chapter 5 energy & enthalpy thermodynamics (rev. 0910)

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Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

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Page 1: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Chapter 5

Energy & EnthalpyThermodynamics

(rev. 0910)

Page 2: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Definition

• Thermodynamics- is the study of energy transformations.

Page 3: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Chemical Reactions

• Chemical reactions involve not just the conversion of reactants into products, but also involve an energy change in the form of heat—heat released as the result of a reaction, or heat absorbed as a reaction proceeds.

• Energy changes accompany all chemical reactions and are due to rearranging of chemical bonding.

Page 4: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Making Bonds

• Addition of energy is always a requirement for the breaking of bonds but the breaking of bonds in and of itself does not release energy.

• Energy release occurs when new bonds are formed.

Page 5: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Bond Energy

• If more energy is released when new bonds form than was required to break existing bonds, then the difference will result in an overall release of energy.

• If, on the other hand, more energy is required to break existing bonds than is released when new bonds form, the difference will result overall in energy being absorbed.

Page 6: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Overall Reaction Energy

• Whether or not an overall reaction releases or requires energy depends upon the final balance between the breaking and forming of chemical bonds.

Page 7: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Energy is...• the ability to do work or produce heat.• conserved.• made of heat and work.• a state function. (Energy is a property that is

determined by specifying the condition or “state” (e.g., temperature, pressure, etc.) of a system or substance.)

• independent of the path, or how you get from point A to B.

Page 8: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Thermodynamics

State functions are properties that are determined by the state of the system, regardless of how that condition was achieved.

Potential energy of hiker 1 and hiker 2 is the same even though they took different paths.

energy, pressure, volume, temperature

6.7

Page 9: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Energy

• While the total internal energy of a system (E) cannot be determined, changes in internal energy (E) can be determined.

• The change in internal energy will be the amount of energy exchanged between a system and its surroundings during a physical or chemical change.

Δ E = E final - E initial

Page 10: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Definitions

• Work is a force acting over a distance.

• Heat is energy transferred between objects because of temperature difference. (Heat is not a property of a system or substance and is not a state function. Heat is a process—the transfer of energy from a warm to a cold object.)

Page 11: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

System vs Surroundings

• The Universe is divided into two halves.• system and the surroundings.

• In a chemistry setting, a system includes all substances undergoing a physical or chemical change.

• The surroundings would include everything else that is not part of the system.

Page 12: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Heat

• Most commonly, energy is exchanged between a system and its surroundings in the form of heat.

• Heat will be transferred between objects at different temperatures.

• Thermochemistry is the study of thermal energy changes.

Page 13: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Definition of Heat

• Heat energy (or just heat) is a form of energy which transfers among particles in a substance (or system) by means of kinetic energy of those particle. In other words, under kinetic theory, the heat is transfered by particles bouncing into each other.

• http://physics.about.com/od/glossary/g/heat.htm

Page 14: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Definition of Temperature

• Temperature is a measurement of the average kinetic energy of the molecules in an object or system and can be measured with a thermometer or a calorimeter. It is a means of determining the internal energy contained within the system.

Page 15: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Heat is the transfer of thermal energy between two bodies that are at different temperatures.

Energy Changes in Chemical Reactions

Temperature is a measure of the thermal energy.

Temperature = Thermal Energy

900C400C

greater thermal energy6.2

Page 16: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Heat vs Temperature

• Note that temperature is different from heat, though the two concepts are linked. Temperature is a measure of the internal energy of the system, while heat is a measure of how energy is transferred from one system (or body) to another. The greater the heat absorbed by a material, the more rapidly the atoms within the material begin to move, and thus the greater the rise in temperature.

• http://physics.about.com/od/glossary/g/temperature.htm

Page 17: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Exo vs Endo

• Exothermic reactions release energy to the surroundings.

• Endothermic reactions absorb energy from the surroundings.

Page 18: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

CH + 2O CO + 2H O + Heat4 2 2 2

CH + 2O 4 2

CO + 2 H O 2 2

Pote

nti

al energ

y

Heat

Page 19: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

N + O2 2

Pote

nti

al energ

y

Heat

2NO

N + O 2NO2 2 + heat

Page 20: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Three Parts

Every energy measurement has three parts:

1. A unit ( Joules of calories).2. A number.3. a sign to tell direction.

negative - exothermic

positive- endothermic

Page 21: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

System

Surroundings

Energy

DE <0

Page 22: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

System

Surroundings

Energy

DE >0

Page 23: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Same rules for heat and work

• Heat given off is “negative”.• Heat absorbed is “positive”.

• Work done by the system on the surroundings is negative.

• Work done on the system by the surroundings is positive.

Page 24: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

First Law of Thermodynamics• The energy of the universe is constant.• It is also called the: • Law of conservation of energy.

q = heat w = work• In a chemical system, the energy exchanged

between a system and its surroundings can beaccounted for by heat (q) and work (w).

DE = q + w• Take the system’s point of view to decide signs.

Page 25: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Thermodynamics

6.7

DE = q + w

DE is the change in internal energy of a system

q is the heat exchange between the system and the surroundings

w is the work done on (or by) the system

w = -PDV when a gas expands against a constant external pressure

Page 26: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Enthalpy and the First Law of Thermodynamics

6.7

DE = q + w

At constant pressure, q = DH and w = -PDV

DE = DH - PDV

DH = DE + PDV

Page 27: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Conservation of Energy

• Energy exchanged between a system and its surroundings can be considered to off set one another.

• The same amount of energy leaving a system will enter the surroundings (or vice versa), so the total amount of energy remains constant.

Page 28: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Metric Units

• The SI (Metric System) unit for all forms of energy is the joule (J).

Page 29: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Heat and Work

• DE = q + w• - q is exothermic -q = -∆H• +q is endothermic• -w is done “by” the system• +w is done “on” the system

• Note: • ∆H stands for enthalpy which is the heat of

reaction

Page 30: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Practice Problem

• A gas absorbs 28.5 J of heat and then performs 15.2 J of work. The change in internal

• energy of the gas is:(a) 13.3 J(b) - 13.3 J(c) 43.7 J(d) - 43.7 J(e) none of the above

Page 31: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Answer

• (b) E = q + w• 28.5 J - 15.2 J = + 13.3 J

Page 32: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Practice Problem

Which of the following statements correctly describes the signs of q and w for the following exothermic process at 1 atmosphere pressure and 370 Kelvin?

H2O(g) → H2O(l)

(a) q and w are both negative(b) q is positive and w is negative(c) q is negative and w is positive(d) q and w are both positive(e) q and w are both zero

Page 33: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Answer

• (c). An exothermic indicates q is negative and the gas is condensing to a liquid so it is exerting less pressure on its surroundings indicating w is positive.

Page 34: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

What is work?

• Work is a force acting over a distance.w= F x DdP = F/ aread = V/areaw= (P x area) x D (V/area)= PDV

• Work can be calculated by multiplying pressure by the change in volume at constant pressure.

• Use units of liter•atm or L•atm

Page 35: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Pressure and Volume Work

• Work refers to a force that moves an object over a distance.

• Only pressure/volume work (i.e., the expansion/contraction of a gas) is of significance in chemical systems and only when there is an increase or decrease in the amount of gas present.

Page 36: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Work needs a sign

• If the volume of a gas increases, the system has done work on the surroundings.

• work is negative• w = - PDV• Expanding work is negative.• Contracting, surroundings do work on the

system W is positive.• 1 L•atm = 101.3 J

Page 37: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Example

• When, in a chemical reaction, there are more moles of product gas compared toreactant gas, the system can be thought of as performing work on its surroundings (making w < 0) because it is “pushing back,” or moving back the atmosphere to make room for the expanding gas. When the reverse is true, w > 0.

Page 38: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Compressing and Expanding Gases

• Compressing gas– Work on the system is positive– Work is going into the system

• Expanding gas– Work on the surroundings is negative– Work is leaving the system

Page 39: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Clarification Info

• If the reaction is performed in a rigid container, there may be a change in pressure,but if there is no change in volume, the atmosphere outside the container didn’t “move” and without movement, no work is done by or on the system.

• If there is no change in volume (V= 0), then no work is done by or on the system (w= 0) and the change in internal energy will be entirely be due to the heat involved ( ΔE = q).

Page 40: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Examples• What amount of work is done when 15 L of

gas is expanded to 25 L at 2.4 atm pressure?• If 2.36 J of heat are absorbed by the gas

above. what is the change in energy?• How much heat would it take to change the

gas without changing the internal energy of the gas?

Page 41: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Enthalpy

• The symbol for Enthalpy is H• H = E + PV (that’s the definition)• DH = DE + PDV (at constant pressure)

Page 42: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Enthalpy (H) is used to quantify the heat flow into or out of a system in a process that occurs at constant pressure.

DH = H (products) – H (reactants)

DH = heat given off or absorbed during a reaction at constant pressure

Hproducts < Hreactants

DH < 0Hproducts > Hreactants

DH > 0 6.3

Page 43: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

DH = DE + PDV

Using DH = DE + PDV

• the heat at constant pressure qp can be

calculated from:

• DE = qp + w (if w = - PDV then…)

• DE = qp – PDV (now rearrange)

• qp = DE + P DV = DH

Page 44: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Examples of Enthapy Changes

• KOH(s) → K(aq) + OH-1 (aq) ΔHsolution = - 57.8 kJ mol1

• C3H8(g) + 5O2(g) → 3CO2(g) + 4H2O(l) ΔHcombustion = -2221kJ/mol

• H2O(s) → H2O(l) ΔHfusion = 6.0 kJ/mol

• Fe2O3(s) + 2Al(s) → Al2O3(s) + 2Fe(s) ΔHreaction - 852 kJ/mol

• Ca(s) + O2(g) H2(g) → Ca(OH)2(s) ΔHformation - 986 kJ/mol1

Page 45: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

3 Methods

• There are a variety of methods for calculating overall enthalpy changes that you should be familiar with.

• The three most common are the:

1. the use of Heats of Formation 2. Hess’s Law 3. the use of Bond Energies

Page 46: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Heat of Reaction

• To compare heats of reaction for different reactions, it is necessary to know the temperatures at which heats of reaction are measured and the physical states of the reactants and products.

• Look in the Appendix of the textbook to find Standard Enthapy tables.

Page 47: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Standard Enthalpy of Formation• Measurements have been made and tables constructed

of Standard Enthalpies of Formation with reactants in their “standard states”.

• Use the symbol DHºf

• Standard state is the most stable physical state of reactants at:

1 atmosphere pressurespecified temperature—usually 25 °C 1 M solutions

• For solids which exist in more than one allotropic form, a specific allotrope must be specified.

Page 48: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Because there is no way to measure the absolute value of the enthalpy of a substance, must I measure the enthalpy change for every reaction of interest?

Establish an arbitrary scale with the standard enthalpy of formation (DH0) as a reference point for all enthalpy expressions.

f

Standard enthalpy of formation (DH0) is the heat change that results when one mole of a compound is formed from its elements at a pressure of 1 atm.

f

The standard enthalpy of formation of any element in its most stable form is zero.

DH0 (O2) = 0f

DH0 (O3) = 142 kJ/molf

DH0 (C, graphite) = 0f

DH0 (C, diamond) = 1.90 kJ/molf6.5

Page 49: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

6.5

Page 50: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

ΔH°formation

• It is important to recognize that the ΔH°formation (abbreviated as ΔH°f) is really just the heat of reaction for a chemical change involving the formation of a compound from its elements in their standard states.

Page 51: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Standard Enthalpies of Formation• The standard heat of formation is the

amount of heat needed to form 1 mole of a compound from its elements in their standard states.

• See the table in the Appendix • Remember: For an element the value is 0

Page 52: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Equation Practice

• You need to be able to write the equation correctly before solving the problem.

Try…• What is the equation for the formation of

NO2 ? Try writing the equation.

Page 53: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Practice Answer

• ½N2 (g) + O2 (g) ® NO2 (g)

• You must make one mole to meet the definition.

Page 54: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

The standard enthalpy of reaction (DH0 ) is the enthalpy of a reaction carried out at 1 atm.

rxn

aA + bB cC + dD

DH0rxn dDH0 (D)fcDH0 (C)f= [ + ] - bDH0 (B)faDH0 (A)f[ + ]

DH0rxn nDH0 (products)f= S mDH0 (reactants)fS-

6.5

Hess’s Law: When reactants are converted to products, the change in enthalpy is the same whether the reaction takes place in one step or in a series of steps.

(Enthalpy is a state function. It doesn’t matter how you get there, only where you start and end.)

Page 55: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Since we can manipulate the equations

• We can use heats of formation to figure out the heat of reaction.

• Lets do it with this equation.

• C2H5OH +3O2(g) ® 2CO2 + 3H2O

• which leads us to this rule. ( H products) - ( H reactants) = Hf

ofo o

Page 56: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Hess’s Law

• Definition:• When a reaction may be expressed as the

algebraic sum of other reactions, the enthalpy change of the reaction is the algebraic sum of the enthalpy changes for the combined reactions.

Page 57: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Hess’ Law

• Enthalpy is a state function.• It is independent of the path.• We can add equations to come up with the

desired final product, and add the DH values.• Two rules to remember:• If the reaction is reversed the sign of DH is

changed• If the reaction is multiplied, so is DH

Page 58: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Enthalpy

• As enthalpy is an extensive property, the magnitude of an enthalpy change for a chemical reaction depends upon the quantity of material that reacts.

• This means: if the amount of reacting material in

an exothermic reaction is doubled, twice the quantity of heat energy will be released.

Page 59: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

H2O (s) H2O (l) DH = 6.01 kJ

• The stoichiometric coefficients always refer to the number of moles of a substance

Thermochemical Equations

• If you reverse a reaction, the sign of DH changes

H2O (l) H2O (s) DH = -6.01 kJ

• If you multiply both sides of the equation by a factor n, then DH must change by the same factor n.

2H2O (s) 2H2O (l)DH = 2 x 6.01 = 12.0 kJ

6.3

Page 60: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

H2O (s) H2O (l) DH = 6.01 kJ

• The physical states of all reactants and products must be specified in thermochemical equations.

Thermochemical Equations

6.3

H2O (l) H2O (g) DH = 44.0 kJ

How much heat is evolved when 266 g of white phosphorus (P4) burn in air?

P4 (s) + 5O2 (g) P4O10 (s) DH = -3013 kJ

266 g P4

1 mol P4

123.9 g P4

x3013 kJ1 mol P4

x = 6470 kJ

Page 61: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

For the oxidation of sulfur dioxide gas

• SO2(g) + ½O2(g) → SO3(g) ΔH° = - 99 kJ/mol

• Doubling the reaction results in:• 2SO2(g) + O2(g) → 2SO3(g)

ΔH° = - 198 kJ/mol

Notice that if you double the reaction, you must double the ΔH° value.

Page 62: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Sign Change of ΔH

• 2SO2(g) + O2(g) → 2SO3(g)

ΔH° = - 198 kJ/mol

• If the reaction is written as an endothermic reaction:

• 2SO3(g) → 2SO2(g) + O2(g)

ΔH° = + 198 kJ/mol

Page 63: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Tips for Hess’s Law Problems

• It is always a good idea to begin by looking for species that appear as reactants and products in the overall reaction.

• This will provide a clue as to whether a reaction needs to be reversed or not.

• Second, consider the coefficients of species that appear in the overall reaction.

• This will help determine whether a reaction needs to be multiplied before the overall summation.

Page 64: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Calculate the standard enthalpy of formation of CS2 (l) given that:

C(graphite) + O2 (g) CO2 (g) DH0 = -393.5 kJrxn

S(rhombic) + O2 (g) SO2 (g) DH0 = -296.1 kJrxn

CS2(l) + 3O2 (g) CO2 (g) + 2SO2 (g) DH0 = -1072 kJrxn

1. Write the enthalpy of formation reaction for CS2

C(graphite) + 2S(rhombic) CS2 (l)

2. Add the given rxns so that the result is the desired rxn.

rxnC(graphite) + O2 (g) CO2 (g) DH0 = -393.5 kJ

2S(rhombic) + 2O2 (g) 2SO2 (g) DH0 = -296.1x2 kJrxn

CO2(g) + 2SO2 (g) CS2 (l) + 3O2 (g) DH0 = +1072 kJrxn+

C(graphite) + 2S(rhombic) CS2 (l)

DH0 = -393.5 + (2x-296.1) + 1072 = 86.3 kJrxn6.5

Page 65: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Example

C(s) + O2(g) → CO2(g) ΔH°f = - 394 kJ/mol

2H2(g) + O2(g) → 2H2O(l) ΔH°f = - 572 kJ/mol

CO2(g) + 2H2O(l) → CH4(g) + 2O2(g) ΔH°f = + 891 kJ/mol

-----------------------------------------------------

C(s) + 2H2(g) → CH4(g) ΔH°f = - 75 kJ/mol

Page 66: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Example

C(s) + O2(g) → CO2(g) ΔH°f = - 394 kJ/mol

2H2(g) + O2(g) → 2H2O(l) ΔH°f = - 572 kJ/mol

CO2(g) + 2H2O(l) → CH4(g) + 2O2(g) ΔH°f = + 891 kJ/mol

-----------------------------------------------------

C(s) + 2H2(g) → CH4(g) ΔH°f = - 75 kJ/mol

Page 67: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Hess’s Law Example

O (g) + H (g) 2OH(g) 2 2 O (g) 2O(g)2 H (g) 2H(g)2

O(g) + H(g) OH(g)

Given

Calculate DHº for this reaction

DHº= +77.9kJDHº= +495 kJ

DHº= +435.9kJ

Page 68: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

H (g) + 1

2O (g) H (l) 2 2 2O

C(s) + O (g) CO (g) 2 2DHº= -394 kJ

DHº= -286 kJ

C H (g) + 5

2O (g) 2CO (g) + H O( ) 2 2 2 2 2 l

Example• Given

calculate DHº for this reaction

DHº= -1300. kJ

2C(s) + H (g) C H (g) 2 2 2

Page 69: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Benzene (C6H6) burns in air to produce carbon dioxide and liquid water. How much heat is released per mole of benzene combusted? The standard enthalpy of formation of benzene is 49.04 kJ/mol.2C6H6 (l) + 15O2 (g) 12CO2 (g) + 6H2O (l)

DH0rxn nDH0 (products)f= S mDH0 (reactants)fS-

DH0rxn 6DH0 (H2O)f12DH0 (CO2)f= [ + ] - 2DH0 (C6H6)f[ ]

DH0rxn=[ 12x–393.5 + 6x–187.6 ] – [ 2x49.04 ] = -5946 kJ

-5946 kJ2 mol

= - 2973 kJ/mol C6H6

6.5

Page 70: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

Problems to Try

• Try 12-3 Practice Problems

Page 71: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

N2 2O2

O2 NO2

68 kJ

NO2180 kJ

-112 kJ

H (

kJ)

Page 72: Chapter 5 Energy & Enthalpy Thermodynamics (rev. 0910)

• Collegeboard. (2007-2008). Professional Development workshop materials: Special focus thermochemistry. http://apcentral.collegeboard.com/apc/public/repository/5886-3_Chemistry_pp.ii-88.pdf