The work done for the each given pathways has to be identified. Concept Introduction: The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below. w = − P ex Δ V The expression for calculating the work of isothermal expansion is shown below. w = − n R T ln ( V f V i )

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Answer 1

Question

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

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Answer 2

Question

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

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Answer 3

Question

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

Expert Solution & Answer

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Answer 4

Question

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

Expert Solution & Answer

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Answer 5

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

Answer 6

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

Answer 7

Chapter 4, Problem 4B.14E

Interpretation Introduction

Interpretation:

The work done for the each given pathways has to be identified.

Concept Introduction:

The system can done two kind of works. The one is the work of expansion which is the work which arises from the change in the volume of the system. On the other hand the second work done is the work of non-expansion which does not involve any change in the volume of the system. The expression for calculating the work of reversible expansion is shown below.

w=−PexΔV

The expression for calculating the work of isothermal expansion is shown below.

w=−nRTln(VfVi)

Answer 8

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Answer 9

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Answer 10

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Answer 11

Ch. 4 - Prob. 4A.1AST Ch. 4 - Prob. 4A.1BST Ch. 4 - Prob. 4A.2AST Ch. 4 - Prob. 4A.2BST Ch. 4 - Prob. 4A.3AST Ch. 4 - Prob. 4A.3BST Ch. 4 - Prob. 4A.4AST Ch. 4 - Prob. 4A.4BST Ch. 4 - Prob. 4A.1E Ch. 4 - Prob. 4A.2E

Solution Summary: The author explains that the system can do two kinds of works: expansion, non-expansion, and isothermal expansion.

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