PHYSICAL CHEMISTRY. VOL.1+2 (LL)(11TH)
PHYSICAL CHEMISTRY. VOL.1+2 (LL)(11TH)
11th Edition
ISBN: 9780198826910
Author: ATKINS
Publisher: Oxford University Press
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Chapter 6, Problem 6B.2P

(a)

Interpretation Introduction

Interpretation:

The value of equilibrium constant for the dissociation of methane, CH4(g) has to be determined.

Concept introduction:

The equilibrium constant of a reaction represents the rate of the forward and backward reactions.  If the equilibrium constant is small, the rate of the backward reaction will be more than the rate of the forward reaction.  If the equilibrium constant is large, the rate of the forward reaction is more than the rate of backward reaction.

(a)

Expert Solution
Check Mark

Answer to Problem 6B.2P

The value of equilibrium constant for the dissociation of methane, CH4(g) is 1.250×10-9_.

Explanation of Solution

The decomposition of CH4(g) is represented by the reaction given below.

    CH4(g)C(s)+2H2(g)

The standard enthalpy change of the reaction (ΔrHΘ) is given by the formula below.

    ΔrHΘ=ΔfHΘproducts-ΔfHΘreactantsΔrHΘ=((2×ΔfHΘ(H2(g))+ΔfHΘ(C(s)))(ΔfHΘ(CH4(g))))        (1)

The values of standard enthalpy of formations are:

  • ΔfHΘ(C(s))=0kJmol1
  • ΔfHΘ(H2(g))=0mol1
  • ΔfHΘ(CH4(g))=74.85kJmol1

Substitute the corresponding values in the equation (1).

    ΔrHΘ=((2×0+0)(74.85kJmol1))=74.85kJmol1

The standard entropy change of the reaction (ΔrSΘ) is given by the formula below.

    ΔrSΘ=ΔSmΘproducts-ΔSmΘreactants

    ΔrSΘ=((2×ΔSmΘ(H2(g))+ΔSmΘ(C(s)))(ΔSmΘ(CH4(g))))        (2)

The values of standard molar entropies are:

  • ΔSmΘ(C(s))=5.740JK1mol1
  • ΔSmΘ(H2(g))=130.68JK1mol1
  • ΔSmΘΘ(CH4(g))=186.26JK1mol1

Substitute the corresponding values in the equation (2).

    ΔrSΘ=(((2×130.68JK1mol1)+5.740JK1mol1)(186.26JK1mol1))=(261.36JK1mol1+5.740JK1mol1)(186.26JK1mol1)=80.84JK1mol1

The formula to calculate ΔrGΘ is given below.

    ΔrGΘ=ΔrHΘTΔrSΘ        (3)

Where,

  • T is the temperature of the reaction

The temperature of the reaction (T) is 298K.

The value of ΔrHΘ is 74.85kJmol1.

The value of ΔrSΘ is 80.84JK1mol1.

Substitute the value of T, ΔrHΘ and ΔrSΘ in equation (3).

    ΔrGΘ=74.85kJmol1(298K×80.85JK1mol1)=(74.85kJmol1×1000J1kJ)(298K×80.84JK1mol1)=74850Jmol124093.3Jmol1=5.08×104Jmol1

The equilibrium constant (K) is calculated by the formula given below.

    lnK=ΔrGΘRT        (4)

Where,

  • R is the gas constant. (8.314JK1mol1).

Substitute the corresponding values in equation (4).

    lnK=5.08×104Jmol18.314JK1mol1×298KK=e20.50=1.250×10-9_

Therefore, the equilibrium constant is 1.250×10-9_.

(b)

Interpretation Introduction

Interpretation:

The equilibrium constant at 50°C has to be calculated.

Concept introduction:

The equilibrium constant of a reaction represents the rate of the forward and backward reactions.  If the equilibrium constant is small, the rate of the backward reaction will be more than the rate of the forward reaction.  If the equilibrium constant is large, the rate of the forward reaction is more than the rate of backward reaction.

(b)

Expert Solution
Check Mark

Answer to Problem 6B.2P

The equilibrium constant at 50°C is 1.216×10-10_.

Explanation of Solution

The value of temperature is 50°C.

The temperature values in degree Celsius is converted to Kelvin using the equation given below.

T(K)=T(°C)+273.15

Substitute the temperature value in the above equation as follows:

T(K)=T(°C)+273=50+273=323K

The formula to calculate equilibrium constant (K) at a given temperature is shown below.

    lnK2lnK1=ΔrHR(1T21T1)        (5)

Where,

  • ΔrHΘ is the standard enthalpy of reaction.
  • T1,T2 are temperatures.
  • K1,K2 are the equilibrium constant corresponding to the temperatures T1,T2.
  • R is the gas constant. (8.314JK1mol1).

The value of ΔrHΘ is 74.85kJmol1.

The conversion of kJmol1 to Jmol1 is shown below.

    1kJmol1=103Jmol1

Therefore, the conversion of 74.85kJmol1 to Jmol1 is shown below.

    74.85kJmol1=74.85×103Jmol1

The value of lnK1 is 20.50.

The value of T1 is 298K.

The value of T2 is 323K.

Substitute the value of ΔrHΘ, lnK1, T1, T2 and R in equation (5).

    lnK2(20.50)=74.85×103Jmol18.314JK1mol1(1323K1298K)lnK2+20.50=2.3383lnK2=22.83K2=1.216×10-10_

Therefore, the equilibrium constant at 50°C is 1.216×10-10_.

(c)

Interpretation Introduction

Interpretation:

The degree of dissociation of methane, α at 298K and a total pressure of 0.010bar has to be calculated.

Concept introduction:

Degree of disassociation of a molecule is the extent to which it has dissociated in its reaction.  Degree of dissociation is directly proportional to the equilibrium constant.

(c)

Expert Solution
Check Mark

Answer to Problem 6B.2P

The degree of dissociation of methane, α at 298K and a total pressure of 0.010bar is 1.76×104_.

Explanation of Solution

The disassociation of CH4(g) is represented by the reaction given below.

    CH4(g)C(s)+2H2(g)

The equilibrium composition is expressed in terms of dissociation constant, α and total pressure, p as shown below.

CH4(g)C(s)+2H2(g)2Initialn  00Change                  -nα       0     2nα             Equilibrium:(1-α)n02

Hence, the total number of moles of reaction at equilibrium is given below.

    (1+α)n

The formula for mole fraction is given below.

    Molefractionofcomponent=NumberofmolesofthecomponentTotalnumberofmoles

Therefore,

The mole fraction of CH4(g) is given below.

    MolefractionofCH4(g)=1-α1+α

The mole fraction of H2(g) is given below.

    MolefractionofH2(g)=1+α

The partial pressure is calculated by the formula given below.

    Partialpressure=Molefraction×Totalpressure

Hence,

The partial pressure of CH4(g) is given below.

    Partial pressureofCH4(g)=(1α)p1+α

The partial pressure of H2(g) is given below

    Partial pressureofH2(g)=p1+α

Where,

  • p is the total pressure.

The equilibrium constant for the given reaction in terms of partial pressure of each component is calculated by the formula shown below.

    K=(pH2)2pCH4        (6)

Where,

  • pH2 is the partial pressure of H2.
  • pCH4 is the partial pressure of CH4.

Substitute the value of pH2 and pCH4 in equation (6).

    K=(p1+α)2(1α)p1+α=2p(1α)2        (7)

As α is very less than 1, it can be neglected in the denominator of equation (7).

Therefore,

    K=2pα=K4p        (8)

The value of K is 1.250×10-9.

The value of p is 0.010bar.

Substitute the value of K and p in equation (8).

    α=1.250×10-94×0.010=1.76×104_

Therefore, the degree of dissociation of methane, α at 298K and a total pressure of 0.010bar is 1.76×104_.

(d)

Interpretation Introduction

Interpretation:

The explanation for the variation of degree of dissociation with pressure and temperature has to be stated.

Concept introduction:

Degree of disassociation of a molecule is the extent to which it has dissociated in its reaction.  Degree of dissociation is directly proportional to the equilibrium constant.

(d)

Expert Solution
Check Mark

Answer to Problem 6B.2P

As the pressure increases, the degree of dissociation decreases.  As the temperature increases, the degree of dissociation increases.

Explanation of Solution

The disassociation of CH4(g) is represented by the reaction given below.

    CH4(g)C(s)+2H2(g)

The moles of gaseous species are higher on the product side than the reactant side.  According to Le Chatelier’s principle, as the pressure of a system is increased the reaction shifts in the direction in which the number of moles of gaseous species decreases.  Therefore, reaction goes backward and degree of dissociation decreases on increasing pressure.

The value of ΔrHΘ is positive for the reaction.  Therefore, the reaction is endothermic. Increasing temperature favors the endothermic reaction according to the Le Chatelier’s principle.  The reaction goes forward and the degree of dissociation increases on increasing the temperature.

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Chapter 6 Solutions

PHYSICAL CHEMISTRY. VOL.1+2 (LL)(11TH)

Ch. 6 - Prob. 6A.2BECh. 6 - Prob. 6A.3AECh. 6 - Prob. 6A.3BECh. 6 - Prob. 6A.4AECh. 6 - Prob. 6A.4BECh. 6 - Prob. 6A.5AECh. 6 - Prob. 6A.5BECh. 6 - Prob. 6A.6AECh. 6 - Prob. 6A.6BECh. 6 - Prob. 6A.7AECh. 6 - Prob. 6A.7BECh. 6 - Prob. 6A.8AECh. 6 - Prob. 6A.8BECh. 6 - Prob. 6A.9AECh. 6 - Prob. 6A.9BECh. 6 - Prob. 6A.10AECh. 6 - Prob. 6A.10BECh. 6 - Prob. 6A.11AECh. 6 - Prob. 6A.11BECh. 6 - Prob. 6A.12AECh. 6 - Prob. 6A.12BECh. 6 - Prob. 6A.13AECh. 6 - Prob. 6A.13BECh. 6 - Prob. 6A.14AECh. 6 - Prob. 6A.14BECh. 6 - Prob. 6A.1PCh. 6 - Prob. 6A.2PCh. 6 - Prob. 6A.3PCh. 6 - Prob. 6A.4PCh. 6 - Prob. 6A.5PCh. 6 - Prob. 6A.6PCh. 6 - Prob. 6B.1DQCh. 6 - Prob. 6B.2DQCh. 6 - Prob. 6B.3DQCh. 6 - Prob. 6B.1AECh. 6 - Prob. 6B.1BECh. 6 - Prob. 6B.2AECh. 6 - Prob. 6B.2BECh. 6 - Prob. 6B.3AECh. 6 - Prob. 6B.3BECh. 6 - Prob. 6B.4AECh. 6 - Prob. 6B.4BECh. 6 - Prob. 6B.5AECh. 6 - Prob. 6B.5BECh. 6 - Prob. 6B.6AECh. 6 - Prob. 6B.6BECh. 6 - Prob. 6B.7AECh. 6 - Prob. 6B.7BECh. 6 - Prob. 6B.8AECh. 6 - Prob. 6B.8BECh. 6 - Prob. 6B.1PCh. 6 - Prob. 6B.2PCh. 6 - Prob. 6B.3PCh. 6 - Prob. 6B.4PCh. 6 - Prob. 6B.5PCh. 6 - Prob. 6B.6PCh. 6 - Prob. 6B.7PCh. 6 - Prob. 6B.8PCh. 6 - Prob. 6B.9PCh. 6 - Prob. 6B.10PCh. 6 - Prob. 6B.11PCh. 6 - Prob. 6B.12PCh. 6 - Prob. 6C.1DQCh. 6 - Prob. 6C.2DQCh. 6 - Prob. 6C.3DQCh. 6 - Prob. 6C.4DQCh. 6 - Prob. 6C.5DQCh. 6 - Prob. 6C.1AECh. 6 - Prob. 6C.1BECh. 6 - Prob. 6C.2AECh. 6 - Prob. 6C.2BECh. 6 - Prob. 6C.3AECh. 6 - Prob. 6C.3BECh. 6 - Prob. 6C.4AECh. 6 - Prob. 6C.4BECh. 6 - Prob. 6C.5AECh. 6 - Prob. 6C.5BECh. 6 - Prob. 6C.1PCh. 6 - Prob. 6C.2PCh. 6 - Prob. 6C.3PCh. 6 - Prob. 6C.4PCh. 6 - Prob. 6D.1DQCh. 6 - Prob. 6D.2DQCh. 6 - Prob. 6D.1AECh. 6 - Prob. 6D.1BECh. 6 - Prob. 6D.2AECh. 6 - Prob. 6D.2BECh. 6 - Prob. 6D.3AECh. 6 - Prob. 6D.3BECh. 6 - Prob. 6D.4AECh. 6 - Prob. 6D.4BECh. 6 - Prob. 6D.1PCh. 6 - Prob. 6D.2PCh. 6 - Prob. 6D.3PCh. 6 - Prob. 6D.4PCh. 6 - Prob. 6D.5PCh. 6 - Prob. 6D.6PCh. 6 - Prob. 6.1IACh. 6 - Prob. 6.2IACh. 6 - Prob. 6.3IACh. 6 - Prob. 6.4IACh. 6 - Prob. 6.7IACh. 6 - Prob. 6.8IACh. 6 - Prob. 6.10IACh. 6 - Prob. 6.12IA
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