Repeat Problem 57, with the pressure now kept constant.

Short Answer

Expert verified

The change in the entropy of the gas at constant pressure is 5.98 J/K

Step by step solution

01

The given data

The number of moles is n = 1.00 mol .

The gas ismonatomic.

The initial temperature isTi=300K.

The final temperature isTf=400K.

The pressure is constant.

02

Understanding the concept of entropy change

By finding the equation for heat absorbed at constant pressure and using Equation 20-1, we can find the change in the entropy of the gas at constant pressure.

Formula:

The energy absorbed as heat by the gas at constant pressure, dQ=52nRdT (1)

The change in entropy of the gas, S=dQT (2)

03

Calculation of the entropy change

Since the pressureis kept constant, substituting the value of equation (1) in equation (2), we can get the change in entropy as given:

S=TiTf5nR2dTT=52nRlnTfTi=52×1.00mol×8.31Jmol·K×400K300K=5.98J/K

Hence, the value of the entropy change is 5.98 J/K

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Figure 20-33 gives the force magnitude Fversus stretch distance xfor a rubber band, with the scale of the Faxis set byFs=1.50Nand the scale of the x-axis set byxs=3.50cm .The temperature is2.00°C . When the rubber band is stretched byx=1.70cm, at what rate does the entropy of the rubber band change during a small additional stretch?

Find the relation between the efficiency of a reversible ideal heat engine and the coefficient of performance of the reversible refrigerator obtained by running the engine backward.

An inventor has built an engine X and claims that its efficiency X is greater than the efficiency of an ideal engine operating between the same two temperatures. Suppose you couple engine X to an ideal refrigerator (Fig. 20-34a) and adjust the cycle of engine X so that the work per cycle it provides equals the work per cycle required by the ideal refrigerator. Treat this combination as a single unit and show that if the inventor’s claim were true(ifεx>ε), the combined unit would act as a perfect refrigerator (Fig. 20-34b), transferring energy as heat from the low-temperature reservoir to the high-temperature reservoir without the need for work.

System Aof three particles and system B of five particles are in insulated boxes like that in Fig. 20-17. What is the least multiplicity W of (a) system A and (b) system B ? What is the greatest multiplicity Wof (c) A and (d) B ? What is the greatest entropy of (e) A and (f) B?

An ideal monatomic gas at initial temperatureT0(in Kelvins) expands from initial volumeV0 to volume2V0by each of the five processes indicated in the T-Vdiagram of Fig. 20-20. In which process is the expansion (a) isothermal, (b) isobaric (constant pressure), and (c) adiabatic? Explain your answers. (d) In which processes does the entropy of the gas decrease?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free