Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat...

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Thermochemistry Chapter 5 BLB 12 th

Transcript of Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat...

Page 1: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Thermochemistry

Chapter 5 BLB 12th

Page 2: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Expectations

Heat & enthalpy – same or different?

Heat calculations:– Temp. change– Phase change (11.4, p. 438)– Reactions

Enthalpy calculations

Read the chapter, study, and apply!

Page 3: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.1 The Nature of Energy

Chemistry ⇐ ? ⇒ Energy

Energy – capacity to do work or transfer heat– Potential – stored energy; chemical– Kinetic – released energy; energy of motion;

thermal

Electrostatic potential – interaction between charged particles

Page 4: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Examples of Kinetic Energy

Page 5: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Energy, cont.

Units of energy:Joule (J) – SI unit of energy;

calorie (cal)– amount of energy required to raise the

temperature of exactly 1 gram of pure water by 1°C (from 14.5°C to 15.5°C)

– 1 cal = 4.184 J (exactly)– Calorie (dietary calorie),Cal

1 Cal = 1000 cal = 1 kcal

2

2

1J1s

mkg

Page 6: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Energy, cont.

System and SurroundingsSystem – component(s) of interest– Open – matter and energy can be exchanged between

system and surroundings– Closed – can exchange energy but not matter– Isolated – neither energy nor matter can be exchanged

Surroundings – everything outside of the system

Page 7: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Energy, cont.

Transferring EnergyWork (w) – energy used to move an object against a force; w = F x dHeat (q) – energy transferred from a hotter object to a cooler one

Energy – capacity to do work or transfer heat;ΔE = q + w

Page 8: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Combustionheat & work

Page 9: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.2 The First Law of Thermodynamics

Energy can be neither created nor destroyed.Energy is conserved.Internal energy, E – sum of all the kinetic and potential energy of the system’s components

What kinds of energy are in here?

What changes could occur?

Page 10: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.2 The First Law of Thermodynamics

More interested in the change in energy:

ΔE = Efinal – Einitial

Need to give number, units, and sign for all thermodynamic quantities.

ΔE > 0 - Efinal > Einitial, system has gained energy; endergonic

ΔE < 0 - Efinal < Einitial, system has lost energy; exergonic

Note: Opposite change occurs with respect to the surroundings.

Page 11: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 12: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Energy, heat & work

ΔE = q + w

Sign of ΔE depends upon sign and magnitude of q and w.

Page 13: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 14: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Exothermic

Efinal < Einitial

Page 15: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Sample Exercise 5.2

A(g) + B(g) → C(s)

System loses 1150 J of heat to the surroundings.

The piston move downwards doing 480 J of work on the system.

ΔE = ?

Page 16: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculate ΔE (in J); exothermic or endothermic?a. Balloon heating by adding 900 J of heat and

expands doing 422 J of work on atmosphere.

b. 50 g of H2O cooled from 30°C to 15°C losing 3140 J of heat.

c. Reaction releases 8.65 kJ of heat, no work done.

Page 17: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat or Thermal Energy (q)Exothermic: system → surroundings– Heat energy released to surroundings– q < 0– e.g. combustion reaction, crystallization– Surroundings get warmer

Endothermic: system ← surroundings– Heat energy flows into the system– q > 0– e.g. melting, boiling, dissolution of NH4NO3

– Surroundings get colder

Page 18: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat, cont.Evidenced by a change in temperature

Spontaneously transferred from the hotter to the cooler object

Atoms or molecules with more energy move faster

Temperature-dependent

Extensive property (depends on amount)

Total energy of system is the sum of the individual energies of all the atoms and molecules of the system.

Page 19: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Work (w)

Force acting over a distancew = F x d = −PΔVCompression: work ← surroundings– Work is done on the system.– ΔV < 0– w > 0

Expansion: work → surroundings– Work is done on the surroundings.– ΔV > 0– w < 0

Page 20: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 21: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat & Work, cont.

Work and heat are pathways by which energy can be transferred.

State function – depends only on the system’s present state; independent of the pathway; internal energy, P, V, ΔE, ΔH, ΔS are state functions

Energy is a state function, as is enthalpy.

Page 22: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 23: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.3 EnthalpyEnthalpy – heat flow at constant pressure; from Gr. enthalpien – to warm

Enthalpy change (ΔH) – energy transferred as heat at constant pressure; ΔH = Hproducts – Hreactants

H = E + PV

For a change @ constant pressure:

ΔH = ΔE + PΔV

ΔH = ΔE − w = qP

Page 24: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.3 EnthalpyΔH < 0 exothermic: reactants → products + heat

ΔH > 0 endothermic: reactants + heat → products

ΔH = q/mol

Enthalpy (or heat) of reaction, ΔHrxn – enthalpy change that accompanies a reaction

Page 25: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.4 Enthalpies of Reaction, ΔHrxn

1. ΔH is an extensive property; value depends upon the BALANCED equation.

2 H2(g) + O2(g) → 2 H2O(g)

ΔH = +483.6 kJ per 2 moles of H2O

H2(g) + ½ O2(g) → H2O(g)

ΔH = −241.8 kJ per mole of H2O

Page 26: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 27: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.4 Enthalpies of Reaction

2. For reverse reactions:

ΔH values are equal in magnitude, but opposite in sign.

For water: ΔHvap = +44.0 kJ/mol

ΔHcond = −44.0 kJ/mol

Page 28: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

For the combustion of methane:

Page 29: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.4 Enthalpies of Reaction

3. ΔH is dependent upon physical state.

ΔHf values:

C6H6(g) = 82.9 kJ/mol

C6H6(l) = 49.0 kJ/mol

H2O(l) → H2O(g) ΔH = +44 kJ

Page 30: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

CH3OH(g) → CO(g) + 2 H2(g) ΔHrxn = +90.7 kJ

a. Exothermic or endothermic?

b. Heat transferred for 1.60 kg CH3OH?

c. If 64.7 kJ of heat were used, how many grams of H2 would be produced?

Page 31: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

d. ΔH of reverse reaction?

Heat (in kJ) released when 32.0 g of CO(g) reacts completely?

CH3OH(g) → CO(g) + 2 H2(g) ΔHrxn = +90.7 kJ

Page 32: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.5 Calorimetry

Calorimetry – science of measuring heat flow

Calorimeter – a device used to measure heat flow

Coffee-cup calorimeter ⇒

Page 33: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat Capacity and Specific Heat

Heat capacity (C) - amount of heat required for a 1°C temperature change:

J/°C = J/K

extensive property

ΔT in K = ΔT in °C

T

q

changeetemperatur

dtransferreheatC

Page 34: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat Capacity and Specific Heat

Specific heat capacity (Cs) – heat capacity for 1 g;J/g·°C or J/g·K

Molar heat capacity – heat capacity for 1 mole; J/mol·°C or J/mol·K

Page 35: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat Capacity and Specific Heat

Specific heat values (more on p. 176):Fe 0.45 J/g·K

glass 0.84 J/g·K water 4.18 J/g·K (highest of all liquids and solids except

ammonia)

Tm

q

changeetemperaturgrams

dtransferreheatCs

Page 36: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculating heat (q)

To calculate the quantity of heat transferred:

q = Cs x m x ΔT

q – heat (J)Cs – specific heat (J/g∙K)m – mass (g)ΔT – change in temp. (K or °C)

Page 37: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculate the heat (in J) required to raise the temperature of 62.0 g toluene from 16.3°C to 38.8°C. The specific heat of toluene is 1.13 J/g·K.

Page 38: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculate the specific heat of lead if 78.2 J of heat were required to raise the temperature of a 45.6-g block of lead by 13.3°C.

Page 39: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Constant-Pressure Calorimetry

Constant-pressure, ΔH = qP and ΔE = qP + w

Assume no heat is lost to surroundings.

Usually exothermic (qrxn < 0)

Applications:– Heat transfer between objects– Reactions in aqueous solutions

Use specific heat of water (4.18 J/g·K).

Use mass (or moles) of solution.

Page 40: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Solution Calorimetry

heat lost by reaction = heat gained by solution

−qrxn = qsoln

qrxn = −(Cs,soln x msoln x ΔT)

Enthalpy of reaction (ΔHrxn) per mole

ΔHrxn = qrxn/mol of specified reactant

Page 41: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

A 19.6-g piece of metal was heated to 61.67°C. When the metal was placed into 26.7 g water, the temperature of the water increased from 25.00 to 35.00°C. Calculate specific heat of the metal.

Page 42: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

A 15.0-g piece of nickel at 100.0°C is dropped into a coffee-cup calorimeter containing 55.0 g H2O at 23.0°C. What is the final temperature of the water and nickel after reaching thermal equilibrium? The specific heat capacity of nickel is 0.444 J/g·K and of water is 4.18 J/g·K.

Page 43: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 44: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

In a coffee-cup calorimeter, 2.50 g of MgO was reacted with 125 mL of 1.0 M HCl. The temperature increased by 9.6°C. Calculate the enthalpy of reaction per mole of MgO for the following reaction. Mg2+(aq) + H2O(l) → MgO(s) + 2 H+(aq)

Page 45: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Constant-Volume Calorimetry (p. 178)

Bomb calorimetry

No work is done (ΔV = 0), so ΔE = qV

Used for combustion reactions

The bomb components absorb the heat lost by the reaction.

Heat capacity of the bomb (Ccal) needed to calculate the heat of combustion (reaction)

qrxn = −(Ccal x ΔT)

Page 46: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Bomb Calorimeter

Page 47: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

A 1.320-g sample of a new organic substance is combusted in a bomb calorimeter (Ccal = 8.74 kJ/K). The temperature of the bomb increased from 22.14°C to 26.82°C. What is the heat of combustion per gram of the substance?

Page 48: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Phase Changes (Fig. 11.20, p. 439)

(or crystallization)

Page 49: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Phase Changes(p. 440)

Endothermic →

← Exothermic

Cs = 4.18 J/g·K

Cs = 2.03 J/g·K

Cs = 1.84 J/g·K

ΔHvap = 40.67 kJ/mol

ΔHfus = 6.01 kJ/mol

Page 50: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Heat transfer – phase changesTo calculate the quantity of heat transferred during a change of state:

q = ΔHprocess x m

or

q = ΔHprocess x mol

No change in temperature, so no ΔT.For a complete process, add together the heat transferred for each segment.

See Sample Exercise 11.3, p. 441.

Page 51: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

11.46 Calculate the heat transferred for the conversion of 35.0 g of the fluorocarbon, C2Cl3F3, from a liquid at 10.00°C to a gas at 105.00°C.Data: b.p. 47.6°C, ΔHvap= 27.49 kJ/mol, Cs(liquid) = 0.91 J/g·K, Cs(gas) = 0.67 J/g·K

Page 52: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.6 Hess’s LawIf a reaction is carried out in a series of steps, ΔHrxn will equal the sum of the ΔH values of the individual steps.

Hess’s Law works because ΔH is a state function, i.e. it only depends upon the initial reactant and the final product states.

Page 53: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Hess’s Law Example

Page 54: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Hess’s Law Example

Page 55: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculation of H

Imagine this as occurringin three steps:

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

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

Page 56: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculation of H

Imagine this as occurringin three 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)

Page 57: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculation of H

Imagine this as occurringin three 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 58: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

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 59: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Based on the following reactions: ΔH, kJN2(g) + O2(g) → 2 NO(g) 180.72 NO(g) + O2(g) → 2 NO2(g) −113.12 N2O(g) → 2 N2(g) + O2(g) −163.2

Calculate the ΔHrxn for the following reaction:N2O(g) + NO2(g) → 3 NO(g)

Page 60: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Based on the following reactions: ΔH, kJC2H2(g) + 5/2 O2(g) → 2 CO2(g) + H2O(l) −1300.C(s) + O2(g) → CO2(g) −394 H2(g) + ½ O2(g) → H2O(l) −286

Calculate the ΔHrxn for the following reaction:2 C(s) + H2(g) → C2H2(g)

Page 61: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.7 Enthalpies of Formation

Standard state of a substance – pure form at atmospheric pressure (1 atm) and temperature of interest (usually 25°C).Standard enthalpy - ΔH°

Standard enthalpy of formation, ΔHf°- the change in enthalpy for the formation of 1 mole of a substance from its elements in their standard states, kJ/mol of product.

ΔHf° of an element in its most stable form = 0 kJ/mol

Page 62: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Standard Enthalpies of Formation(see Appendix C, p. 1059)

Page 63: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Reactions for ΔHf°

Page 64: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculating Enthalpies of Reaction

ΔH°rxn = Σn ΔHf°(products) − Σ n ΔHf°(reactants)

Page 65: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.73 (c) Calculate ΔHrxn for the following reaction:

N2O4(g) + 4 H2(g) → N2(g) + 4 H2O(g)

Page 66: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Calculate ΔHrxn for the following reaction:

2 KOH(s) + CO2(g) → K2CO3(s) + H2O(g)

Page 67: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

5.8 Foods and Fuels

Glucose is our body’s fuel source.

Carbs and fats are metabolized into glucose.

Excess fat is stored.

What’s the big deal? Take a look at the “fuel value”.

Page 68: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.
Page 69: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.

Nonbiological Fuel

Page 70: Thermochemistry Chapter 5 BLB 12 th. Expectations Heat & enthalpy – same or different? Heat calculations: –Temp. change –Phase change (11.4, p. 438) –Reactions.