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Chapter 6 – Energy

Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

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Page 1: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Chapter 6 – Energy

Page 2: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Types of Systems

Page 3: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Energy

First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Energy (E)

The capacity to do work or transfer heat.

Kinetic Energy

The energy of motion.

Potential Energy

Energy due to condition, position, or composition.

Internal Energy

The sum of all kinetic & potential energy contained in a system

Page 4: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

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 (exactly)

Energy Units

Page 5: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

q = Heat

The transfer of energy due to temperature changes

Heat and temperature are not the same

w = Work

Force acting through a distance.

ΔE = q + w

Internal Energy Changes

Energy can be transferred between a system and its surroundings as a result of a temperature difference (q) and/or work being done (w).

Page 6: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

The sign of q and w are from the system’s point of view

Internal Energy Changes

In an endothermic process, heat flows into a system - ΔE is positive

In an exothermic process, heat flows out of a system - ΔE is negative

Page 7: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Calculate ΔE 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.

Page 8: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

• The expansion/compression of the system against the external atmosphere is pressure–volume work.

Pressure – Volume Work

Page 9: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Calculating Energy Changes (ΔE)

When a reaction is run, the internal energy (kinetic, potential) can be transferred as heat and/or pressure-volume work:

ΔE = q + w = q – PΔV

Page 10: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

How much work is associated with the expansion of a gas from 46L to 64L at a constant pressure of 15 atm?

Page 11: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Filling (and heating) a hot air balloon takes 1.3X108 J of heat. At the same time, the volume changes from 4.00X106 L to 4.5X106 L. Assuming a constant pressure of 1 atm, what is the energy change for the process?

Page 12: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Heat capacity, C• Amount of heat needed to raise the temperature of

the system by one degree Kelvin

Heat Capacities

Page 13: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Heat capacity, C• Amount of heat needed to raise the temperature of

the system by one degree Kelvin

Molar heat capacity, C• System = one mole of substance.

Specific heat capacity, c• System = one gram of substance

q = CΔT

q = mcΔT

Heat Capacities

Page 14: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

If we add 500 J of heat to 25g of water initially at 25 °C, what is the final temperature of the water? (the specific heat of water = 4.184 J/g•°C)

Page 15: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

If substances at two different temperatures are mixed and allowed to come to a constant temperature:

Heat Capacity and Conservation of Energy

qa = –qb

Page 16: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

What is the final temperature when 125 g of iron at 92.3 °C is dropped into 50.0 g of water at 27.7 °C? The specific heat of iron is 0.444 J/g•°C and the specific heat of water is 4.184 J/g•°C. (Assume an isolated system)

Page 17: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

A 150.0 gram sample of metal at 75.0 °C is added to 150.0g of water at 15.0 °C . The temperature of the water rises to 23.0 °C. What is the specific heat of the metal? (Assume an isolated system)

Page 18: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

qrxn = –qcal = –CΔT

As long as we know the calorimeter (C):

qcal = CΔT

heat

Reaction (Bomb) Calorimetry

Well insulated – considered isolated

If we run a reaction in an isolated system (a calorimeter), we can very accurately measure the heat transferred as a result of the reaction. Note that this is a constant volume process.

Page 19: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

ΔE = q – PΔV

In a system at constant volume, no pressure-volume work is done:

ΔE = q + 0 = qv

Reactions at Constant Volume

PΔV = P(0) = 0

Therefore, at constant volume, the internal energy change is equal to the heat of reaction:

Page 20: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Well insulated – considered isolated

qrxn = -qcal

A Coffee Cup (Simple) Calorimeter

Note that this is a constant pressure process.

Page 21: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

50.0 mL each of 1.0M HCl and 1.0M NaOH at 25 °C at mixed in a calorimeter. After reaction, the temperature of the calorimeter is 31.9 °C. What is the heat generated for the reaction? (We will estimate that the specific heat of the solution/calorimeter is about the same as that of water = 4.184 J/g•°C)

Page 22: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

State Functions

Any property that has a unique value for a specified state of a system is said to be a State Function.

• Water at 293 K and 1.00 atm is in a specified state.

• In this state, the density of water is 0.99820 g/mL

• This density is a unique function of the state.

• It does not matter how the state was established.

• Capitalized letters are used to identify State functions

Page 23: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

ΔE has a unique value between two states

Internal Energy – A State Function

Page 24: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

In a system at constant volume, no pressure-volume work is done:

ΔE = qv

Reactions at Constant Volume

PΔV = P(0) = 0

Therefore, at constant volume, the internal energy change is equal to the heat of reaction:

Page 25: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

At constant pressure, both heat and pressure-volume work results from energy changes:

Reactions at Constant Pressure

Normally, reactions are run at constant pressure (and changing volume).

Page 26: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Because we are usually only interested in the heat of reaction at constant pressure, we will define a new state function:

ΔE = qP - PΔV qP = ΔE + PΔV

Let H = E + PV

qP = ΔH = ΔE + PΔV

Enthalpy Change

ΔH, the enthalpy change, is the measurement we will generally use to describe thermal changes in a chemical system.

Page 27: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Note: Enthalpy change is an extensive property – it is directly proportional to the amount of substances in the system

Negative ΔH = an exothermic reaction

Positive ΔH = an endothermic reaction

Exothermic and Endothermic Reactions

Page 28: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

How Does a “Hand Warmer” Work?

Page 29: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

How much energy is needed to heat the water used in a 5 minute shower on Colby’s campus? (Assume Colby showers are set to 2 gal/min)

Page 30: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Heat (Enthalpy) of Reaction

All reactions will have an accompanying enthalpy change:

ΔHrxn = ΔHproducts- ΔHreactants

For any reaction, the enthalpy change is the sum of the product enthalpies minus the sum of the starting material enthalpies.

ΔHrxn = Hfinal - Hinitial

Page 31: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Why Do We Use These Energy Sources?

Page 32: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

How much natural gas must we burn to produce the heat (4435 kJ) needed for a single 5 minute hot shower on Colby’s campus?

Page 33: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Changes in States of Matter

Why doesn’t a pot of (boiling) water at 100 °C all become steam at once? Why do we have to continually apply heat?

Page 34: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Changes in States of Matter

Any change of state will cause an enthalpy change :

Unless stated otherwise, ΔH values are assumed to be per mole

Page 35: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Changes in States of Matter

Any change of state will cause an enthalpy change :

How much energy is required to convert 5 g of ice at 0 °C to water at 50 °C? To steam at 100 °C?

Page 36: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Changes in States of Matter

Any change of state will cause an enthalpy change :

Which will cause a more damaging burn: skin exposed to 1 g of water at 100 °C or skin exposed to 1 g of steam at 100 °C?

Page 37: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Manipulating Reaction Enthalpies

The “reverse” of any reaction will have an equal enthalpy change of opposite sign.

Page 38: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Standard States and Standard Enthalpy Changes

• First we must define a particular state as a standard state

• ΔH° is the standard enthalpy of reaction

– The enthalpy change of a reaction in which all reactants and products are in their standard states

• The Standard States are defined as:

– The pure element or compound at a pressure of 1 bar (approximately 1 atm) and at the temperature “of interest” (usually 25 °C).

Page 39: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

• ΔHf° , the standard enthalpy of formation, is the

enthalpy change that occurs in the formation of one mole of a substance in the standard state from the reference (most common) forms of the elements in their standard states.

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

Standard Enthalpies of Formation

Page 40: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Standard Enthalpies of Formation

ΔHf° for CH2O = – 108.6 kJ/mol.

ΔHf° for Al2O3 = – 1670 kJ/mol.

ΔHf° for Fe2O3 = – 822 kJ/mol.

What reactions do these heats of formation represent?

Page 41: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Standard Enthalpies of Formation

Page 42: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Standard Enthalpies of Formation

Page 43: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Reaction Summation – Hess’s Law

Hess’s law:If a process occurs in stages or steps (even hypothetically), then the enthalpy change for an overall process is the sum of the enthalpy changes for the individual steps.

Page 44: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

Manipulating ΔH – Hess’s Law

• The enthalpy change of a chemical transformation is directly proportional to the amounts of substances:

• The reverse of a chemical reaction has an equal but opposite H:

Page 45: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

What is the standard enthalpy of reaction for the thermite reaction? How can we use a table of standard heats of formation to determine this?

ΔHf° for Al2O3 = – 1670 kJ/mol.

ΔHf° for Fe2O3 = – 822 kJ/mol.

Page 46: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

What is the standard enthalpy of reaction for the reaction below? How can we use a table of standard heats of formation to determine this?

Page 47: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

ΔHrxn = ΣΔHf°products- ΣΔHf

°reactants

What is the standard enthalpy of reaction for the reaction below? How can we use a table of standard heats of formation to determine this?

Page 48: Chapter 6 – Energy. Types of Systems Energy First Law of thermodynamics: The energy of the universe is constant (i.e. energy is neither created nor destroyed)

What is the standard enthalpy of reaction for the formation of N2O5 as shown below?