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(II) An inventor claims to have built an engine that produces 2.00 MW of usable work while taking in 3.00 MW of thermal energy at 425 K, and rejecting 1.00 MW of thermal energy at 215 K. Is there anything fishy about his claim? Explain.

Short Answer

Expert verified

Yes, there is something fishy about the claim of the inventor since the engine’s real efficiency is more than its ideal efficiency.

Step by step solution

01

Understanding the efficiency of the engine

The ratio of the work done by the engine to the heat input at high temperature is termed the efficiency of the engine.

The expression for the efficiency is given as:

\(e = \frac{W}{{{Q_{\rm{H}}}}} = 1 - \frac{{{Q_{\rm{L}}}}}{{{Q_{\rm{H}}}}}\) … (i)

Here, W is the work done, \({Q_{\rm{H}}}\) is the heat input at high temperature, and \({Q_{\rm{L}}}\) is the heat exhausted at low temperature.

02

Given data

The work produced by the engine is \(W = 2\;{\rm{MW}}\).

The intake thermal energy is \({Q_1} = 3\;{\rm{MW}}\).

The initial temperature is \({T_1} = 425\;{\rm{K}}\).

The final temperature is \({T_2} = 215\;{\rm{K}}\).

The rejected thermal energy is \({Q_2} = 1\;{\rm{MW}}\).

03

Evaluation of the real efficiency of the engine

The real efficiency of the engine is given by:

\(e = \frac{W}{{{Q_1}}}\)

Substitute the values in the above expression.

\(\begin{array}{l}e = \left( {\frac{{2\;{\rm{MW}}}}{{3\;{\rm{MW}}}}} \right)\\e = 0.66 \times 100\% \\e = 66\% \end{array}\)

04

Evaluation of the ideal efficiency of the engine

The relation of ideal efficiency is given by:

\({e_{\rm{i}}} = 1 - \frac{{{T_1}}}{{{T_2}}}\)

Substitute the values in the above expression.

\(\begin{array}{l}{\eta _{\rm{i}}} = 1 - \left( {\frac{{215\;{\rm{K}}}}{{425\;{\rm{K}}}}} \right)\\{\eta _{\rm{i}}} = 0.49 \times 100\% \\{\eta _{\rm{i}}} = 49\% \end{array}\)

The engine made by the inventor is not possible because the engine’s real efficiency is more than its ideal efficiency. Thus, there is something fishy about his claim.

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Most popular questions from this chapter

Question: (II) Consider the following two-step process. Heat is allowed to flow out of an ideal gas at constant volume so that its pressure drops from 2.2 atm to 1.4 atm. Then the gas expands at constant pressure, from a volume of 5.9 L to 9.3 L, where the temperature reaches its original value. See Fig.15–22. Calculate (a) the total work done by the gas in the process, (b) the change in internal energy of the gas in the process, and (c) the total heat flow into or out of the gas.

What is the change in entropy of\({\bf{1}}{\bf{.00}}\;{{\bf{m}}{\bf{3}}}\)water at 0°C when it is frozen to ice at 0°C?

Question: (II) (a) What is the coefficient of performance of an ideal heat pump that extracts heat from 6°C air outside and deposits heat inside a house at 24°C? (b) If this heat pump operates on 1200 W of electrical power, what is the maximum heat it can deliver into the house each hour? See Problem 35.

Question: An ideal heat pump is used to maintain the inside temperature of a house at \({T_{{\rm{in}}}} = 22{\rm{^\circ C}}\) when the outside temperature is \({T_{{\rm{out}}}}\). Assume that when it is operating, the heat pump does work at a rate of 1500 W. Also assume that the house loses heat via conduction through its walls and other surfaces at a rate given by \(\left( {650\;{{\rm{W}} \mathord{\left/

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Refrigeration units can be rated in “tons.” A 1-ton air conditioning system can remove sufficient energy to freeze 1 ton (2000 pounds = 909 kg) of 0°C water into 0°C ice in one 24-h day. If, on a 35°C day, the interior of a house is maintained at 22°C by the continuous operation of a 5-ton air conditioning system, how much does this cooling cost the homeowner per hour? Assume the work done by the refrigeration unit is powered by electricity that costs $0.10 per kWh and that the unit’s coefficient of performance is 18% that of an ideal refrigerator.\({\bf{1}}\;{\bf{kWh = 3}}{\bf{.60 \times 1}}{{\bf{0}}{\bf{6}}}\;{\bf{J}}\).

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