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Chapter 6
Thermochemistry
Section 6.1The Nature of Energy
What drives chemical reactions? How do they occur?
The first is answered by THERMODYNAMICS and the second by KINETICS.
We have already seen a number of “driving forces” for reactions that are PRODUCT‐FAVORED.
• formation of a precipitate
• gas formation
• H2O formation (acid‐base reaction)
• electron transfer in a battery
Section 6.1The Nature of Energy
ENERGY is the capacity to do work or produce and transfer heat.
WORK ‐ force acting over a distance.
HEAT is the form of energy that flows between 2 samples because of their difference in temperature.
Other forms of energy —
light electricalnuclear
kinetic potential
Section 6.1The Nature of Energy
Temperature reflects random motions of particles, therefore related to kinetic energy of the systemenergy of the system.
Heat (form of energy) involves a transfer of energy between 2 objects due to a temperature difference
Section 6.1The Nature of Energy
The First Law of Thermodynamics = energy can be converted from one form to another but can be neither created nor destroyed.y
The total energy content of the universe is constant.
(Euniverse is constant)
Section 6.1The Nature of Energy
Potential: due to position or composition ‐ can be converted to work
PE = mgh
(m = mass, g = acceleration of gravity, and h = height)
Kinetic: due to motion of the object
KE = 1/2 mv2
(m = mass, v = velocity)
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Section 6.1The Nature of Energy
In the initial position, ball A has a higher potential energy than ball B.
Initial Position
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Section 6.1The Nature of Energy
After A has rolled down the hill, the potential energy lost by A has been converted to random motions of the components of the hill (frictional heating) and to the increase in the potential energy of B.
Final Position
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p gy
Section 6.1The Nature of Energy
Potential energy —energy a motionlessenergy a motionless body has by virtue of
its position.
Section 6.1The Nature of Energy
Kinetic Kinetic energy energy --energy energy of of gygymotion.motion.
• Translation• Translation
• Rotation• Rotation
• Vibration• Vibration
Section 6.1The Nature of Energy
1 calorie = heat required to raise temp. of 1.00 g of H2O by 1.0
oC. (Not an SI Unit)
1000 cal = 1 kilocalorie = 1 kcal
1 kcal = 1 Calorie (a food “calorie”)
But we use the derived SI unit called the JOULE
1 cal = 4.184 joulesJames JouleJames Joule
18181818--188918892
2111
s
mkgmeternewtonJoule
Section 6.1The Nature of Energy
Extensive & Intensive Properties
Extensive properties depends directly on the amount of substance
Intensive properties is not related to the amount of substance.
present.
•mass
•volume
•heat
•heat capacity (C)
•temperature
•concentration
•pressure
•specific heat (s)
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Section 6.1The Nature of Energy
State Function is a property that depends only on the present state of the system ‐ not how it arrived there.
It is independent of pathway.
Energy change is independent of the pathway (and, therefore, a state function), while work and heat are dependent on the pathway.
Section 6.1The Nature of Energy
ENERGY IS A STATE FUNCTION
A person standing at the top of Mt. Everest has the same potential energy whether they got there bywhether they got there by hiking up, or by falling down from a plane
WORK IS NOT A STATE FUNCTION
WHY NOT???
Section 6.1The Nature of Energy
System – part of the universe on which we wish to focus attention.
Surroundings – include everything else in the
Chemical Energy
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universe.
Universe = System + Surroundings
Section 6.1The Nature of Energy
Endothermic Reaction:
Heat flow is into a system.
Absorb energy from the surroundings.
Chemical Energy
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gy g
Exothermic Reaction:
Energy flows out of the system.
Energy gained by the surroundings must be equal to the energy lost by the system.
Section 6.1The Nature of Energy
SurroundingsSurroundings
SystemSystem
heatheat
SurroundingsSurroundings
SystemSystem
heatheat
qqsystemsystem > 0> 0w > 0w > 0
qqsystemsystem < 0< 0w < 0w < 0
ENDOTHERMICENDOTHERMIC EXOTHERMICEXOTHERMICE(system) goes upE(system) goes up E(system) goes downE(system) goes down
Section 6.1The Nature of Energy
Is the freezing of water an endothermic or exothermic process? Explain.
CONCEPT CHECK!CONCEPT CHECK!
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Section 6.1The Nature of Energy
Classify each process as exothermic or endothermic. Explain. The system is underlined in each example.
CONCEPT CHECK!CONCEPT CHECK!
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a) Your hand gets cold when you touch ice.
b) The ice gets warmer when you touch it.
c) Water boils in a kettle being heated on a stove.
d) Water vapor condenses on a cold pipe.
e) Ice cream melts.
Exo
Endo
Endo
Exo
Endo
Section 6.1The Nature of Energy
For each of the following, define a system and its surroundings and give the direction of energy transfer.
CONCEPT CHECK!CONCEPT CHECK!
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gy
a) Methane is burning in a Bunsen burner in a laboratory.
b) Water drops, sitting on your skin after swimming, evaporate.
Section 6.1The Nature of Energy
Hydrogen gas and oxygen gas react violently to form water. Explain.
CONCEPT CHECK!CONCEPT CHECK!
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Which is lower in energy: a mixture of hydrogen and oxygen gases, or water?
Section 6.1The Nature of Energy
• Internal energy (E) of a system is the sum of the kinetic and potential energies of all the “particles” in the system.
Thermodynamics and Internal Energy
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To change the internal energy of a system:ΔE = q + w
q represents heat
w represents work
Section 6.1The Nature of Energy
Work vs Energy Flow
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Section 6.1The Nature of Energy
Thermodynamic quantities consist of two parts:
Number gives the magnitude of the change.
Internal Energy
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Sign indicates the direction of the flow.
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Section 6.1The Nature of Energy
Internal Energy
Sign reflects the system’s point of view.
Endothermic Process:
q is positive
Exothermic Process:
q is negative
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Section 6.1The Nature of Energy
Sign reflects the system’s point of view.
System does work on surroundings:
w is negative
Internal Energy
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Surroundings do work on the system:
w is positive
Section 6.1The Nature of Energy
Expansion Compression (i ) (d )
w P V
+V (increase) -V (decrease)
-w results +w results
Esystem decreasesWork has been done by the system on the surroundings
Esystem increasesWork has been done on the system by the surroundings
Section 6.1The Nature of Energy
Work = P× A× Δh = PΔV
P is pressure.
A i
Work
28
A is area.
Δh is the piston moving a distance.
ΔV is the change in volume.
Section 6.1The Nature of Energy
For an expanding gas, ΔV is a positive quantity because the volume is increasing. Thus ΔV and wmust have opposite signs:
Work
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w = –PΔV
To convert between L∙atm and Joules, use 1 L∙atm = 101.3 J.
Section 6.1The Nature of Energy
w & Δ V must have opposite signs, since work is being done by the system to expand the P = F/AP = F/A
F PAF PA gas.
wsystem = ‐P Δ V
1 Latm = 101.3 J
1 J = kgm2/s2
F = PAF = PAw = F w = F ∆ hhw = PA w = PA ∆ hhw = P w = P ∆ VV
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Section 6.1The Nature of Energy
Which of the following performs more work?
a) A gas expanding against a pressure
EXERCISE!EXERCISE!
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a) A gas expanding against a pressure of 2 atm from 1.0 L to 4.0 L.
b) A gas expanding against a pressure of 3 atm from 1.0 L to 3.0 L.
They perform the same amount of work.
Section 6.1The Nature of Energy
Determine the sign of ΔE for each of the following with the listed conditions:
a) An endothermic process that performs work
CONCEPT CHECK!CONCEPT CHECK!
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a) An endothermic process that performs work.
|work| > |heat|
|work| < |heat|
b) Work is done on a gas and the process is exothermic.
|work| > |heat|
|work| < |heat|
Δ E = negative
Δ E = positive
Δ E = positive
Δ E = negative
Section 6.2Enthalpy and Calorimetry
Change in Enthalpy
State function
ΔH = q at constant pressure
ΔH = H – H ΔH = Hproducts – Hreactants
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Section 6.2Enthalpy and Calorimetry
Enthalpy = H = E + PV
E = H PVH = E + PV
At constant pressure,
qP = E + PV, where qP = H at constant pressure
H = energy flow as heat (at constant pressure)
Section 6.2Enthalpy and Calorimetry
H = Hfinal ‐ Hinitial
If H > H then H is positive If Hfinal > Hinitial then H is positive Process is ENDOTHERMIC
If Hfinal < Hinitial then H is negative Process is EXOTHERMIC
Section 6.2Enthalpy and Calorimetry
Endothermic:
Reactions in
+ qsystem - qsurroundings
Reactions in which energy flows into the system as the reaction proceeds.
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Section 6.2Enthalpy and Calorimetry
Exothermic:
Reactions in which energy
- qsystem + qsurroundings
which energy flows out of the system as the reaction proceeds.
Section 6.2Enthalpy and Calorimetry
Consider the combustion of propane:
C3H8(g) + 5O2(g) → 3CO2(g) + 4H2O(l)
EXERCISE!EXERCISE!
ΔH = –2221 kJ
Assume that all of the heat comes from the combustion of propane. Calculate ΔH in which 5.00 g of propane is burned in excess oxygen at constant pressure.
–252 kJ
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Section 6.2Enthalpy and Calorimetry
Calorimetry
Science of measuring heat
Specific heat capacity:
The energy required to raise the temperature of one The energy required to raise the temperature of one gram of a substance by one degree Celsius. =
J/OC x g or J/K x g
Molar heat capacity:
The energy required to raise the temperature of one mole of substance by one degree Celsius. = J/OC x mol or J/K x mol
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Section 6.2Enthalpy and Calorimetry
Substance Spec. Heat (J/g•K)
H2O 4.184WaterWater
Al 0.902
glass 0.84
AluminumAluminum
Section 6.2Enthalpy and Calorimetry
Calorimetry
If two reactants at the same temperature are mixed and the resulting solution gets warmer, this means the reaction taking place is exothermic.g p
An endothermic reaction cools the solution.
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Section 6.2Enthalpy and Calorimetry
A Coffee–Cup Calorimeter Made of Two Styrofoam Cups
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Section 6.2Enthalpy and Calorimetry
Calorimetry
Energy released (heat) = Cp×m× ΔT
Cp = specific heat capacity (J/g∙OC)
m = mass of solution (g)(g)
ΔT = change in temperature (OC)
or.......
Energy released (heat) = Cn× n× ΔT
Cn = molar heat capacity (J/mol∙OC)
n = number of moles of substance (mol)
ΔT = change in temperature (OC)Copyright © Cengage Learning. All rights reserved 43
Section 6.2Enthalpy and Calorimetry
If 25.0 g of Al cool from 310 oC to 37 oC, how many joules of heat energy are lost by the Al?
where T = Tfinal ‐ Tinitial
heat gain/lost = q = m C T
Section 6.2Enthalpy and Calorimetry
If 25.0 g of Al cool from 310 oC to 37 oC, how many joules of heat energy are lost by the Al?
where T = Tfinal ‐ Tinitial q = (0.902 J/g•K)(25.0 g)(37 ‐ 310)K
q = ‐ 6160 J
heat gain/lost = q = m CT
Section 6.2Enthalpy and Calorimetry
If 25.0 g of Al cool from 310 oC to 37 oC,
how many joules of heat energy are lost
by the Al?
q = ‐ 6160 J
Notice that the negative sign on q signals
heat “lost by” or transferred out of Al.
Section 6.2Enthalpy and Calorimetry
75.0 g of Zn at 310. oC is dropped into 50.0 g of water at 25.0OC. What is the final t t f th t ?temperature of the system?
Cp of Zn = 0.387 J/g x OCheat gain by water = heat lost by metal
86.9OC
Section 6.2Enthalpy and Calorimetry
06_75
StirrerThermometer
Ignitionwires
Water
Insulatingcontainer
Reactantsin samplecup
Steelbomb
Bomb CalorimeterBomb Calorimeter
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Section 6.2Enthalpy and Calorimetry
Calculate heat of combustion of octane.
C8H18 + 25/2 O2 ‐‐> 8 CO2 + 9 H2O
Measuring Heats of ReactionMeasuring Heats of ReactionCALORIMETRYCALORIMETRY
Measuring Heats of ReactionMeasuring Heats of ReactionCALORIMETRYCALORIMETRY
C8H18 + 25/2 O2 > 8 CO2 + 9 H2O
Burn 1.00 g of octane Temp rises from 25.00 to 33.20 oC Calorimeter contains 1200. g water Heat capacity of bomb = 837 J/K
Hcm = ‐(C Δ t + ms Δ t) where Hc is heat of combustion.
Section 6.2Enthalpy and Calorimetry
Step 1 Calc. heat transferred from reaction to water.
q = (4.184 J/g•K)(1200. g)(8.20 K) = 41,170.56 J
St 2 C l h t t f d f ti t b b
Measuring Heats of ReactionMeasuring Heats of ReactionCALORIMETRYCALORIMETRY
Measuring Heats of ReactionMeasuring Heats of ReactionCALORIMETRYCALORIMETRY
Step 2 Calc. heat transferred from reaction to bomb.
q = C Δ t = (837 J/K)(8.20 K) = 6863.4J
Step 3 Total heat evolved
41,170.56 J + 6863.4 J = 48,033.96J
Heat of combustion of 1.00 g of octane = ‐ 48.0 kJ
Heat of combustion of 1.00 mol of octane =
‐ 48.0 kJ/g x 96.26 g/mol = ‐ 4620 kJ/mol
Section 6.2Enthalpy and Calorimetry
A 100.0 g sample of water at 90°C is added to a 100.0 g sample of water at 10°C.
CONCEPT CHECK!CONCEPT CHECK!
The final temperature of the water is:
a) Between 50°C and 90°C
b) 50°C
c) Between 10°C and 50°C
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Section 6.2Enthalpy and Calorimetry
A 100.0 g sample of water at 90.°C is added to a 500.0 g sample of water at 10.°C.
CONCEPT CHECK!CONCEPT CHECK!
The final temperature of the water is:
a) Between 50°C and 90°C
b) 50°C
c) Between 10°C and 50°C
Calculate the final temperature of the water.
23°C
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Section 6.2Enthalpy and Calorimetry
You have a Styrofoam cup with 50.0 g of water at 10.°C. You add a 50.0 g iron ball at 90.°C to the water. (sH2O = 4.18 J/°C∙g and sFe = 0.45 J/°C∙g)
CONCEPT CHECK!CONCEPT CHECK!
The final temperature of the water is:
a) Between 50°C and 90°C
b) 50°C
c) Between 10°C and 50°C
Calculate the final temperature of the water.
18°CCopyright © Cengage Learning. All rights reserved 53
Section 6.3Hess’s Law
In going from a particular set of reactants to a particular set of products, the change in enthalpy is the same whether the reaction takes place in one step or in a p pseries of steps.
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Section 6.3Hess’s Law
This reaction also can be carried out in two distinct steps, with enthalpy changes designated by ΔH2 and ΔH3.
N2(g) + 2O2(g) → 2NO2(g) ΔH1 = 68 kJ
N2(g) + O2(g) → 2NO(g) ΔH2 = 180 kJ
2NO(g) + O2(g) → 2NO2(g) ΔH3 = – 112 kJ
N2(g) + 2O2(g) → 2NO2(g) ΔH2 + ΔH3 = 68 kJ
ΔH1 = ΔH2 + ΔH3 = 68 kJ
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Section 6.3Hess’s Law
The Principle of Hess’s Law
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Section 6.3Hess’s Law
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Section 6.3Hess’s Law
Characteristics of Enthalpy Changes
If a reaction is reversed, the sign of ΔH is also reversed.
The magnitude of ΔH is directly proportional to the quantities of reactants and products in a reaction. If thequantities of reactants and products in a reaction. If the coefficients in a balanced reaction are multiplied by an integer, the value of ΔH is multiplied by the same integer.
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Section 6.3Hess’s Law
Example
Consider the following data:
3 2 21 3
2 2NH ( ) N ( ) H ( ) H = 46 kJ
( ) O ( ) O( )
g g g
Calculate ΔH for the reaction
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2 2 22 H ( ) O ( ) 2 H O( ) H = 484 kJ g g g
2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g
Section 6.3Hess’s Law
Problem‐Solving Strategy
Work backward from the required reaction, using the reactants and products to decide how to manipulate the other given reactions at your p g ydisposal.
Reverse any reactions as needed to give the required reactants and products.
Multiply reactions to give the correct numbers of reactants and products.
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Section 6.3Hess’s Law
Example
Reverse the two reactions:
2 2 31 3
2 2N ( ) H ( ) NH ( ) H = 46 kJ g g g
Desired reaction:
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2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g
2 2 22 H O( ) 2 H ( ) O ( ) H = +484 kJ g g g
Section 6.3Hess’s Law
Example
Multiply reactions to give the correct numbers of reactants and products:
4( ) 4( )
3( ) 3( )
Desired reaction:
2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g
2 2 3
2 2 2
1 3
2 2N ( ) H ( ) NH ( ) H = 46 kJ
2 H O( ) 2 H ( ) O ( ) H = +484 kJ
g g g
g g g
Section 6.3Hess’s Law
Example
Final reactions:
2 2 32 N ( ) 6 H ( ) 4 NH ( ) H = 184 kJ
6 H O( ) 6 H ( ) 3 O ( ) H = +1452 kJ
g g g
g g g
Desired reaction:
ΔH = +1268 kJ
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2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g
2 2 26 H O( ) 6 H ( ) 3 O ( ) H = +1452 kJ g g g
Section 6.4Standard Enthalpies of Formation
Standard Enthalpy of Formation (ΔHf°)
Change in enthalpy that accompanies the formation of one mole of a compound from its elements with all substances in their standard states.
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Section 6.4Standard Enthalpies of Formation
Conventional Definitions of Standard States
For a Compound
For a gas, pressure is exactly 1 atm.
For a solution concentration is exactly 1M For a solution, concentration is exactly 1 M.
Pure substance (liquid or solid)
For an Element
The form [N2(g), K(s)] in which it exists at 1 atm and 25°C.
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Section 6.4Standard Enthalpies of Formation
A Schematic Diagram of the Energy Changes for the Reaction CH4(g) + 2O2(g) CO2(g) + 2H2O(l)
ΔH°reaction = –(–75 kJ) + 0 + (–394 kJ) + (–572 kJ) = –891 kJ
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Section 6.4Standard Enthalpies of Formation
Problem‐Solving Strategy: Enthalpy Calculations
1. When a reaction is reversed, the magnitude of ΔHremains the same, but its sign changes.
2. When the balanced equation for a reaction is multiplied2. When the balanced equation for a reaction is multiplied by an integer, the value of ΔH for that reaction must be multiplied by the same integer.
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Section 6.4Standard Enthalpies of Formation
Problem‐Solving Strategy: Enthalpy Calculations
3. The change in enthalpy for a given reaction can be calculated from the enthalpies of formation of the reactants and products:
Hrxn° = npHf(products) nrHf(reactants)
H is an extensive property‐‐kJ/mol
4. standard states are not included in the ΔHreaction
calculations because ΔHf° for an element in its standard state is zero.
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Section 6.4Standard Enthalpies of Formation
Calculate the heat of combustion of
methanol, i.e., Horxn for
CH3OH(g) + 3/2 O2(g) ‐‐> CO2(g) + 2 H2O(g)
Horxn = Ho
f (prod) ‐ Hof (react)
Section 6.4Standard Enthalpies of Formation
CH3OH(g) + 3/2 O2(g) ‐‐> CO2(g) + 2 H2O(g)
Horxn = Ho
f (prod) ‐ Hof (react)
Ho = Hof (CO2) + 2 Ho
f (H2O) ‐H rxn H f (CO2) + 2 H f (H2O)
{3/2 Hof (O2) + Ho
f (CH3OH)}
= (‐393.5 kJ) + 2 (‐241.8 kJ) ‐ {0 + (‐201.5 kJ)}
Horxn = ‐675.6 kJ per mol of methanol
Horxn is always in terms of moles of reactant.
Section 6.4Standard Enthalpies of Formation
CH4(g)
C(s)
CO2(g)
2H2(g)
(a) (c)
2H2O(l)
2O2(g) 2O2(g)
Reactants Elements Products
(b)
(d)
Pathway for the Combustion of MethanePathway for the Combustion of Methane
Section 6.4Standard Enthalpies of Formation
Calculate ΔH° for the following reaction:
2Na(s) + 2H2O(l) → 2NaOH(aq) + H2(g)
EXERCISE!EXERCISE!
Given the following information:
Δ Hf° (kJ/mol)
Na(s) 0
H2O(l) –286
NaOH(aq) –470
H2(g) 0
Δ H° = –368 kJCopyright © Cengage Learning. All rights reserved 72
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Section 6.5Present Sources of Energy
Fossil Fuels
Petroleum, Natural Gas, and Coal
Wood Wood
Hydro
Nuclear
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Section 6.5Present Sources of Energy
Energy Sources Used in the United States
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Section 6.5Present Sources of Energy
The Earth’s Atmosphere
Transparent to visible light from the sun.
Visible light strikes the Earth, and part of it is changed to infrared radiation.to infrared radiation.
Infrared radiation from Earth’s surface is strongly absorbed by CO2, H2O, and other molecules present in smaller amounts in atmosphere.
Atmosphere traps some of the energy and keeps the Earth warmer than it would otherwise be.
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Section 6.5Present Sources of Energy
The Earth’s Atmosphere
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Section 6.6New Energy Sources
Coal Conversion
Hydrogen as a Fuel
Other Energy Alternatives Other Energy Alternatives
Oil shale
Ethanol
Methanol
Seed oil
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