A Carnot air conditioner takes energy from the thermal energy of a room at 70°Fand transfers it as heat to the outdoors, which is at 96°F. For each joule of electric energy required to operate the air conditioner, how many joules are removed from the room?

Short Answer

Expert verified

The number of joules removed from the room to operate the air conditioner is 20.36 J

Step by step solution

01

The given data 

Temperatures,TL=70°F=294.26Kand

TH=96°F=308.71K

It is given that QH=THand QL=TL

02

Understanding the concept of the Carnot engine

We apply the concept of conservation of energy in the formula for the coefficient of performance of the Carnot engine to find the amount of heat in joules removed from the room.

Formula:

The formula for the coefficient of performance of a Carnot Engine,

K=TLTH-TL (1)

The work done per cycle of a Carnot Engine,

Win=QH-QL (2)

03

Calculation of the number of joules to be removed from the room

Using equation (1), the coefficient of performance of the Carnot air conditioner is given as:

K=294.26K308.71K-294.26K=20.36

But, QH=THandQL=TL

Using equation (2) in equation (1) and the above-given values, we get that

K=QLQH-QL=QLW

QL=K×W=20.361.0J=20.36J

Therefore, the amount of heat in joules removed from the room is 20.36 J

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Most popular questions from this chapter

Point i in Fig. 20-19 represents the initial state of an ideal gas at temperature T. Taking algebraic signs into account, rank the entropy changes that the gas undergoes as it moves, successively and reversibly, from point i to pointsa, b, c, and d, greatest first.

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(a) A Carnot engine operates between a hot reservoir at 320 Kand a cold one at 260 K. If the engine absorbs 500 Jas heat per cycle at the hot reservoir, how much work per cycle does it deliver? (b) If the engine working in reverses functions as a refrigerator between the same two reservoirs, how much work per cycle must be supplied to remove 1000Jas heat from the cold reservoir?

An inventor has built an engine X and claims that its efficiency X is greater than the efficiency of an ideal engine operating between the same two temperatures. Suppose you couple engine X to an ideal refrigerator (Fig. 20-34a) and adjust the cycle of engine X so that the work per cycle it provides equals the work per cycle required by the ideal refrigerator. Treat this combination as a single unit and show that if the inventor’s claim were true(ifεx>ε), the combined unit would act as a perfect refrigerator (Fig. 20-34b), transferring energy as heat from the low-temperature reservoir to the high-temperature reservoir without the need for work.

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