Chapter 5 Thermochemistry - Philadelphia University · 2015. 3. 30. · Thermochemistry . Transfer...

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Chapter 5 Thermochemistry

Transcript of Chapter 5 Thermochemistry - Philadelphia University · 2015. 3. 30. · Thermochemistry . Transfer...

  • Chapter 5 Thermochemistry

  • Topics

    Energy and energy changes

    Introduction to thermodynamics

    Enthalpy

    Calorimetry

    Hess’s Law

    Standard enthalpies of formation

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    5.1 Energy and Energy Changes

    Energy is involved in all types of physical and chemical changes

    Energy: the capacity to do work or transfer heat

    All forms of energy are either

    Kinetic

    Potential

  • Kinetic energy - energy of motion

    Defining equation

    Where m is mass and u is velocity

    Thermal energy - one form of kinetic energy associated with random motion

    •Changes in thermal energy are monitored via changes in temperature

  • Potential energy - energy of position or composition

    Chemical energy is stored within structural units of chemical substances.

    Electrostatic energy is energy resulting from the interaction of charged particles.

    •Dependent on charges and distance between charges (Q = charge and d

    = distance)

    •Defining equation

    •+ Eel: repulsive

    •− Eel: attractive

  • Law of conservation of energy

    Energy can be converted from one form to another but not created or destroyed.

    The total amount of energy in the universe is constant.

    Example

    •A chemical reaction (potential) gives off heat (thermal)

  • System is the part of the universe of interest.

    •Example

    The reactants NaOH and HCl

    Surroundings are the rest of the universe.

    •Example

    When heat is given off from the reaction of NaOH and HCl, the energy is transferred from the system to the surroundings.

    system: what is inside the container. Reactants or products of a chemical reaction

    surroundings: container ,room, etc.

    Energy changes in chemical reactions

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    The study of the transfer of heat (thermal energy) in chemical reactions.

    Exothermic - transfer of heat from the system to the surroundings

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

    Endothermic - the transfer of heat from the surroundings to the system

    energy + 2HgO(s) 2Hg(l) + O2(g)

    Thermochemistry

  • Transfer of Energy

    Exothermic process

    energy is produced in reaction

    energy flows out of system

    container becomes hot when touched

    CH4(g) + 2O2(g) CO2(g) + 2H2O(g) + heat

    Endothermic process

    energy is consumed by the reaction

    energy flows into the system

    container becomes cold when touched

    N2(g) + O2(g) + Energy 2NO(g)

    http://college.hmco.com/chemistry/shared/media/zumdahl/visual/visual.html?name=CH09&vis=_v9a

  • Comparison of Endothermic and Exothermic Processes

  • Joule (J) is the SI unit for energy.

    •The amount of energy possessed by a 2 kg mass moving at a speed of 1 m/s

    Units of Energy

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    Calorie (cal) - commonly used on food labels

    1 cal 4.184 J

    1000 cal = 1 Cal = 1 kcal

    Food calories (Cal) are really 1000 calories (cal).

  • Calculate the kinetic energy of a neon atom

    moving at a speed of 98 m/s.

    226

    k kg)(98m/s)10(3.3522

    1 E

    J101.6 22kE

    kg103.352g 1000

    kg 1

    amu

    g101.661amu 20.18 26

    24

    Example

  • 5.2 Introduction to Thermodynamics

    Types of systems:

    open (exchange of mass and energy)

    closed (exchange of energy)

    isolated (no exchange)

  • State functions depend only on initial and final states of the system and not on how the change was carried out.

    Energy (E)

    Pressure (P)

    Volume (V)

    Temperature (T)

    State function

  • State Function

    energy change is independent of pathway thus it is a state function

    (state property)

    State function: a property of a system that depends only on its present state (it does not depend on system’s past or future, i.e, it does not depend on how the system arrived at the present state)

    work and heat depend on pathway so they are not state functions

  • First Law of Thermodynamics

    Energy can be converted from one form to another but cannot be created or destroyed.

    Based on the law of conservation of energy

    Internal energy (U)

    It is the sum of potential and kinetic energy of all particles in the system

    U = PE + KE

    Kinetic energy - molecular motion

    Potential energy - attractive/repulsive interactions

  • The change in internal energy of a system between final (f) and initial (i) states is defined as:

    U = Uf Ui For a chemical system

    Cannot calculate the total internal energy with any certainty

    Can calculate the change in energy of the system experimentally

    U = U(products) U(reactants)

  • Consider:

    S(s) + O2(g) SO2(g)

    This reaction releases heat, therefore U is negative.

  • Usystem + Usurroundings = 0

    When a system releases heat, some of the chemical energy is released as thermal energy to the surroundings but this does not change the total energy of the universe.

  • Usystem = Usurroundings

    When a system undergoes a change in energy, the surroundings must undergo a change in energy equal in magnitude and opposite in sign.

  • where q is heat, w is work

    Work and heat

    U can be changed (- or + ∆U) by a flow of work, heat, or both

    Usys = q + w

  • Sign Conventions of q and w

  • Calculate the overall change in internal

    energy for a system that absorbs 125 J of

    heat and does 141 J of work on the

    surroundings.

    q is + (heat absorbed)

    w is (work done)

    Usys = q + w = (+125 J) + (141J) = 16 J

  • Work

    common types of work Expansion- work

    done by the system

    Compression- work done on the system

    A

    FP

    hAPhFw

    VPw

    expansion +∆V -w

    compression -∆V +w

    P is external pressure

    Work is force applied over distance

  • Pressure-volume work, w, done by a system is

    w = PV

    Usys = q + w

    Usys = q P V

    Constant volume, V = 0

    qv = Usys qv means a constant-volume process

    5.3 Reactions carried out at constant volume

    or at constant pressure

  • U = q + w

    U = qp PV

    qp = U + PV

    Reactions carried out at constant pressure

  • Enthalpy and enthalpy changes

    Enthalpy is a property of a system definition: H = U + PV

    since U, P and V are all state functions, then H is also a state function

    The term enthalpy is composed of the prefix en-, meaning "to put into" and the Greek word -thalpein, meaning "to heat", that is “to put heat into”

    http://en.wikipedia.org/wiki/Greek_language

  • Enthalpy change

    H = U + PV

    The change in enthalpy

    H = U + (PV)

    When pressure is held

    constant

    H = U + PV

    Since

    qp = U + PV

    qp = H

  • At constant pressure

    qp = H

    Enthalpy of reaction

    H is + for endothermic changes.

    H is − for exothermic changes.

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    Equations that represent both mass and enthalpy changes

    Endothermic reaction H2O(s) H2O(l) H = + 6.01 kJ/mol

    Exothermic reaction

    Thermochemical Equations

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    Comparison of Endothermic and Exothermic Changes

  • Always specify state of reactants and products.

    When multiplying an equation by a factor (n), multiply the H value by same factor.

    Reversing an equation changes the sign but not the magnitude of the H.

    Thermochemical equation guidelines

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    Given the following equation,

    C6H12O6(s) + 6O2(g) → 6CO2(g) + 6H2O(l)

    ΔH = 2803 kJ/mol

    calculate the energy released when 45.00 g of glucose is burned in oxygen.

    kJ 700.0OHC mol 1

    kJ 2803

    OHC g 180.2

    OHC mol 1OHC g 45.00

    61266126

    61266126

  • 5.4 Calorimetry

    The science of measuring

    heat changes

    calorimeter- device used to experimentally find the heat associated with a chemical reaction

    substances respond differently when heated ( to raise T for two substances by 1 degree, they require different amount of heat)

  • Specific heat (s)

    Specific heat (s) - the amount of heat required to raise the temp of 1 g of a substance by 1C.

    Units: J/g C

    Relation to amount of heat (q)

    where q is heat, m is mass, s is specific heat

    and T = change in temp

    (T = Tfinal Tinitial)

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    Heat capacity (C) - the amount of heat required to raise the temp of an object by 1C.

    Units: J/C

    Relation to amount of heat (q)

    where q is heat, C is heat capacity

    and T = change in temp

    (T = Tfinal Tinitial)

  • Calculate the amount of energy required

    to heat 95.0 grams of water from 22.5C

    to 95.5C.

    T = Tfinal – Tinitial = 95.5 oC − 22.5oC

    T = 73.0 oC

    q = (95.0 g) (4.184 J/gC) (73.0C)

    q = 2.90 x 104 J or 29.0 kJ

  • Constant-Pressure Calorimetry

    uses simplest calorimeter (like coffee-cup calorimeter) since it is open to air

    used to find heat exchange

    between the system and

    surroundings of a chemical

    reaction

    i.e., changes in enthalpy

    for reactions occurring

    in a solution

    since qP = ∆H

    System: Reactants & Products

    Surroundings: the water

  • System: reactants and products

    Surroundings: water

    Assuming that the calorimeter

    does not leak or absorb heat

    coffee cup calorimeter

    Constant-pressure calorimetry

    For an exothermic reaction:

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    A metal pellet with a mass of 85.00 grams at an original

    temperature of 92.5C is dropped into a calorimeter\

    with 150.00grams of water at an original temperature of

    23.1C. The final temperature of the water and the pellet

    Is 26.8C. Calculate the heat capacity and the specific

    heat for the metal.

    Example

  • qwater = msT

    = (150.00 g) (4.184 J/gC) (3.7C)

    = 2300 J (water gained energy)

    = -2300 J (pellet released energy)

    Heat capacity of pellet: q = CT

    C = q/T

    = 2300 J/65.7C = 35 J/C

    Specific heat of pellet: J/goC

    s =35 J/oC

    85.00g= 0.41J/goC

  • bomb calorimeter

    Constant-volume calorimetry

    Isolated system

    Here, the ∆V = 0 so -P∆V = w = 0

    ∆U = q + w = qV for constant volume

  • Typical procedure used in a bomb calorimeter

    •Known amount of sample placed in steel

    container and then filled with oxygen gas

    •Steel chamber submerged in known amount of water

    •Sample ignited electrically

    •Temperature increase of water is determined

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    A snack chip with a mass of 2.36 g was burned in a bomb calorimeter. The heat capacity of the calorimeter 38.57 kJ/C. During the combustion the water temp rose by 2.70C. Calculate the energy in kJ/g for the chip

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    qrxn = − Ccal T

    = −(38.57 kJ/C) (2.70C)

    = − 104 kJ

    Energy content is a positive quantity.

    = 104 kJ/2.36 g

    = 44.1 kJ/g

    Food Calories: 10.5 Cal/g

  • Example 3

    Compare the energy released in the combustion of H2 and CH4 carried out in a bomb calorimeter with a heat capacity of 11.3 kJ/°C. The combustion of 1.50 g of methane produced a T change of 7.3°C while the combustion of 1.15 g of hydrogen produced a T change of 14.3°C. Find the energy of combustion per gram for each.

  • Example 3 methane: CH4

    hydrogen: H2

    The energy released by H2 is about 2.5 times the energy released by CH4

    gkJgkJH

    kJCC

    kJH

    TCH rcalorimete

    /555.1/83

    83)3.7()3.11(

    gkJgkJH

    kJCC

    kJH

    TCH rcalorimete

    /14115.1/162

    162)3.14()3.11(

  • 5.5 Hess’s Law

    Hess’s Law: The change in enthalpy that occurs when reactants are converted to products is the same whether the reaction occurs in one step or a series of steps.

    It is sed for calculating enthalpy for a reaction that cannot be determined directly.

  • Example 1

    N2(g) + 2O2(g) 2NO2(g) ∆H = 68 kJ

    OR

    N2(g) + O2(g) 2NO(g) ∆H = 180 kJ

    2NO(g) + O2(g) 2NO2(g)∆H = -112 kJ

    N2(g) + 2O2(g) 2NO2(g) ∆H = 68 kJ

  • Rules

    1. If a reaction is reversed, the sign of ∆H must be reversed as well.

    because the sign tells us the direction of heat flow at constant P

    2. The magnitude of ∆H is directly proportional to quantities of reactants and products in reaction.

    If coefficients are multiplied by an integer, the ∆H must be multiplied in the same way.

    because ∆H is an extensive property

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    Given the following equations:

    H3BO3(aq) HBO2(aq) + H2O(l) Hrxn = 0.02 kJ

    H2B4O7(aq) + H2O(l) 4 HBO2(aq) Hrxn = 11.3 kJ

    H2B4O7(aq) 2 B2O3(s) + H2O(l) Hrxn = 17.5 kJ

    Find the H for this overall reaction.

    2H3BO3(aq) B2O3(s) + 3H2O(l)

  • 2H3BO3(aq) 2HBO2(aq) + 2H2O(l) x 2

    Hrxn = 2(−0.02 kJ) = −0.04 kJ

    2HBO2(aq) 1/2H2B4O7(aq) + 1/2H2O(l) reverse, ÷2

    Hrxn = +11.3 kJ/2 = 5.65 kJ

    1/2H2B4O7(aq) B2O3(s)+ 1/2H2O(l) ÷ 2

    Hrxn = 17.5 kJ/2 = 8.75 kJ

    2H3BO3(aq) B2O3(s) + 3H2O(l)

    Hrxn = 14.36 kJ

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    5.6 Standard Enthalpies of Formation

    Symbol: Hf

    The enthalpy change that results when 1 mole of a compound is formed from its elements in their standard states.

    Hf for an element in its standard

    state is defined as zero.

    Standard state: 1 atm, 25C

    Values found in reference tables

    Used to calculate the Hrxn

  • Standard States

    For a compound:

    for gas: P = 1 atm

    For pure substances, it is a pure liquid or pure solid state

    in solution: concentration is 1 M

    For an element:

    form that exists in at 1 atm and 25°C

    O: O2(g) K: K(s) Br: Br2(l)

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    Hrxn = nHf

    (products) mHf

    (reactants)

    where denotes summation

    n and m are the coefficients in the

    balanced equation

    Defining equation for enthalpy of reaction:

  • Calculate the Hrxn for the following reaction

    from the table of standard values.

    CH4(g) + 2O2(g) CO2(g) + 2H2O(l)

    Hrxn = nHf

    (products) - mHf

    (reactants)

    = [1(393.5) + 2(285.8)] [1(74.8) + 2(0)]

    = 890.3 kJ/mol (exothermic)

    Example:

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    Key Points

    First law of thermodynamics

    Enthalpy (heat of formation; heat of reaction)

    State function

    Calorimetry

    Specific heat

    Hess’s law

    Calculations involving enthalpy, specific heat, energy