Sparks CH301 THERMODYNAMICS and ENTROPY UNIT 4 Day 5 What are we - - PowerPoint PPT Presentation

sparks ch301 thermodynamics and entropy unit 4 day 5 what
SMART_READER_LITE
LIVE PREVIEW

Sparks CH301 THERMODYNAMICS and ENTROPY UNIT 4 Day 5 What are we - - PowerPoint PPT Presentation

Sparks CH301 THERMODYNAMICS and ENTROPY UNIT 4 Day 5 What are we going to learn today? Heats of Formation, Hesss Law, and Bond Energies Second Law of Thermodynamics Concept of Entropy QUIZ: iClicker Question Which of the following is not a


slide-1
SLIDE 1

Sparks CH301 THERMODYNAMICS and ENTROPY UNIT 4 Day 5

slide-2
SLIDE 2

What are we going to learn today?

Heats of Formation, Hess’s Law, and Bond Energies Second Law of Thermodynamics Concept of Entropy

slide-3
SLIDE 3

Which of the following is not a “formation” reaction? (For which would ΔHrxn NOT equal ΔHf?) A) Mg(s) + ½ O2(g)  MgO(s) B) ½ N2(g) + 3/2 H2(g)  NH3(g) C) NaF(s) + Li(s)  LiF(s) + Na(s) D) Li(s) + ½ F2(g)  LiF(s)

QUIZ: iClicker Question

slide-4
SLIDE 4

Standard Enthalpy of Formation ΔH for the formation of 1 mole of a compound from its elements in their most stable form at standard conditions

Standard Enthalpy of Formation, ΔHf

°

slide-5
SLIDE 5
  • Consider combustion of methane, CH4.

Calculate Ho for the reaction below from Ho

fvalues.

CH4(g) + 2 O2(g)  CO2(g) + 2 H2O(l) Hf

  • CH4

= -75 kJ

Hf

  • CO2

= -394 kJ

Hf

  • H2O

= -286 kJ

C (s, graph) + 2H2(g)  CH4(g) ∆Hf = -75 kJ C (s, graph) + O2(g)  CO2(g) ∆Hf = -394 kJ ½ O2(g) + H2(g)  H2O (g) ∆Hf = -286 kJ

slide-6
SLIDE 6

Schematic diagram of the energy changes for combustion of methane

“UN-form” REACTANTS into ELEMENTS “FORM” PRODUCTS from ELEMENTS

CH4(g) + 2 O2(g)  CO2(g) + 2 H2O(l)

slide-7
SLIDE 7

CALCULATING ΔH FROM BOND ENERGIES

slide-8
SLIDE 8

One way to think about energy changes in reactions:

  • Chemical reactions require the

rearrangement of atoms

– Breaking bonds ___________ energy – Forming bonds ___________ energy

  • Net result of bond breaking and bond forming

will give overall enthalpy of reaction

slide-9
SLIDE 9

Consider a reaction for which: Erequired break bonds > Ereleased form bonds This reaction would be:

  • A. endothermic
  • B. exothermic

POLL: iClicker Question

slide-10
SLIDE 10

Bond Enthalpy The heat required to break a mole of bonds at constant pressure. ΔHr

° = ΣBEreactants - ΣBEproducts

Bond Enthalpies

slide-11
SLIDE 11
slide-12
SLIDE 12
  • To calculate the total energy change, we

assume all bonds in reactant molecules are broken and then the atoms are reassembled into product molecules.

slide-13
SLIDE 13

Almost every process in the world happens in only one direction (in isolation = “on its own”) Imagine the following situations. Are they spontaneous? Dropping an object Burning logs A gas expanding into the room Heat flow from high T to low T Ice melting in a glass of water Food dye dropped into water

Spontaneity

slide-14
SLIDE 14

We will refer to any process that happens in isolation as

  • spontaneous. The forward reaction will happen but the reverse

reaction will never happen on its own. How might these processes be reversed? Dropping an object Burning logs A gas expanding into the room Heat flow from high T to low T Ice melting in a glass of water

Spontaneity

slide-15
SLIDE 15

The Second Law of Thermodynamics states that any process that happens spontaneously will lead to an increase in the entropy of the universe

The Second Law of Thermodynamics

slide-16
SLIDE 16

The entropy of the universe is the total entropy of the system and surroundings.

Entropy

Spontaneous

slide-17
SLIDE 17

What is Entropy? What words or ideas pop into your head with respect to Entropy?

Entropy

slide-18
SLIDE 18

Entropy is related to the dispersal of energy at a given temperature.

  • The more energy dispersed, the greater the entropy change.
  • The wider the energy dispersal, the greater the entropy change.
  • The lower the temperature, the greater the entropy change for

a given amount of energy.

Entropy

slide-19
SLIDE 19

When a gas expands in a vacuum, identify the System Surrounding Initial State Final State

Entropy Examples

slide-20
SLIDE 20

When a gas expands in a vacuum, ∆Stotal is A.> 0

  • B. = 0
  • C. < 0

D.No way to know

POLL: iClicker Question

slide-21
SLIDE 21

For a process that is spontaneous

Spontaneity

slide-22
SLIDE 22

When a gas expands in a vacuum, ∆Ssystem is A.> 0

  • B. = 0
  • C. < 0

D.No way to know

POLL: iClicker Question

slide-23
SLIDE 23

A container of gas was opened and the gas was allowed to fill the

  • room. In this example, the system is the gas and the surroundings

is the room. Increasing volume leads to an increase in entropy. The process was spontaneous The surroundings are unchanged The expansion led to an increase in the entropy of the system

Entropy Examples

slide-24
SLIDE 24

Why does the increase in volume lead to an increase in entropy? We must use a microscopic view of dispersal of energy. Unfortunately, it is difficult to “visualize” energy, but it is easy to visualize molecules. States of highest entropy are simply the most likely to happen.

Entropy

slide-25
SLIDE 25

Let’s imagine the gas in our previous example, where the gas is in a container with a left-hand side and a right-hand side What if we only had one gas particle? There are two possibilities, both of which are equally likely

Microstates

slide-26
SLIDE 26

26

slide-27
SLIDE 27

27

slide-28
SLIDE 28

What if we only had Avogadro’s number of particles? It is extremely unlikely that we will find all the molecules entirely

  • n the left or right side. The most likely situation will have half of

the particles on each side.

Microstates

If there are two molecules in the two-bulbed flask, there is

  • ne chance in four that both

molecules will be in the left bulb.

slide-29
SLIDE 29

29

Ω = 1 Ω = 4 Ω = 6

slide-30
SLIDE 30

Entropy is measure of the number of equivalent microstates. More volume more microstates more entropy More molecules more microstates more entropy Higher temperature more microstates more entropy Higher Energy more microstates more entropy

Entropy and Microstates

slide-31
SLIDE 31

It is harder to visualize microstates for energy, but it is the same idea, where more microstates means higher entropy Macroscopically, we can quantify this with heat flow The heat will always be the reversible heat for the processes we investigate in this course

Entropy and Microstates

slide-32
SLIDE 32

The change in Enthalpy can be calculated based on a variety

  • f tabulated data:

Heats of formation/Other Heats of Reaction/Bond Energies Understand the concept of entropy, S, and change in entropy ΔS. Understand the concept of change in entropy of a system, surroundings and universe.

What have we learned today?

slide-33
SLIDE 33

Important Information

HW, LM31, & LM32 Due Wednesday