Physics for Scientists and Engineers, Vol. 1
Physics for Scientists and Engineers, Vol. 1
6th Edition
ISBN: 9781429201322
Author: Paul A. Tipler, Gene Mosca
Publisher: Macmillan Higher Education
bartleby

Videos

Question
Book Icon
Chapter 18, Problem 72P

(a)

To determine

The PV diagram for each process in the cycle.

(a)

Expert Solution
Check Mark

Answer to Problem 72P

The required PV diagram is shown in Figure 1.

Explanation of Solution

Given data:

The amount n of sample of N2 gas is 1mol .

The temperature T1 of the gas is 20°C .

The pressure P1 of the gas is 5atm .

The pressure P2 of the gas after adiabatic expansion is 1atm .

The temperature T2 of the gas after adiabatic process is t1°C .

The pressure P3 of the gas after isobaric expansion is 1atm .

The temperature T3 of the gas after isobaric expansion process is 20°C .

The pressure P4 of the gas after isometric expansion is 5atm .

The temperature T4 of the gas after isometric process is t2°C .

The pressure P5 of the gas after isobaric compression expansion is 5atm .

The temperature T5 of the gas after isobaric compression process is 20°C .

Formula:

The expression to determine the initial volume of the gas is given by,

  V1=nRT1P1

The volume of the gas after the adiabatic process is given by,

  V2=( P 1 P 2 )1γV1

The expression for the temperature of the gas after adiabatic process is given by,

  T2=( V 1 V 2 )γ1T1

The volume of the gas after the isobaric process is given by,

  V3=(T3T2)V2

The expression to determine the temperature of the gas after the isometric expansion is given by,

  T4=P4P3T3

The expression for the volume of the gas after the isobaric process is given by,

  V5=(T5T4)V4

Calculation:

The initial volume of the gas is calculated as,

  V1=nRT1P1=(1)( 0.08206)( 20°C)5atm=(1)( 0.08206)( 20K+273K)5atm=4.81L

The volume of the gas after the adiabatic process is calculated as,

  V2=( P 1 P 2 )1γV1=( 5atm 1atm)1 1.44.81L=15.18L

The temperature of the gas after adiabatic process is calculated as,

  T2=( V 1 V 2 )γ1T1=( 4.81L 15.18L)γ1(293K)=185.02K=(185.02K273°C)

Solve further as,

  T2=88.14°C

The volume of the gas after the isobaric process is calculated as,

  V3=( T 3 T 2 )V2=( 293K 185.02)(15.18L)=24.04L

The expression to determine the temperature of the gas after the isometric expansion is given by,

  T4=P4P3T3=51(293K)=(1465K273K)=1192°C

The expression for the volume of the gas after the isobaric process is given by,

  V5=( T 5 T 4 )V4=( 293K 1465K)(24.04°C)=4.81L

From the above calculations the PV diagram for the different process is shown below.

The required diagram is shown in Figure 1

  Physics for Scientists and Engineers, Vol. 1, Chapter 18, Problem 72P

Figure 1

Conclusion:

Therefore, the required PV diagram is shown in Figure 1.

(b)

To determine

The work done by the gas during the complete cycle.

(b)

Expert Solution
Check Mark

Answer to Problem 72P

The work done in the complete cycle is 6763J .

Explanation of Solution

Formula Used:

The expression to determine the work done by the gas from A to B is given by,

  WAB=P2V2P1V1γ1

The expression to determine the work done by the gas from B to C is given by,

  WBC=P2(V3V2)

The expression to determine the work done by the gas from D to A is given by,

  WDA=P1(V1V4)

The expression for the total work during the complete cycle is given by,

  W=WAB+WBC+WDA=P2V2P1V1γ1P2(V3V2)P1(V1V4)

Calculation:

The total work during the complete cycle is calculated as,

  W=P2V2P1V1γ1P2(V3V2)P1(V1V4)=( 1atm)( 15.82L)( 1.5atm)( 4.81L)1.41(1)(24.04L15.18L)(5atm)(4.81L24.04L)=20.575Latm8.86Latm+96.15Latm=(20.575Latm8.86Latm+96.15Latm)101.3J

Solve further as,

  W=6763J

Conclusion:

Therefore, the work done in the complete cycle is 6763J .

(c)

To determine

The heat absorbed by the gas during the complete cycle.

(c)

Expert Solution
Check Mark

Answer to Problem 72P

The heat absorbed by the gas is 6763J .

Explanation of Solution

Formula:

The expression for the first law of thermodynamics is given by,

  dQin=dW

Calculation:

The heat absorbed by the gas is calculated as,

  dQin=dW=6763J

Conclusion:

Therefore, the heat absorbed by the gas is 6763J .

Want to see more full solutions like this?

Subscribe now to access step-by-step solutions to millions of textbook problems written by subject matter experts!
Students have asked these similar questions
A cylinder with a piston contains 0.153 mol of nitrogen at a pressure of 1.83×105 Pa and a temperature of 290 K. The nitrogen may be treated as an ideal gas. The gas is first compressed isobarically to half its original volume. It then expands adiabatically back to its original volume, and finally it is heated isochorically to its original pressure. Part A Compute the temperature at the beginning of the adiabatic expansion. Express your answer in kelvins. ΕΠΙ ΑΣΦ T₁ = ? K Submit Request Answer Part B Compute the temperature at the end of the adiabatic expansion. Express your answer in kelvins. Π ΑΣΦ T₂ = Submit Request Answer Part C Compute the minimum pressure. Express your answer in pascals. ΕΠΙ ΑΣΦ P = Submit Request Answer ? ? K Pa
Learning Goal: To understand the meaning and the basic applications of pV diagrams for an ideal gas. As you know, the parameters of an ideal gas are described by the equation pV = nRT, where p is the pressure of the gas, V is the volume of the gas, n is the number of moles, R is the universal gas constant, and T is the absolute temperature of the gas. It follows that, for a portion of an ideal gas, pV = constant. Τ One can see that, if the amount of gas remains constant, it is impossible to change just one parameter of the gas: At least one more parameter would also change. For instance, if the pressure of the gas is changed, we can be sure that either the volume or the temperature of the gas (or, maybe, both!) would also change. To explore these changes, it is often convenient to draw a graph showing one parameter as a function of the other. Although there are many choices of axes, the most common one is a plot of pressure as a function of volume: a pV diagram. In this problem, you…
Learning Goal: To understand the meaning and the basic applications of pV diagrams for an ideal gas. As you know, the parameters of an ideal gas are described by the equation pV = nRT, where p is the pressure of the gas, V is the volume of the gas, n is the number of moles, R is the universal gas constant, and T is the absolute temperature of the gas. It follows that, for a portion of an ideal gas, pV = constant. T One can see that, if the amount of gas remains constant, it is impossible to change just one parameter of the gas: At least one more parameter would also change. For instance, if the pressure of the gas is changed, we can be sure that either the volume or the temperature of the gas (or, maybe, both!) would also change. To explore these changes, it is often convenient to draw a graph showing one parameter as a function of the other. Although there are many choices of axes, the most common one is a plot of pressure as a function of volume: a pV diagram. In this problem, you…

Chapter 18 Solutions

Physics for Scientists and Engineers, Vol. 1

Ch. 18 - Prob. 11PCh. 18 - Prob. 12PCh. 18 - Prob. 13PCh. 18 - Prob. 14PCh. 18 - Prob. 15PCh. 18 - Prob. 16PCh. 18 - Prob. 17PCh. 18 - Prob. 18PCh. 18 - Prob. 19PCh. 18 - Prob. 20PCh. 18 - Prob. 21PCh. 18 - Prob. 22PCh. 18 - Prob. 23PCh. 18 - Prob. 24PCh. 18 - Prob. 25PCh. 18 - Prob. 26PCh. 18 - Prob. 27PCh. 18 - Prob. 28PCh. 18 - Prob. 29PCh. 18 - Prob. 30PCh. 18 - Prob. 31PCh. 18 - Prob. 32PCh. 18 - Prob. 33PCh. 18 - Prob. 34PCh. 18 - Prob. 35PCh. 18 - Prob. 36PCh. 18 - Prob. 37PCh. 18 - Prob. 38PCh. 18 - Prob. 39PCh. 18 - Prob. 40PCh. 18 - Prob. 41PCh. 18 - Prob. 42PCh. 18 - Prob. 43PCh. 18 - Prob. 44PCh. 18 - Prob. 45PCh. 18 - Prob. 46PCh. 18 - Prob. 47PCh. 18 - Prob. 48PCh. 18 - Prob. 49PCh. 18 - Prob. 50PCh. 18 - Prob. 51PCh. 18 - Prob. 52PCh. 18 - Prob. 53PCh. 18 - Prob. 54PCh. 18 - Prob. 55PCh. 18 - Prob. 56PCh. 18 - Prob. 57PCh. 18 - Prob. 58PCh. 18 - Prob. 59PCh. 18 - Prob. 60PCh. 18 - Prob. 61PCh. 18 - Prob. 62PCh. 18 - Prob. 63PCh. 18 - Prob. 64PCh. 18 - Prob. 65PCh. 18 - Prob. 66PCh. 18 - Prob. 67PCh. 18 - Prob. 68PCh. 18 - Prob. 69PCh. 18 - Prob. 70PCh. 18 - Prob. 71PCh. 18 - Prob. 72PCh. 18 - Prob. 73PCh. 18 - Prob. 74PCh. 18 - Prob. 75PCh. 18 - Prob. 76PCh. 18 - Prob. 77PCh. 18 - Prob. 78PCh. 18 - Prob. 79PCh. 18 - Prob. 80PCh. 18 - Prob. 81PCh. 18 - Prob. 82PCh. 18 - Prob. 83PCh. 18 - Prob. 84PCh. 18 - Prob. 85PCh. 18 - Prob. 86PCh. 18 - Prob. 87PCh. 18 - Prob. 88PCh. 18 - Prob. 89PCh. 18 - Prob. 90PCh. 18 - Prob. 91PCh. 18 - Prob. 92PCh. 18 - Prob. 93PCh. 18 - Prob. 94PCh. 18 - Prob. 95PCh. 18 - Prob. 96PCh. 18 - Prob. 97PCh. 18 - Prob. 98P
Knowledge Booster
Background pattern image
Physics
Learn more about
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, physics and related others by exploring similar questions and additional content below.
Similar questions
SEE MORE QUESTIONS
Recommended textbooks for you
Text book image
Principles of Physics: A Calculus-Based Text
Physics
ISBN:9781133104261
Author:Raymond A. Serway, John W. Jewett
Publisher:Cengage Learning
Text book image
Physics for Scientists and Engineers, Technology ...
Physics
ISBN:9781305116399
Author:Raymond A. Serway, John W. Jewett
Publisher:Cengage Learning
Text book image
University Physics Volume 2
Physics
ISBN:9781938168161
Author:OpenStax
Publisher:OpenStax
Text book image
Physics for Scientists and Engineers: Foundations...
Physics
ISBN:9781133939146
Author:Katz, Debora M.
Publisher:Cengage Learning
Text book image
College Physics
Physics
ISBN:9781285737027
Author:Raymond A. Serway, Chris Vuille
Publisher:Cengage Learning
Text book image
Physics for Scientists and Engineers
Physics
ISBN:9781337553278
Author:Raymond A. Serway, John W. Jewett
Publisher:Cengage Learning
Thermodynamics: Crash Course Physics #23; Author: Crash Course;https://www.youtube.com/watch?v=4i1MUWJoI0U;License: Standard YouTube License, CC-BY