/*! 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 8 A gasoline engine takes in \(1.6... [FREE SOLUTION] | 91Ó°ÊÓ

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A gasoline engine takes in \(1.61 \times 10^{4} \mathrm{~J}\) of heat and delivers \(3700 \mathrm{~J}\) of work per cycle. The heat is obtained by burning gasoline with a heat of combustion of \(4.60 \times 10^{4} \mathrm{~J} / \mathrm{g}\). (a) What is the thermal efficiency of the engine? (b) How much heat is discarded in each cycle? (c) What mass of fuel is burned in each cycle? (d) If the engine goes through 60.0 cycles per second, what is its power output in kilowatts? In horsepower?

Short Answer

Expert verified
(a) 22.9%; (b) 12400 J; (c) 0.35 g; (d) 222 kW or 298 hp.

Step by step solution

01

Calculating Thermal Efficiency

Thermal efficiency, \( \eta \), is calculated using the formula \( \eta = \frac{W}{Q_{in}} \), where \( W \) is the work done per cycle and \( Q_{in} \) is the heat absorbed. Here, \( W = 3700 \text{ J} \) and \( Q_{in} = 1.61 \times 10^4 \text{ J} \). Thus, \( \eta = \frac{3700}{1.61 \times 10^4} \approx 0.229 \) or 22.9%.
02

Calculating Heat Discarded per Cycle

The heat discarded, \( Q_{out} \), is the difference between the heat absorbed and the work done: \( Q_{out} = Q_{in} - W \). Substituting the given values, \( Q_{out} = 1.61 \times 10^4 - 3700 = 1.24 \times 10^4 \text{ J} \).
03

Finding the Mass of Fuel Burned per Cycle

The mass of fuel burned, \( m \), can be found using the heat absorbed; \( Q_{in} = m \times \text{heat of combustion} \). Solving for \( m \), we have \( m = \frac{Q_{in}}{4.60 \times 10^4} \). Substituting, \( m = \frac{1.61 \times 10^4}{4.60 \times 10^4} \approx 0.35 \text{ grams} \).
04

Determining Power Output in Kilowatts and Horsepower

The power output \( P \) is given by \( P = \text{work done per cycle} \times \text{cycles per second} \). Hence, \( P = 3700 \times 60 = 2.22 \times 10^5 \text{ J/s} = 222 \text{ kW} \). To convert to horsepower (where 1 horsepower = 746 watts), \( P = \frac{222000}{746} \approx 298 \text{ horsepower} \).

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Key Concepts

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

Thermal Efficiency
Understanding thermal efficiency helps you evaluate how well an engine converts heat into work. It is a crucial parameter in thermodynamics for assessing engine performance. Thermal efficiency, denoted by \( \eta \), is calculated using the formula:
  • \( \eta = \frac{W}{Q_{in}} \)
where \( W \) represents the work output per cycle and \( Q_{in} \) stands for the heat input per cycle.
In the provided exercise, we are given \( W = 3700 \text{ J} \) and \( Q_{in} = 1.61 \times 10^4 \text{ J} \). Thus, substituting these values in the formula, we find that the thermal efficiency \( \eta \approx 0.229 \) or 22.9%.
This percentage means that around 22.9% of the input energy is converted into useful work, while the rest is lost as waste heat. Understanding this concept helps in the design and enhancement of engine performance, aiming for higher efficiency.
Heat Combustion
Heat of combustion plays a vital role in determining how much energy can be obtained from burning a specific quantity of fuel. In thermodynamics, it refers to the amount of heat released when a fuel fully combusts, which is crucial for calculating how much fuel an engine needs to produce a certain amount of energy.
  • The heat of combustion is given in the problem as \( 4.60 \times 10^4 \text{ J/g} \).
To find out how much fuel is burned per cycle, the formula \( Q_{in} = m \times \text{heat of combustion} \) is used, where \( m \) represents the mass of fuel. By rearranging and solving for \( m \), we calculate:
  • \( m = \frac{1.61 \times 10^4}{4.60 \times 10^4} \approx 0.35 \text{ grams} \).
Thus, approximately 0.35 grams of fuel is burned per engine cycle. This information is crucial for optimizing fuel consumption and reducing costs.
Power Output
Power output defines the rate at which work is performed or energy is converted in a system. In the context of engines, it’s a measure of the overall performance and is typically expressed in units like kilowatts (kW) or horsepower (hp).
Power output can be calculated using the formula:
  • \( P = \text{work per cycle} \times \text{cycles per second} \).
In the example, the engine performs \( 3700 \text{ J} \) of work per cycle and completes 60 cycles per second. To find the power output, multiply:
  • \( P = 3700 \text{ J} \times 60 = 2.22 \times 10^5 \text{ J/s} = 222 \text{ kW} \).
To convert to horsepower, knowing that 1 hp = 746 watts:
  • \( P = \frac{222000}{746} \approx 298 \text{ hp} \).
This reveals the engine delivers impressive power, critical for applications demanding high energy output.
Engine Cycle Analysis
Engine cycle analysis is a crucial aspect of thermodynamics, helping us to understand and evaluate engine performance comprehensively. It involves examining each component of energy input and output in a cycle to ascertain various characteristics, like efficiency and waste.
  • In practice, an engine cycle includes phases where fuel is combusted, work is done, and heat is expelled.
  • The analysis uses formulas to calculate values like thermal efficiency and power output.
For instance, in the provided problem, the engine absorbs \( 1.61 \times 10^4 \text{ J} \) of heat but only utilizes 22.9% of it for work. By determining the amount of heat discarded, \( Q_{out} = 1.24 \times 10^4 \text{ J} \), we understand that a significant portion of energy is lost.
Assessing how much fuel is consumed per cycle—here, 0.35 grams—also informs us about the efficiency and sustainability of the engine.
Through such analysis, engineers aim to design more efficient engines, minimizing losses and enhancing power.

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Most popular questions from this chapter

A Carnot engine operates between two heat reservoirs at temperatures \(T_{\mathrm{H}}\) and \(T_{\mathrm{C}}\). An inventor proposes to increase the efficiency of the engine by increasing both \(T_{\mathrm{H}}\) and \(T_{\mathrm{C}}\) by a factor of \(2 .\) Will this plan work? Why or why not?

A \(4.50 \mathrm{~kg}\) block of ice at \(0.00^{\circ} \mathrm{C}\) falls into the ocean and melts. The average temperature of the ocean is \(3.50^{\circ} \mathrm{C},\) including all the deep water. By how much does the melting of this ice change the entropy of the world? Does it make it larger or smaller? (Hint: Do you think that the ocean will change temperature appreciably as the ice melts?)

An aircraft engine has a heat efficiency of \(e=0.3 .\) It discards 6400 J each cycle. (a) How much heat is supplied to the engine each cycle? (b) How much work energy does the engine produce each cycle?

A solar water heater for domestic hot-water supply uses solar collecting panels with a collection efficiency of \(50 \%\) in a location where the average solar-energy input is \(200 \mathrm{~W} / \mathrm{m}^{2}\) If the water comes into the house at \(15.0^{\circ} \mathrm{C}\) and is to be heated to \(60.0^{\circ} \mathrm{C},\) what volume of water can be heated per hour if the area of the collector is \(30.0 \mathrm{~m}^{2} ?\)

A Carnot engine whose high-temperature reservoir is at \(620 \mathrm{~K}\) takes in \(550 \mathrm{~J}\) of heat at this temperature in each cycle and gives up \(335 \mathrm{~J}\) to the low-temperature reservoir. (a) How much mechanical work does the engine perform during each cycle? (b) What is the temperature of the low-temperature reservoir? (c) What is the thermal efficiency of the cycle?

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