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 refrigeration cycle having a coefficient of performance of 3 maintains a computer laboratory at \(18^{\circ} \mathrm{C}\) on a day when the outside temperature is \(30^{\circ} \mathrm{C}\). The thermal load at steady state consists of energy entering through the walls and windows at a rate of \(30,000 \mathrm{~kJ} / \mathrm{h}\) and from the occupants, computers, and lighting at a rate of \(6000 \mathrm{~kJ} / \mathrm{h}\). Determine the power required by this cycle and compare with the minimum theoretical power required for any refrigeration cycle operating under these conditions, each in \(\mathrm{kW}\).

Short Answer

Expert verified
3.33 kW vs 0.41 kW

Step by step solution

01

Understand the Coefficient of Performance (COP)

The Coefficient of Performance (COP) of a refrigeration cycle is given by \[ \text{COP} = \frac{Q_L}{W} \]where \( Q_L \) is the heat removed from the cooled space, and \( W \) is the work input. The COP is given as 3 in this problem.
02

Calculate Total Thermal Load

The total thermal load, \( Q_L \), is the sum of energy entering through walls and windows and the energy from occupants, computers, and lighting. This is given as: \[ Q_L = 30000 \frac{\text{kJ}}{\text{h}} + 6000 \frac{\text{kJ}}{\text{h}} = 36000 \frac{\text{kJ}}{\text{h}} \]Convert this to kW: \[ Q_L = \frac{36000}{3600} \text{ kW} = 10 \text{ kW} \]
03

Determine Actual Power Required

Using the COP definition, the actual power required by the refrigeration cycle is given by \[ W = \frac{Q_L}{\text{COP}} \]Substituting the values, \[ W = \frac{10 \text{ kW}}{3} = 3.33 \text{ kW} \]
04

Calculate the Minimum Theoretical Power

The minimum theoretical power required for any refrigeration cycle is determined using the Carnot COP, which is given by \[ \text{COP}_{\text{Carnot}} = \frac{T_L}{T_H - T_L} \]where \( T_L \) is the absolute temperature of the cold reservoir (18°C) and \( T_H \) is the absolute temperature of the hot reservoir (30°C). Convert these temperatures to Kelvin: \[ T_L = 18 + 273 = 291 \text{ K} \]\[ T_H = 30 + 273 = 303 \text{ K} \]Then the Carnot COP is: \[ \text{COP}_{\text{Carnot}} = \frac{291}{303 - 291} = \frac{291}{12} = 24.25 \]The minimum theoretical power is \[ W_{\text{min}} = \frac{Q_L}{\text{COP}_\text{Carnot}} = \frac{10 \text{ kW}}{24.25} = 0.41 \text{ kW} \]
05

Compare the Powers

Compare the actual power required to the minimum theoretical power: - Actual power required: 3.33 kW - Minimum theoretical power: 0.41 kW

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!

Key Concepts

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

Coefficient of Performance (COP)
The Coefficient of Performance, or COP, is a crucial parameter in refrigeration systems. It measures the efficiency of a refrigeration cycle by comparing the amount of heat removed from the cooled space to the work input required to remove it. Mathematically, it is expressed as: \( \text{COP} = \frac{Q_L}{W} \)
where \( Q_L \) is the heat removed from the cooled space, and \( W \) is the work input. The higher the COP, the more efficient the refrigeration system.
In our problem, the COP is given as 3. This means that for every unit of work input, three units of heat are removed from the cooled space. This simple equation helps us understand how well the refrigeration system uses energy to maintain the desired temperature.
Thermal Load Calculation
Thermal load calculation involves determining the total amount of heat that needs to be removed from a space to maintain a specific temperature. In our exercise, the thermal load consists of energy entering through the walls and windows, as well as the energy generated by occupants, computers, and lighting.
To find the total thermal load \( Q_L \), we sum these individual heat loads:
\( Q_L = 30000 \frac{ \text{kJ}}{ \text{h}} + 6000 \frac{ \text{kJ}}{ \text{h}} = 36000 \frac{ \text{kJ}}{ \text{h}} \)
It's often useful to convert the thermal load from kJ/h to kW by dividing by 3600 (the number of seconds in an hour):
\( Q_L = \frac{36000}{3600} \text{ kW} = 10 \text{ kW} \)
This total thermal load is crucial for designing the cooling system and determining the power required to maintain the desired temperature.
Carnot COP
The Carnot Coefficient of Performance (COP) represents the highest possible efficiency for a refrigeration cycle operating between two temperatures. It's derived from the Second Law of Thermodynamics and is a benchmark for the theoretical limit of efficiency. The formula for Carnot COP is: \( \text{COP}_{\text{Carnot}} = \frac{T_L}{T_H - T_L} \)
Here, \( T_L \) is the absolute temperature of the cold reservoir and \( T_H \) is the absolute temperature of the hot reservoir. Remember to convert temperatures to Kelvin by adding 273. For instance, for our problem:
  • \( T_L = 18^{\circ} \mathrm{C} + 273 = 291 \text{ K} \)
  • \( T_H = 30^{\circ} \mathrm{C} + 273 = 303 \text{ K} \)
Plugging these values into the formula gives us: \( \text{COP}_{\text{Carnot}} = \frac{291}{303 - 291} = \frac{291}{12} = 24.25 \) This means that, theoretically, for every unit of work input, 24.25 units of heat can be removed from the cooled space. Using this ideal COP, we can calculate the minimum theoretical power required: \( W_{\text{min}} = \frac{ Q_L}{ \text{COP}_{\text{Carnot}} } = \frac{10 \text{ kW}}{24.25} = 0.41 \text{ kW} \)
Comparing this with the actual power required (3.33 kW) helps us understand the efficiency gap between practical and ideal systems.

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 refrigeration cycle operating between two reservoirs receives energy \(Q_{\mathrm{C}}\) from a cold reservoir at \(T_{\mathrm{C}}=280 \mathrm{~K}\) and rejects energy \(Q_{\mathrm{H}}\) to a hot reservoir at \(T_{\mathrm{H}}=320 \mathrm{~K}\). For each of the following cases determine whether the cycle operates reversibly, irreversibly, or is impossible: (a) \(Q_{\mathrm{C}}=1500 \mathrm{~kJ}, W_{\text {cycle }}=150 \mathrm{~kJ}\). (b) \(Q_{\mathrm{C}}=1400 \mathrm{~kJ}, Q_{\mathrm{H}}=1600 \mathrm{~kJ}\). (c) \(Q_{\mathrm{H}}=1600 \mathrm{~kJ}, W_{\text {cycle }}=400 \mathrm{~kJ}\). (d) \(\beta=5\).

The preliminary design of a space station calls for a power cycle that at steady state receives energy by heat transfer at \(T_{\mathrm{H}}=600 \mathrm{~K}\) from a nuclear source and rejects energy to space by thermal radiation according to Eq. 2.33. For the radiative surface, the temperature is \(T_{\mathrm{C}}\), the emissivity is \(0.6\), and the surface receives no radiation from any source. The thermal efficiency of the power cycle is one- half that of a reversible power cycle operating between reservoirs at \(T_{\mathrm{H}}\) and \(T_{\mathrm{C}}\) - (a) For \(T_{\mathrm{C}}=400 \mathrm{~K}\), determine \(\dot{W}_{\text {cycle }} / \mathrm{A}\), the net power developed per unit of radiator surface area, in \(\mathrm{kW} / \mathrm{m}^{2}\), and the thermal efficiency. (b) Plot \(\dot{W}_{\text {cycle }} / \mathrm{A}\) and the thermal efficiency versus \(T_{\mathrm{C}}\), and determine the maximum value of \(\dot{W}_{\text {cycle }} / \mathrm{A}\). (c) Determine the range of temperatures \(T_{\mathrm{C}}\), in \(\mathrm{K}\), for which \(\dot{W}_{\text {cycle }} / \mathrm{A}\) is within 2 percent of the maximum value obtained in part (b). The Stefan-Boltzmann constant is \(5.67 \times 10^{-8} \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}^{4}\).

If the thermal efficiency of a reversible power cycle operating between two reservoirs is denoted by \(\eta_{\max }\), develop an expression in terms of \(\eta_{\max }\) for the coefficient of performance of (a) a reversible refrigeration cycle operating between the same two reservoirs. (b) a reversible heat pump operating between the same two reservoirs.

A method for generating electricity using gravitational energy is described in U.S. Patent No. \(4,980,572\). The method employs massive spinning wheels located underground that serve as the prime mover of an alternator for generating electricity. Each wheel is kept in motion by torque pulses transmitted to it via a suitable mechanism from vehicles passing overhead. What practical difficulties might be encountered in implementing such a method for generating electricity? If the vehicles are trolleys on an existing urban transit system, might this be a cost-effective way to generate electricity? If the vehicle motion were sustained by the electricity generated, would this be an example of a perpetual motion machine? Discuss.

Write a paper outlining the contributions of Carnot, Clausius, Kelvin, and Planck to the development of the second law of thermodynamics. In what ways did the now-discredited caloric theory influence the development of the second law as we know it today? What is the historical basis for the idea of a perpetual motion machine of the second kind that is sometimes used to state the second law?

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