chapter 5 thermochemistry

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Thermochemistry Chapter 5 Thermochemistry John D. Bookstaver St. Charles Community College St. Peters, MO 2006, Prentice Hall, Chemistry, The Central Science, 10th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten

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Chemistry, The Central Science , 10th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten. Chapter 5 Thermochemistry. John D. Bookstaver St. Charles Community College St. Peters, MO  2006, Prentice Hall, Inc. December 16 HOMEWORK. Do questions 1,2,9,11,17,19,20 - PowerPoint PPT Presentation

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Page 1: Chapter 5 Thermochemistry

Thermochemistry

Chapter 5Thermochemistry

John D. Bookstaver

St. Charles Community College

St. Peters, MO

2006, Prentice Hall, Inc.

Chemistry, The Central Science, 10th editionTheodore L. Brown; H. Eugene LeMay, Jr.;

and Bruce E. Bursten

Page 2: Chapter 5 Thermochemistry

Thermochemistry

December 16HOMEWORK

• Do questions 1,2,9,11,17,19,20

• First law of thermodynamics 23,25,29

• Enthalpy 31 to 45 odd

• Lab Notebook due by next Monday

Page 3: Chapter 5 Thermochemistry

Thermochemistry

Energy

• The ability to do work or transfer heat.Work: Energy used to cause an object that

has mass to move.Heat: Energy used to cause the

temperature of an object to rise.

Page 4: Chapter 5 Thermochemistry

Thermochemistry

Potential Energy

Energy an object possesses by virtue of its position or chemical composition.

Page 5: Chapter 5 Thermochemistry

Thermochemistry

Electrostatic PEArises from the interaction between charged

particles.

Eel = k Q1 Q2 k = 8.99x109 Jm/C2

d Q charge of particles

d distance

If charges are same sign they repel and Eel is positive. If they have opposite sign they attract and Eel is negative.

The lower the energy of system the more stable it is. Thus the more strongly opposite charged particles attract each other.

Page 6: Chapter 5 Thermochemistry

Thermochemistry

Kinetic Energy

Energy an object possesses by virtue of its motion.

12

KE = mv2

Page 7: Chapter 5 Thermochemistry

Thermochemistry

Units of Energy

• The SI unit of energy is the joule (J).

• An older, non-SI unit is still in widespread use: The calorie (cal).

1 cal = 4.184 J

1 J = 1 kg m2

s2

Page 8: Chapter 5 Thermochemistry

Thermochemistry

Joule

• A mass of 2 kg moving at a speed of 1 m/s possesses a kinetic energy of 1 J.

calorie: the amount of heat needed to increase the temperature of 1 g of water from 14.5 0C to 15.5 0C.

• 1 Cal = 1000 cal = 1 kcal

Page 9: Chapter 5 Thermochemistry

Thermochemistry

System and Surroundings• Consider the reaction inside

the piston

• 2H2(g) +O2->2H2O(g)+heat

• The system includes the molecules we want to study (here, the hydrogen and oxygen molecules). Reactants an products.

• The surroundings are everything else (here, the cylinder and piston).

Page 10: Chapter 5 Thermochemistry

Thermochemistry

Work

• Energy is used to move an object over some distance.

• w = F d,

where w is work, F is the force, and d is the distance over which the force is exerted.

Page 11: Chapter 5 Thermochemistry

Thermochemistry

Heat

• Energy can also be transferred as heat.

• Heat flows from warmer objects to cooler objects.

• HEAT THE ENERGY TRANSFERRED BETWEEN A SYSTEM AND ITS SURROUNDINGS AS A RESULT OF THEIR

DIFFERENCE IN TEMPERATURE

Page 12: Chapter 5 Thermochemistry

Thermochemistry

December 17

• First law of thermodynamics

• Internal energy

• Exchange of heat – endo and exo processes

• State functions

• Enthalpy – Heat of a reaction

• Calorimetry

Page 13: Chapter 5 Thermochemistry

Thermochemistry

Transferal of Energy

a) The potential energy of this ball of clay is increased when it is moved from the ground to the top of the wall.

Page 14: Chapter 5 Thermochemistry

Thermochemistry

Transferal of Energy

a) The potential energy of this ball of clay is increased when it is moved from the ground to the top of the wall.

b) As the ball falls, its potential energy is converted to kinetic energy.

Page 15: Chapter 5 Thermochemistry

Thermochemistry

Transferal of Energy

a) The potential energy of this ball of clay is increased when it is moved from the ground to the top of the wall.

b) As the ball falls, its potential energy is converted to kinetic energy.

c) When it hits the ground, its kinetic energy falls to zero (since it is no longer moving); some of the energy does work on the ball, the rest is dissipated as heat.

Page 16: Chapter 5 Thermochemistry

Thermochemistry

First Law of Thermodynamics• Energy is neither created nor destroyed.• In other words, the total energy of the universe is

a constant; if the system loses energy, it must be gained by the surroundings, and vice versa.

Use Fig. 5.5

Page 17: Chapter 5 Thermochemistry

Thermochemistry

Internal EnergyThe internal energy of a system is the sum of all kinetic and potential energies of all components of the system; we call it E.

Use Fig. 5.5

Page 18: Chapter 5 Thermochemistry

Thermochemistry

Internal EnergyBy definition, the change in internal energy, E, is the final energy of the system minus the initial energy of the system:

E = Efinal − Einitial

Use Fig. 5.5

Page 19: Chapter 5 Thermochemistry

Thermochemistry

Changes in Internal Energy

• If E > 0, Efinal > Einitial

Therefore, the system absorbed energy from the surroundings.

This energy change is called endergonic.

Page 20: Chapter 5 Thermochemistry

Thermochemistry

Changes in Internal Energy

• If E < 0, Efinal < Einitial

Therefore, the system released energy to the surroundings.

This energy change is called exergonic.

Page 21: Chapter 5 Thermochemistry

Thermochemistry

Changes in Internal Energy

• When energy is exchanged between the system and the surroundings, it is exchanged as either heat (q) or work (w).

• That is, E = q + w.

Page 22: Chapter 5 Thermochemistry

Thermochemistry

E, q, w, and Their Signs

Page 23: Chapter 5 Thermochemistry

Thermochemistry

Exchange of Heat between System and Surroundings

• When heat is absorbed by the system from the surroundings, the process is endothermic.

Page 24: Chapter 5 Thermochemistry

Thermochemistry

Exchange of Heat between System and Surroundings

• When heat is absorbed by the system from the surroundings, the process is endothermic.

• When heat is released by the system to the surroundings, the process is exothermic.

Page 25: Chapter 5 Thermochemistry

Thermochemistry

State Functions

Usually we have no way of knowing the internal energy of a system; finding that value is simply too complex a problem.

Page 26: Chapter 5 Thermochemistry

Thermochemistry

State Functions• However, we do know that the internal energy

of a system is independent of the path by which the system achieved that state. In the system below, the water could have reached

room temperature from either direction.

Page 27: Chapter 5 Thermochemistry

Thermochemistry

State Functions• Therefore, internal energy is a state function.

• It depends only on the present state of the system, not on the path by which the system arrived at that state.

• And so, E depends only on Einitial and Efinal.

Page 28: Chapter 5 Thermochemistry

Thermochemistry

State Functions

• However, q and w are not state functions.

• Whether the battery is shorted out or is discharged by running the fan, its E is the same.But q and w are different

in the two cases.

Page 29: Chapter 5 Thermochemistry

Thermochemistry

Work

PV work is the work associated with a change of

volume ( V) that occurs against a resisting pressure.

Page 30: Chapter 5 Thermochemistry

Thermochemistry

WorkWe can measure the work done by the gas if the reaction is done in a vessel that has been fitted with a piston.

w = −PV

Page 31: Chapter 5 Thermochemistry

Thermochemistry

Enthalpy

• If a process takes place at constant pressure (as the majority of processes we study do) and the only work done is this pressure-volume work, we can account for heat flow during the process by measuring the enthalpy of the system.

• Enthalpy is the internal energy plus the product of pressure and volume:

H = E + PV

Page 32: Chapter 5 Thermochemistry

Thermochemistry

Enthalpy

• When the system changes at constant pressure, the change in enthalpy, H, is

H = (E + PV)

• This can be written

H = E + PV

Page 33: Chapter 5 Thermochemistry

Thermochemistry

Enthalpy

• Since E = q + w and w = −PV, we can substitute these into the enthalpy expression:

H = E + PV

H = (q+w) − w

H = q

• So, at constant pressure the change in enthalpy is the heat gained or lost.

Page 34: Chapter 5 Thermochemistry

Thermochemistry

Endothermicity and Exothermicity

• A process is endothermic, then, when H is positive.

Page 35: Chapter 5 Thermochemistry

Thermochemistry

Endothermicity and Exothermicity

• A process is endothermic when H is positive.

• A process is exothermic when H is negative.

Page 36: Chapter 5 Thermochemistry

Thermochemistry

Enthalpies of Reaction

The change in enthalpy, H, is the enthalpy of the products minus the enthalpy of the reactants:

H = Hproducts − Hreactants

Page 37: Chapter 5 Thermochemistry

Thermochemistry

Enthalpies of Reaction

This quantity, H, is called the enthalpy of reaction, or the heat of reaction.

Page 38: Chapter 5 Thermochemistry

Thermochemistry

The Truth about Enthalpy

1. Enthalpy is an extensive property.

2. H for a reaction in the forward direction is equal in size, but opposite in sign, to H for the reverse reaction.

3. H for a reaction depends on the state of the products and the state of the reactants.

Page 39: Chapter 5 Thermochemistry

Thermochemistry

Practice problem– Change in enthalpy – Heat of reaction

3CuCl2 + 2Al 3Cu + 2AlCl3 ΔH = -793.5 kJ

1. What is ΔH for the following reaction?

6CuCl2 + 4Al 6Cu + 4AlCl3

2. What is ΔH for the following reaction?

9 Cu + 6 AlCl3 9 CuCl2 + 6 Al

3. Given the equation at the top of the page, how much energy will be given off by the reaction of 2.07 g of Al with excess CuCl2?

Page 40: Chapter 5 Thermochemistry

Thermochemistry

December 20

• Enthalpy practice

• Calorimetry

Page 41: Chapter 5 Thermochemistry

Thermochemistry

Constant Pressure Calorimetry

By carrying out a reaction in aqueous solution in a simple calorimeter such as this one, one can indirectly measure the heat change for the system by measuring the heat change for the water in the calorimeter.

Page 42: Chapter 5 Thermochemistry

Thermochemistry

Heat Capacity and Specific Heat• Calorimeter = apparatus that measures heat flow.• Heat capacity = the amount of energy required to raise

the temperature of an object (by one degree). (J °C-1)

• Molar heat capacity = heat capacity of 1 mol of a substance. (J mol-1 °C-1)

• Specific heat = specific heat capacity = heat capacity of 1 g of a substance. (J g-1 °C-1)

Tq substance of gramsheat specific

Page 43: Chapter 5 Thermochemistry

Thermochemistry

• Remember a change in T in K and in 0C are equal in magnitude

• T in K = T in 0C

Page 44: Chapter 5 Thermochemistry

Thermochemistry

Molar heat capacity

• The heat capacity of one mole of substance. The amount of heat required to increase the temperature of 1 mole of substance 1 K.

Page 45: Chapter 5 Thermochemistry

Thermochemistry

Constant Pressure Calorimetry• Atmospheric pressure is constant!

• HEAT LOST = HEAT GAINED

T

qq

qH P

solution of grams

solution ofheat specificsolnrxn

TmCTmC Object 1 Object 2

Page 46: Chapter 5 Thermochemistry

Thermochemistry

Constant Pressure Calorimetry

Because the specific heat for water is well known (4.184 J/mol-K), we can measure H for the reaction with this equation:

q = m s T

Page 47: Chapter 5 Thermochemistry

Thermochemistry

Heat Capacity and Specific Heat

Specific heat, then, is

Specific heat =heat transferred

mass temperature change

s =q

m T

Page 48: Chapter 5 Thermochemistry

Thermochemistry

Sample problem 1

Find the specific heat of water if 209 J is required to increased the temperature of 50.0 g of water by 1.00K s=q / m T

Page 49: Chapter 5 Thermochemistry

Thermochemistry

Sample Problem 2

• How much heat is needed to warm 250g of water from 25 0C to 75 0C.

• Specific heat of water 4.18 J/gK

• Find the molar heat capacity of water.

Page 50: Chapter 5 Thermochemistry

Thermochemistry

Sample problem 3

25.0 mL of 0.100 M NaOH is mixed with 25.0 mL of 0.100 M HNO3, and the temperature of the mixture increases from 23.1°C to 49.8°C. Calculate ΔH for this reaction in kJ mol-1. Assume that the specific heat of each solution is equal to the specific heat of water, 4.184 J g-1 °C-1.

Page 51: Chapter 5 Thermochemistry

Thermochemistry

Sample problem 4

An unknown metal is to be analyzed for specific heat. A 12.84-g piece of the metal is placed in boiling

water at 101.5°C until it attained that temperature. The metal is then removed from the boiling water

and placed into a styrofoam cup containing 54.92 g of water at 23.2°C. The final temperature of the

water was 26.1°C. What is the specific heat of the metal sample, in J g-1 °C-1?

Page 52: Chapter 5 Thermochemistry

Thermochemistry

Bomb Calorimetry

A more sophisticated model is the bomb calorimeter, it has a chamber where a chemical reaction takes place and a device to start the reaction.

Page 53: Chapter 5 Thermochemistry

Thermochemistry

HEAT CAPACITY OF THE CALORIMETER

• Heat is released when combustion occurs. The heat is absorbed by the calorimeter and the T of the water rises.

• THE HEAT CAPACITY OF THE CALORIMETER HAS TO BE CALCULATED. It is done by measuring T in a reaction that releases a known amount of heat. The heat capacity of the calorimeter Ccal= amount of heat absorbed / T

Page 54: Chapter 5 Thermochemistry

Thermochemistry

TCq calrxn

• Reaction carried out under constant volume.

• Use a bomb calorimeter.• Usually study combustion.

Bomb Calorimetry (Constant Volume Calorimetry)

Page 55: Chapter 5 Thermochemistry

Thermochemistry

Bomb Calorimetry

• Because the volume in the bomb calorimeter is constant, what is measured is really the change in internal energy, E, not H.

• For most reactions, the difference is very small.

Page 56: Chapter 5 Thermochemistry

Thermochemistry

Sample problem 5

A 0.5269 g sample of octane is placed in a bomb calorimeter with a heat capacity of 11.3 kJ °C-1. The original temperature of the water in the calorimeter is 21.93°C. After combustion, the temperature increases to 24.21°C. Determine the enthalpy of combustion per mole and per gram of octane.

Page 57: Chapter 5 Thermochemistry

Thermochemistry

Sample problem 6

• After 50 mL of 1.0 M HCl and 50mL of 1.0M NaOH are mixed in a coffe cup calorimeter, the temperature of the solution increases form 21.0 0C to 27.5 0C. Calculate the enthalpy change for the rx in kJ/mol of HCl assuming that the calorimeter loses only a negligible quantity of heat, total volume of solution is 100mL, that its density is 1.0 g/mL and the specific heat is 4.18J/gk

Page 58: Chapter 5 Thermochemistry

Thermochemistry

December 21

• MORE HESS LAW

• ENTHALPIES OF FORMATION

Page 59: Chapter 5 Thermochemistry

Thermochemistry

Hess’s Law

H is well known for many reactions, and it is inconvenient to measure H for every reaction in which we are interested.

• However, we can estimate H using H values that are published and the properties of enthalpy.

Page 60: Chapter 5 Thermochemistry

Thermochemistry

Hess’s Law

Hess’s law states that “If a reaction is carried out in a series of steps, H for the overall reaction will be equal to the sum of the enthalpy changes for the individual steps.”

Page 61: Chapter 5 Thermochemistry

Thermochemistry

Hess’s Law

Because H is a state function, the total enthalpy change depends only on the initial state of the reactants and the final state of the products.

Page 62: Chapter 5 Thermochemistry

Thermochemistry

Example

The bombardier beetle uses an explosive discharge as a defensive measure. The chemical reaction involved is the oxidation of hydroquinone by hydrogen peroxide to produce quinone and water:

C6H4(OH)2 (aq) + H2O2 (aq) C6H4O2 (aq) + 2 H2O (l)

Page 63: Chapter 5 Thermochemistry

Thermochemistry

C6H4(OH)2 (aq) C6H4O2 (aq) + H2 (g) ΔH = +177.4 kJ

H2 (g) + O2 (g) H2O2 (aq) ΔH = -191.2 kJ

H2 (g) + ½ O2 (g) H2O (g) ΔH = -241.8 kJ

H2O (g) H2O (l) ΔH = -43.8 kJ

C6H4(OH)2 (aq) + H2O2 (aq) C6H4O2 (aq) + 2 H2O (l)

ΔH = ???

Page 64: Chapter 5 Thermochemistry

Thermochemistry

Enthalpies of Formation

An enthalpy of formation, Hf, is defined as the enthalpy change for the reaction in which a compound is made from its constituent elements in their elemental forms.

Page 65: Chapter 5 Thermochemistry

Thermochemistry

Hof .

• Standard conditions (standard state): 1 atm and 25 oC (298 K).

• Standard enthalpy, Ho, is the enthalpy measured when everything is in its standard state.

• Standard enthalpy of formation: 1 mol of compound is formed from substances in their standard states.

• If there is more than one state for a substance under standard conditions, the more stable one is used.

• Standard enthalpy of formation of the most stable form of an element is zero.

Page 66: Chapter 5 Thermochemistry

Thermochemistry

Enthalpies of FormationEnthalpies of Formation

Page 67: Chapter 5 Thermochemistry

Thermochemistry

CONVENTIONAL DEFINITIONS OF STANDARD STATES FOR

ELEMENTS

• Is the form in which the element exist under conditions of 1 atm and 25 C.

• For O2 is gas.

• For Na is solid

• For Hg is liquid

• For C is graphite

• By definition the H of formation of the most stable form of an element is zero.

Page 68: Chapter 5 Thermochemistry

Thermochemistry

Examples – write formation reactions for each:

1. H2SO4

2. C2H5OH

3. NH4NO3

Page 69: Chapter 5 Thermochemistry

Thermochemistry

Examples

Use the tables in the back of your book to calculate ΔH for the following reactions:

1. 4 CuO (s) 2 Cu2O (s) + O2 (g)

2. C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

3. NH3 (g) + HCl (g) NH4Cl (s)

Page 70: Chapter 5 Thermochemistry

Thermochemistry

Using Enthalpies of Formation of Calculate Enthalpies of Reaction

• We use Hess’ Law to calculate enthalpies of a reaction from enthalpies of formation.

Page 71: Chapter 5 Thermochemistry

Thermochemistry

Using Enthalpies of Formation of Calculate Enthalpies of Reaction

• For a reaction

reactantsproductsrxn ff HmHnH

Page 72: Chapter 5 Thermochemistry

Thermochemistry

Calculation of H

We can use Hess’s law in this way:

H = nHf(products) - mHf(reactants)

where n and m are the stoichiometric coefficients.

Page 73: Chapter 5 Thermochemistry

Thermochemistry

Calculation of H

• Imagine this as occurringin 3 steps:

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

C3H8 (g) 3 C(graphite) + 4 H2 (g)

3 C(graphite) + 3 O2 (g) 3 CO2 (g)

4 H2 (g) + 2 O2 (g) 4 H2O (l)

Page 74: Chapter 5 Thermochemistry

Thermochemistry

Calculation of H

• Imagine this as occurringin 3 steps:

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

C3H8 (g) 3 C(graphite) + 4 H2 (g)

3 C(graphite) + 3 O2 (g) 3 CO2 (g)

4 H2 (g) + 2 O2 (g) 4 H2O (l)

Page 75: Chapter 5 Thermochemistry

Thermochemistry

Calculation of H

• Imagine this as occurringin 3 steps:

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

C3H8 (g) 3 C(graphite) + 4 H2 (g)

3 C(graphite) + 3 O2 (g) 3 CO2 (g)

4 H2 (g) + 2 O2 (g) 4 H2O (l)

Page 76: Chapter 5 Thermochemistry

Thermochemistry

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

C3H8 (g) 3 C(graphite) + 4 H2 (g)

3 C(graphite) + 3 O2 (g) 3 CO2 (g)

4 H2 (g) + 2 O2 (g) 4 H2O (l)

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

Calculation of H

• The sum of these equations is:

Page 77: Chapter 5 Thermochemistry

Thermochemistry

C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)

Calculation of H

H = [3(-393.5 kJ) + 4(-285.8 kJ)] - [1(-103.85 kJ) + 5(0 kJ)]

= [(-1180.5 kJ) + (-1143.2 kJ)] - [(-103.85 kJ) + (0 kJ)]

= (-2323.7 kJ) - (-103.85 kJ)

= -2219.9 kJ

Page 78: Chapter 5 Thermochemistry

Thermochemistry

Energy in FoodsMost of the fuel in the food we eat comes from carbohydrates and fats.

Page 79: Chapter 5 Thermochemistry

Thermochemistry

Fuels

The vast majority of the energy consumed in this country comes from fossil fuels.

Page 80: Chapter 5 Thermochemistry

Thermochemistry

HW

• PRELAB FOR HESS LAW LAB DUE TOMORROW (Lab 6 – page 25)

• Remember test on monday

• Hw for Thursday up to 5.77 odd

Page 81: Chapter 5 Thermochemistry

Thermochemistry

Example

Calculate the total energy produced from the combustion of one gram of gasoline (assume it is pure octane, C8H18). Compare that to the energy produced from the combustion of one gram of ethanol (a renewable fuel – C2H5OH)

Page 82: Chapter 5 Thermochemistry

Thermochemistry

• Hess’s law: if a reaction is carried out in a number of steps, H for the overall reaction is the sum of H for each individual step.

• For example:

CH4(g) + 2O2(g) CO2(g) + 2H2O(g) H = -802 kJ

2H2O(g) 2H2O(l) H = -88 kJ

CH4(g) + 2O2(g) CO2(g) + 2H2O(l) H = -890 kJ

Page 83: Chapter 5 Thermochemistry

Thermochemistry

Note that: H1 = H2 + H3

Page 84: Chapter 5 Thermochemistry

Thermochemistry

JANUARY 8

• Prelab

• Foods and fuels. Read from txbook

• Hess law problems

Page 85: Chapter 5 Thermochemistry

Thermochemistry

Foods• Fuel value = energy released when 1 g of substance is

burned.• 1 nutritional Calorie, 1 Cal = 1000 cal = 1 kcal.• Energy in our bodies comes from carbohydrates and fats

(mostly).• Intestines: carbohydrates converted into glucose:

C6H12O6 + 6O2 6CO2 + 6H2O, H = -2816 kJ

• Fats break down as follows:2C57H110O6 + 163O2 114CO2 + 110H2O, H = -75,520 kJ

• Fats: contain more energy; are not water soluble, so are good for energy storage.

Page 86: Chapter 5 Thermochemistry

Thermochemistry

Fuels• In 2000 the United States consumed 1.03 1017 kJ of

fuel.• Most from petroleum and natural gas.• Remainder from coal, nuclear, and hydroelectric.• Fossil fuels are not renewable.

Page 87: Chapter 5 Thermochemistry

Thermochemistry

Sources of Sources of energy energy

consumed in consumed in USAUSA