AP Chemistry Ms. Grobsky - · PDF fileAP Chemistry Ms. Grobsky ... However, m/V is the gas...

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AP Chemistry

Ms. Grobsky

We have already considered 4 laws that describe the behavior of

gases

β€’ Boyle’s law

𝑉 =π‘˜

𝑃

(at constant T and n)

β€’ Charles’ law

𝑉 = π‘˜π‘‡ (at constant P and n)

β€’ Guy-Lussac’s law

𝑃 = π‘˜π‘‡

(at constant V and n)

β€’ Avogadro’s law

𝑉 = π‘˜π‘› (at constant T and P)

You may think a small gas molecule would take up less space than a large gas molecule,

but it doesn’t at the same temperature and pressure!

The previous 4 relationships, which show how the volume of a gas depends on pressure, temperature, and number of moles of gas present, can be combined as follows:

V = RTn

P

β€’ R is the combined proportionality constant called the universal gas constant

Always use the value 0.08206 (0.0821) πΏβˆ™π‘Žπ‘‘π‘š

πΎβˆ™π‘šπ‘œπ‘™ for R

Equation can be rearranged to yield the more familiar ideal gas

law:

PV = nRT

The ideal gas law is an equation of state for a gas

β€’ State of a gas is its condition at a given time

A particular state of a gas is described by its pressure, volume,

temperature, and number of moles

A gas that obeys this equation is said to behave ideally

β€’ Expresses behavior that real gases approach at low pressures

and high temperatures

Thus, an ideal gas is a hypothetical substance

However, most gases obey the ideal gas equation closely enough at

pressure below 1 atm so assume ideal behavior unless stated otherwise

A sample of hydrogen gas (H2) has a

volume of 8.56 L at a temperature of 0Β°C

and a pressure of 1.5 atm. β€’ Calculate the moles of H2 molecules present in

the sample.

A sample of diborane gas (B2H6), a

substance that bursts into flame when

exposed to air, has a pressure of 345 torr

at a temperature of -15Β°C and a volume of

3.48 L. β€’ If conditions are changed so that the

temperature is 36Β°C and the pressure is 468 torr,

what will be the volume of the sample?

One very important use of the ideal gas law is the calculation of the molar mass of a gas from its measured density

𝑛 = π‘”π‘Ÿπ‘Žπ‘šπ‘  π‘œπ‘“ π‘”π‘Žπ‘ 

π‘šπ‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘ =

π‘šπ‘Žπ‘ π‘ 

π‘šπ‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘ =

π‘š

π‘šπ‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘ 

Substituting the above into the ideal gas equation

gives:

𝑃 = 𝑛𝑅𝑇

𝑉=

π‘šπ‘šπ‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘ 

𝑅𝑇

𝑉=

π‘š(𝑅𝑇)

𝑉(π‘šπ‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘ )

However, m/V is the gas density (d) in units of g/L

Substituting and rearranging for molar

mass:

π‘€π‘œπ‘™π‘Žπ‘Ÿ π‘šπ‘Žπ‘ π‘  = 𝑑𝑅𝑇

𝑃

β€œMolar Mass Kitty Cat”

All good cats put dirt

[dRT] over their pee [P]

The density of a gas was measured at

1.50 atm and 27Β°C and found to be 1.95

g/L. β€’ Calculate the molar mass of the gas and give its

identity.

Use PV = NRT to solve for the volume of one mole of gas at STP:

Look familiar? This is the molar volume of a gas at STP

β€’ Use stoichiometry to solve gas problems only if gas is at STP conditions

β€’ Use the ideal gas law to convert quantities that are NOT at STP

Quicklime (CaO) is produced by the

thermal decomposition of calcium

carbonate (CaCO3). β€’ Calculate the volume of CO2 at STP produced

from the decomposition of 152 g CaCO3 by the

reaction:

πΆπ‘ŽπΆπ‘‚3 𝑠 β†’ πΆπ‘Žπ‘‚ 𝑠 + 𝐢𝑂2(𝑔)

A sample of methane gas (CH4) having a

volume of 2.80 L at 25Β°C and 1.65 atm

was mixed with a sample of oxygen gas

having a volume of 35.0 L at 31Β°C and

1.25 atm. The mixture was then ignited to

form carbon dioxide and water. β€’ Calculate the volume of CO2 formed at a

pressure of 2.50 atm and a temperature of 125Β°C

The pressure of a mixture of gases is the sum of the pressures of the different components of the mixture:

π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™ = 𝑃1 + 𝑃2 + β‹― 𝑃𝑛

Dalton’s Law of Partial Pressures

β€’ Uses the concept of mole fractions! Recall:

χ𝐴 =moles A

moles A + moles B + moles C + β‹―

β€’ So now:

𝑃𝐴 = Ο‡π΄π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™

β€’ What does this mean? The partial pressure of each gas in a mixture of gases

in a container depends on the number of moles of that

gas!

Therefore, the total pressure is the SUM of the partial

pressures and depends on the total moles of gas

present – no matter what their identity is!

Mixtures of helium and oxygen are used

in scuba diving tanks to help prevent β€œthe

bends.” For a particular dive, 46 L He at

25Β°C and 1.0 atm and 12 L O2 at 25Β°C and

1.0 atm were pumped into a tank with a

volume of 5.0 L. β€’ Calculate the partial pressure of each gas and

the total pressure in the tank at 25Β°C.

The mole fraction of nitrogen in the air is

0.7904. The mole fraction of oxygen in

the air is .2093. The mole fraction of

carbon dioxide in the air is .0003.

Calculate the partial pressures of all

three major components in air when the

atmospheric pressure is 760. torr.

It is common to collect a gas by water

displacement which means some of the

pressure is due to water vapor collected as

the gas was passing through! β€’ You must correct for this by looking up the partial

pressure of water at that particular temperature!

THIS IS A VERY POPULAR TYPE

OF PROBLEM ON THE AP EXAM!

A sample of solid potassium chlorate was heated in a test tube and decomposed by the following reaction:

2 𝐾𝐢𝑙𝑂3 𝑠 β†’ 2 𝐾𝐢𝑙 𝑠 + 3 𝑂2 𝑔

The oxygen produced was collected by

displacement of water at 22Β°C at a total

pressure of 754 torr. The volume of the

gas collected was 0.650 L, and the vapor

pressure of water at 22Β°C is 21 torr. β€’ Calculate the partial pressure (in atm) of O2 in

the gas collected and the mass of KClO3 in the

sample that was decomposed.

All particles are in constant, random

motion

All collisions between particles are

perfectly elastic

The volume of the particles in a gas is

negligible

The average kinetic energy of the

molecules is in its Kelvin temperature

The KMT model neglects any

intermolecular forces as well β€’ Gases expand to fill their containers

Solids/liquids do not

β€’ Gases are compressible

Solids/liquids are not appreciably compressible

Assumptions of the KMT successfully

account for the observed behavior of an

ideal gas β€’ Recall that there are five gas laws describing the

behavior of gases that were derived from

experimental observations

If the volume is decreased that means that the

gas particles will hit the wall more often Pressure is increased!

When a gas is heated,

the speed of its

particles increase

and thus, hit the walls

more often and with

more force Only way to keep pressure

constant is to INCREASE

the VOLUME of the

container!

When the temperature of a gas increases, the speeds of its particles increase

The particles are hitting the wall with greater force and greater frequency

Since the volume remains the same, this would result in INCREASED gas pressure

An increase in the number of particles at

the same temperature would cause the

pressure to increase if the volume were

held constant The only way to keep constant pressure is to vary the

volume!

The pressure exerted by a mixture of

gases is the SUM of the partial pressures β€’ This is because gas particles are acting

independent of each other and the volumes of

the individual particles DO NOT matter

Root Mean Square Velocity, Effusion, and Diffusion

From the KMT, Kelvin temperature indicates the average kinetic energy of the gas particles

𝑃𝑉

𝑛= 𝑅𝑇 =

2

3(𝐾𝐸)π‘Žπ‘£π‘”

β€’ 2/3 KE comes from the application of velocity, momentum, force, and pressure

when deriving an expression for pressure See Appendix 2 in your book for a complete mathematical explanation!

Thus,

(𝐾𝐸)π‘Žπ‘£π‘” = 3

2𝑅𝑇

ALL gases have the same average kinetic

energy at the same temperature!

This mathematical relationship is very

important because it shows that with

higher temperature comes greater

motion of the gas particles β€’ HEAT β€˜EM UP – SPEED β€˜EM UP!

Look at the graph at right β€’ How do the number

of gaseous molecules with a given velocity change with increasing temperature? By drawing a vertical

line from the peak of each bell curve to the x-axis, the AVERAGE velocity of the sample is derived

Average velocity of a specific gas molecule at a specific temperature is also root mean square velocity (ΞΌrms)

β€’ Can be calculated using Maxwell’s equation:

πœ‡2 = πœ‡π‘Ÿπ‘šπ‘  =3𝑅𝑇

𝑀𝑀

β€’ Where: R is β€œenergy R” = 8.314 J/Kβˆ™mol

T = temperature in Kelvin

MM = molar mass of a single gas particle in KILOGRAMS per mole!

β€’ πœ‡π‘Ÿπ‘šπ‘  has units of m/s!

This equation is important because it shows that molar mass is inversely proportional to velocity

β€’ Massive particles move slowly

β€’ Light particles move quickly

But remember - ALL gases have the same average kinetic energy at the same temperature!

Calculate the root mean square velocity

for the atoms in a sample of helium gas at

25Β°C.

If we could monitor the path of a single

molecule, it would be very erratic β€’ The average distance a particle travels between

collisions is called the mean free path

It’s on the order of a tenth of a micrometer –

waaaaayyyyy small!

Thomas Graham experimentally showed that the rate of effusion of a gas is inversely proportional to the square root of the mass of its particles β€’ Stated in another way, the relative rates of effusion of two

gases at the same temperature and pressure are given by the inverse ratio of the square roots of the masses of the gas particles

π‘…π‘Žπ‘‘π‘’ π‘œπ‘“ π‘’π‘“π‘“π‘’π‘ π‘–π‘œπ‘› π‘“π‘œπ‘Ÿ π‘”π‘Žπ‘  1

π‘…π‘Žπ‘‘π‘’ π‘œπ‘“ π‘’π‘“π‘“π‘’π‘ π‘–π‘œπ‘› π‘“π‘œπ‘Ÿ π‘”π‘Žπ‘  2=

πœ‡π‘Ÿπ‘šπ‘  π‘“π‘œπ‘Ÿ π‘”π‘Žπ‘  1

πœ‡π‘Ÿπ‘šπ‘  π‘“π‘œπ‘Ÿ π‘”π‘Žπ‘  2=

3𝑅𝑇𝑀1

3𝑅𝑇𝑀2

=𝑀2

𝑀1

M1 and M2 = molar masses of the gases in g/mol

We have seen that the postulates of the KMT, when combined with appropriate physical principles, produce an equation that successfully fits the experimentally observed behavior of gases

There are 2 further tests of this model: β€’ Effusion Describes the passage of a gas through a tiny orifice into an

evacuated chamber Rate of effusion measures the speed at which the gas is transferred into

the chamber

β€’ Diffusion Describes the mixing of gases Rate of diffusion is the rate of the mixing!

Calculate the ratio of the effusion rates of

hydrogen gas (H2) and uranium

hexafluoride (UF6), a gas used in the

enrichment process to produce fuel for

nuclear reactors

Quite complicated to describe

theoretically because so many collisions

occur when gases mix

corrected pressure corrected volume

Pideal Videal

At high pressure (smaller volume) and low

temperature (attractive forces become

important) you must adjust for non-ideal gas

behavior using van der Waal’s equation.

2

( )obs

nP a x V nb nRT

V