divided by temperature always gives a constant value allows the volume of a gas at any given temperature to be calculated provided that its volume at some other temperature is known:

V1 = V2

T1 T2

*Note: see pg. 113 table 10.2 and fig. 10.13 for

further explanation

Page 38: Properties of Gases Chpt. 10

Charles Law Summary

V α T

V1 = V2

T1 T2

V = kT

Must also be familiar with associated graphs (3)!!!!!

Page 39: Properties of Gases Chpt. 10

The Combined Gas Law(The General Gas Law)

The results of Boyle’s and Charles’ law can be combined into a single expression which takes the form:

p1 V1 = p2 V2

T1 T2

Using this equation, the volume of a gas at any temperature and pressure can be calculated provided that its volume at some other given temperature and pressure is known.

Page 40: Properties of Gases Chpt. 10

*Points to Note:1. Since combined gas law derived from Charle’s

law MUST convert all temperatures to the KELVIN SCALE

2. Units on both sides of equation must be consistent e.g. if using kPa on left side must use kPa on right side

Page 41: Properties of Gases Chpt. 10

Example 1:A certain mass of gas was found to occupy a volume of 269cm3 when the temperature was 17o C and the pressure 99.7kPa. What volume would the gas occupy at s.t.p.?

Page 42: Properties of Gases Chpt. 10

Example 2:A sample of hydrogen of volume 100cm3 at a pressure of 1 x 105 Pa is compressed to 55cm3 at constant temperature. What is the new pressure of the gas?

Page 43: Properties of Gases Chpt. 10

Gay-Lussac’s Law of Combining Volumes

Following on from work done by Henry Cavendish on the composition of water (electrolysis), Joesph Gay-Lussac confirmed that when hydrogen reacts with oxygen, 2 volumes of hydrogen always react with 1 volume of oxygen

1808 – Gay-Lussac stated his law of combining volumes

Page 44: Properties of Gases Chpt. 10

He studied the reactions of other gases to further investigate whether they also reacted in simple ratios

Hydrogen + Oxygen Steam 2 volumes 1 volume 2 volumes

Hydrogen + Chlorine Hydrogen Chloride 1 volume 1 volume 2 volumes

Nitrogen + Oxygen Nitrogen DioxideMonoxide

2 volumes 1 volume 2 Volumes

*Note: Please read through experiment outline pg’s 114-115

Page 45: Properties of Gases Chpt. 10

In 1808, Gay-Lussac was able to state his law of combining volumes:

Gay-Lussac’s Law of Combining Volumes

In a reaction between gases, the volumes of the reacting gases and the volumes of any gaseous products are in the ratio of small whole numbers provided the volumes are measured at the same temperature and pressure.

Page 46: Properties of Gases Chpt. 10

Avogadro’s Law

An explanation of Gay-Lussac’s law depends on the idea that gases consist of particles. Gay-Lussac’s and Daltons Atomic Theory were published at the same time (1808). However attempts to explain Gay-Lussac’s theory using Dalton’s atomic theory failed.

Amedeo Avogadro, (Professor of Physics in 19th century Italy) put forward a hypothesis, which explained Gay-Lussac’s law, relating molecules and volumes.

Page 47: Properties of Gases Chpt. 10

Avogadro showed experimentally that 100 cm3 of hydrogen react exactly with 100 cm3 of chlorine. This indicates that there must be the same number of molecules of hydrogen and chlorine in each volume:

Hydrogen + Chlorine Hydrogen Chloride

1 volume 1 volume 2 volumes

Applying Avogadro’s Law:

n molecules + n molecules 2n moleculesHydrogen Chlorine Hydrogen

Chloride1 molecule + 1 molecule 2 molecules

H2 Cl2 2HCl

Page 48: Properties of Gases Chpt. 10

Two volumes of hydrogen contain twice as many molecules ………

…. as one volume of oxygen

Each oxygen atom bonds with two hydrogen atoms to form a molecule of water

Page 49: Properties of Gases Chpt. 10

Similarly,

2H2 + O2 2H2O

2NO + O2 2NO

The ratio in which the volumes of gases combine is the same as the ratio in which the molecules of gases combine. Thus, when dealing with gaseous reactions the words volume and molecule can always be interchanged.

Page 50: Properties of Gases Chpt. 10
Page 51: Properties of Gases Chpt. 10

Avogadro’s Law

Equal volumes of gases, under the same temperature and pressure contain equal numbers of molecules

Page 52: Properties of Gases Chpt. 10

Molar Volume

Leading on from Avogadro’s study of gaseous reactions and the words volume and molecule being interchangeable a definition of molar volume was formed

Remember:1 mole = 6 x 1023 particles

By experiment it was found that:

1 mole O2 occupies 22.4L at s.t.p.

Page 53: Properties of Gases Chpt. 10

Since 1 mole of any gas contains 6 x 1023 molecules then according to Avogadro’s Law:

At s.t.p. one mole of any gas occupies a volume of 22.4 L

Molar Volume: the volume occupied by one mole of any gas is called its molar volume

*Note: at r.t.p. (room temperature, pressure) one mole occupies a volume of 24 L

Page 54: Properties of Gases Chpt. 10

Calculations involving Molar Volume

1. Moles → Litres

2. Litres → Moles

3. Litres → Number of particles

4. Litres → Grams

5. General Questions

Page 55: Properties of Gases Chpt. 10

1. Converting moles to litres

Volume (Litres) = moles x Molar Volume (22.4L)

Example 1: What is the volume of 2 moles of H2 ats.t.p.?

Litres = 2 x 22.4 Litres = 44.8L

Page 56: Properties of Gases Chpt. 10

2. Converting litres to moles

Moles = Volume Molar Volume

Note: 22.4L = 22,400cm3

Example 1: How many moles of SO2 are there in 3L of the gas at s.t.p.?

Moles = 3 22.4

Moles = 0.13 moles

Page 57: Properties of Gases Chpt. 10

Example 2:How many moles of NO2 are there in 175cm3 of the gas at s.t.p.?

Moles = Volume Molar Volume

Moles = 175 22,400

Moles = 0.0078125 moles

Page 58: Properties of Gases Chpt. 10

3. Converting litres to number of particles (molecules/atoms)

Step 1. Change litres/cm3 to moles

Step 2. Change moles to molecules/atoms

Example 1:How many molecules are there in 560cm3 of chlorine gas at STP?

Page 59: Properties of Gases Chpt. 10

Example 1 Solution:

Page 60: Properties of Gases Chpt. 10

Example 2:How many atoms are there in 840cm3 of butane gas,C4H10, at STP?

Page 61: Properties of Gases Chpt. 10

4. Converting Litres to Grams

Step 1: Change Litres/cm3 to moles

Step 2: Change moles to grams

Example 1:What is the mass in g of 140cm3 of oxygen gas at STP?

Page 62: Properties of Gases Chpt. 10

Example 1 Solution:

Page 63: Properties of Gases Chpt. 10

5. General QuestionsThis section involves taking what you know from the previous chapter on the Mole and incorporating this into answering the question

Example 1:Calculate the volume occupied by 20g of sulphur dioxide gas at s.t.p.?

Page 64: Properties of Gases Chpt. 10

Example 2:200 cm3 of a certain gas at s.t.p. Have a mass of 0.25g. Calculate the relative molecular mass of the gas.

Page 65: Properties of Gases Chpt. 10

Example 3:Calculate the density of carbon dioxide at s.t.p.

Page 66: Properties of Gases Chpt. 10

Try the following question:What is i) the volume at s.t.p. and ii) the number of molecules in 24g of sulphur dioxide (SO2)

Page 67: Properties of Gases Chpt. 10

Please complete the following questions on the mole and molar volume

Book: 10.5, 10.6, 10.7 pg. 125Workbook: W10.4, W10.5 pg. 19

Page 68: Properties of Gases Chpt. 10

Mandatory Experiment:

To measure the relative molecular mass of a volatile liquid

*Note: A volatile liquid is a liquid that is easily vaporised

Page 69: Properties of Gases Chpt. 10

The Kinetic Theory of Gases

This theory was developed to explain the five gas laws discussed previously. It was based on the idea that all matter is made up of tiny particles in constant motion i.e. Solids – particles vibrate

Liquids – particles can move freely around each other

Gases – particles have complete freedom of movement

Robert Brown, a botanist, was the first to find evidence to support the idea of particles in motion.

Page 70: Properties of Gases Chpt. 10

Brownian Motion

Brownian Motion: the random movement of tiny particles suspended in a liquid or gas

Page 71: Properties of Gases Chpt. 10

In order to understand the behaviour of gases a number of assumptions were developed – Kinetic Theory of Gases

Assumptions of the Kinetic Theory of Gases:1.Gases are made up of particles that are in constant rapid, random motion, colliding with each other and with the walls of the container.

2.*There are no attractive or repulsive forces between the molecules of a gas

3.*Gas molecules are so small and so widely separated that the actual volume of all the molecules is negligible compared with the space they occupy i.e. they take up very little space.

Page 72: Properties of Gases Chpt. 10

4. When molecules collide all collisions are perfectly elastic i.e.

- If particle collides with wall of its container with a speed of 450 m/s it rebounds with the same

speed- No loss of kinetic energy but may be transferred

5. The average Kinetic energy of the molecules is proportional to the Kelvin temperature

Page 73: Properties of Gases Chpt. 10

Limitations to the Kinetic Theory of Gases:

- it is not valid to say that there are no attractive or repulsive forces between the molecules of a gas i.e. dipole-dipole forces between polar molecules and van der Waals forces between non-polar molecules.

- it is not always valid to say that the volume of the gases is negligible compared with the space they occupy i.e. under high pressure, when molecules are crowded close together, it is clear that their volume is not negligible.

Page 74: Properties of Gases Chpt. 10

Ideal GasDue to these limitations it can be seen that all of the assumptions of the kinetic theory do not hold for real gases but only hold for imaginary or ideal gases

An ideal gas is one that obeys all the assumptions of the kinetic theory of gases under all ALL conditions of temperature and pressure

Page 75: Properties of Gases Chpt. 10

Ideal Gases DO NOT EXIST!!!!

A real gas behaves like an ideal gas at:

- low pressure – molecules widely spaced and

- high temperatures – molecules are moving rapidly and forces between the molecules are small

Page 76: Properties of Gases Chpt. 10

Reasons why Gases differ from Ideal Gas behaviour

At low temperatures and high pressures:

- the volume of the particles is not negligible compared with the distances between them

- there are attractive and repulsive forces between the particles i.e. molecules are moving slowly and are packed close together resulting in stronger intermolecular forces

Page 77: Properties of Gases Chpt. 10

*Note:

- Under the same conditions of temperature and pressure non-polar molecules come closer to being ideal gases than polar molecules, since the attractive forces are less in the case of non- polar molecules.

Page 78: Properties of Gases Chpt. 10

Student Question:State which of the following gases you would expect to come closest to ideal behaviour, and which you would expect to deviate most from ideal behaviour:H2, HF, F2 . Explain your answers.

Page 79: Properties of Gases Chpt. 10

Ideal Gas Equation (Equation of State for an Ideal Gas)

Boyles Law, Charles Law and Avogadro’s law may be combined to form an equation relating volume (V), temperature(T), pressure(p) and number of moles(n) of a gas:

Boyle V α 1 constant temperaturep

Charles V α T constant pressure

Avogadro V α n constant temperature & pressure

Page 80: Properties of Gases Chpt. 10

Combining all three equations:

V α (1) Tn(p)

Replacing proportionality symbol with R (constant of proportionality – Universal Gas Constant):

V = R(1) Tn (p)

Rearranging equation:

pV = nRT Ideal Gas Equation

Page 81: Properties of Gases Chpt. 10

The numerical value for R can be found by simply substituting experimental values into the ideal gas equation i.e. we know at s.t.p. I mole of any gas occupies a volume of 22.4L

T = 273KP = 1.013 x 105 N/m2 (Pa)n = 1V = 22.4L – 22.4 x 10-3 = 0.0224m3

pV = nRT R = pV = 1.013 x 105 x .0224 nT 1 mole x 273

R = 8.31 J mol-1 K-1

Page 82: Properties of Gases Chpt. 10

Units and the Ideal Gas EquationMeasure Unit

Volume m3

Pressure PaTemperature KNumber of moles mol

Universal Gas Constant (R)

J mol-1 K-1

(always given to you)

Page 83: Properties of Gases Chpt. 10

Calculations involving the Ideal Gas Equation