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Unit 7Gas Laws and Thermodynamics
Chapters 11 & 16
CHAPTER 11Gases
Pressure and Force
• Pressure is the force per unit area on a surface.
Pressure =Force
Area
Chapter 11 – Section 1: Gases and Pressure
Gases in the Atmosphere
• The atmosphere of Earth is a layer of gases surrounding the planet that is retained by Earth's gravity.
• By volume, dry airis 78% nitrogen, 21% oxygen, 0.9% argon, 0.04% CO2, and small amounts of other gases.
Chapter 11 – Section 1: Gases and Pressure
Atmospheric Pressure
• Atmospheric pressure is the force per unit area exerted on a surface by the weight of the gases that make up the atmosphere above it.
Chapter 11 – Section 1: Gases and Pressure
Measuring Pressure
• A common unit of pressure is millimeters of mercury (mm Hg).
• 1 mm Hg is also called 1 torr in honor of Evangelista Torricelli whoinvented the barometer (used tomeasure atmospheric pressure).
• The average atmospheric pressure at sea level at 0°C is 760 mm Hg, so one atmosphere (atm) of pressure is 760 mm Hg.
Chapter 11 – Section 1: Gases and Pressure
Measuring Pressure (continued)
•Pressure can also be measured in pascals (Pa): 1 Pa = 1 N/m2.
•One pascal is verysmall, so usually kilopascals (kPa) are used instead.
•One atm is equal to 101.3 kPa.
1 atm = 760 mm Hg (Torr) = 101.3 kPa
Chapter 11 – Section 1: Gases and Pressure
Units of PressureChapter 11 – Section 1: Gases and Pressure
Converting PressureSample Problem
The average atmospheric pressure in Denver, CO is 0.830 atm. Express this pressure in:
a. millimeters of mercury (mm Hg)
b. kilopascals (kPa)
Chapter 11 – Section 1: Gases and Pressure
0.830 atmatm
mm Hg1
760x =
0.830 atmatm
kPa1
101.3x =
631 mm Hg
84.1 kPa
Dalton’s Law of Partial Pressures
• Dalton’s law of partial pressures - the total pressure of a gas mixture is the sum of the partial pressures of the component gases.
Chapter 11 – Section 1: Gases and Pressure
PT = P1 + P2 + P3 …
Dalton’s Law of Partial PressuresSample Problem
A container holds a mixture of gases A, B & C. Gas A has a pressure of 0.5 atm, Gas B has a pressure of 0.7 atm, and Gas C has a pressure of 1.2 atm.
a.What is the total pressure of this system?
b. What is the total pressure in mm Hg?
Chapter 11 – Section 1: Gases and Pressure
PT = P1 + P2 + P3 …PT = 0.5 atm+ 0.7 atm + 1.2 atm = 2.4 atm
2.4 atmatm
mm Hg1
760x = 1800 mm Hg
Gases and Pressure• Gas pressure is caused by collisions of the gas
molecules with each other and with the walls of their container.
• The greater the number of collisions, the higher the pressure will be.
Chapter 11 – Section 2: The Gas Laws
Pressure – Volume Relationship
• When the volume of a gas is decreased, more collisions will occur.
• Pressure is caused by collisions.
• Therefore, pressure will increase.
• This relationshipbetween pressure andvolume is inversely proportional.
Chapter 11 – Section 2: The Gas Laws
Boyle’s Law
• Boyle’s Law – The volume of a fixed mass of gas varies inversely with the pressure at a constant temperature.
• P1 and V1 representinitial conditions, andP2 and V2 representanother set of conditions.
Chapter 11 – Section 2: The Gas Laws
P1V1 = P2V2
Boyle’s LawSample Problem
A sample of oxygen gas has a volume of 150.0 mL when its pressure is 0.947 atm. What will the volume of the gas be at a pressure of 0.987 atm if the temperature remains constant?Solution:
Chapter 11 – Section 2: The Gas Laws
P1V1 = P2V2(0.947 atm)(150.0 mL) = (0.987 atm)V2
V2 =(0.947 atm)(150.0 mL)
(0.987 atm)= 144 mL
Volume – Temperature Relationship
• the pressure of gas inside and outside the balloon are the same.
• at low temperatures, the gas molecules don’t move as much – therefore the volume is small.
• at high temperatures, the gas molecules move more – causing the volume to become larger.
Chapter 11 – Section 2: The Gas Laws
• Charles’s Law – The volume of a fixed mass of gas at constant pressure varies directly with the Kelvin temperature.
Charles’s LawChapter 11 – Section 2: The Gas Laws
V1 V2=T1 T2
• V1 and T1 represent initial conditions, and V2 and T2 represent another set of conditions.
The Kelvin Temperature Scale
• Absolute zero – The theoretical lowest possible temperature where all molecular motion stops.
• The Kelvin temperature scale starts at absolute zero (-273oC.)
• This gives the followingrelationship between the two temperature scales:
Chapter 11 – Section 2: The Gas Laws
K = oC + 273
Charles’s LawSample Problem
A sample of neon gas occupies a volume of 752 mL at 25°C. What volume will the gas occupy at 50°C if the pressure remains constant?Solution:
Chapter 11 – Section 2: The Gas Laws
V1 V2=T1 T2
752 mL V2=298 K 323 K
K = oC + 273T1 = 25 + 273 = 298T2 = 50 + 273 = 323
752 mLV2 =298 K
323 Kx = 815 mL
Pressure – Temperature Relationship
• Increasing temperature means increasing kinetic energy of the particles.
• The energy and frequency of collisions depend on the average kinetic energy of the molecules.
• Therefore, if volume is kept constant, the pressure of a gas increases with increasing temperature.
Chapter 11 – Section 2: The Gas Laws
Gay-Lussac’s Law
• Gay-Lussac’s Law – The pressure of a fixed mass of gas varies directly with the Kelvin temperature.
• P1 and T1 representinitial conditions.P2 and T2 representanother set of conditions.
P1 P2=T1 T2
Chapter 11 – Section 2: The Gas Laws
The Combined Gas Law
• The combined gas law is written as follows:
• Each of the other gas laws can be obtained from the combined gas law when the proper variable is kept constant.
Chapter 11 – Section 2: The Gas Laws
P1 P2=T1 T2
V1 V2
The Combined Gas LawSample Problem
A helium-filled balloon has a volume of 50.0 L at 25°C and 1.08 atm. What volume will it have at 0.855 atm and 10.0°C?Solution:
Chapter 11 – Section 2: The Gas Laws
(1.08 atm) (0.855 atm)=
298 K 283 K
K = oC + 273T1 = 25 + 273 = 298T2 = 10 + 273 = 283
(1.08 atm)V2 =(298 K)
(283 K)= 60.0 L
P1 P2=T1 T2
V1 V2
(50.0 L) V2
(50.0 L)(0.855 atm)
Avogadro’s Law
• In 1811, Amedeo Avogadro discovered that the volume of a gas is proportional to the number of molecules (or number of moles.)
• Avogadro’s Law - equal volumes of gases at the same temperature and pressure contain equal numbers of molecules, or:
V1 V2=n1 n2
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
Standard Molar Volume
• Standard Temperature and Pressure (STP) is 0oC and 1 atm.
• The Standard Molar Volume of a gas is the volume occupied by one mole of a gas at STP. It has been found to be 22.4 L.
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
Molar Volume Conversion Factor
• Standard Molar Volume can be used as a conversion factor to convert from the number of moles of a gas at STP to volume (L), or vice versa.
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
Molar Volume ConversionSample Problem
a. What quantity of gas, in moles, is contained in 5.00 L at STP?
b. What volume does 0.768 moles of a gas occupy at STP?
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
5.00 LL
mol22.41x = 0.223 mol
0.768 molmol
L1
22.4x = 17.2 L
Volume Ratios
• You can use the volume ratios as conversion factors just like you would use mole ratios.
2CO(g) + O2(g) → 2CO2(g)2 molecules 1 molecule 2 molecules2 mole 1 mole 2 mol2 volumes 1 volume 2 volumes
• Example: What volume of O2 is needed to react completely with 0.626 L of CO to form CO2?
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
0.626 L COL COL O2
21x = 0.313 L O2
The Mole Map
• You can now convert between number of particles, mass (g), and volume (L) by going through moles.
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
Gas StoichiometrySample Problem
Assume that 5.61 L H2 at STP reacts with excess CuO according to the following equation:
CuO(s) + H2(g) → Cu(s) + H2O(g)
a.How many moles of H2 react?
b.How many grams of Cu are produced?
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
5.61 L H2L H2
mol H2
22.41x = 0.250 mol H2
5.61 L H2L H2
mol H2
22.41x
mol H2
mol Cu1
1xmol Cu
g Cu1
63.5x = 15.9 g Cu
The Ideal Gas Law
• All of the gas laws you have learned so far can be combined into a single equation, the ideal gas law:
• R represents the ideal gas constant which has a value of 0.0821 (L•atm)/(mol•K).
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
PV = nRT
The Ideal Gas LawSample Problem
What is the pressure in atmospheres exerted by a 0.500 mol sample of nitrogen gas in a 10.0 L container at 298 K?Solution:
Chapter 11 – Section 3: Gas Volumes and the Ideal Gas Law
PV = nRTP (10.0 L) = (0.500 mol)(0.0821 L•atm/mol•K)
P =(0.500 mol) (298 K)
(10.0 L)= 1.22
atm
(298 K)
(0.0821 L•atm/mol•K)
Diffusion and Effusion
• Diffusion is the gradual mixing of two or more gases due to their spontaneous, random motion.
• Effusion is the process whereby the molecules of a gas confined in a container randomly pass through a tiny opening in the container.
Chapter 11 – Section 4: Diffusion and Effusion
Graham’s Law of Effusion
• Light molecules move faster than heavy ones. • Graham’s
law of effusion saysthe greaterthe molarmass of a gas,the slower itwill effuse.
Chapter 11 – Section 4: Diffusion and Effusion
CHAPTER 16Thermochemistry
Heat and Temperature
• Temperature – a measure of the average kinetic energy of the particles in a sample of matter.
• The greater the kinetic energy of the particles in a sample, the hotter it feels.
• Heat – energy transferred between samples of matter due to a difference in their temperatures.
• Heat always moves spontaneously from matter at a higher temperature to matter at a lower temperature.
Chapter 16 – Section 1: Thermochemistry
Measuring Heat
• Heat energy is measured in joules (or calories – food only)
• Chemical reactions usually either absorb or release energyas heat.
• The energy absorbed or released as heat in a chemical or physical change is measured in a calorimeter.
Chapter 16 – Section 1: Thermochemistry
Specific Heat
• A quantity called specificheat can be used to compare heat absorptioncapacities for different materials.
• Specific heat – the amount of energy required to raise the temperature of one gram of a substance by 1°C or 1 K.
• Specific heat can be measured in units of J/(g•°C), J/(g•K), cal/(g•°C), or cal/(g•K).
Chapter 16 – Section 1: Thermochemistry
Heat Transfer Equation
• Specific heat can be used to find the quantity of heat energy gained or lost with a change in temperature according to the following equation:
• Where the variables stand for the following:Q = heat transferred (joules or calories)m = mass (g)cp = specific heat∆T = change in temperature (oC or K)
Chapter 16 – Section 1: Thermochemistry
Q = m x cp x ∆T
Heat Transfer EquationSample Problem
A 4.0 g sample of glass was heated from 274 K to 314 K, a temperature increase of 40. K, and was found to have absorbed 32 J of energy as heat.
a.What is the specific heat of this type of glass?
b. How much energy will the same glass sample gain when it is heated from 314 K to 344 K?
Chapter 16 – Section 1: Thermochemistry
Q = m x cp x ∆T 32 J = (4.0 g)(cp) (40. K)
cp = (4.0 g)(40. K)
32 J = 0.20 J/(g•K)
Q = m x cp x ∆T Q = (4.0 g)(0.20 J/(g•K)) (30 K) = 24 J
Enthalpy of Reaction
• The enthalpy of reaction (H) is the quantity of energy transferred as heat during a chemical reaction.
• The change in enthalpy (∆H) of a reaction is always the difference between the enthalpies of the products and the reactants.
Chapter 16 – Section 1: Thermochemistry
∆H = Hproducts - Hreactants
Exothermic Reactions
• In an exothermic reaction, energy is released. Therefore, the energy of the products must be less than the energy of the reactants, and ∆H is negative.
• The great majority ofchemical reactions innature are exothermic.
Chapter 16 – Section 1: Thermochemistry
Endothermic Reactions
• In an endothermic reaction, energy is absorbed. Therefore, the energy of the products must be greater than the energy of the reactants, and ∆H is positive.
Chapter 16 – Section 1: Thermochemistry
Entropy and Reaction Tendency
• Entropy – a measure of the degree of randomness in a system.
• Processes in nature are driven in two directions: towards decreasing enthalpy and towards increasing entropy.
• The combined enthalpy-entropy function is called the Gibbs free energy (G).
Chapter 16 – Section 1: Thermochemistry
Hess’s Law
• Hess’s Law – the overall enthalpy change in a reaction is equal to the sum of enthalpy changes for the individual steps in the process.
• Possible steps in Hess’s Law:1. Reverse equation/
change sign on ΔH.2. Multiply or Divide
coefficients/multiply or divide ΔH.
Chapter 16 – Section 1: Thermochemistry
Hess’s LawSample Problem
Calculate the enthalpy of formation for CH4:C(s) + 2H2(g) → CH4(g) ∆Hf = ?The component reactions are:C(s) + O2(g) → CO2(g) ∆Hc = -393.5 kJH2(g) + ½O2(g) → H2O(l) ∆Hc = -285.8 kJCH4(g) + 2O2(g) → CO2(g) + 2H2O(l) ∆Hc = -890.8 kJCO2(g) + 2H2O(l) → CH4(g) + 2O2(g) ∆Hc = +890.8 kJ- 2 moles of H2 are used to make CH4,
so multiply the 2nd equation by 2 (including ∆H.)- CH4 is on the products side, not the reactants side, so
reverse the 3rd reaction and change the sign on ∆H.- Cancel unwanted terms and add the ∆H’s.
Chapter 16 – Section 1: Thermochemistry
2 2 -571.6 kJ
-74.3 kJ
-74.3 kJ