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

Air is compressed steadily and adiabatically from \(17^{\circ} \mathrm{C}\) and \(90 \mathrm{kPa}\) to \(200^{\circ} \mathrm{C}\) and \(400 \mathrm{kPa} .\) Assuming constant specific heats for air at room temperature, the isentropic efficiency of the compressor is \((a) 0.76\) \((b) 0.94\) \((c) 0.86\) \((d) 0.84\) \((e) 1.00\)

Short Answer

Expert verified
Answer: (a) 0.76

Step by step solution

01

Recall the adiabatic relations for an ideal gas

From the ideal gas law, we know that \(PV^{\gamma}= \text{constant}\) and \(T V^{\gamma-1}=\text{constant}\) for an adiabatic (isentropic) process, where P is pressure, V is volume, T is temperature, and \(\gamma\) is the ratio of specific heats (\(c_p/c_v\)). For air, we can assume \(\gamma = 1.4\).
02

Calculate the actual work required for compression

We first need to find the actual work required to compress the air adiabatically. Since the process is adiabatic, we have: \(W_{actual} = c_p (T_2-T_1)\) where \(T_1\) and \(T_2\) are the initial and final temperatures (in Kelvin), and \(c_p\) is the specific heat at constant pressure (approx \(1005\,\mathrm{J/kg\cdot K}\) for air at room temperature). Converting the temperature to Kelvin: \(T_1 = 17^{\circ} \mathrm{C}+273.15 = 290.15 \,\mathrm{K}\) \(T_2 = 200^{\circ} \mathrm{C}+273.15 = 473.15 \,\mathrm{K}\) Now, we calculate the actual work required: \(W_{actual} = 1005 \,\mathrm{J/kg\cdot K}\times (473.15 \,\mathrm{K} - 290.15 \,\mathrm{K}) = 183768.25\,\mathrm{J/kg}\)
03

Calculate the ideal work required in an isentropic process

Using the adiabatic relations, we can calculate the ideal work required: \(W_{ideal} = \dfrac{R(T_2'-T_1)}{1-\gamma}\) We can find the ideal final temperature \(T_2'\), given by: \(\left(\dfrac{P_1}{P_2}\right)^{\frac{\gamma-1}{\gamma}} = \dfrac{T_2'}{T_1} \Longrightarrow T_2' = T_1 \left(\dfrac{P_1}{P_2}\right)^{\frac{\gamma-1}{\gamma}}\) The gas constant for air, \(R = 287 \,\mathrm{J/kg\cdot K}\). Now we find \(T_2'\): \(T_2' = 290.15 \,\mathrm{K} \times \left(\dfrac{90\,\mathrm{kPa}}{400\,\mathrm{kPa}}\right)^{0.4} = 194.86 \,\mathrm{K}\) Now, we calculate the ideal work required in an isentropic process: \(W_{ideal} = \dfrac{287 \,\mathrm{J/kg\cdot K}(194.86 \,\mathrm{K} - 290.15 \,\mathrm{K})}{1-1.4} = 139251.56 \,\mathrm{J/kg}\)
04

Calculate the isentropic efficiency

The isentropic efficiency of the compressor can be calculated as the ratio of the ideal work to the actual work: \(\eta_{isentropic} = \dfrac{W_{ideal}}{W_{actual}} = \dfrac{139251.56 \,\mathrm{J/kg}}{183768.25 \,\mathrm{J/kg}} = 0.7576\) So, the isentropic efficiency of the compressor, when rounding up, is approximately 0.76. Thus, the correct answer is: \((a) 0.76\).

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

The polytropic or small stage efficiency of a compressor \(\eta_{\infty}, c\) is defined as the ratio of the actual differential work done on the fluid to the isentropic differential work done on the flowing through the compressor \(\eta_{\infty}, c=d h_{s} / d h\) Consider an ideal gas with constant specific heats as the working fluid undergoing a process in a compressor in which the polytropic efficiency is constant. Show that the temperature ratio across the compressor is related to the pressure ratio across the compressor by $$\frac{T_{2}}{T_{1}}=\left(\frac{P_{2}}{P_{1}}\right)^{\left(\frac{1}{\eta_{\infty, C}}\right)\left(\frac{R}{c_{p}}\right)}=\left(\frac{P_{2}}{P_{1}}\right)^{\left(\frac{1}{\eta_{\infty, C}}\right)\left(\frac{k-1}{k}\right)}$$

One ton of liquid water at \(80^{\circ} \mathrm{C}\) is brought into a well- insulated and well-sealed \(4-\mathrm{m} \times 5-\mathrm{m} \times 7-\mathrm{m}\) room initially at \(22^{\circ} \mathrm{C}\) and \(100 \mathrm{kPa}\). Assuming constant specific heats for both air and water at room temperature, determine (a) the final equilibrium temperature in the room and \((b)\) the total entropy change during this process, in \(\mathrm{kJ} / \mathrm{K}\).

In order to cool 1 -ton of water at \(20^{\circ} \mathrm{C}\) in an insulated tank, a person pours \(80 \mathrm{kg}\) of ice at \(-5^{\circ} \mathrm{C}\) into the water. Determine ( \(a\) ) the final equilibrium temperature in the \(\operatorname{tank}\) and \((b)\) the entropy generation during this process. The melting temperature and the heat of fusion of ice at atmospheric pressure are \(0^{\circ} \mathrm{C}\) and \(333.7 \mathrm{kJ} / \mathrm{kg}\).

The inner and outer glasses of a \(2-\mathrm{m} \times 2\) -m double-pane window are at \(18^{\circ} \mathrm{C}\) and \(6^{\circ} \mathrm{C}\), respectively. If the glasses are very nearly isothermal and the rate of heat transfer through the window is \(110 \mathrm{W}\), determine the rates of entropy transfer through both sides of the window and the rate of entropy generation within the window, in \(\mathrm{W} / \mathrm{K}\).

Water at 20 psia and \(50^{\circ} \mathrm{F}\) enters a mixing chamber at a rate of 300 lbm/min where it is mixed steadily with steam entering at 20 psia and \(240^{\circ} \mathrm{F}\). The mixture leaves the chamber at 20 psia and \(130^{\circ} \mathrm{F}\), and heat is lost to the surrounding air at \(70^{\circ} \mathrm{F}\) at a rate of \(180 \mathrm{Btu} / \mathrm{min}\). Neglecting the changes in kinetic and potential energies, determine the rate of entropy generation 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