/*! 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 151 A supply of geothermal hot water... [FREE SOLUTION] | 91Ó°ÊÓ

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A supply of geothermal hot water is to be used as the energy source in an ideal Rankine cycle, with \(\mathrm{R}-134 \mathrm{a}\) as the cycle working fluid. Saturated vapor \(\mathrm{R}-134\) a leaves the boiler at a temperature of \(180 \mathrm{~F}\), and the condenser temperature is \(100 \mathrm{~F}\). Calculate the thermal efficiency of this cycle.

Short Answer

Expert verified
The thermal efficiency of the cycle is approximately 12.54%.

Step by step solution

01

Convert Temperatures to Kelvin

First, convert the given temperatures from Fahrenheit to Kelvin. Use the conversion formula: \[ K = \frac{5}{9}(F - 32) + 273.15 \]For \(T_{ ext{boiler}} = 180 \text{~F}\), the conversion is: \[ T_{ ext{boiler}} = \frac{5}{9}(180 - 32) + 273.15 = 355.372 \text{~K} \]For \(T_{ ext{condenser}} = 100 \text{~F}\), the conversion is: \[ T_{ ext{condenser}} = \frac{5}{9}(100 - 32) + 273.15 = 310.928 \text{~K} \]
02

Use Rankine Cycle Thermal Efficiency Formula

The thermal efficiency \( \eta \) of an ideal Rankine cycle can be expressed as:\[ \eta = 1 - \frac{T_{ ext{condenser}}}{T_{ ext{boiler}}} \]Substitute the temperatures into the formula:\[ \eta = 1 - \frac{310.928}{355.372} \]
03

Calculate Thermal Efficiency

Now, solve the expression from Step 2 to find the thermal efficiency:\[ \eta = 1 - \frac{310.928}{355.372} \approx 1 - 0.8746 = 0.1254 \]The thermal efficiency of the cycle is approximately \(12.54\%\).

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Key Concepts

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

Thermal Efficiency
Thermal efficiency is a crucial concept in thermodynamics and engineering. It measures how effectively a heat engine converts heat into work. In the context of the Rankine Cycle, which is a model used to predict the performance of steam power plants, thermal efficiency is calculated using the temperatures of the boiling and condensing phases. To find the thermal efficiency \( \eta \) in an ideal Rankine Cycle, we use the formula: \[ \eta = 1 - \frac{T_{\text{condenser}}}{T_{\text{boiler}}} \]This formula signifies that efficiency depends on the difference between the boiling (high) and condensing (low) temperatures. A larger temperature difference generally improves efficiency, as it reflects more energy being converted into work rather than wasted. In practical applications, improving thermal efficiency can lead to significant energy savings and reduced environmental impact. Understanding this concept helps optimize energy systems by maximizing output relative to the input.
Geothermal Energy
Geothermal energy is a sustainable energy source harnessed from heat stored beneath the Earth's surface. It originates from the planet's core and can be tapped through the use of steam and hot water reservoirs found underground. This form of energy is particularly beneficial as it provides a renewable and eco-friendly alternative, reducing reliance on fossil fuels and minimizing carbon emissions. In the Rankine Cycle exercise, geothermal energy supplies the necessary heat to vaporize the working fluid, R-134a. This is an application of the geothermal resource, where the heat energy extracted from the earth powers turbines for electricity generation. Benefits of geothermal energy include:
  • Abundant and continuous source.
  • Low operational costs once established.
  • Minimal environmental footprint.
By utilizing geothermal resources efficiently, we make strides towards sustainable energy futures.
Temperature Conversion
Temperature conversion is fundamental to thermodynamic calculations as it standardizes input values across different units of measurement. In the study of the Rankine Cycle, converting temperatures from Fahrenheit to Kelvin is essential because Kelvin is the standard unit for absolute temperature in scientific calculations. The conversion is performed using the formula: \[ K = \frac{5}{9}(F - 32) + 273.15 \]By applying this formula, the boiler and condenser temperatures are turned into Kelvin, which allows accurate calculations of the Rankine Cycle’s thermal efficiency. This process reflects how precision in mathematical operations is vital for ensuring the integrity of scientific investigations. Consistently using Kelvin in thermodynamic equations prevents inconsistencies and errors associated with temperature scale differences.
Working Fluid R-134a
The working fluid in a Rankine Cycle is central to its operation, acting as the medium through which thermal energy is converted to mechanical energy. In this instance, R-134a is the chosen fluid due to its favorable characteristics. R-134a is a hydrofluorocarbon (HFC) and is used extensively in refrigeration and air-conditioning systems. Its key properties make it suitable for the Rankine Cycle:
  • Low boiling point, allowing it to vaporize easily using moderate temperatures.
  • Non-flammable and relatively safe for handling.
  • Good thermodynamic efficiency within common operating conditions.
When used with geothermal energy, R-134a effectively carries the heat needed to drive turbine generators. Selecting the right working fluid impacts the cycle's performance and efficiency, ensuring optimal energy conversion.

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Most popular questions from this chapter

A \(15 \mathrm{~kg} / \mathrm{s}\) steady supply of saturated-vapor steam at \(500 \mathrm{kPa}\) is required for drying a wood pulp slurry in a paper mill (see Fig. P9.79). It is decided to supply this steam by cogeneration; that is, the steam supply will be the exhaust from a steam turbine. Water at \(20^{\circ} \mathrm{C}, 100 \mathrm{kPa}\) is pumped to a pressure of \(5 \mathrm{MPa}\) and then fed to a steam generator with an exit at \(400^{\circ} \mathrm{C}\). What is the additional heat transfer rate to the steam generator beyond what would have been required to produce only the desired steam supply? What is the difference in net power?

A closed FWH in a regenerative steam power cycle heats \(20 \mathrm{~kg} / \mathrm{s}\) of water from \(100^{\circ} \mathrm{C}, 20 \mathrm{MPa}\) to \(200^{\circ} \mathrm{C}, 20 \mathrm{MPa}\). The extraction steam from the turbine enters the heater at \(4 \mathrm{MPa}, 275^{\circ} \mathrm{C}\) and leaves as saturated liquid. What is the required mass flow rate of the extraction steam?

In an actual refrigeration cycle using \(\mathrm{R}-134 \mathrm{a}\) as the working fluid, the refrigerant flow rate is \(0.05 \mathrm{~kg} / \mathrm{s}\). Vapor enters the compressor at \(150 \mathrm{kPa},-10^{\circ} \mathrm{C}\) \(\left(h_{1}=394.2 \mathrm{~kJ} / \mathrm{kg}, s_{1}=1.739 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\right)\) and leaves at \(1.2 \mathrm{MPa}, 75^{\circ} \mathrm{C}\left(h_{2}=454.2 \mathrm{~kJ} / \mathrm{kg}, s_{2}=\right.\) \(1.805 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\) ). The power input to the nonadiabatic compressor is measured and found be \(2.4 \mathrm{~kW}\). The refrigerant enters the expansion valve at \(1.15 \mathrm{MPa}\) \(40^{\circ} \mathrm{C}(h=256.4 \mathrm{~kJ} / \mathrm{kg})\) and leaves the evaporator at \(160 \mathrm{kPa},-15^{\circ} \mathrm{C}(h=389.8 \mathrm{~kJ} / \mathrm{kg}) .\) Determine the entropy generation in the compression process, the refrigeration capacity, and the COP for this cycle.

A Rankine steam power plant should operate with a high pressure of 3 MPa and a low pressure of \(10 \mathrm{kPa}\), and the boiler exit temperature should be \(500^{\circ} \mathrm{C}\). The available high-temperature source is the exhaust of \(175 \mathrm{~kg} / \mathrm{s}\) air at \(600^{\circ} \mathrm{C}\) from a gas turbine. If the boiler operates as a counterflowing heat exchanger in which the temperature difference at the pinch point is \(20^{\circ} \mathrm{C},\) find the maximum water mass flow rate possible and the air exit temperature.

A Rankine cycle flows \(5 \mathrm{~kg} / \mathrm{s}\) ammonia at \(2 \mathrm{MPa}\), \(140^{\circ} \mathrm{C}\) to the turbine, which has an extraction point at \(800 \mathrm{kPa}\). The condenser is at \(-20^{\circ} \mathrm{C},\) and a closed FWH has an exit state (3) at the temperature of the condensing extraction flow and it has a drip pump. The source for the boiler is at constant \(180^{\circ} \mathrm{C}\). Find the extraction flow rate and state 4 into the boiler.

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