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Thermochemistry Chapter 5 (p 165-181) Chapter 11 (11.4 and 11.6) 1

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Thermochemistry. Chapter 5 (p 165-181) Chapter 11 (11.4 and 11.6). ENERGY. Energy is the ability to do work or transfer heat. Energy used to cause an object that has mass to move is called work . Energy used to cause the temperature of an object to rise is called heat. Matter and Energy. - PowerPoint PPT Presentation

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Page 1: Thermochemistry

ThermochemistryChapter 5 (p 165-181)

Chapter 11 (11.4 and 11.6)

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Page 2: Thermochemistry

ENERGY• Energy is the ability to do work or

transfer heat.– Energy used to cause an object that has

mass to move is called work.– Energy used to cause the temperature of

an object to rise is called heat.

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Page 3: Thermochemistry

Matter and EnergyPotential energy is energy an object possesses by virtue of its position or chemical composition.

Kinetic energy is energy an object possesses by virtue of its motion. Potential energy converted to

kinetic energy

Ek = mv212

m = mass, v = speed 3

Page 4: Thermochemistry

Units of EnergyThe SI unit of energy is the joule (J).

Older, non-SI Unit: the calorie (cal).

1 cal = 4.184 J (exactly)

1 J = 1 kg m2

s2

1 cal is amount of energy required to raise the temperature of 1 g of water from 14.5°C to 15.5°C.

Nutritional Calorie: 1 Cal = 1000 cal = 1 kcal

1 J is small, often need kilojoules (kJ), 1 kJ = 1000 J

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Page 5: Thermochemistry

Definitions:System and Surroundings

• The system includes the molecules we want to study (here, the hydrogen and oxygen molecules).

• The surroundings are everything else (here, the cylinder and piston).

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Page 6: Thermochemistry

Energy Transfer: Work and HeatEnergy transferred from racquet to ball:

Energy used to move an object over some distance is work.

w = F dwhere w is work, F is the force,

and d is the distance over which the force is exerted.

• Energy can also be transferred in form of heat.

• Heat flows from warmer objects to cooler objects.

• If differences in temperature between system and surroundings, heat is transferred.

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Page 7: Thermochemistry

First Law of Thermodynamics

• Energy is neither created nor destroyed.• In other words, the total energy of the universe is

a constant; if the system loses energy, it must be gained by the surroundings, and vice versa.

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Page 8: Thermochemistry

Internal Energy

Internal Energy E = the sum of all kinetic and potential energies of all components of the system

In cylinder: internal energy of system includes motion of H2 and O2 molecules through space, rotations, internal vibrations, energies of nuclei of each atom and their electrons.

By definition, the change in internal energy, E, is the final energy of the system minus the initial energy of the system:

E = Efinal − Einitial

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Page 9: Thermochemistry

Internal Energy Change

2 H2 (g) + O2 (g) 2 H2O (g) + energy

Energy lost or gained?By system (reactants) or surrounding?Reverse reaction?

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Page 10: Thermochemistry

• When energy is exchanged between the system and the surroundings, it is exchanged as either heat (q) or work (w).

• Heat gained by system and work done on system increase internal energy E, thus energy change E >0.

ΔE related to heat (q) and work (w)

E = q + w

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Page 11: Thermochemistry

E, q, w, and Their Signs

E = q + wCalculate the change in internal energy of the system:a) A balloon is heated by adding 850 J of heat. It expands, doing 382 J of work on the atmosphere.

b) A 50 g sample of water is cooled from 30C to 15C, thereby losing about 3140 J of heat.

c) A system releases 57.5 kJ of heat while doing 22.5 kJ of work on the surroundings.

q = + 850 J, w = - 382 J ΔE = 850 J – 382 J = 468 J

q = - 3140 J, w = 0 ΔE = -3140 J

q = - 57.5 kJ, w = - 22.5 kJ ΔE = -57.5 kJ – 22.5 kJ = -80.0 kJ

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Page 12: Thermochemistry

Work in a chemical reactionWe can measure the work done by a gas if the reaction is done in a vessel that has been fitted with a piston.

w = -PV

Zn (s) + 2 H+ (aq) Zn2+ (aq) + H2 (g)

Work involved in expansion or compression of gas is called:Pressure-volume work.P = pressureΔV = Vfinal – Vinitial

w done by system on surroundings <0

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Page 13: Thermochemistry

Enthalpy (greek = to warm)

• If a process takes place at constant pressure (most processes we study do) and the only work done is this pressure-volume work, we can account for heat flow during the process by measuring the enthalpy of the system.

• Enthalpy is the internal energy plus the product of pressure and volume of the system:

H = E + PV

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Page 14: Thermochemistry

Enthalpy• When the system changes at constant pressure,

the change in enthalpy, H, is

H = (E + PV)• Or: H = E + PV

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Page 15: Thermochemistry

Endothermic and Exothermic

• A process is endothermic when H is positive, the system absorbs/gains heat from surroundings

• A process is exothermic when H is negative, the system releases/loses heat to the surroundings.

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Page 16: Thermochemistry

Enthalpy of ReactionThe change in enthalpy, H, is the enthalpy of the products minus the enthalpy of the reactants:

H = Hproducts − Hreactants

H is called the enthalpy of reaction, or the heat of reaction.

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Page 17: Thermochemistry

Enthalpies of formation

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Section 5.7Enthalpy of formation (ΔHf) = enthalpy change associated with formation of compound from its constituent elements.

Magnitude depends on conditions of temperature, pressure, state of reactants and products

Standard set of conditions for comparison:Pure form of a compound/substance, 1 atm, 25°C = 298K

Standard enthalpy of formation (ΔH°f) = enthalpy change for reaction that forms 1 mol of compound from its elements with all substances in their standard statesElements (in std states) compound (in std state) ΔH°f

By definition: standard enthalpy of formation (ΔH°f) of most stable form of any element is zero (ΔH°f = 0)

Page 18: Thermochemistry

ΔH°f and enthalpies of reactions: ΔH°rxn

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ΔH°rxn = Σn ΔH°f (products) - Σn ΔH°f (reactants)

n = coefficients of chemical reactions of each reactant and product (varies)

Example: combustion of ethanol

C2H5OH (l) + 3 O2 (g) 2 CO2 (g) + 3 H2O (l)

Calculate the enthalpy change for combustion reaction of 1 mol of ethanol:ΔH°rxn = [2x ΔH°f (CO2) + 3 ΔH°f (H2O)] – [ΔH°f (C2H5OH) + 3x ΔH°f (O2)]Table 5.3, p 189

ΔH°f C2H5OH(l) = -277.7 kJ/molΔH°f CO2(g) = -393.5 kJ/molΔH°f H2O(l) = -285.8kJ/molΔH°f O2(g) = 0 (by definition)

ΔH°rxn = [2x(-393.5) + 3x(-285.8)] – [-277.7 + 0] = -1367 kJ

Page 19: Thermochemistry

Chemical Reactions – Thermochemical Equations

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2 H2 (g) + O2 (g) 2 H2O (g) ΔH = -483.6 kJΔH is negative reaction/system releases/loses heat to surroundings, is exothermic.

ΔH at end of balanced chemical equation, no specific amounts of reactants listed.BUT:Coefficients here represent the moles of reactants (and products) producing the associated enthalpy change,

i.e. 2 mols of H2 reacting with 1 mol O2 to produce 2 mols H2O results in an enthalpy change of -483.6 kJ.

Page 20: Thermochemistry

Facts about Enthalpy

1. Enthalpy is an extensive property, depends on amount of material present.

2. H for a reaction in the forward direction is equal in size, but opposite in sign, to H for the reverse reaction.

3. H for a reaction depends on the state of the products and the state of the reactants.

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2 H2 (g) + O2 (g) 2 H2O (g) ΔH = -483.6 kJ

Page 21: Thermochemistry

Practice

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Consider the following reaction:

CH3OH (g) CO (g) + 2 H2 (g) ΔH = +90.7 kJ

a) Is heat absorbed or released in the course of this reaction?

b) Calculate the amount of heat transferred when 45.0 g of CH3OH (g) is

decomposed by this reaction.

c) For a given sample of CH3OH, the enthalpy change on reaction is 25.8 kJ.

How many grams of hydrogen gas are produced?

d) What is the value of ΔH for the reverse of the reaction?

e) How many kJ of heat are released when 50.9 g of CO(g) reacts completely

with H2(g) to form CH3OH (g) at constant pressure?

ΔH >0,heat is absorbed

45.0g CH3OH x molar massx90.7 kJ/1 mol

25.8 kJ x 2molH2/90.7 kJx molar mass H2

Sign reversed, magnitude same: -90.7 kJ

50.9 g CO(g) x molar mass CO x (-90.7 kJ/mol)

Page 22: Thermochemistry

Enthalpy vs Internal Energy in reactions

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Enthalpy (H) and internal energy (E) are both “state functions” (value depends only on state or condition of system, not on details on how it came to be in that state.But:Using E to describe energy changes in reactions requires measurement of both heat flow and work.H focuses only on the heat flow which is easier to measure.

Page 23: Thermochemistry

Calorimetry

Since we cannot know the exact enthalpy of the reactants and products, we measure H through calorimetry, the measurement of heat flow.

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Page 24: Thermochemistry

Heat Capacity and Specific HeatThe amount of energy required to raise the temperature of a substance by 1 K (1C) is its heat capacity.

We define specific heat capacity (or simply specific heat) as the amount of energy required to raise the temperature of 1 g of a substance by 1 K.

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Page 25: Thermochemistry

Heat Capacity and Specific HeatSpecific heat, quantity of heat transferred, mass of

substance, and temperature change:

Specific heat =heat transferred

mass temperature change

Cs =q

m T

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Page 26: Thermochemistry

BTU – British thermal unit

1 Btu = amount of heat required to raise the temperature of 1 lb of water by 1°F.

How many Joules in 1 Btu?

Specific heat of water: Cs=4.18 J/g-K

Have mass of water: m = 1 lb = 454 g

Need ΔT in K (°C) instead of 1°F (ΔT scale:100°C units = 180°F units thus: ΔT of °F = 5/9°C)

So: 4.18 J/g-K x 454 g x 5/9 = 1054 J = 1 Btu

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Page 27: Thermochemistry

Practice

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The specific heat of iron metal is 0.450 J/g-K. How many Joules of heat are necessary to raise the temperature of a 1.05 kg block of iron from 25°C to 88.5°C?

Specific heat x mass x temperature change = heat required in J.

0.450 J/g-K x 1.05 kg x kg g x dT (88.5-25.0) =30004 J (3 SF) = 3.00 x 104 J = 30.0 kJ

Page 28: Thermochemistry

Phase Changes (11.4)

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Endothermic? Exothermic?

Page 29: Thermochemistry

Phase Changes – Energy Changes

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• Solid melts liquid: units (molecules) are free to move, average separation increases

• Melting process called: “fusion”• Requires input of energy: heat of fusion,

or enthalpy of fusion (ΔHfus)

• ΔHfus for ice: 6.01 kJ/mol

Page 30: Thermochemistry

Phase Changes – Energy Changes

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• Temperature increases• Liquids gas: units (molecules) are

widely separated• Requires input of energy: heat of

vaporization, or enthalpy of vaporization (ΔHvap)

• ΔHvap for water: 40.7 kJ/mol

Page 31: Thermochemistry

Heat of fusion and vaporization

The heat of fusion is the energy required to change a solid at its melting point to a liquid.

The heat of vaporization is defined as the energy required to change a liquid at its boiling point to a gas.

ΔHvap > ΔHfus , all intermolecular interactions are severed.

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Page 32: Thermochemistry

Phase Change: solid to gasSublimation

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Enthalpy change for solid to gas transition = heat of sublimation (ΔHsub)

ΔHsub= ΔHfus + ΔHvap

Page 33: Thermochemistry

Energy Changes Associated with Changes of State

• The heat added to the system at the melting and boiling points goes into pulling the molecules farther apart from each other.

• The temperature of the substance does not rise during a phase change.

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Page 34: Thermochemistry

Practice

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What is the enthalpy change during the process in which 100.0 g of water at 50.0°C is cooled to ice at -30.0°C?

Cs(ice) = -2.03 J/g-K

ΔHfus= -6.01 kJ/mol

Cs(water) = -4.18 J/g-KAB

Heating curve for waterCD

BC

100.0 g water (H2O) = ? mol H2O

Page 35: Thermochemistry

Phase DiagramsPhase diagrams display the state of a substance at various pressures and temperatures and the places where equilibria exist between phases.

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Page 36: Thermochemistry

Phase Diagrams• The circled line is the liquid-vapor interface.• It starts at the triple point (T), the point at

which all three states are in equilibrium.

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Page 37: Thermochemistry

Phase DiagramsIt ends at the critical point (C); above this critical temperature and critical pressure the liquid and vapor are indistinguishable from each other.

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Page 38: Thermochemistry

Phase DiagramsEach point along this line is the boiling point of the substance at that pressure.

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Page 39: Thermochemistry

Phase Diagrams• The circled line in the diagram below is the

interface between liquid and solid.• The melting point at each pressure can be found

along this line.

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Page 40: Thermochemistry

Phase Diagrams• Below the triple point the substance cannot exist

in the liquid state.• Along the circled line the solid and gas phases

are in equilibrium; the sublimation point at each pressure is along this line.

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Page 41: Thermochemistry

Phase Diagram of Water

• Note the high critical temperature and critical pressure.– These are due to the

strong van der Waals forces between water molecules.

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Page 42: Thermochemistry

Phase Diagram of Water• The slope of the solid-

liquid line is negative.– This means that as the

pressure is increased at a temperature just below the melting point, water goes from a solid to a liquid.

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Page 43: Thermochemistry

Phase Diagram of Carbon DioxideCarbon dioxide cannot exist in the liquid state at pressures below 5.11 atm; CO2 sublimes (solid to gas) at normal pressures (1 atm), (dry ice!).

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Page 44: Thermochemistry

Phase diagrams

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Describe any changes in the phases of water when: a) temperature is kept at 0°C, while pressure is decreased from that at point 5 to the pressure at point 1.

b) Pressure is kept at 1 atm, while temperature is decreased from that at point 9 to the temperature at point 6.

Page 45: Thermochemistry

Practice

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Describe all the phase changes that would occur when:a)Water vapor originally at 0.005 atm and -0.5°C is slowly compressed at constant temperature until the final pressure is 20 atm.b)Water originally at 100.0C and 0.5 atm is cooled at constant pressure until the temperature is -10°C.

Page 46: Thermochemistry

Practice

46

Describe the phase changes (and the appr. temperatures at which they occur) when CO2 is heated from -80°C to -20°C at:

a) a constant pressure of 3 atm

b) a constant pressure of 6 atm