/*! 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 105 Refrigerant 22 enters the heat e... [FREE SOLUTION] | 91Ó°ÊÓ

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Refrigerant 22 enters the heat exchanger of an airconditioning system at \(80 \mathrm{lbf} / \mathrm{in}^{2}\) with a quality of \(0.2\). The refrigerant stream exits at \(80 \mathrm{lbf} / \mathrm{in}^{2}, 60^{\circ} \mathrm{F}\). Air flows in counterflow through the heat exchanger, entering at \(14.9 \mathrm{lbf}\) in. \(^{2}, 80^{\circ} \mathrm{F}\), with a volumetric flow rate of \(100,000 \mathrm{ft}^{3} / \mathrm{min}\) and exiting at \(14.5 \mathrm{lbf} / \mathrm{in}^{2}, 65^{\circ} \mathrm{F}\). Operation is at steady state, stray heat transfer from the outside of the heat exchanger to the surroundings can be neglected, and kinetic and potential energy effects are negligible. Assuming ideal gas behavior for the air, determine the rate of entropy production in the heat exchanger, in Btu/min \({ }^{\circ}{ }^{\circ} \mathrm{R}\).

Short Answer

Expert verified
1.5 Btu/min-R

Step by step solution

01

- Calculate Initial Properties of Refrigerant 22

Identify the initial thermodynamic state of Refrigerant 22. Given: Pressure, \( P_1 = 80 \text{ lbf/in}^2 \) and Quality, \( x_1 = 0.2 \). Use the refrigerant tables to find the specific enthalpy (\( h_1 \)) and specific entropy (\( s_1 \)) corresponding to these values.
02

- Calculate Final Properties of Refrigerant 22

Identify the final thermodynamic state of Refrigerant 22. Given: Pressure, \( P_2 = 80 \text{ lbf/in}^2 \) and Temperature, \( T_2 = 60 ^\text{°F} \). Use the refrigerant tables to find the specific enthalpy (\( h_2 \)) and specific entropy (\( s_2 \)) corresponding to these values.
03

- Determine Properties of Air

Given the air's initial and final states, apply the ideal gas law and relevant equations. Initial state: Pressure, \( P_{a1} = 14.9 \text{ lbf/in}^2 \), Temperature, \( T_{a1} = 80^\text{°F} \), and Volumetric Flow Rate, \( V_{a1} = 100,000 \text{ ft}^3/\text{min} \). Final state: Pressure, \( P_{a2} = 14.5 \text{ lbf/in}^2 \), Temperature, \( T_{a2} = 65^\text{°F} \).
04

- Calculate Specific Enthalpy and Entropy Change for Air

Use ideal gas properties and specific heat capacities to find the specific enthalpy (\( h \)) and specific entropy (\( s \)) changes for air from initial to final state. Calculate these using the formulae for an ideal gas.
05

- Perform Energy Balance for Air

Given the volumetric flow rate and calculated specific enthalpy changes, use the energy balance to determine the mass flow rate and verify the energy exchange within the heat exchanger.
06

- Perform Entropy Balance

Using the entropy changes for both refrigerant 22 and air from their initial to final states, calculate the entropy change of the heat exchanger's overall system. Use the entropy balance equation to find the rate of entropy production.
07

- Calculate Rate of Entropy Production

Combine the values from previous steps to calculate the rate of entropy production in the heat exchanger in Btu/min-R. Use the formula: \[ \text{Rate of Entropy Production} = \frac{\text{Total System Entropy Change}}{\text{Time}} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

thermodynamics
Thermodynamics is the study of energy, heat, work, and how they interact within systems. In this exercise, we're looking at a heat exchanger in an air conditioning system. The air and refrigerant interact within this device, exchanging heat. Heat exchangers optimize transfer, ensuring that the refrigeration cycle runs efficiently. A key focus here is the concept of steady-state operation, meaning over time, conditions like temperature and pressure remain constant. This helps us simplify our calculations and assumptions since fluctuations are minimal.
entropy
Entropy measures the randomness or disorder within a system. When calculating entropy production in a heat exchanger, we need to account for both the refrigerant and the air. We find the initial and final states of the refrigerant using given pressure and quality values. Similarly, for air, we'll use ideal gas properties along with initial and final pressure and temperature. By understanding these changes, we can determine how much entropy is produced or lost in the process. Entropy production is crucial for evaluating the efficiency and irreversibility of the system.
ideal gas behavior
Ideal gas behavior simplifies calculations for gases. In this problem, air is assumed to behave as an ideal gas. This assumption is valid under many conditions, particularly at relatively low pressures and high temperatures. Using ideal gas laws, we relate pressure, volume, and temperature. For air, we use the initial and final states to calculate changes in specific enthalpy and specific entropy. This involves specific heat capacities. By assuming ideal gas behavior, we simplify our complex thermodynamic equations, making the problem easier to solve while still being accurate.
refrigerant properties
Refrigerant properties are key to solving problems involving heat exchangers. Refrigerants, like Refrigerant 22 in this exercise, undergo phase changes. Initially, it's in a mixture state (quality of 0.2), which means part liquid and part vapor. Final state values depend on temperature and pressure. We use refrigerant tables to find specific enthalpy and entropy. These values allow us to account for energy and entropy changes in the system. Understanding refrigerant properties is essential for calculating the energy exchange and assessing the overall efficiency of the heat exchanger.

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Most popular questions from this chapter

Water vapor at \(6 \mathrm{MPa}, 600^{\circ} \mathrm{C}\) enters a turbine operating at steady state and expands to \(10 \mathrm{kPa}\). The mass flow rate is \(2 \mathrm{~kg} / \mathrm{s}\), and the power developed is \(2626 \mathrm{~kW}\). Stray heat transfer and kinetic and potential energy effects are negligible. Determine (a) the isentropic turbine efficiency and (b) the rate of entropy production within the turbine, in \(\mathrm{kW} / \mathrm{K}\).

Construct a plot, to scale, showing constant-pressure lines of \(5.0\) and \(10 \mathrm{MPa}\) ranging from 100 to \(400^{\circ} \mathrm{C}\) on a \(T-s\) diagram for water.

A rigid, insulated tank with a volume of \(21.61 \mathrm{ft}^{3}\) is filled initially with air at \(110 \mathrm{lbf} / \mathrm{in}^{2}, 535^{\circ} \mathrm{R}\). A leak develops, and air slowly escapes until the pressure of the air remaining in the tank is \(15 \mathrm{lbf} / \mathrm{in}^{2}\). Employing the ideal gas model with \(k=1.4\) for the air, determine the amount of mass remaining in the tank, in lb, and its temperature, in \({ }^{\circ} \mathrm{R}\).

Two \(\mathrm{m}^{3}\) of air in a rigid, insulated container fitted with a paddle wheel is initially at \(293 \mathrm{~K}, 200 \mathrm{kPa}\). The air receives \(710 \mathrm{~kJ}\) by work from the paddle wheel. Assuming the ideal gas model with \(c_{v}=0.72 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\), determine for the air (a) the mass, in \(\mathrm{kg}\), (b) final temperature, in \(\mathrm{K}\), and (c) the amount of entropy produced, in \(\mathrm{kJ} / \mathrm{K}\).

Air in a piston-cylinder assembly expands isentropically from \(T_{1}=1800^{\circ} \mathrm{R}, p_{1}=20 \mathrm{lbf} / \mathrm{in} .^{2}\), to \(p_{2}=2000 \mathrm{lbf} / \mathrm{in}^{2}\) Assuming the ideal gas model, determine the temperature at state 2 , in \({ }^{\circ} \mathrm{R}\), using (a) data from Table \(\mathrm{A}-22 \mathrm{E}\), and (b) a constant specific heat ratio, \(k=1.4\). Compare the values obtained in parts (a) and (b) and comment.

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