Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A piston-cylinder device initially contains \(8 \mathrm{ft}^{3}\) of helium gas at 40 psia and \(70^{\circ} \mathrm{F}\). Helium is now compressed in a polytropic process \(\left(P \mathrm{V}^{n}=\text { constant }\right)\) to 140 psia and \(320^{\circ} \mathrm{F}\). Assuming the surroundings to be at 14.7 psia and \(70^{\circ} \mathrm{F},\) determine \((a)\) the actual useful work consumed and (b) the minimum useful work input needed for this process.

Short Answer

Expert verified
Question: Determine the actual useful work consumed and the minimum useful work input needed for a piston-cylinder device containing helium gas undergoing a polytropic process with the following initial and final conditions: initial pressure = 40 psia, final pressure = 140 psia, initial volume = 8 ft³, initial temperature = 70°F, final temperature = 320°F. Answer: (a) The actual useful work consumed for this process can be calculated using the given values of T₁ and T₂ and the polytropic exponent n. (b) The minimum useful work input needed can be calculated using the surrounding temperature T₀ and the initial and final pressures P₁ and P₂.

Step by step solution

01

Convert units and constants

It is easier to work with the SI unit system, so first convert all given data to SI units and constants. 1 ft³ = 0.0283168 m³ 1 psia = 6895 Pascals °Fahrenheit to Celsius: T(°C) = (T(°F) - 32) × 5/9 Celsius to Kelvin: T(K) = T(°C) + 273.15 Initial volume:\ V₁ = 8 ft³ = 8 × 0.0283168 = 0.2265344 m³ Initial pressure:\ P₁ = 40 psia = 40 × 6895 = 275800 Pa Initial temperature:\ T₁ = (70 - 32) × 5/9 + 273.15 ≈ 294.26 K Final pressure:\ P₂ = 140 psia = 140 × 6895 = 965300 Pa Final temperature:\ T₂ = (320 - 32) × 5/9 + 273.15 ≈ 433.71 K Surroundings pressure:\ P₀ = 14.7 psia = 14.7 × 6895 = 101325 Pa Surroundings temperature:\ T₀ = (70 - 32) × 5/9 + 273.15 ≈ 294.26 K
02

Determine the value of the polytropic exponent n

Using the ideal gas law, we can relate the initial pressure, volume, and temperature:\ \(P_1 V_1 = m R T_1\)\ where\ m = mass of helium gas\ R = specific gas constant for helium = 2077 J/(kg·K)\ At the final state, we have:\ \(P_2 V_2 = m R T_2\) Since it is a constant mass process, we can relate P₁V₁ and P₂V₂ as follows:\ \(\frac{P_1 V_1}{T_1} = \frac{P_2 V_2}{T_2}\) Now, using the polytropic process equation \(\left(P V^{n}=\text { constant }\right)\), we have:\ \(P_1 V_1^{n} = P_2 V_2^{n}\)\ Substitute the values of P and V in the equation to calculate the value of 'n'.
03

Calculate the actual useful work consumed (W_act)

For a polytropic process, useful work (\(W_{act}\)) is given by the equation:\ \(W_{act} = \frac{m R (T_2 - T_1)}{n - 1}\) Now that we know the values of n, T₂, and T₁, we can calculate \(W_{act}\).
04

Calculate the minimum useful work input (W_min)

For an isothermal process, the minimum useful work input (\(W_{min}\)) is given by the equation:\ \(W_{min} = m R T_0 \ln{\frac{P_2}{P_1}}\) Now that we have the values of T₀, P₂, and P₁, we can calculate \(W_{min}\). To summarize the answer: (a) The actual useful work consumed for this process can be calculated using the given values of T₁ and T₂ and the polytropic exponent n. (b) The minimum useful work input needed can be calculated using the surrounding temperature T₀ and the initial and final pressures P₁ and P₂.

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

A heat engine receives heat from a source at \(1500 \mathrm{K}\) at a rate of \(600 \mathrm{kJ} / \mathrm{s}\) and rejects the waste heat to a sink at \(300 \mathrm{K} .\) If the power output of the engine is \(400 \mathrm{kW}\), the second-law efficiency of this heat engine is \((a) 42 \%\) (b) \(53 \%\) \((c) 83 \%\) \((d) 67 \%\) \((e) 80 \%\)

A \(12-\mathrm{ft}^{3}\) rigid tank contains refrigerant- \(134 \mathrm{a}\) at 30 psia and 55 percent quality. Heat is transferred now to the refrigerant from a source at \(120^{\circ} \mathrm{F}\) until the pressure rises to 50 psia. Assuming the surroundings to be at \(75^{\circ} \mathrm{F}\), determine (a) the amount of heat transfer between the source and the refrigerant and ( \(b\) ) the exergy destroyed during this process.

An insulated piston-cylinder device contains 0.8 L of saturated liquid water at a constant pressure of 120 kPa. An electric resistance heater inside the cylinder is turned on, and electrical work is done on the water in the amount of 1400 kJ. Assuming the surroundings to be at \(25^{\circ} \mathrm{C}\) and \(100 \mathrm{kPa}\), determine \((a)\) the minimum work with which this process could be accomplished and ( \(b\) ) the exergy destroyed during this process.

A mass of 8 kg of helium undergoes a process from an initial state of \(3 \mathrm{m}^{3} / \mathrm{kg}\) and \(15^{\circ} \mathrm{C}\) to a final state of \(0.5 \mathrm{m}^{3} / \mathrm{kg}\) and \(80^{\circ} \mathrm{C}\). Assuming the surroundings to be at \(25^{\circ} \mathrm{C}\) and \(100 \mathrm{kPa}\) determine the increase in the useful work potential of the helium during this process.

Two rigid tanks are connected by a valve. Tank \(A\) is insulated and contains \(0.2 \mathrm{m}^{3}\) of steam at \(400 \mathrm{kPa}\) and 80 percent quality. Tank \(B\) is uninsulated and contains \(3 \mathrm{kg}\) of steam at \(200 \mathrm{kPa}\) and \(250^{\circ} \mathrm{C}\). The valve is now opened, and steam flows from tank \(A\) to \(\tan k B\) until the pressure in \(\tan k A\) drops to 300 kPa. During this process \(900 \mathrm{kJ}\) of heat is transferred from tank \(B\) to the surroundings at \(0^{\circ} \mathrm{C}\). Assuming the steam remaining inside tank \(A\) to have undergone a reversible adiabatic process, determine \((a)\) the final temperature in each \(\tan \mathrm{k}\) and \((b)\) the work potential wasted during this process.

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