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THERMOCHEMISTRY: Part 1. Energy Flow and Chemical Change GENERAL CHEMISTRY LECTURE 6

Lecture 6. Thermochemistry (Part 1)

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Page 1: Lecture 6. Thermochemistry (Part 1)

THERMOCHEMISTRY: Part 1. Energy Flow and Chemical Change

GENERAL CHEMISTRY

LECTURE 6

Page 2: Lecture 6. Thermochemistry (Part 1)

6.1 Define Thermochemistry

6.2 Define Energy, Heat and Work

6.3 Discuss the Principle of Heat Flow

6.4 Define Enthalpy

6.5 Calorimtery: heat capacity and specific heat

Scope

6.6 Stoichiometry of Thermal Equations

6.7 Hess’s Law

6.8 Standard Heats of Reaction (DHo rxn)

6.9 Bond Energies

Page 3: Lecture 6. Thermochemistry (Part 1)

Thermodynamics– the study of the energy transfers accompanying physical and chemical changes

Thermochemistry- part of thermodynamics which deals with heat involved in physical and chemical changes

What is Thermochemistry?

Page 4: Lecture 6. Thermochemistry (Part 1)

What is Energy?

• Energy is the capacity to do work or to produce heat.

• Law of conservation of energy

– Energy can be converted from one form to another but can be neither created nor destroyed

– The total energy content of the universe is constant.

• Potential energy – energy due to position or composition.

• Kinetic energy – energy due to motion of the object and depends on the mass of the object and its velocity.

Page 5: Lecture 6. Thermochemistry (Part 1)

Internal Energy

• Internal energy E of a system is the sum of the kinetic and potential energies of all the “particles” in the system.

• The total amount of energy contained in a system

Page 6: Lecture 6. Thermochemistry (Part 1)

Components of Internal Energy

• Thermal Energy

– Kinetic energy associated with random molecular motion.

– In general proportional to temperature.

• Chemical Energy

– Potential energy associated with chemical bonds and intermolecular forces of attraction.

Page 7: Lecture 6. Thermochemistry (Part 1)

Internal Energy

• System – part of the universe on which we wish to focus attention.

• Surroundings – include everything else in the universe.

• Systems + Surroundings = Universe

Page 8: Lecture 6. Thermochemistry (Part 1)

Types of Systems

Page 9: Lecture 6. Thermochemistry (Part 1)

Energy Transfers

• Heat, q

- involves the transfer of energy between two objects due to a temperature difference.

• Work, w

– force acting over a distance.

• Change in Internal Energy:

• Energy is a state function; work and heat are not.

DE = q + w

Page 10: Lecture 6. Thermochemistry (Part 1)

– It only depends on the difference between the final and initial state.

– Independent of path

What is a State Function?

Page 11: Lecture 6. Thermochemistry (Part 1)

First Law of Thermodynamics

• Law of conservation of energy is often called the first law of thermodynamics.

• Energy gained by the surroundings must be equal to the energy lost by the system.

DEuniverse = DEsystem + DEsurrounding = 0

Page 12: Lecture 6. Thermochemistry (Part 1)

Energy Transfers

• Heat - involves the transfer of energy between two objects due to a temperature difference.

• Work – force acting over a distance.

DE = q + w

Page 13: Lecture 6. Thermochemistry (Part 1)

Heat

• Heat “flows” from hotter to colder.

• Sign reflects the system’s point of view.

• Endothermic Process:

– Heat flow is into a system.

– q is positive

• Exothermic Process: – Heat flows out of the system

– q is negative

Page 14: Lecture 6. Thermochemistry (Part 1)

Heat

heat heat

Exothermic, q < 0 Endothermic, q > 0

Page 15: Lecture 6. Thermochemistry (Part 1)

A system transferring energy as heat only

A. Heat flow out from a system B. Heat flow into a system

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Concept Check

1. Is the freezing of water an endothermic or exothermic process? Explain.

Page 17: Lecture 6. Thermochemistry (Part 1)

Concept Check

2. Classify each process as exothermic or endothermic. Explain. The system is underlined in each example.

– Your hand gets cold when you touch ice.

– The ice gets warmer when you touch it.

– Water boils in a kettle being heated on a stove.

– Water vapor condenses on a cold pipe.

– Ice cream melts.

Page 18: Lecture 6. Thermochemistry (Part 1)

Work

FIGURE 7-7 Illustrating work (expansion) during the chemical reaction

2 KClO3(s) 2 KCl(s) + 3 O2(g)

In addition to heat effects chemical reactions may also do work.

Gas formed pushes against the atmosphere.

The volume changes.

Pressure-volume work.

Page 19: Lecture 6. Thermochemistry (Part 1)

Work

• Work = P × A × Δh = PΔV

– P is pressure.

– A is area.

– Δh is the piston moving a distance.

– ΔV is the change in volume.

Page 20: Lecture 6. Thermochemistry (Part 1)

A system transferring energy as work only

1. Work done by system

2. Work done on a system

w < 0, DE < 0

w > 0, DE > 0

Page 21: Lecture 6. Thermochemistry (Part 1)

Exercise

Which of the following performs more work?

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.

c) They perform the same amount of work.

Page 22: Lecture 6. Thermochemistry (Part 1)

Summary

Page 23: Lecture 6. Thermochemistry (Part 1)

Exercise

Calculate the change in internal energy for a system undergoing an endothermic process in which 15.6 kJ of heat flows and where 1.4 kJ of work is done on the system.

ΔE = q + w

ΔE = 15.6 kJ + 1.4 kJ = 17.0 kJ

Page 24: Lecture 6. Thermochemistry (Part 1)

Change in Enthalpy, ΔH

• Is the heat lost or gained during a chemical or physical change that occurs at constant pressure, qp.

• ΔH = q at constant pressure

• State function

• ΔHrxn = Hproducts – Hreactants

Page 25: Lecture 6. Thermochemistry (Part 1)

Heats of Reaction: DE and DH

Reactants → Products

Ei Ef

DE = Ef - Ei

DE = qrxn + w

In a system at constant volume:

DE = qrxn + 0 = qrxn = qv

But we live in a constant pressure world! How does qp relate to qv?

Page 26: Lecture 6. Thermochemistry (Part 1)

Two different paths leading to the same internal energy change in a system

Page 27: Lecture 6. Thermochemistry (Part 1)

Heats of Reaction

qV = qP + w

We know that w = - PDV and DU = qv, therefore:

DU = qP - PDV

qP = DU + PDV

These are all state functions, so define a new function.

Let enthalpy be H = U + PV

Then DH = Hf – Hi = DU + DPV

If we work at constant pressure and temperature:

DH = DU + PDV = qP

Page 28: Lecture 6. Thermochemistry (Part 1)

How do we measure the heat released (or absorbed)

by a physical or chemical change?

• Calorimetry

– Science of measuring heat

• Specific heat capacity

– The energy required to raise the temperature of one gram of a substance by one degree Celsius.

• Molar heat capacity

– The energy required to raise the temperature of one mole of substance by one degree Celsius.

Page 29: Lecture 6. Thermochemistry (Part 1)

q α ∆T or q = constant x ∆T or q = constant

∆T

Heat Capacity

The quantity of heat required by an objective to change its temperature by 1 ᵒC.

Heat capacity = q

∆T [in units of J/ᵒC]

Heat Capacity

q = C x DT

Page 30: Lecture 6. Thermochemistry (Part 1)

Specific Heat Capacity, c

The quantity of heat required by to change the temperature of 1 gram of a substance by 1 ᵒC

Specific heat capacity, c =

q

mass x ∆T [in units of J/g-ᵒC]

q = mass x c x DT

Molar Heat Capacity

The quantity of heat required by to change the temperature of 1 mole of a substance by 1 ᵒC

Molar heat capacity, C = q

mole x ∆T

[in units of J/mol-ᵒC]

Heat Capacity

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Page 32: Lecture 6. Thermochemistry (Part 1)

Units of heat

• Calorie (cal)

– The quantity of heat required to change the temperature of one gram of water by one degree Celsius.

• Joule (J)

– SI unit for heat

1 cal = 4.184 J

Page 33: Lecture 6. Thermochemistry (Part 1)

A layer of copper welded to the bottom of a skillet weighs 125 g. How much heat is needed to raise the temperature of the copper layer from 25oC to 300.oC? The specific heat capacity (c) of Cu is 0.387 J/g•K.

SOLUTION: q = mass x c x DT

q = 125 g (300oC - 25oC) x x = 1.33 x 104 J 0.387 J/g•K

*DT in oC is the same as for K.

*q = mcDT

Finding the Quantity of Heat from Specific Heat

Capacity

Page 34: Lecture 6. Thermochemistry (Part 1)

Is used to measure the heat released (or absorbed) by a physical or chemical change.

Constant- pressure calorimeters

Constant- volume calorimeters

Assumptions: NO heat flows out of the calorimeter

(Adiabatic system)

Calorimeter

Page 35: Lecture 6. Thermochemistry (Part 1)

Calorimetry

• Energy gained/lost by the system (reaction) is equal to the energy lost/gain by the calorimeter.

• If two reactants at the same temperature are mixed and the resulting solution gets warmer, this means the reaction taking place is exothermic.

• An endothermic reaction cools the solution.

Page 36: Lecture 6. Thermochemistry (Part 1)

- qsys = qsurr

- qsolid = qcal + qH2O

qsolid = msolidcsolid DT qcal = Ccal DT qH2O = mH2OcH2O DT

- qsolid = qH2O

Coffee-cup Calorimeter

Page 37: Lecture 6. Thermochemistry (Part 1)

- qsys = qsurr

- qrxn = qcal + qH2O

qrxn = nLR (DHrxn) qcal = Ccal DT qH2O= mH2OcH2O DT

Measuring Heats of Chemical Reaction

Page 38: Lecture 6. Thermochemistry (Part 1)

You place 50.0 mL of 0.500 M NaOH in a coffee-cup calorimeter at 25.00oC and carefully add 25.0 mL of 0.500 M HCl, also at 25.00oC. After stirring, the final temperature is 27.21oC. Calculate qsoln (in J) and DHrxn (in kJ/mol). (Assume the total volume is the sum of the individual volumes and that the final solution has the same density and specific heat capacity as water: d = 1.00 g/mL and c = 4.184 J/g•K)

qsoln = masssoln x specific heatsoln x DT

DHrxn = qrxn

nLR

- qsol’n =

*[unit: J ]

*[unit: J /mol or kJ/mol]

qsoln = msoln x csoln x DT

nLR

Determining the Heats of a Reaction

Page 39: Lecture 6. Thermochemistry (Part 1)

You place 50.0 mL of 0.500 M NaOH in a coffee-cup calorimeter at 25.00oC and carefully add 25.0 mL of 0.500 M HCl, also at 25.00oC. After stirring, the final temperature is 27.21oC. Calculate qsoln (in J) and DHrxn (in kJ/mol). (Assume the total volume is the sum of the individual volumes and that the final solution has the same density and specific heat capacity as water: d = 1.00 g/mL and c = 4.184 J/g•K)

Determining the Heats of a Reaction

Total volume after mixing = 50.0 mL + 25.0 mL = 75.0 mL

75.0 mL x 1.00 g/mL = 75.0 g of water

qsoln = mass x specific heat x DT

= 75.0 g x 4.184 J/g•oC x (27.21oC - 25.00oC)

qsoln = 693 J

Finding masssoln

qsoln = msoln x csoln x DT

Page 40: Lecture 6. Thermochemistry (Part 1)

You place 50.0 mL of 0.500 M NaOH in a coffee-cup calorimeter at 25.00oC and carefully add 25.0 mL of 0.500 M HCl, also at 25.00oC. After stirring, the final temperature is 27.21oC. Calculate qsoln (in J) and DHrxn (in kJ/mol). (Assume the total volume is the sum of the individual volumes and that the final solution has the same density and specific heat capacity as water: d = 1.00 g/mL and c = 4.184 J/g•K)

Determining the Heats of a Reaction

- (693 J/0.0125 mol)(kJ/103 J) = -55.4 kJ/ mol

For NaOH 0.500 M x 0.0500 L = 0.0250 mol OH-

For HCl 0.500 M x 0.0250 L = 0.0125 mol H+

HCl(aq) + NaOH(aq) NaCl(aq) + H2O(l) H+(aq) + OH-(aq) H2O(l)

HCl is the limiting reactant. 0.0125 mol of H2O will form during the reaction.

DHrxn = ? DHrxn = qrxn

nLR

- qsol’n nLR

=

DHrxn (kJ/mol)=

Page 41: Lecture 6. Thermochemistry (Part 1)

Bomb Calorimeter

- qsys = qsurr

- qsample = qcalorimeter

qsolid = msolidcsolid DT qcal = Ccal DT

Measuring Heats of Combustion

Page 42: Lecture 6. Thermochemistry (Part 1)

A manufacturer claims that its new dietetic dessert has “fewer than 10 Calories per serving.” To test the claim, a chemist at the Department of Consumer Affairs places one serving in a bomb calorimeter and burns it in O2 (the heat capacity of the calorimeter = 8.151 kJ/K). The temperature increases 4.937oC. Is the manufacturer’s claim correct?

- q sample = qcalorimeter

qcalorimeter = heat capacity x DT = 8.151 kJ/K x 4.937 K = 40.24 kJ

1 Calorie = 1 kcal = 4.184 kJ

The manufacturer’s claim is true.

10 Calorie = 41.84 kJ

Calculating the Heat of a Combustion

Reaction

Page 43: Lecture 6. Thermochemistry (Part 1)

A 30.5 g sample of an alloy at 93.0 ᵒC is placed into a 50.0 g of water at 22.0 ᵒC in an insulated coffee cup with a heat capacity of 9.2 J/K. If the final temperature of the system is 31.1 ᵒC, what is the specific heat capacity of the alloy? (cH2O = 4.184 J/g•K)

- qalloy = qcal + qH2O

- (malloy x calloy x DT) = (Ccal x DT) + (mH2O x cH2O x DT )

- [30.5 g x calloy x (31.1 ᵒC - 93.0 ᵒC ) = [( 9.3 J/K) x (31.1 ᵒC - 22.0 ᵒC )] +

[(50.0 g) x (4.184 J/g-K) x (31.1 ᵒC - 22.0 ᵒC )]

calloy = (84.63 J ) + (1903.72 J)

1887.95 g-ᵒC

calloy = 1.053 J/g-ᵒC

Determining the Specific Heat Capacity

Page 44: Lecture 6. Thermochemistry (Part 1)

High purity benzoic acid (C6H5COOH; ∆Hrxn for combustion = 3227 kJ/mol) is used as a standard for calibrating bomb calorimeter. A 1.221-g sample burns in a calorimeter (heat capacity = 1365 J/C) that contains exactly 1.200 kg of water. What temperature change is observed?

- qbenzoic acid = qcal + qH2O

- (DHrxn x nLR) = (Ccal x DT) + (mH2O x cH2O x DT )

[Ccal + (mH2O x cH2O)]x DT

- (3227 kJ/mol x ) = 1.221 g 122.1 g/mol

[1.365 kJ/C + (1200 g x 4.184 x10-3kJ/g-ᵒC)]x DT

- (DHrxn x ) = g

MW

DT = [1.365 kJ/ᵒC + (5.0208 kJ/ᵒC)]

- 32.27kJ

DT = - 5.05 ᵒC

Determining Changes in Temperature

Page 45: Lecture 6. Thermochemistry (Part 1)

Thermochemical Equations

• balanced chemical equation that includes the heat of reaction (DHrxn)

• Examples:

A + B C + D DHrxn= 100 kJ/mol

X + Y XY DHrxn= -120 kJ/mol

A + B + 100 kJ C + D

X + Y XY + 120 kJ

Page 46: Lecture 6. Thermochemistry (Part 1)

1. Sign – will depend on whether the reaction is exothermic (-) or endothermic (+). The forward reaction has the opposite sign of the reverse reaction.

2H2O(l) 2H2(g) + O2(g) DHrxn = 572 kJ

2H2(g) + O2(g) 2H2O(l) DHrxn = -572 kJ

2. Magnitude – DH is proportional to the amount of substance reacting.

286 kJ is thermochemical equivalent to 1 mol of H2(g)

286 kJ is thermochemical equivalent to 1/2 mol of O2(g)

286 kJ is thermochemical equivalent to 1mol of H2O (l)

H2(g) + O2(g) H2O(l) DHrxn = -286 kJ 1

2

Properties of DHrxn

Page 47: Lecture 6. Thermochemistry (Part 1)

In each of the following cases, determine the sign of DH, state whether the reaction is exothermic or endothermic.

(a) H2(g) + O2(g) H2O(l) + 285.8 kJ

(b) 40.7 kJ + H2O(l) H2O(g)

1

2

Solution:

(a) Heat is in the product side , heat is produce in the reaction.

DHrxn < 0 Exothermic reaction

(b) Heat is in the reactant side , heat is gained in the reaction.

DHrxn > 0 Endothermic reaction

Determining the Sign of DHrxn

Page 48: Lecture 6. Thermochemistry (Part 1)

SOLUTION:

Consider the following balanced thermochemical equation for a reaction sometimes used for H2S production.

S8(s) + 8H2(g) 8H2S (g) DHrxn = -20.2 kJ

a. Is this an exothermic or endothermic reaction?

b. What is the DHrxn for the reverse reaction?

c. What is the DH when 2.6 mol of S8 reacts?

d. What is the DH when 25.0 g of H2 reacts?

a. Exothermic reaction

b. DHrxn = 20.2 kJ

c. 2.6 mol S8

- 20.2 kJ

1 mol S8

= - 52.52 kJ x

d. 25.0 g H2

- 20.2 kJ

8 mol H2

= - 505 kJ x

Stoichiometry Involving Heats of Reactions

Page 49: Lecture 6. Thermochemistry (Part 1)

The major source of aluminum in the world is bauxite (mostly aluminum oxide). Its thermal decomposition can be represented by

If aluminum is produced this way, how many grams of aluminum can form when 1.000 x 103 kJ of heat is transferred?

Al2O3(s) 2Al(s) + O2(g) DHrxn = 1676 kJ

1.000 x 103 kJ x 2 mol Al

1676 kJ

26.98 g Al

1 mol Al = 32.20 g Al x

3

2

Solution:

Stoichiometry Involving Heats of Reactions

Page 50: Lecture 6. Thermochemistry (Part 1)

* Indirect Determination of DH:

Hess’s Law

• DH is an extensive property.

–Enthalpy change is directly proportional to the amount of substance in a system.

N2(g) + O2(g) → 2 NO(g) DH° = +180.50 kJ

½N2(g) + ½O2(g) → NO(g) DH° = +90.25 kJ

• DH changes sign when a process is reversed

NO(g) → ½N2(g) + ½O2(g) DH° = -90.25 kJ

Page 51: Lecture 6. Thermochemistry (Part 1)

Hess’s Law

• the enthalpy change, DH of an overall process is the sum of the enthalpy changes of its individual steps

• 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 series of steps.

DH total= DHrxn1 + DHrxn2 + DHrxn3 + …

Page 52: Lecture 6. Thermochemistry (Part 1)

Hess’s Law Schematically

Page 53: Lecture 6. Thermochemistry (Part 1)

Hess’s law of constant heat summation

If a process occurs in stages or steps (even hypothetically), the enthalpy change for the overall process is the sum of the enthalpy changes for the individual steps.

½N2(g) + O2(g) → NO2(g) DH° = +33.18 kJ

½N2(g) + O2(g) → NO(g) + ½ O2 (g) DH° = +90.25 kJ

NO(g) + ½O2(g) → NO2(g) DH° = -57.07 kJ

Page 54: Lecture 6. Thermochemistry (Part 1)

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 disposal.

• Reverse any reactions as needed to give the required reactants and products.

• Multiply reactions to give the correct numbers of reactants and products.

Page 55: Lecture 6. Thermochemistry (Part 1)

Example: Hess’s law of constant heat

summation

• Consider the following data:

• Calculate ΔH for the reaction

3 2 2

2 2 2

1 3

2 2NH ( ) N ( ) H ( ) H = 46 kJ

2 H ( ) O ( ) 2 H O( ) H = 484 kJ

D

D

g g g

g g g

2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g

Page 56: Lecture 6. Thermochemistry (Part 1)

Hess’s law of constant heat summation

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

D

D

g g g

g g g

3 2 2

2 2 2

1 3

2 2NH ( ) N ( ) H ( ) H = 46 kJ

2 H ( ) O ( ) 2 H O( ) H = 484 kJ

D

D

g g g

g g g

Page 57: Lecture 6. Thermochemistry (Part 1)

Hess’s law of constant heat summation

4 ( ) 4( )

3 ( ) 3( )

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

D

D

g g g

g g g

2 2 3

2 2 2

2 N ( ) 6 H ( ) 4 NH ( ) H = 184 kJ

6 H O( ) 6 H ( ) 3 O ( ) H = +1452 kJ

D

D

g g g

g g g

Page 58: Lecture 6. Thermochemistry (Part 1)

Hess’s law of constant heat summation

• Final reactions:

ΔH = +1268 kJ

2 2 2 32 N ( ) 6 H O( ) 3 O ( ) 4 NH ( ) g g g g

2 2 3

2 2 2

2 N ( ) 6 H ( ) 4 NH ( ) H = 184 kJ

6 H O( ) 6 H ( ) 3 O ( ) H = +1452 kJ

D

D

g g g

g g g

Page 59: Lecture 6. Thermochemistry (Part 1)

Oxidation of sulfur to sulfur trioxide

S(s) + O2(g) SO2(g) DH1 = -296.8 kJ Equation 1:

2SO2(g) + O2(g) 2SO3(g) DH2 = -198.4 kJ Equation 2:

S(s) + O2(g) SO3(g) DH3 = ? Equation 3: 3

2

S(s) + O2(g) SO2(g) DH1 = -296.8 kJ Equation 1:

SO2(g) + O2(g) SO3(g) ½(DH2) = -99.2 1/2(Equation 2):

S(s) + O2(g) + SO2(g) + O2(g) SO2(g) + SO3(g)

Equation 3:

1

2

1

2

S(s) + O2(g) SO3(g) DH3 = ? 3

2

DH 3= DH1 + ½(DH2) = -296.8 kJ + (-99.2 kJ) = -396.0 kJ

Using Hess’s Law to Calculate an Unknown ∆H

Page 60: Lecture 6. Thermochemistry (Part 1)

SOLUTION:

PROBLEM: Two gaseous pollutants that form in auto exhaust are CO and NO. An environmental chemist is studying ways to convert them to less harmful gases through the following equation:

CO(g) + NO(g) CO2(g) + N2(g) DH = ?

Given the following information, calculate the unknown DH:

Equation A: CO(g) + O2(g) CO2(g) DHA = -283.0 kJ

Equation B: N2(g) + O2(g) 2NO(g) DHB = 180.6 kJ

DHB = - 90.3 kJ

CO(g) + O2(g) CO2(g) DHA = -283.0 kJ

NO(g) N2(g) + O2(g)

DHrxn = -373.3 kJ CO(g) + NO(g) CO2(g) + N2(g)

1

2

1

2

1

2

1

2

1

2

1

2

Using Hess’s Law to Calculate an Unknown ∆H

Page 61: Lecture 6. Thermochemistry (Part 1)

PROBLEM: Calculate the DH rxn for:

2NOCl(g) N2(g) + O2(g) + Cl2(g) DHrxn = ?

Given the following set of reactions:

N2(g) + O2(g) NO(g) DH1 = 90.3 kJ 1

2

1

2

NO(g) + Cl2(g) NOCl(g) DH2 = 38.6 kJ 1

2

2NOCl(g) 2NO(g) + Cl2(g)

2NO(g) N2(g) + O2(g)

2NOCl(g) N2(g) + O2(g) + Cl2(g)

-2 (DH2) = - 77.2 kJ

-2 (DH1 )= - 180.6 kJ

DHrxn = - 257.8 kJ

Using Hess’s Law to Calculate an Unknown ∆H

Page 62: Lecture 6. Thermochemistry (Part 1)

2. Diamond and graphite are two crystalline forms of carbon. At 1 atm and 250C, diamond changes to graphite so slowly that the ethalpy change of the process must be obtained indirectly. Determine ∆Hrxn for C(diamond) C(graphite)

With equations from the following list:

C(diamond) + O2(g) CO2(g) ∆H= -395.4kJ 2CO2(g) 2CO(g) + O2(g) ∆H= 566.0 kJ C(graphite) + O2(g) CO2(g) ∆H= -393.5kJ 2CO(g) C(graphite) + CO2(g) ∆H= -172.5kJ

1. A coffee-cup calorimeter is used to determine the specific heat of a metallic sample. The calorimeter is filled with 50.0mL of water at 25.0C (density = 0.997 g/mL). A 36.5-gram sample of metallic material is taken from water boiling at 100.0C and placed in the calorimeter. The equilibrium temperature of the water and sample is 32.5C. The calorimeter constant is known to be 1.87 J/C. Calculate the specific heat of the metallic material. The specific heat of water is 4.184 J/g-C.

Homework

Page 63: Lecture 6. Thermochemistry (Part 1)

Standard Enthalpies of Formation, DHf°

•The enthalpy change that occurs in the formation of one mole of a substance in the standard state from the reference forms of the elements in their standard states.

The standard enthalpy of formation of a pure element in its reference state is 0.

Page 64: Lecture 6. Thermochemistry (Part 1)

Conventional Definitions of Standard States

• For a Compound

– For a gas, pressure is exactly 1 atm.

– 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.

– Heat of formation is zero.

Page 65: Lecture 6. Thermochemistry (Part 1)

Standard Enthalpy of Formation

Page 66: Lecture 6. Thermochemistry (Part 1)
Page 67: Lecture 6. Thermochemistry (Part 1)

Some standard enthalpies of formation at 298.15 K

number of carbons

Page 68: Lecture 6. Thermochemistry (Part 1)

Determining the ∆H ᵒrxn from ∆H ᵒf of reactants

and products

• The change in enthalpy for a given reaction can be calculated from the enthalpies of formation of the reactants and products:

DH ᵒrxn = Σ m DHᵒf (products) - Σ n DHᵒf (reactants)

Page 69: Lecture 6. Thermochemistry (Part 1)

Step 1: Each reactants decomposes to its element, the standard enthalpy change is - DHᵒf

Step 2: Each product forms from its elements, the standard enthalpy change is DHᵒf

TiCl4(l) + 2H2O(g) TiO2(s) + 4HCl (g) DHᵒrxn = ?

TiCl4(l) Ti(s) + 2Cl2 (g) -DHᵒf [TiCl4(l)]

2H2O(g) 2H2(g) + O2(g) -2DHᵒf [2H2O(g)]

Ti(s) + O2(g) TiO2(s) DHᵒf [TiO2(s)]

2H2(g) + 2Cl2(g) 4HCl(g) 4 DHᵒf [HCl(g]

TiCl4(l) + 2H2O(g) TiO2(s) + 4HCl (g) DHᵒrxn = ?

DHᵒrxn = {DHᵒf [TiO2(s)] + 4 DHᵒf [HCl(g]} + {-DHᵒf [TiCl4(l)]} + {-2DHᵒf [2H2O(g)]}

DH ᵒrxn = Σ m DHᵒf (products) - Σ n DHᵒf (reactants)

Determining the ∆H ᵒrxn from ∆H ᵒf of reactants and products.

Page 70: Lecture 6. Thermochemistry (Part 1)

Exercise

Calculate ∆H°rxn for the following reaction: 2Na(s) + 2H2O(l) → 2NaOH(aq) + H2(g)

Given the following information: ∆Hf° (kJ/mol) Na(s) 0 H2O(l) –286 NaOH(aq) –470 H2(g) 0 ∆H°rxn = –368 kJ/mol

Page 71: Lecture 6. Thermochemistry (Part 1)

Calculate the DH orxn for the combustion of C3H8 using the following values for DH of.

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

C3H8 (g): DH of = -103.8 kJ CO2(g): DH of = -393.5 kJ H2O (l): DH of = -285.8 kJ

DHrxn = 3 DHᵒf [CO2(g)] + 4 DHᵒf [H2O(g] + -DHᵒf [C3H8(g)] + -5DHᵒf [O2(g)]

DHrxn = 3 (-393.5 kJ) + 4 (-285.8 kJ) + [- (-103.8 kJ) -5(0 kJ)]

DHrxn = - 2219.9 kJ

Calculating the Heat of Reaction from Heats of

Formation

Page 72: Lecture 6. Thermochemistry (Part 1)

SOLUTION:

PROBLEM: Nitric acid, whose worldwide annual production is about 10 billion kilograms, is used to make many products, including fertilizer, dyes, and explosives. The first step in the industrial production process is the oxidation of ammonia:

Calculate DHorxn from DHo

f values.

4NH3(g) + 5O2(g) 4NO(g) + 6H2O(g)

DHrxn = S mDHof (products) - S nDHo

f (reactants)

DHorxn = {4[DHo

f NO(g)] + 6[DHof H2O(g)]} - {4[DHo

f NH3(g)] + 5[DHof O2(g)]}

= (4 mol)(90.3 kJ/mol) + (6 mol)(-241.8 kJ/mol) -

[(4 mol)(-45.9 kJ/mol) + (5 mol)(0 kJ/mol)] DHo

rxn = -906 kJ/mol

Calculating the Heat of Reaction from Heats of

Formation

NH3 (g): DH of = -45.9 kJ/mol NO(g): DH of = 90.3 kJ/mol H2O (l): DH of = -241.8 kJ/mol

Page 73: Lecture 6. Thermochemistry (Part 1)

DHorxn = DHo

reactant bonds broken + DHoproduct bonds formed

Using Bond Energies to Calculate ∆Horxn

DHorxn = Σ m BEreactants - Σ n BE products

Page 74: Lecture 6. Thermochemistry (Part 1)

Using Bond Energies to Calculate ∆Horxn

CH4 (g) + 2O2 (g) CO2 (g) + 2H2O (g)

Page 75: Lecture 6. Thermochemistry (Part 1)

Exercises Using Bond Energies to Calculate DHorxn

SOLUTION:

PROBLEM: Calculate DHorxn for the chlorination of methane to form chloroform:

CH4(g) + 3Cl2(g) CHCl3(g) + 3HCl(g)

H

C H

H

H + Cl Cl3

Cl

C Cl

Cl

H + H Cl3

bonds broken bonds formed

Bond Energy, kJ/mol C-H : 413 kJ/mol Cl-Cl: 243 kJ/mol C-Cl: 339 kJ/mol H-Cl: 427 kJ/mol

Answer: DHorxn = - 330 kJ/mol

Page 76: Lecture 6. Thermochemistry (Part 1)

Exercises Using Bond Energies to Calculate DHorxn

PROBLEM: Calculate DHorxn for the combustion of ethanol.

CH3CH2OH(g) + 3O2(g) 2CO2(g) + 3H2O(g)

Bond Energy, kJ/mol C-H : 413 kJ/mol C-O: 358 kJ/mol C-C: 347 kJ/mol O-H: 467 kJ/mol C=O: 799 kJ/mol O=O: 498 kJ/mol

Page 77: Lecture 6. Thermochemistry (Part 1)

2. Solving enthalpy of reaction (heat of reaction), DHrxn

a. Calorimetry

Skills that you should have learned

b. Hess’s Law

c. Standard Enthalpy of formation, DH of.

1. Solving heat generated (or absorbed) by a chemical reaction, q.

d. Bond energy

Page 78: Lecture 6. Thermochemistry (Part 1)

Additional Exercises

Consider the combustion of propane:

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