/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 78 The work of \(146 \mathrm{~kJ}\)... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

The work of \(146 \mathrm{~kJ}\) is performed in order to compress 1 kilo mole of a gas adiabatically, and in this process, the temperature of the gas increases by \(7^{\circ} \mathrm{C}\). The gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}\right)\) (A) diatomic. (B) triatomic. (C) a mixture of monoatomic and diatomic. (D) monatomic.

Short Answer

Expert verified
Based on the analysis, it can be concluded that the given gas is a mixture of monoatomic and diatomic gases (option C).

Step by step solution

01

Calculate the temperature change in Kelvin

We are given that the temperature increases by 7°C. To convert this temperature change to Kelvin, we need to remember that the Kelvin scale has the same increments as the Celsius scale: \(\Delta T = 7 K\)
02

Use the adiabatic work formula to calculate the heat capacity at constant volume

We are given that the work done is 146 kJ, which we need to convert to J: \(W = 146 × 10^3 J\) We also know that there is 1 kilomole of the gas involved in the process, which means \(n = 1\). Since \(W = nC_V\Delta T\), we can rewrite this formula to find the heat capacity at constant volume: \(C_V = \frac{W}{n\Delta T}\) Now we can substitute the values: \(C_V = \frac{146 × 10^3}{1 × 7}\) \(C_V \approx 20857 J\,K^{-1}\, mol^{-1}\)
03

Compare the obtained value with the heat capacity values for different types of gases

We have the following heat capacity at constant volume for different gases: - Monatomic: \(C_V = \frac{3}{2}R\) - Diatomic: \(C_V = \frac{5}{2}R\) - Triatomic: \(C_V = \frac{f}{2}R\), where \(f\) is the degrees of freedom (usually 3). Substitute the given value of R: - Monatomic: \(C_V = \frac{3}{2} × 8.3 \approx 12.45 J\,K^{-1}\, mol^{-1}\) - Diatomic: \(C_V = \frac{5}{2} × 8.3 \approx 20.75 J\,K^{-1}\, mol^{-1}\) - Triatomic: \(C_V = \frac{3}{2} × 8.3 = 12.45 J\,K^{-1}\, mol^{-1}\) (assuming linear triatomic gas with 3 degrees of freedom) As we can see, the obtained value of \(C_V \approx 20857 J\,K^{-1}\, mol^{-1}\) does not match any of these values. This indicates that the given gas is a mixture.
04

Conclusion

Based on the analysis, it can be concluded that the given gas is a mixture of monoatomic and diatomic gases (option C).

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 91Ó°ÊÓ!

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

Three copper blocks of masses \(M_{1}, M_{2}\), and \(M_{3} \mathrm{~kg}\), respectively, are brought in to thermal contact till they reach equilibrium. Before contact, they were at \(T_{1}, T_{2}, T_{3}\left(T_{1}>T_{2}>T_{3}\right)\). Assuming there is no heat loss to the surroundings, the equilibrium temperature \(T\) is \((s\) is specific heat of copper) (A) \(T=\frac{T_{1}+T_{2}+T_{3}}{3}\) (B) \(T=\frac{M_{1} T_{1}+M_{2} T_{2}+M_{3} T_{3}}{M_{1}+M_{2}+M_{3}}\) (C) \(T=\frac{M_{1} T_{1}+M_{2} T_{2}+M_{3} T_{3}}{3\left(M_{1}+M_{2}+M_{3}\right)}\) (D) \(T=\frac{M_{1} T_{1} s+M_{2} T_{2} s+M_{3} T_{3} s}{M_{1}+M_{2}+M_{3}}\)

\(n\) moles of a gas expands from volume \(V_{1}\) to \(V_{2}\) at constant temperature \(T\). The work done by the gas is (A) \(n R T\left(\frac{v_{2}}{v_{1}}\right)\) (B) \(n R T\left(\frac{v_{2}}{v_{1}}-1\right)\) (C) \(n R T \ln \left(\frac{v_{1}}{v_{2}}\right)\) (D) None of these

Temperature of \(100 \mathrm{gm}\) water in changed from \(0^{\circ} \mathrm{C}\) to \(3^{\circ} \mathrm{C}\). In this process, heat supplied to water will be (specified heat of water \(=1 \mathrm{cal} / \mathrm{gm}{ }^{\circ} \mathrm{C}\) ) (A) Equal to \(300 \mathrm{cal}\) (B) Greater than \(300 \mathrm{cal}\) (C) Less than \(300 \mathrm{cal}\) (D) Data is insufficient

One mole of an ideal monatomic gas is taken from temperature \(T_{0}\) to \(2 T_{0}\) by the process \(P T^{-4}=C\) Considering the following statements, choose the correct alternative. I. Molar heat capacity of the gas is \(-\frac{3 R}{2}\) II. Molar heat capacity of the gas is \(\frac{3 R}{2}\) III. Work done is \(-3 R T_{0}\) IV. Work done is \(3 R T_{0}\) (A) Statements I and IV are correct. (B) Statements I and III are correct. (C) Statements II and IV are correct. (D) Statements II and III are correct.

When a system is taken from state \(i\) to state \(f\) along the path iaf, it is found \(Q=50 \mathrm{cal}\) and \(W=20\) cal. Along the path \(i b f, Q=36\) cal. \(W\) along the path \(i b f\) is [2007] (A) \(6 \mathrm{cal}\) (B) \(16 \mathrm{cal}\) (C) \(66 \mathrm{cal}\) (D) \(14 \mathrm{cal}\)

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.